(a) Magnifying power of a telescope having objective of focal length ($f_{0}$) and image distance $(u_{e})$ is
$M = - \frac{f_{0}}{u_{e}}$
To see with relaxed eye final image should be formed at infinity.
The distance between the objective and eyepiece is so adjusted the image is formed at the focus of the eyepiece.
Substituting $v_{e} = f_{e},$ we get
$|M| = \frac{f_{0}}{f_{e}} = \frac{F_{1}}{F_{2}}$