ML20129G669

Provides Notification of Changes or Errors in BVPS-1 & BVPS-2 LOCA Evaluation Models

ML20129G669
Person / Time
Site:	Beaver Valley
Issue date:	09/26/1996
From:	Jain S DUQUESNE LIGHT CO.
To:	NRC OFFICE OF INFORMATION RESOURCES MANAGEMENT (IRM)
References
NUDOCS 9610070258
Download: ML20129G669 (52)

Text

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, Jo g y gv v ney po..r stauon Shippingport, PA 15077-0004 N$nv . ident September 26, 1996 raxNiN$N U2U$mn l

U. S. Nuclear Regulatory Commission j Attention: Document Control Desk l Washington, DC 20555-0001 ,

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Subject:

Beaver Valley Power Station, Unit No. I and No. 2 BV-1 Docket No. 50 334, License No. DPR-66 BV-2 Docket No. 50-412, License No. NPF-73 l i

10 CFR 50.46 Report of Changes or Errors in i

. ECCS Eval- a Models This report is provided as notification of changes or errors in the BVPS-1 and BVPS-2 LOCA Evaluation Models. The following attachments provide information as requested by 10 CFR 50.46:

-l Attachment 1 Provides a listing of each change or error in an acceptable evaluation model that affects the peak fuel cladding temperature (PCT) calculation for particular transients. It quantifies the  ;

effect of changes with respect to potential plant-specific impact i on PCT for that transient and provides an "index" into l Attachment 2 (Descriptions).

l Attachment 2 Provides a description for each model change or error.

1 Attachment 3 Provides a list of references which occur in the various  !

descriptions. These documents have already been provided to the NRC by Westinghouse.

The PCT eficets, listed in Attachment 1, 'oave been applied as adjustments to the appropriate PCT calculations. This results in calculated PCTs for the Large and Small Break LOCA transients as follows:

l BVPS-1 Large Break LOCA - 2098 F BVPS-1 Small Break LOCA - 1803 F ACDI'/: ,

@N BVPS-2 Large Break LOCA - 2174 F DEllVERING BVPS-2 Small Break LOCA - 1873 F QU ALITY ENEIGV 9610070258 960926 PDR ADOCK 05000334 P PDR

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,' 10 CFR 50.46 Repod of Changes or Errors l in ECCS Evaluation Models l

Page 2 Currently, Duquesne Light plans to complete a Large Break LOCA reanalysis by June of 1999. This effon will be undenaken to support future changes in the fuel cycle design that may necessitate such reanalysis. However, changes in the anticipated date of implementation for such fuel design changes may impact the scheduled completion date for a Large Break LOCA reanalysis. These changes will be noted in future 10 CFR 50.46 annual submittals.

Any questions pertaining to this subject may be directed to Mr. Roy K. Brosi, Manager, Nuclear Safety Department, at (412) 393-5210.

Sincerely, Sushil C. Jain c: Mr. D. M. Kern, Sr. Resident Inspector Mr. H. J. Miller, NRC Region I Administrator Mr. D. S. Brinkm m, Sr. Project Manager l

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I ATTACHMENT 1 l

SUMMARY

OF PCT EFFECTS FOR BVPS LOCA TRANSIENTS

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ATTACHMENT 1

SUMMARY

OF PCT EFFECTS FOR BVPS LOCA TRANSIENTS PCT ATTACHMENT 2 l DESCRIPTION EFFECT (*F) FAfaf l 1

RyfS-1 Laroe Break LOCA

1. MODIFICATIONS TO THE WREFLOOD COMPUTER CODE (NOTE 1) 1 II. MODIFICATIONS TO THE BASH ECCS EVALUATION MODEL (NOTE 1) 2 '

V. FUEL ROD MODEL REVISIONS (NOTE 1) 6 IX. STEAM GENERATOR FLOW AREA 1*F 10 XVil. STRUCTURAL METAL HEAT MODELING -25'F 14 XXil. LARGE BREAK LOCA ROD INTERNAL PRESSURE ISSUES (NOTE 1) 17 XXIV. REVISED BURST STRAIN LIMIT MODEL O'F 19 XXV. VESSEL AND STEAM GENERATOR CALCULATION ERRORS IN LUCIFER -6*F 20 XXXVil. BASH CORE PRESSURE ERROR 73*F 32 XXXIX. CODE STREAM IMPROVEMENT O'F 34 XL. BASH: LOOP / CORE INTERFACE CORRECTIONS 0*F 35 XLI. PELLET POWER RADIAL FLUX DEPRESSION ERROR O'F 36 XLIV. POWER DISTRIBUTION ASSUMPTION 43*F 39 XLV. HOT LEG NOZZLE GAP -111 F 40 BVPS-1 Small Break LOCA IV. MODIFICATIONS TO THE SMALL BREAK LOCTA-IV COMPUTER CODE (NOTE 1) 4 V. FUEL ROD MODEL REVISIONS (NOTE 1) 6 VI. SMALL BREAK LOCA ROD INTERNAL PRESSURE INITIAL CONDITION ASSUMPTION (NOTE 1) 8 Vll. NOTRUMP CODE SOLUTION CONVERGENCE (NOTE 1) 9 XVI. STEAM GENERATOR SECONDARY SIDE MODELING ENHANCEMENTS 0F 13 XX. BVPS-1 TURBINE DRIVEN AFW PUMP ACTUATION (NOTE 1) 15 XXI. NOTRUMP DRIFT FLUX FLOW REGIME MAP ERRORS -13 TO -55*F 16 XXill. SAFETY INJECTION IN THE BROKEN LOOP 150'F 18 XXill. SAFETY INJECTION IN THE BROKEN LOOP -150 F 18 XXIV. REVISED BURST STRAIN LIMIT MODEL -2*F 19 i XXV. VESSEL AND STEAM GENERATOR CALCULATION ERRORS IN LUCIFER -16 F 20 XXVI. HOT ASSEMBLY AVERAGE ROD BURST EFFECTS 2*F 21 XXVil. ISHil DRIFT FLUX ERROR 0F 22 i XXVill. NOTRUMP POINT KINETICS ERROR O'F 23 XXIX. CORE NODE INITIALIZATION ERROR 0*F 24 XXX. NOTRUMP HEAT LINK POINTER ERROR O'F 25 XXXI. FUEL ROD MODEL ERRORS IN SBLOCA 0'F 26 l XXXil. SMALL BREAK LOCA LIMITING TIME IN LIFE 15*F 27 '

i XXXill. BOILING HEAT i 'NSFER CORRELATION ERRORS -6

• F 28 XXXIV. STEAM LINE ISOLATION LOGIC ERRORS 30'F 29 XXXV. CORE NODE ZlRC OXIDE INITIALIZATION ERROR O'F 30 XXXVI. AUTOMATIC ACTUATION OF CONTAINMENT SPRAY 4'F 31

XXXVill. SBLOCTA REVISIONS AND AXlAL NODALIZATION ERRORS 47'F 33

, XLil. PRESSURE SEARCH CONVERGENCE CR'TERIA IN NOTRUMP 0'F 37 XLill. FRICTION VALUE INPUT CORRECTIONS 0*F 38 XLVI. NOTRUMP SPECIFIC ENTHALPY ERROR 20'F 41 XLVil. SBLOCTA FUEL ROD INITIAllZATION ERROR 10'F 42 XLVill. LOOP SEAL ELEVATION ERROR -38'F 43 i

SUMMARY

OF PCT EFFECTS FOR BVPS LOCA TRANSIENTS (Continued)

PCT ATTACHMENT 2 DESCRIPTION EFFECT (*F) P_AfaE BVPS 2 Larne Break LOCA

1. MODIFICATIONS TO THE WREFLOOD COMPUTER CODE (NOTE 1) 1

11. MODIFICATIONS TO THE BASH ECCS EVALUATION MODEL (NOTE 1) 2 V. FUEL ROD MODEL REVISIONS (NOTE 1) 6 IX. STEAM GENERATOR FLOW AREA (NOTE 1) 10 XVil. STRUCTURAL METAL HEAT MODELING (NOTE 1) 14 XXil. LARGE BREAK LOCA ROD INTERNAL PRESSURE ISSUES (NOTE 1) 17 XXIV. REVISED BURST STRAIN LIMIT MODEL 0F 19 XXV. VESSEL AND STEAM GENERATOR CALCULATION ERRORS IN LUCIFER -6*F 20 XXXIX. CODE STREAM IMPROVEMENT O'F 34 XL. BASH: LOOP / CORE INTERFACE CORRECTIONS O'F 35 XLt. PELLET POWER RADIAL FLUX DEPRESSION ERROR O'F 36 XLIV. POWER DISTRIBUTION ASSUMPTION 139'F 39 XLV. HOT LEG NOZZLE GAP -111 *F 40 BVPS-2 Small Break LOCA IV. MODIFICATIONS TO THE SMALL BREAK LOCTA- V COMPUTER CODE (NOTE 1) 4  :

