Suppose we have addition and multiplication tables for the vector space. For the addition table, all the vectors in the space appear in the first column, and likewise for the first row. Then, to determine $\mathbf{v} + \mathbf{w}$ for some vectors $\mathbf{v}, \mathbf{w} \in V$, we simply look at the entry associated with row $\mathbf{v}$ and column $\mathbf{w}$.
For the multiplication table, the first column will list the elements of the scalar field, and first row will list the vectors. To find out what $c \mathbf{v}$ is for some $c \in F$ and $\mathbf{v} \in V$, we simply go down to the row labeled with $c$ and across to the column labeled with $\mathbf{v}$ and read that entry.
We say two vector spaces are isomorphic if their operation tables are the same up to relabeling of the elements. In other words, suppose $V$ is a vector space over $F$ and $V'$ a vector space over $F'$. If we can find bijections $V \rightarrow V'$ and $F \rightarrow F'$ such that applying these to the operation tables for $V$ yields the operation tables for $V'$, then $V \cong V'$.
More generally, linear transformations between vector spaces (that aren't necessarily isomorphisms) still "transport" structure from one vector space to another. Algebra, by and large, is the study of algebraic structures and the transformations / homomorphisms between them; there is quite a bit of analogy to be made between vector space transformations, group homomorphisms, ring homomorphisms, and so forth. My answer here provides more detail in the context of ring homomorphisms, and the ideas are more-or-less applicable to any other structure -- vector spaces, modules, groups -- with only minor changes to the notation / wording.