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Preliminary Draft Evaluation of Control Sys Failures Leading to RCS Overcooling in Oconee 1 Power Plant. NUREG/CR-3692, Possible Modes of Steam Generator Overfill Resulting from Control Sys Malfunctions... Encl
ML20151K219
Person / Time
Site: Oconee Duke Energy icon.png
Issue date: 04/24/1984
From: Mcbride A
SCIENCE APPLICATIONS INTERNATIONAL CORP. (FORMERLY
To:
NRC OFFICE OF NUCLEAR REGULATORY RESEARCH (RES)
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ML20151K225 List:
References
CON-FIN-B-0467, CON-FIN-B-467, RTR-NUREG-CR-3692 NUDOCS 8406270390
Download: ML20151K219 (590)


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i PREllMINARY DRAFT Instrumentation and Controls Division EVALUATION OF CONTROL SYSTEM FAILURES LEADIBC TO REACTOR COOLANT SYSTEM OVERCOOLING IN THE OCONEE-1 POWER PLANT Arthur F. McBride*

Manuscript Completed: April 24, 1984 CScience Applications, Inc., Oak Ridge, TN Prepared for the Division of Facility Operations Office of Nuclear Regulatory Research U.S. Nuclear Regulatory Commission Under Interagency Agreement 40-550-75 NRC Fin No. B0467 Oak Ridge National Laboratory Oak Ridge, Tennessee 37831 operated by Martin Marietta Energy Systems, Inc.

for the U.S. DEPARTMENT OF ENERGY under Contract No. W-7405-eng-26 PREllMINARY ORAFT 8406270390 840424 PDR ADOCK 05000269 P

PDR

l TABLE OF CollTENTS Section

2agg, LIST OF TABIES

. iii

1.0 INTRODUCTION

1 1.1 Sackground 1

1.2 Objective and Approach i'

13 Scope.

2 2.0

SUMMARY

OF RESULTS.

4 30 SELECTION OF SYSTEMS FOR ANALYSIS 14 3.1 Oconee 1 Systems List.

14 32 Systems Affecting the Reactor Coolant System 15 3.3 Systems Affecting Reactor Coolant System Overcooling 26 4.0 SYSTEM DESCRIPTIONS 40 4.1 Nuclear Systems........................

40 4.2 Power Conversion Systems 50 43 Process Auxiliary Systems..........

58 5.0 FMEA 0F SELECTED SYSTEMS.

62 5.1 Nuclear Systems.

63 5.2 Power Conversion Systems 74 53 Process Auxiliary Systems..........

90

6.0 REFERENCES

92 APPENDIX A - OCONEE 1 SYSTEMS NOT SELECTED FOR RCS OVERC00 LING ANALYSIS.

. A-1 APPENDIX B - OCONEE 1 POWER CONVERSION SYSTEMS PROCESS AND INSTRUMENT DIAGRAMS

. B-1 APPENDIX C - OCONEE 1 POWEP CONVERSION SYSTEMS FAILURE MODES AND EFFECTS ANALYSIS TABLES

. C-1 ii l

LIST OF TABLES Table I.aga 2.1 Summary of Potentially Significant RCS Overcooling Failure Modes.............

6 31 Oconee 1 Nuclear Systems (Nxx) 16 32 Oconee 1 Engineered Safeguards Systems (Sxx) 17 33 Oconee 1 Reactor Building / Containment Systems (Cxx) 18 3.4 Oconee 1 Power Conversion Systems (Pxx) 19 35 Oconee 1 Process Auxiliary Systems (Wxx) 20 3.6 Oconee 1 Plant Auxiliary Systems (Xxx) 21 3.7 First Order Reactor Coolant System Interfaces.

23 3.8 Second Order Reactor Coolant System Interfaces 24 39 overcooling Characteristics and Potential Initiating Causes 27 3 10 Potential Impacts of First and Second Order Reactor l

Coolant System Interface Systems on RCS Overcooling.

36 5.1 Summary of RCS Subsystem Failure Modes 64 5.2 Summary of Pressuriser System FMEA: Failures Leading to or Affecting RCS Overcooling Transients 65 53 FMEA of RC Pumps:

Failures Leading to or Affecting RCS Overcooling Transients 71 5.4 FMEA of Steam Generators: Failures Leading to or Affecting RCS Overcooling Transients 72 5.5 Summary of Main Steam and Turbine Bypass FMEA:

Failures Leading to or Affecting RCS Overcooling.

75 5.6 Summary of Condensate and Main Feedwater FMEA:

Failures Leading to or Affecting RCS Overcooling Transients 82 57 Summary of Makeup and Purification System FMEA:

Failures Leading to or Affecting RCS Overcooling Transients 91 l

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1.0 IETRODUCTION

1.1 BACKGROUND

The implications of failures of safety systems on nuclear power plant safety have been studied extensively.

Currently, the safety implications of control system failures in nuclear power plants are being investigated by the Oak i

Ridge National Laboratory.

A major task in this effort is the preparation of Failure Modes and Effects Analyses (FMEA) of plant systems to aid in the analysis of control system malfunctions and identification of possible consequences to safety.

Specifically, the studies are directed at identifying i

failures and scenarios contributing to reactor coolant overcooling, reactor coolant undercooling, steam generator overfilling or degradation of the ability of safety systems to respond on demand.

This work is conducted for Nuclear Regulatory Commission (NRC) under FIN B0467, Safety Implications of Control Systems.

It supports Unresolved Safety Issue A-47.

The purpose of this analysis is to evaluate whether nuclear power plant control systems, either operating as designed or with postulated malfunctions, may interfere with the action of safety systems or may put the plant into a failed state beyond the protection of the safety systems. The effort at Oak Ridge National Laboratory (ORNL) is limited to the study of Babcock and Wilcox Co. and Combustion Engineering Co. Nuclear Steam Supply Systems (NSSS).

NSSS's produced by other vendors are under study at INEL.

The study is intended to be generic by vendors.

However, it is recognized that, for a study of this sort, detailed and realistic plant design information is essential.

Data from two operating plants iere used to represent designs of the two vendors. The Oconee unit 1 and Calvert Cliffs unit 1 plant designs were selected to represent, respectively, Babcock and Wilcox and Combustion Engineering. Although the thrust of the study as a whole is generic, some elements of the study may be plant specific.

A number of other activities supported. by NRC are rei+.ed to this analysis or have provided information related to this work.

Included among them are:

1.

Plant Electrical System Evaluation, FIN B0816.

2.

Evaluation of Pressurized Thermal Shock, FIN B0468.

1

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3 Precursors to Potential Severe Core Damage Accidents, FIN B1583 4.

In Plant Reliability Data Base for Nuclear Plant Components, FIN B0445.

5.

System Interactions in Nuclear Power Plants, FIN B0789.

The general approach to this problem at ORNL is twofold:

the development of a hybrid computer model for simulation of the Oconee 1 Nuclear Power Plant, and a Failure Modes and Effects Analysis (FMEA) based principally on plant design and procedure information, to identify scenarios which may lead to control system initiated plant failures.

The plant simulation will quantitatively predict the respc-.ses of the plant control systems to the identified scenarios. The simulation will examine in detail important cases generated in the FMEA.

The simulation methodology and results will be described fully in other reports.

The FMEA, as it relates to the overcooling of the Reactor Coolant System (RCS), is the subject of this report.

1.2 OBJECTIVE AND APPROACH The objective of this study is to identify control system failures which can contribute to reactor coolant overcooling. The approach to achieving this objective consists of three steps:

1.

Identify those systems which have interfaces with the reactor coolant and can impact the overcooling transient.

2.

Conduct a detailed FMEA of those systems to identify specific system malfunctions and consequences to safety.

3 Based on the identified failures, develop scenarios which could lead to the reactor coolant overcooling transients.

This approach and the results of its application to the Oconee 1 nuclear plant tre presented in this report.

13 SCOPE Although the objectives of the broad study are generic, specific nuclear power plant systems' designs are required for the preparation of a detailed FMEA.

2

For this reason, the FMEA is being performed on systems of the Oconee Nuclear Power Station selected as pertinent to overcooling transients.

This report summarizes the results of previous FMEAs and documents the results for system.'

not previously analyzed.

t The major results of the study are summarized in Section 2.0.

Selection of systems for detailed analysis is discussed in Section 3 0.

Brief system descriptions of the selected systems and interfacing support systems are described in Section 4.0.

The FMEA methodology and analysis results are described in Section 5.0.

i

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3

2.0 SUBSt&RY OF RESULTS i

An analysis to identify control system failures leading to reactor coolant system (RCS) overcooling has been performed on the Oconee Nuclear Station design.

Due to the large number of systems and components comprising a nuclear power station, a syster.atic procedure was developed to identify and analyze these plant systems:

1.

Specifically define RCS overcooling for purposes of the i

analysis.

2.

Identify the Oconee plant systems and system-to-system interfaces.

3 Select the systems which could contribute to RCS overcooling based on an analysis of systems' functions and interfaces, i

4.

Perform failure modes and effects analysis (FMEA) to identify i

component level failure modes leading to RCS overcooling.

1 The purpose of this analysis, as noted in Section 1, is the identification of plant control system failure modes that might lead to RCS overcooling.

A number of failure modes have been identified (and are presented in Section 5) which could cause the RCS temperature to decrease. The rate and amount of such decreases and its possible subsequent effects cannot be determined without simulation of the system's response to the control system failures.

RCS overcooling is not of interest in this study until it approaches an amount which can have safety implications.

Cooling associated with normal shutdown procedures within Technical Specifications is of no concern.

1 Any condition that causes RCS temperature to drop 1000F or more in an hour is considered to be overcooling. Also, tentatively, RCS cooling to a degree that causes system variables to assume values that should cause ESPS - actuation is considered overcooling.

Until plant behavior has been simulated, the proposed control system failures which meet these conditions cannot be determined.

Therefore, additional less restrictive criteria have been followed in proposing failure sequences to onsure.that potentially significant sequences-would not be excluded prematurely. The selection criteria were accordingly expanded to include 4

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transients whose post reactor trip development might include unusual decreases in RC pressure and inventory as well as temperature (see Section 3 3).

j To aid in subsequent analyses, the overcooling criteria were related to RCS transient behavior characteristics.

The analagous RCS characteristics defined were a release of reactor coolant from the RCS, opening the pressurizer spray valve and increased heat transfer through the steam generator tubes.

Based on the RCS overcooling criteria and the systems' function and interface analysis, a number of key plant systems and subsystems were selected for the FMEA. They were the pressurizer, steam generator, and reactor coolant (RC) pump subsystems of the RCS; the condensate and main feedwater system, the main steam and turbine bypass system and the makeup and purification system.

The control instrumentation and required supporting systems for these fluid systems were analyzed as an integral part of the fluid systems selected.

4 l

The results of the FMEA's of the selected systems are presented in detail in Tables 5.1 through 5.7.

The failure modes judges to be potentially significant have been summarized in Table 2.1.

The failure modes are listed by RCS overcooling category:

Release of Reactor Coolant, Pressurizer Spray Valve Opens and Increased Heat Transfer Through Steam Generators.

A fourth category has been added to identify failure modes resulting in multiple RCS overcooling effects.

As part of the FMEA's, potentially undetected failures which could increase the severity of the effects of the overcooling transients have been identified. The effects of significant undetected failures in combination with the initiating failures have been identified in Table 2.1.

Transients which lead to release of reactor coolant transient may be initiated by a failed open pilot operated relief valve (PORV), failure of an RC pump's seals and steam generator tube ruptures. Once identified, an open PORV may be isolated by manual closure of the PORY block valve.

Tube rupture and seal failures cannot be isolated. Although these transients are not expected to result from any particular control system failure, each could result from a 5

TABLE 2.1.

SUletARY OF POTENTIALLY SIGNIFICANT BCS OVERC00 LING FAILURE MODES Failure Potential Effects on RCS Remedial Actions Available Release of Reactor Coolant 1.

Pilot Operated Relief Valve Small Loss of Coolant Accident Follow emergency procedures for (PORV) Fails Open or Fails (LOCA).

RCS pressure and temperature small LOCA.

Identify the open PORV to Close (Failure of a decrease in response to the loss of and close the PORY block valve.

pressurizer code safety valve reactor coolant.

Pressurizer fills.

Reestablish RCS pressure, to close after opening Autoeatic Engineered Safeguards temperture and pressurizer level, initiates o similar transient)

System (ESPS) actuation of High Pressure Injection (HPI) at 1500 psi RCS pressure.

The transient would be complicated by undetected failures of the PORV accoustic monitor or discharge line thermocouples.

An undetected " low" failure of a selected operate range steam generator level as transmitter would result in a steam generator overfill transient following the procedurally required RC pump trip unless manually terminated by the operator.

2.

Failure of RC Pump Seals Small LOCA.

Pressurizer empties.

If possible, trip affected RC pump Automatic Engineered Safeguards Sys?,em prior to seal failure and achieve (ESPS) actuation of High Pressure cold shutdown. Once seal failure Injection (HPI) at 1500 psi RCS occurs, follow emergency procedures pressure.

An undetected " low" failure for small LOCA's.

of a selected operate range steam generator level transmitter would result in a steam generator overfill following the procedurally required RC pump trip unless manually terminated by the operator.

TABLE 2.1.

SERetARY OF POTENTIALLY SIGNIFICANT RCS OVERCOOLING FAILURE MODES (Continued)

Failure Potential Effects on RCS Remedial Actions Available 3

-Steam Generator Tube Rupture Small LOCA.

Pressurizer empties.

Follow emergency procedures of a Automatic ESPS actuation of HPI.

steam generator tube rupture.

Rapid cooldown and depressurization of RCS manually initiated to terminate release of reactor coolant to condenser and environment.

An undetected " low" failure of a selected operate range steam generator level transmitter would result in a steam generator overfill transient following the procedurally required RC pump trip unless manually terminated by the operator.

u Pressurizer Sorav Valve Ooens 4.

Pressurizer Spray Valve Fails Slow depressurization of RCS.

Rate Identify open valve and close spray Open or Fails to Close of depressurization limited by block valve.

automatic actuation of pressurizer heaters.

The transient would be complicated by an undetected failure of the pressurizer spray block valve.

TABLE 2.1.

SINGtARY OF POTENTIALLY SIGNIFICANT RCS OVERC00 LING FAILURE MODES (Continued)

Failure Potential Effects on RCS Remedial Actions Available i

Increased Heat Transfer Through Steam Generators 5.

Turbine Bypass Valves on Either Depending on the response of the Identify the open valves and Steam Generator Fail Open or turbine and reactor, an RCS cooldown manually close the turbine bypass Fail to Close (Failure of a and depressurization transient could valves or their isolation valve.

main steam code safety valve occur following reactor trip.

A to close following turbine trip failed "high" steam line pressure initiates a similar transient) transmitter causing the transient could be confusing to the operator and delay remedial action.

An undetected failure of the associated isolation valve may present isolation depending on the cause of the open turbine bypass valves.

If the RC pumps were tripped in response to an ESPS signal, an undetected " low" failure of a selected operate range steam ger.arator level transmitter would result in a steam generator overfill transient following the procedurally required RC pump trip unless manually terminated by the operator.

6.

Main Turbines Fail to Trip RCS cooldown and depressurization Attempt to manually trip or Following Reactor Trip transient occurs.

If the RC pumps throttle the high or low pressure were tripped in response to an ESPS turbines. Throttle feedwater if signal, an undetected " low" failure required to control RCS of a selected operate range steam depressurization.

generator level transmitter would result in a steam generator overfill transient following the procedurally required RC pump trip unless manually terminated by the operator.

TABLE 2.1.

Smet&RY OF POTENTIALLY SIGNIFICANT BCS OVERC00 LING FAILURE IIDDES (Cantinued)

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Failure Potential Effects on RCS Remedial Actions Available 7

Main Feedvater Control Valves Following reactor trip, rapidly Identify the open valves arm Fail Open or Fail to Close increasing steam generator level (s) manually throttle or trip the main Following Reactor Trip expected to result in RCS cooldown feedwater pumps.

1 and depressurization.

Transient expected to be terminated by a manual or automatic trip of the main feedwater pumps. If the transient were initiated by a crack in the lower steam generator startup range level transmitter level tap, the emergency feedwater system would continue to fill the affected steam generator following main feedwater pump trip.

An undetected failure of the e

automatic high level trip circuit would result in continued main feedwater overfill unless the pumps are manually tripped by the operator.

i Cambined Effect Failures I

i 8.

Pressuriser Pressure Circuit PORV and spray valve open and Identify spurious pressure signal 1

Fails High pressurizer heaters deenergized, and manually control PORV, spray Transient expected to be similar to valve and pressurizer heaters.

"PORV Fails Open," Transient 1, 3

complicated by the indicated and alarmed high RCS pressure.

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TABLE 2.1.

m mY OF FOTENTIALLY SIGNIFICANT RCS OtESC00 LING FAILDRE MODES (Coltint:ed)

Failure Potential Effects on RCS Remedial Actions Available 9.

ICS Panelboard II Branch HEI Depending on manual selection of Identify power failure and manually or HET Fail pressurizer level, steam generator control steam generator and startup level and steam pressure pressurizer level.

If required, transmitters, one or both steam manually trip main feedwater pumps.

generators and the pressurizer may t,e overfilled. Steam generator overfill expected to be automatically terminated by a high level trip of the main feedwater pumps unless an undetected failure of the trip circuit existed.

Pressurizer overfill can be manually terminated. Spurious low steam ges.erator and pressure indications and alarms may delay o

manual remedial actions.

10.

ICS Pamelboard KI Branch H Turbine bypass valves and main Identify power failure and manually or R1 (Auto Power) Fails feedvater control valves transfer to throttle feedwater control and Following a Turbine Trip manual and remain in position. Since turbine bypass valves. Manually Transiest both the turbine bypass and feedwater trip main feedwater pumps if control valves may be open, a required.

combined steam generator depressurization and overfeed transient could occur. Steam generator overfeed automatically terminated by a high level feedwater pump trip unissa the trip circuit was in an undetected failed state. The many spurious alarms and indications may delay manual remedial actions.

Eequence of improper control actions over a period of time.

As such, they have been retained as examples of unisolable LOCA's.

The overcooling effects of a failed open pressurizer spray valve are not oxpected to be significant with respect to other failure categories.

This failure has been retained as an example of this category of overcooling transient.

Failures resulting in increased steam generator heat transfer fell into two tub-categories:

those initiating steam generator depressurization and those initiating steam generator main feedwater overfeed.

Steam generator depressurization is expected, following reactor trip, due to the turbine bypass valves failing open or a failure of the main turbine to trip on demand.

With the exception of a postulated failure of one common setpoint module, the failures affecting the turbine bypass valves resulted only in the steam generator A or steam generator B turbine bypass valves failing open but not both.

An open failure of one of the two sets of valves could result in a consequential reactor and turbine trip.

However, defining the specific effects of these failures will require transient simulation. Once the reactor is tripped, however, RCS overcooling is expected unless the steam generator depressurization is terminated manually.

Failure to trip the turbine following reactor trip has been identified as a transient resulting in steam generator depressurization.

However, due to the unavailability of turbine control instrumentation design, specific turbine trip failure modes could not be identified in detail.

Failure of the reactor trip input signal was identified and could result in some degree of RCS cvercooling; the specific response of the turbine controls to this failure in conjunction with other ICS control inputs could not be specified.

The turbine trip failure has been retained as an example of a potentially large steam generator depressurization transient induced by control failures.

One or both main feedwater control valves failing open or failing to close will result in steam generator overfill and potentially significant RCS cvercooling following reactor trip.

The specific effect of a feedwater control valve opening while the reactor is at power will require transient 11 1

cimulatiom (For instance, if the high steam generator feedwater pump trip ccourred prior to reactor trip, RCS overcooling would not ce expected.)

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The steam generator overfill transients are expected fp be automatically terminated by the high steam generator level main feedwate!r pump trip circuit.

Two failure modes have been identified resulting in coltirued overfeed.

If the steam generator startup level transmitter sensing line developed a cignificant crack, the spurious low transmitter level signal would initiate steam generator overfeed.

If the feedwater pumps were tripped on high steam generator (operate range) level, the emergency feedwater system would be tutomatically started. Since the main feedwater and emergency feedwater level transmitter have a common sensing line, the overfill would be continued by the cpurious low level signal to the emergency feedwater controls.

The second failure mode involves a failure of the high level main feedwater pump trip circuit. Should this circuit fail, no immediate impact on plant cperation may occur and the failure may remain undetected.

In this state, an cverfeed transient initiated by a feedwater control valie failing open or failing to close would not be automatically tereinated.

If the steam generator was allowed to fill, the injection of significant quantities of water into the steam lines could result in damage to the safety valves, the turbine bypass valves, the steam lines, and their supports in addition to initial RCS overcooling.

Three failure modes were identified which resulted in more than one effect on the RCS. Failure of the RCS narrow range pressure signal would result in both the PORY and spray valves opening and deenergizing the pressurizer heaters.

The differences between this transient and the effects of the open PORV alone tre not expected to be significant.

Two failure modes resulting from failures of ICS Panelboard KI branch circuits have been identified as having multiple effects.

The redundant pressurizer level, steam generator level and steam pressure transmitters are powered from branch circuits HEX and HEY. One of the redundant transmitters is selected canually for each parameter for input to the control circuitry.

Based on the transmitter selection, a single failure of branch circuit HEX or HEY may 12

c:ault in overfeeding the pressurizer and either or both steam generato.-s.

If J

selected, the possibly deenergized steam pressure transmitters would result in the turbine bypass valves closing and remining closed challenging the main steam safety valves.

Failure of branch circuit H or H1 (ICS Auto Power) results in transferring Eany ICS controls stations to manual and freezing the controlled components in position including the turbine bypass valves and main feedwater control valves.

If the auto power failure occurred followed by a reactor trip, a a

steam generator overfeed transient would occur with the turbine bypass valves rsmaining closed. However, if the auto power were to fail following a turbine trip (possibly in response to the same initiating failure), both the turbine

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bypass and feedwater control valves may be held open resulting in a combined steam generator overfeed and steam generator depret surization transient.

Although this sequence appears unlikely, similar sequen:e1 power failures have l

occurred.

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30 SELECTION OF SYSTEMS FOR ANALYSIS The objective of this work, as discussed in Section 1.0, is to conduct detailed FMEAs on systems having a major impact on overcooling.

The method of achieving this objective consists of three steps:

1.

Identify the Oconee 1 systems and functional interfaces.

2.

Identify those systems which have a potential impact on the overcooling transient.

3 Conduct a detailed FMEA of the systems identified in (2) above.

The impact of most plant systems on an overcooling transient is minor.

Thus, the purpose of a plant specific system list with clearly identified interfaces is to aid in the selection of only those systems having a potential impact on overcooling.

Due to the large number of systems and components in a nuclear power plant, this preliminary screening is necessary to determine which systems require detailed analysis since it is not possible to make an in-depth study of all of them.

An overcooling transient is defined, for purposes of this report, as a transient resulting in a significant decrease in reactor coolant temperature following reactor trip.

The criteria for the overcooling transients are discussed in Section 3 3 Since the response of reactor coolant system to postulated initiating transients is integral to any overcooling transient, it was concluded that, as a first screening criterion, any system having a direct interface with the reactor coolant system would be a candidate for further analysis.

Other criteria for the final selection are discussed in Section 3 2 and 3 3 31 OCONEE 1 SYSTEMS LIST Based on the previously developed generic list of pressurized water reactor systems list (Reference 1) and the Oconee Unit 1 Final Safety Analysis Report (FSAR) (Reference 2), an Oconee systems list was developed to identify all systems which might contribute to overcooling transients.

The systems and their associated subsystems are grouped according to six major functions:

1.

Nuclear Systems include the reactor core and those systems and subsystems which monitor and control core reactivity, remove 14

heat from the core, and otherwise directly support the safe operation of the reactor.

2.

Engineered Safeguards Systems include those systems, other than containment systems, which are used to mitigate the effects of reactor accidents such as those specified in the FSAR.

3 containment Systems include the reactor building and those systems needed to prevent reactor building overpressure, to prevent excessive leakage from the reactor building to the environment, and to provide a habitable atmosphere inside the reactor building.

4.

Power Conversion Systems include the systems and components that transform, or support the transformation of, heat energy produced by the reactor core into electrical energy.

5.

Process Auxiliary Systems include those systems and subsystems that support the plant systems directly involved in the operation of the reactor coolant systems.

6.

Plant Auxiliary Systems provide support to other plant activities and personnel.

The systems included in each grouping are shown in Tables 31 - 3.6.

A system identification was assigned to each system in order to simplify the subsequent interface analysis.

Note that electrical systems have not been included; the effects of electrical system failures on the plant are being analyzed separately from this study (References 3 and 4).

Af ter the systems lists were generated, specific interfaces were identified, based on the system descriptions in Reference 2.

Interfaces were identified for every system and include the direction (e.g., System A affects System B cnly, System A affects System B and System B affects System A, etc.) as well es interfacing system identification.

32 SYSTEMS AFFECTING OVERC00 LING Based on the systems lists and interfaces, specific systems were identified as having a potential impact on overcooling transients.

The selection criteria used are not specific to overcooling transients; systems potentially affecting 15

TABLE 3 1.

oCoHEE 1 NUCLEAR SYSTEMS (Nxx)

System ID System Name N01 Reactor Core NO2 Regulation Systems NO2.A Control Rod Drive Control System NO2.B Integrated Control System NO2.C Non-Nuclear Instrumentation System NO3 Incore Monitoring System N04 Reactor Coolant System (including reactor vessel and internals)

N04.A Pressurizer N04.B Steam Generator N04.C Reactor Coolant Pumps N04.D Control Rod Drive System N05 Makeup and Purification Systems N05.A Chemical Addition and Sampling System N05.B Coolant Storage System NOS.C Coolant Treatment System N05.D Post-Accident Sampling System N05.E High Pressure Injection System N06 Low Pressure Injection System N07 Reactor Protective System N08 Nuclear Instrumentation System 16

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i TABLE 3 2.

OCORER 1 ENGINEERED SAFEGUARDS SYSTEMS (Sxx)

System ID System Name S01 Engineered Safeguards Protective System SO2 High Pressure Safety Injection System S03 Low Pressure Safety Injection System SO4 Core Flood System SOS Reactor Building Spray System S06 Reactor Building Emergency Cooling System S07 Reactor Building Penetration Room Ventilation System SOS Reactor Building Isolation System SO9 Control Room Habitability System S10 Emergency Feedwater System S11 Emergency Feedwater Control System 17

4 TABLE 3 3 OCONEE 1 REACTOR BUILDING /CONTAIINENT SYSTEMS (Cxx) l System ID System Name i

i C01 Reactor Building / Containment and Penetrations CO2 Reactor Building Hydrogen Purge System C03 Reactor Building Ventilation System l

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i TABLE 3.4.

