ML042800122

From kanterella
Jump to navigation Jump to search
Attachment 2 - Appendix a to Topical Report DOM-NAF-2, Qualification of the F-ANP Bwu CHF Correlations in the Dominion VIPRE-D Computer Code.
ML042800122
Person / Time
Site: Millstone, Surry, North Anna  Dominion icon.png
Issue date: 09/30/2004
From: Hartz L
Dominion Nuclear Connecticut, Dominion Resources, Virginia Electric & Power Co (VEPCO)
To:
Document Control Desk, Office of Nuclear Reactor Regulation
References
04-606 DOM-NAF-2
Download: ML042800122 (45)


Text

Attachment 2 Appendix A to Topical Report DOM-NAF-2 QUALIFICATION OF THE F-ANP BWU CHF CORRELATIONS IN THE DOMINION VIPRE-D COMPUTER CODE Virginia Electric and Power Company (Dominion)

Dominion Nuclear Connecticut (DNC)

DOM-NAF-2, Rev. 0.0 APPENDIX A Qualification of the F-ANP BWU CHF Correlations in the Dominion VIPRE-D Computer Code NUCLEAR ANALYSIS AND FUEL DEPARTMENT DOMINION RICHMOND, VIRGINIA September, 2004 Prepared by:

Rosa M. Bilbao y Leon Reviewed by:

Kurt F. Flaig Recommended for Approval:

Lm / L D. M. Knee Supervisor, Nuclear Safety Analysis Director, Nuclear Analysis and Fuel

CLASS1FlCATlOWDISCLAIMER The data, information, analytical techniques, and conclusions in this report have been prepared solely for use by Dominion (the Company), and they may not be appropriate for use in situations other than those for which they are specifically prepared. The Company therefore makes no claim or warranty whatsoever, expressed or implied, as to their accuracy, usefulness, or applicability. In particular, THE COMPANY MAKES NO WARRANTY OF MERCHANTABILITY OR FITNESS FOR A PARTICULAR PURPOSE, NOR SHALL ANY WARRANTY BE DEEMED TO ARISE FROM COURSE OF DEALING OR USAGE OR TRADE, with respect to this report or any of the data, information, analytical techniques, or conclusions in it. By making this report available, the Company does not authorize its use by others, and any such use is expressly forbidden except with the prior written approval of the Company. Any such written approval shall itself be deemed to incorporate the disclaimers of liability and disclaimers of warranties provided herein. In no event shall the Company be liable, under any legal theory whatsoever (whether contract, tort, warranty, or strict or absolute liability), for any property damage, mental or physical injury or death, loss of use of property, or other damage resulting from or arising out of the use, authorized or unauthorized, of this report ABSTRACT This appendix documents Dominions qualification of the Framatome-ANP (F-ANP)

BWU-N, BWU-Z and BWU-ZM correlations with the VIPRE-D code. This qualification was performed against the same CHF experimental database used by F-ANP to develop and license the correlations. This appendix summarizes the data evaluations that were performed to qualify the VIPRE-D/BWU coddcorrelation pair, and to develop the corresponding DNBR design limits for each correlation.

DOM-NAF-2, APPENDIX A A-2

CLASSIFICATION/DISCLAlMER A-2 ABSTRACT A-2 TABLE OF CONTENTS A-3 LIST OF TABLES A-4 LIST OF FIGURES A-4 ACRONYMS AND ABBREVIATIONS A-5 A.l PURPOSE A-6 A.2 DESCRIPTION OF THE F-ANP CHF CORRELATIONS A-6 A.3 DESCRIPTION OF CHF EXPERIMENTALTESTS A-8 A.3.1 BWU-2 CORRELATION A-8 A.3.2 BWU-ZM CORRELATION A-9 A.3.3 BWU-N CORRELATION A-9 A.4 VIPRE-D RESULTS AND COMPARISON TO LYNXT/LYNX2 A-1 1 A.4.1 VIPRE-D/BWU-Z RESULTS A-12 A.4.2 VIPRE-D/BWU-ZM RESULTS A-23 A.4.3 VIPRE-D/BWU-N RESULTS A-33 A.5 CONCLUSIONS A-43 A.6 REFERENCES A-44 DOM-NAF-2, APPENDIX A A-3

