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The amplitude of polarised light transmi...

The amplitude of polarised light transmitted through a polariser is A. The amplitude of unpolarised light incident on it is

A

`A//2`

B

`A//sqrt(2)`

C

`2A`

D

`sqrt(2)A`

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The correct Answer is:
To find the amplitude of the unpolarized light incident on a polarizer that transmits polarized light with an amplitude \( A \), we can follow these steps: ### Step-by-Step Solution 1. **Understanding the Relationship Between Intensity and Amplitude**: - The intensity \( I \) of a wave is proportional to the square of its amplitude \( A \). This can be expressed mathematically as: \[ I \propto A^2 \] 2. **Intensity of Unpolarized Light**: - When unpolarized light passes through a polarizer, only half of its intensity is transmitted. If the intensity of the unpolarized light is \( I_0 \), the transmitted intensity \( I_t \) becomes: \[ I_t = \frac{I_0}{2} \] 3. **Relating Intensities to Amplitudes**: - Let \( A_0 \) be the amplitude of the unpolarized light incident on the polarizer, and \( A \) be the amplitude of the transmitted polarized light. According to the relationship between intensity and amplitude: \[ I_0 \propto A_0^2 \quad \text{and} \quad I_t \propto A^2 \] 4. **Setting Up the Equation**: - From the previous steps, we can write: \[ I_t = \frac{I_0}{2} \implies A^2 = \frac{A_0^2}{2} \] 5. **Substituting the Intensities**: - Since \( I_t = A^2 \) and \( I_0 = A_0^2 \), we can substitute: \[ A^2 = \frac{A_0^2}{2} \] 6. **Solving for the Amplitude of the Incident Light**: - Rearranging gives: \[ A_0^2 = 2A^2 \] - Taking the square root of both sides, we find: \[ A_0 = \sqrt{2} A \] ### Final Answer The amplitude of the unpolarized light incident on the polarizer is: \[ A_0 = \sqrt{2} A \] ---

To find the amplitude of the unpolarized light incident on a polarizer that transmits polarized light with an amplitude \( A \), we can follow these steps: ### Step-by-Step Solution 1. **Understanding the Relationship Between Intensity and Amplitude**: - The intensity \( I \) of a wave is proportional to the square of its amplitude \( A \). This can be expressed mathematically as: \[ I \propto A^2 ...
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