Alcator C-Mod Run 950111 Information

Back to runs

Miniproposals
Miniproposal:043
Date Filed: 3/31/1994
Title:Effect of edge radiation on divertor detachment
First Author:Gary McCracken
Session Leader:Gary McCracken (shots 1-31)

Operators
Session leader(s):Gary McCracken
Physics operator(s):John Goetz
Engineering operator(s):Vinny Bertolino,Joe Daigle

Engineering Operator Run Comment
diverter detachment

Session Leader Plans

Physics Operators Plans

Session Leader Summaries
Entered: Jul 7 2004 03:49:11:790PM
Author: To Be Determined
Session Leader Report for Run 950111
EO Daigle/Bertolino
PO J Goetz
SL G McCracken

The objective of the run was to study the effect of increasing
radiation on divertor detachment, as described in Miniproposal 043. A single
null diverted discharge was set up with the outer strike point near the bottom
of the vertical target plate (probe 2)and a density ramp which was initially
from 0.8e20 to 1.8e20 m^-2. An increasing amount of neon was then puffed in
successive shots to study the effect on detachment. We initially had early
disruptions when the neon was puffed in at 0.3 s. The feedback control of the
outer strike point had been turned on to try and maintain the strike point at a
constant position during the discharge and it was initially thought that it was
this feed-back control was the cause of the disruptions. However the radiation
was very high even when quite modest amounts of neon was injected and it turned
that this was the cause of the disruptions. When the neon was injected at 0.5
s, after the current flat top had been reached, there were no further problems.
Incidentally at one point the gas puff was turned off during the discharge and
one of the lowest densities so far achieved on C-Mod , nel04<2e19,was
recorded. The measured Zeff reached 30!
Starting with shot #011, an increasing amount of neon was injected and
the critical density for detachment decreased from about 1.4e20 (near the end
of the density ramp) to 0.85e20 m-2, shortly after the neon was injected. With
increasing neon the power radiated also increased so that the power crossing
the LCFS into the SOL decreased from about 800 kW with no neon, to less than
200 kW with a large neon injection. Shot 023 was the one with the maximum
amount of neon without disruption. A number of background shots were run,
with no neon. These were notable for having almost zero neon, ie there was much
less hold up in the walls than argon. With hindsight it was realised the we
should have reduced the starting value of the density ramp and we may well have
got detachment at even lower densities.
The neon was injected through the upper B-side valve. Plenum pressures
from 1.6 to 5 psi were used , but from shot 018 on the pressure was 3 psi. The
valve voltage pulselength was varied from 20 to 60 ms. It was found that up
to 40 ms comparitively little effect was observed but that there was a very
sudden transition between 40 and 60 ms pulse. Good Ne I and Ne VIII signals were
obtained on the oma and the McPherson respectively, for most shots. Scanning
probe profiles were also taken for many discharges.
The last 2 shots 030 and 031 were non standard. For shot 030 a small
puff of neon (3 psi, 20ms) was puffed into a discharge at constant density to
study the recycling of neon in steady state conditions. The neon reached a
maximum and then decayed roughly exponentialy to a steady state level. In the
last shot the density was kept constant at 1e20 m-2 and the neon concentration
increased throughout the shot by a succession of 20 ms puffs, 50 ms apart. The
neon concentration increased in steps resulting in increasing degrees of
detachment and then finally in a disruption at 0.8 s.Towards the end of the
pulse the radiation exceed the input power.

Future studies should examine the effects at even lower densities and
also the effect of other impurity gases (eg Ar)as a means of increasing
radiation and changing the radial profile of radiation in the main chamber.

Shot Summary

001 Good shot, constant density, nel04=8e19 m^-2, no neon
002 Good shot, density ramp from 1e20 to 2e20 no neon
003 Dud
004 Good shot, density ramp from 0.8e20 to 1.8e20, no neon
005 neon puff 5 psi, 20 ms at 0.3 s. No D2 puff due to feedback failure
nel04<2e19, Zeff = 30 maximum
006 Disrupted at 0.47 s
007 Fizzle
008 Disrupted at o.47 s
009 Strike point control turned off, still disrupted.
010 Fizzle
011 No neon in. Detachment at about 0.7 s, but the situation is confused
because the strike point is moving up the target plate
012 Neon injection for 20 ms at 0.5 s. Plenum pressure 1.6 psi. Detachment at
~0.6 s on probe 3, but strike point still moving during the discharge
013 Neon injection for 20 ms at 0.5 s. Plenum pressure 1.6 psi. Detachment at
~0.7 s, Strike point better

