Simple Harmonic Motion — Question 3

Section 15-1 · Physics pages 2236–2237

Question 3 A crossing interval is not always half a period An SHM particle of period T passes x = A/2 moving toward positive x at time zero. It next returns to x = A/2 moving toward negative x. ψ x/A 2π 1 −1 Normalized displacement over one cycle; the horizontal coordinate is phase. (a) Find the interval between these two crossings. (b) Find the interval from that second crossing to the next positive-direction crossing. Explain why the intervals differ.
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Question 3 - Solution A crossing interval is not always half a period ψ x/A 2π 1 −1 (a) Derivation and calculation At x = A/2, cos ψ = 1/2. The direction condition selects v = −Aω sin ψ > 0 ⇒ ψ0 = −π/3. The next equal-position phase is ψ1 = π/3, hence ∆ψ1 = 2π 3 , ∆t1 = ∆ψ1 ω = T 3 . (b) Result and interpretation The following positive-direction crossing has ψ2 = 5π/3: ∆ψ2 = 5π 3 −π 3 = 4π 3 , ∆t2 = 2T 3 . ∆t1 + ∆t2 = T. The shorter arc passes through +A; the longer arc includes the negative turning point. Physical check Only equilibrium crossings divide a sinusoidal cycle into two equal intervals. The stated crossing is displaced from equilibrium.

Question 3

A crossing interval is not always half a period

An SHM particle of period TT passes x=A/2x=A/2 moving toward positive xx at time zero. It next returns to x=A/2x=A/2 moving toward negative xx.

Diagram shown in the original SVG worksheet.

  1. Find the interval between these two crossings.

  2. Find the interval from that second crossing to the next positive-direction crossing. Explain why the intervals differ.

Question 3 - Solution

A crossing interval is not always half a period

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

At x=A/2x=A/2, cos⁡ψ=1/2\cos\psi=1/2. The direction condition selectsv=−Aωsin⁡ψ>0⇒ψ0=−π/3.v=-A\omega\sin\psi>0\quad\Rightarrow\quad\psi_0=-\pi/3.The next equal-position phase is ψ1=π/3\psi_1=\pi/3, henceΔψ1=2π3,Δt1=Δψ1ω=T3.\Delta\psi_1=\frac{2\pi}{3},\qquad\Delta t_1=\frac{\Delta\psi_1}{\omega}=\boxed{\frac T3}.

(b) Result and interpretation

The following positive-direction crossing has ψ2=5π/3\psi_2=5\pi/3:Δψ2=5π3−π3=4π3,Δt2=2T3.\Delta\psi_2=\frac{5\pi}{3}-\frac\pi3=\frac{4\pi}{3},\qquad\Delta t_2=\boxed{\frac{2T}{3}}.Δt1+Δt2=T.\Delta t_1+\Delta t_2=T.The shorter arc passes through +A+A; the longer arc includes the negative turning point.

Physical check

Only equilibrium crossings divide a sinusoidal cycle into two equal intervals. The stated crossing is displaced from equilibrium.