OCORER 1 POWER CONTERSION SYSTEMS (Pzz)

System ID System Name P01 Main Steam and Turbine Bypass System P02 Turbine Generator System P02.A Turbine Gland Seal Subsystem j

P03 Main condenser System P03.A Main Condenser Evacuation System PO4 Condensate and Feedwater System PO4.A Condensate Cleanup System POS Auxiliary Steam System 1

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TABLE 3 5.

OCONEE 1 PROCESS AUIILIARY SYSTEMS (Wxx)

System ID System Name WO1 Radioactive Waste System WO2 Radiation Monitoring System WO3 Reactor Building Component Cooling Water System WO4 Cooling Water Systems WO4.A Condenser Circulating Water (CCW) System UO4.B High Pressure Service Water (HPSW) System WO4.C Low Pressure Service Water (LPSW) System WO4.D Recirculated Cooling Water (RCW) System WOS Fuel Storage and Handling System WO5.A New Fuel Storage System WOS.B Spent Fuel Storage System WO5.C Spent Fuel Pool Cooling System U0S.D Fuel Handling System 806 Auxiliary Service Water System WO7 Compressed Air System WO7.A Service Air System WO7.B Instrument Air System WOS Plant Oas System b

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TABLE 3 6.

OCOREE 1 PLANT AUIILIARY SYSTEMS (Izz)

System ID Systen Name X01 Potable and Sanitary Water System X02 Fire Protection System XO3 Conaunications System XO4 Security Systea X05 Heating, Ventilating, and Air Conditioning Systems X05.A Turbine Building Ventilation System X05.B Reactor Building Purge Systes X05.C Auxiliary Building Ventilation System X05.D Spent Fuel Ventilation System X05.E Reactor Building Cooling System XO6 Non-Radioactive Waste System 21

reactor coolant system transients, in general, are selected.

The following Criteria were used to identify these systemst 1.

All systema having a direct (first order) interface with the reactor coolant system (including the pressurizer and the steam generator) were listed.

These systems are shown in Table 3 7.

2.

From this list, several systems were eliminated for reasons described below and shown in Table 3 7t l

(1) Only non-safety qualified control systems have been selected.

Safety systems were not included because these j

systems are being analy=ed in detail under separate NRC programa (Reference 5).

(2) Only those systems in operation or standby during norma'.

l plant power operation were included.

Systems such as j

those required for refueling or shutdown decay heat l

removal th'ta were not included.

These systems are manually placed in operation only after a controlled shutdown of the reactor coolant system to less than 3000F and less than 300 pai.

(3) only those ayatema directly affecting reactor coolant

)

system response were selected.

Those interfacing systema l

affected by but not affecting reactor coolant ayatem response were eliminated.

(It should be noted that some systems eliminated for this reason may be selected as an l

interfacing system - see Item 3 below.)

3 For the remaining systems, all systems interfacing with the systema selected in Table 3 7 were identified.

This list of second order interfacing systema, excluding those also selected in Table 3 7, is shown in Table 3.8.

The list of systems initially selected for analysia includes all control systems which potentially affect reactor coolant ayates response during plant transients and all ayatens which potentially affect the response of these first order ayatoms.

The specific impact of these systema on reactor coolant system overcooling are evaluated in this report.

22

TABLE 3 7.

FIRST ORDER REACTOR COOLANT SYSTEM INTERFACES Oconee Criteria System ID Systen Name Direction

  • for Elimination N01 Reactor Core 2

4 N02 Regulation Systems 3

l NO3 Incore Monitoring 1

Interface is away from RCS N04 Reactor Coolant System Included N05 Makeup and Purification 3

N06 1ow Pressure Injection 3

Operates during shutdown only N07 Reactor Protective 1

Safety system N08 Nuclear Instrumentation 1

Interface is away from RCS SXX Engineerad Safeguards Systems 1

Safety systems C01 Reactor Building / Containment and 3

Safety systes Penetrations F

002 Reactor Building Hydrogen Purge 1

Interface is away from RC3 C03 Reactor Building Ventilation 2

P01 Main Steam and Turbine Bypass 3

PO4 Condensate and Feedwater 2

l WOI Radioactive Waste System 1

Interface is away from RCS WO3 Reactor Building Component Cooling 3

Water WO5.D ruel Handling 3

Operates durir.g shutdown only et s Interface fzas reactor coolant Ag interfacing systes.

2 e Interface Ag reactor coolant fEsa incertacing system.

3 e Interface Ag and f,Een reactor coolant.

l 23 i

l I

, - 3...

-.m. -

First Second Order Order Systen Systes Criteria for ID ID Systen Name Direction

  • Elimination

[

N01 N04 Reactor Coolant 3

l NO3 Incore Monitoring Systes 1

Interface is away from Re-otor Core i

N02.A NO2.8 Integrated Control 2

I N02.C 304 Core Flood 2

Safety systes C01 Reactor Building 2

Safety system i

WO1 Radioactive Waste 2

N05 WO4.C Low Pressure service Water 3

Safety systen l

WO7 5 Instrument Air Systen 2

C03 307 Reactor Building Penetration Room 3

Safety system Ventilation I

308 Reactor Building Isolation 3

Safety system i

X05.E Reactor Building Cooling 3

P01 N02.8 Integrated Control 2

P02 Turbine-Generator System 3

P06 Auxiliary Stena System 3

Operates during shutdown only P04 N02.B Integrated Control 2

P03 Main condeneer 3

P04.A Condensate Cleanup System 3

W07 5 Instrument Air System 3

WC3 WO4.C Low Pressure Service Water (LPSW) 3 Safety Systes Systee l

24

f TAKE 3 8.

(Continued) i First Second Order Orcer System System Criteria for ID ID Oysten Name Direction #

Elimination i

WO4.D N05.D Fost Accident Sampling 3

Operates during shutdown only WO4.A Condenser Circulating Water 2

WO5.C Spent Fuel Fool Cooling 3

operates during shutdown only j

t el e Interface Itas first order system M second order system.

2 e Interface h first order system Ic a second order system.

i 3 s Interface h and IEga first order system.

Note:

Interfaces with direction a 1 have not been included.

L l

\\

35 l

To ensure completeness and to verify the adequacy of the selection procedure, each of the systems eliminated were briefly evaluated again to assess their potential impact on reactor coolant system overcooling.

The eliminated systems and the results of the reevaluation are presented in Appendix A.

33 SYSTEMS AFFECTING REACTOR COOLANT SYSTEM OVERC00 LING In Section 3 2, the systems which potentially affect the response of the Reactor Coolant System (RCS) have been identified. Of these systems, those potentially affecting RCS overcooling are identified.

Section 3 31 presents the definition of RCS overcooling for purposes of this analysis.

In Section 332, the functions of the systems identified in Tables 3.7 and 3.8 are evaluated to identify those systems potential affecting RCS overcooling as defined.

331 Definition of Sienificant RCS Overecoline RCS overcooling may be defined, in general, as a decrease in the RCS average temperature.

For purposes of this analysis, however, the definition of overcooling should focus on the overcooling transients of potential significance.

Two basic criteria are proposed to define significant overcooling for the purposes of systems selection and failure modes analyses:

1.

Transients terminated by reactor trip and automatically established stable conditions of post-trip RCS pressure, temperature and reactoF coolant inventory should be excluded.

2.

Transients exhibiting the potential for continued post-trip decreases of RCS pressure, temperature or reactor coolant inventory should be included.

These criteria define transients of> potential significance to RCS overcooling.

Transient conditions defined by these criteria and subsequent failure mode analyses will be analyzed using the Oconee hybrid computer model to predict the resulting RCS response and the impact on plant safety.

An RCS overcooling transient, as defined above, is characterized by continuously decreasing RCS temperature, pressure or inventory following reactor trip. These defined overcooling characteristics are interrelated significantly as shown in Table 3 9 26.

t e,

\\

s

TABLE 3 9 OfERC00 LING CHARACTERISTICS AND POTENTIAL INITIATING CAUSES Overcooling Characteristic Principal Causes Secondary Causes 1.

Decrease in 1.1 Net Heat Transfer 1.1.1 Increased Heat RCS Temperature From RCS Transfer Through Steam Generator Tubes 1.1.2 Release of Reactor Coolant From the RCS 2.

Pecrease in 2.1 Decrease in 2.1.1 Increase in RCS Pressure Pressurizer Pressurizer Spray Temperature Flowrate 2.1.2 Release of Steam (Reactor Coolant)

From the Pressurizer 2.2 Decrease in 2.2.1 Be1 ease of Reactor Pressurizer Level Coolant From the RCS 9

2.2.2 Decrease in RCS Temperature 2.3 Release of Reactor 231 POR7 Opens and Coolant From the Remains Open RCS 232 Pressurizer Safety Valve Opens and Remains Open 2.3 3 Net Release of Reactor Coolant From the RCS to the MU&P System 2 3.4 RC Pump Seal Failure Occurs 3

Decrease in RCS 3.1 Release of Reactor 331-334 Inventory Coolant From the (See Items 2 3 1 - 2 3.4)

RCS 27

In Table 3.9, the three defined characteristics of RCS overcooling are expanded in terms of possible functional causes.

Following reactor trip (which is an assumed necessary condition for an overcooling transient), the hsat input from the suberitical core to the reactor coolant (decay heat) is a fixed decreasing function of time. To the extent heat is removed from the reactor coolant at a rate in excess of the decay heat, the total energy content of the coolant and its temperature will decrease.

As shown in Table 3 9, a net heat transfer from the RCS could result from increased heat transfer through the steam generator tubes to the feedwater (secondary coolant) or a direct release of the high temperature reactor coolant from the i

RCS.

RCS pressure is controlled by regulating the saturation temperature of the pre s suriz er.

The RCS pressure will decrease in response to a decreased pressurizer temperature (assuming saturation).

The pressurizer saturation temperature can decrease in response to an increase in the pressurizer spray flowrate which condenses steam in the pressurizer or a direct release of steam from the pressurizer. A decrease in the pressurizcr liquid level also may result in reduced RCS pressure due to the expansion of the steam volume.

The pressurizer level can be reduced in response to a decrease in the reactor coolant temperature and resulting decrease in coolant volume or a direct release of reactor coolant from the RCS.

Decreases in RCS inventory results from a net release of reactor coolant from the RCS as discussed above.

Based on the functional expansion of the RCS overcooling characteristics, three functional causes can be identified:

1.

Increased heat transfer through the steam generators in excess of the decay heat generation rate.

2.

Opening the Pressurizer Spray Valve.

3 Net.elease of Reactor Coolant from the RCS.

28 l

1 1

These three overcooling characteristics are discussed in Sections 3 31.1, 3 31.2 and 3 3.13 to relate the physical overcooling processes occurring in the RCS in response to RCS and interfacing equipment operating modes.

3 3 1.1 Increased Heat Transfer Through the Steam Generators Following reactor and turbine trip, heat transfer from the reactor pumped through the steam' generator tubes is regulated by the mass flowrate and temperature of the feedwater addition to the steam generator "shell" side (outside the tubes) and the saturation pressure maintained in the shell side.

The core power following reactor trip is below 55 full power. This heat is removed, under normal conditions, in the two steam generators by regulating the feedwater flowrate to maintain a feedwater inventory equivalent to approximately 30" of water in the steam generators and regulating the saturation pressure of the steam generators' shell side at approximately 1025 psia using the turbine bypass valves.

Under steady state conditions, the rate

}

at which the feedwater is vaporized is proportional to the small and decreasing decay heat production rates.

The reactor coolant temperatures are within a few degrees of the saturation temperature of the shell side of the steam generators.

The rate of heat transfer from the reactor coolant to the feedwater could be 1

increased by either of two mechanisms:

reducing the saturation temperature of the steam generator shell side or increasing the feedwater flowrate.

A reduction in the saturation pressure could occur by opening the turbine bypass

. valves. This would result in a lower shell side saturation temperature, an increased temperature difference between the reactor coolant and the boiling feedwater and consequently an increased heat transfer rate.

The reactor coolant temperature is expected to decrease under these conditions until a new equilibrium is established.

It should be noted that as the saturation pressure is reduced the volumetric flowrate of steam will decrease.

Furthermore, at the reduced saturation pressures and temperatures, the energy content per unit volume of steam released through the turbine bypass valves will be reduced due to increased specific volume (decreased density) of the steam.

Due to these phenomena, the rate of reactor coolant temperature reduction will decrease as the temperature decreases.

However, reactor 29

0 coolant temperatures of less than 300 F are considered possible after several hours.

An increase in the flowrate of feedwater also can result in a potentially 1

significant decrease in heat transfer from the reactor coolant. Following reactor and turbine trip, the extraction steam to the feedwater heaters is isolated and the feedwater temperature will begin to decrease slowly.

As the rate of feedwater injection increases, the rate of heat transfer from the reactor coolant required to heat the feedwater to saturation temperature increases. Although the rate of steam production will be reduced, the net rate of heat transfer from the reactor coolant can increase significantly due to the large capacity of the main feedwater system.

In addition to increased heat transfer through the steam generators, increased heat transfer through the letdown-makeup flowpath or increased convective heat transfer to the reactor building air is possible.

In either case, however, the effects of these mechanisms on reactor coolant temperature are e::pected to be negligible.

3 3 1.2 Increased Pressurizer Soray Flowrate During operation, the RCS pressure is controlled by regulating the saturation temperature in the pressurizer.

Pressure is increased by heating the saturated water in pressurizer and decreased by 2. praying subcooled water from the RCS inlet pipes into the saturated pressurizer steam space.

A continued spray flow, which could result from the pressurizer spray valve failing open, potentially results in a depressurization transient.

Following reactor trip, the RCS is controlled to a temperature of 0

i opproximately 547 F and a pressure of approximately 2166 psig (pressurizer saturation temperature of 6480F).

If the pressurizer spray valve opened and 0

the 547 F water sprayed into the pressurizer steam space would remained open, result-in a decrease in the pressurizer saturation temperature and RCS pressure.

As the pressure decreases, the effect of the spray is counteracted by the 1638 KW pressurizer heaters.

30

It should be noted that the effect of increased spray flow is a potential j

0 decrease in RCS pressure with the RCS temperature remaining at 547 F.

This transient is of interest due to the potential for initiating safety injection 6t the ESPS low RCS setpoint pressure of 1500 psi.

3313 Release of Reactor Coolant j

The release of reactor coolant potentially involves a reduction of reactor coolant pressure, temperature and inventory depending on the leak rate and the operation of other systems.

Continued power operation typically is allowed with leak rates less than 10 gpm.

Small and large loss of coolant accidents (LOCA's) in contrast, are significant hazards to nuclear power plant safety.

This study considers the effects of control systems failures.

As such, arbitrarily postulated piping failures are not considered.

Release of reactor coolant restiting from pressurizer relief or safety valves opening and remaining open, a net release of reactor coolant via the letdown piping or oteam generator tube cracks is considered to the extent such a failure may result from a control system misoperation.

In general release of reactor coolant :.* alls in the category of RCS leaks or small LOCA's.

The response of nuclear power plants to a release of reactor coolant varies consideratly depending on the rate of loss.

Miscellaneous plant leakage, typically such lower than 1 gpm, is a normal occurrence.

The operator routinely nonitors the makeup tank level to determine the leak rate from the RCS.

Du.-ing the periodic adjustments to the reactor coolant boron concentration, the operator replaces a volume of reactor coolant with demineralized water.

During this process, water would be added to the makeup tank to replace RCS leakage.

If the operator detects an RCS leak rate exceeding 1 gpm, he must determine the location of the leak or shut down the plant.

Leakage through one or more of the pressurizer relief valves, for instance, can be identified by high temperature readings of the discharge line thermocouples.

In addition, if the source of leakage exceeding 1 gpm is the steam generator tubes, the plant must be shutdown.

Steam generator tube leaks are indicated by the monitored 31

- l y

w-. - -+w g-

radioactivity level of the main condenser " air" ejector discharge. All RCS leakage exceeding 10 gpm requires plant shutdown.

RCS leak rates within the makeup capability of the makeup and purification system (MU&P) are classified "RCS Leaks." RCS leaks exceeding the above leak rate limits require shutdown of the plant to a " cold shutdown" state and repair of the pressure boundary failure.

For RCS leaks in the pressurizer water space or the RCS loops, the mass flow rate from the RCS to the containment is balanced automatically by the makeup mass flow rate from the makeup tank to the RCS.

Under this condition, RCS pressure is controlled by the operation of the spray valve and pressurizer heaters. Prior to the draining of the makeup tank, the operator must initiate makeup to the makeup tank or open the valves in the flowpath from the Borated Mater Storage Tank (BWST) to the makeup pump (s).

The shutdown operation with " water space" RCS leaks (as opposed to " steam apace" leaks) is similar to normal shutdown operations.

The operator controls the rate of cooldown and the rate of depressurization to maintain the RCS within pre-established pressure and temperature limits for shutdown. The cooldown rate is maintained by operator control of the turbine bypass valves and the depressurization rate by operator control of the spray valve.

RCS leaks in the pressurizer steam space (>200 lbm/ min) result in an initially uncontrolled depressurization of the RCS even with the pressurizer liquid level maintained.

The operator is instructed to attempt to isolate the leak by manually closing the PORY and/or the PORY block valve.

If the leak is not isolated, the pressurizer heaters are capable of maintaining pressurizer pressure and temperature for leak rates less than 200 lbm/ min. ^ The required makeup rate for these transients is less than 27 gpm.

Makeup rates greater than 10 gpm would require shutdown with conditions similar to " water space" leaks.

The operator can control the depressurization by manually increasing the makeup flow rate and filling the pressurizer.

If the operator fails to take it

.[

32 f

a

~

~

this action, the RCS pressure will decrease to the safety injection setpoint

(~1500 psi).

At this pressure, the high pressure injectien (HPI) mode of the MU&P will be automatically actuated and the pressurizer will be filled.

Once the pressurizer is filled and the leak is in the water space, the RCS pressure is automatically controlled by the PORY and/or safety valves at approximately 2450 psi.

Once the RCS pressure is controlled, the operator can initiate shutdown procedures.

With the HCS subcooled by at least 500F, the operator can reestablish the pressurizer level by throttling the makeup flow. When the leak path is uncovered and steam discharged, the RCS will begin to depressurize. The cooldown is controlled by manual control of the turbine bypass valves.

If the 0

50 F reactor coolant subcooling cannot be maintained 0

with a cooldown rate of 100 F/ hour, the operator must increase the MU&P/HPI flowrate until the required subcooling can be reestablished.

During the depressurization, the leak rate will decrease due to the lower RCS pressures.

If an increased rate of depressurization is required, the operator can manually open the spray valve or the PORV.

Breaks resulting in a leak rate in excess of the capacity of the makeup system are classified Loss of Coolant Accidents (LOCA's). A small break LOCA, such as a failed open PORV, generally will result in the RCS pressure decreasing rapidly to the saturation pressure (approximately 1200 psi) and then slowing considerably (the pressure will rise following very small breaks and limited steam generator cooling). At 1500 psi the HPI is automatically started and begins injecting borated water from the BWST.

The operator is instructed to trip the reactor coolant pumps which results in the steam generators being automatically filled and maintained by the main or emergency feedwater systems 6t the natural circulation setpoint.

Core cooling is maintained by the continued operation of the HPI. Throttling the HPI is not permitted since the reactor coolant will not be 500F subcooled.

t l

To enhance the RCS depressurization and cooldown, the operator may depressurize the steam generators by manually controlling the turbine bypass valves.

l l

t 33

Small break LOCA's result in a gradual net loss of reactor coolant until the RCS depressurizes to a pressure where the net loss is zero and refilling begins. Typically, the reactor coolant rapidly saturates at approximately 1

1000 pst The subsequent response of the RCS depends on the decay (residual) heat generation rate of the core, the coolant nass and energy removal through the break, the rate of coolant mass injection, and the rate of heat removal through the steam generators.

If the rate of core heat generation exceeds the rate of heat removal through the break plus the heat removal through the steam generators, the coolant pressure and temperature will increase. This will increase the heat lost through the break and result in thermal equilibrium.

However, the increased pressure also results in an increase in the rate of coolant mass loss and a decrease in rate of coolant injection.

If more heat is being removed from the RCS than generated in the core a reverse process takes place.

In addition to the above phenomena, the rate of core heat generation is decreasing with time and the rate of heat transfer through the steam generators varies with the RCS coolant inventory.

The RCS coolant inventory typically decreases over the initial period of the LOCA, reaches a minimum and then increases.

If this minimum inventory is sufficient to maintain the core covered with coolant, the plant will recover.

However, if the minimum inventory results in a significant fraction of the core being uncovered, core damage will occur. Typically, nuclear power plants are designed to maintain an adequate minimum inventory following small break LOCA of any size even with assumed partial failures of the HPI and steam generator cooling functions and a conservatively large core heat generation rate.

In addition to the " classical" LOCA scenarios, a failure mode involving brittle failure of the reactor vessel wall has been postulated and is under investigation.

In these Pressurized Thermal Shock (PTS) scenarios, a LOCA, or other initiating accident, results in a low temperature, high stress condition in the reactor vessel wall.

The LOCA recovery actions described above are being analyzed to determine whether they produce conditions sufficiently severe to result in a large through-wall crack in the reactor vessel.

34

4 PTS is of some concern following small break LOCA's. Following a LOCA, the rcactor coolant circulating pumps are tripped. Due to the net loss of reactor l

coolant inventory, natural circulation of liquid coolant from the reactor through the steam generators will cease.

The major flow into the RCS will be from the low temperature BWST into the reactor inlet pipes.

Over the course of the accident, the RCS pressure will be slowly decreasing and the temperature of the coolant in the vessel downcomer (which is thermally asparated from the core region following outlet pipe and pressurizer breaks) will be decreasing.

The combination of the relatively high RCS pressure and relatively low vessel wall temperatures may lead to brittle fracture in rtactor vessels which are particularly sensitive to radiation embrittlement.

One particular small break LOCA of concern is the failed open PORV.

Assuming the failed PORV remains unisolated for the initial phase of the accident, the vessel downcomer temperature will be low.

If the operator then isolates the PORV, the continued injection of coolant and the heat generated in the core will increase the RCS pressure to pressures of up to 2500 psi, which may be of significant PTS concern.

The PTS phenomena is the subject of considerable current research and analysis.

Detailed analysis to determine the pressures and temperatures occurring following small breaks and the response of reactor vessels to these conditions is required to assess the potential for vessel failure.

Detailed information describing the required equipment and operator actions following system leakage and LOCA's is provided in each plant's LOCA emergency procedure (e.g.,

Duke Power emergency procedure EP/0/A/1800/4, " Loss of Reactor Coolant" and OP/0/A/1106/35, " Inadequate Core cooling").

The response characteristics of the RCS to LOCA's is described in vendor topical reports referenced in each plant's FSAR (Reference 2).

332 Evaluation of RCS Overcoolina Resoonse to Systems Failures Based on the definition of RCS overcooling, the systems potentially affecting RCS response identified in Tables 3 7 and 3 8, were briefly evaluated to assess their potential impacts on RCS overcooling.

The results of this cvaluation are summarized in Table 3 10.

35

TABLE 3 10.

POTENTIAL IMPACTS OF FIRST AND SECOND ORDER REACTOR COOLANT SYSTEM INTERFACE SYSTEMS ON RCS 07ERCOOLING Potential Impact System ID System Name on RCS Overcooling i

N01 Reactor Core The response of the reactor core can influence overcooling.

However, " core failures" are considered to be beyond the scope of this study (see Section 4).

NO2 Regulation Systems N02.A Control Rod Drive Control Control rod drive control system has no function in the post-trip mode (see Section 4).

NO2.B Integrated Control Control signal failures considered as part of fluid systems controlled.

NO2.C Non-Nuclear Instrumentation Control signal failures considered as part of fluid systems controlled.

N04 Reactor Coolant N04.A Pressurizer Analyzed in detail.

N04.B Steam Generator Analyzed in detail.

N04.C Reactor Coolant Pumps Analyzed in detail.

N04.D Control Rod Drive Mechanisms Control rod drive mechanisms have no function in the post-trip mode (see Section 4).

NOS Makeup and Purification Makeup and Purification subsystems considered in detail with the exception of the sampling systems. The sampling systems are intermittently used under manual control with sample flowrates less than 1 gpm.

Sampling system failures are not considered to have any significant impact on RCS overcooling.

36

TABLE 3 10.

(Continued)

Potential Impact System ID System Name on RCS Overcooling NOS.A Chemical Addition and-Sampling NOS.B Coolant Storage NOS.C Coolant Treatment System N05.D Post Accident Sampling N05.E High Pressure Injection C03 Reactor Building Ventilation The effect of containment air temperature changes on heat transfer from the RCS is considered to be insignificant.

The effects of loss of ventilation on component operability is considered to be beyond the scope of the study.

PC1 Main Steam and Turbine Power conversion systems and Bypass subsystems analyzed in detail.

P02 Turbine-Generator System P03 Main Condenser PO4 Condensate and Feedwater 801 Radioactive Waste System was selected based on its interface with the Non-Nuclear Instrumentation.

However, the interface consists of providing parameter signals for display only.

Failures of the Radioactive waste system not considered to have any significant impact on RCS overcooling.

WO3 Reactor Building Component Potential impact due to first Cooling Water and second order interfaces.

Cooling water failures considered as part of the process systems served.

i 37

TABLE 3.10.

(Continued)

Potential Impact System ID System Name on RCS Overcooling 604.A Condenser Circulating Water Potential impact due to second order interfaces.

Cooling water failures considered as part of the process systems served.

WO4.D Recirculated Cooling Water Potential impact due to second order interfaces.

Cooling water failures considered as part of the process systems served.

507.B Instrument Air Potential impact due to first and second order interfaces.

Instrument air failures considered as part of the fluid systems served.

X05.E Reactor Building Cooling The effect of containment air temperatures on RCS heat transfer is considered to be insignificant. The effects of high air temperatures on the operability is beyond the scope of this report.

4 1

38

~

=.

I 1

As indicated, most of the systems affecting RCS response have the potential for affecting RCS overcooling.

These systems are analyzed in detail using a failure modes and effects analysis method to evaluate specific effects of system failures on RCS overcooling (see Section 5).

The systems not selected for detailed analysis are discussed below.

i The heat production rate of the reactor core will affect the course of an RCS overcooling transient.

However, the heat production rate will vary depending j

on external factors affecting the core rather than possible core failures.

The potential effects of core failure mechanisms (e.g.,

cladding perforation, gross core movement) are beyond the scope of this analysis.

1 The control rod drive mechanisms and the control rod drive control system I

influence to rate of core heat production during operation.

However, once the reactor is tripped (control rods inserted) neither the drive mechanisms nor the drive control system can influence the resulting transient.

The reactor core, control rod drives and the control rod drive control system are discussed further in Section 4.

i The reactor building ventilation system and the reactor building cooling system control the air temperature in the containment.

The effect of l

containment air temperature or velocity changes are considered to have a negligible effect on heat transfer from the insulated RCS and consequently a negligible effect on RCS overcooling. Although it is recognized that long term operation of components in an adverse (high temperature) reactor building onvironment can effect their performance, the study of such effects is considered beyond the scope of this analysis.

