I'd like to mention another combinatorial result, this time about asymptotics. Let $a_n$ denote the number of ways that $n$ horses can finish in a race (with ties); in other words, $a_n$ is the number of "lists of (nonempty) sets" with $n$ total members. Generating function methods allow you to deduce that
$$A(z) = \sum_{n=0}^{\infty} \frac{a_n}{n!} z^n = \frac{1}{1 - (1 - e^z)} = \frac{1}{2 - e^z}.$$
This function is meromorphic, so the asymptotic behavior of $a_n$ is controlled by its poles. The dominant pole occurs at $z = \ln 2$ with residue $-\frac{1}{2}$, which means that the asymptotic behavior of $a_n$ is given by
$$\frac{a_n}{n!} \approx \frac{1}{2 (\ln 2)^{n+1}}.$$
So far, so real-variable. Where do complex numbers come in? The error in this approximation is controlled by the remaining poles of $A(z)$, all of which are complex. The next two most dominant poles are at $\ln 2 \pm 2 \pi i$ with the same residue, which means that the asymptotic behavior of the error is given by
$$\frac{a_n}{n!} - \frac{1}{2 (\ln 2)^{n+1}} \approx \frac{1}{2 (\ln 2 + 2 \pi i)^{n+1}} + \frac{1}{2 (\ln 2 - 2 \pi i)^{n+1}}.$$
Letting $\frac{1}{\ln 2 + 2 \pi i} = r e^{i \theta}$ where $r = \frac{1}{\sqrt{(\ln 2)^2 + 4 \pi^2}}$ and $\theta = -\arctan \frac{2 \pi}{\ln 2}$, it follows that
$$\frac{a_n}{n!} - \frac{1}{2(\ln 2)^{n+1}} \approx r^{n+1} \cos (n+1)\theta.$$
In other words, the error in the above approximation is quasi-periodic. (Of course there are infinitely many poles, each pair of which also contributes quasi-periodic terms, but as $n$ becomes large these terms become less and less important, most of the time.) This is a phenomenon you can easily see for yourself by actually computing the error for several consecutive values of $n$.
So think about this: even if you correctly guessed the asymptotic behavior of $a_n$ (for instance by making a table of the values $\frac{a_n}{n!}$ (or its inverse, if you are interested in the probability that there are no ties in the race) and noticing that the number of digits grows linearly), and even if you computed experimentally that the error in the approximation is quasi-periodic, how on earth could you possibly have deduced the value of either $r$ or $\theta$ without complex numbers?