Exploring $ \sum_{n=0}^\infty \frac{n^p}{n!} = B_pe$, particularly $p = 2$. I was exploring the fact that $$ \sum_{n=0}^\infty \frac{n^p}{n!} = B_pe,$$
where $B_n$ is the $n$th Bell number. 
I found this result by exploring the series on wolframalpha and looking up the sequence of numbers generated. I have no experience with Bell numbers other than knowing that they represent the number of ways of partitioning a set. 
What I tried
Looking at the base case we can verify
$$\sum_{n=0}^\infty \frac{n}{n!} = \sum_{n=1}^\infty \frac{1}{(n-1)!} = e. $$
But then I realize that $n^2$ is going to be difficult.
Specifically what I want
I am doing this for fun, so I just want to glean some sort of lesson out of this. Resources that let me learn for myself are just as good! 
An accepted answer will have any one of the following:


*

*A proof that $\sum_{n = 0}^{\infty} \frac{n^2}{n!} = 2e$ (this interests me a lot)

*A description of why this series is related to Bell numbers and the number of partitions of a set

*A link to some resource that introduces Bell numbers and/or their connection to this series. 

 A: Notice that
\begin{align}
    S
& = \sum_{n = 0}^{\infty} \frac{n^{2}}{n!} \\
& = \frac{0^{2}}{0!} + \frac{1^{2}}{1!} + \frac{2^{2}}{2!} + \frac{3^{2}}{3!} +
    \cdots \\
& = \frac{1}{0!} + \frac{2}{1!} + \frac{3}{2!} + \frac{4}{3!} + \cdots.
\end{align}
Then
\begin{align}
    S - e
& = \left(
    \frac{1}{0!} + \frac{2}{1!} + \frac{3}{2!} + \frac{4}{3!} + \cdots
    \right) -
    \left(
    \frac{1}{0!} + \frac{1}{1!} + \frac{1}{2!} + \frac{1}{3!} + \cdots
    \right) \\
& = \frac{1}{1!} + \frac{2}{2!} + \frac{3}{3!} + \cdots \\
& = e. \qquad (\text{As shown in the OP.}) \\
\end{align}
Therefore, $ S = e + e = 2 e $.

In fact, using the same type of reasoning, it can be shown that $ \displaystyle \sum_{n = 0}^{\infty} \frac{n^{3}}{n!} = 5 e $.

Here is the connection with Bell numbers.
For each $ p \in \mathbb{N}_{0} $, let $ \displaystyle S_{p} \stackrel{\text{df}}{=} \sum_{n = 0}^{\infty} \frac{n^{p}}{n!} $. Notice that
\begin{align}
\forall p \in \mathbb{N}: \quad
    S_{p}
& = \sum_{n = 0}^{\infty} \frac{n^{p}}{n!} \\
& = \sum_{n = 1}^{\infty} \frac{n^{p}}{n!} \qquad
    \left( \text{As $ \dfrac{0^{p}}{0!} = 0 $.} \right) \\
& = \sum_{n = 1}^{\infty} \frac{n^{p - 1}}{(n - 1)!} \qquad
    (\text{After canceling $ n $’s.}) \\
& = \sum_{n = 0}^{\infty} \frac{(n + 1)^{p - 1}}{n!}. \qquad
    (\text{After re-indexing.})
\end{align}
Hence,
\begin{align}
\forall p \in \mathbb{N}_{\geq 2}: \quad
    S_{p} - S_{p - 1}
& = \sum_{n = 0}^{\infty} \frac{(n + 1)^{p - 1}}{n!} -
    \sum_{n = 0}^{\infty} \frac{n^{p - 1}}{n!} \\
& = \sum_{n = 0}^{\infty}
    \frac{1}{n!} \left[ (n + 1)^{p - 1} - n^{p - 1} \right] \\
& = \sum_{n = 0}^{\infty}
    \left[ \frac{1}{n!} \sum_{k = 0}^{p - 2} \binom{p - 1}{k} n^{k} \right]
    \qquad (\text{By the Binomial Theorem.}) \\
& = \sum_{n = 0}^{\infty} \sum_{k = 0}^{p - 2}
    \binom{p - 1}{k} \frac{n^{k}}{n!} \\
& = \sum_{k = 0}^{p - 2}
    \left[ \binom{p - 1}{k} \sum_{n = 0}^{\infty} \frac{n^{k}}{n!} \right] \\
& = \sum_{k = 0}^{p - 2} \binom{p - 1}{k} S_{k}.
\end{align}
Therefore,
$$
\forall p \in \mathbb{N}_{\geq 2}: \quad
  S_{p}
= \sum_{k = 0}^{p - 2} \binom{p - 1}{k} S_{k} + S_{p - 1}
= \sum_{k = 0}^{p - 1} \binom{p - 1}{k} S_{k}.
$$
As $ S_{0} = S_{1} = e $ by inspection, we see that the $ S_{p} $’s are the Bell numbers multiplied by $ e $.
A: Recall  the species  of set  partitions with  the  constituents marked
which is
$$\mathfrak{P}(\mathcal{U}\mathfrak{P}_{\ge 1}(\mathcal{Z}))$$
which gives the generating function
$$G(z, u) = \exp(u(\exp(z)-1)).$$
It follows that the exponential generating function of Bell numbers is
given by
$$G(z) = \exp(\exp(z)-1).$$
Suppose we are trying to compute
$$\sum_{n\ge 0} \frac{n^p}{n!}.$$
Put $$n^p = \frac{p!}{2\pi i}
\int_{|z|=\epsilon} \frac{1}{z^{p+1}} \exp(nz) \; dz.$$
Observe that this gives $n^p = 0$ when $n=0$ except when $p=0$ as well.
We get for the sum
$$\frac{p!}{2\pi i}
\int_{|z|=\epsilon} \frac{1}{z^{p+1}} 
\sum_{n\ge 0} \frac{\exp(nz)}{n!} \; dz
= \frac{p!}{2\pi i}
\int_{|z|=\epsilon} \frac{1}{z^{p+1}} 
\exp(\exp(z)) \; dz
\\ = \exp(1) \times \frac{p!}{2\pi i}
\int_{|z|=\epsilon} \frac{1}{z^{p+1}} 
\exp(\exp(z)-1) \; dz
\\ = \exp(1)\times B_p$$
as claimed.
