Determining Potential Energy Values — Question 2

Section 8-3 · Physics pages 1054–1055

Question 2 Anchoring a potential at a nonzero position A one-dimensional conservative force is Fx = 6 −4x N with x in meters. A reference measurement gives U(1 m)=3 J. Fx x 6 N 3 m The linear force changes sign; equal positive and negative areas are possible. (a) Find U(x). (b) Find U(0) and U(3). (c) Check the force at x=2 m from your potential and find work from 0 to 3 m.
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Question 2 - Solution Anchoring a potential at a nonzero position Fx x 6 N 3 m (a) Integrate with the correct sign. Integrate dU/dx = −Fx and then impose the reference: U(x) = −6x + 2x2 + C, 3 = −6 + 2 + C ⇒C = 7 J. U(x) = 2x2 −6x + 7 J (x in m). (b) Use the same constant at both states. The two endpoint values coincide: U(0) = 7 J , U(3) = 18 −18 + 7 = 7 J . (c) Differentiate and compare endpoints. Differentiate to recover the force and subtract endpoints for work: Fx = −U′(x) = 6 −4x ⇒Fx(2) = −2 N , W0→3 = U(0) −U(3) = 0 . Positive and negative work contributions cancel; the force need not vanish throughout.

Question 2

Anchoring a potential at a nonzero position

A one-dimensional conservative force is Fx=6−4xF_x=6-4x N with x in meters. A reference measurement gives U(1 m)=3 J.

Diagram shown in the original SVG worksheet.

  1. Find U(x).

  2. Find U(0) and U(3).

  3. Check the force at x=2 m from your potential and find work from 0 to 3 m.

Question 2 - Solution

Anchoring a potential at a nonzero position

Diagram shown in the original SVG worksheet.

(a) Integrate with the correct sign.

Integrate dU/dx=−FxdU/dx=-F_x and then impose the reference: U(x)=−6x+2x2+C,3=−6+2+C⇒C=7J.U(x)=-6x+2x^2+C,\qquad3=-6+2+C\Rightarrow C=7\ \mathrm J. U(x)=2x2−6x+7J(x in m).\boxed{U(x)=2x^2-6x+7\ \mathrm J}\quad(x\text{ in m}).

(b) Use the same constant at both states.

The two endpoint values coincide: U(0)=7J,U(3)=18−18+7=7J.\boxed{U(0)=7\ \mathrm J},\qquad\boxed{U(3)=18-18+7=7\ \mathrm J}.

(c) Differentiate and compare endpoints.

Differentiate to recover the force and subtract endpoints for work: Fx=−U′(x)=6−4x⇒Fx(2)=−2N,F_x=-U'(x)=6-4x\Rightarrow\boxed{F_x(2)=-2\ \mathrm N}, W0→3=U(0)−U(3)=0.\boxed{W_{0\to3}=U(0)-U(3)=0}. Positive and negative work contributions cancel; the force need not vanish throughout.