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<doi>10.3850/S2010428611000043</doi>
<article-title>Deorbiting Dynamics of Electrodynamic Tether</article-title>
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<author>Z. H. Zhu<sup>a</sup> and Rui Zhong<sup>b</sup> </author>
<author-citation>Zhu, Z. H.; Zhong, Rui</author-citation>

<aff>Department of Earth and Space Science and Engineering, York University 4700 Keele Street, Toronto,
Ontario M3J 1P3, Canada.  </aff>

<email><a href="mailto:gzhu@yorku.ca   "><sup>a</sup>gzhu@yorku.ca   </a></email>

<email><a href="mailto:rzhong@yorku.ca   "><sup>b</sup>rzhong@yorku.ca  </a></email>

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<title>ABSTRACT</title>
<p>This paper studies satellite deorbit using electrodynamic tether (EDT)
propulsion. Gaussian perturbation equations are used to model the orbital
dynamics of EDT with environmental perturbations of electrodynamic force,
aerodynamic drag and the effect of Earth&#8217;s oblateness. Differential
equations for the induced voltage-current across EDT are derived and solved
with boundary conditions determined by mission objectives and hardware
devices. A simplified analytical method for solving the equations is
proposed to improve computational efficiency. Simulations find that the
orbit of a satellite deorbited by EDT will become elliptical in near polar
orbits due to the higher-order perturbation of Earth&#8217;s magnetic field. This
is beneficial for the near polar orbits where the electrodynamic force is
less effective, because the atmosphere at a lower perigee will provide
larger air drag to dissipate the orbital kinetic energy of satellite faster.
Moreover, we proved that the polarity reverse of the induced voltage/current
across EDT in near polar orbits does not affect the kinetic energy
dissipation by the current induced Lorentz force. Compared the decay by air
drag only, the orbit decaying time of a satellite with EDT will be reduced
by three and two orders of magnitudes in the equatorial and polar orbits
respectively.  </p><p><italic>Keywords: </italic>Electrtodynamic tether, Deorbit, Dynamics, Tethered satellite, Magnetic field.   </p>
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