2003
DOI: 10.1063/1.1598433
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Shielding of a slowly moving test charge in a dusty plasma with dynamical grain charging

Abstract: The dynamical charging of grains in a dusty plasma enhances the shielding of test charges. Time scales for charging are determined by the ambient plasma parameters and the grain dimensions. They can be very short, approaching the ion plasma period for grain sizes of the order of an electron Debye length. For a slowly moving test charge the response potential is found as a power series in the test charge velocity. Collisional effects are included. Analytical expressions for the response potential, valid for all… Show more

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Cited by 9 publications
(7 citation statements)
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“…If T c <τ in we can argue that the dust charge is at all times derived from local equilibrium conditions in the plasma, while in the opposite case, T c >τ in , there is a "memory" in the system, and the actual charged state of the dust will depend on the preceeding motion through the plasma. Assuming that the dust is moving in a stationary electrostatic field, the forces on a dust grain are generally not conservative when the charged state of a dust grain depends on its path (Raadu and Shafiq, 2003;Shafiq and Raadu, 2004;Zhdanov et al, 2005).…”
Section: Figmentioning
confidence: 99%
“…If T c <τ in we can argue that the dust charge is at all times derived from local equilibrium conditions in the plasma, while in the opposite case, T c >τ in , there is a "memory" in the system, and the actual charged state of the dust will depend on the preceeding motion through the plasma. Assuming that the dust is moving in a stationary electrostatic field, the forces on a dust grain are generally not conservative when the charged state of a dust grain depends on its path (Raadu and Shafiq, 2003;Shafiq and Raadu, 2004;Zhdanov et al, 2005).…”
Section: Figmentioning
confidence: 99%
“…͑42͒ may be shown to reduce to the known results 8,9 for a monosized distribution with a charge relaxation time 0 . ͑43͒-͑45͒ the combination of terms ␣ De / ␦ u0 pi is equal to 1 / 0 ͑␣ −1 ͒ ͓from Eq.…”
Section: ͑49͒mentioning
confidence: 77%
“…[2][3][4][5] The inclusion of a dust component in normal electron-ion plasmas has led to a renewed interest in the test charge response problem. 8,9 The delayed shielding effect due to dynamical charging has also been reported. An important consequence of the potential excited by a moving charge is the energy loss and braking of the velocity due to the resultant electric field at the moving charge.…”
Section: Introductionmentioning
confidence: 92%
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