Some of the parameters of the more interesting shots are shown below.
The power into the SOL is the lowest value occurring during the shot.
The value at detachment is usually higher ~ 600 kW. In some cases, with high
neon injection, detachment occurs very early and then the plasma reattaches,
possibly due to the decay in the neon level. It then detaches again at higher
density, eg shots #020 and 029. Shots #019 and 020 had 5 mm outer gap and
are atypical.

Neon Time of detachment Density at detachment Power into SOL
s nel04 kW

013 1.6psi ,20ms 0.7 1.34 710
014 1.6psi ,30ms 0.7 1.34 670
015 1.6psi ,50ms 0.7 1.35 560
016 5.0psi ,30ms 0.54 1.03 260
017 no neon 0.77 1.41 770
018 3.0 psi ,20ms 0.89 1.39 705
019 3.0 psi ,30ms 0.86 1.37
020 3.0 psi ,40ms 0.55 & 0.81 0.89 & 1.23 340
021 3.0 psi ,30ms 0.88 1.34 670
022 3.0 psi ,40ms 0.81 1.24 640
023 3.0 psi ,60ms 0.56 0.89 <200
024 3.0 psi ,50ms 0.56 0.87 400
025 no neon 800
026 dud
027 3.0 psi ,40ms 0.81 1.28 600
028 3.0 psi ,50ms 0.56 0.89 600
029 3.0 psi ,45ms 0.56 & 0.83 0.89 &1.28 600
030 3.0 psi ,20ms 720
031 5 X3.0 psi ,20ms 0.6 & 0.67 0.96 & 0.96 800 to 0



Physics Operator Summaries
Entered: Jul 7 2004 04:36:52:850PM
Author: To Be Determined
Physics operator summary for 950111

EO: Daigle/Bertilino
PO: Goetz
SL: McCracken

Run 950111 was in support of Mini-Proposal #043 - Effect of edge radiation
on divertor detachment. The goal of this mini-proposal is to investigate
the effect of enhanced radiation on the critical density for detachment and
study the effect of high edge impurity concentrations on the molybdenum
influx (MoI) and central molybdenum (MoXXXI) concentration.

Program for this run:
- Setup a lower SN discharge with the outer strike point halfway up
the outer plate and with parameters: Ip=0.8MA; Nel_04=0.8e20;
outer gap > 1.5cm; and inner gap > 1.5cm
- Raise the density linearly during the discharge to cause detachment
of the divertor
- Puff neon through the valve at B_SIDE_UPPER to observe the changes
in detachment characteristics ( if any ) and observe the
various charge states of molybdenum
- Repeat with argon (if there is time)

These goals were not quite accomplished as there was not time to get to the
argon puffing. Various amounts of neon were puffed into discharges of varying
density. See the SESSION_LEADER summary for a more detailed description of
the physics results.

Some things discovered today:
1) Be careful when puffing impurities into a non-diverted discharge, the
plasma will readily accept the impurity. This leads to a radiation
induced disruption which is easily mistaken for an EF2 rail problem.
2) The startup scenario used today led to a rubbing of the nose
between 0.4 and 0.5 sec. This appears to have only liberated
deuterium and doesn't seem to lead to an increase in moly influx.
So maybe some attention needs to be payed to early control of the
x-point position.
3) At the higher densities run today, the discharge disrupted during
ramp-down. Playing the standard tricks with RCUR and CLEARIN didn't
seem to help. Some attention should be devoted to developing a
rampdown scheme that is independent of plasma current and density.
4) The STRKPSI controller was used today with some success ( once the
physics operator finally realized what 0. meant - 0. is the nominal
strike point, around probe O4). The strike point was held quite
constant, which is important in trying to determine detachment effects
across the divertor plate.

Engineering and computing today: OH2L had two comm. faults today - one after
a discharge and one during precharge. Otherwise, a good day. Once
again a PCS bug was uncovered. When the wires were shuffled to bring
the STRKPSI controller into the segment 2 that was in use, the
unlinking was not performed correctly. This resulted in the STRKPSI
waveform being written into the NL_04 waveform and the resulting shot
had a density approaching zero ( as requested ).