1 i

The radioactive waste system is scratored by the non-nuclear instrumentation.

However, the parameters monitored only are displayed and have no impact on the development of non-nuclear instrumentation control signals.

As such, the radioactive waste system is considered to have no significant impact on RCS l

cvercooling.

39 I

4.0 SYSTEM DESCRIPTIONS Brief system descriptions are provided for each system identified in Section 3.2 as requiring detailed analysis.

Support systems (e.g.,

instrument air and control systems) are discussed with each major system.

4.1 NUCLEAR SYSTEMS DESCRIPTIONS The Nuclear Systems include the reactor core and those systems and subsystems which monitor and control core reactivity, remove heat from the core, and otherwise support safe operation of the reactor.

The major systems and subsystems identified in Section 3 2 requiring detailed analysis are:

N01 - Reactor Core N04 - Reactor Coolant System NO2 - Regulation Systems N05 - Makeup and Purification System Brief descriptions of these systems are provided in this section.

4.1.1 Reactor Core The reactor core consists of the 177 fuel assemblies which produce the thermal power ultimately used to produce electric power in the unit's main generator.

The thermal power is produced by nuclear fission of the slightly enriched uranium in the core. The core fuel assemblies are supported by the reactor internals in the reactor vessel.

The core produces heat at a rate consistent with exterior factors such as the moderator (reactor coolant) density, concentration of boric acid in the coolant, and position of control rods in the core.

The heat is removed from the core by the reactor coolant which is pumped upwards through the core fuel assemblies. The rate of heat transfer depends on the temperatures of the fuel, temperatures of the reactor coolant and on the coolant velocity.

Although the response of the core to external parameters is important to a i

study of reactor coolant system overcooling, a detailed analysis of core l

failure mechanisms initiating a transient is considered beyond the scope of l

this study.

For purposes of this analysis, the reector core is assumed to be 40

operating within technical specification limits at the start of externally initiated transients, and to respond to external factors as designed.

4.1.2 Reactor Coolant System The Oconee reactor coolant system (RCS) is a B&W design nuclear steam supply cystem. It consists of or is impacted by the following major components:

1.

A reactor vessel which houses and supports the reactor core.

2.

Four reactor coolant pumps which circulate reactor through the reactor core and steam generators.

3 A pressurizer which is used to control RCS pressure and maintain the reactor coolant in a subcooled state.

4 Two steam generators which transfer heat from the reactor coolant to produce the steam to drive the plant turbines.

5.

61 Control Rod drive mechanisms which position the individual control rods.

Reactor coolant is pumped from the steam generators into the reactor vessel through the four " cold-leg" inlet pipes.

The coolant flows upward through the pipes where heat is transferred from the fuel elements to the coolant raising its temperature.

The heated coolant flows from the reactor vessel to each of the two steam generators through one of the two " hot-leg" outlet pipes.

Heat is transferred from the high temperature reactor coolant as it flows downward through the tubes of the two steam generators. The heat flowing across the steam generator tube walls vaporizes and slightly superheats the feedwater pumped into the shell side of the steam generators to produce steam. The reduced temperature reactor coolant flows from each steam generator through two pipes, one to each of the four reactor coolant pumps.

The reactor vessel and connecting piping are safety qualified passive pressure boundaries. Consideration of the failure of these pressure boundaries is beyond the scope of this study.

The functions of the reactor coolant pumps, pressurizer, steam generators and associated equipment is discussed below.

4.1.2.1 Reactor Coolant Pumns i

Each reactor coolant loop contains two vertical single stage centrifugal-type l

pumps which employ a controlled leakage seal assembly. Reactor coolant is I

41

pumped by the impeller attached to the bottom of the rotor shaft. The coolant is drawn up through the bottom of the impeller, discharged through passages in the guide vanes and out through a discharge in the side of the casing.

The rotor-impeller can be removed from the casing for maintenance or inspection without removing the casing from the piping.

All parts of the pumps in contact with the reactor coolant are constructed of austenitic stainless steel or equivalent corrosion resistant materials.

The pump employs a primary, high pressure controlled leakage seal assembly to restrict leakage along the pump shaf t, as well as a secondary high pressure seal which directs the controlled leakage out of the pump. A low pressure vapor seal minimizes the leakage of vapor from the pump to the containment atmosphere.

A portion of the high pressure water flow from the high pressure injection pumps is injected into the reactor coolant pump between the impeller and the controlled leakage seal.

Part of the flow enters the Reactor Coolant System through a labyrinth seal in the lower pump shaft to serve as a buffer to keep reactor coolant from entering the upper portion of the pump. The remainder of the injection water flows along the drive shaft, through the controlled leakage seal, and finally out of the pump. A small amount which leaks through the secondary seal is also collected and removed from the pump.

Component cooling water is supplied to the thermal barrier cooling coil.

In the event seal injection from the high pressure injection pumps stops, reactor coolant will flow from the coolant system and through the thermal barrier labyrinth seal.

The temperature of the reactor coolant is reduced in labyrinth seal (thermal barrier cooling coil) prior to passing through the controlled leakage seals.

The reactor coolant pump seals are designed to operate with either high pressure seal injection flow, component cooling water flow or both.

The reactor coolant pump motors are large, vertical, squirrel cage, ' induction motors.

The motors have flywheels to increase the rotational-inertia, thus prolonging pump coastdown and assuring a more gradual loss of main coolant 42

flow to the core in the event pump power is lost.

The flywheel is mounted on the upper end of the rotor, below the upper radial bearing and inside the motor frame.

An anti-reverse device is included in the flywheel assembly to eliminate reverse rotation when there is back flow.

Prevention of back rotation also reduces motor starting time.

The motors are enclosed with water-to-air heat exchangers so as to provide a closed circuit air flow through the motor.

Radial bearings are floating pad type, and the thrust bearing is a double-acting Kingsbury type designed to carry the full thrust of the pump.

A high pressure oil system with separate pumps is provided with each motor to jack and float the rotating assembly bafore starting.

Once started, the motor provides its own oil circulation.

t The bearing oil flows through a heat exchanger where heat is rejected to the component cooling water flow through the heat exchanger.

Loss of the component cooling water flow will result in excessive oil temperature and possible bearing failure in the long term (hours).

Instrumentation is provided to monitor motor cooling, bearing temperature, winding temperature, winding differential current, and speed.

4.1.2.2 Pressurizer The pressurizer in a pressurized water reactor coolant system (RCS) is a large tank containing saturated water and steam. The pressurizer water space is connected to one of the reactor outlet pipes (hot legs) by the surge line which allows a flow of water from or to the RCS during changes of reactor coolant specific volume.

In addition to providing a surge volume, the pressurizer is used to control RCS pressure and provide a measure of the reactor coolant. inventory.

The pressure in the pressurizer (and the RCS) is controlled at a setpoint value to maintain the reactor coolant in the RCS in a subcooled state.

i During transient reductions in the reactor coolant volume, the liquid level in the pressurizer and the RCS pressure both tend to decrease.

The liquid level in the pressurizer is measured and the decrease below setpoint results in a 43

control circuit automatically increasing the net flow rate to the RCS from the Make-up and Purification System (MU&P) to restore the setpoint level. The decreased RCS pressure is mensured and results in a control circuit automatically energizing the pressurizer electric resistance heaters (located in the pressurizer water space). The heaters increase the temperature of the saturated water in the pressurizer and consequently the RCS pressure.

During transient increases in the reactor coolant volume, a reverse process will occur to reestablish actpoint values.

The increased pressurizer liquid level results in a decrease in the net flow rate from the MU&P system. The increased RCS pressure results in an increase in the flow rate from the reactor inlet (cold leg) pipe to the pressurizer steam space through the spray line. The subcooled water sprayed into the steam volume condenses some of the steam, resulting in a decreased saturation temperature in the pressurizer and decrased pressure in the RCS.

4 Transients causing a pressure increase beyond the control capacity of pressurizer spray will result in the actuation of one or more of the three relief valves mounted on the top of the pressurizer (steam space).

The Pilot Operated Relief Valve (PORV) is opened by a control circuit if the RCS pressure setpoint is exceeded.

If the PORY does not limit the pressure, the two spring loaded code safety valves will open through direct action of the steam pressure on the valves' seats (no control circuit is required).

Pressurizer system interfaces, including power supplies and signal destinations, are discussed in detail in Reference 6.

4.1.2 3 steam Generator i

The steam generator is a vertical, straight tube, tube and shell heat exchanger which produces superheated steam at constant pressure over the power range. Reactor coolant flows downward through the tubes and transfers heat to generate steam on the shell side.

The high pressure (reactor coolant pressure) parts of the unit are the hemispherical heads, the tube sheets and the tubes between the tube sheets.

Tube support plates maintain the tubes in a uniform pattern along their length.

The unit is supported by a skirt attached to the bottom head.

44

.~

The shell, the outside of the tubes, and the tube sheets form the boundaries of the steam producing section of the vessel.

Within the shell, the tube bundle is surrounded by a cylindrical baffle.

There are openings in the baffle at the feedwater inlet nozzle elevation to provide a path for steam to Offord contact feedwater heating. The upper part of the annulus formed by the baffle plate and the shell is the superheat steam outlet, while the lower part is the feedwater inlet heating zone.

Vent, drain, and instrumentation nozzles, and inspection handholes are provided on the shell side of the unit.

The reactor coolant side has manway openings in both the top and bottom heads, and a drain nozzle on the bottom head. Venting of the reactor coolant side of the unit is accomplished by a vent connection on the reactor coolant inlet pipe to each unit.

Feedwater is heated to saturation temperature by direct contact heat exchange.

During normal power operation, the feedwater is sprayed into the downcomer annulus formed by the shell and the cylindrical baffle around the tube bundle.

Steam is drawn by aspiration into the downcomer and heats the feedwater to saturation temperature.

The saturated water level in the downcomer provides a static head to balance the static head in the boiling section of the steam generator.

The downcomer water level varies with steam flow from 15 - 100 percent load. A constant minimum level is held below 15 percent load.

t The saturated water enters the tube bundle just above the lower tube sheet and the steam-water mixture flows upward on the outside of the tubes counter-current to the reactor coolant flow.

The vapor content of the mixture increases almost linearly along the tubes to produce saturated steam.

Saturated steam is raised to final temperature in the superheater region. The Omount of surface available for superheat varies inversely with load. As load decreases the superheat section gains surface from the nucleate and film boiling regions. Mass inventory in the steam generator increases with load as the length of the heat transfer regions vary.

Changes in temperature, 45

pressure, and load conditions cause an adjustment in the length of the individual heat transfer regions and result in a change in the inventory requirements. If the inventory is greater than that required, the pressure increases.

Inventory is controlled automatically as a function of load by the feedwater controls in the Integrated Control System.

In the event the main feedwater pumps trip, the emergency feedwater system injects feedwater into the emergency feedwater spray header located near the top of the steam generator.

Main feedwater flow also may be injected through the emergency feedwater header by valve realignment. This action enhances natural circulation of reactor coolant in the event the reactor coolant pumps are tripped or deenergized.

4.1.2.4 control Rod Drive Mechanisms The function of the control rod drive mechanisms (CRDM) is to position the control rods in the core during power operation and release the control rods in response to reactor trip signals from the reactor protection system (RPS).

The (61) CRDM are divided into four safety banks and four control banks.

The safety banks are held completely out of the core during power operation and are released to fall into the core on a reactor trip signal or are fully inserted into the core to achieve a controlled shutdown.

The control (or regulating) banks are inserted or withdrawn sequentially to decrease or increase reactor core power by the control rod drive control system (CRDCS) acting on Integrated Control System (ICS) insert or withdraw signals.

Upon an RPS trip signal, the control banks control rods are released to fall.into the core regardless of CRDCS or ICS control signals.

The control rods are inserted or withdrawn from the core by rotating an sngaged " roller nut" around the threaded control rod lead screw.

The roller nuts both are engaged and rotated in the desired direction by the application of electric power to external coils. The sequenced application of power is performed by the CRDCS in response to ICS signals.

Reactor trip is accomplished by deenergizing the CRDCS in response to RPS signals.

This deenergizes each of the CRDM coils, disengaging the roller nuts and allowing the control rods to fall into the core.

46

Three failure modes can be postulated for the CRDM and associated CRDCS:

mispositioning the control rods in the core, failing to release the control rods on demand or spuriously releasing the control rods.

Of these, only the last of interest to overcooling transients (i.e.,

decreasing RCS temperature, pressure or inventory following reactor trip). Hispositioning the control rods, at most, may result in a reactor trip (release of all control rods).

Failure to release one control rod following a reactor trip signal is a design basis condition analyzed in the FSAR accident analysis. Failure to release more than one control rod has been analyzed in the NRC " Anticipated Transients Without Scram" program and is beyond the scope of this study.

A spurious release of one or more control rods, at most, may result in a reactor trip signal and release of all control rods.

Reactor trip is an expected condition in the context of the overcooling transient considered in this study.

Although malfunctions of the CRDM or CRDCS can produce a reactor trip transient, overcooling will occur only due to independent failures of other systems (reactor trip itself is not an overcooling transient).

As such, detailed analysis of CRDM or CRDCS malfunctions is not required in the study of overcooling transients.

4.1 3 Aerulation systems The operation of the RCS and key interfacing systems is controlled by three major instrumentation systems:

the Control Rod Drive Control System (CRDCS),

the Non-Nuclear Instrumentation System (NNI) and the Integrated Control System (ICS).

The functions of these regulating systems, with emphasis on their relation to RCS overcooling are described below.

4.1 3.1 Control Rod Drive control system The CRDCS, as discussed in Section 4.1.2.4, applies power to the CRDM motors to insert or withdraw the control rods.

The CRDCS inserts and withdraws the control rods in response to commands from the control room manual control station or automatic signals from the ICS during power operation.

Additional CRDCS design information is provided in Reference 2.

Upon reactor trip, which occurs during any overcooling transient of interest, the CRDCS and the CRDM's are deenergized and cannot influence the course of 47

i i

the subsequent transient. As such, failure modes of the CRDCS which relate to reactor trip are not analyzed in this program.

However, failure of the turbine trip auxiliary contacts located in the CRDCS cabinets is considered in the evaluation of the turbine controls.

i 4.1 3 2 Non-Nuclear Instrumentation The NNI is a collection of process instrument circuits used to measure, display and alarm process variables and provide process signals to the ICS.

In addition, the NNI contains control circuits used to control process variables such as RCS inventory (makeup flowrate control), RCS pressure (pressurizer spray, heater and relief valve control) and RC pump seal injection flowrate control. The NNI is described in detail in References 2 and 7 i

4 The NNI is expected to have a significant influence on RCS overcooling transients. In particular, RCS pressure control circuit malfunctions could lead to actuation of the ESPS.

Malfunctions of the steam pressure and steam i

generator level circuits supplying signals to the ICS could lead to continued RCS temperature reductions.

Due to the potential impact on RCS overcooling, i

the NNI control and measurement circuits are analyzed in detail as part of the j

analysis of fluid system controlled components.

j I

j 4.1 3 3 Interrated control system The principal function of the ICS is to develop coordinated control signals to regulate main feedwater flowrate, reactor power and steam pressure during power operation. Based on process parameter signals developed in the NNI, the l

ICS develops signals to modulate the main feedwater control. valves, the i

1

)

turbine throttle and turbine bypass valves and control rod position to meet existing electric power demand and RCS operating limits.

l Following reactor and turbine trip, the ICS continues to modulate the j

feedwater control valves to maintain the steam generators' water level and the-

}

turbine bypass valves to maintain steam line pressure.

Either of these functions can have a significant influence on RCS overcooling and the ICS control circuits are analyzed in detail as part of the analysis of fluid 1

48

system controlled components for this reason. The ICS functions and circuitry is described in detail in References 2 and 7 4.1.4 Makeuo and Purification System The functions performed by the Oconee High Pressure Injection, Coolant Storage, Coolant Treatment and Chemical Addition Systems are sequential and complementary.

The equipment in these systems has been grouped to include a general makeup and purification system.

The Makeup and Purification (MU&P) System consists of the piping and process equipment required to remove, process and replace reactor coolant at the flowrates required to maintain constant Reactor Coolant System (RCS) coolant volume.

The major functions performed by the MU&P System are:

I 1.

Letdown Control:

Controlled removal of reactor coolant from the RCS and reduction of coolant temperature and pressure at a preset flowrate.

2.

Purification:

Removal of impurities from the reactor coolant using boric acid saturated ion exchange resins.

3 Coolant Processing and Chemical Addition:

Recovery of concentrated boric acid and demineralized water from letdown reactor coolant; supply of domineralized (boric acid free) water and concentrated boric acid to adjust reactor coolant l

boric acid concentrations; and supply of lithium hydrox de to control reactor coolant pH.

i 4.

Reactor Coolant Pump (RC Pump) Seal Return:

Collection,

- filtering and cooling of coolant flowing past the RC Pump shaft face seals.

5.

RC Pump Seal Injection:

Injection and filtering of processed letdown coolant to the RC pumps' shaft seals at a constant flowrate.

6.

RC Makeup:

Injection of processed letdown coolant to the RCS i

at a flowrate controlled to maintain constant reactor coolant volume (coolant pressurizer level).

l 49

In addition to the normal functions performed by the MU&P System, portions of the system are used to provide emergency injection of coolant following design basis plant accidents.

Detailed functional descriptions for these subsystems are provided in Reference 8.

4.2 POWER CONVERSION SYSTEMS DESCRIPTIONS The Power Conversion Systems are designed to convert the heat produced in the rsactor to electrical energy.

The superheated steam produced by the steam generators is expanded through the high pressure turbine and then reheated in the moisture separator reheaters.

The moisture separator section removes the moisture from the steam and the two stage reheaters superheat the steam before it enters the low pressure turbines.

The steam then expands through the. low pressure turbines and exhausted into the main condenser where it is condensed and returned to the cycle as condensate. The heat rejected in the main condenser is removed by the Condenser Circulating Water System.

The first stage reheaters are supplied with steam from the A bleed steam line and the condensed steam is cascaded to the B feedwater heaters. The second stage reheaters are supplied with main steam and the condensed steam cascades' to the A feedwater heaters.

Heat for the feedwater heating cycle is supplied by the moisture separator reheater drains and by steam from the turbine extraction points.

The hotwell pumps take suction from the condenser hotwell and pump the ccndensate through the condensate polishing domineralizers.

Downstream of the polishers, the condensate flows through the condensate coolers, generator water coolers, hydrogen coolers, condenser steam air ejectors and the S.P.E.

steam seal condenser to the auction of the condensate booster pumps. The condensate booster pumps pump the condensate through three stages of intermediate pressure feedwater heaters (F, E, and D).

The flow combines with the D heater drain pump discharge before the C feedwater heaters, divides to the suction of the steam generator feedwater pumps.

The steam turbine driven 50

~_-.-.- -

i l

i cain feedwater pumps deliver feedwater through two stages of high pressure l

feedwater heaters (B and A), to a single feedwater distribution header where f

2 l

the feedwater flow is divided into two lines to the steam generators.

1 Brief descriptions of the power conversion systems are provided in the j

following sections.

i 1

i j

4.2.1 Main Steam and Turbine Evnass Systes Main steam is generated in the two steam generators by feedwater absorbing heat from the Reactor Coolant System. Main steam is conveyed by two lines, I

one per steam generator, to the turbine inlet valves.

A pressure equalization l

i j

cnd steam distribution header is connected to each main steam line upstream of the turbine inlet valves.

The main steam and turbine bypass system is shown j

in Oconee FSAR Figure 10 3-1, which is reproduced in Appendix B.

l I

l Eight spring loaded safety valves are located on each main steam line (a total of sixteen) to prevent over-pressurization of the Main Steam System under l

transient conditions. The valves, designated MS-1 through MS-16, are designed to pass 105 percent of the design steam flow at a pressure not exceeding 110 percent of the system design pressure (1050 pais).

i r

-l The turbine bypass system (TBS) is designed to reduce the steam line pressure 6

i following large turbine load reductions by dumping main steam directly to the I

main condenser. Two turbine bypass valves, MS-19 and MS-22, release steam l

1 from the A steam line; valves MS-28 and MS-31 release steam from the B steam i

line to the main condenser shells.

Steam supply piping from each turbine bypass header. feeds the startup steam header.

Check valves are installed to l

prevent crossflow between the main steam lines.

I High pressure steam supply piping provides steam from each main feedwater pump j

turbine following main turbine trip. In addition to an isolation valve in j

each line, the steam flow to each turbine is controlled by a governor and stop valve separate from the governor and stop valves controlling the low pressure l

bleed steam flow.

The high pressure governor and stop valves are designated i

MS-41 and 40 and MS-44 and 43 for feedwater pump turbines A and B, respectively. In addition to the steam supply to feedwater pump turbine 8, I

l l

51

the steam header from main steam line B supplies the three condenser steam air ojectors.

Separate lines are installed to supply high pressure steam from the two main steam lines to the two reheaters.

The two main steam lines supply the tuergency feedwater pump turbine. Check valves are installed to prevent cross flow between the main steam lines through the emergency feedwater pump turbine header.

Each of the supply headers off the main steam lines can be isolated by actor driven isolation valves.

Although not described, the branch steam piping has numerous steam traps in operation to remove condensate and normally isolated drain lines.

4.2.2 Turbine-Generator Svaten The turbine-generator system converts the thermal energy of steam produced in the steam generators into mechanical shaft power and then into electrical cnergy. The Oconee turbine-generator system normally is operated with an olectrical power output of 866 MW, but may be operated with reduced power output when required. Each unit's turbine-generator consists of a tanden (single shaft) arrangement of a double-flow high-pressure turbine, and three identical double-flow low pressure turbines driving a direct-coupled generator at 1800 rps. The Oconee high and low pressure turbines, extraction steam piping and moisture separator-reheaters are shown in Oconee FSAR Figures 10 3-4 and 10 3-7 which are reproduced in Appendix 5.

1 Main steam from the steam generators is directed to the high-pressure turbine through four parallel stop valves and four parallel control valves. After expanding through the high-pressure turbine, the exhaust steam passes through cxternal noisture separators and two stage steaa-to-steam shell and tube type reheaters. Extraction steam from the high-pressure turbine is supplied to the first reheater stage tube bundle in each reheater.- Main steam is supplied to the second reheater stage tube bundle in each reheater.

Reheated steam is cdaitted to the three low pressure turbines and expands through the low-pressure turbines to the main condensers.

52

- - - -. =- -

Part of the steam expanding through the turbines is extracted at selected points (pressures) to heat the feedwater pumped to the steam generators.

The

'A" (highest pressure), "B" and "C" feedwater henters are supplied from the l

high pressure turbine (or its exhaust).

The "A" bleed lines also supplies the first stage reheater.

The "D", "E" and "F" feedwater heaters are supplied i

from the low pressure turbines.

The "D" bleed lines also supply the main 4

feedwater pump turbines during power operation.

f Turbine-generator functions are monitored and controlled automatically by the Turbine Control System (TCS).

The TCS regulates the electric power production l

rate of the turbine-generator based on power demand signals from the I

i Integrated Control System. The TCS also includes redundant mechanical and

{

olectrical trip devices to prevent excessive everspeed of the turbine-generator.

Additional external trips are provided to ensure operation within j

conditions that preclude damage to the turbine-generator.

A standby manual control system is also provided in the event that the automatic control system is noc available.

I i

}

Based on turbine, generator, or condenser parameters exceeding limits, or on I

l loss of power to the turbine trip circuits or reactor trip auxiliary contacts in the CRDCS, the TCS develops trip signals to deenergize trip solenoid valves. These valves depressurize turbine hydraulic controls and result in closing the four high pressure turbine stop valves, four high pressure turbine f

governor valves and the six low pressure turbine intercept valves.

In i

cddition, low hydraulic system pressure signals are sent to the RPS to trip 1

the reactor upon turbine trip.

I l

4.2 3 Condenaar The condenser is designed to condense turbine exhaust steam for reuse in the steam cycle.

The condenser also serves as a collecting point for various j

cteam cycle vents and drains to conserve condensate which is stored in the condenser hotwell.

The condenser also serves as a heat sink for the turbine bypass system and is capable of handling 25 percent of rated main steam flow.

j Rejected heat is removed from the main condenser by the Condenser Circulating Water System. The condenser and condenser evacuation systems are shown in

.l Oconee FSAR Figures 10.4 1 and 10.4-4 which are reproduced in Appendix B.

53

~,

1 The condenser consists df three surface type deaerating condenser shells with cach shell condensing the exhaust steam from one of the three low pressure turbines.

The condensee shells are conventional shell and tube design with steam on the shell-side and circulating water in the tubes. A low pressure feedwater heater is mounted in the neck of each of the three condenser shells.

The combined hotwells of the three condenser shells have a water storage capability equivalent to approximately ten minutes of full load operation (nominally 142,000 gallons).

The condenser provides for condensing of steam, scavenging'and removal of noncondensible gases, and the deaeration of the condensate.

Impingement baffles are provided to protect the tubes from incoming drains and steam dumps.

The condenser can accept a bypass steam flow of approximately 18 percent of rated main steam flow without exceeding the turbine high backpressure trip point with design-inlet circulating water temperature. This bypass steam dump to the condenser is in addition to the normal duty expected.

The condenser evacuation subsystem is designed to remove noncondensible gases and air inleakage from the steam space of the three shells of the main condenser.

It consistr.f of 'the condenser steam air ejector subsystem and the main vacuum subsystem.

The condenser steam air ejector subsystem consists of three condenser steam air ejectors (CSAE) per unit. Normally each CSAE draws the noncondensible gases and water vapor mixture from one of the three main condenser shells to the first air ejector stage. The mixture then flows to the intercondenser where it is cooled to condense the water vapor and motive steam.

The second nir ejector stage draws the uncondensed portion of the cooled mixture from the intercondenser and compresses it further.

The compressed mixture then passes through the after condenser where it is cooled and more water vapor and motive steam are condensed. The intercondenser drains back to the main condenser and the aftercondenser drains to the condensate storage tank.

The main vacuum subsystem consists of three main vacuum pumps connected to the condenser crossties on the condenser steam air ejector subsystem to allow the 54

i main vacuum pumps to evacuate the main condenser, the main turbine casing, and the upper surge tanks during startup.

These pumps are only used during startup since normal operation requires the use of the CSAE only.

4.2.4 Condensate and Feedwater System The condensate and feedwater system purifies, heats and pumps the condensate from the condenser hotwells to the two steam generators to complete the steam-feedwater cycle.

The condensate and feedwater system is shown on Oconee FSAR Figures 10.4-4,10.4-7,10.4-8 and 10.4-13 which are reproduced in Appendix B.

Two of the three hotwell pumps normally are in operation to pump the condensate from the three condenser shell hotwells to the condensate booster pumps. From the hotwell pumps, a portion of the condensate normally flows through four of the five polishing demineralizers.

