(c) $L = 2\pi R$
$\therefore\ \ R = \frac{L}{2\pi}$
$2T\sin{(d\theta) = F_{m}}$
[image:4_image104.emf]
For small angles, $\sin{(d\theta) \approx d\theta}$
$\therefore\ \ \ \ \ \ \ \ \ \ \ \ 2T(d\theta) = I\ (dL)B\sin{90{^\circ}}$
$\ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ = I\ (2R\ .d\theta).B$
⦁ $\therefore\ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ T = IRB = \frac{ILB}{2\pi}$