ML100610104: Difference between revisions

From kanterella
Jump to navigation Jump to search
(Created page by program invented by StriderTol)
(StriderTol Bot change)
 
(One intermediate revision by the same user not shown)
Line 18: Line 18:


=Text=
=Text=
{{#Wiki_filter:Dominion Nuclear Connecticut, Inc.5000 Dominion Boulevard, Glen Allen, Virginia 23060 Web Address: www.dom.com March 1, 2010 U.S.Nuclear Regulatory Commission Attention:
{{#Wiki_filter:Dominion Nuclear Connecticut, Inc.
Document Control Desk Washington, DC 20555 Serial No.: NLOSIWDC Docket No.: License No.: 10-072 RO 50-423 NPF-49 DOMINION NUCLEAR CONNECTICUT, INC.MILLSTONE POWER STATION UNIT 3 RESPONSE TO REQUEST FOR ADDITIONAL INFORMATION QUESTIONS 26, 27 AND 29 REGARDING A SPENT FUEL POOL CRITICALITY LICENSE AMENDMENT REQUEST Dominion Nuclear Connecticut, Inc.(DNC)submitted a stretch power uprate (SPU)license amendment request (LAR)for Millstone Power Station Unit 3 (MPS3)in letters dated July 13, 2007 (Serial Nos.07-0450 and 07-0450A).
5000 Dominion Boulevard, Glen Allen, Virginia 23060 Web Address: www.dom.com March 1, 2010 U. S. Nuclear Regulatory Commission                           Serial No.:  10-072 Attention: Document Control Desk                             NLOSIWDC    RO Washington, DC 20555                                         Docket No.: 50-423 License No.: NPF-49 DOMINION NUCLEAR CONNECTICUT, INC.
The SPU license amendment request was supplemented in a letter dated December 13, 2007 (Serial No.07-0450C).
MILLSTONE POWER STATION UNIT 3 RESPONSE TO REQUEST FOR ADDITIONAL INFORMATION QUESTIONS 26, 27 AND 29 REGARDING A SPENT FUEL POOL CRITICALITY LICENSE AMENDMENT REQUEST Dominion Nuclear Connecticut, Inc. (DNC) submitted a stretch power uprate (SPU) license amendment request (LAR) for Millstone Power Station Unit 3 (MPS3) in letters dated July 13, 2007 (Serial Nos. 07-0450 and 07-0450A). The SPU license amendment request was supplemented in a letter dated December 13, 2007 (Serial No. 07-0450C). The SPU LAR included a revised spent fuel pool (SFP) criticality analysis with proposed changes in technical specification (TS) requirements. DNC separated the MPS3 SFP TS change request from the MPS3 SPU request via letter dated March 5, 2008 (Serial No. 07-0450D).
The SPU LAR included a revised spent fuel pool (SFP)criticality analysis with proposed changes in technical specification (TS)requirements.
In a letter dated August 8, 2008, the Nuclear Regulatory Commission (NRC) transmitted a request for additional information (RAI) regarding the SFP TS. DNC responded to RAI questions 1 through 19 in a letter dated September 30, 2008 (Serial No. 08-0511A). Additionally, in a letter dated February 2, 2009, the NRC requested additional information. DNC responded to RAI questions 20, 22, 23, and 25 in a letter dated March 5, 2009 (Serial No. 09-084) and to RAI questions 21 and 24 in a letter dated March 23, 2009 (Serial No. 09-084A). Subsequently, in a letter dated January 26,2010, the NRC requested additional information.
DNC separated the MPS3 SFP TS change request from the MPS3 SPU request via letter dated March 5, 2008 (Serial No.07-0450D).In a letter dated August 8, 2008, the Nuclear Regulatory Commission (NRC)transmitted a requestforadditional information (RAI)regarding the SFP TS.DNC responded to RAI questions 1 through 19 in a letter dated September 30, 2008 (Serial No.08-0511A).
Attachment 1 of this letter provides responses to RAI questions 26, 27 and 29.
Additionally, in a letter dated February 2, 2009, the NRC requested additional information.
Responses to RAI questions 28 and 30 will follow in a separate letter.
DNC responded to RAI questions20,22, 23, and 25 in a letter dated March 5, 2009 (Serial No.09-084)and to RAI questions 21 and 24 in a letter dated March 23, 2009 (Serial No.09-084A).Subsequently, in a letter dated January 26,2010, the NRC requested additional information.
The information provided by this letter does not affect the conclusions of the significant hazards consideration discussion in the December 13, 2007 DNC letter (Serial No. 07-0450C).
Attachment 1 of this letter provides responses to RAI questions 26, 27 and 29.Responses to RAI questions 28 and 30 will follow in a separate letter.The information provided by this letter does not affect the conclusions of the significant hazards consideration discussion in the December 13, 2007 DNC letter (Serial No.07-0450C).
 
Serial No.10-072 Docket No.50-423 Response to RAI for the MPS3 Spent Fuel Pool Criticality LAR Page 2 of 3 Should you have any questions in regard to this submittal, please contact Wanda Craft at 804-273-4687.
Serial No. 10-072 Docket No. 50-423 Response to RAI for the MPS3 Spent Fuel Pool Criticality LAR Page 2 of 3 Should you have any questions in regard to this submittal, please contact Wanda Craft at 804-273-4687.
Sincerely, ciYJ,L/{j Leslie N.Hartz Vice President-Nuclear Support Services Commitments made in this letter: 1.None.COMMONWEALTH OF VIRGINIA))COUNTY OF HENRICO)The foregoing document was acknowledged before me, in and for the County and Commonwealth aforesaid, today by Leslie N.Hartz, who is Vice President-Nuclear Support Services of Dominion Nuclear Connecticut, Inc.She has affirmed before me that she is duly authorized to execute and file the foregoing document in behalf of that Company, and that the statements in the document are true to the best of her knowledge and belief.Acknowledged before me this/51 day of/VJ ttYCM..J My Commission Expires: 4/CO I J3 ,2010.GINGER l.AlliGOOD Notary Public Commonwealth Of Virglni, 310847 My COmmission Expires Apr 30.2013H C!M:ttsNotary Public Serial No.10-072 Docket No.50-423 Response to RAI for the MPS3 Spent Fuel Pool Criticality LAR Page 3 of 3  
Sincerely, ciYJ,L/{j Leslie N. Hartz Vice President - Nuclear Support Services Commitments made in this letter:
: 1. None.
COMMONWEALTH OF VIRGINIA                     )
                                              )
COUNTY OF HENRICO                             )
The foregoing document was acknowledged before me, in and for the County and Commonwealth aforesaid, today by Leslie N. Hartz, who is Vice President - Nuclear Support Services of Dominion Nuclear Connecticut, Inc. She has affirmed before me that she is duly authorized to execute and file the foregoing document in behalf of that Company, and that the statements in the document are true to the best of her knowledge and belief.
Acknowledged before me this           /51   day of   /VJ ttYCM..J       ,2010.
My Commission Expires:                 4/CO IJ3 GINGER l. AlliGOOD Ld~    ~H                C!M:tts Notary Public Notary Public Commonwealth Of Virglni, 310847 My COmmission Expires Apr 30.2013
 
Serial No. 10-072 Docket No. 50-423 Response to RAI for the MPS3 Spent Fuel Pool Criticality LAR Page 3 of 3


