Coherent Sources of Light and interference of Light Constructive, Distractive
WAVE OPTICS

283258 In the case of light waves from two coherent sources \(S_1\) and \(S_2\), there will be constructive interference at an arbitrary point \(P\), if the path difference \(S_1 P-S_2 P\) is

1 \(\left(n+\frac{1}{2}\right) \lambda\)
2 \(\mathrm{n} \lambda\)
3 \(\left(\mathrm{n}-\frac{1}{2}\right) \lambda\)
4 \(\frac{\lambda}{2}\)
WAVE OPTICS

283259 Two coherent sources of intensity ratio \(1: 4\) produce an interference pattern. The fringe visibility will be

1 1
2 0.8
3 0.4
4 0.6
WAVE OPTICS

283262 Two coherent monochromatic lights make constructive interference when their phase difference is

1 \(\frac{3}{2} \pi\)
2 \(2 \pi\)
3 \(\pi\)
4 \(\frac{\pi}{2}\)
WAVE OPTICS

283267 The maximum constructive interference of 2 waves cannot occur if the phase difference is

1 \(2 \pi\)
2 \(4 \pi\)
3 \(5 \pi\)
4 0
WAVE OPTICS

283269 Interference was observed in an interference chamber when air was present. Now, the chamber is evacuated and if the same light is used, a careful observation will show

1 No interference
2 Interference with dark bands
3 Interference with dark bands
4 Interference in which breadth of the fringe will slightly increased
WAVE OPTICS

283258 In the case of light waves from two coherent sources \(S_1\) and \(S_2\), there will be constructive interference at an arbitrary point \(P\), if the path difference \(S_1 P-S_2 P\) is

1 \(\left(n+\frac{1}{2}\right) \lambda\)
2 \(\mathrm{n} \lambda\)
3 \(\left(\mathrm{n}-\frac{1}{2}\right) \lambda\)
4 \(\frac{\lambda}{2}\)
WAVE OPTICS

283259 Two coherent sources of intensity ratio \(1: 4\) produce an interference pattern. The fringe visibility will be

1 1
2 0.8
3 0.4
4 0.6
WAVE OPTICS

283262 Two coherent monochromatic lights make constructive interference when their phase difference is

1 \(\frac{3}{2} \pi\)
2 \(2 \pi\)
3 \(\pi\)
4 \(\frac{\pi}{2}\)
WAVE OPTICS

283267 The maximum constructive interference of 2 waves cannot occur if the phase difference is

1 \(2 \pi\)
2 \(4 \pi\)
3 \(5 \pi\)
4 0
WAVE OPTICS

283269 Interference was observed in an interference chamber when air was present. Now, the chamber is evacuated and if the same light is used, a careful observation will show

1 No interference
2 Interference with dark bands
3 Interference with dark bands
4 Interference in which breadth of the fringe will slightly increased
WAVE OPTICS

283258 In the case of light waves from two coherent sources \(S_1\) and \(S_2\), there will be constructive interference at an arbitrary point \(P\), if the path difference \(S_1 P-S_2 P\) is

1 \(\left(n+\frac{1}{2}\right) \lambda\)
2 \(\mathrm{n} \lambda\)
3 \(\left(\mathrm{n}-\frac{1}{2}\right) \lambda\)
4 \(\frac{\lambda}{2}\)
WAVE OPTICS

283259 Two coherent sources of intensity ratio \(1: 4\) produce an interference pattern. The fringe visibility will be

1 1
2 0.8
3 0.4
4 0.6
WAVE OPTICS

283262 Two coherent monochromatic lights make constructive interference when their phase difference is

1 \(\frac{3}{2} \pi\)
2 \(2 \pi\)
3 \(\pi\)
4 \(\frac{\pi}{2}\)
WAVE OPTICS

283267 The maximum constructive interference of 2 waves cannot occur if the phase difference is

1 \(2 \pi\)
2 \(4 \pi\)
3 \(5 \pi\)
4 0
WAVE OPTICS

283269 Interference was observed in an interference chamber when air was present. Now, the chamber is evacuated and if the same light is used, a careful observation will show

1 No interference
2 Interference with dark bands
3 Interference with dark bands
4 Interference in which breadth of the fringe will slightly increased
WAVE OPTICS

283258 In the case of light waves from two coherent sources \(S_1\) and \(S_2\), there will be constructive interference at an arbitrary point \(P\), if the path difference \(S_1 P-S_2 P\) is

1 \(\left(n+\frac{1}{2}\right) \lambda\)
2 \(\mathrm{n} \lambda\)
3 \(\left(\mathrm{n}-\frac{1}{2}\right) \lambda\)
4 \(\frac{\lambda}{2}\)
WAVE OPTICS

283259 Two coherent sources of intensity ratio \(1: 4\) produce an interference pattern. The fringe visibility will be

1 1
2 0.8
3 0.4
4 0.6
WAVE OPTICS

283262 Two coherent monochromatic lights make constructive interference when their phase difference is

1 \(\frac{3}{2} \pi\)
2 \(2 \pi\)
3 \(\pi\)
4 \(\frac{\pi}{2}\)
WAVE OPTICS

283267 The maximum constructive interference of 2 waves cannot occur if the phase difference is

1 \(2 \pi\)
2 \(4 \pi\)
3 \(5 \pi\)
4 0
WAVE OPTICS

283269 Interference was observed in an interference chamber when air was present. Now, the chamber is evacuated and if the same light is used, a careful observation will show

1 No interference
2 Interference with dark bands
3 Interference with dark bands
4 Interference in which breadth of the fringe will slightly increased
WAVE OPTICS

283258 In the case of light waves from two coherent sources \(S_1\) and \(S_2\), there will be constructive interference at an arbitrary point \(P\), if the path difference \(S_1 P-S_2 P\) is

1 \(\left(n+\frac{1}{2}\right) \lambda\)
2 \(\mathrm{n} \lambda\)
3 \(\left(\mathrm{n}-\frac{1}{2}\right) \lambda\)
4 \(\frac{\lambda}{2}\)
WAVE OPTICS

283259 Two coherent sources of intensity ratio \(1: 4\) produce an interference pattern. The fringe visibility will be

1 1
2 0.8
3 0.4
4 0.6
WAVE OPTICS

283262 Two coherent monochromatic lights make constructive interference when their phase difference is

1 \(\frac{3}{2} \pi\)
2 \(2 \pi\)
3 \(\pi\)
4 \(\frac{\pi}{2}\)
WAVE OPTICS

283267 The maximum constructive interference of 2 waves cannot occur if the phase difference is

1 \(2 \pi\)
2 \(4 \pi\)
3 \(5 \pi\)
4 0
WAVE OPTICS

283269 Interference was observed in an interference chamber when air was present. Now, the chamber is evacuated and if the same light is used, a careful observation will show

1 No interference
2 Interference with dark bands
3 Interference with dark bands
4 Interference in which breadth of the fringe will slightly increased