Current drive experiments in SST1 tokamak with lower hybrid waves

2021 ◽  
Author(s):  
P K Sharma ◽  
D Raju ◽  
Surya Kumar Pathak ◽  
R Srinivasan ◽  
Kiran Ambulkar ◽  
...  

Abstract The steadystate superconducting tokamak (SST1) is aimed to demonstrate long pulse plasma discharges employing non-inductive current drive by means of lower hybrid current drive (LHCD) system. The major and minor radius of the machine is 1.1m and 0.2m respectively. The LHCD system for SST1 comprises of klystrons, each rated for 0.5MW-CW rf power at a frequency of 3.7 GHz. The grill antenna comprises of two rows, each row accommodating 32 waveguide elements. Electron cyclotron resonance (ECR) breakdown assisted Ohmic plasma is formed in SST1 to overcome the issues associated with low loop voltage start-ups. With recent modifications in the poloidal coils configuration, even with narrow EC pulse (~50ms), good repeatable and consistent Ohmic plasmas could be produced which helped in carrying out LHCD current drive experiments on SST1. These experiments demonstrated both fully as well as partially driven non-inductive plasma current in SST1 tokamak. Discharges with zero loop voltages were obtained. The interaction of lower hybrid waves with plasma and generation of suprathermal electrons could be established using energy spectra measured by CdTe detectors. Various other signatures like drop in loop voltages, negative loop voltages, spikes in hard x-rays and increase in 2nd harmonic ECE signal, further confirmed the current drive by LHW’s. The beneficial effect of LHW’s in suppressing hard x-rays was also demonstrated in these experiments. The non-inductive current drive in SST1 could also be established by modulating LH power. The longest discharge of ~650ms could be obtained in SST1 with the help of LHW’s. In this paper, the experimental results obtained with LHCD experiments on SST1 is reported and discussed in more details.

1989 ◽  
Vol 42 (1) ◽  
pp. 1-12
Author(s):  
Aldo Nocentini

The dependence of the efficiency of current drive by lower-hybrid waves on the shape and intensity of the wave spectrum is discussed in the case where no d.c. electric field is present. The discussion is based on a simple formula arising from a one-dimensional kinetic treatment of the problem.


1981 ◽  
Vol 26 (2) ◽  
pp. 359-367 ◽  
Author(s):  
M. Y. Yu ◽  
P. K. Shukla ◽  
H. U. Rahman

Nonlinear excitation of electrostatic and magnetostatic zero-frequency modes by finite-amplitude lower-hybrid waves is considered. It is found that modulational instabilities can give rise to enhanced plasma vortices. Dispersion relations, as well as analytical expressions for the growth rates, are obtained. The enhanced vortices may cause anomalous cross-field diffusion which can affect plasma confinement in tokamak devices when lower-hybrid waves are used for plasma heating or current drive. We found that magnetic fluctuations associated with the parametrically driven magnetostatic mode are of particular importance in tokamak plasmas.


2017 ◽  
Vol 157 ◽  
pp. 03011 ◽  
Author(s):  
Annika Ekedahl ◽  
Bojiang Ding ◽  
Xianzu Gong ◽  
Marc Goniche ◽  
Miaohui Li ◽  
...  

2017 ◽  
Vol 24 (3) ◽  
pp. 032502 ◽  
Author(s):  
Youlei Yang ◽  
Nong Xiang ◽  
Ye Min Hu

1993 ◽  
Author(s):  
S. von Goeler ◽  
R. Kaita ◽  
S. Bernabei ◽  
W. Davis ◽  
H. Fishman ◽  
...  

1989 ◽  
Author(s):  
M. Brusati ◽  
C. Gormezano ◽  
S. Knowlton ◽  
M. Lorentz-Gottardi( ◽  
F. Rimini

1993 ◽  
Author(s):  
S. von Goeler ◽  
R. Kaita ◽  
S. Bernabei ◽  
W. Davis ◽  
H. Fishman ◽  
...  

1985 ◽  
Vol 107 ◽  
pp. 505-508
Author(s):  
Motohiko Tanaka ◽  
K. Papadopoulos

It is commonly anticipated that high-energy electrons play an important role for the wave emission in flare bursts. For instance, electrons with >100 KeV are considered to create microwave emissions through gyro-synchrotron process and hard x-rays may be due to bremstrahlung with >25 KeV electrons. However, electron acceleration mechanism itself is still in speculations.


Author(s):  
S. Tanaka ◽  
Y. Terumichi ◽  
T. Maekawa ◽  
M. Nakamura ◽  
T. Cho ◽  
...  

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