Polarization of Light
WAVE OPTICS

283623 A ray of light is incident at an angle \(i\) on a glass slab of refractive index \(\mu\). The angle between reflected and refracted light is \(90^{\circ}\). Then, the relationship between \(i\) and \(\mu\) is

1 \(\mathrm{i}=\tan -1\left(\frac{1}{\mu}\right)\)
2 \(\tan \mathrm{i}=\mu\)
3 \(\sin \mathrm{i}=\mu\)
4 \(\cos \mathrm{i}=\mu\)
WAVE OPTICS

283561 Two rays of light \(A\) and \(B\) are falling on a glass slab at the angles of incidence \(45^{\circ}\) and \(60^{\circ}\). If the reflected ray of \(A\) is partially polarized and that of \(B\) is completely polarized, then the refractive index of glass is

1 1.33
2 1.414
3 1.5
4 1.65
5 1.732
WAVE OPTICS

283565 If \(\theta_P\) is the polarizing angle for a glass plate of refractive index \(\mu\) and critical angle \(\theta_{\mathrm{C}}\) then

1 \(\theta_{\mathrm{p}}=\theta_{\mathrm{C}}\)
2 \(\tan \theta \cdot \sin \theta_{\mathrm{C}}=1\)
3 \(\theta_{\mathrm{p}} \theta_{\mathrm{C}}=1\)
4 \(\tan \theta_{\mathrm{p}}=\sin \theta_{\mathrm{C}}\)
5 \(\tan \theta_{\mathrm{p}} \sin \theta_{\mathrm{C}}=\mu\)
WAVE OPTICS

283577 Light is incident on a polarizer with intensity \(I_0\). A second prism called analyzer is kept at an angle of \(15^0\), from the first polarizer then the intensity of final emergent light will be :

1 \(0.46 \mathrm{I}_0\)
2 \(0.56 \mathrm{I}_0\)
3 \(0.66 \mathrm{I}_0\)
4 \(0.76 \mathrm{I}_0\)
WAVE OPTICS

283580 The refractive index \(\mu\) and the polarizing angle \(\theta_{\mathrm{p}}\) of a medium are related as

1 \(\theta_{\mathrm{p}}=\sin ^{-1}(\mu)\)
2 \(\theta_{\mathrm{p}}=\tan ^{-1}(\mu)\)
3 \(\theta_{\mathrm{P}}=\sin ^{-1}\left(\frac{1}{\mu}\right)\)
4 \(\theta_{\mathrm{P}}=\tan ^{-1}\left(\frac{1}{\mu}\right)\)
WAVE OPTICS

283623 A ray of light is incident at an angle \(i\) on a glass slab of refractive index \(\mu\). The angle between reflected and refracted light is \(90^{\circ}\). Then, the relationship between \(i\) and \(\mu\) is

1 \(\mathrm{i}=\tan -1\left(\frac{1}{\mu}\right)\)
2 \(\tan \mathrm{i}=\mu\)
3 \(\sin \mathrm{i}=\mu\)
4 \(\cos \mathrm{i}=\mu\)
WAVE OPTICS

283561 Two rays of light \(A\) and \(B\) are falling on a glass slab at the angles of incidence \(45^{\circ}\) and \(60^{\circ}\). If the reflected ray of \(A\) is partially polarized and that of \(B\) is completely polarized, then the refractive index of glass is

1 1.33
2 1.414
3 1.5
4 1.65
5 1.732
WAVE OPTICS

283565 If \(\theta_P\) is the polarizing angle for a glass plate of refractive index \(\mu\) and critical angle \(\theta_{\mathrm{C}}\) then

1 \(\theta_{\mathrm{p}}=\theta_{\mathrm{C}}\)
2 \(\tan \theta \cdot \sin \theta_{\mathrm{C}}=1\)
3 \(\theta_{\mathrm{p}} \theta_{\mathrm{C}}=1\)
4 \(\tan \theta_{\mathrm{p}}=\sin \theta_{\mathrm{C}}\)
5 \(\tan \theta_{\mathrm{p}} \sin \theta_{\mathrm{C}}=\mu\)
WAVE OPTICS

283577 Light is incident on a polarizer with intensity \(I_0\). A second prism called analyzer is kept at an angle of \(15^0\), from the first polarizer then the intensity of final emergent light will be :

