The Angular Momentum of a System of Particles — Question 6

Section 11-8 · Physics pages 1702–1703

Question 6 Uniform gravity accelerates the center without changing internal angular momentum A collection of particles interacts through internal central forces and moves in uniform gravity. Ignore air resistance. Define internal angular momentum using positions and velocities relative to its center of mass. C⃗ g Uniform gravity accelerates all masses equally; the mass-weighted relative position sum is zero. (a) Find the external gravity torque about the center. (b) Explain whether internal angular momentum changes even though the center accelerates.
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Question 6 - Solution Uniform gravity accelerates the center without changing internal angular momentum C⃗ g (a) Derivation and calculation About the center, the gravity torque is⃗ τC = ∑⃗ ρi × mi⃗g = (∑ mi⃗ρi ) ×⃗g. By the center-of-mass identity,⃗ τC =⃗0 . (b) Result and interpretation For relative velocities, differentiating internal angular momentum introduces the acceleration correction − ∑⃗ ρi × mi⃗aC = − (∑ mi⃗ρi ) ×⃗aC = 0. Internal central-force torques cancel, so d⃗LC dt =⃗τC = 0 ,⃗ aC =⃗g. The center can accelerate while internal angular momentum stays constant. Physical check About another fixed origin, gravity can have a nonzero moment and change the orbital contribution.

Question 6

Uniform gravity accelerates the center without changing internal angular momentum

A collection of particles interacts through internal central forces and moves in uniform gravity. Ignore air resistance. Define internal angular momentum using positions and velocities relative to its center of mass.

Diagram shown in the original SVG worksheet.

  1. Find the external gravity torque about the center.

  2. Explain whether internal angular momentum changes even though the center accelerates.

Question 6 - Solution

Uniform gravity accelerates the center without changing internal angular momentum

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

About the center, the gravity torque is τ→C=∑ρ→i×mig→=(∑miρ→i)×g→.\vec\tau_C=\sum\vec\rho_i\times m_i\vec g =\left(\sum m_i\vec\rho_i\right)\times\vec g. By the center-of-mass identity, τ→C=0→.\boxed{\vec\tau_C=\vec0}.

(b) Result and interpretation

For relative velocities, differentiating internal angular momentum introduces the acceleration correction −∑ρ→i×mia→C=−(∑miρ→i)×a→C=0.-\sum\vec\rho_i\times m_i\vec a_C =-\left(\sum m_i\vec\rho_i\right)\times\vec a_C=0. Internal central-force torques cancel, so dL→Cdt=τ→C=0,a→C=g→.\boxed{\frac{d\vec L_C}{dt}=\vec\tau_C=0},\qquad\vec a_C=\vec g. The center can accelerate while internal angular momentum stays constant.

Physical check

About another fixed origin, gravity can have a nonzero moment and change the orbital contribution.