Alcator C-Mod Run 960223 Information

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Miniproposals
Miniproposal:
Date Filed:
Title:
First Author:
Session Leader:Chris Rost (shots 1-36)
Session Leader:John Reardon (shots 1-36)
Miniproposal:125a
Date Filed:11/27/1995
Title:ICRF Reversed Shear Mode
First Author:Miklos Porkolab
Session Leader:Miklos Porkolab (shots 37-50)

Operators
Session leader(s):Chris Rost,John Reardon,Miklos Porkolab
Physics operator(s):Robert Granetz,Steve Wolfe
Engineering operator(s):Vinny Bertolino,Joe Daigle

Engineering Operator Run Comment
plasma run

Session Leader Plans

Physics Operators Plans

Session Leader Summaries
Entered: Jul 7 2004 03:49:15:523PM
Author: To Be Determined


SL Summary for Run 960223
Topic: ERS/ PEP Mode Experiment: MP
SL: M. Porkolab
PO: S. Wolfe
EO: J. Daigle
The run went very well, in that there was only one fizzle, the last shot.
All other shots were executed with substantial RF power being coupled into
the plasma early into the discharge, typically 2 MW, with highly variable
plasma conditions as the current was being ramped. Typical plasma
conditions were nel=0.5-1.5, Ip=0.8 MA, Bt=5.3T. RF power was coupled in at
times 0.08-0.14 s, at power levels 1-2 MW, quite successfully, initially
without feedback, and during later shots with feedback. Occasionally RF was
also injected at 0.8 sec to form PEP modes. Typical electron temperatures
were 4 keV at 1 MW, and 5 kev (+) with 2 MW RF pulse during the ramp phase
as long as the density was low enough (i.e., no pellet injection). Ion
temperatures were of the order of 3 keV (needs to be confirmed). Zeff = 2-3
in the initial low density phase, and this may be lower than the previous
ERS run w/o boronization (need to be confirmed!). So, in principle we
should have had a better chance to get into the ERS mode than before
boronization. This was the idea behind this run. Pellets were injected at
two differrent times, early into the discharge (0.18 sec) and late into the
discharge (0.8 sec). Evidence of PEP mode was apparent. H-modes were
obtained with H-factors of the order of 2, but were transient in nature.
Typical stored energies were of the order of 100 kJ, with the best
approaching 120 kJ at 2 MW of RF power. An attempt was made to measure the
q profile during the ERS mode, as well to peak the density profile, using
Li pellet injection. However, owing to the high temperatures (5 keV),
pellet penetration was poor even for the medium sized pellets (Rmin = 78
cm). The latter half of the shots had lithium pellets injected for PEP mode
studies. A few important observations were made. First, the early
collapse of the mode often seen with D pellet PEP modes and post-boronized
Li PEP modes was eliminated by reducing the RF input power to 1 MW. Ni was
injected with the laser blowoff diagnostic and was seen to exist in the
plasma as long as the PEP mode existed, indicating an extremely long
particle confinement time. In summary, it is not clear whether the ERS mode
was obtained. Initially the electron temperatures were hollow during the
ramp, but quickly peaked up to 4-5 keV during RF injection by 02sec.
According to Yuichi, these temperatures are consistent with L-Mode
confinement at these low densities without any ERS mode. It should be noted
that at these low densities we do not expect much coupling of RF power to
ions, and the minority tail should heat mostly electrons. Therefore, a
detailed TRANSP analysis may be required to determine whether there is any
evidence of ERS mode confinement.

Recommendation for future experiments:
(1)The RF pulse shape could be altered, in particular inject at maximum
power ( 2 MW ) initially as now, but once the electron temperature
increased to its maximum value, cut the power into half (1 MW), to see if
the high electron temperatures would hold up at reduced power -this would
indicate that the plasma may be in the ERS mode. The timing of the RF
power drop should be varied to optimize the results. The tail slowing down
must be assessed for this experiment, to be sure it does not dominate the
temporal evolution of the discharge. (2) Another variation on this
experiment might include a minor Bt field scan (10%) to attempt slight
off-axis heating ( r/a=0.3-0.4); this might aid in increasing the off-axis
electron heating and current, thus lowering q(r) off axis, thus creating a
reversed shear equilibria while still maintaining good core heating.





Entered: Jul 7 2004 03:49:15:540PM
Author: To Be Determined
960223(a) Session Leader Summary

The purpose of today's run is to study the thresholds and saturation
levels of edge ion heating and RF decay waves during Parametric Decay
Instabilities in ICRH plasmas, and impurity generation by these effects.
The plan is to have 3-4 good shots at each of 2.75T, 3.4T, 3.0T toroidal
fields, to perform scans in the PCX and RF probes. The RF will fire in pulses
of increasing height, with the maximum at less than .5MW. Then we will return
to the magnetic field of greatest interest to do 1-2 shot scans in density and
outer gap, and switch to D port antenna. Next, we'll try to achieve a 2.35T
plasma for more scans.

Most of the goals were attacked to some degree, though definitive scans
eluded us. We got a good number of shots at 3.4T and 2.81T, which had
resonances in the edge, and at 2.75T which did not. The PCX got measures
of energetic neutral flux during edge heating versus RF power for three pitch
angles at the different fields. As expected, the apparent tail temperature
decreased at pitch angles away from perpendicular, and was hotter for higher
RF power. The tail was larger in D at 2.81T, and large in H at 3.4T, and small
at 2.75T. Quantitative analysis to follow.

