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The polaroids P(1), P(2) & P(3) are arra...

The polaroids `P_(1), P_(2) & P_(3)` are arranged coaxially. The angle between `P_(1)` and `P_(2)` is `37^(@)`. The angle between `P_(2)` and `P_(3)` is, if intensity of emerging light is a quarter of intensity of unploarized light

A

`theta = cos^(-1) ((5)/(4))`

B

`theta = cos^(-1) ((4)/(5))`

C

`theta = cos^(-1) ((4)/(5sqrt(2)))`

D

`theta = cos^(-1)((5)/(4sqrt(2)))`

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To solve the problem involving three polaroids arranged coaxially, we will apply Malus's Law, which relates the intensity of polarized light transmitted through a polaroid to the angle between the light's polarization direction and the polaroid's axis. ### Step-by-Step Solution 1. **Understanding the Initial Setup**: - We have three polaroids: P1, P2, and P3. - The angle between P1 and P2 is given as \(37^\circ\). - The light incident on P1 is unpolarized. 2. **Intensity After P1**: - When unpolarized light passes through the first polaroid (P1), the intensity of the transmitted light is halved. - Therefore, if \(I_0\) is the intensity of the unpolarized light incident on P1, the intensity after P1 (\(I_1\)) is: \[ I_1 = \frac{I_0}{2} \] 3. **Intensity After P2**: - The intensity after passing through P2 can be calculated using Malus's Law: \[ I_2 = I_1 \cdot \cos^2(\theta) \] - Here, \(\theta\) is the angle between P1 and P2, which is \(37^\circ\). - Substituting the values: \[ I_2 = \frac{I_0}{2} \cdot \cos^2(37^\circ) \] 4. **Calculating \(\cos^2(37^\circ)\)**: - We know that \(\cos(37^\circ) \approx 0.8\) (exact value is \(\frac{4}{5}\)). - Therefore: \[ \cos^2(37^\circ) = \left(\frac{4}{5}\right)^2 = \frac{16}{25} \] - Now substituting this back into the equation for \(I_2\): \[ I_2 = \frac{I_0}{2} \cdot \frac{16}{25} = \frac{16 I_0}{50} = \frac{8 I_0}{25} \] 5. **Intensity After P3**: - We know that the intensity of the emerging light from the system is given as a quarter of the initial intensity: \[ I_3 = \frac{I_0}{4} \] - Using Malus's Law again for P3: \[ I_3 = I_2 \cdot \cos^2(\phi) \] - Here, \(\phi\) is the angle between P2 and P3, which we need to find. 6. **Setting Up the Equation**: - We can equate the two expressions for \(I_3\): \[ \frac{I_0}{4} = \frac{8 I_0}{25} \cdot \cos^2(\phi) \] - Canceling \(I_0\) from both sides: \[ \frac{1}{4} = \frac{8}{25} \cdot \cos^2(\phi) \] 7. **Solving for \(\cos^2(\phi)\)**: - Rearranging gives: \[ \cos^2(\phi) = \frac{25}{32} \] 8. **Finding \(\phi\)**: - Taking the square root: \[ \cos(\phi) = \sqrt{\frac{25}{32}} = \frac{5}{\sqrt{32}} = \frac{5}{4\sqrt{2}} \] - Finally, to find \(\phi\): \[ \phi = \cos^{-1}\left(\frac{5}{4\sqrt{2}}\right) \] ### Final Answer The angle between P2 and P3 is \(\phi = \cos^{-1}\left(\frac{5}{4\sqrt{2}}\right)\).

To solve the problem involving three polaroids arranged coaxially, we will apply Malus's Law, which relates the intensity of polarized light transmitted through a polaroid to the angle between the light's polarization direction and the polaroid's axis. ### Step-by-Step Solution 1. **Understanding the Initial Setup**: - We have three polaroids: P1, P2, and P3. - The angle between P1 and P2 is given as \(37^\circ\). - The light incident on P1 is unpolarized. ...
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