| Miniproposals | ||||||||||
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| Operators | |
| Session leader(s): | Yunxing Ma |
| Physics operator(s): | Bill Rowan |
| Engineering operator(s): | Bill Cochran,Ed Fitzgerald,Gary Dekow |
| Engineering Operator Run Comment |
| automatically entered by signon - please replace with real comment |
| Session Leader Plans |
| Entered: Jan 12 2011 05:52:20:687PM |
| Author: Yunxing Ma |
| Run plan for 1110114
SL: Yunxing Ma PO: Bill Rowan MP: MP631 The main goal of this run is to investigate the dependence of power deposition profile (heating locations, on-axis/off-axis) on H-mode power threshold and L-H transition. Results from this experiment serve the companion objectives of exploring the proposal of I-mode at low densities (nl04<0.6), Bt dependence of H-mode access at higher densities. *** This will be an 80Mhz+70Mhz, multiple BTs run *** *** This run plan should not be rigorously followed. The targets are subject to immediate minor adjustments based on the judgments SL makes during the run *** Operational parameter space: Bt/Ip = 5.2T/1.0MA, 4.5T/0.9MA, 3.9T/0.8MA (### note that the target Bt and Ip are one-to-one matched ###) nl04 = 0.3, 0.8 RF antenna is set up to work at two frequencies: D&E at 80Mhz, J at 70Mhz cryopump ON Diagnostics requirement: TS (core+edge, edge fiber need to be optimized for normal magnetic configuration) GPC/GPC2 (set up for 3.9T), FRCECE X-mode reflectometer (ready for profile and fluctuation measurements) CXRS, Hirex PCI, GPI, O-mode reflectometer, magnetics Discharges sequence: First, load the magnetic geometry from the target discharge of shot 1101221006, and modify the plasma parameters to be Bt=5.2T, Ip=1.0MA, and nl04(L-mode)= 0.3. The value of density is close to ITER L-mode operational target. Also, an I-mode like phase was previously discovered near this density level. Then scan Bt/Ip at the 3 targets indicated above. For each combination RF antennas will be operated at one individual frequency (either 80Mhz or 70Mhz) a time (in a single discharge); while both frequencies need to be tried. The 2nd harmonics resonance layers are separated and sample a number of locations ranging from far off-axis (rho=0.9) to on-axis heating from the Bt scan (see figure below). Required RF power for H-mode access is anticipated to be high at the low density level, can be as much as 3+ MW with Bt=5.4T. Pth of 80Mhz vs 70Mhz heating from the same Bt will be compared, looking for what/where the effect of power deposition is. Since Pth is strongly nonlinear (enhance substantially with decreasing ne) at below H-mode low density limit, a good density control is highly desired for this comparison. Unfortunately, the power of cryopump may not be fully used in LSN, but we request it to be turned on in order to ameliorate the situation as much as it can. If the density can't be controlled very well, a few shots would be required at each operational target to cover the density variation. If there are difficulties to access H-mode at Bt=5.2T even with maximum allowed RF power from one frequency, then increase the target L-mode density to nl04=0.4 where Pth can be reduced by ~1.0MW. The second section of the run is simply repeating the above steps with nl04=0.8. This part is relatively less demanding in rigorous density control than the above one (low ne), since it's already known that the density dependence of Pth near this value of nl04 is very weak. Furthermore, the required target RF power for H-mode is much less here (1~2MW will be adequate). If time permits, we'll spend a few shots to make up the CXSR and GPI measurements for MP625, which we missed last time from previous run 1101221. Minimum required discharges (24 shots): Bt=5.2T, Ip=1.0MA, nl04=0.3-0.4, RF=80MHz, 2 shots Bt=5.2T, Ip=1.0MA, nl04=0.3-0.4, RF=70MHz, 2 shots Bt=4.5T, Ip=0.9MA, nl04=0.3-0.4, RF=80Mhz, 2 shots Bt=4.5T, Ip=0.9MA, nl04=0.3-0.4, RF=70Mhz, 2 shots Bt=3.9T, Ip=0.8MA, nl04=0.3-0.4, RF=80Mhz, 2 shots Bt=3.9T, Ip=0.8MA, nl04=0.3-0.4, RF=70Mhz, 2 shots Bt=5.2T, Ip=1.0MA, nl04~0.8, RF=80MHz, 2 shots Bt=5.2T, Ip=1.0MA, nl04~0.8, RF=70MHz, 2 shots Bt=4.5T, Ip=0.9MA, nl04~0.8, RF=80Mhz, 2 shots Bt=4.5T, Ip=0.9MA, nl04~0.8, RF=70Mhz, 2 shots Bt=3.9T, Ip=0.8MA, nl04~0.8, RF=80Mhz, 2 shots Bt=3.9T, Ip=0.8MA, nl04~0.8, RF=70Mhz, 2 shots
