sa1988 said:
So far it's the most 'non-physics' feeling of a subject I've done so far, because it's all just pure maths at the moment, so I need to quickly get to grips with what's going on.
O.k. "so far" is probably right, since you certainly know it better than me. In general it's not true. Relativity theory, particle physics, differential equations, esp. because of the initial conditions, and thus basically everything in physics involves topologies. There is a fundamental difference between open and closed sets and important to get a feeling about them. Mostly you will meet topologies induced by a metric, because in the end, physics is about measurements and therefore distances in some context. Also important here is, that mathematical objects come in pairs: objects and mappings between those objects. E.g. vector spaces and linear mappings, manifolds and diffeomorphisms, groups and homomorphisms, functions and operators, and in this case, topolopgies and continuous functions. You need a topology to define continuity, because a function is continuous in ##\xi## if for every open neighborhood ##U## of ##f(\xi)## the pre-image ##f^{-1}(U)## is an open neighborhood of ##\xi##. This shows the local nature of the concept and that it is not about ##\xi## but the neighborhoods of ##\xi## and ##f(\xi)##. It also shows the physical importance, since really many functions, which are investigated in physics are continuous.
Riiiight, I'm beginning to get it now, thanks. And yeah, I realize now that I missed ##X=\{2,4,6,8\}## for the topology I created, as it needs ##X## to satisfy the first axiom, heh.
Yes.
So now what I'm generally getting from this is that the topology on a set is essentially a way of setting out the first step in how the elements in that set are to be used or understood for the given problem.
Here you begin to miss the essential point. Open and closed are local properties of a space. It has nothing to do with the elements in the space. It is about its regions, i.e. its subsets. Intuitively it's simply:
without the boundary then open, with the boundary then closed. Of course this doesn't mean a lot if you consider finite sets, but usually we deal with infinite sets like functions with some property, the Euclidean space or various other spaces. As you see, the elements or their nature are not decisive here, neighborhoods and (infinite) sequences of points are.
From this, I think I'd be right in saying that metrics can (or must?) then be applied to really start making use of what topology is about? For example, if you place the standard topology on ##R^2## and use a metric ##d(x,y) = max|x_i - y_i|##, you can create an open square with the balls ##B_\epsilon (x) = \{y \in X : d(x,y) < \epsilon \}## , so the square has a vertical and horizontal radius ##\epsilon##. And this only works because ##R^2## is equipped with the standard topology which means all the elements in that square are open, hence a square is described.
The standard topology usually refers to the Euclidean metric ##d(x,y)=\sqrt{x^2+y^2}##. Because of this we talk about open balls. Didn't it sound strange to you as you wrote "the square has a vertical and horizontal radius"? But you are right as it isn't important which metric of the two we chose here. It won't change the properties of the topological space ##\mathbb{R}^2##. But "ball" and "diameter" is a bit weird, if your basis open sets are cubes. A metric is nothing else than a ruler to measure distances. O.k. with spaces of functions or sequences, the ruler might be not as obvious as if we measure the Euclidean distance, but in principle it's nothing else. Now what does "by the metric induced topology" mean? As you wrote, we take the balls ##B_\varepsilon(x) = \{y \in X \, : \, d(x,y) < \varepsilon\}## as open sets. With them we have infinite unions of them as open sets as well. And again, since we define those open balls by a strictly ##<## relation, the boundaries don't belong to them. If we include the boundaries, i.e. ##d(x,y) \leq \varepsilon##, then we get closed sets ##\overline{B}_\varepsilon(x)##. And if you remove some (not all) points, for which ##d(x,y)=\varepsilon## holds, then this set is neither open nor closed. So you see, it's not about points,
it's all about what is around them. And with a metric, we have a measure to define "around". Without a measure (metric), we have to define what we mean by "around", e.g. via a list of open sets if nothing else is available.