Continuum Electric Probes

  • Paul M. Chung
  • Lawrence Talbot
  • Kenell J. Touryan
Part of the Applied Physics and Engineering book series (APPLIED PHYS, volume 11)

Abstract

The effects of collisions in the sheath formed around an electrostatic probe were discussed in some detail in Chapter II. In this chapter, we will study continuum electrostatic probes, which represent the limit of “many collisions” within the sheath. As outlined in Chapter I, one can identify two regimes of continuum probe operation and one hybrid case, depending on the relative magnitude of the smallest mean free path λ and the Debye length λD. They are
  1. (a)

    L ≫ λD ≫ λ: collisional thin sheath

     
  2. (b)

    λD ≫ L ≫ λ: collisional thick sheath

     
  3. (c)

    L ≫ λ ≫ λD: collisionless thin sheath (hybrid dense case)

     

Here L is a characteristic length of the plasma retion affected by the particular continuum probe, which will be defined more precisely in the course of subsequend discussions. When the Probe consists of an entire body immersed in the plasma, which is the case we shall be mostly dealing with, then L is the characteristic dimension of the body. However, when the probe consists of an element embedded in the surface of a larger body, both the characteristic length of the body and the probe enter the problem. Also, the above thin-sheath criteria (a) and (c) are based on the premise that |χ p | = O(1) at most. As will be discussed subsequently, χ p must be included in more general definitions of thin and thick sheath criteria.

Keywords

Microwave Convection Enthalpy Argon Recombination 

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Copyright information

© Springer-Verlag New York Inc. 1975

Authors and Affiliations

  • Paul M. Chung
    • 1
  • Lawrence Talbot
    • 2
  • Kenell J. Touryan
    • 3
  1. 1.University of ChicagoUSA
  2. 2.University of CaliforniaBerkeleyUSA
  3. 3.Sandia LaboratoriesAlbuquerqueUSA

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