V. FUEL ROD MODEL REVISIONS (NOTE 1) 6 VI. SMALL BREAK LOCA ROD INTERNAL PRESSURE INITIAL CONDITION ASSUMPTION (NOTE 1) 8 Vll. NOTRUMP CODE SOLUTION CONVERGENCE (NOTE 1) 9 XVI. STEAM GENERATOR SECONDARY SIDE MODELING ENHANCEMENTS (NOTE 1) 13 XX. BVPS-1 TURBINE DRIVEN AFW PUMP ACTUATION (NOTE 1) 15 <

XXI. NOTRUMP DRIFT Fi.UX FLOW REGIME MAP ERRORS -13 TO -55'F 16 XXill. SAFETY INJECTION IN THE BROKEN LOOP 150 F 18 XXill. SAFETY INJECTION IN THE BROKEN LOOP -150*F 18 XXIV. REVISED BURST STRAIN LIMIT MODEL -2 0 F 19 i XXV. VESSEL AND STEAM GENERATOR CALCULATION ERRORS IN LUCIFER -16

• F 20 XXVI. HOT ASSEMBLY AVERAGE ROD BURST EFFECTS 2'F 21 XXVil. ISHil DRIFT FLUX ERROR 0*F 22 XXIX. CORE NODE INITIALIZATION ERROR 0F 24 XXX. NOTRUMP HEAT LINK POINTER ERROR O'F 25 XXXI. FUEL ROD MODEL ERRORS IN SBLOCA 0'F 26 XXXil. SMALL BREAK LOCA LIMITING TIME IN LIFE 24*F 27 XXXill. BOILING HEAT TRANSFER CORRELATION ERRORS -6 ' F 28 XXXIV. STEAM LINE ISOLATION LOGIC ERRORS 30*F 29 XXXV. CORE NODE ZlRC OXIDE INITIALIZATION ERROR O'F 30 XXXVI. AUTOMATIC ACTUATION OF CONTAINMENT SPRAY O'F 31 XXXVill. SBLOCTA REVISIONS AND AXtAL NODALIZATION ERRORS 610F 33 XLil. PRESSURE SEARCH CONVERGENCE CRITERIA IN NOTRUMP 0'F 37 XLill. FRICTION VALUE INPUT CORRECTIONS O'F 38 XLVI. NOTRUMP SPECIFIC ENTHALPY ERROR 20'F 41 XLVil. SBLOCTA FUEL ROD INITIALIZATION ERROR 10'F 42 Note 1:The specific impact on PCT for this item is no longer being estimated because a re-analysis has incorporated the change.

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l ATTACHMENT 2 1

DESCRIPTIONS OF MODEL CHANGES OR ERRORS J

1. $10DIFICATIONS TO THE WREFLOOD COMPUTER CODE

Background:

A modification was made to delay downcomer overfilling. The delay corresponds to backfilling of the intact cold l@gs. Data from tests simulating cold leg injection during the post large break LOCA reflood phase which gave adequate safety injection flow to condense all of the available steam flow show a significant amount of subcooled liquid to be present in the cold leg pipe test section. This situation corresponds to the so-called maximum safety injection scenario of ECCS Evaluation Model analyses.

For maximum safety injection scenarios, the reflooding models in the Westinghouse 1981 ECCS Evaluation Model, the Westinghouse 1981 ECCS Evaluation Modelincorporating the BART analysis technology, and the Westinghouse 1981 ECCS Evaluation Modelincorporating the BASH analysis technology use WREFLOOD code versions which predict the downcomer to overfil!. Flow through the vessel side of the break is computed based upon the available head of water in the downcomer in WREFLOOD using an incompressible flow in an open channel method. A modification to the WREFLOOD computer code was made to consider the cold leg inventory which would be present in conjunction with the enhanced downcomer level in the non-faulted loops.

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Change

Description:

WREFLOOD code logic was altered to consider the f;!!ing of the cold legs togethe with downcomer overfilling.  ;

Under this coding update, when the downcomer level exceeds its maximum value as input to WREFLOOD, liquid '

flow into the intact cold leg, as ws!! as spillage out the break, is considered. This logic modification stabilizes the overfilling of the vessel downcomer as it approaches equilibrium level. The appropriate WREFLOOD code versions associated with the 1981 Westinghouse ECCS Evaluation Model and the 1981 Westinghouse ECCS Evaluation ,

Modelincorporating the BART and BASH technology have been modified to incorporete the downcomer overfill  ;

logic update. I Effect of Change: i This change represents a model enhancement in terms of the consistency of the approach in the WREFLOOD code and the actual response of the downcomer level, in some cases this change could delay the overfilling process, which could result in a peak cladding temperature (PCT) penalty. The magnitude of the possible PCT penalty was assessed by reanalyzing the plant which is maximum safeguards limited (CD =0.6 DECLG case) and which is most sensitive to the t.hanges in the WREFLOOD code. The PCT penalty of 16*F which resulted for this case represents the maximum PCT penalty which could be exhibited for any plant due to the WREFLOOD logic change.

For both BVPS-1 and BVPS-2, the effect of this change on PCT is no longer being estimated because a reanalysis has incorporated the change.

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11. NIODIFICATIONS TO THE BASH ECCS EVALUATION MODEL

Background:

In the 3 ASH ECCS Evaluation Model (reference 3), the BART core modelis coupled with equilibrium-NOTRUMP computer code to calculate the dynamic interaction between the core thermohydraulics and system behavior in the reactor coolant system during core reflood. The BASH code reflood model replaces the WREFLOOD calculation to produce a more dynamic flooding transient which reflects the close coupling between core thermohydraulic and loop behavior. Special treatment of the BASH computer code outputs is used to provide the core flooding rate for use in the LOCBART computer code. The LOCBART computer code resul's from the direct coupling of the BART computer code and the LOCTA computer code to directly calculate the pak cladding temperature.

Change

Description:

l Modifications to the BASH ECCS Evaluation Modelinclude the modifications made to the 1981 ECCS Evaluation Model, discussed previously, and the following previously unreported modifications; Ssveralimprovements were made to the BASH computer code to treat special analysis cases which are related to the tracking of fluid interfaces;

1) A modification, to prevent the code from aborting, was made to the heat transfer model for the special situation I when the quench front region moves to the bottom the BASH core channel. The quench heat supplied to the fluid node below the bottom of the active fuel was set to zero.

2) A modification, to prevent the code from aborting, was made to allow negative initial movement of the liquid /two-phase and liquid-vapor interfaces. The coding these areas was generalized to prevent mass imbalance in the special case where the liquid /two-phase interface reaches the bottom of the BASH core channel.

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3) Modifications, to prevent the code from aborting, were made to increase the dimensions of certain arrays for i special applications.

4) A modification was made to write additional variables to the tape of information to be provided to LOCBART.

5) Typographical errors in the coding of some convective heat transfer terms were corrected, but the corrections have no effect on the BASH analysis results since the related terms are always set equal to zero.

6) A modification was made to the BASH coding to reset the cold leg conditions, in a conservative manner, when the accumulators empty. The BASH model is initialized at the bottom of core recovery with the intact cold legs, lower plenum full of liquid. Flow into the downcomer then equals the accumulator flow. The modification removed most of the intact cold leg water at the accumulator empty time by resetting the intact cold leg conditions to a high quality two phase mixture, in a typical BASH calculation, the downcomer is nearly full when the accumulators emptied. The delay time, prior to the intact cold leg water reaching saturation, is sufficient to allow the downcomer to fill from the ,

addition of safety injection fluid before the water in the cold legs reaches saturation. When the intact cold leg )

water reached saturation it merely flowed out of the break. The cold leg water therefore, did not affect the reflood transient. i However, in a special case, a substantial time was required to fill the downcomer after the accumulators emptied. The fluid in the intact cold legs reached saturation before the downcomer filled, which artificially perturbed the transient response by incorrectly altering the downcomer fluid conditions causing the code to abort.  !

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e Effe'ct cf Change:

Fcr typical calculations, there is no effect on the PCT calculation for the majority of the changes discussed above.

A conservative estimate of the effect of the modifications on the calculations was determined to be less than 10*F  !

singularly or in combination.

For both BVPS-1 and BVPS-2, the effect of this change is no longer being estimated because a reanalysis has incorporated the change. '

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IV. ' MODIFICATIONS TO THE SMALL BREAK LOCTA-IV COMPUTER CODE The following modifications to the LOCTA-IV computer code in the small break LOCA ECCS Evaluation Model have b;en made:

A. Change

Description:

A test was added in the rod-to-steam radiation heat transfer coefficient calculation to preclude the use of the correlation when the wall-to-steam temperature differential dropped below the useful range of the correlation.

This limit was derived based upon the physical limitations of the radiation phenomena.

Effect of Change:

There is no effect of the modification on reported PCTs since the erroneous use of the correlation forced the calculations into aborted conditions.

B. Change

Description:

An update was performed to allow the use of fuel rod performance data from the revised Westinghouse (PAD 3.3) model. ,

i Effect of Change:

An evaluation indicated that there is an insignificant effect of the modification on reported PCTs.

