The problem involves finding the focal length ($f$) of a thin lens using the concept of magnification ($m$) when an object is placed at two different distances, resulting in images of equal size.
The magnification $m$ can also be expressed in terms of $u$ and $f$: $m = \frac{f}{u+f}$.
Given two object distances $u_1 = -8 \text{ cm}$ and $u_2 = -24 \text{ cm}$ (negative by convention as objects are typically placed to the left of the lens).
The condition $|m_1| = |m_2|$ implies $m_1 = \pm m_2$. Since the object distances are different, $m_1$ cannot equal $m_2$. Therefore, $m_1 = -m_2$.
This leads to:
$ \frac{f}{u_1+f} = -\frac{f}{u_2+f} $Dividing both sides by $f$ (assuming $f \neq 0$):
$ \frac{1}{u_1+f} = -\frac{1}{u_2+f} $Cross-multiplying gives:
$ u_2+f = -(u_1+f) $ $ u_2+f = -u_1-f $Rearranging to solve for $f$:
$ 2f = -u_1 - u_2 $ $ f = -\frac{u_1 + u_2}{2} $Substitute the given object distances into the derived formula:
$ f = -\frac{(-8 \text{ cm}) + (-24 \text{ cm})}{2} $ $ f = -\frac{-32 \text{ cm}}{2} $ $ f = -(-16 \text{ cm}) $ $ f = 16 \text{ cm} $Case 1: $u_1 = -8 \text{ cm}$, $f = 16 \text{ cm}$
Using the lens formula $\frac{1}{v_1} = \frac{1}{f} - \frac{1}{u_1}$:
$ \frac{1}{v_1} = \frac{1}{16} - \frac{1}{-8} = \frac{1}{16} + \frac{2}{16} = \frac{3}{16} $Wait, the derivation $m = \frac{f}{u+f}$ is correct. Let's re-verify the calculation based on $f = -\frac{u_1 + u_2}{2}$.
The condition $m_1 = -m_2$ correctly yielded $f = -\frac{u_1 + u_2}{2}$.
Let's recalculate $v$ and $m$ using $f=16$ cm.
Case 1 ($u_1 = -8$ cm):
$ \frac{1}{v_1} = \frac{1}{f} + \frac{1}{u_1} = \frac{1}{16} + \frac{1}{-8} = \frac{1 - 2}{16} = -\frac{1}{16} $ $ v_1 = -16 \text{ cm} $ $ m_1 = \frac{v_1}{u_1} = \frac{-16}{-8} = 2 $Case 2 ($u_2 = -24$ cm):
$ \frac{1}{v_2} = \frac{1}{f} + \frac{1}{u_2} = \frac{1}{16} + \frac{1}{-24} = \frac{3 - 2}{48} = \frac{1}{48} $ $ v_2 = 48 \text{ cm} $ $ m_2 = \frac{v_2}{u_2} = \frac{48}{-24} = -2 $The magnitudes $|m_1| = |2| = 2$ and $|m_2| = |-2| = 2$ are equal. The focal length is indeed $16 \text{ cm}$.
A ring is placed at the bottom of a trough containing four immiscible liquids of refractive indices $1.0, 2.0, 3.0$ and $4.0$ poured one above the other of heights $10$ cm, $20$ cm, $30$ cm, and $40$ cm respectively. The apparent depth at which the ring appears, when seen from outside is____________ cm.
A plane polarized light is incident on a polariser with its pass axis making angle $\theta$ with x-axis, as shown in the figure. At four different values of $\theta$, $\theta = 8^\circ, 38^\circ, 188^\circ$ and $218^\circ$, the observed intensities are same. What is the angle between the direction of polarization and x-axis ?
