| Miniproposals | ||||||||||
|
| Operators | |
| Session leader(s): | Roman Ochoukov |
| Physics operator(s): | Robert Granetz |
| Engineering operator(s): | Sam Pierson,Bill Parkin,Ed Fitzgerald |
| Engineering Operator Run Comment |
| automatically entered by signon - please replace with real comment |
| Session Leader Plans |
| Entered: Aug 27 2009 06:50:55:090PM |
| Author: Roman Ochoukov |
| /////////////////////////////////////////////////////////////////////////////
This run is the continuation of MP558 (Characterization of ICRF induced sheaths) that started on July 17th/2009. The previous run did not have the emissive probe operating for plasma potential measurements. The emissive probe is now running and available. Start with a regular 1.0 MA discharge, same as 1090717001: 5.4 T, nl_04 ~0.8, right gap ~1.0 cm, elongation ~1.6, upper triangularity ~0.55, lower triangularity ~0.3. Run ICRF in a staircase form starting with the D and followed by E and J if possible (if can't fit three staircased waveforms then use two with E and J alternating). The RF steps are 0.5, 1.0, and 1.5 MW per step. First perform a density scan at 1.0 MA: nl_04 = 0.5 - 1.1 --> 7 shots. Then scan the current (0.8 MA, 0.6 MA, 1.2 MA) keeping the density constant at nl_04 ~1.1, repeat at nl_04 = 0.8 and 0.6 --> 9 shots Scan the toroidal field at constant Ip = 1 MA and nl_04 = 1.0 between 5 and 6 T --> 6 shots Scan the outer gap between 0.5 and 2 cm at const current, Bt, and nl_04 --> 4 shots May change the order of some scans depending on the results from the emissive, Katsumata, and bdot probes. /////////////////////////////////////////////////////////////////////////// |
| Physics Operators Plans |
| Entered: Aug 28 2009 09:17:11:770AM |
| Author: Robert Granetz |
Engineering setup for Friday 2009/08/28
MP558 - Characterization of ICRF sheaths
Session leader: R. Ochoukov
Physics operator: R. Granetz
Standard overnight ECDC and 60 C bake
Run will start at 09:00 and end at 17:00.
Power systems as on 1090717001 (Bt=5.3T, Ip=1.0 MA)
A-coil configuration: +Dtop -Dbot -Jtop +Jbot; Enabled (standard
configuration)
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)
leave NINJA as is DISABLED
Enable the following gate valves and shutters, assuming no vacuum problems:
ECE, VUV, Z-bolo
Torvac setup: keep gate valves open during PULSE
Specific diagnostics: Emissive probe, Bdot probes
------------------------------------------------------------------------------
ICRF Setup: all systems in run-on by 08:30
LH Setup: no
DNB: no
Cryopump: no
------------------------------------------------------------------------------
Run plan: Start with seg 2 of 1090717005 (1 MA, 5.4 T, 0.8e20 m-2,
elong=1.6-1.7, lower triang=0.3, upper triang=0.55.
Program each ICRF antenna to execute a specific staircase
waveform, but with no overlap. Density scan, Btor scan, outer
gap scan.
|
| Session Leader Summaries |
| Entered: Aug 28 2009 06:45:43:780PM |
| Author: Roman Ochoukov |
| MP558 "Characterization of ICRF induced sheaths using emissive, Katsumata, and bdot probes"
Available diagnostics: Emissive probe 3d Bdot probe Katsumata probe Probes are located on lower B side of the split AB limiter and are magnetically connected to D and E antennae. ////////////////////////////////////////////////////////////////////////////// Session summary: The purpose of this run was to determine the governing parameters that lead to high ICRF rectified DC voltages in the presence of RF. The highest observed voltages, as measured with a hot emissive probe, were +220 V in the presence of RF power from the D antenna, in L mode plasma (see shot 033). The highest voltages due to E antenna RF power are +30 V, also in L mode plasmas (shot 033). The RF power from the J antenna has the weakest effect on measured voltages, ~+10 V or lower. The DC voltages and RF signal on the bdot probes are also modified by the presence of sawteeth -- voltages spikes of up to 80 V_pp were observed (see shot 025, 030, 033). The probe response (both the bdot signals and the floating potentials of the hot emissive and katsumata probes) appears to be the weakest when plasma enters into an H-mode. The highest DC voltages are now only +25-30 V with the D antenna on (see shots 014 and 015). The plasma current scan (Ip = 0.6 -- 1.2 MA) revealed that the highest voltages occur at 1.0 and 1.2 MA during the L mode phase, and H to L transition phases in the presence of D antenna RF power (see shots 004 through 012). Voltages up to +180 V were measured. The toroidal field scans (Bt = 4.7-6.0 T) revealed that the highest voltages occur at Bt = 5.6-5.8 T (see shots 027 and 028) and correspond to +100-150 V, again in presence of D RF power. The lowest measured voltages were at 6.0 T and 4.7-5.2 T, corresponding to only +15-30 V (see shots 029-032). The linear ramp of RF power (D followed by E) at Bt = 5.4 T and Ip = 1.0 MA produced the highest observed voltages during the run with the voltages scaling with the D antenna RF power. /////////////////////////////////////////////////////////////////////////////// shot specifics: shot 001: good shot -- plasma, no RF, emissive probe is off (cold) -- V_float = -1 V 1 MA current nl_o4 = 0.8e20 1 late H mode Next: repeat with RF on: staircased with D, then E, then J steps are 0.5, 1, and 1.5 MW. Turn emissive probe on. shot 002: good shot -- plasma, RF on, emissive probe is on (hot) -- V_float = +10-20 V when E is on, +2 V when J is on Bdot signal is strongest when E is on, correlating with V_float on emiss. probe. 1 MA current nl_04 = 0.8e20 several H modes no D ant J is trippy Next: repeat with D RF on. shot 003: good shot -- plasma, RF on but no D. J was first followed by E emissive probe is on (hot) -- V_float = +10-30 V when E is on, +2 V when J is on with initial spike of +30 V before entering H mode Bdot signal is strongest when E is on, correlating with V_float on emiss. probe. 