Electron thermal conductivity from heat wave propagation in Wendelstein 7-AS

Heat wave propagation experiments have been carried out on the Wendelstein 7-AS stellarator. The deposition of electron cyclotron resonance heating power is highly localized in the plasma centre, so that power modulation produces heat waves which propagate away from the deposition volume. Radiometry of the electron cyclotron emission is used to measure the generated temperature perturbation. The propagation time delay of the temperature perturbation as a function of distance to the power deposition region is used to determine the electron thermal conductivity χe. This value is then compared with the value determined by global power balance. In contrast to sawtooth propagation experiments in tokamaks, it is found that the value of χe from heat wave propagation is comparable to that calculated by power balance. In addition, inward propagating waves were produced by choosing a power deposition region away from the plasma centre. Experiments were carried out at 70 GHz in the ordinary mode and at 140 GHz in the extraordinary mode. Variations of the modulation power amplitude have demonstrated that the inferred value of χe is independent of the amplitude of the induced temperature perturbations

[1]  Tadashi Sekiguchi,et al.  Plasma Physics and Controlled Nuclear Fusion Research , 1987 .

[2]  G. Hogeweij,et al.  Evidence of coupling of thermal and particle transport from heat and density pulse measurements in JET , 1991 .

[3]  J. Callen,et al.  On measuring the electron heat diffusion coefficient in atokamak from sawtooth oscillation observations , 1979 .

[4]  Kenneth W Gentle,et al.  Dependence of heat pulse propagation on transport mechanisms: Consequences of nonconstant transport coefficients , 1988 .

[5]  G. L. Jahns,et al.  Experimental Measurement of Electron Heat Diffusivity in a Tokamak , 1977 .

[6]  W. Goedheer Inference of electron heat conductivity from the propagation of a temperature perturbation in the outer confinement region of a Tokamak , 1986 .

[7]  Kim,et al.  Experimental measurement of electron particle diffusion from sawtooth-induced density-pulse propagation in the Texas Experimental Tokamak. , 1988, Physical review letters.

[8]  G. Hogeweij,et al.  Tokamak transport studies using perturbation analysis , 1990 .

[9]  G. L. Jahns,et al.  Internal disruptions in tokamaks , 1977 .

[10]  Measurement of thermal transport by synchronous detection of modulated electron cyclotron heating in the Doublet III tokamak , 1986 .

[11]  H. J. Hartfuss,et al.  Fast multichannel heterodyne radiometer for electron cyclotron emission measurement on stellarator W VII‐A , 1985 .

[12]  E. Powers Spectral techniques for experimental investigation of plasma diffusion due to polychromatic fluctuations , 1974 .

[13]  H. Maassberg,et al.  Evaluation of the local heat conductivity coefficient by power-modulated electron cyclotron heating in the Wendelstein VII-A Stellarator , 1986 .

[14]  P. Mantica,et al.  Determination of diffusive and nondiffusive transport in modulation experiments in plasmas , 1991 .

[15]  Modelling of temperature profiles and transport scaling in auxiliary heated tokamaks , 1987 .

[16]  K. Riedel,et al.  ASDEX heat pulse propagation as a forced boundary value problem , 1988 .

[17]  F. Sardei,et al.  Optimum-confinement in the wendelstein 7-AS stellarator , 1991 .

[18]  B. Tubbing,et al.  Tokamak heat transport – a study of heat pulse propagation in JET , 1987 .

[19]  Heat-Pulse Propagation in Tokamaks and the Role of Density Perturbations , 1990 .

[20]  J. D. Bell,et al.  Heat pulse propagation studies in TFTR , 1986 .

[21]  F. Hinton,et al.  Effect of impurity particles on the finite-aspect ratio neoclassical ion thermal conductivity in a tokamak , 1986 .