Angular momentum is the rotational analogue of momentum . For a rotating body holds, and like 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 is zero, then the total angular momentum about is conserved:
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 has a fixed mass, in the rotational case contains , which the system can change by redistributing its own mass. If decreases, must increase to keep 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:
As the package moves further away (), the system’s moment of inertia grows and the angular velocity decreases: the system slows down. It is the same mechanism as the skater, in reverse.
Rotational analogue of
Angular momentum is roughly what momentum is for translation. It is conserved if , and it is the pivot around which every problem in this section turns.
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)