(c) The emf developed between the ends of the conductor
$\ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ e = \frac{1}{2}B\lambda^{2}\omega$
$\ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ = \frac{1}{2} \times 0.2 \times 10^{- 4} \times (1)^{2} \times 5 = 50\mu V$