Pedestals and Fluctuations in C-Mod Enhanced D α α α H-modes Presented by A.E.Hubbard With Contributions from R.L. Boivin, B.A. Carreras 1 , S. Gangadhara, R. Granetz, M. Greenwald, J. Hughes, I. Hutchinson, J. Irby, V. Klein 2 , B. LaBombard, Y. Lin, E. S. Marmar, A. Mazurenko, D. Mossessian, T. Sunn Pedersen 4 , M. Porkolab, J.A. Snipes, J. Terry, S. Wolfe, S. Wukitch, S. Zweben 3 and the Alcator C-Mod Group MIT Plasma Science and Fusion Center 1 Oak Ridge National Laboratory 2 Univ. New Mexico 3 Princeton Plasma Physics Laboratory 4 Columbia University Research supported by US. Dept. of Energy APS-DPP Meeting Quebec, Canada 23 October 2000
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C-Mod Enhanced D Pedestals and Fluctuations in H-modes · 2008. 9. 18. · • Weakly enhanced particle transport is seen in discharges near EDA boundary. • As QC mode strength
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Alcator
C-Mod
Pedestals and Fluctuations inC-Mod Enhanced Dαααα H-modes
Presented by A.E.HubbardWith Contributions from
R.L. Boivin, B.A. Carreras1, S. Gangadhara, R. Granetz, M. Greenwald,J. Hughes, I. Hutchinson, J. Irby, V. Klein2, B. LaBombard, Y. Lin,E. S. Marmar, A. Mazurenko, D. Mossessian, T. Sunn Pedersen4,
M. Porkolab, J.A. Snipes, J. Terry, S. Wolfe, S. Wukitch, S. Zweben3
and the Alcator C-Mod GroupMIT Plasma Science and Fusion Center
1Oak Ridge National Laboratory2Univ. New Mexico
3Princeton Plasma Physics Laboratory4Columbia University
Research supported by US. Dept. of Energy
APS-DPP MeetingQuebec, Canada23 October 2000
Alcator
C-Mod
Pedestals and Fluctuations inC-Mod Enhanced Dαααα H-modes
• Description of EDA H-Mode• Pedestals
– Profiles– Stability– Time evolution
• Quasi-coherent edge fluctuations• Conditions for achieving EDA• Possible physical mechanisms
Alcator
C-ModGlobal Features of EDA H-Mode
• EDA H-modes have:– good energy
confinement– Low particle
confinement– Low radiation– No large ELMs– Steady State (>8ττττE)
• Obtained with bothOhmic and RF heating,PRF<5 MW, W<240 kJ.
• Highly attractive reactorregime(no ELM erosion).
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High Resolution Diagnostics ofEdge Pedestals and Fluctuations
Scanning Langmuir probe
Scanning Langmuir probe
Top edge xray array
Outboard edge xray array
(38 chords, dZ=1.1 mm)
(38 chords, dR=1.5 mm)
Edge Thomson scattering(22 points, dZ=2.5 mm)
Helium beam
Reflectometer
(14 pts, dR=3 mm)
( 5 channels)ECE ( 9 & 19 channels){Edge bolo array
Edge vis. brem. array
(20 ch, dR=2 mm)
(dR=1 mm)
Lyman α(20 channels, dR=2 mm)
Phase Contrast Imaging (12 ch, dR=3mm)
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Pedestals are few mm wide, showdifferences in structure, position
• Density width 2-5 mm.• Steepest Te region
(~60 keV/m) few mm wide,Wider region with ~25 keV/m(2-3X core gradient).
• X-ray (impurity) pedestal attop of ne gradient, consistentwith neoclassical pinch.
• Only the impurity width issignificantly wider in EDA vsELM-free; Te, ne pedestalsshow little difference.
• Only impurity width getsnarrower at high Ip.
