Class 12 Wave Optics CBSE Questions & Answers
Class 12 · Wave Optics
This is Physics Class 12 Wave Optics CBSE Questions & Answers. There are 15 questions in this test with each question having around four answer choices.
Questions & Answers
1
Is light a particle or a wave?
- ALight is a set of waves
- BLight is schizophrenic i.e. sometimes it behaves like a particle and other times like a wave.
- CLight is a set of particles
- DBoth particle and wave approaches help us understand different phenomenonCorrect
2
The propagation of light is best described by,
- Aparticle model
- Ba wave modelCorrect
- CNone of the above
- Ddual / schizophrenic model
3
Emission and absorption is best described by,
- Aparticle modelCorrect
- Ba wave model
- CNone of the above
- Ddual / schizophrenic model
4
wave front is
- Alocus of all adjacent points at which the phase of vibration of a physical quantity associated with the wave is the sameCorrect
- Blocus of all adjacent points at which the Electric field is the same
- Cseries of points on the wave with same amplitude
- Dseries of points on the wave with same frequency
5
A ray is an imaginary
- Aline from source to horizon
- Bline along the direction perpendicular to travel of the wave
- Cline along the direction at an angle to the travel of the wave
- Dline along the direction of travel of the waveCorrect
6
According to Huygens principle
- Aeach point on a wave front is a source of secondary wavesCorrect
- BNo point on a wave front is a source of secondary waves
- CNone of the above
- Deach point on a wave front is a sink of secondary waves
7
According to Huygens construction relation between old and new wave fronts is
- Anew wave front is parallel to old wave front
- Bnew wave front is perpendicular to old wave front
- Cnew wave front is tangential to old wave front
- Dnew wave front is the forward envelope of the secondary wavesCorrect
8
Relation between ray and wave front is
- ARays are tangential to wave front
- BRays are parallel to wave front
- CRays are perpendicular to wave frontCorrect
- DRays are at acute angle to wave front
9
Approximate Doppler shift formula for light is
- A\({{\Delta \upsilon } \over \upsilon } = {{{v_{rad}}} \over c}\)
- B\({{\Delta \upsilon } \over \upsilon } = - {{{v_{rad}}} \over c}\)Correct
- C\({{\Delta \upsilon } \over \upsilon } = - {{{v_{rad}}} \over {2c}}\)
- D\({{\Delta \upsilon } \over \upsilon } = 2{{{v_{rad}}} \over c}\)
10
According to superposition principle in relation to displacements produced by a number of waves
- Aresultant displacement is the vector sum of the displacements producedCorrect
- Bresultant displacement is the dot product of the displacements produced
- Cresultant displacement is the scalar sum of the displacements produced
- Dresultant displacement is the arithmetic sum of the displacements produced
11
Two sources of light are coherent if they have
- Adifferent frequency and random phases
- Bsame frequency and with a constant phase relationshipCorrect
- Csame frequency and change phase randomly
- Ddifferent frequency and with a constant phase relationship
12
Interference effects of light from two sources can be observed if
- Athe sources are of different frequency
- Bthe sources are independent
- Cthe sources are different frequency and random phases
- Dthe sources are coherentCorrect
13
If we have two coherent sources \({{\rm{S}}_{\rm{1}}}{\rm{and }}{{\rm{S}}_{\rm{2}}}\) vibrating in phase, then for an arbitrary point P constructive interference is observed whenever the path difference is
- AAn even multiple of wavelength
- BA fraction of a wavelength
- CAn odd multiple of wavelength
- DAn integral multiple of wavelengthCorrect
14
If we have two coherent sources \({{\rm{S}}_{\rm{1}}}{\rm{and }}{{\rm{S}}_{\rm{2}}}\) vibrating in phase, then for an arbitrary point P destructive interference is observed whenever the path difference is
- A\(n\lambda where{\rm{ }}n = 0,1,2,3 \ldots \)
- B\((n + {1 \over 2})\lambda where{\rm{ }}n = 0,1,2,3 \ldots \)Correct
- C\((n + {1 \over {2}})\lambda where {\rm{ }}n = 0,3,5 \ldots \)
- D\((n + {1 \over {3}})\lambda where{\rm{ }}n = 0,1,2,3 \ldots \)
15
If we have two coherent sources \({{\rm{S}}_{\rm{1}}}{\rm{and }}{{\rm{S}}_{\rm{2}}}\) vibrating in phase with same amplitude, then for an arbitrary point P with path difference corresponding to \(\phi \) , the resultant intensity if the intensity due to each is I0 would be
- A\({I_0}co{s^2}\left( \emptyset \right)\)
- B\(4{I_0}co{s^2}\left( {\emptyset /2} \right)\)Correct
- C\({I_0}co{s^2}\left( {\emptyset /2} \right)\)
- D\(4{I_0}co{s^2}\left( \emptyset \right)\)