The magnetic moment \( \mu \) of a current loop is \( \mu = I A \), where \( I \) is the current and \( A \) is the loop's area. The magnetic field \( B \) at the center of a circular loop of radius \( r \) due to current \( I \) is \( B = \frac{\mu_0 I}{2r} \). Rearranging for \( I \), we get \( I = \frac{2r B}{\mu_0} \). Substituting this into the magnetic moment equation gives \( \mu = \left( \frac{2r B}{\mu_0} \right) A \). Since \( A = \pi r^2 \), we have \( r = \sqrt{\frac{A}{\pi}} \). Substituting this radius into the equation yields \( \mu = \frac{2B A}{\mu_0} \sqrt{\frac{A}{\pi}} \). Therefore, the magnetic moment of the loop is \( \mu = \frac{2BA}{\mu_0} \sqrt{\frac{A}{\pi}} \).
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 ________. (\( \mu_0 = 4\pi \times 10^{-7}\,\text{T m A}^{-1} \)) 