44th AIAA Aerospace Sciences Meeting and Exhibit 2006
DOI: 10.2514/6.2006-865
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Analysis of ISS Plasma Interaction

Abstract: In this paper we shall present the interaction mechanisms between the ISS and the surrounding plasma and give an overview of the PIM components. PIM predictions are compared with available data followed by a discussion of the variability of plasma parameters and the conductive area on the ISS.

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Cited by 4 publications
(4 citation statements)
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“…Magnetic induction charging (V ISS x B· L) has been previously reported [Ferguson et al, 2001Mikatarian et al,2004;Ferguson, 2004;Reddell et al, 2006]. Eclipse exit has also been recognized as an area where charging is likely to be maximized Reddell et al, 2006] and this is seen in our normal eclipse charging as well as in data previously obtained on the ISS by the Glenn Research Center Floating Potential Probe in 2001 [Ferguson et al 2001;. Three apparently new categories can be added based on this survey: equatorial, high latitude night-time, and rapid eclipse exit charging.…”
Section: Discussionmentioning
confidence: 99%
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“…Magnetic induction charging (V ISS x B· L) has been previously reported [Ferguson et al, 2001Mikatarian et al,2004;Ferguson, 2004;Reddell et al, 2006]. Eclipse exit has also been recognized as an area where charging is likely to be maximized Reddell et al, 2006] and this is seen in our normal eclipse charging as well as in data previously obtained on the ISS by the Glenn Research Center Floating Potential Probe in 2001 [Ferguson et al 2001;. Three apparently new categories can be added based on this survey: equatorial, high latitude night-time, and rapid eclipse exit charging.…”
Section: Discussionmentioning
confidence: 99%
“…Magnetic induction charging shows a sinusoidal-like character. This is a well explained behavior of spacecraft potentials [Whipple, 1981;Mikatarian et., 2004;Ferguson, 2004;Reddell et al, 2006], is always present throughout the ISS orbit, and is dependent on the velocity of the ISS, the earth's magnetic field, and the position of the FPMU on the truss through the relation V ISS xB·L, where V ISS is the ISS velocity, B is the local magnetic field strength, and L is a position vector to the FPMU. With the ISS in +XVV attitude, the potential at the FPMU location is largest at the higher northern latitudes and smallest at the higher southern latitudes where the high V ISS xB·L potential is on the end of the truss opposite the position of the FPMU.…”
Section: Magnetic Inductionmentioning
confidence: 99%
“…(2019) and Reddell et al. (2006), from the solar wind by Eriksson et al. (2006, 2007), and from the polar lobes by Engwall, Eriksson, Cully, André, Puhl‐Quinn, et al.…”
Section: Wakes In Different Situationsmentioning
confidence: 99%
“…Relevant parameters for LEO (sounding rockets and the International Space Station) are given by Paulsson et al (2019) and Reddell et al (2006), from the solar wind by Eriksson et al (2006Eriksson et al ( , 2007, and from the polar lobes by Engwall, Eriksson, Cully, André, Puhl-Quinn, et al (2009), André et al (2015), and Haaland et al (2017). Sketches of corresponding wakes are given in Figure 1.…”
Section: Wake In the Solar Wind (Narrow Wake)mentioning
confidence: 99%