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Next: 3.3 Orbital elements Up: III. Satellite Orbital Motion Previous: 3.1 Two-Body Problem

3.2 Elliptic motion of the satellite

We are going to express the temporal dependence of the satellite motion in the orbit.


The parametric equation of the ellipse referred to one of the focus can be written as:

 

being E the eccentric anomaly (see figure), a major semiaxis,

 

and b the minor semiaxis .

The distance of the satellite to the Earth center from equation 3.2 is:

 

and dividing both components also from equation 3.2:

 

And the angular momentum can be written as:

 

Taking into account that if n is the mean angular velocity of the satellite along one orbit and h/2 is the constant area velocity:

 

And from the last two relationships the Kepler equation is obtained

 

being the perigee pass time and n the mean angular velocity:

. The term is known as mean anomaly. Finally, from equations 9 and 6 we can get the third Kepler law:

where T is the orbit period.


Manuel Hernandez Pajares
Thu Jun 4 14:25:37 GMT 1998