Scorecard: 31 shots = 27 plasmas + 3 fizzles + 1 p.s. dud

Shot summary for Run 950111

Reload of 950110032

Changes to shot 950110032:
NL_04 draw to 0.8e20

Shot change result
____ _____ ______
1 plasma - 0.8MA - good rampdown
nl_04=0.8e20

2 draw nl_04 ramp from 0.8e20 @ 0.3 plasma - 0.8MA, but drooping
to 2.0e20 @ 0.95 disrupts at 1.3sec from a
modified shark fin
nl_04 ramps to 2.0e20

3 density ramp to 1.8e20 fizzle - nothing out of the
ramp up Ip waveform ordinary
slow down RCUR and CLEARIN ramps

4 P_0=1.5e-5 plasma - disr @ 1.4 - disr@1.4
outer strike point drifting up

5 move NL_04 to wire 14 and STRKPSI plasma - disr. @ 1.44
to wire 9 in segment 2 outer strike better
enable B_SIDE_UPPER nl_04 < 0.2e20 due to PCS bug

6 repair NL_04 waveform plasma - disr. @ 0.45
P_0=1.6e-5 EF2's on the rail
STRKPSI=-.0011

7 stairstep on P gain of STRKPSI fizzle

8 P_0=1.5e-5 plasma - disr. @ 0.46
EF2's on the rail

9 turn off gain on STRKPSI controller plasma - disr. @ 0.47
blame it on the neon

10 remove hybrid enable from B_SIDE_UPPER fizzle

11 no changes plasma - disr. @ 1.38

12 P gain on STRKPSI on @ 0.5 plasma - disr. @ 1.38
pressure in B_SIDE_UPPER = 1.6PSIA STRKPSI was still off
hybrid enable B_SIDE_UPPER
PG2 = 100Vx.02sec @ 0.5sec

13 turn on STRKPSI P gain plasma - disr. @ 1.38
outer strike still moving

14 STRKPSI=-.00125 plasma - disr @ 1.36
PG2 = 100V x .03sec outer strike still moving 3cm

15 P gain on ZXL=2.5 @ 0.5sec plasma - disr. @ 1.34
PG2 = 100V x .05sec outer strike o.k. @ 0.9sec

16 PG2=100Vx.02sec and pressure = 5.0PSIA plasma - disr @ 1.24
STRKPSI = -.0011 all time strike point terrible

17 disable B_SIDE_UPPER plasma - disr @ 1.39
STRKPSI=-1e-4 - P gain=6
RXL=-.01 - P gain = 1
ZXL=-.005 - P gain = 3

18 nl_04 ramp from 0.6e20 to 1.5e20 plasma - disr. @ 1.30
enable B_SIDE_UPPER with 3.1 PSIA strike point good after 0.65sec

19 PG2=100Vx.03sec plasma - disr. @ 1.32
RCUR=.667 no EFIT

20 PG2=100Vx.04sec plasma - disr. @ 1.28
RXL gain=2 @ 1.0sec and STRKPSI gain outer gap is 0.5cm!!
off @ .95

21 RCUR=0.6655 plasma - disr. @ 1.33
PG2=100Vx.03sec back to where we were on 018

22 PG2=100Vx.04sec plasma - disr. @ 1.30

23 PG2=100Vx.06sec plasma - disr. @ 1.28

24 PG2=100Vx.05sec plasma - disr. @ 1.28

25 disable B_SIDE_UPPER plasma - disr. @ 1.33

26 PG2=100Vx.04sec and hybrid enable power supply dud
OH2L comm. fault

27 no changes plasma - disr. @ 1.29

28 PG2=100Vx.05sec plasma - disr. @ 1.30

29 PG2=100Vx.045sec plasma - disr. @ 1.29

30 NL_04=1.0e20 from 0.5 to 0.95sec plasma - disr. @ 1.35
PG2=100Vx.02sec no div. detachment

31 [PG2=100Vx.02sec] x 7 pulses plasma - disr. @ 0.79
starting at 0.5sec every .07sec due to too much neon

Session Leader Comments
Jan 11 1995 08:32:59:840AMGary McCrackenObjective: Mini-Proposal#043: To investigate the effect of enhanced radiation on
the critical density for detachment. To study the effect of high edge impurity
concentrations on the Mo influx (MoI) and central Mo concentration

