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APS/DPP 2008 GO3.00008 Politzer 01
Demonstration of ITER Operational Scenarios on DIII-D
P. A. Politzer1
for
E.J. Doyle2, R.V. Budny3, J.C. DeBoo1, J.R. Ferron1, G.L. Jackson1,T.C. Luce1, M. Murakami4, T.H.Osborne1, J.-M. Park4, H. Reimerdes5,T.A. Casper6, C.D. Challis7, R.J. Groebner1, C.T. Holcomb6, A.W. Hyatt1,R.J. La Haye1, J. Kinsey1, G.R. McKee8, T.W. Petrie1, C.C. Petty1, T.L. Rhodes2, M.W. Schafer8, P.B. Snyder1, E.J. Strait1, M.R. Wade1, G. Wang2, W.P.West1, and L. Zeng2
1 General Atomics, 2 UCLA, 3 PPPL, 4 ORNL, 5 Columbia Univ., 6 LLNL, 7 Euratom/UKAEA, Culham, 8 U. Wisconsin, Madison
50th Annual Meeting of the APS/DPPDallas, TexasNovember 17-21, 2008
APS/DPP 2008 GO3.00008 Politzer 02
ITER demonstration discharges support further development of operating scenarios
•Develop sample discharges for further experiments in support of ITER
•Provide a better basis for projection to ITER performance
• Identify issues requiring further study
➤ This talk will – describe the discharges we’ve developed, – discuss some of the ITER physics issues raised by these experiments, and– present projections to ITER performance
APS/DPP 2008 GO3.00008 Politzer 03
DIII-D demonstration discharges meet ITER normalized performance targets
Four ITER scenarios are addressed on DIII-D:
Baseline: conventional ELMy H-mode, with Q=10 at I=15 MA.
Steady-state: fully noninductive operation, with Q~5 at I~9 MA.
Hybrid: high neutron fluence, long pulse at reduced current, with Q~5-10 at I~11 MA.
Advanced inductive: high performance, Q=20+, Pfus~700 MW, I=15+ MA. G = βNH89/q952 is a useful control
room measure of expected fusion performance.
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G
G = βNH89/q952
advancedinductive
baselinehybrid
steady-state
Q=10
Q=5
131499131208131265133137
q95=3.3
q95=3.1
q95=4.7
q95=4.1
ITER
APS/DPP 2008 GO3.00008 Politzer 04
DIII-D has the unique capability to evaluate ITER scenarioswhile matching the design shape and aspect ratio
• Reduce all ITER plasma dimensions by a factor of 3.7
• The DIII-D plasmas match the ITER design values for – plasma shape– aspect ratio– value of I/aB (normalized current)
• Target values for βN and H98y2 were matched or exceeded– evaluate performance in the current flat-top phase– co-NBI used throughout
1.0 1.5 2.0-1.5
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m
ScaledITER (÷3.7)
DIII-D
ITER startup study: JP6.082 G. Jackson, PO3.014 T. Casper
APS/DPP 2008 GO3.00008 Politzer 05
ITER baseline scenario parameters matched on DIII-D
➔ I/aB equivalent to 15 MA in ITER, q95 = 3.1
➔ 3 second H-mode is ~ 3τR, approximately the same as in ITER
➔ Absolute density ~ same as in ITER, n/nGW ~ 0.65 (vs. 0.85 in ITER)
➔ Operation limited to βN ≤ 2,– occasional disruptions when 2/1 tearing modes appear
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H98y2
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t (sec)
ITER target (1.8)
ITER target (1.0)
ITER target (Q=10)
APS/DPP 2008 GO3.00008 Politzer 06
Concerns identified for the baseline scenario include ELMs and internal inductance
• Fractional energy loss at ELMs substantially exceeds ITER limits– type I ELMs have large radial extent– energy loss/ELM > 0.1×Wtot➔ strong motivation for more work on ELM control/modification/mitigation
• Internal inductance, li(3), for all scenarios in DIII-D was outside original ITER range for adequate control of plasma shape and position➔ has helped to successfully motivate change in ITER PF control range requirements
baseline
advanced inductivehybrid
steady-state
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l i(3
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original ITER design range
