The Force Law for Simple Harmonic Motion — Question 7

Section 15-2 · Physics pages 2264–2265

Question 7 The slope of a force curve determines local stability A one-dimensional force is F(x) = αx −βx3, with α, β > 0. A particle of mass m is free to move along x. x F A cubic force curve has three zero-force locations; local slope determines stability. (a) Find all equilibria and classify their linear stability from the force slope. (b) Find the small-oscillation angular frequency about each stable equilibrium. Does this imply exact SHM for arbitrary amplitude?
Show solutionHide solution
Question 7 - Solution The slope of a force curve determines local stability x F (a) Derivation and calculation F = x(α −βx2) = 0 ⇒xe = 0, xe = ± √ α/β. F ′(x) = α −3βx2. F ′(0) = +α > 0 (unstable), F ′(xe) = −2α < 0 (stable outer points). (b) Result and interpretation Expand about either stable point, x = xe + q: F(xe + q) = −2αq −3βxeq2 −βq3. m¨q ≃−2αq ⇒ω = √ 2α/m . The higher-order terms remain; the linear approximation requires excursions small compared with |xe| = √ α/β. It is not global finite-amplitude SHM. Physical check The two stable equilibria have the same linear curvature and frequency, although their quadratic corrections have opposite signs.

Question 7

The slope of a force curve determines local stability

A one-dimensional force is F(x)=αx−βx3F(x)=\alpha x-\beta x^3, with α,β>0\alpha,\beta>0. A particle of mass mm is free to move along xx.

Diagram shown in the original SVG worksheet.

  1. Find all equilibria and classify their linear stability from the force slope.

  2. Find the small-oscillation angular frequency about each stable equilibrium. Does this imply exact SHM for arbitrary amplitude?

Question 7 - Solution

The slope of a force curve determines local stability

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

F=x(α−βx2)=0⇒xe=0,xe=±α/β.F=x(\alpha-\beta x^2)=0\Rightarrow x_e=0,\quad x_e=\pm\sqrt{\alpha/\beta}.F′(x)=α−3βx2.F^{\prime}(x)=\alpha-3\beta x^2.F′(0)=+α>0(unstable),F′(xe)=−2α<0(stable outer points).F^{\prime}(0)=+\alpha>0\quad(\text{unstable}),\qquad F^{\prime}(x_e)=-2\alpha<0\quad(\text{stable outer points}).

(b) Result and interpretation

Expand about either stable point, x=xe+qx=x_e+q:F(xe+q)=−2αq−3βxeq2−βq3.F(x_e+q)=-2\alpha q-3\beta x_e q^2-\beta q^3.mq̈≃−2αq⇒ω=2α/m.m\ddot q\simeq-2\alpha q\Rightarrow\boxed{\omega=\sqrt{2\alpha/m}}.The higher-order terms remain; the linear approximation requires excursions small compared with |xe|=α/β|x_e|=\sqrt{\alpha/\beta}. It is not global finite-amplitude SHM.

Physical check

The two stable equilibria have the same linear curvature and frequency, although their quadratic corrections have opposite signs.