Step 1: Understanding the Question:
A vehicle with a mass of $m$ is travelling down a straight road at an initial speed $u$. Over a continuous time frame $t$, it accelerates until its final speed becomes exactly double its initial value ($2u$). We need to determine the average mechanical power output delivered by the engine during this process.
Step 2: Key Formula or Approach:
1. According to the Work-Energy Theorem, the total net work done ($W$) on an object equals its change in kinetic energy ($\Delta K.E.$):
$$W = K.E._f - K.E._i = \frac{1}{2}mv_f^2 - \frac{1}{2}mv_i^2$$
2. Average power ($P$) is defined as the total mechanical work completed divided by the time interval taken:
$$P = \frac{W}{t}$$
Step 3: Detailed Explanation:
Let's define the initial and final velocity conditions:
Initial velocity, $v_i = u$
Final velocity, $v_f = 2u$
Calculate the initial kinetic energy of the car:
$$K.E._i = \frac{1}{2}mu^2$$
Calculate the final kinetic energy after doubling its speed:
$$K.E._f = \frac{1}{2}m(2u)^2 = \frac{1}{2}m(4u^2) = 2mu^2$$
Now, determine the total work done ($W$) using the work-energy relation:
$$W = K.E._f - K.E._i = 2mu^2 - \frac{1}{2}mu^2 = \frac{3}{2}mu^2$$
To find the average power delivered by the engine over the duration $t$, divide this work expression by time:
$$P = \frac{W}{t} = \frac{\frac{3}{2}mu^2}{t} = \frac{3mu^2}{2t}$$
Step 4: Final Answer:
The power delivered by the engine is $\frac{3mu^2}{2t}$, which matches option (A).