You should not try to "visualize" a single vector as whatever by all means, tried this ever for a five-dimensional one? We can't "visualise" such high-dimensional vectors, but we want to talk of concepts of parallelism or planes or projections (in such vector spaces). You can't "visualise" the vector $(1,2,3,4,5)$, but you may say that it's parallel to $(2,4,6,8,10)$ and that it's projection on the (not visualisable) plane spanned by $(1,0,0,0,0)$ and $(0,1,0,0,0)$ is $(1,2,0,0,0)$. And that transfer can be done with sets of functions.
Take, for example, $\mathbb R^J$ (where $J$ is a non-empty set), the set of real-valued functions defined on $J$. We want consider each member, that is: each function, of $\mathbb R^J$ as a single vector.
First we recall that two functions $f$ and $g$, defined on the same domain, are defined equal, iff they are pointwise equal, that is, $f=g$ iff for all $x$ from the common domain we have $f(x)=g(x)$.
From here we may define the sum of two functions $f$ and $g$, which is a function of its own, pointwise:
Define for $f,g\in \mathbb R^J$ their sum $f+g$ by $(f+g)(x):=f(x)+g(x)$ for all $x\in J$. Furthermore we may define for any real number $c$ the new function $c\cdot f$ by $(c\cdot f)(x):=c\cdot f(x)$.
It's easy to verify that now $\mathbb R^J$ is a real vector space. (It may be infinite-dimensional, but that doesn't matter in this case.) For example, one has to verify that
$$c\cdot (f+g)=c\cdot f+c\cdot g.$$
But that's nearly trivial since by the above definitions
$$\begin{align}\bigl({\bf c\cdot(f+g)}\bigr)(x)&=c\cdot\bigl((f+g)(x)\bigr)\\
&=c\cdot\bigl(f(x)+g(x)\bigr)\\
&=c\cdot f(x)+c\cdot g(x)\\
&=(c\cdot f)(x)+(c\cdot g)(x)\\
&=({\bf c\cdot f+c\cdot g})(x).\end{align}
$$
To give an example, recall that for any non-zero vector $f$ of a vector space $V$ the set $g=\{c\cdot f|c\in \mathbb R\}$ is a straight line through the origin. Now let $J=\mathbb R$, hence $V=\mathbb R^{\mathbb R}$ and let $f$ be a well known function defined by $f(t)=t^2$.
From this point of view the set $g=\{c\cdot f|c\in \mathbb R\}$ is a straight line in $V$ through the origin. Any point $p$ of $g$ is a function $p$ which is defined by $p(t)=c\cdot t^2$.
By the way, the "usual" vector space $\mathbb R^n=\mathbb R^{\{1,\dots,n\}}$ is nothing else as the set of functions $\vec v\colon\{1,\dots,n\}\to\mathbb R$, can you see this? Such a $\vec v$ is determined by the values it takes for $1,\dots,n$, that is by $\vec v(1).\dots,\vec v(n)$; commonly one writes $v_k$ instead of $\vec v(k)$ for $1\leq k\leq n$. And the notation
$$\vec v=\begin{pmatrix}v_1\\
\vdots\\
v_n\end{pmatrix}$$
is nothing else but an abbreviate form of the table of values that $\vec v$ takes on $\{1,\dots, n\}$.
Now take another function $\vec w$ from $\mathbb R^n$. From the above definitions we may compute $\vec v+\vec w$, namely by $(\vec v+\vec w)(k)=\vec v(k)+\vec w(k)$. Now this boils down, abbreviated, to
$$\vec v+\vec w=\begin{pmatrix}v_1+w_1\\
\vdots\\
v_n+w_n\end{pmatrix}.$$