I was watching a video on Riemannian Geometry. The lecturer mentions that given the defining condition for a connection on a Riemannian manifold $M$ i.e. :
$$\nabla_X(Y) : \chi(M) \times \chi(M) \to \chi(M),$$ where $\chi(M)$ is the set of $C^{\infty}$ vector fields on M, the second of the Cartesian product from where Y comes as does the resulting quantity itself can be looked at as sections of a tangent bundle, while X is supposed to be looked at as a vector field.
The metric compatibility condition as well as the linearity condition in X and the derivative rule in Y makes sense in such a case.
However, when we move onto the torsion-free condition $$\nabla_{X} Y - \nabla_Y X = [X,Y]$$ inherent in Levi-Civita connections, both X,Y and the resulting $\nabla_{X} Y$ are all to be seen as vector fields. So the torsion free condition does not lend itself to the section of a bundle approach.
Can anyone please explain what this means? I was not able to fathom for myself. Thanks.