| Miniproposals | ||||||||||
|
| Operators | |
| Session leader(s): | Joseph Snipes |
| Physics operator(s): | Ron Parker |
| Engineering operator(s): | Sam Pierson,Ed Fitzgerald,Bill Byford |
| Engineering Operator Run Comment |
| Session Leader Plan for MP559 Comparison of H-mode threshold in He and D |
| Session Leader Plans |
| Entered: Aug 21 2009 03:35:23:450AM |
| Author: Joseph Snipes |
| Session Leader Plan for MP559 Comparison of H-mode threshold in He and D
Session Leader: Joseph Snipes (ITER) Physop: Ron Parker We will begin the run at 8:00 am following overnight ECDC in helium to remove the deuterium from the walls and hopefully begin the day with nearly pure helium plasmas. We will begin with 1090812013 as a 1 MA, 5.4 T shot with a lower single null equilibrium with a slightly non-standard shape since it has high strike points and an elongation of 1.56 to avoid an apparently protruding row of tungsten tiles in the divertor that led to disruptions last week. 1) The density from that shot will need to be lowered to nl04 = 4 x 10^19 m^-2. We will also start with a helium startup for the pre-puff to avoid deuterium contamination. Program a slow ICRF power ramp from 0.75 MW up to 3 MW to try to find the H-mode threshold. If the H-mode is obtained, we will change to a staircase RF waveform starting just below the previous threshold power and stepping up in 0.25 MW steps for at least 0.1 s each and maybe longer for a few steps. Keep an eye on the neutron rate as a monitor to see if the deuterium is really gone. If the neutron rate is dropping from shot to shot with otherwise similar conditions, that may mean we need to repeat a few shots until the neutron rate stops decreasing. 2) If the H-mode was obtained at nl04 = 4 x 10^19 m^-2, then decrement nl04 by 1 x 10^19 m^-2 steps and repeat to look for the low density limit. 3) If the H-mode was not obtained, we will increment nl04 by 1 x 10^19 m^-2 steps to see if we are below the low density limit for the threshold up to a maximum of nl04 = 9 x 10^19 m^-2, adjusting the power ramp depending on the threshold range. When H-modes are achieved, document the threshold with dedicated staircase power steps near the threshold. Map out the H-mode threshold in helium as a function of density. 4) Changeover to D plasmas by changing the pre-puff to D as well as the main gas puff. Set nl04 = 9 x 10^19 m^-2 and ramp the ICRF from 1.5 to 3 MW to get rid of the helium and replace it with D. Look for changes in the threshold and H-mode characteristics during the changeover to D. Monitor the D content with the neutron rate and Zeff. We may consider ECDC in D between shots if the changeover seems to be taking too many shots. 5) Repeat in D the same density points of the H-mode threshold that were found in helium and compare the threshold. Dedicated staircase power steps should be used to document the threshold as was done in helium. Map out the H-mode threshold as a function of density in D paying particular attention to the low density limit and compare with the helium results. Depending on how slow the changeover goes and how easily the density dependence of the threshold is mapped out in both helium and deuterium, we may extend the run up to 18:00 (midnight here in France). |
| Physics Operators Plans |
| Entered: Aug 20 2009 01:35:25:020PM |
| Author: Ron Parker |
| Engineering Setup for Run 1090821
----------------------------------- MP559: Comparison of H-mode threshold in He and D Session leader: Snipes Physop: Parker Run begins at ** 08:00 ** and ends at ** 18:00 ** Power systems as on: 1090812013 Acoil: +Dtop -Dbot -Jtop +Jbot (standard) Hybrid Enabled Gas setup: Fill B-Top with 6 psi **He** Hybrid enabled (PG4) fill B-side lower with 1 psi Ar Hybrid DISABLED (PG1) fill B-side upper with 40 psi **He** Hybrid DISABLED (PG2) fill B-main (C-side) with 40 psi **He** Hybrid enabled (PG3) Leave NINJA fill as is, DISABLED Enable gatevalves and shutters: ECE, VUV, Z-bolo Torvac gatevalve toggle (yes/no): no Boronization(yes/no): no Overnight ECDC (yes/no): YES ICRF(yes/no): yes -- all transmitters run on by 7:30 AM! LH(yes/no): no DNB(yes/no): no Cryopump (yes/no): no Vessel temperature: 60/60/60 overnight ------------------------------ ECDC Parameters ------------------------------ gas and pressure: **He** at 5e-5 Torr sweep: 44/45/103 cm scan: 20/120 s --------- Shot Plan --------- We'll start with a segment 1 of 1090804002 for startup in helium, and segment 2 from 1090812013, with the density lowered to 4e19. Note that the feedback P and D gains on nl_04 should be set at 2 for He. This shape should avoid strong interaction with the W tiles. See SL plan for detailed shotplan. |
| Session Leader Summaries |
| Entered: Aug 21 2009 06:15:39:753PM |
| Author: Joseph Snipes |
| MP559 Comparison of the H-mode threshold in He and D
The run went reasonably well despite a couple of air leaks after shot 27 and 33 and a data system hang on shot 33 that cost us a couple of hours. The H-mode thresholds in helium were consistently 2 to 2.5 times the latest deuterium threshold scalings produced by Yves Martin. The H-mode thresholds in deuterium, on the other hand, decreased relative to the scaling for lower density. At high density, the deuterium thresholds were up to 2 x the scaling, but at moderately low density, the thresholds were down to 1.2 - 1.3 times the scaling. In absolute terms, the threshold at nebar = 1.5 x 10^20 m^-3 was 1.9 MW = POH + 0.9*PRF - dW/dt in deuterium whereas in helium, the threshold was about 3.4 MW, which is a factor of 1.8 times higher in helium. More detailed analysis needs to be done to determine more precisely the differences between the helium and deuterium thresholds, but it is clear that the threshold is considerably higher in helium than it is in deuterium, by at least 40% or more. The results are therefore more consistent with the JET results than with the recent ASDEX Upgrade results and are not very good news for ITER. If these results extrapolate directly to ITER, it will be difficult for ITER to achieve H-mode before deuterium is introduced. However, given the differences between machines, a better physics understanding is required to extrapolate these results to ITER. |
| Physics Operator Summaries |
| Entered: Aug 21 2009 06:14:07:363PM |
| Author: Ron Parker |
| The run started slowly with several early disruptions and fizzles, mainly caused by too much gas from the fill pressure and post breakdown gas pulses. Finally, after tuning up, a full length discharge was produced in helium on shot 7, and from then on the machine ran well through shot 27, including the scheduled transition from helium to deuterium on shot 17. However, after shot 27 a leak developed which took the pressure up to the mid -5 range. After turning off the cooling, the leak sealed itself and plasma operation was resumed without consequence. However, the leak reappeared and became serious on shot 33. At the same time a data system hangup occurred. After the data system problem was fixed and the cooling turned off to reseal the leak, only one more shot could be run before the scheduled end of the run at 6:00 PM. (But it was worth it.)
One other problem that occurred early on was a problem with the J-port transmitter crowbar, which took the J antenna out of operation for the day. This limited the maximum power to ~ 3.4 MW, which was a bit unfortunate for the H-Mode threshold studies. Overall, the run produced useful and interesting data on the threshold in He relative to D2, not as much as one would have wanted from the extended run, but nevertheless of good quality and value. Scorecard: 34 plasma attempts, 5 fizzles, 3 disruptions and 26 full length plasmas |
| Session Leader Comments | |||
| Aug 21 2009 07:59:04:130AM | 1090821001 | Joseph Snipes | Shot 1: Breaker pulled. Early disruption at 0.41 s. Density needs to be flattened out at nl04 = 4 x 10^19 m^-2. |
