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A transverse wave is described by the eq...

A transverse wave is described by the equation
`y=y_(0)sin4pi(upsilont-(x)/(lambda))`.
The maximum particle velocity is equal to four times the wave velocity if

A

`lambda=piy_(0)//4`

B

`lambda=2piy_(0)`

C

`lambda=pi//y_(0)`

D

`lambda=piy_(0)`

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The correct Answer is:
To solve the problem, we need to analyze the given wave equation and derive the necessary relationships between the maximum particle velocity and the wave velocity. ### Step-by-Step Solution: 1. **Identify the Wave Equation:** The given wave equation is: \[ y = y_0 \sin\left(4\pi\left(\nu t - \frac{x}{\lambda}\right)\right) \] Here, \(y_0\) is the amplitude, \(\nu\) is the frequency, and \(\lambda\) is the wavelength. 2. **Determine Angular Frequency (\(\omega\)) and Wave Number (\(k\)):** From the wave equation, we can identify: - Angular frequency \(\omega = 4\pi\nu\) - Wave number \(k = \frac{2\pi}{\lambda}\) 3. **Calculate Wave Velocity (\(v\)):** The wave velocity \(v\) can be calculated using the formula: \[ v = \frac{\omega}{k} \] Substituting the values of \(\omega\) and \(k\): \[ v = \frac{4\pi\nu}{\frac{2\pi}{\lambda}} = 2\nu\lambda \] 4. **Find the Particle Velocity:** The particle velocity \(v_p\) is the rate of change of displacement with respect to time. We find it by differentiating \(y\) with respect to \(t\): \[ v_p = \frac{\partial y}{\partial t} = y_0 \cdot \frac{\partial}{\partial t}\left(\sin(4\pi(\nu t - \frac{x}{\lambda}))\right) \] Using the chain rule: \[ v_p = y_0 \cdot 4\pi\nu \cos(4\pi(\nu t - \frac{x}{\lambda})) \] 5. **Determine Maximum Particle Velocity (\(V_{max}\)):** The maximum particle velocity occurs when \(\cos(4\pi(\nu t - \frac{x}{\lambda})) = 1\): \[ V_{max} = y_0 \cdot 4\pi\nu \] 6. **Set Up the Relationship:** According to the problem, the maximum particle velocity is equal to four times the wave velocity: \[ V_{max} = 4v \] Substituting the expressions we derived: \[ y_0 \cdot 4\pi\nu = 4(2\nu\lambda) \] 7. **Simplify the Equation:** Simplifying the equation gives: \[ y_0 \cdot 4\pi\nu = 8\nu\lambda \] Dividing both sides by \(4\nu\) (assuming \(\nu \neq 0\)): \[ y_0 \pi = 2\lambda \] 8. **Final Result:** Rearranging gives: \[ \lambda = \frac{y_0 \pi}{2} \] ### Summary: The condition for the maximum particle velocity to be equal to four times the wave velocity is: \[ \lambda = \frac{y_0 \pi}{2} \]
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