Let rp and ra be the distances of the satellite from the centre of the Earth at perigee and apogee, respectively. Let vp and va be its linear (tangential) velocities at perigee and apogee.
Data : rp = 2R + R = 3R, va = \(\frac14 V_p\)
Let Lp and La be the angular momenta of the satellite about the Earth’s centre. Because the gravitational force (\(\vec F\)) on the satellite due to the Earth is always radially towards the centre of the Earth, its direction is opposite to that of the position vector (\(\vec r\)) of the satellite relative to the centre of the Earth, so that the torque \(\vec \tau\) = \(\vec r\)x \(\vec F\) = 0 . Hence, the angular momentum of the satellite about the Earth’s centre is constant in time.
\(\therefore\) Lp = La
If m is mass of the matellite,
At apogee, the distance of the satellite from the Earth’s surface is 12R – R = 11R.