| Aug 21 2009 08:28:35:100AM | 1090821002 | Joseph Snipes | Shot 2: Very similar to shot 1. Need higher density. |
| Aug 21 2009 08:38:07:527AM | 1090821003 | Joseph Snipes | Shot 3: Fizzle. |
| Aug 21 2009 08:57:02:753AM | 1090821004 | Joseph Snipes | Shot 4: Slightly better, but disrupted just after 1 s. Got nearly 2 MW of ICRF by that time and no sign of an H-mode. Let's increase nl04 to 5 x 10^19 m^-2 and try again. |
| Aug 21 2009 09:03:27:067AM | 1090821005 | Joseph Snipes | Shot 5: Fizzle. |
| Aug 21 2009 09:28:13:170AM | 1090821006 | Joseph Snipes | Shot 6: Fizzle. |
| Aug 21 2009 09:49:14:880AM | 1090821007 | Joseph Snipes | Shot 7: Good shot. Got > 2.5 times the deuterium threshold scaling values with no H-mode up to 2 MW of ICRF. So, we may be below the low density limit or else the threshold in He is significantly higher than in D. Raise nl04 to 6 x 10^19 m^-2 for shot 8. |
| Aug 21 2009 10:04:30:463AM | 1090821008 | Joseph Snipes | Shot 8: Good shot. Got slightly higher density and > 2 times the deuterium threshold scaling values with no H-mode up to 2 MW of ICRF. The RF is tripping out at the higher power. Raise nl04 to 7 x 10^19 m^-2. |
| Aug 21 2009 10:29:36:070AM | 1090821009 | Joseph Snipes | Shot 9: Good shot. Got slightly higher density and two brief H-modes. The threshold is about 2 times the D threshold scaling. The first H-mode starts at 2.6 MW. Do a staircase ICRF pulse around the threshold for shot 10. |
| Aug 21 2009 10:48:21:827AM | 1090821010 | Joseph Snipes | Shot 10: Good shot. Got two brief H-modes. The threshold is about 2.5 to 2.7 times the D threshold scaling. The first H-mode starts at 2.8 MW. |
| Aug 21 2009 10:51:27:233AM | 1090821011 | Joseph Snipes | Shot 11: Good shot. Got a brief H-mode. The threshold is about 2.5 times the D threshold scaling. The first H-mode starts at 2.6 MW. |
| Aug 21 2009 10:57:11:157AM | 1090821012 | Joseph Snipes | Shot 12: Good shot. Density set to nl04 = 9 x 10^19 m^-2. H-mode near the end of the RF pulse at just over 3 MW of RF. It is about 2.4 x D threshold scaling. |
| Aug 21 2009 11:10:37:867AM | 1090821013 | Joseph Snipes | Shot 13: Try a staircase RF waveform at 3.0, 3.2, and 3.4 MW to narrow down the threshold value. Got a brief H-mode at the end of the RF pulse around 3.3 MW.
This corresponds to 2.3 to 2.4 times the D threshold scaling. |
| Aug 21 2009 11:31:54:233AM | 1090821014 | Joseph Snipes | Shot 14: Increase nl04 to 1 x 10^20 m^-2. RF ramp from 2.5 MW to 3.4 MW. RF trips out at the highest power levels, but there was no H-mode up to about 3.4 MW. |
| Aug 21 2009 11:48:56:083AM | 1090821015 | Joseph Snipes | Shot 15: RF programed at 3.4 MW straight across. Higher power is not available. Got an H-mode with about 3.2 MW of RF. This is about 2.3 to 2.4 x the D threshold. |
| Aug 21 2009 12:02:52:963PM | 1090821016 | Joseph Snipes | Shot 16: Raised nl04 to 1.1 x 10^20 m^-2. Keep RF pulse programmed at 3.4 MW.
No H-mode with 3.2 MW of RF corresponding to 2.2 to 2.3 x D threshold scaling assuming 90% of the RF power is coupled. |
| Aug 21 2009 12:29:59:083PM | 1090821017 | Joseph Snipes | Shot 17: Changeover to deuterium plasmas keeping nl04 = 1.1 x 10^20 m^-2. Ramp the ICRF from 1 MW to 3 MW. Got 3 H-modes with the first at Prf = 2.2 MW. So, the threshold is already lower with only some D. This corresponds to about 2 times the D threshold scaling. |
| Aug 21 2009 12:40:33:887PM | 1090821018 | Joseph Snipes | Shot 18: Repeat with higher gain on the density feedback to get the density up to nl04 = 1.1 x 10^20 m^-2. Density rises too much early leading to a MARFE. Then, the density settles down to the requested value. D-port RF antenna tripped out leaving < 1 MW of power. No H-modes. |
| Aug 21 2009 12:52:13:890PM | 1090821019 | Joseph Snipes | Shot 19: Fizzle. |
| Aug 21 2009 01:09:35:380PM | 1090821020 | Joseph Snipes | Shot 20: Density is fine, but the D port antenna tripped again leaving only just over 1 MW of RF and no H-modes.
