A 2.0 MW CW lower hybrid current drive (LHCD) system based on 3.7 GHz klystron sources, is in advanced stage of commissioning, which would drive and sustain plasma current, non-inductively, in superconducting steadystate tokamak (SST1) for long pulse operation. Four klystrons, each rated for 0.5 MW CW rf power, delivers 2.0 MW of rf power to four layer of the LHCD system, which finally feeds the rf power to grill antenna. The antenna system along with vacuum window and vacuum transmission line is successfully integrated on the machine. Its vacuum and pressurization compatibility has been successfully established. To validate the high power performance of LHCD system for SST1 machine, stage-wise commissioning of LHCD system in staggered manner is planned. It has been envisaged that LHCD power may be gradually increased initially, since full power may not be required during the initial phases of SST1 plasma operation. Also if the system is integrated in steps or in phases, then integration issues, as well as high power operational issues, if any, can be addressed, attended and handled in a simpler way before integrating all the layers to the grill antenna. To begin with, one klystron is connected to one layer, out of four layers, which energizes a quarter of the grill antenna. Gradually, the rf power and its pulse length is increased to validate high power performance of the system. Arcing and reflections are observed as rf power is gradually increased. The problems are analysed and after taking appropriate remedial action the system performance is improved for operation up to 160kW. Several trains of short pulses are launched in SST1 vacuum vessel for rf conditioning of the LHCD system. Normally, reflections are high when power is launched in vacuum; therefore the pulse length is restricted up to 100 milliseconds. The high power performance of this layer, connected with grill antenna is validated by launching high power microwaves in vacuum vessel of SST1 machine and experimental results obtained during the validation is presented in this paper. Based on this experience, the rest of the layers would be connected to the grill antenna to validate the LHCD system for full rated power.
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12 February 2014
RADIOFREQUENCY POWER IN PLASMAS: Proceedings of the 20th Topical Conference
25–28 June 2013
Sorrento, Italy
Research Article|
February 12 2014
Integration of LHCD system with SST1 machine and its high power rf performance in vacuum
P. K. Sharma;
P. K. Sharma
Institute for Plasma Research, Bhat, Gandhinagar-382428, Gujarat,
India
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K. K. Ambulkar;
K. K. Ambulkar
Institute for Plasma Research, Bhat, Gandhinagar-382428, Gujarat,
India
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S. Dalakoti;
S. Dalakoti
Institute for Plasma Research, Bhat, Gandhinagar-382428, Gujarat,
India
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P. R. Parmar;
P. R. Parmar
Institute for Plasma Research, Bhat, Gandhinagar-382428, Gujarat,
India
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C. G. Virani;
C. G. Virani
Institute for Plasma Research, Bhat, Gandhinagar-382428, Gujarat,
India
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A. L. Thakur
A. L. Thakur
Institute for Plasma Research, Bhat, Gandhinagar-382428, Gujarat,
India
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AIP Conf. Proc. 1580, 470–473 (2014)
Citation
P. K. Sharma, K. K. Ambulkar, S. Dalakoti, P. R. Parmar, C. G. Virani, A. L. Thakur; Integration of LHCD system with SST1 machine and its high power rf performance in vacuum. AIP Conf. Proc. 12 February 2014; 1580 (1): 470–473. https://doi.org/10.1063/1.4864590
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