Reading a Potential Energy Curve — Question 8

Section 8-5 · Physics pages 1106–1107

Question 8 Comparing equal-energy motion in wells of different width Assume one-dimensional classical motion with K = E −U(x) and Fx = −dU/dx, with no dissipation. Two equal-mass particles each have E=8 J. One moves in UA = x2 J, the other in UB = 4x2 J, with x in meters. x U A B The two wells have the same minimum value but different horizontal widths. (a) Compare their speeds at x=0. (b) Find the positive turning coordinate in each well. (c) Compare the restoring force magnitudes at x=1 m and explain why equal bottom speeds do not mean identical motion.
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Question 8 - Solution Comparing equal-energy motion in wells of different width x U A B (a) Use the equal potential minima. Both wells have U(0) = 0, giving identical bottom kinetic energies: KA(0) = KB(0) = 8 J ⇒vA(0) = vB(0) = √ 16 J/m . (b) Solve U=E separately. Solve the separate turning equations: x2 A = 8 ⇒xA = 2 √ 2 m , 4x2 B = 8 ⇒xB = √ 2 m . (c) Compare local slopes. The restoring slopes differ: FA = −2x, FB = −8x ⇒|FA(1)| = 2 N, |FB(1)| = 8 N . The second well has half the amplitude and four times the force at this position. One common speed does not determine the full trajectory.

Question 8

Comparing equal-energy motion in wells of different width

Assume one-dimensional classical motion with K=E−U(x)K=E-U(x) and Fx=−dU/dxF_x=-dU/dx, with no dissipation. Two equal-mass particles each have E=8 J. One moves in UA=x2U_A=x^2 J, the other in UB=4x2U_B=4x^2 J, with x in meters.

Diagram shown in the original SVG worksheet.

  1. Compare their speeds at x=0.

  2. Find the positive turning coordinate in each well.

  3. Compare the restoring force magnitudes at x=1 m and explain why equal bottom speeds do not mean identical motion.

Question 8 - Solution

Comparing equal-energy motion in wells of different width

Diagram shown in the original SVG worksheet.

(a) Use the equal potential minima.

Both wells have U(0)=0U(0)=0, giving identical bottom kinetic energies: KA(0)=KB(0)=8J⇒vA(0)=vB(0)=16J/m.K_A(0)=K_B(0)=8\ \mathrm J\Rightarrow\boxed{v_A(0)=v_B(0)=\sqrt{16\ \mathrm J/m}}.

(b) Solve U=E separately.

Solve the separate turning equations: xA2=8⇒xA=22m,4xB2=8⇒xB=2m.x_A^2=8\Rightarrow\boxed{x_A=2\sqrt2\ \mathrm m},\qquad4x_B^2=8\Rightarrow\boxed{x_B=\sqrt2\ \mathrm m}.

(c) Compare local slopes.

The restoring slopes differ: FA=−2x,FB=−8x⇒|FA(1)|=2N,|FB(1)|=8N.F_A=-2x,\qquad F_B=-8x\Rightarrow\boxed{|F_A(1)|=2\ \mathrm N,\quad|F_B(1)|=8\ \mathrm N}. The second well has half the amplitude and four times the force at this position. One common speed does not determine the full trajectory.