The flow is controlled by automatically regulating the pressure drop across the demineralizer bypass valve, C-14.

Ammonia and hydrazine are added to the condensate downstream of the demineralizers to control pH and reduce oxygen concentration.

The condensate flows through the hydrogen coolers and generator water coolers in parallel. The flow through the generator water and hydrogen coolers is controlled automatically by bypass valve C-81 to regulate the pressure drop across the coolers.

The flew through the hydrogen coolers is controlled independently by control valve C-58 to regulate hydrogen temperature. The condensate flows through the three condenser steam air ejector coolers to the auction of the condensate booster pumps.

Two of the three condensate booster pumps normally operate to pump the condensate through the low pressure feedwater heaters to the main feedwater pumps.

The condensate is heated in four stages of low pressure feedwater heaters:

F, E, D and C.

Three parallel F heaters heat the condensate by l

condensing steam from the three low pressure turbines. The E, D and C heaters tre arranged in two parallel flow paths.

The E and D heaters condense extraction steam from the low pressure turbine and the C heaters condense extraction steam from the high pressure turbine.

I 55 m.

4

,v-e

l From the low pressure heaters the condensate flows to the two main feedwater pumps.

The flowrate through the two feedwater pumps is controlled by the two j

main feedwater control valves based on reactor / turbine demand.

To increase the efficiency of the pumps, the pressure drop across the feedwater control l

valves is limited to 35 psi by regulating the speed of the feedwater pumps.

Under conditions of low flow demand with the control valves closing, the increasing pressure drop is measured and the pump speed demand signal from the ICS is reduced.

The resulting lower pump speed results in a decreased pressure drop across the valves.

In addition to the pump speed and feedwater flowrate controls, the minimum flow through each pump is limited to approximately 2500 gpm to protect the pumps.

Lower flowrates measured in the pump suction lines result in automatically opening bypass valves FDW-53(?) and FDW-45(?) which divert feedwater from the pump discharge lines to the upper surge tank.

i From the feedwater pumps, the water (which may at this point be termed feedwater) flows through the two parallel B high pressure feedwater heaters l

and two parallel "A" high pressure feedwater heaters.

The feedwater is heated to its final temperature in these feedwater heaters which condense extraction steam from the high pressure turbine.

Downstream of the common line from A feedwater heaters, the flow divided into two lines which individually feed the two steam generators.

i l

The equipment described above comprises the main flowpath from the condensers to the two mai'n feedwater lines.

However, the main flowrate pumped from the condenser hotwells (normal flowrate: 6.6x106 lba/hr) is approximately half of 6

the flowrate delivered to the two steam generators (normal flowrate:

11 3x10 1

)l lbm/hr).

The balance of the flow is pumped into the condensate and feedwater j

lines by the heater _ drain system.

The extraction steam condensed in the steam reheaters and the high and low pressure feedwater heaters is collected and pumped into the condensate lines at points of comparable temperature. The 4

i heater drain system is shown on Oconee FSAR Figure 10 3-7, included in this section, and Duke Power Drawing PO-123 A which was not available for this Gnalysis.

i i

I I

56

4 The heated feedwater flows to the two main steam generators through the two main feedwater lines.

The flowrate in each normally is controlled by the feedwater control valves, FDW-32 and FDW-41, which are positioned based on feedwater demand signals developed in the ICS.

At low flow conditions, the main feedwater control valves and the main feedwater block valves, FDW-31 and FDW-40, located in series with the control valves, are closed on automatic control signals from the ICS.

The feedwater flow s to the two steam generators, under these conditions, bypass the main control and block valves and are controlled by the two startup feedwater control valves, FDW-35 and FDW-44, which are positioned based on automatic control signals from the ICS.

Downstream of the feedwater control valves, the two feedwater lines penetrate the reactor building and inject the feedwater into the steam generators through the main feedwater ring headers.

As described above, the feedwater flowrate is controlled by ICS control signals to the main and startup feedwater control valves.

During power operation, the feedwater flowrates to the two steam generators are controlled principally to maintain constant and equal average reactor coolant temperatures in the two reactor coolant loops over the range of power production rates from approximately 155 to 1005 full power.

The control signals are modified as functions of steam generator heat balances (BTU limits), the status of key plant equipment (e.g.,

turbine trip, RC pump trip) i and steam generator level limits.

The feedwater control valve demand signals are limited based on high steam generator level as measured by pressure drops in the steam generator. Exceeding the high level control limit in either steam generator will result in ICS generated signals which trip the main f

feedwater pumps.

As the reactor power decreases below approximately 155 full power, the i

feedwater demand required to maintain reactor coolant average temperature i

results in a steam generator level less than the minimum level control limit.

As a result, the feedwater demand is controlled to maintain the minimum stea's

_ enerator level (approximately 30") allowing the reactor coolant average g

temperature to decrease over the reactor power range from 15% to of full

{

power.

57

As feedwater demand decreases, the main control valves and then the startup control valves will be closing.

As the startup valves close to a position more than 50% closed (based on measured valve positions), signals will be generated to close the main feedwater block valves.

These valves are closed to prevent possible leakage through the main control valves from interfering with the control of the startup valves. The block valves are automatically opened as the startup valves are positioned more than 80% open.

Following reactor trip, the feedwater flowrate is controlled to maintain steam gsnerator levels of approximately 30" with one or more RC pumps in operation.

If all four RC pumps are tripped, the ICS automatically increases the minimum level setpoint to approximately 20 feet to maintain the desired rate of natural (convective) circulation of reactor coolant through the core.

43 PROCESS AUXILIARY SYSTEMS Process Auxiliary Systems include those systems and subsystems that support the operation of the Nuclear System and Power Conversion Systems.

The major systems and subsystems identified in Section 3 2 as requiring detailed analysis are:

WO3 - Reactor Building Component Cooling Water WO4.A - Condenser Circulating Water WO4.D - Recirculated Cooling Water Brief descriptions of these systems are provided in the remainder of this section.

4.3 1 Reactor Building Comoonent Cooline Water This system is designed to provide cooling water for various components in the Reactor Building including: the letdown coolers, reactar coolant pump cooling jacket and seal coolers, quench tank cooler, and control rod drive cooling coils.

The design cooling requirement for the system is based on the maximum heat loads from these sources. The system also provides an additional barrier between high pressure reactor coolant and service water to prevent an inadvertent release of activity.

l l

58

The following is a brief functional description of the major components of the system.

Comoonent Cooler. Each component cooler is designed for the total system heat load for a reactor unit. Oconee 1 and 2 each have a single component cooler with a shared common spare. Oconee 3 has two coolers. The coolers reject the heat load to the Low Pressure Service Water System.

Comoonent Cooline Pumos.

Each component cooling pump is designed to deliver the necessary flows to the letdown' coolers, reactor coolant pump cooling jackets and seal coolers, quench tank cooler, and rod drive cooling coils.

Each unit has one operating pump and one spare.

Component cooline Surge Tank. This tank allows for thermal expansion and contraction of the water in the closed-loop system.

It also provides the required suction head for the component cooling pumps.

During operation, one component cooling pump and one component cooler recirculate and cool water to accommodate the system heat loads for each reactor unit.

The component cooling surge tank accommodates expansion, contraction, and leakage of coolant into or out of the system.

The surge tank would provide a reservoir of component cooling water until a leaking cooling line can be isolated. Makeup water and corrosion inhibiting chemicals are added to the system in the surge tank.

432 condenser circulatina water (ccw)

The Little River arm of Lake Keowee is the source of water for the CCW cystems. Each unit has four condenser circulating water pumps supplying water via two 11 ft. conduits into a common condenser intake header under the turbine building floor.

The discharge from the condenser is returned to the Keowee River arm of Lake Keowee.

The intake of the condenser circulating pumps extends below the maximum drawdown of the lake. The intake structure is provided with screens which can be manually removed for periodic cleaning.

59 I

The CCW systems are designed to take advantage of the siphon effect so the pumps are required only to overcome pipe and condenser friction loss. The siphon is initiated at start-up by plant vacuum pumps and sustained during operation by the continuous priming vacuum pumps.

The CCW system has a 48 inch emergency discharge line to the Keowee hydro ta11 race.

This discharge is connected to each of the three condensers of each i

unit.

Under a loss-of-power situation, the emergency discharge line will automatically open and the CCW system will continue to operate as an unassisted siphon system supplying sufficient water to the condenser for decay htat removal and emergency cooling requirements.

The vacuum is sustained by steam air ejectors.

4.3 3 Recirculated cooline water (RcW)

This system provides inhibited closed cycle cooling water to various components outside the Reactor Building including:

o RC pump seal return coolers o

Spent fuel cooling o

Sample coolers o

Evaporator systems o

Various pumps and coolers in the Turbine Building o

Instrument Air Compressors.

i i

The RCW system consists of four motor-driven pumps and four RCW heat exchangers to supply cooling water service to the three Oconee units.

A 25,000 gallon surge tank provides a surge volume to accommodate temperature changes and leakage. Condenser circulating water is used to cool the RCW heat exchangers.

l RCW effluent from the Auxiliary Building is mon.itored for radioactivity.

Leakage of radioactive fluids from any of the coolers in the Auxiliary Building will be indicated by these monitors.

Separate monitors are provided I

on the return lines from the Oconee 1 and 2 Auxiliary Building and the Oconee 3 Auxiliary Building.

60

During normal operation of the three Oconee units, three RCW pumps and three RCW heat exchangers will be in service.

One pump and one heat exchanger are installed as spares common to the three units.

61 e

_e.,

,~,

5.0 FAILURE MODES AND EFFECTS ANALYSIS OF SELECTED SYSTEMS 1

The analysis results documented in this report have been developed using failure modes and effects analysis (FMEA) techniques.

A FMEA identifies system level failure modes of concern and traces their effects on components, subsystems, and other systems.

Emphasis is placed on identifying significant effects associated with specific failures.

The advantage of the analysis technique is that while it is simple to apply, it provides for an orderly cxamination of potentially important failure modes throughout a plant.

In a FMEA, the impact or effect of a potential fault is documented in tables which identify the failure being considered.

Support systems associated with the failure (for example, instrument air for pneumatic diaphram operated valves) also must be considered.

Potential component fault modes due to internal failures or unavailability of support systems, the impact of the fault on system operation, and potential remedial action if the fault occurs are listed in the FMEA tables.

Analysis of the completed tables permits identification of failures which may have significant impact on system and plant operation.

The major systems identified in Section 3 as potentially affecting RCS overcooling have been analyzed using the FMEA techniques. The results of these analyses, including the effects of control instrumentation and supporting systems failures have been discussed in separate reports 6, 8 and 9.

The specific effects of failures in the systems identified in Table 310 as they relate to RCS overcooling are discussed in Section 5.

The majority of these RCS overcooling effects have been obtained from the more general FMEA's of the identified systems.

The RCS overcooling effects resulting from failures in the RCS subsystems (Pressurizer, RC Pumps and Steam Generators) and associated control instrumentation and support systems are identified and discussed in Section 5.1.

The RCS overcooling effects of failures in the Power Conversion and Makeup and Purification systems are discussed in Sections 5.2 and 5 3, respectively.

62

5.1 REACTOR COOLANT SUBSYSTEMS As discussed in Section 3, three RCS subsystems have been identified as potentir211y contributing to overcooling transients:

the Pressurizer, RC Pump and Steam Generator subsystems. The overcooling failure modes and interfacing systems associated with the failure modes are listed for each RCS subsystem in Table 5.1.

As noted, component level FMEA's of each of these subsystems are presented in Tables 5.2, 5.3 and 5.4 The results of the FMEA's are discussed below in Sections 5.1.1, 5.1.2 and 5.1 3 for the Pressurizer, RC Pump and Steam Generator subsystems.

5.1.1 Pressurizer Subsystem Two overcooling failure modes have been identified for the pressurizer

~

subsystem:

Release of reactor coolant and excessive pressurizer spray flow rate. In Table 5.2 the specific component level failures leading to or contributing to these failure modes are identified with the potential causes of the failure, its effect on the RCS and possible remedial actions listed for each.

A release of reactor coolant (a small LOCA) will result initially from either the PORV or pressurizer code safety valve opening and failing to close.

Code safety valves are passive devices which open when the fluid pressure on the valve's seat overcomes the spring force holding the valve closed.

The valves are designed to close when the fluid pressure is no longer sufficient to hold the valve open (which is typically lower than the opening pressure).

Safety valves could fail to close due to improper valve maintenance or possibly l

severe operating conditions (e.g.,

liquid discharge) which could result from control systems failures.

If one of the safety valves does fail to close, the leak path cannot be isolated (see Item 1, POR7 Fails Open).

The PORY (pilot operated relief valve) opens and closes in response to external control signals.

The relief valve is opened by applying power to the pilot valve solenoid. This results in the pilot valve opening and applying fluid pressure to the relief valve operator which opens the relief valve.

The relief valve is closed by deenergizing the pilot valve solenoid.

f l

63

TABI.E 5.1.

SUMMARY

OF RCS SUBSYSTEM FAII.URE MODES Interfacing Systems and Components RCS Subsystem Overcooling Failure Mode Affecting Failure Mode Comments 1.

Pressurizer 1.1 Release of Reactor Coolant 1.1.1 PORV FMEA of Pressurizer System presented in Table 5.2.

1.1.2 HNI 1.1.3 Pressurizer Code safety valve 1.2 Opening the Pressurizer 1.2.1 Pressurizer Spray Valve Spray valve 1.2.2 NHI 2.

RC Pumps 2.1 Release of Reactor Coolant 2.1.1 RC Pump Shaf t Seals FMEA of RC Pumps presented in Table 5.3.

2.1.2 RB Component Cooling j[

Water System 2.1.3 MULP System 3.

Steam Generators 3.1 Release of Peactor Coolant 3.1.1 Steas. Generator Tubes FMEA of Steam Generators presented in Table 5.4.

3.1. 2 Main Steam and Turbine Dypass System 3.2 Increased Heat Transfer 3.2.1 Main Steam and Turbine Bypass System 3.2.2 Feedwater and Condensate System 4.

Balance of RCS 4.1 Release of Reactor Coolant 4.1.1 MU5P System FMEA of MU&P System presented in Table 5.7.

(

I

TaaLE 5.2.

susuutaf 0F PRESSORIERR SYSTERI FIISA: FAIIARES LEADIIIG TO Det AFFECTIIIG BCS OFE3000LIIIG TRAII51EIFFS Failure Possible causes Effects Remedial Actions belease of Reactor Coolmat 1.

FORV RC-RV3 IIechanical failure of valve small I.OCA.

Pressurizer fills Emergency procedures for small Fails Open resulting in valve opening during RCS depressur ization.

LOCA's must be followed. Open or failure to close once Pressuriser heaters energized.

FORV may be identified by PORV

open, accoustic monitor (detail s unavailable) and/or discharge pipe high temp. fr.dication. LOCA may be terminated by closure of the PORV Block valve, RC-4.

2.

Pressuriser IIechanical f ailure of Small LOCA or RCS leak.

Emergency procedures for small Code safety valve (s) to close after Pressuriser fills during LOCA must be followed. Open valve Fails

opening, depressurization. Pressurizer valve may be identified by to close heaters energized.

discharge pipe high temperature indication.

eu 3.

Power to rostV o IWII Pressuse sultch Pottv opena resulting in n Bnergency procedures for smalI solenoid (RC3-PSS) er Controller small LOCA.

Pressuriser fills LOCA's must be followed. Open Fails on (RC3-IIIS2) Failure during depressurization.

PORV may be identified by PORV Pressuriser heaters accoustic monitor (details energized, unavailable) and/or discharge pipe high temp. Indication. LOCA may be terminated by closure of the FORV Block valve, RC-4.

POttV manual control may be operable.

.-. - - - - --.~ - -

t TARES 5.2.

(Continued)

Failure Possible Causes Effects Remedial Actions o Wul narrow range RCS PORV opens resulting in a Emergency procedures for small pressure transmitter or small LOCA.

Pressurizer fills LOCA's must be followed. Open signal conditioning modules during depressurization.

PORV may be identified by PORV produce spurious high RCS Pressuriser spray valve RC-V1 accoustic monitor (detalla pressure signal.

opens and pressurizer heaters unacallable) and/or discharge pipe are deemergized.

high temp. Indication. 1ACA may be terminated by manual closure of the FORV, RC-Rv3 or its block valve RC-4.

The pressuriser spray l

valve, RC-VI, may be manually closed and the pressuriser heaters manually controlled.

L fraammalaer spray Walee Falla Open 4.

Pressuriser mechanical failure of valve Slow RCS depressurization with Identify open valve and close spray valve, resulting in valve opening the pressuriser heaters spray block valve, RC-V5.

g RC-VI Fails or failing to close once energized. ESPS 1500 psi RCS cpen open.

pressure setpoint may be reached depending on the spray flourate i

and beater capacity.

i 5.

sewer to e Rul pressure switch, RC-PS3 cpray valve opens resultir.g in Identify open valve and close spray valve or controller (RC-W181) a slow RCS depressurization with spray block valve, RC-V5.

Spray solemeld failure.

the pressuriser heaters valve manual control may be Falls on energized. ESPS 1594 ps! RCS

operable, f

[

pressure setpoint may be reached

(

l depending on the spray flourate and heater capacity.

t i

r l

t

?

L I

I i

L

_m

.._._m

.m t

r 3

l i

i Tass.a 5.2.

(Continued)

I i

Failure Possible Causes Effects Remedial Actions o Rut naseou range RCS FORV opens resulting in a Roergency procedereo for small pressure transmitter or small s.oCA.

Pressurizer fills IACA's mest be followed. Open l

signal conditioning modules during depressurization.

FORY may be identified by PORW l

produce sperious high RCS Pressuriser spray valve DC-VI accoustic monitor (details pressere signal.

opens and presser 1:er heaters unavailable) and/or discharge pipe are deemergized, high temp. Indication. LOCA may be terminated by manual closure of the FORV, RC-RV3 or its block valve RC-4.

The pressuriser spray valve, RC-VI, may be manually closed and the pressuriser heaters manually controlled.

4 Cankz1hatlag Failures D

6.

Failure of Transmitter fa!!ure or a A selected low pressuriser level The operator can compare the three Selected failure of the selected signal results in the makeup pressuriser level measurements Pressoriser transmitter's power supply valve opening and filling the through the computer and manually 1.evel (ICS Pamelheard RI branches pressuriser, deemergizing the select an operable transmitter for

-Transmitter 3RI, ARY or Computer pressoriser heaters and possibly control and indication. Manual Output Si p t Penelheard RS)

-Smitiating a steam generator control of the makeup valve (and 1

Emu everfill transient (see Table feeduster control valves) is l

5.3, FREA of the Steam available. The loss of a i

Generators). If the pressurizer transmitter power supply is is allowed to fill, the FORV alarmed in the control room.

will be opened and the possible ligold discharge through the i

valve could contritete to its failure.

I r

.L

. _. ~_.._. -

TABLE 5.2.

(Continued)

Failure Possible Causes Effects Remedial Actions 7.

Failure of T/C opens or circuitry Low indicated discharge line This failure may bo difficult to the Bellef/

deenergized.

temperature. This failure detect and may remain undetected would be confusing to the for some period of time. The safety valve Discharge Line operator if the associated failure may be detected by a valve leaked or failed open.

comparison of the three T/f*

Thermocouple readings and confirmed by test (prior to a postulated relief or safety valve failure).

S.

Failure of Monitors fall to operate Monitor incapable of detecting This failure may be difficult to the FORY (details unavailable),

an open or leaking PORV.

This detect and may remain undetected failure would be confusing to for some period of time. Failure Accoastic Monitor the operator if the PORV may be detected by periodic leaked or f ailed open.

surveillance testing (detalls unavailable).

9.

Failure of Valve or valve motor Isolation valve would be These fa!!ures may be difficult to DORV or power failure.

incapable of isolating the detect and may remain undetected Pressurizer relief or spray flow in the for some period of time. An event the associated FORV or unisolated open FORV tranJient le Spray valve Isolation spray valve failed open.

controlled by emergency twocedures for a small LOCA. An unisolated Valve Open spray valve could require tripping the associated RC g amp er I using i

the PORV for depre...Jurization or careful control of RCS temperature.

- The P0HV may fail open in response to mechanical failures of the relief valve j

or pilot valve (Item 1) or a control circuit failure which energizes the pilot l

vcive solenoid or fails to deenergize the solenoid (Item 3).

Certain circuit j

failures such as a failure of the valve's control switch or pressure switch i

may occur with other pressurizer components operating normally.

The d: creasing pressurizer pressure will be detected resulting in the spray valve i

{

closing and the pressurizer heaters being energized.

Other failures, such as those generating spurious high pressurizer pressure signal, will result in the l

l PORV and spray valve opening and deenergizing the pressurizer heaters. In I

contrast to safety valve failures, a failed open PORY may be isolated by

{

canually initiating PORY block valve closure. Closure of the block valve will i

tsrminate the release of reactor coolant.

}

Opening the pressurizer spray valve results in a flow of reactor coolant from the discharge of the reactor coolant pumps to the lower pressure pressurizer steam space. This results in a condensation of steam in the pressurizer hnd a l

raduction in RCS pressure.

If the spray valve opened and failed to close, the rssulting RCS pressure decrease could result in a reactor trip and possibly a I

spurious actuation of the ESPS.

1 The pressurizer spray valve is an "on-off" solenoid operated valve.

When the 1

i high pressurizer pressure setpoint is reached, the solenoid is energized which opens the valve.

Deenergizing the solenoid closes the valve.

As shown in Table 5.2, the pressurizer spray valve could fail open or fail to close due to mechanical failure of the valve or a control circuit failure snergizing the solenoid. Circuit failures include failures of the pressure cwitch or valve control switch which result in the spray valve opening with cther components remaining operable.

The resulting pressure decrease will I

result in the pressurizer heaters being energized which may reduce cignificantly the rate of depressurization.

Failure of the pressurizer pressure transmitter or associated signal j!

conditioning modules producing a spurious high pressuriser pressure signal clso will result in the spray valve opening.

The effects of the spurious high 69 9

v.

,rg,-

-,e<

-s,,.

-+

a-

,--n

---4

pressure signal include opening the PORY (a small LOCA) and deenergizing the pressurizer heaters in addition to opening the spray valve.

In addition to failures which directly result in a potential overcooling transient, other Pressurizer System failures which may exacerbate the effects of such a transient have been identified in Table 5.2, Items 6-9 These failures include instrumentation failures which could impede the detection of en open relief or safety valve, failures of the PORY or spray ve.lve isolation valves which could prevent rapid termination of a transient resulting from a failed open PORV or spray valve. Failure of the selected pressurizer level transmitter low has been included in this category since a pressurizer overfill transient could occur. If the overfill was allowed to result in liquid discharge through the PORV or safety valves, valve damage could occur.

5.1.2 RC Pumo Subsystem One RCS overcooling mechanism has been identified in the RC pump subsystem, a ralease of reactor coolant due to failure of the RC pump shaft seals. RC pump i

a:al failures may result from several possible causes as shown in Table 5 3 l

If degraded performance of the RC pump seals is recognized by the operator

'l prior to complete failure of the seals, seal failure may be delayed by l

tripping the affected pump.

Once seal failure occurs, however, the resulting small LOCA cannot be isolated.

5.1 3 steam cenerator subsystem Two potential overcooling mechanisms have been identified for the steam generator subsystem:

release of reactor coolant due to steam generator tube failure and increased heat transfer rate across the steam generator tubes.

The FMEA of the steam generator subsystem is presented in Table 5.4.

Steam generator tube leaks occur during normal operation typically due to a combination of causes as listed in Table 5.4.

Although control system failures have not been identified as a single, sole cause of a tube leak or failure, control system failures may initiate a tube failure in combination with other existing conditions or increase the rate of tube degradation.

i 70

TARI.E 5.3.

FleEA OF EC PUI8PS: FAII,URES I.EADIBIG TO OR AFFECTING RCS OVERCOOLifIG TRANSIEtr.'S Failure Possible Causes Effects Remedial Actions Releast._9L Reactor Coolant 1.

RC Pump Seal o Simultaneous loss of Small I OCA.

Seal f ailures can Trip pump prior to seal failure Failure pump seal injection and not be isolated.

and achieve cold shutdown.

RB component cooling Emergency procedures for small water.

LOCA's must be followed once seal failure occurs.

o Failure of seal Same as above.

Same as above.

Injection following operation with excessive seal wear or damage.

o Undetected seal Same as above.

Same as above, materiale defects.

9

>d o Injection of Same as above.

Same as above, particulates into seal-staft surface, o Excessive thermal Same as above.

Same as above, cycling of seals.

TamLE 5.4.

PsetA OF STRAft CENERATURS: FAII.URES LEADING TO OR AFFRCTIhG RCS OVERCOOLING TRANSIENTS Failure Possible Causes Effects Remedial Actions pelease ol_RCSK1gr coolant 1.

Steam Generator o Material def ect n in tutses.

Steam generator tube rupture Emergency procedures for steam Tube Failure accidents a small break I4WA generator tube rupture accident with the reactor coolant must be followed.

released to the main steam system and condenser.

o I.ong term operation with Same as above.

Same as above, adverse feedwater chemistry.

O Escessive magnitude /

Same as above.

Same as above.

frequency of ccapression and tension cycles on tubes with undetected defects in y

tube material.

O Severe cocidown of RCS with Same as aleve.

Same as above.

undetected defects in tube material.

Increased Beal _ Transfer Ratt 2.

Depr essuri-o Turbine bypass valve (s)

Small steam line " break" Identify leak path and isolate if zation of fail open.

accident. Rapid cooldown of possible. Follow emergency 8 Balm Steam RCS.

for steamline breaks. See FMEA System of Main Steam Systems, Table 5.5.

Main steam code safety Same as above.

Same as above.

o valve (s) fall open.

o Failure to trip or runback Same as aleve.

Same as above.

turbine following teactor trip.

- - ~.. - _ - -. - -. _.. -.- -

4 7A882 5.4.

(Continued)

Fat Ier e Fossible Causes Effects Remedial Actions 3.

Injection of o noin feedwater control steam generator level increases Manually trip main feedwater pumps Feedwater at valve f alls ogen or until main feedwater pumps are and confirm automatic initiation mates in Escoes fails to close.

tripped on high steam generator and control of emergency feedwater of DCS Dep tre-level. Emergency feedwater system. See FMEA of Main meets (steams system automatically started and Condensate and Feedwater System, Generator controlled.

Table 5.6.

Deerfilt) o Startup feedwater control Same as atme.

Same as above, valve falls ci,en or falls to close, w

bB

[

L

The impact on RCS overcooling depends on the rate of release of reactor coolant.

The more common small leaks may not result in overcooling, as d; fined, if the makeup system is capable of injecting coolant at the tube leak rate.

However, the less frequent tube rupture transients resulting in a leak rate of hundreds of gallons per minute are small LOCA's. In addition to the direct effects of the release of reactor coolant, steam generator tube rupture procedures typically require a rapid cooldown and depressurization of the RCS, Under these conditions, the potential for an overcooling transient resulting from improperly controlling the RCS cooldown exist even for smaller tube leak rates.

