Work Done by a General Variable Force — Question 5

Section 7-7 · Physics pages 980–981

Question 5 Identical endpoints can give different work for a variable field A planar force is⃗F = (2yˆi) N, with y in meters. Move a particle from O=(0,0) to B=(3,2). Route A goes horizontally first; route B goes vertically first. x y O B A B route Solid: horizontal-first route A. Dashed: vertical-first route B. (a) Find work along route A. (b) Find work along route B. (c) Find work around the loop that follows A outward and reverses B back to O.
Show solutionHide solution
Question 5 - Solution Identical endpoints can give different work for a variable field x y O B A B route (a) Keep the height on the horizontal segment. The governing relation is WC = ∫ C 2y dx On A, the horizontal segment lies at y=0, so the force vanishes. The vertical segment has dx = 0. Hence WA = 0. (b) Use the different horizontal force. On B, the vertical segment does zero work; the horizontal segment at y=2 has Fx = 4 N through 3 m. Thus WB = 12 J. (c) Reverse the displacement on the return route. The reverse of B contributes −12 J, so loop work is −12 J. These explicit integrals show that endpoint coordinates alone do not specify work for this force field.

Question 5

Identical endpoints can give different work for a variable field

A planar force is F→=(2yî)\vec F=(2y\,\hat i)\,N, with y in meters. Move a particle from O=(0,0) to B=(3,2). Route A goes horizontally first; route B goes vertically first.

Diagram shown in the original SVG worksheet.

  1. Find work along route A.

  2. Find work along route B.

  3. Find work around the loop that follows A outward and reverses B back to O.

Question 5 - Solution

Identical endpoints can give different work for a variable field

Diagram shown in the original SVG worksheet.

(a) Keep the height on the horizontal segment.

The governing relation is WC=∫C2ydx\boxed{W_C=\int_C2y\,dx} On A, the horizontal segment lies at y=0, so the force vanishes. The vertical segment has dx=0dx=0. Hence WA=0W_A=0.

(b) Use the different horizontal force.

On B, the vertical segment does zero work; the horizontal segment at y=2 has Fx=4NF_x=4\ \mathrm N through 3 m. Thus WB=12J.W_B=12\ \mathrm J.

(c) Reverse the displacement on the return route.

The reverse of B contributes −12J-12\ \mathrm J, so loop work is −12J-12\ \mathrm J. These explicit integrals show that endpoint coordinates alone do not specify work for this force field.