|
| Aug 21 2009 01:26:20:043PM | 1090821021 | Joseph Snipes | Shot 21: Similar to shot 20. The D port antenna tripped again leaving only just over 1 MW of RF and no H-modes.
|
| Aug 21 2009 01:35:57:170PM | 1090821022 | Joseph Snipes | Shot 22: Similar to shots 20 and 21. The D port antenna tripped again leaving only just over 1 MW of RF and no H-modes. Reduce nl04 to 1 x 10^20 m^-2.
|
| Aug 21 2009 01:46:39:643PM | 1090821023 | Joseph Snipes | Shot 23: Fizzle. |
| Aug 21 2009 02:09:52:497PM | 1090821024 | Joseph Snipes | Shot 24: Good shot with RF ramp from 1 to 3 MW. nl04 = 1 x 10^20 m^-2. No H-modes. Threshold is apparently high in this condition, more than 2 times the D threshold scaling. |
| Aug 21 2009 02:29:37:410PM | 1090821025 | Joseph Snipes | Shot 25: RF trips out some of the time, but the power varies from 2.5 to 1.6 MW with 3 H-modes with thresholds 1.5 to 2 x the D threshold scaling. |
| Aug 21 2009 02:43:10:540PM | 1090821026 | Joseph Snipes | Shot 26: Good shot. 3 H-modes with RF ramp. First H-mode at 2.7 MW of RF at about 2 x the D threshold scaling. So, the He threshold is about 40% higher than the D threshold in agreement with the JET results and disagreement with the AUG results.
|
| Aug 21 2009 03:00:25:737PM | 1090821027 | Joseph Snipes | Shot 27: RF steps programmed for 2.6, 2.8, and 3.0 MW to narrow down the threshold. H-mode at the first step with 2.5 MW at 1.8 - 2 x D scaling. Need to repeat starting with lower power.
|
| Aug 21 2009 04:07:03:293PM | 1090821028 | Joseph Snipes | Shot 28: RF steps programmed for 2.2, 2.4, and 2.6 MW to narrow down the threshold. H-mode at the first step with 2.3 MW at 1.7 - 1.8 x D scaling. Need to repeat starting with lower power.
|
| Aug 21 2009 04:25:57:173PM | 1090821029 | Joseph Snipes | Shot 29: RF steps programmed for 1.8, 2.0, and 2.2 MW to narrow down the threshold. No H-mode. Move on to lower density for shot 30.
|
| Aug 21 2009 04:41:16:650PM | 1090821030 | Joseph Snipes | Shot 30: nl04 set to 9 x 10^19 m^-2. RF ramp from 1 - 3 MW. 3 H-modes with the first one at 1.6 MW of RF. This corresponds to 1.5 - 1.6 x D threshold scaling. |
| Aug 21 2009 04:51:54:823PM | 1090821031 | Joseph Snipes | Shot 31: nl04 set to 8 x 10^19 m^-2. RF ramp from 1 - 3 MW. 4 H-modes with the first one at 1.4 MW of RF. This corresponds to 1.4 - 1.5 x D threshold scaling. |
| Aug 21 2009 05:18:13:763PM | 1090821032 | Joseph Snipes | Shot 32: nl04 set to 7 x 10^19 m^-2. RF ramp from 0.5 - 2.5 MW. 4 H-modes, 1st one at 0.9 MW about 1.2 - 1.3 x D threshold scaling. |
| Aug 21 2009 05:28:35:770PM | 1090821033 | Joseph Snipes | Shot 33: nl04 set to 7 x 10^19 m^-2. RF steps from 0.7, 0.9, 1.1 MW. An air leak has opened up again due to cooling like it did before shot 28, but it was not as bad this time. 3 H-modes with the first one just before 0.8 s. However, the RF power data may be lost. |
| Aug 21 2009 06:09:41:283PM | 1090821034 | Joseph Snipes | Shot 34: nl04 set to 6 x 10^19 m^-2. RF ramp from 0.5 to 2.5 MW. No power shot due to a data system hang.
