An engine pumps water continuously through a hose water leares the hose with a velocity \(\mathrm{V}\) and \(\mathrm{m}\) is the mass per unit length of the water Jet what is the rate at which kinetic energy is imparted to water. (A) \((1 / 2) \mathrm{mV}^{3}\) (B) \(\mathrm{mV}^{3}\) (C) \((1 / 2) \mathrm{mV}^{2}\) (D) \((1 / 2) \mathrm{mV}^{\alpha} \mathrm{V}^{2}\)

Short Answer

Expert verified
The short answer is: The rate at which kinetic energy is imparted to water is \((1/2) mV^{3}\), where m is the mass per unit length of the water jet and V is the velocity.

Step by step solution

01

1. Recalling kinetic energy formula

The formula for kinetic energy (K) is given by: \[K = \frac{1}{2}mv^2\] Where m is the mass and v is the velocity. Since the question mentioned mass per unit length, we can modify the equation as follows: Let m' be the mass per unit length and L be the length of water segment inside the hose. Then, the total mass m of the water segment is: \[m = mL\]
02

2. Calculate the kinetic energy of the water segment

Substitute the expression for mass m in the kinetic energy formula: \[K = \frac{1}{2}(m'L)(V^2)\]
03

3. Calculate the rate of kinetic energy transfer

We are interested in finding the rate of change of kinetic energy with respect to time. To do this, we will differentiate the kinetic energy K with respect to time t. The first step is to differentiate the length L with respect to time t. From the problem's information, we know that the water jet moves at velocity V. As a result, the length of the water segment L changes with time (t) at the same rate. Therefore, the rate of change of length L with respect to time t is equal to the velocity V: \[\frac{dL}{dt} = V\] Now, we differentiate K with respect to time: \[\frac{dK}{dt} = \frac{1}{2}\left(\frac{d(m'LV^2)}{dt}\right)\] Here, m' is a constant, so we just need to differentiate the product (LV^2) with respect to time using the product rule: \[\frac{dK}{dt} = \frac{1}{2}\left(m' \left(\frac{dL}{dt}V^2 + L\frac{d(V^2)}{dt}\right)\right)\] Now, substitute the value of \(\frac{dL}{dt}\) into the equation: \[\frac{dK}{dt} = \frac{1}{2}\left(m' \left(VV^2 + L\frac{d(V^2)}{dt}\right)\right)\] Since the velocity V is constant, the derivative \(\frac{d(V^2)}{dt}\) is equal to zero. Therefore, the equation simplifies to: \[\frac{dK}{dt} = \frac{1}{2}m'V^3\] Comparing this result with the given options, we can see that the correct answer is: (A) \((1 / 2) \mathrm{mV}^{3}\)

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