Natural Derivation of the Closed Form
The first way of handling geometric series I saw, was to derive the closed form for the finite sum. Discovering this derivation seems pretty reasonable if one stares at the geometric sum long enough:
$$
\begin{align}
S&=1+a+a^2+\dots+a^{n-1}\tag{1a}\\
aS&=\phantom{1+{}}a+a^2+\dots+a^{n-1}+a^n\tag{1b}\\
(1-a)S&=1\phantom{{}+a+a^2+\dots+a^{n-1}}-a^n\tag{1c}\\
S&=\left.\left(1-a^n\right)\middle/(1-a)\right.\tag{1d}
\end{align}
$$
Explanation:
$\text{(1a)}$: write out the summation
$\text{(1b)}$: multiply by $a$
$\text{(1c)}$: subtract $\text{(1b)}$ from $\text{(1a)}$
$\text{(1d)}$: divide by $1-a$
Euler-Maclaurin Sum Formula
The Euler-Maclaurin Sum Formula can also be applied. If we ignore the error term, the Euler-Maclaurin Sum Formula becomes $\frac{D}{1-e^{-D}}D^{-1}f$, where $D^{-1}$ is indefinite integration (which introduces the constant that appears in the formula). This is discussed a bit in this answer.
Let $a\gt0$ and $a\ne1$. Note that $D^{-1}a^x=\frac{a^x}{\log(a)}+C$. For non-negative $k\in\mathbb{Z}$, $D^ka^x=\log(a)^ka^x$.
$$
\begin{align}
\frac{D}{1-e^{-D}}D^{-1}a^x
&=\frac{D}{1-e^{-D}}\left(\frac{a^x}{\log(a)}+C\right)\tag{2a}\\[3pt]
&=\frac{\log(a)}{1-\frac1a}\frac{a^x}{\log(a)}+C\tag{2b}\\
&=\frac{a^{x+1}-1}{a-1}\tag{2c}
\end{align}
$$
Explanation:
$\text{(2a)}$: apply $D^{-1}$
$\text{(2b)}$: each application of $D$ simply introduces a factor of $\log(a)$
$\phantom{\text{(2b):}}$ thus, an application of $f(D)$ simply multiplies by $f(\log(a))$
$\text{(2c)}$: simplify and set $C=-\frac1{a-1}$ to match $\sum\limits_{k=0}^xa^k$ at $x=0$
For $a\in\left(e^{-2\pi},e^{2\pi}\right)\setminus\{1\}$, the series given by the Euler-Maclaurin Sum Formula actually converges, rather than merely giving an asymptotic expansion.
I am not proposing the Euler-Maclaurin Sum Formula as a way to initially approach the Geometric Sum Formula. I present it more as a point of interest. A demonstration of analyzing the series as one might other, more complicated, series.