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An undamped oscillator has period ro = 1 second. When weak
Chapter 5, Problem 5.29(choose chapter or problem)
An undamped oscillator has period \(\tau_{\mathrm{o}}=1\) second. When weak damping is added, it is found that the amplitude of oscillation drops by 50% in one period \(\tau_{1}\). (The period of the damped oscillations is defined as the time between successive maxima, \(\tau_{1}=2 \pi / \omega_{1}\). See Problem 5.25.) How big is \(\beta\) compared to \(\omega_{0}\)? What is \(\tau_{1}\)?
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QUESTION:
An undamped oscillator has period \(\tau_{\mathrm{o}}=1\) second. When weak damping is added, it is found that the amplitude of oscillation drops by 50% in one period \(\tau_{1}\). (The period of the damped oscillations is defined as the time between successive maxima, \(\tau_{1}=2 \pi / \omega_{1}\). See Problem 5.25.) How big is \(\beta\) compared to \(\omega_{0}\)? What is \(\tau_{1}\)?
ANSWER:Step 1 of 4
The expression for the period of an undamped oscillator in terms of the natural frequency of the undamped oscillator is,
\( {\tau _o} = \frac{{2\pi }}{{{\omega _o}}} \)
The period of the undamped oscillator is \({\tau _o} = 1\;{\rm{s}}\). Thus, the equation becomes as:
\(\frac{{2\pi }}{{{\omega _o}}} = 1\;{\rm{s}}\;\;\;\;...\;\left( 1 \right)\)
Here, \({\omega _o}\) is the natural frequency of the undamped oscillator.
The expression for the period of the damped oscillator in terms of the damped oscillator is,
\({\tau _1} = \frac{{2\pi }}{{{\omega _1}}}\;\;\;\;\;\;\;...\;\left( 2 \right)\)
Here, \({\omega _1}\) is the frequency of the damped oscillator.
The frequency of the damped oscillator is,
\({\omega _1} = \sqrt {\omega _o^2 - {\beta ^2}} \)
Here, \(\beta\) is the damping constant.
Substitute \(\sqrt {\omega _o^2 - {\beta ^2}}\) for \({\omega _1}\) in the equation (2).
\({\tau _1} = \frac{{2\pi }}{{\sqrt {\omega _o^2 - {\beta ^2}} }}\;\;\;\;\;\;\;\;...\;\left( 3 \right)\)
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