ML18319A094
ML18319A094 | |
Person / Time | |
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Site: | Fermi |
Issue date: | 10/15/2018 |
From: | DTE Electric Company |
To: | Document Control Desk, Office of Nuclear Reactor Regulation |
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Download: ML18319A094 (33) | |
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DETROIT EDISON - FERMI 2 AUTOMATED RECORD MANAGEMENT DISTRIBUTION CONTROL LIST 10/16/1.8 .
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Ref: u20061
- Fermi 2 Technical Requirements Manual Volume I DTE Electric
- DTC: TMTRM Date 10/15/2018 I File: 1754 ARMS - INFORMATION DSN: TRM VOL I Recipient C7/
I Rev: 117 rJ.....'-J
LICENSING DOCUMENT TRANSMITTAL FERMI 2 TECHNICAL REQUIREMENTS MANUAL -VOL I
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Destroy the removed pages. Be sure that Revision 116 has been inserted prior to inserting these pages.
SECTION REMOVE and DESTROY INSERT In Front of TRM Manual Title Page Rev 116 10/12/2018 Title Page Rev 117 10/15/2018 Immediately following List of Effective Pages List of Effective Pages Title Page LEP-1 throughLEP-4Rev 116 LEP-1 throughLEP-4Rev 117 10/15/2018 10/12/2018 Core Operating Limits Cycle 19, Revision 0 Cycle 20, Revision 0 Report 24 pages 26 pages END
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FERMI 2 - TECHNICAL REQUIREMENTS MANUAL VOL I LIST OF EFFECTIVE PAGES
- CORE OPERATING LIMITS REPORT COLR 20, Revision 0 Page Revision Notation Page 1 0 2 0 3 0 4 0 5 0 6 0 7 0 8 0 9 0 10 0 11 0 12 0 13 0 14 0 15 0 16 0 17 0 18 0 19 0 20 0
,21 0 22 0 23 0 24 0 25 0 26 0
- TRM Vol. I LEP-4 REV 117 10/15/2018
COLR - 20 Revision 0 Page 1 of26
- FERMI2 CORE OPERATING LIMITS REPORT CYCLE 20 REVISIONO Prepared by:
t:1kt?/)q Paul R. Kiel * ~
Principal Technical Expert, Reactor Engineering Reviewed by: 4/ze,/,g Date 7 ngineer, Reactor Engineering
, Approved by: , .. a., .. ,r Michael A. Lake Date Supervisor, Reactor Engineering
- October 2018
- TABLE OF CONTENTS COLR - 20 Revision 0 Page 2 of26 J 1.0 IN"TRODUCTION AND SU1\1MARY ..................................................................................... 4 2.0 AVERAGE PLANAR LINEAR HEAT GENERATION RATE ............................................. 5 2.1 Definition .......................... ~ ................................................................._..................... 5 2.2 Determination of MAPLHGR Limit ........................................................................ 5 2.2.1 Calculation ofMAPFAC(P) ....................................................................... ,7 2.2.2 Calculation of MAPPAC(F) ........................................................................ 9 3.0 MINIMUM CRITICAL POWER RATI0 .............................................................................. 10 3 .1 Definition ............................................................................................................... 10 3 .2 Determination of Operating Limit MCPR ............................................................. 10 3.3 Calculation ofMCPR(P) .......................................................... :............................. 12 3.3.1 Calculation of Kp ....................................................................................... 12 3.3.2 Calculation of'C"..................................... :.................................................... 14.
3.4 Calculation ofMCPR(F) ........................................................................................ 15 4.0 LINEAR HEAT GENERATION RATE ................................................................................ 16 4.1 Definition ............................................................................................................... 16 4.2 Determination of LHGR Limit .............................................................................. 16 4.2.1 Calculation of LHGRFAC(P) ......... ,.......................................................... 18 4.2.2 Calculation of LHGRFAC(F) .................................................................... 20 5.0 CONTROL ROD BLOCK IN"STRUMENTATION .............................................................. 21 5.1 Definition ......................................................................... ."..................................... 21 6.0 BACKUP STABILITY PROTECTION REGIONS .............................................................. 22 6.1 Definition ........................................ :...................................................................... 22
7.0 REFERENCES
................................................ , ...................................................................... 25
- LIST OF TABLES COLR - 20 Revision 0 Page 3 of26 TABLE 1 FUEL TYPE-DEPENDENT STANDARD MAPLHGR LIMITS ............................. 6 TABLE 2 FLOW-DEPENDENT MAPLHGR LIMIT COEFFICIENTS ................................... 9 TABLE 3 OLMCPR10011os AS A FUNCTION OF EXPOSURE AND 'C .................................. 11 TABLE 4 FLOW-DEPENDENT MCPR LIMIT COEFFICIENTS ......................................... 15 TABLE 5 STANDARD LHGRLIMITS FOR VARIOUS FUEL TYPES ............................... 17 TABLE 6 FLOW-DEPENDENT LHGR LIMIT COEFFICIENTS ........................................... 20 TABLE 7 CONTROL ROD BLOCK INSTRUMENTATION SETPOINTS WITH FILTER .................................................................................................................... 21
- LIST OF FIGURES FIGURE 1 BSP REGIONS FOR NOMINAL FEEDWATER TEMPERATURE ............. 23 FIGURE 2 ESP.REGIONS FOR REDUCED FEEDWATER TEMPERATURE ............. 24
1.0 INTRODUCTION
AND
SUMMARY
- COLR - 20 Revision 0 P~ge 4 of26 This report provides the cycle specific plant operating limits, which are listed below, for Fermi 2, Cycle 20, as required by Technical Specification 5.6.5. The analytical methods used to determine these core operating limits are those previously reviewed and approved by the Nuclear Regulatory Commission in GESTAR II (Reference 7).
