ML20235Q078

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Application for Amend to License NPF-3,increasing Reactor Protection Sys Response Time Requirement for High Flux/ Number of Reactor Coolant Pumps on Trip Function
ML20235Q078
Person / Time
Site: Davis Besse Cleveland Electric icon.png
Issue date: 02/21/1989
From: Shelton D
TOLEDO EDISON CO.
To:
Shared Package
ML20235Q063 List:
References
NUDOCS 8903020486
Download: ML20235Q078 (11)


Text

. . . l Docket Number 50-346 License Number NPF-3 Serial Number 1634 Enclosure l Page 1 APPLICATION FOR AMENDMENT TO FACILITY OPERATING LICENSE NUMBER NPF-3 DAVIS-BESSE NUCLEAR POWER STATION UNIT NO. 1 Attached are requested changes to the Davis-Besse Nuclear Power Station, Unit No. 1 Facility Operating License No. NPF-3. Also included are the Technical Description and Significant Hazards Consideration.

The proposed changes (submitted under cover letter Serial Number 1634) concern:

Section 3/4.3.1.1, Reactor Protection System Instrumentation, Table 3.3-2,  !

Reactor Protection System Instrumentation Response Times.

By: \

D. C. $helton', Vice President', Nuclear Sworn and subscribed before me this 21st day of February, 1989.

f, LL(_ 4fL b Notar9 Public, State of Ohio l

LAURIE A. HINKLE l tk'xy Public. Shte of Ohio l Uy Commissicn Exp!m May 15.1991 l qqo302nns6 pjfjjy$h46 pas nocci poc  !

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' docket Number 50-346 l License Number NPF-3 Serfal Number 1634 Enclosure Page 2 The following information is provided to support issuance of the requested f changes to the Davis-Besse Nuclear Power Station, Unit No. 1 Operating License Number NPF-3, Appendix A, Technical Specification, Section 3/4.3.1.1, Table i 3.3-2.

A. Time Required to Implement: This change is to be implemented within 45 i

days after the NRC issuance of the License Amendment or prior to startup from the sixth refueling outage, whichever is later. l B. Reason for Change (License Amendment Request Number 89-0001):

I The present response time of 451 milliseconds is close to the physical limit of the system. The revised re ponse time is allowed by new analyses l l

and vill provide additional margin for surveillance testing. The l

increased response time may prevent unnecessary plant outage time. ,

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l C. Technical

Description:

See attached Technical Description (Attachment 1). l l

D. Significant Hazards Consideration: See attached Significant Hazards I Consideration (Attachment 2).

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' Docket Number 50-346

. License Number NPF-3 Serial Number 1634 At'tachment 1 Page 1 TECHNICAL DESCRIPTION Description of Proposed Technical Specification Change I

The purpose of this technical description is to describe a proposed change to the Davis-Besse Nuclear Power Station Technical Specifications Table 3.3-2, Reactor Protection System Instrumentation Response Times. The chenge proposes an increase in the response time requirement for the High Flux / Number of Reactor Coolant Pumps on (pover/ pumps) trip function of the Reactor Protection System (RPS) provided in Table 3.3-2 (Item number 8) from 451 milliseconds to 631 milliseconds. This proposed change is based on an analysis performed with the NRC, topically approved, computer code: VIPRE (Reference 1).

Systems Affected The proposed change affects the Reactor Protection System (RPS). However, increasing the response time in the Technical Specification does not affect j

the present logic configuration and hardware design of the RPS. ,

l Safety Function of Systems Affected The safety function of the RPS is to trip the reactor when an unsafe  ;

condition; e.g. high flux, high pressure or Departure from Nucleate Boiling ,

(DNB), is approached. The Technical Specification definition of the reactor  !

protection system response time is "that time interval from when the monitored I parameter exceeds its trip setpoint at the channel sensor until povar )

interruption at the control rod drive breakers". The Updated Safety Analysis Report (USAR) Chapter 15 safety analyses also includes the control rod drive release delay and a dedicated margin for uncertainty. The safety function of the Pover/ Pumps trip is to provide DNB protection for (1) multiple Reactor '

Coolant Pump (RCP) coastdowns, (2) single RCP coastdowns from partial pump operation or (3) RCP coastdowns resulting in the loss of both pumps in either loop. I Each RCP has four current monitors that provide running /not running status of  !

