
(c) Terminal velocity of the rod is attained when magnetic force on the rod $(Bil)$ balances the component of weight of the rod$(mg\sin{\theta)},\ figure$.
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$ie\ ,\ \ Bil = mg\sin\theta$
$B\left( \frac{e}{R} \right)l = mg\sin\theta$
$\frac{Bl}{R}(e) = \ mg\sin\theta$
$\frac{Bl}{R}\left( Blv_{r} \right) = mg\sin\theta$
$r_{T} = \ \frac{mg\ R\sin\theta}{B^{2}l^{2}}$