C. Change

Description:

Modifications supporting a general upgrade of the computer program were implemanted as follows:

1) the removal of unused or redundant coding,

2) better coding organization to increase the efficiency of calculations, and

3) Imrrovements in user friendliness a) through defaulting of some input variables, l

b) simplification of input, c) input diagnostic checks, and d) clarification of the output. j i

Effect of Change:

l Verification analyses calculations demonstrated that there was no effect on the calculated output resulting from j these changes. '

D. Change

Description:

l Two modifications improving the consistency between the Westinghouse fuel rod performance data (PAD) and l the small break LOCTA-IV fuel rod models were implemented:

1) The form of the equation for the density of uranium-dioxide in the specific heat correlation, which modeled three dimensional expansion was corrected to account for only two-dimensional thermal expansion due to the way the fuel rod is modeled.

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2) An error in the equation for the pellet / clad contact pressure was corrected. The contact resistance is never i used in licensing calculations. I Effect of Change:

The uranium-dioxide density correction is estimated to have a maximum PCT benefit of less than 2'F, while the l contact resistance modification has no PCT effect since it is not used.

For both BVPS-1 and BVPS-2, the effect of this change is no longer being estimated because a reanalysis has incorporated the change.

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T V. FUEL ROD MODEL REVISIONS

Background:

During the review of the original Westinghouse ECCS Evaluation Model following the promulgation of 10CFR50.46 in 1974, Westinghouse committed to maintain consistency between future loss-of-coolant accident (LOCA) fuel rod computer models and the fuel rod design computer models used to predict fuel rod normal operation performance.

These fuel rod design codes are also used to establish initial conditions for the LOCA analysis.

l Change

Description:

l It was found that the large break and small break LOCA code versions were not consistent with fuel design codes in the following areas:

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1. The LOCA codes were not consistent with the fuel rod design code relative to the flux depression factors at higher fuel enrichment.

2. The LOCA codes were not consistent with the fuel rod design code relative to the fuel rod gap gas conductivities and pellet surface roughness models.

3. The coding of the pellet / clad contact resistance model required revision.

Modifications were made to the fuel rod models used in the LOCA Evaluation Models to maintain consistency with the latest approved version of the fuel rod design code. i la addition, it was determined that integration of the cladding strain rate equation used in the large break LOCA Evaluation Model, as described in Reference 5, was being calculated twice each time step instead of once. The coding was corrected to properly integrate the strain rate equation.

Effect of Changes:

The changes made to make the LOCA fuel rod models consistent with the fuel design codes were judged to be insignificant, as defined by 10CFR50.46(a)(3)(i). To quantify the effect on the calculated peak cladding temperature )

(PCT), calculations were performed which incorporated the changes, including the cladding strain model correction '

for the large break LOCA. For the large break LOCA Evaluation Model, additional calculations, incorporating only the cladding strain corrections were performed and the results supported the conclusion that compensating effects were not present. The PCT effects reported below will bound the effects taken separately for the large break LOCA.

c) Large Break LOCA The effect of the changes on the large break LOCA peak cladding temperature was determined using the BASH large break LOCA Evaluation Model. The effects were judged applicable to older evaluation models. Several calculations were performed to assess the effect of the changes on the calculated results as follows:

1. Blowdown Analysis -

it was determined that the changes will have a small effect on the core average rod and hot assembly average rod performance during the blowdown analysis. The effect of the changes on the blowdown analysis was determined by performing a blowdown depressurization computer calculation for a typical three-loop plant and a typical four-loop plant using the SATAN-VI computer code.

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'2. Hot Assembly Rod Heatup Analysis -

The hot rod heatup calculations would typically show the largest effect of the changes. Hot rod heatup computer analysis calculations were performed using the LOCBART computer code to assess the effect of the changes on the hot assembly average rod, hot rod and adjacent rod.

3. Determination of the Effect on the Peak Cladding Temperature -

The effect of the changes on the calculated peak cladding temperature was determined by performing a calculation for typical three-loop and four loop plants using the BASH Evaluation Model. The analysis calculations confirmed that the effect of the ECCS Evaluation Model changes were insignificant as defined by 10CFR50.46(a)(3)(i). The calculations showed that the peak cladding temperatures increased by less than by 10*F for the BASH Evaluation Model. It was judged that 25*F would bound the effect on the peak cladding temperature for the BART Evaluation Model, while calculWons performed for the Westinghouse 1981 Evaluation Model showed that the peak cladding temperature could increase by approximately 41'F.

For both BVPS-1 and BVPS-2, the effect of this change is no longer being estimated because a reanalysis has incorporated the change.

b) Small Break LOCA The effect of the c.hanges on the small break LOCA analysis peak cladding temperature calculations was determined using the 1985 small break LOCA Evaluation Model by performing a computer analysis calculations for a typical three-loop plant and a typical four-loop plant. The analysis calculations confirmed that the effect of the changes on the small break LOCA ECCS Evaluation Model were insignificant as defined by 10CFR50.46(a)(3)(i). The calculations showed that 37*F would bound the effect on the calculated peak cladding temperatures for the four-loop plants and the three-loop plants, it was judged that an increase of 37 F would bound the effect of the changes for the 2-loop plants.

For both BVPS-1 and BVPS-2, the effect of this change is no longer being estimated because a reanalysis has incorporated the change.

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l VI. 'SMALL BREAK LOCA ROD INTERNAL PRESSURE INITIAL CONDITION ASSUMPTION l Change

Description:

The Westinghouse small break loss-of-coolant accident (LOCA) emergency core cooling system (ECCS) Evaluation Model analyses assume that higher fuel rod initial fill pressure leads to a higher calculated peak cladding t:mperature (PCT), as found in studies with the Westinghouse large break LOCA ECCS Evaluation Model.

However, lower fuel rod internal pressure could result in decreased cladding creep (rod swelling) away from the fuel ptllets when the fuel rod internal pressure was higher than the reactor coolant system (RCS) pressure. A lower fuel rod initial fill pressure could then result in a higher calculated peak cladding temperature. l l

The Westinghouse small break LOCA cladding strain modelis based upon a correlation of Hardy's data, as '

described in Section 3.5.1 of Reference 5. Evaluation of the limiting fuel rod initial fill pressure assumption revealed that this model was used outside of the applicable range in the small break LOCA Evaluation Model calculations, allowing the cladding to expand and contract more rapidly than it should. The model was corrected to fit applicable data over the range of small break LOCA conditions. Correction of the cladding strain model affects the small break LOCA Evaluation Model calculations intough the fuel rod internal pressure initial condition assumption.

Effect of Changes: j Implementation of the corrected cladding creep equation results in a small reduction in the pellet to cladding gap when the RCS pressure exceeds the rod internal pressure and increases the gap after RCS pressure falls below the rod internal pressure. Since the cladding typically demonstrates very little creep toward the fuel pellet prior to core uncovery when the RCS pressure exceeds the rod internal pressure, implementation of the correlation for the '

appropriate range has a mgligible benefit on the peak cladding temperature calculation during this portion of the transient. However, aftu the RCS pressure falls below the rod internal pressure, implementation of an accurate correlation for cladding creep in small break LOCA analyses would reduce the expansion of the cladding away from the fuel compared to what was previously calculated and results in a PCT penalty because the cladding is closer to i the fuel.

l Calculations were performed to assess the effect of the cladding strain modifications for the limiting three-inch equivalent diameter cold leg break in typical three-loop and four-loop plants. The results indicated that the change to the calculated peak cladding temperature resulting from the cladding strain model change would be less than 20 F. The effect on the calculated peak cladding temperature depended upon when the peak cladding temperature occurs and whether the rod internal pressure was above or below the system pressure when the peak cladding temperature occurs. For the range of fuel rod internal pressure initial conditions, the combined effect of the fuel rod internal pressure and the cladding strain model revision is typically bounded by 40 F. However, in an extreme case the combined effect could be as large as 60'F.

Westinghouse is currently evalusting a SBLOCA Burst / Blockage issue which is potentially more limiting than the issue discussed above. The Rod Internal Pressure item is associated with a transient configuration where rod burst does not occur. On the other hand, the Burst / Blockage issue applies if the rod bursts at the limiting time in life.

The rod burst causes a rather sharp PCT spike as both sides of the clad react with water. Since a rod cannot both burst and not burst, the higher PCT penalty from either scenario is applied to PCT. The Burst / Blockage evaluation technique is PCT dependent, in an exponential fashion due to the dependence of the Zirc-water reaction on clad teroperature, and therefore is derived after inclusion of other changes and error estimates affecting the model.

For both BVPS-1 and BVPS-2, the effect of this change is no longer being estimated because a reanalysis has incorporated the change.

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Vll. NOTRUMP CODE SOLUTION CONVERGENCE Change

Description:

In the development of the NOTRUMP small break LOCA ECCS Evaluation Model, a number of noding sensitivity studies were performed to demonstrate acceptable solution convergence as required by Appendix K to 10CFR50.