the associated RCP to each of the four pump monitor relay cabinets. The four pump monitor relay cabinets in turn provide the interface with four RPS channels. The RPS channels utilize the pump monitor relay cabinet inputs to determine the total number of RCPs running and in which RCS loops they are running. Once it determines the total number of RCPs running and 11 which RCS loops they are running, it utilizes this information as a setpoint for the power to pumps reactor trip bistable. The bistable receives an analog signal from the power range channel proportional to the reactor power leve). .The bistable trips when the reactor power signal exceeds the setpoint signal input from the contact monitor. For a coastdown of a single RCP from a four RCP initial condition, the flux / delta flux / flow trip ensures that there is sufficient flow, i.e., heat removal capability for the reactor power level while the rc. actor is automatically running back in power. Therefore, the pover/ pumps trip is only needed to provide protection for those instances mentioned previously.

' Docket Number 50-346 License Number NPF-3 Serfal Number 1634 Attachment 1 Page 2 Effects on Safety The Loss of Forced Reactor Coolant Flow transient is described in Section 15.2.5 of the USAR. This analysis was performed using the closed-channel computer code RADAR, as summarized in the NRC approved B&V topical report -

BAV-10069A, Rev. 01, (Reference 2) to determine DNC as a function of time.

The most limiting transient for the Loss of Forced Reactor Coolant Flow that relies on this protective feature of the RPS is the four pump coastdown transient. This analysis summarized in Section 15.2.5 of the USAR uses a total response time of 620 milliseconds. The 620 milliseconds is comprised of 371 milliseconds for the sensor and EPS delay (including 240 milliseconds for the pump monitor), 80 milliseconds for the control rod drive (CRD) breaker delay, 125 milliseconds for the CRD release delay and 44 milliseconds for a dedicated margin for uncertainty. The resultant calculated minimum DNB Ratio (DNBR) using the Westinghouse correlation V3R is 1.49. The four pump coastdown has been reanalyzed twice since the conduct of the analysis provided l

in the Davis-Besse FSAR. The first time was to account for densification effects. This reanalysis, summarized in References 3 and 4, resulted in a minimum DNBR, using the Babcock & Vilcox correlation B&V-2 and a response time of 620 milliseconds, of 1.816. The seccnd reanalysis, summarized in Reference 5, was during Cycle 1 when the Burnable Poison Rod Assemblies (BPRAs) and Orifice Rod Assemblies were removed from the core. This reanalysis resulted in a minimum DNBR of 1.85 also using the B&V-2 correlation and a response time of 620 milliseconds. The acceptance criteria for the four pump coastdown transient is a minimum DNBR greater than or equal to 1.30.

Subsequent to the completion of the above analyses, crossflow codes, i.e.,

open channel codes have been developed and approved by the NRC. Crossflov l

codes can predict the flow redistribution effects in an open lattice reactor l core. The crossflow methodology provides significant DNBR improvements (by I allowing the coolant to mix) over the traditional closed-channel methodology.

A reanalysis of the four pump coastdown was performed by Toledo Edison using VIPRE-01 (Reference 1). This code utilizes crossflov. First the VIPRE code was benchmarked against the LYNXT (Reference 6) crossflow code. The benchmark chosen to perform was a comparison to the locked rotor transient. A reanalysis of this particular transient had been performed by B&V for Davis-Besse Cycle 6 using LYNXT as summarized in the Cycle 6 Reload Report (Reference 7). A brief summary of the benchmark is given in Appendix A of this Technical Description. The comparfson of VIPRE and LYNXT DNBR are l plotted as a function of time in Figure 1 of Appendix A. As can be seen from Figure 1, the VIPRE DNBR results are conservative with respect to LYNXT at the point of interest, i.e., the minimum DNLR (MDNBR).

Once the model was benchmarked, the four pump coastdown was run using a total response time of 800 milliseconds. The minimum DNBR calculated using the B&V-2 correlation was 1.885 as shown in Figure 2 of Appendix A. This value obtained using open channel methodology and longer response time shows greater j margin to DNB than the three previous analyses given above using closed l

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. Docket Number 50-346 License. Number NPF-3 Se. rial Number 1634 Attachment 1 Page 3 channel methodology (1.49, 1.816 and 1.85). Using the same response times as are prr<;ently being used for the control rod drive release delay and dedicated margin for uncertainty (125 and 44 milliseconds respectively), the resultant response time for Technical Specification Table 3.3-2 can be increased to 631 )

milliseconds for sensor, reactor protection system, and control rod drive i breaker delay. (The 631 milliseconds is derived from the nev 800 milliseconds total response time less the dedicated margin for uncertainty of 44 milliseconds and the control rod drive release delay of 125 milliseconds.)

