Turbulence in Electrostatic Ion Acoustic Shocks.

Three types of collisionless electrostatic ion‐acoustic shocks are investigated using the University of California, Los Angeles, double plasma device: (a) laminar shocks; (b) small amplitude turbulent shocks in which the turbulence is confined to be upstream of the shock potential jump; and (c) large amplitude turbulent shocks in which the wave turbulence occurs throughout the shock transition. The wave turbulence is generated by ions which are reflected from the shock potential; linear theory spatial growth increments agree with experimental values. The experimental relationship between the shock Mach number and the shock potential is shown to be inconsistent with theoretical shock models which assume that the electrons are isothermal. Theoretical calculations which assume a trapped electron equation of a state and a turbulently flattened velocity distribution function for the reflected ions yields a Mach number vs potential relationship in agreement with experiment.

[1]  D. L. Kelly,et al.  Electromagnetic wavefunctions for parabolic plasma density profiles , 1974 .

[2]  A. Baños Calculation of reflection and transmission coefficients for a class of one‐dimensional wave propagation problems in inhomogeneous media , 1973 .

[3]  F. Coroniti,et al.  Electrostatic Instability of Ring Current Protons Beyond the Plasmapause During Injection Events , 1972 .

[4]  R. Thorne,et al.  Parasitic pitch angle diffusion of radiation belt particles by ion cyclotron waves , 1972 .

[5]  C. Kennel,et al.  External Production and Control of Electrojet Irregularities , 1972 .

[6]  A. Wong,et al.  Threshold and Saturation of the Parametric Decay Instability , 1972 .

[7]  C. Kennel,et al.  Relativistic electron precipitation during magnetic storm main phase , 1971 .

[8]  N. Booth Nonlinear Collisionless Interaction Between Electron and Ion Modes in Inhomogeneous Magnetoactive Plasmas. , 1971 .

[9]  Francis F. Chen,et al.  REMOTE PLASMA CONTROL, HEATING, MEASUREMENTS OF ELECTRON DISTRIBUTION, AND TRAPPED PARTICLES BY NONLINEAR ELECTROMAGNETIC INTERACTIONS. , 1971 .

[10]  R. Taylor,et al.  Formation and Interaction of Ion-Acoustic Solitions , 1970 .

[11]  C. Olson Electromagnetic plasma wave propagation along a magnetic field. Ph.D. Thesis , 1970 .

[12]  D. Baker,et al.  EFFICIENT MODULATION COUPLING BETWEEN ELECTRON AND ION RESONANCES IN MAGNETOACTIVE PLASMAS. , 1970 .

[13]  R. Taylor Steepening of Ion Acoustic Waves and Formation of Collisionless Electrostatic Shocks. , 1970 .

[14]  R. Taylor,et al.  Perturbed Ion Distributions in Ion Waves and Echoes , 1970 .

[15]  G. L. Johnston Linear and nonlinear theory of grid excitation of low frequency waves in a plasma , 1969 .

[16]  M. Goldman Theory of stability of large amplitude periodic /BGK/ waves in collisionless plasmas , 1969 .

[17]  V. Formisano,et al.  Small amplitude waves in high β plasmas , 1969, Journal of Plasma Physics.

[18]  B. Fried,et al.  LOW BETA PLASMA PENETRATION ACROSS A MAGNETIC FIELD , 1969 .

[19]  D. Baker,et al.  Measurements of Diffusion in Velocity Space from Ion-Ion Collisions , 1969 .

[20]  G. Knorr Inhomogeneous Two‐Stream Instability , 1968 .

[21]  D. Baker,et al.  ION-WAVE ECHOES. , 1968 .

[22]  C. Kennel,et al.  Magnetic Turbulence in Shocks , 1968 .