Path Independence of Conservative Forces — Question 6

Section 8-2 · Physics pages 1042–1043

Question 6 A separable force admits an endpoint calculation A force field is⃗F = (−2xˆi −6y ˆj) N, with x,y in meters. Consider A=(0,0) and B=(2,1). x y A B Compare a two-leg route with the straight diagonal; the coordinate values are stated in the prompt. (a) Find work along a horizontal-then-vertical path. (b) Find work along x = 2t, y = t for 0 ≤t ≤1. (c) Construct a potential and explain why it establishes more than agreement between these two paths.
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Question 6 - Solution A separable force admits an endpoint calculation x y A B (a) Integrate the separate components. Integrate along each coordinate leg: W = ∫2 0 (−2x)dx + ∫1 0 (−6y)dy = [−x2]2 0 + [−3y2]1 0 = −7 J . (b) Evaluate the parametrized route. With⃗r(t) = (2t, t), d⃗r = (2, 1)dt and⃗F = (−4t, −6t): W = ∫1 0 [(−4t)(2) + (−6t)(1)]dt = ∫1 0 −14t dt = −7 J . (c) Exhibit a global potential. A globally defined potential is U = x2 + 3y2 + C , −∇U = (−2x, −6y) =⃗F. Therefore WAB = UA −UB on every route in the plane. This construction proves more than agreement between two examples.

Question 6

A separable force admits an endpoint calculation

A force field is F→=(−2xî−6yĵ)\vec F=(-2x\,\hat i-6y\,\hat j) N, with x,y in meters. Consider A=(0,0) and B=(2,1).

Diagram shown in the original SVG worksheet.

  1. Find work along a horizontal-then-vertical path.

  2. Find work along x=2tx=2t, y=ty=t for 0≤t≤10\le t\le1.

  3. Construct a potential and explain why it establishes more than agreement between these two paths.

Question 6 - Solution

A separable force admits an endpoint calculation

Diagram shown in the original SVG worksheet.

(a) Integrate the separate components.

Integrate along each coordinate leg: W=∫02(−2x)dx+∫01(−6y)dy=[−x2]02+[−3y2]01=−7J.W=\int_0^2(-2x)dx+\int_0^1(-6y)dy=[-x^2]_0^2+[-3y^2]_0^1=\boxed{-7\ \mathrm J}.

(b) Evaluate the parametrized route.

With r→(t)=(2t,t)\vec r(t)=(2t,t), dr→=(2,1)dtd\vec r=(2,1)dt and F→=(−4t,−6t)\vec F=(-4t,-6t): W=∫01[(−4t)(2)+(−6t)(1)]dt=∫01−14tdt=−7J.\boxed{W=\int_0^1[(-4t)(2)+(-6t)(1)]dt=\int_0^1-14t\,dt=-7\ \mathrm J}.

(c) Exhibit a global potential.

A globally defined potential is U=x2+3y2+C,−∇U=(−2x,−6y)=F→.\boxed{U=x^2+3y^2+C},\qquad-\nabla U=(-2x,-6y)=\vec F. Therefore WAB=UA−UBW_{AB}=U_A-U_B on every route in the plane. This construction proves more than agreement between two examples.