Angular momentum L\vec{L} is the rotational analogue of momentum p\vec{p}. For a rotating body L=IωL = I\omega holds, and like p\vec{p} it obeys a conservation law: it is conserved when the system is subject to no net external moments.

Conservation of angular momentum

If the sum of the moments of the external forces about a pole PP is zero, then the total angular momentum about PP is conserved: Mext=0        LtotA=LtotB\ev{\sum\vec{M}_\text{ext} = \vec{0} \;\;\Longrightarrow\;\; \vec{L}_\text{tot}^A = \vec{L}_\text{tot}^B}

The intuition is the same as for momentum: without an external “rotational push”, the system’s overall rotation stays unchanged. But there is a spectacular difference: whereas in translation p=mv\vec{p} = m\vec{v} has a fixed mass, in the rotational case L=IωL = I\omega contains II, which the system can change by redistributing its own mass. If II decreases, ω\omega must increase to keep LL constant — and that is exactly what a skater does when pulling in their arms.

A first example: the disc with the rope

Consider a disc rotating about a pivot while a rope unwinds from its rim, dragging a package that progressively moves away from the centre. Choosing the pivot as the pole, both the pivot’s reaction and the (radial) tension have zero arm or a radial direction: they produce no moment. Hence the total angular momentum is conserved:

(12mdR2+mprA2)ωA=(12mdR2+mprB2)ωB\left(\tfrac{1}{2}m_d R^2 + m_p r_A^2\right)\omega_A = \left(\tfrac{1}{2}m_d R^2 + m_p r_B^2\right)\omega_B

As the package moves further away (rB>rAr_B > r_A), the system’s moment of inertia grows and the angular velocity ωB\omega_B decreases: the system slows down. It is the same mechanism as the skater, in reverse.

Rotational analogue of p\vec{p}

Angular momentum is roughly what momentum is for translation. It is conserved if Mext=0\sum M_\text{ext} = 0, and it is the pivot around which every problem in this section turns.

Anti-Gravity Wheel and angular momentum — Veritasium

Collegamenti

Argomenti: Dinamica rotazionale Concetti: Conservazione del momento angolare · Momento angolare Competenze: Conservazione del momento angolare

Esercizi collegati: Il tuffatore che ruota · Cometa al perielio e all’afelio · Problema — Momento torcente rettangolare e L(t)