Orbits & Satellites

01Orbits & Satellites

Circular orbits

This section covers how gravitational force provides the centripetal force needed for a circular orbit.

Gravity as the centripetal force

A planet or satellite moving in a circular orbit is continually accelerating because the direction of its velocity changes.

The gravitational force is directed towards the centre of the body being orbited, so in a circular orbit it provides the required centripetal force.

MmFgvr

For a satellite of mass mm orbiting a body of mass MM at orbital radius rr,

Fg=Fcentripetal.F_g=F_{\text{centripetal}}.

The satellite's velocity is tangential to the orbit while the gravitational force points radially inwards, so the two directions are perpendicular.

Equating the force expressions gives

GMmr2=mv2r.\frac{GMm}{r^2}=\frac{mv^2}{r}.

The orbital radius rr is measured from the centre of the body being orbited. For altitude hh above a planet of radius RR, use r=R+hr=R+h.

Exam Tip: In an explanation of a circular orbit, identify gravitational force as the centripetal force and state that it acts towards the centre of the orbit.

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