Interference of Waves
PHXII10:WAVE OPTICS

367755 Four light waves are represented by
(i) \({y_1} = {a_1}\sin (\omega t + \phi )\)
(ii) \({y_2} = {a_2}\sin \omega t\)
(iii) \({y_3} = {a_3}\sin 2(\omega t + \phi )\)
(iv) \({y_4} = {a_4}\sin 2{\rm{ }}\omega t\)
Interference fringes may be observed due to superposition of

1 (i) and (iii)
2 (i) and (ii)
3 (ii) and (iv)
4 (ii) and (iii)
PHXII10:WAVE OPTICS

367756 The phenomenon of interference is shown by

1 Electromagnetic waves only
2 Longitudinal mechanical waves only
3 Transverse mechanical waves only
4 All the above types of waves
PHXII10:WAVE OPTICS

367757 To demonstrate the phenomenon of interference, we require two sources which emit radiations

1 of the same frequency and having definite phase relationship
2 of nearly the same frequency
3 of the same frequency
4 of different wavelength
PHXII10:WAVE OPTICS

367758 Two interfering light waves are mathematically represented as \(y_{1}=4 \sin \omega t\) and \(y_{2}=3 \cos (\omega t)\). The amplitude of the resultant wave on superposition is \(\left(y_{1}\right.\) and \(y_{2}\) are in \(C G S\) system)

1 \(5\;cm\)
2 \(7\;cm\)
3 \(1\;cm\)
4 Zero
PHXII10:WAVE OPTICS

367755 Four light waves are represented by
(i) \({y_1} = {a_1}\sin (\omega t + \phi )\)
(ii) \({y_2} = {a_2}\sin \omega t\)
(iii) \({y_3} = {a_3}\sin 2(\omega t + \phi )\)
(iv) \({y_4} = {a_4}\sin 2{\rm{ }}\omega t\)
Interference fringes may be observed due to superposition of

1 (i) and (iii)
2 (i) and (ii)
3 (ii) and (iv)
4 (ii) and (iii)
PHXII10:WAVE OPTICS

367756 The phenomenon of interference is shown by

1 Electromagnetic waves only
2 Longitudinal mechanical waves only
3 Transverse mechanical waves only
4 All the above types of waves
PHXII10:WAVE OPTICS

367757 To demonstrate the phenomenon of interference, we require two sources which emit radiations

1 of the same frequency and having definite phase relationship
2 of nearly the same frequency
3 of the same frequency
4 of different wavelength
PHXII10:WAVE OPTICS

367758 Two interfering light waves are mathematically represented as \(y_{1}=4 \sin \omega t\) and \(y_{2}=3 \cos (\omega t)\). The amplitude of the resultant wave on superposition is \(\left(y_{1}\right.\) and \(y_{2}\) are in \(C G S\) system)

1 \(5\;cm\)
2 \(7\;cm\)
3 \(1\;cm\)
4 Zero
PHXII10:WAVE OPTICS

367755 Four light waves are represented by
(i) \({y_1} = {a_1}\sin (\omega t + \phi )\)
(ii) \({y_2} = {a_2}\sin \omega t\)
(iii) \({y_3} = {a_3}\sin 2(\omega t + \phi )\)
(iv) \({y_4} = {a_4}\sin 2{\rm{ }}\omega t\)
Interference fringes may be observed due to superposition of

1 (i) and (iii)
2 (i) and (ii)
3 (ii) and (iv)
4 (ii) and (iii)
PHXII10:WAVE OPTICS

367756 The phenomenon of interference is shown by

1 Electromagnetic waves only
2 Longitudinal mechanical waves only
3 Transverse mechanical waves only
4 All the above types of waves
PHXII10:WAVE OPTICS

367757 To demonstrate the phenomenon of interference, we require two sources which emit radiations

1 of the same frequency and having definite phase relationship
2 of nearly the same frequency
3 of the same frequency
4 of different wavelength
PHXII10:WAVE OPTICS

367758 Two interfering light waves are mathematically represented as \(y_{1}=4 \sin \omega t\) and \(y_{2}=3 \cos (\omega t)\). The amplitude of the resultant wave on superposition is \(\left(y_{1}\right.\) and \(y_{2}\) are in \(C G S\) system)

1 \(5\;cm\)
2 \(7\;cm\)
3 \(1\;cm\)
4 Zero
PHXII10:WAVE OPTICS

367755 Four light waves are represented by
(i) \({y_1} = {a_1}\sin (\omega t + \phi )\)
(ii) \({y_2} = {a_2}\sin \omega t\)
(iii) \({y_3} = {a_3}\sin 2(\omega t + \phi )\)
(iv) \({y_4} = {a_4}\sin 2{\rm{ }}\omega t\)
Interference fringes may be observed due to superposition of

1 (i) and (iii)
2 (i) and (ii)
3 (ii) and (iv)
4 (ii) and (iii)
PHXII10:WAVE OPTICS

367756 The phenomenon of interference is shown by

1 Electromagnetic waves only
2 Longitudinal mechanical waves only
3 Transverse mechanical waves only
4 All the above types of waves
PHXII10:WAVE OPTICS

367757 To demonstrate the phenomenon of interference, we require two sources which emit radiations

1 of the same frequency and having definite phase relationship
2 of nearly the same frequency
3 of the same frequency
4 of different wavelength
PHXII10:WAVE OPTICS

367758 Two interfering light waves are mathematically represented as \(y_{1}=4 \sin \omega t\) and \(y_{2}=3 \cos (\omega t)\). The amplitude of the resultant wave on superposition is \(\left(y_{1}\right.\) and \(y_{2}\) are in \(C G S\) system)

1 \(5\;cm\)
2 \(7\;cm\)
3 \(1\;cm\)
4 Zero