A mass m = 50g is dropped on a vertical spring of spring constant 500N/m from a height h = 10cm as shown in figure. The mass sticks to the spring and executes simple harmonic oscillations after that. A concave mirror of focal length 12cm facing the mass is fixed with its principal axis coinciding with the line of motion of the mass, its pole being at a distance of 30cm from the free end of the spring. Find the length in which the image of the mass oscillates.
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Due to weight of the body suppose the spring is compressed by which is the mean position of oscillation.
$m = 50 \times 10^{-3}kg, g = 10ms^{-2}, k = 500Nm^{-2}, h = 10cm = 0.1m$
For equilibrium, $\text{mg}=\text{kx}\Rightarrow\text{x}=\frac{\text{mg}}{\text{k}}=10^{-3}\text{m}=0.1\text{cm}$
So, the mean position is at 30 + 0.1 = 30.1cm from P (mirror).
Suppose, maximum compression in spring is $\delta.$
Since, E.K.E. - I.K.E. = Work done
$\Rightarrow0-0=\text{mg}(\text{h}+\delta)-\frac{1}{2}\text{k}\delta^2$ (work energy principle)
$\Rightarrow\text{mg}(\text{h}+\delta)-\frac{1}{2}\text{k}\delta^2\Rightarrow50\times10^{-3}\times10(0.1+\delta)-\frac{1}{2}500\delta^2$
So, $\delta=\frac{0.5\pm\sqrt{0.25+50}}{2\times250}=0.015\text{m}=1.5\text{cm}$

Amplitude of the vibration $= 31.5 - 30.1 - 1.4.$
Position A is $30.1 - 1.4 = 28.7cm$ from pole.
For A $u = -31.5, f = -12cm$
$\therefore \ \frac{1}{\text{v}}=\frac{1}{\text{f}}-\frac{1}{\text{u}}=-\frac{1}{12}+\frac{1}{31.5}$
$\Rightarrow\text{V}_{\text{A}}=-19.38\text{cm}$
For B $ f = -12cm, u = -28.7cm$
$\frac{1}{\text{v}}=\frac{1}{\text{f}}-\frac{1}{\text{u}}=-\frac{1}{12}+\frac{1}{28.7}$
$\Rightarrow \ \text{V}_\text{B}=-20.62\text{cm}$
The image vibrates in length $(20.62 - 19.38) = 1.24cm.$
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