Temporal solution convergence sensitivity studies were performed by varying input parameters which govern the rate of change of key process variables, such as changes in the pressure, mass, and internal energy. StandJrd input values were specified for the input parameters which govern the time step size selection. However, since the initial studies, modifications were made to the NOTRUMP computer program to enhance code performance and implement necessary modifications (Reference 7). Subsequent to the modifications, solution convergence was not re-confirmed.

To analyze changes in plant operating conditions, sensitivity studies were performed with the NOTRUMP computer code for variations in initial RCS pressure, auxiliary feedwater flow rates, power distribution, etc., which resulted in peak cladding temperature (PCT) variations which were greater than anticipated based upon engineering judgment.

In addition, the direction of the PCT variation conflicted with engineering judgment expectations in some cases.

The unexpected variability of the sensitivity study results indicated that the numerical solution may not be properly converged.

S!nsitivity studies were performed for the time step size selection criteria which culminated in a revision to the recommended time step size selection criteria inputs. Fixed input values originally recommended for the steady state and all break transient calculations were modified to assure converged results. The NOTRUMP code was re-vsrified against the SUY-08 Semiscale experiment and it was confirmed that the code adequately predicts key small break phenomena.

Effect of Changes:

Generally, the modifications result in small shifts in timing of core uncovery and recovery. However, these changes may result in a change in the calculated peak cladding temperature which exceeds 50 F for some plants. Based on rzpresentative calculations, however, this change will most likely result in a reduction in the calculated peak cladding temperature. Since the potential beneficial effect of a non-converged solution is plant specific, a generic PCT effect cannot be provided. However, it has been concluded that current licensing basis results remain valid since the results are conservative relative to the change.

For both BVPS-1 and BVPS-2, the effect of this change is no longer being estimated because a reanalysis has incorporated the change.

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IX. ' STEAM GENERATOR FLOW AREA

Background:

Licensees are normally required to provide assurance that there exists only an extremely low probability of abnormalleakage or gross rupture of any part of the reactor coolant pressure boundary (General Design Criteria 14 and 31). The NRC issued a regulatory guide (RG 1.121) which addressed this requirement specifically for steam generator tubes in pressurized water reactors. In that guide, the staff required analytical and experimental evidence to show that steam generator tube integrity will be maintained for the combinations of the loads resulting from a LOCA and the loads from a safe shutdown earthquake (SSE). These loads are combined for added consarvatism in tha calculation of structuralintegrity. This analysis provides the basis for establishing criteria for removing tubes from service which had experienced significant degradation.

Analyses performed by Westinghouse in support of the above requirement for various utilities combined the most severe LOCA loads with the plant specific SSE as delineated in the design criteria and the Regulatory Guide.

Grnerally, these analyses showed that while tube integrity was maintained, the combined loads led to some tube diformation. This deformation reduces the flow area through the steam generator. The reduced flow area ,

increases the resistance through the steam generator to the flow of steam from the core during a LOCA, which '

potentially could increase the ca!culated PCT.

Change

Description:

i Th3 effect of tube deformation and flow area reduction in the steam generator was analyzed and evaluated for some plants by Westinghouse in the late 1970's and early 1980's. The combination of LOCA and SSE loads led to tha following calculated phenomena:

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1. LOCA and SSE loads cause the steam generatur tube bundle to vibrate.

2. The tube support plates may be deformed as a result of lateralloads at the wedge supports at the periphery of the plate. The tube support plate deformation may cause tube deformation.

3. During a postulated large LOCA, the primary side depressurizes to containment pressure. Applying the resulting pressure differential to the deformed tubes causes some of these tubes to collapse, and reduces the  !

effective flow area through the steam generator.

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4. The reduced flow area increases the resinnce to venting of steam generated in the core during the reflood phase of the LOCA, increasing the calculatt ' peak cladding temperature (PCT). j 1

Thi ability of the steam generator to continue to perform its safety function was established by evPluating the I cffect of the resulting flow area reduction on the LOCA PCT. The postulated break examined was the steam generator outlet break because this break was judged to result in the greatest loads on the steam generator and thus the greatest flow area reduction. It was concluded that the steam generator would continue to meet its safety function because the degree of flow area reduction was small, and the postulated break at the steam generator outlet resulted in a low PCT.

In April of 1990, in considering the effect of the combination of LOCA + SSE loadings on the steam generator l component, it was determined that the potential for flow area reduction due to the contribution of SSE loadings should be included in other LOCA analyses. With SSE loadings, flow area reduction may occur in all steam generators (not just the faulted loop). Therefore, it was concluded that the effects of flow area reduction during the most limiting primary pipe break affecting LOCA PCT, i.e., the reactor vessel inlet break (cold leg break LOCA), had to be evaluated to confirm that 10CFR50.46 limits continue to be met and that the affected steam generators will continue to perform their intended safety function.

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Con's equently, Ection was taken to address the safety significance of steam g:nerator tubs collapse during a cold irg break LOCA. The effect of flow area reduction from combined LOCA and SSE loads was estimated. The magnitude of the flow area reduction was considered equivalent to an increased level of steam generator tube plugging. Typically, the area reduction was estimated to range from 0 to 7.5%, depending on the magnitude of the s:ismic loads. Since detailed non-linear seismic analyses are not available for Series 51 ar.d earlier design steam generators, some area reductions had to be estimated based on available information. For most of these plants, a 5 percent flow area reduction was assumed to occur in each steam generator as a result of the SSE. For these svaluations, the contribution of loadings at the tube support plates from the LOCA cold leg break was assumed n:gligible, since the additional area reduction, if it occurred, would occur only in the broken loop steam generator.

Westinghouse recognizes that, for most plants, as required by GDC 2, " Design Basis for Protection Against Natura' Phenomena", that steam generators must be able to withstand the effects of combined LOCA + SSE loadings and continue to perform their intended safety function. It is judged that this requirement applies to undegraded as well as locally degraded steam generator tubes. Compliance with GDC 2 is addressed below for both conditions.

For tubes which have not experienced cracking at the tube support plate elevations, it is Westinghouse's engineering judgment that the calculation of steam generator tube deformation or collapse as a result of the combination of LOCA loads with SSE loads does not conflict with the requirements of GDC 2. During a large break LOCA, the intended safety functions of the steam generator tubes are to provide a flow path for the venting of steam generated in the core through the RCS pipe break and to provide a flow path such that the other plant systems can perform their intended safety functions in mitigating the LOCA event.

Tube deformation has the same effect on the LOCA event as the plugging of steam generator tubes. The effect of tube deformation and/or coll 4:e can be taken into account by assigning an appropriate PCT penalty, or accounting for the area reduction directly in the analysis. Evaluations completed to date show that tube deformation results in acceptable LOCA PCT. From a steam generator structuralintegrity perspective, Section ill of the ASME Code recognizes that inelastic deformation can occur for faulted condition loadings. There are no requirements that equate steam generator tube deformation with loss of safety function. Cross-sectional bending stresses in the tubes at the tube support plate elevations are considered secondary stresses within the definitions of the ASME Code and need not be considered in establishing the limits for allowable steam generator tube wall degradation.

Therefore, for undegraded tubes, for the expected degree of flow area reduction, and despite the calculation showing potential tube collapse for a limited number of tubes, the steam generators continuc to perform their required safety functions after the combination of LOCA + SSE loads, and thus, meeting the requirements of GDC 2.

During a November 7,1990 meeting with a utility and the NRC staff on this subject, a concern was raised that tubes with partial wall cracks at the tube support plate elevations could progress to through-wall cracks during tube deformation. This may result in the potential for significant secondary to primary inleakage during a LOCA event; it was noted that inleakage is not addressed in the existing ECCS analysis. Westinghouse did not consider the potential for secondary to primary inleakage during resolution of the steam generator tube collapse item. This is a r:latively new item, not previously addressed, since cracking at the tube support plate elevations had been insignificant in the early 1980's when the tube collapse item was evaluated in depth. There is ample data available which demonstrates that undegraded tubes maintain their integrity under collapse loads. There is also some data which shows that cracked tubes do not behave significantly differently from uncracked tubes when collapse loads are applied. However, cracked tube data is available only for round or slightly ovalized tubes.

It is important to recognize that the core melt frequency resulting from a combined LOCA + SSE event, subsequent tube collapse, and significant steam generator tube inleakage is very low, on the order of 10-8/RY or less. This estimate takes into account such factors as the possibility of a seismically induced LOCA, the expected occurrence of cracking in a tube as a function of height in the steam generator tube bundle, the localized effect of the tube support plate deformation, and the possibility that a tube which is identified to deform during LOCA + SSE loadings would also contain a partial through-wall crack which would result in significant inleakage.

