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High Fusion Performance in Super H-Mode Experiments on Alcator C-Mod and DIII-D
P.B. Snyder1, J.W. Hughes2, T.H. Osborne1, C. Paz-Soldan1, W. Solomon1, D. Eldon1, T. Evans1, T. Golfinopoulous2, B. Grierson4, R.J. Groebner1, A. Hubbard2, A. Jarvinen3, M. Knolker4, B. LaBombard2, F. Laggner4, A. Leonard1, O. Meneghini1, S. Mordijck5, T. Petrie1, S. Scott4, H.Q. Wang6, J.G. Watkins7, H.R. Wilson8, Y.B. Zhu9
Presented at 2018 IAEA Fusion Energy Conference Ahmedabad, Gujarat, India October 22–27, 2018
1 General Atomics 2 MIT Plasma Science and Fusion Center 3 Lawrence Livermore National Lab 4 Princeton University / PPPL 5 College of William and Mary 6 Oak Ridge Associated Universities
7 Sandia National Laboratory 8 York Plasma Institute, University of York, York UK 9 University of California-Irvine, Irvine CA
P.B. Snyder/IAEA/October 2018
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• This material is based upon work supported by the U.S. Department of Energy, Office of Science, Office of Fusion Energy Sciences, under Awards DE-FC02-04ER54698, DE-FC02-99ER54512, DE-FG02-95ER54309, DE-FC02-06ER54873, DE-SC0014264, and DE-SC0017992, using the DIII-D National Fusion Facility and Alcator C-Mod, DOE Office of Science user facilities. Extensive discussions with the ITPA pedestal group, as well as the numerous contributions of the Alcator C-Mod team, DIII-D team, and OMFIT group are gratefully acknowledged.
• DISCLAIMER: This report was prepared as an account of work sponsored by an agency of the United States Government. Neither the United States Government nor any agency thereof, nor any of their employees, makes any warranty, express or implied, or assumes any legal liability or responsibility for the accuracy, completeness, or usefulness of any information, apparatus, product, or process disclosed, or represents that its use would not infringe privately owned rights. Reference herein to any specific commercial product, process, or service by trade name, trademark, manufacturer, or otherwise does not necessarily constitute or imply its endorsement, recommendation, or favoring by the United States Government or any agency thereof. The views and opinions of authors expressed herein do not necessarily state or reflect those of the United States Government or any agency thereof.
Acknowledgments
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Super H-Mode Experiments on Alcator C-Mod and DIII-D Achieve High Fusion Performance, Record Pedestal Pressure
• Super H-mode (SH) predicted in strongly shaped plasmas: high pped, increases with ne [Snyder NF15]
• Record pedestal pressures (~80 kPa) achieved in C-Mod SH experiments [Hughes NF18] • Successful tests of EPED model up to ~90% of predicted ITER pped
• Record DIII-D fusion gain (QDT,eq~ 0.54). QDT,eq/IaB and QDT,eq/(RB)2 highest reported on any tokamak