The RF probes took spectra on all shots, and additionally the new
scanning probe was used to measure radial profiles of the pump and decay waves.
At 3.4T, a shot-to-shot radial scan of the RF probe showed that the 80 MHz
power level dropped off slowly behind the limiter. The RF probe unexpectedly
did not detect any power at the local Deuterium fundamental (19 MHz or
thereabouts). After the change to Bt of 2.75T, weak decay waves at about 20
and 45 MHz were observed. We moved to 2.8 T for shot 28 and found
what appeared to be two types of PDI, one into the outer edge Deuterium
fundamental and the other into the outer edge hydrogen fundamental. The
highest level of PDI recorded during the day appeared on shot 32, but wasn't
accompanied by a moly outburst. The RF probe was scanned in radius again
for shots 32, 34, and 36 and found that a. the PDI level decreased quickly
with radius and b. the frequency of the detected PDI fundamental varied
with radius, as if the PDI were being generated at the same radius as the
probe.

One goal of the run was to generate large PDI levels and large amounts
of energetic edge particles in the absence of large RF powers and look for a
correlation with impurity levels. Examining data from the moly monitor, 2pi
bolometer, and the calculated main plasma power from the bolo array, we see that
there is no measurable increase in impurity level due to PDI or energetic edge
particles on Alcator C-Mod.

The run was plagued by fizzles and disruptions: on 36 attempts we had
16 full plasmas, 10 disruptions before 550ms, 7 fizzles, and 3 duds. Also,
the PCX lost several shots because the gate valve closed early (this is part of
a system to prevent excess gas pressure from damaging detectors).

In the 2.8 T range, there was apparently a very weak ohmic h-mode
throughout the flattop on almost every shot, with some stronger elm-free
periods during RF. The density crept up during the dithering, and rose
sharply during the elm-free h-mode periods.

The disruptions were unfortunately quite repeatable. In the 3.4T
low-field startup part of the run, the plasmas that disrupted did so at 220ms,
with concurrent moly injections. The plasma would then limp along at 200kA
until around 450ms. These plasmas had a dip in q95 at 220ms, but only down to
3.2 in some cases. The plasmas that went all the way also had q95 down to 3.1
at the same period, but without a problem.
The second half of the run, with the high-field startup, had disruptions
characterized by a density droop down to nl04=.34e20 at 500ms. All the settings
were identical to those of shots that went. Wild speculation is that this might
be related to wall fueling.

These are the full length shots:

03 Plasma remains outboard limited, only 1 7kW RF pulse, Bt=3.47T, nl04~=.6
06 .5cm outer gap, 4 RF pulses in flattop, up to 80kW
11 1cm outer gap, PCX at 20cm (sightline ~40° from perpendicular at LCFS)
13 similar, PCX at 10cm
16 sim., added a 500kW RF pulse, PCX at perpendicular
Install breaker, go to 5T startup and 2.75T flattop
20 long dithering h-mode, with elm-free periods, density slowly rising
throughout, flux to PCX much lower than expected (erroneously believing this
to be due to h-mode, we tried to get rid of h-mode and left analyzer at
perpendicular)
21 sim.
22 sim., JT injecting stuff at ~600ms (and for many shots after)
24 sim., PCX gate valve closed
25 sim.,
26 sim., put 20kW RF in TF ramp, see that PCX flux is more sensitive to field
today than past measurements indicate, so slightly modify TF. These shots
give good info on how sensitive threshold is to exact edge Bt.
28 good plasma at 2.82T, early PCX GV, mistrigger RF SpecAn. Outer gap ~1cm
29 sim., but got data!
32 sim., early PCX GV, PCX at 20cm
34 sim., but lost an RF pulse. Mike F. is looking for it.....
36 sim., but rearranged RF pulse heights PCX at 10cm

Physics Operator Summaries
Entered: Jul 7 2004 04:36:56:223PM
Author: To Be Determined
Physop Summary for 960223 (second part)

MP125A ERS/PEP
SL Porkolab
PO wolfe
EO Daigle

We began the run at 5PM after the conclusion of the MP141 run.
The breaker had been repaired during the afternoon, allowing us to operate at
5.3T again. The EF1 problem has not recurred since the PF breaker was pulled
yesterday, and seems to in fact have been a consequence of the breaker
problem.

Started from shot 960221035, the successful shot from the first try at this
run. A-side, which had had a D2/H2 mix for the first part of the run, was
purged and filled with D2. The H concentration was therefore dropping through
the run, starting from about 10%.

In view of the fact that we only had four hours, it was decided to try
combining the PEP mode and ERS studies in the same shots, with a pellet
injected at .8sec.

Proposed run plan for ERS/PEP run on 960223, same as on 960221. .

Part I. Negative central shear
------------------------------
Start from a standard fast 800kA startup, like a fiducial, but bring RF on as
early as possible. Things to try:
reduce early density
move position out earlier to match antenna (maybe use loading
feedback?)
Try small pellet during current rise, before RF.

Monitor sawtooth onset, neutron rate. Note that automatic EFIT stored energies
will be meaningless for inverted pressure profiles, but we may be able to get
something from w_diamagnetic.

If we seem to be getting anything reproducible, try popping some Li pellets to
get a cigar measurement of Bz(R).

Part II. PEP modes
-------------------
If feasible, this part can be started during the late flattop of shots from
the first part of the run.

Set up standard 800MA plasma. Vary pellet timing relative to RF turn-on to
optimize neutron rate. Document it to death, including Sc injections for
tau_p. May want to try a pre-pellet Sc injection as well.

Results:
--------
All of the technical objectives were achieved, except that moving the RCUR
programming to better match the antenna was not tried. We did turn on the RF
loading feedback at the beginning of Seg 1, at low gain (-1000.). RF turned on
as early as 70msec, with 2MW by 100msec. Yuichi is to be congratulated for
accomplishing the tuning necessary to couple to this moving target. The peak
electron temperatures reached before sawtoothing were over 5keV. H-modes were
obtained on all shots, with lots of dropouts; good but not great H-factors
(transiently above 2). The first H-mode seemed to start at about the time of
sawtooth onset, possibly triggered by the first sawtooth.

