Consider the solution of
\begin{equation}
f(x) = 0,
\end{equation}
where $f : \mathbb{R} \rightarrow \mathbb{R}$ is at least two times differentiable with continuous derivatives and has a single root $x=r$ of multiplicity $1$. This last assumption ensures
\begin{equation}
f'(r) \not = 0
\end{equation}
which will be needed later. Let $x_n$ denote an approximation of $r$ obtained by any means necessary. Then by doing a Taylor expansion at $x=x_n$ we obtain
\begin{equation}
0 = f(r) = f(x_n) + f'(x_n)(r-x_n) + \frac{f''(\xi)}{2}(r-x_n)^2
\end{equation}
or equivalently
\begin{equation}
- f(x_n) = f'(x_n)(r-x_n) + \frac{f''(\xi)}{2}(r-x_n)^2
\end{equation}
for at least one $\xi_n$ between $r$ and $x_n$. This allows us to express Newton's iteration as
\begin{equation}
x_{n+1} = x_n - \frac{f(x_n)}{f'(x_n)} = x_n + \frac{f'(x_n)(r-x_n) + \frac{f''(\xi_n)}{2}(r-x_n)^2}{f'(x_n)}
\end{equation}
While obscure, this representation allows us to immediately conclude that
\begin{equation}
r- x_{n+1} = -\frac{f''(\xi_n)}{2 f'(x_n)}{(r-x_n)^2}
\end{equation}
This is the equation which you can use to show convergence of Newton's method. Let us define the error at the $n$th step as
\begin{equation}
e_n = r - x_n
\end{equation}
then we can write
\begin{equation}
e_{n+1} = - \frac{f''(\xi_n)}{2 f'(x_n)} e_n^2
\end{equation}
Now since $f'(r) \not = 0$ we can find an interval $I = [r-\delta,r+\delta]$ surrounding the root and determine a constant $M > 0$ such that
\begin{equation}
\forall : x, y \in I \: : \: \left| \frac{f''(x)}{2 f'(y)} \right| \leq M.
\end{equation}
Here the continuity of $f'$ and $f''$ is critical. Then we can write
\begin{equation}
|e_{n+1}| \leq M |e_n|^2 = (M|e_n|) |e_n|.
\end{equation}
It follows that if $x_0 \in I$ is picked such that
\begin{equation}
M|e_n| \leq \rho < 1
\end{equation}
then not only will the error decrease, but (and this is critical) $x_1$ will belong to $I$, allowing the argument to be repeated, leading to the (pessimistic) estimate
\begin{equation}
e_n \leq \rho^n |e_0|
\end{equation}
which nevertheless establishes (local) convergence of Newton's method.
As the iteration converges, it will sooner rather than later do so quadratically, as
\begin{equation}
\frac{e_{n+1}}{e_n^2} = - \frac{f''(\xi_n)}{2 f'(x_n)} \rightarrow -\frac{f''(r)}{2 f'(r)}, \quad n\rightarrow \infty, \quad n \in \mathbb{N}.
\end{equation}
Here it is critical that Taylor's theorem ensure that $\xi_n$ is betweeen $x_n$ and $r$. Since $x_n \rightarrow r$ the squeeze lemma will ensure that $\xi_n \rightarrow r$ as $n \rightarrow \infty$.