The cycle specific limits contained within this report are valid for the full range of the licensed operating domain.
OPERATING LIMIT TECHNICAL SPECIFICATION APLHGR 3.2.l
- MCPR LHGR RBM 3.2.2 3.2.3 3.3.2.l BSPREGIONS 3.3.1.1 APLHGR = AVERAGE PLANAR LINEAR HEAT GENERATION RATE MCPR MINIMUM CRITICAL POWER RATIO LHGR = LINEARHEATGENERATIO NRATE RBM = ROD BLOCK MONITOR BSP = BACKUP STABILITY PROTECTION
- 2.0 AVERAGE PLANAR LINEAR HEAT GENERATION RATE COLR - 20 Revision 0 Page 5 of26 2.1 Definition __/
TECH SPEC IDENT OPERATING LIMIT 3.2.1 APLHGR The AVERAGE PLANAR LINEAR HEAT GENERATION RATE (APLHGR) shall be applicable to a specific planar height and is equal to the sum of the LINEAR HEAT GENERATION RATEs (LHGRs) for all the fuel rods in the specified bundle at the specified height divided by the number of fuel rods in the fuel bundle at the height.
2.2 Determination of MAPLHGR Limit The maximum APLHGR (MAPLHGR) limit is a function of reactor power, core flow, fuel type, and average planar exposure. The limit is developed, using NRC approved methodology described in References 7 and 8, to ensure gross cladding failure will not occur following a loss of coolant accident (LOCA). The MAPLHGR limit ensures that the peak clad temperature during a LOCA will not exceed the limits as specified in I0CFR50.46(b)(1) and that the fuel design analysis criteria defined in References 7 and 8 will be met.
- The MAPLHGR limit during dual loop operation is calculated by the following equation:
. MAPLHGR== J\1IN (}!APLHGR (P), MAPLHGR (F))
where:
MAPLHGR (P) = MAPFAC (P) xMAPLHGRsm MAPLHGR (F) = MAPFAC (F) xMAPLHGRsm Within four hours after entering single loop operation, the MAPLHGR limit is calculated by the following equation:
MAPLHGRuMrr= J\1IN (MAPLHGR (P), MAPLHGR (F))
where:
MAPLHGR (P) = MAPFAC (P) x MAPLHGRsm MAPLHGR (F) = MAPFAC (F) xMAPLHGRsro MAPFAC (P) and MAPFAC (F) are limited to 0.80.
The Single Loop multiplier limit is 0.80 (Reference 2) based on assuring a Loss of Coolant Accident (LOCA) while in single loop will be bounded by the two loop LOCA (Reference 12).
J
- COLR - 20 Revision 0 Page 6 of26 MAPLHGRsro, the standard MAPLHGR limit, is defined at a power of 3486 MWth and flow of 105 Mlbs/hr for each fuel type as a function of average planar exposure and is presented in Table
- 1. (Reference 2) When hand calculations are required, MAPLHGRsro shall be determined by interpolation from Table 1. MAPFAC(P), the core power-dependent MAPLHGR limit adjustment factor, shall be calculated by using Section 2.2.1. MAPFAC(F), the core flow-dependent MAPLHGR limit adjustment factor, shall be calculated by using Section 2.2.2.
TABLEl FUEL TYPE-DEPENDENT STANDARD MAPLHGR LIM]TS GE14 Exposure GE14 MAPLHGR GWD/ST kW/ft 0.0 12.82 19.13 12.82 57.61 8.00 63.50 5.00
- 2=
3=
4=
5=
Fuel Types GE14-PIOCNAB381-4G6.0/11G5.0-100T-150-T6-4372 GE14-PlOCNAB381-4G6.0/9G5.0-lOOT-150-T6-4371 GE14-P10CNAB381-15G5.0-100T-150-T6-4373 GE14-PlOCNAB381-6G6.0/9G5.0-lOOT-150-T6-4374 6= GE14-PIOCNAB385-13GZ-100T-150-T6-4571 7= GE14-PlOCNAB384-15GZ-100T-150-T6-4572 8 = GE14-PI0CNAB383-13GZ-100T-150-T6-4573 9 = GE14-PIOCNAB377-15GZ-100T-150-T6-4574 14 = GE14-P10CNAB376-4G6.0/9G5.0/2G2.0-100T-150-T6-4061 15 = GE14-PlOCNAB373-7G5.0/6G4.0-lOOT-150-T6-4064 16 = GE14-PI0CNAB376 -15GZ-100T-l50-T6 -4063 17 = GE14-PI0CNAB379 -14GZ-100T-l50-T6 -4259 18 = GE14-PIOCNAB381-4G6.0/11G5.0-100T-l50-T6-4260 19 = GE14-PlOCNAB381-4G6.0/12G5.0-lOOT-150-T6-4261, 20 = GE14-P10CNAB379:-15GZ-100T-150-T6-4262 21 = GE14-PIOCNAB383-8G6.0/5G5.0-100T-150-T6-4478 22 = GE14-PlOCNAB383-8G6.0/7G5.0-lOOT-150-T6-4479 23 = GE14-P10CNAB383-2G6.0/11G5.0-IOOT-150-T6-4480 24 = GE14-PlOCNAB383-lOG6.0/5G5.0-lOOT-150-T6-4481
- 2.2.1 Calculation ofMAPFAC(P)
COLR - 20 Revision 0 Page 7 of26 The core power-dependent MAPLHGR limit adjustment factor, MAPFAC(P) (Reference 2, 3, 11
& 15), shall be calculated by one of the following equations:
For O$ P < 25 :
No thermal limits monitoring is required.
