Unit: Energy and Momentum of Rotating Systems

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When an extended object undergoes translation while also rotating about its own axis, its total angular momentum has two parts: orbital and spin.

Orbital angular momentum comes from the motion of the center of mass with respect to some pivot. Treat the object as a point particle at its center of mass:

Lorbital=MvCMrL_{\mathrm{orbital}} = M v_{\mathrm{CM}} r_{\perp}

Here MM is the total mass of the object, vCMv_{\mathrm{CM}} is the center-of-mass speed, and rr_{\perp} is the perpendicular distance from the pivot to the velocity vector.

Spin angular momentum comes from rotation about the center of mass:

Lspin=ICMωL_{\mathrm{spin}} = I_{\mathrm{CM}} \omega

Here ICMI_{\mathrm{CM}} is the rotational inertia about the center of mass and ω\omega is the angular velocity of self-rotation.

The total angular momentum about the pivot is the sum:

Ltotal=Lorbital+LspinL_{\mathrm{total}} = L_{\mathrm{orbital}} + L_{\mathrm{spin}}

For motion in 2D, use signs to indicate direction. Counterclockwise is positive; clockwise is negative. The two contributions may reinforce or oppose each other.

... continued in the full lesson.

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