Determining Potential Energy Values — Question 9

Section 8-3 · Physics pages 1068–1069

Question 9 An infinite reference for a decaying force For y at least zero, a downward force is Fy = −A/(1 + y/L)2, with A = 12 N and L = 2 m. Define U to approach zero as y approaches infinity. This force law is supplied; no gravitational inverse-square law is assumed. y/L Fy/A −1 The force magnitude decays toward zero; the area of the entire tail is finite. (a) Find U(y) satisfying the reference. (b) Find U(0), U(2 m), and work from 0 to 2 m. (c) Find the total quasistatic external work needed to move from 0 to arbitrarily large y.
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Question 9 - Solution An infinite reference for a decaying force y/L Fy/A −1 (a) Integrate and impose the limiting value. Integrate the negative force: dU dy = A (1 + y/L)2 ⇒U = − AL 1 + y/L + C. The limit U(∞) = 0 fixes C = 0: U(y) = − 24 1 + y/2 J . (b) Evaluate the finite states. Evaluate endpoints and use the sign convention: U(0) = −24 J, U(2) = −12 J , W0→2 = U(0) −U(2) = −12 J . (c) Use the convergent potential rise. Quasistatic external work equals the potential rise: Wext = lim H→∞[U(H) −U(0)] = 0 −(−24) = 24 J . The force decreases sufficiently rapidly for the work integral to converge despite unbounded travel distance.

Question 9

An infinite reference for a decaying force

For y at least zero, a downward force is Fy=−A/(1+y/L)2F_y=-A/(1+y/L)^2, with A=12A=12 N and L=2L=2 m. Define U to approach zero as y approaches infinity. This force law is supplied; no gravitational inverse-square law is assumed.

Diagram shown in the original SVG worksheet.

  1. Find U(y) satisfying the reference.

  2. Find U(0), U(2 m), and work from 0 to 2 m.

  3. Find the total quasistatic external work needed to move from 0 to arbitrarily large y.

Question 9 - Solution

An infinite reference for a decaying force

Diagram shown in the original SVG worksheet.

(a) Integrate and impose the limiting value.

Integrate the negative force: dUdy=A(1+y/L)2⇒U=−AL1+y/L+C.\frac{dU}{dy}=\frac{A}{(1+y/L)^2}\Rightarrow U=-\frac{AL}{1+y/L}+C. The limit U(∞)=0U(\infty)=0 fixes C=0C=0: U(y)=−241+y/2J.\boxed{U(y)=-\frac{24}{1+y/2}\ \mathrm J}.

(b) Evaluate the finite states.

Evaluate endpoints and use the sign convention: U(0)=−24J,U(2)=−12J,\boxed{U(0)=-24\ \mathrm J,\quad U(2)=-12\ \mathrm J}, W0→2=U(0)−U(2)=−12J.\boxed{W_{0\to2}=U(0)-U(2)=-12\ \mathrm J}.

(c) Use the convergent potential rise.

Quasistatic external work equals the potential rise: Wext=limH→∞[U(H)−U(0)]=0−(−24)=24J.\boxed{W_{\mathrm{ext}}=\lim_{H\to\infty}[U(H)-U(0)]=0-(-24)=24\ \mathrm J}. The force decreases sufficiently rapidly for the work integral to converge despite unbounded travel distance.