LIST OF TABLES Table A.3.1-1: BWU-Z CHF Experimental Database A-0 Table A.3.2-1: BWU-ZM CHF Experimental Database A-9 Table A.3.3-1: BWU-N CHF Experimental Database A-10 Table A.4.1-1: VIPRE-D/BWU-Z M/P Ratio Results A-13 Table A.4.1-2: VIPRE-D/BWU-Z DNBR Design Limit A-14 Table A.4.1-3: VIPRE-D/BWU-Z DNBR Limits for Pressure Groups A-15 Table A.4.2-1: VIPRE-D/BWU-ZM M/P Ratio Results A-23 Table A.4.2-2: VIPRE-D/BWU-ZM DNBR Design Limit A-24 Table A.4.3-1: VIPRE-D/BWU-N M/P Ratio Results A-33 Table A.4.3-2: VIPRE-D/BWU-N DNBR Design Limit A-34 Table A.4.3-3: VIPRE-D/BWU-N DNBR Limits for Pressure Groups A-35 Table A.5-1: VIPRE-D DNBR Limits for BWU-Z, BWU-ZM and BWU-N A-43 Table A.5-2: Range of validity for BWU-Z, BWU-ZM and BWU-N A-43 LIST OF FIGURES Figure A.4.1-1: Measured vs. Predicted CHF for BWU-Z A-16 Figure A.4.1-2: M/P vs. Pressure for BWU-Z A-17 Figure A.4.1-3: M/P vs. Quality for BWU-Z A-10 Figure A.4.1-4: M/P vs. Mass Velocity for BWU-Z A-19 Figure A.4.1-5: DNBR vs. Pressure for BWU-Z A-20 Figure A.4.1-6: DNBR vs. Quality for BWU-Z A-21 Figure A.4.1-7: DNBR vs. Mass Velocity for BWU-Z A-22 Figure A.4.2-1: Measured vs. Predicted CHF for BWU-ZM A-26 Figure A.4.2-2: M/P vs. Pressure for BWU-ZM A-27 Figure A.4.2-3: M/P vs. Quality for BWU-ZM A-28 Figure A.4.2-4: M/P vs. Mass Velocity for BWU-ZM A-29 Figure A.4.2-5: DNBR vs. Pressure for BWU-ZM A-30 Figure A.4.2-6: DNBR vs. Quality for BWU-ZM A-31 Figure A.4.2-7: DNBR vs. Mass Velocity for BWU-ZM A-32 Figure A.4.3-1: Measured vs. Predicted CHF for BWU-N A-36 Figure A.4.3-2: M/P vs. Pressure for BWU-N A-37 Figure A.4.3-3: WP vs. Quality for BWU-N A-30 Figure A.4.3-4: M/P vs. Mass Velocity for BWU-N A-39 Figure A.4.3-5: DNBR vs. Pressure for BWU-N A-40 Figure A.4.3-6: DNBR vs. Quality for BWU-N A-41 Figure A.4.3-7: DNBR vs. Mass Velocity for BWU-N A-42 DOM-NAF-2, APPENDIX A A-4

ACRONYMS AND ABBREVIATIONS ARC Alliance Research Center CHF Critical Heat Flux DNB Departure from Nucleate Boiling DNBR Departure from Nucleate Boiling Ratio F-ANP Framatome Advanced Nuclear Power HTRF Heat Transfer Research Facility at Columbia University M/P Ratio of Measured-to-PredictedCHF MSMG Mid-Span Mixing Grid MVG Mixing Vane Grid NMVG Non-MixingVane Grid P/M Ratio of Predicted-to-MeasuredCHF (equivalent to DNBR)

PWR PressurizedWater Reactor USNRC US Nuclear Regulatory Commission DOM-NAF-2, APPENDIX A A-5

A.l PURPOSE Dominion has purchased fuel assemblies from Framatome ANP (F-ANP) for use at North Anna Power Station, Units 1 and 2. These new fuel assemblies are designated as Advanced Mark-BW fuel and are a one-for-one replacement for the resident fuel product, which is the North Anna Improved Fuel with ZIRLO components and PERFORMANCE+

debris resistant features (a Westinghouse fuel product). The thermal-hydraulic analysis of the F-ANP fuel product requires the use of the F-ANP BWU CHF correlations (References A1 andA2).

To be licensed for use, a critical heat flux (CHF) correlation must be tested against experimental data that span the anticipated range of conditions over which the correlation will be applied. Furthermore, the population statistics of the database must be used to establish a departure from nucleate boiling ratio (DNBR) design limit such that the probabilityof avoiding departure from nucleate boiling (DNB) will be at least 95% at a 95%

confidence level.

This appendix documents Dominions qualification of the BWU-N, BWU-Z and BWU-ZM correlations with the VIPRE-D code. This qualificationwas performed against the same CHF experimental database used by F-ANP to develop and license the correlations. This appendix summarizes the data evaluations that were performedto qualify the VIPRE-D/BWU code/correlationpair, and to develop the corresponding DNBR design limits for each correlation.

A.2 DESCRIPTION OF THE F-ANP CHF CORRELATIONS In pressurized water reactor (PWR) cores, the energy generated inside the fuel pellets leaves the fuel rods at their surface in the form of heat flux, which is removed by the reactor coolant system flow. The normal heat transfer regime in this configuration is nucleate boiling, which is very efficient. However, as the capacity of the coolant to accept heat from the fuel rod surface degrades, a continuous layer of steam (a film) starts to blanket the tube. This heat transfer regime, termed film boiling, is less efficient than nucleate boiling and can result in significant increases of the fuel rod temperaturefor the same heat flux.

Since the increase in temperature may lead to the failure of the fuel rod cladding, PWRs are designed to operate in the nucleate boiling regime and protection against operation in film boiling must be provided.

The heat flux at which the steam film starts to form is called CHF or the point of DNB. For design purposes, the DNBR is used as an indicator of the margin to DNB. The DNBR is the ratio of the predicted CHF to the actual local heat flux under a given set of conditions.

DOM-NAF-2, APPENDIX A A-6

Thus, DNBR is a measure of the thermal margin to film boiling and its associated high temperatures. The greater the DNBR value (above 1.O),the greater the thermal margin.

The CHF cannot be predictedfrom first principles, so it is empirically correlated as a function of the local thermal-hydraulic conditions, the geometty, and the power distribution measured in the experiments. Since a CHF correlation is an analyticalfit to experimental data, it has an associated uncertainty, which is quantified in a DNBR design limit. A calculated DNBR value greater than this design limit provides assurance that there is at least a 95% probability at the 95% confidence level that a departure from nucleate boiling will not occur.

F-ANP has developed and uses the B&W-2, the BWC and the BWCMV CHF correlations.

