
Here $I=\frac{m l^{2}}{3}+\frac{m l^{2}}{3}=\frac{2 m g l^{2}}{3}$
From figure: $\sin 45^{\circ}=\frac{L}{l / 2}$
$\therefore \mathrm{L}=\frac{l}{2 \sqrt{2}}$
$\therefore \quad \mathrm{T}=2 \pi \sqrt{\frac{2 \mathrm{m} l^{2}}{3 \times \frac{l}{2 \sqrt{2}} \mathrm{mg}}}=2 \pi \sqrt{\frac{2 \sqrt{2} l}{3 \mathrm{g}}}$
$1.$ If the total energy of the particle is $E$, it will perform periodic motion only if
$(A)$ $E$ $<0$ $(B)$ $E$ $>0$ $(C)$ $\mathrm{V}_0 > \mathrm{E}>0$ $(D)$ $E > V_0$
$2.$ For periodic motion of small amplitude $\mathrm{A}$, the time period $\mathrm{T}$ of this particle is proportional to
$(A)$ $\mathrm{A} \sqrt{\frac{\mathrm{m}}{\alpha}}$ $(B)$ $\frac{1}{\mathrm{~A}} \sqrt{\frac{\mathrm{m}}{\alpha}}$ $(C)$ $\mathrm{A} \sqrt{\frac{\alpha}{\mathrm{m}}}$ $(D)$ $\mathrm{A} \sqrt{\frac{\alpha}{\mathrm{m}}}$
$3.$ The acceleration of this particle for $|\mathrm{x}|>\mathrm{X}_0$ is
$(A)$ proportional to $\mathrm{V}_0$
$(B)$ proportional to $\frac{\mathrm{V}_0}{\mathrm{mX}_0}$
$(C)$ proportional to $\sqrt{\frac{\mathrm{V}_0}{\mathrm{mX}_0}}$
$(D)$ zero
Give the answer qustion $1,2$ and $3.$



$y_1 = \sin \left( {\omega t + \frac{\pi }{3}} \right)$ and $y_2 = \sin \omega t$ is :