*** Figure shows the 2nd harmonic resonance layers at 3 BTs for 80/70Mhz RF frequencies. Also illustrated are the LCFS and rho=0.9, rho=0.8 flux surfaces *** |
| Physics Operators Plans |
| Entered: Jan 13 2011 01:56:54:693PM |
| Author: Bill Rowan |
| -----------------
Engineering Setup ----------------- Run begins at 09:00 and ends at 17:00 Power systems as on: 1101221006 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 NINJA with 10 psi D2 DISABLED Enable gate-valves and shutters: ECE, VUV, HiREX Sr, Xeus Leave z-bolo shutter as is (should be open) Torvac gatevalve toggle (yes/no): no Boronization(yes/no): no Overnight ECDC (yes/no): yes, ECDC in helium ICRF(yes/no): yes LH(yes/no): no Cryopump (yes/no): yes DNB (yes/no): yes Vessel temperature: 35/35/35 ------------------------------ ECDC Parameters (if requested) ------------------------------ gas and pressure: Helium at 5e-5 Torr sweep: 44/45/103 cm scan: 20/120 s If there are difficulties in keeping ECDC going, increase Helium pressure to 1.0e-04 Torr ECDC at the higher pressure copies the prescription used for the Thursday run. ------------------------------ Diagnostics required ------------------------------ TS (core+edge, edge fiber need to be optimized for normal magnetic configuration) GPC/GPC2 (set up for 3.9T), FRCECE X-mode reflectometer (ready for profile and fluctuation measurements) CXRS, Hirex PCI, GPI, O-mode reflectometer, magnetics |
| Session Leader Summaries |
| Entered: Jan 18 2011 10:26:09:127PM |
| Author: Yunxing Ma |
| Run summary of 1110114
The goal of this run is to investigate the effect of heating deposition profile on the H-mode power threshold and L-H transition. Companion goals of the run are exploring the Bt dependence of Pth at lower density (nbar>1.0n20), and low density H-mode behavior. The run is successful. Totally 34 shots were created, with 3 disruptions and 1 fizzle. We got a number of meaningful results: 1. The first half of the run was conducted at intermediate density of nl04~0.8 (nbar~1.5n20), with 3 Bt scans at 5.2,4.5,3.9T. For each target 70Mhz (J ant) and 80Mhz (D&E) were applied once at a time (in a single shot). Pth was compared between these two heating scenarios (comparison between on-axis with off-axis). It was found that Pth was basically unchanged (~2.0MW), unless the 2nd harmonic resonance was far off-axis in the HFS (3.9T, 80MHz), where Pth doubled (Pth~4MW). The reason could be due to RF physics, e.g. one conjecture is that the coupling there was very poor, verified by very slight enhancement of Wmhd even with 3MW RF injection. However, the real reason(s) need to be worked out after a certain amount of analysis (perhaps running RF code is requred to figure out the specific power deposition profile). By comparing the off-axis heating shots (res layer all nearly midway in minor radii), we found that Pth was almost the same ~2.0MW for different Bts. This confirms that the Bt dependence does go away at higher densities, as speculated before based on database mining. 2. The second half of the run is to explore the Pth and H-mode behavior at low densities. The target density was maintained around nl04=0.45, equivalently, nebar=0.9n20 for Bt=5.2T at L-H; and nl04=0.4,nebar=0.7 for Bt=4.5T at L-H. Again, so significant difference was found between 70Mhz and 80Mhz heating schemes. In addition, Pth does decrease with lowering Bt, say Pth~2.5MW at 5.4T, 0.9n20, expected to be around 3.0MW at 0.7n20; and Pth~2.0MW for Bt=4.5T,nbar=0.75n20 (comparison in on-axis heating scenario). But Pth tends to go up again for 3.9T, but that (only) one was the last shot today, with HFS off-axis heating (70Mhz). So the conclusion might be that Pth would increase in HFS minority case. More details will be worked out after careful analysis. A WCM at about 100Khz was persistent in these low density shots, but the 200Khz WCM as in I-mode was just marginally found in shot 25 (seems coexistence with the 100Khz one). This frequency range is about the QCM, but this mode occurs even in early RF L-mode phase. 