The late PEP modes were similar to others since boronization, not well
sustained and neutron rates around 2e13. Ni injection before the second pellet
showed essentially infinite impurity confinement in the PEP phase, before the
H-mode set in.

On shot 42 the density programming was lowered to .5e20, which increased the
Te and may have helped delay sawtoothing some.

Sawtoothing was not delayed further than 230msec, compared to 180msec without
early RF. There was no evidence of ERS mode improved confinement. Darren got
some cigar data from the early pellets, although the data is limited because
he had a problem with his tracker and because the penetration was low even for
the big pellets. The density perturbation was surprisingly small. There seemed
to be little effect on the sawtooth onset, and the neutron rate seemed to be
suppressed if affected at all.

The current rise disruptions (before 100msec) were partly suppressed by the
early RF. Shot 44 has a good example of MHD on the ECE during the current
rise. On shot 45 Joe moved the fast magnetics to .080-.210sec to look at
activity around the disruption at 90msec and the pellet at 180. The disruption
was found to be associated with an m=4 locked mode. Reducing the OH voltage
between 50 and 100msec on shot 49 seemed to get rid of the last vestiges of
the locked mode.

The last shot (50) was an attempt to get better pellet penetration by shooting
two big pellets, but the shot fizzled.

The plasma was surprisingly robust, disrupting only on two shots (39,, after the
second pellet when there was no RF following it.

There was a problem with the cell air to the Li pellet injector caused by a
freeze up in the air hose due to ice from the bus tunnel building up as far as
Kport. This was corrected between shots 42 and 43. This could have caused a
serious problem, and should be dealt with on a more permanent basis.

Scorecard
---------
Shots 14 (37-50)
Plasmas 13
Fizzles 1


Entered: Jul 7 2004 04:36:56:240PM
Author: To Be Determined
Physics operator's summary for run 960223A:

MP #141, RF edge physics.

SL: Rost/Reardon
PO: Granetz
EO: V. Bertolino

Today's run will study the parametric decay of RF waves at the edge of the
plasma. This is most easily studied at low fields in L-mode. About four
shots at each of three fields (2.75, 3.40, and 3.00 T) will be required.
The plasma current will be 0.55 MA. The plasma composition will be 7.5% H and
92.5% D. RF power will be varied in steps from 0.1 to 0.8 MW.

Summary: The first half of the run was spent trying to get breakdown at 3.4
tesla. This was partially successful, with about 1 out of every
3 shots providing good RF probe data. Shortly after noontime, the
faulty breaker was fixed and installed, allowing for more typical
(and reliable) plasma initiation at 4.8 tesla, ramping down to
2.75 tesla (2.82 tesla late in the day). The plasmas we obtained
here were very good, with Ip=450-550 kA, nl_04=0.5-0.7e20 m-2, and
flattops lasting to 1.5 s. Lots of RF probe data were obtained. There
were, however, ohmic H-modes on every shot, although they were really
wimpy. There were no power supply problems today.

Scorecard: 26 plasmas (but 10 disrupted before RF turnon)
7 fizzles
0 tests
3 duds (none due to power supplies)
----------
36 total

Run plan:

Load from yesterday's low-field (3.4 T breakdown) shot #960222027,
except decrease early Ip programming demand to try and avoid reaching
q=3. This particular shot lasted less than 0.2 s, but it's the only
recent shot with low-field breakdown and current rise. The low-field
breakdown is necessary because of a problem with 2 breakers, which
has temporarily left only 2 of 4 TF cabinets operational. This is
also why we cannot begin the run with a fiducial plasma shot.

If we are successful at getting good 3.4 tesla plasmas, we will switch
to hybrid control of the TF so that we can run shots at 3.0 and 2.75 tesla.

Engineering setup for Tuesday 23 Feb 1996:

Discharge clean in helium for a couple of hours before the run.

A-side (actually K-side) plenum: 1.5 psi of H2 and 18.5 psi of D2
B-top plenum: 5 psi of deuterium.
B-side-lower plenum: 4 psi of argon.
NINJA plenum: make sure this is pumped out.
Enable hybrid control of A-side, B-top, and B-side-lower valves for start
of run.
Enable the ECE, VUV, Moly monitor, PCX, and TCX valves, assuming status of
each is okay.

Use engineering settings from shot 960222027 (low-field breakdown shot
from yesterday).

After (if?) we establish a 3.4 tesla shot, we will ask for hybrid control
of the TF so that we can go to 3.0 and 2.75 tesla.

Detailed shot log:

Shot 01 -- Plasma, but it looks like it got hit by a brick at 0.2 s, leading
to a termination at 0.44 s. q95 stayed above 3.1, and the plasma
was well away from the outboard limiter at the brick injection time.

Next shot: repeat with no changes.

Shot 02 -- Fizzle. Null looks reasonable. Pre-fill pulse duration is 19 ms,
but this is what Joe found was necessary yesterday, so I'll keep
it that long for now.

Next shot: repeat with no changes.

Shot 03 -- Plasma. Good shot, except that the plasma was limited on the
outboard limiter for nearly the entire duration. Ip=0.56 MA,
Bt=3.4 T, nl_04=0.68e20 m-2. q95=4 during flattop, but briefly
touches 3.0 early in the shot. No ohmic H-modes.

Next shot: reduce RCUR by 5 mm in order to generate an outer gap
of about 1 cm

Shot 04 -- Plasma, but a series of moly injections starting at 0.2 s finally
terminates the plasma at 0.46 s. Very similar to shot 001. The
injections begin at about the same time that q95 briefly drops to
3.0, so perhaps there's a connection.

Next shot: reduce early Ip programming demand to try and keep
q95 above 3 at all times.

Shot 05 -- Fizzle. No surprise, given the 001/002 shot sequence.

