Conceptual Design of Mixed- spectrum Supercritical Water Reactor T. K. Kim T. K. Kim Argonne...
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Transcript of Conceptual Design of Mixed- spectrum Supercritical Water Reactor T. K. Kim T. K. Kim Argonne...
Conceptual Design of Mixed-Conceptual Design of Mixed-spectrum Supercritical Water spectrum Supercritical Water
ReactorReactor
T. K. KimT. K. Kim
Argonne National LaboratoryArgonne National Laboratory
2Argonne National LaboratoryArgonne National Laboratory
Challenges of SCWR design in NeutronicsChallenges of SCWR design in Neutronics
• Axial power shape controlAxial power shape control– Large coolant density variation axiallyLarge coolant density variation axially
– Smaller control rod worthSmaller control rod worth
• Radioactive waste control Radioactive waste control – Fast spectrum of SCWR can burn higher actinides Fast spectrum of SCWR can burn higher actinides
• Neutronics code systemNeutronics code system– Multi-group, 3 dimensional, T/H coupling systemMulti-group, 3 dimensional, T/H coupling system
– HTC correlation in supercritical conditionsHTC correlation in supercritical conditions
• Other issuesOther issues– Proliferation resistance and economyProliferation resistance and economy
3Argonne National LaboratoryArgonne National Laboratory
Mixed Spectrum SCWR ConceptMixed Spectrum SCWR Concept
• Advanced spectrum control is needed to Advanced spectrum control is needed to maximize merits of SCWRmaximize merits of SCWR
• Mixed-spectrum supercritical water reactorMixed-spectrum supercritical water reactor– Separation fast and thermal spectrum radiallySeparation fast and thermal spectrum radially
• Smaller power peaking factor and easier reactivity Smaller power peaking factor and easier reactivity controlcontrol
– Multi-purposed reactorMulti-purposed reactor• Maximize thermal efficiency and economy of SCWR Maximize thermal efficiency and economy of SCWR
concept without additional design featuresconcept without additional design features
• Electric production and actinide Burning in fast Electric production and actinide Burning in fast spectral corespectral core
4Argonne National LaboratoryArgonne National Laboratory
MSMS22 core core
Outer core
Coolant inlet
Core plate
Coolant outlet
Control rod
Inner core
Thermal shield
> 0.1 g/cm3~ 0.7 g/cm3 ~ 0.7 g/cm3
~ 0.2 g/cm3
Void assembly
Inner core fuel assembly (397)
High enriched fuel
Low enriched fuel
Instrument tube
Control rod tube
20.76
Outer core fuel assembly (271)
High enriched fuel
Low enriched fuel
Instrument tube
Control rod tube
20.76
Low enriched fuel
High enriched fuel
Control rod
5Argonne National LaboratoryArgonne National Laboratory
Comparison of SCWR AssembliesComparison of SCWR Assemblies
Inner core fuel assembly (397)
High enriched fuel
Low enriched fuel
Instrument tube
Control rod tube
20.76
Water rod
(Moderator)
Control rod
Stagnant water
Coolant
Fuel rod
23.18
22.18
Fuel
Control blade
Solid rod
Moderator
Coolant
MSMS2 2 assemblyassembly
SCLWR-HSCLWR-H and INEELand INEEL
SCLWR-H old SCLWR-H old
6Argonne National LaboratoryArgonne National Laboratory
Comparison of SCWR DesignsComparison of SCWR Designs
SCLWR-H SCLWR-H 1)1)
SCFR-H SCFR-H 1)1)
INEEL INEEL 2)2)
MSMS22
PWRPWR
Inner coreInner core Outer coreOuter core
Thermal power, MWThermal power, MW 35863586 38933893 30223022 34003400 34113411
Number of fuel assemblyNumber of fuel assembly
Active height, cmActive height, cm
Power density, MW/mPower density, MW/m33
Fuel materialFuel material
Cladding materialCladding material
Fuel radius, cmFuel radius, cm