Run Plan: Set up a single null diverted discharge with the outer strike
point about probe 6 on the outer target. Divert at 0.3 s and arrange a
density ramp with the feedback control to obtain detachment at the end of the
ramp. Then in successive discharges puff in neon at a gradually increasing
levels to try and induce detachment at lower density. The neon puff will be for a
short pulse at 0.3 s from the B side top valve, similar to the HIREX argon pulse.
If time permits we will use argon in the same mode. The intention is to go
to close to 100% radiation, so that power into the SOL is a minimum.

Jan 11 1995 06:21:38:420PMGary McCrackenSummary: Overall a successfull day with the main objectives of MP 043 being
achieved. By increasing the amount of neon injected in sucessive shots the
amount of power radiated was increased and the power into the SOL decreased
from about 800 kW to nearly zero. As a result the density for detachment was
decreased from nel04= 1.4e20 to at least 1e20. m^-2.

Jan 11 1995 08:59:41:640AM950111001Gary McCrackenObjective: Mini-Proposal#043: To investigate the effect of enhanced radiation on
the critical density for detachment. To study the effect of high edge impurity
concentrations on the Mo influx (MoI) and central Mo concentration

Start with a repeat of yesterdays shot #950110032. Good shot. nel04=8.2e19 m-2
from 0.3 - 0.9 s. H-mode started at 0.91 s. Very clean, no ELMS. Nice, but we hope
that it will go away when we ramp the density. Attempt density ramp in the next
shot

Jan 11 1995 09:19:15:960AM950111002Gary McCrackenObjective: Mini-Proposal#043: To investigate the effect of enhanced radiation on
the critical density for detachment. To study the effect of high edge impurity
concentrations on the Mo influx (MoI) and central Mo concentration
Good shot. Density ramp up to 2e20 at 0.95 s. Divertor detachment occurs at about
0.64 s. This is a bit early since we want toreduce the density of detachment
further with the neon. We will slow down the density ramp in the next shot.
Incidentally the FMP probes are configured for disruption. The domed
probes however show the detachment

Jan 11 1995 09:33:05:180AM950111003Gary McCrackenDud

Jan 11 1995 10:00:36:740AM950111004Gary McCrackenGood shot. Density rose to 1.8e20 at 0.93 s. The detachment occurred on probe 6
around 0.8 s, but the detachment was more gradual than in the previous shot. This
seems to be because the outer strike point is moving up the target plate. We
will try and control the strike point better in the next shot. .

Jan 11 1995 10:19:25:880AM950111005Gary McCrackenPoor shot. After trying to reset the strike point the density feedback did not
work. Low density and X rays. We had put in a small test neon pulse at 0.3 s.
5 psi. Valve opened but no direct evidence that the neon went in
The strike point position was much better.

Jan 11 1995 10:38:53:340AM950111006Gary McCrackenDisruption at 0.47 s. No obvious reason why. Try again

Jan 11 1995 10:45:31:210AM950111007Gary McCrackenFizzle

Jan 11 1995 11:08:42:650AM950111008Gary McCrackenDisrupted at 0.47 s. Perhaps due to the strike point control

Jan 11 1995 11:21:04:360AM950111009Gary McCrackenDisrupted at 0.47 s. Strike control turned off so it can't be that. Radiated
power is exceeding the input power so possibly it is due to the neon injection.
We will turn this off for the next shot.

Jan 11 1995 11:27:24:050AM950111010Gary McCrackenFizzle

Jan 11 1995 11:48:09:120AM950111011Gary McCrackenNo neon injected. Good shot. Detached at 0.72 s, but the strike point is now
moving again. We are really back to shot 004. Next shot put in neon at
0.5 s with 1.6 psi pressure in the plenum

Jan 11 1995 12:07:03:320PM950111012Gary McCracken Good shot. Neon injected at 0.5 s with 1.6 psi pressure in the plenum. However
detachment has not occurred any earlier. Also there is still a problem with the
strike point moving. Lastly there is a problem with the McPherson which is not
giving any signal. Since this neon signal is critical to the measurements we
have decided to have brief cell access to see if the problem with the McPherson
can be fixed. The fault was found and rectified.

