12.07.2015 Views

Mission Design for the CubeSat OUFTI-1

Mission Design for the CubeSat OUFTI-1

Mission Design for the CubeSat OUFTI-1

SHOW MORE
SHOW LESS

Create successful ePaper yourself

Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.

CHAPTER 8.POWER SYSTEM8.3.2 Elliptic orbit with orbital elements after one yearmission and circular orbitAs in this analysis <strong>the</strong> orbital parameters are supposed to be constant, we wouldlike to have an idea of <strong>the</strong> power available after one year mission, assuming that<strong>the</strong> system will be able to work till that moment. We imposed <strong>the</strong>n <strong>the</strong> orbitalparameters obtained by <strong>the</strong> perturbation study:Table 8.3: Elliptic orbit with orbital parameters after one yearPerigee altitude [Km] 341Apogee altitude [Km] 1036Semi-major axis [Km] 7067Eccentricity 0.0491Right ascension of ascending node ◦ 279Argument of perigee ◦ 128Inclination ◦ 71Starting with those parameters, we have <strong>the</strong> power produces represented infigure 8.7Figure 8.7: Total power and integrated power <strong>for</strong> <strong>the</strong> orbital parameters afterone year missionAs we can see, <strong>the</strong> difference is really small: we can <strong>the</strong>re<strong>for</strong>e assume thatafter one year mission we will still have enough power.The same analysis has been per<strong>for</strong>med <strong>for</strong> <strong>the</strong> circular orbit at 350 Kmaltitude: <strong>the</strong> results are in figure 8.8We find out that <strong>the</strong> total integrated power is lower than in <strong>the</strong> ellipticcase. Even if this lack in power could appear as a main drawback, <strong>the</strong> situationGalli Stefania 81 University of Liège

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!