I don't disagree with the other answers but I always found that these kinds of limits and interesting properties came much more naturally from what I thought the definition of $e$ really was: that $e^x$ is its own derivative.
From that starting point, let $y=e^x$, so $dy/dx = e^x$. Now, $x = \ln(y)$. And $dx/dy = 1/e^x = 1/y$. So the derivative of $\ln(x)$ is $1/x$.
By first principles, you get:
\begin{equation}
\frac{d\ln(x)}{dx}=\lim_{h->0}\frac{\ln(x+h)-\ln(x)}{h}=\lim_{h->0}\frac{\ln((x+h)/x)}{h}=\lim_{h->0}\ln((1+h/x)^{1/h})=1/x
\end{equation}
So swapping $x$ with $1/x$ and $h$ with $1/n$:
\begin{equation}
x = \lim_{n->\infty}\ln((1+x/n)^n)
\end{equation}
Exponentiating:
\begin{equation}
e^x = \lim_{n->\infty}(1+x/n)^n
\end{equation}
Obviously you just let $x=1$ to get a limit for $e$. For the other side, it's just the Taylor series. The series is super-differentiable and its derivative is itself. In fact, all of $e^x$'s derivatives are $1$ when $x=0$.
If you think about it, there can only be one function which is its own derivative and which goes through (0, 1). Technically, it's a first order differential equation with one initial condition. You can easily approximate it with arbitrary precision by programming or using a spreadsheet: https://docs.google.com/spreadsheet/ccc?key=0Am_ePpIZW9YMdFI3dFlHOFoxWnpXOTVvWnh5X3FOeGc&hl=en_US
You could also just show that the limit on the right is its own derivative as well.
Alternate method using first principles with $e^x$:
\begin{equation}
\frac{de^x}{dx}=\lim_{h->0}\frac{e^{x+h}-e^x}{h}=e^x\lim_{h->0}\frac{e^{h}-1}{h}
\end{equation}
So:
\begin{equation}
\lim_{h->0}\frac{e^h-1}{h}=1
\end{equation}
Rearranging to make $e$ the subject:
\begin{equation}
e=\lim_{h->0}(h+1)^{1/h}=\lim_{n->\infty}(1+\frac{1}{n})^n
\end{equation}