Simple Harmonic Motion and Uniform Circular Motion — Question 4

Section 15-6 · Physics pages 2338–2339

Question 4 Two same-frequency oscillations combine as fixed vectors Two displacements along one line add: x1 = .030 cos ωt and x2 = .040 cos(ωt + π/2), in meters. The frequency is the same for both. .030 .040 R Phasors add by components; the perpendicular phasor lengths are labeled in meters (schematic scale). (a) Express their sum as R cos(ωt + ϕ) with R > 0. (b) Find the allowed resultant amplitude range if the relative phase can vary. Explain why adding the amplitudes directly fails for the specified phase.
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Question 4 - Solution Two same-frequency oscillations combine as fixed vectors .030 .040 R (a) Derivation and calculation x = .030 cos ωt −.040 sin ωt = R cos(ωt + ϕ). R cos ϕ = .030, R sin ϕ = .040. R = .0500 m , ϕ = atan2(.040, .030) = .92730 rad . (b) Result and interpretation For arbitrary relative phase δ, R2 = A2 1 + A2 2 + 2A1A2 cos δ. |A1 −A2| ≤R ≤A1 + A2 ⇒.0100 ≤R ≤.0700 m . The upper bound requires equal phase; the specified quadrature gives the vector magnitude instead. Physical check At t = 0, x = .0300 m and v = −.0400ω, both reproduced by the resultant phasor.

Question 4

Two same-frequency oscillations combine as fixed vectors

Two displacements along one line add: x1=.030cos⁡ωtx_1=.030\cos\omega t and x2=.040cos⁡(ωt+π/2)x_2=.040\cos(\omega t+\pi/2), in meters. The frequency is the same for both.

Diagram shown in the original SVG worksheet.

  1. Express their sum as Rcos⁡(ωt+ϕ)R\cos(\omega t+\phi) with R>0R>0.

  2. Find the allowed resultant amplitude range if the relative phase can vary. Explain why adding the amplitudes directly fails for the specified phase.

Question 4 - Solution

Two same-frequency oscillations combine as fixed vectors

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

x=.030cos⁡ωt−.040sin⁡ωt=Rcos⁡(ωt+ϕ).x=.030\cos\omega t-.040\sin\omega t=R\cos(\omega t+\phi).Rcos⁡ϕ=.030,Rsin⁡ϕ=.040.R\cos\phi=.030,\qquad R\sin\phi=.040.R=.0500m,ϕ=atan2⁡(.040,.030)=.92730rad.\boxed{R=.0500\,\mathrm m},\qquad\boxed{\phi=\operatorname{atan2}(.040,.030)=.92730\,\mathrm{rad}}.

(b) Result and interpretation

For arbitrary relative phase δ\delta,R2=A12+A22+2A1A2cos⁡δ.R^2=A_1^2+A_2^2+2A_1A_2\cos\delta.|A1−A2|≤R≤A1+A2⇒.0100≤R≤.0700m.|A_1-A_2|\le R\le A_1+A_2\Rightarrow\boxed{.0100\le R\le.0700\,\mathrm m}.The upper bound requires equal phase; the specified quadrature gives the vector magnitude instead.

Physical check

At t=0t=0, x=.0300mx=.0300\,\mathrm m and v=−.0400ωv=-.0400\omega, both reproduced by the resultant phasor.