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

283270 Two coherent sources whose intensity ratio is \(64: 1\) produce interference fringes. The ratio of intensities of maxima and minima is

1 \(4: 7\)
2 \(8: 1\)
3 \(81: 49\)
4 \(81: 7\)
WAVE OPTICS

283271 Two slits, separated by a distance of \(1 \mathrm{~mm}\) are illuminated with red light of wavelength
\(6.5 \times 10^{-7} \mathrm{~m}\). The interference fringes are observed on a screen placed \(1 \mathrm{~m}\) from the slits. The distance of the third dark fringe from the central fringe will be equal to

1 \(0.65 \mathrm{~mm}\)
2 \(1.30 \mathrm{~mm}\)
3 \(1.62 \mathrm{~mm}\)
4 \(1.95 \mathrm{~mm}\)
WAVE OPTICS

283272 The interference pattern is obtained with two coherent light sources of intensity ratio \(n\). In the interference pattern, the ratio \(\frac{I_{\max }-I_{\text {min }}}{I_{\max }+I_{\text {min }}}\) will be

1 \(\frac{\sqrt{\mathrm{n}}}{\mathrm{n}+1}\)
2 \(\frac{2 \sqrt{\mathrm{n}}}{\mathrm{n}+1}\)
3 \(\frac{\sqrt{\mathrm{n}}}{(\mathrm{n}+1)^2}\)
4 \(\frac{2 \sqrt{n}}{(n+1)^2}\)
WAVE OPTICS

283276 Two coherent monochromatic light sources are located at two vertices of an equilateral triangle. If the intensity due to each of the sources independently is \(1 \mathrm{Wm}^{-2}\) at the third vertex, the resultant intensity due to both the sources at the point (i.e., at the third vertex) is: (in \(\mathbf{W m}^{-2}\) )

1 Zero
2 \(\sqrt{2}\)
3 2
4 4
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WAVE OPTICS

283270 Two coherent sources whose intensity ratio is \(64: 1\) produce interference fringes. The ratio of intensities of maxima and minima is

1 \(4: 7\)
2 \(8: 1\)
3 \(81: 49\)
4 \(81: 7\)
WAVE OPTICS

283271 Two slits, separated by a distance of \(1 \mathrm{~mm}\) are illuminated with red light of wavelength
\(6.5 \times 10^{-7} \mathrm{~m}\). The interference fringes are observed on a screen placed \(1 \mathrm{~m}\) from the slits. The distance of the third dark fringe from the central fringe will be equal to

1 \(0.65 \mathrm{~mm}\)
2 \(1.30 \mathrm{~mm}\)
3 \(1.62 \mathrm{~mm}\)
4 \(1.95 \mathrm{~mm}\)
WAVE OPTICS

283272 The interference pattern is obtained with two coherent light sources of intensity ratio \(n\). In the interference pattern, the ratio \(\frac{I_{\max }-I_{\text {min }}}{I_{\max }+I_{\text {min }}}\) will be

1 \(\frac{\sqrt{\mathrm{n}}}{\mathrm{n}+1}\)
2 \(\frac{2 \sqrt{\mathrm{n}}}{\mathrm{n}+1}\)
3 \(\frac{\sqrt{\mathrm{n}}}{(\mathrm{n}+1)^2}\)
4 \(\frac{2 \sqrt{n}}{(n+1)^2}\)
WAVE OPTICS

283276 Two coherent monochromatic light sources are located at two vertices of an equilateral triangle. If the intensity due to each of the sources independently is \(1 \mathrm{Wm}^{-2}\) at the third vertex, the resultant intensity due to both the sources at the point (i.e., at the third vertex) is: (in \(\mathbf{W m}^{-2}\) )

1 Zero
2 \(\sqrt{2}\)
3 2
4 4
WAVE OPTICS

283270 Two coherent sources whose intensity ratio is \(64: 1\) produce interference fringes. The ratio of intensities of maxima and minima is

1 \(4: 7\)
2 \(8: 1\)
3 \(81: 49\)
4 \(81: 7\)
WAVE OPTICS

283271 Two slits, separated by a distance of \(1 \mathrm{~mm}\) are illuminated with red light of wavelength
\(6.5 \times 10^{-7} \mathrm{~m}\). The interference fringes are observed on a screen placed \(1 \mathrm{~m}\) from the slits. The distance of the third dark fringe from the central fringe will be equal to

1 \(0.65 \mathrm{~mm}\)
2 \(1.30 \mathrm{~mm}\)
3 \(1.62 \mathrm{~mm}\)
4 \(1.95 \mathrm{~mm}\)
WAVE OPTICS

283272 The interference pattern is obtained with two coherent light sources of intensity ratio \(n\). In the interference pattern, the ratio \(\frac{I_{\max }-I_{\text {min }}}{I_{\max }+I_{\text {min }}}\) will be

1 \(\frac{\sqrt{\mathrm{n}}}{\mathrm{n}+1}\)
2 \(\frac{2 \sqrt{\mathrm{n}}}{\mathrm{n}+1}\)
3 \(\frac{\sqrt{\mathrm{n}}}{(\mathrm{n}+1)^2}\)
4 \(\frac{2 \sqrt{n}}{(n+1)^2}\)
WAVE OPTICS

283276 Two coherent monochromatic light sources are located at two vertices of an equilateral triangle. If the intensity due to each of the sources independently is \(1 \mathrm{Wm}^{-2}\) at the third vertex, the resultant intensity due to both the sources at the point (i.e., at the third vertex) is: (in \(\mathbf{W m}^{-2}\) )

1 Zero
2 \(\sqrt{2}\)
3 2
4 4
WAVE OPTICS

283270 Two coherent sources whose intensity ratio is \(64: 1\) produce interference fringes. The ratio of intensities of maxima and minima is

1 \(4: 7\)
2 \(8: 1\)
3 \(81: 49\)
4 \(81: 7\)
WAVE OPTICS

283271 Two slits, separated by a distance of \(1 \mathrm{~mm}\) are illuminated with red light of wavelength
\(6.5 \times 10^{-7} \mathrm{~m}\). The interference fringes are observed on a screen placed \(1 \mathrm{~m}\) from the slits. The distance of the third dark fringe from the central fringe will be equal to

1 \(0.65 \mathrm{~mm}\)
2 \(1.30 \mathrm{~mm}\)
3 \(1.62 \mathrm{~mm}\)
4 \(1.95 \mathrm{~mm}\)
WAVE OPTICS

283272 The interference pattern is obtained with two coherent light sources of intensity ratio \(n\). In the interference pattern, the ratio \(\frac{I_{\max }-I_{\text {min }}}{I_{\max }+I_{\text {min }}}\) will be

1 \(\frac{\sqrt{\mathrm{n}}}{\mathrm{n}+1}\)
2 \(\frac{2 \sqrt{\mathrm{n}}}{\mathrm{n}+1}\)
3 \(\frac{\sqrt{\mathrm{n}}}{(\mathrm{n}+1)^2}\)
4 \(\frac{2 \sqrt{n}}{(n+1)^2}\)
WAVE OPTICS

283276 Two coherent monochromatic light sources are located at two vertices of an equilateral triangle. If the intensity due to each of the sources independently is \(1 \mathrm{Wm}^{-2}\) at the third vertex, the resultant intensity due to both the sources at the point (i.e., at the third vertex) is: (in \(\mathbf{W m}^{-2}\) )

1 Zero
2 \(\sqrt{2}\)
3 2
4 4
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