RCS overcooling transients resulting from increased steam generator heat transfer rate have been identified in Table 5.4, Items 2 and 3 In either case, however, the initiating control system failures occur in the main steam or main feedwater systems.

These failures are considered, in detail, in the FMEA's of the Main Steam and Turbine Bypass System and the Condensate and M n Feedwater System discussed in Sections 5.2.1 and 5.2.2.

5.2 POWER CONVERSION SYSTEMS l

As discussed in Section 5.13, the increased steam generator heat transfer RCS overcooling mechanism can be initiated by failures in the main steam and main feedwater systems.

Specific failures in these systems leading to potential RCS ovaret oling are discussed in Sections 5.2.1 and 5.2.2.

5.2.1 Main steam and Turbine Bvoass system The principal effect of failures in the main steam and turbine bypass system l

on RCS overcooling is the potential for depressurizing the steam generators.

l As discussed in Section 3, reducing the steam generators' pressure reduces the l

caturation temperature on the secondary side of the steam generators and l

increases the heat transfer rate from the RCS.

Failures in the main steam and turbine bypass system depressurizing the main steam system and the resulting offects on the RCS are listed in Table 5.5.

The information in this table was 4

cxtracted from more general FHEA's of the Power Conversion Systems which are presented in Appendix C.

74 i

-.m.

TABLE 5.5.

SulutARY OF RAIN STRAR AND TURBINE BYPASS FMEA: FAIIJ8RES LRADING 10 OR AFFECTING RCS OVERCOOLING Failure Possible Causes Effects Remedial Actions Depressuriaallon of main stama_Eystem 1.

One or More Main Mechanical failure of valve, Steam leakage to the atmosphere.

Emergency procedures for a small Steam Safety improper maintenance, Depending on the response of the steam line break must be followed.

Valves (MS-1 discharge of entrained turbine and reactor controls, Isolation of feedwater to affected through MS-16) liquid through valves, automatic reactor and turbine steam generator may be required to 0

Falls to Close trip and potentially overcooling prevent exceeding 100 F/hr RCS Following of the RCS could occur.

cooldown rate.

Turbine Trip 2.

One or Both Steam Mechanical failure of Steam diverted to condenser.

Identify open valve (s) and j

Generator A valve (s) or transducers, Depending on the resionse of the manually close isolation valve Turbine Bypass improper maintenance, turbine and reactor controls and MS-17 as required to control RCS Valves (MS-19, the main condenser, automatic cooldown rate.

22) Fail Open or reactor and turbine trip and Fall to Close potentially overcooling of RCS y

un Following Turbine could occur.

d Trip 3.

Both Steam o Spurious output of manual Steam diverted to condenser.

Identify open valve (s) and Generator A control station SSISA-MC Depending <m the response of the manually close isolation valve Turbine Bypass (aux. shutdown panel) turbine a J reactor controls and MS-17 as required to control RCS Valves (RS-19, signals valves to open.

the main condenser, automatic cooldown rate.

22) Open in reactor turbine trip and l

Response to a potentially overcooling of RCS Spurious could occur.

Control Signal o Spurious high output from Steam diverted to condenser.

Identify open valves and manually selected steam generator A Depending on the response of the control. Close isolation valve outlet pressure transmitter turbine and reactor controls and MS-17 if required to limit RCS (SS6A-PTl or PT2) or train the main condenser, automatic cooldown rate.

A control circuit modules, reactor and turbine trip and potentially overcoollag of RCS coutd occur.

l

_m i

TABLB 5.5.

(continued)

Failure Possible Causes Effects Remedial Act.lons 4.

One or Both Steam Mechanical failure of Steam diverted to condenser.

Identify open valve (s) and Generator B valve (s) or transducers, Depending on the response of the manually close isolation valve Turbine Bypass improper maintenance.

turbine and reactor controls and MS-26 as required to control RCS Valves (MS-20, the main condenser, automatic cooldown rate.

31) Fall Open or reactor and turbine trip and Fall to Close potentially overcooling of RCS Following Turbine could occur.

Trip 5.

Both Steam

.o Spurious output of manual Steam diverted to condenser.

Identify open valve (s) and Generator B control station SS15A-MC Depending on the response of the manually close isolation valve Turbine Bypass (aux. shutdown panel) turbine and reactor controls and MS-26 as required to control RCS Valves (MS-28, signal valves to open.

the main condenser, automatic cooldown rate.

31) Open in reactor and turbine trip and Response to a potentially overcooling of RCS Spurious could occur.

Control Signal y

o Spurious high output from Steam diverted to condenser.

Identify open valves and manually selected steam generator B Depending on the response of the control. Close isolation valve outlet pressure transmitter turbine and reactor controls and MS-26 if required to limit RCS i

(SS6A-PTl or PT2) or train the main condenser, automatic cooldown rate.

A control circuit modules.

reactor and turbine trip and potentially overcooling of RCS could occur, 6.

Steam Generator common setpoint module Steam diverted to condenser.

Identify open valve (s) and A and B Turbine generates a spurious low Depending on the response of the manually close isolation valve Bypass Valves setpoint pressure.

turbine and reactor controls and MS-17 and MS-26 as required to (MS-19, 22, 28, the main condenser, automatic control RCS cooldown rate.

31) Open in reactor and turbine trip and Response to a potentially overcooling of RCS Spurious could occur.

Control Signal 4

1

f TABLE 5.5.

(Continued)

Failure Possible Causes Effects Remedial Actions 7.

Steam Generator An initiating transient Steam diverted to condenser Manually control turbine bypass A and R Turbine causing turbine trip followed coupled with a main feedwater and main feedwater control valves.

Bypass Valves by a loss of ICS Panelboard overfeeding of the steam If required, trip main feedwater (MS-19, 22, 28, RI branch a or Ill ( Auto generators. Unless manually pumps and verify automatic

31) Fall to Power).

terminated, the potential for initiation and control of

~

Close Following RCS overcooling is significant.

emergency feedwater.

Turbine Trip 8.

Diversion of Unknown - PO-284-1 not Steam diverted f rom IIP turbine -

Identify diversion of steam and Steam to available, may cause turbine and reactor close isolation valves MS-24 and Startup trip and potential overcooling 33.

3 team Neader of RCS.

9.

Main Turbines o Contacts in CRDCS fall to Following reactor trip, Attempt to manually trip the high Fall to Trip open on reactor trip, continued steam flow through the and/or low pressure turbines.

Following turbines would result in Hanually throttle main feedwater y

Reactor Trip depressurization of the tushine to control RCS depressurization 4

header, throttling of the turbine if required.

governor valve and possible overcooling of the RCS., Feed-water flowrate to steam generators initially throttled until low steam generator level setpoint is reached. The extent' of RCS overcooling following this transient is unknown.

o Unspecified failures in same as above.

Same as above.

turbine control system (details of turbine control instrumentation unavailable).

TAmt.E 5.5.

(Continued)

Failure Possible Causes Effects Remedial Actions Contribaattag_yallurgs 18.

Failure of Mechanical failure of valve Failure of normally open isota-Identify and repair open valve.

Turbine Bypass or or operator, loss of electric valves may remain undetected If a steam release should occur, Startup meader power to valve.

during normal operation. Under follow emergency procedures for a Isolation Valves these conditions, an open startup steam line break.

(ns-17, 26, 24, header or turbine bypass flow-33) path could not te isolated.

11.

Failure of a contact " sticks

  • in position.

The redundancy of turbine trip Identify the closed contact and CRDCs Turbine contacts would provide a turbine repair. This failure would be Trip contact to trip signal. However, failure difficult to identify and may Open on Demand of a contact would reduce the remain undetected for a available redundancy.

significant period of time depending on the testing y

procedurally required.

ce

I l

1 i

l The failures potentially resulting in depressurizat'.on of the main steam t

i cystem include failures of main steam safety valves or turbine bypass valves to close as designed, a diversion of steam to the startup steam header and j

failure of the main turbine to trip following reactor trip.

l i

l The sixteen main steam code safety valves (eight valves per steam generator) f cre spring loaded valves that open due to high steam pressurg on the valve meat.

As the steam pressure decreases, the valves automatically close due to l

}

the force of the springs on the valve seats.

Following turbine trip, some of f

the safety valves are expected to open.

Improper valve maintenance could result in one or more safety valves failing to close at their (closure) l I

a setpoint pressure potentially leading to RCS overocoling.

I' In addition to the safety valves, four turbine bypass valves are installed to j

control the steam line pressure following turbine trip.

Two turbine bypass l

valves are connected to the steam line from each steam generator and may be J

isolated from the steam line by a manually operated isolation valve. Each pair of valves is controlled by a separate control circuit based on the i

pressure of the associated steam line.

i l

Failure modes of the turbine bypass valves include those affecting one of the t

valves, both valves on either steam line and, potentially, all four valves.

I Failure of a single valve open or its failure to close (Items 2 and 4) could t

i be caused by a mechanical failure of the valve, its pneumatio operator or the j

i associated E/P transducer. Failure of both valves on either steam line to I

cpen or their failure to close (Items 3 and 5) would be caused by failures in f

the common control instrumentation strings, j

i

}

{

Two failure modes were identified which potentially could cause all four l

valves to open.

Failure of the pressure setpoint module common to both 1

instrument strings (Item 6) could result in both instrument strings signalling l

l the four turbine bypass valves to open.

The second failure mode resulting in j

the four turbine bypass valve failing to close (Ites 7) involves a sequenced loss of the ICS Panelboard II branch H or M1 (auto power).

The specifie offect of a loss of auto power is to transfer the turbine bypass valve to j

canual control.

The valves would then remain in their esisting position.

If 1

i 79 3

the power failure occurred immediately following turbine trip, the four turbine bypass valves would be open and thus remain open.

For the case of this particular power supply failure, the main feedwater control valves also transfer to manual and remain open (see Table 5.6).

Although this failure mode sequence appears highly unlikely, similar events have occurred (Oconee Reactor Trip ?-35, 11/10/79).

It is believed tnat the response of the control instrumentation to a transient (which may be caused by control instrumentation failure) increases the likelihood of subsequent isolation of the instrumentation pot er supplies.

It should be noted that most power supply failures other than branch H or H1 will cause the turbine bypass valves to close and remain closed.

For any of the turbine bypass valve failure modes identified, the operator has the option of closing one or both inslation valves and terminating the depressurization.

Diversion of steam to the startup steam header has been identified as a possible cause of steam line depressurization affecting both steam generators.

However, information concerning the distribution of steam to the startup steam piping has been unavailable. Should a control failure in the startup steam piping result in a significant diversion of steam from the steam lines, the operator has the option of terminat,ing the depressurization by manually aloning both startup header isolation valves.

Failure of the main turbine to trip following reactor trip has been identified ca a possible cause of significant ateam generator depressurization.

However, the potential for auch a transient to occur, while believed to be very unlikely, remain unevaluated due to unavailability of turbine control instrumentation design information.

Following reactor trip, contacts in the j

CRDCS open to signal the turbine controls to automatically trip the turbine.

Should the CRDCS turbine trip contacta fail, the steam lines will begin to depressurize. The lower steam pressure would be sensed by ICS and a signal sent to the turbine controls to close the turbine throttle valves. Whether cther parameters input to the turbine controls (e.g., turbine speed) would override the ICS signal and maintain the turbine throttle valves open is 80

unknown.

However, should the turbine trip and throttle valves fail to close following a reactor trip, RCS overcooling potentially could occur.

Two failures have been identified which would result in an immediate steam line depressurization but could increase the severity of other subsequent failures (Items to and 11).

The failures identified are failures of the turbine bypass valves' isolation valves and a failure of a CRDCS turbine trip contact.

It is believed that either failure could occur and remain undetected for a significant period of time.

5.2.2 Condensate and Main reedwater system The principal effect of failuran tr. Lne Condensato and Main Feedwater system on RCS overonelir.e is the potential for overfeeding the steam generators.

Following reactor trip, the potentially rapid increase in stsam generator inventory is expected to result in RCS overcooling until manually or cutomatically terminated.

Specific failures in the Condensate and Main Feedwater System leading to overfeeding the steam generators and the overall effects of these failures are identified in Table 5.6 and discussed below.

Steam generator overfeeding will occur if either main feedwater control valve fails open or fails to close following a reduction in feedwater demand such as a reactor trip.

Typically, failing the control valve open would be expected to have a greater impact on RCS overcooling at Icw reactor power levels while the failure to close would be more severe at higher reactor power levels.

Failure of one of the two control valves to the open position could occur due to a mechanical failure of the valve or its operator, failure of the E/P transducer or failure of the associated ICS loop A or loop B feedwater control circuit (Item 1).

In the event one of the control valves failed open, the cperator has the option of manually closing the main valve and controlling the startup valve, if possible, or tripping the main feedwater pumps.

If the cperator fails to control main feedwater flow, the main feedwater pumps will be tripped automatically on high level in either steam generator.

The extent cf RCS overcooling prior to automatic pump trip is unknown.

81

TABLE 5.6.

SUNNARY OF CONDFNSATE AND NAIN FEEDWATER FNEA: FAILURRS LEADING M OR AFFECTING RCS OVERC00 LING TRANSIENTS Failure possible Cappes Effects Remedial Actions Excessive Mdition of FegdwatgLtG_StgaptGepergL.Qgg 1.

Main Feedwater o Unspecified failure in Steam generator A or p level Trip main feedwater pumps manually control Valve valve operator or increases possibly resulting in if required to control RCS FDW-12 or

. associated valve control reactor trip. Continued feed-overcooling. Confirm automatic FDW-41 Falle s ta t.lon.

water injection following reactor initiation and control of Open trip expected to result in RCS emergency feedwater.

overcooling until tetminated by high steam generator level trip of main feedwater pumps and subsequent automatic initiation and control of emergency feedwater. (Automatic clonure of associated main feedwater block valve FDW-31 or FtW-40 is expected; however, this slowly closing valve is not expected to prevent the high level feedwater pump trip.)

o ILJ Lcop A or Loop 3 Steam generator A or B level Manually close main feedwater feedwater control cfrcuit increases possibly resulting in control valve and manually control generates a spurious high reactor trip. Continued feed-startup control valve in the demand signal due to a water injection following reactor affected loop. Trip main module failure.

trip expected to result in RCS feedwater pumps manually if overcooling until terminated by required to control RCS high steam generator level overcooling. Confirm automatic control setpoint or high steam initiating and control of generator level trip of main emergency feedwater.

feedwater pumps and subsequent automatic initiation and control of emergency feedwater.

TABLE 5.6.

(Continued)

Failure Possible Causos Effects Remedial Actions o Failure of Steam Generator Steam generator A or D level Manually close main feedwater Startup aange bevel increases possibly resulting in control valve and manually control Transmitter Senelog Tap.

reactor trip. Continued feed-startup control valve in the water injection f ollowing reactor af fected loop. Trip main trip expected to result in RCS feedwater pumps manually if overcooling until terminated by required to control RCS high steam generator level overcooling. Confirm automatic control setpoint or high steam initiating and control of generator level trip of main emergency feedwater. Manually feedwater pumps and subsequent control emergency feedwater based automatic initiation of emergency on steam generator operator range feedwater. Emergency feedvater level signals.

continues to overfill affected steam generator, ao 2.

Main Feedwater Power to selected startup Degending on the manual selection Manually close main feedwater Ld Control Valves level transmitter falls of the HEX or HEY powered startup control and startup valves and FDW-32 and/or (ICS Panelboard KI, branch level trensmitters, either or makeup control valves. Automatic FDW-41 Fall HEX or HEY).

both main feedwater control control may be restored by manual Open valves open resulting in over-nelection of operable steam feeding of the associated steam generator startup level and generators and possible RCS over-pressure transmitters and cooling. The transient is auto-pressurizer level transmitters.

natically terminated by high steam generator level trip of the main feedwater pumps and auto-matic initiation and control of emargency feedwates. In addition to effects on feedwater control, these power failures could result in opening the makeup control valve and closing the loop A and/or B turbine bypass valves depending on manual transmitter selection.

TABb8 5.6.

(Continued)

Failure Possible Causes Ef fect s Remedial Actions 3.

Main Feedwater o boss of Instrument Air Following reactor trip, the Manually trip main feedwater pumps Control valves Pr essur e.

supply of feedwater to the steam if required to control RCS over-FDW-32 and/or generators exceeds the RCS demand cooling. Follow emergency proce-FDW-41 Fall to resulting in increasing steam dure for loss of instrument air.

Close Following generator levels and possible RCS Reactor Trip overcooling. The transient is terminated by an automatic high steam generator level trip of the main feedwater pumps and auto-matic initiation and control of emergency feedwater using the backup nitrogen system.

I.oss of instrument air also results in closure of the turbine bypass valves, the makeup control valve o3 a-and RC pump seal return valve and opening the RC pump seal injection control valve.

o 1.osa cf ICS Panelboard KI Following reactor trip, the steam Manually close main feedwater Auto Power branch (H, lill generators will be overted control valves and manually or manual transfer of main resulting in [essible RCS over-control main feedwater startup feedwater control valve to cooling. 1he transient termina-turbine bypass and makeup control manual control, ted automatically by a high steam valves if required.

generator level trip of the main feedwater pumps.

I.oss of auto power also results in the makeup, PC pump seal injection and turbine bypass valves trano-ferring to manual and freezing in position. If the power failure occurred following turbine trip, the turbine bypass valves could fail in an open position resultitsg in a steam generator depressurization.

TABLE 5.6.

(Continued)

Failure Potsibis Causes Effects Remedial Actions o Loss of ICS Panelboard KI Main feedwater control valses Manually trip main feedwater pumps Hand Power branch (HX, HlX) freeze in position and main feed-if required to control RCS over-or unspecified failure of water pumps run back to a speed cooling. Transfer power supplies feedwater control valve or corresponding to a 0 volt signal. to Panelboard EU to retain auto-operator.

Turbine bypass valves close and matic control of makeup and remain closed. Initial over-turbine bypass valves.

filling of steam generatore and possible overcooling of itCS may occur. The transient would be terminated automatically by a high steam generator level trip of the main feedwater pumps or closure of the main feedwater block valves, FDW-31 and 40.

oo Contributina Failutta' 4.

Main reedwater FFTX relay or associated Failure could occur and remain If required, manually trip main Pumps Fall to steam genetator operate range undetected during normal feedwater, condensated booster or to Trip level transmitters or high operation. The automatic rain hotwell pumps to terminate Automatically level bistables fall to feedwater pump trip would not

overfill, on High Steara generate a main feedwater pump terminate a steam generator Generator Level trip signal on demand.

overfill transient if required.

5.

RC Pumps Trip Problems associated with pump A trip of the RC pumps transfers Manually control the affected seal og bearing cooling, control of the startup f eedwater startup valve. Trip the main electric power loss to RC valves to the selected operate feedwater pumps if required to pumps (and not affecting range level transmitters. If a control steam generator overfill.

feedwater pumpo), ESPS signal. selected transmitter was in an undetected f ailed low state, a steam generator overfill transfent could occur with a simultaneous failure of the automatic high steam generator level feedwater immp t r ip.

TADLR 5.6.

(Continued)

= _ _ _

Failure Porsible Causes Effectn Remedial Actions

- - - - - ~ ~ ~

6.

Main Feedwater Failure of the valve, its Failure could occur and remain If required, manually trip main Block Valves motor operator or electric undetected during normal feedwater, condensated booster or FDW-31, 40 Fall power supply.

ope rat ion.

Failure of the block hotwell pumps to terminate valve eliminates one possible overfill.

open means of limiting steam generator feedwater injection.

7.

Cracks in vibration corrosion, Increased concentrations of Monitor condenser pressure and Condenser oxygen in condensate.

If not condensate water quality to removed by the air ejectors or in identify the problem and repair.

Resulting in the condensate system, the out-If condensate impurities exceed Air In-Leakage of-specification oxygen concen-specifications, shut down the trations could have a deleterious reactor, effect on the steam generator tubes in the long term.

00 8.

Condensate Instrumentation, valve Increased condensate flow Monitor condensate water quality D'

Demineralizer operator or maintenance bypassing demineralizers possibly to identify the problem and Bypass Valves

failure, resulting in out-of-specification r epair. If condensate impurities condensate water quality. This exceed specifications, shut down Spuriously open could have a deleteriouc effect the reactor.

on the steam generator tubes in the long term.

9.

Condensate Maintenance / operations This operating mode could result Monitor condensate water quality Demineralizers

failure, in out-of-specification to identify the problem and condensate water quality. This repair. It condensate impurities Allowed to could have a deleterious ef fect exceed specifications, shut down Operate After on the steam generator tubes in the reactor.

Depletion the long term.

TABLR 5.6.

(Continued)

Failure posalble Causes Effects Remedial Actions 10.

Hydraz ne Feed Unspecified (PO-5G)

Increased concentrations of Monitor condensate water quality Isolated unavailable.

oxygen in condensate. The out-to identify the problem and of-specification oxygen repair. If condensate impurities concentrations could have a exceed specifications, shut down deleterious effect on ttie steam the reactor.

generator tubes in the long term.

om N

Single failures in the common loop A and B control circuitry are not expected to result in RCS overcooling due to downstream, loop specific signal modification (ICS BTU limits or RCS Tav controls).

However, if the manually selected loop A and loop B startup level transmitters were powered from the same power source (ICS Panelboard KI branch HEX or HEY), a failure of this single power source would result in the loop A and loop B control valves failing open (Item 2). The operator has the option of manually controlling the main and startup feedwater control valves in each loop or tripping the feedwater pumps if required.

Loss of the instrument air system or failure of selected ICS Panelboard KI branch circuits will result in the loop A and loop B main feedwater control valves failing in an "as is" position (Item 3).

Loss of instrument air or failure of Panelboard KI branch HX, H1X (ICS Hand Power), result in the feedwater control valves failing as is, the turbine bypass valves closing and the reactor subsequently tripping. The resulting steam generator overfeed transient is terminated by manual or automatic trip of the main feedwater pumps. Failure of Panelboard KI branch H, H1 (ICS Auto Power) results in many plant components, including the feedwater control valves, automatically transferring to manual control and remaining in position.

If the plant was in steady state operation prior to the auto power, an automatic reactor trip may not occur in the short term. However, other effects of the loss of Auto Power such as the generation of many spurious control room alarms, may induce the operator to manually trip the reactor. Once the reactor is tripped, the steam generators will be initially overfed. The operator has the option of manually controlling the feedwater control valves or tripping the feedwater pumps.

The feedwater pumps will be automatically tripped on high steam generator level if the level is not manually controlled. As noted in Table 5.6 and 5.5, if the loss of Auto Power occurred following a turbine / reactor trip transient, the turbine bypass valves would be open.- The loss of Auto Power, in this case, would transfer the turbine bypass valves to manual control while they were open. This could result in a combined steam generator depressurization, steam generator overfeed transient initially. The operator can manually control both the turbine bypass and feedwater control valves.

If required, to control steam generator level, thc operator may trip the main feedwater pumps and verify the automatic initiation and control of emergency feedwater.

88

i In addition to Condensate and Feedwater system failures which directly result in overfeeding the steam generators, a number of failures could increase the severity of a transient in combination with other failures.

These contributing failures are listed in Table 5.6, Items 4 through 10.

Of the failures listed, possibly the most significant is the failure of the automatic high steam generator level main feedwater pump trip.

This failure, Item 4, in combination with steam generator overfeed failures (Items 1, 2, and 3), could result in the introduction of significant quantities of water into the steam lines unless the overfeed was manually terminated by the operator.

The specific effects of overfilling the steam generators have been addressed in Reference 9 These effects include, in addition to the increased severity of RCS overcooling, possible damage of the main steam safety and turbine bypass valves and significantly increased stresses imposed on the main steam lines and their supports.

Although the effects of increased stresses, possibly intensified by the opening and closing of turbine bypass or safety valves, have not been evaluated in detail, the conditional probability of consequential steam line failure would be increased.

Trip of the four RC pumps has been listed as a contributing failure (Item 5).

Following a trip of the four pumps, the control of the startup feedwater valves transfers to the operate range level transmitters at a 20 foot steam generator level setpoint. This action alone may produce some degree of RCS overcooling. However, the increased level is required to promote material circulation in the RCS and the rate of increase in steam generatcr would be less rapid than following transients initiated by the main feedwater valves failing open or failing to close.

If the selected operate range level transmittar on either steam generator were in a failed low state, the feedwater ficwrate to the affected steam generator would continue beyond the 20 foot level setpoint and the automatic steam generator high level feedwater pump trip would be defeated.

Other contributing failures include failure of the main feedwater block valves and failures potentially resulting in exceeding f eedw ater chemistry 89

1 specifications.

As noted in Table 5.4, adverse feedwater chemistry could 4

contribute to long term degradation of the steam generator tube integrity.

53 MAKEUP AND PURIFICATION SYSTEM The makeup and purification (MU&P) system continuously processes reactor coolant and returns the purified coolant *o the RCS.

In addition to coolant purification, the MU&P system supplies the RC pumps' seal injection flow.

A detailed FMEA of the MU&P system has been performed and the effects of MU&P i

equipment failures identified (Reference 8). The MU&P failures potentially affecting RCS overcooling have been summarized in Table 5.7 The failures listed result in or contribute to the release of reactor coolant RCS overcooling mechanism. An isolatable small LOCA can result from a letdown cooler tube failure (Item 1).

Two failures (Items 2 and 3) have been identified which contribute to the potential for a small LOCA.

If a drain path from the standby letdown cooler were left open following maintenance, the failure may remain undetected since the cooler is isolated from the RCS, Should the standby cooler subsequently be placed in operation (isolation valves manually opened), a small LOCA would result.

Failure of the operating reactor building component cooling water flow results in isolation of cooling water to the letdown coolers and RC pumps.

This failure would result in automatic isolation of letdown flow.

If the letdown storage tank (LST) was allowed to drain resulting in damage to the operating HPI pumps or the HPI pumps were manually tripped to protect them, a simultaneous losa of RC pump seal injection and cooling water flow would occur.

As identified in Table 5 3, this condition could lead to RC pump seal failures.

i For the three MU&P failures listed, the LST will be drained unless an alternate supply of water is provided to the HPI pumps. Following a small LOCA, this action may occur automatically if the '1500 psi ESPS setpoint is reached prior to draining the LST.

If the LST is allowed to drain, the

' operating HPI pump would be dameged degrading the HPI safety function required for mitigation of small LOCA's.

90

TABLE 5.7.

SUMMARY

OF MAKEUP AND FUltIFICATION SYSTEM FMEA: FAII.URES f.PADING 'IV OE AFFECTING RCS OVERC00 LING TRANSIENTS Failure Possible Causes Effects Remedial Actions ReleAng 9LRCAGLOL.C991RDL 1.

Letdown Cooler Corrosion, stress on tubes.

