1968
DOI: 10.1088/0032-1028/10/7/304
|View full text |Cite
|
Sign up to set email alerts
|

Inverse third power law for the shielding of test particles

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1
1

Citation Types

4
65
0

Year Published

1970
1970
2020
2020

Publication Types

Select...
6
2
1

Relationship

0
9

Authors

Journals

citations
Cited by 110 publications
(69 citation statements)
references
References 3 publications
4
65
0
Order By: Relevance
“…I have not attempted a complete literature search, but note that the research project must have been topical at the time as the inverse third power asymptotic behaviour in Eq. (3.8) was announced a year later by Montgomery, Joyce and Sugihara, 32 in a paper that has been cited 58 times. In fact the problem is even more topical today with the rise of interest in dusty plasmas-for instance the paper by Ishihara and Vladimirov 33 on the wake potential of a dust grain in a plasma with ion flow has been cited more than 80 times.…”
Section: Resultsmentioning
confidence: 99%
“…I have not attempted a complete literature search, but note that the research project must have been topical at the time as the inverse third power asymptotic behaviour in Eq. (3.8) was announced a year later by Montgomery, Joyce and Sugihara, 32 in a paper that has been cited 58 times. In fact the problem is even more topical today with the rise of interest in dusty plasmas-for instance the paper by Ishihara and Vladimirov 33 on the wake potential of a dust grain in a plasma with ion flow has been cited more than 80 times.…”
Section: Resultsmentioning
confidence: 99%
“…MONTGOMERY et al (1968) have shown for an electron plasma that for a moving test particle, the far field is not exponentially decreasing as in Debye screening, but rather exhibits a'quadrupole field in lowest significant order.…”
Section: \ IV the Far Field Test Particle Potentialmentioning
confidence: 99%
“…Far field wake potential decays as the inverse cube of the distance between the origin of the test charge and the location of the observer. It is interesting to note that for far field, the effective potential of a moving "test charge" in an isotropic collision-less classical plasma also falls off as the inverse cube of the distance of the observer from the test charge [31]. The effect of far field wake potential is very small on the binding energy of atom.…”
Section: Introductionmentioning
confidence: 99%