Damped Simple Harmonic Motion — Question 8

Section 15-7 · Physics pages 2366–2367

Question 8 The quality factor and logarithmic decrement agree only in a limit Define Q = ω0/(2β) for an underdamped viscous oscillator. Its same-side logarithmic decrement is δ = ln(xn/xn+1) = βTd. t x Exponential decay envelope and oscillatory motion; scales are schematic. (a) Derive the exact relation between Q and δ. (b) For δ = 1.0, compute Q and compare with the weak-damping estimate π/δ. Why is Q > 1/2 necessary here?
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Question 8 - Solution The quality factor and logarithmic decrement agree only in a limit t x (a) Derivation and calculation Q = ω0 2β , ω2 d = ω2 0 −β2 = 4β2(Q2 −1/4). δ = 2πβ ωd = π √ Q2 −1/4. Q = √(π δ )2 + 1 4 . (b) Result and interpretation δ = 1 : Q = 3.18113 , Qweak = π = 3.14159. Q −Qweak Q × 100% = 1.2430%. ω2 d > 0 ⇐⇒β < ω0 ⇐⇒ Q > 1/2 . The approximation Q ≃π/δ requires the 1/4 term to be negligible. Physical check At or below Q = 1/2, a damped period and a sequence of same-side oscillation peaks no longer exist.

Question 8

The quality factor and logarithmic decrement agree only in a limit

Define Q=ω0/(2β)Q=\omega_0/(2\beta) for an underdamped viscous oscillator. Its same-side logarithmic decrement is δ=ln⁡(xn/xn+1)=βTd\delta=\ln(x_n/x_{n+1})=\beta T_d.

Diagram shown in the original SVG worksheet.

  1. Derive the exact relation between QQ and δ\delta.

  2. For δ=1.0\delta=1.0, compute QQ and compare with the weak-damping estimate π/δ\pi/\delta. Why is Q>1/2Q>1/2 necessary here?

Question 8 - Solution

The quality factor and logarithmic decrement agree only in a limit

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

Q=ω02β,ωd2=ω02−β2=4β2(Q2−1/4).Q=\frac{\omega_0}{2\beta},\quad\omega_d^2=\omega_0^2-\beta^2=4\beta^2(Q^2-1/4).δ=2πβωd=πQ2−1/4.\delta=\frac{2\pi\beta}{\omega_d}=\frac\pi{\sqrt{Q^2-1/4}}.Q=(πδ)2+14.\boxed{Q=\sqrt{\left(\frac\pi\delta\right)^2+\frac14}}.

(b) Result and interpretation

δ=1:Q=3.18113,Qweak=π=3.14159.\delta=1:\quad\boxed{Q=3.18113},\qquad Q_{\mathrm{weak}}=\pi=3.14159.Q−QweakQ×100%=1.2430%.\frac{Q-Q_{\mathrm{weak}}}Q\times100\%=1.2430\%.ωd2>0⇔β<ω0⇔Q>1/2.\omega_d^2>0\iff\beta<\omega_0\iff\boxed{Q>1/2}.The approximation Q≃π/δQ\simeq\pi/\delta requires the 1/41/4 term to be negligible.

Physical check

At or below Q=1/2Q=1/2, a damped period and a sequence of same-side oscillation peaks no longer exist.