Simple Harmonic Motion and Uniform Circular Motion — Question 5

Section 15-6 · Physics pages 2340–2341

Question 5 Counterrotating circles can generate motion along one line Two mathematical vectors of equal length a rotate about the same origin. Their angles are ωt + α and −ωt + β. Their vector sum is r(t). x y Equal vectors rotate in opposite senses; their sum remains on a fixed bisector line. (a) Find the direction of the line traced by the sum and the scalar displacement along it. (b) For a = .020 m, α = π/3 and β = −π/3, find the amplitude and initial displacement. What changes if the two lengths are unequal?
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Question 5 - Solution Counterrotating circles can generate motion along one line x y (a) Derivation and calculation Put γ = (α + β)/2 and η = ωt + (α −β)/2. Then cos(γ + η) + cos(γ −η) = 2 cos γ cos η, sin(γ + η) + sin(γ −η) = 2 sin γ cos η. r = 2a cos η (cos γ, sin γ) . (b) Result and interpretation a = .0200, α = π/3, β = −π/3 : γ = 0, η = ωt + π/3. A = 2a = .0400 m , x(0) = .0400 cos(π/3) = .0200 m . For lengths a1̸ = a2, coordinates along and across the bisector are u = (a1 + a2) cos η, w = (a1 −a2) sin η, u2 (a1 + a2)2 + w2 (a1 −a2)2 = 1. Physical check The equal-length limit sets the perpendicular coordinate to zero, collapsing the ellipse to a line.

Question 5

Counterrotating circles can generate motion along one line

Two mathematical vectors of equal length aa rotate about the same origin. Their angles are ωt+α\omega t+\alpha and −ωt+β-\omega t+\beta. Their vector sum is 𝒓(t)\mathbf r(t).

Diagram shown in the original SVG worksheet.

  1. Find the direction of the line traced by the sum and the scalar displacement along it.

  2. For a=.020ma=.020\,\mathrm{m}, α=π/3\alpha=\pi/3 and β=−π/3\beta=-\pi/3, find the amplitude and initial displacement. What changes if the two lengths are unequal?

Question 5 - Solution

Counterrotating circles can generate motion along one line

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

Put γ=(α+β)/2\gamma=(\alpha+\beta)/2 and η=ωt+(α−β)/2\eta=\omega t+(\alpha-\beta)/2. Thencos⁡(γ+η)+cos⁡(γ−η)=2cos⁡γcos⁡η,\cos(\gamma+\eta)+\cos(\gamma-\eta)=2\cos\gamma\cos\eta,sin⁡(γ+η)+sin⁡(γ−η)=2sin⁡γcos⁡η.\sin(\gamma+\eta)+\sin(\gamma-\eta)=2\sin\gamma\cos\eta.𝒓=2acos⁡η(cos⁡γ,sin⁡γ).\boxed{\mathbf r=2a\cos\eta\,(\cos\gamma,\sin\gamma)}.

(b) Result and interpretation

a=.0200,α=π/3,β=−π/3:γ=0,η=ωt+π/3.a=.0200,\quad\alpha=\pi/3,\quad\beta=-\pi/3:\quad\gamma=0,\quad\eta=\omega t+\pi/3.A=2a=.0400m,x(0)=.0400cos⁡(π/3)=.0200m.\boxed{A=2a=.0400\,\mathrm m},\qquad\boxed{x(0)=.0400\cos(\pi/3)=.0200\,\mathrm m}.For lengths a1≠a2a_1\ne a_2, coordinates along and across the bisector areu=(a1+a2)cos⁡η,w=(a1−a2)sin⁡η,u=(a_1+a_2)\cos\eta,\quad w=(a_1-a_2)\sin\eta,u2(a1+a2)2+w2(a1−a2)2=1.\frac{u^2}{(a_1+a_2)^2}+\frac{w^2}{(a_1-a_2)^2}=1.

Physical check

The equal-length limit sets the perpendicular coordinate to zero, collapsing the ellipse to a line.