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A vibratory motion is represented by x=2...

A vibratory motion is represented by `x=2Acosomegat+Acos(omegat+(pi)/(2))+Acos(omegat+pi)+(A)/(2)cos(omegat+(3pi)/(2))`.
the resultant amplitude of the motion is

A

`(9A)/(2)`

B

`(sqrt(5)A)/(2)`

C

`(5A)/(2)`

D

2A

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To find the resultant amplitude of the given vibratory motion represented by \[ x = 2A \cos(\omega t) + A \cos\left(\omega t + \frac{\pi}{2}\right) + A \cos(\omega t + \pi) + \frac{A}{2} \cos\left(\omega t + \frac{3\pi}{2}\right), \] we can break down the expression step by step. ### Step 1: Rewrite the cosine terms using trigonometric identities 1. The term \( \cos\left(\omega t + \frac{\pi}{2}\right) \) can be rewritten as \( -\sin(\omega t) \). 2. The term \( \cos(\omega t + \pi) \) can be rewritten as \( -\cos(\omega t) \). 3. The term \( \cos\left(\omega t + \frac{3\pi}{2}\right) \) can be rewritten as \( \sin(\omega t) \). Substituting these identities into the equation gives: \[ x = 2A \cos(\omega t) + A(-\sin(\omega t)) + A(-\cos(\omega t)) + \frac{A}{2}\sin(\omega t) \] ### Step 2: Combine like terms Now, combine the terms involving \( \cos(\omega t) \) and \( \sin(\omega t) \): \[ x = (2A - A) \cos(\omega t) + \left(-A + \frac{A}{2}\right) \sin(\omega t) \] This simplifies to: \[ x = A \cos(\omega t) - \frac{A}{2} \sin(\omega t) \] ### Step 3: Express in terms of a single cosine function To express this in a single cosine function, we can use the phasor method. We can represent the coefficients of \( \cos(\omega t) \) and \( \sin(\omega t) \) as vectors. Let: - \( A_1 = A \) (the coefficient of \( \cos(\omega t) \)) - \( A_2 = -\frac{A}{2} \) (the coefficient of \( \sin(\omega t) \)) ### Step 4: Calculate the resultant amplitude The resultant amplitude \( R \) can be calculated using the Pythagorean theorem: \[ R = \sqrt{A_1^2 + A_2^2} \] Substituting the values: \[ R = \sqrt{A^2 + \left(-\frac{A}{2}\right)^2} \] Calculating \( R \): \[ R = \sqrt{A^2 + \frac{A^2}{4}} = \sqrt{A^2\left(1 + \frac{1}{4}\right)} = \sqrt{A^2 \cdot \frac{5}{4}} = A \sqrt{\frac{5}{4}} = \frac{A \sqrt{5}}{2} \] ### Final Result Thus, the resultant amplitude of the motion is: \[ \frac{A \sqrt{5}}{2} \]

To find the resultant amplitude of the given vibratory motion represented by \[ x = 2A \cos(\omega t) + A \cos\left(\omega t + \frac{\pi}{2}\right) + A \cos(\omega t + \pi) + \frac{A}{2} \cos\left(\omega t + \frac{3\pi}{2}\right), \] we can break down the expression step by step. ### Step 1: Rewrite the cosine terms using trigonometric identities 1. The term \( \cos\left(\omega t + \frac{\pi}{2}\right) \) can be rewritten as \( -\sin(\omega t) \). ...
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