Let $n \geqslant 2$ be an integer and consider the vector space $V=F^{2n}$ with the standard basis $e_1,\ldots,e_{2n}$.
Now the second exterior power $\Lambda^2(V)$ contains the element $$\omega=e_1 \wedge e_2 + e_3 \wedge e_4 + \cdots + e_{2n-1} \wedge e_{2n}.$$
Since $\Lambda^{2n}(V)$ is spanned by $x := e_1 \wedge \cdots \wedge e_{2n}$, we know that the $n$-fold wedge product $\omega \wedge \cdots \wedge \omega$ is a scalar multiple of $x$.
Question: How do we compute this scalar?
First distribute all terms in the product defining $\omega \wedge \cdots \wedge \omega$ (there are $n$ products). Notice that all of the terms with repeated $x_j$ will vanish by antisymmetricity of the wedge product. Thus you get $$ \omega^{\wedge n} = \sum_{\sigma \in S^*_n} e_{\sigma(1)}\wedge e_{\sigma(1)+1} \wedge \cdots \wedge e_{\sigma(n)}\wedge e_{\sigma(n)+1}$$
where $S_n^*$ denotes the group of all bijections from $\{1,3,5,...,2n-1\}$ unto itself. Next notice that if $\sigma \in S_n^*$, then $e_{\sigma(1)}\wedge e_{\sigma(1)+1} \wedge \cdots \wedge e_{\sigma(n)}\wedge e_{\sigma(n)+1} = e_1 \wedge \cdots \wedge e_n$, because reordering the terms two at a time does not change the sign of the $2n$-form. Consequently, $$\omega^{\wedge n} = \big| S_n^* \big| \cdot e_1 \wedge \cdots \wedge e_n = n! \cdot e_1 \wedge \cdots \wedge e_n$$