Terribly sorry if this has been asked, but I'm not about to search 382 pages of technical questions in the field.
I am trying to develop a very basic understanding of what algebraic topology is about. Tried Hatcher, who simply dives into vague terminology I've not heard for reasons that are not clear. The heck is an $n$-cell...? What do you mean, "attached?" How in the heck are $f'$ and $f''$ from $X\to Y$ "connected" by a homotopy...?
I go into May's "Concise" book, which has at least clarified the fundamental idea of the field (algebraic invariants under continuous deformations of the topology, I gather), but the first two sentences leave me wondering how intuitive this book is actually going to be, when it comes to structures with which I'm not already familiar. And he clarifies what Hatcher meant by "connected": $h(x,0) = p(x)$ and $h(x,1) = q(x)$ "connects" $p$ and $q$ by a homotopy $h$... I can see that. But extrapolating from many answers on this site I have read, I will be judged harshly for not simply intuiting this from the vague wording. That's okay, you can think I'm stupid. I've got no problem with that.
But what I'm grasping for, and not finding anywhere, is why I should be interested in algebraic topology in the first place. What does it actually tell us about geometry? I am interested in what can be done in a space where algebraic structures is commensurable with continuous maps, but I am seriously questioning whether the field, as it is, has any true insight to offer me here. It doesn't seem like they're investigating structures with any real relevance to anything, anywhere. I am sure that I am simply lacking imagination here. I'm struggling enough to even grasp the basic concepts in any other light than pure symbol-games, let alone understand what the 'big' theorems are about. Why should I care about fundamental groups or homotopy type? What does it MEAN...? What is algebraic topology REALLY about...? What's the point of it? What does it apply to? I am sure it applies to many results in higher math, but this doesn't interest me. What disciplines in sciences and engineering have made the greatest use of results and language of algebraic topology?
I am starting to have the feeling that nobody really has any idea what they're talking about in these fields. Please prove me wrong. I am utterly perplexed as to what the point is.
Topology immediately poses a question:
This happens because homeomorphisms are the structure-preserving maps of topological spaces, so we are interested in being able to determine when two spaces are "the same thing".
Now, we have compactness: I know that $S^1$ is not the same as $\mathbb{R}$, since "compactness" is invariant under continuous maps. It is arguably the first topological invariant we encounter.
We also have connectedness: I know that one ball is not the same as two separated balls, since one space is connected and the other isn't. I also know that $GL(n,\mathbb{R})$ is not the same as $\mathbb{R}^{n^2}$. Diving a bit more, we also know that $[0,1)$ is not the same as $\mathbb{R}$, since taking $0$ out of the first still leaves a connected set, but taking one point out of $\mathbb{R}$ separates it into two connected components.
Okay, we can also say that $\mathbb{R}$ is not the same as $\mathbb{R}^2$ for a similar reason: taking a point out of $\mathbb{R}$ separates it into two connected components, and taking a point out of $\mathbb{R}^2$ is still connected.
But, unfortunately, those tools are not so powerful as we want. How would you argue that $\mathbb{R}^5$ is not the same as $\mathbb{R}^6$?
Algebraic topology gives us better tools to answer these questions (although it is a homotopy-type "tester" a priori).
Not only that, but homotopy and homology are clearly related to a notion of "holes" in a given space: a notion that is very geometric.
An interesting highly non-trivial application of algebraic topology is Morse Theory. Essentially, it allows you to estimate the number of critical points of a given well-behaved differentiable function of a manifold using the homology of the manifold, and vice-versa.