Plasma probe
Mariner IV plasma probe to measure density, velocity distribution, and bulk direction of proton flux component of solar plasma - components, operation, and performance
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Mariner IV plasma probe to measure density, velocity distribution, and bulk direction of proton flux component of solar plasma - components, operation, and performance
An ionospheric plasma probe was constructed which consists of a long cylinder with the end facing the flow closed by an end plate made up of multiple annular rings and a center disk. A theoretical argument is given which yields the plasma potential and electron temperature in terms of known plasma parameters and the currents to the various rings of the end plate. This probe was successfully operated in an ionospheric flow simulation facility and the resulting plasma potential is in excellent agreement with the traditional Langmuir analysis (1.22 volts).
Small plasma probe using tungsten wire collector in tubular shield
Annotated bibliography on two plasma probe techniques using plasma resonance probe, and Langmuir probe
Small plasma probes with guard rings and thermocouples
Laboratory work dealing with the frequency characteristic of the plasma impedance of spherical and cylindrical electrode systems is reported. The influence of the ion sheath on various features of the impedance characteristic is emphasized. Those features are the series and parallel resonance as well as additional resonances due to the excitation of electroacoustic and cyclotron harmonic waves. The dependence of the series and parallel resonances on dc biasing leads to a method of determining the ion sheath capacity for a cylindrical electrode system. The obtained values agree fairly well with those obtained from a theoretical model for the density and potential distribution in the sheath of a cylindrical sensor aligned with a supersonic plasma flow. The amplitude of resonances due to excitation of longitudinal plasma waves (electroacoustic and cyclotron harmonic) is reduced or even vanishes for sufficiently negative dc bias. Positive bias first leads to an increased amplitude up to a certain dc bias value above which, however, the amplitude decreases again due to electron absorption at the sensor surface.
Physical description, module fabrication, sensor construction and calibration details of plasma probe carried on Mariner IV
Plasma proton probe instrumentation of explorer x, giving essential features enabling it to measure arrival direction and energy distribution of photons
Magnetospheric plasma probe results with Pioneer 6 and 7, discussing plasma fluctuations and solar wind interaction with geomagnetic field
Mathematical model of arc Pioneer 6/7 plasma probe electrostatic analyzer responding to monoenergetic unidirectional charged particle beam
Explorer XIV plasma probe observations during October 7, 1962 geomagnetic disturbance
Boundary correction factors for three coil conductivity/velocity plasma probe
Integral electron flux and current in retarding- potential plasma probes, considering application to nonconcave geometry and spacecraft probes
Low energy proton detector instrumentation as plasma probe on explorer x
Plasma resonance probe to determine some properties of plasma environment
Boundary corrections for coaxial three coil conductivity/velocity plasma probe
Plasma probe for Pioneer spacecraft to measure ion and electron density and angular distribution in space
Development of a radio-frequency sheath model for a spherical probe in a collisionless plasma. The method of solution is based on the quasi-static approximation and the electrostatic probe theory of Bernstein and Rabinowitz (1959). The resistive part of the admittance is ascribed to the sheath transit-time collisionless dissipation mechanism suggested by Mayer (1963) and developed by Gould (1964). Expressions are obtained for the effective sheath thickness and the equivalent resistance of the transit-time dissipation. The sheath model and, hence, the admittance are completely determined in terms of the bias potential, the probe radius, the plasma frequency, and the Debye length - i.e., there are no adjustable parameters in the proposed theory which are to be determined by experiment. The results obtained agree favorably with Cohen and Bekefi's (1971) experimental data on the conductance resonant frequency and the width of the conductance peak.