Next shot: repeat with no changes.

Shot 06 -- Plasma, good shot. Bt=3.4 T, nl_04=7.3e20 m-2. Density is
higher than previous good shot, even though no changes have been
made. Outer gap was only a couple of mm at best. q95 briefly
went down to 3.1, but plasma managed to survive this time. RF
pulses look very good.

Next shot: decrease RCUR by another 4 mm, and decrease early Ip
programming again.

Shot 07 -- Plasma, but a series of moly injections starting at 0.2 s finally
terminates the plasma at 0.46 s. Very similar to shot 001 and 003,
even though q95 is no longer flirting with 3.0.

Next shot: if I do nothing, I bet there'll be a fizzle, so I'll
do something: shorten pre-pulse puff duration from 19 to 17 ms.

Shot 08 -- Plasma, but a series of moly injections starting at 0.2 s finally
terminates the plasma at 0.35 s. q95 doesn't go below 3.2. At
least it didn't fizzle! Unfortunately, there's no fast infrared
camera, so we can't see where these moly injections are coming
from.

Next shot: no changes.

Shot 09 -- Dud. It turns out that for the last several shots we've been having
a small RF pulse at t=0. For this shot, it was turned off. Looks
like it might have been doing something after all.

Next shot: repeat, except have the RF turned on at t=0.

Shot 10 -- Fizzle.

Next shot: increase pre-pulse gas puff durations from 17 to 19 ms.

Shot 11 -- Plasma. Good shot. Outer gap is about 1 cm. Good RF performance.
Nice RF probe data. It's showing different stuff than on shot 006,
which had a much smaller outer gap.

Next shot: repeat with no changes.

Shot 12 -- Dud. How's that for reproducibility!

Next shot: increase Br by 0.5 mT (from 4.5 to 5.0 mT).

Shot 13 -- Plasma. Good shot. Good RF. Good data.

Next shot: no changes. Jim Reardon is changing his RF probe
position.

Shot 14 -- Fizzle. %*$#&#@^!!

Next shot: repeat with no changes.

Shot 15 -- Fizzle again.

Next shot: on Steve W's suggestion, I'll raise Bz by increasing
I_EF4 from -1200 to -1185 amps.

Shot 16 -- Plasma. It turned out to be an okay shot, only because it just
barely survived two huge moly injections at 0.2 s. The plasma
current trace looks truly bizarre. But the data are good, and
there was an additional RF pulse late in the flattop which reached
0.5 MW.

Next shot: repeat with no changes.

Shot 17 -- Plasma. Disrupted at 0.36 s, accompanied by a large Mo injection.

At this point in the run, the breaker has been repaired, and we are having a
short pause to install it. All four TF cabinets will now be available.

Next shot: repeat with no changes. Keep the PLC limit at 100 kA
(3.4 T startup)

Shot 18 -- Plasma. Disrupted at 0.35 s, just like the last shot. The plasma
is hitting the outboard limiter around this time.

Next shot: since we now have all four TF cabinets, we will abandon
low-field startups and recall a shot which started at 4.8 tesla
and ramped down to 2.6 tesla (960118032). However, changes will be
made to ramp the field down to 2.75 tesla (under hybrid control),
AND THE FLATTOP WILL BE EXTENDED TO 1.5 s!

Shot 19 -- Dud. Not surprising, since the startup from 960118032 needed to
be adjusted last Tuesday as well.

Next shot: reduce Br from 6.6 to 5.5 mT.

Shot 20 -- Plasma. Good shot, except there were H-modes at the higher RF
powers and lower fields. Bt=2.75 T, flattop lasted until the
plasma disrupted at t=1.54 s. Outer gap is small. Don't quite
know what to do to prevent H-modes.

Next shot: tweak RXL at the request of Brian L.

Shot 21 -- Plasma. Good shot. Very similar to previous shot. H-modes even
in ohmic phase.

Next shot: reduce Ip demand from 580 to 550 kA, and reduce density
a bit as well.

Shot 22 -- Plasma. Good shot. A little less H-modey than the previous shots,
at least until the higher RF powers.

Next shot: slightly lower density. Also bring CLEARIN down faster
after t=1.5 s.

Shot 23 -- Plasma, but disrupted at t=0.48 s. I don't think this one was
caused by any moly injections. Not sure what caused it.

Next shot: tweak up the density around 0.4 s.

Shot 24 -- Plasma. Good shot, but there are still some H-modes.

Next shot: lower Ip and nl some more.

Shot 25 -- Plasma. Good shot. Ip is now down to 0.50 MA. There are still
H-modes.

Next shot: no changes

Shot 26 -- Plasma. Good shot. Still have H-modes.

Next shot: reduce Ip to 450 kA. Also increase Bt from 2.75 to 2.82
tesla.

Shot 27 -- Plasma, but disrupted at 0.48 s for unknown reasons.

Next shot: repeat with no changes.

Shot 28 -- Plasma. Good shot. Ip is now 450 kA. Bt=2.82 T.

Next shot: no changes

Shot 29 -- Plasma. Good shot. Same as previous one.

Next shot: no changes

Shot 30 -- Fizzle. Null looks okay.

Next shot: repeat

Shot 31 -- Plasma, but disrupted at 0.53 s. On the shots that disrupt early,
the density is noticeably lower than on shots which don't disrupt.

Next shot: tweak the density up around 0.4 s.

Shot 32 -- Plasma. Good shot. Same as 028 and 029.

Next shot: no changes

Shot 33 -- Fizzle. Null is okay.

Next shot: repeat with no changes

Shot 34 -- Plasma. Good shot. Same as 028, 029, and 032.

Next shot: repeat with no changes

Shot 35 -- Plasma, but disrupted at 0.54 s.

Next shot: repeat

Shot 36 -- Plasma. Good shot. Same as 028, 029, 032, and 034.

