
The force on a current-carrying wire segment in a uniform magnetic field is calculated using F = IBLsinθ, where I represents current, B is the magnetic field strength, L is the wire length, and θ is the angle between the wire and the field. In this case, the magnetic field is perpendicular to the wire, making sinθ = 1. The wire comprises two straight sections and a semicircular arc.
The total wire length L is the sum of these parts:
\(L = 2R + πR\)
Consequently, the total magnetic force on the wire is:
\(F = IB(2R + πR)\)
The force direction, determined by the right-hand rule with the magnetic field directed out of the plane, is vertically downward. The final answer is therefore \(BI(2R + πR)\), vertically downward.
Three long straight wires carrying current are arranged mutually parallel as shown in the figure. The force experienced by \(15\) cm length of wire \(Q\) is ________. (\( \mu_0 = 4\pi \times 10^{-7}\,\text{T m A}^{-1} \)) 