Isolatable small I.OCA or PC leak. Manually open a flowpath f rom the Tube Failure Prior to ESPS actuation, BWST to the IIPI pumps prior to operating 11PI pumps will be depleting the LST.

Isolate the depleting letdown storage tank affected letdown cooler, and place (LST).

If the LST is allowed to alternate cooler in operation, drain, the operating IIPI pumps would be consequentially damaged.

ConL111stlag EA11uxen 2.

Open Letdown Undetected, improper Isolatable small I.OCA or PC leak.

Manually open a flowpath f rom the Cooler Drain maintenance resulting in open Prior to ESPS actuation, BWST to the IIPI pumps prior to Path drain path from an isolated operating IIPI pumps will be depleting the LST.

Isolate the to cooler and subsequently depleting letdren storage tank affected letdown cooler, and place placing the cooler into (LST).

If the LST is allowed to alternate cooler in operation, operation.

drain, the operating IIPI pumps would be conserguentially damaged.

3.

Reactor Building Spurious containment isolation Letdown path isolated resulting Manually open a flowpath f rom the Component Cooling valve closure or trip of a in the RC pump seal injection BWST to the IIPI pumps prior to Water Flow to component cooling water pump flow being pumped from the LST.

draining LST.

If component Letdown Cooler and failure to start spare If the LST is allowed to drain, cooling water flow cannot be and RC Pumps

pump, the resulting pump damage could restored, trip RC pumps to prevent Terminated result in a simultaneous loss of damage to pump bearings.

component cooling water flow and RC pump seal injection flow.

i l

6.0 REFERENCES

l t

1.

A Ranking g Nuclear Plant Systems f.2r Failure Modes Ans[ Effects Analysis, ORNL #62B-13819C/62X-30, SAI #1-245-08-492-02, December 31, 1982.

2.

Fint'. Safety Analysis Recort, Duke Power Company Oconee Nuclear Station.

3 Oconee 1 Electrical Distribution Control mi Protection Desistn Features, ORNL Letter Report, March 29, 1984.

4.

Failure Modes Ang[ Effects Analysis qf j;Ag ICS/NNI Electric Power Distribution Circuitry, SAI #1-147-08-701-00, March 1984.

5.

In addition to plant specific studies of safety systems performed and reported in FSAR's, numerous generic safety system studies have been sponsored by the U.S. NRC such as the Auxiliary Feedwater and Residual Heat Removal System evaluations.

6.

Failure Modes Ansi Effects Analysis g j;Ag Pressurizer Ansi Associated Eauicment, SAI Letter Report, May 31, 1983 7.

Instruction HQ2k ISE Integrated Control AD51 Non-Nuclear Instrumentation Systems, Oconee Nuclear Plant, Unit 1, Bailey Meter Company, March 15, 1977 8.

Failure Mode Ansi Effects Annivsis f.gr j;ht Oconee 1 Nuclear Power Station Makeno Ansi Purification System, ORNL #62B-13819C/62X-30, SAI #1-147 492-00, October 28, 1983 9.

Nuclear Power Plant Steam Generator Overfill Resultina from Control Action, F. H. Clark, N. E. Clapp, R. Broadwater, NUREG/CR-3692, ORNL/TM-9061, February 28, 1984.

92

APPENDIX g OT SEECTED FOR RCS OVERC00 LING Angygg l

t

APPENDII A OCONEE 1 SYSTEMS NOT SELECTED FOR RCS 07ERC00 LING ANALYSIS Potential Impact System ID System Name on RCS Overcooling NO3 Incore Monitoring System Provided for operator information only.

However, high core temperature may induce operator to trip the reactor and initiate High Pressure Safety Injection (S02), a safety system.

No other impact on RCS overcooling is apparent.

N05.C Coolant Treatment System Processes coolant stored in the Coolant Storage System producing demineralized water and boric acid solution which also is stored in the Coolant Storage System (N05.B). No impact on RCS overcooling apparent.

N05.D Post-Accident Sampling System only operates in the post-System accident, RCS shutdown mode. No impact on RCS overcooling apparent.

N05.F Low Pressure Injection This system is a safety system System used only to remove core decay heat in an RCS shutdown mode belcw 0

300 F and 300 psi.

NC6 Reactor Protective System System is a safety system used to initiate reactor trip and has no impact on post trip overcooling.

NO7 Nuclear Instrumentation System provides signals to System regulate plant power generation.

Although the system may induce spurious reactor trip, it has no impact on post-trip overcooling.

N09 Emergency Feedwater Control System potentially may have a System significant impact on RCS overcooling but it is a safety system and beyond the scope of this scudy.

A-1

APPENDII A (Continued)

Potential Impact System ID System Name on RCS Overcooling 301 Engineered Safeguards Engineered safeguards systems may Protective System have significant impacts on ECS overcooling but are safety systems and beyond the scope of this study.

S02 High Pressure Safety Injection System S03 Low Pressure Safety Injection Systen 304 Core Flood System SOS Reactor Building Spray System S06 Reactor Building Emergency Cooling Systen S07 Reactor Building Penetration Room Ventilation System S08 Reactor Building Isolation System SO9 Control Room Habitability System C01 Reactor Building / Containment The function of the containment is and Pe'.etrations to prevent release of radioactivity to the environment following accidents.

The effects of containment pressure boundary valves on RCS overcooling are considered in the analysis for the systems relected for analysis.

CO2 Reactor Building Hydrogen The function of the hydrogen purge Purge System system is to prevent hydrogen concentrations in the containment from reaching explosive levels.

The effects of hydrogen explosives are beyond the scope of the study.

Other impacts on RCS overcooling apparent.

A-2

APPEllDII A (Continued)

Potential Impact System ID System Name on RCS Overcooling P02.A Turbine Gland Seal Subsystem The gland seal system is designed to prevent air in-leakage to the turbines and condenser.

During power operation, failure of the system may result in turbine trip.

Following turbine trip, the system requires steam from the main steam system via the startup steam header (see Auxiliary Steam System, P06). No other potential impcets on RCS overcooling are apparent.

P03.A Main Condenser Evacuation The function of the evacuation System system is to remove non-condensible gases from the condenser.

Failure of the system may result in turbine trip; however, no impacts on RCS overcooling are apparent.

4 POS Emergency Feedwater System The emergency feedwater system may have significant impact on RCS overcooling.

However, this system is a safety system and beyond the scope of this program.

P06 Auxiliary Steam System During startup and shutdown operations, the Auxiliary Steam System provides steam to selected components from the startup steam i

header or the auxiliary boiler.

Failure to prcvide steam to required components is addressed in the analyses of the selected systems.

The interface with the main steam system (P01) is addressed in the analysis of the main steam system.

No other potential impacts on RCS overcooling are apparent.

l l

A-3 l

APPENDII A (Continued)

Potential Impact System ID System Name on RCS Overcooling U01 Radioactive Waste System The redirective waste system collects and processes redirective materials prior to reuse or disposal.

Interfaces with the RCS are isolated during operation.

No impacts on RCS overcooling are apparent.

WO2 Radiation Monitoring System The radiative monitoring system detects the release of radioactivity.

No impacts on RCS overcooling are apparent.

UO4.B High Pressure Service The HPSW is a safety system Water (HPSW) System designed to supress plant fires and serve as a backup to the LPSW.

No impacts on RCS overcooling are apparent.

WO4.C Low Pressure Service The LPSW is required to support Water (LPSW) System the operation of safety systems.

As a safety system, its analysis is beyond the scope of this program.

U05 Fuel Storagu and Handling The fuel storage and handling System system have no interface with the RCS or RCS suppcrt systems except during refueling shutdewn operations.

As such, no impact on RCS overcooling is possible.

WOS.A New Fuel Storage System WOS.B Spent Fuel Storage System WOS.C Spent Fuel Pool Ccoling System WOS.D Fuel Handling System A-4

APPENDII A (Continued)

Potential Impact System ID System Name on RCS Overcooling WO6 Auxiliary Service Water The auxiliary service water system System is manually placed in operation following a postulated concurrent failure of the main and emergency feedwater systems and the decay heat removal system. No impacts on RCS overcooling are apparent.

UO7.A Service Air System 808 Plant Gas System X01 Potable and Sanitary Water These plant auxiliary systems have System no interface with the RCS or RCS 3

support systems.

Potential effects of severe operating environment on the operation of plant equipments are beyond the scope of this study.

X02 Fire Protection System XO3 Communications System XO4 Security System XO5 Heating, Yentilating, and Air Conditioning Systems X05.A Turbine Building Ventilation System XOS.B Reactor Building Purge System X05.C Auxiliary Building Ventilation System X05.D Spent Fuel Ventilation System XO6 Non-Radioactive Waste System A-5

APPENDII B OCONEE 1 POWER CONVERSION SYSTEMS PROCESS AND INSTRUMENT DIAGRAMS (LATER)

.___m

_~__,_

APPENDII C OCONEE 1 POWER CONTERSION SYSTEMS FAILURE MODES AND EFFECTS ANALYSIS TABLES (LATER) i i

i e

9

ppg f$1G11EIgg'0$Uh y f 6 %,B4 p: '

f.

NUREC/CR-3692

(,f.. 2,'.-

ORNL/TM-9061 NRC Dist. R1 f

i Instrumentation and Controls Division POSSIBLE MODES OF STEAM GENERATOR OVERFILL RESULTING FROM CONTROL SYSTEM MALFUNCTIONS AT 'IHE OCONEE-1 NUCLEAR PLANT F. H. Clark N. E. C1 app R. Broadwater*

i Manuscript Completed:

February 28, 1984 Date Issued CTGnnessee Technological University, Cookeville.

l Prepared for the Division of Facility Operations Office of Nuclear Regulatory Research U.S. Nuclear Regulatory Commissio4:

Unde r Interagercy Agreer.ent 40-550-75 j

NRC Fin No. B0467 Prepared by the Oak Ridge National Laboratory l

Oak Ridge, Tennessee 37831 j

operated by l

UNION CARBIDE CORPORATION

(

for the U.S. DEPARTMENT OF ENERGY under Contract No. W-7405-eng-26 9

-o CONTENTS 1.

Introduction........

................. 1 1.1 General Considerations.....................................

1 1.1.1 Work Scope........................................

...... 1 1.1.2 Related Work Efforts....................

.1 1.1.3 Approach to Program.....

.................................)

1.1.4 Outline of This Report................................

.. 2 1.2 Steam Generator Overfill Summary...........................

3 1.2.1 Scope of Steam Generator 0verfill..............

......... 3 1.2.2 Principal Results of Steam Generator Overfill Study......

3 1.2.3 Methods Used.....................................

...... 4 1.2.4 Effects of Steam Generator Overfill......................

4 2.

Description Of Once Through Steam Generator....................

5 2.1 Functional Design of Steam Genera. tor.......................

5 2.2 Steam Generator Controls...................................

8 2.2.1 Operating Control........................................

8 2.2.2 Steam Generator Level Limits and Sensors................

14 2.2.3 High Level Main Feedwater Pump Trip Circuitry...........

17 3.

S y s t e m s S e l e c t e d................................................ 19 4.

Control System Failures That Contribute To Steam Generator 0verfill.........................................

21 4.1 Classification of Failures................................

21 4.2 Detailed Description of Failure Sequences.................

25 4.3 Simulation Recommendations................................

34 5.

Possible Consequences of Steam Gererator Overfill............... 33 5.1 Direct Primary Side Effects............................... 35 5.2 Possible Secondary Side Damage............................

3G 6.

Tentative Conclusions........................................... 38 References.......................................................... 39 i

Appendix A - Inf orma t ion Sources.................................... 4 0 i

l Appendix B - Steam Generator Tube Problems At Oconee 1..............

43 l

APPENDIX C - Review of Draft By Duke Power C0.................

..... 44 t

l I

l

ABSTRACT A study has been made of control system failures which might lead to everfill of the steam generator la Babcock and Wilcox nuclear plants.

The steam generator and its control system are described.

Only one sequence has been found in which a single failure would lead to overfill, and in that case the final stages of the overfill would proceed rather slowly.

Because of high level protective features all other failure sequences we have examined require at least two failures to produce overfjll beyond the point of high level protection. Several sequences are described in which high level protection features can be placed in an undetected failed state by a control system failure; a subsequent additional failure, occurring prior to the detection and correction of the first failure, could then produce system overfill. Mechanical damage is identified which might be consequent upon steam generator overfill and water entry into the main steam line.

Several ways of reducing the probability of steam generator overfill are suggested.

No assessment has been made of the probability of occurrence of any of the sequences.

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l

1.

INTRODUCTION 1.1 GENERAL CONSIDERATIONS 1.1.1 Work Scope This work is conducted for the U.S. Nuclear Regulatory Commission (NRC) under FIN No. B0467 Safety laplications of Control Systems.

It supports the resolution of Unresolved Safety Issue A-47.

The purpose of this contract is to determine whether nuclear power plant control systems, either in designed interaction or in credible malfunction, may interfere with the action of safety systems or may put the plant into a failed state beyond the protection of the safety systems.

The effort at Oak Ridge National Laboratory is limited to the study of Babcock and Wilcox Co. and Combustion Engineering Co. plants.

Plants designed by other vendors are under study at the Idaho National Engineering Laboratory (INEL).

The study is, therefore, intended to be generic by vendor.

Because it is recognized that detailed and realistic plant descriptive information is essential for a study of this sort, data from two existing nuclear poner plants Oconee-1 and Calvert Cliffs-1, were used to represent the designs of labcock and Wilcox and Combustion Engineering respectively.

While some elements of the study may be unavoidably plant specific, the thrust of the study as a whole is generic. Work to date covers only the Babcock and Wilcox design as represented by Oconee-1.

1.1.2 Related Work Efforts A number of other activities supported by NRC are related to or develop information related to this work.

We have maintained close liaison with them.

Included among them are:

a.

Plant Electrical System Evaluation. FIN B0816 b.

Evaluation of Pressurized Thermal Shock, FIN B0468 c.

Precursors to Potential Sevece Core Damage Accidents. FIN B1583 d.

In Plant Reljubility Date Base For Nuclear Plant Components, FIM B0445.

e.

System Interactions In Nuclear Power Plants, FIN B0789 1.1.3 Approach to Program The general apprcach to this problem at ORNL is twofold: (1) a study of teenarina which could lead to control system initiated plant failures, produced in the failure mode and effects (FMEA) format, and based on plant design and procedure information, and (2) the supportive development of a hybrid computer codel for simulation of the nuclear power plant. The plant simulation details tuch more explicitly than is customary the plant control system and its capabilities and effects.

The simulation will examine in detail important cases generated in the FMEA study.

The simulation will be described fully in another report.

The FMEA study, as it relates to the Babcock and Wilcox steam generator everfill problem, is the subject of this report, and the remainder of this report will deal with it.

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1.1.4 Outline of This Report Section 1, this section, the Introduction, deals with general program objectives and with some of the results of this study.

Section 2 is concerned with description of the Steam Generator and its controls.

Section 3 relates what systems received the most emphasis and why.

Section 4 presents the failure codes considered along with some possible failure scenarios.

The more casual reader might wish to skip some of the material in Section 2 through 4. but should in no event skip Section 2.2.2. 2.2.3, or 4.1.

Section 5 considers some possible consequences of a Steam Generator overfill: Section 6 makes some observntions about possible design or procedure changes if they are felt to be necessary.

The Appendices A B, and C deal, respectively, with Information Sources, past Steam Generator tube problems at Oconee 1. and a review by Duke Power Co.

of an early draft of this report.

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3 1.2 STEAM GENERATOR OVERFILL

SUMMARY

1.2.1 Scope of Steam Generator Overfill There are four conditions of Steam Generator alsoperation of interest to this project, n.

Overfeed of the Steam Generator to the point where 11guld water issues from its outlet. We shall consider this overfill, b.

Overfeed of steam generator beyond pump trip level.

We shall consider this overfill.

c.

Overfeed of the Steam Generator without exceeding pump trip level.

However, primary coolant temperatures are lowered and thermodynamic conditions at the turbine inlet may be off their operational norms. We will consider this overcool.

d.

Underfeed of the Steam Generator.

Primary coolant temperatures are increased, and thermodynamic conditions at the turbine inlet may be off their operational norms.

In severe cases the Steam Generator may dry out.

This report will concern itself principally with (a) and (b).

Succeeding reports will deal with (c) and (d).

1.2.2 Principal Results of Steam Generator Overfill Study The following are the major results of the Steam Generator overfill study.

a.

There are two high level protection features: a high level Main Feedwater pump trip and a high level Main Feeduater control valve closure. The system will not overfill undar Main Feedwater action unless these features are defeated. They do not act on the Auxiliary Feedwater.

(See Sect. 2.2.2 and 2.2.3).

b.

Both the above protection features receive level indication from the same instrumentation. They are, tFerefore, subject to common ceuse failure (See Section 2.2.2),

c.

The Main Feedwater pump trip circuitry is separate frosi the Integrated i

Control System (ICS).

Hence, a failure in this circuitry would affect the pump trip but not the high level control valve closure which is I

governed by the ICS. There are several ways that the pump trip l

circuitry can be placed in undetected failed state.

(See Sect. 2.2.3).

i d.

A low level indication overrides the high level control valve closure

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signal and creates a flow demand signal.

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4 e.

A sufficient leak in the selected low level pressure tap, or its connecting pipe, or the packing of either blocking valve to which it connects can lead to Steam Generator overfill by the Auxiliary Feedwater system (AFW).

Such an overfill would be the result of a single failure.

However, overfill by the AFW proceeds more slowly than overfill by the MFW, affording more time for corrective measures.

The water pumped by the AFW, having less velocity, is likely to cause less mechanical damage than water from the MFW might.

All MFW overfill scenarios we have found require more than one failure.

We have identified a number which are brought about by two failures, the first of which leaves part of the system in an undetected failed state.

(See Section 4.1).

1.2.3 Methods Used Initially over one hundred plant systems were screened to estimate their probable importance to Steam Generator overfill.

They were classfied according to:

a.

potential to be the proximate cause of SG overfeed b.

potential to disable high level protection systems c.

potential to affect the function of (a) or (b) type systems d.

whether they a.e administratively removed from consideration.

(by reason of being dealt with in other contracts).

This classification is dealt with in Section 3.

The systems identified as important were then subject to intensive study.

Among the most important systems were the Integrated control System, the Non Nuclear Instrument System, the Feedwater system, the Main Steam system, the Reactor Coolant system, and the Instrument Air system.

1.2.4 Fffects of Steam Generator Overfill The assessment of mechanical damage is not a part of the scop? of this project. We have, however. Indicated some areas on the secondary side that could be subject to unusual stresses and possible damage in the event of a Cerious overfill.

See Section 5.

Direct primary side effects stemming from Steam Generator oserfill would initially be an overcooling and would require simulation for adequate assessment.

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DESCRIPTION OF ONCE THROUGH STEAM GENERATOR This section describes the functional design and the controls of the Steam Generator.

2.1 FUNCTIONAL DESIGN OF STEAM GENERATOR The Once Through Steam Generator (OTSG) is a straight-tube, straight-shell heat exchanger.

The reactor coolant is on the tube side, and the secondary fluid is on the shell side.

The reactor coolant from the reactor outlet enters the 36-in. OTSG primary inlet nozzle at a temperature of about 603'F.

The reactor coolant gives up heat to the secondary fluid as it flows through the tubes and leaves through the two 28-in.-l.d. outlet nozzles at a temperature of 555'F.

The tubes are supported by tube support plates which have broached openings to permit flow between the plate and the tube.

The support plates are fixed longitudinally by a system of support rods that are welded to the lower tubesheet.

Spacer tubes are installed over the support rods between each pair of adjacent support plates. This system permits positive placement of the supports within the cylindrical baffle.

The cylindrical baffle comprises two pieces:

the lower section is bolted to the bottom tubesheet, and the upper section is welded to the shell just below the steam outlet nozzles.

Aligna.ent pins hold both sections radially in the shell.

Feedwater enters the OTSG through 32 spray nozzles connected to the 14-in.-o.d. main feedwater header.

The condensing action of the cold feedwater (455'F at full load) draws steam through the circumferential space between the upper and lower cylindrical baffles.

This steam heats the feedwater rapidly to the saturation temperature of about 535'F: this prevents thermal shocking of the shell. The flow of bleed steam is inherently self-regulating. Any change in feedwater flow changes the rate of condensation, thus changing the rate of bleed steam flow.

A mixture of saturated steam and water forms in the downcomer of the OTSG.

The level and density of the downcomer fluid are set by the static head and pressure drop between the bottom of the tube nest and the bleed point. There is cn adjustable orifice in the lower section of the downconer to ensure the I

dynamic stability of the recirculated loop. The fluid enters the tube nest through the ports in the lower portion of the cylindrical baffle (or wrapper).

Since the fluid is at saturation temperature it begins to boil as soon as it comes in contact with the hot tubes.

The boiling fluid flows upward in counterflow with the primary fluid.

The boiling taking place in the lower section is in the regime called nucleate boiling.

The tubes are wetted and small bubbles rapidly form and break tway from the surface.

Nucleate boiling provides a very high heat transfer l

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coefficient because of the turbulence resulting from bubble formation. Most of the heat is transferred in this region of the boiler.

Nucleate boiling continues until enough water has vaporized to allow a blanket of superheated steam to form on the tubes; this condition is called film bolling.

The steam blanket forms gradually as the steam quality reaches a high value.

It is fully l

developed in only a very short section of the boiler.

l The steam quality at the top of the film boiling region is 100%. This saturated steam is then heated to at least 35'F above saturation temperature in the superheat section of the boiler.

The full-load steam temperature at the

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cutlet nozzle will approach 590*F with a clean boiler; the steam temperature 2

will change as the boiler fouls. At the top of the tube nest the steam flows i

into the annulus between the upper wrapper and the shell.

The steam heats the j

upper part of the shell to the steam temperature; this minimizes the tube-to-shell temperature difference.

The steam exits through the two 24-in.-l.d. steam outlet nozzles.

The steam generator is fed water from the feedwater systems, main or auxiliary, and heat from the primary loop.

It is built to operate with 11guld 4

mater and steam each occupying approximately half of its secondary side volume.

1 If the pumps and valving systems which supply water to the steam generator supply it at a rate greater than the heat from the primary side is able to vaporize it, the steam generator will begin to overfill.

Hence. the proper cperation and control of the steam generator depends upon a balanced flow of cass through the secondary loop and energy from the primary to the secondary 4

loop.

Figure 1 is an outline sketch of the thermohydraulic aspects of the pressurized water reactor system of the Oconee plant. Much of it would apply to cny B&W PWR system.

Generally, the lower half of the diagram along with the i

secondary sides of the steam generators comprise the feedwater system.

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co=es fron the condensate, through the FX pumps into a common hea ler.

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then split into loop A and loop B flow.

In each loop there is a startup valve cnd a main FW valve in parallel. There is a flowmeter in the startup leg I

J censitive to low flows, and downstream beyond where the two legs have come together is a flommeter receiving the combined flow through both vnives. This l

meter may be relatively inaccurate at low flows.

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Control of the feedwater system is provided through the MFW and start up valves and the FW pump speed.

Sensed signals which are sent to the Integrated Control System (ICS) and there processed to produce control signals for the FW cystem include the following:

1.

Feedwater flow measures, both loops 2.

Level indicators (startup and operating) both SGs 3.

FW temperature, both SGs 4.

Temperature difference between cold legs in the primary system 5.

Turbine header pressure signal 6.

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SG outlet pressure 10.

Reactor coolant average temperature error 11.

Pressure drops across FW valves In maintaining total feedwater flow equal to total feedwater demand, the Feedwater Control subsystem manipulates two start-up valves, two main valves, end two pumps.

The Feedwater Control includes the following considerations, cach of which will be discussed below (see Figure 2 - all references to Points cnd Blocks are on Figure 2):

normal control mode feedwater temperature compensation high and low cross limits with the reactor power level TAVG control to feedwater correct feedwater flow ratio between the two steam generators for control of inlet reactor temperatures total flow control on large reactor coolant flow error minimum steam generator degrees superheat limits minimum and maximum steam generator level limits 8

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10 Legend for Fig. 2 FG = function generator VGM = variable gain multiplier BIA = bias PG = proportional gain F0F = first order filter DBM = deadband monitor HA = hand-auto station DER = derivative LM = low signal monitor INT = integrator AMINI = select minimum OIA = operator input analog AMAX1 = select maximum i

HIM = high signal monitor TRA = transfer A0 = analog out PI = proportional integral controller I

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Normal Control Mode In this mode, the feedwater demand from the Integrated Master (Point A) is used for feedback control of the valves and feedforward control of the pumps.

Under balanced system conditions, the total feedwater demand from the Integ:ated Master is split evenly between feedwater loops A and B (Point B and Block 1).

The measured feedwater flow to each steam generator is compared with the 2ndividual loop demand; the individual (Blocks 2 and 3) feedwater errors then pass through proportional plus integral controllers (Blocks 4 and 5) to establish the control valve positions.

The individual loop demands are summed together (Block 6) and used to generate a feedforward pump speed demand signal.

The operations of the start up valve and main valve in each loop are sequenced. Normally, as the loop demand varies from 0 to 15%, the start-up valve gain is adjusted to cause the start-up valve position demand to vary from 0 to 100% (Blocks 7, 8, 9, and 10).

Then, as the loop demand varies from 15 to 100%, the gain on the main valve and the bias (Blocks 11, 12, 13 and 14) are cdjusted to cause the main valve position demand to vary from 0 to 100%. When the start up valve becomes 80% open, a block valve in series with the main valve is opened, and when the start-up valve becomes 50% closed, the blocking valve is closed.

The minimum pressure drop across the control valves is selected (Block 15) and used to form a feedback signal to the feedwater pump speed demand. The cinimum pressure drop is compared with a setpoint, the resulting error passed through a proportional plus integral controller, and the feedback demand added to the feedforward pump speed demand (Blocks 16, 17, and 18).

The feedback gain l

for the value pressure drop error varies with the size of the error (Block 19).

The feedwater demands for each loop are passed through loop master Hand / Automatic stations (Blocks 20 and 21) so that the operator has the capability of establishing a manual feedwater demand for either or both loops.

Valve position and pump speed demands can be manually specified for all actuators from Hand / Automatic stations (Blocks 22 through 27).

Feedwater Temperature Compensation A function generator (Block 28) is used to compute the feedwater temperature based on feedwater demand and exit conditions required on the cecondary side of the steam generator. An error signal that is based on the difference between the desired feedwater temperature and the measured feedwater temperature (Block 29) is used to modify the total feedwater demand (Block 30).

The purpose of this modification of feedwater demand is to reduce the demand on the primary side of the OTSG while maintaining the desired exit conditions.

Thus, when the feedwater temperature varies from that used in plotting the function generator, a correction to the total feedwater flow demand is applied.

The correction to the total feedwater demand i: applied in such a direction as to maintain the outlet steam generator temperatures at the values used in plotting the function generator.

