Simple Harmonic Motion and Uniform Circular Motion — Question 3

Section 15-6 · Physics pages 2336–2337

Question 3 Changing the viewing axis changes phase rather than amplitude A point has coordinates x = A cos ωt and y = A sin ωt. An observer measures its signed projection u on a fixed axis making angle α counterclockwise from the positive x axis. x y u A fixed viewing axis rotates the projection phase; it does not change the circle radius. (a) Derive u(t) and state its amplitude, period and phase relative to x(t). (b) For α = π/3, find u(0) and ˙u(0). Does measuring on an oblique axis reduce the full projection amplitude?
Show solutionHide solution
Question 3 - Solution Changing the viewing axis changes phase rather than amplitude x y u (a) Derivation and calculation ˆeu = (cos α, sin α), u = r · ˆeu. u = A cos ωt cos α + A sin ωt sin α = A cos(ωt −α) . Au = A , T = 2π/ω , ϕu = −α. (b) Result and interpretation For α = π/3, u(0) = A/2 , ˙u(0) = Aω sin α = √ 3Aω/2 . max t |r · ˆeu| = A. During a complete rotation the vector aligns with every fixed viewing axis, so the full amplitude remains A. Physical check The initial projection can be smaller than A without reducing the maximum over a cycle.

Question 3

Changing the viewing axis changes phase rather than amplitude

A point has coordinates x=Acos⁡ωtx=A\cos\omega t and y=Asin⁡ωty=A\sin\omega t. An observer measures its signed projection uu on a fixed axis making angle α\alpha counterclockwise from the positive xx axis.

Diagram shown in the original SVG worksheet.

  1. Derive u(t)u(t) and state its amplitude, period and phase relative to x(t)x(t).

  2. For α=π/3\alpha=\pi/3, find u(0)u(0) and u̇(0)\dot u(0). Does measuring on an oblique axis reduce the full projection amplitude?

Question 3 - Solution

Changing the viewing axis changes phase rather than amplitude

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

𝒆̂u=(cos⁡α,sin⁡α),u=𝒓⋅𝒆̂u.\hat{\mathbf e}_u=(\cos\alpha,\sin\alpha),\quad u=\mathbf r\cdot\hat{\mathbf e}_u.u=Acos⁡ωtcos⁡α+Asin⁡ωtsin⁡α=Acos⁡(ωt−α).u=A\cos\omega t\cos\alpha+A\sin\omega t\sin\alpha=\boxed{A\cos(\omega t-\alpha)}.Au=A,T=2π/ω,ϕu=−α.\boxed{A_u=A},\qquad\boxed{T=2\pi/\omega},\qquad\phi_u=-\alpha.

(b) Result and interpretation

For α=π/3\alpha=\pi/3,u(0)=A/2,u̇(0)=Aωsin⁡α=3Aω/2.\boxed{u(0)=A/2},\qquad\boxed{\dot u(0)=A\omega\sin\alpha=\sqrt3A\omega/2}.maxt|𝒓⋅𝒆̂u|=A.\max_t|\mathbf r\cdot\hat{\mathbf e}_u|=A.During a complete rotation the vector aligns with every fixed viewing axis, so the full amplitude remains AA.

Physical check

The initial projection can be smaller than AA without reducing the maximum over a cycle.