1 MA current nl_04 = 0.8e20 several H modes no D ant Next: repeat with D RF on. shot 004: good shot -- plasma, RF on, first D, then J, then E emissive probe is on (hot) -- V_float = +50-120 V when D is on, +10-20 V when J is on, and +10-20 V when E is on V_float is quietest (lowest values) when in H mode Bdot signal is strongest when D is on, followed by E, then J 1 MA current nl_04 = 0.8e20 3 H modes Next: repeat with J always on on top of D and E staircases. shot 005: good shot -- plasma, RF on, J always on, D staircase followed by E staircase D is trippy emissive probe is on (hot) -- V_float = +25-75 V when D is on, +25 V when J is on before H mode (first antenna to be on), and +5-10 V when E is on Bdot signal is strongest when J just turns on before entering H mode 1 MA current nl_04 = 0.8e20 several H modes on top of one large H mode Next: repeat with improved D coupling shot 006: good shot -- plasma, RF on, J always on, D staircase followed by E staircase D is trippy again emissive probe is on (hot) -- V_float = +50-175 V when D is on, +25 V when J is on before H mode (first antenna to be on) but reduces to +2 V when in H mode, and +10-20 V when E is on Bdot signal is strongest when J just turns on before entering H mode, H mode clearly quiets Bdot and emissive probe response 1 MA current nl_04 = 0.8e20 4 H modes Next: try one more time to improve D shot 007: Disruption at 1.48 s, RF on, J always on, D staircase followed by E staircase D is trippy again emissive probe is on (hot) -- V_float = +50-150 V when D is on, +25 V when J is on before H mode (first antenna to be on) but reduces to +2-10 V when in H mode, and +10 V when E is on Bdot signal is strongest when J just turns on before entering H mode, H mode clearly quiets Bdot and emissive probe response 1 MA current nl_04 = 0.8e20 2 H modes Next: raise Ip to 1.2 MA, keep everything else same shot 008: good shot -- plasma, RF on, J always on, D staircase followed by E staircase D is trippy emissive probe is on (hot) -- V_float = +50-150 V when D is on, +25 V when J is on before H mode (first antenna to be on) but reduces to +2 V when in H mode, and +5-30 V when E is on Bdot signal is strongest when J just turns on before entering H mode and when V_float spikes to +150 V when D is on. 1.2 MA current nl_04 = 0.8e20 several H modes on top of one large H mode Next: repeat shot 009: good shot -- plasma, RF on, J always on, D staircase followed by E staircase emissive probe is on (hot) -- V_float = +50-200 V (spiky) when D is on, +25 V when J is on before H mode (first antenna to be on) but reduces to +2 V when in H mode, and +5 V when E is on with occasional 20 - 80 V spikes Bdot signal is strongest when J just turns on before entering H mode and when V_float spikes to +150 V when D is on. 1.2 MA current nl_04 = 0.8e20 several H modes on top of one large H mode Next: make Ip = 0.8 MA, everything else same shot 010: disruption at 0.91 s, RF on, J always on, D just turned on, no E emissive probe is on (hot) -- V_float = +15 V when D is on, +20 V when J is on just before H mode (first antenna to be on) but reduces to +2 V when in H mode Bdot signal is strongest when J just turns on before entering H mode. 0.8 MA current nl_04 = 0.8e20 1 H mode Next: repeat shot 011: disruption at 1.2 s, RF on, J always on, D turned on, no E emissive probe is on (hot) -- V_float = +50-150 V when D is on, +30 V when J is on just before H mode (first antenna to be on) but reduces to +2 V when in H mode Bdot signal is strongest when J just turns on before entering H mode and during high voltage spikes when D is on. 0.8 MA current nl_04 = 0.8e20 2 H modes Next: repeat with raised strike point to avoid disruption and change D and E order (first E then D) shot 012: disruption at 1.2 s, RF on, J always on, E staircase, then D staircase emissive probe is on (hot) -- V_float = +50-150 V when D is on, +30 V when J is on just before H mode (first antenna to be on) but reduces to +5 V when in H mode, +10 V when E is on Bdot signal is strongest when J just turns on before entering H mode and during high voltage spikes when D is on. 0.8 MA current nl_04 = 0.8e20 several H modes Next: 0.6 MA Ip, same for everything else shot 013: disruption at 1.03 s, RF on, J always on, E staircase, no D emissive probe is on (hot) V_float = +10-20 V when J is on (first antenna to be on), +15-20 V when E is on Bdot signal is strongest when J just turns on before entering H mode and quiets when in H mode 0.6 MA current nl_04 = 0.8e20 1 weak H mode Next: repeat with raised strike point shot 014: good shot -- plasma RF on, J always on, E staircase, then D staircase emissive probe is on (hot) V_float = +15-20 V when J is on (first antenna to be on), +15 V when E is on +25 V when D is on No V_float spikes, essentially flat voltage but goes up with D power Bdot signal is strongest when J just turns on before entering H mode and quiets when in H mode 0.6 MA current nl_04 = 0.8e20 1 long H mode Next: repeat with D and E exchanged (first D then E) shot 015: good shot -- plasma RF on, J always on, D staircase, then E staircase emissive probe is on (hot) V_float = +10-20 V when J is on (first antenna to be on), +10-25 V when D is on (staircased V_float increase) +10-20 V when E is on (staircased V_float increase) No V_float spikes, staircased voltage increases when D and E are on Bdot signal is strongest when J just turns on before entering H mode and quiets when in H mode 0.6 MA current nl_04 = 0.8e20 1 long H mode Next: raise Ip to 0.8 MA and no J ant. while keeping D and E staircased to see if we can have no H modes. shot 016: good shot -- plasma, RF on, J is off, D tripped, then E staircase emissive probe is on (hot) V_float = +5-15 V when E is on, no D and no J (V_float = +2 V) Bdot signal is strongest before H mode 0.8 MA current nl_04 = 0.8e20 1 late H mode Next: repeat shot 017: good shot -- plasma, RF on, J is off, D staircase, then E staircase emissive probe is on (hot) V_float = +20-40 V when D is on, V_float = +5V when E is on Bdot signal is strongest when E is on 0.8 MA current nl_04 = 0.8e20 no H modes Next: repeat but with increased emission on filament (I_filament up from 1.8 A to 2.0 A) shot 018: good shot -- plasma, RF on, J is off, D staircase, then E staircase. essentially no difference from shot 017 in probe signals. emissive probe is on (hot) V_float = +20-40 V when D is on, V_float = +5V when E is on Bdot signal is strongest when E is on, by a lot, no idea why 0.8 MA current