design point for a 1mw fusion neutron source
TRANSCRIPT
Design Point for a 1MW Fusion Neutron Source
P. E. Sieck1, S.Woodruff1, P. A. Melnik1, J. E. Stuber1,C.A.Romero-Talamas2, J. O’Bryan2, R. L. Miller3
1Woodruff Scientific Inc, 4000 Aurora Ave N, Suite 6, Seattle WA 98103
2University of Maryland Baltimore County, 1000 Hilltop Circle, Engineering 222Baltimore, Maryland 21250
3Decysive Systems, 813 Calle David Santa Fe, NM 87506
2016 US-Japan CT WorkshopAugust 24th 2016, Irvine, CA
Work supported by DARPA grant N66001-14-1-4044Work completed as part of the IAEA CRP on Compact Fusion
Neutron Sources
Motivation: IAEA CRP Compact Fusion n-Sources
I CRP 2014-1016 aiming forPn=1-100MW (1017 − 1019n/s)design points for wastetransmutation, fuel reprocessing.
I Tokamak, mirror, ST and other DTconcepts considered.
I Ours: magnetically compressedSpheromak with convergence CR
(=R0/Rf ) < 3.
I Based on prior results from SSPX[2] and S1 [3].
I Could readily fall into the ARPA-EIDEAS or ALPHA programs.
Motivation: high nTτ adiabatically with 1m system
I Historical: ATC [4], TUMAN-3M[5]
I Current: ARPA-E, private (FRCs, spheromaks and STs)
I Adiabatic means faster than τE .
Method: 0D, 2D and 3D time-dependent simulation
Tools:
I 0D analytic modeling
I 3D resistive MHD [6] analysis ofcompression to compare with0D analytic modeling
I CORSICA 2D equilibrium andstability code [7]
I Engineering design (CAD andforce/stress analysis)
I ARIES-like systems code writtenfor Matlab [1]
Method:
1. A 0D design point is defined
2. A CORSICA model is definedwith coil positions to supportequilibrium, and for formation.
3. NIMROD is used to test forstability, examine dynamics
4. Given coil currents fromCORSICA, a bank design isdeveloped.
5. Knowing the size of bank andcoils, an engineering designpoint is developed.
6. With all components defined, acost analysis is produced.
Results: 0D modeling for adiabatic compression
I P . V = N . R . T
I For processes that are adiabatic,(γ=5/3): P0 . Vγ0 = Pf . Vγf .
I If the compression is adiabatic, thenPV5/3 = const.
I and for self-similar compression (C =a0 / af )
I P0V0γ=Pf Vf
γ and since Vf =V0C3
then: Pf = P0 . C5 and since P ∼n.T and Tf = T0 . C2
Results: Device design point from 0D modeling
Parameter Symbol Value Units
Radial Convergence Cr 3Volumetric Convergence CV 27Initial Plasma Radius r0 0.5 mFinal Plasma Radius rf 0.166 m
Initial Volume V0 0.55 m3
Converged Volume Vf 0.16 m3
Initial Beta β0 15 %
Initial Density n0 2 ×1020m−3
Initial Magnetic Field B0 0.5 TInitial Temperature T0 244 eVFinal Temperature Tf 2196 eV
Final Density nf 54 ×1020m−3
Final Magnetic Field Bf 4.5 TInitial plasma current I0 0.75 MAFinal plasma current If 6.75 MAFinal Beta βf 45 %Final Magnetic Energy Uf 1.37 MJSteady State Fusion Power from neutrons Pn 1.27 MWSteady State Neutron Rate Γn 5.7E+17 n/s
Results: 3D MHD simulations of compression in cylindricalgeometry
E_tan applied
in bands along Z
I NIMROD simulation campaign with broad range of ICs, 20cmradius can, 5µs compression
I Full Braginskii (T-dependent) 2 fluid transport modelcalibrated to SSPX
Results: 3D MHD results follow 0D adiabatic scaling
2 4 6 8Volume Convergence
2´ 1020
4´ 1020
6´ 1020
8´ 1020
nd
1.5 2.0 2.5 3.0 3.5 4.0Area Convergence
0.1
0.2
0.3
0.4
0.5
bep
2 4 6 8 10 12Volume Convergence
5000
10000
15000
20000
pres
2 4 6 8 10 12Volume Convergence
20
40
60
80
100
tele
Results: CORSICA uncompressed, radial formation
I Injection from outboard side using solenoid and conicalannular electrodes (somewhat like S1)
I T0 = 200eV, and n0= 1e20m−3.
Results: CORSICA peak compression
I Plasma current increases to 6.75MA
I Fusion power of 1.3MW at 5keV
Results: Pressure optimization with shaping
I At peak compression, the shape of the plasma dictates theattainable beta (stable to Mercier (pressure-driven) modes).
