Alcator C-Mod Run 1000915 Information

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Miniproposals
Miniproposal:276
Date Filed: 6/1/2000
Title:Transport Experiments in the Scrape-Off Layer during Ohmic L- andH-mode using Gas-Injection Plumes
First Author:Sanjay Gangadhara
Session Leader:Brian Labombard (shots 1-29)
Session Leader:Sanjay Gangadhara (shots 1-29)

Operators
Session leader(s):Brian Labombard,Sanjay Gangadhara
Physics operator(s):Joseph Snipes
Engineering operator(s):Bill Parkin,Gary Dekow

Engineering Operator Run Comment
MP 276 Transport Experiment SL:Gangadhara/LaBomvard PO:Snipes EO:Dekow/P

Session Leader Plans

Physics Operators Plans

Session Leader Summaries
Entered: Jul 7 2004 03:49:24:883PM
Author: To Be Determined
Run Plan and Engineering setup for 1000915

MP276 Transport Experiments in the Scrape-Off Layer during
Ohmic L- and H-mode using Gas-Injection Plumes

Session Leader: S. Gangadhara/B. LaBombard
Physics Operator: J. Snipes

Engineering setup for Friday, 15 September 2000:

Overnight ECDC in Detuterium, stopping 1-2 hours prior to the run.

Run begins at 9:00 and ends at 17:00.

Power system setup as on 1000829018

Gas setup - fill B-top with 6 psi of D2 Hybrid enabled
fill B-side lower with 1 psi of Ar Hybrid enabled
fill B-side upper with 35 psi of He Hybrid DISABLED (Yes, HELIUM)
(available for between-shot ECDC)
fill C-side with 30 psi of D2 Hybrid enabled
leave J-bottom as is Hybrid DISABLED

The following gate valves should be enabled, assuming no vacuum problems:
ECE, VUV
--------------------------------------------------------------------------------

Impurity transport in the scrape-off layer (SOL) is of fundamental
importance in tokamak plasmas. It is clear that the physical processes
involved must be fully characterized and understood in order to
predict core impurity levels in future tokamak reactors. A direct
means of inferring information about impurity transport in the edge
plasma is to inject impurities locally into the SOL through the
``fast-burping'' probe and study the resultant impurity dispersal
patterns (``plumes''). Plumes can yield information about local
parallel and cross-field transport in the edge, as well as information
about local electric field structure.

Experiments will be conducted using deuterated ethylene (C2D4) as the
injected gas, with typically ~ 5 x 10^16 molecules of gas injected per
probe scan. C^+1 (CII) and C^+2 (CIII) emission will be imaged
simultaneously from two near-perpendicular views (F-top, F-side) using
optical systems containing coherent fiber bundles coupled to gated,
intensified CCD cameras through beam-splitter optics and bandpass
interference filters. Experiments will be conducted during ohmic
conditions, to obtain optimal FSP data. We wish to investigate: (1)
the dependence of cross-field spreading (i.e. cross-field transport)
of C^+1 and C^+2 emission at fixed locations in the SOL as a function
of density (or collisionality) during Ohmic L-mode, and (2) the
dependence of cross-field transport on SOL location (rho) for fixed
discharge conditions during both Ohmic L-mode and Ohmic H-mode.

Run Plan:
Day 2: Ohmic H-mode

At constant discharge conditions, the depth of injection will be varied
to determine transport variation with cross-field coordinate (rho) during
H-mode. Timing of the injection will also be varied to catch various phases
in the discharge, e.g. L-mode, L-H transition, ELM-free H-mode, EDA H-mode.

Set-up B-field ramp so as to obtain Ohmic H-mode
plasmas similar to 1000518022, but staying at I_p = 0.8 MA.
Start with NL04 = 0.8e20/m^2.

Shot plan:
1-6 Setup FSP target, gas, optimal camera exposures
7-12 Vary FSP timing, inject into far SOL (> ~ +15 mm)
13-17 Vary FSP timing, inject into near SOL (< ~ +3 mm)
18-20 Vary FSP timing, inject near and past separatrix

--------------------------------------------------------------------------------
Results:

A good day, though we didn't quite follow the run plan as scheduled.
The first shot of the day was used to assess background carbon levels,
with gas injection starting on shot 2. The first part of the run was
used to investigate plumes generated at various scrape-off layer depths
during ELM-free H-mode. For many of these discharges the probe was
scanned only once, to ensure that during that scan the probe reached
its desired target in the scrape-off layer. Injection timing was also
varied to ensure catching the H-mode phase. No clear differences in the
cross-field plume structure were seen for these cases. One explanation
is that though the electric field is varying strongly as the injection
depth varies, the local electron density and temperature, and hence the
ionization lifetime for the impurities, is also varying strongly, and
thus these two effects on cross-field dispersion are effectively
cancelling. In contrast, the parallel structure of the plumes seemed
to change with injection depth, and parallel flow reversal was evident
for plumes closer to the separatrix. Further analysis is required.

The second part of the run was dedicated to studying plumes close to
the separatrix for both ELM-free and EDA phases. In general, plumes
generated in EDA exhibited less cross-field dispersal than plumes in
ELM-free phases. For a plume generated during the EDA H-mode phase on
shot 23, the cross-field dispersal of the plume was indicative of an
inward directed radial electric field. This is the first time this has
been observed with the plumes. Unfortunately, the probe experienced
serious arcing during this time, and probe data may not be useful. The
probe was switched to a double-probe mode for the remainder of the run
to alleviate this problem. However, this cross-field behaviour was not
reproduced, though there was some evidence of the plumes experiencing
shearing due to being generated in a region of radial electric field
reversal. One reason the full reversal of the plume dispersion is not
being seen consistently has been tracked down, and involves the camera
exposure timing being late relative to the probe injection timing. This
issue has been sorted out. With radial electric field reversal having
now been observed, further collection of plume data near the separatrix
is desired. That data could then be used as a tool for understanding the
behaviour of the radial electric field structure near the separatrix.
This also would serve as a useful cross-calibration of probe measurements
of the local electric field.

Physics Operator Summaries
Entered: Jul 7 2004 04:37:12:037PM
Author: To Be Determined
Engineering setup for Friday, 15 September 2000:

Overnight ECDC in Detuterium, stopping 1-2 hours prior to the run.

Run begins at 9:00 and ends at 17:00.