Cladding thickness, cmCladding thickness, cm
Fuel pitch, cmFuel pitch, cm
P/D of fuel cellP/D of fuel cell
Assembly ShapeAssembly Shape
Number of fuel rodsNumber of fuel rodsAssembly pitch, cmAssembly pitch, cm
211211
420.00420.00
102.58102.58
UOUO22
Ni-AlloyNi-Alloy
0.40000.4000
0.04000.0400
0.95000.9500
1.081.08
hexagonalhexagonal
258258
21.3421.34
278278
320.00320.00
206.02206.02
MOXMOX
Ni-AlloyNi-Alloy
0.44000.4400
0.05200.0520
1.01001.0100
1.031.03
hexagonalhexagonal
198198
15.6615.66
121121
427.00427.00
69.0769.07
UOUO22
ODS steelODS steel
0.44700.4470
0.06300.0630
1.10001.1000
1.081.08
squaresquare
300300
29.1029.10
7373
280.00280.00
131.75131.75
MOXMOX
Ni-AlloyNi-Alloy
0.44000.4400
0.04000.0400
1.00001.0000
1.041.04
hexagonalhexagonal
378378
20.7120.71
204204
280.00280.00
113.15113.15
MOXMOX
Ni-AlloyNi-Alloy
0.40950.4095
0.05720.0572
1.20001.2000
1.291.29
hexagonalhexagonal
252252
20.7120.71
193193
366.00366.00
104.00104.00
UOUO22
ZrZr
0.40950.4095
0.05720.0572
1.25001.2500
1.341.34
squaresquare
264264
21.5021.50
Inlet temperature (in/out), Inlet temperature (in/out), ooCC 280/508280/508 280/526280/526 280/500280/500 387/553387/553 280/387280/387 300/332300/332
Coolant mass flow rate, kg/sCoolant mass flow rate, kg/s 18161816 16941694 15611561 19001900 1722217222
Coolant velocity (in/out) ,m/secCoolant velocity (in/out) ,m/sec 2.5 / 2.12.5 / 2.1 3.2 / 29.5 3.2 / 29.5 1.4 / 12.51.4 / 12.5 12.6 / 41.6 12.6 / 41.6 0.7 / 2.0 0.7 / 2.0 4.6 / 5.24.6 / 5.2
1. High Temperature Supercritical thermal reactor (O. Oka, "Design Concept of Once-Through Cycle Supercritical-Pressure Light Water Reactors," SCR-2000, Tokyo (2000)
2. INEEL design (tentative)
7Argonne National LaboratoryArgonne National Laboratory
WIMS8/SOLTRAN Code SystemWIMS8/SOLTRAN Code System
• WIMS8 used for lattice calculationsWIMS8 used for lattice calculations
• Zonal cross sections are functionalized by state parameters, Zonal cross sections are functionalized by state parameters,
• SOLTRAN used for core calculationsSOLTRAN used for core calculations
– Interface current nodal formulation of diffusion and simplified PInterface current nodal formulation of diffusion and simplified P22 equation in multi-dimensional hex-Z and X-Y-Z geometryequation in multi-dimensional hex-Z and X-Y-Z geometry
– Multi-group, microscopic depletionMulti-group, microscopic depletion
– Single-phase heat balance equation for T/H feedbackSingle-phase heat balance equation for T/H feedback
– HTC is updated by DB-, Modified DB-, and Jackson’s correlationsHTC is updated by DB-, Modified DB-, and Jackson’s correlations
8Argonne National LaboratoryArgonne National Laboratory
MSMS22 Core Analysis (1) Core Analysis (1)• BurnerBurner
– Inner core : MOXInner core : MOX• Th/TRU/U = 32.5/15/32.5 %Th/TRU/U = 32.5/15/32.5 %
• Fissile fraction = 11%Fissile fraction = 11%
– Outer core : MOX Outer core : MOX • Th/Pu/U = 3/8/89 %Th/Pu/U = 3/8/89 %
• Fissile fraction = 6.5%Fissile fraction = 6.5%
• ConverterConverter
– Inner core : MOXInner core : MOX• Th/Pu/U = 3/8/89 %Th/Pu/U = 3/8/89 %
• Fissile fraction = 6.5%Fissile fraction = 6.5%
– Outer core : MOX Outer core : MOX • Th/Pu/U = 3/8/89 %Th/Pu/U = 3/8/89 %
• Fissile fraction = 6.5%Fissile fraction = 6.5%Inner Core(73)
Outer Core(204)
Thermal shield(36)
Void assembly(18)
9Argonne National LaboratoryArgonne National Laboratory
MSMS22 Core Analysis (2) Core Analysis (2)
Power sharing, %
0.0
10.0
20.0
30.0
40.0
50.0
60.0
70.0
80.0
90.0
Burnuer-BOC Burnuer-EOC Converter-BOC Converter-EOC
Power Sharing (%)
Inner
Outer
Axial power distribution
0.0
0.5
1.0
1.5
