Question
A small block oscillates back and forth on a smooth concave surface of radius R figure. Find the time period of small oscillation.



$\therefore$ Acceleration $\text{a}=\text{g}\theta$
Let ‘x’ be the displacement from the mean position of the body,$\therefore\theta=\frac{\text{x}}{\text{R}}$
$\Rightarrow\text{a}=\text{g}\theta=\text{g}\Big(\frac{\text{x}}{\text{R}}\Big)\Rightarrow\Big(\frac{\text{a}}{\text{x}}\Big)=\Big(\frac{\text{g}}{\text{R}}\Big)$
So the body makes S.H.M.$\therefore\text{T}=2\pi\sqrt{\frac{\text{Displacement}}{\text{Acceleration}}}=2\pi\sqrt{\frac{\text{x}}{\frac{\text{gx}}{\text{R}}}}=2\pi\sqrt{\frac{\text{R}}{\text{g}}}$

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| wavelength (nm) | 350 | 400 | 450 | 500 | 550 |
| stopping potential(V): | 1.45 | 1.00 | 0.66 | 0.38 | 0.16 |
Plot the stopping potential against inverse of wavelength
$\big(\frac{1}{\lambda}\big) $ on a graph paper and find$\text{mg}$
$\frac{\text{mg}}{\cos\theta}$
$\text{mg}\cos\theta$
$\text{mg}\tan\theta$

