Soliton-like Regime of Neutron Transport in a Multiplying ......Soliton-like Regime of Neutron...
Transcript of Soliton-like Regime of Neutron Transport in a Multiplying ......Soliton-like Regime of Neutron...
SolitonSoliton--like Regime of Neutron like Regime of Neutron Transport in a Multiplying Medium. Transport in a Multiplying Medium.
Physical Ground of Traveling Wave ReactorPhysical Ground of Traveling Wave Reactor
S.P. FominS.P. Fomin, A.S. Fomin, M.S. Malovytsia, V.V. Pilipenko, N.F. Shul, A.S. Fomin, M.S. Malovytsia, V.V. Pilipenko, N.F. Shul’’gaga
Akhiezer Institute for Theoretical PhysicsAkhiezer Institute for Theoretical PhysicsNSC NSC ““Kharkov Institute of Physics and TechnologyKharkov Institute of Physics and Technology””
e-mail: [email protected]
Channeling 2018 23Channeling 2018 23--28 September 201828 September 2018 Ischia, ItalyIschia, Italy
National Academy of Sciences of UkraineNational Academy of Sciences of UkraineNational Science Center National Science Center
““Kharkov Institute of Physics and TechnologyKharkov Institute of Physics and Technology””
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Outlook:Outlook:
• Historical introduction• Nuclear Burning Wave concept• Mathematical approach• Results of our calculations• Mixed Th-U-Pu fuel cycle• Stability study of NBW regime• Negative reactivity feedback (!)• Transient processes in NBW reactor• Main features of NBW reactor & possibility
to solve the nuclear power problems
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Nuclear Burning Wave concept
Lev Feoktistov (USSR, 1988):L.P. Feoktistov. Preprint IAE-4605/4, 1988.L.P. Feoktistov. Sov. Phys. Doklady, 34 (1989) 1071.
Edward Teller (USA, 1997): Traveling Wave Reactor Monte Carlo simulation
E.Teller. Preprint UCRL-JC-129547, LLNL,1997. Th-U fuel cycleHiroshi Sekimoto (Japan, 2001): CANDLE Deterministic approach
H.Sekimoto et al., Nucl. Sci. Eng., 139 (2001) 306. U-Pu fuel cycle, Stationary problem: x = z + Vt
238U (n,) 239U () 239Np () 239Pu (n,fission) ...T1/2 2.35 days
Concept & Analytical approach
Feoktistovcriterion
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8 8 Pu2 Pua a fn nD vn N Nt z
88 8 ;a
N vn Nt
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8 8 91
aN vn N Nt
Pu9 PuPu
1a f
N N vn Nt
x z Vt
8 8Pu aeq Pu Pu
f a
NN
( 1)ai iPu i
cr Puf
NN
Pu Pueq crN N
Goldin & Anistratov (USSR, 1992): Nuclear Burning Wave Deterministic approachV. Goldin, D. Anistratov. Preprint IMM RAS # 43, 1992. U-Pu fuel cycle 1d non-stationary problem
232232ThTh 233Th
233Pa
233233UU 234U 235U 236U 237U
T½ = 22.2 min
T½ = 27 days
237NpT½ = 6.75 days
238238UU 239U
239Np
239239PuPu 240Pu 241Pu 242Pu 243Pu
T½ = 23.5 min
T½ = 2,35 days
243Am
T½ = 4.98 hours
241Am
T½ = 14,3 years
ThTh--U fuel cycleU fuel cycle
UU--Pu fuel cyclePu fuel cycle
Nuclear fuel reproductionNuclear fuel reproduction
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L z
rR
Lign
j ext
Breeding zoneIgnition zone
238 U 100 %238 U 90 %
239 Pu 10 %
2D Non2D Non--Stationary Theory of Nuclear Burning WaveStationary Theory of Nuclear Burning WaveS. Fomin, et al. - 1st IC “Global 2009”, Paris, paper 9456.