nl_04 = 0.8e20 no H modes Next: increase Ip to 1.0 MA, everything else same. shot 019: good shot -- plasma, RF on, J is off, D staircase, then E staircase. late disruption at 1.6 s emissive probe is on (hot) V_float = +40-80 V (sawtooth correlated spikes) when D is on, V_float = +10-15V (much smaller sawteeth compared to D) when E is on B_phi dot probe signal correlates well with V_float on emissive probe when D is on. Sawteeth on Bdot probes as well. 1.0 MA current nl_04 = 0.8e20 no H modes Next: increase Ip to 1.2 MA, everything else same. shot 020: good shot -- plasma, RF on, J is off, D staircase, no E. disruption at 1.16 s emissive probe is on (hot) V_float = +40-180 V (sawtooth correlated spikes) when D is on, no E Appears to have little correlation between Bdot and emissive probe signals Sawteeth on Bdot probes as well. 1.2 MA current nl_04 = 0.8e20 no H modes Next: repeat shot 021: good shot -- plasma, RF on, J is off, D staircase, no E. disruption at 1.16 s emissive probe is on (hot) V_float = +40-150 V (sawtooth correlated spikes) when D is on, no E Appears to have little correlation between Bdot and emissive probe signals Sawteeth on Bdot probes as well. 1.2 MA current nl_04 = 0.8e20 no H modes very similar to shot 020 Next: repeat but switch D and E (E first) shot 022: disrupt., J is off, no D, no E. very early disruption at 0.54 s Next: repeat but increase nl_04 to 0.9e20 shot 023: disrupt., J is off, no D, no E. very early disruption at 0.59 s Next: Bring Ip down to 1.0 MA, nl_04 down to 0.8e20, run emissive probe cold shot 024: good shot -- plasma, RF on, J is off, D staircase, then E staircase. late disruption at 1.57 s. emissive probe is off (cold) V_float = -3 V when D is on, V_float = -2 V when E is on Bdot signal is about same between D and E 1.0 MA current nl_04 = 0.8e20 no H modes Next: repeat but with J on top of D and E, emiss. filament is on (I_filament = 2.0 A) shot 025: good shot -- plasma, RF on, J is on all time, D staircase, then E staircase. late disruption at 1.64 s emissive probe is on (hot) V_float = +30-60 V (sawtooth correlated spikes) when D is on, V_float = +15-20V (much smaller sawteeth compared to D) when E is on Sawteeth on Bdot probes as well. 1.0 MA current nl_04 = 0.8e20 no H modes similar in signal shape (but lower in magnitude) to shot019 except for spike when J turns on Next: drop Ip to 0.8 MA, increase nl_04 to 1e20 shot 026: good shot -- plasma, RF on, J is off, D tripped, then E staircase emissive probe is on (hot) V_float = +5-10V when E is on Strong Bdot signal but very low V_float before H mode. Bdot signal drops when plasma enters H mode as expected. Sawteeth on Bdot probes as well. 0.8 MA current nl_04 = 1.0e20 1 very late H mode Next: back to inner wall limited, Ip = 1.0 MA, nl_04 = 0.8e20, Bt up to 5.6 T (from 5.4 T), same as shot 025 but at 5.6 T. shot 027: good shot -- plasma, RF on, J is off, D staircased, then E staircase emissive probe is on (hot) V_float = +20-100 V (spiky sawteeth) when D is on V_float = +10V when E is on B_phi bdot probe correlates with V_float Bdot signal is bigger when D is on Sawteeth on Bdot probes as well. 1.0 MA current nl_04 = 0.8e20 no H modes Next: Bt up to 5.8 T shot 028: good shot -- plasma, RF on, J is off, D staircased, then E staircase emissive probe is on (hot) V_float = +50-130 V (spiky sawteeth) when D is on V_float = +10-20V when E is on B_p bdot probe correlates with V_float Bdot signal is bigger when D is on Sawteeth on Bdot probes as well. 1.0 MA current nl_04 = 0.8e20 Bt = 5.8 T no H modes Next: Bt up to 6.0 T. shot 029: good shot -- plasma, RF on, J is off, D staircased, then E staircase late disrupt. at 1.66 s emissive probe is on (hot) V_float = +10-25 V when D is on V_float = +5-15V when E is on Bdot signal is correlated with D but not E RF power 1.0 MA current nl_04 = 0.8e20 Bt = 6.0 T no H modes Next: Bt down to 5.2 T shot 030: good shot -- plasma, RF on, J is off, D staircased, then E staircase late disrupt. at 1.60 s emissive probe is on (hot) V_float = +20-40 V when D is on V_float = +20-25V when E is on Bdot signal is correlated with D but not E RF power Bdot signal is strongest when D is on 1.0 MA current nl_04 = 0.8e20 Bt = 5.2 T no H modes Next: Bt down to 5.0 T shot 031: good shot -- plasma, RF on, J is off, D staircased, then E staircase emissive probe is on (hot) V_float = +10-25 V when D is on V_float = +10-15V when E is on Bdot signal is strongest when D is on 1.0 MA current nl_04 = 0.8e20 Bt = 5.0 T no H modes Next: Bt down to 4.7 T shot 032: good shot -- plasma, RF on, J is off, D staircased, then E staircase late disruption at 1.60 s emissive probe is on (hot) V_float = +20-40 V when D is on V_float = +15-30V when E is on Bdot signal is strongest when E is on Bdot signal is correlated with RF when E is on 1.0 MA current nl_04 = 0.8e20 Bt = 5.0 T no H modes Next shot: 1 MA, 5.4 T, ramping D and E power shot 033: good shot -- plasma, RF on, J is off, D ramped up, then E ramped up late disruption at 1.61 s Very large sawteeth on Bdot and emissive probes signals emissive probe is on (hot) V_float = ramps from +40 to +200 V when D is on V_float = ramps from +10 to +15 V when E is on Bdot signal is strongest when D is on Bdot signal is correlated with RF when D is on 1.0 MA current nl_04 = 0.8e20 Bt = 5.4 T no H modes Last shot of this run |
| Physics Operator Summaries |
| Entered: Aug 28 2009 10:22:51:273PM |
| Author: Robert Granetz |
Run summary for Friday 2009/08/28
MP558 - Characterization of ICRF sheaths
Session leaders: R. Ochoukov
Physics operator: R. Granetz
This run involved measurements with the emissive probe and the bdot probes
to look at RF sheaths over a range of plasma current and toroidal field, in
both diverted (H-mode) and limited (L-mode) configurations. The D and E
antenna power was scanned in a staircase pattern on each shot. J-antenna
was run mostly at constant power in the diverted plasmas, and was not used
in the limited plasmas. RF performance today was very reliable. The run was
quite successful. Note that the latest boronization was a full week ago,
and we're going to repeat this run next week immediately after a
boronization in order to compare results.