|
| Aug 21 2009 06:14:47:880PM | 1090821035 | Joseph Snipes | Shot 35: nl04 set to 6 x 10^19 m^-2. RF ramp from 0.5 to 2.5 MW. Many H-modes. The threshold is between 1.2 and 1.4 x the D scaling. |
| Physics Operator Comments | |||
| Aug 21 2009 08:03:03:533AM | 1090821001 | Ron Parker | First shot occurred just before 8:00. The shot disrupted at 0.4 s.
|
| Aug 21 2009 08:30:50:197AM | 1090821002 | Ron Parker | Shot 2: More or less the same problem as in shot 1, an early disruption.
The density during rampup seems too low -- falling to nl_04 ~ 0.16e20 --, so we'll revert to the shot 33 startup from last night, including an early PG 3 pulse. |
| Aug 21 2009 08:49:17:560AM | 1090821003 | Ron Parker | Shot 3 fizzled. |
| Aug 21 2009 09:00:06:160AM | 1090821004 | Ron Parker | Shot 4 started up better, disrupting after 1 s. RF ramped from 1 to 1.8 MW with no sign of H-mode.
Next: Raise density to 5e19. |
| Aug 21 2009 09:03:18:613AM | 1090821005 | Ron Parker | Fizzle. |
| Aug 21 2009 09:16:57:790AM | 1090821005 | Ron Parker | Delay while RF checks things in power room |
| Aug 21 2009 09:31:06:577AM | 1090821006 | Ron Parker | Shot fizzled. Drop the prepuff from 25 to 23 ms. |
| Aug 21 2009 09:57:21:930AM | 1090821007 | Ron Parker | Finally success! A full length shot, RF ramps up close to 3 MW, density during RF increased to 5e19 from 4e19.
Next:increase density (nl_04) by 1e19. |
| Aug 21 2009 10:06:49:420AM | 1090821008 | Ron Parker | Shot 8 ran full length. It appears that there is a problem with J's crowbar which cannot be fixed without long delay. We are stuck with maximum of 3 MW from D and E.
Next: Raise nl_04 to 7e19. |
| Aug 21 2009 10:21:40:207AM | 1090821009 | Ron Parker | Again, a full length shot. SW reports two tiny H-modes.
Next: Step RF power pulse in 150 - 200 ms each, 2.4, 2.6, and 2.8 MW. |
| Aug 21 2009 10:33:40:460AM | 1090821010 | Ron Parker | Shot 10 again ran full length. RF stepped and H-mode transitions transiently occurred at RF power of 2.7 MW
Next: Raise density another 1e19 with ramped RF |
| Aug 21 2009 10:45:53:793AM | 1090821011 | Ron Parker | Shot 11 ran full length, RF ramped and an H-mode appeared at about 2.6 MW.
Next: Raise density by another 1e19 on nl_04. RF ramp start at 1.5 MW instead at 1.0 MW |
| Aug 21 2009 10:56:02:017AM | 1090821012 | Ron Parker | Shots continue to roll, another one at full length.
Next: Staircase 2.8, 3.0, 3.2 MW -- same density as in shot 12 |
| Aug 21 2009 11:10:45:880AM | 1090821013 | Ron Parker | Good shot, with H-mode transition at 3.3 MW, confirming ramp threshold.But RF trips and so H-mode is not sustained.
Next: Increase density again by 1e19 on nl_04 |
| Aug 21 2009 11:30:13:577AM | 1090821014 | Ron Parker | Shot 14 ran well, no H-mode although some RF trips make the conclusion a bit ambiguous.
Next: Repeat with 3.4 MW RF pulse |
| Aug 21 2009 11:47:29:957AM | 1090821015 | Ron Parker | Shot 15 ran full length. Surprisingly, an H-mode developed at ~ 3.2 MW.
Next: Increase n to 1.1e20 (another 1e19) |
| Aug 21 2009 12:04:26:293PM | 1090821016 | Ron Parker | Shot 16 ran full length, no H-mode.
Next: Change to D2, ramp 1 to 3, same density. P-gain on density feedback increased from 2 to 8. |
| Aug 21 2009 12:44:23:747PM | 1090821017 | Ron Parker | Shot 17 ran full length. Gain change on nl_04 wasn't loaded so density didn't reach 1.1e20.