Power system setup as on 1000829018

Gas setup - fill B-top with 6 psi of D2 Hybrid enabled
fill B-side lower with 1 psi of Ar Hybrid enabled
fill B-side upper with 35 psi of He Hybrid DISABLED (Yes, HELIUM)
(available for between-shot ECDC)
fill C-side with 30 psi of D2 Hybrid enabled
leave J-bottom as is Hybrid DISABLED

The following gate valves should be enabled, assuming no vacuum problems:
ECE, VUV

We only got two hours of ECDC before the run because of a mixup. There was
also a problem with the hybrid this morning because the A matrix did not
respond to the coldstart. However, thanks to an e-mail from Steve Wolfe, a ccl
remcam resolved the problem. Apparently, SPANNA had been rebooted and did not
have the correct definitions prior to the ccl remcam.

Summary: It was a very good run with several shots with peaked density H-modes
most notably shots 1, 6, and 19. We also independently verified the density
threshold that Amanda found yesterday for the ELM-free/EDA boundary. It is
still at 0.6 x 10^20 m^-2 for nl04 programming even at low field with Ohmic
H-mode rather than RF H-mode. The probe studies also went well. See the
session leader's summary for the plume results. The machine ran very well,
though we did have a few unexplained disruptions and some resulting fizzles.

Shot,Duration(s),Ipmax(MA) Shot,Duration(s),Ipmax
1 1.923 0.814 2 1.919 0.814
3 1.403 0.809 4 0.000 0.037
5 1.471 0.812 6 1.927 0.814
7 1.924 0.814 8 1.929 0.810
9 1.932 0.809 10 0.000 0.034
11 1.933 0.809 12 1.919 0.812
13 1.921 0.814 14 1.916 0.809
15 1.923 0.809 16 1.919 0.809
17 1.918 0.809 18 1.922 0.809
19 1.923 0.812 20 1.368 0.807
21 1.920 0.809 22 1.271 0.810
23 1.920 0.812 24 1.924 0.809
25 0.891 0.809 26 1.460 0.812
27 0.000 0.037 28 1.922 0.812
29 1.178 0.817
Finished summary for 1000915 Total of 29 shots.
29 shots. 26 plasmas. 3 fizzles. 0 duds.

Shot 1: Copied shot 1000829018 despite the changes in EFIT, which may mean we
will have to change the gaps somewhat to get what we want. Good shot.
Nice long H-mode of varying flavors.
Shot 2: Put in an additional ramp in ZXL by 15 mm from 0.8 to 1.4 s, then held
constant to 1.5 s to give the FSP a constant target. Good shot. FSP
target still not right. Brian wants to double the ramp rate for the
next shot.
Shot 3: Increased ramp rate to ramp another 15 mm from 0.8 to 1.4 s in ZXL and
then held constant until 1.5 s. Good shot. Disrupted at 1.5 s
apparently because the ZXL ramp was too far.
Shot 4: Reduced ZXL ramp by 7 mm. Increased RCUR by 2 mm to reduce the outer
gap as well. Reduced nl04 from 6.5 to 6.0 x 10^19 m^-2. Fizzle!
Shot 5: Sparker did not have as high a current as on shot 4. Try again with 2 ms less pre-puff.
Good shot. Disrupted again at 1.5 s. FSP target still not quite flat.
Shot 6: Try flattening out the FSP target with a triangle in the ZXL program
at about 1.1 s. Then, reduce the ramp further out past 1.2 sec to try
to avoid pushing things too hard and causing a disruption. Changed
Br0 from 0.5 mT to 1 mT to try to avoid another fizzle, though the
disruption may cause a fizzle regardless.
Shot 7: Change Br0 from 1 mT to 1.5 mT to try to preempt a possible fizzle.
Good shot.
Shot 8: Ramped Bt up faster and removed the flat in Bt around 1.2 s to try to
get out of ELM-free H-mode and into EDA H-mode faster to avoid impurity
buildup that leads to the L-H transition at about 1.0 s. Good shot.
Shot 9: Raised nl04 to 6.5 x 10^19 m^-3 to try to get a longer EDA H-mode.
Good shot.
Shot 10: Try between shot ECDC before this shot to see if we can improve the
quality of the H-mode. Also, disabling the Ar puff to see if it
is increasing the radiation. Returning to 6.0 x 10^19 m^-2. Fizzle!
I suspect the gas pressure did not get low enough to get breakdown
after the ECDC was turned off. Try again without ECDC before the shot.
Shot 11: One more time without ECDC before this shot. Good shot. Still did
not get the long EDA phase we wanted.
Shot 12: Try cutting off the return Bt ramp up at 1.0 s to see if we can keep
the EDA longer by keeping the H-mode threshold lower for longer to
avoid the Type III ELMy regime. Re-enabled the Ar puff. Good shot.
Still did not get a long EDA H-mode though.
Shot 13: Try cutting off the TF 0.1 s earlier because of delays in the change
in the TF relative to the programming. Good shot. ELM-free phase
integrates up the impurities, then collapses into L-mode, then returns
into a long EDA phase.
Shot 14: Try increasing nl04 to 6.5 x 10^19 m^-2. Excellent shot! Long EDA
H-mode from 0.88 - 1.5 s. Brian is still not happy. Picky, picky,
picky! Nice peaked density H-mode though.
Shot 15: Try nl04 = 6.25 x 10^19 m^-2 and pull in on RXU by another 1.5 cm to
increase the upper triangularity. Good shot. ELM-free with transition
then long EDA phase.
Shot 16: Tweak nl04 up to 6.3 x 10^19 m^-2. Increase upper triangularity some
more by decreasing RXU by another 1.5 cm from 0.65 s to 1.4 s. Too
much! The upper X point touches the inner wall and keeps the plasma
in L-mode throughout the shot.
Shot 17: Bring RXU back by 1.5 cm to about what it was on shot 15 and try again.
Good shot. Brief ELM-free then L-mode then long EDA H-mode.
Shot 18: Changed RXU from -0.035 to -0.03 m to slightly lower the upper
triangularity. Good shot. Nice long EDA from 0.89 - 1.57 s.
Shot 19: Brian is still not happy. Reduce nl04 to 6.1 x 10^19 m^-2. Excellent
shot. ELM-free phase early, then suddenly becomes EDA with no L-mode
phase in between. The H-mode lasts from 0.88 - 1.53 s.
Shot 20: Repeat. Disrupted at 1.35 s. A spike on the bolometers at 1.2 s
indicates that the probe may have caused the plasma to drop out of
H-mode and perhaps led to the disruption as well.
Shot 21: Repeat. Good shot. ELM-free, then L-mode, then long EDA phase.
Shot 22: Raise nl04 to 6.2 x 10^19 m^-2. Disrupted again at 1.26 s at the probe
injection time.
Shot 23: Repeat. Good shot. Two ELM-free H-modes. We have apparently found the
same density threshold for the ELM-free/EDA boundary that Amanda found
yesterday in RF H-modes at about 0.6 x 10^20 m^-2 on nl04, which
corresponds to about 1.3 x 10^20 m^-3 on NEBAR_EFIT.
Shot 24: Increase nl04 to 6.5 x 10^19 m^-2. Good shot.
Shot 25: Decrease nl04 to 6.0 x 10^19 m^-2 to ensure ELM-free H-mode. Disruption
at 0.88 s before first probe scan. Bolometer increases dramatically
at 0.86 s, which leads to a large oscillating MHD mode, which then
locks and disrupts right afterward. The probe guys will not take
credit for this one. Perhaps it was an injection of some UFO.
Shot 26: Repeat. Disrupted at 1.46 s. Probe guys do not take credit for this
one either. Big impurity injection at 0.82 s. Finally enters H-mode
at 1.08 s, then had a large H-L transition at 1.4 s, which took a bite
out of the current and led to the disruption.
Shot 27: Repeat. Fizzle!
Shot 28: Took 2 ms off of the pre-puff to 20 ms duration. Try again.
Good shot.
Shot 29: Repeat. Disrupted at 1.1 s. There were several injections that the
probe guys do not take credit for that I think led to the final
disruption.

