2009
DOI: 10.1134/s0018151x09020011
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The new screening characteristics of strongly non-ideal and dusty plasmas. Part 3: Properties and applications

Abstract: The physical sense and the properties of a group screening parameters which are determined in the previous papers (Part 1 and Part 2) for single-and two-component systems is discussed in this paper. On the base of data from the mentioned papers are determined two new characteristic lengths which complete a new hierarchy system of screening lengths in plasma. It was shown that the methods developed in Part 1 and Part 2 generates results which are applicable to the strongly non-ideal gaseous and dusty plasmas, a… Show more

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Cited by 6 publications
(14 citation statements)
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“…In the subsequent considerations, several characteristic lengths are used that are connected with the parameters N 1,2,e and Z 1,2 , namely, the Wigner-Seit's (WS) radii and the "ion self-spheres" radii (see [3]), denoted here by r 1,2,e and r s;1,2 , respectively. These are defined by the relations…”
Section: The Initial System and Basic Characteristicmentioning
confidence: 99%
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“…In the subsequent considerations, several characteristic lengths are used that are connected with the parameters N 1,2,e and Z 1,2 , namely, the Wigner-Seit's (WS) radii and the "ion self-spheres" radii (see [3]), denoted here by r 1,2,e and r s;1,2 , respectively. These are defined by the relations…”
Section: The Initial System and Basic Characteristicmentioning
confidence: 99%
“…where x = κ e r e , r κ;e ≡ 1/κ e , and the coefficients γ s;e (x) and γ κ;e (x) are connected with the electron non-ideality parameters Γ e = e 2 /(kT e r e ) and γ e = e 2 /(kT e r κ;e ) as described in [3].…”
Section: Determination Of the Parametersmentioning
confidence: 99%
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