(d) $Bqv = \frac{mv^{2}}{r}\ \Rightarrow r = \frac{mv}{Bq}\ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ldots(i)$
Since particle was initially at rest and gained a velocity $v$ due to a potential difference of $V$ volt. So,
KE of particle $= \frac{1}{2}\ mv^{2} = qV$
$v = \sqrt{\frac{2qV}{m}}\ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ldots(ii)$
From Eqs. (i) and (ii), we get
$r = \frac{m}{Bq}\sqrt{\frac{2qV}{m}}$
$r = \frac{1}{B}\sqrt{\frac{2mV}{q}}$
$\therefore$ Diameter of the circular path
$d = 2r = \frac{2}{B}\sqrt{\frac{2mV}{q}}$