Question

A particle of mass m is driven by a machine that delivers a constant power $k$ watts. If the particle starts from rest the force on the particle at time t is

• A. $\sqrt{2mk}{t}^{-1/2}$
• B. $\frac{1}{2}\sqrt{mk}{t}^{-1/2}$
• C. $\sqrt{\frac{mk}{2}}{t}^{-1/2}$
• D. $\sqrt{mk}{t}^{-1/2}$

Answer 1

Answer: (C)

Constant power acting on the particle of mass $m$ is k watt.
or P = k
$\frac{dw}{dt}=k;dw=kdt$
Integrating both sides $\underset{0}{\overset{w}{\int }}dw=\underset{0}{\overset{t}{\int }}kdt$
$\Rightarrow w=kt...(i)$
Using work energy theorem, $W=\frac{1}{2}m{v}^2-\frac{1}{2}m(0{)}^2$
$kt=\frac{1}{2}m{v}^2$ [using equation (i)]
$v=\sqrt{\frac{2kt}{m}}$
Acceleration of the particle, $a=\frac{dv}{dt}$
$a=\frac{1}{2}\sqrt{\frac{2k}{m}}\frac{1}{\sqrt{t}}=\sqrt{\frac{k}{2mt}}$
Force on the particle, $F=ma=\sqrt{\frac{mk}{2r}}=\sqrt{\frac{mk}{2}}{t}^{-1/2}$