Satgen317 In Orbit by GM4IHJ 22 April 95 A satellite takes up an orbit appropriate to its orbital velocity and, the mass,of the planet or moon,around which it is travelling. Thereafter, subs quent events depend on the various forces which can perturb the orbit. In the case of a satellite of the Earth, these perturbation agencies will be :- The ATMOSPHERE for any satellite coming below 1000 kms altitude for part or all of its orbit. Drag in the atmosphere slows the satellite down , forcing it to fall to a lower altitude in order to maintain orbital velocity. Drag is variable, being greatest at Solar 11 year cycl maximum when the atmosphere supplemented by material from the Sun is at its densest. Drag also varies spasmodically , when Solar Coronal Mass Eject ons briefly increase the upper atmospheres density, what ever the phase of the Solar sunspot cycle. The EQUATORIAL BULGE of the Earth, which exerts a force on the satellite pulling the plane of its orbit, so that the satellites track with respect to the stars changes gradually with time. The GRAVITATIONAL PULL of the Sun and the Moon, which is particularly noticable on satellites going more that 20000 kms from the earth for part or all of their orbit. This effect is therefore not of great interest in respect of low earth orbit satellites , but it can make a great deal of difference over months to the orbits of both geostationary satellites out at 36000 kms, or Molinya elliptical orbiters like Oscar 13 which go out to 36000 kms or more at the apogee high point of their orbit. In order to predict where a satellite is at any time , we can predict the effect on it of the Earths mass, and measure the parameters of its orbital ellipse at a particular EPOCH time. Then making allowance for the effect of the earths equatorial bulge, we can calculate where it will be at some future time. Provided that is we remenber the problem posed by atmospheric drag, and accept that we will have to measure a full set of new parameters every month or so , if the satellite is at low altitude such as Mir. Or about every 3 months if it is below 1000 kms around solar cycle maximum. For satellites at solar cycle minimum we can stretch the time between providing new orbital parameters to two or three times those given above, but for longer periods new parameters must be measured if we are to avoid errors due to Solar and Lunar gravitational effects on the satellites at higher altitude. For many years now the North American Radar NORAD, has measured and supplied the orbital information for near earth orbit satelcites. With NASA being the public contact point for distribution of this data, which we call Keplerian Elements. Satgens over the next few weeks will discuss thele elements and their usage , together with a look at the very different orbital data and methods of calculation which we must use for objects outside the Earths gravitational sphere of influence , such as the Sun, Moon, Planets , Comets and Deep Space craft.