For 25 $ P $ 29.5 :
With Turbine Bypass OPERABLE,'
For core flow < 50 Mlbs/hr, MAPFAC (P) = 0.604 + 0.0038 (P-29.5)
For core flow ;::: 50 Mlbs/hr, MAPFAC (P) = 0.584 + 0.0038 (P-29.5)
- With Turbine Bypass INOPERABLE, For core flow < 50 Mlbs/hr, MAPFAC (P) = 0.488 + 0.0051 (P-29.5)
For core flow*;::: 50 Mlbs/hr, MAPFAC (P) = 0.436 + 0.0051 (P-29.5)
For29.5<P$100:
MAPFAC (P) = 1.0 + 0.005233 (P-100) where: P = Core power (fraction ofrated power times 100).
Note: This range applies with pressure regulator in service and, for power >85%, it also applies with the pressure regulator out of service
- MAPFAC(P) for Pressure Regulator Out of Service Limits COLR - 20 Revision 0 Page 8 of26 With one Turbine Pressure Regulator Out of Service and Reactor Power Greater Than or Equal to 29.5% and Less Than or Equal to 85% and both Turbine Bypass and Moisture Separator Reheater Operable:
For 25 :5 P :5 29.5 :
For core flow < 50 Mlbs/hr, MAPFAC (P) ~ 0.604+ 0.0038 (P-29.5)
For core flow ~ 50 Mlbs/hr, MAPFAC (P) = 0.583 + 0.0036 (P-29.5)
For 29.5 < P < 45 MAPFAC (P) = 0.680 + 0.00627 (P-45)
For 45 :5 P < 60 :
MAPFAC (P) = 0.758 + 0.0052 (P- 60)
For 60 :5 P :5 85 :
MAPFAC (P) = 0.831 + 0.00292 (P-85) where: P = Core power (fraction of rated power times 100).
- 2.2.2 Calculation ofMAPFAC(F)
COLR - 20 Revision 0 Page 9 of26 The core flow-dependent MAPLHGR limit adjustment factor, MAPFAC(F) (Reference 2 & 3),
shall be calculated by the following equation:
- WT MAPFAC(F)=MIN(C,AFx-+ BF)
JOO where:
WT = Core flow (Mlbs/hr).
AF = Given in Table 2.
BF = Given in Table 2.
C = 1.0 in Dual Loop and 0.80 in Single Loop.
TABLE 2 FLOW-DEPENDENT MAPLHGR LIMIT COEFFICIENTS Maximum Core Flow*
(Mlbs/hr) 110 0.6787 0.4358
- 3.0 MINIMUM CRITICAL POWER RATIO COLR - 20 Revision 0 Page 10 of26 TECH SPEC IDENT OPERATING LIMIT 3.2.2 MCPR 3.1 Definition The :tv1INIMUM CRITICAL POWER RATIO (MCPR) shall be the smallest Critical Power Ratio
- (CPR) that exists in the core for each type of fuel. The CPR is that power in the assembly that is calculated by application of the appropriate correlation(s) to cause some point in the assembly to experience boiling transition, divided by the actual assembly operating power.
3.2 Determination of Operating Limit MCPR The required Operating Limit MCPR (OLMCPR) (Reference 2) at steady-state rated power and flow operating conditions is derived from the established fuel cladding integrity Safety Limit MCPR and an analysis of abnormal operational transients. To ensure that the Safety Limit MCPR is not exceeded during any anticipated abnormal operational transient, the most limiting transients have been analyzed to determine which event will cause the largest reduction in CPR.
Three different core average exposure conditions are evaluated. The result is an Operating Limit MCPR which is a function of exposure and 'C. 'C is a measure of scram speed, and is defined in Section 3.3.2. Cycle 20 operating limits are based on the Two Loop SLMCPR of 1.08.
The limiting OLMCPR shall be represented by the following equation:
OLMCPR = MAX.(MCPR(P), MCPR(F))
The process to calculate MCPR(P), the core power-dependent MCPR operating limit, 1s illustrated in Section 3.3.
