To solve this problem, we need to understand how constant power delivered by a machine affects the distance moved by a body over time.
When a machine delivers constant power \( P \) to a moving body, power is defined as:
P = \frac{dW}{dt}
where \( W \) is the work done. Work done \( W \) is also given by the product of force \( F \) and distance \( s \), so:
W = F \cdot s
Using the definition of power:
P = F \cdot v
where \( v \) is the velocity. Rearranging gives us:
v = \frac{P}{F}
Newton’s second law relates force to acceleration as:
F = m \cdot a
Thus, we can express velocity \( v \) as:
v = \frac{P}{m \cdot a}
At constant power, the kinetic energy \( KE \) is proportional to work done:
\frac{1}{2}mv^2 = P \cdot t
Rearranging gives:
v^2 = \frac{2P \cdot t}{m}
This means:
v \propto \sqrt{t}
Velocity is also defined as the rate of change of distance over time:
v = \frac{ds}{dt}
Substituting \( v \propto \sqrt{t} \) into the equation gives:
\frac{ds}{dt} \propto \sqrt{t}
Integrating both sides with respect to time \( t \), we get:
s \propto \int \sqrt{t} \, dt \propto t^{3/2}
Therefore, the distance moved by the body in time \( t \) is proportional to t^{3/2}.
The correct answer is t^{3/2}.