Nuclear Burning Wave
/ / / / / /
/ / /
1 1
1
1 1 1
1 1
( ) ( )
g g gg g g g g g g g g g
a in mod in modg
gG Gg g g j j g g j j j g g gf f f d l f f l d l l inj l j l
g g g
rD Dv t r r r z z
C
( 1) ( 1) ( 1)g gg gl
al l l c l l lg g
N N Nt
Non-Stationary Nonlinear Multi-Group Diffusion Equation of Neutron Transport
Together with Fuel Burn-up Equations and Equations of Nuclear Kinetics
of Precursor Nuclei of Delayed Neutrons
96 6
N Nt
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1,4,5,6,7
ggfl l
l g
N Nt
( )j
j j j g g gll l l f f l
g
C Ct
Metal fuel (44%)Metal fuel (44%)
PbPb--Bi coolant (36%)Bi coolant (36%)
CM CM -- Fe (20%)Fe (20%)
jjext ext ~ ~ 10101155 cmcm--22 ss--11
ttoff off = 400 days= 400 days
( 1 8);, l
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NBW Reactor : R=117 cm, L = 500 cmNBW Reactor : R=117 cm, L = 500 cm , , ttoff off = 950 days= 950 days
,1017 cм-2 с-1
,1021 cм-3
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NBW reactor with mixed ThNBW reactor with mixed Th--UU--Pu fuelPu fuelSS. . Fomin et al.,Fomin et al., ICAPP 2010ICAPP 2010 (San Diego, USA)(San Diego, USA) paper 10302.paper 10302.SS. . Fomin et al.,Fomin et al., Progress in Nuclear Energy,Progress in Nuclear Energy, 52 52 ((2012011) 8001) 800--805.805.
L z
r
R
L зап
Jext
Breeding zoneIgnition zone
238 U 50 %238 U 90 %
239 Pu 10 % 232Th 50 %
ExampleExample: Metallic fuel : Metallic fuel 232232Th (62%) + Th (62%) + 238238U (48%) volume fraction = 55%, U (48%) volume fraction = 55%, fuel porosity p = 0.35;fuel porosity p = 0.35; Coolant (Pb-Bi eutectic) vol. frac. = 30%,frac. = 30%,
Constr. materials (Fe) vol. frac. = 15%; R = 390 cmfrac. = 15%; R = 390 cm
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Fuel burnFuel burn--upup for Thfor Th--UU--Pu cyclePu cycle
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Stability of the NBW Regime Stability of the NBW Regime -- Negative Reactivity FeedbackNegative Reactivity Feedback (!)(!)
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Variation of the reactivity ρ (dollars) with time t (days) along the variation of the volume-averaged neutron flux Fav (1015 cм-2 с-1)
-1 0 1 2 3 4 5 6 7 8
1
2
3
4
t - t0
av
-0,20
-0,15
-0,10
-0,05
0,00
0,05
0,10
0,15
0,20
av
Stability of the NBW Regime Stability of the NBW Regime -- Negative Reactivity FeedbackNegative Reactivity Feedback (!)(!)
S. Fomin et al., IC “Fast Reactors 20132013“ (Paris, France) paper CN-199-457
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Stability of the NBW RegimeStability of the NBW Regime(enriched region in the breeding zoon)(enriched region in the breeding zoon)
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Stability of the NBW RegimeStability of the NBW Regime
0 10 20 30 40 50
2468
1012141618
Pint , GW
t, years
62% Th, R=230 cm, 5% brick, z=300÷320 cm
62% Th, R=230 cm, 10% brick, z=300÷320 cm
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0 1 2 3 4 5 6 7
5
10
15
20
25
30
P, GW
t, years
Smooth Startup of the NBW Reactor
O. Fomin et al., Journal of Kharkiv National University, #1041, physical series «Nuclei, Particles, Fields», 2 /58/ (20132013) 49-56.
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0 1 2 3 4 5 6 7
5
10
15
20
25
30
P, GW
t, years
Smooth Startup of the NBW Reactor
0
1
2
3
4
0 10 20 30 40 50 60 70 80 90-4
-3
-2
-1
0, $ P, GW
0 10 20 30 40 50 60 70 80 900
10
20
30
40
50
N Np , N Pu
t, days
0
1
2
3
4
0 10 20 30 40 50 60 70 80 90-4
-3
-2
-1
0, $ P, GW
0 10 20 30 40 50 60 70 80 900
10
20
30
40
50
N Np , N Pu
t, days
Shutdown and Restart of the NBW ReactorShutdown and Restart of the NBW Reactor
Shutdown and Restart of the NBW ReactorShutdown and Restart of the NBW Reactor
0,0
0,5
1,0
1,5
2,0
2,5
3,0
3,5
4,0
0 30 60 90 120 150 180 210 240 270 300-7
-6
-5
-4
-3
-2
-1
0
1
t , days
, $ P , GW
t = 250Restart
ShutdownRestart
0 30 60 90 120 150 180 210 240 270 3000
10
20
30
40
ShutdownRestart
NNp
NU233
NPu
NPa
N & N , 1017cm-3
t , days
S. Fomin et al., IC Global 20201515 (Paris, France) paper 5254.
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- negative feedback on reactivity - intrinsic safety (!!!)
- long-term (decades!!) operation without refueling and external control
- possibility of 232Th and 238U utilization as a fuel
- fuel burn-up depth for both 238U and 232Th ≈ 50% (one through cycle !)