• High performance sustained w/ 3D magnetic perturbations to control ne and impurity accumulation • Predicted to enable high performance on ITER, and be compatible with high separatrix density for
divertor solutions
0.0 0.5 1.0 1.5 2.0 2.5
0
5
10
15
Minor Radius (m)
Fusio
n P
erf
orm
ance M
etr
ic (
<p>
W/P
hIa
B)
ITER
DIII-D Super H
DIII-D H
C-Mod Super H
C-Mod H
JET H
TFTR L16MW
Q=5, 15MA
Q=10, 15MA
Q=10, 11MA
Q=inf, 15MA
2 atm
C-ModDIII-D
JET ITER
TFTR L-Mode
H-Mode
Super H-Mode/NSH
Q=inf, 11MA
4
EPED Model Predicts a High Pedestal “Super H-Mode” Solution
• EPED (Snyder NF11) normally predicts a single pedestal solution – Intersection of calculated peeling-ballooning (PB) and KBM criticality
– Predicted using sets of realistic model equilibria w/ self-consistent bootstrap current
• At strong shaping, fixed input parameters (including density), PB mode can go from stable to unstable (pressure driven) and back to stable again with increasing pressure and current: multiple roots for two “equations”, PB and KBM
0.00 0.02 0.04 0.06 0.080
5
10
15
20
25
30
35
Pedestal Width ( N)
Pedesta
l H
eig
ht (p
pe
d, kP
a)
Illustration of EPED1 Model, Multiple Roots
Peeling-Ballooning
KBM
EPED1 Prediction
S
SU
U
P.B. Snyder/IAEA/October 2018
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EPED Model Predicts a High Pedestal “Super H Mode” Solution
• Expect only lowest solution to be accessible for these parameters. However, can move in third dimension (eg density) to access higher roots (Super H)
• SH predicted by theory [Snyder12,15], discovered and explored in counter Ip campaigns on DIII-D [Solomon14, Snyder15, Garofalo15, Solomon16]
2016 C-Mod: L-I-H transition to explore Super H regime access 2017-18: DIII-D: co-Ip SH expts explore performance and core-edge
0.00 0.02 0.04 0.06 0.080
5
10
15
20
25
30
35
Pedestal Width ( N)
Pedesta
l H
eig
ht (p
pe
d, kP
a)
Illustration of EPED1 Model, Multiple Roots
Peeling-Ballooning
KBM
EPED1 Prediction
S
SU
U
1 2 3 4 5 6 7 8 9 100
5
10
15
20
25
Pedestal Density (1019 m-3)
Pede
stal H
eight
(kPa)
EPED Predicted Pedestal Height vs Density
Super H-ModeH-ModeNear Super H
P.B. Snyder/IAEA/October 2018
6
High peak performance in Super H-Mode experiments
P.B. Snyder/IAEA/October 2018
7
Pedestal Density [ne,ped(Zeff /2)1/2 ,1019 m-3 ]
Pede
stal
Pre
ssur
e (k
Pa)
Very High Super H Mode Pressure Predicted for C-Mod
• Alcator C-Mod is a compact, high field device (here Bt~5.3T), capable of high δ – After discovery of Super H-Mode on DIII-D, predictions were made for C-Mod (right)
• Test SH theory at high Bt & Bp, zero injected torque (RF), high Z metal wall – Following the right parametric trajectory should enable very high pressure
• Need to reach densities much lower than typical for C-Mod H-mode to access Super H • Challenging to do on a high-Z metal wall device like C-Mod
?
P.B. Snyder/IAEA/October 2018
8
Access to Super H Mode on C-Mod Achieved via L-I-H Transition
• Transitioning first to I-mode, then to H-mode leads to a low ne, low impurity H-mode (left) • As pedestal approaches predicted kink/peeling limit, low n mode observed (center) • Discharges at 1MA, 5.4T reach SH regime, pped~70 kPa (right)