==Attachment:==
==Attachment:==
: 1. Attachment 1: Response to Request for Additional Information (RAI)
Questions 26, 27 and 29 Regarding the Spent Fuel Pool Criticality License Amendment Request cc:    U.S. Nuclear Regulatory Commission Region I Regional Administrator 475 Allendale Road King of Prussia, PA 19406-1415 Ms. C. J. Sanders Project Manager U.S. Nuclear Regulatory Commission One White Flint North 11555 Rockville Pike Mail Stop 08-B3 Rockville, MD 20852-2738 NRC Senior Resident Inspector Millstone Power Station Director Bureau of Air Management Monitoring and Radiation Division Department of Environmental Protection 79 Elm Street Hartford, CT 06106-5127
Serial No. 10-072 Docket No. 50-423 ATTACHMENT 1 RESPONSE TO RAI QUESTIONS 26, 27 AND 29 REGARDING THE SPENT FUEL POOL CRITICALITY LICENSE AMENDMENT REQUEST DOMINION NUCLEAR CONNECTICUT, INC.
MILLSTONE POWER STATION UNIT 3
Serial No. 10-072 Docket No. 50-423 Response to RAI for the MPS3 Spent Fuel Pool LAR Attachment 1. Page 1 of 11 RESPONSE TO RAI QUESTIONS 26 THROUGH 30 REGARDING THE SPENT FUEL POOL CRITICALITY LICENSE AMENDMENT REQUEST Question 26 In response to RAI # 5 ONC states:
NUREG/CR-6665. Reference 4, identifies both specific power and operating history effects as weakly correlated to increased reactivity for discharged fuel assemblies. The maximum impact noted in Reference 4 is approximately 0.00200 11 Keff. This result is caused by reduced power operation near the end of assembly depletion. The depletion calculations supporting the analysis presented in WCAP-16721-P do not include part power operation. Instead, the soluble boron concentration is maintained at a constant value above the cycle average value for the entire depletion.
The spectral hardening from the presence of boron, especially at the end of the cycle when the concentration is several hundred ppm above physical values, provides additional margin to account for this potential impact. The use of additional margin is the approach suggested in Reference 4 for accounting for the potential for operating history effects.
In order to determine if the conservatism gained from taking credit for using a higher than actual soluble boron concentration during the simulated depletion of the fuel in the reactor is enough to cover the 0.00200 11 Keff. the NRC staff needs to know how much more than the actual boron concentration was used. Please provide additional information regarding how much soluble boron concentration was used during the simulated depletion of the fuel in the reactor compared to the actual.
===Response===
With regard to specific power and operating history effects, NUREG/CR-6665, Reference 4, makes the following recommendation:
    "It appears that the optimum approach would be to assume a simple continuous-power operating history, and add in a margin to account for operating-history-induced effects."
Consistent with this recommendation, the depletions performed for WCAP-16721-P (including those for request for additional information (RAI) responses through RAI 30) used a constant power throughout the entire burnup range. The power modeled is consistent with uprated core conditions.
Serial No. 10-072 Docket No. 50-423 Response to RAI for the MPS3 Spent Fuel Pool LAR Attachment 1, Page 2 of 11 NUREG/CR-6665 cites a maximum power history effect of 0.00200 L1keff, but gives no guidance as to whether the effect should be considered a bias or uncertainty. The source of the recommendation of 0.00200 L1keff is ORNLlTM-12973 (Reference 3).
According to Section 3.4 of ORNLfTM-12973:
    "However, the maximum nonconservatism is less than 0.2%. Thus for simplicity, it is probably best to assume a no-downtime exposure history for cases with both actinides and fission products present, and then include a 0.2% uncertainty in keff" Also, it is important to note that the power history effect is not constant but varies with burnup and does not need to be applied to fresh fuel.
If the power history effect is treated as an uncertainty and is root-sum-squared with the other uncertainties, the maximum increase in total bias and uncertainty would be less than 0.00025 L1keff. For simplicity and conservatism, however, the power history effect will be treated as a constant bias of 0.00200 L1keff applied to burnt fuel in Regions 2 and
: 3. This bias will be converted into equivalent burnup using the relationship discussed in the response to RAI 30. For Region 1, the burnup limits are too low to be affected and no penalty for power history is needed because the power history effect is due to reduced power near the end of assembly depletion as noted in the RAI and increases with increasing burnup.
Regarding soluble boron, all simulated depletions were performed using 1000 ppm boron. Table 1 gives the cycle average boron concentration for Cycles 1-12 and the expected average for Cycle 13, which is currently operating at an uprated power of 3650 Mega Watts thermal (MWt).
Table 1- C;yc Ie Avera~ e B oron C oncen t ra f10 ns Average Boron in parts Cycle        per million (ppm) 1                624 2                  785 3                  737 4                  929 5                  912 6                1094 7                930 8                812 9                865 10                883 11                905 12                918 13                902
Serial No. 10-072 Docket No. 50-423 Response to RAI for the MPS3 Spent Fuel Pool LAR Attachment 1, Page 3 of 11 For fuel that will be depleted in uprated power cycles, recent cycles are indicative of current and projected fuel management and cycle average boron concentrations. The maximum cycle average boron concentration for the last 5 completed operating cycles is 918 ppm. Cycle 13 is currently operating at the uprated power (3650 MWt) and is designed to have a cycle average boron concentration of 902 ppm. For future cycles, cycle average boron is expected to remain 50 to 100 ppm below the assumed 1000 ppm.
Millstone Power Station Unit 3 (MPS3) fuel cycles, except for Cycle 6, have had cycle average boron concentrations below 930 ppm. Cycle 6 is an outlier because it was designed as a transition cycle to move from 18 month cycles to 24 month cycles. That transition was not pursued. In addition, Cycle 6 experienced a three year mid-cycle outage and was shut down prior to reaching the design end of cycle. The cycle average boron concentration for Cycle 6 was 1094 ppm. However, all fuel in Cycle 6 was depleted in at least one other cycle and all other cycles had lower cycle average boron concentrations. The highest two cycle average boron concentration for MPS3 cycles is 1008 ppm (lifetime weighted average of Cycles 6 and 7). NUREG/CR-6665 indicates that this amount of excess depletion boron (8 ppm) is worth less than 30 pcm for spent fuel pool (SFP) criticality.
There are several sources of margin to accommodate the 8 ppm of excess boron concentration for Cycle 6-7 fuel, including as-built fuel density and the pre-uprate as-operated moderator temperature. The core average moderator exit temperature for Cycle 6-7 fuel is more than 8 OF lower than the value assumed for uprated core conditions with minimum flow. NUREG/CR-6665 indicates that this amount of moderator temperature difference (-4 OK) amounts to at least 140 pcm margin for depletion history.
The moderator temperature effect alone provides more than sufficient margin to offset the effect of the 8 ppm excess cycle average boron for the Cycle 6-7 fuel. Considering these factors, the assumption of 1000 ppm for simulated depletion of the fuel for the calculation of burnup credit requirements is sufficient for application in past MPS3 cycles and is conservative for application in projected future cycles.
Serial No. 10-072 Docket No. 50-423 Response to RAI for the MPS3 Spent Fuel Pool LAR Attachment 1, Page 4 of 11 Question 27 In RAI #21 the licensee performed new criticality analysis using site specific burnup profiles.
: a. In RAI #21 the licensee determined penalties for burnups where the original analysis in WCAP-16721 was shown to be non-conservative.
Those penalties were determined using a depletion code and criticality code different than that used in WCAP-16721. Since the development and utilization of the penalties constitutes more than just a comparison study, either provide a code validation or justify not performing a criticality code validation for the new code.
: b. In Table 21-6 there is a Burnup Worth column that is used to determine the penalty. Explain the basis and origin for that column.
: c. In RAI #21 the licensee indicates the depletion parameters used were the same as for WCAP-16721. Provide a list of the fuel assembly and depletion parameters used for each case in RAI #21.
: d. As part of the response to RAI # 21 the licensee states, "Since the limiting Top-1/3 assembly comparison covers only existing No Blanket fuel from completed MPS3 cycles, credit has been taken for as-built fuel density, dish and chamfer fractions, Pre-Uprate (3411 Mwt) core power, and as operated cycle soluble boron concentration." In earlier RAI responses the licensee took credit for having modeled these parameters conservatively.
: i. Since the No Blanket fuel modeling no longer has those conservatisms explain how the earlier RAI responses are affected.
ii. Since these parameters had been modeled conservatively in the original analysis there were no biases or uncertainties included for these parameters. Since the No Blanket fuel modeling no longer has those conservatisms explain how the biases and uncertainties*
are affected.
: e. In its RAI #21 response, the licensee states the title to technical specification (TS) Figure 3.9-4 will be changed. That change was not provided as part of the revised TS markup. Please revise the marked-up TS page to indicate that change.


