[guided]We now expand the left-hand side in the only place where a sign can enter: the antisymmetrised definition of the wedge product. Let $\operatorname{Sh}(k,\ell)$ be the set of $(k,\ell)$-shuffles of the ordered index set $\{0,1,\dots,k+\ell-1\}$. Thus $\sigma\in\operatorname{Sh}(k,\ell)$ means that the first $k$ selected indices remain increasing and the last $\ell$ selected indices remain increasing:
\begin{align*}
\sigma(1)<\cdots<\sigma(k),
\qquad
\sigma(k+1)<\cdots<\sigma(k+\ell).
\end{align*}
For a permutation $\sigma$ of this finite ordered set, let $\operatorname{sgn}(\sigma)\in\{1,-1\}$ denote its permutation sign: $\operatorname{sgn}(\sigma)=1$ when $\sigma$ is even and $\operatorname{sgn}(\sigma)=-1$ when $\sigma$ is odd.
The wedge product is therefore
\begin{align*}
(\alpha\wedge\beta)_p(Y_0,\dots,Y_{k+\ell-1})
=
\sum_{\sigma\in\operatorname{Sh}(k,\ell)}
\operatorname{sgn}(\sigma)\,
\alpha_p(Y_{\sigma(1)},\dots,Y_{\sigma(k)})
\beta_p(Y_{\sigma(k+1)},\dots,Y_{\sigma(k+\ell)}).
\end{align*}
We split this sum into two pieces. In the first piece, the inserted vector $Y_0=V_p$ is one of the arguments of $\alpha_p$. Since the $\alpha$-indices are increasing and $0$ is the smallest possible index, this forces $\sigma(1)=0$. After deleting this first entry, the remaining indices form a $(k-1,\ell)$-shuffle of $\{1,\dots,k+\ell-1\}$. The deletion does not change the sign, because the index $0$ was already in the first position. Hence this first piece is
\begin{align*}
\sum_{\tau\in\operatorname{Sh}(k-1,\ell)}
\operatorname{sgn}(\tau)\,
\alpha_p(V_p,X_{\tau(1)},\dots,X_{\tau(k-1)})
\beta_p(X_{\tau(k)},\dots,X_{\tau(k+\ell-1)}).
\end{align*}
By the definition of interior product,
\begin{align*}
\alpha_p(V_p,X_{\tau(1)},\dots,X_{\tau(k-1)})
=
(\iota_V\alpha)_p(X_{\tau(1)},\dots,X_{\tau(k-1)}).
\end{align*}
Substituting this into the preceding shuffle sum gives exactly the shuffle formula for
\begin{align*}
\bigl((\iota_V\alpha)\wedge\beta\bigr)_p(X_1,\dots,X_{k+\ell-1}).
\end{align*}[/guided]