Simple Harmonic Motion — Question 5

Section 15-1 · Physics pages 2240–2241

Question 5 A camera can mistake fast oscillation for slow oscillation A camera samples displacement every ∆t = 0.10 s. One possible motion is x1(t) = A cos(2πft) with f = 2.0 Hz. A second is x2(t) = A cos(2πf2t) with f2 = 8.0 Hz. Both start at +A. t x/A Two continuous motions share the same sampled positions (dots); sample spacing is 0.10 s. (a) Show that their recorded positions agree at every camera sample. (b) Would a signed velocity measurement at t = 0.10 s distinguish them? Compare the two velocities in units of A s−1.
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Question 5 - Solution A camera can mistake fast oscillation for slow oscillation t x/A (a) Derivation and calculation At frame time tn = 0.10n s, ψ1n = 2π(2)(0.10n) = 0.4πn, ψ2n = 2π(8)(0.10n) = 1.6πn = 2πn −ψ1n. x2(tn) = A cos(2πn −ψ1n) = A cos ψ1n = x1(tn) . (b) Result and interpretation Differentiate the continuous fields before evaluating the time: v1(0.10) A = −4π sin(0.4π) = −11.9513 s−1 , v2(0.10) A = −16π sin(1.6π) = +47.8053 s−1 . A signed velocity measurement distinguishes both direction and magnitude, although the sampled positions coincide. Physical check The frame rate is 10 Hz and f2 = 10 −f1, giving the cosine sampling alias shown explicitly.

Question 5

A camera can mistake fast oscillation for slow oscillation

A camera samples displacement every Δt=0.10s\Delta t=0.10\,\mathrm{s}. One possible motion is x1(t)=Acos⁡(2πft)x_1(t)=A\cos(2\pi ft) with f=2.0Hzf=2.0\,\mathrm{Hz}. A second is x2(t)=Acos⁡(2πf2t)x_2(t)=A\cos(2\pi f_2t) with f2=8.0Hzf_2=8.0\,\mathrm{Hz}. Both start at +A+A.

Diagram shown in the original SVG worksheet.

  1. Show that their recorded positions agree at every camera sample.

  2. Would a signed velocity measurement at t=0.10st=0.10\,\mathrm{s} distinguish them? Compare the two velocities in units of As−1A\,\mathrm{s^{-1}}.

Question 5 - Solution

A camera can mistake fast oscillation for slow oscillation

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

At frame time tn=0.10nst_n=0.10n\,\mathrm s,ψ1n=2π(2)(0.10n)=0.4πn,\psi_{1n}=2\pi(2)(0.10n)=0.4\pi n,ψ2n=2π(8)(0.10n)=1.6πn=2πn−ψ1n.\psi_{2n}=2\pi(8)(0.10n)=1.6\pi n=2\pi n-\psi_{1n}.x2(tn)=Acos⁡(2πn−ψ1n)=Acos⁡ψ1n=x1(tn).x_2(t_n)=A\cos(2\pi n-\psi_{1n})=A\cos\psi_{1n}=\boxed{x_1(t_n)}.

(b) Result and interpretation

Differentiate the continuous fields before evaluating the time:v1(0.10)A=−4πsin⁡(0.4π)=−11.9513s−1,\frac{v_1(0.10)}A=-4\pi\sin(0.4\pi)=\boxed{-11.9513\,\mathrm{s^{-1}}},v2(0.10)A=−16πsin⁡(1.6π)=+47.8053s−1.\frac{v_2(0.10)}A=-16\pi\sin(1.6\pi)=\boxed{+47.8053\,\mathrm{s^{-1}}}.A signed velocity measurement distinguishes both direction and magnitude, although the sampled positions coincide.

Physical check

The frame rate is 10Hz10\,\mathrm{Hz} and f2=10−f1f_2=10-f_1, giving the cosine sampling alias shown explicitly.