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The displacement of a particle executing...

The displacement of a particle executing simple harmonic motion is given by `y=A_(0)+A sin omegat+B cos omegat`. Then the amplitude of its oscillation is given by

A

`A+B`

B

`A_(0)+sqrt(A^(2)+B^(2))`

C

`sqrt(A^(2)+B^(2))`

D

`sqrt(A_(0)^(2)+(A+B)^(2))`

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To find the amplitude of a particle executing simple harmonic motion given by the displacement equation \( y = A_0 + A \sin(\omega t) + B \cos(\omega t) \), we can follow these steps: ### Step-by-Step Solution: 1. **Identify the Components**: The displacement equation is given as: \[ y = A_0 + A \sin(\omega t) + B \cos(\omega t) \] Here, \( A_0 \) is a constant (the mean position), \( A \) is the coefficient of the sine term, and \( B \) is the coefficient of the cosine term. 2. **Recognize the Form of SHM**: The general form of simple harmonic motion can be expressed as: \[ y = A \sin(\omega t + \phi) \] where \( A \) is the amplitude and \( \phi \) is the phase angle. 3. **Combine the Sine and Cosine Terms**: We can express \( A \sin(\omega t) + B \cos(\omega t) \) as a single sinusoidal function. The resultant amplitude \( R \) can be calculated using the formula: \[ R = \sqrt{A^2 + B^2} \] 4. **Calculate the Resultant Amplitude**: Since the sine and cosine functions can be represented as a single sinusoidal function, we can ignore the constant \( A_0 \) when calculating the amplitude of the oscillation. Thus, the amplitude of the oscillation is: \[ \text{Amplitude} = \sqrt{A^2 + B^2} \] 5. **Final Result**: Therefore, the amplitude of the oscillation is given by: \[ \text{Amplitude} = \sqrt{A^2 + B^2} \]

To find the amplitude of a particle executing simple harmonic motion given by the displacement equation \( y = A_0 + A \sin(\omega t) + B \cos(\omega t) \), we can follow these steps: ### Step-by-Step Solution: 1. **Identify the Components**: The displacement equation is given as: \[ y = A_0 + A \sin(\omega t) + B \cos(\omega t) ...
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Knowledge Check

  • The displacement of a particle executing simple harmonic motion is given by y=A_(0)+Asinomegat+Bcosomegat Then the amplitude of its oscillation is given by :

    A
    `A_(0)+sqrt(A^(2)+B^(2))`
    B
    `sqrt(A^(2)+B^(2))`
    C
    `sqrt(A_(0)^(2)+(A+B)^(2))`
    D
    `A+B`
  • The instantaneous displacement x of a particle executing simple harmonic motion is given by x=a_1sinomegat+a_2cos(omegat+(pi)/(6)) . The amplitude A of oscillation is given by

    A
    `sqrt(a_1^2+a_2^2+2a_1a_2cos((pi)/(6)))`
    B
    `sqrt(a_1^2+a_2^2+2a_1a_2cos((pi)/(3)))`
    C
    `sqrt(a_1^2+a_2^2-2a_1a_2cos((pi)/(6)))`
    D
    `sqrt(a_1^2+a_2^2-2a_1a_2cos((pi)/(3)))`
  • A simple harmonic motion is represented by x(t) = sin^2 omegat - 2 cos^(2) omegat . The angular frequency of oscillation is given by

    A
    `omega`
    B
    `2 omega`
    C
    `4 omega`
    D
    `(omega)/2`
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