- neutron flux in active zone ≈ 2·1015 n/сm2s
- neutron fluence during the whole reactor campaign ≈ 3·1024 n/сm2
- energy production density in active zone ≈ 200 W/сm3
- total power at the steady-state regime ≈ 1.2 GWt
- wave velocity at the steady-state regime ≈ 2 сm/year
- possibility of nuclear waste burn out (expected)
Main features of NBW reactor with mixed ThMain features of NBW reactor with mixed Th--UU--Pu fuel cyclePu fuel cycleReactor composition (vol. frac.):Fuel = 55% (FTh = 62%, p = 0.20), Coolant = 30%, CM = 15%, R = 215 cm
2010:
http://www.ted.com/talks/bill_gates.html
TravelingTraveling--Wave ReactorWave Reactor
““TerraPowerTerraPower”” ++ ChinaChina == TWRTWR (2020)(2020)
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Minister Zhang of National Energy Minister Zhang of National Energy Administration Received Bill GatesAdministration Received Bill Gates
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Map of World’s Nuclear Power Plants
Reactors Start to Spread in Reactors Start to Spread in Waves Around the WorldWaves Around the World
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List of our publications on the NBW reactor List of our publications on the NBW reactor ::S. Fomin et al., S. Fomin et al., Annals of Nuclear EnergyAnnals of Nuclear Energy, 32 (, 32 (20052005) ) 14351435--1456.1456.S. Fomin et al., S. Fomin et al., Problems of Atomic Science & TechnologyProblems of Atomic Science & Technology, , 6 (6 (20052005) 106) 106--113.113.S. Fomin et al., ICENES (S. Fomin et al., ICENES (20052005) (Brussels, Belgium) paper IC058.) (Brussels, Belgium) paper IC058.S. Fomin et al., S. Fomin et al., Nuclear Science & Safety in EuropeNuclear Science & Safety in Europe. Springer (. Springer (20062006) 239) 239--251. 251. S. Fomin et al., S. Fomin et al., ICAPPICAPP’’06 (06 (20062006) (Reno, USA) paper 6157.) (Reno, USA) paper 6157.S. Fomin et al., S. Fomin et al., Problems of Atomic Science & TechnologyProblems of Atomic Science & Technology, 3 (, 3 (20072007)) 156156––163.163.S. Fomin et al., S. Fomin et al., ICAPPICAPP’’07 07 ((20072007) ) (Nice, France) paper 7499(Nice, France) paper 7499..S. Fomin, S. Fomin, Reactor Physics and Technology. . PINP WS, , StSt--Perersburg, XLPerersburg, XL--XLIXLI (20072007) 154-198.S. Fomin et al., S. Fomin et al., PProgress in Nuclear Energy, 50 (20082008) 163-169.
Yu.Mel’nik et al., Atomic Energy, 107 (20092009) 288-295.S. Fomin et al., Global 20092009 (Paris, France) paper 9456.S. Fomin et al., ICAPP 20102010 (San Diego, USA) paper 10302.S. Fomin et al., Progress in Nuclear Energy, 52 (20120111) 800-805.O. Fomin et al., Journal of KNU, #104, «Nuclei, Particles, Fields», issue 2 /58/ (20132013) 49-56.S. Fomin et al., IC “Fast Reactors 20201313“ (Paris, France) paper CN-199-457.S. Fomin et al., IC “Global 20201515”” (Paris, France) paper 5254.
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1A1A--11--2:2: Sustainable Burning ReactorsSustainable Burning Reactors - Chairs: Kevan Weaver (TerraPower, USA)Traveling-Wave Reactors: Challenges and Opportunities - Kevan Weaver et al. (TerraPower, USA)Feasibility of LBE Cooled Breed and Burn Reactors - Ehud Greenspan (UC, Berkeley, USA)Preliminary Engineering Design of Sodium-Cooled CANDLE Core - Hiroshi Sekimoto (TIT, Japan)Nuclear Burning Wave in Fast Reactor with Mixed Th-U Fuel - Sergii Fomin et al (NSC KIPT, Ukraine)Nuclear Traveling Wave in a Supercritical Water Cooled Fast Reactor – W. Maschek (KIT, Germany)Development and Prospects of TWR Project in China - Zheng Mingguang (Shanghai NER&DI, China)Special PresentationSpecial Presentation: Traveling-Wave Reactors - John Gilliland. (Director of TerraPower, USA)
1A1A--3: Thorium Fuel Reactors3: Thorium Fuel Reactors - Chair: Sergii Fomin (NSC KIPT, Ukraine)(Th-U-Pu) - Mixed Fuel Cycle and Proliferation– E. Kryuchkov et al, (MEPhI, Russia)Large Scale Utilization of Thorium in Gas Cooled Reactors - V. Jagannathan (Bhabha ARC, India). . .
24Thank you for attention !Thank you for attention !