| Miniproposals | ||||||||||
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| Operators | |
| Session leader(s): | Amanda Hubbard |
| Physics operator(s): | Ron Parker |
| Engineering operator(s): | Sam Pierson,Gary Dekow,Ed Fitzgerald |
| Engineering Operator Run Comment |
| MP592 - L-H threshold dependence on fueling location, density, & neutral |
| Session Leader Plans |
| Entered: Feb 24 2010 06:39:53:063PM |
| Author: Amanda Hubbard |
| MP592 - L-H threshold dependence on fueling location, density, & neutral pressure
Session Leader: Amanda Hubbard Physics Operator: Ron Parker Request overnight ECDC in Helium. Require Cryopump available in the morning - probably use all day although we will assess its effect in the first few shots. NINJA on HFS should be filled with deuterium. (pressure?) 1). Set up target discharge, 800 kA, 5.4 T, Ssep -0.5 cm. Program nel 5e19 m-2, so that we will not get much fuelling from low field side. CRYOPUMP ON. Shot 1091022024 could be a good starting point for the shape. Check Ip, Ssep programming. Also reduce target density, and adjust the startup for the cryopump. 2) Enable NINJA, starting puff at 0.5 s and leaving on for the flat top. Aim for target nel 0.7 x 1020 m-2, (near typical minimum L-H, to allow comparison with C-Mod database and scalings.) This may take some variation of NINJA pressure. Turn on ICRF 0.7 secs, Increase ICRF power in steps, probably two levels per discharge, find threshold. 3-4 discharges. 3). Repeat with Cryopump OFF, compare neutral pressure and threshold. If no effect, leave off for remaining LSN shots. If it DOES reduce p0, turn on for subsequent discharges. 1-2 discharges. 4. Leave preprogrammed density alone, scan density UP by varying NINJA puff, in coarse steps to start, and finer as pressure increases, to maximum for which MARFE can be avoided and enough ICRF coupled to obtain L-H transition. (eg, approximately nel 0.9, 1.0, 1.1, 1.2, 1.3 x 1020 m-2 ). Use NINJA settings on Steve Wukitch's run 1091023 as a guide to needed pressures. Step RF for each density; expect to need multiple shots per density 12-15 discharges. 5. Turn off NINJA, Switch to LFS gas puffing. Repeat density scan, focusing on nebar 1.5-2 1020 m-3 for which we expect a higher outer midplane neutral pressure, and H-mode access. Select programmed values based on what we obtained in Step 4. Compare L-H thresholds. Anticipate we cannot get as high in ne due to ICRF limits. 10 discharges. Should we get through all this, continue with other steps in the MP. But I doubt we will. It is critical we get several overlapping points in steps 4 and 5 during the same run day, to answer the first order question of whether there is an effect of fuelling location on the L-H threshold and it is worth continuing another run day. So, we may decide to alternate a few shots each in steps 4 and 5 at the moderate densities to make sure we get this, and to reduce changes in wall loading between the two sets. |
| Physics Operators Plans |
| Session Leader Summaries |
| Entered: Mar 1 2010 10:58:46:960AM |
| Author: Amanda Hubbard |
| MP592 - L-H threshold dependence on fueling location, density, & neutral pressure
Session Leader: Amanda Hubbard Physics Operator: Ron Parker The main element of this run was to use high field side (HFS) fuelling with the NINJA in RF heated plasmas, following up successful use in high density ohmic plasma in MP xx on Run xxx, which indicated differences in neutral pressure with LFS and HFS fuelling for given density. The goals of this experiment were 1) To compare L-H thresholds in discharges with HFS and LFS fuelling. 2) To see if the density range with ICRF heated plasmas, and L-H transition densities, could be extended using HFS fuelling (the issue here is the neutral pressure limit for ICRF). 