Work Done by the Gravitational Force — Question 1

Section 7-5 · Physics pages 932–933

Question 1 Gravity counts signed height changes along a multistage route Take a uniform gravitational field with g = 10 m/s2, upward y positive, and neglect air resistance. A 2 kg parcel moves from y=1 m up to y=5 m, then down to y=3 m. Other agents prescribe the motion. y 5 m 3 m 1 m The two arrows show successive vertical legs, separated horizontally for clarity. (a) Find gravitational work on each segment. (b) Find total gravitational work and compare with a direct move from y=1 to y=3 m. (c) Why is −mg times the total vertical distance not the correct total work?
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Question 1 - Solution Gravity counts signed height changes along a multistage route y 5 m 3 m 1 m (a) Use the signed displacement in each segment. The governing relation is Wg = ∫yf yi (−mg) dy = −mg(yf −yi) Wg,1 = −20(5 −1) = −80 J, Wg,2 = −20(3 −5) = +40 J. (b) Add and telescope the heights. Total is −40 J, equal to −20(3 −1). In a uniform field, Wg = −mg(yf −yi) for any route. (c) Keep upward and downward contributions distinct. Total vertical distance is 6 m, but gravity does negative work during ascent and positive work during descent. Assigning the same negative sign to both would wrongly give −120 J.

Question 1

Gravity counts signed height changes along a multistage route

Take a uniform gravitational field with g=10g=10 m/s2^2, upward y positive, and neglect air resistance. A 2 kg parcel moves from y=1 m up to y=5 m, then down to y=3 m. Other agents prescribe the motion.

Diagram shown in the original SVG worksheet.

  1. Find gravitational work on each segment.

  2. Find total gravitational work and compare with a direct move from y=1 to y=3 m.

  3. Why is −mg-mg times the total vertical distance not the correct total work?

Question 1 - Solution

Gravity counts signed height changes along a multistage route

Diagram shown in the original SVG worksheet.

(a) Use the signed displacement in each segment.

The governing relation is Wg=∫yiyf(−mg)dy=−mg(yf−yi)\boxed{W_g=\int_{y_i}^{y_f}(-mg)\,dy=-mg(y_f-y_i)}

Wg,1=−20(5−1)=−80J,Wg,2=−20(3−5)=+40J.W_{g,1}=-20(5-1)=-80\ \mathrm J,\qquad W_{g,2}=-20(3-5)=+40\ \mathrm J.

(b) Add and telescope the heights.

Total is −40J-40\ \mathrm J, equal to −20(3−1)-20(3-1). In a uniform field, Wg=−mg(yf−yi)W_g=-mg(y_f-y_i) for any route.

(c) Keep upward and downward contributions distinct.

Total vertical distance is 6 m, but gravity does negative work during ascent and positive work during descent. Assigning the same negative sign to both would wrongly give −120J-120\ \mathrm J.