The machine ran flawlessly today. There were no fizzles, duds, power
supply problems, or computer problems. One operational thing that we noted
today is that limited plasmas are much more susceptible to locked mode
disruptions compared to diverted plasmas. Possibly our error field
calculations need to be improved.
Scorecard: 33 plasmas
0 duds
0 fizzles
0 power supply tests
0 no-power MDS shot cycles
--------------
Total: 33 shot cycles (100% reliability)
|
| Session Leader Comments | |||
| Aug 28 2009 09:10:56:050AM | 1090828001 | Roman Ochoukov | shot 001: good shot -- plasma, no RF,
emissive probe is off (cold) -- V_float = -1 V 1 MA current nl_o4 = 0.8e20 1 late H mode Next: repeat with RF on: staircased with D, then E, then J steps are 0.5, 1, and 1.5 MW. Turn emissive probe on. |
| Aug 28 2009 09:35:27:687AM | 1090828002 | Roman Ochoukov | shot 002: good shot -- plasma, RF on,
emissive probe is on (hot) -- V_float = +10-20 V when E is on, +2 V when J is on Bdot signal is strongest when E is on, correlating with V_float on emiss. probe. 1 MA current nl_04 = 0.8e20 several H modes no D ant J is trippy Next: repeat with D RF on. |
| Aug 28 2009 09:45:25:940AM | 1090828003 | Roman Ochoukov | shot 003: good shot -- plasma, RF on but no D. J was first followed by E
emissive probe is on (hot) -- V_float = +10-30 V when E is on, +2 V when J is on with initial spike of +30 V before entering H mode Bdot signal is strongest when E is on, correlating with V_float on emiss. probe. 1 MA current nl_04 = 0.8e20 several H modes no D ant Next: repeat with D RF on. |
| Aug 28 2009 10:02:09:180AM | 1090828004 | Roman Ochoukov | shot 004: good shot -- plasma, RF on, first D, then J, then E
emissive probe is on (hot) -- V_float = +50-120 V when D is on, +10-20 V when J is on, and +10-20 V when E is on V_float is quietest (lowest values) when in H mode Bdot signal is strongest when D is on, followed by E, then J 1 MA current nl_04 = 0.8e20 3 H modes Next: repeat with J always on on top of D and E staircases. |
| Aug 28 2009 10:17:18:077AM | 1090828005 | Roman Ochoukov | shot 005: good shot -- plasma, RF on, J always on, D staircase followed by E staircase
D is trippy emissive probe is on (hot) -- V_float = +25-75 V when D is on, +25 V when J is on before H mode (first antenna to be on), and +5-10 V when E is on Bdot signal is strongest when J just turns on before entering H mode 1 MA current nl_04 = 0.8e20 several H modes on top of one large H mode Next: repeat with improved D coupling |
| Aug 28 2009 10:46:04:883AM | 1090828006 | Roman Ochoukov | shot 006: good shot -- plasma, RF on, J always on, D staircase followed by E staircase
D is trippy again emissive probe is on (hot) -- V_float = +50-175 V when D is on, +25 V when J is on before H mode (first antenna to be on) but reduces to +2 V when in H mode, and +10-20 V when E is on Bdot signal is strongest when J just turns on before entering H mode, H mode clearly quiets Bdot and emissive probe response 1 MA current nl_04 = 0.8e20 4 H modes Next: try one more time to improve D |
| Aug 28 2009 10:45:34:197AM | 1090828007 | Roman Ochoukov | shot 007: Disruption at 1.48 s, RF on, J always on, D staircase followed by E staircase
D is trippy again emissive probe is on (hot) -- V_float = +50-150 V when D is on, +25 V when J is on before H mode (first antenna to be on) but reduces to +2-10 V when in H mode, and +10 V when E is on Bdot signal is strongest when J just turns on before entering H mode, H mode clearly quiets Bdot and emissive probe response 1 MA current nl_04 = 0.8e20 2 H modes Next: raise Ip to 1.2 MA, keep everything else same |
| Aug 28 2009 10:59:04:967AM | 1090828008 | Roman Ochoukov | shot 008: good shot -- plasma, RF on, J always on, D staircase followed by E staircase
D is trippy emissive probe is on (hot) -- V_float = +50-150 V when D is on, +25 V when J is on before H mode (first antenna to be on) but reduces to +2 V when in H mode, and +5-30 V when E is on Bdot signal is strongest when J just turns on before entering H mode and when V_float spikes to +150 V when D is on. 1.2 MA current nl_04 = 0.8e20 several H modes on top of one large H mode Next: repeat |
| Aug 28 2009 11:14:41:957AM | 1090828009 | Roman Ochoukov | shot 009: good shot -- plasma, RF on, J always on, D staircase followed by E staircase
emissive probe is on (hot) -- V_float = +50-200 V (spiky) when D is on, +25 V when J is on before H mode (first antenna to be on) but reduces to +2 V when in H mode, and +5 V when E is on with occasional 20 - 80 V spikes Bdot signal is strongest when J just turns on before entering H mode and when V_float spikes to +150 V when D is on. 1.2 MA current nl_04 = 0.8e20 several H modes on top of one large H mode Next: make Ip = 0.8 MA, everything else same |
| Aug 28 2009 11:28:31:493AM | 1090828010 | Roman Ochoukov | shot 010: disruption at 0.91 s, RF on, J always on, D just turned on, no E
emissive probe is on (hot) -- V_float = +15 V when D is on, +20 V when J is on just before H mode (first antenna to be on) but reduces to +2 V when in H mode Bdot signal is strongest when J just turns on before entering H mode. 0.8 MA current nl_04 = 0.8e20 1 H mode Next: repeat |
