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XP407: Passive Stabilization Physics of the RWM in High b N ST Plasmas – 4/13/04. Goals Define RWM stability boundary in (V f , b N ) space Use past XP experience and new theories to determine boundary Present theory and NSTX data suggests: W crit / w A ~ 1/4q 2 - PowerPoint PPT Presentation
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NSTX S. A. Sabbagh
XP407: Passive Stabilization Physics of the RWM in High N ST Plasmas – 4/13/04
Goals Define RWM stability boundary in (V, N) space
• Use past XP experience and new theories to determine boundary Present theory and NSTX data suggests: crit/A ~ 1/4q2
• Define the operating space and criteria for active stabilization Measure n > 1 resistive wall modes
• Present high N plasmas are computed to be n = 2 unstable
• Compare to theoretical computation of n > 1 stability (structure?)
• Look for finite mode frequency Set up conditions to examine physics of RWM passive
stabilization in high N ST plasmas to compare to theory
• Critical rotation frequency: XP by A. Sontag
• Rotation damping physics: XP408 by W. Zhu
NSTX S. A. Sabbagh
Stability boundary probed and modes observed q and pressure peaking variation were main techniques
q variation through slow Bt reduction
Bt reduction placed discharge in stabilized high /A region
Bt reduction yielded variation of pressure peaking
Low frequency 370Hz mode observed before mode lock Global collapse in rotation profile observed as in past RWM XPs
High targets reached at high toroidal rotation speed /A = 0.48; N = 6.7 (highest value at constant Ip); t = 38%
New diagnostic capabilities used to measure RWM Internal locked mode sensor array shows n=1 ~ 10-20G; n=2 ~ 5G 51 channel, 10 ms resolution CHERS yields unprecedented detail
• detail of global rotation collapse
USXR data taken at two toroidal positions (not yet examined)
NSTX S. A. Sabbagh
Past experiments show crit depends on q
Chu/Bondeson critical rotation crit/A = 1/(4q2) applies across the profile in CY02 plasmas
/
A
q1 2 3 4 5
0.0
0.1
0.2
0.3
0.41084201076361/(4q2)
(a)
stabilized region
1/(4q2)
0.27 s0.29 s0.31 s0.33 s0.35 s
108197
/
A
0.1
0.2
0.3
0.4
q1 2 3 4 5
0.0
(b)
NSTX S. A. Sabbagh
Approaches to probing (V, N) stability boundary
Rapidly drive across increasing growth rate contours This is the standard approach
Destabilize RWM by increasing crit
Decrease Bt slowly in stable discharge
Stabilize RWM once triggered Decrease crit by increasing Bt slowly in unstable discharge
NBI step-down after destabilization
Drop out of H mode with N >> NNo-wall
Vary timing of NBI and Bt variation to change position in (V, N ) space
NSTX S. A. Sabbagh
Schematic approach to probing stability boundary
Technique 3 was most extensively used Technique 4 occurred as pressure peaking increased at lower Bt
N
/A
Unstable
UnstableN wall
N no-wall
decreased qincreased q
1
2
3
4 drop N no-wall
NSTX S. A. Sabbagh
XP407 Passive RWM - Waveforms: 4/13/04
Aspect ratio in 110184 increased in time – vary A in similar way
6
0 0.1 0.2 0.3 0.4 0.50
0.5
1.0
X10
Am
ps
2
4
6
(arb
)
Time (Seconds)
Source B
Source C (start with this source delayed)
Default NBI timing
Plasma current
0 0.1 0.2 0.3 0.4 0.50
Source A
4.5
Run NBI at max power
0.6 0.7
0.6 0.7
Use setup shot 111957 LSN
4.0
3.5
Toroidal field
Optional delayed Ip ramp
NSTX S. A. Sabbagh
XP407 Passive RWM - Run plan: 4/13/04 Scan boundary of passive stabilization space (F, N)
Task Number of Shots
A) Restore shot 111957, ~ 2.1 LSN (or newer similar target)
(Ip ramped to 0.9 MA Bt = 4.4 kG (or above), =2.1, li ~ 0.65)
(i) 3 NBI sources (rerun 111957 with 3rd source at t = 0.4s) 1
(ii) 2 NBI + delayed 1 NBI if collapse occurs before 0.5 s 2
B) Use toroidal field ramp to influence rotation evolution
(i) Bt = 4.4 kG, reduced to Bt = 3.5 kG, vary start time of ramp 3
(ii) Bt = 4.4 kG, reduced to Bt ~ 4.0 kG, vary start time of ramp 3
(iii) choose best Bt ramp, vary start time (2 or 3 unique times)4
(iv) Bt ~ 4.0 kG, reproduce collapse time, ramp Bt up to delay crash 4
C) Vary NBI timing to best cover (F, N) space
(i) 3 NBI sources with source step-down / vary TS laser timing 5
D) Take plasma out of H-mode (ramp PF2) for high N / NNo-wall 4
Total shots: 26
NSTX S. A. Sabbagh
RWM mode locking and slow phase rotation observed
Low frequency ~ 440Hz precursor to mode lock
Mode locks at t=0.49s Rotating modes (typically
islands) are clearly rotating at this time
Very slow rotation of n=1 phase observed after lock Apparent f ~ 50 Hz
NSTX S. A. Sabbagh
Global rotation collapse when core n=1 is triggered
Global rotation collapse when core n=1 is triggered n=1 RWM appears to trigger core n=1 mode RWM locks at least 30 ms before islands eventually lock
No apparent momentum transfer, which would be observed if braking were due to electromagnetic torque at island
rotation profile evolution
Radius (cm)
rapid globalcollapse
440 Hz odd-nobserved
core n=1 triggered,RWM locked
V = 1kHz (> 440 Hz)
PRELIMINARY
NSTX S. A. Sabbagh
Slower collapse – RWM near marginal stability?
RWM rotation frequency ~ 370 Hz in this case Mode locks/unlocks before plasma rotation terminates
Momentum transfer across rational surface observed before insland lock at 0.51s RWM “marginally stable” near 0.5s, collapses plasma again and locks at 0.52s
rotation profile evolution
Radius (cm)
PRELIMINARY
370 Hz odd-nobserved
core n=1 triggered,RWM locks