Jan 11 1995 12:25:11:610PM950111013Gary McCracken Good shot. Neon again injected at 0.5 s with 1.6 psi pressure in the plenum.
However detachment has not occurred any earlier. We now have good neon signals on
the McPherson and on the oma We will increase neon for the next shot.

Jan 11 1995 12:41:18:200PM950111014Gary McCracken Good shot. Neon again injected at 0.5 s with 1.6 psi pressure in the plenum, but
increaased the neon pulse width from 20 to 30 ms.
Detachment now occurring at about 0.7 s . Neon signals on
the McPherson and on the oma are up nearly a factor 2 We will increase neon
again for the next shot.to 50 ms pulse

Jan 11 1995 01:01:09:230PM950111015Gary McCracken Good shot. Neon again injected at 0.5 s with 1.6 psi pressure .
Increased the neon pulse width again from 30 to 50 ms. Detachment now occurring
a little earlier but it is hard to define exactly when it occurs . Neon signals
on the McPherson and on the oma are up nearly another factor 2. Power into the
SOL is down from about 680 kW to 580 kW.
We will increase neon again for the next shot.

Jan 11 1995 01:26:20:720PM950111016Gary McCracken Neon again injected at 0.5 s but with pressure up to 5 psi
Decreased the neon pulse width again from 50 to 30 ms so neon in should be
similar to the previous shot. In fact the amount of neon was up a factor of 3
according to the McPherson
Detachment now occurring at 0.54 s . The power radiated in the core is going up
from 0.55 MW to 1.3 MW maximum and it is then falling slowly. The power into the
SOL is now down to about 300 kW.
Unfortunately we are having some problems with the equilibrium and the
last shot was a slot divertor for a while

Jan 11 1995 01:41:46:280PM950111017Gary McCrackenNeon off. Good shot. Detachment occurs at about 0.77 s. Power into the SOL
is back up to 770 kW The neon has completely
disappeared in the McPherson giving us a good background.
Much improved stike point stability

Jan 11 1995 01:59:32:040PM950111018Gary McCrackenNeon on again. Pressure 3 psi pulse width 20 ms. Reduced density ramp rate.
Good shot.Density now reaching a maximum of 1.5e20 at 0.95 s. Detachment now
occurring later, about 0.88 s. About 700 kW into the SOL



G

Jan 11 1995 02:14:21:060PM950111019Gary McCrackenNeon increased. Pressure 3 psi pulse width 30 ms.
Good shot. Detachment now about 0.86 s Power into the SOL not known, EFIT
did not run



G

Jan 11 1995 02:32:01:970PM950111020Gary McCrackenNeon increased again. Pressure 3 psi, pulse width 40 ms.

Good shot. Detachment now about 0.81 s Power into the SOL is 370 kW. However
the outer gap has been reduced to 5mm

Jan 11 1995 02:46:35:200PM950111021Gary McCrackenNeon reduced to repeat shot 019. Pressure 3 psi, pulse width 30 ms. Outer gap
put back to the value in 018
Good shot. Detachment at 0.88 s Power into the SOL is 640 kW. Outer gap now
back to 20 mm and inner gap is 13 mm

Jan 11 1995 02:59:10:090PM950111022Gary McCrackenNeon Pressure 3 psi, pulse width 40 ms.

Good shot. Detachment difficult to see. Power into SOL is 650 kW

Jan 11 1995 03:18:11:750PM950111022Gary McCrackenNeon Pressure 3 psi, pulse width 60 ms.

Good shot. Detachment has jumped to much earlier time about 0.56 s
Power into SOL drops to less than 200 kW around 650 ms.
The amount of neon seems to be very critical at this level

Jan 11 1995 03:17:46:620PM950111023Gary McCrackenNeon Pressure 3 psi, pulse width 60 ms.

Good shot. Detachment has jumped to much earlier time about 0.56 s
Power into SOL drops to less than 200 kW around 650 ms.
The amount of neon seems to be very critical at this level

Jan 11 1995 03:24:47:650PM950111024Gary McCrackenNeon Pressure 3 psi, pulse width 50 ms.

