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Equations of a stationary and a travelling waves are as follows `y_(1) = sin kx cos omega t` and `y_(2) = a sin ( omega t - kx)`. The phase difference between two points `x_(1) = pi//3k` and `x_(2) = 3 pi// 2k is phi_(1)` in the standing wave `(y_(1))` and is `phi_(2)` in the travelling wave `(y_(2))` then ratio `phi_(1)//phi_(2)` is

A

`1`

B

`5//6`

C

`3//4`

D

`6//7`

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To solve the problem, we need to find the phase differences \(\phi_1\) and \(\phi_2\) for the standing wave \(y_1\) and the travelling wave \(y_2\) at the specified positions \(x_1\) and \(x_2\). Then, we will calculate the ratio \(\frac{\phi_1}{\phi_2}\). ### Step 1: Identify the equations of the waves The equations of the waves are given as: - Standing wave: \(y_1 = \sin(kx) \cos(\omega t)\) - Travelling wave: \(y_2 = a \sin(\omega t - kx)\) ### Step 2: Determine the phase of the standing wave at \(x_1\) and \(x_2\) The phase of the standing wave \(y_1\) at position \(x\) is given by: \[ \phi_1 = kx \] For \(x_1 = \frac{\pi}{3k}\): \[ \phi_1(x_1) = k \left(\frac{\pi}{3k}\right) = \frac{\pi}{3} \] For \(x_2 = \frac{3\pi}{2k}\): \[ \phi_1(x_2) = k \left(\frac{3\pi}{2k}\right) = \frac{3\pi}{2} \] ### Step 3: Calculate the phase difference \(\phi_1\) The phase difference \(\phi_1\) between the two points in the standing wave is: \[ \Delta \phi_1 = \phi_1(x_2) - \phi_1(x_1) = \frac{3\pi}{2} - \frac{\pi}{3} \] To subtract these fractions, we need a common denominator. The least common multiple of 2 and 3 is 6: \[ \Delta \phi_1 = \frac{9\pi}{6} - \frac{2\pi}{6} = \frac{7\pi}{6} \] ### Step 4: Determine the phase of the travelling wave at \(x_1\) and \(x_2\) The phase of the travelling wave \(y_2\) at position \(x\) is given by: \[ \phi_2 = \omega t - kx \] At \(x_1\): \[ \phi_2(x_1) = \omega t - k\left(\frac{\pi}{3k}\right) = \omega t - \frac{\pi}{3} \] At \(x_2\): \[ \phi_2(x_2) = \omega t - k\left(\frac{3\pi}{2k}\right) = \omega t - \frac{3\pi}{2} \] ### Step 5: Calculate the phase difference \(\phi_2\) The phase difference \(\phi_2\) between the two points in the travelling wave is: \[ \Delta \phi_2 = \phi_2(x_2) - \phi_2(x_1) = \left(\omega t - \frac{3\pi}{2}\right) - \left(\omega t - \frac{\pi}{3}\right) \] This simplifies to: \[ \Delta \phi_2 = -\frac{3\pi}{2} + \frac{\pi}{3} \] Again, we need a common denominator (6): \[ \Delta \phi_2 = -\frac{9\pi}{6} + \frac{2\pi}{6} = -\frac{7\pi}{6} \] ### Step 6: Calculate the ratio \(\frac{\phi_1}{\phi_2}\) Now we can find the ratio of the phase differences: \[ \frac{\Delta \phi_1}{\Delta \phi_2} = \frac{\frac{7\pi}{6}}{-\frac{7\pi}{6}} = -1 \] ### Final Answer Thus, the ratio \(\frac{\phi_1}{\phi_2}\) is: \[ \frac{\phi_1}{\phi_2} = 1 \]

To solve the problem, we need to find the phase differences \(\phi_1\) and \(\phi_2\) for the standing wave \(y_1\) and the travelling wave \(y_2\) at the specified positions \(x_1\) and \(x_2\). Then, we will calculate the ratio \(\frac{\phi_1}{\phi_2}\). ### Step 1: Identify the equations of the waves The equations of the waves are given as: - Standing wave: \(y_1 = \sin(kx) \cos(\omega t)\) - Travelling wave: \(y_2 = a \sin(\omega t - kx)\) ### Step 2: Determine the phase of the standing wave at \(x_1\) and \(x_2\) ...
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