Equilibrium — Question 9

Section 12-1 · Physics pages 1788–1789

Question 9 A local minimum need not have nonzero curvature A particle moves along x with potential U(x) = cx4, where c > 0. At x = 0 both U′ and U′′ vanish. x U Quartic minimum: flat at the origin but higher on both sides. (a) Classify the equilibrium without relying only on the second derivative test. (b) Compare the restoring force at displacements d and 2d, with d > 0.
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Question 9 - Solution A local minimum need not have nonzero curvature x U (a) Derivation and calculation The force is F(x) = −U′(x) = −4cx3. For every x̸ = 0, U(x) −U(0) = cx4 > 0, xF(x) = −4cx4 < 0. Thus the origin is a strict energy minimum with a restoring force: x = 0 is stable . (b) Result and interpretation At the two positive displacements, F(d) = −4cd3, F(2d) = −4c(2d)3 = −32cd3. |F(2d)|/|F(d)| = 8 . The vanishing second derivative makes the quadratic test inconclusive; the leading potential and force terms are quartic and cubic, respectively. Physical check The restoring force is nonzero for every nonzero displacement, unlike a flat neutral potential.

Question 9

A local minimum need not have nonzero curvature

A particle moves along xx with potential U(x)=cx4U(x)=cx^4, where c>0c>0. At x=0x=0 both U′U^{\prime} and U′′U^{\prime\prime} vanish.

Diagram shown in the original SVG worksheet.

  1. Classify the equilibrium without relying only on the second derivative test.

  2. Compare the restoring force at displacements dd and 2d2d, with d>0d>0.

Question 9 - Solution

A local minimum need not have nonzero curvature

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

The force is F(x)=−U′(x)=−4cx3.F(x)=-U'(x)=-4cx^3. For every x≠0x\ne0, U(x)−U(0)=cx4>0,xF(x)=−4cx4<0.U(x)-U(0)=cx^4>0,\qquad xF(x)=-4cx^4<0. Thus the origin is a strict energy minimum with a restoring force: x=0 is stable.\boxed{x=0\text{ is stable}}.

(b) Result and interpretation

At the two positive displacements, F(d)=−4cd3,F(2d)=−4c(2d)3=−32cd3.F(d)=-4cd^3,\qquad F(2d)=-4c(2d)^3=-32cd^3. |F(2d)|/|F(d)|=8.\boxed{|F(2d)|/|F(d)|=8}. The vanishing second derivative makes the quadratic test inconclusive; the leading potential and force terms are quartic and cubic, respectively.

Physical check

The restoring force is nonzero for every nonzero displacement, unlike a flat neutral potential.