
The magnetic field at the center of a circular loop with current \(I\) is \(B = \frac{{\mu_0 I}}{{2R}}\). For a semicircular loop, this field is halved: \(B = \frac{{\mu_0 I}}{{4R}}\).
Given two semicircular loops with radii \(R_1 = 2\pi \, m\) and \(R_2 = 4\pi \, m\), the magnetic fields at the center \(O\) are \(B_1 = \frac{{\mu_0 I}}{{4R_1}}\) and \(B_2 = \frac{{\mu_0 I}}{{4R_2}}\).
The net magnetic field is the difference due to opposite directions: \(B_{\text{net}} = B_2 - B_1 = \frac{{\mu_0 I}}{{4R_2}} - \frac{{\mu_0 I}}{{4R_1}} = \frac{{\mu_0 I}}{{4}} \left(\frac{1}{R_2} - \frac{1}{R_1}\right)\).
Substituting \(I = 4A\), \(R_1 = 2\pi \, m\), \(R_2 = 4\pi \, m\), and \(\mu_0 = 4\pi \times 10^{-7} \, T\cdot m/A\):
\(B_{\text{net}} = \frac{{4\pi \times 10^{-7} \times 4}}{4} \left(\frac{1}{4\pi} - \frac{1}{2\pi}\right) = \pi \times 10^{-7} \left(\frac{1-2}{4\pi}\right) = -\pi \times 10^{-7} \times \frac{1}{4\pi} = -\frac{1}{4} \times 10^{-7} \, T\).
Therefore, \(\alpha = 3\), which is within the range of 3,3.
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 ________. (\( \mu_0 = 4\pi \times 10^{-7}\,\text{T m A}^{-1} \)) 