A block is on an inclined plane of angle \(\theta\).
The weight of the block is:
\[
mg.
\]
The component of weight along the inclined plane downward is:
\[
mg\sin\theta.
\]
The normal reaction is:
\[
N=mg\cos\theta.
\]
The frictional force is:
\[
f=\mu N.
\]
Substitute \(N=mg\cos\theta\):
\[
f=\mu mg\cos\theta.
\]
Now, the block is to be moved up the inclined plane.
When the block moves upward, friction acts downward along the plane.
So the applied force must overcome two downward forces:
\[
mg\sin\theta
\]
and
\[
\mu mg\cos\theta.
\]
Therefore, required force is:
\[
F=mg\sin\theta+\mu mg\cos\theta.
\]
Hence, the force required is:
\[
mg\sin\theta+\mu mg\cos\theta.
\]