The first two of these correlations apply to fuel assemblies with non-mixing vane spacer grids of inconel or zircaloy. The BWCMV correlation applies to fuel assemblies with mixing vane grids. These correlationsare limited to applications in a high flow regime, but modem applications require the use of a correlation in the middle and low flow regimes. Using the response surface model and sequential optimization techniques, F-ANP developed a universal local conditions CHF correlation form. This correlation form, designated BWU, was modified and applied to three different fuel design types over the wider required ranges in ReferenceA l . This reference describes the CHF tests that providedthe bases for the new correlations, analyzes the performance of the correlation for each fuel type, and provides limits and guidelines for its application.

The F-ANP BWU CHF correlations are defined in Reference A1 as:

[A.2.1]

where QCHFis the critical heat flux in Btu/hr-ff?,FMsMis a dimensionless performance factor dependent on the grid arrangement of the assembly and defined in ReferencesA1 and A2, FLS is a dimensionless length spacing factor, F Tis the ~ dimensionless non-uniformflux shape factor (Tong factor) and Qunf is the uniform heat flux in Btuhr-v. The specific formulations for each one of these components, as well as the corresponding constants are F-ANP proprietary and can be found in ReferencesA1 and A2.

References A1 and A2 discuss the application of the BWU correlation form to three different grid types:

BWU-N, which is only applicable in the presence of non-mixing vane grids (NMVG).

DOM-NAF-2, APPENDIX A A-7

BWU-Z, which is the enhanced mixing vane correlation, is applicable to the DNB analysis of the fuel assembly in the mixing region.

BWU-ZM, which is BWU-Z with a multiplicative enhancement factor, is applicable in the presence of mid-span mixing grids (MSMGs).

A.3 DESCRIPTION OF CHF EXPERIMENTAL TESTS A.3.1 BWU-2 CORRELATION F-ANP developed the BWU-Z correlation to be used for fuel designs with mixing spacer grids based on the experimental data obtained at the Heat Transfer Research Facility of Columbia University (HTRF) and with the Mark BW17 spacer grid designs. The HTRF is a ten-megawatt electric facility capable of testing full length (up to 14 ft heated length) rod arrays in up to a 6-by-6 matrix. HTRF testing conditions cover the full range of PWR operating conditions with pressures up to 2,500psia, mass velocities up to 3.5 Mlbm/hr-ft* and inlet temperatures approaching saturation. Seven series of tests were used to develop the BWU-Z CHF correlation (References A1 and A4). These same tests were also used by Dominion to qualify the VIPRE-D/BWU-Z code correlation pair. Seven full assembly models were created for VIPRE-D to model these experimental test sections. Table A.3.1-1 summarizes the seven series of tests in the BWU-Z CHF experimental database.

Table A.3.1-1: BWU-Z CHF Experimental Database

~

TEST BW 12.0 BW 13.1 1 1 1;; 1 1 TYPE Unit Cell Unit Cell AXIAL HEAT FLUX SHAPE 11.55Symmetric 1.55 Symmetric

'IN OD' GUIDE TUBE OD

[Inches]

0.374 I -

0.374 I -

HEATED LENaTH

[Inches]

143.4 143.4 GRID SPACING

[Inches]

20.5 20.5 20.5 NUMBER OF TESTS 99 I BW 14.1 Guide Tube 5x5 1.55 Symmetric 0.374 10.482 143.4

~ ~~

BW 15.1 CddUnit 5x5 1.55 Symmetric 0.374 I - 143.4 20.5 BW 16.0 Cdd Row 5x5 1.55 Symmetric 0.374 I - 143.4 20.5 48

~ ~~~~~

BW 19.0 Guide Tube 5x5 1.55 Symmetric 0.374 10.482 143.4 20.5 94 0w 20.0 Unit Cell 5x5 1.55 Symmetric 0.374 I - 143.4 20.5

  • 8/

DOM-NAF-2, APPENDIX A A-8

F-ANP developed the BWU-ZM correlation to be used for fuel designs with MSMGs based on the experimental data obtained at the HTRF and with the Mark BW17 spacer grid designs. Three series of tests were used to validate the BWU-ZM CHF correlation (ReferencesA2 and A4). These same tests were also used by Dominion to qualify the VIPRE-D/BWU-ZMcode correlation pair. Three full assembly models were created for VIPRE-D to model these experimental test sections. Table A.3.2-1 summarizes the three series of tests in the BWU-ZM CHF experimental database.

Table A.3.2-1: BWU-ZM CHF Experimental Database PIN OD/ GUIDE HEATED NUMBER TEST AX'AL HEAT TUBE OD LENGTH OF TYPE FLUX SHAPE [Inches]

[Inches] TESTS 20.5 BW 18.0 Unit Cell 5x5 1.55 Symmetric 0.374 I - 143*4 [mid-span grid]

18 20.5 BW 18.1 Unit Cell 5x5 1.55 Symmetric 0.374 I- 143'4 [mid-span grid]

58 20.5 72 BW 43.0 Guide Tube 5x5 1.55 Symmetric 0.374 10.482 143'4 , [mid-span grid] ,

A.3.3 BWU-N CORRELATION F-ANP developed the BWU-N correlation for fuel designs with NMVGs based on the experimental data obtained at the heat transfer facility at the Alliance Research Center (ARC) with the Mark C and Mark BZ non-mixing spacer grid designs. This experimental facility was similar in capacity to HTRF, but has since been decommissioned. Seven Mark C tests and 3 Mark BZ tests were used to develop the correlation (References A1 and A3). These same tests were also used by Dominion to qualify the VIPRE-D/BWU-N code correlation pair. Ten full assembly models were created for VIPRE-D to model these experimental test sections. Table A.3.3-1 summarizes the ten series of tests in the BWU-N CHF experimental database.

