I'd like to understand higher homotopy groups better and I guess there's no simpler way than understanding them for as simple spaces as possible; therefore $S^2$.
My question essentially has two parts, one geometrical and one computational. First part is not really about spheres per se but I think it should be easier to answer in this context
what do those groups really tell us about $S^2$ and where does all the complexity come from? I mean, naively, I would expect most of the groups to be trivial (as for $S^1$). This probably means that I don't yet have an intuitive grasp of higher homotopy groups; so intuition is what I am looking for in this part.
have those groups been computed completely (or at least, is there an algorithm to compute them)? I know the theory of higher-dimensional spheres is complicated but perhaps the case of $S^2$ (and therefore also $S^3$) might be a bit simpler.
Regarding 2., wikipedia page mentions that the problem has been reduced to combinatorial group theory of Brunnian braids. Could someone expound on this or provide additional reductions to purely combinatorial problems?
For a pointed space $X$ let $\Omega X$ denote the loop space of loops $S^1 \to X$ respecting base-points. For non-pathological $X$ we can equip $\Omega X$ with the compact-open topology and we have the natural identification $\pi_n(\Omega X) \cong \pi_{n+1}(X)$.
Now $\pi_1$ is pretty intuitive. It tells us how complicated loops in $X$ can be up to homotopy. Equivalently, it tells us about the connected components of $\Omega X$. But it doesn't tell us how complicated those connected components themselves are. To think about that we look at $\pi_1(\Omega X) \cong \pi_2(X)$. When this is nontrivial, it means that there are loops in $\Omega X$ (or "loops between loops") that are not homotopy-equivalent.
Similarly $\pi_3(X) \cong \pi_2(\Omega X) \cong \pi_1(\Omega^2 X)$ tells us about how complicated "loops between loops between loops" are. In other words, the fact that the higher homotopy groups of $S^2$ are nontrivial tells us that the iterated loop spaces of $S^2$ are complicated.
By contrast, every connected component of $\Omega S^1$ is contractible by looking at the universal cover.