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The equation of a simple harmonic motion...

The equation of a simple harmonic motion of a particle is `(d^(2)x)/(dt^(2)) + 0.2 (dx)/(dt) + 36x = 0`. Its time period is approximately

A

`(pi)/(2) sec`

B

`(pi)/(4) sec`

C

`(pi)/(3) sec`

D

`(pi)/(6)sec`

Text Solution

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The correct Answer is:
To find the time period of the simple harmonic motion described by the equation \[ \frac{d^2x}{dt^2} + 0.2 \frac{dx}{dt} + 36x = 0, \] we can follow these steps: ### Step 1: Identify the coefficients The given equation can be compared to the standard form of a damped harmonic oscillator: \[ \frac{d^2x}{dt^2} + \frac{y}{m} \frac{dx}{dt} + \frac{k}{m} x = 0. \] From the equation, we can identify: - \(y = 0.2\) - \(k = 36\) ### Step 2: Calculate \(\omega^2\) and \(\beta\) From the standard form, we know: - \(\omega^2 = \frac{k}{m}\) - \(\beta = \frac{y}{2m}\) We need to find \(\omega\) and \(\beta\). However, we don't have \(m\) explicitly, but we can express \(\omega\) in terms of \(k\) and \(m\). Given: \[ \omega^2 = 36 \implies \omega = \sqrt{36} = 6. \] Next, we can find \(\beta\): \[ \beta = \frac{0.2}{2m}. \] ### Step 3: Determine the time period The time period \(T\) of the oscillation is given by the formula: \[ T = \frac{2\pi}{\omega}. \] Substituting the value of \(\omega\): \[ T = \frac{2\pi}{6} = \frac{\pi}{3}. \] ### Conclusion Thus, the time period of the simple harmonic motion is approximately: \[ T \approx \frac{\pi}{3} \text{ seconds}. \]
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Knowledge Check

  • If a simple harmonic motion is represented by (d^(2)x)/(dt^(2)) + alphax = 0 , its time period is :

    A
    `(2pi)/(alpha)`
    B
    `(2pi)/(sqrt(alpha))`
    C
    `2pialpha`
    D
    `2pisqrt(alpha)`
  • If a simple harmonic motion is represented by (d^(2)x)/(dt^(2)) + alphax = 0 , its time period is :

    A
    `(2pi)/(alpha)`
    B
    `(2pi)/(sqrt(alpha))`
    C
    `2pialpha`
    D
    `2pisqrt(alpha)`
  • The equation of a damped simple harmonic motion is 2m(d^(2)x)/(dt^(2))+2a_(0)(dx)/(dt)+kx=0 . Then the angualr frequency of oscillation is

    A
    `omega=((k)/(m)-(a_(0)^(2))/(2m^(2)))^(1//2)`
    B
    `omega=((k)/(m)-(a_(0))/(4m))^(1//2)`
    C
    `omega=((k)/(2m)-(a_(0)^(2))/(4m^(2)))^(1//2)`
    D
    `omega=((k)/(m)-(a_(0)^(2))/(4m^(2)))^(1//2)`
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