active control of mhdinstabilitiy 2002/11/19 s.ohdachi et.al. sawtooth-like phenomena in lhd s....
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Active Control of MHDinstabilitiy 2002/11/19 S.Ohdachi et.al.
Sawtooth-like phenomena in LHD
S. Ohdachi, S.Yamamoto, K. Toi, K. Y.Watanabe, S.Sakakibara, H. Yamada, LHD Exp.Group
Active Control of MHDinstabilitiy 2002/11/19 S.Ohdachi et.al.
Outline
• MHD stability in LHD.• Sawtooth activities in high density plas
ma with pellet injection.• Observations with a tangentially viewing
SX camera.• Edge activities in inward shifted plasma
s.
Active Control of MHDinstabilitiy 2002/11/19 S.Ohdachi et.al.
Large Helical Device(LHD)
VacuumVessel
Helical Coil
Poloidal Coil
L = 2, m=10 Heliotron type device R = 3.5 - 3.9m, a ~ 0.6m Bt = 0.5 – 2.8 TNBI ~ 9MW, ICH~2.5MW, ECH~1.9MW Te < 10keV, Ti < 5keV
Best performance of plasma can be produced with Rax = 3.6m configuration where anomalous/neo-classical transports are improved.
Superconducting coil system
Active Control of MHDinstabilitiy 2002/11/19 S.Ohdachi et.al.
MHD stability and Magnetic Axis Position
• In inward shifted plasma (Rax = 3.6m), magnetic hill region is wider.
• Magnetic well region extend as the beta increases.
• We have rational surfaces, = n/m = (1/2), 2/3, 1/1, 4/3, 3/2, in the hill region at ~ 1%(3.6m).
• P=P0(1-8)2 is assumed.
Active Control of MHDinstabilitiy 2002/11/19 S.Ohdachi et.al.
Coherent Modes in inward-shifted plasmas
• Operation with Mercier Unstable conditions. (Rax = 3.53m 3.6m)
• Many coherent modes are simultaneously observed. (broad density profile)
• However, they do not affect the confinement so much.
• There are several case where MHD instabilities lead to sawtooth-like collapse.
Active Control of MHDinstabilitiy 2002/11/19 S.Ohdachi et.al.
Operation Regime
• Sawtooth-like events are observed in the high-density with pellet injection.
Pellet
0 2 4 6 8 10 12 140
250
500
750
1000
1250
Wp [kJ]
ne [ 1019 m-3 ]
Active Control of MHDinstabilitiy 2002/11/19 S.Ohdachi et.al.
Sawtooth-like activitySatooth-like activities are observed in pellet injected high-density plasmas.
While the electron density decreases after pellet injection the electron pressure profile become peaked gradually.
Sawtooth activities around i = 1/2 surface can be seen.
Active Control of MHDinstabilitiy 2002/11/19 S.Ohdachi et.al.
Inversion radius and profile
• Difference between before and after are shown.
• Inversion radius is around = 1/2.
Active Control of MHDinstabilitiy 2002/11/19 S.Ohdachi et.al.
Pressure gradient and Magnetic shear
Small change in iota profile(10kA).
Shear at the rational surface is affected.
Active Control of MHDinstabilitiy 2002/11/19 S.Ohdachi et.al.
Electron temperature profile with/without sawtooth activitiy
• With ST activities, the electron temperature profile becomes flat.
Active Control of MHDinstabilitiy 2002/11/19 S.Ohdachi et.al.
Fluctuation with ST
• Fluctuations are analyzed by SVD.
• Slightly inside the inversion radius, m=2 oscillations are seen. Its amplitude decreases with ST crash.
• Heat pulse triggered by ST crash excite edge mode with m/n = 1/1.
Active Control of MHDinstabilitiy 2002/11/19 S.Ohdachi et.al.
Sawtooth observed by a fast framing tangentially viewing SX camera
Two dimensional image with a framing rate of 4.5kHz can be measured with this system without complicated tomographic reconstruction.
Sample Image
Framing rate4.5kHz(256x256)13.5kHz(128x128)
Response of phosphor is fast enough ( s order).
Active Control of MHDinstabilitiy 2002/11/19 S.Ohdachi et.al.
Energy flow with ST crash
• Energy flow seems to be isotropic.
Active Control of MHDinstabilitiy 2002/11/19 S.Ohdachi et.al.
Core Fluctuations with Rax = 3.53m
• In Rax=3.53 another collapse are found with lower beta plasma. In this case, energy flow is m=2 nature.
31083.mov
Active Control of MHDinstabilitiy 2002/11/19 S.Ohdachi et.al.
SVD component• #4-5 component
represent represent m=2 rotation mode. (r=0.5 Dr=0.1)
• Exhaust from the core region can be seen in .#3 component, which synchronizes with the m=2 rotation.
• We are trying to find out the detailed structure like this event, at ST-crash with faster camera.
Active Control of MHDinstabilitiy 2002/11/19 S.Ohdachi et.al.
= 4/3 and 1/1• In further inward shifted plas
ma, Rax = 3.53 and 3.6m, collapse events in the peripheral region also can be seen.
• The effect on the plasma performance, e.g., the stored energy is larger.
Active Control of MHDinstabilitiy 2002/11/19 S.Ohdachi et.al.
Summary 1
• Sawtooth-like events observed in LHD is similar to the sawtooth in tokamks.
• It is localized on = 1/2 surface with revered shear (tokamaks).
• When pressure gradient exceed the limit, activities are exited. Critical pressure gradient are affected by the local magnetic shear.
Active Control of MHDinstabilitiy 2002/11/19 S.Ohdachi et.al.
Summary 2
• One events takes ms order. Slower than tokamak sawtooth.
• Energy flow at the events seems to be isotropic.
• Events at various rational surface can be observed in inward-shifted plasma with Mercier unstable conditions.
Active Control of MHDinstabilitiy 2002/11/19 S.Ohdachi et.al.
Sawtooth and pre/post Cursor• m=2 pre/post curs
or can be seen in SX fluctuations.
• In high beta discharges (Bt = 1.3, 1.5T),
magnetic flucutuations with n/m = 1/2
syncronized with SX fluctuations are observed.