Session Leader Comments
Sep 15 2000 08:38:28:390AM Run plan for 1000915: MP 276 -- Transport Experiments in the Scrape-Off
Layer during Ohmic L- and H-mode using Gas-Injection Plumes

Run Day 2: Ohmic H-mode

At constant discharge conditions, the depth of injection will be varied
to determine transport variation with cross-field coordinate (rho) during
H-mode. Timing of the injection will also be varied to catch various phases
in the discharge, e.g. L-mode, L-H transition, ELM-free H-mode, EDA H-mode.

Set-up B-field ramp so as to obtain Ohmic H-mode
plasmas similar to 1000518022, but staying at I_p = 0.8 MA.
Start with NL04 = 0.8e20/m^2.

Shot plan:
1-6 Setup FSP target, gas, optimal camera exposures
7-12 Vary FSP timing, inject into far SOL (> ~ +15 mm)
13-17 Vary FSP timing, inject into near SOL (< ~ +3 mm)
18-20 Vary FSP timing, inject near and past separatrix
Sep 15 2000 09:21:48:873AM1000915001 BFSP background shot

For the first shot, not firing the probe or injecting gas.
Use to determine background carbon light levels, for
setting exposures.

Exposures taken at: 0.7, 0.9, 1.1 sec
PPPL Xybion gates (SVC): 0.65 ms, 0.65 ms, 0.65 ms
LANL Xybion gates (TVC): 0.85 ms, 0.85 ms, 0.85 ms

Very low levels of emission on each view.

Good discharge! Got H-mode around 0.9 seconds,
and EDA around 1.1 seconds.

Next shot - change FSP timings slightly to make
sure we catch the H-mode phases, and inject.
Sep 15 2000 11:50:05:983AM1000915002 BFSP Injection of C2D4

17.0 torr of C2D4 in FSP plenum

FSP firing at 0.75, 0.95, 1.15 seconds
NINJA timing: trigger: -1.0 sec, duration: 1.25 sec
"shallow" insertion of FSP (~ +10-12 mm, as LCFS pulls away from probe)

PPPL Xybion gates (SVC): 0.65 ms, 0.65 ms, 0.65 ms
LANL Xybion gates (TVC): 0.85 ms, 0.85 ms, 0.85 ms
Viewing through CII/CIII beam-splitter

Good data. Exposures were somewhat low, especially for
LANL camera. Second scan is good ELM-free H-mode, and
plumes from both views are very, very diffuse in nature.
Third scan is in some sort of EDA, with dithering in Dalpha.
Plumes are less diffuse in this case.

Next shot - increase exposures, try and flatten FSP target.
Sep 15 2000 10:14:59:030AM1000915003 BFSP Injection of C2D4

16.9 torr of C2D4 in FSP plenum

FSP firing at 0.75, 0.95, 1.15 seconds
NINJA timing: trigger: -1.0 sec, duration: 1.25 sec
"shallow" insertion of FSP (~ +10-12 mm)

PPPL Xybion gates (SVC): 0.75 ms, 0.80 ms, 0.75 ms
LANL Xybion gates (TVC): 1.00 ms, 1.15 ms, 1.10 ms
Viewing through CII/CIII beam-splitter

Good data. Similar to last shot, and increasing exposures
helped. Saw some saturation on CII at probe head from
top view. Plumes during second scan are more spread than
during third scan (it seems), but more intense as well -
may have to do with slightly higher exposure.

Next shot - repeat, modify exposures slighty, lower density
slightly to try and make sure ELM-free phase is solidly
ELM-free.
Sep 15 2000 10:15:29:013AM1000915004 BFSP Injection of C2D4

16.9 torr of C2D4 in FSP plenum

FSP firing at 0.75, 0.95, 1.15 seconds
NINJA timing: trigger: -1.0 sec, duration: 1.25 sec
"shallow" insertion of FSP (~ +10-12 mm)

PPPL Xybion gates (SVC): 0.85 ms, 0.85 ms, 0.85 ms
LANL Xybion gates (TVC): 1.05 ms, 1.10 ms, 1.10 ms
Viewing through CII/CIII beam-splitter

Fizzle. Try again next shot.
Sep 15 2000 11:49:45:857AM1000915005 BFSP Injection of C2D4

16.8 torr of C2D4 in FSP plenum

FSP firing at 0.75, 0.95, 1.15 seconds
NINJA timing: trigger: -1.0 sec, duration: 1.25 sec
"deep" insertion of FSP (~ +0-2 mm)

PPPL Xybion gates (SVC): 0.85 ms, 0.85 ms, 0.85 ms
LANL Xybion gates (TVC): 1.00 ms, 1.10 ms, 1.10 ms
Viewing through CII/CIII beam-splitter

Good data. First scan hits the separatrix, and this
is apparent on the plumes - they look very thin from
the top, and as though they "hit a wall" on the side.
Next two scans are H-modes, further out. First one
ELM-free, and second one EDA-ish. Again, we can see
difference in plume widths, with ELM-free plumes
exhibiting less cross-field spreading in the field
of view.