1.Attachment 1: Response to Request for Additional Information (RAI)Questions 26, 27 and 29 Regarding the Spent Fuel Pool Criticality License Amendment Request cc: U.S.Nuclear Regulatory Commission Region I Regional Administrator 475 Allendale Road King of Prussia, PA 19406-1415 Ms.C.J.Sanders Project Manager U.S.Nuclear Regulatory Commission One White Flint North 11555 Rockville Pike Mail Stop 08-B3 Rockville, MD 20852-2738 NRC Senior Resident Inspector Millstone Power Station Director Bureau of Air Management Monitoring and Radiation Division Department of Environmental Protection 79 Elm Street Hartford, CT 06106-5127 Serial No.10-072 Docket No.50-423 ATTACHMENT 1 RESPONSE TO RAI QUESTIONS 26, 27 AND 29 REGARDING THE SPENT FUEL POOL CRITICALITY LICENSE AMENDMENT REQUEST DOMINION NUCLEAR CONNECTICUT, INC.MILLSTONE POWER STATION UNIT 3 Serial No.10-072 Docket No.50-423 Response to RAI for the MPS3 Spent Fuel Pool LAR Attachment 1.Page 1 of 11 RESPONSE TO RAI QUESTIONS 26 THROUGH 30 REGARDING THE SPENT FUEL POOL CRITICALITY LICENSE AMENDMENT REQUEST Question 26 In response to RAI#5 ONC states: NUREG/CR-6665.
Serial No. 10-072 Docket No. 50-423 Response to RAI for the MPS3 Spent Fuel Pool LAR Attachment 1, Page 5 of 11 Response, Part 27a:
Reference 4, identifies both specific power and operating history effects as weakly correlated to increased reactivity for discharged fuel assemblies.
The analysis reported in WCAP-16721-P uses the PHOENIX-P lattice code to generate depleted isotopic number densities and SCALE Version 4.4 for three-dimensional Monte Carlo calculations to determine neutron multiplication factors (Keff) in the SFP environment. SCALE Version 4.4 uses the BONAMI and NITAWL modules for cross section processing and the KENO V.a module for transport calculations. Reference 1 allows the use of NITAWL-KENO V.a and PHOENIX-P for SFP criticality safety calculations.
The maximum impact noted in Reference 4 is approximately 0.00200 11 Keff.This result is caused by reduced power operation near the end of assembly depletion.
The depletion calculations supporting the analysis presented in WCAP-16721-P do not include part power operation.
Instead, the soluble boron concentration is maintained at a constant value above the cycle average value for the entire depletion.
The spectral hardening from the presence of boron, especially at the end of the cycle when the concentration is several hundred ppm above physical values, provides additional margin to account for this potential impact.The use of additional margin is the approach suggested in Reference 4 for accounting for the potential for operating history effects.In order to determine if the conservatism gained from taking credit for using a higher than actual soluble boron concentration during the simulated depletion of the fuel in the reactor is enough to cover the 0.00200 11 Keff.the NRC staff needs to know how much more than the actual boron concentration was used.Please provide additional information regarding how much soluble boron concentration was used during the simulated depletion of the fuel in the reactor compared to the actual.Response: With regard to specific power and operating history effects, NUREG/CR-6665, Reference 4, makes the following recommendation: "It appears that the optimum approach would be to assume a simple power operating history, and add in a margin to account for induced effects." Consistent with this recommendation, the depletions performed for WCAP-16721-P (including those for request for additional information (RAI)responses through RAI 30)used a constant power throughout the entire burnup range.The power modeled is consistent with uprated core conditions.
Serial No.10-072 Docket No.50-423 Response to RAI for the MPS3 Spent Fuel Pool LAR Attachment 1, Page 2 of 11 NUREG/CR-6665 cites a maximum power history effect of 0.00200 L1k eff , but gives no guidance as to whether the effect should be considered a bias or uncertainty.
The source of the recommendation of 0.00200 L1k e ff is ORNLlTM-12973 (Reference 3).According to Section 3.4 of ORNLfTM-12973: "However, the maximum non conservatism is less than 0.2%.Thus for simplicity, it is probably best to assume a no-downtime exposure history for cases with both actinides and fission products present, and then include a 0.2%uncertainty in k" eff Also, it is important to note that the power history effect is not constant but varies with burnup and does not need to be applied to fresh fuel.If the power history effect is treated as an uncertainty and is root-sum-squared with the otheruncertainties,the maximum increase in total bias and uncertainty would be less than 0.00025 L1k e ff.For simplicity and conservatism, however, the power history effect will be treated as a constant bias of 0.00200 L1k e ff applied to burnt fuel in Regions 2 and 3.This bias will be converted into equivalent burnup using the relationship discussed in the response to RAI 30.For Region 1, the burnup limits are too low to be affected and no penalty for power history is needed because the power history effect is due to reduced power near the end of assembly depletion as noted in the RAI and increases with increasing burn up.Regarding soluble boron, all simulated depletions were performed using 1000 ppm boron.Table 1 gives the cycle average boron concentration for Cycles 1-12 and the expected average for Cycle 13, which is currently operating at an uprated power of 3650 Mega Watts thermal (MWt).t f ns C B;yc e e oron oncen ra 10 Average Boron in parts Cycle per million (ppm)1 624 2 785 3 737 4 929 5 912 6 1094 7 930 8 812 9 865 10 883 11 905 12 918 13 902 Table 1-CIA Serial No.10-072 Docket No.50-423 Response to RAI for the MPS3 Spent Fuel Pool LAR Attachment 1, Page 3 of 11 For fuel that will be depleted in uprated power cycles, recent cycles are indicative of current and projected fuel management and cycle average boron concentrations.
The maximum cycle average boron concentration for the last 5 completed operating cycles is 918 ppm.Cycle 13 is currently operating at the uprated power (3650 MWt)and is designed to have a cycle average boron concentration of 902 ppm.For future cycles, cycle average boron is expected to remain 50 to 100 ppm below the assumed 1000 ppm.Millstone Power Station Unit 3 (MPS3)fuel cycles, except for Cycle 6, have had cycle average boron concentrations below 930 ppm.Cycle 6 is an outlier because it was designed as a transition cycle to move from 18 month cycles to 24 month cycles.That transition wasnotpursued.
In addition, Cycle 6 experienced a three year mid-cycle outage and was shut down prior to reaching the design end of cycle.The cycle average boron concentration for Cycle 6 was 1094 ppm.However, all fuel in Cycle 6 was depleted in at least one other cycle and all other cycles had lower cycle average boron concentrations.
The highest two cycle average boron concentration for MPS3 cycles is 1008 ppm (lifetime weighted average of Cycles 6 and 7).NUREG/CR-6665 indicates that this amount of excess depletion boron (8 ppm)is worth less than 30 pcm for spent fuel pool (SFP)criticality.
There are several sources of margin to accommodate the 8 ppm of excess boron concentration for Cycle 6-7 fuel, including as-built fuel density and the pre-uprateoperated moderator temperature.
The core average moderator exit temperature for Cycle 6-7 fuel is more than 8 OF lower than the value assumed for uprated core conditions with minimum flow.NUREG/CR-6665 indicates that this amount of moderator temperature difference
(-4 OK)amounts to at least 140 pcm margin for depletion history.The moderator temperature effect alone provides more than sufficient margin to offset the effect of the 8 ppm excess cycle average boron for the Cycle 6-7 fuel.Considering these factors, the assumption of 1000 ppm for simulated depletion of the fuel for the calculation of burnup credit requirements is sufficient for application in past MPS3 cycles and is conservative for application in projected future cycles.
Serial No.10-072 Docket No.50-423 Response to RAI for the MPS3 Spent Fuel Pool LAR Attachment 1, Page 4 of 11 Question 27 In RAI#21 the licensee performed new criticality analysis using site specific burnup profiles.a.In RAI#21 the licensee determined penalties for burnups where the original analysis in WCAP-16721 was shown to be non-conservative.
Those penalties were determined using a depletion code and criticality code different than that used in WCAP-16721.
Since the development and utilization of the penalties constitutes more than just a comparison study, either provide a code validation or justify not performing a criticality code validation for the new code.b.In Table 21-6 there is a Burnup Worth column that is used to determine the penalty.Explain the basis and origin for that column.c.In RAI#21 the licensee indicates the depletion parameters used were the same as for WCAP-16721.
Provide a list of the fuel assembly and depletion parameters used for each case in RAI#21.d.As part of the response to RAI#21 the licensee states,"Since the limitingTop-1/3assembly comparison covers only existing No Blanket fuel from completed MPS3 cycles, credit has been taken for as-built fuel density, dish and chamfer fractions, Pre-Uprate (3411 Mwt)core power, and as operated cycle soluble boron concentration." In earlier RAI responses the licensee took credit for having modeled these parameters conservatively.
i.Since the No Blanket fuel modeling no longer has those conservatisms explain how the earlier RAI responses are affected.ii.Since these parameters had been modeled conservatively in the original analysis there were no biases or uncertainties included for these parameters.
Since the No Blanket fuel modeling no longer has those conservatisms explain how the biases and uncertainties*
are affected.e.In its RAI#21 response, the licensee states the title to technical specification (TS)Figure 3.9-4 will be changed.That change was not provided as part of the revised TS markup.Please revise the marked-up TS page to indicate that change.
Serial No.10-072 Docket No.50-423 Response to RAI for the MPS3 Spent Fuel Pool LAR Attachment 1, Page 5 of 11 Response, Part 27a: The analysis reported in WCAP-16721-P uses the PHOENIX-P lattice code to generate depleted isotopic number densities and SCALE Version 4.4 for three-dimensional Monte Carlo calculations to determine neutron multiplication factors (Keff)in the SFP environment.
SCALE Version 4.4 uses the BONAMI and NITAWL modules for cross section processing and the KENO V.a module for transport calculations.
Reference 1 allows the use of NITAWL-KENO V.a and PHOENIX-P for SFP criticality safety calculations.
RAI 21 presents results from differential calculations performed using the PARAGON lattice code to generate depleted isotopic number densities and SCALE Version 5.1 for three-dimensional Monte Carlo K-eff calculations in the spent fuel environment.
RAI 21 presents results from differential calculations performed using the PARAGON lattice code to generate depleted isotopic number densities and SCALE Version 5.1 for three-dimensional Monte Carlo K-eff calculations in the spent fuel environment.
PARAGON was approved for use in reactor physics calculations by the Nuclear Regulatory Commission (NRC)in Reference 2, which evaluated a large body of PARAGON benchmarking data.PARAGON is intended for use as a stand alone code or as a replacement for PHOENIX-P.
PARAGON was approved for use in reactor physics calculations by the Nuclear Regulatory Commission (NRC) in Reference 2, which evaluated a large body of PARAGON benchmarking data. PARAGON is intended for use as a stand alone code or as a replacement for PHOENIX-P. Reference 2 states that PARAGON is "well qualified as a stand-alone code replacement for the PHOENIX-P lattice code, wherever the PHOENIX-P code is used in NRC-approved methodologies" and that "The PARAGON code can be used as a replacement for the PHOENIX-P lattice code". It is therefore concluded that PARAGON is an acceptable code for the generation of depleted isotopic number densities.
Reference 2 states that PARAGON is"well qualified as a stand-alone code replacement for the PHOENIX-P lattice code, wherever the PHOENIX-P code is used in NRC-approved methodologies" and that"The PARAGON code can be used as a replacement for the PHOENIX-P lattice code".It is therefore concluded that PARAGON is an acceptable code for the generation of depleted isotopic number densities.
In order to address the concern about use of SCALE Version 5.1, penalty calculations that account for the effect of different axial nodalization and burnup profiles (RAI 21),
In order to address the concern about use ofSCALEVersion 5.1, penalty calculations that account for the effect of different axial nodalization and burnup profiles (RAI 21), the effect of Integral Fuel Boron Absorber (IFBA)(RAI 28), and the effect of higher assembly moderator exit temperature (RAI 30)will be performed using PARAGON and SCALE Version 4.4.The combined effect of higher assembly moderator temperature, axial nodalization, and conservative burnup profiles will be presented as part of the RAI 30 response.In this way, use of SCALE 5.1 has been limited to comparison studies and will not be used for any of the calculations used to determine TS burnup and enrichment requirements.
the effect of Integral Fuel Boron Absorber (IFBA) (RAI 28), and the effect of higher assembly moderator exit temperature (RAI 30) will be performed using PARAGON and SCALE Version 4.4. The combined effect of higher assembly moderator temperature, axial nodalization, and conservative burnup profiles will be presented as part of the RAI 30 response. In this way, use of SCALE 5.1 has been limited to comparison studies and will not be used for any of the calculations used to determine TS burnup and enrichment requirements.
Response, Part 27b: The burnup worth of a reactivity penalty was calculated by assuming a linear reactivity change over an interval of burnup near the point of potential non-conservatism.
Response, Part 27b:
The difference in twoSCALEVersion 4.4 keff values was divided by the associated burnup difference to determine the reactivity worth associated with an increase in assembly average burnup.New reactivity and burnup penalties are being determined as part of the response to RAI 30, which will be submitted by separate correspondence.
The burnup worth of a reactivity penalty was calculated by assuming a linear reactivity change over an interval of burnup near the point of potential non-conservatism. The difference in two SCALE Version 4.4 keff values was divided by the associated burnup difference to determine the reactivity worth associated with an increase in assembly average burnup. New reactivity and burnup penalties are being determined as part of the response to RAI 30, which will be submitted by separate correspondence. The determination of the burnup worth will be described in detail as part of that response.
The determination of the burnup worth will be described in detail as part of that response.
 