3) If so, see if steady EDA H-modes can be more readily obtained using the higher density. The machine ran very smoothly today and we accomplished most of the run plan - thanks to excellent physics and engineering operators, and cryopump operators. The cryopump ran so well, and seemed to be beneficial in keeping a level density, that we decided to skip the step of turning it off. Special thanks to Jim Terry for NINJA operation. The majority of discharges were 5.4 T, 800 kA with ssep -0.5 cm, selected so as to give low L-H threshold but still enable the cryopump to reduce neutral pressure. Many discharges used HFS NINJA puffing, obtained by pre-programming a low target density ( 4 or 5e19 m-2) and then adding a strong NINJA puff; the LFS piezo then closed. NINJA pressure was scanned from 10 to 40 psi, and we obtained target densities between 0.64 and 1.4e20 m-2. ICRF was added in the flat top (typically 0.7 or 0.8 s) and its power stepped to determine L-H thresholds, as evidenced by long delays after turnon. At the lower densities, early in the day, ICRF did cause a small (~ 10e19 m-2) increase in density. With HFS fuelling, L-H thresholds were remarkably constant, 1.3-1.5 MW, over a wide range of target densities, nel 0.74 (shot 5) to 1.2e20m-2 (Shot 23). Details are in session leader shot comments. At even higher densities, 1.3 and 1.4 e20 (shots 29, 30) L-H transitions were still obtained, with thresholds between 1.8 abnd 2.1 MW. This was the maximum obtainable density with NINJA, though further increases might have been obtained with higher pregrogrammed density. They had clear particle barriers but little or no change in edge temperature. With LFS fuelling, L-H thresholds were even more frustratingly variable than usual. At nel 0.94e20, threshold was 1.5 MW, the same as with HFS fuelling (shot 10). Shot 16, with very slightly higher density, required 1.9 MW and shot 17, nel 0.99 e20, 2.2 MW indicating a steep upward trend. But, then shots 20 and 21, with higher density (1.18e20 m-3) transitioned to H-mode with only 1.2 MW! This was the upper limit which could be obtained with LFS fuelling - J-port stopped working after 1.0e20 and D and E above 1.2. This is typical of past results. So, while further detailed analysis is certainly required, in terms of local parameters, neutral pressure etc, the first order answers to the questions seem to be: 1) The L-H power thresholds are variable and not systematically very different with high and low field side fuelling. They do NOT, in either case, follow a simple density scaling. 2) A we had hoped, ICRF operation and L-H transitions can be obtained to higher density with HFS fuelling than with LFS fuelling - limit of at least 1.4e20 m-2 vs 1.2 m-2. Further extension might be possible. Since 800 kA high density H-modes were not very interesting, for the last few shots of the day we decided to raise Ip (1.1 MA) reducing q95 to 3.1, near the ITER range - though not ITER shape. Note that all shots used a raised x-point to avoid the damaged W tiles. Shots 32 and 33 were nice examples - in our first attempts, we obtained very steady EDA H-modes with a clear QC mode and nel 2.7 e20 m-2. A pleasant surprise was that all three ICRF antennas performed well at the high density and pressure, with up to 4.75 MW on shot 33. Plasmas were rather cold, with YAG Te0 ~ 1 keV, leading to high collisionality, and global confinement was rather low - near L-Mode. EDA at this q95 is not unique, but has been hard to obtain routinely. This run suggests that HFS fuelling is a useful technique to achieve high target density H-modes - more shots to optimize heating would be useful, perhaps in the ITER shape once tiles are fixed. One could also try to further decrease q95 - our attempt on the last shot disruptedat q=3, and a low ne locked mode. |
| Physics Operator Summaries |
| Entered: Feb 25 2010 04:58:05:707PM |
| Author: Ron Parker |
| Great run, as far as the machine was concerned!
Reliable startup, no disruptions, no fizzles and no duds. For the most part the machine wasn't pushed too hard, with most shots at 800 kA, 5.4 T. Toward the end of the run, current was increased to 1.1 MA and the last few shots ran full length at this current. The most interesting result of the run was production of steady EDA modes at q = 3.15 (shots 32-33) Scorecard: 34 plasma attempts, 32 full length discharges, 1 hardware failure (Shot 27) and, yes, 1 disruption (at q = 3.) |
| Session Leader Comments | |||
| Feb 25 2010 09:58:25:040AM | 1100225001 | Amanda Hubbard |
Good plasma. 5.46 T, 800 kA. Cryopump ON, no NINJA. Ssep starts -0.5 cm as we want, drifts up a little. nel 0.8e19 m-2. 1 MW ICRF, clean, L-Mode. |
| Feb 25 2010 09:57:36:800AM | 1100225002 | Amanda Hubbard | This shot programmed density was 5e19 m-3; got about 5.6, from C Piezo.
