The position of the \( m \)-th bright fringe for wavelength \( \lambda \) is given by: \[ y_m = \frac{m \lambda D}{d} \]
For the bright fringes due to both wavelengths to coincide, their positions must be the same: \[ \frac{m \lambda_1 D}{d} = \frac{n \lambda_2 D}{d} \] Simplifying: \[ m \lambda_1 = n \lambda_2 \] \[ \frac{m}{n} = \frac{\lambda_2}{\lambda_1} \]
\[ \frac{m}{n} = \frac{\lambda_2}{\lambda_1} = \frac{450 \times 10^{-9}}{600 \times 10^{-9}} = \frac{3}{4} \]
Thus, the smallest values of \( m = 3 \) and \( n = 4 \).
The least distance \( y \) where the fringes coincide is: \[ y = \frac{m \lambda_1 D}{d} = \frac{3 \times 600 \times 10^{-9} \times 1}{0.5 \times 10^{-3}} = 3.6 \, \text{mm} \]
The least distance from the central maximum where the bright fringes due to both wavelengths coincide is **3.6 mm**.
The magnitude of heat exchanged by a system for the given cyclic process ABC (as shown in the figure) is (in SI units):

As shown below, bob A of a pendulum having massless string of length \( R \) is released from \( 60^\circ \) to the vertical. It hits another bob B of half the mass that is at rest on a frictionless table in the center. Assuming elastic collision, the magnitude of the velocity of bob A after the collision will be (take \( g \) as acceleration due to gravity):


Bittu and Chintu were partners in a firm sharing profit and losses in the ratio of 4 : 3. Their Balance Sheet as at 31st March, 2024 was as follows:
On 1st April, 2024, Diya was admitted in the firm for \( \frac{1}{7} \)th share in the profits on the following terms:
Prepare Revaluation Account and Partners' Capital Accounts.