3. Another important harvest is that at the low target density (nl04~0.4), we got clear direct transition to ELMy H-mode at Bt=4.5T and Bt=3.9T (see shot 28,32,34). It's worthi mentioning that these ELMs were formed with normal magnetic geometry, NOT the JFT-2M one, which we used have to go for at higher densities. Further, the H-mode density is very low, for exmaple, in shot 34 (Bt=3.9T), nl04 in H-mode was 0.55! As Amanda mentioned in logbook, this may be the remedy for LHCD in H-mode. In shot 2, whereBt=5.4T, an ELMy H-mode formed following the ELMy free phase, and again, H-mode density become well regulated, very likely due to the onset of ELMs. This is an interesting outcome, which may call for furthure research efforts on ELMs at lower densities. Diagnostics: We have an almost complete existing C-mod diagnostics set working today! CXRS was working the entire day, which will give good measurements of edge Ti and Vt in L- and H-mode and L-H transition; Hirex was on to monitor core Ti and rotation; X-mode reflectometer was on every shot, worth mentioning that it may provide a whole edge density profile (up to pedestal top) evolution in ~ms time scale at for some shots (e.g. shot 34); GPI have collected good data for fluctuation dynamics studies at L-H. Unfortunately, PCI was not available after shot 6 due to a chiller issue. *** Summary of Pth as shots (rough cal based on "analysis" tree *** shot# t(L->H) ne Ploss Pnet Bt Ip q95 ssep fRF Rres ELMY 1110114001 1.260 0.88 2.3 1.75 5.2 1.0 3.3 -0.9 80 65 Y 1110114002 1.070 0.87 2.3 1.60 5.2 1.0 3.3 -0.9 70 75 Y 1110114003 0.720 1.57 2.1 1.76 5.2 1.0 3.4 -0.9 80 65 N 1110114004 0.837 1.60 1.55 1.20 5.2 1.0 3.4 -0.9 80 65 N 1110114005 0.770 1.57 1.53 1.20 5.2 1.0 3.4 -0.9 80 65 N 1110114006 0.963 1.62 2.16 1.92 5.2 1.0 3.4 -0.9 70 75 N 1110114007 0.932 1.63 2.0 1.72 5.2 1.0 3.4 -0.9 70 75 N 1110114008 NA 1110114009 1.050 1.68 2.10 1.60 4.6 0.9 3.3 -0.9 80 57 N 1110114010 0.896 1.45 2.0 1.51 4.6 0.9 3.3 -0.9 80 57 N 1110114011 NA 1110114012 0.916 1.58 2.0 1.50 4.6 0.9 3.3 -0.9 80 57 N 1110114013 NA 4.0 0.8 3.3 -0.9 80 50 1110114014 NA 4.0 0.8 3.3 -0.9 80 50 1110114015 1.265 1.59 3.8 3.0 4.0 0.8 3.3 -0.9 80 50 N 1110114016 1.186 1.44 4.1 3.3 4.0 0.8 3.3 -0.9 80 50 N 1110114017 1.355 1.44 4.1 3.3 3.9 0.8 3.3 -0.9 80 49 N 1110114018 0.963 1.42 2.0 1.7 4.0 0.8 3.3 -0.9 70 57 N 1110114019 0.927 1.48 2.1 1.8 4.0 0.8 3.3 -0.9 70 57 N 1110114020 0.839 1.54 2.0 1.7 4.6 0.9 3.3 -0.9 70 65 N 1110114021 0.950 1.56 2.0 1.7 4.6 0.9 3.3 -0.9 70 65 N 1110114022 NA 1110114023 1.100 0.90 2.2 1.4 5.2 1.0 3.4 -0.9 80 65 Y 1110114024 NA 1110114025 0.880 0.92 1.5 0.73 5.2 1.0 3.3 -0.9 70 75 N 1110114026 1.245 0.92 2.3 1.6 5.2 1.0 3.4 -0.9 70 75 N 1110114027 1.200 0.75 2.9 1.9 5.2 1.0 3.4 -0.9 70 75 N 1110114028 0.860 0.72 2.0 1.25 4.6 0.9 3.3 -0.9 70 65 Y 1110114029 NA 1110114030 NA 1110114031 NA 1110114032 0.922 0.72 2.0 1.38 4.6 0.9 3.3 -0.9 70 65 Y 1110114033 NA 1110114034 0.860 0.72 2.2 1.60 3.9 0.8 3.2 -0.9 70 57 Y *** Summary of Pth as BT,ne (more accurate cal based on "efit01" tree (fast EFIT) *** ========= 5T, 0.9n20 ============ shot# t(L->H) ne Ploss Pnet Bt Ip q95 ssep fRF Rres ELMY 1110114001 1.260 0.87 1.94 1.44 5.2 1.0 3.3 -0.9 80 65 Y 1110114002 1.070 0.84 2.38 1.70 5.2 1.0 3.3 -0.9 70 75 Y 1110114023 1.100 0.91 2.40 1.61 5.2 1.0 3.4 -0.9 80 65 Y 1110114024 NA 1110114025 0.880 0.94 1.50 1.20 5.2 1.0 3.3 -0.9 70 75 N 1110114026 1.249 0.90 2.52 1.63 5.2 1.0 3.4 -0.9 70 75 N 1110114027 1.200 0.74 3.00 2.00 5.2 1.0 3.4 -0.9 70 75 N 1110114027 1.355 1.02 2.70 1.70 5.2 1.0 3.4 -0.9 70 75 N ========= 5T, 0.9n20 ============ 1110114003 0.720 1.55 1.88 1.58 5.2 1.0 3.4 -0.9 80 65 N 1110114003 0.872 1.89 2.40 1.71 5.2 1.0 3.4 -0.9 80 65 N 