Serial No.10-072 Docket No.50-423 Response to RAI for the MPS3 Spent Fuel Pool LAR Attachment 1, Page 6 of 11 Response, Part 27c: Table 5 summarizes the fuel assembly and depletion parameters used in the original WCAP-16721-P analysis and in response to RAI 21 for fuel with natural andenriched blankets.No blanket fuel was treated differently as discussed in response to RAI 21 but is no longer relevant as discussed in response to Part 27d.t bl PdF IA T bl5DI fae-eple Ion an ue ssem Iy arame ers RAI 21, natural and mid-Parameter WCAP-16721-P enriched blankets Profile 5 from DOE Topical Axial Burnup Distribution Report MPS3 specific Number of axial zones modeled 4 24 Tin 556.4 OF 556.4 OF Tout 628 OF 628 OF Soluble Boron present during depletion constant 1000 ppm constant 1000 ppm Core Power 3650 MWt 3650 MWt Theoretical Density of fuel 97.5%97.5%solid, right cylinder (Le.no solid, right cylinder (Le.no Fuel pellet shape dishing or chamfering) dishing or chamfering)
Serial No. 10-072 Docket No. 50-423 Response to RAI for the MPS3 Spent Fuel Pool LAR Attachment 1, Page 6 of 11 Response, Part 27c:
Design Basis Fuel Assembly Westinghouse 17x17 STD Westinghouse 17x17 STD 3.0, 4.0, and 5.0 weight Fuel initial enrichments percent (wt%)3.0, 4.0, and 5.0 wt%Blankets modeled?No Yes Response, Part 27d: This question concerns the use of actual fuel parameters (fuel density, power level, boron concentration, etc.)for existing fuel instead of using bounding fuel parameters in Dominion Nuclear Connecticut's (ONC)response to RA121.RAI 21 was concerned about fuel reactivity effects due to axial burnup and isotopic conditions at the axial ends of the fuel assembly.The use of actual fuel parameters in ONC's response to RAI 21 was only for those existing fuel assemblies which have no axial blankets, and only for storage in Region 2.ONC did not credit actual fuel parameters in the RAI 21 response for fuel with natural blankets or mid-enriched blankets.MPS3 fuel with no axial blankets is confined to fuel batches A, B, C and 0, which were all operated at the pre-up rate power level of 3411 MWt.Fuel after batches A thru 0 have axial fuel blankets with an enrichment of 2.6 wt%(nominal)U235 or less.To eliminate the need to take credit for actual fuel parameters for these batches, ONC will Serial No.10-072 Docket No.50-423 Response to RAI for the MPS3 Spent Fuel Pool LAR Attachment 1, Page 7 of 11 add a footnote to proposed TS Figure 3.9-3 for Region 2, which will preclUde storage of fuel batches A, 8, C and 0 in Region 2.The basis for storage of no blanket fuel in the MP3 SFP is summarized as follows: 1)New no blanket fuel in Stretch Power Uprate (SPU)cycles a.In the response to RAI 21, ONC proposed adding a footnote to revised TS Figure 3.9-3 (all Region 2 fuel)and Figure 3.9-5 (Region 3 uprate fuel)requiring a maximum nominal blanket enrichment of 2.6 wt%U235 and a minimum nominal blanket length of 6 inches for fuel operated at uprate conditions.
Table 5 summarizes the fuel assembly and depletion parameters used in the original WCAP-16721-P analysis and in response to RAI 21 for fuel with natural and mid-enriched blankets. No blanket fuel was treated differently as discussed in response to RAI 21 but is no longer relevant as discussed in response to Part 27d.
No blanket fuel depleted at SPU conditions will be precluded from storage in Regions 2 and 3 by this footnote.This effectively precludes use of new no blanket fuel.b.The Region 1 maximum burnup requirement is 8000 megawatt day per metric ton uranium (MWd/MTU)at 5 wt%U235.At or below this low burnup value, axial reactivity effects are not significant and a flat axial power shape is bounding, so the type of blanket is not important.
Ta bl e 5 - Deple  I f Ion an d F ue IAssem blIy Parame ters RAI 21, natural and mid-Parameter                       WCAP-16721-P                 enriched blankets Profile 5 from DOE Topical Axial Burnup Distribution                     Report                   MPS3 specific Number of axial zones modeled                       4                             24 Tin                             556.4 OF                     556.4 OF Tout                               628 OF                       628 OF Soluble Boron present during depletion                     constant 1000 ppm             constant 1000 ppm Core Power                           3650 MWt                     3650 MWt Theoretical Density of fuel                     97.5%                         97.5%
Since a flat axial burnup profile was one of the considered shapes in16721, and the flat axial shape is bounding at these burnup values, axial reactivity effects have been appropriately considered, at both theuprate and uprated power levels for storage in Region 1 of"no blanket" fuel.2)Existing no blanket fuel from pre-SPU cycles a.Region 1 storage of existing no blanket fuel is acceptable for the reasons given for new no blanket fuel.In addition, the maximum fuel enrichment of batch A-O fuel is 3.8 w/o U235.Per TS Figure 3.9-1 (Region 1), this 3.8 wt%U235 enrichment requires less than 1000 MWd/MTU of fuel burnup for storage in Region 1 of the spent fuel pool in a 4-out-of-4 configuration, which is too Iowa burnup for axial effects to be significant.
solid, right cylinder (Le. no solid, right cylinder (Le. no Fuel pellet shape               dishing or chamfering)         dishing or chamfering)
In addition, the minimum burnup on any of the batch A-O fuel assemblies is more than 17,000 MWd/MTU (including 4%reduction for measured burnup uncertainty).
Design Basis Fuel Assembly           Westinghouse 17x17 STD       Westinghouse 17x17 STD 3.0, 4.0, and 5.0 weight Fuel initial enrichments                 percent (wt%)             3.0, 4.0, and 5.0 wt%
Further, ONC has not proposed any changes to TS Figure 3.9-1, which is the current basis for storage of this fuel.ONC has submitted, as part ofWCAP-16721, an analysis for Region 1 that shows the required fuel enrichments and fuel burnup limits for fuel at the SPU power level are bounded by TS Figure 3.9-1.b.ONC will add a footnote to proposed TS Figure 3.9-3 for Region 2, which will preclude storage of fuel batches A, 8, C and 0 from being stored in Region 2.
Blankets modeled?                             No                           Yes Response, Part 27d:
Serial No.10-072 Docket No.50-423 Response to RAI for the MPS3 Spent Fuel Pool LAR Attachment 1, Page 8 of 11 c.For Region 3 of the spent fuel pool, TS Figure 3.9-4 provides the required enrichment and fuel burnup to allow storage of fuel in Region 3 foruprate fuel.The current design basis, including TS Figure 3.9-4, is not altered or affected by the WCAP-16721 analysis provided in this Technical Specification change, and the only change to TS Figure 3.9-4 (as proposed in the original TS change for this amendment) is to change the title of the figure to reflect it is valid only for fuel assemblies fromuprate (3411 Mwt)cores.MPS3 no blanketfuel currently in the SFP from pre-uprate (3411 MWt)cores continues to be able to be stored in Region 3 per this TS figure.This figure was previously approved by the NRC, and was retained in the Technical Specifications to allow fuel from pre-uprate (3411 Mwt)cores to be stored in Region 3, provided the fuel meets the requirements of the TS figure.Response, Part 27e: This question concerns whether there are additional changes to TS Figure 3.9-4 that have not yet been provided.TS Figure 3.9-4 was proposed to be changed in the original submittal (Dominion Letter Serial Number 07-0450)by adding to the title of the figure to reflect it is valid only for fuel assemblies from pre-uprate (3411 MWt)cores.The proposed TS Figure 3.9-4 was not changed byanysubsequent RAI response.The DNC response to RAI question 21 was referring to the title change previously proposed for TS Figure 3.9-4 in the original submittal.  
This question concerns the use of actual fuel parameters (fuel density, power level, boron concentration, etc.) for existing fuel instead of using bounding fuel parameters in Dominion Nuclear Connecticut's (ONC) response to RA121. RAI 21 was concerned about fuel reactivity effects due to axial burnup and isotopic conditions at the axial ends of the fuel assembly. The use of actual fuel parameters in ONC's response to RAI 21 was only for those existing fuel assemblies which have no axial blankets, and only for storage in Region 2. ONC did not credit actual fuel parameters in the RAI 21 response for fuel with natural blankets or mid-enriched blankets.
*.Serial No.10-072 Docket No.50-423 Response to RAI for the MPS3 Spent Fuel Pool LAR Attachment 1, Page 9 of 11 Question 29 In DNC's response to RAI#5 DNC states their fuel management does not use fixed burnable absorbers.
MPS3 fuel with no axial blankets is confined to fuel batches A, B, C and 0, which were all operated at the pre-uprate power level of 3411 MWt. Fuel after batches A thru 0 have axial fuel blankets with an enrichment of 2.6 wt% (nominal) U235 or less. To eliminate the need to take credit for actual fuel parameters for these batches, ONC will
a.Has MPS3 ever used any other flux suppression devices such as hafnium inserts to reduce the neutron dose to reactor vessel welds?b.If so, how do they affect the reactivity of the discharged fuel assemblies?
 