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Description:

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As noted above, detailed analyses which provide an estimate of the degree of flow area reduction due to both )

I siismic and LOCA forces are not available for all steam generators. The information that does exist indicates that I

the flow area reduction may range from 0 to 7.5 percent, depending on the magnitude of the postulated forces, )

and accounting for uncertainties. It is difficult to estimate the flow area reduction for a particular steam generator j d2 sign, based on the results of a different design, due to the differences in the design and materials used for the tube support plates.

l While a specific flow area reduction has not been determined for some earlier design steam generators, the risk rs ociated with flow area reduction and tube leakage from a combined seismic and LOCA event has been shown to be. exceedingly low. Based on this low risk, it is cc idered adequate to assume, for those plants which do not have a detailed analysis, that 5 percent of the tubes se susceptible to deformation.

l The effect of potential steam generator area reduction on the cold leg break LOCA peak cladding temperature has bnn either analyzed or estimated for each Westinghouse plant. A value of 5 percent area reduction has been l applied, unless a detailed non-linear analysis is available. The effect of tube deformation and/or collapse will be taken into account by allocating the appropriate PCT margin, or by representing the area reduction by assuming )

additional tube plugging in the analysis.

W:stinghouse has determint,d, for BVPS-1, that the effect of this change on Large Break LOCA PCT is 1 *F. For BVPS-2, the effect of this change is no longer being estimated because a reanalysis has incorporated the change.

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XVI. STEAM GENERATOR SECONDARY SIDE MODELING ENHANCEMENTS Change

Description:

l A s:t of related changes which make steam generator secondary side modeling more convenient for the user were l implemented into NOTRUMP. This modelimprovement involved several facets of feedwater flow modeling. First, tha common donor boundary node for the standard evaluation model nodalization has been separated into two idIntical boundary nodes. These donor nodes are used to set the feedwater enthalpy. The common donor node configuration did not allow for loop specific enthalpy changeover times in cases where asymmetric AFW flow rates or purge volumes were being modeled for plant specific sensitivities.

Tha second improvement is the additional capability to initiate main feedwater isolation on either loss of offsite power coincident with reactor trip (Iow pressurizer pressure) or alternatively on safety injection signal low-low pr:ssurizer pressure). The previous model allowed this function only on loss of offsite power coincident with reactor trip. The auxiliary feedwater pumps are still assumed to start after a loss of offsite power with an i appropriate delay time to model diesel generator start-up and buss loading times.

I Th3 finalimprovement is in the area of modeling the purging of high enthalpy main feedwater after auxiliary ferdwater is calculated to start. This was previously modelod through an approximate time delay necessary to purge the lines of the high enthalpy main feedwater before credit could be taken for the much lower enthalpy auxiliary feedwater reaching the steam generator secondary. This time delay was a function of the plant specific purge volume and the auxiliary feedwater flow rate. The new modeling allows the user to input the purge volume directly. This then is used together with the code calculated integrated feedwater flow to determine the appropriate time at which the feedwater enthalpy can be assumed tu change.

Thise improvements are considered to be a " Discretionary Change" as described in Section 4.1.1 of WCAP-13451.

Since they involve only enhancements to the capabilities and useability of the evaluation model, and not changes to results calculated consistently with the previous model, these changes were implemented without prior review as discussed in Section 4.1.1 of 'E AP-13451. l l

Eff:ct of Change:

l Because these enhancements only allow greater ease in modeling plant specific steam generator secondary side i

behavior over the previous model, it is estimated that no effect will be seen in evaluation model calculations.

1 l Westinghouse has determined, for BVPS-1 that the effect of this change on Small Break LOCA PCT is 0*F. For BVPS-2, the effect of this change is no longer being estimated because a reanalysis has incorporated the change.

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XVit. STRUCTURAL METAL HEAT MODELING Change

Description:

1 A discrepancy was discovered during review of the finite element heat conduction model used in the WREFLOOD-INTERIM code to calculate heat transfer from structural metalin the vessel during the reflood phase. It was noted thSt the material properties available in the code corresponded to those of stainless steel. While this is correct for tho internal structures, it is inappropriate for the vessel wall which consists of carbon steel with a thin stainless internal clad. This was defined as a "Non-discretionary Change" per Section 4.1.2 of WCAP-13451, since there was thought to be potential for increased PCT with a more sophisticated composite model. The model was revised by replacing it with a more flexible one that allows detailed specification of structures.

Effect of Change: ,

l The estimated effect of this correction is a 25'F PCT benefit.

l WGstinghouse has determined, for BVPS-1, that the effect of this change on Large Break LOCA PCT is -25*F. For BVPS-2, the effect on this change is no longer being estimated because a reanalysis has incorporated the change.  ;

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XX.' BVPS-1 TURBINE DRIVEN AFW PUMP ACTUATION i

Background:

The BVPS-1 and BVPS-2 Small Break LOCA (SBLOCA) analyses differ from the approved model by (1) the removal j of credit for the Turbine Driven AFW actuation via Loss-of-Offsite Power Undervoltage Relays and (2) as a compensatory measure, installing a Si actuation circuit for the Turbine Driven (TD) AFW pump using a delay time of 60 seconds.

Tha BVPS-1 and BVPS-2 SBLOCA analyses of record are NOTRUMP Evaluation Model analyses which assume that l AFW delivery actuates on the combination of Reactor Trip / coincident Loss-of-Offsite Power (LOOP), consistent with th3 model presented in the NOTRUMP Topice' Report, in the new design, the Motor Driven (MD) pumps and Turbine Driven pump will actuate, with a 60 second delay.

Although two MD and one TD AFW pumps are available, the existing analysis credits only one MD and one TD pump due to the limiting single failure, of one Diesel Generator, which precludes operation of the second MD pump (as well as 1 train of SI Pumps).

. in the SBLOCA analysis, the Low Pressurizer Pressure (LPP) Si and LPP Reactor Trip times are both modeled, with I the SI signal occurring approximately 5 seconds later due to its lower setpoint. In addition, the analysis assumed a

! 60 second delay time for AFW pumps actuation. Therefore, crediting AFW operation based on LPP Si signal l

instead of LPP Reactor Trip / coincident LOOP represents an additional 5 second delay for AFW delivery.

! Effect of Change:

l For both BVPS-1 and BVPS-2, the effect of this change is no longer being estimated because a reanalysis has j incorporated the change.

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b XXI.' NOTRUMP DRIFT FLUX FLOW REGIME MAP ERRORS Change

Description:

Errors were discovered in both WCAP-10079-P-A and related coding in NOTRUMP subroutine DFCORRS where the improved TRAC-P1 vertical flow regime map is evaluated. This model is only used during counter-current flow '

conditions in vertical flow links. The affected equation in WCAP-10079-P-A is Equation G-65 which previously l allowed for unbounded values of the parameter Ce contrary to the intent of the original source of this equation. ,

This allowed a discontinuity to exist in the flow regime map under some circumstances. This was corrected by i placing an upper limit of 1.3926 on the parameter C. as reasoned from the discussion in the original source. As  !'

stated, this correction returned NOTRUMP to consistency with the original source for the affected equation.

Further investigation of the DFCORRS uncovered an additional closely related logic error which led to discontinuities {

l under certain other circumstances. This error was also corrected and returned the coding to consistency with WCAP-10079-P-A.

Effect of Change: i i

l Wastinghouse has determined, for both BVPS-1 and BVPS-2, that the effect of this change on Small Break LOCA I PCT is -13 to -55 F. l I

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XXil. LARGE BREAK LOCA ROD INTERNAL PRESSURE ISSUES Change

Description:

Westinghouse recently compit,ted an evaluation of a potential issue concerning the impact of increased beginning of lifa rod internal pressure (RIP) uncertainties on LOCA analyses. Historically, beginning of life fuel pressure and ttmperature uncertainties, were based upon end of life considerations. These RIP uncertainties were found to be potentially nonconservative. During the evaluation of this issue, a second issue related to the applicability of generic IFBA fuel analyses to updated LOCA Evaluation Models was also identified and combined with this issue b:cause the underlying mechanisms were the same.

The technical evaluation of this issue concluded that both the RIP uncertainty and the current IFBA fuel designs with 200 psig initial fill pressure typically wiil result in a maximum i15'F PCT variation. Consequently, RIP l manufacturing uncertainties and 200 psig initial fill pressure IFBA fuel do not have significant effects on the large break LOCA analyses. Also, based on these results, it was concluded that only nominal RIP (with an upper bound bias) should be used in the LOCA analyses for fuel designs with an initial cold fill pressure 2 200 psig. This is j consistent with past LOCA analysis.

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Effect of Change

1 For both BVPS-1 and BVPS-2, the effect of this change on PCT is no longer being estimated because a reanalysis

! has incorporated the change.

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XXill. SAFETY INJECTION IN THE BROKEN LOOP i

Change

Description:

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Westinghouse recently completed an evaluation of a potentialissue concerning the modeling of Safety injection (SI) 1 flow into the broken RCS loop for small break loss of coolant accidents (SBLOCA). Previously it had been assumed ,

that Si to the broken RCS loop would result in a lower calculated PCT. Therefore, the ECCS broken loop branch  !

line was modeled to spill the Si to the containment sump. The basis for this assumption included consideration for the effect of back pressure on the spilling ECCS line for cold leg breaks, which would see a higher back pressure ,

for Si connected to the broken RCS loop when compared to spilling against containment back pressure. Spilling to l the higher RCS pressure would increase Si to the intact loops, which is a benefit for PCT. The effect on intact loop '

Si flow rates as well as the assumption that some of the Si to the broken loop would aid in RCS/ Core recovery resulted in the Westinghouse ECCS model assumption that Si to the broken loop was a benefit. However, when Si is modeled to enter into the broken loop, a significant PCT penalty is calculated by the NOTRUMP small break evaluation model.

