In Young’s double slit experimental set-up, the intensity of the central maximum is \( I_0 \). Calculate the intensity at a point where the path difference between two interfering waves is \( \frac{\lambda}{3} \).
The intensity in Young’s double slit experiment is given by:
\[ I = I_0 \cos^2\left( \frac{\pi \Delta x}{\lambda} \right) \]
Where:
- \( I_0 \) is the intensity of the central maximum,
- \( \Delta x \) is the path difference between the two waves,
- \( \lambda \) is the wavelength of the light.
Given: \( \Delta x = \frac{\lambda}{3} \), we substitute into the equation:
\[ I = I_0 \cos^2\left( \frac{\pi}{3} \right) \]
Since \( \cos\left( \frac{\pi}{3} \right) = \frac{1}{2} \), we get:
\[ I = I_0 \left( \frac{1}{2} \right)^2 = \frac{I_0}{4} \]
Final Answer:
The intensity at the point where the path difference is \( \frac{\lambda}{3} \) is: \[ I = \frac{I_0}{4} \]
When light travels from an optically denser medium to an optically rarer medium, at the interface it is partly reflected back into the same medium and partly refracted to the second medium. The angle of incidence corresponding to an angle of refraction 90° is called the critical angle (ic) for the given pair of media. This angle is related to the refractive index of medium 1 with respect to medium 2. Refraction of light through a prism involves refraction at two plane interfaces. A relation for the refractive index of the material of the prism can be obtained in terms of the refracting angle of the prism and the angle of minimum deviation. For a thin prism, this relation reduces to a simple equation. Laws of refraction are also valid for refraction of light at a spherical interface. When an object is placed in front of a spherical surface separating two media, its image is formed. A relation between object and image distance, in terms of refractive indices of two media and the radius of curvature of the spherical surface can be obtained. Using this relation for two surfaces of lens, ’lensemaker formula’ is obtained.
