In this problem, the crate is not accelerating vertically. The forces acting in a vertical direction are the normal force and the weight of the crate.
Also, the angle between the pushing force (F) and the direction of motion is zero.
Given data:
The mass of the crate is\(m = 46\;{\rm{kg}}\).
The height is\(h = 10.3\;{\rm{m}}\).
The coefficient of friction is\({\mu _k} = 0.5\).
The free body diagram of the crate is as follows:

The relation of force in the y-direction is given as:
\(\begin{array}\Sigma {F_{\rm{y}}} &= 0\\N - W &= 0\\N &= W &= mg\end{array}\)
The relation between the forces in the x-direction is given by:
\(\begin{array}\Sigma {F_{\rm{x}}} &= 0\\F - {F_{\rm{f}}} &= 0\\F &= {F_{\rm{f}}}\\F &= {\mu _k}mg\end{array}\)
Here, F is the pushing force, g is the gravitational acceleration, and \({F_{\rm{f}}}\) is the frictional force.