Response: No flux suppression devices have been used at MPS3.MPS3 fuel designs do not currently use fixed neutron absorbers, nor are any planned.From Cycle 3 thru the present (Cycle 13), only Integral Fuel Burnable Absorber (IFBA)has been used as a neutron absorber.MPS3 did use some fixed neutron absorbers in Cycles 1 and 2 at the pre-uprate power level of 3411 MWt.The fixed absorbers were Pyrex glass rods, which were used in selected fuel assemblies in fuel batches B, C and D in Cycles 1 and 2.An explanation is provided next as to why these fuel assemblies in batches B, C and D which contained Pyrex rods in Cycles 1 and 2 may be stored in the MPS3 SFP under the proposed TS amendment.
Serial No. 10-072 Docket No. 50-423 Response to RAI for the MPS3 Spent Fuel Pool LAR Attachment 1, Page 7 of 11 add a footnote to proposed TS Figure 3.9-3 for Region 2, which will preclUde storage of fuel batches A, 8, C and 0 in Region 2.
*Region 1 Fuel Storage: Storage of fuel in Region 1 is restricted to the fuel enrichment and fuel burnup limits of TS Figure 3.9-1.DNC has not proposed any changes to TS Figure 3.9-1.DNC has submitted, as part ofWCAP-16721, an analysis for Region 1 that shows therequiredfuel enrichments and fuel burnup limits for fuel at the SPU power level are bounded by TS Figure 3.9-1.Since TS Figure 3.9-1 limits bound SPU operation, no changes were proposed for TS Figure 3.9-1.TS Figure 3.9-1 does not require any fuel burnup for storage of fuel in the 4-out-of-4 configuration for enrichments below 3.7 wt%U235.Batch Band C fuel and most of the batch D fuel are below an enrichmentof 3.7 wt%U-235 and therefore require no fuel burnup to be stored in Region 1 in a 4-out-of-4 configuration.
The basis for storage of no blanket fuel in the MP3 SFP is summarized as follows:
Therefore, there is no need to consider the fuel history effects of fixed neutron absorber on fuel reactivity for this fuel with a required fuel burnup of 0 MWd/MTU.A small number of batch D fuel assemblies have a maximum fuel enrichment of 3.8 wt%U235, which per TS Figure 3.9-1 requires less than 1000 MWd/MTU of fuel burnup to allow storage in Region 1 in a 4-out-of-4 configuration.
: 1) New no blanket fuel in Stretch Power Uprate (SPU) cycles
All of the batch D fuel assemblies with a fuel enrichment greater than 3.7 wt%U235 have at least a fuel burnup of 38000 MWd/MTU, including a 4%reduction for burnup uncertainity.
: a. In the response to RAI 21, ONC proposed adding a footnote to revised TS Figure 3.9-3 (all Region 2 fuel) and Figure 3.9-5 (Region 3 uprate fuel) requiring a maximum nominal blanket enrichment of 2.6 wt% U235 and a minimum nominal blanket length of 6 inches for fuel operated at uprate conditions. No blanket fuel depleted at SPU conditions will be precluded from storage in Regions 2 and 3 by this footnote. This effectively precludes use of new no blanket fuel.
The fuel history effects of a fixed neutron absorber on fuel reactivity at 1000 MWd/MTU of fuel burnup is very small, and negligible when considering the 38000 MWd/MTU actual minimum fuel burnup.In summary, the storage of batch B, C and D fuel assemblies Serial No.10-072 Docket No.50-423 Response to RAI for the MPS3 Spent Fuel Pool LAR Attachment 1, Page 10 of 11 that contained fixed neutron absorbers in Cycles 1 and 2 are acceptable for4 storage in Region 1 per TS Figure 3.9-1.*Region 2 Fuel Storage: As described in the response to RAI question 27(d), ONC has modified proposed TS Figure 3.9-3 to preclude the storage of fuel batches A, B, C and 0 in Region 2 of the SFP.The proposed TS Figure 3.9-3 covers bothuprate fuel and post-up rate (SPU)fuel.Since batch B, C and 0 (which contained Pyrex rods)are not allowed to be stored in Region 2, this eliminates any question of fixed neutron absorber history effects for fuel batches B, C and 0 on assembly reactivity for Region 2 fuel storage.*Region 3 Fuel Storage: TS Figure 3.9-4 specifies the enrichment and fuel burnup limits for storage of fuel in Region 3 for pre-uprate fuel.Proposed TS Figure 3.9-5 specifies the enrichment and fuel burnup limits for storage of fuel in Region 3 for SPU uprate fuel.ONC has proposed changing the title of TS Figure to make it clear it applies only to pre-uprate fuel.The analysis that supports application of TS Figure 3.9-4 for pre-uprate fuel was previously approved by the NRC.Fuel batches B, C and 0 which contained fixed neutron absorbers in Cycles 1 and 2 are acceptable for fuel storage in Region 3 per TS Figure 3.9-4, consistent with the existing NRC approved analysis for Region 3.The entire set of proposed TS changes, including proposed TS Figures 3.9-3 and 3.9-5 which are being modified as a result of the presently submitted responses to RAIRAI 30, will be included as part of the separate responses to be submitted with RAI 28 and RA130.
: b. The Region 1 maximum burnup requirement is 8000 megawatt day per metric ton uranium (MWd/MTU) at 5 wt% U235. At or below this low burnup value, axial reactivity effects are not significant and a flat axial power shape is bounding, so the type of blanket is not important. Since a flat axial burnup profile was one of the considered shapes in WCAP-16721, and the flat axial shape is bounding at these burnup values, axial reactivity effects have been appropriately considered, at both the pre-uprate and uprated power levels for storage in Region 1 of "no blanket" fuel.
Serial No.10-072 Docket No.50-423 Response to RAI for the MPS3 Spent Fuel Pool LAR Attactlment 1, Page 11 of 11  
: 2) Existing no blanket fuel from pre-SPU cycles
: a. Region 1 storage of existing no blanket fuel is acceptable for the reasons given for new no blanket fuel. In addition, the maximum fuel enrichment of batch A-O fuel is 3.8 w/o U235. Per TS Figure 3.9-1 (Region 1), this 3.8 wt% U235 enrichment requires less than 1000 MWd/MTU of fuel burnup for storage in Region 1 of the spent fuel pool in a 4-out-of-4 configuration, which is too Iowa burnup for axial effects to be significant. In addition, the minimum burnup on any of the batch A-O fuel assemblies is more than 17,000 MWd/MTU (including 4% reduction for measured burnup uncertainty). Further, ONC has not proposed any changes to TS Figure 3.9-1, which is the current basis for storage of this fuel. ONC has submitted, as part ofWCAP-16721, an analysis for Region 1 that shows the required fuel enrichments and fuel burnup limits for fuel at the SPU power level are bounded by TS Figure 3.9-1.
: b. ONC will add a footnote to proposed TS Figure 3.9-3 for Region 2, which will preclude storage of fuel batches A, 8, C and 0 from being stored in Region 2.
 
Serial No. 10-072 Docket No. 50-423 Response to RAI for the MPS3 Spent Fuel Pool LAR Attachment 1, Page 8 of 11
: c. For Region 3 of the spent fuel pool, TS Figure 3.9-4 provides the required enrichment and fuel burnup to allow storage of fuel in Region 3 for pre-uprate fuel. The current design basis, including TS Figure 3.9-4, is not altered or affected by the WCAP-16721 analysis provided in this Technical Specification change, and the only change to TS Figure 3.9-4 (as proposed in the original TS change for this amendment) is to change the title of the figure to reflect it is valid only for fuel assemblies from pre-uprate (3411 Mwt) cores. MPS3 no blanketfuel currently in the SFP from pre-uprate (3411 MWt) cores continues to be able to be stored in Region 3 per this TS figure. This figure was previously approved by the NRC, and was retained in the Technical Specifications to allow fuel from pre-uprate (3411 Mwt) cores to be stored in Region 3, provided the fuel meets the requirements of the TS figure.
Response, Part 27e:
This question concerns whether there are additional changes to TS Figure 3.9-4 that have not yet been provided. TS Figure 3.9-4 was proposed to be changed in the original submittal (Dominion Letter Serial Number 07-0450) by adding to the title of the figure to reflect it is valid only for fuel assemblies from pre-uprate (3411 MWt) cores.
The proposed TS Figure 3.9-4 was not changed by any subsequent RAI response. The DNC response to RAI question 21 was referring to the title change previously proposed for TS Figure 3.9-4 in the original submittal.
 
Serial No. 10-072 Docket No. 50-423 Response to RAI for the MPS3 Spent Fuel Pool LAR Attachment 1, Page 9 of 11 Question 29 In DNC's response to RAI #5 DNC states their fuel management does not use fixed burnable absorbers.
: a. Has MPS3 ever used any other flux suppression devices such as hafnium inserts to reduce the neutron dose to reactor vessel welds?
: b. If so, how do they affect the reactivity of the discharged fuel assemblies?
 
===Response===
No flux suppression devices have been used at MPS3. MPS3 fuel designs do not currently use fixed neutron absorbers, nor are any planned. From Cycle 3 thru the present (Cycle 13), only Integral Fuel Burnable Absorber (IFBA) has been used as a neutron absorber.
MPS3 did use some fixed neutron absorbers in Cycles 1 and 2 at the pre-uprate power level of 3411 MWt. The fixed absorbers were Pyrex glass rods, which were used in selected fuel assemblies in fuel batches B, C and D in Cycles 1 and 2. An explanation is provided next as to why these fuel assemblies in batches B, C and D which contained Pyrex rods in Cycles 1 and 2 may be stored in the MPS3 SFP under the proposed TS amendment.
* Region 1 Fuel Storage: Storage of fuel in Region 1 is restricted to the fuel enrichment and fuel burnup limits of TS Figure 3.9-1. DNC has not proposed any changes to TS Figure 3.9-1. DNC has submitted, as part ofWCAP-16721, an analysis for Region 1 that shows the required fuel enrichments and fuel burnup limits for fuel at the SPU power level are bounded by TS Figure 3.9-1. Since TS Figure 3.9-1 limits bound SPU operation, no changes were proposed for TS Figure 3.9-1.
TS Figure 3.9-1 does not require any fuel burnup for storage of fuel in the 4-out-of-4 configuration for enrichments below 3.7 wt% U235. Batch Band C fuel and most of the batch D fuel are below an enrichmentof 3.7 wt% U-235 and therefore require no fuel burnup to be stored in Region 1 in a 4-out-of-4 configuration. Therefore, there is no need to consider the fuel history effects of fixed neutron absorber on fuel reactivity for this fuel with a required fuel burnup of 0 MWd/MTU. A small number of batch D fuel assemblies have a maximum fuel enrichment of 3.8 wt% U235, which per TS Figure 3.9-1 requires less than 1000 MWd/MTU of fuel burnup to allow storage in Region 1 in a 4-out-of-4 configuration. All of the batch D fuel assemblies with a fuel enrichment greater than 3.7 wt% U235 have at least a fuel burnup of 38000 MWd/MTU, including a 4% reduction for burnup uncertainity. The fuel history effects of a fixed neutron absorber on fuel reactivity at 1000 MWd/MTU of fuel burnup is very small, and negligible when considering the 38000 MWd/MTU actual minimum fuel burnup. In summary, the storage of batch B, C and D fuel assemblies
 
Serial No. 10-072 Docket No. 50-423 Response to RAI for the MPS3 Spent Fuel Pool LAR Attachment 1, Page 10 of 11 that contained fixed neutron absorbers in Cycles 1 and 2 are acceptable for 4-out-of-4 storage in Region 1 per TS Figure 3.9-1.
* Region 2 Fuel Storage: As described in the response to RAI question 27(d), ONC has modified proposed TS Figure 3.9-3 to preclude the storage of fuel batches A, B, C and 0 in Region 2 of the SFP. The proposed TS Figure 3.9-3 covers both pre-uprate fuel and post-uprate (SPU) fuel. Since batch B, C and 0 (which contained Pyrex rods) are not allowed to be stored in Region 2, this eliminates any question of fixed neutron absorber history effects for fuel batches B, C and 0 on assembly reactivity for Region 2 fuel storage.
* Region 3 Fuel Storage: TS Figure 3.9-4 specifies the enrichment and fuel burnup limits for storage of fuel in Region 3 for pre-uprate fuel. Proposed TS Figure 3.9-5 specifies the enrichment and fuel burnup limits for storage of fuel in Region 3 for SPU uprate fuel. ONC has proposed changing the title of TS Figure 3~9-4 to make it clear it applies only to pre-uprate fuel. The analysis that supports application of TS Figure 3.9-4 for pre-uprate fuel was previously approved by the NRC. Fuel batches B, C and 0 which contained fixed neutron absorbers in Cycles 1 and 2 are acceptable for fuel storage in Region 3 per TS Figure 3.9-4, consistent with the existing NRC approved analysis for Region 3.
The entire set of proposed TS changes, including proposed TS Figures 3.9-3 and 3.9-5 which are being modified as a result of the presently submitted responses to RAI 26-RAI 30, will be included as part of the separate responses to be submitted with RAI 28 and RA130.
 