2.0
2.5
0 40 80 120 160 200 240 280
Axial height (cm)
Normalized power
Burner-inner Burner-outer Converter-inner Converter-outer
Axial cladding susrface temperature
550
600
650
700
750
800
850
900
950
0 40 80 120 160 200 240 280
Axial height (cm)
Cladding temperature (K)
Burner-inner Burner-outer Converter-inner Converter-outer
HTC = Jackson’s correlation 2.392
1.155 2.262
1.130
2.111
1.094
1.810
1.008
1.898
1.035
1.035
1.898
1.623
0.957
1.623
0.957
1.212
0.895
1.311
0.908
0.931
1.373
1.373
0.931
1.311
0.908
0.918
1.230
0.962
1.301
1.344
0.994
1.011
1.367
1.011
1.367
0.994
1.344
0.962
1.301
0.781
1.014
0.843
1.104
1.161
0.883
0.906
1.193
0.914
1.204
0.906
1.193
0.883
1.161
0.843
1.104
0.610
0.796
0.693
0.896
0.961
0.745
0.776
1.000
0.791
1.018
0.791
1.018
0.776
1.000
0.745
0.961
0.693
0.896
0.339
0.471
0.494
0.658
0.738
0.563
0.602
0.782
0.622
0.806
0.629
0.813
0.622
0.806
0.602
0.782
0.658
0.494
0.494
0.658
Burner
Converter
10Argonne National LaboratoryArgonne National Laboratory
Comparison of Axial Power and Comparison of Axial Power and TemperatureTemperature
0
0.5
1
1.5
2
2.5
3
3.5
4
0 70 140 210 280 350 420
Axial height(cm)
Normalized power
Burner-inner
Burner-outer
SCLWR-H
SCWR
500
550
600
650
700
750
800
850
0 70 140 210 280 350 420
Axial height(cm)
Coolant temperature, K
Burner-inner
Burner-outer
SCLWR-H
SCWR
Axial power distribution
Axial cladding surface temperature distribution
Axial coolant temperature distribution
550
600
650
700
750
800
850
0 70 140 210 280 350 420
Axial height(cm)
Cladding surface temperature
Burner-inner
Burner-outer
SCLWR-H
11Argonne National LaboratoryArgonne National Laboratory
Comparison of MSComparison of MS22 Cores Cores
• BurnerBurner– Heterogeneous core (higher TRU and fissile content in inner Heterogeneous core (higher TRU and fissile content in inner
core)core)
– 40/60 % power sharing in inner/outer cores40/60 % power sharing in inner/outer cores
– Higher power peaking factor in inner core due to higher fissile Higher power peaking factor in inner core due to higher fissile contentcontent
– Cladding temperature of outer core is much lower than criteria Cladding temperature of outer core is much lower than criteria due to lower power peaking factordue to lower power peaking factor
• ConverterConverter– Homogeneous core (same fuel composition of inner and outer Homogeneous core (same fuel composition of inner and outer
cores)cores)
– 25/75 % power sharing in inner/outer cores due to coolant 25/75 % power sharing in inner/outer cores due to coolant density differencedensity difference
– Higher power peaking factor in outer core, which causes higher Higher power peaking factor in outer core, which causes higher cladding surface temperaturecladding surface temperature
12Argonne National LaboratoryArgonne National Laboratory
Conclusions and Future WorksConclusions and Future Works
• Conceptual design of MSConceptual design of MS22 core was core was performedperformed– WIMS/SOLTRAN code system was developed for WIMS/SOLTRAN code system was developed for
supercritical water reactor core analysissupercritical water reactor core analysis
– Feasibility of burner and converter with mixed-Feasibility of burner and converter with mixed-spectrum SCWR was evaluated, but design spectrum SCWR was evaluated, but design optimizations are necessaryoptimizations are necessary
• Future worksFuture works– Optimize the core design for burner and converterOptimize the core design for burner and converter
– Fuel cycle analysisFuel cycle analysis
– Evaluation of waste and economicsEvaluation of waste and economics