Work Done by the Gravitational Force — Question 7

Section 7-5 · Physics pages 944–945

Question 7 Gravity work follows the field direction in rotated coordinates In a perpendicular but tilted laboratory coordinate system, uniform gravitational acceleration has components (6, −8) m/s2. A 2 kg particle is displaced by (4, 3) m. Other agents may prescribe the route. x y⃗ g ∆⃗r The drawn coordinate axes are tilted relative to true horizontal and vertical. (a) Find gravity work for this displacement. (b) Explain the geometric meaning of the result. (c) Find gravity work for displacement (0, −4) m in the same coordinates.
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Question 7 - Solution Gravity work follows the field direction in rotated coordinates x y⃗ g ∆⃗r (a) Use the complete gravitational force vector. The governing relation is Wg = m⃗g · ∆⃗r⃗ Fg = 2(6, −8) = (12, −16) N. Thus Wg = 12(4) −16(3) = 0. (b) Check perpendicularity to the field. (6, −8) · (4, 3) = 0, so the displacement is perpendicular to true down. A change in the coordinate labeled y need not be a change in physical height when the axes are tilted. (c) Project the second displacement. Wg = 12(0) + (−16)(−4) = 64 J. Its magnitude is less than mg(4) = 80 J because the displacement is not exactly along gravity.

Question 7

Gravity work follows the field direction in rotated coordinates

In a perpendicular but tilted laboratory coordinate system, uniform gravitational acceleration has components (6,−8)(6,-8) m/s2^2. A 2 kg particle is displaced by (4,3)(4,3) m. Other agents may prescribe the route.

Diagram shown in the original SVG worksheet.

  1. Find gravity work for this displacement.

  2. Explain the geometric meaning of the result.

  3. Find gravity work for displacement (0,−4)(0,-4) m in the same coordinates.

Question 7 - Solution

Gravity work follows the field direction in rotated coordinates

Diagram shown in the original SVG worksheet.

(a) Use the complete gravitational force vector.

The governing relation is Wg=mg→⋅Δr→\boxed{W_g=m\vec g\cdot\Delta\vec r}

F→g=2(6,−8)=(12,−16)N.\vec F_g=2(6,-8)=(12,-16)\ \mathrm N. Thus Wg=12(4)−16(3)=0.W_g=12(4)-16(3)=0.

(b) Check perpendicularity to the field.

(6,−8)⋅(4,3)=0,(6,-8)\cdot(4,3)=0, so the displacement is perpendicular to true down. A change in the coordinate labeled y need not be a change in physical height when the axes are tilted.

(c) Project the second displacement.

Wg=12(0)+(−16)(−4)=64J.W_g=12(0)+(-16)(-4)=64\ \mathrm J. Its magnitude is less than mg(4)=80Jmg(4)=80\ \mathrm J because the displacement is not exactly along gravity.