| Aug 28 2009 11:44:48:017AM | 1090828011 | Roman Ochoukov | shot 011: disruption at 1.2 s, RF on, J always on, D turned on, no E
emissive probe is on (hot) -- V_float = +50-150 V when D is on, +30 V when J is on just before H mode (first antenna to be on) but reduces to +2 V when in H mode Bdot signal is strongest when J just turns on before entering H mode and during high voltage spikes when D is on. 0.8 MA current nl_04 = 0.8e20 2 H modes Next: repeat with raised strike point to avoid disruption and change D and E order (first E then D) |
| Aug 28 2009 11:54:57:067AM | 1090828012 | Roman Ochoukov | shot 012: disruption at 1.2 s, RF on, J always on, E staircase, then D staircase
emissive probe is on (hot) -- V_float = +50-150 V when D is on, +30 V when J is on just before H mode (first antenna to be on) but reduces to +5 V when in H mode, +10 V when E is on Bdot signal is strongest when J just turns on before entering H mode and during high voltage spikes when D is on. 0.8 MA current nl_04 = 0.8e20 several H modes Next: 0.6 MA Ip, same for everything else |
| Aug 28 2009 12:07:08:307PM | 1090828013 | Roman Ochoukov | shot 013: disruption at 1.03 s, RF on, J always on, E staircase, no D
emissive probe is on (hot) V_float = +10-20 V when J is on (first antenna to be on), +15-20 V when E is on Bdot signal is strongest when J just turns on before entering H mode and quiets when in H mode 0.6 MA current nl_04 = 0.8e20 1 weak H mode Next: repeat with raised strike point |
| Aug 28 2009 12:20:09:437PM | 1090828014 | Roman Ochoukov | shot 014: good shot -- plasma RF on, J always on, E staircase, then D staircase
emissive probe is on (hot) V_float = +15-20 V when J is on (first antenna to be on), +15 V when E is on +25 V when D is on No V_float spikes, essentially flat voltage but goes up with D power Bdot signal is strongest when J just turns on before entering H mode and quiets when in H mode 0.6 MA current nl_04 = 0.8e20 1 long H mode Next: repeat with D and E exchanged (first D then E) |
| Aug 28 2009 12:41:36:600PM | 1090828015 | Roman Ochoukov | shot 015: good shot -- plasma RF on, J always on, D staircase, then E staircase
emissive probe is on (hot) V_float = +10-20 V when J is on (first antenna to be on), +10-25 V when D is on (staircased V_float increase) +10-20 V when E is on (staircased V_float increase) No V_float spikes, staircased voltage increases when D and E are on Bdot signal is strongest when J just turns on before entering H mode and quiets when in H mode 0.6 MA current nl_04 = 0.8e20 1 long H mode Next: raise Ip to 0.8 MA and no J ant. while keeping D and E staircased to see if we can have no H modes. |
| Aug 28 2009 12:54:57:263PM | 1090828016 | Roman Ochoukov | shot 016: good shot -- plasma, RF on, J is off, D tripped, then E staircase
emissive probe is on (hot) V_float = +5-15 V when E is on, no D and no J (V_float = +2 V) Bdot signal is strongest before H mode 0.8 MA current nl_04 = 0.8e20 1 late H mode Next: repeat |
| Aug 28 2009 01:16:22:920PM | 1090828017 | Roman Ochoukov | shot 017: good shot -- plasma, RF on, J is off, D staircase, then E staircase
emissive probe is on (hot) V_float = +20-40 V when D is on, V_float = +5V when E is on Bdot signal is strongest when E is on 0.8 MA current nl_04 = 0.8e20 no H modes Next: repeat but with increased emission on filament (I_filament up from 1.8 A to 2.0 A) |
| Aug 28 2009 01:27:50:987PM | 1090828018 | Roman Ochoukov | shot 018: good shot -- plasma, RF on, J is off, D staircase, then E staircase
essentially no difference from shot 017 in probe signals. emissive probe is on (hot) V_float = +20-40 V when D is on, V_float = +5V when E is on Bdot signal is strongest when E is on, by a lot, no idea why 0.8 MA current nl_04 = 0.8e20 no H modes Next: increase Ip to 1.0 MA, everything else same. |
| Aug 28 2009 01:45:22:993PM | 1090828019 | Roman Ochoukov | shot 019: good shot -- plasma, RF on, J is off, D staircase, then E staircase
late disruption at 1.6 s emissive probe is on (hot) V_float = +40-80 V (sawtooth correlated spikes) when D is on, V_float = +10-15V (much smaller sawteeth compared to D) when E is on B_phi dot probe signal correlates well with V_float on emissive probe when D is on. Sawteeth on Bdot probes as well. 1.0 MA current nl_04 = 0.8e20 no H modes Next: increase Ip to 1.2 MA, everything else same. |
| Aug 28 2009 02:00:45:060PM | 1090828020 | Roman Ochoukov | shot 020: good shot -- plasma, RF on, J is off, D staircase, no E
disruption at 1.16 s emissive probe is on (hot) V_float = +40-180 V (sawtooth correlated spikes) when D is on, no E Appears to have little correlation between Bdot and emissive probe signals Sawteeth on Bdot probes as well. 1.2 MA current nl_04 = 0.8e20 no H modes Next: repeat |
| Aug 28 2009 02:12:50:473PM | 1090828021 | Roman Ochoukov | shot 021: good shot -- plasma, RF on, J is off, D staircase, no E
disruption at 1.16 s emissive probe is on (hot) V_float = +40-150 V (sawtooth correlated spikes) when D is on, no E Appears to have little correlation between Bdot and emissive probe signals Sawteeth on Bdot probes as well. 1.2 MA current nl_04 = 0.8e20 no H modes very similar to shot 020 Next: repeat but switch D and E (E first) |
| Aug 28 2009 02:26:30:057PM | 1090828022 | Roman Ochoukov | shot 022: disrupt., J is off, no D, no E