DOM-NAF-2, APPENDIX A A-9

Table A.3.3-1: BWU-N CHF Experimental Database

'IN OD' HEATED GRID AXIAL HEAT W I D E TUBE LENOTH NUMBER TEST TYPE SPACING FLUX SHAPE OD OF TESTS

[Inches] [inches]

[Inches]

c-3 Unit Cell I 3x3' I 1.O Uniform I ~~

0.3791- 1 ~ 72.0 21.0 107 C-6 Unit Cell 1 5x5 1 1.0 Uniform I 0.37971- I 144.0 21.o 130 c-7 GuideTube I 5 x5 I 1.0 Uniform I 0.379 10.465 I 144.0 21.o 122 1.662 Cosine b C-8 Unit Cell 5x5 Symmetric 0.379 I - 144.0 155 c-9 Guide Tube 5x5 1'662 Cosine 0.379 10.465 144.0 b 85 Symmetric 1.595 Sine c-11 Unit Cell 5x5 0.379 I - 144.0 b 34 Svmmetric c-12 GuideTube 1 5x5 1 1.595 Sine Symmetric I 0.379 10.465 1 144.0 b 133 8-15 Guide Tube 5x5 1'68 Cosine 0.430 10,554 144.0 21.1 47 Symmetric 1.68 Cosine B-16 Unit Cell 5x5 Symmetric 0.430 I - 144.0 21.1 131 Intersection 1.68 Cosine 8-17 Cell 5x5 Symmetric 0.430 I - 144.0 21.1 157 a Bundle C-3 has a heated strip in each of the four walls (1.381" x 72.0").

Grid centerline distances from the end of the heated length are 15.66,37.66", 59.41", 80.91",

102.16", 123.16", 143.53".

DOM-NAF-2, APPENDIX A A-10

A.4 VIPRE-D RESULTS AND COMPARISON TO LYNXT/LYNX2 References A3 and A4 describe the mathematical model for each separate test section by providing the bundle and cell geometry, the rod radial peaking values, the rod axial flux shapes, the types, axial locations and form losses associated to the spacer grids, as well as the thermocouple locations. References A1 and A2 provide the data for each CHF observation within a test, including power, flow, inlet temperature, pressure and CHF location (rod and axial location).

Each test section was modeled for analysis with the VIPRE-D thermal-hydraulic computer code as a full assembly model following the modeling methodology discussed in Section 4 in the main body of this report. For each set of bundle data, VIPRE-D produces the local thermal-hydraulic conditions (mass velocity, thermodynamic quality, heat flux, etc) at every axial node along the heated length of the test section. The ratio of measured-to-predicted CHF (WP) is the variable that is normally used to evaluate the thermal-hydraulic performance of a code/correlationpair. The measured CHF is the local heat flux at a given location, while the predicted CHF is calculated by the code using the CHF correlation of interest (BWU-2, BWU-ZM or BWU-N). The ratio of these two values provides the M/P ratio, which is the inverse of the DNB ratio. MIP ratios are frequently used to validate CHF correlations instead of DNB ratios, because their distribution is usually a normal distribution, which simplifies their manipulation and statistical analysis.

The axial location, the hot rod and the hot channel that are used to perform the M/P comparison are important. For each test, the M/P ratio must be evaluated at the axial location where burnout was observed experimentally, as listed in References A3 and A4.

The axial nodalization for the various VIPRE-D models was developed taking into account the actual test location of the thermocouples, as well as the locations of the various spacer grids. The criteria used to select the hot channel and hot rod are supported by engineering judgment and use the information regarding burnout location provided by References A3 and A4. In general, when burnout was observed experimentally in a hot rod, a hot rod and a central (hot) channel were selected to perform the comparison. When the burnout was observed experimentally on a cold rod, a hot rod was still selected because it was considered unphysical to observe burnout in a cold rod earlier than in a hot rod (experimentally, even though a cold rod was reported to experience burnout first, the reality was that several rods saw bumout almost simultaneously and the limitations of the instrumentation and a desire to minimize damage to the test cell, caused the discrepancy). In this case, however, an external channel (cold) was selected to be the hot channel.

In addition to comparing to the experimental results, the results obtained by VIPRE-D when modeling the Mark BW, Mark C and Mark BZ experiments were benchmarked against the results obtained by F-ANP with the LYNXT/LYNX2 codes (References A1 DOM-NAF-2, APPENDIX A A-1 1

and A2). This comparison was just a sanity check to verify that there are no suspect datapoints and that the statepoint conditions were correctly input to the code.

Some of the tests analyzed were discarded prior to their incorporation into the VIPRE-D/BWU database. Two criteria were used to justify data deletions.

1) If the M/P ratio obtained for a given data point was greater than 3.5 standard deviations from the average, the data point was eliminated. This criterion is consistent with the methodology used by F-ANP in Reference A1 .
2) If any of the local conditions (pressure, mass velocity or thermodynamic quality) was outside the range of applicability of the correlation as given in References A1 and A2, the data point was eliminated. This criterion is also consistent with the methodology used by F-ANP in Reference A1 .

