Path Independence of Conservative Forces — Question 3

Section 8-2 · Physics pages 1036–1037

Question 3 One matched pair of routes is not a universal proof A planar position force is⃗F = (y2ˆi) N, with coordinates in meters. Between (0,0) and (2,0), compare paths that rise vertically to y=+1 m or y=−1 m, cross horizontally, then return vertically. A B y = +1 y = −1 Three routes share endpoints; the dashed route lies at y=0. (a) Find work on each of these two paths. (b) Find work along the straight path y=0. (c) What does this imply about using only the first two measurements to establish a potential?
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Question 3 - Solution One matched pair of routes is not a universal proof A B y = +1 y = −1 (a) Only horizontal segments contribute. Only the horizontal legs contribute because⃗F · d⃗r = y2dx: W+ = Z 2 0 (+1)2dx = 2 J , W−= Z 2 0 (−1)2dx = 2 J . (b) Test a third route. On the straight route, y = 0 throughout: W0 = Z 2 0 02dx = 0 . (c) Use the counterexample logically. One detour followed by a straight return forms a counterexample: I⃗ F · d⃗r = W+ −W0 = 2 J̸ = 0. Agreement between two selected routes does not establish path independence. No single-valued potential reproduces the field throughout this region.

Question 3

One matched pair of routes is not a universal proof

A planar position force is F→=(y2î)\vec F=(y^2\,\hat i) N, with coordinates in meters. Between (0,0) and (2,0), compare paths that rise vertically to y=+1 m or y=−1-1 m, cross horizontally, then return vertically.

Diagram shown in the original SVG worksheet.

  1. Find work on each of these two paths.

  2. Find work along the straight path y=0.

  3. What does this imply about using only the first two measurements to establish a potential?

Question 3 - Solution

One matched pair of routes is not a universal proof

Diagram shown in the original SVG worksheet.

(a) Only horizontal segments contribute.

Only the horizontal legs contribute because F→⋅dr→=y2dx\vec F\cdot d\vec r=y^2dx: W+=∫02(+1)2dx=2J,W−=∫02(−1)2dx=2J.\boxed{W_{+}=\int_0^2(+1)^2dx=2\ \mathrm J},\qquad\boxed{W_{-}=\int_0^2(-1)^2dx=2\ \mathrm J}.

(b) Test a third route.

On the straight route, y=0y=0 throughout: W0=∫0202dx=0.\boxed{W_0=\int_0^2 0^2dx=0}.

(c) Use the counterexample logically.

One detour followed by a straight return forms a counterexample: ∮F→⋅dr→=W+−W0=2J≠0.\oint\vec F\cdot d\vec r=W_+-W_0=2\ \mathrm J\ne0. Agreement between two selected routes does not establish path independence. No single-valued potential reproduces the field throughout this region.