NASA Scientific and Technical Aerospace Reports
NASA Scientific and Technical Aerospace Reports
NASA Scientific and Technical Aerospace Reports
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distribute across the spacecraft <strong>and</strong> how rapidly charge imbalance will dissipate. To underst<strong>and</strong> these processes requires<br />
knowledge of how charge is deposited within the insulator, the mechanisms for charge trapping <strong>and</strong> charge transport within<br />
the insulator, <strong>and</strong> how the profile of trapped charge affects the transport <strong>and</strong> emission of charges from insulators. One must<br />
consider generation of mobile electrons <strong>and</strong> holes, their trapping, thermal de-trapping, mobility <strong>and</strong> recombination.<br />
Conductivity is more appropriately measured for spacecraft charging applications as the ‘decay’ of charge deposited on the<br />
surface of an insulator, rather than by flow of current across two electrodes around the sample. We have found that<br />
conductivity determined from charge storage decay methods is 102 to 104 smaller than values obtained from classical ASTM<br />
<strong>and</strong> IEC methods for a variety of thin film insulating samples. For typical spacecraft charging conditions, classical<br />
conductivity predicts decay times on the order of minutes to hours (less than typical orbit periods); however, the higher charge<br />
storage conductivities predict decay times on the order of weeks to months leading to accumulation of charge with subsequent<br />
orbits. We found experimental evidence that penetration profiles of radiation <strong>and</strong> light are exceedingly important, <strong>and</strong> that<br />
internal electric fields due to charge profiles <strong>and</strong> high-field conduction by trapped electrons must be considered for space<br />
applications. We have also studied whether the decay constants depend on incident voltage <strong>and</strong> flux or on internal charge<br />
distributions <strong>and</strong> electric fields; light-activated discharge of surface charge to distinguish among differing charge trapping<br />
centers; <strong>and</strong> radiation-induced conductivity. Our experiments also show that ‘Malter’ electron emission occurs for hours after<br />
turning off the electron beam. This Malter emission similar to emission due to negative electron affinity in semiconductors is<br />
a result of the prior radiation or optical excitations of valence electrons <strong>and</strong> their slow drift among traps towards the surface<br />
where they are subsequently emitted. This work is supported through funding from the <strong>NASA</strong> Space Environments <strong>and</strong> Effects<br />
Program.<br />
Author<br />
Charge Transfer; Dissipation; Insulators; Conduction Electrons; Spacecraft Charging<br />
20040111091 QinetiQ Ltd., Farnborough, UK<br />
ECSS-E-20-06 Draft St<strong>and</strong>ard on Spacecraft Charging: Environment-Induced Effects on the Electrostatic Behaviour<br />
of Space Systems<br />
Rodgers, D. J.; Hilgers, A.; 8th Spacecraft Charging Technology Conference; March 2004; 12 pp.; In English; See also<br />
20040111031; No Copyright; Avail: CASI; A03, Hardcopy<br />
ECSS (European Cooperation on Spacecraft St<strong>and</strong>ardisation) is an initiative to develop a coherent, single set of<br />
user-friendly st<strong>and</strong>ards for use in all European space activities. One part of this initiative has covered environment-induced<br />
effects on the electrostatic behaviour of space systems, including spacecraft charging. This has resulted in a draft st<strong>and</strong>ard,<br />
ECSS-E-20-06, that describes the performance <strong>and</strong> verification requirements needed to control these effects. Contributions to<br />
the st<strong>and</strong>ard have come from European governmental agencies, the European Space Agency <strong>and</strong> industry. Before adoption,<br />
the st<strong>and</strong>ard will be subject to wider circulation <strong>and</strong> amendment as a result of feed-back. This draft st<strong>and</strong>ard attempts to bring<br />
together good practice <strong>and</strong> de facto st<strong>and</strong>ards, from a wide range of sources, into a single reference document. In addition,<br />
it provides an explanation of the main physical processes of spacecraft electrical interactions <strong>and</strong> their effects, covering sheath<br />
effects, wakes, tethers, electric propulsion, internal <strong>and</strong> surface charging, <strong>and</strong> discharges <strong>and</strong> transients. Requirements are<br />
given for surface materials, solar arrays, internal materials, tethers <strong>and</strong> electric propulsion systems. Finally, useful information<br />
is provided into ways of carrying out the required tests <strong>and</strong> simulations.<br />
Author<br />
St<strong>and</strong>ardization; Electrostatics; Spacecraft Charging; Propulsion System Performance; Electric Propulsion; <strong>Aerospace</strong><br />
Systems<br />
20040111096 Air Force Research Lab., Hanscom AFB, MA, USA<br />
Onset of Spacecraft Charging in Single <strong>and</strong> Double Maxwellian Plasmas in Space: A Pedagogical Review<br />
Lai, Shu T.; 8th Spacecraft Charging Technology Conference; March 2004; 12 pp.; In English; See also 20040111031; No<br />
Copyright; Avail: CASI; A03, Hardcopy<br />
This paper reviews some recent advances in the onset of spacecraft charging. Current balance determines the spacecraft<br />
potential. The electron flux intercepted by an object in a plasma exceeds that of ions by orders of magnitude because of the<br />
ion-electron mass difference. Negative voltage charging occurs when the incoming electron flux exceeds the outgoing<br />
secondary <strong>and</strong> backscattered electron flux. The secondary electron emission coefficient depends on the surface material,<br />
typically exceeds unity at about 40 to 1800 eV of primary electron energy, <strong>and</strong> falls below unity at higher energies. Beyond<br />
a critical temperature T*, the incoming electron flux exceeds that of the secondary electrons, thereby negative charging occurs.<br />
Scarce evidence of T* was observed on ATS-5 <strong>and</strong> ATS-6 satellites. Recently, abundant evidence was observed on the Los<br />
Alamos National Laboratory geosynchronous satellites. The existence of T* enables accurate prediction of spacecraft charging<br />
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