Let's look at it from the point of view of the dimension of the eigenspace. Being an eigenvalue means that there's a nontrivial corresponding eigenspace, i.e. the dimension has to be at least $1$. And on the other hand, this dimension cannot exceed the multiplicity of the eigenvalue. So we have the following double inequality:
$$1\le\dim(\text{eigenspace})\le\text{multiplicity of eigenvalue}.$$
If the multiplicity is $1$, then from this double inequality we immediately see that the dimension has to be $1$ too.
In fact, I find the following terminology more illuminating. There are two types of multiplicities defined for an eigenvalue $\lambda$: the algebraic multiplicity of $\lambda$ is its multiplicity as a root of the characteristic equation, while the geometric multiplicity of $\lambda$ is the dimension of the corresponding eigenspace. With this terminology, the double inequality above can be stated as
$$1\le\text{geom.mult.}(\lambda)\le\text{alg.mult.}(\lambda).$$
Even if we really care about the geometric multiplicity, i.e, about eigenspaces and their dimensions, it's not easy to find, as that requires much more work. That's one reason why we care about algebraic multiplicities: they are easier to find, and at least they tell us something, some bounds on those dimensions. And if we're lucky to discover that all eigenvalues are distinct, we know all dimensions (all equal to $1$) without doing too much work!