Next: reload with Pgain on nl_04 = 8. |
| Aug 21 2009 12:48:26:683PM | 1090821018 | Ron Parker | Shot ran full length, disupting on current rampdown.
Prefill and PG 3 puff killed runaways, but resulted in MARFE. Next: reduce density rise demand |
| Aug 21 2009 12:51:57:077PM | 1090821019 | Ron Parker | Shot 19 fizzled. Drop prefill by 3 ms, to 22 ms pulse. |
| Aug 21 2009 01:10:09:240PM | 1090821020 | Ron Parker | Shot 20 ran full length, RF had trips |
| Aug 21 2009 01:20:19:103PM | 1090821021 | Ron Parker | Shot 21 ran full length. RF continues to trip |
| Aug 21 2009 01:34:31:047PM | 1090821022 | Ron Parker | Shot 22 was OK, but RF still not up to requested power due to high neutral density.
Next: reduce nl_04 to 1e20 |
| Aug 21 2009 01:51:52:647PM | 1090821023 | Ron Parker | Shot 23 fizzled. Reduce fill by 2 ms, also move pg3 pulse out by 10 ms. |
| Aug 21 2009 02:07:42:730PM | 1090821024 | Ron Parker | Shot ran full length, but no H-mode up to 3 MW!
Next: Repeat with power up to 3.4 MW |
| Aug 21 2009 02:44:57:807PM | 1090821025 | Ron Parker | Shot 25 ran full length. |
| Aug 21 2009 02:43:01:477PM | 1090821026 | Ron Parker | Shot 26 ran full length and RF power ramp produced an H-mode at ~2.8 MW.
Next: Same pulse, but with steps in RF power. |
| Aug 21 2009 02:54:50:607PM | 1090821027 | Ron Parker | Shot 27 ran full length. H-mode developed in first RF step at ~ 2.5 MW.
Repeat with lower steps |
| Aug 21 2009 03:59:56:150PM | 1090821027 | Ron Parker | Ooops, the base pressure is rising into the mid -5 range. Cell access to investigate. After turning off cooling, the leak appears to have sealed. Base pressure is now in the mid - 7 range and cooling is back on
|
| Aug 21 2009 04:06:42:620PM | 1090821028 | Ron Parker | In spite of the leak problem, the shot ran full length and the H-mode transition occurred at 2.4 MW.
Next:Repeat with different RF steps -- 1.8, 2.0, 2.2 |
| Aug 21 2009 04:20:01:220PM | 1090821029 | Ron Parker | Shot 29 ran well, full length. No H mode, bracketing the threshold.
Next: reduce nl_04 to 0.9e20 |
| Aug 21 2009 04:40:43:447PM | 1090821030 | Ron Parker | Shot 30 ran full length, H-mode appeared.
Next: Lower nl_04 to 8e19. |
| Aug 21 2009 05:13:04:500PM | 1090821031 | Ron Parker | Shot 31 ran full length |
| Aug 21 2009 05:17:31:327PM | 1090821032 | Ron Parker | Shot 32 ran full length, ramp threshold ~ 0.9 MW.
