Trying to go in historical order here and begin with Bernoulli's formulation for $e$:
$$e = \lim_{n \to \infty} (1 + 1/n)^n$$
How do we then make the jump to
$$e^x = \lim_{n \to \infty} (1 + x/n)^n$$
I had tried doing this:
$$e^x = (\lim_{n \to \infty} (1 + 1/n)^n)^x$$
$$e^x = \lim_{n \to \infty} (1 + 1/n)^{nx}$$
Let $m = nx$ so $n = m/x$. As $n$ goes to infinity, $m$ also goes to infinity, so:
$$e^x = \lim_{m \to \infty} (1 + x/m)^{m}$$
(although we could relabel with $n=m$ I just use $m$ to use a different one)
But I was told that I'm skipping many unproven assumptions doing this. Is there an easy way to prove what I am missing or is there an easier way to arrive at the result?
Firstly observe that for $y\in \mathbb{R}\quad y\to +\infty$ with $y\in(n,n+1)$
$$\left(1+\frac{1}{n+1}\right)^n=\frac{ \left(1+\frac{1}{n+1}\right)^{n+1} }{\left(1+\frac{1}{n+1}\right)}\le\left(1+\frac{1}{y}\right)^y\le\left(1+\frac{1}{n}\right)^{n+1}=\left(1+\frac{1}{n}\right)^{n}\left(1+\frac{1}{n}\right)$$
thus for squeeze theorem
$$\left(1+\frac{1}{y}\right)^y\to e$$
It easy to see that the same limit holds also for $y\in \mathbb{R}\quad y\to -\infty$.
Then note that $\forall x\in\mathbb{R}\setminus\{0\}$ fixed, since $y=\frac{n}{x}\to \pm\infty\,$ by continuity and algebraic rules for limits we have that
$$\lim_{n \to \infty}\left(1+\frac{x}{n}\right)^n=\lim_{n \to \infty}\left[\left(1+\frac{x}{n}\right)^{\frac{n}x}\right]^x=\left[\lim_{y \to \pm\infty}\left(1+\frac{1}{y}\right)^{y}\right]^x\to e^x$$
For $x=0 \implies e^0 = \lim_{n \to \infty} (1 + 0/n)^n=1$.
Thus the identity holds $\forall x\in\mathbb{R}$.