To solve the problem of deriving the force on the wire in a uniform magnetic field, we use the formula for magnetic force on a segment of a current-carrying wire which is given by the equation: F = IBLsinθ, where I is the current, B is the magnetic field, L is the length of the wire, and θ is the angle between the wire and the magnetic field. In this scenario, the magnetic field is perpendicular to the wire, so sinθ = 1. The wire is bent in an arc of circle combined with two straight sections.
Therefore, the total length L of the wire is:
\(L = 2R + πR\)
Thus, the total force on the wire is:
\(F = IB(2R + πR)\)
The direction of the force is determined using the right-hand rule, considering the convention that the magnetic field emerges out from the plane, leading to a force directed vertically downward. Hence, the solution to the problem is \(BI(2R + πR)\), vertically downward.