Energy in Simple Harmonic Motion — Question 10

Section 15-3 · Physics pages 2290–2291

Question 10 A one-sided auxiliary spring makes unequal turning distances A mass moves on a frictionless line with a main spring of constant k. At x > 0 it also compresses an auxiliary spring of constant 3k, initially just touching at x = 0. At x < 0 the auxiliary spring loses contact. Both natural equilibria are at x = 0, and contacts are ideal and elastic. Release the mass from rest at x = −A. x U Piecewise quadratic potential: the additional spring stiffens only the positive side. (a) Find the positive turning position and the speed at x = 0. (b) Find the full cycle period and explain why the motion is periodic but not one global sinusoid.
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Question 10 - Solution A one-sided auxiliary spring makes unequal turning distances x U (a) Derivation and calculation U(x) = {1 2kx2, x ≤0, 1 2(4k)x2, x ≥0. E = 1 2kA2. 2kx2 + = 1 2kA2 ⇒x+ = A/2 . 1 2mv2 0 = E ⇒|v0| = A √ k/m . (b) Result and interpretation Let ω = √ k/m. The negative and positive excursions each occupy a half-cycle of their own oscillator: t−= π ω, t+ = π 2ω. T = t−+ t+ = 3π 2 √ m/k . Position and velocity join continuously at zero; the two half-cycles have different frequencies. Physical check The period is independent of amplitude within the ideal piecewise-linear model, although the complete waveform is not sinusoidal.

Question 10

A one-sided auxiliary spring makes unequal turning distances

A mass moves on a frictionless line with a main spring of constant kk. At x>0x>0 it also compresses an auxiliary spring of constant 3k3k, initially just touching at x=0x=0. At x<0x<0 the auxiliary spring loses contact. Both natural equilibria are at x=0x=0, and contacts are ideal and elastic. Release the mass from rest at x=−Ax=-A.

Diagram shown in the original SVG worksheet.

  1. Find the positive turning position and the speed at x=0x=0.

  2. Find the full cycle period and explain why the motion is periodic but not one global sinusoid.

Question 10 - Solution

A one-sided auxiliary spring makes unequal turning distances

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

U(x)={12kx2,x≤0,12(4k)x2,x≥0.E=12kA2.U(x)=\begin{cases}\tfrac12kx^2,&x\le0,\\\tfrac12(4k)x^2,&x\ge0.\end{cases}\qquad E=\tfrac12kA^2.2kx+2=12kA2⇒x+=A/2.2kx_+^2=\tfrac12kA^2\Rightarrow\boxed{x_+=A/2}.12mv02=E⇒|v0|=Ak/m.\tfrac12mv_0^2=E\Rightarrow\boxed{|v_0|=A\sqrt{k/m}}.

(b) Result and interpretation

Let ω=k/m\omega=\sqrt{k/m}. The negative and positive excursions each occupy a half-cycle of their own oscillator:t−=πω,t+=π2ω.t_- =\frac\pi\omega,\qquad t_+=\frac\pi{2\omega}.T=t−+t+=3π2m/k.\boxed{T=t_-+t_+=\frac{3\pi}{2}\sqrt{m/k}}.Position and velocity join continuously at zero; the two half-cycles have different frequencies.

Physical check

The period is independent of amplitude within the ideal piecewise-linear model, although the complete waveform is not sinusoidal.