End of this portion of the run (i.e. MP #141)

Following this, Steve Wolfe and Miklos Porkolab will take over for the extended
portion of today's run, which is devoted to the ERS/PEP MP.

Session Leader Comments
Feb 23 1996 05:46:51:480PM960223037Miklos PorkolabExperimental Plan:
To continue ERS run from 960221 starting at 5:00 pm;
Machine operating at 5.3 Tesla;

SL: M. Porkolab
PO: S. Wolfe
EO: J. Daigle

Shot was successfull, operate at 800 kA, RF power about 600 kA.
No pellets yet.

Feb 23 1996 05:56:29:750PM960223038Miklos PorkolabGood shot, Early RF first about 1 MW and then step up with
second transmitter to 2 MW. No pellet.

Feb 23 1996 06:03:41:560PM960223039Miklos PorkolabGood shot, first pellet injected around 0.8 second, RF power between
1-2 MW in a ragged form. Plasma decays away rather quickly after
pellet injection. Stored energy around 100 kJ. Not a good pellet shot
performance - wise.

Feb 23 1996 07:00:50:390PM960223040Miklos PorkolabGood shot,but Rf power only about 1 MW.

Feb 23 1996 07:03:01:910PM960223041Miklos PorkolabGood shot, RF power about 2 MW, early into the shot. But no evidence
of ERS mode ?

Feb 23 1996 07:34:46:890PM960223042Miklos PorkolabGood shot, Rf power about 1.9 MW, max. stored energy about
120kJ, early on. Electron temperature above 4.2 keV. No pellet.

Feb 23 1996 07:42:00:700PM960223043Miklos PorkolabInitial power only 1 MW, electron temperature 4 keV,
pellet at 0.8 sec, but no RF during pellet.

Feb 23 1996 07:53:07:840PM960223044Miklos PorkolabInitial power only 1 MW, quickly rising to 2 mW around 120 ms.
Electron temperature up to 5 keV due to low initial density.
Pellet injected at 0.8 sec, and there was 1 MW of RF power
on top of it. PEP mode ??

Feb 23 1996 08:25:07:770PM960223046Miklos PorkolabInitial power only 1 MW, quickly rising to 2 MW around 200 ms.
Electron temperature up to 5 keV during 2 MW, but only 3 keV
during pellet. 1st small pellet injected at 180 ms, 2nd pellet at 800 ms..

Feb 23 1996 08:40:36:280PM960223047Miklos PorkolabWe got 5.0 keV Te, at 1.8 MW RF power early on, before sawteeth
came on at 200 ms. No pellet in this shot.

Feb 23 1996 08:56:30:980PM960223048Miklos PorkolabGood shot, 1.9 MW RF power early, at 100 ms, pellet injected at
200 ms, Te drops from 5.0 keV to 3.8 keV, then sawteeth enter.
Apparently we have small locked mode activity around 80-90 ms.

Feb 23 1996 09:03:59:970PM960223048Miklos PorkolabGood shot, 1.9 MW RF power early, at 100 ms, pellet injected at
200 ms, Te drops from 5.0 keV to 3.8 keV, then sawteeth enter.
Apparently we have small locked mode activity around 80-90 ms.

Feb 23 1996 09:14:03:280PM960223049Miklos PorkolabGood shot, slowed down current ramp initially. Did not make much
difference in parameters.

Feb 23 1996 09:14:50:920PM960223050Miklos PorkolabFizzle.

Physics Operator Comments
Feb 23 1996 08:18:21:170AMRobert GranetzMP #141, RF edge physics.

SL: Rost/Reardon
PO: Granetz
EO: V. Bertolino

Today's run will study the parametric decay of RF waves at the edge of the
plasma. This is most easily studied at low fields in L-mode. About four
shots at each of three fields (2.75, 3.40, and 3.00 T) will be required.
The plasma current will be 0.55 MA. The plasma composition will be 7.5% H and
92.5% D. RF power will be varied in steps from 0.1 to 0.8 MW.

Feb 23 1996 08:18:42:100AMRobert GranetzRun plan:

Load from yesterday's low-field (3.4 T breakdown) shot #960222027,
except decrease early Ip programming demand to try and avoid reaching
q=3. This particular shot lasted less than 0.2 s, but it's the only
recent shot with low-field breakdown and current rise. The low-field
breakdown is necessary because of a problem with 2 breakers, which
has temporarily left only 2 of 4 TF cabinets operational. This is
also why we cannot begin the run with a fiducial plasma shot.

If we are successful at getting good 3.4 tesla plasmas, we will switch
to hybrid control of the TF so that we can run shots at 3.0 and 2.75 tesla.

Feb 23 1996 08:19:14:300AMRobert GranetzEngineering setup for Tuesday 23 Feb 1996:

Discharge clean in helium for a couple of hours before the run.

A-side (actually K-side) plenum: 1.5 psi of H2 and 18.5 psi of D2
B-top plenum: 5 psi of deuterium.
B-side-lower plenum: 4 psi of argon.
NINJA plenum: make sure this is pumped out.
Enable hybrid control of A-side, B-top, and B-side-lower valves for start
of run.
Enable the ECE, VUV, Moly monitor, PCX, and TCX valves, assuming status of
each is okay.

Use engineering settings from shot 960222027 (low-field breakdown shot
from yesterday).

After (if?) we establish a 3.4 tesla shot, we will ask for hybrid control
of the TF so that we can go to 3.0 and 2.75 tesla.

Feb 23 1996 08:35:34:470AM960223001Robert GranetzShot 01 -- Plasma, but it looks like it got hit by a brick at 0.2 s, leading
to a termination at 0.44 s. q95 stayed above 3.1, and the plasma
was well away from the outboard limiter at the brick injection time.

Next shot: repeat with no changes.

