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Sounds from two identical sources `S_(1)` and `S_(2)` reach a point `P`. When the sounds reach directly, and in the same phase, the intensity at `P` is `I_(0)`. The power of `S_(1)` is now reduced by `64%` and the phase difference between `S_(1)` and `S_(2)` is varied continuously. The maximum and minimum intensities recorded at `P` are now `I_("max")` and `I_("min")`

A

`I_(max) = 0.64 I_(0)`

B

`I_(min) = 0.36 I_(0)`

C

`(I_(max))/(I_(min)) = 16`

D

`(I_(max))/(I_(min)) = (1.64)/(0.36)`

Text Solution

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To solve the problem, we need to determine the maximum and minimum intensities at point P when the power of source S1 is reduced by 64% and the phase difference between S1 and S2 is varied continuously. ### Step-by-Step Solution: 1. **Understanding Initial Conditions:** - When both sources S1 and S2 are in phase, the intensity at point P is given as \( I_0 \). - Since both sources are identical, we can denote their amplitudes as \( A \). 2. **Calculating Initial Intensity:** - The intensity \( I_0 \) when both sources are in phase is given by: \[ I_0 = k (A + A)^2 = k (2A)^2 = 4kA^2 \] - Here, \( k \) is a constant that relates intensity to amplitude. 3. **Power Reduction of Source S1:** - The power of S1 is reduced by 64%. Therefore, the remaining power is 36% of the original. - Since power is proportional to the square of the amplitude, the new amplitude \( A' \) of S1 can be calculated as: \[ A' = A \sqrt{0.36} = 0.6A \] 4. **New Amplitudes:** - The amplitude of S2 remains \( A \). - The new amplitudes are: - For S1: \( A' = 0.6A \) - For S2: \( A = A \) 5. **Calculating Maximum Intensity:** - The maximum intensity occurs when the waves from S1 and S2 are in phase. The resultant amplitude \( A_{max} \) is: \[ A_{max} = A + A' = A + 0.6A = 1.6A \] - The maximum intensity \( I_{max} \) is then: \[ I_{max} = k (A_{max})^2 = k (1.6A)^2 = 2.56kA^2 \] 6. **Calculating Minimum Intensity:** - The minimum intensity occurs when the waves from S1 and S2 are out of phase. The resultant amplitude \( A_{min} \) is: \[ A_{min} = A - A' = A - 0.6A = 0.4A \] - The minimum intensity \( I_{min} \) is then: \[ I_{min} = k (A_{min})^2 = k (0.4A)^2 = 0.16kA^2 \] 7. **Finding the Ratios:** - We can express \( I_{max} \) and \( I_{min} \) in terms of \( I_0 \): \[ I_0 = 4kA^2 \] - Thus, \[ I_{max} = 2.56kA^2 = \frac{2.56}{4} I_0 = 0.64 I_0 \] \[ I_{min} = 0.16kA^2 = \frac{0.16}{4} I_0 = 0.04 I_0 \] ### Final Results: - The maximum intensity \( I_{max} = 0.64 I_0 \) - The minimum intensity \( I_{min} = 0.04 I_0 \)

To solve the problem, we need to determine the maximum and minimum intensities at point P when the power of source S1 is reduced by 64% and the phase difference between S1 and S2 is varied continuously. ### Step-by-Step Solution: 1. **Understanding Initial Conditions:** - When both sources S1 and S2 are in phase, the intensity at point P is given as \( I_0 \). - Since both sources are identical, we can denote their amplitudes as \( A \). ...
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