Reading a Potential Energy Curve — Question 10

Section 8-5 · Physics pages 1110–1111

Question 10 A cusp minimum and the limits of a derivative test Assume one-dimensional classical motion with K = E −U(x) and Fx = −dU/dx, with no dissipation. An ideal potential is U(x) = 2|x| J with x in meters. A 1 kg particle is released from rest at x=2 m. Away from zero, use the ordinary one-sided slopes; no additional impulse acts at zero. x (m) U (J) 4 2 −2 The continuous V-shaped potential has a stable cusp at the origin. (a) Find force for x<0 and x>0. (b) Find speed as the particle crosses x=0. (c) Explain why the cusp is a stable minimum even though dU/dx is not defined there.
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Question 10 - Solution A cusp minimum and the limits of a derivative test x (m) U (J) 4 2 −2 (a) Take slopes on the open sides. The one-sided slopes give F(x) = { +2 N, x < 0, −2 N, x > 0. Both forces point toward the cusp. (b) Use continuity of potential and kinetic energy. The release energy is E = U(2) = 4 J. At the origin, 1 2(1)v2 = 4 −0 ⇒v = 2 √ 2 m/s . The finite force switch supplies no extra impulse, so velocity remains continuous. (c) Use the minimum and restoring directions. The energy minimum is strict: U(x) −U(0) = 2|x| > 0 (x̸ = 0). Small displacements increase U and produce a restoring force. The smooth condition U′ = 0 is inapplicable at a cusp; assigning zero static force exactly at the origin does not alter the crossing work.

Question 10

A cusp minimum and the limits of a derivative test

Assume one-dimensional classical motion with K=E−U(x)K=E-U(x) and Fx=−dU/dxF_x=-dU/dx, with no dissipation. An ideal potential is U(x)=2|x|U(x)=2|x| J with x in meters. A 1 kg particle is released from rest at x=2 m. Away from zero, use the ordinary one-sided slopes; no additional impulse acts at zero.

Diagram shown in the original SVG worksheet.

  1. Find force for x<0 and x>0.

  2. Find speed as the particle crosses x=0.

  3. Explain why the cusp is a stable minimum even though dU/dxdU/dx is not defined there.

Question 10 - Solution

A cusp minimum and the limits of a derivative test

Diagram shown in the original SVG worksheet.

(a) Take slopes on the open sides.

The one-sided slopes give F(x)={+2N,x<0,−2N,x>0.\boxed{F(x)=\begin{cases}+2\ \mathrm N,&x<0,\\-2\ \mathrm N,&x>0.\end{cases}} Both forces point toward the cusp.

(b) Use continuity of potential and kinetic energy.

The release energy is E=U(2)=4E=U(2)=4 J. At the origin, 12(1)v2=4−0⇒v=22m/s.\tfrac12(1)v^2=4-0\Rightarrow\boxed{v=2\sqrt2\ \mathrm{m/s}}. The finite force switch supplies no extra impulse, so velocity remains continuous.

(c) Use the minimum and restoring directions.

The energy minimum is strict: U(x)−U(0)=2|x|>0(x≠0).U(x)-U(0)=2|x|>0\quad(x\ne0). Small displacements increase U and produce a restoring force. The smooth condition U′=0U'=0 is inapplicable at a cusp; assigning zero static force exactly at the origin does not alter the crossing work.