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Precise Orbit Determination of Global Navigation Satellite System of ...

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Chapter 5 Perturbation Models <strong>of</strong> IGSO,GEO and MEO <strong>Satellite</strong>s <strong>Orbit</strong>s<br />

5.2 The Solar and Lunar Attractions<br />

Due to the great distance between the Earth and the Sun and between the Earth and Moon, it is unnecessary to<br />

take the nospherical part <strong>of</strong> the Sun and Moon into account. For this reason, in the perturbation models the Sun<br />

and Moon are considered as point mass. The solar and lunar attractions on the satellite may be expressed in the<br />

inertial coordinate system as follows<br />

(Kovalevsky 1967, Beutler 1996)<br />

�<br />

=<br />

� �<br />

2 ϖ<br />

�<br />

ϖ ϖ ϖ<br />

d r µ ϖ<br />

r − �<br />

i r ri<br />

= − r + µ i � −<br />

2 3<br />

ϖ ϖ<br />

(5-23)<br />

3 3<br />

dt r i s,<br />

m ��<br />

| ri<br />

− r | ri<br />

�<br />

where<br />

ϖ<br />

r<br />

ϖ<br />

rs ϖ<br />

rm position vector <strong>of</strong> satellite<br />

position vector <strong>of</strong> Sun<br />

position vector <strong>of</strong> Moon<br />

µ , µ s, µ m gravity constants <strong>of</strong> the Earth, Sun and Moon respectively.<br />

In order to evaluate the influences <strong>of</strong> Sun and Moon on IGSO, GEO and MEO satellites, the accelerations<br />

produced by the solar and lunar attractions on IGSO and GEO satellites are computed using JPL Planetary<br />

Ephemeris DE200 and Eq.(5-23). The quantities <strong>of</strong> the accelerations and orbit errors by these two perturbation<br />

forces are listed in Table 5-6, Table 5-7 and Table 5-8 as well as are drawn in Figures 5-24, 5-25, 5-26 and 5-27.<br />

Table 5-6 The Effect <strong>of</strong> Solar and Lunar Attraction on IGSO <strong>Satellite</strong><br />

(<strong>Satellite</strong> Parameters: a=42164.174km, λ=20°, i=63°)<br />

Perturbation Force Acceleration <strong>Orbit</strong> Errors (m)<br />

(m/sec 2 ) One Day Ten Days<br />

Solar Attraction 3×10 -6 945 8915<br />

Lunar Attraction 6×10 -6 2590 77 (km)<br />

Table 5-7 The Effect <strong>of</strong> Solar and Lunar Attraction on GEO <strong>Satellite</strong><br />

(<strong>Satellite</strong> Parameters: a=42164.174km, λ=20°, i=0°)<br />

Perturbation Force Acceleration <strong>Orbit</strong> Errors (m)<br />

(m/sec 2 ) One Day Ten Days<br />

Solar Attraction 3×10 -6 2263 23183<br />

Lunar Attraction 6×10 -6 2311 14 (km)<br />

Table 5-8 The Effect <strong>of</strong> Solar and Lunar Attraction on MEO (GPS) <strong>Satellite</strong>*<br />

Perturbation Force Acceleration <strong>Orbit</strong> Errors (m)<br />

(m/sec 2 ) One Day Ten Days<br />

Solar Attraction 2×10 -6 800 3500<br />

Lunar Attraction 5×10 -6 3000 8000<br />

*Feltens, 1991; Landau, 1988<br />

56

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