Next shot - pull FSP out some (saw arcing on first scan)
and change timings slightly, to catch L-H transition.
Also, change exposures slightly.
Sep 15 2000 11:49:54:607AM1000915006 BFSP Injection of C2D4

16.6 torr of C2D4 in FSP plenum

FSP firing at 0.65, 0.90, 1.15 seconds
NINJA timing: trigger: -1.0 sec, duration: 1.25 sec
"deep" insertion of FSP (~ +0-2 mm)

PPPL Xybion gates (SVC): 0.85 ms, 0.85 ms, 0.90 ms
LANL Xybion gates (TVC): 1.00 ms, 1.10 ms, 1.15 ms
Viewing through CII/CIII beam-splitter

Good data. First scan is L-mode, Second scan is ELM-free
H-mode, and third scan looks like L-mode again. Probe
gets "hammered" on third scan, and plumes are saturated
on top view. Both first and third scans look like typical
L-mode plumes at the separatrix.

Next shot - going to only two scans, try and get deep
insertion on both H-modes (change timing).
Sep 15 2000 11:49:26:827AM1000915007 BFSP Injection of C2D4

16.5 torr of C2D4 in FSP plenum

FSP firing at 0.90, 1.10 seconds
NINJA timing: trigger: -1.0 sec, duration: 1.25 sec
"deep" insertion of FSP (~ +0-2 mm)

PPPL Xybion gates (SVC): 0.85 ms, 0.90 ms
LANL Xybion gates (TVC): 1.20 ms, 1.25 ms
Viewing through CII/CIII beam-splitter

Interesting data. First scan is at L-H transition,
but plumes look somewhat L-mode-ish, with low light
signals. Very small plumes. Plumes in second scan
are also small, but more intense light (more than
would be expected from small exposure increase).
Second scan shows ELMy behaviour on scanning probe
data.

Next shot - change timing of scan to make sure to get
ELM-free H-mode, and try and get good EDA as well.
Sep 15 2000 11:48:54:997AM1000915008 BFSP Injection of C2D4

16.4 torr of C2D4 in FSP plenum

FSP firing at 0.916666, 1.11666 seconds
NINJA timing: trigger: -1.0 sec, duration: 1.25 sec
"deep" insertion of FSP (~ +0-2 mm)

PPPL Xybion gates (SVC): 0.90 ms, 0.90 ms
LANL Xybion gates (TVC): 1.20 ms, 1.20 ms
Viewing through CII/CIII beam-splitter

Good data. Strong ExB flow in plumes on first
scan, which is in ELM-free phase. During second
scan, plume dispersal is less, but still have
strong evidence of boomeranging on side view,
even though it looks like we are in an L-mode
phase here. FSP was further out in the separatrix
than desired.

Next shot - push FSP further in.
Sep 15 2000 11:48:42:640AM1000915009 BFSP Injection of C2D4

16.3 torr of C2D4 in FSP plenum

FSP firing at 0.916666, 1.11666 seconds
NINJA timing: trigger: -1.0 sec, duration: 1.25 sec
"deep" insertion of FSP (~ +0-2 mm)

PPPL Xybion gates (SVC): 0.90 ms, 0.90 ms
LANL Xybion gates (TVC): 1.20 ms, 1.20 ms
Viewing through CII/CIII beam-splitter

Good data First scan looks similar to lost
shot. Second scan is in some sort of ELMy H-mode.
Plumes in this second scan have a structure
somewhat in between ELM-free H-mode and L-mode,
in terms of plume dispersion.

Next shot - go to having only one scan (in
ELM-free H-mode) and really try and go deep,
look for E_r reversal.
Sep 15 2000 11:59:46:450AM1000915010 BFSP Injection of C2D4

16.2 torr of C2D4 in FSP plenum

FSP firing at 0.916666 seconds
NINJA timing: trigger: -1.0 sec, duration: 1.25 sec
"deep" insertion of FSP (~ +0-2 mm)

PPPL Xybion gates (SVC): 0.90 ms
LANL Xybion gates (TVC): 1.20 ms
Viewing through CII/CIII beam-splitter

Fizzle. Try again next shot.
Sep 15 2000 12:28:13:343PM1000915011 BFSP Injection of C2D4

16.2 torr of C2D4 in FSP plenum

FSP firing at 0.916666 seconds
NINJA timing: trigger: -1.0 sec, duration: 1.25 sec
"deep" insertion of FSP (~ +0-2 mm)

PPPL Xybion gates (SVC): 0.90 ms
LANL Xybion gates (TVC): 1.20 ms
Viewing through CII/CIII beam-splitter

Good data. Exposures were somewhat low for both
cameras. In both fields of view, the plumes look
like they have a slice cut out of them, in the
direction upstream of the gas injection location.
Flows look like they are reversed in side view,
but not so clear the case from the top view.
Saw some arcing on the East probe of the FSP.

Next shot - lower Bt to try and produce EDA, and
keep FSP at this location.
Sep 15 2000 12:45:19:607PM1000915012 BFSP Injection of C2D4

16.1 torr of C2D4 in FSP plenum

FSP firing at 0.916666 seconds
NINJA timing: trigger: -1.0 sec, duration: 1.25 sec
"deep" insertion of FSP (~ +0-2 mm)

PPPL Xybion gates (SVC): 0.90 ms
LANL Xybion gates (TVC): 1.20 ms
Viewing through CII/CIII beam-splitter

Interesting probe data. Caught the L-H
transitions. Plumes look like "hybrids" --
part L-mode like and part H-mode like.
Some saturation at probe head in top
view.