Serial No. 10-072 Docket No. 50-423 Response to RAI for the MPS3 Spent Fuel Pool LAR Attactlment 1, Page 11 of 11


==References:==
==References:==
 
: 1. Laurence Kopp (USNRC), "Guidance on the Regulatory Requirements for Criticality Analysis of Fuel Storage at Light-Water Reactor Power Plants," August 19, 1998.
1.Laurence Kopp (USNRC),"Guidance on the Regulatory Requirements for Criticality Analysis of Fuel Storage at Light-Water Reactor Power Plants," August 19, 1998.2.Letter from H.N.Berkow (NRC)to J.A.Gresham (Westinghouse),"Final Safety Evaluation for the Westinghouse Topical Report WCAP-16045-P, Revision 0,'Qualification of the Two-Dimensional Transport Code PARAGON'(TAC No.MB8040)," March 18,2004, ADAMS Accession Number: ML040780402.
: 2. Letter from H. N. Berkow (NRC) to J.A. Gresham (Westinghouse), "Final Safety Evaluation for the Westinghouse Topical Report WCAP-16045-P, Revision 0,
3.M.D.DeHart,"Sensitivity and Parametric Evaluations of Significant Aspects of Burnup Credit for PWR Spent Fuel Packages", ORNLrrM-12973, May 1996 4.C.V.Parks et.a!.,"Review and Prioritization of Technical Issues Related to Burnup Credit for LWR Fuel," NUREG/CR-6665, February, 2000.}}
  'Qualification of the Two-Dimensional Transport Code PARAGON' (TAC No.
MB8040)," March 18,2004, ADAMS Accession Number: ML040780402.
: 3. M. D. DeHart, "Sensitivity and Parametric Evaluations of Significant Aspects of Burnup Credit for PWR Spent Fuel Packages", ORNLrrM-12973, May 1996
: 4. C. V. Parks et.a!., "Review and Prioritization of Technical Issues Related to Burnup Credit for LWR Fuel," NUREG/CR-6665, February, 2000.}}

Latest revision as of 19:42, 21 March 2020

Response to Request for Additional Information Questions 26, 27 & 29 Re Spent Fuel Pool Criticality License Amendment Request
ML100610104
Person / Time
Site: Millstone Dominion icon.png
Issue date: 03/01/2010
From: Hartz L
Dominion Nuclear Connecticut
To:
Document Control Desk, Office of Nuclear Reactor Regulation
References
10-072, FOIA/PA-2011-0115
Download: ML100610104 (15)


Text

Dominion Nuclear Connecticut, Inc.

5000 Dominion Boulevard, Glen Allen, Virginia 23060 Web Address: www.dom.com March 1, 2010 U. S. Nuclear Regulatory Commission Serial No.: 10-072 Attention: Document Control Desk NLOSIWDC RO Washington, DC 20555 Docket No.: 50-423 License No.: NPF-49 DOMINION NUCLEAR CONNECTICUT, INC.

MILLSTONE POWER STATION UNIT 3 RESPONSE TO REQUEST FOR ADDITIONAL INFORMATION QUESTIONS 26, 27 AND 29 REGARDING A SPENT FUEL POOL CRITICALITY LICENSE AMENDMENT REQUEST Dominion Nuclear Connecticut, Inc. (DNC) submitted a stretch power uprate (SPU) license amendment request (LAR) for Millstone Power Station Unit 3 (MPS3) in letters dated July 13, 2007 (Serial Nos. 07-0450 and 07-0450A). The SPU license amendment request was supplemented in a letter dated December 13, 2007 (Serial No. 07-0450C). The SPU LAR included a revised spent fuel pool (SFP) criticality analysis with proposed changes in technical specification (TS) requirements. DNC separated the MPS3 SFP TS change request from the MPS3 SPU request via letter dated March 5, 2008 (Serial No. 07-0450D).

In a letter dated August 8, 2008, the Nuclear Regulatory Commission (NRC) transmitted a request for additional information (RAI) regarding the SFP TS. DNC responded to RAI questions 1 through 19 in a letter dated September 30, 2008 (Serial No. 08-0511A). Additionally, in a letter dated February 2, 2009, the NRC requested additional information. DNC responded to RAI questions 20, 22, 23, and 25 in a letter dated March 5, 2009 (Serial No.09-084) and to RAI questions 21 and 24 in a letter dated March 23, 2009 (Serial No. 09-084A). Subsequently, in a letter dated January 26,2010, the NRC requested additional information.

Attachment 1 of this letter provides responses to RAI questions 26, 27 and 29.

Responses to RAI questions 28 and 30 will follow in a separate letter.

The information provided by this letter does not affect the conclusions of the significant hazards consideration discussion in the December 13, 2007 DNC letter (Serial No. 07-0450C).

Serial No.10-072 Docket No. 50-423 Response to RAI for the MPS3 Spent Fuel Pool Criticality LAR Page 2 of 3 Should you have any questions in regard to this submittal, please contact Wanda Craft at 804-273-4687.

Sincerely, ciYJ,L/{j Leslie N. Hartz Vice President - Nuclear Support Services Commitments made in this letter:

1. None.

COMMONWEALTH OF VIRGINIA )

)

COUNTY OF HENRICO )

The foregoing document was acknowledged before me, in and for the County and Commonwealth aforesaid, today by Leslie N. Hartz, who is Vice President - Nuclear Support Services of Dominion Nuclear Connecticut, Inc. She has affirmed before me that she is duly authorized to execute and file the foregoing document in behalf of that Company, and that the statements in the document are true to the best of her knowledge and belief.

Acknowledged before me this /51 day of /VJ ttYCM..J ,2010.

My Commission Expires: 4/CO IJ3 GINGER l. AlliGOOD Ld~ ~H C!M:tts Notary Public Notary Public Commonwealth Of Virglni, 310847 My COmmission Expires Apr 30.2013

Serial No.10-072 Docket No. 50-423 Response to RAI for the MPS3 Spent Fuel Pool Criticality LAR Page 3 of 3

Attachment:

1. Attachment 1: Response to Request for Additional Information (RAI)

Questions 26, 27 and 29 Regarding the Spent Fuel Pool Criticality License Amendment Request cc: U.S. Nuclear Regulatory Commission Region I Regional Administrator 475 Allendale Road King of Prussia, PA 19406-1415 Ms. C. J. Sanders Project Manager U.S. Nuclear Regulatory Commission One White Flint North 11555 Rockville Pike Mail Stop 08-B3 Rockville, MD 20852-2738 NRC Senior Resident Inspector Millstone Power Station Director Bureau of Air Management Monitoring and Radiation Division Department of Environmental Protection 79 Elm Street Hartford, CT 06106-5127

Serial No.10-072 Docket No. 50-423 ATTACHMENT 1 RESPONSE TO RAI QUESTIONS 26, 27 AND 29 REGARDING THE SPENT FUEL POOL CRITICALITY LICENSE AMENDMENT REQUEST DOMINION NUCLEAR CONNECTICUT, INC.

MILLSTONE POWER STATION UNIT 3

Serial No.10-072 Docket No. 50-423 Response to RAI for the MPS3 Spent Fuel Pool LAR Attachment 1. Page 1 of 11 RESPONSE TO RAI QUESTIONS 26 THROUGH 30 REGARDING THE SPENT FUEL POOL CRITICALITY LICENSE AMENDMENT REQUEST Question 26 In response to RAI # 5 ONC states:

NUREG/CR-6665. Reference 4, identifies both specific power and operating history effects as weakly correlated to increased reactivity for discharged fuel assemblies. The maximum impact noted in Reference 4 is approximately 0.00200 11 Keff. This result is caused by reduced power operation near the end of assembly depletion. The depletion calculations supporting the analysis presented in WCAP-16721-P do not include part power operation. Instead, the soluble boron concentration is maintained at a constant value above the cycle average value for the entire depletion.

The spectral hardening from the presence of boron, especially at the end of the cycle when the concentration is several hundred ppm above physical values, provides additional margin to account for this potential impact. The use of additional margin is the approach suggested in Reference 4 for accounting for the potential for operating history effects.

In order to determine if the conservatism gained from taking credit for using a higher than actual soluble boron concentration during the simulated depletion of the fuel in the reactor is enough to cover the 0.00200 11 Keff. the NRC staff needs to know how much more than the actual boron concentration was used. Please provide additional information regarding how much soluble boron concentration was used during the simulated depletion of the fuel in the reactor compared to the actual.

Response

With regard to specific power and operating history effects, NUREG/CR-6665, Reference 4, makes the following recommendation:

"It appears that the optimum approach would be to assume a simple continuous-power operating history, and add in a margin to account for operating-history-induced effects."

Consistent with this recommendation, the depletions performed for WCAP-16721-P (including those for request for additional information (RAI) responses through RAI 30) used a constant power throughout the entire burnup range. The power modeled is consistent with uprated core conditions.

