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Debye sheath : ウィキペディア英語版
Debye sheath
The Debye sheath (also electrostatic sheath) is a layer in a plasma which has a greater density of positive ions, and hence an overall excess positive charge, that balances an opposite negative charge on the surface of a material with which it is in contact. The thickness of such a layer is several Debye lengths thick, a value whose size depends on various characteristics of plasma (e.g. temperature, density, etc.).
A Debye sheath arises in a plasma because the electrons usually have a temperature on the order of magnitude or greater than that of the ions and are much lighter. Consequently, they are faster than the ions by at least a factor of \sqrt}. At the interface to a material surface, therefore, the electrons will fly out of the plasma, charging the surface negative relative to the bulk plasma. Due to Debye shielding, the scale length of the transition region will be the Debye length \lambda_\mathrm. As the potential increases, more and more electrons are reflected by the sheath potential. An equilibrium is finally reached when the potential difference is a few times the electron temperature.
The Debye sheath is the transition from a plasma to a solid surface. Similar physics is involved between two plasma regions that have different characteristics; the transition between these regions is known as a double layer, and features one positive, and one negative layer.
==Description==

Sheaths were first described by American physicist Irving Langmuir. In 1923 he wrote:
:"Electrons are repelled from the negative electrode while positive ions are drawn towards it. Around each negative electrode there is thus a ''sheath'' of definite thickness containing only positive ions and neutral atoms. () Electrons are reflected from the outside surface of the sheath while all ''positive'' ions which reach the sheath are attracted to the electrode. () it follows directly that no change occurs in the positive ion current reaching the electrode. The electrode is in fact perfectly screened from the discharge by the positive ion sheath, and its potential cannot influence the phenomena occurring in the arc, nor the current flowing to the electrode."〔Langmuir, Irving, "(Positive Ion Currents from the Positive Column of Mercury Arcs )" (1923) ''Science'', Volume 58, Issue 1502, pp. 290-291〕
Langmuir and co-author Albert W. Hull further described a sheath formed in a thermionic valve:
:"Figure 1 shows graphically the condition that exists in such a tube containing mercury vapor. The space between filament and plate is filled with a mixture of electrons and positive ions, in nearly equal numbers, to which has been given the name "plasma". A wire immersed in the plasma, at zero potential with respect to it, will absorb every ion and electron that strikes it. Since the electrons move about 600 times as fast as the ions, 600 times as many electrons will strike the wire as ions. If the wire is insulated it must assume such a negative potential that it receives equal numbers of electrons and ions, that is, such a potential that it repels all but 1 in 600 of the electrons headed for it."
:"Suppose that this wire, which we may take to be part of a grid, is made still more negative with a view to controlling the current through the tube. It will now repel all the electrons headed for it, but will receive all the positive ions that fly toward it. There will thus be a region around the wire which contains positive ions and no electrons, as shown diagrammatically in Fig. 1. The ions are accelerated as they approach the negative wire, and there will exist a potential gradient in this sheath, as we may call it, of positive ions, such that the potential is less and less negative as we recede from the wire, and at a certain distance is equal to the potential of the plasma. This distance we define as the boundary of the sheath. Beyond this distance there is no effect due to the potential of the wire."〔Albert W. Hull and Irving Langmuir, "(Control of an Arc Discharge by Means of a Grid )", ''Proc Natl Acad Sci'' U S A. 1929 March 15; 15(3): 218–225〕

抄文引用元・出典: フリー百科事典『 ウィキペディア(Wikipedia)
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