Good shot. Detachment still at earlier time about 0.56 s
Power into SOL drops to 400 ms just after detachment and then rises again to
600 kW by 700 ms

Jan 11 1995 03:35:53:280PM950111025Gary McCrackenNo Neon

Good shot. Just hardly get to detachment by the end of the density ramp at 0.95 s
Power into SOL was 800 kW

Jan 11 1995 04:14:59:840PM950111027Gary McCrackenNeon set 3 psi 40 ms similar to shot 022
Delay due to engineering problems. However when it came it was a good shot.
Detachment at about 0.81 s, similar to shot 022. Power into SOL = 600 kW
Increase neon pulse to 50 ms in next shot

Jan 11 1995 04:31:34:920PM950111028Gary McCrackenNeon set 3 psi 50 ms
Detachment at about 0.56 s on the lower probes from about probe 5 down. Thus the
behaviour is pretty reproducible with a sudden change of the detachment between
a 40 and a 50 ms neon pulse. However it appears to reattach, probably due to
decay of the neon with time
Power into SOL = 570 kW . This is not as low as last time with 50 ms pulse

Jan 11 1995 04:47:57:470PM950111029Gary McCrackenNeon set 3 psi 45 ms
Detachment at about 0.56 s
It then reattaches and detaches again at about 0.8 s, similar to the lower
neon injection pulses
Power into SOL = 580 kW .

Jan 11 1995 05:01:13:870PM950111030Gary McCrackenNeon set 3 psi 20 ms. Constant plasma density at 1e20 to study the recycling
properties of the neon.
Good shot
Got nice data on the McPherson with the neon decaying
to a constant level
Power into SOL = 720 kW .

Jan 11 1995 05:27:01:310PM950111030Gary McCrackenConstant plasma density at 1e20
Neon injected in a succession of 20 ms pulse every 50 ms to try and induce
detachment at constant density by an increasing neon concentration.

This worked well with the neon brightness going up almost linearly to the
highest value of the day. Plasma detached at 677 ms and disrupted at 800 ms. The
density increased slightly at detachment but remained fairly constant. The power
radiated increased almost exponentially from about 0.5 s and exceeded the power
in after 0.77 s.

Physics Operator Comments
Jan 11 1995 08:14:43:420AMJohn GoetzToday's run is in support of MiniProposal #043 - Effect of edge
radiation on divertor detachment.

The run will be divided into segments as follows:
1 - obtain a lower SN plasma with outer strike point
about halfway up the outer plate and parameters
Ip=0.8MA; nl04=0.8e20; inner gap>1.5cm; outer gap>1.5cm
2 - do density ramps until detachment is observed
3 - puff neon through B_SIDE_UPPER and observe changes in
detachment characteristics
4 - repeat with argon

To achieve these goals, the discharge obtained on 950110032 will be
used as the starting point. The only change to be made will be to
draw the NL_04 waveform as 0.8e20.

Jan 11 1995 09:00:39:460AM950111001John GoetzShot 950111001:
Start from 950110032 and draw NL_04 as 0.8e20
Plasma - ramps all the way down
nl_04=0.82e20

For shot 002:
draw nl_04 ramp from 0.8e20 @ 0.3 to 2.0e20 @ 0.95

Jan 11 1995 09:19:04:170AM950111002John GoetzShot 950111002:
Plasma - disrupts at 1.31 (some sort of modified shark fin)
density ramps to 2.0e20
divertor detachment observed around 0.65sec

For shot 003:
density ramp to 1.8e20
ramp up Ip waveform to -.85MA
slow down RCUR and CLEARIN ramps

Jan 11 1995 09:37:14:900AM950111003John GoetzShot 950111003:
fizzle - nothing untoward - disruption related?!

For shot 004:
drop fill pressure to 1.5e-5

Jan 11 1995 10:03:12:940AM950111004John GoetzShot 950111004:
plasma - disr @ 1.40sec - Ip=0.8MA and rising slightly
outer strike point is drifting up the plate and makes it
difficult to diagnose the divertor detachment

For shot 005:
move NL_04 to wire 14 in segment 2 and move STRKPSI from
wire 9 in segment 3 to wire 9 in segment 2
enable B_SIDE_UPPER (for neon puff)

Jan 11 1995 10:20:50:170AM950111005John GoetzShot 950111005:
plasma - disr @ 1.44sec - Ip=0.8MA and rising slightly
outer strike point much better behaved
nl_04 < 0.2e20 because of PCS bug related to the wire
switching performed for this shot

For shot 006:
fix NL_04 waveform
P_0=1.6e-5
STRKPSI=-.0011 (to help with the strike point)

Jan 11 1995 10:37:19:300AM950111006John GoetzShot 950111006:
plasma - disr @ 0.45sec
EF2's stay on the rail instead of just kissing the rail
is it related to STRKPSI??

