Chapter 18: Problem 117
Total numbers of fringes can be seen on the screen will be (A) 2001 (B) 4001 (C) 6001 (D) 8001
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Chapter 18: Problem 117
Total numbers of fringes can be seen on the screen will be (A) 2001 (B) 4001 (C) 6001 (D) 8001
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A concave lens of focal length \(10 \mathrm{~cm}\) and a convex lens of focal length \(20 \mathrm{~cm}\) are placed certain distance apart. If parallel rays incident on one lens become converging after passing through other lens, then the separation between the lenses must be greater than (A) Zero (B) \(5 \mathrm{~cm}\) (C) \(10 \mathrm{~cm}\) (D) \(9 \mathrm{~cm}\)
In a Young's double slit experiment, the slit separation is \(1 \mathrm{~mm}\) and the screen is \(1 \mathrm{~m}\) from the slit. For a monochromatic light of wavelength \(500 \mathrm{~nm}\), the distance of third minimum from the central maximum is (A) \(0.50 \mathrm{~mm}\) (B) \(1.25 \mathrm{~mm}\) (C) \(1.50 \mathrm{~mm}\) (D) \(1.75 \mathrm{~mm}\)
A microscope is focused on a needle lying in an empty tank. Now, the tank is filled with benzene to a height \(120 \mathrm{~mm}\). The microscope is moved \(40 \mathrm{~mm}\) to focus the needle again. The refractive index of benzene is (A) \(1.5\) (B) \(2.5\) (C) \(3.0\) (D) \(4.5\)
Interference fringes were produced in Young's double slit experiment using light of wavelength \(5000 \AA\). When a film of thickness \(2.5 \times 10^{-3} \mathrm{~cm}\) was placed in front of one of the slits, the fringe pattern shifted by a distance equal to 20 fringe-widths. The refractive index of the material of the film is (A) \(1.25\) (B) \(1.35\) (C) \(1.4\) (D) \(1.5\)
If \(\varepsilon_{0}\) and \(\mu_{0}\) represent the permittivity and permeability of vacuum, \(\varepsilon\) and \(\mu\) represent the permittivity and permeability of medium, then refractive index of the medium is given by (A) \(\sqrt{\frac{\mu_{0} \varepsilon_{0}}{\mu \varepsilon}}\) (B) \(\sqrt{\frac{\mu \varepsilon}{\mu_{0} \varepsilon_{0}}}\) (C) \(\sqrt{\frac{\varepsilon}{\mu_{0} \varepsilon_{0}}}\) (D) \(\sqrt{\frac{\mu_{0} \varepsilon_{0}}{\mu}}\)
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