1110114003 1.013 1.98 2.10 1.41 5.2 1.0 3.4 -0.9 80 65 N 1110114003 1.144 2.36 3.57 2.41 5.2 1.0 3.4 -0.9 80 65 N 1110114003 1.258 2.15 2.40 1.65 5.2 1.0 3.4 -0.9 80 65 N 1110114003 1.385 2.23 2.26 1.54 5.2 1.0 3.4 -0.9 80 65 N 1110114004 0.837 1.58 1.60 1.22 5.2 1.0 3.4 -0.9 80 65 N 1110114004 0.998 1.87 2.15 1.63 5.2 1.0 3.4 -0.9 80 65 N 1110114004 1.111 2.24 3.24 2.39 5.2 1.0 3.4 -0.9 80 65 N 1110114004 1.113 2.27 2.36 1.54 5.2 1.0 3.4 -0.9 80 65 N (2nd) 1110114004 1.219 2.31 2.77 1.91 5.2 1.0 3.4 -0.9 80 65 N 1110114004 1.330 2.34 3.21 2.41 5.2 1.0 3.4 -0.9 80 65 N 1110114004 1.332 2.35 2.90 2.15 5.2 1.0 3.4 -0.9 80 65 N (2nd, Te0 Oscillation) 1110114005 0.770 1.57 1.63 1.32 5.2 1.0 3.4 -0.9 80 65 N 1110114005 1.369 2.45 3.06 2.34 5.2 1.0 3.4 -0.9 80 65 N 1110114006 0.963 1.60 2.03 1.78 5.2 1.0 3.4 -0.9 70 75 N 1110114006 1.257 2.01 2.14 1.72 5.2 1.0 3.4 -0.9 70 75 N 1110114007 0.932 1.60 1.88 1.61 5.2 1.0 3.4 -0.9 70 75 N 1110114007 1.124 1.63 2.01 1.77 5.2 1.0 3.4 -0.9 70 75 N 1110114008 NA ========= 4.6T, 0.9n20 ============ 1110114028 0.860 0.71 2.20 1.43 4.6 0.9 3.3 -0.9 70 65 Y 1110114032 0.922 0.71 2.30 1.76 4.6 0.9 3.3 -0.9 70 65 Y ========= 4.6T, 1.5n20 ============ 1110114009 1.050 1.62 2.11 1.53 4.6 0.9 3.3 -0.9 80 57 N 1110114009 1.257 2.12 2.40 1.70 4.6 0.9 3.3 -0.9 80 57 N 1110114009 1.050 2.29 2.56 1.83 4.6 0.9 3.3 -0.9 80 57 N 1110114010 0.896 1.39 2.07 1.51 4.6 0.9 3.3 -0.9 80 57 N 1110114010 1.205 1.76 2.15 1.44 4.6 0.9 3.3 -0.9 80 57 N 1110114010 1.316 1.95 2.01 1.40 4.6 0.9 3.3 -0.9 80 57 N 1110114011 NA 1110114012 0.916 1.52 1.91 1.46 4.6 0.9 3.3 -0.9 80 57 N 1110114012 1.026 1.75 2.08 1.45 4.6 0.9 3.3 -0.9 80 57 N 1110114012 1.125 1.82 1.90 1.41 4.6 0.9 3.3 -0.9 80 57 N 1110114012 1.218 1.89 2.00 1.40 4.6 0.9 3.3 -0.9 80 57 N 1110114020 0.839 1.54 2.04 1.72 4.6 0.9 3.3 -0.9 70 65 N 1110114020 0.954 1.72 2.02 1.57 4.6 0.9 3.3 -0.9 70 65 N 1110114020 1.335 2.30 2.76 2.10 4.6 0.9 3.3 -0.9 70 65 N 1110114021 0.950 1.48 1.64 1.30 4.6 0.9 3.3 -0.9 70 65 N 1110114021 1.061 1.67 1.89 1.60 4.6 0.9 3.3 -0.9 70 65 N 1110114021 1.174 1.63 1.87 1.61 4.6 0.9 3.3 -0.9 70 65 N 1110114021 1.325 2.12 2.65 2.06 4.6 0.9 3.3 -0.9 70 65 N ========= 4.0T, 0.9n20 ============ 1110114034 0.860 0.71 1.87 1.31 3.9 0.8 3.2 -0.9 70 57 Y ========= 4.0T, 1.5n20 ============ 1110114013 NA 4.0 0.8 3.3 -0.9 80 50 1110114014 NA 4.0 0.8 3.3 -0.9 80 50 1110114015 1.263 1.51 3.51 2.93 4.0 0.8 3.3 -0.9 80 50 N 1110114016 1.186 1.40 4.03 3.30 4.0 0.8 3.3 -0.9 80 50 N 1110114017 1.355 1.39 4.11 3.30 3.9 0.8 3.3 -0.9 80 49 N 1110114018 0.963 1.41 1.98 1.72 4.0 0.8 3.3 -0.9 70 57 N 1110114018 1.073 1.58 2.02 1.71 4.0 0.8 3.3 -0.9 70 57 N 1110114018 1.165 1.65 2.18 1.75 4.0 0.8 3.3 -0.9 70 57 N 1110114018 1.267 1.84 2.08 1.62 4.0 0.8 3.3 -0.9 70 57 N 1110114018 1.358 1.77 2.06 1.66 4.0 0.8 3.3 -0.9 70 57 N 1110114019 0.927 1.45 2.09 1.76 4.0 0.8 3.3 -0.9 70 57 N 1110114019 1.384 2.15 2.40 1.84 4.0 0.8 3.3 -0.9 70 57 N |
| Physics Operator Summaries |
| Entered: Jan 17 2011 01:11:42:680PM |
| Author: Bill Rowan |
| Purpose: MP631, H-mode power threshold scaling with plasma density using off-axis ICRF heating, SL: Yunxing Ma
In this experiment, the h-mode power threshold was sought for various ICRF locations (that is, various BT settings) and for two densities. The startup was loaded from 1110113035. That startup had worked well throughout run 1110113 with only one minor change. For this run, most of the data was taken for the higher of the two densities and without problems. The low density discharge ran adequately, but there is a locked mode just below the density at which we ran the low density cases. It appeared near 0.5 s on several shots. The EF1U early commutation appeared again for one shot and resulted in the single dud of the day. Score card 32 plasmas 1 fizzle 1 dud (engineering, power supply) 34 total |
| Session Leader Comments | |||
| Jan 14 2011 09:13:20:867AM | 1110114001 | Yunxing Ma | nl04=0.2 at L-H. very low density. RF D&E 3MW, seem to work, although trips a little. Pth~4MW.
