The Center of Gravity — Question 10

Section 12-3 · Physics pages 1830–1831

Question 10 Suspension above the center gives a restoring gravity moment A rigid object of mass M pivots freely about a fixed point a distance d above its center of gravity in uniform gravity. Let θ measure tilt from the hanging-down equilibrium. d G Schematic; labels, not drawing lengths, specify the data. (a) Find its gravity torque and change in potential energy. (b) Compare with the inverted configuration in which the center is directly above the pivot.
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Question 10 - Solution Suspension above the center gives a restoring gravity moment d G (a) Derivation and calculation For a pivot a distance d above G, an angular displacement θ from the hanging orientation gives τ = −Mgd sin θ , ∆U = Mgd(1 −cos θ) . For small displacement, τ ≃−Mgdθ, ∆U ≃1 2Mgdθ2. (b) Result and interpretation Thus the hanging state has positive potential curvature and restoring torque: U′′(0) = Mgd > 0. For a small displacement ϕ from the inverted orientation, U ≃Umax −1 2Mgdϕ2, τ ≃+Mgdϕ. The inverted state is unstable because displacement lowers the energy and the torque increases it. Physical check The sign of the second derivative distinguishes two orientations that both have zero torque at exact alignment.

Question 10

Suspension above the center gives a restoring gravity moment

A rigid object of mass MM pivots freely about a fixed point a distance dd above its center of gravity in uniform gravity. Let θ\theta measure tilt from the hanging-down equilibrium.

Diagram shown in the original SVG worksheet.

  1. Find its gravity torque and change in potential energy.

  2. Compare with the inverted configuration in which the center is directly above the pivot.

Question 10 - Solution

Suspension above the center gives a restoring gravity moment

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

For a pivot a distance dd above GG, an angular displacement θ\theta from the hanging orientation gives τ=−Mgdsin⁡θ,ΔU=Mgd(1−cos⁡θ).\boxed{\tau=-Mgd\sin\theta},\qquad \boxed{\Delta U=Mgd(1-\cos\theta)}. For small displacement, τ≃−Mgdθ,ΔU≃12Mgdθ2.\tau\simeq-Mgd\theta,\qquad\Delta U\simeq\frac12Mgd\theta^2.

(b) Result and interpretation

Thus the hanging state has positive potential curvature and restoring torque: U″(0)=Mgd>0.U''(0)=Mgd>0. For a small displacement ϕ\phi from the inverted orientation, U≃Umax−12Mgdϕ2,τ≃+Mgdϕ.U\simeq U_{\max}-\frac12Mgd\phi^2,\qquad\tau\simeq+Mgd\phi. The inverted state is unstable because displacement lowers the energy and the torque increases it.

Physical check

The sign of the second derivative distinguishes two orientations that both have zero torque at exact alignment.