Alcator C-Mod Weekly Highlights Jan 26, 1998 Plasma operations continued at Alcator C-Mod last week. Four run days were scheduled and completed, with nearly a hundred plasmas successfully produced. Overall machine performance was good. Startup reliability, always low after a boronization, rose from less than 50% on Tuesday to over 95% on Friday. This week's runs included some of the highest performance plasmas of the campaign, with stored energy (W_mhd) over 200kJ. Thursday and Friday had the 2nd and 4th highest daily neutron production of any C-Mod run, reflecting a large number of long, quasi-steady, high quality H-mode plasmas. Over the previous Friday night and Saturday morning a fresh boronization was carried out. 137 psi of diborane was used, for an average coverage of about 2000 Angstroms. This boronization processed the most diborane ever used during a single C-Mod boronization. In addition, we scanned the ECDC resonance out past the Faraday shield midplane location to just behind the current strap. Previous boronizations during this run campaign have been limited to just up to the Faraday shield.The first part of the run on Tuesday was devoted to standard (fiducial) discharges to evaluate the impact of the new boronization, and to complete the wall conditioning by running tokamak discharges. As expected from previous experience, startup reliability was poor during this phase. The walls were clearly pumping quite strongly, as evidenced by a lower than normal pressure rise from the initial puff, and the current rise was slower than normal. Once a series of successful startups was obtained, the fiducial shots evolved quickly, indicating improving wall conditions. EDA H-modes were readily obtained at 1MW of RF power. Moly levels at input powers up to 2MW of RF were significantly reduced from the previous week. After eight or nine successful discharges, we obtained early L-H transitions and the stored energy and H-factors were similar to the best obtained in the previous weeks. The second part of Tuesday's run was an investigation (MP#173B) of the relative efficiency of inboard and outboard gas fueling into limiter plasmas. This experiment was inspired by ASDEX results indicating that pellet fueling from the inboard side was more effective than with outside launched pellets. It was reasoned that if a deep source was not essential, similar physics might obtain for a gas puff directly into a limited plasma at the plasma-limiter contact point. An experiment was carried out using inside and outside limited plasmas, with deuterium fueling by gas capillaries in the respective limiter structures. We can conclude that gas fueling into the high-field side does NOT show any enhanced fueling efficiency compared to the low-field side. The actual density rises were small, and the absolute fueling efficiencies may be affected by marfe activity, but the comparative null result is clear. Wednesday's run investigated the effect of the prototype cryopump on impurity transport (MP #177). Ohmic plasmas with density ramps to divertor detachment and EDA H-mode plasmas were investigated. Argon or neon gas was puffed into these types of plasmas with the cryopump on or off. When on, the single module was determined to have deuterium pumping speeds in the range of 700-1000 l/sec. The core impurity ion densities were monitored with x-ray and VUV spectrometers and the divertor impurity neutral densities with an RGA. In Ohmic plasmas, the core argon and the edge neon were "pumping out", i.e., the time history of the signal was decaying away. Comparing the core argon density with and without the cryopump operational indicates that the pump had no effect on the decay rate. This indicates that something else, most likely the wall, is doing the pumping. Neon line brightnesses from charge states in the edge plasma (temperature < 150eV) do show a decrease in the equilibrium value with the cryopump operational. However, the initial "pumpout" is nearly identical with and without the cryopump, also indicating a strong wall sink. The density in these Ohmic plasmas was ramped to divertor detachment. After divertor detachment, the cryopump is observed to make a difference in core argon density. The penetration factor for puffed argon entering the core is lower after detachment with the cryopump on than it is after detachment with the cryopump off. Measurements of the neutral particle density in the divertor indicate that the density is lower by approximately 20% with the pump operational. In EDA H-modes, the "pump out" effect is still evident on the core argon density and there is no difference between plasmas with and without the cryopump operational. Core neon brightness measurements show no "pump out" behavior, although the SNR is small. There is also no discernible difference in the core neon behavior with and without the cryopump. However, there is a slight decrease, <20%, in both the divertor neutral neon and argon with the cryopump operational. These results are in contrast to those obtained with the non-recycling impurity gas nitrogen on 970617. During that run, the edge nitrogen brightness was reduced by a factor of two with the cryopump operational. Further analysis of these data continues. MP 192 Dynamic q scans in Enhanced D alpha H-mode was performed Thursday, with long (~1 sec) EDA H-modes during plasma current and toroidal field ramps to vary the edge safety factor. Confinement clearly increased with increasing plasma current and the best H-modes had H factors up to nearly 1.8. Stored energies up to 200 kJ were obtained with less than 3 MW of ICRF. It is more difficult to obtain EDA at higher current, but by starting in EDA at 0.8 MA, the EDA can be maintained up to at least 1.2 MA. Indeed, the last shot remains in EDA H-mode up to nearly 1.4 MA. The variation in q had little effect on the enhanced D alpha nature of the H-mode and preliminary analysis shows little increased MHD activity at rational edge q values, though this still needs to be analyzed in detail. This suggests that if MHD activity is responsible for the enhancement in D alpha emission, it must be broadband multiple mode numbers not linked to particular rational q