[step:Compute the local coordinate expression of the induced field]
Let $(U,\varphi)$ be a coordinate chart on $M$ with coordinate functions
\begin{align*}
x_i:U&\to\mathbb{R}
\end{align*}
defined by
\begin{align*}
x_i(q)=\pi_i(\varphi(q)),
\end{align*}
where $\pi_i:\mathbb{R}^n\to\mathbb{R}$ is the $i$th coordinate projection and $n=\dim M$.
For each $p\in U$, define the coordinate derivation $\partial_{x_i}\big|_p:C^\infty(M)\to\mathbb{R}$ by
\begin{align*}
\partial_{x_i}\big|_p(f)=\frac{\partial ((f|_U)\circ\varphi^{-1})}{\partial x_i}(\varphi(p)).
\end{align*}
This is the tangent vector at $p$ associated to the $i$th coordinate direction in the chart $(U,\varphi)$.
For each $i\in\{1,\ldots,n\}$, define a function $a_i:U\to\mathbb{R}$ as follows. Given $p\in U$, choose an open neighbourhood $W\subset U$ of $p$ and a bump function $\chi\in C^\infty(M)$ such that $\chi=1$ on $W$ and $\operatorname{supp}\chi\subset U$. Define a smooth extension $\widetilde{x}_i:M\to\mathbb{R}$ by setting $\widetilde{x}_i=\chi x_i$ on $U$ and $\widetilde{x}_i=0$ on $M\setminus U$. Then $\widetilde{x}_i=x_i$ on $W$, and the extension is smooth because $\chi$ vanishes on a neighbourhood of $M\setminus U$. Set
\begin{align*}
a_i(p)=D(\widetilde{x}_i)(p).
\end{align*}
By the locality proved above, $a_i(p)$ is independent of the chosen neighbourhood, bump function, and extension.
For every $f\in C^\infty(M)$, the tangent vector $X_p$ has the coordinate expression
\begin{align*}
X_p(f)=\sum_{i=1}^n a_i(p)\,\partial_{x_i}\big|_p(f).
\end{align*}
Indeed, the coordinate functions $(x_1,\ldots,x_n)$ form a coordinate system near $p$, and the previous step showed that $X_p$ is a derivation at $p$. Hence the coordinate-basis theorem for tangent derivations in a chart applies: every derivation $v\in T_pM$ has the form
\begin{align*}
v(f)=\sum_{i=1}^n v(x_i)\,\partial_{x_i}\big|_p(f)
\end{align*}
for all smooth functions $f$ defined near $p$, after replacing the local coordinate functions by any global smooth extensions. Applying this to $v=X_p$, the coefficient of $\partial_{x_i}\big|_p$ is its value on the $i$th coordinate function. Here that value is
\begin{align*}
X_p(\widetilde{x}_i)=D(\widetilde{x}_i)(p)=a_i(p),
\end{align*}
where locality justifies using the global extension $\widetilde{x}_i$ because $\widetilde{x}_i=x_i$ near $p$.
[/step]