In a Cassegrain telescope, the primary mirror is a concave mirror and the secondary mirror is a convex mirror.
Object is at infinity, so the primary (concave) mirror forms an image at its focus.
For the primary mirror: Radius of curvature $R_1 = -25$ cm (concave).
Focal length $f_1 = R_1/2 = -12.5$ cm.
The image $I_1$ is formed at the focus, 12.5 cm from the primary mirror.
This image $I_1$ acts as a virtual object for the secondary (convex) mirror.
The distance between the mirrors is $d=2.5$ cm.
The object distance for the secondary mirror ($u_2$) is the distance from the secondary mirror to $I_1$.
The secondary mirror is between the primary mirror and its focus.
$u_2 = f_1 - d = 12.5 - 2.5 = 10$ cm. (The object is virtual, so $u_2$ is positive).
For the secondary mirror: Radius of curvature $R_2 = +16$ cm (convex).
Focal length $f_2 = R_2/2 = +8$ cm.
Now, we use the mirror formula for the secondary mirror to find the final image position ($v_2$).
$\frac{1}{v_2} + \frac{1}{u_2} = \frac{1}{f_2}$.
$\frac{1}{v_2} + \frac{1}{10} = \frac{1}{8}$.
$\frac{1}{v_2} = \frac{1}{8} - \frac{1}{10} = \frac{5-4}{40} = \frac{1}{40}$.
$v_2 = 40$ cm.
Since $v_2$ is positive, the final image is formed 40 cm to the right of the secondary (convex) mirror.