very early disruption at 0.54 s Next: repeat but increase nl_04 to 0.9e20 |
| Aug 28 2009 02:39:09:890PM | 1090828023 | Roman Ochoukov | shot 023: disrupt., J is off, no D, no E
very early disruption at 0.59 s Next: Bring Ip down to 1.0 MA, nl_04 down to 0.8e20, run emissive probe cold |
| Aug 28 2009 02:54:10:613PM | 1090828024 | Roman Ochoukov | shot 024: good shot -- plasma, RF on, J is off, D staircase, then E staircase
late disruption at 1.57 s. emissive probe is off (cold) V_float = -3 V when D is on, V_float = -2 V when E is on Bdot signal is about same between D and E 1.0 MA current nl_04 = 0.8e20 no H modes Next: repeat but with J on top of D and E, emiss. filament is on (I_filament = 2.0 A) |
| Aug 28 2009 03:17:53:560PM | 1090828025 | Roman Ochoukov | shot 025: good shot -- plasma, RF on, J is on all time, D staircase, then E staircase
late disruption at 1.64 s emissive probe is on (hot) V_float = +30-60 V (sawtooth correlated spikes) when D is on, V_float = +15-20V (much smaller sawteeth compared to D) when E is on Sawteeth on Bdot probes as well. 1.0 MA current nl_04 = 0.8e20 no H modes similar in signal shape (but lower in magnitude) to shot019 except for spike when J turns on Next: drop Ip to 0.8 MA, increase nl_04 to 1e20 |
| Aug 28 2009 03:30:25:707PM | 1090828026 | Roman Ochoukov | shot 026: good shot -- plasma, RF on, J is off, D tripped, then E staircase
emissive probe is on (hot) V_float = +5-10V when E is on Strong Bdot signal but very low V_float before H mode. Bdot signal drops when plasma enters H mode as expected. Sawteeth on Bdot probes as well. 0.8 MA current nl_04 = 1.0e20 1 very late H mode Next: back to inner wall limited, Ip = 1.0 MA, nl_04 = 0.8e20, Bt up to 5.6 T (from 5.4 T), same as shot 025 but at 5.6 T. |
| Aug 28 2009 04:41:09:000PM | 1090828027 | Roman Ochoukov | shot 027: good shot -- plasma, RF on, J is off, D staircased, then E staircase
emissive probe is on (hot) V_float = +20-100 V (spiky sawteeth) when D is on V_float = +10V when E is on B_phi bdot probe correlates with V_float Bdot signal is bigger when D is on Sawteeth on Bdot probes as well. 1.0 MA current nl_04 = 0.8e20 no H modes Next: Bt up to 5.8 T |
| Aug 28 2009 04:41:28:890PM | 1090828028 | Roman Ochoukov | shot 028: good shot -- plasma, RF on, J is off, D staircased, then E staircase
emissive probe is on (hot) V_float = +50-130 V (spiky sawteeth) when D is on V_float = +10-20V when E is on B_p bdot probe correlates with V_float Bdot signal is bigger when D is on Sawteeth on Bdot probes as well. 1.0 MA current nl_04 = 0.8e20 Bt = 5.8 T no H modes Next: Bt up to 6.0 T |
| Aug 28 2009 04:42:20:157PM | 1090828029 | Roman Ochoukov | shot 029: good shot -- plasma, RF on, J is off, D staircased, then E staircase
late disrupt. at 1.66 s emissive probe is on (hot) V_float = +10-25 V when D is on V_float = +5-15V when E is on Bdot signal is correlated with D but not E RF power 1.0 MA current nl_04 = 0.8e20 Bt = 6.0 T no H modes Next: Bt down to 5.2 T |
| Aug 28 2009 04:41:51:233PM | 1090828030 | Roman Ochoukov | shot 030: good shot -- plasma, RF on, J is off, D staircased, then E staircase
late disrupt. at 1.60 s emissive probe is on (hot) V_float = +20-40 V when D is on V_float = +20-25V when E is on Bdot signal is correlated with D but not E RF power Bdot signal is strongest when D is on 1.0 MA current nl_04 = 0.8e20 Bt = 5.2 T no H modes Next: Bt down to 5.0 T |
| Aug 28 2009 04:42:43:610PM | 1090828031 | Roman Ochoukov | shot 031: good shot -- plasma, RF on, J is off, D staircased, then E staircase
emissive probe is on (hot) V_float = +10-25 V when D is on V_float = +10-15V when E is on Bdot signal is strongest when D is on 1.0 MA current nl_04 = 0.8e20 Bt = 5.0 T no H modes Next: Bt down to 4.7 T |
| Aug 28 2009 05:02:22:740PM | 1090828032 | Roman Ochoukov | shot 032: good shot -- plasma, RF on, J is off, D staircased, then E staircase
late disruption at 1.60 s emissive probe is on (hot) V_float = +20-40 V when D is on V_float = +15-30V when E is on Bdot signal is strongest when E is on Bdot signal is correlated with RF when E is on 1.0 MA current nl_04 = 0.8e20 Bt = 5.0 T no H modes Next shot: 1 MA, 5.4 T, ramping D and E power |
| Aug 28 2009 05:13:19:997PM | 1090828033 | Roman Ochoukov | shot 033: good shot -- plasma, RF on, J is off, D ramped up, then E ramped up
late disruption at 1.61 s Very large sawteeth on Bdot and emissive probes signals emissive probe is on (hot) V_float = ramps from +40 to +200 V when D is on V_float = ramps from +10 to +15 V when E is on Bdot signal is strongest when D is on Bdot signal is correlated with RF when D is on 1.0 MA current nl_04 = 0.8e20 Bt = 5.4 T no H modes Last shot of this run |
| Physics Operator Comments | |||
| Aug 28 2009 09:18:19:290AM | Robert Granetz | Setup seg 2 from seg 2 of shot 1090717005 (1 MA, 5.4 T, 0.8e20 m-2, specific shape parameters. | |
| Aug 28 2009 09:10:57:033AM | 1090828001 | Robert Granetz |
Shot 01 -- Plasma, full length. 1.0 MA, 5.4 T, 0.8e20 m-2, elong=1.68, lower triang=0.50,
upper triang=0.25. RF not enabled yet. This equilibrium is acceptable for the session
leader. There was an ohmic H-mode late in the flattop (t>1.3 s).
