Question
Consider the situation described in the previous problem. Where should a point source be placed on the principal axis so that the two images form at the same place?
Let the source be placed at a distance ‘x’ from the lens as shown, so that images formed by both coincide. For the lens, $\frac{1}{\text{v}_\ell}-\frac{1}{-\text{x}}=\frac{1}{15}\Rightarrow\text{v}_\ell=\frac{15\text{x}}{\text{x}-15} \ ...(1)$ For the mirror, $\text{u}=-(50-\text{x}), \ \text{f}=-10\text{cm}$ So, $\frac{1}{\text{v}_\text{m}}+\frac{1}{-(50-\text{x})}=-\frac{1}{10}$ $\Rightarrow\frac{1}{\text{v}_\text{m}}=\frac{1}{-(50-\text{x})}-\frac{1}{10}$
$\text{v}_\text{m}=\frac{10(50-\text{x})}{\text{x}-40} \ ...(2)$
Since the lens and mirror are 50cm apart,$\text{v}_\ell-\text{v}_{\text{m}}=50\Rightarrow\frac{15\text{x}}{\text{x}-15}-\frac{10(50-\text{x})}{(\text{x}-40)}=50$
$\Rightarrow\text{x}=30\text{cm}.$
So, the source should be placed 30cm from the lens.Generate a complete, print-ready paper with questions like this in minutes — across 16+ boards, with answer keys.


Damped oscillations
We know that the motion of a simple pendulum, swinging in air, dies out eventually. Why does it happen? This is because the air drag and the friction at the support oppose the motion of the pendulum and dissipate its energy gradually. The pendulum is said to execute damped oscillations. In damped oscillations, the energy of the system is dissipated continuously; but, for small damping, the oscillations remain approximately periodic. The dissipating forces are generally the frictional forces. The damping force is generally proportional to velocity of the bob and acts opposite to the direction of velocity. If the damping force is denoted by Fd, we have Fd = –bv where the positive constant b depends on characteristics of the medium (viscosity, for example) and the size and shape of the block, is usually valid only for small velocity.