The process to calculate MCPR(F), the core flow-dependent MCPR operating limit, is illustrated in Section 3.4. ..J In case of Single Loop Operation, the Safety Limit MCPR (Reference 2) is increased to account for increased uncertainties in core flow measurement and TIP measurement. For Single Loop Operation, the OLMCPR is increased by 0.03 from the Two Loop OLMCPR.
- COLR - 20 Revision 0 Page 11 of26 In case of operation with one Turbine Pressure Regulator out of service, OLMCPR limits are bounding when reactor power is less than 29.5% or greater than 85%. When reactor power is greater than or equal to 29.5% and less than or equal to 85%, then operation with one Turbine Pressure Regulator out of service is permitted if both Turbine Bypass Valves and the Moisture Separator Reheater are operable. (Reference 2 and 11)
TABLE 3 OLMCPR100110s AS A FUNCTION OF EXPOSURE AND 't (Reference 2 and 11)
_./
EXPOSURE CONDITION (MWD/ST) OLMCPR100110s BOTH Turbine Bypass Valves AND Moisture Separator Reheater Two Loop Single Loop OPERABLE BOCto EOR-4991 't =O 1.26 1.29
't = 1 1.38 1.41 EOR-4991 to EOR-2991 't=O 1.27 1.30
't = 1 1.44 1.47 EOR-2991 to EOC 't=O 1.32 1.35
't = 1 1.49 1.52 ONE Turbine Pressure Regulator Out of Service AND Reactor Power between 29.5% and 85%
AND BOTH Turbine Bypass Valves and Moisture Separator Reheater Operable BOCtoEOC 't=O 1.32 1.35
't = 1 1.49 1.52 Moisture Separator Reheater INOPERABLE BOCtoEOC 't=O 1.36 1.39
't = 1 1.53 1.56 Turbine Bypass Valve INOPERABLE BOCtoEOC 't =O 1.36 1.39
't = 1 1.53 1.56 BOTH Turbine Bypass Valve AND Moisture Separator Reheater INOPERABLE BOCtoEOC 't =O 1.42 1.45 "C= 1 1.59 1.62 BOC= Beginning of Cycle EOC = End of Cycle EOR = End of Rated Conditions.
EOR is defined as 100% power, 100% core flow, and all control rods fully withdrawn.
EOR-4991 means 4991 MWD/ST before End of Rated Conditions.
- 3.3 Calculation ofMCPR(P)
COLR - 20 Revision 0 Page 12 of26 MCPR(P), the core power-dependent MCPR operating limit (Reference 2, 3, 11, & 15), shall be calculated by the following equation:
MCPR(P) = KP x OLMCPR1001105 Kp, the core power-dependent MCPR Operating Limit adjustment factor, shall be calculated by using Section 3.3.1. OLMCPR100110s shall be determined by interpolation on 't from Table 3 (Reference 2), and 't shall be calculated by using Section 3.3.2.
3.3.1 Calculation of Kp The core power-dependent MCPR operating limit adjustment factor, KP (Reference 2, 3, 11, &
15), shall be calculated by using one of the following equations:
Note: P = Core power (:fraction of rated power times 100) for all calculation of Kp For O::: P < 25 No thermal limits monitoring is required.
For 25::: P < 29.5 When Turbine Bypass is OPERABLE, KP= ( KBYP + (0.032 x (29.5 -P)))
OLMCPR 1001105 For two loop operation, where: KBYP = 2.18 for core flow < 50 Mlbs/hr
= 2.46 for core flow ~ 50 Mlbs/hr For single loop operation, where: KBYP = 2.21 for core flow< 50 Mlbs/hr
= 2.49 for core flow ~ 50 Mlbs/hr When Turbine Bypass is INOPERABLE,
. .:. . ( KBYP + (0.076 x (29.5- P)))
KP-~~~~~~~~~~
OLMCPR 1001105 For two loop operation, where: KBYP = 2.65 for core flow< 50 Mlbs/hr
= 3.38 for core flow~ 50 Mlbs/hr For single loop operation, where: KBYP = 2.68 for core flow < 50 Mlbs/hr
= 3 .41 for core flow ~ 50 Mlbs/hr
- For 29.5<P<45 Kp = 1.28 + (0.0134 x (45-P))
COLR - 20 Revision 0 Page 13 of26 For 45::; P < 60 KP= 1.15 +(0.00867x (60-P))
KP for Moisture Separator Reheater Operable and Turbine Bypass Valves Operable or Inopera hie ,
- For 60 ::; P < 85 :
Kp = l.065+(0.0034x(85 -P))
For 85 ::; P ::; 100 :
Kp = l.0+(0.004333x(JOO-P))
KP for Moisture Separator Reheater Inoperable and Turbine Bypass Valves Operable or Inoperable For 60 ::; P < 85 :
Kp = l.076+(0.00296x(85 -P))
For 85 ::; P ::; 100 :
Kp = l.0+(0.00507x(JOO-P))
Kp for Pressure Regulator Out of Service Limits With one Turbine Pressure Regulator Out of Service, Reactor Power greater than 29.5%, and both Turbine Bypass and Moisture Separator Reheater Operable:
For 29.5::: P < 45 KP= 1.52+(0.01193x (45-P))
For 45 ::: P < (,0 :
KP= 1.362 + (0. OJ 053x (60-P))
For 60 ::: P ::: 85 :
KP= 1.217 + (0.0058 x (85 -P))
For Reactor* Power > 85%, the Pressure Regulator Out of Service condition is not limiting (Reference 11). Calculate I(p using the applicable equations above based on Moisture Separator
- Reheater and Turbine Bypass Valve operabiHty.