Next shot: repeat, with RF in specific staircase waveform.
|
| Aug 28 2009 09:27:48:900AM | 1090828002 | Robert Granetz |
Shot 02 -- Plasma, full length. Good staircase power waveform on E-port; J staircase was partially
successful. D-port still needs some work before it can be turned on. Several H-modes.
Next shot: repeat; get D-port on
|
| Aug 28 2009 09:50:59:880AM | 1090828003 | Robert Granetz | Shot 03 -- Plasma, full length. Got J and E staircases. D is still being worked on. Next shot: repeat, this time definitely with D-port on. |
| Aug 28 2009 10:05:34:620AM | 1090828004 | Robert Granetz |
Shot 04 -- Plasma, full length. All three antennas executed good power staircase waveforms (with
no overlap). 3 H-modes. Target nl_04=0.8e20 m-2.
Next shot: repeat; change RF antenna ordering, programming, and overlap.
|
| Aug 28 2009 10:19:42:547AM | 1090828005 | Robert Granetz |
Shot 05 -- Plasma, full length. Lots of H-modes. Prf_J=1.6 for 0.9 s. D and E executed
staircases while J was one steady.
Next shot: tweaking the RF; no DPCS changes
|
| Aug 28 2009 10:33:10:113AM | 1090828006 | Robert Granetz |
Shot 06 -- Plasma, full length. J on steady for entire flattop, D & E staircases.
Some faulting. Multiple H-modes.
Next shot: repeat to see if we can improve RF faulting; no DPCS changes
|
| Aug 28 2009 10:41:46:587AM | 1090828007 | Robert Granetz |
Shot 07 -- Plasma, disrupted at t=1.48 s. Metallic injection. J and E worked well, D faulted at
the highest power.
Next shot: raise Ip to 1.2 MA; keep nl_04 at 0.8e20 m-2.
|
| Aug 28 2009 10:57:21:467AM | 1090828008 | Robert Granetz | Shot 08 -- Plasma, full length. Ip=1.2 MA. Lots of short H-modes. Next shot: repeat, no changes |
| Aug 28 2009 11:13:14:677AM | 1090828009 | Robert Granetz | Shot 09 -- Plasma, full length. 1.2 MA. J-port faulting more. Next shot: decrease Ip to 0.8 MA; keep nl_04=0.8e20 m-2 |
| Aug 28 2009 11:26:43:197AM | 1090828010 | Robert Granetz |
Shot 10 -- Plasma, disrupted at t=0.91 s due to high-Z injection at t=0.90 s. We'll have to repeat this
shot.
Next shot: repeat, no changes (0.8 MA)
|
| Aug 28 2009 11:41:58:640AM | 1090828011 | Robert Granetz | Shot 11 -- Plasma, disrupted at t=1.2 s due to injection at t=1.16 s. Next shot: raise ZXL by about 3.5 cm (to +0.020 m) to get strike point above W tiles. |
| Aug 28 2009 11:53:01:800AM | 1090828012 | Robert Granetz |
Shot 12 -- Plasma, full length. 0.8 MA. Multiple H-modes. No injections, which might mean that raising ZXL
on this shot actually solved the problem. Very good RF performance.
Next shot: reduce Ip to 0.6 MA.
|
| Aug 28 2009 12:08:02:277PM | 1090828013 | Robert Granetz |
Shot 13 -- Plasma, disrupted at t=1.03 s due to high-Z injection at t=0.99 s. 0.6 MA. The strike point
dropped a bit at this lower plasma current.
Next shot: raise ZXL another 1 cm.
|
| Aug 28 2009 12:22:12:000PM | 1090828014 | Robert Granetz | Shot 14 -- Plasma, full length. 0.6 MA. Nice RF performance. One long H-mode. Next shot: no DPCS changes; swap D & E timing. |
| Aug 28 2009 12:44:18:773PM | 1090828015 | Robert Granetz |
Shot 15 -- Plasma, full length. 0.6 MA. Good RF performance. One long H-mode. Early hard x-rays.
Next shot: set Ip at 0.8 MA; switch to inner wall limited in order to stay in L-mode. (set CLEARIN at
-0.015 m and ZXL at -.005 m)
|
| Aug 28 2009 12:57:38:083PM | 1090828016 | Robert Granetz |
Shot 16 -- Plasma, full length. 0.8 MA. Plasma is limited until about 1.3 s, and this results
in an H-mode after t=1.3 s.
Next shot: tweak CLEARIN to stay limited throughout the flattop.
|
| Aug 28 2009 01:13:28:450PM | 1090828017 | Robert Granetz |
Shot 17 -- Plasma, full length. 0.8 MA, limited, L-mode. Good RF. nl_04=0.8e20 m-2.
No J power (on purpose).
Next shot: repeat, no DPCS changes
|
| Aug 28 2009 01:26:35:830PM | 1090828018 | Robert Granetz | Shot 18 -- Plasma, full length. 0.8 MA, 0.8e20 m-2, limited, L-mode. Good RF performance. Next shot: raise Ip to 1.0 MA |
| Aug 28 2009 01:41:38:960PM | 1090828019 | Robert Granetz | Shot 19 -- Plasma, disrupted at t=1.60 s. 1.0 MA, limited, no H-modes, good RF. Next shot: raise Ip to 1.2 MA |
| Aug 28 2009 01:59:48:843PM | 1090828020 | Robert Granetz | Shot 20 -- Plasma, disrupted at t=1.16 s. Not sure why. 1.2 MA, limited. Next shot: tweak CLEARIN to keep plasma against inboard wall. |
| Aug 28 2009 02:16:47:053PM | 1090828021 | Robert Granetz |
Shot 21 -- Plasma, disrupted at t=1.16 s again. Identical to the preceding shot. The sawteeth get
very small and ragged for 20 ms before the disruption, but I think they're still there.