For shot 007:
stairstep on P gain of STRKPSI

Jan 11 1995 10:54:06:830AM950111007John GoetzShot 950111007:
fizzle

For shot 008:
P_0=1.5e-5

Jan 11 1995 11:05:17:930AM950111008John GoetzShot 950111008:
plasma - disr. @ 0.46sec - EF2's on the rails

For shot 009:
turn off gain on STRKPSI controller

Jan 11 1995 11:29:26:630AM950111009John GoetzShot 950111009:
plasma - disr. @ 0.47sec - EF2's on the rails
blame it on the neon

For shot 010:
turn off B_SIDE_UPPER hybrid enable

Jan 11 1995 11:32:02:450AM950111010John GoetzShot 950111010:
fizzle - no bounce

For shot 011:
no changes

Jan 11 1995 11:49:17:680AM950111011John GoetzShot 950111011:
plasma - high density disr. @ 1.38
divertor detachment @ 0.72 but outer strike point is moving

For shot 012:
P gain on STRKPSI stairstep on @ 05.sec to 0.5 @ 0.6sec
PULSE_GAS_2 waveform is 100V x .02sec @ 0.5sec
pressure in B_SIDE_UPPER = 1.6PSIA and hybrid enable

Jan 11 1995 12:06:10:710PM950111012John GoetzShot 950111012:
plasma - high density disr. @ 1.38
divertor detachment @ 0.72 but outer strike point is moving
STRKPSI was not turned (must not have hit o.k.)

For shot 013:
STRKPSI P gain=0.5 @ 0.6sec

Jan 11 1995 12:29:21:100PM950111013John GoetzShot 950111013:
plasma - high density disr. @ 1.38
outer strike still moving but not as much
NeVIII seen on McP and NeI seen on OMA

For shot 014:
STRKPSI = -.00125
PG2 = 100V x .03sec

Jan 11 1995 12:41:39:960PM950111014John GoetzShot 950111014:
plasma - high density disr. @ 1.36
outer strike still moving

For shot 015:
lower P gain on ZXL to 2.5 @ 0.5sec
PG2 = 100V x .05sec

Jan 11 1995 01:02:47:890PM950111015John GoetzShot 950111015:
plasma - high density disr. @ 1.34
outer strike starts out in the wrong place ends up o.k. @ 0.9sec

For shot 016:
PG2 = 100V x .02sec and P(B_SIDE_UPPER)=5.0PSIA

Jan 11 1995 01:29:21:080PM950111016John GoetzShot 950111016:
plasma - high density disr. @ 1.24
outer strike on the floor, then drifts up

For shot 017:
disable B_SIDE_UPPER
STRKPSI=-1E-4 - P gain = 6
RXL = -.01 - P gain = 1
ZXL = -.005 - P gain = 3

Jan 11 1995 01:47:22:710PM950111017John GoetzShot 950111017:
plasma - high density disr. @ 1.39
outer strike well controlled - only moves by 1cm
no neon

For shot 018:
enable B_SIDE_UPPER with P(B_SIDE_UPPER)=3.1PSIA
nl_04 ramp from 0.6e20 to 1.5e20

Jan 11 1995 02:00:09:190PM950111018John GoetzShot 950111018:
plasma - high density disr. @ 1.30
outer strike well controlled - only oscillates a bit after 0.65s

For shot 019:
RCUR=.667 (inner gap is too small)
PG2=100Vx.03sec

Jan 11 1995 02:14:41:580PM950111019John GoetzShot 950111019:
plasma - high density disr. @ 1.32

For shot 020:
PG2=100Vx.04sec
RXL gain = 2 @ 1.0sec and STRKPSI gain off @ .95 ( the
plasma has been rubbing the nose around 1.0 sec)

Jan 11 1995 02:32:37:210PM950111020John GoetzShot 950111020:
plasma - high density disr. @ 1.28
inner gap still rather small and outer gap is 0.5cm!!

