(b) Bernoulli’s theorem for unit mass of liquid
$\frac{P}{\rho} + \frac{1}{2}v^{2}\ constant$
As the liquid starts flowing , it pressure energy decreases
$\frac{1}{2}v^{2} = \frac{P_{1} - P_{2}}{\rho}$
$\Longrightarrow \ \ \ \ \frac{1}{2}v^{2} = \frac{3.5 \times 10^{5} - 3 \times 10^{5}}{10^{3}}$
$\Longrightarrow \ \ v^{2} = \frac{2 \times 0.5 \times 10^{5}}{10^{3}}$
$\Longrightarrow v^{2} = 100$
$\Longrightarrow v = 10\ {ms}^{- 1}$