Simple Harmonic Motion and Uniform Circular Motion — Question 10

Section 15-6 · Physics pages 2350–2351

Question 10 A phase relation determines both path shape and circulation A planar motion has x = A cos ωt and y = A cos(ωt + δ), with A, ω > 0. Consider 0 < δ < π. x y A non-quadrature phase offset produces an inclined ellipse; the stated positive phase range gives clockwise circulation. (a) Eliminate time to find the path equation and identify when it is a circle. (b) Compute x ˙y −y ˙x and infer the circulation direction. Describe the limits δ →0 and δ →π.
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Question 10 - Solution A phase relation determines both path shape and circulation x y (a) Derivation and calculation y/A = (x/A) cos δ −sin ωt sin δ. (y −x cos δ A sin δ )2 + x2 A2 = 1. x2 + y2 −2xy cos δ = A2 sin2 δ . δ = π/2 ⇒x2 + y2 = A2 . (b) Result and interpretation x ˙y −y ˙x = A2ω[sin ωt cos(ωt + δ) −cos ωt sin(ωt + δ)] x ˙y −y ˙x = −A2ω sin δ < 0 . The motion circulates clockwise for 0 < δ < π. δ →0 : y = x; δ →π : y = −x. Physical check Equal coordinate amplitudes yield a circle only in quadrature; the endpoint phases give degenerate straight paths.

Question 10

A phase relation determines both path shape and circulation

A planar motion has x=Acos⁡ωtx=A\cos\omega t and y=Acos⁡(ωt+δ)y=A\cos(\omega t+\delta), with A,ω>0A,\omega>0. Consider 0<δ<π0<\delta<\pi.

Diagram shown in the original SVG worksheet.

  1. Eliminate time to find the path equation and identify when it is a circle.

  2. Compute xẏ−yẋx\dot y-y\dot x and infer the circulation direction. Describe the limits δ→0\delta\to0 and δ→π\delta\to\pi.

Question 10 - Solution

A phase relation determines both path shape and circulation

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

y/A=(x/A)cos⁡δ−sin⁡ωtsin⁡δ.y/A=(x/A)\cos\delta-\sin\omega t\sin\delta.(y−xcos⁡δAsin⁡δ)2+x2A2=1.\left(\frac{y-x\cos\delta}{A\sin\delta}\right)^2+\frac{x^2}{A^2}=1.x2+y2−2xycos⁡δ=A2sin⁡2δ.\boxed{x^2+y^2-2xy\cos\delta=A^2\sin^2\delta}.δ=π/2⇒x2+y2=A2.\delta=\pi/2\Rightarrow\boxed{x^2+y^2=A^2}.

(b) Result and interpretation

xẏ−yẋ=A2ω[sin⁡ωtcos⁡(ωt+δ)−cos⁡ωtsin⁡(ωt+δ)]x\dot y-y\dot x=A^2\omega[\sin\omega t\cos(\omega t+\delta)-\cos\omega t\sin(\omega t+\delta)]xẏ−yẋ=−A2ωsin⁡δ<0.\boxed{x\dot y-y\dot x=-A^2\omega\sin\delta<0}.The motion circulates clockwise for 0<δ<π0<\delta<\pi.δ→0:y=x;δ→π:y=−x.\delta\to0:\ y=x;\qquad\delta\to\pi:\ y=-x.

Physical check

Equal coordinate amplitudes yield a circle only in quadrature; the endpoint phases give degenerate straight paths.