Approximating Damped Oscillator Time Period and Frequency with Large n

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Homework Help Overview

The discussion revolves around the time period and frequency of a damped oscillator, particularly focusing on approximations when the number of oscillations, n, is large. The original poster presents a problem involving the relationship between the time periods and frequencies of damped and undamped oscillators, with specific equations provided for analysis.

Discussion Character

  • Exploratory, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants explore the derivation of the time period ratio and frequency ratio for a damped oscillator. There are attempts to clarify the mathematical approximations involved, particularly regarding the square root and the behavior of functions as n becomes large.

Discussion Status

Some participants have provided clarifications on the approximations used in the derivations, particularly for part (a). There is ongoing exploration of how these approximations apply to part (b), with suggestions to apply similar reasoning. The discussion reflects a collaborative effort to understand the mathematical relationships without reaching a consensus on the final approach.

Contextual Notes

Participants are working under the assumption that n is a large number, which influences the approximations being discussed. The original poster expresses uncertainty about the application of known approximations, indicating a need for further exploration of the concepts involved.

Allan McPherson
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Homework Statement



An oscillator when undamped has a time period T0, while its time period when damped. Suppose after n oscillations the amplitude of the damped oscillator drops to 1/e of its original value (value at t = 0).

(a) Assuming that n is a large number, show that $$\frac{T}{T_0}=\left (1+\frac{1}{4n^2\pi^2}\right) \approx 1 + \frac{1}{8n^2\pi^2}$$
(b) Assuming that n is a large number, show that $$\frac{\omega}{\omega_0} \approx 1 - \frac{1}{8n^2\pi^2}$$

Homework Equations


$$x(t) = A e^{-\gamma t}cos(\omega t + \phi)$$
$$T = \frac{2 \pi}{\omega}$$
$$\omega = \sqrt{\omega_0^2 - \gamma^2}$$

The Attempt at a Solution


[/B]
I've managed to get the equality for both parts. We want $$\frac{A}{e} = A e^{-\gamma t}cos(\omega t + \phi)$$
which is only true if
##\gamma n T = 1,## ##\omega n T = 2n\pi## and ##\phi = 2m\pi##​
which implies $$T = \frac{1}{\gamma n} = \frac{2\pi}{\omega}$$
So $$\omega_0 = \gamma\sqrt{1 + 4n^2\pi^2}$$
And
$$\frac{T}{T_0} = \frac{\omega_0}{\omega}=\frac{\gamma\sqrt{1+4n^2\pi^2}}{2n\pi\gamma}$$ $$=\frac{\sqrt{1+4n^2\pi^2}}{4n^2\pi^2} = \left ( 1 + \frac{1}{4n^2\pi^2} \right )^{1/2}$$
The answer to part (b) will clearly involve taking the inverse of the right-hand side of the equality and applying the same or a similar approximation.

I know I've seen this approximation before, but I can't for the life of me remember how it works. l would appreciate any help that can be offered.
 
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Allan McPherson said:

Homework Statement



An oscillator when undamped has a time period T0, while its time period when damped ?. Suppose after n oscillations the amplitude of the damped oscillator drops to 1/e of its original value (value at t = 0).

(a) Assuming that n is a large number, show that $$\frac{T}{T_0}=\left (1+\frac{1}{4n^2\pi^2}\right) \approx 1 + \frac{1}{8n^2\pi^2}$$
You miss a square root:
$$\frac{T}{T_0}=\sqrt{\left (1+\frac{1}{4n^2\pi^2}\right)} \approx 1 + \frac{1}{8n^2\pi^2}$$

If x << 1,
##\sqrt{1+x}=\sqrt{(1+x/2)^2-(x/2)^2 }\approx \sqrt{(1+x/2)^2}=1+x/2##

Also ##\frac{1}{1+x}## is the sum of the geometric series 1-x+x^2-x^3+..., approximately 1-x if x << 1.
 
Allan McPherson said:
$$=\frac{\sqrt{1+4n^2\pi^2}}{4n^2\pi^2} = \left ( 1 + \frac{1}{4n^2\pi^2} \right )^{1/2}$$
You meant
$$=\sqrt{\frac{1+4n^2\pi^2}{4n^2\pi^2}} = \left ( 1 + \frac{1}{4n^2\pi^2} \right )^{1/2}$$
 
Thank you. That clarifies the approximation for part (a). I'm not sure how that helps with part (b), though.

For part (b) I have $$\frac{\omega}{\omega_0} = \frac{2n\pi}{\sqrt{1+4n^2\pi^2}} = \sqrt{\frac{4n^2\pi^2}{1+4n^2\pi^2}} = \sqrt{1 - \frac{1}{4n^2\pi^2}}$$
 
Last edited:
Allan McPherson said:
Thank you. That clarifies the approximation for part (a). I'm not sure how that helps with part (b), though.

For part (b) I have $$\frac{\omega}{\omega_0} = \frac{2n\pi}{\sqrt{1+4n^2\pi^2}} = \sqrt{\frac{4n^2\pi^2}{1+4n^2\pi^2}} = \sqrt{1 - \frac{1}{4n^2\pi^2}}$$
Let be ##x=-\frac{1}{4n^2\pi^2}## . |x|<<1, apply the approxiamation for the square root as in Post #2.
 
Last edited:
Right. Looking at that again, I'm not sure how I thought that could be right. Thank you for your help.
 

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