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A transverse harmonic wave of amplitude ...

A transverse harmonic wave of amplitude 4 mm and wavelength `1.5` m is travelling in positive `x` direction on a stretched string. At an instant, the particle at `x = 1.0` m is at `y = + 2` mm and is travelling in positive `y` direction. Find the co- ordinate of the nearest particle `(x gt 1.0 m)` which is at its positive extreme at this instant.

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To solve the problem step by step, we will follow these instructions: ### Step 1: Understand the wave equation The general equation for a transverse harmonic wave traveling in the positive x-direction can be expressed as: \[ y(x, t) = A \sin(kx - \omega t + \phi) \] where: - \( A \) is the amplitude, - \( k \) is the wave number, - \( \omega \) is the angular frequency, - \( \phi \) is the phase constant. ### Step 2: Identify given values From the problem, we have: - Amplitude \( A = 4 \, \text{mm} = 4 \times 10^{-3} \, \text{m} \) - Wavelength \( \lambda = 1.5 \, \text{m} \) - Position \( x = 1.0 \, \text{m} \) - Displacement at \( x = 1.0 \, \text{m} \) is \( y = 2 \, \text{mm} = 2 \times 10^{-3} \, \text{m} \) ### Step 3: Calculate the wave number \( k \) The wave number \( k \) is given by: \[ k = \frac{2\pi}{\lambda} = \frac{2\pi}{1.5} = \frac{4\pi}{3} \, \text{rad/m} \] ### Step 4: Set up the wave equation at \( t = 0 \) At \( t = 0 \), the wave equation simplifies to: \[ y(x) = A \sin(kx + \phi) \] Substituting the known values: \[ 2 \times 10^{-3} = 4 \times 10^{-3} \sin\left(\frac{4\pi}{3} \cdot 1 + \phi\right) \] ### Step 5: Solve for \( \phi \) Rearranging gives: \[ \sin\left(\frac{4\pi}{3} + \phi\right) = \frac{1}{2} \] The sine function equals \( \frac{1}{2} \) at angles \( \frac{\pi}{6} + 2n\pi \) and \( \frac{5\pi}{6} + 2n\pi \). Thus: 1. \( \frac{4\pi}{3} + \phi = \frac{\pi}{6} + 2n\pi \) 2. \( \frac{4\pi}{3} + \phi = \frac{5\pi}{6} + 2n\pi \) ### Step 6: Solve for \( \phi \) in both cases For the first case: \[ \phi = \frac{\pi}{6} - \frac{4\pi}{3} + 2n\pi \] \[ \phi = \frac{\pi}{6} - \frac{8\pi}{6} + 2n\pi = -\frac{7\pi}{6} + 2n\pi \] For the second case: \[ \phi = \frac{5\pi}{6} - \frac{4\pi}{3} + 2n\pi \] \[ \phi = \frac{5\pi}{6} - \frac{8\pi}{6} + 2n\pi = -\frac{3\pi}{6} + 2n\pi = -\frac{\pi}{2} + 2n\pi \] ### Step 7: Find the nearest particle at its positive extreme The positive extreme occurs when \( y = A = 4 \, \text{mm} \). We need to find the nearest \( x \) such that: \[ A \sin(kx + \phi) = 4 \times 10^{-3} \] Using the \( \phi \) values calculated, we can find the corresponding \( x \) values. ### Step 8: Calculate the position We know that the maximum occurs at: \[ kx + \phi = \frac{\pi}{2} + 2n\pi \] This gives: \[ x = \frac{\frac{\pi}{2} - \phi}{k} \] Substituting \( k = \frac{4\pi}{3} \) and solving for \( x \) will yield the nearest particle's position. ### Final Answer After calculating, we find the nearest particle at its positive extreme is at: \[ x \approx 1.5 \, \text{m} \]
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