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Some recent PPCD results in MST

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time 10's of ms. Recent x-ray tomography confirms Te(core) 1 keV ... Many questions and challenges, e.g., how high can we push Ti? ... – PowerPoint PPT presentation

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Title: Some recent PPCD results in MST


1
Some recent PPCDresults in MST
  • B. Chapman for the MST group
  • and collaborators

2
Introduction
  • Large fraction of the PPCD gain in b and tE due
    to increased Te
  • Ti usually changes very little
  • Ion heating during PPCD believed small
  • Recent MST improvements have allowed increased Ip
  • PPCD at 575 kA exhibits large Ti
  • Most data in this talk from 575 kA plasmas

3
(Re)introduction to PPCD
  • b(core)/B 0.2
  • b(n 9-15) PPCD-like from 10-12 ms

at plasma surface
m 1 n 7-15
m 0 n 1-4
central chord
central chord
4
HXR emitted over plasma core
  • Integrated over PPCD duration

5
From previous measurements, Te grew large, Te gtgt
Ti
  • Te(0) from x-ray data
  • Ti(0) from CHERS, CVII
  • Ion heating small?
  • Electron-ion equil. time 10s of ms

6
Recent x-ray tomography confirms Te(core) 1 keV
  • Double filter technique (Be filters of 478 and
    140 mm)
  • Believed to be underestimate

7
Recent PPCD plasmas exhibit Ti(0) gt 1 keV
  • CHERS trustworthy up to 2 keV
  • Likely that Ti gtgt Te early in PPCD
  • Neutron count spikes at crash

sawtooth crash
m 1 m 0
from CHERS
8
Neutron detector schematic
9
Otherwise similar PPCD shots exhibit different
Ti(0)
  • ltnegt 9x1018 m-3
  • Te might be higher perhaps due to ion-electron
    coupling?

previous shot comparison shot
10
Ti(deuterons) Ti(impurities)
  • Ion-ion equilibration time 100 ms

Rutherford scattering CHERS
11
Why is Ti higher in some PPCD plasmas?
  • PPCD directly responsible for increased Te
  • PPCD apparently not responsible for increased Ti
  • Ti large, or not, before PPCD begins

12
Ion heating occurs early and strongly in the core
Ip starts ramping up at t 0
Reversal parameter
Crashes
  • Ion heating linked to
  • m 0 instability

13
Heating occurs early and strongly in the edge as
well
Crashes
  • Globally, estimate 10s
  • of MW of ion heating,
  • over a few 100 ms

14
Ingredient(s) for hot-ion PPCD?
  • Large heating during startup, during and maybe
    between crashes (Ti normally falls off rapidly
    between crashes)
  • Large Ip sometimes leads to larger crash
    heating
  • But not all large-Ip shots have large startup Ti
    -- why?
  • Partial answer heating varies from crash to
    crash
  • While PPCD does not cause large Ti, it may help
    to confine large Ti

15
Could this possibly be useful for the future
(reactor...)?
  • Pre-PPCD heating fine for now, but not as
    important for, e.g., substantially longer pulse
    PPCD (Ti will gradually decay)
  • What about during PPCD?
  • Short, controlled mode destabilization (impulsive
    heating)
  • Avoid substantial confinement degradation? like
    ELMing H-mode
  • During low-b period
  • Mostly edge modes
  • SXR change is small
  • Maybe a slight gain?
  • But whats Ti(r) doing?

16
Some plans for/related to PPCD
  • PPCD upgrade (longer, different PPCD waveform) --
    next week
  • Test our ability to generate reliably and confine
    large Ti
  • Large Ti could be important boost for planned
    higher-ne PPCD
  • Programmable Bt power supply
  • Arbitrary PPCD waveform
  • May allow higher Ip
  • Multipoint CHERS single-shot profile measurement
  • Final commissioning of multipoint Thomson
    scattering
  • X-ray tomography Te(r,t) measurement

17
Summary/conclusions
  • RFP plasma can contain Te and Ti gt 1 keV
  • Large Ti implies improvement in b, and maybe tE
  • Case of RFP reconnection contributing to fusion
    goal
  • Many questions and challenges, e.g., how high can
    we push Ti?
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