Next shot, increase nl04 to 0.4, J antenna only, ramp up from 1.0 to 3.0MW |
| Jan 14 2011 09:34:22:737AM | 1110114003 | Yunxing Ma | increase nl04 to 0.8, D&E 1.0MW to 3.0MW |
| Jan 14 2011 09:46:49:693AM | 1110114003 | Yunxing Ma | Multiple H-modes
Defined first transition at 0.55s, nbar=1.5, Pth=2.0MW. |
| Jan 14 2011 09:41:56:080AM | 1110114004 | Yunxing Ma | Bt=5.2T, keep nl04 to be 0.8, D&E only, ramp up from 0.5MW to 2.0MW.
|
| Jan 14 2011 09:53:58:083AM | 1110114004 | Yunxing Ma | L-H at 0.837s, nbar~1.6, Pth back to 1.5MW |
| Jan 14 2011 09:56:11:070AM | 1110114005 | Yunxing Ma | This shot, RF D&E only, step waveform, 0.8->1.0->1.2MW |
| Jan 14 2011 10:08:16:513AM | 1110114005 | Yunxing Ma | L-H at 0.767s, nbar=1.5, Pth~1.55MW
next shot, J antenna (70Mhz), power ramp from 0.5 to 2.0MW |
| Jan 14 2011 10:38:06:770AM | 1110114006 | Yunxing Ma | L-H at 0.962s, nbar=1.62, Pth~2.0MW
J ant, 70Mhz |
| Jan 14 2011 10:25:16:223AM | 1110114007 | Yunxing Ma | this shot, lower the targe density a little, to 8.0 |
| Jan 14 2011 10:37:25:253AM | 1110114007 | Yunxing Ma | L-H at 0.933s, nbar=1.63n20, Pth=2.0MW
J ant, 70MHz heating |
| Jan 14 2011 10:41:58:020AM | 1110114008 | Yunxing Ma | this shot, J ant, power step 0.8->1.0->1.2MW
lower the targe density slightly, to 7.8 |
| Jan 14 2011 10:47:15:470AM | 1110114008 | Yunxing Ma | no RF this shot |
| Jan 14 2011 10:53:25:830AM | 1110114009 | Yunxing Ma | this shot, Bt=4.5, Ip=0.9MA
target ne=7.8 D&E ant, 80Mhz, off axis, ramp up from 0.5 to 2.0MW |
| Jan 14 2011 11:03:09:070AM | 1110114009 | Yunxing Ma | L-H at 1.05s, nbar=1.66, Pth=2.3MW |
| Jan 14 2011 11:06:55:553AM | 1110114010 | Yunxing Ma | decrease target ne to 7.6
D&E ant, RF steps 1.1->1.3->1.5MW |
| Jan 14 2011 11:16:05:913AM | 1110114010 | Yunxing Ma | L-H at 0.895s, nbar=1.45, Pth=2.0MW |
| Jan 14 2011 11:21:38:840AM | 1110114011 | Yunxing Ma | this shot, J ant (70Mhz, on axis heating), power ramp from 0.5 to 2.0MW
|
| Jan 14 2011 11:30:03:440AM | 1110114011 | Yunxing Ma | no RF this shot. |
| Jan 14 2011 11:33:18:253AM | 1110114012 | Yunxing Ma | this shot, repeat shot 10, with target density=7.7
D&E ant, 80Mhz, off-axis |
| Jan 14 2011 11:45:04:030AM | 1110114012 | Yunxing Ma | L-H at 0.915s, nbar=1.58, Pth = 2.0MW |
| Jan 14 2011 11:47:14:893AM | 1110114013 | Yunxing Ma | this shot, Bt=3.9T, Ip=0.8MA, ne=7.7
RF: D&E ant (80Mhz, far off axis heating), power ramp, from 0.5 to 2.0MW |
| Jan 14 2011 12:14:47:050PM | 1110114014 | Yunxing Ma | this shot, repeat shot 13, D&E, ramp up from 0.5 to 3.0MW |
| Jan 14 2011 12:23:24:747PM | 1110114014 | Yunxing Ma | this shot, repeat shot 13, D&E, ramp up from 0.5 to 3.0MW
|
| Jan 14 2011 12:33:18:420PM | 1110114014 | Yunxing Ma | No H-mode even with 1.5MW E ant alone.
