Condition for Coincidence of Bright Fringes in Young’s Double Slit Experiment
For the bright fringes of two different wavelengths to coincide, the path difference must be an integer multiple of both wavelengths. This happens when the path difference is equal to the least common multiple (LCM) of the two wavelengths.
The condition for constructive interference is given by:
\[ \Delta y = m \lambda_1 = n \lambda_2 \]
where \( m \) and \( n \) are integers.
Given:
Wavelengths: \( \lambda_1 = 500 \, \text{nm}, \lambda_2 = 600 \, \text{nm} \)
LCM of \( 500 \, \text{nm} \) and \( 600 \, \text{nm} \) is \( 3000 \, \text{nm} = 3.0 \times 10^{
-6} \, \text{m} \)
To find the position \( y \) on the screen where both bright fringes coincide, we use the fringe position formula:
\[ y = \frac{m \lambda D}{d} \]
Substitute values:
\( \lambda = 3.0 \times 10^{
-6} \, \text{m} \)
\( D = 1.0 \, \text{m} \)
\( d = 1.0 \times 10^{
-3} \, \text{m} \)
\[ y = \frac{1 \cdot 3.0 \times 10^{
-6} \cdot 1.0}{1.0 \times 10^{
-3}} = 3.0 \times 10^{
-3} \, \text{m} = 3.0 \, \text{mm} \]
Final Answer:
The least distance from the central maximum where the bright fringes due to both wavelengths coincide is 3.0 mm.
Light from a point source in air falls on a spherical glass surface (refractive index, \( \mu = 1.5 \) and radius of curvature \( R = 50 \) cm). The image is formed at a distance of 200 cm from the glass surface inside the glass. The magnitude of distance of the light source from the glass surface is 1cm.