- 3.3.2
- Calculation of't COLR - 20 Revision 0 Page 14 of26 The value of 'C, which is a measure of the conformance of the actual control rod scram times to the assumed average control rod scram time in the reload licensing analysis (References 4 & 24),
shall be calculated by using the following equation:
where: 'CA = 1.096 seconds
'fB - 0.830 + 0.019 x 1.65 ~ Seconds
- n = number of surveillance tests performed to date in cycle, M = number of active control rods measured in the ith surveillance test,
'Ci = average scram time to notch 36 of all rods measured in the ith surveillance test, and N1 = total number of active rods measured in the initial control rod scram time .
test for the cycle (Technical Specification Surveillance Requirement 3.1.4.4).
The value of 'C shall be calculated and used to determine the applicable OLMCPR100110s value from Table 3 within 72 hours8.333333e-4 days <br />0.02 hours <br />1.190476e-4 weeks <br />2.7396e-5 months <br /> of the conclusion of each control rod scram time surveillance test required by Technical Specification Surveillance Requirements 3.1.4.1, 3.1.4.2, and 3.1.4.4 .
- 3.4 Calculation ofMCPR(F)
- COLR - 20 Revision 0 Page 15 of26 MCPR(F), the core flow-dependent MCPR operating limit (Reference 2 & 3), shall be calculated by using the following equation:
WT For Two Loop Operation MCPR(F)= MAX(l.21, ( AFx-+ BF))
JOO WT For Single Loop Operation MCPR(F)= MAX(l.24,(AFx-+ BF))
JOO where:
WT = Core flow (Mlbs/hr).
AF = Given in Table 4.
BF = Given in Table 4.
TABLE 4 FLOW-DEPENDENT MCPR LIMIT COEFFICIENTS
- Two Loop Operation Maximum Core Flow*
(Mlbs/hr) 110 -0.601 1.743 Single Loop Operation 110 -0.601 1.773
- 4.0 LINEAR HEAT GENERATION RATE COLR- 20 Revision 0 Page 16 of26 TECH SPEC IDENT ) OPERATING LIMIT 3.2.3 LHGR 4.1 Definition The LINEAR HEAT GENERATION RATE (LHGR) shall be the heat generation rate per unit l~ngth of fuel rod. It is the integral of the heat flux over the heat transfer area associated with the unit length. By maintaining the operating LHGR below the applicable LHGR limit, it is assured that all thermal-mechanical design bases and licensing limits for the fuel will be satisfied.
4.2 Determination of LHGR Limit The maximum LHGR limit is a function of reactor power, core flow, fuel and rod type, and fuel rod nodal exposure. The limit is developed, using NRC approved methodology described in References 7 and 8, to ensure.the cladding will not exceed its yield stress and that fuel thermal-mechanical design criteria will not be violated during any postulated transient events. The
- LHGR limit ensures the fuel mechanical design requirements as defined in References 1 & 21 will be met.
The LHGR limit during dual loop operation is calculated by the following equation:
LHGR= = MIN (LHGR (P), LHGR (F))
where:
LHGR (P) = LHGRFAC (P) x LHGRsm LHGR (F) = LHGRFAC (F) x LHGRsm Within four hours after entering single loop operation, the LHGR limit is calculated by the following equation:
where:
LHGR (P) = LHGRFAC (P) x LHGRsm LHGR (F) = LHGRFAC (F) x LHGRsm LHGRFAC (P) and LHGRFAC (F) are limited to 0.80 The Single Loop multiplier limit is 0.80 (Reference 2) based on assuring a LOCA in single loop
- will be bounded by the two loop LOCA (Reference 12).
- COLR - 20 Revision 0 Page 17 of26 LHGRsm, the standard LHGR limit, is defined at a power of 3486 MWth and flow of_ 105 Mlbs/hr for each fuel and rod type as a function of fuel rod nodal exposure and found in the Table 5 reference. When hand calculations are required, LHGRsm shall be determined by interpolation from the Table 5 reference. LHGRFAC(P), the core power-dependent LHGR limit adjustment factor, shall be calculated by using Section 4.2.1. LHGRF AC(F), the core flow-dependent LHGR limit adjustment factor, shall be calculated by using Section 4.2.2.
TABLES STANDARD LHGR LIMITS FOR VARIOUS FUEL TYPES For GE14 fuel listed below, the most limiting LHGR for Uranium Only fuel rod is found in NEDC-32868P Revision 6 Table D-2 (References 1 & 21).