Hughes et al, NF 58 112003 (2018) Pedestal Density [ne,ped(Zeff /2)1/2 ,1019 m-3 ]
Pede
stal
Pre
ssur
e (k
Pa)
680ms720ms
760ms790ms
C-Mod 1160922020, 0.8MA
Pede
stal
Pre
ssur
e (k
Pa)
Pedestal Density [ne,ped(Zeff /2)1/2 ,1019 m-3 ]
750ms
770ms
790ms810ms
830ms
850ms870ms
930ms
C-Mod 1160922032, 1MA
P.B. Snyder/IAEA/October 2018
9
100 101 102100
101
102
EPED Predicted Pedestal Height (kPa)
Mea
sure
d Pe
dest
al H
eigh
t (kP
a) C-Mod (3, SH expt)C-Mod (10, ELMing H-mode)DIII-D (124)JET (137)JT-60U (16)Compass (23)AUG (13)ITER
0 2 4 6 8 10 12 14 16 18 20 220
102030405060708090
100110120
Pedestal Density [ne,ped(Zeff/2)1/2,1019m-3]
Pede
stal
Pre
ssur
e (k
Pa)
EPED Predictions 1.4MA (based on 1160930042)
H-ModeNear Super HSuper H-ModeMeasured (C-Mod)
Super H-Mode Experiments on C-Mod Yield ITER-like pped
• Super H-Mode expt at 1.4MA achieved record 81 kPa pedestal pressure on last day of Alcator C-Mod operations, ITER-like pressure at ITER-like field [Hughes NF 2018] – EPED model successfully tested over 2 orders of magnitude in pressure on 6 tokamaks
• No indication of significant variation of model accuracy with ρ* or pped
P.B. Snyder/IAEA/October 2018
10
• High pedestal pressure enables good confinement, high global MHD limits – C-Mod: Bt=5.3-5.8T, Ip=0.8-1.4MA, a=0.19m, R=0.67m, δ~0.5
• <p> ~ 100-170 kPa, pped ~ 50 - 80 kPa – DIII-D: Bt=2.1-2.2T, Ip=1.6-2.0MA, a=0.6m, R=1.67m, δ~0.5-0.7
• <p> ~ 70 – 110 kPa, pped ~ 20 – 32 kPa, Ti,0 ~ 14 -18 keV
Broad Profiles and High Pressure Obtained in Both C-Mod and DIII-D
Electron Density (10 m )
0 2 4 6 8
Electron Temperature (keV)
02468
Ion Temperature (keV)
0.2 0.4 0.6 0.8 1.005
1015
DIII-D 177007 @ 2190ms
0Normalized Radius (ψ )
19 -3
N
177007.2190.00Electron Density (10 m )
Electron Temperature (keV)
Pressure (kPa)
19 -3
(Total)
(Electron)
C-Mod 1160930042 @ 900ms
Normalized Radius (ψ )N
0.2 0.4 0.6 0.8 1.000
100200300
400
510152025
0
0
2
4
6
8
P.B. Snyder/IAEA/October 2018
11
• Deep access into Super-H regime, good agreement with EPED predictions – Bt=2.17T, Ip=1.6-2.0MA, a=0.6m, δ~0.5-0.7 – pped~30kPa, W~2 - 3.2 MJ (highest in present DIII-D config.) at modest Pnbi ~ 8-12 MW – Peak τ~0.4-0.7s, H98~2.2-2.9, <p>τE ~ 30-67 kPa s, nTτ ~ 4 - 8 1020 keV m-3 s
Very High Pedestal Pressure, Stored Energy, and Confinement Time in Recent co-Ip Super H-Mode Experiments on DIII-D
3 4 5 6 7 8 9 10 11 120
5
10
15
20
25
30
35
Pedestal Density [ne,ped(Zeff/2)1/2,1019m-3]
Pede
stal
Pre
ssur
e [2
*pe,
ped,
kPa]
Access to High Performance Super H-Mode Regime on DIII-D
H-ModeNear Super HSuper H
t=2.1s
t=2.2st=2.3s t=2.4s
P.B. Snyder/IAEA/October 2018
12
• DD neutron rates up to 1.85 1016/s – ~2/3 thermal, Pfus,DD ~ 22 kW, Pfus,DT,eq ~ 4.8 MW (at Pnbi ~ 9 MW)
High Pedestal Pressure and Ti Enable High Peak Fusion Performance on DIII-D
P.B. Snyder/IAEA/October 2018
1.95 2.10 2.25 2.400.0
0.4
0.8
1.2
1.6
2.0174809
Total(TRANSP)
Measured
