We are given a rectangular loop with current \( I = 10 \, {A} \) and dimensions of \( 25 \, {cm} \) and \( 10 \, {cm} \), placed parallel to a long straight conductor carrying a current \( I_{{wire}} = 25 \, {A} \), with the loop placed at a distance of \( d = 10 \, {cm} \) from the wire. The formula for the magnetic force on a current-carrying conductor due to a magnetic field is given by: \[ F = I L B \] where \( L \) is the length of the conductor and \( B \) is the magnetic field produced by the wire.
Step 1: The magnetic field at a distance \( r \) from a long straight conductor carrying a current \( I_{{wire}} \) is given by Ampere's law: \[ B = \frac{\mu_0 I_{{wire}}}{2 \pi r} \] where \( \mu_0 = 4\pi \times 10^{-7} \, {T} \cdot {m/A} \) is the permeability of free space. For the given problem, the distance from the wire is \( r = 10 \, {cm} = 0.1 \, {m} \), and the current in the wire is \( I_{{wire}} = 25 \, {A} \). Substituting the values into the formula for the magnetic field: \[ B = \frac{(4\pi \times 10^{-7}) \times 25}{2 \pi \times 0.1} = \frac{10^{-7} \times 25}{0.1} = 2.5 \times 10^{-6} \, {T}. \]
Step 2: Now, the force on the side of the loop of length \( L = 0.25 \, {m} \) (longer side of the rectangle) carrying current \( I = 10 \, {A} \) is: \[ F = I L B = 10 \times 0.25 \times 2.5 \times 10^{-6} = 6.25 \times 10^{-5} \, {N}. \] Thus, the net force on the loop is \( 6.25 \times 10^{-5} \, {N} \).
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