Serial No.10-072 Docket No. 50-423 Response to RAI for the MPS3 Spent Fuel Pool LAR Attachment 1, Page 2 of 11 NUREG/CR-6665 cites a maximum power history effect of 0.00200 L1keff, but gives no guidance as to whether the effect should be considered a bias or uncertainty. The source of the recommendation of 0.00200 L1keff is ORNLlTM-12973 (Reference 3).

According to Section 3.4 of ORNLfTM-12973:

"However, the maximum nonconservatism is less than 0.2%. Thus for simplicity, it is probably best to assume a no-downtime exposure history for cases with both actinides and fission products present, and then include a 0.2% uncertainty in keff" Also, it is important to note that the power history effect is not constant but varies with burnup and does not need to be applied to fresh fuel.

If the power history effect is treated as an uncertainty and is root-sum-squared with the other uncertainties, the maximum increase in total bias and uncertainty would be less than 0.00025 L1keff. For simplicity and conservatism, however, the power history effect will be treated as a constant bias of 0.00200 L1keff applied to burnt fuel in Regions 2 and

3. This bias will be converted into equivalent burnup using the relationship discussed in the response to RAI 30. For Region 1, the burnup limits are too low to be affected and no penalty for power history is needed because the power history effect is due to reduced power near the end of assembly depletion as noted in the RAI and increases with increasing burnup.

Regarding soluble boron, all simulated depletions were performed using 1000 ppm boron. Table 1 gives the cycle average boron concentration for Cycles 1-12 and the expected average for Cycle 13, which is currently operating at an uprated power of 3650 Mega Watts thermal (MWt).

Table 1- C;yc Ie Avera~ e B oron C oncen t ra f10 ns Average Boron in parts Cycle per million (ppm) 1 624 2 785 3 737 4 929 5 912 6 1094 7 930 8 812 9 865 10 883 11 905 12 918 13 902

Serial No.10-072 Docket No. 50-423 Response to RAI for the MPS3 Spent Fuel Pool LAR Attachment 1, Page 3 of 11 For fuel that will be depleted in uprated power cycles, recent cycles are indicative of current and projected fuel management and cycle average boron concentrations. The maximum cycle average boron concentration for the last 5 completed operating cycles is 918 ppm. Cycle 13 is currently operating at the uprated power (3650 MWt) and is designed to have a cycle average boron concentration of 902 ppm. For future cycles, cycle average boron is expected to remain 50 to 100 ppm below the assumed 1000 ppm.

Millstone Power Station Unit 3 (MPS3) fuel cycles, except for Cycle 6, have had cycle average boron concentrations below 930 ppm. Cycle 6 is an outlier because it was designed as a transition cycle to move from 18 month cycles to 24 month cycles. That transition was not pursued. In addition, Cycle 6 experienced a three year mid-cycle outage and was shut down prior to reaching the design end of cycle. The cycle average boron concentration for Cycle 6 was 1094 ppm. However, all fuel in Cycle 6 was depleted in at least one other cycle and all other cycles had lower cycle average boron concentrations. The highest two cycle average boron concentration for MPS3 cycles is 1008 ppm (lifetime weighted average of Cycles 6 and 7). NUREG/CR-6665 indicates that this amount of excess depletion boron (8 ppm) is worth less than 30 pcm for spent fuel pool (SFP) criticality.

There are several sources of margin to accommodate the 8 ppm of excess boron concentration for Cycle 6-7 fuel, including as-built fuel density and the pre-uprate as-operated moderator temperature. The core average moderator exit temperature for Cycle 6-7 fuel is more than 8 OF lower than the value assumed for uprated core conditions with minimum flow. NUREG/CR-6665 indicates that this amount of moderator temperature difference (-4 OK) amounts to at least 140 pcm margin for depletion history.

The moderator temperature effect alone provides more than sufficient margin to offset the effect of the 8 ppm excess cycle average boron for the Cycle 6-7 fuel. Considering these factors, the assumption of 1000 ppm for simulated depletion of the fuel for the calculation of burnup credit requirements is sufficient for application in past MPS3 cycles and is conservative for application in projected future cycles.

Serial No.10-072 Docket No. 50-423 Response to RAI for the MPS3 Spent Fuel Pool LAR Attachment 1, Page 4 of 11 Question 27 In RAI #21 the licensee performed new criticality analysis using site specific burnup profiles.

a. In RAI #21 the licensee determined penalties for burnups where the original analysis in WCAP-16721 was shown to be non-conservative.

Those penalties were determined using a depletion code and criticality code different than that used in WCAP-16721. Since the development and utilization of the penalties constitutes more than just a comparison study, either provide a code validation or justify not performing a criticality code validation for the new code.

b. In Table 21-6 there is a Burnup Worth column that is used to determine the penalty. Explain the basis and origin for that column.
c. In RAI #21 the licensee indicates the depletion parameters used were the same as for WCAP-16721. Provide a list of the fuel assembly and depletion parameters used for each case in RAI #21.
d. As part of the response to RAI # 21 the licensee states, "Since the limiting Top-1/3 assembly comparison covers only existing No Blanket fuel from completed MPS3 cycles, credit has been taken for as-built fuel density, dish and chamfer fractions, Pre-Uprate (3411 Mwt) core power, and as operated cycle soluble boron concentration." In earlier RAI responses the licensee took credit for having modeled these parameters conservatively.
i. Since the No Blanket fuel modeling no longer has those conservatisms explain how the earlier RAI responses are affected.

ii. Since these parameters had been modeled conservatively in the original analysis there were no biases or uncertainties included for these parameters. Since the No Blanket fuel modeling no longer has those conservatisms explain how the biases and uncertainties*

are affected.

e. In its RAI #21 response, the licensee states the title to technical specification (TS) Figure 3.9-4 will be changed. That change was not provided as part of the revised TS markup. Please revise the marked-up TS page to indicate that change.

Serial No.10-072 Docket No. 50-423 Response to RAI for the MPS3 Spent Fuel Pool LAR Attachment 1, Page 5 of 11 Response, Part 27a:

The analysis reported in WCAP-16721-P uses the PHOENIX-P lattice code to generate depleted isotopic number densities and SCALE Version 4.4 for three-dimensional Monte Carlo calculations to determine neutron multiplication factors (Keff) in the SFP environment. SCALE Version 4.4 uses the BONAMI and NITAWL modules for cross section processing and the KENO V.a module for transport calculations. Reference 1 allows the use of NITAWL-KENO V.a and PHOENIX-P for SFP criticality safety calculations.

RAI 21 presents results from differential calculations performed using the PARAGON lattice code to generate depleted isotopic number densities and SCALE Version 5.1 for three-dimensional Monte Carlo K-eff calculations in the spent fuel environment.

PARAGON was approved for use in reactor physics calculations by the Nuclear Regulatory Commission (NRC) in Reference 2, which evaluated a large body of PARAGON benchmarking data. PARAGON is intended for use as a stand alone code or as a replacement for PHOENIX-P. Reference 2 states that PARAGON is "well qualified as a stand-alone code replacement for the PHOENIX-P lattice code, wherever the PHOENIX-P code is used in NRC-approved methodologies" and that "The PARAGON code can be used as a replacement for the PHOENIX-P lattice code". It is therefore concluded that PARAGON is an acceptable code for the generation of depleted isotopic number densities.

In order to address the concern about use of SCALE Version 5.1, penalty calculations that account for the effect of different axial nodalization and burnup profiles (RAI 21),

the effect of Integral Fuel Boron Absorber (IFBA) (RAI 28), and the effect of higher assembly moderator exit temperature (RAI 30) will be performed using PARAGON and SCALE Version 4.4. The combined effect of higher assembly moderator temperature, axial nodalization, and conservative burnup profiles will be presented as part of the RAI 30 response. In this way, use of SCALE 5.1 has been limited to comparison studies and will not be used for any of the calculations used to determine TS burnup and enrichment requirements.

Response, Part 27b:

The burnup worth of a reactivity penalty was calculated by assuming a linear reactivity change over an interval of burnup near the point of potential non-conservatism. The difference in two SCALE Version 4.4 keff values was divided by the associated burnup difference to determine the reactivity worth associated with an increase in assembly average burnup. New reactivity and burnup penalties are being determined as part of the response to RAI 30, which will be submitted by separate correspondence. The determination of the burnup worth will be described in detail as part of that response.

Serial No.10-072 Docket No. 50-423 Response to RAI for the MPS3 Spent Fuel Pool LAR Attachment 1, Page 6 of 11 Response, Part 27c:

Table 5 summarizes the fuel assembly and depletion parameters used in the original WCAP-16721-P analysis and in response to RAI 21 for fuel with natural and mid-enriched blankets. No blanket fuel was treated differently as discussed in response to RAI 21 but is no longer relevant as discussed in response to Part 27d.

Ta bl e 5 - Deple I f Ion an d F ue IAssem blIy Parame ters RAI 21, natural and mid-Parameter WCAP-16721-P enriched blankets Profile 5 from DOE Topical Axial Burnup Distribution Report MPS3 specific Number of axial zones modeled 4 24 Tin 556.4 OF 556.4 OF Tout 628 OF 628 OF Soluble Boron present during depletion constant 1000 ppm constant 1000 ppm Core Power 3650 MWt 3650 MWt Theoretical Density of fuel 97.5% 97.5%

solid, right cylinder (Le. no solid, right cylinder (Le. no Fuel pellet shape dishing or chamfering) dishing or chamfering)

Design Basis Fuel Assembly Westinghouse 17x17 STD Westinghouse 17x17 STD 3.0, 4.0, and 5.0 weight Fuel initial enrichments percent (wt%) 3.0, 4.0, and 5.0 wt%

Blankets modeled? No Yes Response, Part 27d:

This question concerns the use of actual fuel parameters (fuel density, power level, boron concentration, etc.) for existing fuel instead of using bounding fuel parameters in Dominion Nuclear Connecticut's (ONC) response to RA121. RAI 21 was concerned about fuel reactivity effects due to axial burnup and isotopic conditions at the axial ends of the fuel assembly. The use of actual fuel parameters in ONC's response to RAI 21 was only for those existing fuel assemblies which have no axial blankets, and only for storage in Region 2. ONC did not credit actual fuel parameters in the RAI 21 response for fuel with natural blankets or mid-enriched blankets.

