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THEORY OF AN ELECTROSTATIC PROBE IN A STRONG MAGNETIC FIELD. PART II

Journal Article · · Physics of Fluids (U.S.)
DOI:https://doi.org/10.1063/1.1706698· OSTI ID:4790989
S>A probe is considered in a magnetic field so strong as to impair collective transverse drifts. In this case, the charges sipplied to the probe come mainly from a long tube of force whose radius is about one Larmor radius larger than the probe. It is assumed that there is acting a diffusion process, more efficient than ordinary drifts, which continuously exchanges particles between the inside of the tube of force and the rest of the plasma. A one- dimensional model of this process, leading to an integro-differential Poisson's equation, is investigated in the case of slow diffusion. The solution consists of a chargeless, slowly decaying potential, which describes the geometrical screening effect of the probe; while in the sheath an approximate boundary-layer solution matches with the probe's potential V/sub p/. The asymptotic relation between the current collected and V/sub p/ is computed. This model may be suited to the case of diffusion caused by random wave fields. (auth)
Research Organization:
Princeton Univ., N.J.
Sponsoring Organization:
USDOE
NSA Number:
NSA-17-000976
OSTI ID:
4790989
Journal Information:
Physics of Fluids (U.S.), Journal Name: Physics of Fluids (U.S.) Vol. Vol: 5; ISSN PFLDA
Country of Publication:
Country unknown/Code not available
Language:
English

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