A lot of algebraic geometry is developed by analogy with differential geometry.
In differential geometry, we speak of manifolds rather than varieties. The main feature of the definition of a manifold is that it is covered by coordinate charts: open sets $U$ together with a (smooth) homeomorphism $x : U \to \mathbb{R}^n$ (or alternatively, to an open subset of $\mathbb{R}^n$). The individual components of $x$ are called coordinates.
As an example, consider the pair of functions $(x,y)$ defined on the Euclidean plane after choosing coordinate axes.
The situation here is not too different. On $\mathbb{A}^n_K$, affine $n$-space over a field $K$, the standard 'coordinate chart' has coordinates given by the $n$ variables. Since we're doing algebra, the 'functions' we can make out of these are polynomials.
The term "coordinate function" here refers to a function we can build out of coordinates — much like the ring of smooth continuous real-valued functions on a manifold. The coordinate ring is the ring of all such functions. (although, I don't think the phrase "coordinate function" tends to be used this way in differential geometry)
For subvarieties $V \subseteq \mathbb{A}^n_K$, we understand coordinate functions to be restrictions of coordinate functions on $\mathbb{A}^n_K$, thus we use the quotient ring of the coordinate ring of $\mathbb{A}^n_K$.
Furthermore, since every element of $K[V]$ can be viewed as the image of $t$ under a unique $K$-homomorphism $K[t] \to K[V]$, we can actually identify coordinate functions on $V$ with algebraic maps $V \to \mathbb{A}^1_K$.
(if we're doing absolute geometry, the target would instead be $\mathbb{A}^1_\mathbb{Z} = \operatorname{Spec} \mathbb{Z}[t]$)