Even if one advocates the breaking down of any torus which is moving/rotating relative to a stationary observer, he must explain why it breaks. And to explain the asymmetry created with this breakdown. Which internal/external forces caused it?
Each piece of the ring is longer as measured by an inertial observer comoving
We, at this problem, don’t care for a “comoving” inertial observer. We care for the stationary observer in the center, who first see stationary and then rotating torus, which should contract. But only in the direction of moving.
Why wouldn’t that also apply to my rope example?
We, at this problem, don’t care for a “comoving” inertial observer. We care for the stationary observer in the center, who first see stationary and then rotating torus, which should contract. But only in the direction of moving.