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When sound wave of wavelength lambda is ...

When sound wave of wavelength `lambda` is propagating in a medium, the maximum velocity of the particle is equal to the wave velocity. The amplitude of wave is

A

`lambda`

B

`(lambda)/(2)`

C

`(lambda)/(2pi)`

D

`(lambda)/(4pi)`

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The correct Answer is:
To solve the problem, we need to find the amplitude of a sound wave given that the maximum velocity of the particle is equal to the wave velocity. Let's break down the solution step by step. ### Step 1: Understand the relationship between particle velocity and wave velocity The maximum velocity of a particle in a wave can be expressed as: \[ v_{p_{\text{max}}} = A \omega \] where: - \( A \) is the amplitude of the wave, - \( \omega \) is the angular frequency of the wave. ### Step 2: Express wave velocity in terms of wavelength and angular frequency The wave velocity \( v \) can be expressed in terms of wavelength \( \lambda \) and angular frequency \( \omega \) as: \[ v = \frac{\omega}{k} \] where \( k \) (the wave number) is given by: \[ k = \frac{2\pi}{\lambda} \] Thus, we can rewrite the wave velocity as: \[ v = \omega \cdot \frac{\lambda}{2\pi} \] ### Step 3: Set the maximum particle velocity equal to wave velocity According to the problem, we have: \[ v_{p_{\text{max}}} = v \] Substituting the expressions we derived: \[ A \omega = \frac{\omega \lambda}{2\pi} \] ### Step 4: Cancel out \( \omega \) from both sides Assuming \( \omega \neq 0 \), we can divide both sides of the equation by \( \omega \): \[ A = \frac{\lambda}{2\pi} \] ### Step 5: Conclusion Thus, the amplitude \( A \) of the wave is: \[ A = \frac{\lambda}{2\pi} \] Therefore, the correct answer is option **C: \( \frac{\lambda}{2\pi} \)**. ---
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