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Two monochromatic coherent point sources...

Two monochromatic coherent point sources `S_(1)` and `S_(2)` are separated by a distance L. Each sources emits light of wavelength `lambda`, where `L gt gt lambda`. The line `S_(1) S_(2)` when extended meets a screen perpendicular to it at point A. Then

A

the interference fringe on the screen are straight lines shape

B

the interference fringes on the screen are strainght lines perpendicular to the line `S_(1) S_(2) A`

C

point A is an intensity maxima if `L = n lambda`

D

point A is always an intensity maxima for any separation L

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To solve the problem, we need to analyze the interference pattern created by two coherent point sources \( S_1 \) and \( S_2 \) separated by a distance \( L \) and emitting light of wavelength \( \lambda \). ### Step-by-Step Solution: 1. **Understanding the Setup**: - We have two coherent sources \( S_1 \) and \( S_2 \) separated by a distance \( L \). - A screen is placed perpendicular to the line joining the two sources, and it meets the line at point \( A \). 2. **Path Difference**: - For any point on the screen, the light waves from \( S_1 \) and \( S_2 \) will travel different distances to reach that point. - The path difference \( \Delta r \) between the two waves arriving at point \( A \) can be expressed as: \[ \Delta r = r_2 - r_1 \] where \( r_1 \) and \( r_2 \) are the distances from \( S_1 \) and \( S_2 \) to point \( A \), respectively. 3. **Condition for Constructive Interference**: - Constructive interference occurs when the path difference is an integer multiple of the wavelength: \[ \Delta r = n\lambda \quad (n = 0, 1, 2, \ldots) \] - This means that at points where this condition is satisfied, we will observe bright fringes. 4. **Condition for Destructive Interference**: - Destructive interference occurs when the path difference is a half-integer multiple of the wavelength: \[ \Delta r = (n + \frac{1}{2})\lambda \quad (n = 0, 1, 2, \ldots) \] - This means that at points where this condition is satisfied, we will observe dark fringes. 5. **Fringe Pattern**: - The interference pattern will consist of alternating bright and dark fringes on the screen. - Since \( L \) is much greater than \( \lambda \), the fringes will be closely spaced, and the pattern will be approximately linear. 6. **Maxima and Minima**: - The point \( A \) can be considered as a point of maximum intensity if the path difference \( \Delta r \) at that point satisfies the condition for constructive interference. - Specifically, if \( L = n\lambda \), then point \( A \) will be a maximum. ### Final Conclusion: - The interference fringes on the screen will be straight lines, and point \( A \) will be an intensity maximum if \( L \) is an integer multiple of \( \lambda \).

To solve the problem, we need to analyze the interference pattern created by two coherent point sources \( S_1 \) and \( S_2 \) separated by a distance \( L \) and emitting light of wavelength \( \lambda \). ### Step-by-Step Solution: 1. **Understanding the Setup**: - We have two coherent sources \( S_1 \) and \( S_2 \) separated by a distance \( L \). - A screen is placed perpendicular to the line joining the two sources, and it meets the line at point \( A \). ...
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