Not only can it be done, it is how Taylor did it: B. Taylor, Methodus incrementorum directa et inversa (1715), 21--23,
Prop. VII Theor. III & Coroll. II..
Taylor developed Taylor series through uniformly spaced nodes at $t_j=t_0+j\,\Delta t$, interpolating $x=x(t)$ between $t_0$ (Taylor uses $z$ equally for $t$ and $t_0$) and $t_0+v$, for some increment $v$ in $n$ steps. From Newton's interpolation formula, Taylor derived the formula (Prop. VII)
$$
\sum_{k=0}^n {(t-t_0) \strut\over\strut 1}{(t-t_0-\Delta t) \strut\over\strut 2}
{(t-t_0-2\Delta t) \strut\over\strut 3}\cdots{(t-t_0-(k-1)\Delta t) \strut\over\strut k}
{\Delta^k x \over \Delta t^k}\,.
$$
He wrote the proposition in terms of forward differences, but it is, of course, equivalent to divided differences.
Letting $\Delta t \rightarrow 0$ (Si pro Incrementis evanescentibus scribantur fluxiones...),
Taylor obtained that ${\Delta^k y / \Delta t^k} \rightarrow {d^ky /dt^k}$ and the other factors approach $(t-t_0)^k/k!$, which yields the Taylor series, since $n$ is determined by $v$ and $\Delta t$.
Klein called it a "a limit-taking of unheard-of boldness"
("Hierin liegt nun tatsächlich Grenzübergang von unerhörter Kühnheit"),
Elementarmathematik vom höheren Standpunkte aus: Arithmetik, Algebra, Analysis (1908).