Ip flat-top
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baselineadvanced inductive
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steady-state
ITPA multi-tokam
ak
databaseν* (ITER)
ITER maximum
APS/DPP 2008 GO3.00008 Politzer 07
Fully noninductive operation demonstrated in ITER shape
• Fully noninductive operation achieved in 8.5 MA (ITER equivalent) discharge with βN = 3.1– high bootstrap fraction, ~70%
• Note trade-off between fusion performance (G) and noninductive fraction with varying q95
1343721.0
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t (sec)
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fbs
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ITER targetQ=5
APS/DPP 2008 GO3.00008 Politzer 08
Hybrid plasmas lead to long pulse & high fluence in ITER;advanced inductive discharges provide a path to Q ≥ 20
• AI: I/aB → 14.8 MA in ITER, q95 = 3.3hybrid: I/aB → 11.6 MA, q95 = 4.1
• Both hybrid and advanced inductive scenario plasmas have sustained high performance (βN = 2.8) with excellent confinement (H98y2 = 1.5)
• Some issues to be addressed: – requirements and methods for access to these regimes in ITER,– performance with conditions more relevant to ITER (rotation, collisionality, divertor parameters, …)– ELM mitigation
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PNB (MW)
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H98y2
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133137
ITER targetfor Q=10
hybrid
131265
advanced inductive
APS/DPP 2008 GO3.00008 Politzer 09
A good fit to pedestal parameters in the ITER scenarios is obtained from a new predictive model
• Compare the ITER scenario pedestal heights with the EPED1 predictive model➞ very good fit.
• For ITER parameters, in the baseline scenario EPED1 gives βN,ped = 0.65 at ρ = 0.96.
0 5 10 15 20 25EPED1-Predicted Pedestal Height (kPa)
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to te
st m
odel
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asu
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l He
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a)
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EPED1 model: NI1.001 P. Snyder
APS/DPP 2008 GO3.00008 Politzer 10
Performance projections indicate ITER will meet its physicsand technology objectives, with a good margin
Base- Hybrid AI Steady- line state
Pfus(ITER) 400 400 700 350
βN 1.8 2.8 2.8 3.1
QITER 10 5 ≥20 589P 10.3 5.8* 13.5 2.7*
98y2 22.4+ 23.3 ∞ 5.8*
DS03 ∞+ ∞+ ∞ 19.8
* Paux(required) > Paux(ITER) = 73 MW + Pconduction < PL-H (Y. Martin)
– all scaled cases yield Pfusion ≥ ITER scenario value
• Project using various confinement scalings:– ITER 89P (Bohm-like)– IPB 98y2 (intermediate)– DS03 (gyroBohm-like)
• Use the same βN, H, and profiles as in DIII-D;reset n/nGW = 0.85;assume Ti = Te
• Solve for required Paux (or H if ignited), Pfus and Q
APS/DPP 2008 GO3.00008 Politzer 11
Summary: DIII-D has demonstrated the performance required to meet ITER goals for four key scenarios
• The DIII-D ITER Demonstration discharge study addresses many of the key ITER physics issues, – ELMs, L-H transition, pedestal scaling, beta limits, …
• DIII-D results have influenced the ITER design,– expanding the operating range of the plasma shape control system
• DIII-D evaluation of ITER scenarios should be extended and improved– vary NBI power and torque to operate with reduced plasma rotation– extend operation with Te = Ti– determine sensitivity of performance to shape– assess impact of ELM suppression– include startup and rampdown constraints in demonstration discharges
➜ For more detail on this topic, visit Edward Doyle’s poster (JP6.061) this afternoon