Feb 23 1996 08:49:06:650AM960223002Robert GranetzShot 02 -- Fizzle. Null looks reasonable. Pre-fill pulse duration is 19 ms,
but this is what Joe found was necessary yesterday, so I'll keep
it that long for now.

Next shot: repeat with no changes.

Feb 23 1996 09:03:43:110AM960223003Robert GranetzShot 03 -- Plasma. Good shot, except that the plasma was limited on the
outboard limiter for nearly the entire duration. Ip=0.56 MA,
Bt=3.4 T, nl_04=0.68e20 m-2.

Next shot: reduce RCUR by 5 mm in order to generate an outer gap
of about 1 cm

Feb 23 1996 09:20:35:980AM960223004Robert GranetzShot 04 -- Plasma, but a series of moly injections starting at 0.2 s finally
terminates the plasma at 0.46 s. Very similar to shot 001. The
injections begin at about the same time that q95 briefly drops to
3.0, so perhaps there's a connection.

Next shot: reduce early Ip programming demand to try and keep
q95 above 3 at all times.

Feb 23 1996 09:22:29:240AM960223005Robert GranetzShot 05 -- Fizzle. No surprise, given the 001/002 shot sequence.

Next shot: repeat with no changes.

Feb 23 1996 09:53:00:820AM960223006Robert GranetzShot 06 -- Plasma, good shot. Bt=3.4 T, nl_04=7.3e20 m-2. Density is
higher than previous good shot, even though no changes have been
made. Outer gap was only a couple of mm at best. q95 briefly
went down to 3.1, but plasma managed to survive this time. RF
pulses look very good.

Next shot: decrease RCUR by another 4 mm, and decrease early Ip
programming again.

Feb 23 1996 10:07:27:140AM960223007Robert GranetzShot 07 -- Plasma, but a series of moly injections starting at 0.2 s finally
terminates the plasma at 0.46 s. Very similar to shot 001, even
though q95 is no longer flirting with 3.0.

Next shot: if I do nothing, I bet there'll be a fizzle, so I'll
do something: shorten pre-pulse puff duration from 19 to 17 ms.

Feb 23 1996 10:26:41:790AM960223008Robert GranetzShot 08 -- Plasma, but a series of moly injections starting at 0.2 s finally
terminates the plasma at 0.35 s. q95 doesn't go below 3.2. At
least it didn't fizzle! Unfortunately, there's no fast infrared
camera, so we can't see where these moly injections are coming
from.

Next shot: no changes.

Feb 23 1996 10:32:16:640AM960223009Robert GranetzShot 09 -- Dud. It turns out that for the last several shots we've been having
a small RF pulse at t=0. For this shot, it was turned off. Looks
like it might have been doing something after all.

Next shot: repeat, except have the RF turned on at t=0.

Feb 23 1996 10:43:26:920AM960223010Robert GranetzShot 10 -- Fizzle.

Next shot: increase pre-pulse gas puff durations from 17 to 19 ms.

Feb 23 1996 11:00:31:460AM960223011Robert GranetzShot 11 -- Plasma. Good shot. Outer gap is about 1 cm. Good RF performance.

Next shot: repeat with no changes.

Feb 23 1996 11:07:27:960AM960223012Robert GranetzShot 12 -- Dud. How's that for reproducibility!

Next shot: increase Br by 0.5 mT (from 4.5 to 5.0 mT).

Feb 23 1996 11:21:29:010AM960223013Robert GranetzShot 13 -- Plasma. Good shot. Good RF. Good data.

Next shot: no changes. Jim Reardon is changing his RF probe
position.

Feb 23 1996 11:25:06:810AM960223014Robert GranetzShot 14 -- Fizzle. %*$#&#@^!!

Next shot: repeat with no changes.

Feb 23 1996 11:38:28:400AM960223015Robert GranetzShot 15 -- Fizzle again.

Next shot: on Steve W's suggestion, I'll raise Bz by increasing
I_EF4 from -1200 to -1185 amps.

Feb 23 1996 11:54:31:590AM960223016Robert GranetzShot 16 -- Plasma. It turned out to be an okay shot, only because it just
barely survived two huge moly injections at 0.2 s. The plasma
current trace looks truly bizarre. But the data are good, and
there was an additional RF pulse late in the flattop which reached
0.5 MW.

Next shot: repeat with no changes.

Feb 23 1996 12:26:16:410PM960223017Robert GranetzShot 17 -- Plasma. Disrupted at 0.36 s, accompanied by a large Mo injection.

At this point in the run, the breaker has been repaired, and we are having a
short pause to install it. All four TF cabinets will now be available.

Next shot: repeat with no changes. Keep the PLC limit at 100 kA
(3.4 T startup)

Feb 23 1996 12:58:17:660PM960223018Robert GranetzShot 18 -- Plasma. Disrupted at 0.35 s, just like the last shot. The plasma
is hitting the outboard limiter around this time.

Next shot: since we now have all four TF cabinets, we will abandon
low-field startups and recall a shot which started at 4.8 tesla
and ramped down to 2.6 tesla (960118032). However, changes will be
made to ramp the field down to 2.75 tesla (under hybrid control),
AND THE FLATTOP WILL BE EXTENDED TO 1.5 s!

Feb 23 1996 01:03:46:860PM960223019Robert GranetzShot 19 -- Dud. Not surprising, since the startup from 960118032 needed to
be adjusted last Tuesday as well.

Next shot: reduce Br from 6.6 to 5.5 mT.

Feb 23 1996 01:24:03:950PM960223020Robert GranetzShot 20 -- Plasma. Good shot, except there were H-modes at the higher RF
powers and lower fields. Bt=2.75 T, flattop lasted until the
plasma disrupted at t=1.54 s. Outer gap is small. Don't quite
know what to do to prevent H-modes.

Next shot: tweak RXL at the request of Brian L.