Results: PSpice design point for coil banks
0
0
0
0
0
0
0
0
0
0
0
0
0
0
0
00
0
0
0
0
0
0
0
I
I
I
I
IC
20k
+
R8
1e-5
V4
TD = 100m
TF = 1n
PW = 1
PER = 2
V1 = 0
TR = 100n
V2 = 5
+-
+-
S3
S
VON = 1.0V
VOFF = 0.0V
R11
2.8
K K47
COUPLING = .104
K_Linear
V8
TD = 100m
TF = 1n
PW = 1
PER = 2
V1 = 0
TR = 100n
V2 = 5
R9
2
C60
5m
+-
+-
S1
S
VON = 1.0V
VOFF = 0.0V
R3
.1m
R6
1e-5
R2
.1m
K K27
COUPLING = .113
K_Linear
K K45
COUPLING = .0452
K_Linear
L4
946u
R12
9
V5
TD = 2.3m
TF = 1n
PW = 1
PER = 2
V1 = 0
TR = 1n
V2 = 5
+
-
+
-
S6
S
VON = 1
VOFF = 0
V6
TD = 100m
TF = 1n
PW = 1
PER = 2
V1 = 0
TR = 100n
V2 = 5
K K67
COUPLING = .0322
K_Linear
L10
42n
IC
20k
+
L13
42n
K K12
COUPLING = .248
K_Linear
C1
1m
V1
TD = 1.5m
TF = 1n
PW = 1
PER = 2
V1 = 0
TR = 1n
V2 = 5
K K25
COUPLING = .0379
K_Linear
K K36
COUPLING = .0452
K_Linear
L2
792u
K K17
COUPLING = .113
K_Linear
K K56
COUPLING = .0487
K_Linear
K K16
COUPLING = .0379
K_Linear
L8
42n
R15
9
+-
+-
S5
S
VON = 1.0V
VOFF = 0.0V
C2
1m
K K15
COUPLING = .0489
K_Linear
K K23
COUPLING = .106
K_Linear
K K34
COUPLING = .0806
K_Linear
K K14
COUPLING = .106
K_Linear
C61
5.16e-8
+
-
+
-
S8
S
VON = 1
VOFF = 0
R16
.1m
V7
TD = 1n
TF = 1n
PW = 1
PER = 2
V1 = 0
TR = 1n
V2 = 5
R1
.1m
R18
1e-5
+-
+-
S7
S
VON = 1.0V
VOFF = 0.0V
L6
574u
IC
20k
+
K K13
COUPLING = .174
K_Linear
K K46
COUPLING = .131
K_Linear
+
-
+
-
S2
S
VON = 1
VOFF = 0
K K26
COUPLING = .0489
K_Linear
L3
946u
R5
1e-5
C59
5.16e-8R14
2.8
R7
1
R10
1.9
L7
1.23109e-3
+
-
+
-
S4
S
VON = 1
VOFF = 0
C55
5.16e-8
IC
40k
+
V3
TD = 1.9m
TF = 1n
PW = 1
PER = 2
V1 = 0
TR = 1n
V2 = 5
K K37
COUPLING = .104
K_Linear
R20
2.8
R17
1e-5
L9
42n
R4
1e-5
K K57
COUPLING = .0322
K_Linear
K K24
COUPLING = .174
K_Linear
V2
TD = 100m
TF = 1n
PW = 1
PER = 2
V1 = 0
TR = 100n
V2 = 5
L5
574u
C58
5.16e-8
C3
0.05m
R13
1.9
L1
792u
K K35
COUPLING = .131
K_Linear
Results: PSpice design point for banks
I Fast compression: 1ms rise for coils
Time
0s 1.0ms 2.0ms 3.0ms 4.0ms 5.0ms
I(L2) I(L6) I(L4) I(L7)
-5KA
0A
5KA
10KA
15KA
Results: Engineering design point for banksI Bank engineering point design based on WSI prior design [8]I Shown are two 120kJ modules, 20kV caps. $200k per set.
Results: Engineering design coils
I Coils to be actively cooledin vacuum.
I Design point current forcopper at 20C, althoughcooling will allow bank tobe reduced in size.
I Outer-most coil will useHT superconducting tape(REBCO), since itremains energized.
Results: Full assy for in-vacuum componentsI Coil casings, windings, support for in-vacuum operation.
Results: full system engineering design point
I Test compression and optimize neutron production
I Banks, chamber and diagnostics would fit in a 2000sqft lab
Results: Diagnostics requirements for system
I Thomson, interferometry,magnetics, electrostaticprobes.
I Engineering design pointscompleted as part ofPhase II SBIR
Results: costing for n-Source prototype over 5 years
I Forecast costs by category(materials, labor andoverhead), based onexperience at WSI.
I Build-out over Y1-Y3.
I Labor Y3-Y5.
I Prototype costs are $10M
I Full neutron source:$50M
Further Work
I Neutronics analysis with MCNP6 awaits - coming up inSeptember.
I Design point can be further optimized for efficiency, and forrep-rate.
I CORSICA analysis can be performed to address transport andshape optimization during run-in - this would form part of aSBIR proposal.
I Concept fits into ARPA-E IDEAS program, seeking to usefusion to resolve fission issues.
Summary
I Design point for a n-Source prototype has been examinedanalytically and numerically, using state-of-the-art tools (2Dand 3D time-dependent MHD).
I A full engineering point design has been developed, based onphysics design point.
I Cost of prototype source would be $10M, full source likely$50M.
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