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Two choherent waves represented by y1 =...

Two choherent waves represented by `y_1 = A sin ((2pi x_1)/(lamda) - wt + pi/3) " and " y_2 = A sin ((2pi x_2)/(lamda) - wt + pi/6)` are superposed. The two waves will produce

A

Constructive interference at `(x_1-x_2) = 2lamda`

B

Constructive interference at`(x_1 - x_2) = (23 lamda)/(24)`

C

destructive interference at `(x_1 - x_2) = 1.5 lamda`

D

destructive interference `(x_1 - x_2) = (11 lamda)/(24)`

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To solve the problem involving the superposition of two coherent waves, we will follow these steps: ### Step 1: Identify the given waves The two coherent waves are given as: - \( y_1 = A \sin\left(\frac{2\pi x_1}{\lambda} - \omega t + \frac{\pi}{3}\right) \) - \( y_2 = A \sin\left(\frac{2\pi x_2}{\lambda} - \omega t + \frac{\pi}{6}\right) \) ### Step 2: Determine the phase difference The phase difference between the two waves can be calculated from their equations. The phase of \( y_1 \) is: - \( \phi_1 = \frac{2\pi x_1}{\lambda} - \omega t + \frac{\pi}{3} \) The phase of \( y_2 \) is: - \( \phi_2 = \frac{2\pi x_2}{\lambda} - \omega t + \frac{\pi}{6} \) The phase difference \( \Delta \phi \) is given by: \[ \Delta \phi = \phi_1 - \phi_2 = \left(\frac{2\pi x_1}{\lambda} - \omega t + \frac{\pi}{3}\right) - \left(\frac{2\pi x_2}{\lambda} - \omega t + \frac{\pi}{6}\right) \] This simplifies to: \[ \Delta \phi = \frac{2\pi (x_1 - x_2)}{\lambda} + \left(\frac{\pi}{3} - \frac{\pi}{6}\right) \] Calculating \( \frac{\pi}{3} - \frac{\pi}{6} \): \[ \frac{\pi}{3} - \frac{\pi}{6} = \frac{2\pi}{6} - \frac{\pi}{6} = \frac{\pi}{6} \] Thus, the phase difference becomes: \[ \Delta \phi = \frac{2\pi (x_1 - x_2)}{\lambda} + \frac{\pi}{6} \] ### Step 3: Determine the path difference The path difference \( \Delta x \) can be related to the phase difference by the formula: \[ \Delta \phi = \frac{2\pi \Delta x}{\lambda} \] Setting the two expressions for \( \Delta \phi \) equal gives: \[ \frac{2\pi (x_1 - x_2)}{\lambda} + \frac{\pi}{6} = \frac{2\pi \Delta x}{\lambda} \] Rearranging gives: \[ \Delta x = (x_1 - x_2) + \frac{\lambda}{12} \] ### Step 4: Analyze for constructive and destructive interference For constructive interference, the condition is: \[ \Delta \phi = 2n\pi \quad (n = 0, 1, 2, \ldots) \] For destructive interference, the condition is: \[ \Delta \phi = (2n - 1)\pi \quad (n = 0, 1, 2, \ldots) \] ### Step 5: Substitute and solve for \( n \) 1. **Constructive Interference**: \[ \frac{2\pi (x_1 - x_2)}{\lambda} + \frac{\pi}{6} = 2n\pi \] Rearranging gives: \[ \frac{2\pi (x_1 - x_2)}{\lambda} = 2n\pi - \frac{\pi}{6} \] Simplifying: \[ \frac{2(x_1 - x_2)}{\lambda} = 2n - \frac{1}{6} \] 2. **Destructive Interference**: \[ \frac{2\pi (x_1 - x_2)}{\lambda} + \frac{\pi}{6} = (2n - 1)\pi \] Rearranging gives: \[ \frac{2\pi (x_1 - x_2)}{\lambda} = (2n - 1)\pi - \frac{\pi}{6} \] Simplifying: \[ \frac{2(x_1 - x_2)}{\lambda} = 2n - 1 - \frac{1}{6} \] ### Conclusion The two coherent waves will produce regions of constructive and destructive interference based on the path difference and phase difference derived above.
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