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3.4 Perburbed Satellite Motion
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III. Satellite Orbital Motion
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3.2 Elliptic motion of
It can be show than only 6 of the 8 motion integrals obtained are
independent.
The motion integrals are usually expressed in terms of the orbital
elements,
defined as:
- Argument of the ascending node ( ): angle between the
X-axis and the direction of the ascending node, i.e. the point where
the
satellite cross the XY-plane (equator) with Z-velocity component
positive.
- Orbit inclination (i): is the angle between the
orbit plane
and the XY-plane defined as the angle between the angular momentum and the
Z-unitary vector .
- Perigee argument ( ): angle between the perigee and the
ascending node direction, extended on the orbital plane.
- Eccentricity (e).
- Perigee pass epoch ( ).
- Major semiaxis (a).
From equations 2,4 and 5:
and
From the orbital elements is posible to compute the position and
velocity
of the satellite in any epoch t:
- The mean anomaly is computed.
- By means of the Kepler equation 10 we estimate (iteratively)
the mean anomaly E:
- Now, with equations 7, 8, we get the geocentric
satellite distance and the true anomaly, r and :
- From the polar coordinates in the orbit plane, we have to
perform
several rotations to get the coordinates in the equatorial reference
frame:
- Z-rotation of angle
- X-rotation of angle -i (following the new X axis)
- Z-rotation of angle (following the new Z axis)
To get finally:
Manuel Hernandez Pajares
Thu Jun 4 14:25:37 GMT 1998