NINJA on at 0.6 s, raised nel only slightly (10 psi). RF on at 0.8 s, w step at 1.1 s to 2 MW. Notable outgassing during ICRF; nel to 6.9e19. Got H-mode in 2 MW step, so threshold is between 1 and 2 MW. Ssep -0.5, much steadier. Useful shot. |
| Feb 25 2010 09:55:54:223AM | 1100225003 | Amanda Hubbard | This shot programmed density was 4e19 m-3. Got 0.43 by 0.5 s
NINJA on at 0.5 s, 15 psi. Piezo turns OFF as we hoped. Gives steady nel 0.63. C-side MKS 6 mTorr. RF also moved earlier, request 1.5 MW. Got L-H transition 0.855 s, (ie fairly long delay) at 1.5 MW. So we are close to the threshold. Drop starting power to 1.25 MW next shot. Nice Ssep -0.6 s constant until about 1.3 s. A useful point - keep the plasma the same and nail down threshold. |
| Feb 25 2010 10:06:29:127AM | 1100225004 | Amanda Hubbard |
No H-mode. RF steps 1.4, 1.6 MW. So threshold is in this range. nel is 0.63e20 before RF, peaks at 0.78 with RF and then decreases from 1 sec to 0.7. Note that NINJA switches off at 1 sec. Next shot, extend this to see if density stays steadier. And increase RF slightly to check threshold. |
| Feb 25 2010 10:43:38:497AM | 1100225005 | Amanda Hubbard | Good threshold point. Delayed H-mode (0.93 s) with 1.5 MW heating.
NINJA fuelling, 15 psi. Cryopump ON (it seems to be working well, and giving steady targets, so I am just going to leave it on rather than spend shots comparing). nel was 0.65 e20 pre-RF, 0.74 in RF, at L-H transition. Steady, and the RF fuelling seems lower than a few shots ago. A good point to come back to later. For now, move on to higher nel with NINJA - program 20 psi. |
| Feb 25 2010 10:35:38:613AM | 1100225006 | Amanda Hubbard | Another good threshold point. Delayed H-mode (1.03 s) with 1.5 MW heating. SO as we half-expected, the threshold is not varying much with nel, near the minimum.
NINJA fuelling, 20 psi. Cryopump ON. nel was 0.75 e20 pre-RF, 0.89 in RF, at L-H transition. JT notes that the increase around 0.9 s is the second NINJA puff- which may be overkill in duration. For next shot, shorten second puff, increase pressure to 25 psi. |
| Feb 25 2010 10:43:20:057AM | 1100225007 | Amanda Hubbard |
NINJA 25 psi. Got only a slight increase in density (0.81e20 ohmic, 0.87 at L-H with ICRF) Surprisingly, got an earlier L-H transition, 0.78 s, again with 1.5 MW ICRF. Next shot, go to 30 psi NINJA for a bigger step in density. |
| Feb 25 2010 11:00:10:000AM | 1100225008 | Amanda Hubbard | NINJA 30 psi. Got an increase in density (0.87e20 ohmic, 0.96 at L-H with ICRF)
We are still getting an L-H transition, now 0.87 s so quite delayed, in the 1.5 MW RF step. This lack of density dependence is interesting - normally I think PLH would be rising. May indicate a fuelling effect. Next shot: Reduce RF power to check we have the threshold. |
| Feb 25 2010 11:14:32:157AM | 1100225009 | Amanda Hubbard | NINJA 30 psi. Got similar increase in density (0.86e20 ohmic, up to 1.0 e20 m-2 with ICRF)
With RF reduced only slightly (1.4 MW) we did NOT get an L-H transition. So 1.5 MW on shot 8 was clearly a good threshold point. For next shot, turning OFF the NINJA, pre-programming 0.9e20 with normal piezo (LFS). We will compare L-H thresholds (and LFS pressures). |
| Feb 25 2010 11:35:25:307AM | 1100225010 | Amanda Hubbard |
First comparison shot, with NINJA OFF, programmed nel 0.9 e20 m-2 (ie normal piezo fueling). Got nel 0.85e20 ohmic, 0.94 with ICRF. And got a very late L-H transition (1.04 secs) at 1.5 MW ICRF. So, to first order at least, threshold is the same at this density. Pressure (F Rat) is 1.7e-4 T at the L-H, only slightly higher than 1.5e-4 on shot 8. Note that it peaks at 2.2e-4 earlier in RF pulse, then drops. Could this be partly why the L-H transition does not occur earlier? |
