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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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The correct Answer is:
To solve the problem, we need to find the phase difference between two points in a stationary wave and a traveling wave, and then calculate the ratio of these phase differences. ### Step 1: Identify the wave equations The stationary wave is given by: \[ y_1 = \sin(kx) \cos(\omega t) \] The traveling wave is given by: \[ y_2 = a \sin(\omega t - kx) \] ### Step 2: Determine the positions We have two positions: - \( x_1 = \frac{\pi}{3k} \) - \( x_2 = \frac{3\pi}{2k} \) ### Step 3: Calculate the phase difference in the stationary wave (\( \phi_1 \)) For the stationary wave, the phase at \( x_1 \) is: \[ \phi_1(x_1) = kx_1 = k \left(\frac{\pi}{3k}\right) = \frac{\pi}{3} \] For the stationary wave at \( x_2 \): \[ \phi_1(x_2) = kx_2 = k \left(\frac{3\pi}{2k}\right) = \frac{3\pi}{2} \] Now, the phase difference \( \phi_1 \) between these two points in the stationary wave is: \[ \phi_1 = \phi_1(x_2) - \phi_1(x_1) = \frac{3\pi}{2} - \frac{\pi}{3} \] To subtract these fractions, we need a common denominator: - The common denominator of 2 and 3 is 6. Converting the fractions: \[ \frac{3\pi}{2} = \frac{9\pi}{6} \] \[ \frac{\pi}{3} = \frac{2\pi}{6} \] Now, substituting back: \[ \phi_1 = \frac{9\pi}{6} - \frac{2\pi}{6} = \frac{7\pi}{6} \] ### Step 4: Calculate the phase difference in the traveling wave (\( \phi_2 \)) For the traveling wave, the phase difference \( \phi_2 \) is given by: \[ \phi_2 = k \Delta x \] where \( \Delta x = x_2 - x_1 \). Calculating \( \Delta x \): \[ \Delta x = \frac{3\pi}{2k} - \frac{\pi}{3k} \] Finding a common denominator (which is 6k): \[ \Delta x = \frac{9\pi}{6k} - \frac{2\pi}{6k} = \frac{7\pi}{6k} \] Now substituting into the phase difference formula: \[ \phi_2 = k \Delta x = k \left(\frac{7\pi}{6k}\right) = \frac{7\pi}{6} \] ### Step 5: Calculate the ratio \( \frac{\phi_1}{\phi_2} \) Now we can find the ratio of the phase differences: \[ \frac{\phi_1}{\phi_2} = \frac{\frac{7\pi}{6}}{\frac{7\pi}{6}} = 1 \] ### Final Answer The ratio \( \frac{\phi_1}{\phi_2} \) is: \[ \frac{\phi_1}{\phi_2} = 1 \] ---

To solve the problem, we need to find the phase difference between two points in a stationary wave and a traveling wave, and then calculate the ratio of these phase differences. ### Step 1: Identify the wave equations The stationary wave is given by: \[ y_1 = \sin(kx) \cos(\omega t) \] The traveling wave is given by: \[ y_2 = a \sin(\omega t - kx) \] ...
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Knowledge Check

  • Equations of a stationery and a travelling waves are y_(1)=a sin kx cos omegat and y_(2)=a sin (omegat-kx) The phase differences between two between x_(1)=(pi)/(3k) and x_(2)=(3pi)/(2k) are phi_(1) and phi_(2) respectvely for the two waves. The ratio (phi_(1))/(phi_(2)) is

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    D
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    `pi//4`
    B
    `pi`
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    `pi//8`
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    `pi//2`
  • Two waves are represented by Y_1=a_1 cos (omegat-kx) and Y-2 =a_2 sin (omegat-kx+pi//3) Then the phase difference between them is-

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