For GE14 fuel listed below, the most limiting LHGR for Gadolinia Bearing fuel rods is found in NEDC-32868P Revision 6 Table D-4 (References 1 & 21 ). Utilize the row for 6% Rod/Section wt-%
Gd203 Fuel Types 2 = GE14-PIOCNAB38I-4G6.0/11G5.0-IOOT-150-T6-4372 3 = GEI4-PIOCNAB381-4G6.0/9G5.0-100T-150-T6-4371 4 = GEI4-PIOCNAB381-15G5.0-100T-150-T6-4373 5 = GE14-PIOCNAB381-6G6.0/9G5.0-l00T-I50-T6-4374 6 = GEI4-PIOCNAB385-l3GZ-100T-l50-T6-4571 7 = GE14-P10CNAB384-15GZ-IOOT-150-T6-4572 8 = GE14-PIOCNAB383-13GZ-IOOT-150-T6-4573 9 = GE14-P10CNAB377-15GZ-100T-I50-T6-4574 14 = GE14-PIOCNAB376-4G6.0/9G5.0/2G2.0-100T-I50-T6-4061 15 = GE14-PIOCNAB373-7G5.0/6G4.0-IOOT-150-T6-4064 16 = GE14-PI0CNAB376-15GZ-100T-l50-T6-4063 17 = GEi 4-Pl OCNAB379-14GZ-l OOT-150-T6-4259 18 =. GEI4-Pl0CNAB381-4G6.0/11G5.0-100T-l50-T6-4260 19 = GEI4-P10CNAB381-4G6.0/12G5.0-100T-150-T6-4261 20 = GEI4-P10CNAB379-15GZ-100T-l50-T6-4262 21 = GE14-PIOCNAB383-8G6.0/5G5.0-IOOT-150-T6-4478 22 = GE14-PlOCNAB383-8G6.0/7G5.0-lOOT-150-T6-4479 23 = GE14-PIOCNAB383-2G6.0/11G5.0-100T-I50-T6-4480 24 = GE14-PIOCNAB383-10G6.0/5G5.0-IOOT-150-T6-4481
- 4.2.1 Calculation ofLHGRFAC(P)
COLR - 20 Revision 0 Page 18 of26 The core power-dependent LHGR limit adjustment factor, LHGRFAC(P) (Reference 2, 3, 11,&
15), shall be calculated by one of the following equations:
For 0.:::P <25:
No thermal limits monitoring is required.
For 25 :SP :S 29.5 :
With Turbine Bypass OPERABLE, For core flow < 50 Mlbs/hr, LHGRFAC (P) = 0.604 + 0.0038 (P-29.5)
For core flow ~ 50 Mlbs/hr, LHGRFAC (P) = 0.584 + 0.0038 (P-29.5)
- With Turbine Bypass INOPERABLE, For core flow < 50 Mlbs/hr,
/
LHGRFAC (P) = 0.488 + 0.0051 (P-29.5)
For core flow ~ 50 Mlbs/hr, LHGRFAC (P) = 0.436 + 0.0051 (P-29.5)
For 29.5 < P :S 100 :
LHGRFAC (P) = 1.0 + 0.005233 (P-100) where: P = Core power (fraction ofrated power times 100).
Note: This range applies with pressure regulator in service and, for power >85%, it also applies with the pressure regulator out of service '
- LHGRFAC(P) for Pressure Regulator Out of Service Limits COLR - 20 Revision 0 Page 19 of26 With one Turbine Pressure Regulator Out of Service and Reactor Power Greater Than or Equal to 29 .5% and Less Than or Equal to 85% and both Turbine Bypass and Moisture Separator Reheater Operable:
For 25 :5 P :5 29.5 :
For core flow < 50 Mlbs/hr, MAPFAC (P) = 0.604 + 0.0038 (P-29.5)
For core flow ~ 50 Mlbs/hr, MAPFAC (P) = 0.583 + 0.0036 (P- 29.5)
Fo:r 29.5 < P <45 :
LHGRFAC (P) = 0.680 + 0.00627 (P-45)
For 45 :5 P < 60 :
LHGRFAC (P) = 0. 758 + 0.0052 (P - 60)
For 60 $ P :5 85 :
LHGRFAC (P) = 0.831 + 0.00292 (P - 85) where: P = Core power (fraction of rated power times 100).
- 4.2.2 Calculation ofLHGRFAC(F)
COLR - 20 Revision 0 Page 20 of26 The core flow-dependent LHGR limit adjustment factor, LHGRFAC(F) (Reference 2 & 3), shall be calculated by the following equation:
where:
WT = Core flow (Mlbs/hr).
AF = Given in Table 6.
BF = Given in Table 6.
C = 1.0 in Dual Loop and 0.80 in Single Loop.
TABLE 6 FLOW-DEPENDENT LHGR LIMIT COEFFICIENTS Maximum Core Flow*
(Mlbs/hr) 110 0.6787 0.4358
- 5.0 CONTROL ROD BLOCK INSTRUMENTATION COLR - 20 Revision 0 Page 21 of26 TECH SPEC IDENT SETPOINT 3.3.2.l RBM 5.1 Definition The nominal trip setpoints and allowable values of the control rod withdrawal block instrumentation are shown in Table 7. These values are consistent with the bases of the APRM Rod Block Iechnical .fuJecification Improvement Program (ARTS) and the MCPR operating limits. (Referenc~s 2, 5, & 10).