Overall, 23 data points were excluded from the BWU-Z database (F-ANP discarded 21 data points in Reference Al), and 11 were excluded from the BWU-N database (F-ANP eliminated 8 data points in Reference Al). No data points were eliminated from the BWU-ZM database. The reason the VIPRE-D/BWU database is slightly smaller than the LYNXTBWU database is that the local conditions predicted by VIPRE-D for a few test data were just barely outside the range of validity of the BWU correlations as given in Reference A1 ,

This section summarizes the VIPRE-D results and the associated significant statistics. In addition, this section shows a comparison to the results obtained by F-ANP with the LYNXT/LYNX2 codes as reported in References A1 and A2. This section also shows the variation of the M/P ratio with each independent variable to assess if there are any biases in the data. Finally, it provides the VIPRE-D overall statistics for the seven BWU-Z tests, the three BWU-ZM tests and the ten BWU-N tests, and generates the DNBR design limits for the various BWU CHF correlations with VIPRE-D.

A.4.1 VI PRE-D/BW U-Z RESULTS The BWU-Z correlation was developed by F-ANP correlating the CHF experimental results obtained in tests BW 12.0, BW 13.1, BW 14.1, BW 15.1, BW 16.0, BW 19.0 and BW 20.0. Dominion used those same experimental data to develop the VIPRE-D/BWU-2 DNBR limit. Table A.4.1-1 summarizes the relevant statistics for each test, and calculates the aggregate statistics for the entire set of data.

One-sided tolerance theory (Reference A5) is used for the calculation of the VIPRE-D/BWU-Z DNBR design limit. This theory allows us to calculate a DNBR limit so that, for a DNBR equal to the design limit, DNB will be avoided with 95% probability at a 95%

confidence level.

DOM-NAF-2, APPENDIX A A-12

Table A.4.1-1: VIPRE-D/BWU-Z M/P Ratio Results Because all the statistical techniques used below assume that the original data distribution is normal, it is necessary to v e r i i that the overall distribution for the M/P ratios is a normal distribution. To evaluate if the distribution is normal, the D normality test was applied (Reference A6). A value of D equal to 3,430.23was obtained for the VIPRE-D/BWU-Z database. This D value is within the range of acceptability for 528 data points with a 95% confidence level (3,387.6to 3,449.4). Thus, it is concluded that the M/P distribution for the VIPRE-DBWU-Z database is indeed normal.

Based on the results listed in Table A.4.1-1 , the deterministic DNBR design limit can be calculated as:

1.o DNBR, = [A.4.1.l]

lp- N,C,P O M IP where M/P = average measured-to-predictedCHF ratio (3wp = standard deviation of the measured-to-predictedCHF ratios of the database KN,C,P = one-sided tolerance factor based on N degrees of freedom, C confidence level, and P portion of the population protected. This number is taken from Table 1.4.4of Reference A5.

~

From Table 5 in Reference A6 D Lower Limit (528)[P = 0.0251 = 3,310+ (8/ 20)x (3,504- 3,310)= 3,387.6 D Upper Limit (528)[P = 0.9751 = 3,371 + (8/ 20)x (3,567- 3,371)= 3,449.4 DOM-NAF-2, APPENDIX A A-13

Then, the DNBR design limit for the VIPRE-D and the BWU-Z correlation can be calculated as described in Table A.4.1-2:

Table A.4.1-2: VIPRE-D/BWU-Z DNBR Design Limit Figures A.4.1-1 through A.4.1-4 displgy the performance of the WP ratio, and its distributions as a function of the pressure, mass velocity and quality. The objective of these plots is to show that there are no biases in the WP ratio distribution, and that the performance of the BWU-Z correlation is independent of the three variables of interest.

The plots show a mostly uniform scatter of the data and no obvious trends or slopes.

These plots also show that all the tests in the BWU-2 database are within 3.5 standard deviations from the average. Figures A.4.1-5 through A.4.1-7 display the performance of the P/M ratio (i.e. the DNBR) against the major independent variables for the BWU-Z database. These plots also include a DNBR design limit line at 1.20. It can be seen that only 19 data points (3.6% of the database) are above the DNBR design limit, and that these data in excess of the limit are distributed over the variable ranges tested.

In Reference A1 ,the USNRC argued that the performance of the BWU-Z correlation might be deficient at the extremely low end of the pressure range. For that reason, F-ANP developed individual DNBR design limits for each low pressure group in the database. This approach allows users to use the BWU-Z correlation at low pressures but imposes a higher DNBR limit to ensure that the correlation is used conservatively. Table A.4.1-3 summarizes the VIPRE-D/BWU-Z DNBR limits calculated for the different pressure groups and compares them with the BWU-Z DNBR design limits obtained by F-ANP in Reference A l .

DOM-NAF-2, APPENDIX A A-14

Table A.4.1-3: VIPRE-D/BWU-Z DNBR Limits for Pressure Groups I 400psia I 700 psia I 1000 psia -

11500 2400 pslal AVERAGE WP 0.8504 1.0452 1.0623 0.9883 STDEV 0.0121 0.0879 0.0787 0.0883

  1. DATA I 4 I 20 I 40 I 464 I K(N,0.95,0.95) I 6.882 I 2.396 1 2.125 I 1.768 I VIPRE-D 1.304 1.198 1.117 1.202 DNBR LIMIT

~ LyNfi! 1.590 1.199 1.125 1.193 Dominion will take the VIPRE-D/BWU-Z DNBR limit to be 1.20 for pressures greater than or equal to 700 psia, and 1.59 at pressures lower than 700 psia. Since the VIPRE-D/BWU-Z database at 400 psia only has four datapoints, Dominion has used the F-ANP more conservative DNBR limit of 1.59.