Next shot - move probe timing to catch
H-mode, pull probe out because of worry
about arcing.
Sep 15 2000 12:55:36:810PM1000915013 BFSP Injection of C2D4

16.1 torr of C2D4 in FSP plenum

FSP firing at 0.95 seconds
NINJA timing: trigger: -1.0 sec, duration: 1.25 sec
"deep" insertion of FSP (~ +0-2 mm)

PPPL Xybion gates (SVC): 0.90 ms
LANL Xybion gates (TVC): 1.20 ms
Viewing through CII/CIII beam-splitter

Good data. Similar to shot 11. Exposures are somewhat
low, but still have good plumes. On side view, see the
double structure again in the plume - not so clear on
the side view.

Next shot - pull probe out a bit, and increase exposures.


Sep 15 2000 01:10:40:467PM1000915014 BFSP Injection of C2D4

16.0 torr of C2D4 in FSP plenum

FSP firing at 0.95 seconds
NINJA timing: trigger: -1.0 sec, duration: 1.25 sec
"deep" insertion of FSP (~ +2-4 mm)

PPPL Xybion gates (SVC): 1.05 ms
LANL Xybion gates (TVC): 1.35 ms
Viewing through CII/CIII beam-splitter

Good data on both views. Similar to some of the
other ELM-free H-mode data, though we seemed to
be in a dithering phase. Exposures are good.

Next shot - pull probe back further, to continue
doing a position scan of the ELM-free H-mode.


Sep 15 2000 01:23:55:403PM1000915015 BFSP Injection of C2D4

15.9 torr of C2D4 in FSP plenum

FSP firing at 0.916667 seconds
NINJA timing: trigger: -1.0 sec, duration: 1.25 sec
"medium" insertion of FSP (~ +9-11 mm)

PPPL Xybion gates (SVC): 1.05 ms
LANL Xybion gates (TVC): 1.35 ms
Viewing through CII/CIII beam-splitter

Good data from both cameras. Even further out,
plumes show similar behaviour - very cross-field
spread during the ELM-free H-mode.

Next shot - pull probe even further out, and
see what happens.
Sep 15 2000 01:44:38:450PM1000915016 BFSP Injection of C2D4

15.8 torr of C2D4 in FSP plenum

FSP firing at 0.933333 seconds
NINJA timing: trigger: -1.0 sec, duration: 1.25 sec
"shallow" insertion of FSP (~ +16-18 mm)

PPPL Xybion gates (SVC): 1.00 ms
LANL Xybion gates (TVC): 1.35 ms
Viewing through CII/CIII beam-splitter

Good data, though we never got into H-mode.
Plumes still exhibit a lot of cross-field
dispersion, but this may be just reproducing
our results from last week - in the far SOL,
when things are cold, ion lifetimes are long
enough that even for small ExB flow velocities
the cross-field drift can be large. Thus,
the plumes are based more on local conditions
(n_e, T_e, local E_r) rather than global
confinement mode.

Next shot - repeat shot, with corrections to
upper triangularity to get H-mode.
Sep 15 2000 01:54:01:403PM1000915017 BFSP Injection of C2D4

15.7 torr of C2D4 in FSP plenum

FSP firing at 0.933333 seconds
NINJA timing: trigger: -1.0 sec, duration: 1.25 sec
"shallow" insertion of FSP (~ +16-18 mm)

PPPL Xybion gates (SVC): 1.00 ms
LANL Xybion gates (TVC): 1.35 ms
Viewing through CII/CIII beam-splitter

Again, good data. Got an ELM-free H-mode at FSP
injection time. Exposures were slightly low. Data
exhibits significant cross-field spreading.

Next shot - push probe back in to separatrix.
Sep 15 2000 02:13:34:997PM1000915018 BFSP Injection of C2D4

15.6 torr of C2D4 in FSP plenum

FSP firing at 0.933333 seconds
NINJA timing: trigger: -1.0 sec, duration: 1.25 sec
"deep" insertion of FSP (~ +0-2 mm)

PPPL Xybion gates (SVC): 1.10 ms
LANL Xybion gates (TVC): 1.50 ms
Viewing through CII/CIII beam-splitter

Good probe data. Looks like we were in an EDA-type
phase. Plumes are different relative to ELM-free
cases at this location - less cross-field spreading.
See coherent mode on FSP.

Next shot - try and get an ELM-free H-mode.
Sep 15 2000 02:32:46:170PM1000915019 BFSP Injection of C2D4

15.6 torr of C2D4 in FSP plenum

FSP firing at 0.933333 seconds
NINJA timing: trigger: -1.0 sec, duration: 1.25 sec
"deep" insertion of FSP (~ +0-2 mm)

PPPL Xybion gates (SVC): 1.10 ms
LANL Xybion gates (TVC): 1.50 ms
Viewing through CII/CIII beam-splitter

Good data, and a good discharge. Plasma went
from ELM-free into EDA, and FSP injection occurs
during ELM-free portion. However, plumes look
more similar to previous shot (018) than shots
earlier in the day (006,011). Will have to correlate
with local conditions.

Next shot - probe into EDA portion of discharge.
Sep 15 2000 02:45:25:450PM1000915020 BFSP Injection of C2D4

15.5 torr of C2D4 in FSP plenum

FSP firing at 0.933333, 1.2 seconds
NINJA timing: trigger: -1.0 sec, duration: 1.25 sec
"deep" insertion of FSP (~ +0-2 mm)

PPPL Xybion gates (SVC): 1.10 ms, 1.10 ms
LANL Xybion gates (TVC): 1.50 ms, 1.50 ms
Viewing through CII/CIII beam-splitter

Interesting data. Got a good ELM-free scan
the first plume, and an EDA phase for the
second plume. For both plumes there seems to
be this double-structure, at least as observed
on the side view. Emission near the probe is
near symmetric in this view. Top view picture
isn't as clear.

Exposures were too high during EDA phase - got
saturation in both views.

Next shot - keep things here, adjust exposures.
Sep 15 2000 02:58:23:107PM1000915021 BFSP Injection of C2D4

15.4 torr of C2D4 in FSP plenum

FSP firing at 0.933333, 1.2 seconds
NINJA timing: trigger: -1.0 sec, duration: 1.25 sec
"deep" insertion of FSP (~ +0-2 mm)

PPPL Xybion gates (SVC): 1.20 ms, 0.95 ms
LANL Xybion gates (TVC): 1.60 ms, 1.10 ms
Viewing through CII/CIII beam-splitter

Good data. First scan, ELM-free case, looks
similar to earlier shots, and different from
last shot! Especially clear in side view. Will
be interesting to find what differences exist
in local conditions. Second scan was in an L-mode
type phase, and plumes reflect that.

