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A detector at x=0 receives waves from th...

A detector at `x=0` receives waves from three sources each of amplitude `A` and frequencies `f + 2,f` and `f-2`.
The equation of waves are : `y_(1)=A sin[2 pi(f+2),y_(2)=A sin 2 pift` and `y_(3)=A sin[2pi (f-2)t]`. The time at which intensity is minimum is

A

`t=0,1//4,1//2,3//4,…sec`

B

`t=1//6,1//3,2//3,5//6,…sec`

C

`t=0,1//2,3//2,5//2,..sec`

D

`t=1//2,1//4,1//6,1//8,…sec`

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To find the time at which the intensity is minimum when three waves are received at a detector, we can follow these steps: ### Step 1: Write the equations of the waves The equations of the waves from the three sources are given as: - \( y_1 = A \sin(2 \pi (f + 2)t) \) - \( y_2 = A \sin(2 \pi ft) \) - \( y_3 = A \sin(2 \pi (f - 2)t) \) ### Step 2: Combine the wave equations The total displacement \( y \) at the detector is the sum of the individual wave displacements: \[ y = y_1 + y_2 + y_3 = A \sin(2 \pi (f + 2)t) + A \sin(2 \pi ft) + A \sin(2 \pi (f - 2)t) \] ### Step 3: Use the sine addition formula We can use the sine addition formula to combine the waves. The formula states: \[ \sin A + \sin B = 2 \sin\left(\frac{A + B}{2}\right) \cos\left(\frac{A - B}{2}\right) \] We can group the terms as follows: \[ y = A \left( \sin(2 \pi (f + 2)t) + \sin(2 \pi (f - 2)t) \right) + A \sin(2 \pi ft) \] Using the sine addition formula on the first two terms: \[ y = A \left( 2 \sin\left(2 \pi ft\right) \cos(2 \pi t) \right) + A \sin(2 \pi ft) \] This simplifies to: \[ y = 2A \sin(2 \pi ft) \cos(2 \pi t) + A \sin(2 \pi ft) \] ### Step 4: Factor out common terms Factoring out \( \sin(2 \pi ft) \): \[ y = A \sin(2 \pi ft) (2 \cos(2 \pi t) + 1) \] ### Step 5: Find the intensity The intensity \( I \) is proportional to the square of the amplitude: \[ I \propto y^2 = A^2 \sin^2(2 \pi ft) (2 \cos(2 \pi t) + 1)^2 \] To find the minimum intensity, we need to find when \( (2 \cos(2 \pi t) + 1)^2 \) is minimum. ### Step 6: Set the expression to zero The expression \( (2 \cos(2 \pi t) + 1) = 0 \) gives: \[ 2 \cos(2 \pi t) + 1 = 0 \implies \cos(2 \pi t) = -\frac{1}{2} \] ### Step 7: Solve for \( t \) The cosine function is equal to \(-\frac{1}{2}\) at: \[ 2 \pi t = \frac{2\pi}{3} + 2\pi n \quad \text{and} \quad 2 \pi t = \frac{4\pi}{3} + 2\pi n \] Solving for \( t \): \[ t = \frac{1}{3} + n \quad \text{and} \quad t = \frac{2}{3} + n \] Where \( n \) is any integer. ### Step 8: Conclusion The times at which the intensity is minimum are: \[ t = \frac{1}{3}, \frac{2}{3}, \frac{5}{6}, \ldots \]

To find the time at which the intensity is minimum when three waves are received at a detector, we can follow these steps: ### Step 1: Write the equations of the waves The equations of the waves from the three sources are given as: - \( y_1 = A \sin(2 \pi (f + 2)t) \) - \( y_2 = A \sin(2 \pi ft) \) - \( y_3 = A \sin(2 \pi (f - 2)t) \) ...
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