Simple Harmonic Motion — Question 2

Section 15-1 · Physics pages 2234–2235

Question 2 Two speed measurements reveal the hidden amplitude An ideal SHM particle has speed 0.80 m/s at displacement 0.060 m and speed 0.60 m/s at displacement 0.080 m. Both displacements are measured from equilibrium. x v State-space schematic; the state follows the ellipse clockwise. (a) Derive v2 = ω2(A2 −x2) from sinusoidal kinematics and infer ω and A. (b) Can the two speed measurements determine the phase or the direction of travel at either point? Explain.
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Question 2 - Solution Two speed measurements reveal the hidden amplitude x v (a) Derivation and calculation Eliminate the phase from x = A cos ψ and v = −Aω sin ψ: x2 A2 + v2 A2ω2 = 1 ⇒ v2 = ω2(A2 −x2). ω2 = v2 1 −v2 2 x2 2 −x2 1 = 0.802 −0.602 0.0802 −0.0602 = 100 s−2. ω = 10 rad/s , A = √ 0.0602 + 0.802 100 = 0.100 m . (b) Result and interpretation Each speed permits two signed velocities: x = 0.060 : v = ±0.80, x = 0.080 : v = ±0.60 (m/s). ψ = atan2 ( −v Aω, x A ) , ϕ = ψ −ωt (mod 2π). Neither velocity sign nor observation time is specified, so the initial phase is undetermined. Physical check Both states satisfy x2 + v2/ω2 = 0.0100 m2; inferred amplitude exceeds both measured displacements.

Question 2

Two speed measurements reveal the hidden amplitude

An ideal SHM particle has speed 0.80m/s0.80\,\mathrm{m/s} at displacement 0.060m0.060\,\mathrm{m} and speed 0.60m/s0.60\,\mathrm{m/s} at displacement 0.080m0.080\,\mathrm{m}. Both displacements are measured from equilibrium.

Diagram shown in the original SVG worksheet.

  1. Derive v2=ω2(A2−x2)v^2=\omega^2(A^2-x^2) from sinusoidal kinematics and infer ω\omega and AA.

  2. Can the two speed measurements determine the phase or the direction of travel at either point? Explain.

Question 2 - Solution

Two speed measurements reveal the hidden amplitude

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

Eliminate the phase from x=Acos⁡ψx=A\cos\psi and v=−Aωsin⁡ψv=-A\omega\sin\psi:x2A2+v2A2ω2=1⇒v2=ω2(A2−x2).\frac{x^2}{A^2}+\frac{v^2}{A^2\omega^2}=1\quad\Rightarrow\quad v^2=\omega^2(A^2-x^2).ω2=v12−v22x22−x12=0.802−0.6020.0802−0.0602=100s−2.\omega^2=\frac{v_1^2-v_2^2}{x_2^2-x_1^2}=\frac{0.80^2-0.60^2}{0.080^2-0.060^2}=100\,\mathrm{s^{-2}}.ω=10rad/s,A=0.0602+0.802100=0.100m.\boxed{\omega=10\,\mathrm{rad/s}},\qquad A=\sqrt{0.060^2+\frac{0.80^2}{100}}=\boxed{0.100\,\mathrm m}.

(b) Result and interpretation

Each speed permits two signed velocities:x=0.060:v=±0.80,x=0.080:v=±0.60(m/s).x=0.060:\ v=\pm0.80,\qquad x=0.080:\ v=\pm0.60\quad(\mathrm{m/s}).ψ=atan2⁡(−vAω,xA),ϕ=ψ−ωt(mod⁡2π).\psi=\operatorname{atan2}\!\left(-\frac v{A\omega},\frac xA\right),\qquad\phi=\psi-\omega t\pmod{2\pi}.Neither velocity sign nor observation time is specified, so the initial phase is undetermined.

Physical check

Both states satisfy x2+v2/ω2=0.0100m2x^2+v^2/\omega^2=0.0100\,\mathrm{m^2}; inferred amplitude exceeds both measured displacements.