Next shot - move FSP timing slightly to catch EDA,
and repeat.
Sep 15 2000 03:15:13:077PM1000915022 BFSP Injection of C2D4

15.4 torr of C2D4 in FSP plenum

FSP firing at 0.933333, 1.25 seconds
NINJA timing: trigger: -1.0 sec, duration: 1.25 sec
"deep" insertion of FSP (~ +0-2 mm)

PPPL Xybion gates (SVC): 1.20 ms, 0.95 ms
LANL Xybion gates (TVC): 1.60 ms, 1.10 ms
Viewing through CII/CIII beam-splitter

Very good data. See both an ELM-free and EDA
phase, and a significant difference in the
plume structure. Saturation near the probe
head for the EDA scan. EDA phase also had
some ELMs present.

Next shot - repeat, and move FSP timing to
avoid ELMs.
Sep 15 2000 03:31:33:187PM1000915023 BFSP Injection of C2D4

15.3 torr of C2D4 in FSP plenum

FSP firing at 0.933333, 1.2 seconds
NINJA timing: trigger: -1.0 sec, duration: 1.25 sec
"deep" insertion of FSP (~ +0-2 mm)

PPPL Xybion gates (SVC): 1.20 ms, 0.95 ms
LANL Xybion gates (TVC): 1.60 ms, 1.00 ms
Viewing through CII/CIII beam-splitter

Great data!! Both scans are in ELM-free. First
scan is typical ELM-free plume. On second scan,
we get in deeper - and see asymmetry in plumes
change direction! This indicates a reversal of
E_r at this location. FSP gets hammered - tons
of arcing. Brian is changing to a double-probe
mode to try and reduce energy flux to FSP.

Next shot - increased density slightly to get
EDA, keep probes going in deep to investigate
this reversal layer.
Sep 15 2000 03:39:48:547PM1000915024 BFSP Injection of C2D4

15.3 torr of C2D4 in FSP plenum

FSP firing at 0.933333, 1.2 seconds
NINJA timing: trigger: -1.0 sec, duration: 1.25 sec
"deep" insertion of FSP (~ +0-2 mm)

PPPL Xybion gates (SVC): 1.20 ms, 0.95 ms
LANL Xybion gates (TVC): 1.60 ms, 1.00 ms
Viewing through CII/CIII beam-splitter

Good data, though we didn't get into the E_r
reversal region. First scan looks like L-mode,
and second scan was EDA. Exposure for LANL
camera on second scan was low. Good FSP data -
coherent mode was clearly seen.

Next shot - try to go back to shot 023, look
for reversal and probe deep.
Sep 15 2000 03:59:48:950PM1000915025 BFSP Injection of C2D4

15.3 torr of C2D4 in FSP plenum

FSP firing at 0.933333, 1.2 seconds
NINJA timing: trigger: -1.0 sec, duration: 1.25 sec
"deep" insertion of FSP (~ +0-2 mm)

PPPL Xybion gates (SVC): 1.20 ms, 1.00 ms
LANL Xybion gates (TVC): 1.60 ms, 1.15 ms
Viewing through CII/CIII beam-splitter

Plasma disrupts before we inject (0.88 sec).
Try again next shot.
Sep 15 2000 04:10:28:013PM1000915026 BFSP Injection of C2D4

15.3 torr of C2D4 in FSP plenum

FSP firing at 0.933333, 1.2 seconds
NINJA timing: trigger: -1.0 sec, duration: 1.25 sec
"deep" insertion of FSP (~ +0-2 mm)

PPPL Xybion gates (SVC): 1.20 ms, 1.00 ms
LANL Xybion gates (TVC): 1.60 ms, 1.15 ms
Viewing through CII/CIII beam-splitter

First scan isn't too exciting - plasma looks
to be in L-mode. During the second scan we
are in ELM-free H-mode. The CIII plume from
the side view looks as though it is sheared
(double-structure), where (perhaps) one portion
of the plume is flowing one way and the other
portion the opposite way. This looks to be
happening along a "shear front". Not clear
on the top view, but exposures were low (I
was anticipating EDA).

Next shot - assume that both scans will be ELM-
free, and adjust exposures accordingly. Moving
in FSP slightly.
Sep 15 2000 04:18:40:560PM1000915027 BFSP Injection of C2D4

Before this shot, replenished FSP NINJA system

16.5 torr of C2D4 in FSP plenum

FSP firing at 0.933333, 1.2 seconds
NINJA timing: trigger: -1.0 sec, duration: 1.25 sec
"deep" insertion of FSP (~ +0-2 mm)

PPPL Xybion gates (SVC): 0.90 ms, 0.90 ms
LANL Xybion gates (TVC): 1.25 ms, 1.25 ms
Viewing through CII/CIII beam-splitter

Fizzle. Try again next shot.
Sep 15 2000 04:47:32:373PM1000915028 BFSP Injection of C2D4

Before this shot, replenished FSP NINJA system

16.4 torr of C2D4 in FSP plenum

FSP firing at 0.933333, 1.2 seconds
NINJA timing: trigger: -1.0 sec, duration: 1.25 sec
"deep" insertion of FSP (~ +0-2 mm)

PPPL Xybion gates (SVC): 0.95 ms, 0.95 ms
LANL Xybion gates (TVC): 1.25 ms, 1.25 ms
Viewing through CII/CIII beam-splitter

First scan is in L-mode, second in ELM-free
H-mode. H-mode scan has some characteristics
of shear-layer behaviour in the plumes, and
definitely in the FSP data. However, the probe
is peaking early, and so our exposure may be
occuring just slightly after the peak insertion,
i.e. where all the action is! Try and just this
in PUT_GATE_SETPTS, and see what happens.
Sep 15 2000 05:18:27:590PM1000915029 BFSP Injection of C2D4

Before this shot, replenished FSP NINJA system

16.3 torr of C2D4 in FSP plenum

FSP firing at 1.0, 1.25 seconds
NINJA timing: trigger: -1.0 sec, duration: 1.25 sec
"deep" insertion of FSP (~ +0-2 mm)

PPPL Xybion gates (SVC): 0.95 ms, 0.95 ms
LANL Xybion gates (TVC): 1.25 ms, 1.25 ms
Viewing through CII/CIII beam-splitter

Only got one scan - plasma disrupts at 1.16 ms.
First scan was in ELM-free H-mode. Plumes look
similar to previous shot.