MPS3 fuel with no axial blankets is confined to fuel batches A, B, C and 0, which were all operated at the pre-uprate power level of 3411 MWt. Fuel after batches A thru 0 have axial fuel blankets with an enrichment of 2.6 wt% (nominal) U235 or less. To eliminate the need to take credit for actual fuel parameters for these batches, ONC will

Serial No.10-072 Docket No. 50-423 Response to RAI for the MPS3 Spent Fuel Pool LAR Attachment 1, Page 7 of 11 add a footnote to proposed TS Figure 3.9-3 for Region 2, which will preclUde storage of fuel batches A, 8, C and 0 in Region 2.

The basis for storage of no blanket fuel in the MP3 SFP is summarized as follows:

1) New no blanket fuel in Stretch Power Uprate (SPU) cycles
a. In the response to RAI 21, ONC proposed adding a footnote to revised TS Figure 3.9-3 (all Region 2 fuel) and Figure 3.9-5 (Region 3 uprate fuel) requiring a maximum nominal blanket enrichment of 2.6 wt% U235 and a minimum nominal blanket length of 6 inches for fuel operated at uprate conditions. No blanket fuel depleted at SPU conditions will be precluded from storage in Regions 2 and 3 by this footnote. This effectively precludes use of new no blanket fuel.
b. The Region 1 maximum burnup requirement is 8000 megawatt day per metric ton uranium (MWd/MTU) at 5 wt% U235. At or below this low burnup value, axial reactivity effects are not significant and a flat axial power shape is bounding, so the type of blanket is not important. Since a flat axial burnup profile was one of the considered shapes in WCAP-16721, and the flat axial shape is bounding at these burnup values, axial reactivity effects have been appropriately considered, at both the pre-uprate and uprated power levels for storage in Region 1 of "no blanket" fuel.
2) Existing no blanket fuel from pre-SPU cycles
a. Region 1 storage of existing no blanket fuel is acceptable for the reasons given for new no blanket fuel. In addition, the maximum fuel enrichment of batch A-O fuel is 3.8 w/o U235. Per TS Figure 3.9-1 (Region 1), this 3.8 wt% U235 enrichment requires less than 1000 MWd/MTU of fuel burnup for storage in Region 1 of the spent fuel pool in a 4-out-of-4 configuration, which is too Iowa burnup for axial effects to be significant. In addition, the minimum burnup on any of the batch A-O fuel assemblies is more than 17,000 MWd/MTU (including 4% reduction for measured burnup uncertainty). Further, ONC has not proposed any changes to TS Figure 3.9-1, which is the current basis for storage of this fuel. ONC has submitted, as part ofWCAP-16721, an analysis for Region 1 that shows the required fuel enrichments and fuel burnup limits for fuel at the SPU power level are bounded by TS Figure 3.9-1.
b. ONC will add a footnote to proposed TS Figure 3.9-3 for Region 2, which will preclude storage of fuel batches A, 8, C and 0 from being stored in Region 2.

Serial No.10-072 Docket No. 50-423 Response to RAI for the MPS3 Spent Fuel Pool LAR Attachment 1, Page 8 of 11

c. For Region 3 of the spent fuel pool, TS Figure 3.9-4 provides the required enrichment and fuel burnup to allow storage of fuel in Region 3 for pre-uprate fuel. The current design basis, including TS Figure 3.9-4, is not altered or affected by the WCAP-16721 analysis provided in this Technical Specification change, and the only change to TS Figure 3.9-4 (as proposed in the original TS change for this amendment) is to change the title of the figure to reflect it is valid only for fuel assemblies from pre-uprate (3411 Mwt) cores. MPS3 no blanketfuel currently in the SFP from pre-uprate (3411 MWt) cores continues to be able to be stored in Region 3 per this TS figure. This figure was previously approved by the NRC, and was retained in the Technical Specifications to allow fuel from pre-uprate (3411 Mwt) cores to be stored in Region 3, provided the fuel meets the requirements of the TS figure.

Response, Part 27e:

This question concerns whether there are additional changes to TS Figure 3.9-4 that have not yet been provided. TS Figure 3.9-4 was proposed to be changed in the original submittal (Dominion Letter Serial Number 07-0450) by adding to the title of the figure to reflect it is valid only for fuel assemblies from pre-uprate (3411 MWt) cores.

The proposed TS Figure 3.9-4 was not changed by any subsequent RAI response. The DNC response to RAI question 21 was referring to the title change previously proposed for TS Figure 3.9-4 in the original submittal.

Serial No.10-072 Docket No. 50-423 Response to RAI for the MPS3 Spent Fuel Pool LAR Attachment 1, Page 9 of 11 Question 29 In DNC's response to RAI #5 DNC states their fuel management does not use fixed burnable absorbers.

a. Has MPS3 ever used any other flux suppression devices such as hafnium inserts to reduce the neutron dose to reactor vessel welds?
b. If so, how do they affect the reactivity of the discharged fuel assemblies?

Response

No flux suppression devices have been used at MPS3. MPS3 fuel designs do not currently use fixed neutron absorbers, nor are any planned. From Cycle 3 thru the present (Cycle 13), only Integral Fuel Burnable Absorber (IFBA) has been used as a neutron absorber.

MPS3 did use some fixed neutron absorbers in Cycles 1 and 2 at the pre-uprate power level of 3411 MWt. The fixed absorbers were Pyrex glass rods, which were used in selected fuel assemblies in fuel batches B, C and D in Cycles 1 and 2. An explanation is provided next as to why these fuel assemblies in batches B, C and D which contained Pyrex rods in Cycles 1 and 2 may be stored in the MPS3 SFP under the proposed TS amendment.

  • Region 1 Fuel Storage: Storage of fuel in Region 1 is restricted to the fuel enrichment and fuel burnup limits of TS Figure 3.9-1. DNC has not proposed any changes to TS Figure 3.9-1. DNC has submitted, as part ofWCAP-16721, an analysis for Region 1 that shows the required fuel enrichments and fuel burnup limits for fuel at the SPU power level are bounded by TS Figure 3.9-1. Since TS Figure 3.9-1 limits bound SPU operation, no changes were proposed for TS Figure 3.9-1.

TS Figure 3.9-1 does not require any fuel burnup for storage of fuel in the 4-out-of-4 configuration for enrichments below 3.7 wt% U235. Batch Band C fuel and most of the batch D fuel are below an enrichmentof 3.7 wt% U-235 and therefore require no fuel burnup to be stored in Region 1 in a 4-out-of-4 configuration. Therefore, there is no need to consider the fuel history effects of fixed neutron absorber on fuel reactivity for this fuel with a required fuel burnup of 0 MWd/MTU. A small number of batch D fuel assemblies have a maximum fuel enrichment of 3.8 wt% U235, which per TS Figure 3.9-1 requires less than 1000 MWd/MTU of fuel burnup to allow storage in Region 1 in a 4-out-of-4 configuration. All of the batch D fuel assemblies with a fuel enrichment greater than 3.7 wt% U235 have at least a fuel burnup of 38000 MWd/MTU, including a 4% reduction for burnup uncertainity. The fuel history effects of a fixed neutron absorber on fuel reactivity at 1000 MWd/MTU of fuel burnup is very small, and negligible when considering the 38000 MWd/MTU actual minimum fuel burnup. In summary, the storage of batch B, C and D fuel assemblies

Serial No.10-072 Docket No. 50-423 Response to RAI for the MPS3 Spent Fuel Pool LAR Attachment 1, Page 10 of 11 that contained fixed neutron absorbers in Cycles 1 and 2 are acceptable for 4-out-of-4 storage in Region 1 per TS Figure 3.9-1.

  • Region 2 Fuel Storage: As described in the response to RAI question 27(d), ONC has modified proposed TS Figure 3.9-3 to preclude the storage of fuel batches A, B, C and 0 in Region 2 of the SFP. The proposed TS Figure 3.9-3 covers both pre-uprate fuel and post-uprate (SPU) fuel. Since batch B, C and 0 (which contained Pyrex rods) are not allowed to be stored in Region 2, this eliminates any question of fixed neutron absorber history effects for fuel batches B, C and 0 on assembly reactivity for Region 2 fuel storage.
  • Region 3 Fuel Storage: TS Figure 3.9-4 specifies the enrichment and fuel burnup limits for storage of fuel in Region 3 for pre-uprate fuel. Proposed TS Figure 3.9-5 specifies the enrichment and fuel burnup limits for storage of fuel in Region 3 for SPU uprate fuel. ONC has proposed changing the title of TS Figure 3~9-4 to make it clear it applies only to pre-uprate fuel. The analysis that supports application of TS Figure 3.9-4 for pre-uprate fuel was previously approved by the NRC. Fuel batches B, C and 0 which contained fixed neutron absorbers in Cycles 1 and 2 are acceptable for fuel storage in Region 3 per TS Figure 3.9-4, consistent with the existing NRC approved analysis for Region 3.

The entire set of proposed TS changes, including proposed TS Figures 3.9-3 and 3.9-5 which are being modified as a result of the presently submitted responses to RAI 26-RAI 30, will be included as part of the separate responses to be submitted with RAI 28 and RA130.

Serial No.10-072 Docket No. 50-423 Response to RAI for the MPS3 Spent Fuel Pool LAR Attactlment 1, Page 11 of 11

References:

1. Laurence Kopp (USNRC), "Guidance on the Regulatory Requirements for Criticality Analysis of Fuel Storage at Light-Water Reactor Power Plants," August 19, 1998.
2. Letter from H. N. Berkow (NRC) to J.A. Gresham (Westinghouse), "Final Safety Evaluation for the Westinghouse Topical Report WCAP-16045-P, Revision 0,

'Qualification of the Two-Dimensional Transport Code PARAGON' (TAC No.

MB8040)," March 18,2004, ADAMS Accession Number: ML040780402.

3. M. D. DeHart, "Sensitivity and Parametric Evaluations of Significant Aspects of Burnup Credit for PWR Spent Fuel Packages", ORNLrrM-12973, May 1996
4. C. V. Parks et.a!., "Review and Prioritization of Technical Issues Related to Burnup Credit for LWR Fuel," NUREG/CR-6665, February, 2000.