Reading a Potential Energy Curve — Question 6

Section 8-5 · Physics pages 1102–1103

Question 6 A tangent gives force while the curve gives kinetic energy Assume one-dimensional classical motion with K = E −U(x) and Fx = −dU/dx, with no dissipation. Near x=2 m, U(x) = (x −3)2 + 2 J. The tangent at x=2 passes through (1 m,5 J) and (3 m,1 J). A 2 kg particle there has E=7 J. x (m) U (J) (1,5) (3,1) U(x) Dashed line: the tangent at x=2. Solid curve: the actual potential. (a) Find force at x=2 from the tangent. (b) Find speed at x=2 from the actual curve. (c) Would substituting the tangent value at x=3 into a later energy calculation be exact?
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Question 6 - Solution A tangent gives force while the curve gives kinetic energy x (m) U (J) (1,5) (3,1) U(x) (a) Use the tangent slope. The tangent gives the local derivative: dU dx 2 = 1 −5 3 −1 = −2 J/m ⇒F(2) = +2 N . (b) Read the potential itself. Use the actual potential value for energy: U(2) = (2 −3)2 + 2 = 3 J, K = 7 −3 = 4 J. v(2) = q 2(4)/2 = 2 m/s . (c) Keep a local linearization local. The tangent model and exact function differ away from the contact point: Utan(x) = 3 −2(x −2), Uexact(x) −Utan(x) = (x −2)2. At x = 3, they give 1 J and 2 J respectively. A tangent supplies the local slope, not exact finite-interval energy values.

Question 6

A tangent gives force while the curve gives kinetic energy

Assume one-dimensional classical motion with K=E−U(x)K=E-U(x) and Fx=−dU/dxF_x=-dU/dx, with no dissipation. Near x=2 m, U(x)=(x−3)2+2U(x)=(x-3)^2+2 J. The tangent at x=2 passes through (1 m,5 J) and (3 m,1 J). A 2 kg particle there has E=7 J.

Diagram shown in the original SVG worksheet.

  1. Find force at x=2 from the tangent.

  2. Find speed at x=2 from the actual curve.

  3. Would substituting the tangent value at x=3 into a later energy calculation be exact?

Question 6 - Solution

A tangent gives force while the curve gives kinetic energy

Diagram shown in the original SVG worksheet.

(a) Use the tangent slope.

The tangent gives the local derivative: dUdx|2=1−53−1=−2J/m⇒F(2)=+2N.\left.\frac{dU}{dx}\right|_2=\frac{1-5}{3-1}=-2\ \mathrm{J/m}\Rightarrow\boxed{F(2)=+2\ \mathrm N}.

(b) Read the potential itself.

Use the actual potential value for energy: U(2)=(2−3)2+2=3J,K=7−3=4J.U(2)=(2-3)^2+2=3\ \mathrm J,\quad K=7-3=4\ \mathrm J. v(2)=2(4)/2=2m/s.\boxed{v(2)=\sqrt{2(4)/2}=2\ \mathrm{m/s}}.

(c) Keep a local linearization local.

The tangent model and exact function differ away from the contact point: Utan(x)=3−2(x−2),Uexact(x)−Utan(x)=(x−2)2.U_{\mathrm{tan}}(x)=3-2(x-2),\qquad U_{\mathrm{exact}}(x)-U_{\mathrm{tan}}(x)=(x-2)^2. At x=3x=3, they give 1 J and 2 J respectively. A tangent supplies the local slope, not exact finite-interval energy values.