Intuition for $N(\mu, \sigma^2)$ in terms of its infinite expansion To gain deeper insight to the Poisson and exponential random variables, I found that I could derive the random variables as follows: 
I consider an experiment which consists of a continuum of trials on an interval $[0,t)$. The result of the experiment takes the form of an ordered $n$-tuple $\forall n \in \mathbb{N}$ containing distinct points on the interval. Every outcome is equally likely and I measure the size of the set containing tuples of $n$ different points by $I_n$ as:
$$ I_n = \int_0^{t}  \int_0^{x_{n}} \int_0^{x_{n-1}} \cdots \int_0^{ x_2 } dx_1 dx_{2} dx_{3} \dots dx_{n-1} dx_{n} = \frac{ t^n } { n! }$$
It follows that on some interval, $[0,t)$, the probability that the experiment results in an $k$-tuple, $k \in \mathbb{N}$ is
$$P(X(t) = k) = \frac{I_k}{\sum_{n = 0}^{\infty} I_n} = \frac{e^{-t} t^k}{k!}$$
And for $k = 0$, we have $P(X(t) = 0) = e^{-t}$. 
Question:
I was wondering if some similar intuition can applied to derive the Gaussian:
$$\frac{1}{\sqrt{2 \pi \sigma^2}} \exp \big(-\frac{(x-\mu)^2}{2\sigma^2} \big)
\ \text{ or the standard normal, }\  \frac{e^{-x^2}}{\sqrt{\pi}}$$ 
I think that such an intuition might be obtained by gaining more insight into each term in the expansion of $\text{erf}(x)$ as is done for Poisson:
$$
\begin{align}
\text{erf}(x) &= \frac{1}{\sqrt \pi } \int_{-x}^{x} e^{-t^2} dt\\
&= \frac{2}{\sqrt \pi } \big( \sum_{n=0}^{\infty} \frac{ x^{2n+1} }{ n! (2n+1) } \big)^{-1}
\end{align}
$$
Any ideas aside from dismissal of the question are much appreciated!
 A: Take an experiment that has two outcomes, success (S) and failure (F), of probability $p$ and $q=1-p$ respectively. The probability of S after one trial is $p$. The probability of two S after two trials is $p^2$, for one S and one F is $2pq$ and for two F is $q^2$. In general, for $N$ trials, the probability of having k S is given by the Binomial distribution $P_S(k,N)= \frac{N!}{k!(N-k)!}p^k q^{N-k}$. These are just the coefficients in front of the terms in $(p+q)^N$ after multiplying them out
What happens if we take the limit of large $N$? The Binomial coefficients at large $N$ approximate a Gaussian, which can be seen visually by looking at a low row Pascal's Triangle. We can derive it from the above formula. To make this simple let's work with the symmetric case $p=q=1/2$, so that we have
$$
P_S(k,N)= \frac{N!}{k!(N-k)!}\frac{1}{2^N}
$$
An easy way to get the desired result is to exchange the index $k$ for one that starts from the center of the triangle where values are largest $ x\in (-N/2,N/2),\; k=x+N/2$. Then we swap this in and apply Stirling's approximation $n!=\sqrt{2\pi}n^ne^{-n}$:
$$
P_S(x,N)= \frac{N!}{(N/2+x)!(N/2-x)!}\frac{1}{2^N} \approx \frac{2}{\sqrt{2\pi N}}\frac{1}{(1-\frac{4 x^2}{N^2})^{(N+1)/2}}\left(\frac{1-\frac{2x}{N}}{1+\frac{2x}{N}}\right)^x
$$
Finally exponentiation and taking the log we get
$$
P_S(x,N) \approx \frac{2}{\sqrt{2\pi N }} e^{-\frac{1}{2}(N+1)\log(1-\frac{4 x^2}{N^2}) +x(\log(1-\frac{2x}{N})-\log(1+\frac{2x}{N}))
}
$$
Using the expansion $\log(1+x)=x-x^2/2+ \cdots$,  keep everything to order $1/N$
$$
P_S(x,N) \approx \frac{2}{\sqrt{2\pi N}} e^{-\frac{2 x^2}{N}
}
$$
Now you can feel free to tack a on $dx$ and use a transformation of variables to scale $x \rightarrow \sqrt N x/2$ -- then $x$ is an "implicit" variable.
$$
P_S(x,N)dx \approx \frac{1}{\sqrt{2\pi}} e^{-\frac{ x^2}{2}} dx
$$
For general $p,q$, the derivation is similar, see for example 
http://scipp.ucsc.edu/~haber/ph116C/NormalApprox.pdf 
This isn't exactly an infinite expansion like in your example, but there's a similar vein of thought in the conclusion that $N$ choose $k$ limits to a Gaussian type shape for large $N$. 