TABLE7 CONTROL ROD BLOCK INSTRUMENTATION SE'rPOINTS WITH FILTER
- Setpoint Low power setpoint Intermediate power setpoint .
High power setpoint Trip Setpoint 27.0 62.0 82.0 Allowable Value 28.4 63.4 83.4 Low trip setpoint 117.0 118.9 Intermediate trip setpoint 112.2 114.l High trip setpoint 107.2 109.1 Downscale trip setpoint 94.0 92.3 For Cycle 20, the analyzed high trip setpoint of 111 % bounds the setpoints in Table 7. The OLMCPR associated with the RBM setpoint of 111 % is 1.26 for dual loop operation.
- 6.0 BACKUP STABILITY PROTECTION REGIONS I
COLR - _20 Revision 0 Page 22 of26 TECH SPEC REFERENCE OPERATING LIMIT 3.3.1.1 Action Condition J Alternate method to detect and suppress thermal hydraulic instability oscillations TRM REFERENCE OPERATING LIMIT 3.4.1.1 Scram, Exit, and Stability Awareness Regions 6.1 Definition The Backup Stability Protection (BSP) Regions are an integral part of the Tech Spec required alternative method to detect and suppress thermal hydraulic instability oscillations in that they identify areas of the power/flow map where there is an increased probability that the reactor core could experience a thermal hydraulic instability. The BSP Regions are required if the Oscillation Power Range Monitors are inoperable. Regions are identified (refer to Figures 1 and 2) that are
- either excluded from planned entry (Scram Region), or where specific actions are required to be taken to immediately leave the region (Exit Region). A region is also identified where operation is allowed provided that additional monitoring is performed to verify that the reactor core is not exhibiting signs of core thermal hydraulic instability (Stability Awareness Region). (Reference 2)
The boundaries of the Scram and Exit regions are established on a cycle specific basis based upon core decay ratio calculations performed using NRC approved methodology.
The Cycle 20 BSP boundaries defined in Figure 1 are applicable when final feedwater temperature is near the optimum range as illustrated in 20.107.02, Loss of Feedwater Heating Abnormal Operating Instruction. Figure 2 is applicable to operation with Feedwater Heaters Out-Of-Service (FWHOOS) or~with Final Feedwater Temperature Reduction (FFWTR) or when final feedwater temperature is below the optimum range .
- COLR - 20 Revision 0 Page 23 of26 80 l00%QTP - 3486MWI Rat ed Core Flow - 100.0Mlb/hr t---.
Figure 1- BSP Regions for Nominal Feedwater Temperature LLlA Rod line
+-- - - - - - - - - - - - - - + - - - -~ - - ~--,=_-+--+-.- - -~ - - - -
I 70 I ~- --- - - - -- - - + -I 7:.,
"- 40+- -- - I QPB~ -
Enabled Region
- 20 ..-<----+---+---1----1----+---+-----+--+----+---+-----+--+-----+--
30 40 Percent {%) of Rated Core Flow 50 Nominal feedwater heating exists with all feedwater heaters in service, the moisture separator
-+-----+---'
60 reheaters in service, and reactor water cleanup in or out of service. Nominal Feedwater temperature is determined with the Loss ofFeedwater Heating Abnormal Operating Procedure, 20.107.02. Iffeedwater temperature is less than 15 degrees Fahrenheit below the Optimum Line of the Feedwater Inlet Temperature vs. Reactor Power graph of Enclosure A of20.107.02, Loss ofFeedwater Heating, then Figure 1 can be used .
- COLR - 20 Revision 0 Page 24 of26 Figure 2 - BSP Regions for Reduced Feedwater Temperature 80 100%ClTP = 3486MWt Rated Core Flow= 100.0Mlb/hr MELLIA Rod Line
~
i
! 60i----'r-- -- - =---c...._----+-- ---::-,,£-- - - - --7"' - - - + - - - - " -- - - - - - t - -1
~
..,f=
i~ 5.0 +-- --I
~
C
~
~ ~ - - -- -- - ~ - - - + - - - - - -- -- -- - - +- - - - - - - - - . = a . - - - i - - 1
. OPR_M__
En_abJed Region
- 20 +-~-+---+- ->---
30
-+-- -+--
40
-+- --<>--- -+---+---+-
Percent(%) of Rated Core Flow 50 Reduced feedwater temperature is analyzed for a 50 degree Fahrenheit reduction in feedwater
- - - -- -+----+--+---'
60 temperature. If feedwater temperature is more than 15 degrees Fahrenheit below the Optimum Line of the Feedwater Inlet Temperature vs. Reactor Power graph of Enclosure A of20.107.02, Loss ofFeedwater Heating, then Figure 2 can be used .
7.0 REFERENCES
COLR - 20 Revision 0 Page 25 of26 Core Operating Limits Report references are cited for two purposes. Many references are used as the basis for information, numbers, and equations found in COLR. These references tend to be fuel type or cycle specific. Other references are listed as basis information for the content and structure ofCOLR but are not Cycle specific.
