Physics 238—Intermediate Physics Lab
Homework Assignment #4
Due Monday, April 21, 2025, 1:15 p.m.

In this assignment, you will explore the relation between the width of a resonance peak and the lifetime of a damped oscillator.

1 Background Theory

Damped Oscillations

To start, consider the decaying oscillations of a damped torsional oscillator. The differential equation for a damped, torsional oscillator of torsional constant κ and rotational inertia I is

θ¨ = -ω02θ - γ˙θ

where ω0 = 2πf0 = ∘ κ-
  --
  I is the natural (undamped) frequency of the oscillator, and γ is a term proportional to the drag, with units of rads-1. If released from rest from an initial angle θ0, the resulting motion is a damped oscillation:

θ(t) = θ0 e-γt∕2 cos(ω vt + ϕ) .

For this assignment, the key observation is to note that the amplitude decays exponentially:

A = θ0e-γt∕2 = θ 0e-t∕(2τ)

where τ = 1∕γ is the time constant, or lifetime, associated with the motion. Recall that the energy of a simple harmonic oscillator is proportional to the amplitude squared, so we can also describe the decay in terms of energy:

A2 = E = E 0e-γt = E 0e-t∕τ (1)

Driven Oscillations

If periodic forcing at frequency ωd is added, the new differential equation is

¨θ = -ω02θ - γθ˙ + α 0 sin(ωdt)

where α0 = τ0
I is the amplitude of the driving. After an initial transient, the steady state motion is given by a sinusoidal oscillation with an amplitude θ0 given by

θ0 =           α
∘--(-------0)----------
    ω20 - ω2d 2 + (γωd)2

As with the decaying oscillation, the energy is related to the amplitude squared

θ02 =           2
(-------α)-0--------
 ω20 - ω2d 2 + (γωd)2 (2)

In this assignment, you will explore the relation between the lifetime τ of the damped oscillations and the width of the peak in Eq. 2. Throughout, it will be simpler to leave things in terms of ω and γ (or τ), rather than using f and Q.

Hint: Assume that the damping is small, so that γ ω0 (or equivalently Q 1) so that you may drop higher order terms in γ∕ω0, and use the binomial expansion when appropriate.

Assignment 1: What frequency ωd gives the maximum for θ02 in Eq. 2? Call that frequency ωp. What is the magnitude of θ02 at that frequency?

Assignment 2: What are the two frequencies that give an amplitude in Eq. 2 equal to one half of that maximum? Only keep terms up to the lowest order in γ∕ω0.

Assignment 3: Define the full width at half maximum—FWHM—as the difference between the two frequencies you found in assignment 2. Find the relation between the FWHM and τ in Eq. 1.

Assignment 4: Test your prediction for your mechanical resonance curve for the torsional oscillator. Note that since you measured amplitude θ and not θ2, you will measure the FWHM by noting the frequencies at which your curve is at a height of √12- of the maximum. Note too that you measured linear frequencies f, not angular frequencies ω, so you will need to manually handle the factor of 2π.

Assignment 5: Test your prediction for your electrical resonance curve for the RLC oscillator. Again, you will actually need to measure the frequencies at which your curve is at a height of √1-
 2 of the maximum, and compensate for factors of 2π.

Conclusion

Your result should illustrate a quite general relation between the width of a resonance curve and the lifetime of the corresponding state.