When a newer conservative model based on prototypic test is used to model the configuration of the SI piping to i the RCS cold leg in a Westinghouse designed PWR, a not PCT benefit is calculated, improved condensation of the loop steam in the intact loops results in lower RCS pressure and larger Si flow rates. The increase in Si flow rates, due to lower RCS pressure, leads to the lower calculated PCT. Thus, the negative effects of Si into the broken l loop can be offset by an improved Si condensation model in the intact RCS loops.

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The improved condensation model is based on data obtained from the COSI test facility. The COSI test facility is a 1/100 scale representation of the cold leg and Si injection ports in a Westinghouse designed PWR COSI tests I demonstrated that the current NOTRUMP condensation model under-predicted condensation in the intact loops a during Si and thus is a conservative model. Use of the improved condensation model has demonstrated that the current NOTRUMP small break LOCA analyses without the improved condensation model and no Si into the broken '

loop are more conservative (higher calculated PCT) than a case which includes Si into the broken loop and the improved condensation model.

Effect of Change:

Westinghouse has determined, for both BVPS-1 and BVPS-2, that the effect of the erroneous assumption on Small Break LOCA PCT is 150*F. However, this nonconservatism is more than offset by the overconservatism of condensation modeling. Therefore, the improved condensation modeling is credited with a 150'F reduction in PCT resulting in no net effect on PCT.

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i XXI\/. REVISED BURST STRAIN LIMIT MODEL Change

Description:

i A revised burst strain limit model which limits strains is being implemented into the rod heat up codes used in both Large Break and Small Break LOCA. This model, which is identical to that previously approved for use in Appendix K analyses of Upper Plenum injection plants with WCOBRA/ TRAC, as described in WCAP-10924-P-A, Rev.1, Vol.

1, Add. 4, " Westinghouse Large Break LOCA Best Estiraate Methodology: Volume 1: Model Description and Validation, Addendum 4: Model Revisions," 1991.

Effect of Change: l i

The estimated effect on Large Break LOCA PCT's ranges from negligible, to a moderate unquantified benefit, which will be inherent in calculations once this model is implemented, in Small Break LOCA, representative plant calculations indicate that the magnitude of the benefit is conservatively estimated to be exactly offsetting to the penalty introduced by the Hot Assembly Average Rod Burst issue.

Wastinghouse has determined, for both BVPS-1 and BVPS-2, that the effect of this change on Small Break LOCA PCT is 2*F. For Large Break LOCA, the effect was determined to be O'F foi both plants.

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XX0. VESSEL AND STEAM GENERATOR CALCULATION ERRORS IN LUCIFER Change

Description:

The LUCIFER code is used to generate the component databases, from raw input data, to be used in the small and l large break LOCA analyses. Errors were found in the VESCAL subroutine of the LUCIFER code. These errors were i in the geometric and mass calculations of the vessel and steam generator portions of the needed data. All LOCA analyses using the LUCIFER code outputs are affected by these error corrections. The errors were corrected in a manner to maintain the consistency of the LUCIFER code.

! Effect of Change:

Rrpresentative plant calculations indicate a net PCT effect of -16*F for small break LOCA and a -6*F for large break LOCA. Westinghouse has determined that these values are applicable to both BVPS-1 and BVPS-2, 1

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XXVI. HOT ASSEMBLY AVERAGE ROD BURST EFFECTS l

l Change

Description:

I The rod heat up code used in Small Break LOCA calculations contains a model to calculate the amount of clad I strain that accompanies rod burst. However, the methodology which has historically been used is to not apply this I burst strain model to the hot assembly average rod. This was done so as to minimize the rod gap and therefore maximize the heat transferred to the fluid channel, which in turn would maximize the hot rod temperature.

l However, due to mechanisms governing the zirc water temperature excursion (which is the subject of the SBLOCA l Limiting Time-in-Ufe penalty for the hot rod), modeling of clad burst strain for the hot assembly average rod can l result in a penalty for the hot rod by increasing the channel enthalpy at the time of PCT. Therefore, the i i methodology has been revised ::ach that burst strain will also be modeled on the hot assembly average rod. l l

l Effect of Change:

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Representative plant calculations have shown that this change introduces an approximate 10 percent increase in ths SBLOCA Limiting Time-in-Life penalty on the hot rod. However, this penalty is being offset, in affected plants, by the revised Burst Strain Limit Model.

Westinghouse has determined, for both BVPS-1 and BVPS-2, that the effect of this change on Small Break LOCA PCT is 2'F.

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1 XXVl!. ISHil DRIFT FLUX ERROR

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Change

Description:

An error was discovered both in WCAP-10079 P-A and the relevant coding in NOTPUMP subroutine ISHilA which led to an incorrect calculation of the drift flux in NOTRUMP when a laminar film annular flow was predicted. The affected equation in WCAP-10079 P-A is Equation G-74 wherein a factor of 'g', the gravitational constant, was inadvertentl/ omitted from both the documentation and the equivalent coding. The correction of this error returned NOTRUMP to consistency with the ultimate reference for the affected correlation.

Effect of Change: i Westinghouse has determined, for both BVPS-1 and BVPS-2, that the effect of this error on Small Break LOCA PCT is O'F.

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XXVlit. NOTRUM.' POINT KINETICS ERROR Change

Description:

An error was discovered in the coding used in the NOTRUMP user external subroutine VOLHEAT. The coding did not correctly perform the calculation described by Equation 3-12-28 of WCAP-10054-P-A. This calculation is only used during the time when the Point Kinetics option is used to <totormine the core power before reactor trip.

Therefore, any analysis which used the more conservative : aion of constant core power until reactor trip time is not affected by this error. The correction of this error re: lTRUMP to consistency with l

WCAP-10054-P-A. 1 1

Effect of Change:

Westinghouse has determined, for BVPS-1, that the effect of this error on Smail Break LOCA PCT is 0 F.

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XXIX CORE NODE INITIAllZATION ERROR Change

Description:

An error was discovered in how the properties of CORE NODE components were initialized for non-existent regions in the adjoining FLUID NODE. In particular, this led to artificially high core temperatures during the timestep when the core mixture level crossed a node boundary, conservatively causing slightly more core mixture level depression than appropriate during this timestep. Correction of this error allows for a smoother mixture level uncovery transient during node crossings.

Effect of Change:

Westinghousa had determined, for both BVPS-1 and BVPS-2, that the effect of this error on Small Break LOCA PCT is O'F.

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XXX. NOTRUMP HEAT LINK POINTER ERROR Change

Description:

An error was discovered in how NOTRUMP initialized certain HEAT LINK pointer variables at the start of a calculation. Correction of this error returned NOTRUMP to consistency with the originalintent of this section of coding.

Effect of Change:

Westinghouse has determined, for both BVPS-1 and BVPS-2, that the effect of this error on Small Break LOCA PCT l is O'F.

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i XXXi FUEL ROD MODEL ERRORS IN SBLOCA l

l Change

Description:

A number of minor programming errors were corrected in the fuel rod heat up code used in SBLOCA analyses. l These corrections were related to I

1. Individual rod plenum temperatures

2. Individual rod stack lengths f 3, Clad thinning logic

4. Pellet / clad contact logic i

5. Corrected gamma redistribution  !

6. Including ZrO2 thickness at t=0 initialization  !

7. Numerics and convergence criteria of initialization.

Effect of Change:

The cumulative effect of the error corrections and convergence criteria change was found to be less than approximately i4*F. This change is therefore judged to have a negligible effect on PCT. i j

W:stinghouse has determined, for both BVPS-1 and BVPS-2, that the effect of these errors on Small Break LOCA j

PCT is O'F.

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XXXII. SMALL BREAK LOCA LIMITING TIME IN LIFE .

l Change

Description:

]

Westinghouse recently completed an evaluation of a potentialissue with regard to burst / blockage modeling in the Westinghouse small break LOCA evaluation model. This potential issue involved a number of synergistic effects, all related to the manner in which the small break model accounts for the swelling and burst of fuel rods, modeling of the rod burst strain, and resulting effects on clad temperature and oxidation from the metal / water reaction models and channel blockage.

I Fuel rod burst during the course of a small break LOCA analysis was found to potentially result in a significant 1:mperature excursion above the clad temperature transient for a non-burst case. Since the methodology for SBLOCA analyses had been to perform the analyses at or near beginning of life (BOL) condition, where rod internal pressures are relatively low, most analyses did not result in the occurrence of rod burst, and therefore may not  ;

have reflected the most limiting time in life PCT. In order to evaluate the effects of this phenomenon, i Westinghouse has developed an analytical model which allows the prediction of rod burst PCT effects based upon the existing analysis of record.

Effect of Change-i Westinghouse has determined, for BVPS-1 and BVPS-2, that the effect of this change on Small Break LOCA PCT is l

15'F and 24*F respectively.

