Study on Principle of Spacecraft Surface Charge and Discharge

Abstract:

Spacecraft surface charge and discharge is an important reason for the failure of the spacecraft in the space environment. This paper introduces the principle of spacecraft surface charging and discharging , from the spacecraft surface charging discharging phenomenon found to the harm of charge and discharge, elaborated the spacecraft surface charging protection method.

• Periodical: Advanced Materials Research (Volumes 765-767)
• Pages: 217-221
• DOI: https://doi.org/10.4028/www.scientific.net/AMR.765-767.217
• Online since: September 2013
• Authors: Pei Zhang, Qing Yun Yuan, Bin Xu
• Keywords: Protection, Spacecraft, Surface Charging

References

[1] Ervin Beloni and Edward L. Dreizin. Ignition of Different Size Al Particles in a Powder Bed by Electro-Static Discharge (ESD) Stimulation. 45th AIAA, (2009).

DOI: 10.2514/6.2009-5079

[2] M. J. Mandell, V. A. Davist and B. M. Gardner. Charge Control of Geosynchronous Spacecraft Using Field Effect Emitters. 45th AIAA, (2007).

DOI: 10.2514/6.2007-284

[3] Hirokazu Masui, Tomoki Kitamura, Teppei Okumura. Laboratory Test Campaign for ISO Standardization of Solar Array ESD Test Methods. 45th AIAA, (2007).

DOI: 10.2514/6.2007-277

[4] G.B. Hillard and D.C. Ferguson. LEO Spacecraft Charging Design Guidelines: A Proposed NASA Standard . IEEE Trans on Magn. 42nd AIAA, (2004).

DOI: 10.2514/6.2004-1259

[5] Dale C. Ferguson. New NASA See LEO Spacecrafe Charging design Guidelines – How to survive in LEO Rather than GEO.

[6] Orjubin G, Richalot E, Mengue S, et al. On the FEM modal approach for a reverberation chamber analysis[J]. IEEE Trans Electromagn Compat, 2007, 49(1): 76-85.

DOI: 10.1109/temc.2006.888187

[7] Lerosey G, Rosny J. Scattering cross section measurement in reverberation chamber[J]. IEEE Trans Electromagn Compat, 2007, 49(2): 280-284.

DOI: 10.1109/temc.2007.893332

[8] Zhao H P, Shen Z X. Efficient modeling of three-dimensional reverberation chambers using hybrid discrete singular convolution-method of moments[J]. IEEE Transactions on Antennas and Propagation, 2011, 59(8): 2943-2953.

DOI: 10.1109/tap.2011.2158966

[9] Xiao K, Pommerenke D J, Drewniak J L. A three-dimensional FDTD subgridding algorithm with separated temporal and spatial interfaces and related stability analysis[J]. IEEE Transactions on Antennas and Propagation, 2007, 55(7): 1981-(1990).

DOI: 10.1109/tap.2007.900180

[10] Orjubin G, Petit F, Richalot E, et al. Cavity losses modeling using lossless FDTD method[J]. IEEE Transactions on Electromagnetic Compatibility, 2006, 48(2): 429-431.

DOI: 10.1109/temc.2006.873854

[11] Waldschmidt G, Taflove A. Three-dimensional cad-based mesh generator for the dey–mittra conformal FDTD algorithm[J]. IEEE Transactions on Antennas and Propagation, 2004, 52(7): 1658-1664.

DOI: 10.1109/tap.2004.831334

[12] Sypek P, Dziekonski A, Mrozowski M. How to render FDTD computations more effective using a graphics accelerator [J]. IEEE Transactions on Magnetics, 2009, 45(3): 1324-1327.

DOI: 10.1109/tmag.2009.2012614

[13] Teixeira F L. Time-domain finite-difference and finite-element methods for maxwell equations in complex media[J]. IEEE Trans Antennas Propag, 2008, 55(8): 2150-2166.

DOI: 10.1109/tap.2008.926767

[14] Waldschmidt G, Taflove A. Three-dimensional cad-based mesh generator for the dey–mittra conformal FDTD algorithm[J]. IEEE Transactions on Antennas and Propagation, 2004, 52(7): 1658-1664.

DOI: 10.1109/tap.2004.831334

[15] Orjubin G, Petit F, Richalot E, et al. Cavity losses modeling using lossless FDTD method[J]. IEEE Transactions on Electromagnetic Compatibility, 2006, 48(2): 429-431.

DOI: 10.1109/temc.2006.873854

[16] Kobidze G. Implementation of collocated surface impedance boundary conditions in FDTD[J]. IEEE Transactions on Antennas and Propagation, 2010, 57(7): 2394-2403.

DOI: 10.1109/tap.2010.2048859

[17] Clegg J, Marvin A C, Dawson J F, et al. Optimization of stirrer designs in a reverberation chamber[J]. IEEE Transactions on Electromagnetic Compatibility, 2005, 47(4): 824-832.

DOI: 10.1109/temc.2005.860561