We can find the speed \(v\) required for a circular orbit of radius \(r\) from Equation 3-17 for the acceleration in uniform circular motion \(a_{\mathrm{cent}} = v^2/r\). For a satelite of mass \(m\) orbiting Earth, the acceleration is provided by Earth's gravitational force. From Newton's second law, this says
\(F_{\mathrm{Earth\ on\ satelite}} = ma_{\mathrm{cent}}\)
or from Equation 3-17 for uniform circular motion and Equation 10-2 for the law of universal gravitation,
\(\frac{Gm_{\mathrm{Earth}}m}{r^2} = m\frac{v^2}{r}\)
To solve for \(v\), multiply both sides of this equation by \(r/m\)
\(\frac{Gm_{\mathrm{Earth}}}{r} = v^2\)
and take the square root: