(c) Let $p$ be the atmospheric pressure, $\rho$ the density of the liquid and $v$ the velocity of the efflux of the liquid coming out from the orifice.
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From Bernoulli’s theorem,
$p + 0 + \rho gH = p + \frac{1}{2}\rho v^{2} + \rho g(H - h)$
$\Longrightarrow \ \ \frac{1}{2}\rho v = \rho gh$
$\Longrightarrow \ v =$ $\sqrt{2gh}$