| Feb 25 2010 11:44:03:613AM | 1100225011 | Amanda Hubbard |
Back to HFS NINJA fuelling, 35 psi. Got nel 1.0 to 1.1 e20 m-2, a little variable. Only got 1.3 MW ICRF, no H-mode. Next shot: Retune, retry. Jim will also adjust pulse length and attemp to smooth out ne time trace. F-Rat 2.5 to 4e-4. |
| Feb 25 2010 12:01:11:943PM | 1100225012 | Amanda Hubbard | HFS NINJA fuelling, 35 psi.
Got nel up to 1.2 e20 m-2, max about 1.1 secs. Got up to 1.36 MW RF. L-H comes late, 1.2 secs, when nel and pressure have started to droop a little. But nel is still 1.17 at L-H, so quite a low threshold. |
| Feb 25 2010 12:13:50:100PM | 1100225013 | Amanda Hubbard | HFS NINJA fuelling, 35 psi.
nel is lower, with same NINJA - 1.0e20 m-2. Got an L-H transition in first RF step at 1.5 MW. But it is very gradual/timing indistinct (0.925 s or a bit later?). Must be close to L-H, given the long delay. |
| Feb 25 2010 12:29:19:303PM | 1100225014 | Amanda Hubbard | HFS NINJA fuelling, 40 psi. Pulse until 1.0 sec. Gave nice steady nel 1.27 m-2 until 1.0 secs.
ICRF at 1.5 MW did NOT give L-H at this density (finally, some dependence). DID get L-H at 1.1 secs (very indistinct again) at 1.5 M, and nel 1.2e20. F-rat was 4.9e-4 at L-H, up to 5.4 at peak. For next shot, increase RF power and try for H-mode in first phase. Also extend NINJA puff. |
| Feb 25 2010 12:42:42:133PM | 1100225015 | Amanda Hubbard | HFS NINJA fuelling, 40 psi. Pulse until 1.1 sec. Peak nel 1.2e20, slightly variable - may be some periodic MARFEing.
Got L-H transition in the first RF pulse at 1.6 MW, Timing, again, is rather indinstict - there are two steps in nel at 0.82, 0.89 s. Resembles D3D "slow transitions". MARFE-related? F-rat 4.0e-5 before L-H. Next shot: Turn OFF NINJA, try to repeat this density with normal feedback fuelling. Will RF stay on? Will the threshold change? Stay tuned... |
| Feb 25 2010 12:56:32:370PM | 1100225016 | Amanda Hubbard |
LFS fueling. Got steady nel of 0.95-0.98 m-2 (lower than prior shots). And L-H threshold is definitely HIGHER. L-H very late, 1.4 secs, and takes 1.9 MW. Did NOT get H-mode at 1.75 MW. F-Rat is not higher - only 2.5e-4 at L-H. Note that it is actually dropping (from 2.9) just before L-H. A factor in finally transitioning? The L-H dynamics is quite different - clear jump in nel, unlike the HFS fuelled H-modes. Next: Increase RF power, try for earier H-mode. |
| Feb 25 2010 01:10:14:540PM | 1100225017 | Amanda Hubbard | LFS fueling. Repeat nel of 0.95-0.98 m-2
Did NOT get H-mode at 2 MW. Transitioned early in 2.2 MW step. 1.136 s. So this nicely brackets the threshold power, and is clearly higher than with NINJA at the same nel (which was about 1.5 MW). nebar is 1.8. Frat 2.26e-4. Still have some headroom. Increase programmed nel to 1.2e20 m-2. |
| Feb 25 2010 01:18:01:097PM | 1100225018 | Amanda Hubbard |
Increase programmed nel to 1.2e20 m-2. Got about 1.1e20. Transitioned right away at 2.2 MW, so apparently not a strong ne dependence. Frat is 3.5e-4 at L-H. Increase density demand, want to get into non-linear region. Threshold here is somewhere below 2.2 MW, but presumably at least 2 MW. |
| Feb 25 2010 01:36:21:150PM | 1100225019 | Amanda Hubbard | Increase programmed nel to 1.3e20 m-2. Got about 1.18e20. Pretty good match to shots 14, 15. But RF (J) now struggling. F-rat is 4.8e-4.
