A small square loop of wire of side $l$ is placed inside a large square loop of wire of side $L (L>>l)$. The loops are co- planar and their centres coincide. The mutual inductance of the system is proportional to |
$\frac{l}{L}$ $\frac{l^2}{L}$ $\frac{L}{l}$ $\frac{L^2}{l}$ |
$\frac{l^2}{L}$ |
The correct answer is Option (2) → $\frac{l^2}{L}$ Given: Small loop of side $l$ inside large loop of side $L$ ($L \gg l$), co-planar, centres coincide. Mutual inductance $M$ is given by: $M = \frac{\text{Flux through small loop due to current in large loop}}{\text{Current in large loop}}$ Magnetic field at the centre of a large square loop carrying current $I$: $B \propto \frac{\mu_0 I}{L}$ Flux through small loop: $\Phi = B \cdot \text{area of small loop} \propto \frac{\mu_0 I}{L} \cdot l^2$ Mutual inductance: $M = \frac{\Phi}{I} \propto \frac{\mu_0 l^2}{L}$ Answer: Mutual inductance $M \propto \frac{l^2}{L}$ |