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XXXlli. BOILING HEAT TRANSFER CORRELATION ERRORS Change

Description:

This closely related set of errors deals with how the mixture velocity is defined for use in various boiling heat transfer regir 3 correlations. The previous definition for mixture velocity did not properly account for drift and slip eFects calculated in NOTRUMP. This error particularly affected NOTRUMP calculations of heat transfer coefficient when using the Westinghouse Transition Boiling Correlation and the Dougall-Rohsenow Saturated Film Boiling Correlation.

In addition, a minor typographical error was also corrected in the Westinghouse Transition Boiling Correlation.

Effect of Changes:

Westinghouse has determined, for both BVPS-1 and BVPS-2, that the effect of this change on Small Break LOCA PCT is -6'F.

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XXXIV. STEAM LINE ISOLATION LOGIC ERRORS l

Change

Description:

l I  !

This error consists of two portions: a possible plant specific effect which only applies to analyses which assumed l Main Feedwater isolation (FWI) to occur on a safety infection signal (SI), and a generic effect applying to all previous analyses.

The possible plant specific effect was the result of incorrect logic which caused the main steam line isolation to I occur on the same signal (SI) as FWI. This is inconsistent with the NRC accepted assumption of steam line  !

isolation on Loss of Offsite Power coincident with the Reactor Trip signal which occurs prior to St.

Thz generic effect was the result of incorrect logic which always led to the isolation functions occurring at a _;

slightly later time than when the appropriate signal was generated.  ;

! Effect of Change:

l Representative plant calculations for this issue resulted in the estimated PCT effect of + 12*F for the plant specific l portion, if applicable, and + 18'F for the generic portion. Westinghouse has determined, for both BVPS-1 and BVPS-2, that the effect of this change on Small Break LOCA PCT is 30*F.

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XXXV. CORE NODE ZlRC OXIDE INITIAllZATION ERROR Change

Description:

NOTRUMP models :wo regions for each core node analogous to the two (mixture and vapor) regions in adjoining fluid nodes. During the course of a transient, NOTRUMP tracks region specific quantitics for each core node.

i Erroneous logic caused incorrect initialization of the region-specific fuel cladding zirc oxide thickness at times prior .

l to the actual creation of the relevant region during the core boitoff transient.

Effect of Change:

l Westinghouse has determined, for both BVPS-1 and BVPS-2, that the effect of this change on Small Break LOCA

! PCT is O'F.

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XXXVI. AUTOMATIC ACTUATION OF CONTAINMENT SPRAY l

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Description:

Through analyses it has been found that breaks as small as two inches or less may actuate the containment spray system within several minutes of break initiation for some plants. As a result of the high containment spray flow I rat 3 and the prolonged nature of the small break LOCA, switchover to sump recirculation may be required before

the event is completely resolved (ECCS injection flow exceeds break flow, RCS mass is increasing and peak clad l t

:mperature is decreasing or the core is fully quenched). The current small break licensing basis does not address severalissues related to ECCS switchover and long term recirculation.

SIction D of 10 CFR 50, Appendix K requires that the containment pressure used in the ECCS evaluation models l

account for the effects of all installed containm ent heat removat equipment. The current Westinghouse small break ECCS evaluation modelis not considered to be sensitive to containment pressure effects because the calculated braik flow is critically limited throughout the transient. As such, the small break ECCS evaluation model does not account for actuation and operation of the containment spray system. Furthermore, since the small break ECCS evaluation model does not account for operation of the containment spray system, the ECCS evaluation model does not include switchover to ECCS recirculation. This approach may no longer be bounding with respect to maximum PCT.

Th3 current Westinghouse small break evaluation model assumes a continuous supply of ECCS water at injection rnode flow rates and the enthalpy of the injection fluid throughout the transient. At the time of switchover to recirculation during a small break LOCA, the ECCS pumps may be shut down for realignmer't resulting in a period l of no Si delivery for some plants in addition, some plants may have less available ECCS recirculation flow than ECCS injection flow due to closure of the safety injection pump discharge cross-tie valves. Furthermore, the l current small break licensing basis analysis does not account for the change in enthalpy due to recirculation since it I had been assumed that the event would be resolved before retirculation.

This issue also has the potential to effect the limiting single failure assumption used in the small break ECCS evaluation model. The current single failure assumption is the failure of an emergency diesel generator and loss of ons entire safeguards train. If both emergency diesel generators start and supply power to the containment spray pumps, the RWST would drain earlier in the transient. The loss of a single intermediate head pump or charging pump could conceivably be more limiting than the loss of a complete train of safeguards systems.

Th3 modeling of these effects could potentially lead to worse results than those predicted in the current analyses.

Effect of Change:

Westinghouse has determined, for BVPS-1 and BVPS-2, thet the effect of this change on Small Break LOCA PCT is 4*F and O'F respectively.

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i XXXVil. BASH CORE PRESSURE ERROR

, i 1-Change

Description:

The Beaver Valley Power Station (BVPS) Unit 1 Large Break LOCA (LBLOCA) analysis of record is a BASH  !

evcluation model analysis An input error has been identified for the BVPS Unit 1 LBLOCA analysis which involves '

tho value of the core pressure which was used for the reflood phase of the LBLOCA transient. An incorrect value -

was inadvertently transcribed for use as an input to this phase of the model.

l Effect of Change:

, i Wostinghouse has determined for BVPS-1 that the effect of this change on Large Break LOCA PCT is 73'F.

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l XXXVill. SBLOCTA REVISIONS AND AXIAL NODAllZATION ERRORS Change

Description:

Westinghouse has completed an evaluation of issues concerning the SBLOCTA code which 's a part of both the NOTRUMP and WFLASH SBLOCA ECCS Evaluation Models. The potentialissue originally identified was a deficiency in the amount of detail used for the axial nodalization of the fuel rod, as it affected the solution of the channel fluid equations. Further investigation identified several additional related issues associated with nodalization and the overall solution of the fluid conservation equations which have subsequently been corrected.

As a separate, but related issue, a revised model for calculating transient fuel rod interrial pressure was implemented in the SBLOCTA code. The NRC was informed of these modeling changes, which were summarized in the closeout notification of reference 15.

Effect of Change:

Westinghouse has determined, for BVPS-1 and BVPS-2, that the effect of this change on small break LOCA PCT is 47*F and 61*F respectively.

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• i XXXIX. CODE STREAM IMPROVEMENT '

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Change Description.

Revisions were made to the proc.edures used to interface the various codes that comprise the entire execution stream for performing a large break LOCA analysis with the BASH evaluation m' del. Previously, the coupled i WREFLOOD/ COCO code for calculating containment pressure response was tran ferred res a boundary condition to l

the BASH code. This transfer has been replaced with direct coupling of the BASH and COCO codes such that the same code used to calculated the RCS conditions during reflood, also supplies the boundary conditions for the containment pressure calculation. In conjunction with this, the portion of the WREFLOOD code which calculated the refill phase of the transient has been reprogrammed into a separate, but identical code called REFILL, which is also coupled with COCO.

This methodology revision was made only as a process improvement for conducting analyses and involved no changes to the approved physical models, nor basic solution techniques governing the solutions provided by the individual computer codes. The NRC was advised of the implementa. ion of this methodology on a forward-fit basis via reference 16.

Effect of Change:

Wastinghouse has determined, for both BVPS-1 and BVPS-2, that the effect of this change on large break LOCA PCT is O'F.

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XL. BASH: LOOP / CORE INTERFACE CORRECTIONS  ;

t Change

Description:

Corrections were made to the logic for interfacing the loop model and BART code model. One correction prevents the possibility of an occasional inconsistency in how the core timestep was limited by the loop timestep. Another l corrects the fluid density used in the interface calculation when the inlet flowrate is negative.

t Eff:ct of Change: l l

WIstin0 house has determined, for both BVPS 1 and BVPS-2, that the effect of this change on large break LOCA PCT is 0"F.

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XLI. PELLET POWER RADIAL FLUX DEPRESSION ERROR Change

Description:

A coding error (an incorrect sign) was discovered and corrected in a subroutine that calculates radial distribution I

power factors in the fuel pellet for the LOCBART code. Sensitivity studies found the error correction to result in I IGss than a 0.1F effect on predicted peak clad temperature.

l l Effect of Change:

l WCstinghouse has determined, for both BVPS-1 and BVPS-2, that the effect of this change on large break LOCA i

PCT is 0*F.

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XLil! PRESSURE SEARCH CONVERGENCE CRITERIA IN NOTRUMP Change

Description:

Tha convergence criteria used during the pressure search in NOTRUMP do not ensure a sufficiently accurate value for Fluid Node pressure when conditions approach the boundary between subcooled and saturated in some cases.

The resulting effects on predicted pressure were more pronouriced at pressures below those normally seen during  !

standard evaluation model calculations. The previously hardwired convergence criteria values have been replaced by user input. Appropriate values have been determined and will be implemented in all future analyses.

Effect of Change:

Westinghouse has determined, for both BVPS-1 and BVPS-2, that the effei t. of this change on small break LOCA PCT is 0 F.

