To solve the problem, we first relate power, kinetic energy, and displacement. The power \( P \) imparted to the body results in kinetic energy \( E \) given by:
\( E = \frac{1}{2}mv^2 \)
Since the body starts from rest, the work done in time \( t \) is equal to the kinetic energy, and for constant power:
\( P \times t = \frac{1}{2}mv^2 \)
Rearranging for velocity \( v \), we have:
\( v = \sqrt{\frac{2Pt}{m}} \)
The displacement \( s \) under constant acceleration is given by:
\( s = \int v \, dt = \int \sqrt{\frac{2Pt}{m}} \, dt \)
To find this, evaluate:
\( s = \frac{1}{3} \sqrt{\frac{2P}{m}} \, t^{3/2} \bigg|_{0}^{4} \)
Substituting values \( m = 2 \, kg \), \( t = 4 \, s \), and equating to the given expression for displacement:
\( \frac{1}{3} \alpha^2 \sqrt{P} = \frac{1}{3} \sqrt{\frac{2P}{2}} \times 4^{3/2} \)
Simplify:
\( \alpha^2 \sqrt{P} = \sqrt{P} \times 8 \)
Equating coefficients of \(\sqrt{P}\):
\( \alpha^2 = 8 \)
Solving for \(\alpha\):
\( \alpha = \sqrt{8} = 2\sqrt{2} \approx 4 \)
Verify that \(\alpha\) (\(\approx 4\)) is within the given range (4, 4). Conclude the solution, \(\alpha = 4\), is valid.