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On the superposition of the two waves gi...

On the superposition of the two waves given as `y_1=A_0 sin( omegat-kx)` and `y_2=A_0 cos ( omega t -kx+(pi)/6)` , the resultant amplitude of oscillations will be

A

`sqrt(3)A_0`

B

`(A_0)/(2) `

C

`A_0`

D

`(3)/(2)A_0`

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To find the resultant amplitude of the superposition of the two waves given by \( y_1 = A_0 \sin(\omega t - kx) \) and \( y_2 = A_0 \cos(\omega t - kx + \frac{\pi}{6}) \), we can follow these steps: ### Step 1: Convert \( y_1 \) to cosine form We can express \( y_1 \) in terms of cosine: \[ y_1 = A_0 \sin(\omega t - kx) = A_0 \cos\left(\frac{\pi}{2} - (\omega t - kx)\right) = A_0 \cos\left(\omega t - kx + \frac{\pi}{2}\right) \] This gives us: \[ y_1 = A_0 \cos\left(\omega t - kx + \frac{\pi}{2}\right) \] ### Step 2: Identify the phases Now we can identify the phases of the two waves: - For \( y_1 \), the phase \( \phi_1 = \omega t - kx + \frac{\pi}{2} \) - For \( y_2 \), the phase \( \phi_2 = \omega t - kx + \frac{\pi}{6} \) ### Step 3: Calculate the phase difference Next, we calculate the phase difference \( \Delta \phi = \phi_2 - \phi_1 \): \[ \Delta \phi = \left(\omega t - kx + \frac{\pi}{6}\right) - \left(\omega t - kx + \frac{\pi}{2}\right) = \frac{\pi}{6} - \frac{\pi}{2} \] Converting \( \frac{\pi}{2} \) to sixths: \[ \frac{\pi}{2} = \frac{3\pi}{6} \] Thus, \[ \Delta \phi = \frac{\pi}{6} - \frac{3\pi}{6} = -\frac{2\pi}{6} = -\frac{\pi}{3} \] ### Step 4: Calculate the resultant amplitude Using the formula for the resultant amplitude of two waves with equal amplitudes \( A_0 \) and a phase difference \( \Delta \phi \): \[ A_{resultant} = \sqrt{A_0^2 + A_0^2 + 2A_0A_0 \cos(\Delta \phi)} \] Substituting \( \Delta \phi = -\frac{\pi}{3} \): \[ A_{resultant} = \sqrt{A_0^2 + A_0^2 + 2A_0^2 \cos\left(-\frac{\pi}{3}\right)} \] Since \( \cos(-\theta) = \cos(\theta) \): \[ \cos\left(-\frac{\pi}{3}\right) = \cos\left(\frac{\pi}{3}\right) = \frac{1}{2} \] Thus, \[ A_{resultant} = \sqrt{A_0^2 + A_0^2 + 2A_0^2 \cdot \frac{1}{2}} = \sqrt{A_0^2 + A_0^2 + A_0^2} = \sqrt{3A_0^2} = A_0 \sqrt{3} \] ### Final Result The resultant amplitude of oscillations is: \[ A_{resultant} = A_0 \sqrt{3} \]
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