Determining Potential Energy Values — Question 1

Section 8-3 · Physics pages 1052–1053

Question 1 Choosing a gravitational datum below the laboratory origin A 3 kg object has upward coordinate y measured from a laboratory floor. Gravity is uniform with g = 10 m/s2. Define gravitational potential energy to be zero at y=−2 m. y datum: −2 m floor: 0 m position: 1 m Reference levels are schematic; their numerical heights determine the energy. (a) Determine U(y). (b) Find U at y=1 m and the change from y=1 to y=4 m. (c) What changes if the laboratory floor is chosen as the zero instead?
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Question 1 - Solution Choosing a gravitational datum below the laboratory origin y datum: −2 m floor: 0 m position: 1 m (a) Apply the reference through a definite integral. Use the specified reference in the definite integral: U(y) −U(−2) = − Z y −2 (−mg) ds = 30(y + 2). U(y) = 30(y + 2) J (y in m). (b) Evaluate the function and the difference. Evaluate both states with the same datum: U(1) = 90 J , U(4) = 180 J, ∆U = 180 −90 = 90 J . (c) Shift only the additive constant. Choosing the floor as zero subtracts a constant: eU(y) = 30y = U(y) −60 J, ∆eU = ∆U = 90 J. Forces and gravitational works are unchanged.

Question 1

Choosing a gravitational datum below the laboratory origin

A 3 kg object has upward coordinate y measured from a laboratory floor. Gravity is uniform with g=10g=10 m/s2^2. Define gravitational potential energy to be zero at y=−2-2 m.

Diagram shown in the original SVG worksheet.

  1. Determine U(y).

  2. Find U at y=1 m and the change from y=1 to y=4 m.

  3. What changes if the laboratory floor is chosen as the zero instead?

Question 1 - Solution

Choosing a gravitational datum below the laboratory origin

Diagram shown in the original SVG worksheet.

(a) Apply the reference through a definite integral.

Use the specified reference in the definite integral: U(y)−U(−2)=−∫−2y(−mg)ds=30(y+2).U(y)-U(-2)=-\int_{-2}^{y}(-mg)\,ds=30(y+2). U(y)=30(y+2)J(y in m).\boxed{U(y)=30(y+2)\ \mathrm J}\quad(y\text{ in m}).

(b) Evaluate the function and the difference.

Evaluate both states with the same datum: U(1)=90J,U(4)=180J,ΔU=180−90=90J.\boxed{U(1)=90\ \mathrm J},\qquad U(4)=180\ \mathrm J,\qquad\boxed{\Delta U=180-90=90\ \mathrm J}.

(c) Shift only the additive constant.

Choosing the floor as zero subtracts a constant: Ũ(y)=30y=U(y)−60J,ΔŨ=ΔU=90J.\widetilde U(y)=30y=U(y)-60\ \mathrm J,\qquad\Delta\widetilde U=\Delta U=90\ \mathrm J. Forces and gravitational works are unchanged.