Abstract

Microwave heat pulse propagation experiments have demonstrated a correlation between millimeter-scale turbulence and deposition profile broadening of electron cyclotron (EC) waves on the DIII-D tokamak. In a set of discharges in DIII-D, a variation in edge density fluctuations on the mm-scale is associated with 40%–150% broader deposition profiles, expressed in terms of normalized minor radius, as compared with equilibrium ray tracing. The 1D power profile is determined from transport analysis of the electron temperature response to EC power modulation using perturbative analysis with a square wave power modulation at 20–70 Hz, producing a series of Fourier harmonics that are fit collectively to resolve transport. Fitting an integrated heat flux expressed in the Fourier basis of the modulation to diffusive, convective, and coupled transport terms in a linear model can resolve the broadened EC deposition width from the power perturbation to resolve a broadening in each case. The best fit degree of beam broadening observed scales approximately linearly with the Doppler backscattering measured fluctuation level in the steep gradient region. Quantifying the effect of edge fluctuation broadening on EC current drive power needs of future devices will require 3D full-wave codes that can be validated on the current generation of machines. These DIII-D experiments provide a quantitative measure of fluctuation effects and a dataset to benchmark full-wave simulations that can model and eventually predict nonlinear effects neglected by 1D equilibrium beam and ray tracing.

Highlights

  • Electron cyclotron current drive (ECCD) is used to drive current in tokamak plasma and is the key means of stabilizing tearing modes, magnetohydrodyanmic structures that limit plasma confinement and drive disruptions.[1]

  • The behavior of microwaves used for electron cyclotron heating (ECH) in a tokamak plasma equilibrium is frequently simuluated with quasi-optical propagation

  • A linear transport model was used to fit the electron heat flux generated by electron cyclotron heating

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Summary

INTRODUCTION

Electron cyclotron current drive (ECCD) is used to drive current in tokamak plasma and is the key means of stabilizing tearing modes, magnetohydrodyanmic structures that limit plasma confinement and drive disruptions.[1]. Propegation through the plasma edge, where mm-scale fluctuations are strongest due to the steep gradient, results in multiple interactions, increasing divergence, and wider deposition at the same power.[8] Magnetic fluctuations can theoretically cause microwave scattering, but the predicted effect is much weaker and is not considered in this study.[15] For EC waves, parametric studies[8] with full-wave simulations suggest mm-scale structures with a correlation length of approximately half the RF vacuum wavelength, kvac 1⁄4 2:7 mm for the 110 GHz power used on DIII-D. This study quantifies the deposition width of EC heating across a range of edge conditions over which the Doppler Backscattering measured millimeter-scale fluctuations vary by a factor of 4, sufficient to produce a first experimental scaling of beam broadening with fluctuation level. An order of magnitude variation of the scattering fluctuations allows for a scaling of deposition broadening

Defining and assessing beam broadening
Measuring fluctuations
Generating a scaling in fluctuation amplitude
Perturbation measurements
Heat flux calculations
Defining transport coefficients
Methodology
Comparison of coefficients with the differential heat transport formulation
Fit transport coefficients
Findings
CONCLUSIONS
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