(b) [image:10_image75.jpeg]
Apply Bernoullis, theorem
$p_{1} + 0\rho gH = p_{2 +}\frac{1}{2}{\rho v}^{2} + \rho gH$
$p_{1} - p_{2} = \frac{1}{2}{\rho v}^{2}$
$3 \times 10^{5} - 1 \times 10^{5} = \frac{1}{2}\rho v^{2}\ \ \ \ \ \ \ \ \ \ \ \ \ \ \ $
$2 \times 10^{5} = \frac{1}{2}\rho v^{2}$
$2 \times 10^{5} = \frac{1}{2} \times 10^{3} \times v^{2}$
$v^{2} = 400$
$v = \sqrt{400}$