Relationship between period and time in oscillators

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SUMMARY

The discussion focuses on the relationship between the period and frequency of weakly damped oscillators. It establishes that if the amplitude of a weakly damped oscillator decreases to 1/e of its initial value after n periods, the frequency of the oscillator is approximately [1 − (8π²n²)⁻¹] times the frequency of an undamped oscillator with the same natural frequency. Key equations include x(t) = Ae⁻ᵝᵗcos(ω₁t - δ) and ω₁ = sqrt(ωₒ² - ᵝ²), which are critical for understanding the behavior of damped oscillators.

PREREQUISITES
  • Understanding of weakly damped harmonic oscillators
  • Familiarity with the equations of motion for oscillators
  • Knowledge of natural frequency and decay constant
  • Basic grasp of angular frequency and its relationship to period
NEXT STEPS
  • Study the derivation of the equation x(t) = Ae⁻ᵝᵗcos(ω₁t - δ)
  • Learn about the implications of the decay constant (β) in oscillator behavior
  • Explore the relationship between angular frequency (ω₁) and period (T) in detail
  • Investigate the effects of damping on the frequency of oscillators in various physical systems
USEFUL FOR

Students and professionals in physics, particularly those studying oscillatory motion, as well as engineers involved in designing systems with oscillatory behavior, will benefit from this discussion.

Vitani11
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Homework Statement


If the amplitude of a weakly damped oscillator decreased to 1/e of its initial value after n periods, show that the frequency of the oscillator must be approximately [1 − (8π2n2)-1] times the frequency of an undamped oscillator with the same natural frequency.

Homework Equations


The equation for a weakly damped harmonic oscillator is x(t) =Ae-βtcos(ω1t-δ) where ω1 = sqrt(ωo22)
A = amplitude
β = decay constant
ω1 = period for damped oscillator
ωo = natural frequency
T = period
t = time
δ = phase angle

The Attempt at a Solution


Since the amplitude was initially Ae-βt and finally 1/e, I solved for t=1/β or β=1/t. I then took the equation ω1 = sqrt(ωo22) and did an expansion to the second term which gave me that ω1o(1-β2/2ωo2). Ridding of β2 for 1/t gives me ω1o(1-1/2ωo2t2). I can then replace ωo with 2πn/T and then I would almost have the correct answer, but for that t= T which doesn't make sense. Also as an aside do I not have to include the phase angle (so I can make it zero) since I'm not measuring the oscillator in reference to another one? Or is it there due to impedance or something?
 
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You're introducing ##n## in the wrong place. If ##1/\beta## is the time for ##n## periods, you can say ##1/\beta = n(2\pi/\omega_1)##.
 
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Okay, can you explain why that is?
 
How are the angular frequency of the damped oscillator ##\omega_1## and the period ##T## related?
 

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