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SPORE Mission Design - Georgia Tech SSDL - Georgia Institute of ...

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⃗⃗⃗ [ ̇ ̇ ̇ ] (29)<br />

⃗ ⃗ (30)<br />

Inertial Fixed<br />

As seen in Equation 31 and 32, rotate the inertial coordinate system by angle α to transform velocity and<br />

position into a fixed coordinate system. The following method was used for PESST to find the<br />

atmospheric relative position and velocity.<br />

⃗⃗⃗⃗ [ ] ( ⃗⃗⃗ ̂ ⃗⃗⃗⃗ ) (31)<br />

⃗⃗⃗⃗ [ ] ⃗⃗⃗⃗ (32)<br />

The angle α is given by the following equation.<br />

Here α 0 is the initial angle between the inertial and fixed x-axes (at time t 0 ), Ω E is the rotation <strong>of</strong> the<br />

earth in degrees per second (~0.0042), and t is the amount <strong>of</strong> time elapsed in seconds since t 0 . For a<br />

start time <strong>of</strong> 9 Feb 2011 17:00:00.000 UTCG as specified in the STK model, α 0 is equal to 34.294°. The<br />

above transformation does not take into account the effects <strong>of</strong> precession and nutation. Therefore it is<br />

not equivalent to the STK transformation.<br />

Fixed Inertial<br />

Use the transpose <strong>of</strong> the rotation matrix given in Equation 32 to transfer between fixed and inertial<br />

axes. These relations are given in Equation 33 and 34.<br />

(16)<br />

⃗⃗⃗⃗ [ ] ⃗⃗⃗⃗ (33)<br />

⃗⃗⃗ [ ] ( ⃗⃗⃗⃗ ̂ ⃗⃗⃗⃗ ) (34)<br />

The transformation in Equation 33 and 34 does not take into account the effects <strong>of</strong> precession and<br />

nutation. Therefore it is not equivalent to the STK transformation.<br />

4.2 Baseline Orbital Trajectories<br />

The LEO and GTO trajectories can be found in Table 6, Table 7, and

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