End of run.

Physics Operator Comments
Sep 15 2000 09:06:52:107AM1000915001Joseph SnipesEngineering setup for Friday, 15 September 2000:

Overnight ECDC in Detuterium, stopping 1-2 hours prior to the run.

Run begins at 9:00 and ends at 17:00.

Power system setup as on 1000829018

Gas setup - fill B-top with 6 psi of D2 Hybrid enabled
fill B-side lower with 1 psi of Ar Hybrid enabled
fill B-side upper with 35 psi of He Hybrid DISABLED (Yes, HELIUM)
(available for between-shot ECDC)
fill C-side with 30 psi of D2 Hybrid enabled
leave J-bottom as is Hybrid DISABLED

The following gate valves should be enabled, assuming no vacuum problems:
ECE, VUV
Sep 15 2000 09:08:16:217AM1000915001Joseph SnipesShot 1: Copied shot 1000829018 despite the EFIT changes. So, we will probably
need to change the gaps to get what we want. Good shot.
Sep 15 2000 09:11:32:763AM1000915001Joseph SnipesWe only got two hours of ECDC before the run because of a mixup. There was
also a problem with the hybrid this morning because the A matrix did not
respond to the coldstart. However, thanks to an e-mail from Steve Wolfe, a ccl
remcam resolved the problem. Apparently, SPANNA had been rebooted and did not
have the correct definitions prior to the ccl remcam.
Sep 15 2000 10:57:54:030AM1000915001Joseph SnipesShot 1: John Rice and Chris Boswell noted that shot 1 had a clear ITB with
peaked density, though the visible bremmstrahlung profile was not
available for that shot.
Sep 15 2000 11:27:33:233AM1000915001Joseph SnipesShot 8: Ramped Bt up faster and removed the flat in Bt around 1.2 s to try to
get out of ELM-free H-mode and into EDA H-mode faster to avoid impurity
buildup that leads to the L-H transition at about 1.0 s. Good shot.
Sep 15 2000 09:35:32:590AM1000915002Joseph SnipesShot 2: Put in an additional ramp in ZXL by 15 mm from 0.8 to 1.4 s, then held
constant to 1.5 s to give the FSP a constant target. Good shot. FSP
target still not right. Brian wants to double the ramp rate of ZXL for
the next shot.
Sep 15 2000 09:56:43:450AM1000915003Joseph SnipesShot 3: Increased ramp rate to ramp another 15 mm from 0.8 to 1.4 s in ZXL and
then held constant until 1.5 s. Good shot. Disrupted at 1.5 s
apparently because the ZXL ramp was too far.
Sep 15 2000 10:12:49:733AM1000915004Joseph SnipesShot 4: Reduced ZXL ramp by 7 mm. Increased RCUR by 2 mm to reduce the outer
gap as well. Reduced nl04 from 6.5 to 6.0 x 10^19 m^-2. Fizzle!
Sep 15 2000 10:28:02:263AM1000915005Joseph SnipesShot 5: Sparker did not have as high a current as on shot 4. Try again with
2 ms less pre-puff. Good shot. Disrupted again at 1.5 s. FSP target
still not quite flat.
Sep 15 2000 10:40:27:467AM1000915006Joseph SnipesShot 6: Try flattening out the FSP target with a triangle in the ZXL program
at about 1.1 s. Then, reduce the ramp further out past 1.2 sec to try
to avoid pushing things too hard and causing a disruption. Changed Br0
from 0.5 mT to 1 mT to try to avoid another fizzle, though the
disruption may cause a fizzle regardless. Good shot. FSP target looks
pretty good. Disruption has gone away.
Sep 15 2000 10:54:09:590AM1000915007Joseph SnipesShot 7: Change Br0 from 1 mT to 1.5 mT to try to preempt a possible fizzle.
Good shot.
Sep 15 2000 11:51:06:700AM1000915009Joseph SnipesShot 9: Raised nl04 to 6.5 x 10^19 m^-3 to try to get a longer EDA H-mode.
Good shot. DNB gate valve opened though the beam did not fire. The
prefill was effected changing from 0.054 to 0.065 mTorr between shots 8
and 9.
Sep 15 2000 12:02:22:623PM1000915010Joseph SnipesShot 10: Try between shot ECDC before this shot to see if we can improve the
quality of the H-mode. Also, disabling the Ar puff to see if it
is increasing the radiation. Returning to 6.0 x 10^19 m^-2. Fizzle!
I suspect the gas pressure did not get low enough to get breakdown
after the ECDC was turned off. Try again without ECDC before the shot.
Sep 15 2000 12:25:34:310PM1000915011Joseph SnipesShot 11: One more time without ECDC before this shot. Good shot. Still did
not get the long EDA phase we wanted.
Sep 15 2000 12:39:32:560PM1000915012Joseph SnipesShot 12: Try cutting off the return Bt ramp up at 1.0 s to see if we can keep
the EDA longer by keeping the H-mode threshold lower for longer to
avoid the Type III ELMy regime. Re-enabled the Ar puff. Good shot.
Still did not get a long EDA H-mode though.
Sep 15 2000 12:54:55:030PM1000915013Joseph SnipesShot 13: Try cutting off the TF 0.1 s earlier because of delays in the change
in the TF relative to the programming. Good shot. ELM-free phase
integrates up the impurities, then collapses into L-mode, then returns
into a long EDA phase.
Sep 15 2000 01:13:41:827PM1000915014Joseph SnipesShot 14: Try increasing nl04 to 6.5 x 10^19 m^-2. Excellent shot! Long EDA
H-mode from 0.88 - 1.5 s. Brian is still not happy. Picky, picky,
picky! Nice peaked density H-mode though.
Sep 15 2000 01:26:09:390PM1000915015Joseph SnipesShot 15: Try nl04 = 6.25 x 10^19 m^-2 and pull in on RXU by another 1.5 cm to
increase the upper triangularity. Good shot. ELM-free with transition
then long EDA phase.
Sep 15 2000 01:41:42:373PM1000915016Joseph SnipesShot 16: Tweak nl04 up to 6.3 x 10^19 m^-2. Increase upper triangularity some
more by decreasing RXU by another 1.5 cm from 0.65 s to 1.4 s. Too
much! The upper X point touches the inner wall and keeps the plasma
in L-mode throughout the shot.
Sep 15 2000 01:51:57:483PM1000915017Joseph SnipesShot 17: Bring RXU back by 1.5 cm to about what it was on shot 15 and try again.
Good shot. Brief ELM-free then L-mode then long EDA H-mode.
Sep 15 2000 02:11:12:263PM1000915018Joseph SnipesShot 18: Changed RXU from -0.035 to -0.03 m to slightly lower the upper
triangularity. Good shot. Nice long EDA from 0.89 - 1.57 s.
Sep 15 2000 02:27:29:967PM1000915019Joseph SnipesShot 19: Brian is still not happy. Reduce nl04 to 6.1 x 10^19 m^-2. Excellent
shot. ELM-free phase early, then suddenly becomes EDA with no L-mode
phase in between. The H-mode lasts from 0.88 - 1.53 s.
Sep 15 2000 02:39:12:700PM1000915020Joseph SnipesShot 20: Repeat. Disrupted at 1.35 s. A spike on the bolometers at 1.2 s
indicates that the probe may have caused the plasma to drop out of
H-mode and perhaps led to the disruption as well.
Sep 15 2000 02:55:25:373PM1000915021Joseph SnipesShot 21: Repeat. Good shot. ELM-free, then L-mode, then long EDA phase.
Sep 15 2000 03:05:59:857PM1000915022Joseph SnipesShot 22: Raise nl04 to 6.2 x 10^19 m^-2. Disrupted again at 1.26 s at the probe
injection time.
Sep 15 2000 03:28:27:247PM1000915024Joseph SnipesShot 23: Repeat. Good shot. Two ELM-free H-modes. We have apparently found the
same density threshold for the ELM-free/EDA boundary that Amanda found
yesterday in RF H-modes at about 0.6 x 10^20 m^-2 on nl04, which
corresponds to about 1.3 x 10^20 m^-3 on NEBAR_EFIT.
Sep 15 2000 03:36:47:860PM1000915024Joseph SnipesShot 24: Increase nl04 to 6.5 x 10^19 m^-2. Good shot.
Sep 15 2000 03:48:23:920PM1000915025Joseph SnipesShot 25: Decrease nl04 to 6.0 x 10^19 m^-2 to ensure ELM-free H-mode. Disruption
at 0.88 s before first probe scan. Bolometer increases dramatically
at 0.86 s, which leads to a large oscillating MHD mode, which then
locks and disrupts right afterward. The probe guys will not take
credit for this one. Perhaps it was an injection of some UFO.
Sep 15 2000 04:03:30:747PM1000915026Joseph SnipesShot 26: Repeat. Disrupted at 1.46 s. Probe guys do not take credit for this
one either. Big impurity injection at 0.82 s. Finally enters H-mode
at 1.08 s, then had a large H-L transition at 1.4 s, which took a bite
out of the current and led to the disruption.
Sep 15 2000 04:18:49:170PM1000915027Joseph SnipesShot 27: Repeat. Fizzle!
Sep 15 2000 04:37:06:200PM1000915028Joseph SnipesShot 28: Took 2 ms off of the pre-puff to 20 ms duration. Try again.
Good shot.
Sep 15 2000 04:54:32:043PM1000915029Joseph SnipesShot 29: Repeat. Disrupted at 1.1 s. There were several injections that the
probe guys do not take credit for that I think led to the final
disruption.
Sep 15 2000 04:58:23:920PM1000915029Joseph SnipesSummary: It was a very good run with several shots with peaked density H-modes
most notably shots 1, 6, and 19. We also independently verified the density
threshold that Amanda found yesterday for the ELM-free/EDA boundary. It is
still at 0.6 x 10^20 m^-2 for nl04 programming even at low field with Ohmic
H-mode rather than RF H-mode. The probe studies also went well. See the
session leader's summary for the plume results. The machine ran very well,
though we did have a few unexplained disruptions and some resulting fizzles.

