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The displacement of a progressive wave i...

The displacement of a progressive wave is represented by `y=Asin(omegat-kx)` where x is distance and t is time. The dimensions of `(omega)/(k)` are same as those of

A

velocity

B

wave number

C

wavelength

D

frequency

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To solve the question, we need to analyze the given equation for the displacement of a progressive wave, which is represented as: \[ y = A \sin(\omega t - kx) \] where: - \( y \) is the displacement, - \( A \) is the amplitude, - \( \omega \) is the angular frequency, - \( k \) is the wave number, - \( x \) is the distance, - \( t \) is the time. We are asked to find the dimensions of the ratio \( \frac{\omega}{k} \) and determine what physical quantity it corresponds to. ### Step 1: Understand the terms involved The term \( \omega t - kx \) must be dimensionless because it represents an angle in the sine function. This means that the dimensions of \( \omega t \) must equal the dimensions of \( kx \). ### Step 2: Find the dimensions of \( \omega \) The angular frequency \( \omega \) is defined as: \[ \omega = \frac{2\pi}{T} \] where \( T \) is the time period. Thus, the dimensions of \( \omega \) can be expressed as: \[ [\omega] = [T]^{-1} = T^{-1} \] ### Step 3: Find the dimensions of \( k \) The wave number \( k \) is defined as: \[ k = \frac{2\pi}{\lambda} \] where \( \lambda \) is the wavelength. The dimensions of \( k \) can be expressed as: \[ [k] = [\lambda]^{-1} = L^{-1} \] ### Step 4: Calculate the dimensions of \( \frac{\omega}{k} \) Now we can find the dimensions of the ratio \( \frac{\omega}{k} \): \[ \frac{\omega}{k} = \frac{T^{-1}}{L^{-1}} = T^{-1} \cdot L = \frac{L}{T} \] ### Step 5: Identify the physical quantity The dimensions \( \frac{L}{T} \) correspond to the dimensions of velocity. Therefore, we conclude that: \[ \frac{\omega}{k} \text{ has the same dimensions as velocity.} \] ### Final Answer The dimensions of \( \frac{\omega}{k} \) are the same as those of velocity. ---

To solve the question, we need to analyze the given equation for the displacement of a progressive wave, which is represented as: \[ y = A \sin(\omega t - kx) \] where: - \( y \) is the displacement, - \( A \) is the amplitude, - \( \omega \) is the angular frequency, ...
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