Class 12 Ray Optics And Optical Instruments CBSE Questions & Answers
Class 12 · Ray Optics And Optical Instruments
This is Physics Class 12 Ray Optics and Optical Instruments CBSE Questions & Answers. There are 15 questions in this test with each question having around four answer choices.
Questions & Answers
1
Light rays from a point object
- Aradiate only to the side
- Bradiate in some lines
- Cradiate only at the front
- Dradiate in all directionsCorrect
2
According to Cartesian sign convention.
- Aall distances are measured from the bottom of the mirror or the lens
- Ball distances are measured from the top of the mirror or the lens
- Call distances are measured from infinity
- Dall distances are measured from the pole of the mirror or the optical centre of the lensCorrect
3
According to Cartesian sign convention the heights measured
- Adownwards with respect to x-axis and normal to the principal axis (x-axis) of the mirror/lens are taken as positive
- Brightwards with respect to x-axis and normal to the principal axis (x-axis) of the mirror/lens are taken as positive
- Cleftwards with respect to x-axis and normal to the principal axis (x-axis) of the mirror/lens are taken as positive
- Dupwards with respect to x-axis and normal to the principal axis (x-axis) of the mirror/lens are taken as positiveCorrect
4
Focal length of a mirror is given by
- Af = R/4, R=radius of curvature
- Bf = R, R=radius of curvature
- Cf = \({{\rm{R}}^{\rm{2}}}\), R=radius of curvature
- Df = R/2, R=radius of curvatureCorrect
5
According to the mirror equation
- A\({1 \over f} = {1 \over u} + {1 \over v}\)Correct
- B\({2 \over f} = {1 \over u} + {1 \over v}\)
- C\({1 \over f} = {2 \over u} + {1 \over v}\)
- D\({1 \over f} = {1 \over u} + {2 \over v}\)
6
Magnification for spherical mirrors m is given by
- A\({u \over v}\)
- B\({u \over v}\)
- C- \({v \over u}\)Correct
- D\({v \over u}\)
7
Refraction is
- AReversal of direction of propagation of light
- BNone of the above
- CThe change of direction of propagation of light
- DChange of direction of propagation of light at the interface of two media as light passes from one medium to anotherCorrect
8
According to Snell’s law
- AThe ratio of the angle of incidence to the angle of refraction is constant
- BThe ratio of the cosine of the angle of incidence to the cosine of angle of refraction is constant
- CThe ratio of the sine of the angle of incidence to the sine of angle of refraction is constantCorrect
- DThe ratio of the tangent of the angle of incidence to the tangent of angle of refraction is constant
9
For a rectangular slab, refraction takes place at
- AThree interfaces
- BOne interfaces
- CFour interfaces
- DTwo interfacesCorrect
10
Total internal reflection can take place only if light is travelling from
- ANo two media
- Bany two media
- CDenser to rarer mediumCorrect
- DRarer to denser medium
11
Total internal reflection can take place only if
- Atan(incidence angle) = 1/\({{\rm{n}}_{{\rm{21}}}}\), \({{\rm{n}}_{{\rm{21}}}}\) = refractive index travelling from 2 to 1
- Bincidence angle = 1/\({{\rm{n}}_{{\rm{21}}}}\), \({{\rm{n}}_{{\rm{21}}}}\) = refractive index travelling from 2 to 1
- Ccos(incidence angle) = 1/\({{\rm{n}}_{{\rm{21}}}}\)1, \({{\rm{n}}_{{\rm{21}}}}\) = refractive index travelling from 2 to 1
- Dsin(incidence angle) = 1/ \({{\rm{n}}_{{\rm{21}}}}\), \({{\rm{n}}_{{\rm{21}}}}\) = refractive index travelling from 2 to 1Correct
12
Optical fibre communication uses the principle of
- Alight scattering
- Blight path reversibility
- CTotal internal reflectionCorrect
- Dleast action
13
For small angles Snell’s law becomes
- A\({{\rm{n}}_{\rm{1}}}{\rm{i}}\) = \({{\rm{n}}_{\rm{2}}}\)
- B\({{\rm{n}}_{\rm{1}}}\)= \({{\rm{n}}_{\rm{2}}}\)r
- Ci = r
- D\({{\rm{n}}_{\rm{1}}}{\rm{i}}\) = \({{\rm{n}}_{\rm{2}}}\)rCorrect
14
Lens maker’s formula is
- A\({1 \over f} = \left( {{n_{21}} - 1} \right)({1 \over {{R_1}}} + {1 \over {{R_2}}})\)
- B\({1 \over f} = \left( {{n_{21}} + 1} \right)({1 \over {{R_1}}} + {1 \over {{R_2}}})\)
- C\({1 \over f} = \left( {{n_{21}} + 1} \right)({1 \over {{R_1}}} - {1 \over {{R_2}}})\)
- D\({1 \over f} = \left( {{n_{21}} - 1} \right)({1 \over {{R_1}}} - {1 \over {{R_2}}})\)Correct
15
Thin lens approximation for a lens is
- A\({1 \over v} - {1 \over u} = {1 \over f}\)Correct
- B\({1 \over v} + {1 \over u} = {1 \over f}\)
- C\({1 \over v} + {1 \over u} = - {1 \over f}\)
- D\({1 \over v} - {1 \over u} = - {1 \over f}\)