Thermal(TRANSP)
Beam-Target (TRANSP)
Beam-Beam (TRANSP)
Time (s)
Neu
tron
Rat
e (1
0
/s)
16
13
• Equivalent QDT,eq = Pfus,DTeq/Pnbi ~ 0.54. Q*DT,eq=Pfus,DTeq/(Pnbi-dW/dt) ~ 1
– Previous DIII-D record Q = 0.32, Lazarus96 in negative central shear discharges with 2.2MA, 22m3
– Achieved at modest B = 2.17T, Ip=2MA, V=20 m3. DTeq Fusion power density ~0.2 MW/m3
High Pedestal Pressure and Ti Enable High Peak Fusion Performance on DIII-D, Record Fusion Gain
Appears to be highest QDT,eq and <p>τ on any medium size (R<2m) tokamak, and highest QDT,eq/IaB or QDT,eq/R2B2 on any MFE device
0.54
0.32
P.B. Snyder/IAEA/October 2018
14
Sustainment and Core-Edge Compatibility of
Super H-Mode Regime
15
0
1
2
3
0
1
0
1
2
2000 2500 3000 3500 4000 4500
171322
Time (ms)
3
2
• High performance condition sustained by applying 3D magnetic perturbation – Controls density and impurity
accumulation – Feedback control of pedestal or
average density demonstrated – Sustained W~1.9MJ, QDT,eq~ 0.15, τ~0.2s, H98~1.6, βN ~ 2.9
– ~2s sustainment (hardware limited)
Super H-Mode Sustained Using 3D Magnetic Perturbations to Control Density and Impurity Accumulation
High sustained βN
Excellent confinementH98~1.6-2.5, τE~0.2-0.6s
Highest WMHD (~2.3-3.2MJ) since 2002Sustained WMHD~ 2 MJ
i-coil enables stationarydensity, pressure
WMHD
(MJ)
βN
H98
P.B. Snyder/IAEA/October 2018
16
• Super H (J-limited) solution predicted not to show degradation of pedestal pressure w/ ne,sep – P-limited solution degrades with increasing ne,ped
and ne,sep (eg high gas puff in JET ILW)
• Scan D2 gas rate, and introduce radiative impurities (N2) into the Div/SOL to test predictions on DIII-D – Use 3D magnetic perturbations (i-coil) to control particle and
impurity accumulation in core
– Use i-coil feedback to maintain ~constant density in pedestal & core as separatrix, divertor and SOL density are increased
• Test EPED predictions of sensitivity of pedestal to separatrix conditions
Connecting a High Performance Super H Pedestal & Core to a High Density, Radiative Divertor & SOL
3 4 5 6 7 8 9 10 11 120
5
10
15
20
25
30
35
Pedestal Density [ne,ped(Zeff/2)1/2,1019m-3]
Pede
stal
Pre
ssur
e [k
Pa]
Separatrix density half of pedestal (Bt=2.17T, Ip=1.6MA, tri=0.56)
EPED (H-Mode)EPED (Near Super H-Mode)EPED (Super H-Mode)
J-limited
P-limited
P.B. Snyder/IAEA/October 2018
17
• D2 gas scan in Super H mode experiment at Ip=2MA, Bt=2.1T. Gas rate varied ~30x – Pedestal pressure and τE remain ~fixed, high – i-coil feedback control of ne,ped ~ 7-8 1019 m-3
successful up to~110 torrL/s of D2 gas – Separatrix density rises from ~2.5 – 4 1019 m-3
– Strike point density rises from ~2.5 – 7 1019 m-3
D2 gas Scan Increases Separatrix and Divertor Density while Pedestal Pressure and Confinement Remain High
Both pedestal and separatrix density reach ITER values while maintaining high confinement and pped
P.B. Snyder/IAEA/October 2018
Super H-mode compatible with both high fusion performance and high separatrix density for
divertor solutions.
