
To solve this problem, we will use the concept of magnetic force between two parallel current-carrying wires. According to Ampère's force law, the force per unit length \( F/L \) between two parallel wires carrying currents \( I_1 \) and \( I_2 \) and separated by a distance \( d \) is given by the formula:
F/L = \frac{μ_0 I_1 I_2}{2\pi d}
In this problem, we have three parallel wires carrying the same current \( I \) in the same direction. Let us label the wires as \( A \), \( B \), and \( C \), with wire \( B \) being the middle one.
We must find the net force per unit length on wire \( B \). The forces from both wire \( A \) and wire \( C \) are in opposite directions, hence:
The net force is the vector sum of these forces. Since they are in opposite directions, the total force will be:
F_{\text{net}}/L = 2 \times \frac{μ_0 I^2}{2\pi d} \cos 45^\circ
Given that \(\cos 45^\circ = \frac{1}{\sqrt{2}}\):
F_{\text{net}}/L = 2 \times \frac{μ_0 I^2}{2\pi d} \times \frac{1}{\sqrt{2}} = \frac{μ_0 I^2}{\sqrt{2}\pi d}
Therefore, the magnitude of force per unit length on the middle wire \( B \) is given by:
\(\frac{μ_0 I^2}{\sqrt{2} \pi d}\)