Magnetic islands with complex structure in NSTX K. L. Wong PPPL and the NSTX Research Team 53 rd...
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Transcript of Magnetic islands with complex structure in NSTX K. L. Wong PPPL and the NSTX Research Team 53 rd...
Magnetic islands with complex structure in NSTX
K. L. Wong
PPPL
and the NSTX Research Team
53rd APS-DPP annual meeting at Salt Lake City-UT
November 14-18, 2011
College W&MColorado Sch MinesColumbia UComp-XGeneral AtomicsINELJohns Hopkins ULANLLLNLLodestarMITNova PhotonicsNew York UOld Dominion UORNLPPPLPSIPrinceton USNLThink Tank, Inc.UC DavisUC IrvineUCLAUCSDU ColoradoU MarylandU RochesterU WashingtonU Wisconsin
Culham Sci CtrU St. Andrews
York UChubu UFukui U
Hiroshima UHyogo UKyoto U
Kyushu UKyushu Tokai U
NIFSNiigata UU Tokyo
JAEAHebrew UIoffe Inst
RRC Kurchatov InstTRINITI
KBSIKAIST
POSTECHASIPP
ENEA, FrascatiCEA, Cadarache
IPP, JülichIPP, Garching
ASCR, Czech RepU Quebec
NSTXNSTX Supported by
NSTXNSTX Meeting name – abbreviated presentation title (last name) Month day, 20** 2
NSTX plasmas are rich in MHD activities
• Alfvén Eigenmodes: 100 kHz – 2 MHz• Kink, tearing and ballooning modes: 1 – 100 kHz• Resistive wall modes < 1 kHz• Locked modes (due to tearing or RW modes) f 0• Typical Mirnov signal
NSTXNSTX Meeting name – abbreviated presentation title (last name) Month day, 20**
Low frequency multiple harmonic oscillations (MHO)#138326: Ip=0.8MA H-mode, Pb=2MW, Prf=0.9MW turned on at 0.25s
Mirnov signal: fn ~ n Δf ~ n f1
Island identified by a flat region in fΦ is rotating with fΦ ~ 20 kHz ~ Δf
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NSTXNSTX Meeting name – abbreviated presentation title (last name) Month day, 20**
Doppler shift: ω’ = ω + k.V = ω + kϕVϕ= ω + nVϕ/R
This relation was used to determine the
toroidal mode number n of TAEs in TFTR
Ref: Wong et al, PPCF(1994)
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For low-n tearing modes, ω << ω’ ~ nVϕ/R
Let B =m,n bmn exp[i(m+n)]
If an island localized at q=m/n has
multiple toroidal mode numbers,
then the island observed in the lab
should have multiple harmonic
frequencies with fn = n fϕ
Resonance condition: m/n=q
Multiple n multiple m
Large m => corrugated island surface/
irregular boundary in Poincaré plot
NSTXNSTX Meeting name – abbreviated presentation title (last name) Month day, 20**
Most likely scenario in #138326: Prf turned on at 0.25s & form 1/1 island enhanced transport (or sawtooth crash?) between 0.2817-0.2983s during MHO
RF turned on at 0.25s, ELMy H-mode,
Wmhd & neutron rate level off after 0.3s
- enhanced transport due to MHO
(no broadband noise in Mirnov signal)
Te in core drops between
0.2817 – 0.2983s
5
NSTXNSTX Meeting name – abbreviated presentation title (last name) Month day, 20**
Stochastic magnetic field near separatrix of an island
Stochastic B during sawtooth crash
- due to the overlap for second order
island chains (action-angle variables)Ref: Lichtenberg et al., Nucl. Fusion (1992)
Express the perturbed B in Fourier series:
B =m,n bmn exp[i(m+n)]
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When the island has many m, n
harmonics, we can also expect a
larger region of multiple stochastic
layers and separatrix.
NSTXNSTX Meeting name – abbreviated presentation title (last name) Month day, 20**
Island at q = 2 near r~0 (from MSE) after RF turned off#130608: 1MA, Pb=2MW, Prf~1.8MW tripped off by an ELM –TRANSP130608Z10
Δf~22kHz at 0.386s,
droops to 12kHz at 0.4s
RF tripped off by an ELM at 0.376s,
Then Wmhd & neutron rate drop
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NSTXNSTX Meeting name – abbreviated presentation title (last name) Month day, 20**
Island fΦ approx. corresponds to Δf in Mirnov signal
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NSTXNSTX Meeting name – abbreviated presentation title (last name) Month day, 20**
MHOs enhance plasma energy transport
Grad.Te reduced in plasma core (r/a<0.6)
after MHOs appear
Grad.Ti reduced in plasma core (r/a<0.6)
after MHOs appear
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NSTXNSTX Meeting name – abbreviated presentation title (last name) Month day, 20**
MHO during RF flat-top#[email protected], Ip=1MA, Pb~2MW, Prf~1.9MW,
There was an ELM just before 0.4s that may triggered the MHO
Prf & Pb remained constant in 0.4-0.44s
At t=0.406s, only 1 island @ q~1, 30kHz
At t=0.416s, another island @ q~2, 16 kHz
m/n = 2/1, 4/2, 6/3, 8/4 . . . .