Only 1.3 MW, no L-H until density drops at the end of the flat top (it was programmed down at 1.3). Try again for more RF from D and E. |
| Feb 25 2010 01:45:17:207PM | 1100225020 | Amanda Hubbard | Repeat programmed nel 1.3e20 m-2. Got about 1.17e20.
Very low power threshold this time - L-H at 1.04 s, only 1.2 MW! With D only. Ratiomatic (I've been using logp_fport) is 4.8 e-4 Torr. So what is different!? |
| Feb 25 2010 01:51:09:447PM | 1100225020 | Amanda Hubbard | Repeat programmed nel 1.3e20 m-2. Got about 1.17e20.
Very low power threshold this time - L-H at 1.04 s, only 1.2 MW! With D only. Ratiomatic (I've been using logp_fport) is 4.8 e-4 Torr. So what is different!? f-side-rat is 1.27 mTorr. |
| Feb 25 2010 02:01:33:240PM | 1100225021 | Amanda Hubbard | Repeat shot. With extremely similar, if perplexing, results. Why is threshold so much lower than a few shots ago? J vs D?
Next: raise programmed density. |
| Feb 25 2010 02:22:37:233PM | 1100225022 | Amanda Hubbard | Raised target to 1.4e20, got 1.26 e 20. At this point neutral pressure is too high for any RF. 1.3-2.1 mTorr.
So, go back to NINJA puffing. |
| Feb 25 2010 02:31:41:760PM | 1100225023 | Amanda Hubbard | NINJA, 40 psi. Got a nice 1.3 e20 m-2 plasma. nel droops from 1.15 s, we don't get L-H until about 1.25 s, when nel back to 1.2 and RF 1.44 MW.
Fairly consistent with threshold earlier in the day at least. F-side 1.46 mT max, 1.18 at L-H. Next, increase RF earlier. And stretch NINJA pulse to avoid the droop. |
| Feb 25 2010 02:43:41:820PM | 1100225024 | Amanda Hubbard | NINJA, 40 psi. Got a nice density, 1.1 slowly rising to 1.35 e20 m-2.
RF too low (1.3 MW) stayed L-mode. F-side up to 1.7 mTorr. |
| Feb 25 2010 02:58:36:570PM | 1100225025 | Amanda Hubbard | NINJA, 40 psi. Got a nice density, slowly rising to 1.32 e20 m-2.
No L-H at 1.5 or 1.6 MW. More power, IGOR. F-side up to 1.8 mT. |
| Feb 25 2010 03:18:04:840PM | 1100225026 | Amanda Hubbard | NINJA, 40 psi.
Repeat. RF to 1.8 MW, no H-mode. |
| Feb 25 2010 03:42:12:480PM | 1100225028 | Amanda Hubbard | Raised RF power to 2.3 MW. Got a transition of some kind about 0.98 secs. We'll call it an H-mode, but it is almost entirely in the particle channel - ne_95 clearly jumps, but hardly any change visible in Te (sort of an inverse I-mode).
