AlephClo said:
i) The definition of continuity that is used is:
The map F: M into N is continuous if for all V that belongs to Powersets(N) the preimage,f(V) is an open in Powersets(M). M and N are sets on which the differentiable manifolds are built
Well, the purpose of my post was to make you aware of some more intuitive definitions, which are equivalent to the less intuitive definitions that you are questioning. In terms of neighborhoods, continuity of ##F## at a point ##x\in M## just means that for every neighborhood ##V## of ##f(x)##, there exists a neighborhood ##U## of ##x## such that ##F(U)\subseteq V##. A function is then said to be continuous, if it is continuous everywhere. The similarity to the ##\epsilon##-##\delta## definition of continuity in ##\mathbb R^n## should be apparent. If you define an open set to be a set, which is a neighborhood of all of its points, then the standard topology definition of continuity follows automatically. (By the way, the set of open sets is usually
not the whole power set. Otherwise, the space would only admit a ##0##-dimensional manifold structure.)
However, you don't need to worry about this, if you just adopt the manifold definition given in do Carmo's book. It doesn't require any knowledge about general topology at all.
ii) The particular application is General Relativity, if this can help to nail the physical meaning.
In GR, we use manifolds to generalize the idea of Minkowski spacetime to spacetimes that look like Minkowski spacetime only locally. The notion of open sets in such spacetimes just arises as a mathematical consequence of the definition. It doesn't have any physical significance, but if you study objects that look like Minkowski spacetime locally, you cannot not have open sets.