[guided]The purpose of this step is to extract only the part of the exterior derivative identity whose bidegree corresponds to $\partial$. Define
\begin{align*}
\pi_{a,b}: A^\bullet(X) \to A^{a,b}(X)
\end{align*}
to be the projection onto the smooth forms of type $(a,b)$. Since $\alpha \in A^{p,q}(X)$ and $\beta \in A^{r,s}(X)$, the wedge product $\alpha \wedge \beta$ has bidegree $(p+r,q+s)$. Applying $d = \partial + \bar\partial$ to such a form produces two possible bidegrees: $\partial(\alpha \wedge \beta)$ has bidegree $(p+r+1,q+s)$, and $\bar\partial(\alpha \wedge \beta)$ has bidegree $(p+r,q+s+1)$. Therefore
\begin{align*}
\pi_{p+r+1,q+s}\bigl(d(\alpha \wedge \beta)\bigr) = \partial(\alpha \wedge \beta).
\end{align*}
Now examine the right-hand side of the exterior derivative Leibniz identity. Since
\begin{align*}
d\alpha = \partial\alpha + \bar\partial\alpha,
\end{align*}
the term $d\alpha \wedge \beta$ splits into two bidegree components. The form $\partial\alpha$ has bidegree $(p+1,q)$, so $\partial\alpha \wedge \beta$ has bidegree $(p+r+1,q+s)$. The form $\bar\partial\alpha$ has bidegree $(p,q+1)$, so $\bar\partial\alpha \wedge \beta$ has bidegree $(p+r,q+s+1)$. Consequently the projection onto bidegree $(p+r+1,q+s)$ keeps exactly the $\partial\alpha$ term:
\begin{align*}
\pi_{p+r+1,q+s}(d\alpha \wedge \beta) = \partial\alpha \wedge \beta.
\end{align*}
The same bookkeeping applies to $d\beta$. Since
\begin{align*}
d\beta = \partial\beta + \bar\partial\beta,
\end{align*}
with $\partial\beta \in A^{r+1,s}(X)$ and $\bar\partial\beta \in A^{r,s+1}(X)$, the wedge product $\alpha \wedge \partial\beta$ has bidegree $(p+r+1,q+s)$, while $\alpha \wedge \bar\partial\beta$ has bidegree $(p+r,q+s+1)$. Therefore
\begin{align*}
\pi_{p+r+1,q+s}(\alpha \wedge d\beta) = \alpha \wedge \partial\beta.
\end{align*}
Applying the projection $\pi_{p+r+1,q+s}$ to
\begin{align*}
d(\alpha \wedge \beta) = d\alpha \wedge \beta + (-1)^{p+q}\alpha \wedge d\beta
\end{align*}
therefore gives
\begin{align*}
\partial(\alpha \wedge \beta) = \partial\alpha \wedge \beta + (-1)^{p+q}\alpha \wedge \partial\beta.
\end{align*}
The sign is unchanged by projection because it came from the ordinary exterior derivative Leibniz rule, where the sign depends on the total degree $p+q$ of $\alpha$.[/guided]