DOM-NAF-2, APPENDIX A A-15

8z Figure A.4.1-1: Measured vs. Predicted CHF for BWU-2 2

D P

h) 1.20 71 1.10 2

D 1.oo 0.90 a

E 0.60 k!

t 3c 0.50 0

5 f! 0.40 n

0.30 0.20 0.10 0.00

? 0.00 0.10 0.20 0.30 0.40 0.50 0.60 0.70 0.80 0.90 1.oo 1.10 1.20 A

m Measured CHF (MBtu/hr-ft**2)

H DOM-NAF-2,APPENDIX A A-17

0 Figure A.4.1-3: M/P vs. Quality for BWU-2 1.50 D

-u

-0 rn 1.40 z

B D

1.30

+

1.20 0

--t--11--

1.10 2 1.00 0.90 0.80 0.70 0.60 0.50 I

1 i

I II Ii II It

-0.20 -0.10 0.00 0.10 0.20 0.30 0.40 0.50 0.60 0.70 0.80

?

2 Q, Quality

0 u?

T 0

t r -

0 c? 0 Y

v-0 v-7 0

9 T

0 2

0 2

0 k

0 0

2 2 dMI DOM-NAF-2, APPENDIX A A-19

[trpd] emssaid 0 cu 0006 oos2 0002 00s1 0001 00s 0 a

00'0 01'0 02'0 08'0 OV'O OS'O 09'0 OL'O 08'0 06'0 $

It 00'1 0 01'1 i5 3

01' 1 08'1 OP'1 0s-1 09'1 a OL'1 2z 08'1 Q Q

06'1 a cu-00'2 5 PnMg JOJ aJtlSSaJd 'SA UaNQ :S-L'p't/ a ~ n b ! j z

8

BI Figure A.4.1-6: DNBR vs. Quality for BWU-Z

-0.20 -0.10 0.00 0.10 0.20 0.30 0.40 0.50 0.60 0.70 0.80 P

c! Quality

0.10 0.00 1 1 I I I 0.00 0.50 1 .oo 1.50 2.00 2.50 3.00 3.50 4.00 Mass Velocity (Mlbmlhr-ft**P)

The BWU-ZM correlation was developed by F-ANP correlating the CHF experimental results obtained in tests BW 12.0, BW 13.1, BW 14.1, BW 15.1, BW 16.0, BW 19.0 and BW 20.0. F-ANP used the experimental data obtained in tests BW 18.0, BW 18.1 and BW 43.0 to determine F ~ and M to calculate the DNBR limit for the BWU-ZM correlation (Reference A2).

Dominion has used those same experimental data to determine the VIPRE-D/BWU-ZM DNBR limit. Table A.4.2-1 summarizes the relevant statistics for each test, and calculates the aggregate statistics for the entire set of data.

One-sided tolerance theory (Reference A5) is used for the calculation of the VIPRE-D/BWU-ZM DNBR design limit. This theory allows us to calculate a DNBR limit so that, for a DNBR equal to the design limit, DNB will be avoided with 95% probability at a 95%

confidence level.

Table A.4.2-1: VIPRE-D/BWU-ZM M/P Ratio Results NUMBER WP RATIO WP RATIO M/P RATIO M/P RATIO TEST OFTESTS AVERAGE STDEV MAX BW 18.0 18 0.9931 0.1 136 1.1467 BW 18.1 58 1.0322 0.0945 1.2299 BW 43.0 72 1.0041 0.0715 1.1747 BWU-ZM 148 1.0138 0.0875 1.2299 Because all the statistical techniques used below assume that the original data distribution is normal, it is necessary to verify that the overall distribution for the M/P ratios is a normal distribution. To evaluate if the distribution is normal, the D normality test was applied (Reference A6). A value of D equal to 510.55, was obtained for the VIPRE-D/BWU-ZM database. This D value is within the range of acceptability for 148 data points with a 95% confidence level (497.82 to 515.04)d. Thus, it is concluded that the M/P distribution for BWU-ZM is indeed normal.

Based on the results listed in table A.4.2-1 , the deterministic DNBR design limit can be calculated as:

From Table 5 in Reference A6 D Lower Limit (148) [P = 0.0251= 456.9 .t (8 / 20) x (559.2 456.9) = 497.82 D Upper Limit (148) [P = 0.9751 = 473.2 + (8 / 20) x (577.8 473.2) = 515.04 DOM-NAF-2, APPENDIX A A-23

1 .o DNBR, =

'- N,C,P 'O M I P

[A.4.2.1]

where M/P = average measured to predicted CHF ratio (TWP = standard deviation of the measured to predicted CHF ratios of the database KN,C,P= one-sided tolerance factor based on N degrees of freedom, C confidence level, and P portion of the population protected. This number is taken from Table 1.4.3 of Reference A5.

Then, the DNBR design limit for the VIPRE-D and the BWU-ZM correlation can be calculated as described in Table A.4.2-2:

Table A.4.2-2: VIPRE-D/BWU-ZM DNBR Design Limit I

Number of data n 148 Degrees of freedom N =n-1 147 Average WP WP 1.0138 Standard Deviation O M 0.0875 lowen Factor I K(147,0.95,0.95)

K(147,0.95,0.95) I I 1.872 I

IBWU-ZM Design limit I DNBRL I=1 / (1.0138 - 1.872 a0.0875)

(1.0138

  • 0.0875)

~ I 1.1765 I

Figures A.4.2-1 through A.4.2-4 display the performance of the M/P ratio, and its distributions as a function of the pressure, mass velocity and quality. The objective of these plots is to show that there are no biases in the M/P ratio distribution, and that the performance of the BWU-ZM correlation is independent of the three variables of interest.

The plots show a mostly uniform scatter of the data and no obvious trends or slopes.

