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Mission Design for the CubeSat OUFTI-1

Mission Design for the CubeSat OUFTI-1

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CHAPTER 9.THERMAL-CONTROL SYSTEM9.3.3 Hot and cold caseWe are dealing with a simplified model: we are not expecting to have a detailed<strong>the</strong>rmal description of our <strong>CubeSat</strong>. The goal of this preliminary study is toidentify <strong>the</strong> maximum and minimum temperatures reached during lifetime inorder to avoid <strong>the</strong> overpass of <strong>the</strong> imposed limits.We identify <strong>the</strong>re<strong>for</strong>e three possible cases:• <strong>the</strong> hot case: <strong>the</strong> satellite is in sunlight and <strong>the</strong> solar arrays do not produceany power but only cumulate solar heat flux. The solar flux is injected ona face and <strong>the</strong> absorption coefficient is α 0 as <strong>the</strong> efficiency is null.• <strong>the</strong> operating case: <strong>the</strong> satellite is in sunlight and <strong>the</strong> solar arrays areproviding <strong>the</strong> necessary power. The payload is on and we need to radiate0.5 W corresponding to <strong>the</strong> losses in <strong>the</strong> communication system convertedinto heat. In this case, <strong>the</strong> absorption factor of solar cells needs to beupdated as a function of <strong>the</strong> solar cell temperature• <strong>the</strong> cold case: <strong>the</strong> satellite is in eclipse and <strong>the</strong> payload is off. In this case<strong>the</strong> solution seems to be trivial: <strong>the</strong> equilibrium temperature is practically<strong>the</strong> T cold but it doesn’t respect <strong>the</strong> reality. Fur<strong>the</strong>rmore in this case <strong>the</strong>hypo<strong>the</strong>sis of steady-state cannot be applied integrally. We added <strong>the</strong>re<strong>for</strong>ea flux of 847W/m2, which is <strong>the</strong> solar flux weighed on <strong>the</strong> averagetime of eclipse.For <strong>the</strong> operating case, we needed to add a worksheet to Thermal-Excel inorder to update <strong>the</strong> solar cells properties as a function <strong>the</strong>ir temperatures.9.4 Thermal results <strong>for</strong> <strong>OUFTI</strong>-1Once decided <strong>the</strong> kind of model to study and identified <strong>the</strong> material properties,we passes to <strong>the</strong> implementation into <strong>the</strong> software Thermal-Excel.As above mentioned, a starting guess temperature is demanded and <strong>for</strong> eachcase we calculated it as explained in section 9.2 respecting <strong>the</strong> characteristicsof each case.At <strong>the</strong> beginning, we had some problems as <strong>the</strong> final results depended on <strong>the</strong>starting temperature, which is impossible <strong>for</strong> <strong>the</strong> static case. With an accuratereflection we find out <strong>the</strong> reason: <strong>the</strong> standard algorithm used by <strong>the</strong> softwarehas a really slow convergence when <strong>the</strong> number of radiative exchange is importantrespect to <strong>the</strong> conductive. As <strong>the</strong> criterion of convergence is <strong>the</strong> differencebetween successive temperatures, <strong>the</strong> software thought to have converged evenif it was not true. We needed <strong>the</strong>re<strong>for</strong>e to strongly reduce <strong>the</strong> convergence criterionin order to have <strong>the</strong> good solution.Galli Stefania 93 University of Liège

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