Leak is opening again, so we are slowing the cooling down. |
| Aug 21 2009 05:33:35:363PM | 1090821033 | Ron Parker | Shot 33 ran full length, but vessel still leaking
Data system problem |
| Aug 21 2009 06:09:42:377PM | 1090821034 | Ron Parker | Shot 34 will be a no power shot |
| Aug 21 2009 06:14:55:240PM | 1090821035 | Ron Parker | Shot 35 ran full length. |
| Engineering Operator Comments | ||||
| Shot | Time | Type | Status | Comment |
| 1 | 07:54:22:570AM | Plasma | Bad | PF breaker opened |
| 2 | 08:20:31:520AM | Plasma | Bad | PF Breaker opened |
| 3 | 08:35:46:167AM | Plasma | Ok | |
| 4 | 08:48:29:233AM | Plasma | Ok | |
| 5 | 09:01:14:300AM | Plasma | Ok | |
| 6 | 09:26:16:480AM | Plasma | Ok | |
| 7 | 09:38:48:317AM | Plasma | Ok | |
| 8 | 09:55:20:430AM | Plasma | Ok | |
| 9 | 10:11:54:593AM | Plasma | Ok | |
| 10 | 10:24:47:097AM | Plasma | Ok | |
| 11 | 10:37:53:243AM | Plasma | Ok | |
| 12 | 10:50:29:360AM | Plasma | Ok | |
| 13 | 11:04:05:990AM | Plasma | Ok | |
| 14 | 11:24:26:950AM | Plasma | Ok | |
| 15 | 11:40:39:377AM | Plasma | Ok | |
| 16 | 11:54:59:477AM | Plasma | Ok | |
| 17 | 12:19:06:910PM | Plasma | Ok | |
| 18 | 12:34:05:447PM | Plasma | Ok | |
| 19 | 12:48:30:247PM | Plasma | Ok | |
| 20 | 01:01:00:360PM | Plasma | Ok | |
| 21 | 01:15:25:693PM | Plasma | Ok | |
| 22 | 01:29:56:967PM | Plasma | Ok | |
| 23 | 01:44:33:520PM | Plasma | Ok | |
| 24 | 02:01:03:447PM | Plasma | Ok | |
| 25 | 02:15:26:593PM | Plasma | Ok | |
| 26 | 02:33:00:380PM | Plasma | Ok | |
| 27 | 02:47:35:150PM | Plasma | Ok | |
| 28 | 04:00:15:803PM | Plasma | Ok | |
| 29 | 04:13:57:263PM | Plasma | Ok | |
| 30 | 04:30:11:223PM | Plasma | Ok | |
| 31 | 04:44:35:773PM | Plasma | Ok | |
| 32 | 04:57:23:360PM | Plasma | Ok | |
| 33 | 05:17:35:983PM | Plasma | Ok | |
| 35 | 06:09:21:707PM | Plasma | Ok | |
| System Availability | ||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||
| Aug 21 2009 07:54:02:090AM | ||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||
| ||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||
| Aug 21 2009 05:10:34:220PM | ||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||
| alignment looks ok. YAG one cannot be adjusted due to the broken mirror adjustment. Now Yag 1 alignment is perfect on top machine (bot plate) and that's the most important thing. | ||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||
| Aug 21 2009 05:17:18:343PM | ||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||
| ||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||
| Aug 23 2009 04:40:09:900PM | ||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||
| A laser head interlock for YAG2 between shot 34 and shot 35. Shot 34 is a no power shot and met a control problem. Both YAGs fired in shot 33, and only YAG 1 fired in shot 35. The laser head could be overheated due to longer flashing.
Sat, 08/22/09 I checked in the lab that the deionized filter for YAG2 was newly replaced on 07/06/09. The water level is reasonable. The water should be pure (there is no LED indicating water purity for YAG2) according to experience. I'll keep an eye on the laser head interlock during Monday run. The top motor alignment has received weak signals since this week. (first plasma Wed afternoon). I tried minor adjustment during Thur and Fri (within 10 steps since last Aug 14). No significant change yet, while the signal level looked normal, so I gave up the trial. I checked the fiber plate today and saw the 3 top alignment fibers stuck out from the holder surface for about half an inch. No doubt these fibers were not on focal plane so that's why the signals were low. I's very likely happened when we took out the fiber plate after Aug 14 run (before Jerry left). I toggle the fibers back and now they are back on the focal plane. Due to only YAG2 operation and bad alignment on Thursday, the cross calibration results was not quite successful. Calculated fudge factors for core channels (not all) are about 1.05~1.10. This verified that the precious calculation is quite close, and the bad alignment gave us information that in extreme case the density should still within 10% error. Shot 1090820029 is a cut-off shot with good bot plate alignment (no idea on top, signals were low). Next wed afternoon Martin will repeat the high density fueling experiment. Now Mirror 1 is fixed by 3 washers so that the HeNe's on TV are well on target. Minor adjustment available for Mirror 2 in x,y direction and Mirror 1 in y direction. Bot motor in perfect alignment Friday. So if everything remains well and YAG2 not affected by Friday laser head interlock, we could get quite good cutoffs. | ||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||