18
• Significant cooling with ~5MW of divertor radiated power using feedback on N2
– Peak Te near strike point drops more than 3x – Pedestal pressure and confinement remain
~constant – Future experiments needed to explore full
detachment and impact of closed divertor
N2 Injection Effective for Cooling Divertor while Maintaining High Performance Core & Pedestal
Outer divertor
0102030405060
0.99 1.00 1.01 1.02 1.03 1.04ψn,out
0
2
4
6
8
10
177018,2300−2600ms177018,3300−3600ms
T (eV)
n (10 m )
e
e19 -3
P.B. Snyder/IAEA/October 2018
19
Predictions for ITER, Implications for Compact, High Performance Fusion
20
Super H/NSH Regime Access is Predicted for ITER: DIII-D has Achieved Needed βN,ped, ne,sep, ne,ped Consistently
Open issue: Physics of the Greenwald density limit which constrains degree of Super H
access and predicted performance for ITER and DEMO concepts
• Core-pedestal simulations find ITER high performance (Q>10) at high ne [Meneghini16]
• DIII-D SH experiments reproduce many characteristics of the predicted ITER regime, including βN,ped~0.8, ne,sep~3-4, ne,ped~7-10. C-Mod produces pped~80 kPa
– Potential for substantial improvements in ITER performance, consistent with ne,sep
0 2 4 6 8 10 12 14 16 180
20
40
60
80
100
120
140
160
Pedestal Density * (Zeff/2)1/2 (1019 m-3)
Pede
stal
Pre
ssur
e (k
Pa)
EPED Predicted Pedestal Height vs Density for ITER Baseline
H-ModeNear Super HSuper H
P.B. Snyder/IAEA/October 2018
21
Super H and Near Super H Operation Enables Very High Fusion Performance per IpaBt
• Simple metric of fusion performance (Q or <p>W/P) per IpaBt – Colored points are observations (<p> > 50 kPa), red points are SH/NSH experiments – High Q/IaB enables ITER success, and compact, cost attractive pilot plant
Open issues: Challenges for Super H-mode operation include
sustainment, impurity control, and ELM control.
For JET and ITER, compatibility of strong shaping and nearby
metal walls
P.B. Snyder/IAEA/October 2018
0.0 0.5 1.0 1.5 2.0 2.5
0
5
10
15
Minor Radius (m)
Fu
sio
n P
erf
orm
an
ce
Me
tric
(<
p>
W/P
hIa
B)
ITER
DIII-D Super H
DIII-D H
C-Mod Super H
C-Mod H
JET H
TFTR L16MW
Q=5, 15MA
Q=10, 15MA
Q=10, 11MA
Q=inf, 15MA
2 atm
C-ModDIII-D
JET ITER
TFTR L-Mode
H-Mode
Super H-Mode/NSH
Q=inf, 11MA
22
• Theoretical prediction of Super H Mode has guided successful expts on C-Mod and DIII-D – Entering new era where theory can enable predictable, higher MFE performance
• Record pedestal pressures (~80 kPa) achieved in C-Mod SH experiments [Hughes NF18]
– Successful tests of EPED model up to ~90% of predicted ITER pped
• Record DIII-D fusion gain (QDT,eq~ 0.54, Q*DT,eq~ 1). QDT,eq/IaB ~ 0.21 and QDT,eq/(RB)2 ~ 0.04
• Projects (theoretically & empirically) to excellent ITER performance, compact attractive pilot plant
• High performance sustained w/ 3D magnetic perturbations to control ne and impurity accumulation (DIII-D: W~1.9MJ, QDT,eq~ 0.15, τ~0.2s, H98~1.6, βN ~ 2.9)
• High performance maintained with strong D2 gas puffing and N2 injection • Separatrix density reaches ITER values, divertor T reduced by ~3x
High Fusion Performance and Promising Core/Edge Solutions Developed via Super H Theory & Experiment
Super H-mode compatible with both high fusion performance and high separatrix density for divertor solutions. Projects to excellent
ITER performance and compact, attractive pilot plant
P.B. Snyder/IAEA/October 2018