Is there a simple physical interpretation for the off-diagonal entries of the moment of inertia tensor?
I know that those entries are de facto necessary to use the tensor to calculate quanties like angular momentum or rotational kinetic energy, and that they can be dispsensed of by switching to principal axes, but that's more of a tautology than a way of understanding them, at least in my opinion.
Another way to phrase this question (I guess): why isn't any set of (linearly independent) axes a set of principal axes for a rigid body?