To determine the rate at which kinetic energy is being imparted to the water, we start by considering the kinetic energy of a small element of water as it leaves the nozzle. The mass of water ejected per unit time is given by:
\( \dot{m} = khv \)
where \( k \) is the mass per unit length and \( v \) is the velocity of water. The kinetic energy \( KE \) of a small element of mass per unit time moving with velocity \( v \) is given by:
\( KE = \frac{1}{2} \dot{m} v^2 \)
Substituting the expression for \( \dot{m} \):
\( KE = \frac{1}{2} (kv)v^2 = \frac{1}{2} kv^3 \)
Since the water is being continuously pumped, the rate at which kinetic energy is imparted is simply twice this expression:
\( \text{Rate of KE} = kv^3 \)
Thus, the power required (or the rate of kinetic energy imparted) by the engine to pump the water is given by the correct option:
\( 2kv^2 \)
Two simple pendulums having lengths $l_{1}$ and $l_{2}$ with negligible string mass undergo angular displacements $\theta_{1}$ and $\theta_{2}$, from their mean positions, respectively. If the angular accelerations of both pendulums are same, then which expression is correct?
In the system shown below, $x(t)=\sin(t)u(t)$. In steady-state, the response $y(t)$ will be 
The time constant of the network shown in the figure is 
The parallel RLC circuit shown in the figure is in resonance. In this circuit, 