2000
DOI: 10.1063/1.873863
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Energy loss of a test charge in partially ionized dusty plasmas

Abstract: The energy loss of a test charge particle in an unmagnetized dusty plasma is estimated, by incorporating the dust–neutral collisions. A slowly damping large amplitude wake field is observed which moves ahead of the test charge position for large dust–neutral collision frequencies. A critical test charge velocity is determined for a particular dust–neutral collision frequency below which the test charge gains energy instead of losing. The collisions enhance the energy loss only for the test charge velocities gr… Show more

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Cited by 21 publications
(8 citation statements)
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“…where λ g =0.182 is a constant, Z, A and ρ are the atomic number, atomic mass and density of the material, respectively, and E 0 is the EB energy [26,27]. The stopping power is important in dusty plasmas for evaluating the deceleration of a fast test charge crossing a plasma crystal, such as an ion, a projectile or an assembly of projectiles with mass comparable with that of the MPs [28][29][30][31]. The range R CSDA of an electron as it continuously slows down to rest in the material is obtained from the relation ( ) Ar -10 7 g cm −3 .…”
Section: Eb Stopping-power and Rangementioning
confidence: 99%
“…where λ g =0.182 is a constant, Z, A and ρ are the atomic number, atomic mass and density of the material, respectively, and E 0 is the EB energy [26,27]. The stopping power is important in dusty plasmas for evaluating the deceleration of a fast test charge crossing a plasma crystal, such as an ion, a projectile or an assembly of projectiles with mass comparable with that of the MPs [28][29][30][31]. The range R CSDA of an electron as it continuously slows down to rest in the material is obtained from the relation ( ) Ar -10 7 g cm −3 .…”
Section: Eb Stopping-power and Rangementioning
confidence: 99%
“…In the present discussion, however, we shall consider only the equilibrium charge state, ignoring its £uctuations. The latter e¡ect has been discussed earlier by the authors [18,19]. During the charging process, the dust particles pile up charge as more and more electrons are attached to them.…”
Section: E¡ect Of the Dust Charge Statementioning
confidence: 67%
“…Later they also found that the dust charge £uctuation enhances the energy loss of a test charge in a dusty plasma when the charge relaxation rate is very high and vice versa [17,18]. The energy loss of a test charge was also investigated [19] in a partially ionized dusty plasma and it was found that a slow test charge gains energy and can thus accelerate up to the thermal speed of the ambient plasma. There is, however, a need to investigate collisional e¡ects on the electrostatic (ES) potential as well as on the energy loss of the test charge particles as they propagate through a multi-component dusty plasma having di¡erent dust parameters such as dust-charge state, dust-number density, dust-charge £uctuations and dust-neutral collisions.…”
Section: Introductionmentioning
confidence: 97%
“…Stenflo et al 13 incorporated electron-neutral collisions using Bhatnagar-Gross-Krook ͑BGK͒ model and studied its effects on the electrostatic potential of a slowly moving test charge. Since the dust grain charges are not constant, Nasim et al 14,15 investigated the effects of dust charge fluctuations and the dust-neutral collisions on the electrostatic potential and the energy loss due to a single projectile both analytically and numerically. Recently, Shukla and Stenflo 16 calculated the potential for a slowly moving test charge in a positive dust-electron plasma incorporating the charge fluctuation and the collisional effects.…”
Section: Introductionmentioning
confidence: 99%