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ELMs / LLD

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The (apparent) extreme efficacy of Li aerosol at increasing confinement. The extremely 'square' Te and ne profiles seen during the NBI overdriven L-H transition ... – PowerPoint PPT presentation

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Title: ELMs / LLD


1
The Two Types of Discharges in XP-913
ELMs / LLD
Standard Fiducial
2
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3
Six Interesting Features from XP-828
  • The (apparent) extreme efficacy of Li aerosol at
    increasing confinement
  • The extremely square Te and ne profiles seen
    during the NBI overdriven L-H transition
  • The reduced OH consumption during aerosol
    injection
  • The transient suppression of ELMs
  • The concomitant reduction in radiated power /
    Zeff
  • The lack of CS gas fuelling

4
Standard Fiducial
Baseline XP-913
Baseline XP-913 No CS Gas
5
Standard Fiducial
Baseline XP-913
129012
130388
LFS
CS
Li Flux
Baseline XP-913 (No CS Gas)
130389
Flux Profile A
Li Flux
6
Flux Profile B
Flux Profile C
Li Flux
7
Shot 121522 A Discharge Used to Deposit Li on
the CS for the Benefit of the
Following Discharge
30 ms
250 ms
500 ms
600 ms
8
Another Tactic for Directing Li Ions - In This
Case to the Lower Divertor
Example Shot 128279
9
Extra Slides
10
Comparison Zeff(0) from Metals
No Li 700 mg LITER 7mg Early Li Aerosol
Estimated Contribution of Metals to Zeff
0.6
LITER
0.4
Dimensionless
Aerosol Injection
0.2
No Li
0
0
0.2
0.4
0.6
0.8
S. Paul
Time (sec)
11
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12
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13
Goal(s) of the XP
  • Establish whether or not the 1st aerosol
    experiment was a fluke.
  • Fiducials H mode by early NBI overdrive - no
    CS gas
  • Early aerosol injection before L-to-H
    transition
  • 10 mg/s and higher probe the limit of
    Li aerosol mass flux
  • Push plasma performance
  • If problems try OH shot or two
  • -------------------------- If time permits
    ------------------------------------
  • 2. Investigate effects on ELMs.
  • Can aerosol trigger small ELMs at higher flux
    rates (gt35mg/s)?
  • 3. Investigate whether more Li atoms can be
    injected than D2 atoms.
  • LLD loading - need relevant discharge
  • 4. Investigate Li efficacy with double null
    discharges

14
Shot 130388 Early Injection of Li Powder
  • Nominal aerosol trajectories shown by red
    vertical lines

Plasma Encounters Aerosol Particles
X-Point Established (H-mode _at_ 180 ms)
Stored Energy Steady State
Li1 Rings Observed (Fig 12)
25 ms
509 ms
102 ms
80 ms
58 ms
15
2005 First LSN NBI D Shot After 25 mg of Li
Pellet Injection Exhibited Factor 50 Decrease
in Density
Lower single-null divertor discharges, 0.45T, D2
gas fueling 3.5mg
  • 25 mg of Li pumping of edge density saturated
    after the 3 similar D discharges and returned to
    pre-Li wall conditions, as expected if most
    injected gas reacts with the deposited Li.
  • Rate of density rise is below NBI fueling rate.

H. Kugel M. Bell
16
Camera View of Early Li Aerosol InjectionTaken
at t 60 ms
17
The Subtle Difference Between 130386 and 130389
130386 _at_ 85 ms No Li
130389 _at_85 ms Early Powder
18
Why a Double Null Discharge Would be Interesting
Powder Injector
Li Ions Head Preferentially for Upper Strike
Points
19
Getting Toward the Center Stack ( or LLD) -
Early (Using a Splash Plate)
45 Deg Inverted Spoon
45 Deg Flat Plate
Present Design
Flat Plate LLD
20
Aerosol Injection
10 mg/s
21
Aerosol Injection
10 mg/s
22
Early Powder Injection
23
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24
Early Li 2 sec shot
25
Li Has Unique Energy Structure Easy to Create
Li1
Can We Exploit This to Save Early Volt Secs ?
H He Li Be B C N O
13.6 24.6 5.39 9.32 8.30 11.3 14.5 13.6
54.4 76.6 18.2 25.1 24.4 29.6 35.1
123 154 37.9 47.9 47.4 54.9
1
Ionization Energy (eV)
2
3
26
Shot 121522
30 ms
250 ms
500 ms
600 ms
27
Shot 123862
30 ms
250 ms
500 ms
800 ms
28
(No Transcript)
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