Dispersion, Cauchy's Theorem, Angular Dispersion, Dispersion Power
NEET Test Series from KOTA - 10 Papers In MS WORD WhatsApp Here
Ray Optics

282790 A person has been using spectacles of power1.0 Dioptre for distant vision and a separate reading glass of power 2.0 Dioptres. What is the least distance of distinct vision for this person:

1 \(10 \mathrm{~cm}\)
2 \(40 \mathrm{~cm}\)
3 \(30 \mathrm{~cm}\)
4 \(50 \mathrm{~cm}\)
Ray Optics

282791 For light diverging from a finite point source

1 The wave front is parabolic
2 The intensity at the wave front does not depend on the distance
3 The wave front is cylindrical
4 The intensity decreases in proportion to the distance squared
Ray Optics

282792 To produce dispersion without deviation, a thin prism of angle \(15^{\circ}\) made of glass of refractive index 1.45 is combined with another prism made of glass of refractive index 1.75. The two prisms are arranged such that the refracting angles are in opposite direction. The angle of second prism is

1 \(10^{\circ}\)
2 \(12^{\circ}\)
3 \(6^{\circ}\)
4 \(9^{\circ}\)
Ray Optics

282793 Fresnel distance for an aperture of size a is illuminated by a parallel beam of light of wavelength \(\lambda\), deciding the validity of ray optics is

1 \(\frac{\lambda}{\mathrm{a}^2}\)
2 \(\lambda \mathrm{a}\)
3 \(a^2 \lambda\)
4 \(\frac{a^2}{\lambda}\)
(e) \(\mathrm{a}^2 \lambda^2\)
Ray Optics

282790 A person has been using spectacles of power1.0 Dioptre for distant vision and a separate reading glass of power 2.0 Dioptres. What is the least distance of distinct vision for this person:

1 \(10 \mathrm{~cm}\)
2 \(40 \mathrm{~cm}\)
3 \(30 \mathrm{~cm}\)
4 \(50 \mathrm{~cm}\)
Ray Optics

282791 For light diverging from a finite point source

1 The wave front is parabolic
2 The intensity at the wave front does not depend on the distance
3 The wave front is cylindrical
4 The intensity decreases in proportion to the distance squared
Ray Optics

282792 To produce dispersion without deviation, a thin prism of angle \(15^{\circ}\) made of glass of refractive index 1.45 is combined with another prism made of glass of refractive index 1.75. The two prisms are arranged such that the refracting angles are in opposite direction. The angle of second prism is

1 \(10^{\circ}\)
2 \(12^{\circ}\)
3 \(6^{\circ}\)
4 \(9^{\circ}\)
Ray Optics

282793 Fresnel distance for an aperture of size a is illuminated by a parallel beam of light of wavelength \(\lambda\), deciding the validity of ray optics is

1 \(\frac{\lambda}{\mathrm{a}^2}\)
2 \(\lambda \mathrm{a}\)
3 \(a^2 \lambda\)
4 \(\frac{a^2}{\lambda}\)
(e) \(\mathrm{a}^2 \lambda^2\)
Ray Optics

282790 A person has been using spectacles of power1.0 Dioptre for distant vision and a separate reading glass of power 2.0 Dioptres. What is the least distance of distinct vision for this person:

1 \(10 \mathrm{~cm}\)
2 \(40 \mathrm{~cm}\)
3 \(30 \mathrm{~cm}\)
4 \(50 \mathrm{~cm}\)
Ray Optics

282791 For light diverging from a finite point source

1 The wave front is parabolic
2 The intensity at the wave front does not depend on the distance
3 The wave front is cylindrical
4 The intensity decreases in proportion to the distance squared
Ray Optics

282792 To produce dispersion without deviation, a thin prism of angle \(15^{\circ}\) made of glass of refractive index 1.45 is combined with another prism made of glass of refractive index 1.75. The two prisms are arranged such that the refracting angles are in opposite direction. The angle of second prism is

1 \(10^{\circ}\)
2 \(12^{\circ}\)
3 \(6^{\circ}\)
4 \(9^{\circ}\)
Ray Optics

282793 Fresnel distance for an aperture of size a is illuminated by a parallel beam of light of wavelength \(\lambda\), deciding the validity of ray optics is

1 \(\frac{\lambda}{\mathrm{a}^2}\)
2 \(\lambda \mathrm{a}\)
3 \(a^2 \lambda\)
4 \(\frac{a^2}{\lambda}\)
(e) \(\mathrm{a}^2 \lambda^2\)
Ray Optics

282790 A person has been using spectacles of power1.0 Dioptre for distant vision and a separate reading glass of power 2.0 Dioptres. What is the least distance of distinct vision for this person:

1 \(10 \mathrm{~cm}\)
2 \(40 \mathrm{~cm}\)
3 \(30 \mathrm{~cm}\)
4 \(50 \mathrm{~cm}\)
Ray Optics

282791 For light diverging from a finite point source

1 The wave front is parabolic
2 The intensity at the wave front does not depend on the distance
3 The wave front is cylindrical
4 The intensity decreases in proportion to the distance squared
Ray Optics

282792 To produce dispersion without deviation, a thin prism of angle \(15^{\circ}\) made of glass of refractive index 1.45 is combined with another prism made of glass of refractive index 1.75. The two prisms are arranged such that the refracting angles are in opposite direction. The angle of second prism is

1 \(10^{\circ}\)
2 \(12^{\circ}\)
3 \(6^{\circ}\)
4 \(9^{\circ}\)
Ray Optics

282793 Fresnel distance for an aperture of size a is illuminated by a parallel beam of light of wavelength \(\lambda\), deciding the validity of ray optics is

1 \(\frac{\lambda}{\mathrm{a}^2}\)
2 \(\lambda \mathrm{a}\)
3 \(a^2 \lambda\)
4 \(\frac{a^2}{\lambda}\)
(e) \(\mathrm{a}^2 \lambda^2\)