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NSTXNSTX Meeting name – abbreviated presentation title (last name) Month day, 20**
MHO with rising freq after Prf switched off (#138143)
Prf turned off at 0.46s. An island
appears at R>130cm & grows in size
and rotation speed. Te(r) falls when
island gets large (after 0.5s)
11
NSTXNSTX Meeting name – abbreviated presentation title (last name) Month day, 20**
Combination of several sets of MHOs at different regions
At 0.37s, several sets of MHOs appear at the same time with different Δf: fϕ slowing down in plasma core & spinning up at plasma edge
Several islands at different regions overlap – avalanche : severe deterioration of global plasma confinement – big drop in stored energy & neutron emission
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NSTXNSTX Meeting name – abbreviated presentation title (last name) Month day, 20**
MHO near edge (q~4) developed into locked mode#129169: Ip=1MA, Pb=2MW, Prf=1.2MW, L-mode edge
Rapid MHD growth at 0.27s,
RF tripped off at 0.28s,
Locked mode ( f ~ 0 ) at 0.293s
13
NSTXNSTX Meeting name – abbreviated presentation title (last name) Month day, 20**
Change of fΦ(R) due to MHO (0.27s - 0.29s)plasma core has reversed magnetic shear before 0.27s
fΦ(R) from TRANSP: 0.2s< t <0.3s
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NSTXNSTX Meeting name – abbreviated presentation title (last name) Month day, 20**
fΦ pedestal outside region of reversed magnetic shearfΦ and q measured with 10ms resolution
ΩΦ(R) changes slowly from .27-.29s :
ΩΦ pedestal in region with positive magnetic shear reversed magnetic shear improves momentum confinement
Sudden change of q(R) at .27s :Appearance of MHOs coincides with q(0) collapse (from 3.0 to 1.2)
- double tearing modes at 0.27s?
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NSTXNSTX Meeting name – abbreviated presentation title (last name) Month day, 20**
Enhanced momentum & edge electron energy transportdue to locked mode
Grad ΩΦ(r/a:.4-.9) at .27s, .28s, .29s, .3s : falls with time after locked mode appears
Grad Te(r/a:.6-1) at .27s, .28s, .29s, .3s :
falls with time at plasma edge (r/a>0.85) due to edge cooling at r/a>0.8
16
NSTXNSTX Meeting name – abbreviated presentation title (last name) Month day, 20**
Enhanced core impurity transport & edge cooling due to MHOs MHOs at edge have similar effect as EHOs in DIII-D QH-mode plasmas
Te drops at r/a>0.8 during MHO
During MHO :
Zeff increases at r/a>0.8 , and
decreases at r/a<0.8
17
NSTXNSTX Meeting name – abbreviated presentation title (last name) Month day, 20**
Relevance to conventional tokamak experiments
Quiescent H-mode in D3D
- edge harmonic oscillations
- are these MHOs at plasma edge
that work as ergodic divertor ?
Current ribbon at q=4 in JET- Can be constructed by choosing bmn
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NSTXNSTX Meeting name – abbreviated presentation title (last name) Month day, 20**
Why no MHOs in the core of conventional tokamaks?
• δB from unstable tearing
modes resonate at q=m/n to
form magnetic islands.
• Microtearing modes are
unstable from core to edge in
NSTX beam heated plasmas
MHOs from core to edge.
• They are stable in core of
conventional tokamaks
No MHOs in core.
• Microtearing modes can exist in
edge region of conventional
tokamaks.
Conjecture :
• When they appear at edge of
DIIID at quasi steady state
EHOs which reduce Zeff
QH-mode.
• When they appear at edge of
JET current ribbon.
19
NSTXNSTX Meeting name – abbreviated presentation title (last name) Month day, 20**
Multiple harmonics in high-k scattering dataThese data are rare : It requires a big island, and the scattering volume must be at the right place
nth harmonic of island rotating at fϕ produces EM fields in plasma with fn = n fϕ and the plasma will
respond at the same freq fn = n fϕ : Oscillations need not be normal mode - D(ω,k)~0
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NSTXNSTX Meeting name – abbreviated presentation title (last name) Month day, 20**
Summary
MHOs are common in NSTX
• It can happen under many different
plasma conditions.
• It is associated with a rotating
magnetic island with complex
structure - multiple helicity.
• The island location varies from
core to edge.
• They can produce stochastic B and
enhance plasma transport.
• Can cause multiple peaks in high-k
scattering signal.
Is this a special feature of ST?
• The cause for this behavior in NSTX
may be due to microtearing modes.
• Microtearing modes in NSTX beam-
heated plasmas can be unstable
from core to edge, but only at the
edge in conventional tokamaks.
• EHOs in DIII-D QH-mode may be a
rotation island with multiple helicity
at the plasma edge. Appropriate
values of bmn at q=4 can lead to
current ribbon in JET.
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