Figures A.4.2-5 through A.4.2-7 display the performance of the P/M ratio (i.e. the DNBR) against the major independent variables for the BWU-ZM database. These plots also include a DNBR design limit line at 1.1 8. It can be seen that only 4 data points (2.7% of the database) are above the DNBR design limit, and that these data in excess of the limit are distributed over the variable ranges tested.

DOM-NAF-2, APPENDIX A A-24

For the BWU-ZM database, no individual DNBR design limits were calculated for the low pressure data. However, in order to extend the validity of the BWU-ZM CHF correlation over the same range as the BWU-Z CHF correlation, the VIPRE-D/BWU-ZMDNBR design limit at pressures less than 594 psia was set to 1.59 (The same as for BWU-Z at low pressures). The DNBR design limit for VIPRE-D/BWU-ZM for pressures equal to or greater than 594 psia is 1.18.

DOM-NAF-2, APPENDIX A A-25

DOM-NAF-2, APPENDIX A A-26 0

0 0

c9 8

In (v

4 4 **

0 0

0 (v

  • +

n 0

u)

P 0 -

M gi!!

r = I u) to p!

n 0

0 z

0 0

In 0

0 v,

7 0

9 7

9 7

0 c\!

7 0

F -

0 9

dMI 0

2 0

2 s 0 0 2

0 2

DOM-NAF-2, APPENDIX A A-27

DOM-NAF-2, APPENDIX A A-28 s z 0 0 0 2

DOM-NAF-2, APPENDIX A A-29

[u!s~]eJIlSSeJd s:

a 0008 oosz oooz 00s 1 0001 00s 0 00'0 01'0 02'0 08'0 OP'O 0s.o 09'0 OL'O 08'0

'p 06'0 3 II 00'1 0 01'1 OZ' 1 08'1 OP' 1 0s-1 09'1 ~

OL'L g 08'1 aa 06'1 2 cu-00'2 $

f I

W p n M g JOJ amssadd -SA HgNa :s-zmpmvamQj B

tlma = w d DOM-NAF-2, APPENDIX A A-31

Figure A.4.2-7: DNBR vs. Mass Velocity for BWU-ZM D

? 0.00 0.50 1-00 1.50 2.00 2.50 3.00 3.50 4.00 w Mass Velocity (Mlbm/hr-ft**2)

A.4.3 VI PRE-DBW U-N RESULTS The BWU-N correlation was developed by F-ANP correlating the CHF experimental results obtained in the ARC tests (2-3, C-6, C-7, C-8, C-9, C-11, C-12, 8-15, B-16 and B-

17. Dominion has used those same experimental data to determine the VIPRE-D/BWU-N DNBR limit. Table A.4.3-1 summarizes the relevant statistics for each test, and calculates the aggregate statistics for the entire set of data.

Table A.4.3-1: VIPRE-D/BWU-N M/P Ratio Results One-sided tolerance theory (Reference A5) is used for the calculation of the VIPRE-D/BWU-N DNBR design limit. This theory allows us to calculate a DNBR limit so that, for a DNBR equal to the design limit, DNB will be avoided with 95% probability at a 95% confidence level.

Because all the statistical techniques used below assume that the original data distribution is normal, it is necessary to verify that the overall distribution for the M/P ratios is a normal distribution. To evaluate if the distribution is normal, the D normality test was applied (Reference A6). A value of D equal to 9,963.21 was obtained for the VIPRE-D/BW U-N database. This D value is not within the range of acceptability for 1090 data points with a 95% confidence level (10,082.0 to 10,210.60)e.Since the value of D is less than the lower critical value, the BWU-N distribution has greater kurtosis From Table 5 in Reference A6 D Lower Limit (1090) [P = 0.0251 = 9,530 + (40 / 50) x (10,220 9,530) = 10,082.0 D Upper Limit (1090) [P = 0.9751 = 9,653 + (40 / 50) x (10,350 9,653) = 10,210.6 DOM-NAF-2, APPENDIX A A-33

than a normal distribution. Therefore, the one-sided theory is conservative for VIPRE-D/BWU-N. This behavior was also observed by F-ANP in Reference A1 .

Based on the results listed in Table A.4.3-1, the DNBR limit can be calculated as:

1.o DIVBR, = [A.4.3.1]

1p - K N , C , P ' %41P where M/P = average measured to predicted ratio (TMUI/P = standard deviation of the measured to predicted ratios of the database KN,C,P= one-sided tolerance factor based on N degrees of freedom, C confidence level, and P portion of the population protected. This number is taken from Table 1.4.4 of Reference A5.

Then, the DNBR design limit for the VIPRE-D/BWU-N code/correlation pair can be calculated as described in Table A.4.3-2:

Table A.4.3-2: VIPRE-D/BWU-N DNBR Design Limit VIPRE-D/BWU-N Number of data n 1090 I Degrees of freedom I N (=n-1-14 I 1075 1 IAverage M/P I I 1 1.0018 I Standard Deviation (JMIP I 0.1038 Corrected Standard Deviation (JN = oMlp. [ (n -1) / N ] ' 0.1045 Owen Factor K(1075,0.95,0.95) 1.7239 BWU-N Design limit DNBRL = 1 / (1.0018 - 1.7239

  • 0.1045) 1.2170 Figures A.4.3-1 through A.4.3-4 display the performance of the M/P ratio, and its distributions as a function of the pressure, mass velocity and quality. The objective of these plots is to show that there are no biases in the M/P ratio distribution, and that the performance of the BWU-N correlation is independent of the three variables of interest.

The plots show a mostly uniform scatter of the data and no obvious trends or slopes.