Next shot: no DPCS changes; swap D & E timings
|
| Aug 28 2009 02:24:16:913PM | 1090828022 | Robert Granetz | Shot 22 -- Plasma, disrupted at t=0.54 s. Looks like 2 small injections just before the disruption. Next shot: increase nl_04 a bit to 0.9e20 m-2 |
| Aug 28 2009 02:43:37:687PM | 1090828023 | Robert Granetz | Shot 23 -- Plasma, disrupted at t=0.59 s. Looks like a locked mode. Next shot: set Ip at 1.0 MA; put nl_04 back at 0.8e20 m-2 |
| Aug 28 2009 02:55:20:050PM | 1090828024 | Robert Granetz |
Shot 24 -- Plasma, disrupted at t=1.57 s. 1.0 MA, limited. Good RF. The sawteeth disappear again just
before the disruption, so maybe this is another locked mode. Apparently the error fields
are different in limited discharges compared to diverted discharges, and we're not
compensating them properly.
Next shot: no DPCS changes; modify the RF waveform programming
|
| Aug 28 2009 03:06:38:743PM | 1090828025 | Robert Granetz |
Shot 25 -- Plasma, disrupted at t=1.64 s. 1.0 MA, limited. Good RF. Looks like another locked
mode disruption, but it's too late in the shot to matter.
Next shot: change back to diverted, 0.8 MA, and set nl_04 to 1.0e20 m-2. Reload shot
12 from earlier today and change the density
|
| Aug 28 2009 03:30:27:300PM | 1090828026 | Robert Granetz |
Shot 26 -- Plasma, full length. 0.8 MA, DIVERTED. Maybe there's a problem with our error field
compensation which manifests itself on limited discharges. Only E antenna ran on this shot.
One brief H-mode late in the flattop.
J-port transmitter has a problem which won't be resolved before this run ends.
Next shot: change back to inner wall limited, 1.0 MA, 0.8e20 m-2, and Btor=5.6 T (158.5 kA). I reloaded
shot 25 from today and changed I_TF in seg 2.
|
| Aug 28 2009 03:44:27:413PM | 1090828027 | Robert Granetz |
Shot 27 -- Plasma, full length. 1.0 MA, limited, AND 5.6 T. Good RF.
Next shot: increase Btor to 5.8 T (164.1 kA); keep everything else the same. Note that
the TF PLC limit will be raised from 165 to 170 kA.
|
| Aug 28 2009 03:54:44:247PM | 1090828028 | Robert Granetz | Shot 28 -- Plasma, full length. 1.0 MA, limited, Btor=5.8 T. Good RF Next shot: raise Btor to 6.0 T (169.9 kA); keep all else the same |
| Aug 28 2009 04:09:56:690PM | 1090828029 | Robert Granetz |
Shot 29 -- Plasma, disrupted at t=1.66 s. 1.0 MA, 6.0 T, limited. Lots of hard x-rays. The disruption is
too late to matter, but it does look like another locked mode.
Next shot: change Btor to 5.2 T (147.1 kA); keep all else the same
|
| Aug 28 2009 04:28:33:370PM | 1090828030 | Robert Granetz | Shot 30 -- Plasma, disrupted at t=1.60 s. 1.0 MA, 5.2 T, limited. Good RF. Another locked mode disruption. Next shot: decrease Btor to 5.0 T; keep all else the same |
| Aug 28 2009 04:41:47:920PM | 1090828031 | Robert Granetz | Shot 31 -- Plasma, full length. 1.0 MA, 5.0 T, limited. Good RF. Next shot: decrease Btor to 4.7 (133.0 kA), keep all else the same |
| Aug 28 2009 04:57:29:503PM | 1090828032 | Robert Granetz |
Shot 32 -- Plasma, disrupted at t=1.60 s. 1.0 MA, 4.75 T, limited. Lots of early hard x-rays.
Good RF.
Next shot: set Btor back at 5.4 T; all else the same (1.0 MA, 0.8e20 m-2, limited)
|
| Aug 28 2009 05:07:45:900PM | 1090828033 | Robert Granetz |
Shot 33 -- Plasma, disrupted at t=1.62 s. 1.0 MA, 5.4 T, 0.8e20 m-2, limited. D & E ramped this
time, rather than staircase. Good RF.
End of run
|
| Engineering Operator Comments | ||||
| Shot | Time | Type | Status | Comment |
| 1 | 09:03:53:390AM | Plasma | Ok | |
| 2 | 09:20:05:850AM | Plasma | Ok | |
| 3 | 09:35:31:153AM | Plasma | Ok | |
| 4 | 09:52:40:677AM | Plasma | Ok | |
| 5 | 10:07:08:980AM | Plasma | Ok | |
| 6 | 10:22:05:187AM | Plasma | Ok | |
| 7 | 10:36:03:647AM | Plasma | Ok | |
| 8 | 10:49:19:777AM | Plasma | Ok | |
| 9 | 11:04:59:453AM | Plasma | Ok | |
| 10 | 11:19:03:583AM | Plasma | Ok | |
| 11 | 11:31:59:607AM | Plasma | Ok | |
| 12 | 11:44:44:170AM | Plasma | Ok | |
| 13 | 11:59:07:520AM | Plasma | Ok | |
| 14 | 12:12:09:043PM | Plasma | Ok | |
| 15 | 12:28:30:003PM | Plasma | Ok | |
| 16 | 12:45:24:117PM | Plasma | Ok | |
| 17 | 01:03:20:560PM | Plasma | Ok | |
| 18 | 01:19:48:843PM | Plasma | Ok | |
| 19 | 01:35:10:210PM | Plasma | Ok | |
| 20 | 01:49:53:180PM | Plasma | Ok | |
| 21 | 02:04:20:673PM | Plasma | Ok | |
| 22 | 02:19:08:507PM | Plasma | Ok | |
| 23 | 02:32:06:950PM | Plasma | Ok | |
| 24 | 02:44:45:033PM | Plasma | Ok | |
| 25 | 02:57:19:177PM | Plasma | Ok | |
| 26 | 03:16:43:653PM | Plasma | Ok | |
| 27 | 03:31:02:753PM | Plasma | Ok | |
| 28 | 03:47:01:820PM | Plasma | Ok | |
| 29 | 04:02:26:577PM | Plasma | Ok | |
| 30 | 04:20:00:583PM | Plasma | Ok | |
| 31 | 04:34:30:463PM | Plasma | Ok | |
| 32 | 04:49:26:860PM | Plasma | Ok | |
| 33 | 05:02:31:943PM | Plasma | Ok | |
| System Availability | ||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||
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