2011
DOI: 10.21236/ada542582
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Plasma Interactions with Spacecraft. Volume 2, NASCAP-2K Scientific Documentation for Version 4.1

Abstract: Public reporting burden for this collection of information is estimated to average 1 hour per response, including the time for reviewing instructions, searching existing data sources, gathering and maintaining the data needed, and completing and reviewing this collection of information. Send comments regarding this burden estimate or any other aspect of this collection of information, including suggestions for reducing this burden to Department of Defense, Washington Headquarters Services, Directorate for Info… Show more

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Cited by 3 publications
(4 citation statements)
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“…Backscattering occurs when an electron is reflected from the spacecraft rather than absorbed. This analysis uses the model for energy‐dependent backscattering provided in Davis and Mandell (): η(E)=()H(1E)H(E0.05)log()E0.05log(20)+H(E1)×()eE/510+1(2/e)0.037Z where E is the landing energy in keV, H ( x ) is the Heaviside step function, and Z is the atomic number of the material (aluminum in this analysis). The formulas above can be added to produce the total yield Y ( E ) = η ( E ) + δ ( E ) for normally incident monoenergitic electrons.…”
Section: Spacecraft Chargingmentioning
confidence: 99%
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“…Backscattering occurs when an electron is reflected from the spacecraft rather than absorbed. This analysis uses the model for energy‐dependent backscattering provided in Davis and Mandell (): η(E)=()H(1E)H(E0.05)log()E0.05log(20)+H(E1)×()eE/510+1(2/e)0.037Z where E is the landing energy in keV, H ( x ) is the Heaviside step function, and Z is the atomic number of the material (aluminum in this analysis). The formulas above can be added to produce the total yield Y ( E ) = η ( E ) + δ ( E ) for normally incident monoenergitic electrons.…”
Section: Spacecraft Chargingmentioning
confidence: 99%
“…However, since the ion current is usually much smaller than the electron current, ion‐induced SEE is neglected in many cases. In this analysis the two parameter Nascap‐2k model Davis and Mandell () is used δ(E)=βE1/21+E/EM where E is the energy in keV and for aluminum β = 1.36 and E M = 40 are fitting parameters.…”
Section: Spacecraft Chargingmentioning
confidence: 99%
“…We computed the sheath structure and ion collection using a hybrid PIC approach with PIC ions and fluid barometric electron densities [1]. The plasma response, collected ion currents, and chassis floating potential were computed self-consistently with a 1 kV near-square-wave bias applied to the antenna elements.…”
Section: Dsx Antenna Impedance From Nascap-2k Calculations-first Estimentioning
confidence: 99%
“…We used the results of these calculations to calculate the current flowing along the antenna elements, the electron current density throughout the surrounding volume, and the vector potential field [1]. One of the results of the pseudopotential algorithm used to compute the current flowing along each antenna element is the injected current.…”
Section: Dsx Antenna Impedance From Nascap-2k Calculations-first Estimentioning
confidence: 99%