Reading a Potential Energy Curve — Question 1

Section 8-5 · Physics pages 1092–1093

Question 1 Reading slopes and kinetic-energy gaps Assume one-dimensional classical motion with K = E −U(x) and Fx = −dU/dx, with no dissipation. A potential graph joins (0 m,6 J), (2 m,2 J), and (4 m,6 J) by straight lines. A 2 kg particle has E=8 J. x (m) U (J) E = 8 6 2 2 4 Straight segments define the potential exactly; the dashed line marks total energy. (a) Find force at x=1 and x=3 m. (b) Find speed at x=1 m and the largest speed on the plotted interval. (c) Explain why the point of largest speed need not have a well-defined derivative in this idealized graph.
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Question 1 - Solution Reading slopes and kinetic-energy gaps x (m) U (J) E = 8 6 2 2 4 (a) Use the negative segment slopes. Take the negative slope on each straight segment: F(1) = −2 −6 2 −0 = +2 N , F(3) = −6 −2 4 −2 = −2 N . (b) Read the vertical energy gap. On the left segment, U(1) = 4 J: v(1) = √ 2(8 −4)/2 = 2 m/s . At the minimum U(2) = 2 J, vmax = √ 2(8 −2)/2 = √ 6 m/s . (c) Separate energy continuity from force smoothness. The continuous energy gap fixes a continuous speed: v(x) = √ 2[E −U(x)]/m. A corner in U changes its one-sided slopes and therefore the force, but does not create a jump in U or speed. The speed maximum exists even without a unique derivative at the corner.

Question 1

Reading slopes and kinetic-energy gaps

Assume one-dimensional classical motion with K=E−U(x)K=E-U(x) and Fx=−dU/dxF_x=-dU/dx, with no dissipation. A potential graph joins (0 m,6 J), (2 m,2 J), and (4 m,6 J) by straight lines. A 2 kg particle has E=8 J.

Diagram shown in the original SVG worksheet.

  1. Find force at x=1 and x=3 m.

  2. Find speed at x=1 m and the largest speed on the plotted interval.

  3. Explain why the point of largest speed need not have a well-defined derivative in this idealized graph.

Question 1 - Solution

Reading slopes and kinetic-energy gaps

Diagram shown in the original SVG worksheet.

(a) Use the negative segment slopes.

Take the negative slope on each straight segment: F(1)=−2−62−0=+2N,F(3)=−6−24−2=−2N.\boxed{F(1)=-\frac{2-6}{2-0}=+2\ \mathrm N},\qquad\boxed{F(3)=-\frac{6-2}{4-2}=-2\ \mathrm N}.

(b) Read the vertical energy gap.

On the left segment, U(1)=4U(1)=4 J: v(1)=2(8−4)/2=2m/s.\boxed{v(1)=\sqrt{2(8-4)/2}=2\ \mathrm{m/s}}. At the minimum U(2)=2U(2)=2 J, vmax=2(8−2)/2=6m/s.\boxed{v_{\max}=\sqrt{2(8-2)/2}=\sqrt6\ \mathrm{m/s}}.

(c) Separate energy continuity from force smoothness.

The continuous energy gap fixes a continuous speed: v(x)=2[E−U(x)]/m.v(x)=\sqrt{2[E-U(x)]/m}. A corner in U changes its one-sided slopes and therefore the force, but does not create a jump in U or speed. The speed maximum exists even without a unique derivative at the corner.