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For simple harmonic vibrations y(1)=8c...

For simple harmonic vibrations
`y_(1)=8cos omegat`
`y_(2)=4 cos (omegat+(pi)/(2))`
`y_(3)=2cos (omegat+pi)`
`y_(4)=cos(omegat+(3pi)/(2))` are superimposed on one another. The resulting amplitude and phase are respectively

A

`sqrt(45) and tan^(-1)((1)/(2))`

B

`sqrt(45) and tan^(-1)((1)/(3))`

C

`sqrt(75) and tan^(-1)(2)`

D

`sqrt(75) and tan^(-1)((1)/(3))`

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To solve the problem of finding the resulting amplitude and phase of the superimposed simple harmonic vibrations given by: 1. \( y_1 = 8 \cos(\omega t) \) 2. \( y_2 = 4 \cos\left(\omega t + \frac{\pi}{2}\right) \) 3. \( y_3 = 2 \cos\left(\omega t + \pi\right) \) 4. \( y_4 = \cos\left(\omega t + \frac{3\pi}{2}\right) \) we will follow these steps: ### Step 1: Identify the Amplitudes and Phases - For \( y_1 \): Amplitude \( A_1 = 8 \), Phase \( \phi_1 = 0 \) - For \( y_2 \): Amplitude \( A_2 = 4 \), Phase \( \phi_2 = \frac{\pi}{2} \) - For \( y_3 \): Amplitude \( A_3 = 2 \), Phase \( \phi_3 = \pi \) - For \( y_4 \): Amplitude \( A_4 = 1 \), Phase \( \phi_4 = \frac{3\pi}{2} \) ### Step 2: Convert to Phasor Representation We can represent these amplitudes and phases as vectors (phasors) in the complex plane: - \( y_1 \) corresponds to the vector \( 8 \) at angle \( 0 \) - \( y_2 \) corresponds to the vector \( 4 \) at angle \( \frac{\pi}{2} \) - \( y_3 \) corresponds to the vector \( -2 \) at angle \( \pi \) - \( y_4 \) corresponds to the vector \( -1 \) at angle \( \frac{3\pi}{2} \) ### Step 3: Calculate the Resultant Amplitude To find the resultant amplitude, we need to add these vectors. We will first calculate the x and y components of each vector: - For \( y_1 \): - \( x_1 = 8 \) - \( y_1 = 0 \) - For \( y_2 \): - \( x_2 = 0 \) - \( y_2 = 4 \) - For \( y_3 \): - \( x_3 = -2 \) - \( y_3 = 0 \) - For \( y_4 \): - \( x_4 = 0 \) - \( y_4 = -1 \) Now, summing the components: - Total \( x \) component: \[ X = x_1 + x_2 + x_3 + x_4 = 8 + 0 - 2 + 0 = 6 \] - Total \( y \) component: \[ Y = y_1 + y_2 + y_3 + y_4 = 0 + 4 + 0 - 1 = 3 \] ### Step 4: Calculate the Resultant Amplitude The resultant amplitude \( A \) can be calculated using the Pythagorean theorem: \[ A = \sqrt{X^2 + Y^2} = \sqrt{6^2 + 3^2} = \sqrt{36 + 9} = \sqrt{45} = 3\sqrt{5} \] ### Step 5: Calculate the Phase Angle The phase angle \( \phi \) can be calculated using: \[ \tan(\phi) = \frac{Y}{X} = \frac{3}{6} = \frac{1}{2} \] Thus, \[ \phi = \tan^{-1}\left(\frac{1}{2}\right) \] ### Final Result The resulting amplitude and phase are: - Amplitude: \( 3\sqrt{5} \) - Phase: \( \tan^{-1}\left(\frac{1}{2}\right) \)
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