Shot,Duration(s),Ipmax(MA) Shot,Duration(s),Ipmax
1 1.923 0.814 2 1.919 0.814
3 1.403 0.809 4 0.000 0.037
5 1.471 0.812 6 1.927 0.814
7 1.924 0.814 8 1.929 0.810
9 1.932 0.809 10 0.000 0.034
11 1.933 0.809 12 1.919 0.812
13 1.921 0.814 14 1.916 0.809
15 1.923 0.809 16 1.919 0.809
17 1.918 0.809 18 1.922 0.809
19 1.923 0.812 20 1.368 0.807
21 1.920 0.809 22 1.271 0.810
23 1.920 0.812 24 1.924 0.809
25 0.891 0.809 26 1.460 0.812
27 0.000 0.037 28 1.922 0.812
29 1.178 0.817
Finished summary for 1000915 Total of 29 shots.
29 shots. 26 plasmas. 3 fizzles. 0 duds.

Engineering Operator Comments
ShotTimeTypeStatusComment
109:06:14:873AMPlasmaOk
209:26:57:843AMPlasmaOk
309:41:58:543AMPlasmaOk
409:58:13:687AMPlasmaOk
510:13:31:593AMPlasmaOk
610:31:40:140AMPlasmaOk
710:50:37:873AMPlasmaOk
811:15:29:950AMPlasmaOk
911:35:55:547AMPlasmaOk
1011:57:17:840AMPlasmaOk
1112:14:30:170PMPlasmaOk
1212:29:12:670PMPlasmaOk
1312:43:32:717PMPlasmaOk
1412:59:07:530PMPlasmaOk
1501:14:54:873PMPlasmaOk
1601:31:45:513PMPlasmaOk
1701:45:32:937PMPlasmaOk
1802:03:58:513PMPlasmaOk
1902:17:55:340PMPlasmaOk
2002:32:09:657PMPlasmaOk
2102:47:18:390PMPlasmaOk
2203:01:07:110PMPlasmaOk
2303:14:45:247PMPlasmaOk
2403:28:06:903PMPlasmaOk
2503:41:19:060PMPlasmaOk
2603:54:41:217PMPlasmaOk
2704:16:47:343PMPlasmaOk
2804:31:19:513PMPlasmaOk
2904:45:03:200PMPlasmaOk