- 1. "Fuel Bundle Information Report for Enrico Fermi 2 Reload l 9*Cycle 20," Global Nuclear Fuel, DRF 004N4270, Revision 0, July 2018 (LHGR Limits), DTC: TRVEND, DSN: Cycle 20FBIR
- 2. "Supplemental Reload Licensing Report for Enrico Fermi 2 Reload 19 Cycle 20," Global Nuclear Fuel, DRF: 004N4269, Revision 0, July 2018 (MAPLHGR Limits, SLO Multiplier, MCPR Limits, SLMCPR, Off-Rated Limits, Backup Stability Regions, OPRM setpoints, RBM setpoint), DTC: TRVEND, DSN: Cycle 20 SRLR
- 3. "GE14 Fuel Cycle-Independent Analyses for Fermi Unit 2", GE-NE-0000-0025-3282-00 dated November 2004 (ARTS Limits equations, RR Pump Seizure)
- 4. Letter from Greg Porter to B. L. Myers, "Scram Times for Improved Tech Specs." GP-99014, October 22, 1999 containing DRF A12-00038-3, Vol. 4 information from G. A.
Watford, GE, to Distribution,
Subject:
Scram Times versus Notch Position (TAU Calculation), Edison File No. Rl-7242 *
- 5. NUMAC Power Range Neutron Monitoring System (PRNM) Surveillance Validation, Design Calculation DC-4608 Volume 1, Revision G (RBM A and B Setpoints), DTC:
TDPINC, DSN: DC-4608 VOL I
- 6. Detroit Edison Fermi-2 Thermal Power Optimization Task T0201: Operating Power/Flow Map, Edison File No. T13-050, (P-F Map for BSP figures)
- 7. "General Electric Standard Application for Reactor Fuel (GESTAR II)," NEDE-24011-P-A, Revision 27 with amendments
- 8. "The GESTR-LOCA and SAFER Models for the Evaluation of the Loss-of-Coolant Accident - SAFER/GESTR Application Methodology," NEDE 23785-1-PA, Revision 1, October 1984
- 9. "Fermi-2 SAFER/GESTR-LOCA, Loss-of-Coolant Accident Analysis," NEDC-31982P, July 1991, and Errata and Addenda No. 1, April 1992 *
- 10. "Maximum Extended Operating Domain Analysis for Detroit Edison Company Enrico Fermi
- Energy Center Unit 2," GE Nuclear Energy, NEDC-31843P, July 1990
J \
- COLR - 20 Revision 0 Page 26 of26
- 11. Fermi 2 Pressure Regulator Out of Service Evaluation - Verified Final Report, Letter l-2LHRMS-4 dated February 10, 2011. DTC: TRVEND, DSN: l-2LHRMS-4 Edison File Number: Rl-8100 (PROOS ,Limits)
- 12. "DTE Energy Enrico Fermi 2 SAFER/PRIJ\1E-LOCA Loss of Coolant Accident Analysis" DRF: OOON1319-RO datedMarch2015
- 13. Letter from T. G. Colburn to W. S. Orser, "Fermi Amendment No. 87 to Facility Operating License No. NPF-43 (TAC NO. M82102)," September 9, ,1992
- 14. Letter from J. F. Stang to W. S. Orser, "Amendment No. 53 to Facility Operating License No. NPF-43: (TAC No. 69074)," July 27, 1990
- 15. "Fermi 2 TRACG Implementation for Reload Licensing Transient Analysis", Revision 1, 0000-0128-8831-RI; June 2014, Edison File No. Rl-8124.
- 16. Methodology and Uncertainties for Safety Limit MCPR Evaluations, NEDC-3260IP-A, August 1999
- 17. Power Distribution Uncertainties for Safety Limit MCPR Evaluation, NEDC-32694P-A, August 1999
- 18. R-Factor Calculation Method for GE11, GEI2, and GEI3 Fuel, NEDC-32505P-A, Revision 1, July 1999
- 19. "Turbine Control Valve Out-Of-Service for Enrico Fermi Unit-2/' GE-Nuclear Energy, GE-NE-Jl l-03920-07-01, October 2001
- 20. Letter from David P. Beaulieu (USNRC) to William T. O'Connor, Jr. (Detroit Edison),
"Ferrni Issuance of Amendment RE: Changes to the Safety Limit Minimum Critical Power Ratio (TAC NO. MC4748)," dated November 30, 2004 (SLMCPR Limit)
- 21. "GEI4 Compliance with Amendment 22 ofNEDE-24011-P-A (GESTAR II)", NEDC-32868P, Revision 6, March 2016 (LHGR Limits), Edison File No: Rl-7307
- 22. "Fermi 2 - Issuance of Amendment Re: Measurment Uncertainty Recapture Power Uprate (TAC No. MF0650)" Letter from Thomas Wengert, NRC, to Joseph Plona, DTE Electric dated February 10, 2014.
- 23. Qualification of the One-Dimensional Core Transient Model for Boiling Water Reactors-Volume 1, NED0-24154-A, August 1986, Edison File No. Rl-7389.
- 24. Letter from G. G. Jones to A. D. Smart, "Fermi 2 Technical Specification Changes,"
, February 17, 1989 ,