1 \(0.46 \mathrm{I}_0\)
2 \(0.56 \mathrm{I}_0\)
3 \(0.66 \mathrm{I}_0\)
4 \(0.76 \mathrm{I}_0\)
WAVE OPTICS

283580 The refractive index \(\mu\) and the polarizing angle \(\theta_{\mathrm{p}}\) of a medium are related as

1 \(\theta_{\mathrm{p}}=\sin ^{-1}(\mu)\)
2 \(\theta_{\mathrm{p}}=\tan ^{-1}(\mu)\)
3 \(\theta_{\mathrm{P}}=\sin ^{-1}\left(\frac{1}{\mu}\right)\)
4 \(\theta_{\mathrm{P}}=\tan ^{-1}\left(\frac{1}{\mu}\right)\)
WAVE OPTICS

283623 A ray of light is incident at an angle \(i\) on a glass slab of refractive index \(\mu\). The angle between reflected and refracted light is \(90^{\circ}\). Then, the relationship between \(i\) and \(\mu\) is

1 \(\mathrm{i}=\tan -1\left(\frac{1}{\mu}\right)\)
2 \(\tan \mathrm{i}=\mu\)
3 \(\sin \mathrm{i}=\mu\)
4 \(\cos \mathrm{i}=\mu\)
WAVE OPTICS

283561 Two rays of light \(A\) and \(B\) are falling on a glass slab at the angles of incidence \(45^{\circ}\) and \(60^{\circ}\). If the reflected ray of \(A\) is partially polarized and that of \(B\) is completely polarized, then the refractive index of glass is

1 1.33
2 1.414
3 1.5
4 1.65
5 1.732
WAVE OPTICS

283565 If \(\theta_P\) is the polarizing angle for a glass plate of refractive index \(\mu\) and critical angle \(\theta_{\mathrm{C}}\) then

1 \(\theta_{\mathrm{p}}=\theta_{\mathrm{C}}\)
2 \(\tan \theta \cdot \sin \theta_{\mathrm{C}}=1\)
3 \(\theta_{\mathrm{p}} \theta_{\mathrm{C}}=1\)
4 \(\tan \theta_{\mathrm{p}}=\sin \theta_{\mathrm{C}}\)
5 \(\tan \theta_{\mathrm{p}} \sin \theta_{\mathrm{C}}=\mu\)
WAVE OPTICS

283577 Light is incident on a polarizer with intensity \(I_0\). A second prism called analyzer is kept at an angle of \(15^0\), from the first polarizer then the intensity of final emergent light will be :

1 \(0.46 \mathrm{I}_0\)
2 \(0.56 \mathrm{I}_0\)
3 \(0.66 \mathrm{I}_0\)
4 \(0.76 \mathrm{I}_0\)
WAVE OPTICS

283580 The refractive index \(\mu\) and the polarizing angle \(\theta_{\mathrm{p}}\) of a medium are related as

1 \(\theta_{\mathrm{p}}=\sin ^{-1}(\mu)\)
2 \(\theta_{\mathrm{p}}=\tan ^{-1}(\mu)\)
3 \(\theta_{\mathrm{P}}=\sin ^{-1}\left(\frac{1}{\mu}\right)\)
4 \(\theta_{\mathrm{P}}=\tan ^{-1}\left(\frac{1}{\mu}\right)\)
NEET Test Series from KOTA - 10 Papers In MS WORD WhatsApp Here
WAVE OPTICS

283623 A ray of light is incident at an angle \(i\) on a glass slab of refractive index \(\mu\). The angle between reflected and refracted light is \(90^{\circ}\). Then, the relationship between \(i\) and \(\mu\) is

1 \(\mathrm{i}=\tan -1\left(\frac{1}{\mu}\right)\)
2 \(\tan \mathrm{i}=\mu\)
3 \(\sin \mathrm{i}=\mu\)
4 \(\cos \mathrm{i}=\mu\)
WAVE OPTICS

283561 Two rays of light \(A\) and \(B\) are falling on a glass slab at the angles of incidence \(45^{\circ}\) and \(60^{\circ}\). If the reflected ray of \(A\) is partially polarized and that of \(B\) is completely polarized, then the refractive index of glass is

