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A beam of unpolarised light of intensity...

A beam of unpolarised light of intensity `I_(0)` is passed through a polaroid "A" and then through another polaroid "B" which is oriented so that its principal plane makes an angle of `45^(@)` relative to that of "A" .The intensity of emergent light is:

A

`I_(0)//2`

B

`I_(0)//8`

C

`I_(0)`

D

`I_(0)//4`

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The correct Answer is:
To solve the problem, we will follow these steps: ### Step 1: Understanding the Initial Conditions We have a beam of unpolarized light with an intensity \( I_0 \) passing through two polaroids, A and B. The polaroid A will polarize the light, and then polaroid B will further modify the intensity based on its orientation. **Hint:** Remember that unpolarized light has equal intensity in all directions, and a polaroid only allows light oscillating in its principal plane to pass through. ### Step 2: Applying Malus's Law for Polaroid A When unpolarized light passes through the first polaroid (A), the intensity of the light that emerges is given by: \[ I_A = \frac{I_0}{2} \] This is because a polaroid reduces the intensity of unpolarized light by half. **Hint:** Malus's Law states that the intensity of polarized light after passing through a polaroid is proportional to the cosine square of the angle between the light's polarization direction and the polaroid's axis. ### Step 3: Applying Malus's Law for Polaroid B Now, the light emerging from polaroid A is polarized. When this light passes through the second polaroid (B), which is oriented at an angle of \( 45^\circ \) to the first polaroid, we apply Malus's Law again: \[ I_B = I_A \cdot \cos^2(\theta) \] where \( \theta = 45^\circ \). Substituting the value from step 2: \[ I_B = \frac{I_0}{2} \cdot \cos^2(45^\circ) \] **Hint:** Remember that \( \cos(45^\circ) = \frac{1}{\sqrt{2}} \). ### Step 4: Calculating \( \cos^2(45^\circ) \) Calculating \( \cos^2(45^\circ) \): \[ \cos^2(45^\circ) = \left(\frac{1}{\sqrt{2}}\right)^2 = \frac{1}{2} \] **Hint:** Squaring the cosine value will give you the fraction of intensity that passes through the second polaroid. ### Step 5: Final Calculation of Intensity Now substituting back into the equation for \( I_B \): \[ I_B = \frac{I_0}{2} \cdot \frac{1}{2} = \frac{I_0}{4} \] **Hint:** This final result shows how much of the original intensity remains after passing through both polaroids. ### Conclusion The intensity of the emergent light after passing through both polaroids is: \[ \boxed{\frac{I_0}{4}} \]
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