Next, reduce RF to 2 MW - we know LH threshold between 1.8 and 2.3 at this density. nel nearly 1.4 e 20 at transition,nel 2.6 e20 - so pretty high for a transition, with modest power. . |
| Feb 25 2010 03:56:28:180PM | 1100225029 | Amanda Hubbard | Still NINJA at 40 T.
Reduced RF power to 2.1 MW. Still got a transition, a bit clearer, at 0.97 s, nel 1.3e20, nebar 2.5 e 20. This is higher than we are usually able to get at LFS, and not extremely high power. (using D and E only). F side 1.2 mT, levelling off in H-mode. Next, try for even higher density by increasing the preprogram. |
| Feb 25 2010 04:10:44:323PM | 1100225030 | Amanda Hubbard |
Increased starting density. Got marginally higher nel (1.4e20) at the time of the L-H transition. Which still happens at 2.1 MW, 1.01 s. This is I think higher than we've managed with LFS fuelling (certainly today, we made it to nel 1.17 e20). And it would be hard to increase much further without enormous gas loads. For last few shots, go to Ip 1.1 MA (q95 near 3) to see if higher target densities are useful operationally in producing steadier H-modes. |
| Feb 25 2010 04:20:42:880PM | 1100225031 | Amanda Hubbard | Good discharge, 1.1 MA, q95 3.1. nel 1.2 to 1.37 e 20, nebar to 2.5e20.
D and E stayed on OK, to 2.5 MW. But no H-mode. F-side 1.2 mT when RF comes on, peaks at 1.8. Next: More power, earlier. |
| Feb 25 2010 04:40:09:700PM | 1100225032 | Amanda Hubbard |
Got a very nice EDA at 1.1 MA, q95=3.1. Clear QC mode. RF 3-4 MW. nel 1.3e20 m-3 at L-H, steady 2.7e20 in H-mode. This is lower q95 than we usually obtain EDA. For shot 33, asked students to reduce second NINJA puff, stopping at 1.0 s since we are in H-mode by then. |
| Feb 25 2010 04:48:02:100PM | 1100225033 | Amanda Hubbard | Even better EDA at 1.1 MA, q95=3.15. RF 3.5-4.5 MW.
155 kJ. nel 1.3e20 m-3 at L-H, steady 2.7e20 in H-mode. F-side peaks at 1.6 mTorr. But Steve reports J is happy, so we will leave the NINJA alone. |
| Feb 25 2010 04:59:49:223PM | 1100225034 | Amanda Hubbard | Tried for 1.2 MA, but got a locked mode and a q=3 disruption. Worth trying on another run day - likely needed higher early density. |
| Physics Operator Comments | |||
| Feb 24 2010 06:31:03:537PM | Ron Parker | Engineering Setup for Thursday, 25 February 2010
----------------- MP592 - L-H threshold dependence on fueling location, density, & neutral pressure Session Leader: Amanda Hubbard Physics Operator: Ron Parker Run begins at 09:00 and ends at 17:00 Power systems as on: 1091022024 Acoil: +Dtop -Dbot -Jtop +Jbot (standard) Hybrid Enabled Gas setup: Fill B-Top with 6 psi D2 Hybrid enabled (PG4) fill B-side lower with 1 psi Ar Hybrid DISABLED (PG1) leave B-side upper as is Hybrid DISABLED (PG2) fill B-main (C-side) with 40 psi D2 Hybrid enabled (PG3) fill H-bottom with 2psi Ne Hybrid DISABLED (PG5) fill NINJA with 10 psi D2 DISABLED Enable gatevalves and shutters: ECE, VUV, HiREX Sr, Z-bolo Torvac gatevalve toggle (yes/no): no Boronization(yes/no): no Overnight ECDC (yes/no): yes, standard settings ICRF(yes/no): yes, Prf = up to 4 MW, all antennas (78 to 80 MHz) LH(yes/no): no Cryopump (yes/no): YES, ready for the start of the run Vessel temperature: 35/35/35 ------------------------------ Overnight ECDC Parameters: Gas: He sweep: 44/45/103 cm scan: 20/120 s Pressure: 5e-5 Torr | |
| Feb 25 2010 09:56:46:300AM | 1100225001 | Ron Parker | Counting down for first shot @ 9:05 |
| Feb 25 2010 09:57:49:693AM | 1100225001 | Ron Parker | Shot 1 ran full length, startup from 1100218030.