Feb 23 1996 01:36:06:120PM960223021Robert GranetzShot 21 -- Plasma. Good shot. Very similar to previous shot. H-modes even
in ohmic phase.

Next shot: reduce Ip demand from 580 to 550 kA, and reduce density
a bit as well.

Feb 23 1996 01:51:01:050PM960223022Robert GranetzShot 22 -- Plasma. Good shot. A little less H-modey than the previous shots,
at least until the higher RF powers.

Next shot: slightly lower density. Also bring CLEARIN down faster
after t=1.5 s.

Feb 23 1996 02:02:11:640PM960223023Robert GranetzShot 23 -- Plasma, but disrupted at t=0.48 s. I don't think this one was
caused by any moly injections. Not sure what caused it.

Next shot: tweak up the density around 0.4 s.

Feb 23 1996 02:10:25:870PM960223024Robert GranetzShot 24 -- Plasma. Good shot, but there are still some H-modes.

Next shot: lower Ip and nl some more.

Feb 23 1996 02:28:11:010PM960223025Robert GranetzShot 25 -- Plasma. Good shot. Ip is now down to 0.50 MA. There are still
H-modes.

Next shot: no changes

Feb 23 1996 02:42:51:150PM960223026Robert GranetzShot 26 -- Plasma. Good shot. Still have H-modes.

Next shot: reduce Ip to 450 kA. Also increase Bt from 2.75 to 2.82
tesla.

Feb 23 1996 02:54:40:820PM960223027Robert GranetzShot 27 -- Plasma, but disrupted at 0.48 s for unknown reasons.

Next shot: repeat with no changes.

Feb 23 1996 03:15:13:990PM960223028Robert GranetzShot 28 -- Plasma. Good shot. Ip is now 450 kA. Bt=2.82 T.

Next shot: no changes

Feb 23 1996 03:28:13:610PM960223029Robert GranetzShot 29 -- Plasma. Good shot. Same as previous one.

Next shot: no changes

Feb 23 1996 03:37:09:950PM960223030Robert GranetzShot 30 -- Fizzle. Null looks okay.

Next shot: repeat

Feb 23 1996 03:53:36:180PM960223031Robert GranetzShot 31 -- Plasma, but disrupted at 0.53 s. On the shots that disrupt early,
the density is noticeably lower than on shots which don't disrupt.

Next shot: tweak the density up around 0.4 s.

Feb 23 1996 04:09:28:150PM960223032Robert GranetzShot 32 -- Plasma. Good shot. Same as 028 and 029.

Next shot: no changes

Feb 23 1996 04:15:44:010PM960223033Robert GranetzShot 33 -- Fizzle. Null is okay.

Next shot: repeat with no changes

Feb 23 1996 04:24:13:260PM960223034Robert GranetzShot 34 -- Plasma. Good shot. Same as 028, 029, and 032.

Next shot: repeat with no changes

Feb 23 1996 04:53:29:760PM960223035Robert GranetzShot 35 -- Plasma, but disrupted at 0.54 s.

Next shot: repeat

Feb 23 1996 05:03:05:250PM960223036Robert GranetzShot 36 -- Plasma. Good shot. Same as 028, 029, 032, and 034.

End of this portion of the run (i.e. MP #141)

Following this, Steve Wolfe and Miklos Porkolab will take over for the extended
portion of today's run, which is devoted to the ERS/PEP MP.

Feb 23 1996 05:25:19:100PM960223037Steve Wolfe Proposed run plan for ERS/PEP run on 960221. May be modified in progress.

Part I. Negative central shear
------------------------------
Start from a standard fast 800kA startup, like a fiducial, but bring RF on as
early as possible. Things to try:
reduce early density
move position out earlier to match antenna (maybe use loading
feedback?)
Try small pellet during current rise, before RF.

Monitor sawtooth onset, neutron rate. Note that automatic EFIT stored energies
will be meaningless for inverted pressure profiles, but we may be able to get
something from w_diamagnetic.

If we seem to be getting anything reproducible, try popping some Li pellets to
get a cigar measurement of Bz(R).

Feb 23 1996 05:25:41:750PM960223037Steve Wolfe Part II. PEP modes
-------------------
If feasible, this part can be started during the late flattop of shots from
the first part of the run.

Set up standard 800MA plasma. Vary pellet timing relative to RF turn-on to
optimize neutron rate. Document it to death, including Sc injections for
tau_p. May want to try a pre-pellet Sc injection as well.

Feb 23 1996 05:26:47:570PM960223037Steve WolfeShot 960223037 - Changing experiments in mid-stream. Now going to
MP #125A ERS/PEP
SL Porkolab
PO wolfe

For run plan see Wednesday, 960221
Load shot 960221035
Purge a-side valve and refill with D2

Plasma, H-modes, full length.

Feb 23 1996 05:34:03:880PM960223037Steve WolfeShot 960223037 - only 1MW from RF. Sawteeth start at 180msec. Multiple
h-modes on and off.

Next shot - better RF, RF off at .7, pellet at .8

Feb 23 1996 05:48:41:160PM960223038Steve WolfeShot 960223038 - try for better RF, RF off at .7, No Li pellet at .8
because I forgot to tell them to open the gate valve.
Plasma full length. Rf faulting all the way through. On at .13 at 1MW
level, 2MW @ .157, sawteeth at .211.

Feb 23 1996 06:05:30:910PM960223039Steve WolfeShot 960223039 - try for better RF, RF off at .7, Li pellet at .8

ONly 1MW in early. Disrupted at .9sec, after pellet. No PEP mode.
Next shot drop density at .2sec to ,9e20 (from 1.0) and turn on RF
feedback at -1000 at .1sec

Feb 23 1996 06:23:38:510PM960223040Steve WolfeShot 960223040 - try for better RF, RF off at .7, Li pellet at .8,RF on
at .825. Drop density at .2sec to ,9e20 (from 1.0) and turn on RF
feedback at -1000 at .1sec
Plasma - multiple h-modes. pellet, possible PEP mode. sawteeth at .2sec,
when Te=3keV. RF only on at .15sec and only 1MW.