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XLill. FRICTION VALUE INPUT CORRECTIONS i Change

Description:

The SPADES code is used to generate input decks for the small break analysis code, NOTRUMP. An error was found in the code which involved the values assigned to some of the friction factor input. The erroneous values i had no impact on transient calculations and were corrected in order to maintain the consistency of the SPADES code with the relevant documentation. i Effect of Change. ,

Wzstinghouse has determined, for both BVPS-1 and BVPS-2, that the effect of this change on small break LOCA {

PCT is O'F. l 1

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XLIV. POWER DISTRIBUTION ASSUMPTION Change

Description:

Lerge Break LOCA analyses have been traditionally performed using a symmetric, chopped cosine, core axial power distribution. Under certain conditions, calculations have shown that there is a potential for top-skewed power distributions to result in Peak Cladding Temperatures (PCTs) greater than those calculated with chopped cosine exial power distributions. In 1991 Westinghouse developed a statistical methodology to evaluate and assure that the cosine distribution remains the limiting distribution. This methodo!ogy, Power Shape Sensitivity Model (PSSM),

was submitted to the NRC for review and approval via Reference 8 and has beer.1pplied to both BVPS-1 and BVPS-2. Although Westinghouse believed that PSSM was conservative without additional modifications, Westinghouse later decided not to continue pursuing licensing of PSSM.

An alternate methodology to replace PSSM, ESHAPE (Explicit Shape Analysis for PCT Effects), is based on an explicit analysis of the Large Break LOCA transient with a set of skewed axial power shapes to supplement the standard analysis done with the chopped cosine. Development of this methodology was completed in June 1995.

A submittal notifying the NRC of this substitution was made by Reference 17.

Effect of Change:

Westinghouse has determined, for BVPS-1 and BVPS-2, that the effect of this change on large break LOCA PCT is 43 F and 139'F respectively.

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XLV. HOT LEG NOZZLE GAP 1

i Change

Description:

This improvement to the Large Break LOCA evaluation model allows for the modeling of flow through the hot leg nczzle gap. A PCT reduction is obtained by including stecm flow through the reactor vessel hot leg nozzle gap I (between the core barrel and the reactor vessel) in the calculations. This hot leg gap model allows steam flow to l the break in the latter phases of the Large Break LOCA transient making it effective for offsetting skewed power i shape effects which occur in the same time period. Further description of this methodology was submitted for NRC  ;

review by Reference 18.

1 Effect of Change:

l Westinghouse has determined, for both BVPS-1 and BVPS-2, that the effect of this change on large break LOCA ,

PCT is -111 *F.

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l XLVI. NOTRUMP SPECIFIC ENTHALPY ERROR l l

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Description:

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A typographical error was found in a line of coding in the NOTRUMP code. This line of coding was intended to model the calculation found in Equation L-127 of WCAP-10079-P-A. Although the equation in the topical report is i correct, the coding represented the last term as a partial derivative with respect to the fluid node mixture region i l total energy instead of the mixture region total mass.

[ Effect of Change:

1 Westinghouse has determined, for both BVPS-1 and BVPS-2, that the effect of this error on small break LOCA PCT is 20*F.

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l XLVil. SBLOCTA FUEL ROD INITIAllZATION Change

Description:

1 An error was discovered in the SBLOCTA code related to adjustments which are made as part of the fuel rod l initialization process which is used to obtain agreement between the SBLOCTA model and the fuel data supplied from the fuel thermal-hydraulic design calculations at full power, steady-state conditions. Specifically, an adjustment to the power, which is made to compensate for adjustments to the assumed pellet diameter was incorrect. Additionally, updates were made to the fuel rod clad creep and strain model to correct logic errors that could occur in certain transient conditions. These model revisions had a small effect on the fuel rod initialization '

process, and could produce small effects during the transient. Due to the small magnitude of effects, and the interaction between the two items, they are being evaluated as a single, closely related effect.

Effect of Change:

l l Representative plant calculations with the corrected model demonstrated that these revisions result in a predicted

! peak clad temperature increase on the order of +10'F.  ;

Westinghouse has determined, for both BVPS-1 and BVPS-2, that the effect of these errors on small break LOCA PCT is 10*F.

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.XLVill. LOOP SEAL ELEVATION ERROR Change

Description:

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I An error was discovered in raw plant geometric data that supports input to the evaluation model codes. The l erroneous datum was a term associated with the relative elevation of the crossover leg. j

! Effect of Change:  !

Th3 erroneous elevation terms are estimated to have a negligible effect on large break LOCA evaluation model l c:lculations. Representative sensitivity calculations with NOTRUMP have determined that a PCT effect is to be h expected due to the influence of the erroneous elevation on the loop seal clearing process. PCT effects ranging from -44'F to + 24*F have been assigned to affected plants depending on the magnitude and direction of the error.

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Wastinghouse has determined, for BVPS-1, that the effect of this error on small break LOCA PCT is -38'F. l t

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e ATTACHMENT 3 REFERENCES

ATTACHMENT 3  !

REFERENCES  !

1. NS-NRC-89-3464

• Correction of Errors and Modifications to the NOTRUMP Code in the Westinghouse )

Small Break LOCA ECCS Evaluation Model Which Are Potentially Significant," I. meter from W. J. Johnson (Westinghouse) to T. E. Murley (NRC), Dated October 5,1989.  ;

2. WCAP-9220-P-A, Revision 1 (Proprietary), WCAP-9221-A, Revision 1 (Non-Proprietary), " Westinghouse ECCS Evaluation Model - 1981 Version," 1981, Eicheidinger, C.

1'

3. WCAP-10266-P-A, Revision 2 (Proprietary), WCAP-10267-A, Revision 2 (Non-Proprietary), Besspiata.

l J.J., et. al., "1981 Version of the Westinghouse ECCS Evaluation Model Using the BASH Code,' March 1987, i

4. WCAP-10054-P-A (Proprietary), WCAP-10081-A (Non-Proprietary), ' Westinghouse Small Break ECCS Evaluation Model Using the NOTRUMP Code,' Lee, N., et. al., August 1985.

1

5. 'LOCTA-IV Program: Loss-of-Coolant Transient Analysis," WCAP-8305, (Non-Proprietary), June 1974.

6. "BART-Al A Computer Code for the Best Estimate Analysis of Reflood Transients," WCAP-%95-A (Non-Proprietary), March 1984.

7. *10CFR50.46 Annual Notification for 1989 of Modifications in Westinghouse ECCS Evaluation Models," I NS-PRC-89-3463, Letter from W. J. Johnson (Westinghouse) to T. E. Murley (NRC), Dated October 5, l 10.

l

8. WCAP-12909-P (Proprietary), " Westinghouse ECCS Evaluation Model Revised LBLOCA Power i Distribution Methodology," Dated May 22,1991, i i

9. NS-NRC-91-3578, ' Westinghouse ECCS Evaluation Model Revised LBLOCA Power Distribution .

Methodology," Dated May 22,1991.

10. WCAP-13451, ' Westinghouse Methodology For Implementation of 10 CFR 50.46 Reporting."

11. WCAP-10484, Addendum 1, " Spacer Grid Heat Transfer Effects During Reflood,' Shimeck, December l 1992.

12. ET-NRC-91-3633, " Methodology Clarifications to WCAP-12909-P," Ietter from S.R. TRITCH (Westinghouse) to R.C. Jones (NRC), Dated November 21,1991.

13. ET-NRC-93-3971, ' Notification of a Significant Change To Westinghouse Small Break LOCA ECCS Evaluation Model, Pursuant To 10 CFR 50.46(a)(3)(ii): Safety Injection (SI) in the Broken loop," Letter from N. J. Liparulo (Westinghouse) to R. C. Jones (NRC), Dated September 21,1993.

14. WCAP-10924-P-A, Revision 1, Volume 1, Addendum 4, " Westinghouse Large Break LOCA Best Estimate Methodology," 1991.

15. NTD-NRC-94-4343, ' Interim Report of an Evaluation of a Failure to Comply Pursuant to 10 CFR 21.21(a)(2)-Closeout 94-002,* letter from N. J. Liparulo (Westinghouse) to NRC, Dated November 15, 1994.

, 16. NTD-NRC-94-4143, " Change in Methodology for Execution of Bash Evaluation Model,' letter from i N. J. Liparuto (Westinghouse) to W. T. Russell (NRC), Dated May 23,1994.  !

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! i c ATTAC1BIENT 3

, REERENCES l

(Continued) l

17. NTD-NRC-95-4518, " Withdrawal of WCAP 12909-P on Power Shape Sensitivity Model (PSSM)," letter  ;

from N. J. Liparuto (Westinghouse) to NRC, Dated August 7,1995. '

4

18. NTD-NRC-95-4477, " Transmittal of Topical Reports WCAP-14404-P and WCAP-14405-P, " Methodology l for Incorporating Hot Leg Nozzle Gaps into BASH," letter from N. J. Lipamlo (Westinghouse) to  !

R. C. Jones (NRC), Dated July 25,1995. l.

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