1 1.33
2 1.414
3 1.5
4 1.65
5 1.732
WAVE OPTICS

283565 If \(\theta_P\) is the polarizing angle for a glass plate of refractive index \(\mu\) and critical angle \(\theta_{\mathrm{C}}\) then

1 \(\theta_{\mathrm{p}}=\theta_{\mathrm{C}}\)
2 \(\tan \theta \cdot \sin \theta_{\mathrm{C}}=1\)
3 \(\theta_{\mathrm{p}} \theta_{\mathrm{C}}=1\)
4 \(\tan \theta_{\mathrm{p}}=\sin \theta_{\mathrm{C}}\)
5 \(\tan \theta_{\mathrm{p}} \sin \theta_{\mathrm{C}}=\mu\)
WAVE OPTICS

283577 Light is incident on a polarizer with intensity \(I_0\). A second prism called analyzer is kept at an angle of \(15^0\), from the first polarizer then the intensity of final emergent light will be :

1 \(0.46 \mathrm{I}_0\)
2 \(0.56 \mathrm{I}_0\)
3 \(0.66 \mathrm{I}_0\)
4 \(0.76 \mathrm{I}_0\)
WAVE OPTICS

283580 The refractive index \(\mu\) and the polarizing angle \(\theta_{\mathrm{p}}\) of a medium are related as

1 \(\theta_{\mathrm{p}}=\sin ^{-1}(\mu)\)
2 \(\theta_{\mathrm{p}}=\tan ^{-1}(\mu)\)
3 \(\theta_{\mathrm{P}}=\sin ^{-1}\left(\frac{1}{\mu}\right)\)
4 \(\theta_{\mathrm{P}}=\tan ^{-1}\left(\frac{1}{\mu}\right)\)
WAVE OPTICS

283623 A ray of light is incident at an angle \(i\) on a glass slab of refractive index \(\mu\). The angle between reflected and refracted light is \(90^{\circ}\). Then, the relationship between \(i\) and \(\mu\) is

1 \(\mathrm{i}=\tan -1\left(\frac{1}{\mu}\right)\)
2 \(\tan \mathrm{i}=\mu\)
3 \(\sin \mathrm{i}=\mu\)
4 \(\cos \mathrm{i}=\mu\)
WAVE OPTICS

283561 Two rays of light \(A\) and \(B\) are falling on a glass slab at the angles of incidence \(45^{\circ}\) and \(60^{\circ}\). If the reflected ray of \(A\) is partially polarized and that of \(B\) is completely polarized, then the refractive index of glass is

1 1.33
2 1.414
3 1.5
4 1.65
5 1.732
WAVE OPTICS

283565 If \(\theta_P\) is the polarizing angle for a glass plate of refractive index \(\mu\) and critical angle \(\theta_{\mathrm{C}}\) then

1 \(\theta_{\mathrm{p}}=\theta_{\mathrm{C}}\)
2 \(\tan \theta \cdot \sin \theta_{\mathrm{C}}=1\)
3 \(\theta_{\mathrm{p}} \theta_{\mathrm{C}}=1\)
4 \(\tan \theta_{\mathrm{p}}=\sin \theta_{\mathrm{C}}\)
5 \(\tan \theta_{\mathrm{p}} \sin \theta_{\mathrm{C}}=\mu\)
WAVE OPTICS

283577 Light is incident on a polarizer with intensity \(I_0\). A second prism called analyzer is kept at an angle of \(15^0\), from the first polarizer then the intensity of final emergent light will be :

1 \(0.46 \mathrm{I}_0\)
2 \(0.56 \mathrm{I}_0\)
3 \(0.66 \mathrm{I}_0\)
4 \(0.76 \mathrm{I}_0\)
WAVE OPTICS

283580 The refractive index \(\mu\) and the polarizing angle \(\theta_{\mathrm{p}}\) of a medium are related as

1 \(\theta_{\mathrm{p}}=\sin ^{-1}(\mu)\)
2 \(\theta_{\mathrm{p}}=\tan ^{-1}(\mu)\)
3 \(\theta_{\mathrm{P}}=\sin ^{-1}\left(\frac{1}{\mu}\right)\)
4 \(\theta_{\mathrm{P}}=\tan ^{-1}\left(\frac{1}{\mu}\right)\)