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MHT CET 202623 AprilEvening Shift
Exam
MHT CET
Year
2026
Date
23 April
Shift
Evening Shift
Subject
Physics
Chapter
Wave Optics

MHT CET 2026 · 23 April · Evening Shift · Physics · Wave Optics

Two coherent sources of intensity ratio α interfere. In...

Two coherent sources of intensity ratio α\alpha interfere. In interference pattern, \dfrac{I_\max-I_\min}{I_\max+I_\min} is

Options

  1. A2α1+α\dfrac{2\alpha}{1+\alpha}
  2. B2α1+α\dfrac{2\sqrt{\alpha}}{1+\alpha}
  3. C2α1+α\dfrac{2\alpha}{1+\sqrt{\alpha}}
  4. D1+α2α\dfrac{1+\alpha}{2\alpha}

Correct answer

B. 2α1+α\dfrac{2\sqrt{\alpha}}{1+\alpha}

Step-by-step solution

Let the intensities of the two coherent sources be I1I_1 and I2I_2.

Given the intensity ratio I1I2=α\dfrac{I_1}{I_2} = \alpha.

The maximum intensity in the interference pattern is given by:

I_\max = (\sqrt{I_1} + \sqrt{I_2})^2 = I_1 + I_2 + 2\sqrt{I_1 I_2}

The minimum intensity is given by:

I_\min = (\sqrt{I_1} - \sqrt{I_2})^2 = I_1 + I_2 - 2\sqrt{I_1 I_2}

Calculating the difference and sum of the maximum and minimum intensities:

I_\max - I_\min = 4\sqrt{I_1 I_2}

I_\max + I_\min = 2(I_1 + I_2)

Taking the ratio of these two quantities:

\dfrac{I_\max-I_\min}{I_\max+I_\min} = \dfrac{4\sqrt{I_1 I_2}}{2(I_1 + I_2)} = \dfrac{2\sqrt{I_1 I_2}}{I_1 + I_2}

Dividing the numerator and the denominator by I2I_2:

\dfrac{I_\max-I_\min}{I_\max+I_\min} = \dfrac{2\sqrt{\dfrac{I_1}{I_2}}}{\dfrac{I_1}{I_2} + 1}

Substituting I1I2=α\dfrac{I_1}{I_2} = \alpha:

\dfrac{I_\max-I_\min}{I_\max+I_\min} = \dfrac{2\sqrt{\alpha}}{\alpha + 1}

Answer: 2α1+α\dfrac{2\sqrt{\alpha}}{1+\alpha}
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