Since the four pump coastdown is the bounding transient for the pump monitors and has been analyzed showing greater margin to DNB, the consequences of all other accidents analyzed in the safety analysis report requiring the pump i monitors are also acceptable. l l

In addition, an editorial change to Technical Specification Table 3.3-2 is included. The footnote designated a "***" refers to the pump contact monitor. -

Toledo Edison uses the nomenclature pump monitor for this device. Therefore, the word " contact" is being eliminated from the Technical Specification.

Unreviewed Safety Question Evaluation Conclusions The following conclusions are provided as a result of Toledo Edison's review of the proposed changes to the Davis-Besse Nuclear Power Station, Unit No. 1, Operating License, Appendix A, Technical Specification and Bases.

The proposed action would not increase the probability of occurrence of an i

accident previously evaluated in the USAR because there have been no hardware changes or design modifications which would affect the probability of an  ;

accident. (10CFR50.59(a) (2) (i)) I 1

The proposed action would not increase the consequences of an accident )

previously evaluated in the USAR because the analysis performed shows the USAR l DNBR remains bounding. (10CFR50.59(a) (2) (i))

The proposed action would not increase the probability of occurrence of a malfunction of equipment important to safety because there have been no hardware changes or design modifications which would affect the probability of a malfunction. (10CFR50.59(a) (2) (i))

The proposed action vould not increase the consequence of a malfunction of equipment important to safety because the analysis performed shows the USAR DNBR remains bounding. (10CFR50.59(a) (2) (i))

The proposed action vould not create a possibility for an accident of a different type than any evaluated previously in the USAR because there have been no hardware changes or design modifications. (10CFR50.59(a) (2) (ii))

The proposed action would not create the possibility for a malfunction of equipment of a different type than any evaluated previously in the USAR because there have been no hardware changes or design modifications.

(10CFR50.59(a) (2) (ii))

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" Docket Number 50-346 Licenso Number NPF-3 3

Serial Number 1634 1 Attachment 1 I Page 4 The proposed action vould not reduce the margin of safety as defined in the basis for the Technical Specifications because the analysis performed shows the previous analysis remains bounding. (10CFR50.59(a) (2) (iii))

Pursuant to the above, this change to Technical Specification Table 3.3-2 does not involve an unreviewed safety question.

I References

1. VIPRE-01, A Thermal-Hydraulic Analysis Code for Reactor Cores (EPRI NP-2511).
2. RADAR, Reactor Thermal and Hydraulic Analysis During Reactor Flow Coastdown, Babcock & Vilcox, Nuclear Power Generation Division, Lynchburg, VA (BAV-10069A, Rev. 01, October, 1974).
3. B&W Calculation 32-10176-00, Densification Transients, DB Osborne, 3-11-75, Babcock & Wilcox, Nuclear Power Generation Division, Lynchburg, VA.

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4. B&V Report BAV-1401, Davis-Besse Unit 1, Fuel Densification Report, April, 1975.
5. B&V Calculation 32-9234-00, Re-Evaluation of Accidents, DB Osborne, 6-5-78, Babcock & Vilcox, Nuclear Power Generation Division, Lynchburg, VA.
6. LYNXT, Core Transient Thermal Hydraulic Program (BAV-10156-A).
7. Cycle 6 Reload Report (BAV-2038, April 1988).
8. LYNX 1, Reactor Fuel Assembly Thermal-Hydraulic Analysis Code, 7-85, Babcock & Wilcox, Nuclear Power Generation Division, Lynchburg, VA (BAV-10129-A, Rev. 00).
9. LYNX 2, Subchannel Thermal Analysis Program, 7-85, Babcock & Vilcox, Nuclear Power Generation Division, Lynchburg, VA (BAV-10130-A, Rev. 00).

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'60cket Number 50-346 License Number NPF-3 Serjal Number 1634 Attachment 1 Page 5 APPENDIX A VIPRE-01 11-CHANNEL H0 DEL DESCRIPTION A VIPRE-01 11-channel model has been developed to perform a thermal anal; sis of the complete loss of reactor coolant flow transient. The VIPRE-01 11-channel model was verified by compar$ng VIPRE-01 results of a locked rotor '

analysis to those computed by the fuel vendor, Babcock & Wilcox. This appendix summarizes the general characteristics of the VIPRE-01 11-channel model and also discusses the locked rotor analysis comparison.

