1986
DOI: 10.1029/ja091ia05p05719
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The use of electrostatic noise to control high‐voltage differential charging of spacecraft

Abstract: High differential charging is known to occur on geostationary satellites between two electrically isolated pieces of the same material. This happens because current balance with the ambient space environment on each surface can be satisfied by different surface potentials. Three such potentials (two stable and one unstable) are found for the two-Maxwellian plasmas considered in this study and in the absence of photoelectron emission. Thus two isolated surfaces can have significantly different potentials leadin… Show more

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Cited by 5 publications
(3 citation statements)
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“…For gold the root in Figure 12 is negative, and JT(eO = 0) for gold is also negative. No triple-root jump occurs for gold on day 114; this agrees with Hastings [1986], who also made the same remark about gold on day 114. Had we used isotropic instead of normal incidence, the exact jumping point for Cu-Be would be slightly different, but both the triple-root jump behavior of Cu-Be and the "no-jump" behavior of gold would be unchanged.…”
Section: Modeling Boom-satellite Potential Differencesupporting
confidence: 86%
“…For gold the root in Figure 12 is negative, and JT(eO = 0) for gold is also negative. No triple-root jump occurs for gold on day 114; this agrees with Hastings [1986], who also made the same remark about gold on day 114. Had we used isotropic instead of normal incidence, the exact jumping point for Cu-Be would be slightly different, but both the triple-root jump behavior of Cu-Be and the "no-jump" behavior of gold would be unchanged.…”
Section: Modeling Boom-satellite Potential Differencesupporting
confidence: 86%
“…In contrast to the single Maxwellian case, both the temperatures (eq.9J and the densities (eq.11) are the parameters controlling spacecraft charging in the double Maxwellian model environment [4,5,6,7,16,21,23].…”
Section: Stable Unstaelementioning
confidence: 99%
“…For analytic investigation of the charging behavior near the threshold, the potential ϕ is calculated as follows [ Prokopenko and Lamframboise , ; Hastings , ]: Jnormalnnormalenormalt()ϕ=truetrue∑k=12{Jnormalinormalk()0()1+Q}Jnormalenormalk()0normalexp()Q()1<δ+η>k,.5emnormalfnormalonormalr0.55emϕ<0, and leftleftJnetϕ=k=12Jik0expQJek01<η>k1+Qleft+Jek0<δ>kexpeϕkBTs1+eϕkBTs,.5emnormalfnormalonormalr.5emϕ>0. …”
Section: Charging Behavior In Double‐maxwellian Plasmamentioning
confidence: 99%