For shot 021:
PG2=100Vx.03sec
RCUR=0.6655 (go back to 018)

Jan 11 1995 02:45:09:360PM950111021John GoetzShot 950111021:
plasma - high density disr. @ 1.33
gaps back to where they were - restart the neon scan

For shot 022:
PG2=100Vx.04sec

Jan 11 1995 02:58:24:360PM950111022John GoetzShot 950111022:
plasma - high density disr. @ 1.30


For shot 023:
PG2=100Vx.06sec

Jan 11 1995 03:10:31:430PM950111023John GoetzShot 950111023:
plasma - high density disr. @ 1.28
clear divertor detachment

For shot 024:
PG2=100Vx.05sec

Jan 11 1995 03:20:52:080PM950111024John GoetzShot 950111024:
plasma - high density disr. @ 1.28
clear divertor detachment

For shot 025:
disable B_SIDE_UPPER hybrid enable

Jan 11 1995 03:32:34:740PM950111025John GoetzShot 950111025:
plasma - high density disr. @ 1.33
background shot - no detachment

For shot 026:
PG2=100Vx.04sec and hybrid enable B_SIDE_UPPER

Jan 11 1995 03:59:50:460PM950111026John GoetzShot 950111026:
power supply dud - OH2L comm. fault during precharge

For shot 027:
no changes

Jan 11 1995 04:11:33:870PM950111027John GoetzShot 950111027:
plasma - high density disruption @ 1.29
divertor detachment

For shot 028:
PG2=100Vx0.05sec

Jan 11 1995 04:24:57:470PM950111028John GoetzShot 950111028:
plasma - high density disruption @ 1.29
divertor detachment right after neon comes in

For shot 029:
PG2=100Vx0.045sec

Jan 11 1995 04:41:25:480PM950111029John GoetzShot 950111029:
plasma - high density disruption @ 1.29
local divertor detachment

For shot 030:
PG2=100Vx0.02sec
nl_04=1e20 from 0.5 to 0.95

Jan 11 1995 04:56:46:260PM950111030John GoetzShot 950111030:
plasma - high density disruption @ 1.35
no divertor detachment

For shot 031:
PG2=[100Vx0.02sec] x 7 pulses - starting at 0.5sec and
coming every 0.07sec

Jan 11 1995 05:16:03:880PM950111031John GoetzShot 950111031:
plasma - radiative disruption @ 0.79
divertor detachment @ 0.67sec
plasma survives until the fourth neon puff

Engineering Operator Comments
ShotTimeTypeStatusComment
108:48:43:230AMPlasmaOkNo Faults
209:01:15:950AMPlasmaOkNo Faults.
309:21:31:370AMPlasmaOkNo Faults.
409:40:01:880AMPlasmaOkNo Faults.
510:03:21:900AMPlasmaOkNo faults.
610:22:04:590AMPlasmaOkNo faults.
710:41:50:170AMPlasmaOkNo faults.
810:54:57:010AMPlasmaOkNo Faults
911:08:35:510AMPlasmaOkno faults
1011:23:02:210AMPlasmaOkNo Faults.
1111:34:00:000AMPlasmaOkNo Faults.
1211:48:46:550AMPlasmaOkNo Faults.
1312:09:22:010PMPlasmaOkNo Faults.
1412:26:35:070PMPlasmaOkNo Faults.
1512:43:26:180PMPlasmaOkno faults
1601:02:33:140PMPlasmaOkno faults
1701:28:53:970PMPlasmaOkno faults
1801:45:13:310PMPlasmaOkno faults
1902:00:19:730PMPlasmaOkno faults
2002:14:33:470PMPlasmaOkno faults
2102:33:32:120PMPlasmaOkNo Faults.
2202:47:18:680PMPlasmaOkNo Faults.
2303:00:22:780PMPlasmaOk
2403:12:17:800PMPlasmaOkno faults
2503:25:25:320PMPlasmaOkcomm faults oh2l, oh1, ef1u after disruption
2603:42:03:030PMPlasmaBadoh2l comm fault when switch closed
2704:03:58:160PMPlasmaOkno faults
2804:18:47:350PMPlasmaOkno faults
2904:33:10:120PMPlasmaOkno faults
3004:46:35:950PMPlasmaOkno faults
3105:04:53:820PMPlasmaOkno faults