365016
A ray of light passes through four transparent media with refractive indices \({n_1},{n_2},{n_3}\) and \({n_4}\) as shown. The surface of all media are parallel. If the emergent ray \(DE\) is parallel to incident ray \(AB\) then
365017
Monochromatic light is refracted from air into glass of refractive index \(\mu\). The ratio of the wavelength of incident and refracted waves is:
1 \(1: \mu\)
2 \(1: \mu^{2}\)
3 \(\mu: 1\)
4 \(1: 1\)
Explanation:
As we know, \(\begin{aligned}& \lambda \propto \dfrac{1}{\mu} \\& \dfrac{\lambda_{1}}{\lambda_{2}}=\dfrac{\mu_{2}}{\mu_{1}}=\dfrac{\mu}{1} \\& \dfrac{\lambda_{1}}{\lambda_{2}}=\dfrac{\mu}{1} .\end{aligned}\)
365016
A ray of light passes through four transparent media with refractive indices \({n_1},{n_2},{n_3}\) and \({n_4}\) as shown. The surface of all media are parallel. If the emergent ray \(DE\) is parallel to incident ray \(AB\) then
365017
Monochromatic light is refracted from air into glass of refractive index \(\mu\). The ratio of the wavelength of incident and refracted waves is:
1 \(1: \mu\)
2 \(1: \mu^{2}\)
3 \(\mu: 1\)
4 \(1: 1\)
Explanation:
As we know, \(\begin{aligned}& \lambda \propto \dfrac{1}{\mu} \\& \dfrac{\lambda_{1}}{\lambda_{2}}=\dfrac{\mu_{2}}{\mu_{1}}=\dfrac{\mu}{1} \\& \dfrac{\lambda_{1}}{\lambda_{2}}=\dfrac{\mu}{1} .\end{aligned}\)
365016
A ray of light passes through four transparent media with refractive indices \({n_1},{n_2},{n_3}\) and \({n_4}\) as shown. The surface of all media are parallel. If the emergent ray \(DE\) is parallel to incident ray \(AB\) then
365017
Monochromatic light is refracted from air into glass of refractive index \(\mu\). The ratio of the wavelength of incident and refracted waves is:
1 \(1: \mu\)
2 \(1: \mu^{2}\)
3 \(\mu: 1\)
4 \(1: 1\)
Explanation:
As we know, \(\begin{aligned}& \lambda \propto \dfrac{1}{\mu} \\& \dfrac{\lambda_{1}}{\lambda_{2}}=\dfrac{\mu_{2}}{\mu_{1}}=\dfrac{\mu}{1} \\& \dfrac{\lambda_{1}}{\lambda_{2}}=\dfrac{\mu}{1} .\end{aligned}\)
365016
A ray of light passes through four transparent media with refractive indices \({n_1},{n_2},{n_3}\) and \({n_4}\) as shown. The surface of all media are parallel. If the emergent ray \(DE\) is parallel to incident ray \(AB\) then
365017
Monochromatic light is refracted from air into glass of refractive index \(\mu\). The ratio of the wavelength of incident and refracted waves is:
1 \(1: \mu\)
2 \(1: \mu^{2}\)
3 \(\mu: 1\)
4 \(1: 1\)
Explanation:
As we know, \(\begin{aligned}& \lambda \propto \dfrac{1}{\mu} \\& \dfrac{\lambda_{1}}{\lambda_{2}}=\dfrac{\mu_{2}}{\mu_{1}}=\dfrac{\mu}{1} \\& \dfrac{\lambda_{1}}{\lambda_{2}}=\dfrac{\mu}{1} .\end{aligned}\)
365016
A ray of light passes through four transparent media with refractive indices \({n_1},{n_2},{n_3}\) and \({n_4}\) as shown. The surface of all media are parallel. If the emergent ray \(DE\) is parallel to incident ray \(AB\) then
365017
Monochromatic light is refracted from air into glass of refractive index \(\mu\). The ratio of the wavelength of incident and refracted waves is:
1 \(1: \mu\)
2 \(1: \mu^{2}\)
3 \(\mu: 1\)
4 \(1: 1\)
Explanation:
As we know, \(\begin{aligned}& \lambda \propto \dfrac{1}{\mu} \\& \dfrac{\lambda_{1}}{\lambda_{2}}=\dfrac{\mu_{2}}{\mu_{1}}=\dfrac{\mu}{1} \\& \dfrac{\lambda_{1}}{\lambda_{2}}=\dfrac{\mu}{1} .\end{aligned}\)