[step:Compute the matrices of the induced maps in the chosen dual bases]
Let $(w_1^*,\dots,w_n^*)$ be the [dual basis](/theorems/414) of $W^*$ and let $(v_1^*,\dots,v_n^*)$ be the dual basis of $V^*$. For each $j \in \{1,\dots,n\}$ and each $i \in \{1,\dots,n\}$,
\begin{align*}
\Psi(w_j)(v_i)=B(v_i,w_j)=a_{ij}.
\end{align*}
Therefore
\begin{align*}
\Psi(w_j)=\sum_{i=1}^n a_{ij}v_i^*.
\end{align*}
So the matrix of $\Psi:W \to V^*$ with respect to the basis $(w_1,\dots,w_n)$ of $W$ and the dual basis $(v_1^*,\dots,v_n^*)$ of $V^*$ is $A$.
Likewise, for each $i,j \in \{1,\dots,n\}$,
\begin{align*}
\Phi(v_i)(w_j)=B(v_i,w_j)=a_{ij}.
\end{align*}
Hence
\begin{align*}
\Phi(v_i)=\sum_{j=1}^n a_{ij}w_j^*.
\end{align*}
Thus, with the usual column-coordinate convention, the matrix of $\Phi:V \to W^*$ is $A^\top$. Since $\det(A^\top)=\det A$, the determinant of the matrix of $\Phi$ is nonzero exactly when $\det A$ is nonzero.
[/step]