Next: reduce density to nel_o4 = 8e19 m-2 |
| Feb 25 2010 09:58:57:180AM | 1100225002 | Ron Parker | Shot 2 ran full length. ZCUR had been reduced by 0.5 mm to try to keep ssep at -0.5 cm -- this seemed to work |
| Feb 25 2010 09:59:16:350AM | 1100225003 | Ron Parker | Shot 3 ran full length. No PO changes for next shot |
| Feb 25 2010 10:01:40:400AM | 1100225004 | Ron Parker | Shot 4 ran full length. No PO changes for next shot |
| Feb 25 2010 10:10:29:550AM | 1100225005 | Ron Parker | Shot 5 ran full length. No PO changes for next shot. Ho hum |
| Feb 25 2010 10:34:21:547AM | 1100225006 | Ron Parker | Shot 6 ran full length. |
| Feb 25 2010 10:36:54:770AM | 1100225007 | Ron Parker | Shot 7 ran full length, no PO changes. |
| Feb 25 2010 10:52:54:880AM | 1100225008 | Ron Parker | Shot 8 ran full length |
| Feb 25 2010 11:16:26:080AM | 1100225009 | Ron Parker | Shot 9 ran full length.
Next: Ninja off, nel_04 programmed for 0.9e20 m-2. |
| Feb 25 2010 02:10:14:873PM | 1100225010 | Ron Parker | Shot 10 ran full length.
Next: Reload shot 9, programmed nel_04 =0.4e20 m-2. |
| Feb 25 2010 12:04:17:243PM | 1100225011 | Ron Parker | Shot 11 ran full length. |
| Feb 25 2010 12:04:39:200PM | 1100225012 | Ron Parker | Shot 12 ran full length |
| Feb 25 2010 12:05:08:230PM | 1100225013 | Ron Parker | Shot 13 ran full length |
| Feb 25 2010 12:19:10:370PM | 1100225014 | Ron Parker | Shot 14 went off as programmed, full length. |
| Feb 25 2010 12:34:23:107PM | 1100225015 | Ron Parker | Shot 15 ran full length.
I would say that the shots continue to roll, but I don't want to jinx it. |
| Feb 25 2010 12:38:28:237PM | 1100225015 | Ron Parker | Next: Programmed nel_04 will be set at 1.0e20 m-2. |
| Feb 25 2010 12:52:13:533PM | 1100225016 | Ron Parker | Shot 16 ran full length |
| Feb 25 2010 01:03:32:110PM | 1100225017 | Ron Parker | Shot 17 ran full length.
Next: Raise target density to 1.2e20 m-2. |
| Feb 25 2010 01:17:17:643PM | 1100225018 | Ron Parker | Shot 18 ran full length, but density didn't make it to 1.2e20 m-2.
Next:set programmed density to 1.3e20 m-2. |
| Feb 25 2010 01:37:25:430PM | 1100225019 | Ron Parker | Shot 19 ran full length, but density programming ramped down before H-mode transition.
We'll extend density programming to 1.4 s. |
| Feb 25 2010 01:52:09:667PM | 1100225020 | Ron Parker | Shot 20 ran full length.
Next: no change for PO |
| Feb 25 2010 02:02:02:660PM | 1100225021 | Ron Parker | Shot 21 ran full length.
Next: Set programmed density to 1.4e20 m-2 |
| Feb 25 2010 02:07:34:417PM | 1100225022 | Ron Parker | Another full length shot. |
| Feb 25 2010 02:13:26:580PM | 1100225022 | Ron Parker | So now it's NINJA's turn to feed the tokamak.
Programmed nel_04=0.4e20 m-2 |
| Feb 25 2010 02:33:21:133PM | 1100225023 | Ron Parker | Shot 23 ran full length.
No change form PO for next shot |
| Feb 25 2010 02:37:14:267PM | 1100225024 | Ron Parker | Shot 24 ran well, but RF wasn't ready.