values. During these ramped field and current discharges, the edge xray pedestal width was found to scale faster than linear with 1/Ip, and had no dependence on Btor. These data were obtained during steady state enhanced D-alpha H-modes by ramping plasma current and/or toroidal field up and down. Interpretation of these results is complicated by the fact that the observed quantity is the soft xray emissivity profile, not T, n, or p directly. Friday's run was the latest devoted to the multi-day experiment MP#166, "High q_parallel Dissipative Divertor". his proposal is an attempt to achieve simultaneously a good confinement H-mode with low Zeff and a detached divertor. The goal is to determine the threshold amount of impurity gas necessary to detach the divertor. Also, operation just above and just below the detachment threshold will be investigated. The run was successful in producing enhanced Dalpha (EDA) H-modes with 'steady-state' H-factors of about 1.6. Up to 3MW of power was coupled to the plasma. SOL power was up to 2.5MW, corresponding to an estimated q_parallel > 0.5GW per square meter. Divertor detachment was achieved with a combination of deuterium, helium, and nitrogen gas puffing. The first half of the run consisted of attempts to achieve a good EDA H-mode and to increase the divertor radiation. The deuterium gas puff during the H-mode was determined to be important in keeping the molybdenum levels low and the neutron rate high, and seemed to eliminate the H->L transitions. The puffing of helium and nitrogen in the divertor led to "death-ray" formation, high divertor radiated power, and eventually divertor detachment. It was later determined that the helium puffing was not necessary for detachment as nitrogen puffing alone was sufficient, although the amount of nitrogen needed was increased. Impurity gas feedback was also accomplished during this run. Feedback was done on an edge bolometer channel in the core array. This channel was identified earlier as a likely candidate to indicate when detachment was ocurring. The waveforms drawn were trapezoidal in shape (in detachment the waveform is triangular). Essentially this means we were trying to clip the bolometer signal off by using feedback on the impurity gas, in this case, nitrogen. The day started with hand drawn waveforms for the gas voltage. When detachment was observed, the feedback was switched on with a drawn waveform close to that of the previous shot. The feedback worked well, trying to keep the bolometer waveform close to that requested. With the helium puff turned off, the feedback requested extra nitrogen to match the drawn waveform and reached detachment. The goal of simultaneously achieving good confinement, low Zeff, and a detached divertor was not quite reached. On the best shot, H-factors of 1.6 decreased to 1.4 after the divertor detached, but did not decrease any further as detachment progressed. Zeff was high all day, never much less than 1.7 after the EDA H-mode was fully established. With impurity puffing, the typical change in Zeff was about 0.5. There is now a starting point for H-mode detachment studies. Comparison of plasma and divertor performance above and below the detachment threshold can now proceed (and other experiments requiring a detached H-mode). Also during Friday's run, reconstructions (Boswell-Terry) of the fish-eye view in D-gamma light show the regions where recombination is occuring. There is a region above the outer strike point that moves up the plate as the detachment proceeds. When the impurity gas flow is stopped, the region jumps back to just above the strike point. More of the delta(stored energy) vs. delta(toroidal rotation) space was filled in by Rice. Progress continued on development of the DNB for C-Mod. Assembly tests of the high capacitance section of the HV transmission line allowed completion of the mechanical design. Design of controls for the Accelerator supply continued. In-situ conditioning of the oil for the supply achieved a breakdown voltage of 40 kV and thus has shown continued improvement. The thermocouple system to be used for measurement of the beam footprint was tested in its final configuration. This included test of thermocouples, amplifiers and CAMAC data acquisition as well as setting up of the acquisiton modules in the DNB tree, and writing of test programs for data analysis. Gary Taylor and Bob Cutler of PPPL visited last week. Good signals are now being obtained on the new 19-channel polychromator. Some further optimization for the fields used on C-Mod is planned. The LANL IR camera was pulled off of C-Mod last week, and brought back to LANL for some repair and improvements. A broken calibration wire deep within the camera, which had been preventing us from doing remote-controlled internal hot/cold calibrations, was fixed. In addition, the camera was sent out to a prospective vendor for testing of a 1.2 Gigabit/second 12-bit digital interface over a fiber optic link, into a PCI card for a PC. The digital fiber link would allow direct 12-bit resolution capture into the PC, which would improve the system's dynamic range from the present standard 8-bit video, to 12-bits digital. We expect to have the unit back at C-Mod next week. Miklos Porkolab and Steve Witch attended 2nd European RF Conference in Brussels. Porkolab presented an invited talk, "Recent Progress in ICRF Physics", and Wukitch presented a poster on "D-He3 heating in Alcator C-Mod" Martin Greenwald spent 3 days in Washington DC attending a meeting of the ESnet Steering Committee, where he represents the interests of the FES program. Highlights include finalization of the ESnet Program Plan and a white paper on advanced network applications; proposed changes in the MICs network research program; NGI initiatives; progress in network performance monitoring; and discussion of an ESnet supported "telepresence" toolkit. Earl Marmar attended FESAC meeting in Germantown (Jan. 22). This week is a scheduled maintenance week at Alcator C-Mod. No runs are scheduled, although power system tests will be carried out. A review of the C-Mod five-year plan, and a meeting of the C-Mod Physics Advisory Committee, will take place at MIT this week.