Two masses $m_1$ and $m_2$ connected by a spring of spring constant $k$ rest on a frictionless surface. If the masses are pulled apart and let go, the time period of oscillation is
$T=2 \pi \sqrt{\frac{1}{k}\left(\frac{m_1 m_2}{m_1+m_2}\right)}$
$T=2 \pi \sqrt{k\left(\frac{m_1+m_2}{m_1 m_2}\right)}$
$T=2 \pi \sqrt{\frac{m_1}{k}}$
$T=2 \pi \sqrt{\frac{m_2}{k}}$
Two identical spring of constant $K$ are connected in series and parallel as shown in figure. A mass $m$ is suspended from them. The ratio of their frequencies of vertical oscillations will be
A uniform stick of mass $M$ and length $L$ is pivoted at its centre. Its ends are tied to two springs each of force constant $K$ . In the position shown in figure, the strings are in their natural length. When the stick is displaced through a small angle $\theta $ and released. The stick
A mass $M$ is suspended from a spring of negligible mass. The spring is pulled a little and then released so that the mass executes $S.H.M.$ of time period $T$. If the mass is increased by m, the time period becomes $5T/3$. Then the ratio of $m/M$ is
Force constant of a spring is $K$ . If half part is detached then force constant of the remaining spring will be
Two masses $M_{A}$ and $M_{B}$ are hung from two strings of length $l_{A}$ and $l_{B}$ respectively. They are executing SHM with frequency relation $f_{A}=2 f_{B}$, then relation