One end of a spring of force constant k is fixed to a vertical wall and the other to a block of mass m resting on a smooth horizontal surface. There is another wall at a distance ${x_0}$ from the black. The spring is then compressed by $2{x_0}$ and released. The time taken to strike the wall is
$\frac{1}{6}\pi \sqrt {\frac{k}{m}} $
$\sqrt {\frac{k}{m}} $
$\frac{{2\pi }}{3}\sqrt {\frac{m}{k}} $
$\frac{\pi }{4}\sqrt {\frac{k}{m}} $
The total spring constant of the system as shown in the figure will be
The frequency of oscillation of a mass $m$ suspended by a spring is $v_1$. If length of spring is cut to one third then the same mass oscillates with frequency $v_2$, then
Two springs of force constants $K$ and $2K$ are connected to a mass as shown below. The frequency of oscillation of the mass is
How the period of oscillation depend on the mass of block attached to the end of spring ?
A block is placed on a frictionless horizontal table. The mass of the block is m and springs are attached on either side with force constants ${K_1}$ and ${K_2}$. If the block is displaced a little and left to oscillate, then the angular frequency of oscillation will be