Mass $${m_1}$$ strikes $${m_2}$$ which is at rest. The ratio of masses for which they will collide again (collision between ball and wall are elastic, coefficient of restitution between $${m_1}$$ and $${m_2}$$ is $$e$$ and all the surfaces are smooth.)
A.
$$ < \frac{e}{{2 + e}}$$
B.
$$ > \frac{{2e}}{{2 + e}}$$
C.
$$ \geqslant \frac{e}{{2\left( {2 + e} \right)}}$$
A particle of mass $$m$$ is moving in a circular path of constant radius $$r$$ such that its centripetal acceleration $${a_c}$$ is varying with time $$t$$ as $${a_c} = {k^2}r{t^2}$$ where $$k$$ is a constant. The power delivered to the particles by the force acting on it is:
A.
$$2\pi m{k^2}{r^2}t$$
B.
$$m{k^2}{r^2}t$$
C.
$$\frac{{\left( {m{k^4}{r^2}{t^5}} \right)}}{3}$$
A spring of force-constant $$k$$ is cut into two pieces such that one piece is double the length of the other. Then the long piece will have a force-constant of-