Work — Question 2

Section 7-3 · Physics pages 894–895

Question 2 A constant force ignores the route but not the endpoints For a constant force, use W =⃗F · ∆⃗r. A constant force (4, −3) N acts while a particle goes from O=(0,0) to B=(3,2) m. Route I is straight; route II goes first to A=(3,0), then to B. II I O A B Route II follows the two solid legs; route I is the dashed diagonal. (a) Find work on route I. (b) Find work on each leg of route II and the total. (c) Find work by this same force on the return straight from B to O, and on the complete loop.
Show solutionHide solution
Question 2 - Solution A constant force ignores the route but not the endpoints II I O A B (a) Use total displacement. The governing relation is Wif = Fx(xf −xi) + Fy(yf −yi) WI = 4(3) −3(2) = 6 J. (b) Add signed segment contributions. O to A gives 12 J; A to B gives −6 J. The total is 6 J because the constant force can be factored out of the sum of displacement vectors. (c) Reverse the endpoint difference. Return work is −6 J and loop work is zero. The traveled distance is nonzero on the loop, but ∑ ∆⃗r = 0 for this unchanged force.

Question 2

A constant force ignores the route but not the endpoints

For a constant force, use W=F→⋅Δr→W=\vec F\cdot\Delta\vec r. A constant force (4,−3)(4,-3) N acts while a particle goes from O=(0,0) to B=(3,2) m. Route I is straight; route II goes first to A=(3,0), then to B.

Diagram shown in the original SVG worksheet.

  1. Find work on route I.

  2. Find work on each leg of route II and the total.

  3. Find work by this same force on the return straight from B to O, and on the complete loop.

Question 2 - Solution

A constant force ignores the route but not the endpoints

Diagram shown in the original SVG worksheet.

(a) Use total displacement.

The governing relation is Wif=Fx(xf−xi)+Fy(yf−yi)\boxed{W_{if}=F_x(x_f-x_i)+F_y(y_f-y_i)}

WI=4(3)−3(2)=6J.W_I=4(3)-3(2)=6\ \mathrm J.

(b) Add signed segment contributions.

O to A gives 12 J; A to B gives −6J-6\ \mathrm J. The total is 6 J because the constant force can be factored out of the sum of displacement vectors.

(c) Reverse the endpoint difference.

Return work is −6J-6\ \mathrm J and loop work is zero. The traveled distance is nonzero on the loop, but ∑Δr→=0\sum\Delta\vec r=0 for this unchanged force.