One H mode at 1.45s, perhaps ramp down? But it might also be due to 1.0MW J there. |
| Jan 14 2011 12:34:11:600PM | 1110114015 | Yunxing Ma | this shot, repeat shot 14, with D&E
D didn't work well last shot |
| Jan 14 2011 12:48:19:897PM | 1110114015 | Yunxing Ma | there seems to be a brief H-mode at 1.262s, nbar=1.53, Pth~3.5MW!
|
| Jan 14 2011 01:02:40:427PM | 1110114016 | Yunxing Ma | 2 H-modes
1st L-H at 1.18s, nbar=1.45, Pth=3.8MW 2nd L-H at 1.31s, nbar=1.50, Pth=3.73MW |
| Jan 14 2011 01:13:01:000PM | 1110114017 | Yunxing Ma | 1st H-mode at 1.354s, nbar=1.43, Pth=4.0MW
Worst Pth. |
| Jan 14 2011 01:13:50:133PM | 1110114018 | Yunxing Ma | this shot, target Bt=3.9T
J ant, ramp, 0.5 to 2.0MW |
| Jan 14 2011 01:26:56:887PM | 1110114018 | Yunxing Ma | several H-modes
1st H-mode at 0.96s, nbar=1.4, Pth=2.0MW |
| Jan 14 2011 01:41:47:277PM | 1110114019 | Yunxing Ma | H-mode at 0.927s, nbar=1.48, Pth=2.1MW |
| Jan 14 2011 01:48:21:780PM | 1110114020 | Yunxing Ma | this shot, Bt=4.5T, Ip=0.9MA, J ant (70Mhz, on axis) |
| Jan 14 2011 01:57:50:040PM | 1110114020 | Yunxing Ma | Many H-modes
1st transition at 0.84s, nbar=1.54, Pth=2.0MW |
| Jan 14 2011 02:12:02:050PM | 1110114021 | Yunxing Ma | Many H-modes
1st L-H at 0.951s, nbar=1.58, Pth=2.0MW |
| Jan 14 2011 02:15:44:987PM | 1110114022 | Yunxing Ma | Repeat the targets from shot 1: Bt=5.2T, Ip=1.0MA, nl04=0.3
D&E ant, ramp from 1.0 to 3.0MW |
| Jan 14 2011 02:27:25:933PM | 1110114022 | Yunxing Ma | early disruption, some injections
next, repeat |
| Jan 14 2011 02:46:09:140PM | 1110114023 | Yunxing Ma | L-H at 1.1s, nbar=0.9, Pth=2.3MW
Next shot, try decrease target density to 0.35 |
| Jan 14 2011 02:57:20:827PM | 1110114025 | Yunxing Ma | this shot, go back to the targe to shot 23 (nl04=0.4)
J ant, off-axis, ramp from 1.0 to 3.0MW |
| Jan 14 2011 03:13:12:127PM | 1110114025 | Yunxing Ma | L-H at 0.88s, nbar=0.92, Pth=1.5MW
next, repeat |
| Jan 14 2011 03:31:47:517PM | 1110114026 | Yunxing Ma | brief H-mode
L-H at 1.248s, nbar=0.93, Pth=2.3MW |
| Jan 14 2011 03:36:15:397PM | 1110114027 | Yunxing Ma | Clear L-H at 1.2s, nbar=0.75, Pth=2.9MW
next shot, set Bt=4.5T, Ip=0.9MA, J ant |
| Jan 14 2011 03:51:01:000PM | 1110114028 | Yunxing Ma | L-H at 0.86s, nbar=0.71, Pth=2.0MW. seemingly some ELMy like behavior
next, repeat |
| Jan 14 2011 04:20:23:350PM | 1110114029 | Yunxing Ma | disruption |
| Jan 14 2011 04:20:36:157PM | 1110114030 | Yunxing Ma | fizzle |
| Jan 14 2011 04:26:01:447PM | 1110114031 | Yunxing Ma | fizzle |
| Jan 14 2011 04:45:24:540PM | 1110114032 | Yunxing Ma | Back to get H-mode
L-H at 0.922s, nbar=0.72, Pth=2.0MW, ELMy behavior next, switch to D&E, same ramp up |
| Physics Operator Comments | |||
| Jan 14 2011 08:24:41:620AM | Bill Rowan | ecdc in D2 until 6 am
switch over to helium at 1.0e-04 Torr at 6 am about 90 minutes in helium Use shot 1110113035 for the startup. Recommended by the PO for that run. Note that it followed a fizzle and has a small change in EF4 The starting shot requested by SL is 1101221006 It uses segment 02. Load 1110113035 dpcs_fizzle turned on dpcs_xjump turned on dpcs_piezo_chopper turned on 50 ms on PG4 import segment 2 from 1101221006 into segment 2 turn off segment 3 which was used for 1110113035 turned on segment 2 change/check BT=5.2 T (-144800 A) IP=1.0 MA ml_04=0.3e+20 Load. | |
| Jan 14 2011 09:14:08:990AM | 1110114001 | Bill Rowan | 001.