12 Croco Limits With Reactor Cross limits are used to maintain the feedwater flow in percent within a certsin ratio of the reactor power in percent (Blocks 31 through 36). Whenever tha measured neutron power is more than 5% different from the neutron power ds=:nd, a correction is made to increase or decrease the feedwater flow demand cccordingly.

For instance, if the neutron power error is -7%, then the cross limits will cause the feedwater flow demand to be decreased by 2% (Blocks 33 and 34). If the neutron power error is 6%, then the cross limits will cause the fecdwater flow demand to be increased by 1% (Blocks 35 through 36).

TAVG Control to Feedwater Under certain conditions, the Reactor Control subsystem cannot control TAVG (i.e., reactor coolant average temperature). One such condition occurs when the reactor Hand / Automatic station is in manual. When the Reactor Control subsystem cannot control TAVG, conditions are satisfied, TAVG control is transferred to the Feedwater Control subsystem. When this occurs TAVG error is operated on by a proportional plus integral controller (Point C), and the resulting feedback dsmand is summed with the feedforward total feedwater demand (Block 37).

Plant conditions which would prevent Feedwater Control from accepting the centrol of Tryg are:

- both steam generators meeting level limits

- either steam generator on a Btu limit

- botn feedwatet hand /Autouttic waster stations in staani.

Delto-T Control e

To insure a uniform reactor inlet temperature distribution,-the Feedwater Centrol ratios the two feedwater loop flows in such a manner as to maintain the terparature of the reactor coolant in cold leg A equal to the temperature of the rocctor coolant in cold leg B.

This may be expressed as TCA = TCB, or delta-Tc

=TCA - TCB = 0.

Ratioing the feedwater flow between the two steam generators fer the control of reactor inlet temperature is referred to as delta-T control.

e Bath reactor coolant cold leg temperature measurements and reactor coolant flow toccurements are used in implementing feedback control of delta-T. A variable e

gain is modified by the delta-T feedback control signals and applied to loop A e

feedwater demand (Block 48). The loop A demand is then subtracted from the totc1 demand (Block 1) to create the loop B demand modified by delta-Te facdback.

The delta-T setpoint is normally entered as zero (Block 49). A e

prep:rtional gain, a calibrating integral, and high/ low limiters operate on the cold leg temperature difference delta-T error (Blocks 38 through 43).

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j Both the proportional and calibrating integral actions are blocked if either l

feedwater loop Rand / Automatic station is in manual or if either steam generator is en level limit. The calibrating integral action only, and not the proportional action, will be blocked if the megawatt electric demand is changing footer than a specified rate or if a reactor coolant flow transient exists. A dalta-T Hand / Automatic station (Block 44) may be used to replace the demand e

created by delta-T feedback error with manual ratioing of the feedwater flow e

dsmands.

i There are four reactor coolant pumps, with two > umps operating in parallel in sach loop. If an imbalance in the primary flows through the steam generators exists, as when the number of reactor coolant pumpt running in each of the two will deviate from zero unless the primary loops are not equal, then delta-Te equal to feedwater flows are ratioed properly. To aid in mainttining delta-Te zero in this situation, derivative and proportiorial control actions are used to oparate on the difference between the reacter coalant flowa (Blocks 45 and 46, 50 and 51). The feedbacks due to delta-T error and primary loop flow imbalance e

are summed (Block 47) to create the variable gain applied to loop A feedwater demand (Block 48).

l Total Flow Control If the reactor coolant flow error becomes greater than 10% (Point D), then the total feedwater flow error passed through a proportional plus integral controller is used to modify each of the individual loop demands (Blocks 52 j

through 55). The effect of this controller is modified by conditions in the following manner. If both reactor coolant pumps on one loop are tripped then i

the controller output is bled to 0% with a 60 s time constant.

If steam

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gaatracot A is on icw level control and ses.m ge7<<rrtor P is on rarS31 ccAtrel 4

l than the output of the total flow controller due to integral action is held canotant. The same output will occur if the roles of A and B are reversed and whsn both steam generators A and B are on low level control.

Btu Limits To insure steam with a minimum specified number of degrees superheat (unually 19.4*C-35'F) BTU limit calculations are implemented. The BTU limits i

cro the maximum allowable feedwater flow demands for each loop. A low l

cuctioneer is used in implementing the BTU limits in each loop (Blocks 56 thrcugh 57). Feedwater flow demands higher than the BTU limit would result in the degrees superheat at the outlet of the steam generator falling below the tinimum specified degrees superheat.

t The BTU limit calculations are based upon measurements of the reactor coolant flow, primary coolant temperature at the reactor outlet, the feedwater tczperature, and the steam generator outlet pressure (Blocks 58 through 70).

4 Thsce variables are used to determine the amount of energy available from the l

stoca generator at the desired steam temperature.

If the normal feedwater i

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steam generators than is available for the desired steam temperature. then the BTU limits override the normal feedwater demands.

2.2.2 Steam Generator Level Limits and Sensors Low and high level limits are imposed on the operation of the steam generators.

In the high level limit control, a low auctioneer is used to compare the feedwater flow error against an appropriately gained operate level error signal, and the minimum error signal is passed on to the valve control (Blocks 71 through 78).

In the low level limit control, a high auctioneer is used to compare the feedwater flow error against an appropriately gained start-up level error signal, and the maximum error signal is passed on to the valve control (Blocks 79 through 89).

Note that this is not level control, that no attempt is made to maintain a set level; the limits simply give assurance that the level remains between pre-selected high and low points.

Note further that a low level error signal, if present, will dominate.

Figure 3 shows a schematic of the Oconee 1 Steam Generator, water level sensing pressure taps (labeled A,A',B,B',D.D', and e), the MFW and AFW delta-P cells associated with the A,B,D taps, and the valves and pipes that connect the teps to the cells.

There is an identical set of valves, cells and pipes associated with taps A',B',

D'.

Referenced from the bottom tube sheet as 0, the tap heights are A,A' - 6 in., B.B' - 102 in., D.D' - 394 in., E - 60G in.

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The operator selects which group of taps, A-B-D or A'-B'-D', will have its sensed $2gnala ment tu the 1C5 and the coau ul t uou display. Thl. 1. Lallc0 the

" selected" set.

The path from each pressure tap to the (normally open) blocking valves (Figure 3) is open as shown, clear of obstructions or other valves. When the cater level is above a tap it flows into the connecting pipe. When the water level is below tap D (D'), as it is normally, the pipe from that tap is filled to tap level by evaporation from the SG and condensation in the pipe. D(D') is the refe ence tap, and the water in it is maintained in this manner at height D-D'.

The following failure possibilities are noted below for this arrangement of sensing equipment.

Each of these failures, in addition to sending oisinformation to the control system, would send misinformation to the control room display. This misinformation would be inconsistent with other information sva11able in the control room display.

The failure would be undetected until the operator observed the inconsistency and deduced its cause.

(a) sufficient leak in the selected A,A' tap or the connecting pipe or the packing of the packing of the blocking valves between the tap and the corresponding AFW or MFW delta-P cell can cause an apparent drop in the sensed

15 Icw level of the SG and bring on an overriding requirement to increase feedwater ficw. This misinformation would go to both AFW and MFW controls.

(b) A sufficient leak in the selected B-B' level tap or connecting pipe or packing if the terminating blocking valves will similarly cause the operating leval (or high level) sensing equipment to sense a lower level than is actually present.

This failure can defeat both high level protection systems - the high level MFW pump trip and the high level control valve closure.

(c) Failure of the selected B-D (B'-D') MFW delta-P cell so that it reads low when the level is high will also defeat both high level protection systems.

(d)

The blocking valve in the selected set, marked V in Figure 3, if failed into a closed position during operation, will isolate the B-D MFW delta-P call from sensing any further pressure changes at the B level tap.

The other cids of the cell " sees" the water column from the D level. This should remain escantially invariant until the water level exceeds the D level. At that point the cell should "see" a relative increase in the D over the B level, or, equivalently, a decrease in the B under the D level.

This should be interpreted es a falling water level. Hence, this failure also defeats the two high level protection systems.1 1

1 e

l 6

-,---r--

ORNL-DWG 83 19467 TE

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STEEL DIAPHRAGM COUPLING AP CELL TO CONNECTING

$ WATER LINE g*j

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D H

M W

_ [

_ g

_ g __ @m

_ g i

8' 8

M MFW AFW M

--H--

X-b A

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MFW AFW SCHEMATIC OF STEAM GENERATOR PRESSURE TAPS AND AP CELLS Fig. 3 4

0

17 2.2.3 High Level Main Feedwater Pump Trip Circuitry Figure 4 is a schematic of the circuit transmitting SG high level sensed signals to the high level MFW pump trip and alarm. The following failures can place this system in an undetected failed state.

(a) For purposes of high level MFW pump trip and high level alarm the signals from both pairs B-D and B'-D' are used. The signals B-D and B'-D' from SG-A (Fig.3) go respectively to contacts 2A and 3A (Fig. 4); similarly, B-D and B'-D' from SG-B go to 2B and 3B.

Note that if either 2A or 3A is in a failed cpen condition SG-A cannot cause a high level MFW pump trip.

Trips from SG-B are similarly blocked if either 2B or 3B is failed open.

(b)

If the relay FPTX is failed open, all high level MFW pump trips from whatever source are blocked.

The circuitry of Figure 4 is not part of the Integrated Control System.

Hence, failures within this circuitry will not fall protective features, like the high level main feedwater control valve closure, which are operated from the ICS.

1 e

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3.

SYSTEMS SELECTED

,4 l

Search for possible safety problems in the operation or malfunction of l

j control systems requires deep and detailed examination of possibly offending j

systems or components. This is because nuclear power plants are designed with great care for safety; they are further subject to severe original and continuing scrutiny by the regulatory authorities for safe design and operation.

It is therefore most unlikely that serious problems will be found with less than cn in-depth search.

The number of systems and components in the plant is so

)

great that it would not be possible within allocated resources to make an in-depth study of all of them.

Hence, a preliminary screening of systems was 1

necessary to determine where the deeper effort should be applied.

?

i Approximately 100 systems in the Oconee 2 nuclear plant were considered to determine whether they might have a significant effect on Steam Generator overfill. The systems were put into five classes as follows:

l Class A - This class consists of those systems which, for administrative reasons, are etteluded from consideration.

It includes most safety systems and all plant electrical systems.

The reason for the exclusion is that j

responsibility for consideration of these systems has been placed elsewhere.

In i

the case of a few safety systems, for example, the Auxiliary Feedwater System, i

te have been unable to avoid some consideration. A total of 24 electrical and i

7 safety systems were placed in Class A.

i l

Class B - This class consists of systems which contain components whose j

function or malfunction can directly increase the pressure difference between the main feedwater pump discharge and the Steam Generator or decrease the flow of heat from the primary coolant to the secondary side of the Steam Generator.

Also in this class we include the control signals which motivate such components cnd the control circuitry associated with them.

Class B Systems j

l Main Steam System Turbine Generator System l

Main Feedwater System Turbine Bypass System Auxiliary Feedwater System Reactor Coolant System Integrated Control System I

Class C - This class consists of systems which generate signals that are cent to the control systems (which, in turn, generate the signals which motivate the Class B components).

i Class C Systems 1

i Nuclear Instrumentation Turbine Generator System i

Non Nuclear Instrumentation Feedwater System 1

System Steam Generator l

Main Steam System Reactor Protection System i

I l

19 m

20 Class D - This class consists of systems having components whose operation cr malfunction can directly affect the performance of Class B or Class C components.

Class D Systems Cooling Water System Essential Service Water Reactor Bldg Service System Water System Compressed Air System Instrument Air System Heating. Ventilation and Reactor Core Air Conditioning Class E - This class contains all other systems.

Class E Systems Control Rod Drive System Chemical and Volume Control Radioactive Waste System System Gaseous Radwaste System Liquid Radwaste System Solid Radwaste System Radiation Monitoring System Plant Area Radiation Environmental Radiation Monitors Monitors Process Radiation Monitors Refueling System Spent Fuel Storage System Fuel Pool Cooling and Cleanup Service Air System System Process Sampling System Plant Gas System Nitrogen System Hydrogen System Potable and Sanitary Water Fire Protection System System Water System (Fire)

Carbon Dioxide System Communication System Control Room Habitability Diesel Bldg Ventilation System

. System Fuel Bldg Ventilation System Non Radioactive Waste System Gaseous Waste Liquid Waste Solid Waste Turbine Gland Seal System Turbine Lubrication System Stator Cooling Syste.a Hydrogen Seal 011 System Condenser Evacuation System Condensate Cleanup / Polishing Condensate Hecter Drain System System Feedwater Heater Drain System Auxillary Steam System Nine Containment Systems

4.

CONTROL SYSTEM FAILURES THAT CONTRIBUTE TO STEAM GENERATOR OVERFILL

~

The Oconee 1 MFW control system has an overriding requirement to feed the Steam Generator as long as the water level is sensed below low level. (36 in. on the selected A-D (A'-D') sensor - see Figure 3).

Between 36 in. and 282 in.

control is not based on level during normal operations.

A complex of demand related signals is met by the control system.

Most simple aberrations that cight occur in a component are compensated by action of the Integrated Control System in this region. When the sensed level exceeds 282 in, the ICS sends a signal to close the MFW control valve.

If despite this the level rises to 394 in. a signal is sent by circuitry outside the ICS (see Figure 4) to trip the MFW pumps.

Note that this last signal will cause actuation of the trip only if signals are sent from both the B-D and the B'-D' sensor sets.

(See Sections 2.2.2 and 2.2.3.)

It is apparent, therefore, that the MFW cannot overfill a Steam Generator (above the 394" level) unless both high level protection features are defeated and an overfeed mechanism is initiated which is not controlled by cross limits or any of the other compensatory features of the ICS. We have accordingly classified possible failures as they may cause one or another of these.

The Auxiliary Feedwater system (AFW) is not subject to the high level protection features.

Therefore, once the system is on AFW, less control system failure is required to bring on SG overfill.

Two things should be borne in oind.

There must have been a prior failure or unusual circumstance to bring on the AFW. And the AFW pumps water much more slowly than the MFW with full open or nearly full open control valve. Hence, in the AFW case, there is more time for intervention and less potentially damaging momentum carried by the water.

4.1 CLASSIFICATION OF FAILURES Type A - Failures Which Place Both The High Level MFW Pump Trip and The High Level Control Valve Closure In Failed State - Since both these systems depend on the same level detection equipment, a failure there would affect both equivalently.

a.

a sufficient leak in selected pressure tap B (B') or connecting pipe from it or packing of either blocking valve on which the connecting pipe terminates - 2.2.2, b b.

failure of valve V (Figure 3) of the selected set in the closed position during operation - 2.2.2, c c.

any failure of the selected B-D (B'-D') MFW delta-P cell, mechanical, hydraulic, or electrical, which causes the cell to read a low level when the level is high - 2.2.h. d Further description of these failures appears in Section 2.2.2.

As observed there, since these are failures of level indications of the selected set, the indications are brought to the control 22

o 22 room display where they are inconsistent with other level indications displayed there.

The failure should be detected when the operator notices and understands the inconsistency.

Type B - Failures Which Place The High Level MFW Pump Trip In Undetected Failed l

State - As noted before the MFW pump trip circuitry is independent of the ICS which controls toe high level control valve closure. Further, the pump trip requires a confirming signal from the non-selected B-D (B'-D') set.

a.

Any failure causing relay 2A or 3A (Figure 4) to fall with contacts open places SG-A pump trip in undetected failed state. Analogously, 2B and 3B for SG-B.

2.2.3, a b.

Any failure causing relay FPTX (Figure 4) to fail with contacts open will put trip signals of both SGs in undetected failed state.

2.2.3, b c.

A sufficient leak in non selected pressure tap B (B') or connecting pipe from it or packing of either blocking valve on which the connecting pipe terminates - 2.2.2, b d.

Failure of valve V (Figure 3) of the non selected set in the closed position during operation - 2.2.2, c e.

Any failure of the non selected B-D (B'-D') MFW delta-P cell, mechanical, hydraulic, or electrical, which causes the cell to read a low level when the level is high - 2.2.2, d Failures a and b are undetected by their nature.

Failures c d. and e are undetected because they are failures of the non selected set which is not displayed in the control room.

Type C - Failures Which Block the High Level MFW Control Valve Closure and Also Initiate Steam Generator Overfead a.

Selected low level signal falls low. - Sect. 4. 2, r; 2. 2.2, a b.

Hard limiter on Turbine Header Pressure error signal falls.

Or the summer immediately downstream of the limiter produces a false signal. Either may have the effect of calling for increased flow, c.

Failure high of the low level setpoint. - Sect. 4.2 w Type D - Failures Which May Initiate Fast Overfeed By MFW - Whether or not these failures would be controlled by the ICS and cross limits prior to challenging high levels is not clear.

Simulation is required to determine this. - Sect. 4.2, q,t n

e -

6 23

. 0,,

a.

Delta-P measurement on FW control valve falls at O.

Sect. 4.2, a.

b.

FW temperature measurement in one loop falls high.

Sect. 4.2, c.

9 c.

MFW flow signal falls showing no flow.

Sect. 4.2, d.

i d.

Hot leg temperature measurement fails high. - Sect. 4.2, g.

4 e.

Delta-Tc signal falls either way. - Sect. 4.2, 1.

f.

TAVG determination fails high. - Sect. 4.2, J.

g.

Neutron flux measurement falls high. - Sect. 4.2, k.

h.

MFW blocking valve position indicator fails in closed position.

- Sect. 4.2, a 1.

Reactor Coolant flow measurement falls low. - Sect. 4.2,u.

J.

Main Steam Line Safety, Atmospheric, or Turbine Bypass Valve falls open. - Sect. 4.2. v.

k.

MFW control valve falls open or valve control signal falls demanding valve opening. - Sect. 4.2, o Type E - Failures That Would Cause MFW Overfeed At Relatively Low Rate - These would afford more time for intervention.

If water were ejected from the SG lt would be with relatively less energy and momentum than in the foregoing cases, a.

Delta-P signal across MFW control falls between 0 and set point. -

Sect. 4.2, b.

b.

MFW flow measurement falls at low value greater than zero. - Sect.

4.2, e.

c.

Reactor inlet temperature measurement in one loop falls low. -

Sect. 4.2, h.

d.

Start up FW control valve position indicator falls with valve less than 50% open. - Sect. 4.2, 1.

e.

MFW pump speed governor falls. - Sect. 4.2, n.

f.

MFW Start Up valve falls open. - Sect. 4.2, p.

g.

MWe demand falls high. - Sect. 4.2, s.

24 i

I a

Type F - Single Failure Causing Relatively Slow Overfill of Steam Generator i

A sufficient leak in selected pressure tap A (A') - see Figure 3 - or the connecting pipe from that tap or the packing of the blocking valves on which the connecting pipe terminates.

Sect. 4.2 r; 2.2.2, a.

The foregoing classification is useful in the further analysis of the consequences of the failures or the failures in combination.

Type C failures, taken alone, should cause a rapid filling of the Steam Generator to the 394 in. level followed by MFW pump, reactor, and turbine trip, cnd initiation of AFW.

j Type D and E failures, taken alone, may be controlled by the ICS.

In some cases they will lead to system trips.

Type D failures are expected to lead to greater and more rapid SG overfeeds than Type E failures.

Type A and B failures do not cause SG overfeed, but block some or all of the high level protection.

Type A failures, which bring inconsistent information to the control room display, are. expected to be detected sooner than Type B failures, which do not.

l There is one Type F failure.

This is a single failure which causes the rapid filling of the Sc to the 394 in. point and the relatively slow continued j

cverfilling of it thea after.

i Any Type A failure or any Type

' allure followed by any Type C failure (coming before the detection and cor etion of the Type A/B failure) will cause rapid overfill of the SG with the MF6. pumps operating at high speed.

1 No operator intervention (ameliorative or otherwise) has been assumed in the above discussion. We have made no estimate of the probabilities of these

failures, a

l I

r k

e

.-r

25 1

4.2 DETAILED DESCRIPTIONS OF FAILURE SEQUENCES The component parts of the FW system. Its controls and control signals.

constitute a functional group that could have failures which could initiate a SG cverfeed. We have examined this group to find failures that can lead to overfill of the SG at Oconee.

All but one of the overfeed sequences we have found would be terminated by successful action of the high level trip of the FW pumps. The exception is sequence r (below) in which overfeed comes also from the aux *11ary FW pump, which does not have a high level trip.

The following event sets have been identified as having the potential to cause steam generator overfeed.

In each case the initiating event appears to lead to increase of the steam generator water level. The sequence of events i

suggested in each scenario beyond the initiating events is not intended to be 1

taken as predictive.

Event sequences can depend upon many things, and surprising results often ensue. These scenarios are constructed and presented as guides for the modelers and simulators to highlight features that may have special significance. Where indicated they will be analyzed on a system simulator in the next phase of this study which will be the augmented Failure f

Hodes and Effects Analysis.

1 A most helpful source, which suggested a number of these sequences, was reference (2).

a.

The delta-P signal across the FW control valves in loop A fails at its lowest value.

The FW pumps go to high speed stop in an attempt to control the failed delta-P signal back to setpoint.

Excessive feedwater flow results from the increased pump speed.

Throttle pressure will increase. T yc will start to A

j fall, and the FW flow error will cause the FW valves to begin to close.

Hegawatts generated will begin to increase as the throttle valves move to control pressure back to setpoint.

The control rods will pull, increasing reactor power, to control T yo back up to setpoint.

A However, as long as the tracking mode is not activated, the FW control, valves should control the FW flow back to the original setpoint.

Hence, the plant should settle out at its original condition, except that the high pump speed would result in a higher pressure drop across the FW control valves.

Also, with the higher control valve pressure drop, the flow control would be more sensitive and would not be as smooth as normal. The FW valve flow control should be rapid enough to prevent a high level in the steam generators from occurring.

However, failure of the FW control valves to act rapidly enough still leaves the high level pump trip protection.

b.

The delta-P signal across the FW control valve falls at some point below the setpoint. Qualitatively, the effects are the same as in (a).

However (a) appears to be the bounding case; so the effects should be less severe. A failure of the delta-P signal above the setpoint value should not lead to SG overfeed.

26

~

c.

The FW temperature measurement in loop A fails high at 500*F.

FW l

terpsrature compensation will cause the total FW flow demand to increase, resulting in overfeeding both steam generators and overcooling the core. TAVG will start to drop, causing control rods to pull and reactor power to increase.

Th2 cteam pressure will increase, causing the turbine valves to open and the t2gnvatt electric generation to increase.

Because of negative megawatt electric errcr, the megawatt electric calibrating integral will cause the feedforward control demands to the reactor and feedwater to decrease.

If the megawatt oloctric calibrating integral does not reach a low limit, then the unit will settle out at its original condition. If the megawatt electric calibrating integral goes onto its low limit (generally set at -5%), then the plant will esttle out at a higher power level than its original condition. If the FW tcmparature measurement failure occurs at a low load level, a higher probability of reactor trip due to low AC pressure exists than at a high load level. This to because at the low load level the FW temperature is lower than at the high load level.

Hence, a greater percentage increase in FW flow will occur at the low load level. Further at low load levels BTU limits are less restrictive.

d.

The main FW flow signal in loop A fails showing zero flow. The loop A FW control valve will open fully trying to control the FW flow to setpoint.

j Tha delta-P across the loop AFW control valve wi.11 decrease below setpoint, and th2 FW pumps will speed up to control the delta-P back to setpoint.

Steam ganarator A is overfed because control valve A goes fully open and the pumps cpssa up.

Steam generator B is initially underfed when control valve A goes fully open, is probably overfed for a short period of time when the pumps speed up, cnd eventually FW control valve B should control loop B FW flow to setpoint.

1 l

TAVG will fall and the control rods will pull to increase reactor power.

l Th2 FW flow imbalance between loops A and B will cause a negative delta-Te error. The delta-T control will start to decrease the FW demand in loop A and e

increase the FW demand in loop B.

This transient may result in a reactor trip ccussd by low RC pressure or the trip of the FW pumps caused by a high level in etcco generator A.

e.

Main FW flow signal fails at a level between 0 and demand. Transient precceds as in (d) but less severe.

f.

This transient is initiated by the startup level signal in loop A fciling low.

As a result of this, loop A FW valve opens fully and the FW pumps opssd up in an attempt to restore the level in SC-A.

In order to control loop B fico, loop B FW valve closes. Neither cross limits nor BTU limits are expected l

during this initial portion of the transient.

Because of excessive FW flow, the prie:ry system may be rapidly overcooled.

A reactor trip may occur, probably j

dua to low RC pressure. Also, a high SG 1evel FW pump trip may occur to prevent i

SC cverfill (expected to occur in SG-A).

A turbine trip would immediately follow the reactor trip.

Because of excessive FW flow, steam pressure should be running high, and operation of steam relief as well as turbine bypass is cxp:cted to occur at moderate to high power levels.

If the reactor trip occurs b2 fore the high steam generator level is reached there is the potential for

~

27 centinued overcooling of the primary due to the open relief valves and the failed level acasurement causing the continuing supply of feedwater to SG-A.

Popping of the relief valves would cause rapid loss of steam pressure and high flows to be drawn from the steam generators.

A possible loss of pressurizer invantory along with initiation of HPI may occur.

Following the turbine trip, tha steam source for the FW pump turbines switches from the low pressure to the high pressure steam supply. Without the high trip SGA should overfill.

g.

This transient is initiated when one of the reactor hot leg temperature ceasurements fails high. Let TAVG = reactor average temperature measurement THi = hot leg temperature measurement, i = A,B TCi = cold leg temperature measurement, i = A,B.

Thare are 3 methods of determining TAVG: namely, i

T 4T 4 T 4 T HA HB CA CB 1.

T

=

AVG 4

T 4T HA CA 2.

T

=

AVG 2

T 4T HB CB 3.

T

=

AVG 2

9 l

For a failure of THA high, method 3 above will give the least error in the calculation of TAVG,, and method 2 will give the greatest error.

Two cases will be considered. The first case will consider complete cutematic operation of the ICS.

In the second case, the reactor H/A (i.e.,

H:nd/ Auto) station is in manual with all other H/A stations in automatic.

In to be computed erroneously high.

both cases, a failure of THA will cause TAVG Hanca, the TAVG error in the ICS, given by Error (T yc) = Setpoint - TAVG A

will be negative.

With the ICS in complete automatic, the TAVG signal modifies the l

rarctor demand. A negative TAVG will cause the control rods to insert., If TAVG 1

i l

i 28

-1 is Isrge enough it can cause the feedwater flow demand to be modified through th2 cross limits from neutron error to feedwater control. A sufficiently n2g3tive TAVG will cause the feedwater demand to be increased.

Hence, with the p:ver generation of the reactor decreasing and the feedwater flow increasing, this transient is in the direction of a steam generator overfill.