Feb 23 1996 06:47:21:970PM960223041Steve WolfeShot 960223041 - try for better RF, RF off at .7, Li pellet at .8,RF on
at .825 at 1MW. Raise seg1 PG3 to slow current rise a bit, get
rid of CR disruption.
Got 2MW in at 130msec. sawtoothing at 200msec; it ain't working.
PEP mode looks puny.

Feb 23 1996 07:02:09:460PM960223042Steve WolfeShot 960223042 -No pellet this time. Lowered nl04 at .2 to .5e20.
Try to start RF at .12sec. Darren has a problem- low cell air pressure.

Sawtoothing at .216, Te=4.7kev. Neutrons peak at 3e13 at .4sec

Feb 23 1996 07:22:49:850PM960223043Steve WolfeShot 960223043 - Try to get RF on at 50msec!
Darren's problem was a frozen air line! Fixed now.

Disruption at .9sec No RF before .1, only 1MW until .35.
No PEP mode.

Feb 23 1996 07:41:31:920PM960223044Steve WolfeShot 960223044 - Try to get RF on at 50msec!
5.2keV at 220msec when st start; RF on at .07sec (1MW) , 2MW at .1.
Early disruption is stil there - see ECE outer channels show MHD
Weak PEP mode.

Feb 23 1996 08:01:17:200PM960223045Steve WolfeShot 960223045 - Pop a small pellet at .180sec, fast magnetics to .08-.21

It survived!! Not much pellet effect. Looks similar to 44, but only 4.5keV
Might be a fragment

Feb 23 1996 08:10:02:820PM960223046Steve WolfeShot 960223046 - Pop a small pellet at .180sec, fast magnetics to .08-.21
same as 45 except SC injection 10msec before second pellet.

Looks similar to 45. Cigar on first pellet looks weird, sort of hollow.
Still hardly any density increase????
Second PEP mode still puny.

Feb 23 1996 08:25:46:010PM960223047Steve WolfeShot 960223047 - Pop a BIG pellet at .180sec, fast magnetics to .08-.21
same as 45 except SC injection 10msec before second pellet.
Darren's tracking system is screwed up, he needs a pit run to fix it
after this shot.

No pellets this time - operator error. Joe identifies the current rise
disruption as a locked mode.

Feb 23 1996 08:42:28:130PM960223048Steve WolfeShot 960223048 - Pop a BIG pellet at .180sec, fast magnetics to .08-.21
same as 45 except SC injection 10msec before second pellet.
Darren's tracking system is probably still screwed up, he couldn't
find anything. He may be able to reconstruct.

Still only a small density perturbation! Where are the particles?
Neutron rate looks lower???

Feb 23 1996 08:58:18:030PM960223049Steve WolfeShot 960223049 - Drop the OH1 and 2 voltages by 100V and 20V, respectively
Big pellet at 180 instead of 200 this time.

It survived. got the pellet in, around 4kev. sawteeth start around the same
time.

Feb 23 1996 09:09:56:520PM960223050Steve WolfeShot 960223050 - Two big pellets 180,185 msec.
fizzle. That's all!

Engineering Operator Comments
ShotTimeTypeStatusComment
108:24:09:630AMPlasmaBadef2l pulled out
208:41:16:920AMPlasmaOk
308:51:36:980AMPlasmaOk
409:04:31:460AMPlasmaOk
509:19:17:440AMPlasmaOk
609:37:36:440AMPlasmaOk
709:52:46:070AMPlasmaOk
810:13:44:230AMPlasmaOk
910:26:37:190AMPlasmaOk
1010:37:50:570AMPlasmaOk
1110:46:08:790AMPlasmaOk
1210:59:25:450AMPlasmaOk
1311:08:53:100AMPlasmaOk
1411:21:26:160AMPlasmaOk
1511:30:32:090AMPlasmaOk
1611:40:10:030AMPlasmaOk
1711:55:55:320AMPlasmaOk
1812:35:41:870PMPlasmaOk
1912:57:32:060PMPlasmaOk
2001:07:46:480PMPlasmaOk
2101:24:20:030PMPlasmaOk
2201:37:53:030PMPlasmaOk
2301:51:17:610PMPlasmaOk
2402:03:20:080PMPlasmaOk
2502:14:34:070PMPlasmaOk
2602:28:27:860PMPlasmaOk
2702:41:47:500PMPlasmaOk
2803:03:59:040PMPlasmaOk
2903:18:08:310PMPlasmaOk
3003:31:50:490PMPlasmaOk
3103:41:41:560PMPlasmaOk
3203:56:00:260PMPlasmaOk
3304:09:45:780PMPlasmaOk
3404:19:49:950PMPlasmaOk
3504:45:20:620PMPlasmaOk
3604:58:22:580PMPlasmaOkcomm fault OH1 & OH2L
3705:24:41:670PMPlasmaOk
3805:41:31:570PMPlasmaOk
3905:53:18:980PMPlasmaOk
4006:12:43:940PMPlasmaOk
4106:33:51:830PMPlasmaOk
4206:51:10:260PMPlasmaOk
4307:15:29:530PMPlasmaOk
4407:31:35:560PMPlasmaOk
4507:48:58:170PMPlasmaOk
4608:02:25:120PMPlasmaOk
4708:17:25:560PMPlasmaOk
4808:33:48:450PMPlasmaOk
4908:47:37:200PMPlasmaOk
5009:03:37:040PMPlasmaOkOH2u Bypass comm Fault OH1 self powered fired.