(c) When the particle moves along a circle in the magnetic field $B$, the magnetic force is radially inward. If an electric field of proper magnitude is switched on which is directed radially outwards, the particle may experience no force. It will then move along a straight line with uniform velocity. This will be the case when $qE = qvB \Rightarrow E = vB$
Also $r = \frac{mv}{qB} \Rightarrow v = \frac{qBr}{m}$
So $E = \frac{qB^{2}r}{m}$
$= \frac{(10 \times 10^{- 6}) \times (0.1)^{2} \times 10 \times 10^{- 2}}{1 \times 10^{- 3} \times 10^{- 6}} = 10V/m$