With the reactor H/A station in manual and all other H/A stations in autcmatic, the Tgyg error signal modifies the total feedwater demand through a proportional / integral controller. A step increase in the Tgyg signal, such as wculd be caused by THA failing high, has the potential for driving this control i

loop unstable. The negative TAVG signal would initially cause the feedwater 4

d: mand to increase rapidly while the reactor demand remains constant. Again, thin transient is in the direction of a steam generator overfill.

i h.

This transient is initiated by the reactor inlet temperature in loop A failing low.

Proportional control action in the delta-T control will e

immsdiately cause the flow demand in loop A to decrease and the flow demand in loop B to increase. This proportional control action is limited to 5%.

Integral action in the delta-T control will eventually cause the variable gain e

l tultiplier in the flow ratioing circuit to be decreased by an additional 20%.

j Hznce, because of the delta-T control, the flow' demand for loop A flow equals e

(100% - 5% - 20%) times the total flow demand. The flow demand for loop B flow th2n equals 200% (100%-5%-20%)

times the total flow demand.

Therefore, the flew demand in loop A is reduced by 25% and the flow demand in loop B is j

increased by 25% on account of delta-T control. The low failure of the reactor e

i inlet temperature in loop A will also cause an error in the calculation of TAVG' l

Thsro are three methods of determining TAVG. They are J

T 4T 4T 4T HA HB CA CB

1. T

=

AVG 4

T 4T HA CA

2. T

=

i AVG 2

T T

HB 4 CB

3. T

=

AVG 2

Fct c failure of TCA 1 w, method (3) will result in no error and method (2) will racult in the greatest error in the calculation of TAVG.

It will be assumed that either method (1) or (2) is being used to calculate TAVG. For TCA f*III"8 low, TAVG will be calculated low. This will cause the reactor power to be increased. Also, the low Tgyg will, through the reactor cross limits to the FW system, cause the total FW demand to be lowered.

Hence, the reactor power i

29 increases; the TAVG control causes the FW flow to SG-B to decrease, and the d21to-T control causes the FW flow to SG-B to increase. Whether or not SG-B e

cill have excessive PW flow is not clear.

i fails high.

1.

The reactor inlet temperature loop A-B difference delta-Te A high failure of delta-T conveys the false information that on the primary e

sida, the temperature of cold leg A is higher than cold leg B.

The delta-T i

e orrer is apportioned in equal magnitude but opposite sign to the loop A and loop B ficw demands. However, the change in demand in each loop is limited to 25% of t h,2 total flow demand.

If the initial unit load is high enough, the Btu limits will be activated cnd limit the increased FW flow in loop A.

This will cause a net reduction of The control rods will insert, th? total FW flow, and an increase in TAVG.

reducing reactor power, to try to control TAVG back to setpoint. A reactor trip en high RC pressure is possible.

If the plant is not at high load so that the Btu limits are not activated, then the unit will probably settle out at a new oteady state with a cold leg temperature imbalance. Hence, for a high failure of dalta-T, steam generator A will be overfed and steam generator B will be e

undarfed.

j. The reactor average temperature, TAVG, fails high. The high failure is cocused to be due to on of the following three failures:
1. Failure of the hot leg temperature measurement in primary side loop A (i.e., THA)*
2. Failure of the cold leg temperature measurement in primary side loop A (i.e., TCA)*
3. A high failure of TAVG for some reason other than (1) or (2).

E:ch of the three failures will be considered separately. Also, it is assumed that TAVG is calculated by (see scenario g):

T 4T RA CA T

=

AVG 2

fer this results in the largest error in T yg for the assumed failures.

If A

TAVG fails high because THA fails high then scenario g applies.

In this case, th2 high TRA (assuming THA is the outlet temperature selected by the operator) will increase the allowable maximus FW flow demands calculated by the Btu licits.

If TAVG is determined to be too high for some other reason there should b2 no ef fect on the Btu limits.

a

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failing high, then scenario g must be If TAVG fails high as a result of TCA modified to account for the effects of the delta-T control loop. With delta-T e

e csntrol coming into play, the steam generator overfeed will not be symmetric as l

censidered in scenario g.

Instead, because delta-T control reratios the FW e

ficw2, overfeed of steam generator A will be greater than of steam generator B.

R:nca, with a high failure of TCA, the overfeed of steam generator A should be vsrsa than that considered in scenario g.

j If a high failure of TAVG occurs for some reason other than r AVG high l

fcilure of THA or TCA, then scenario g will again apply except for the above cantioned effect on the Btu limits.

4 4

With all three failure modes resulting in high failure of TAVG, the steam l

32narators are overfed.

In every case there is the possibility that the reactor coy trip on low RC pressure or the FW pumps may be tripped on high steam 32n2rator level.

j k.

The neutron flux density reading fails high. The control rods will i

b2 gin to insert continuously in trying to reduce the failed neutron flux density reading. The lower the unit load, the larger the neutron error will be.

Thrcugh the cross limits, the large neutron error calls for an increase in the FW flow.

Both steam generators are overfed and the primary is overcooled. The Btu limits will probably be activated and will limit the maximum feedwater flow dreands. The cross l'aits will cause the unit to go into the track mode, and I

b2ccuse of the increasea FW flow and steam pressure, the unit megawatt electric dsmand will track up.

A reactor trip on low pressure is highly probable.

j Fo11cwing the reactor trip, the turbine will trip and the megawatt electric g2n2 ration will go to zero. The unit is still in the track mode at this time, l

cud the feedwater demand from the integrated master goes to zero.

However, j

folicwing the reactor trip, the cross limits from reactor control to feedwater centrol increase, calling for feedwater flow close to 100%. Hence, the Stu licits, and not the feedforward signal from the integrated master, must be rolisd upon to run the FW system back.

2 js When the loop A startup FW control valve becomes less than 50% open.

1.

th2 loop A startup FW control valve position signal fails to indicate that the valva is less than 50% open. Hence, the main feedwater blocking valve in loop A dess not receive a signal to close. The leakage through loop A main FW control valva, if excessive, may cause steam generator A to be overfed.

Also, since the i

main feedwater blocking valve in loop A does not close, the flow measurement u:cd in feedwater control is not switched from the main FW flow measurement, which is highly inaccurate at such low flows, to the start-up FW flow cocsurement. Thus, control will not be as smooth as normal. If the leakage l

thrcugh the main FW control valve is large enough, the start-up FW valve may j

close completely while steam generator A continues to be overfed from the lockage. This condition would probably result fr a steam generator high level trip of the FW pumps.

i c-

,w-,.,

e n--.,

---,-,-.,----,-....-g


4.-.

-. ~ ~ - _.

l f

32 I

L

m. MFW blocking valve in loop A is open, but its position indicator falls in closed position.

This causes ICS to take flow measures from startup line.

i l

If reactor is at high power a flow demand signal is sent causing increase in i

flow in both loops.

Cross limits cause rod insertion signals.

BTU limit may be j

cctuated. SGs are overfed. Reactor may trip on low pressure, i

n.

The speed governor on FW pump A falls high.

This will cause FW pump A l

to go to its high speed stop and the feedwater flow to the steam generators to increase.

Flow control will cause the feedwater control valves to close to i

control the feedwater flows back to setpoint.

As the control valves close.

delta-P control will cause the speed of feedwater pump B to decrease.

1 Concerning the operation of pump B during this transient, three conditions may l

cccur. The plant may settle out with pump B at a reduced speed, with both pumps i

supplying flow to the steam generators, or the plant may settle out with the l

check valve in series with pump B closed, and pump B supplying no flow to the j

steam generators.

Finally, pump B may end up operating in an oscillatory mode.

I uith the check valve cycling open und closed.

In any event, pump A will be at

}

its high speed stop. Also, a delta-P higher than setpoint may exist across the j

control valves following the transient.

Some overfeed of the steam generators j

uill occur, but a reactor trip is not anticipated.

t j

o.

The MFW control valve in loop A falls open.

(This transient will be j

core serious if it is initiated well below full power - say at 25%).

The flow j

in A increases with the valve full open.

The low delta-P signal across control j

valve A leads to pump speed up.

The delta-Tc error will attempt to reduce flow in A and increase flow in B.

The total flow demand error will attempt to reduce

}

flow in both A and B.

Because of the valve failure loop A is not affected by i

these signals.

On account of the srbstantial increase in total flow (resulting from the loop A failure) the total flow demand error should dominate the delta-Tc error signal in loop B either immediately or very quickly, and i

continue to do so.

SG-A therehre fills while SG-B empties.

If SG-B level drops to low level indication before high level pump trip occurs in SG-A. the i

low level signals in SG-B will override and prevent the level from falling j

further.

Hence, the low level signal in B along with the total flow demand i

crror signal should between them keep the level in SG-B at about the low level I

indicator until the pumps are tripped.

I The NFW pumps should trip on a high level signal in SG-A.

I p.

The loop A feedwater startup valve falls open.

There would be no offect during operation at power and probably the failure would not be detected. However, during plant shutdown, the excessive flow in loop A would i

j prevent the steam generators from going on low level control. Appropriate

]

canual control actions could be used to shut the plant down safely, i

I Following a reactor trip, this failure would result in overfeed of stema generator A if proper manual control actions are not taken.

When the reactor trips, the turbine also trips the steam system goes on bypass controls the feedwater flow demand runs back to low value and the steam generators are

p.

e 32 cre supposed to go on low level control. With the start up valve in loop A failed wide open. steam generator A will be overted. Without manual control intervention, feedwater pump trip on high level in steen generator A is likely.

Simulation of failure with reactor trip is needed.

g.

The control system summer which suas the start up level and turbine header pressure signal falls, giving low indication. This failure is equivalent to the corresponding failure in any of the component signals and causes increased flow to the SG.

The high level FW pump trips occurs at high level Indication.

r.

A sufficient leak in selected SG pressure tap A (A') or in the pipe connecting it to b'ocking valves, or in the packing of either blocking valve on thich the pipe terminates will cause a low level signal and an overriding demand for feedwater.

The SG will fill to the high level pump trip level. 394 in.

and cause trip of the MFW pumps. The AFW will come on, and, with the low level signal still present and no high level constraints the AFW will continue the overfeed causing SG overfill.

Consult Section 2.2.2.

s.

Failure of the NWe demand signal high will lead to demand for more FW flow and more reactor power. The FW demand / response is much faster than the core power demand / response. However, cross limits would be activated and limit the rate of increase of feedwater flow. Hence the feedwater system response could be approximately coordinated with that of the reactor.

That is. If the systeu energy balance is taken into account the feedwater system should run just slightly ahead of the reactor. The cross limits should hold the feedwater j

system back.

Some steam generator overfeed should result, but it should not be i

severe.

t.

Under rarmal conditions the Turbine Needer Pressure error signal compensates the startup level measurement.

It is first put through a hard limiter to limit its effect on the level indication to not more than 8 inches.

However, a failure of the hard limiter signal could negate the limiting effect.

This error is then potentially equivalent to sequence f.

u.

Both high and low failures of.th'e RC flow measurement in loop A will be considered.

Consider first a high failure. The reactor coolant flow Imbalance feedwater ratioins circuit will immediately reratio the feedwater flows. The feedwater flow in loop A will be increased and the feedwater flow in loop B will be decreased.

This will lead to overfeed of atwas generator A and underfeed of steam generator D.

After a short time lag the delta-Tc control will decrease the feedwater flow in loop A,6nd increase the feedwater flow in loop 8. thus providing some compensation for the original failure. Whether or not a reactor trip will occur during the course of events is uncertain, a

Next consider the RC flow measurement in loop A falsely indicating zero flow. The low failure has a much larger effect than the high failure because there is more room on the low side than on the high side of the RC flow

,f 4

,q f

6

i I

33 4

)

-i measurement range.

A front end runback to a lower load level will immediately be implemented in the unit load demand load limit circuitry.

Again, the reactor coolant flow labalance feedwater ratioing circuit will immediately reratio the feedwater loop flows.

However. In this case the reratioing will be in the cpposite direction and much larger.

The feedwater flow in loop A should be decreased to the point that steam generator A goes on low level control.

In

]

loop B. the Btu lJaits should be activated and thus restrain the increase in

{

feedwater flow.

Hence, in this case, overfeed of steam generator B and underfeed of steam generator A occur.

When loop B goes on Stu limits, cross limits to the reactor will reduce reactor power, and the unit will also go into the track mode.

During the initial phase of this transient, there is a net reduction in feedwater flow when i

steam generator B goes on Btu limits, and a reactor trip on high RC pressure is j

probable.

Simulation, especially initialized at high load, is needed.

]

v.

Failure in the open position of the Atmospheric Dump. Turbine Bypass, cr any safety valve in the Main Steam Line will cause an increase in the l

pressure drop across the Steam Generator and an initial increase in feed of the SG.

This event is bounded by the small break in the Main Steam Line.

w. The low level setpoint falls giving a reading at its highest level.

This failure is functionally equivalent to r.

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f 34 7-4.3 SIMULATION REC 0KMENDATIONS The criteria which we follow in recommending that sequences be simulated are as follows:

a.

The scenario is sufficiently complex that we cannot be sure our speculations as to its course are correct both in magnitude and in sequence of events. These uncertainties are especially pronounced in those events where compensatory ICS action is initiated.

b.

Primary side effects cannot be quantitatively evaluated without simulation.

If primary side effects seem significant simulation is indicated.

c.

If there are strong arguments that the event is insignificant it need not be simulated.

d.

If there are strong arguments that the event is bounded by another and if simulation shows the bounding event is not significant the bounded event need not be simulated. This would be a special case of c.

However, if the bounding event proves significant, the bounded event should then be simulated, e.

An event sufficiently similar to a simulated event need not be simulated.

With these criteria, our recommendations for simulation at present are as follows.

(1) Any one Type C (Sect. 4.1) event.

(2) Any one Type A or B (Sect. 4.1) event followed by any one Type C event while the A/B is still undetected.

(3) The single Type F (Sect. 4.1) event.

(4) We cannot eliminate from consideration at this time any of the following: Sect. 4.2 c d.g,1,J,k,m u.

All these are Type D (Sect.

4.1).

We expect that exploratory calculations will permit us to eliminate a number of thta on the basis of similarity or bounding.

(5) We recommend no Type E (Sect. 4.1) simulations at this time in anticipation that a numbe; of them will be shown to be bounded and insignificant.

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5.

POSSIBLE CONSEQUENCES OF STEAM GENERATOR OVERFILL Steam generator overfill can produce both primary side and secondary side effects which may have safety consequences for the plant.

Secondary side effects may indirectly produce significant primary side effects.

5.1 DIRECT PRIMARY SIDE EFFECTS Overfilling of the steam generator will produce overcooling of the primary coolant.

This, in turn, can in some instances produce one or more of the following results:

a. density increase and liquid phase shrinkage with attendant increase reactor coolant pressure
b. pressurizer dryout
c. steam in primary flow passages with possible blockage of flow
d. possible loss of natural circulation
e. possible reactivity insertion from high density moderation 35

m l

l i

36 52 POSSIBLE SECONDARY SIDE DAMAGE f

Overfill of the Steam Generator to the point where liquid water enters the i

Main Steam Line may cause damage on the secondary side.

In Section 4.1 we have c1ccaified, in various ways, control system failures that car. lead to Steam G2narator overfill. One way was according to the rate at which the overfill cccurred.

Overfills brought on by Type E and F failures (Section 4.1) are expseted to occur rather slowly: E because the MFW pumps and control valve are not wide open, and F because the final overfill mechanism is the AFW. Type C overfills would involve control valves fully open or nearly so and MFW pumps operating at high speed. These would be rapid overfills. Type D events are not yet cufficiently analyzed and may prove to produce overfills of either kind.

The rapid overfill appears more threatening for two reasons. First, it parmits minimal time for effective recognition and counter measures.

Second, it injsets water into the Main Steam Line at maximum speed and therefore with the maxitum kinetic energy / momentum that the MFW pumps are able to provide, only cinically dissipated in the open control valve.

All references we have found relating to the ability of a B. and W.

Main Steau Line to withstand stresses from liquid water deal only with the static load of the water, that is, motionless water, zero energy / momentum.3,4,5 There appear to have been no testa made of the ability of these lines to bear the dynamic stresses associated with the influx of water of high energy / momentum content such as might come from a Type C failure.

(In fact, there appear to be no tests to show whether the dynamic stresses from a Type E or F failure could be borne.) Under the circumstances, it would not be prudent to assume that the probability of Main Steam Line rupture in that dynamically stressful environment is n2gligible.

The possible results of such a rupture should be considered.

Main Steam Line Rupture ir one of the accidents analyzed in the Oconee-1 FSAR. We are particularly interested here in the effect such a rupture can have en the Steam Generator tubes. The tubes are subject to considerable wear and '

damage during normal operation. There are approximately 16,000 of them in an Oconte 1 Steam Generator. Oconee has experienced a number of observed tube 1stko, and a number of tubes have been plugged as a precautionary measure during maintenance on account of observed wear. Appendix B summarizes references to a number of Steam Generator tube problems which have occurred at Oconee.

During normal operation the tubes and the massive supporting tube sheets era at elevated temperatures, and, consequently, in thermally expanded state.

If now the tubes are suddenly cooled more rapidly than the supporting tube sheets, the tubes, in attempting to contract, are placed under tensile stress.

A Main Steam Line Break causes the water in the Steam Generator to flash, cuddsnly cooling the tubes. The water is in more contact with the tubes than with the tube sheets. Further, the tube sheets, being massive, would have lenger thermal time characteristics and would cool more slowly. All the tubes in the Steam Generator are simultaneously subject to the added thermal stress.

It is apparent that for large stresses in these circumstances multiple tube ruptures could occur.

~

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37 7

The Oconee 1 FSAR examines this effect (on SG tubes) in its Main Steam Line Brock analysis (Section 15.13.5, oconee 1, FSAR). In that section the edditional stress (maximum) on SG tubes due to the flashing of the water in the SG whsn the Steam Line Break occurs is given as 39 ksi.

That is compared with 42 ksi, said to be the " maximum allowable stress", but otherwise undefined.

Thio cnalysis initiated the Steam Line Break with the Steam Generator less than two-thirds full of water. Apparently no account was taken of the severe vibrational stresses that would be experienced during the blowdown of the sacondary side through the ruptured steam line.

In the scenario proposed here a Steam Generator fills with high an2rgy/ momentum content water; the water enters the Steam Line producing dynamic strasses that lead to rupture of the line. Hence, the Steam Line Break occurs with a full Steam Generator, 50% more water content than in the case computed in tha Oconee 1 FSAR. With that much additional water flashing in the Steam G2narctor there should be substantially more Steca Generator tube cooling and oubstantially more resultant thermal stress.

These additional thermal stresses and the vibrational stresses of blowdown, wh2n considered in analysis, may show that there is sufficient additional ctress present to cause multiple tube rupture in the steam generator.

Multiple tube rupture taken together with main stream line rupture provides o leckage path through and out of the secondary system for radioactive materials centsined in the primary fluid.6,7,8,9,10

6.

TENTATIVE CONCLUSIONS

~~

This study has not proceeded to a point where serious system inadequacies have been demonstrated.

In the course of this study, however, we have, we believe, uncovered some potential concerns, in particular, control system failure that might lead to the failure sequence discussed in Section 5.

We have cade no assessment of the probability of occurrence of any of these things.

Therefore, it would be premature to suggest that any corrective measures are required.

We have noted some places where improvements might be made if it is found they are desirable. We present them here for consideration.

a.

The high level MFW pump trip originating in each steam generator is of primary importance in preventing steam generator overfill.

We have already noted that contacts 2A and 3A in Figure 4 are in series as are contacts 2B and 3B.

Revising these circuits to parallel configuration would afford important redundancy to this circuit.

b.

Also in Figure 4, functional replication in parallel of the FPTX solenold/ contact would provide additional important redundancy.

Both a and b would, of course, increase the likelihood of spurious pump trips.

We~have observed that pressure taps,and some connecting equipment are c.

shared in common by the MFW and the AFW.

It may be useful to examine the desirability of modifyng the gang selection switching so that when the operator selects A-B-D (Figure 3) for MFW, A'-B'-D' is selected for AFW.

d.

The plant computer could be programmed to track both sets of signals in c for consistency and to provide appropriate alarms when an inconsistency is noted.

e.

The full range Steam Generator level sensor, which makes use of information from tap E Figure 3, is the only sensor providing level information ance the SG water level exceeds the high level pump trip height (level D.D' in Figure 3).

This information does not go to the control system, but it is svallable to the operator.

It is apparently not explicitly referenced in.the procedures governing steam generator overfills. An explicit reference might be useful.

t I

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l 38 1

REFERENCES 1.

Delta-P Transmitter For Nuclear Service, Product Instruction E21-20, Bailey Meter Co.

2.

BAW 1743. R. W. Enzinna, R. W. Winks, S. D. Swartzell, R. P. Broadwater, M. S. Kai, and W. E. Wilson, Failure Modes and Effects Analysis of the Midland NNI and ICS, July 1982, Babcock & Wilcox Co.

3.

NRC Memo, Power Reactor Events - Steam Generator Overfill, Richard H.

Vollmer to Thomas Novak, May 13, 1981.

4.

Letter, K. S. Canady, Duke Power Co., to A. L. Lotts, ORNL, August 31, 1983.

5.

B. & W. Owners Group, Probabilistic Evaluation of Pressurized Thermal Shock, Phase 1 Report, BAW 1791, June 1983, ppg 6-48, Babcock & Wilcox Co.

6.

NUREG-0909, NRC Report on the January 25, 1982 Steam Generator Tube Rupture at R. E. Ginna Nuclear Power Plant, April 1982.

7.

NUREG-0651, L. B. Marsh, Evaluation of Steam Generator Tube Rupture Events, March 1980.

8.

Preliminary Notification of Event-PNO-V-82-45A, November 15, 1982, San Onofre Unit 2 Excessive Cooldown Transient and Automatic Initiation of Safety Injection.

9.

C. Michelson, Case Study of the Abnormal Transient Operating Guidelines (ATOG) as Applied to the April 1981, Overfill Event at Arkansas Nuclear One, Unit 1, USNRC, August 30, 1982.

10.

EPRI 3065, C. S. Davis, J. M. Thomas, S. W. Winder, D. E. Allison, Engineering and Probabilistic Analysis of Tube Cracking Performance in Once Through Steam Generators, Vol 1 July 1983.

39

Appendix A - Information Sources This program has the major aim of identifying control system malfunctions which might significantly impact safety systems and lead to a serious transient, or which might cause a transient for which there has been inadequate provision in the safety systems.

With such a mission it is clear that our major sources of information would, of necessity, be design and procedural data.

In fact, this has proved to be the case. Documentation that has been of

" mainstream" use to us has included the following.

Duke Power Company Oconee Nuclear Station Final Safety Analysis Report Oconee Nuclear Station P& ids (very limited number available)

Bailey Instruction Book Duke Power Company Oconee Nuclear Plant, Unit No. 1 Manual IC/NNI System. Vol. 4 Oconee Nuclear Plant No. 1 Integrated Control system Reliability Analysis, prepared for NRC by B&W Abnormal Transient Operating Guidelines, BWNP-20807 Babcock and Wilcox Control of a Nuclear Power Plant with Once Through Steam Generator ASME, 80-WA/DSC-24 L. L. Joyner, R. P. Broadwater Oconee Units 1, 2, and 3 Training Manual In addition, there have been numerous conversations with former employees cf B&W and of Duke Power. There has also been much examination of " loose" copies of circuits, sometimes poorly identified as to source.

We have made a number of aearches of the LER literature covering the period 1973-83.

LERs have not provided one of the more useful primary sources for this report. There are several reasons for this.

40

41

.. ~

1.

As noted above, design and procedure are the major areas investigated for failure in this work.

LERs deal very little with these two topics.

2.

Steam generator overfill as such has not been a required LER reportable event. Hence, not only when they occur alone may such events go unreported, but also when they occur in conjunction with other reportable events the steam generator overfill aspect may be neglected.

In those cases where we have found it reported its extent and consequences are not detailed.

3.

LERs are written with a brevity that tends to render their descriptions of events too incomplete for a study of this kind.

On account of the above considerations, 2 in particular, retrieval of useful steam generator overfill information from the LER data base has not been especially productive.

Searches on various steam generator related conditions for the period 1973-83 produced 70 LER references of which 21 were found to be related to performance of once through steam generators.

The LERs did not produce any failure modes in addition to those deduced from study of design and procedure documents.They confirmed experience with certain kinds of failure.

Their usefulness to this project probably will lie in their provision of counts of certain kinds of failures for aid in quantification.

Since SG overfill has not of itself constituted a requirement for submission of an LER in the past, we have no assured method of identifying all or most such events which have occurred.

A number of LER searches along with resort to secondary sources have disclosed 21 cases of SG overfill of some kind in once through steam generators.

We have identified only three events where water definitely entered the main steam line:

San Onofre 11/9/82 Ginna 1/25/82, and Arkansas Nuclear One 4/8/81.

Of these, only the last involved a once through SG.

In none of these cases was there any reported damage to steam line or to supports as a result of the influx of water.

(However, operation of a safety valve was compromised in the Ginna case).

On the other hand, conversations with workers in the field suggest to us that there may have been a number of additional SG overfill events not documented in the available literature.

Various secondary sources, some of them heavily based on LERs, have been useful.

These are reports of NRC and NRC contractors which clarify, and to some extent, quantify various kinds of failures or which make in-depth studies of particular failures which have occurred.

Prominent among these are:

NUREG/CR-2497, Precursors to Potential Severe Core Accidents Summary of Event Tree Development, Branch Probability Estimation and Sequence Qualification for the Oconee Pressurized Thermal Shock Evaluation, SAI NUREG-0909, NRC report on January 25, 1982 Steam Generator Tube l

Rupture at R. E. Ginna Nuclear Plant

O 42

~*

NUREG-0651 Evaluation of Steam Generator Tube Rupture Events Case Study of the Abnormal Transient Operating Guidelines as Ap-plied to the April 1981 Overfill Event at Arkansas Nuclear One. USNRC, August 30, 1982.

Current Events Power Reactors, USNRC, 1 March-30 April 1978.

Loss of Non-Nuclear Instruments (Rancho Seco).

Also of considerable use have been:

BAW 1743 Failure Modes and Effect Analysis of Midland NNI and ICS Control of a Nuclear Power Plant with once through Steam Generator.

ASME 1980.

l 6

I I

l Appendix D -SG Tube Leak Problems at Oconee 1 DATE/LER SG No. of Tubes Remark 3/6/82 LER 2B 1

0.08 gpm leak 2/9/82 LER 1A 1

0.11 gpm leak 5/29/80 Deficiency in FSAR NSIC 00Z0158256 analysis of tube rupture 7/23/79 LER IB 1

0.3 gpm leak 10/12/78 LER Tubes misplugged 4/20/78 LER 4

Leak observed 1977 NSIC 00ZO128689 Status report on tube 5/7/77 LER IB 2

Leak observed 3/27/77 LER 1-6 Leak observed 2/28/77 1-6 Leaks observed 12/22/76 LER IB 1-3 Leak observed 1976 NSIC 00ZO120234 1A 2

Leak observed 43

.