Figures A.4.3-5 through A.4.3-7 display the performanceof the P/M ratio (i.e. the DNBR)

DOM-NAF-2, APPENDIX A A-34

against the major independent variables for the BWU-N database. These plots also include a DNBR design limit line at 1.22. It can be seen that only 65 data points are above the DNBR design limit, and that these data in excess of the limit are distributed over the variable ranges tested.

In Reference A1 ,the USNRC argued that the performance of the BWU-N correlation might be deficient at the extremely low end of the pressure range. For that reason, F-ANP developed individual DNBR design limits for each low pressure group in the database. This approach allows users to use the BWU-N correlation at low pressures but imposes a higher DNBR limit to ensure that the correlation is used conservatively.

Table A.4.3-3 summarizes the VIPRE-DBWU-N DNBR limits calculated for the different pressure groups and compares them with the DNBR design limits obtained by F-ANP in Reference A1 .

Table A.4.3-3: VIPRE-D/BWU-N DNBR Limits for Pressure Groups 800 psia 1200 psia 1500 - 2616 psia AVERAGE M/P 1.0019 1.0598 1.0007 STDEV 0.1 186 0.0865 0.1036 N, # DATA 20 20 1050 K(N,0.95,0.95) 2.396 2.396 1.7249 VIPRE-D 1.393 1.173 1.217 DNBR LIMIT L YNX2 1.387 1.290 1.207 DNBR LIMIT Dominion will take the VIPRE-D/BWU-N DNBR limit to be 1.22 for pressures equal to or greater than 1200 psia, and 1.39 at pressures less than 1200 psia.

DOM-NAF-2, APPENDIX A A-35

DOM-NAF-2, APPENDIX A A-36 0

0 0

m 0

0 10 cu 0

0 0

cu n

Q u)

P 0 -

0 2

? u) =

u) 2 P

0 0

z i i 0 0

v) 0 0 0 L?

7 t

7 0

c?

7 0

7 0

7 r

0 9

7 0

2 0

s 0 0 2

0 2

dfW DOM-NAF-2, APPENDIX A A-37

Figure A.4.3-3: M/P vs. Quality for BWU-N I

-0.60 -0.40 -0.20 0.00 0.20 0.40 0.60 0.80 Quality

DOM-NAF-2, APPENDIX A A-39 B Figure A.4.3-5: DNBR vs. Pressure for BWU-N B

57 Iu D

-0

-0 rn z

D

? 0 500 1000 1500 2000 2500 3000 8 Pressure [psia]

Figure A.4.3-6: DNBR vs. Quality for BWU-N

-0.60 -0.40 -0.20 0.00 0.20 0.40 0.60 0.80 Quality

8 Figure A.4.3-7: DNBR vs. Mass Velocity for BWU-N 5

z D

n IU

'D rn z

0 X

D 0.00 0.50 1.oo 1.50 2.00 2.50 3.00 3.50 4.00 4.50

?

R Mass Velocity (Mlbmlhr-ft**P)

A.5 CONCLUSIONS The BWU-Z, BWU-ZM and BWU-N correlations have been qualified with Dominion's VIPRE-D computer code. Table A.5-1 summarizes the DNBR design limits for VIPRE-D/BWU-Z, VIPRE-D/BWU-ZM and VIPRE-D/BWU-N that yield a 95% non-DNB probability at a 95% confidence level.

Table A.5-2 summarizes the applicability and the ranges of validity for all three CHF correlations, which are the same as those reported by F-ANP in References A1 and A2.

Table A.5-1: VIPRE-D DNBR Limits for BWU-Z, BWU-ZM and BWU-N VIPRE-D/BWU-Z DNBR limit below 700 psia I 1.59 DNBR limit 700 - 2,400 psia I 1.20 VIP RE-D/BW U-ZM DNBR limit below 594 psia 1.59 DNBR limit above 594 psia 1.18 DNBR limit below 1200 psia 1.39 DNBR limit above 1200 psia 1.22 Table A.5-2: Range of validity for BWU-2, BWU-ZM and BWU-N BWU-Z BWU-ZM BWU-N Pressure 400 to 2,465 400 to 2,465 788 to 2,616

[PSM Mass Velocity 0.36 to 3.55 0.47 to 3.55 0.25 to 3.83

[Mlbmhr-ff]

Thermodynamic Less than 0.74 Less than 0.68 Less than 0.70 Quality at CHF Mid-Span Mixing Non-Mixing Vane Applicability Mixing Vane Grids Grids Grids DOM-NAF-2, APPENDIX A A-43

A1 . Technical Report, BAW-1O199P-Al The BWU Critical Heat Flux Correlations, Framatome Cogema Fuels, August 1996, including Addendum 1, December 2000.

A2. Technical Report, BAW-10199P-A, Addendum 2, Application of the BWU-Z CHF Correlation to the Mark-BW17 Fuel Design with Mid-Span Mixing Grids, Framatome Cogema Fuels, June 2002.

A3. Technical Report, BAW-lOl43P-A, BWC Correlation of Critical Heat Flux, Babcock & Wilcox, April 1985.

A4. Technical Report, BAW-10189P-A, CHF Testing and Analysis of the Mark-BW Fuel Assembly Design, Framatome Technologies, January 1996.

A5. Technical Report, Tables for Normal Tolerance Limits, Sampling Plans, and Screening, R. E. Odeh and D. B. Owen, 1980.

A6. Technical Report, Assessment of the Assumption of Normality (employing individual observed values), American National Standards Institute, ANSI N15.15.1974.

DOM-NAF-2, APPENDIX A A-44