Equilibrium — Question 5

Section 12-1 · Physics pages 1780–1781

Question 5 The force slope distinguishes restoring and destabilizing equilibria A particle constrained to the x axis has potential energy U(x) = a(x2 −b2)2, with a, b > 0. No other force acts along the axis. x/b U/(ab4) −1 1 Dimensionless double-well potential; equilibria occur where the slope vanishes. (a) Find all equilibrium positions. (b) Classify their response to a small displacement using the local force.
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Question 5 - Solution The force slope distinguishes restoring and destabilizing equilibria x/b U/(ab4) −1 1 (a) Derivation and calculation Differentiate the potential: F(x) = −U′(x) = −4ax(x2 −b2). Equilibrium requires F = 0, hence x∗= 0, x∗= +b, x∗= −b . (b) Result and interpretation For a small displacement ξ = x −x∗, F(x∗+ ξ) ≃−U′′(x∗)ξ, U′′(x) = 12ax2 −4ab2. At the origin, U′′(0) = −4ab2, F ≃+4ab2ξ ⇒ unstable . At either outer point, U′′(±b) = 8ab2, F ≃−8ab2ξ ⇒ stable . Physical check The outer equilibria are potential minima; the origin is a local maximum.

Question 5

The force slope distinguishes restoring and destabilizing equilibria

A particle constrained to the xx axis has potential energy U(x)=a(x2−b2)2U(x)=a(x^2-b^2)^2, with a,b>0a,b>0. No other force acts along the axis.

Diagram shown in the original SVG worksheet.

  1. Find all equilibrium positions.

  2. Classify their response to a small displacement using the local force.

Question 5 - Solution

The force slope distinguishes restoring and destabilizing equilibria

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

Differentiate the potential: F(x)=−U′(x)=−4ax(x2−b2).F(x)=-U'(x)=-4ax(x^2-b^2). Equilibrium requires F=0F=0, hence x*=0,x*=+b,x*=−b.\boxed{x_*=0,\quad x_*=+b,\quad x_*=-b}.

(b) Result and interpretation

For a small displacement ξ=x−x*\xi=x-x_*, F(x*+ξ)≃−U″(x*)ξ,U″(x)=12ax2−4ab2.F(x_*+\xi)\simeq-U''(x_*)\xi,\qquad U''(x)=12ax^2-4ab^2. At the origin, U″(0)=−4ab2,F≃+4ab2ξ⇒unstable.U''(0)=-4ab^2,\quad F\simeq+4ab^2\xi\quad\Rightarrow\quad\boxed{\text{unstable}}. At either outer point, U″(±b)=8ab2,F≃−8ab2ξ⇒stable.U''(\pm b)=8ab^2,\quad F\simeq-8ab^2\xi\quad\Rightarrow\quad\boxed{\text{stable}}.

Physical check

The outer equilibria are potential minima; the origin is a local maximum.