Temperature
Density
Emissivity
J. W. Hughes UP1.095Thurs. am.
Alcator
C-ModEdge Gradients Challenge MHD Limit
• Edge electron profiles fromhigh resolution Thomsonscattering– assume Ti = Te
• Modeling shows gradients are~30% above the first stabilityballooning limit with onlyohmic current.– Edge bootstrap current
increases stability limit• No Type I ELMs
(PRF≤≤≤≤5 MW, P′≤′≤′≤′≤12 MPa/m)– Small ELMs when βN≥1.2
Major Radius (m)
Te
ne
Plasma Pressure (kPa)
dP/dR (MPa/m)
LCFS
n e (1
020
m-3
)
T e (k
eV)
Pres
sure
(kPa
)P'
(MPa
/m)
D. MossessianUP1.096 Thurs. am.
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Time evolution of Te, ne pedestalsstudied using power ramps
• RF input power continuouslyvariable, ramped slowly upand down.
• Te, ne measured with ms timeresolution by ECE,bremsstrahlung array.
• Strong hysteresis in net P.• H-mode threshold in Tedge is
found.• Te pedestal varies in height
and width with P• ne pedestal independent of P
(above LH threshold).
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Transients at LH transition consistentwith sudden drop of χ in pedestal
• Rate of increase is largestnear top of pedestal.dwped/dt requires ‘blocking’most of the heat flux Q.
• No time delays in pedestalregion, within ms resolution.
• Transients in core are slower,appear diffusive.
• Contributions of n, T arecomparable at moderate ne.
• wped(t)~ t1/2 , well fit by powerbalance analysis.
( ) ( ) ( )( )1/ 2 1/ 2
/0
χ χπ χ χ χ
−= +
+A b
ped pedb A A
Q Aw t w t
B. Carreras
R/a=0.86
Alcator
C-ModAt lower density, Te rise dominates
• Density rise is smaller.Measured neutral ionizationrate also ~10x lower.
• Te pedestal higher (900 eV)• Discharge is ELM-free• Pressure rise about the
same, still fit by the sametransport model, χ s.
• At even lower ne, no densitypedestal is formed and theH-mode is not sustained.This might be part of thereason for the ‘low densitylimit’
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Quasi-Coherent Mode seen in DensityFluctuations in EDA H-modes
• Seen with both favorable andunfavorable drift direction.
Alcator
C-ModHigher density at L-H favours EDA
Low density, ELM-free Higher density, EDA
•Actual threshold may be in neutral density, local ne or gradient orcollisionality (all are correlated; ν*ped < 1 at low ne, 5-10 at high ne)
• 1.2×1020 m-3 quite low for C-mod. ~0.15 nGW , low ne limit ~0.9 ×1020
enen
αDαD
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A Continuum of QC Mode Amplitude,EDA Particle Transport is seen
• ELM-free to EDA transitioncan be progressive(unlike the L-H transition).
• Weakly enhanced particletransport is seen indischarges near EDAboundary.
• As QC mode strengthincreases:– Rate of rise of ne drops
(more steady state,Deff increasing).
– X-ray ped width (~Dimp)increases.
• Similar trends have beenseen in scans of q, δ.
EF steady EDA
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Comparison with other‘small ELM’ regimes
EDA H-mode shares some characteristics of other steadyregimes without large ELMS.
• Low Particle Confinement regime on JET– Appears similar to EDA, but not easily reproduced.
• Quasi-coherent Fluctuations on PDX– Fluctuations similar to those in EDA, present in short bursts in
most H-modes. Coexisted with ELMs.• Type II or Grassy ELMs on DIII-D, JT60U, Asdex UG
– Conditions in q, δ=very similar to EDA– Similar to small ELMs seen in EDA at high βN?– Does a quasi-coherent mode play a role in these regimes?
• Quiescent H-Mode on DIII-D– Globally similar, but longer wavelength mode, different access
conditions (esp density/neutrals).
Loarte, Snipes et alDO1.004, Mon. pm.
Alcator
C-ModPhysical origin of EDA, fluctuations
• Since pedestal profiles are not much different in EDA, ELM-free H-modes, it seems likely to be the mode stability criteria whichchange with q,δ, ν* etc.
• One possibility is that EDA is related to drift ballooning turbulence.Diamagnetic stabilization threshold scales as m1/2/q.A lower q threshold wasfound for EDA in H than D.
• Initial scalings of QC mode characteristics show
• Electromagnetic edge turbulence simulations by Rogers et al haveshown a feature similar to QC mode, with .Gyrokinetic simulations of growth rates (GS2 code) are in progress.