Plasma full length BT=5.2 T IP=1 MA nl_04=0.24e+20 Next shot. Raise nl_04 by approximately 1e+19 RF ramp added |
| Jan 14 2011 09:33:43:410AM | 1110114002 | Bill Rowan | 002.
Plasma full length nl_04 = 3e+19 before H-mode JT: ELMs after 1.2 s, maybe clamped density Next shot. cell access to change TS fibers nl_04 = 0.8e+20 |
| Jan 14 2011 09:38:52:930AM | 1110114003 | Bill Rowan | 003.
plasma full length nl_04 = 0.84e+20 multiple h-modes Next shot. no pcs changes |
| Jan 14 2011 09:58:19:660AM | 1110114004 | Bill Rowan | 004.
plasma full length multiple h-modes Next shot. enabled b-side lower (Ar) PG1 (Ar) 35 ms starting at 0.3 Inner wall gas puff enabled and will go at 1.2s nl_04 = 0.82e+20 (SL request) |
| Jan 14 2011 10:10:13:707AM | 1110114005 | Bill Rowan | 005.
plasma full length nl_04 = 0.82e+20 multiple h-modes Next shot no pcs changes RF changing frequency -- 70 MHz |
| Jan 14 2011 10:23:14:237AM | 1110114006 | Bill Rowan | 006.
Plasma full length 3 h-modes Next shot. lower target density to 0.82e_20 |
| Jan 14 2011 10:35:04:690AM | 1110114007 | Bill Rowan | 007.
plasma full length several h-modes RF is affecting density slightly next shot. increase argon. PG1 to 45 ms duration lower target density to 0.78e+20 |
| Jan 14 2011 10:54:31:157AM | 1110114008 | Bill Rowan | 008.
plasma full length nl_04 constant at 0.8e+20 No h-modes on that shot No RF on that shot. Next shot. Lower BT to 4.5 T (125300A) IP = 0.9 MA nl_04 demand unchanged from 0.78e+20 |
| Jan 14 2011 11:07:30:220AM | 1110114009 | Bill Rowan | 009.
plasma full length multiple h-modes BT=4.5 T after 0.35 s IP = 0.9 MA after 0.5 s next shot. cell access for GPI nl_04 demand to 0.76e+20 |
| Jan 14 2011 11:20:32:293AM | 1110114010 | Bill Rowan | 010.
plasma full length multiple h-modes nl_04=0.76e+20 just before first h-mode dithering before the first transition next shot. No change in the target -- no change in the pcs |
| Jan 14 2011 11:33:57:887AM | 1110114011 | Bill Rowan | 011.
plasma full length no rf on that shot no h-modes on that shot nl_04 = 0.75e+20 next shot nl_04 demand changed to 0.77e+20 |
| Jan 14 2011 11:48:44:670AM | 1110114012 | Bill Rowan | 012.
plasma full length multiple h-modes next shot cell access for RF BT = 3.9 T (108600A) IP = 0.8 MA |
| Jan 14 2011 12:26:18:727PM | 1110114013 | Bill Rowan | 013.
Plasma full length IP=0.8 MA BT=4.0T nl_04 = 0.73e+20 No h-modes next shot cell access for RF |
| Jan 14 2011 12:35:14:187PM | 1110114014 | Bill Rowan | 014.
Plasma full length -- disruption in ramp down no h-modes during plateau -- maybe in ramp down next shot. No change in target No pcs changes |
| Jan 14 2011 12:46:14:163PM | 1110114015 | Bill Rowan | 015,
Plasma almost full length at 1.44s Injections throughout shot next shot no change in target change in rf -- steps |
| Jan 14 2011 12:59:50:440PM | 1110114016 | Bill Rowan | 016.
Plasma full length 2 small h-modes Next shot Bt=3.8 T (105700 A) |
| Jan 14 2011 01:15:38:933PM | 1110114017 | Bill Rowan | 017.
Plasma full length BT=3.9T one small h-mode next shot cell access for RF extended nl_04 to 1.5 s BT increased to 3.9T (108600A) |
| Jan 14 2011 01:31:01:690PM | 1110114018 | Bill Rowan | 018.
Plasma full length multiple h-modes BT=4.0 T Next shot nl_04 = 0.78e+20 also decreased the rate of fall during rampdown |
| Jan 14 2011 01:49:27:320PM | 1110114019 | Bill Rowan | 019.
plasma full length multiple h-modes next shot BT to 4.5 T (125300A) IP = 0.9 DNB 0ff for MSE |
| Jan 14 2011 01:58:21:420PM | 1110114020 | Bill Rowan | 020.
