Work — Question 1

Section 7-3 · Physics pages 892–893

Question 1 Only the force component along displacement contributes For a constant force, use W =⃗F · ∆⃗r. A cart moves 5 m horizontally right while a constant 20 N pull acts 60◦above the horizontal. The cart has no vertical displacement. cart 20 N at 60◦ 5 m right The force direction and displacement direction are separate data. (a) Find the work of the pull. (b) Find the separate contributions from horizontal and vertical force components. (c) If the same force acts during a 2 m horizontal leftward displacement, find its work.
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Question 1 - Solution Only the force component along displacement contributes cart 20 N at 60◦ 5 m right (a) Take the dot product. The governing relation is W =⃗F · ∆⃗r = Fd cos θ W = 20(5) cos 60◦= 50 J. The full force magnitude times distance would overcount. (b) Inspect both displacement components. Resolve the force along the displacement axes: Fx = 20 cos 60◦= 10 N, Fy = 20 sin 60◦= 10 √ 3 N. Wx = Fx∆x = 10(5) = 50 J, Wy = Fy∆y = 0. A nonzero transverse force contributes no work when its corresponding displacement vanishes. (c) Reverse displacement, not force. Now ∆x = −2 m and the force remains unchanged, so W = 10(−2) = −20 J. Work is a signed scalar.

Question 1

Only the force component along displacement contributes

For a constant force, use W=F→⋅Δr→W=\vec F\cdot\Delta\vec r. A cart moves 5 m horizontally right while a constant 20 N pull acts 60∘60^\circ above the horizontal. The cart has no vertical displacement.

Diagram shown in the original SVG worksheet.

  1. Find the work of the pull.

  2. Find the separate contributions from horizontal and vertical force components.

  3. If the same force acts during a 2 m horizontal leftward displacement, find its work.

Question 1 - Solution

Only the force component along displacement contributes

Diagram shown in the original SVG worksheet.

(a) Take the dot product.

The governing relation is W=F→⋅Δr→=Fdcos⁡θ\boxed{W=\vec F\cdot\Delta\vec r=Fd\cos\theta}

W=20(5)cos⁡60∘=50J.W=20(5)\cos60^\circ=50\ \mathrm J. The full force magnitude times distance would overcount.

(b) Inspect both displacement components.

Resolve the force along the displacement axes: Fx=20cos⁡60∘=10N,Fy=20sin⁡60∘=103N.F_x=20\cos60^\circ=10\ \mathrm N,\qquad F_y=20\sin60^\circ=10\sqrt3\ \mathrm N. Wx=FxΔx=10(5)=50J,Wy=FyΔy=0.W_x=F_x\Delta x=10(5)=50\ \mathrm J,\qquad W_y=F_y\Delta y=0. A nonzero transverse force contributes no work when its corresponding displacement vanishes.

(c) Reverse displacement, not force.

Now Δx=−2m\Delta x=-2\ \mathrm m and the force remains unchanged, so W=10(−2)=−20J.W=10(-2)=-20\ \mathrm J. Work is a signed scalar.