MIT Plasma Science and Fusion CenterFusion Technology & Engineering Division
J.H. SchultzM.I.T. Plasma Science and Fusion Center
NSO PAC 2 Meeting
January 17-18, 2001
MIT Plasma Science and Fusion CenterFusion Technology & Engineering Division
1. IPB98(y.2) Scaling
- reduced 2.0 m Wedged FIRE from Q=10 to Q=5 at 10 T
- parametric study explores bucked/wedged option for cost/mission improvements
2. Equalization of TF/CS "burn times"
- optimization of TF/CS interface
3. Scan of A, Bt for "Fixed Mission"
- Margin=2 and Margin=1
4. Detailed Cost vs. Ro Sensitivities
MIT Plasma Science and Fusion CenterFusion Technology & Engineering Division
τ κEIPB p o t e avH y I R a B AMU n P980 93 1 39 0 58 0 15 0 78 0 19
200 41 0 690144 2= −. ( , ) . . . . . . . .d i
Physics EngineeringH(y,2)=1.1 Pw < 3 MW/m2
αN=0.2 Thot,TF < 373 K
βN =0.016 Thot,CS < 300 K
qlim = 3.104
τp∗/τΕ = 6
fGreenwald< 1
MIT Plasma Science and Fusion CenterFusion Technology & Engineering Division
(1) TF/OH interface optimization
tburn,TF = tburn,OH (TF/OH interface optimum for fixed Ro
Subtract 3 s from TF flattop for heating
e.g. 24.5 s flattop = 24.5 s I flattop = 3 s heat + 21.5 s burn
No scaling of theat with plasma parameters
(2) Minimum Ro for "Mission Margin"
Mission: Long-pulse α-dominated plasmas
Margin=2: Q>=10; tflattop/max(τE, τp*, τJ) >= 2
Margin=1: Q>=5; tflattop/max(τE, τp*, τJ) >= 1
MIT Plasma Science and Fusion CenterFusion Technology & Engineering Division
Instead of fixing Ro and varying A
Vary Ro and A, while holding Margin=1,2
Margin=min(Pα/Pheat, tflattop/τJ)
3 Variations:
1) Minimum Ro(fixed A,B)with M=min(Pα/Pheat, tflattop/τJ)
2) Minimum Ro(fixed A, Bvariable @ low A); M=Const
3) Minimum Ro(fixed A,B, f(q) @ high B); M=Const
MIT Plasma Science and Fusion CenterFusion Technology & Engineering Division
Alpha margin=Time margin=2 at optimum A=2.0/0.525
Rapid rise in time margin and heating margin off optimum A
MIT Plasma Science and Fusion CenterFusion Technology & Engineering Division
Reduced Mission: M=1, Q=5,tburn/τJ=1
R o,min = 1.59 m at Bt=11.5 T & A=(2.0/0.525)=3.8095
Bt=11.5 T for A=3.8
Bt=10.5 T for A=3.6
R(low A) nonlinear, but not pathological
MIT Plasma Science and Fusion CenterFusion Technology & Engineering Division
Ro (m) grows pathologically at high
Bt and qlim=3.1
Well-behaved if M=2,Q=10,t/τJ=2
(qlim > 3.1 at Bt>Bt,opt)Romin=1.86 m, A=3.8
Romin (A=3.6) = 1.925 m
MIT Plasma Science and Fusion CenterFusion Technology & Engineering Division
Romin = 1.86 m@
Bt=11.5, A=3.8
Ro (m) pathological at
low A
Cured by lowering Bt;
Q=10, M=2
(no effect on Romin)
MIT Plasma Science and Fusion CenterFusion Technology & Engineering Division
M2:Minimum Cost =$1.06 B @ Ro= 1.86 m, A=3.8, Bt=11.5 T
- M2 < $1 B, if phase auxiliary power
M1:Minimum Cost = $0.92 B @ Ro=1.59 m, A=3.8, Bt=11.5 T
MIT Plasma Science and Fusion CenterFusion Technology & Engineering Division
Vary Ro; Bt=11.5 T, A=3.8,
qL=3.1, not fixed mission
$/Ro Sensitivity = 1.01
$/Ro: Paux, I&C = 0
Magnets=1.64
Basic Machine=1.25
Buildings=1.14
MIT Plasma Science and Fusion CenterFusion Technology & Engineering Division
Ro can be reduced to 1.86 m and retain M=2 mission
Mission reduction x 2 allows reduction of Ro to 1.59 m (1st order!)
Margin=2 mission requires lowering B @ A<3.5 or q @ B>13 T
d$/dR = 1: Machine sensitivity ~ 1.25 + nearly fixed costs
Recommendation: Reduce Ro to 1.87 m, Day 1 RF = 10 MW
Achieve all cost/mission objectives: Q=10, τflat/τJ=2, Cost<$1 B
Historic first: A noncatastrophic reduction in NSO Ro