DNB off IP = 0.9 MA BT = 4.6 T multiple h-modes next shot DNB 0n No PCS changes Same target |
| Jan 14 2011 02:17:19:117PM | 1110114021 | Bill Rowan | 021
DNB on multiple h-modes Next shot. reload 1110114001 BT = 5.2 T IP = 1.0MA nl_04 = 0.3e+20 returned PG1 (argon) to 45 ms pulse beginning at 0.3 s |
| Jan 14 2011 02:37:32:570PM | 1110114022 | Bill Rowan | 022.
disruption at 0.46 s injection or locked mode Next shot. Increase nl_04 demand to 0.4e+20 |
| Jan 14 2011 02:43:26:247PM | 1110114023 | Bill Rowan | 023.
plasma full length tci data stops at 1.13 s Next shot. decrease nl_04 demand to 0.35e+20 no other changes |
| Jan 14 2011 02:54:29:720PM | 1110114024 | Bill Rowan | 024.
disruption at 0.61 Next shot increase nl_04 demand to 0.4e+20 |
| Jan 14 2011 03:12:02:260PM | 1110114025 | Bill Rowan | 025.
plasma full length multiple h-modes next shot No pcs changes |
| Jan 14 2011 03:23:34:077PM | 1110114026 | Bill Rowan | 026.
plasma full length next shot no beam increase nl_04 demand to 0.42e+20 |
| Jan 14 2011 03:49:08:313PM | 1110114028 | Bill Rowan | 028.
plasma full length BT = 4.6 T IP=0.9 MA nl_04 = 0.4e+20 Next shot. No pcs changes |
| Jan 14 2011 04:38:49:030PM | 1110114029 | Bill Rowan | 029.
plasma disrupted at 0.4 s appear to be locked modes again next shot increase nl_04 slightly |
| Jan 17 2011 12:19:55:080PM | 1110114030 | Bill Rowan | 030.
dud, EF1U early communtation ratiomatic off next shot turned ratiomatic on ef4 changed from -1300 to -1280 startup was copied from 1110113035 returning ef4 to setting used for many shots prior to 1110113035 |
| Jan 14 2011 04:35:43:243PM | 1110114031 | Bill Rowan | 031.
fizzle Next shot reloaded 1110104029 increased nl_04 to 0.44e+20 |
| Jan 17 2011 12:22:31:197PM | 1110114033 | Bill Rowan | 033.
disruption at 0.5 s next shot pg3 back porch 35 to 55 add 2 ms to prefill gas changes based on perception that the locked mode is only the last in a series of problems which may originate with a hollow profile that develops in ramp-up. BT = 3.9T IP = 0.8 MA |
| Jan 14 2011 05:06:36:867PM | 1110114034 | Bill Rowan | 034.
plasma full length final shot |
| Engineering Operator Comments | ||||
| Shot | Time | Type | Status | Comment |
| 1 | 09:00:46:667AM | Plasma | Ok | |
| 2 | 09:17:12:280AM | Plasma | Ok | |
| 3 | 09:34:49:300AM | Plasma | Ok | |
| 4 | 09:47:30:593AM | Plasma | Ok | |
| 5 | 10:01:23:417AM | Plasma | Ok | |
| 6 | 10:14:31:570AM | Plasma | Ok | |
| 7 | 10:27:36:910AM | Plasma | Ok | |
| 8 | 10:42:59:917AM | Plasma | Ok | |
| 9 | 10:56:40:047AM | Plasma | Ok | |
| 10 | 11:11:05:720AM | Plasma | Ok | |
| 11 | 11:25:22:430AM | Plasma | Ok | |
| 12 | 11:38:04:000AM | Plasma | Ok | |
| 13 | 12:09:22:773PM | Plasma | Ok | |
| 14 | 12:26:37:727PM | Plasma | Ok | |
| 15 | 12:39:01:220PM | Plasma | Ok | |
| 16 | 12:51:44:920PM | Plasma | Ok | |
| 17 | 01:06:34:043PM | Plasma | Ok | |
| 18 | 01:21:49:637PM | Plasma | Ok | |
| 19 | 01:36:46:777PM | Plasma | Ok | |
| 20 | 01:53:00:527PM | Plasma | Ok | |
| 21 | 02:07:27:883PM | Plasma | Ok | |
| 22 | 02:21:15:833PM | Plasma | Ok | |
| 23 | 02:35:09:260PM | Plasma | Ok | |
| 24 | 02:48:04:047PM | Plasma | Ok | |
| 25 | 03:03:17:397PM | Plasma | Ok | |
| 26 | 03:15:59:370PM | Plasma | Ok | |
| 27 | 03:28:39:920PM | Plasma | Ok | |
| 28 | 03:42:06:147PM | Plasma | Ok | |
| 29 | 03:54:51:230PM | Plasma | Ok | |
| 30 | 04:07:21:653PM | Plasma | Bad | |
| 31 | 04:19:51:283PM | Plasma | Ok | |
| 32 | 04:38:52:020PM | Plasma | Ok | |
| 33 | 04:51:31:840PM | Plasma | Ok | |
| 34 | 05:04:01:220PM | Plasma | Ok | |
| System Availability | |||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||
| Jan 14 2011 09:00:31:777AM | |||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||
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