The VIPRE-01 code predicts the three-dimensional velocity, pressure and temperature fields for single and two-phase flow in a PVR reactor core. It solves the finite-difference equations for mass, energy and momentum (

conservation for an interconnected array of channels assuming incompressible l' thermally expandable homogeneous flow. VIPRE-01 has undergone generic reviev l

by the NRC and has been found acceptable for use in licensing applications.

The VIPRE-01 11-channel model was developed using the subchannel analysis l j

technique described in reference 1 in which the coreEach is divided into channel is parallel uniquely i computational cells or " channels" of vatying *,12es.

identified by number, cross-sectional area, vetted perimeter and heated l l

perimeter and can communicate laterally through gaps by diversion crossflow. j The 11-channel model consists of six channels which model individual '

subchannels of the hot bundle. The remaining channels model varying numbers of subchannels and bundles. The conservation equations for mass, energy and l momentum are solved for each channel. General characteristics of the i l

l 11-channel model are listed in Table 1.

f i The thermal-hydraulic (T-H) codes used by the fuel vendor (starting with j i

Davis-Besse Cycle 6) are LYNX 1 (Referenre 8), LYNX 2 (Reference 9) and LYNXT l (Reference 6). LYNX 1 is designed to compute steady-state bundle average T-H l

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parameters including mass flow rates, bulk fluid temperatures and pressure drops. The bundle boundary conditions irom LYNX 1 are input to LYNX 2 which I computes T-H parameters on a subchannel basis for a single assembly. The l LYNXT code is used for transient analyses and is capable of modeling computational cells of varying sizes. I A !??NXT model is currently used by the ruel vendor for thermal analyses of .

loss-of-flow transients. This model has been benchmarked to the more detailed LYNX 1/ LYNX 2 analysis.

The VIPRE-01 and LYNXT models use the same design parameters which describe l the fuel assembly geometries carrently in use at Davis-Besse. These data include form loss coefficients, bypass flow and hot channel factors. The modeling technique previously described was used to construct a VIPRE model consisting of 11 channels and was derived independently of the LYNXT model.

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'bocket Number 50-346 License Wumber NPF-3 Ser,ial Number 1634 Attachment 1 Page 6 A VIPRE-01 analysis of the locked rotor transient using the 11-channel model has been performed and compared to results obtained using the LYNXT model.

The locked rotor transient is initiated by an instantaneous seizure of a reactor coolant pump rotor. The large flow resistance caused by the stationary impeller results in a rapid decrease in reactor coolant flow and minimum DNBR. The locked rotor transient was chosen la order to compare the VIPRE-01 and LYNXT models during a large change in minimum DNBR. Results are l

plotted in Figure 1 and show that VIPRE-01 and LYNXT minimum DNBR's are within 4 DNBR points (1 DNBR point = 0.01 DNBR) during the transient. This variation is small and the comparison demonstrates that the VIPRE-01 11-channel model produces minimum DNBR's that are nearly identical to those predicted by LYNXT.

i The lock rotor comparison demonstrates that the VIPRE 11-channel model is capable of accurately predicting T-H parameters during a loss-of-flov transient. Therefore, the 11-channel model may be used to analyze the l

complete loss-of-flow transient.

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' Docket Number 50-346 License Number NPF-3 Serial Number 1634 Att'achment 1 Page 7 l

APPENDIX A TABLE 1 VIPRE-01 11-CHANNEL MODEL CHARACTERISTICS Geometry Symmetry eighth core Number of Axial Nodes 48 11 Total Number of Channels Modeled 6

Number of Individual Subchannels in Hot Bundle Number of Lumped Channels in Hot Bundle 2 Number of Lumped Channels Modeled in 3 Remainder of Eighth Core Total Number of Fuel Rods Modeled 13 Number of Individual Fuel Rods 8 Number of Lumped Fuel Rods 5 Number of Conduction Rods 4 Number of Dummy Rods 9 gl Power Distribution Radial x Local Peaking Factor 1.71 Axial Flux Shape 1.65 chopped cosine located at midplane Flow Correlations Single Phase Friction VIPRE-01 Default Two Phase Friction Multiplier EPRI Subcooled Void EPRI Bulk Void EPRI Heat Transfer Correlations Single Phase Forced Convection Identical to LYNXT Subcooled Nucleate Boiling Thom Saturated Nucleate Boiling Thom Film Boiling None Mixing Model Turbulent Momentum Factor 0.8 Turbulent Mixing Coefficient 0.02 Lateral Resistance Factor 0.5 x Length / Pitch critical Heat Flux CL? Correlation B&V-2

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