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  • Impact of Solar Array Designs on High Voltage Operation in Space

    Paper number

    IAC-06-C3.1.05

    Author

    Dr. Henry Brandhorst, Auburn University, United States

    Coauthor

    Mr. Mark J. O'Neill, ENTECH, Inc., United States

    Coauthor

    Mr. Michael Piszczor, National Aeronautics and Space Administration (NASA)/Glenn Research Center, United States

    Coauthor

    Dr. Dale C. Ferguson, National Aeronautics and Space Administration (NASA)/Marshall Space Flight Center, United States

    Year

    2006

    Abstract

    As power levels of advanced spacecraft climb above 25 kW, higher solar array operating voltages become attractive. Even in today’s satellites, operating spacecraft buses at 100 V and above has led to arcing in GEO communications satellites, so the issue of spacecraft charging and solar array arcing remains a design problem. In addition, micrometeoroid impacts on all of these arrays can also lead to arcing if the spacecraft is at an elevated potential. For example, tests on space station hardware disclosed arcing at 75V on anodized Al structures that were struck with hypervelocity particles in Low Earth Orbit (LEO) plasmas. Thus an understanding of these effects is necessary to design reliable high voltage solar arrays of the future, especially in light of the Vision for Space Exploration of NASA.

    In the future, large GEO communication satellites, lunar bases, solar electric propulsion missions, high power communication systems around Mars can lead to power levels well above 100 kW. As noted above, it will be essential to increase operating voltages of the solar arrays well above 80 V to keep the mass of cabling needed to carry the high currents to an acceptable level. Thus, the purpose of this paper is to discuss various solar array approaches, to discuss the results of testing them at high voltages, in the presence of simulated space plasma and under hypervelocity impact

    Three different types of arrays will be considered. One will be a planar array using thin film cells, the second will use planar single or multijunction cells and the last will use the Stretched Lens Array (SLA – 8-fold concentration). Each of these has different approaches for protection from the space environment. The thin film cell-based arrays have minimal covering due to their inherent radiation tolerance, conventional GaAs and multijunction cells have the traditional cerium-doped microsheet glasses (of appropriate thickness) that are usually attached with Dow Corning DC 93-500 silicone adhesive. In practice, these cover glasses and adhesive do not cover the cell edges. Finally, in the SLA, the entire cell and cell edges are fully encapsulated by a cover glass that overhangs the cell perimeter and the silicone adhesive covers the cell edges providing a sealed environment.

    These three types of blanket technology have been tested at GRC and Auburn. The results of these tests will be described. For example, 15 modules composed of four state-of-the-art 2x4 cm GaAs solar cells with 150 micrometer thick cover glasses connected in two-cell series strings were tested at high voltage, in plasma under hypervelocity impact. These were prepared by standard industry practice from a major supplier and had efficiencies above 18

    These results will show significant differences in resistance to arcing that are directly related to array design and manufacturing procedures. Finally, the approaches for mitigating the problems uncovered by these tests will be described. These will lay the foundation for future higher voltage array operation, even including voltages above 300-600 V for direct drive SEP applications.

    Abstract document

    IAC-06-C3.1.05.pdf

    Manuscript document

    IAC-06-C3.1.05.pdf (🔒 authorized access only).

    To get the manuscript, please contact IAF Secretariat.