Repeat for next shot, waiting for RF to be ready. |
| Feb 25 2010 02:59:16:990PM | 1100225025 | Ron Parker | Shot 25 ran full length.
No PO changes for next shot. |
| Feb 25 2010 03:07:35:330PM | 1100225026 | Ron Parker | Same story, full length shot. |
| Feb 25 2010 03:27:27:650PM | 1100225027 | Ron Parker | Failure in EF1 Upper circuit. Commutated early. No plasma.
We'll run the shot again. |
| Feb 25 2010 03:31:14:310PM | 1100225028 | Ron Parker | OK, the shot is back. |
| Feb 25 2010 03:49:09:580PM | 1100225029 | Ron Parker | Shot 29 ran, and ran full length.
Next: increase programmed nel_04 to 6e19 m-2. |
| Feb 25 2010 04:04:31:410PM | 1100225030 | Ron Parker | Shot 30 ran full length
Next: Increase i_p to 1.1 MA |
| Feb 25 2010 04:15:29:360PM | 1100225031 | Ron Parker | Shot 31 ran full length, low RF power.
Next: Igor is asked for more power. |
| Feb 25 2010 04:27:54:763PM | 1100225032 | Ron Parker | Shot 32 ran full length. |
| Mar 10 2010 04:43:00:263PM | 1100225033 | Ron Parker | Ran full length at 1.1 MA |
| Mar 10 2010 04:44:06:607PM | 1100225034 | Ron Parker | Went for 1.2 MA, but plasma disrupted as q passed through 3 |
| Engineering Operator Comments | ||||
| Shot | Time | Type | Status | Comment |
| 1 | 09:06:24:760AM | Plasma | Ok | |
| 2 | 09:23:38:747AM | Plasma | Ok | |
| 3 | 09:37:38:390AM | Plasma | Ok | |
| 4 | 09:51:48:827AM | Plasma | Ok | |
| 5 | 10:05:00:200AM | Plasma | Ok | |
| 6 | 10:18:04:983AM | Plasma | Ok | |
| 7 | 10:32:19:013AM | Plasma | Ok | |
| 8 | 10:49:18:377AM | Plasma | Ok | |
| 9 | 11:02:47:643AM | Plasma | Ok | |
| 10 | 11:19:53:303AM | Plasma | Ok | |
| 11 | 11:33:34:523AM | Plasma | Ok | |
| 12 | 11:47:08:367AM | Plasma | Ok | |
| 13 | 12:00:16:897PM | Plasma | Ok | |
| 14 | 12:14:50:553PM | Plasma | Ok | |
| 15 | 12:29:31:290PM | Plasma | Ok | |
| 16 | 12:43:14:917PM | Plasma | Ok | |
| 17 | 12:56:31:087PM | Plasma | Ok | |
| 18 | 01:09:55:040PM | Plasma | Ok | |
| 19 | 01:23:20:460PM | Plasma | Ok | |
| 20 | 01:36:34:570PM | Plasma | Ok | |
| 21 | 01:51:44:713PM | Plasma | Ok | |
| 22 | 02:05:17:430PM | Plasma | Ok | |
| 23 | 02:19:23:353PM | Plasma | Ok | |
| 24 | 02:33:32:347PM | Plasma | Ok | |
| 25 | 02:47:22:423PM | Plasma | Ok | |
| 26 | 03:01:18:087PM | Plasma | Ok | |
| 27 | 03:15:13:743PM | Plasma | Bad | EF1L commutation problem |
| 28 | 03:28:51:713PM | Plasma | Ok | |
| 29 | 03:42:02:743PM | Plasma | Ok | |
| 30 | 03:55:10:447PM | Plasma | Ok | |
| 31 | 04:08:53:367PM | Plasma | Ok | |
| 32 | 04:23:06:557PM | Plasma | Ok | |
| 33 | 04:37:57:760PM | Plasma | Ok | |
| 34 | 04:51:09:137PM | Plasma | Ok | |
| System Availability | |||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||
| Feb 25 2010 09:05:44:947AM | |||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||
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