1958
DOI: 10.1063/1.1724371
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Plasma Motions Induced by Satellites in the Ionosphere

Abstract: The electrohydrodynamic phenomena associated with the high-velocity motion of a charged body in a plasma are investigated with a view to applications to satellite motion in the ionosphere. It is shown that the effect of the electric field due to the charge on the body in inducing collective motion leads to similar results both for high- and low-density gases. By using a linearized theory, formulas are obtained for the electrohydrodynamic drag and for the increased ionization in the Mach cone behind the body.

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Cited by 59 publications
(16 citation statements)
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“…Plasma flowing past a spacecraft will create a wake downstream of this obstacle, as has been studied from the beginning of the space age (e.g., Kraus andWatson 1958, Rand 1960). However, most earlier wake studies are not directly applicable to the case of a positively charged spacecraft in a low-density supersonic polar wind.…”
Section: The Solutionmentioning
confidence: 99%
“…Plasma flowing past a spacecraft will create a wake downstream of this obstacle, as has been studied from the beginning of the space age (e.g., Kraus andWatson 1958, Rand 1960). However, most earlier wake studies are not directly applicable to the case of a positively charged spacecraft in a low-density supersonic polar wind.…”
Section: The Solutionmentioning
confidence: 99%
“…We do not however restrict ourselves to a one-component plasma. In connection with the field around a small satellite, considered by Kraus and Watson,22 it is necessary to consider the ions since the satellite velocity is comparable more with the ion velocity than the electron velocity. In this plasma there are two modes of longitudinal excitation, namely, ion acoustic waves and electron plasma waves, but if the test particle is much slower than the electron thermal velocity then only the ion waves can be excited-the case considered by the above authors.…”
mentioning
confidence: 99%
“…We note that the term J(u)6 (r) in Equation (3,10), which was deduced from simple considerations, is in fact identical with the corresponding term in Equation (2,59) which was obtained as a result of a Fourier transformation with a rigorous limiting procedure corresponding to q ~ 0. It must, of course, be remembered that in Equation (2,58) the magnetic field H has been set equal to zero.…”
Section: (U -Vo) + [Un] + = J (U)~ (R)mentioning
confidence: 96%
“…,~r ou lw~c ~foU~ (3,10) where the condition Ofo/eU = -(Mifo/kT)u has been allowed for. We note that the term J(u)6 (r) in Equation (3,10), which was deduced from simple considerations, is in fact identical with the corresponding term in Equation (2,59) which was obtained as a result of a Fourier transformation with a rigorous limiting procedure corresponding to q ~ 0.…”
Section: (U -Vo) + [Un] + = J (U)~ (R)mentioning
confidence: 99%