Given three vectors $\vec u$, $\vec v$, $\vec w$, and their reciprocals $$ \vec u^{\,\prime} := \frac{\vec v \times \vec w}{(\vec u,\vec v, \vec w)} \qquad \vec v^{\,\prime} := \frac{\vec w \times \vec u}{(\vec u,\vec v, \vec w)} \qquad \vec w^{\,\prime} := \frac{\vec u \times \vec v}{(\vec u,\vec v, \vec w)}$$ where ($(\vec u,\vec v, \vec w) := \vec u \cdot (\vec v \times \vec w)$ is the scalar triple product), show that the reciprocals of $\vec u^{\,\prime}$, $\vec v^{\,\prime}$, and $\vec w^{\,\prime}$ are $\vec u$, $\vec v$, and $\vec w$.
Taking $\vec u$ for instance, which is equal to $$\frac{\vec v^{\,\prime} \times \vec w^{\,\prime}}{(\vec u^{\,\prime},\vec v^{\,\prime}, \vec w^{\,\prime})}$$ what identities can I use to simplify the fraction?
This feels like it'd be somewhat of a trivial proof, but I still couldn't find anything to get closer to a solution.
First of all, $\vec u''$ is a multiple of $\vec v'\times \vec w'$, so it's a multiple of $(\vec u \times \vec w) \times (\vec u \times \vec v)$. We know that the $1$-dimensional subspace of $\mathbb R^3$ orthogonal to $\vec x$ and $\vec y$ is spanned by $\vec x \times \vec y$. Well, $\vec u \times \vec w$ and $\vec u \times \vec v$ are both orthogonal to $\vec u$, so $(\vec u\times \vec w) \times (\vec u \times \vec v)$ is a multiple of $\vec u$, and this means that $\vec u''$ is a multiple of $\vec u$.
To see that it's actually equal to $\vec u$, notice that $$\vec u \cdot \vec u'= \vec u \cdot \frac{\vec v\times \vec w}{\vec u \cdot (\vec v \times\vec w)} =\frac{\vec u \cdot (\vec v\times \vec w)}{\vec u \cdot (\vec v \times\vec w)} = 1$$ and also $$\vec u'' \cdot \vec u' = \vec u' \cdot \frac{\vec v' \times \vec w'}{\vec u' \cdot (\vec v' \times \vec w')} = \frac{\vec u' \cdot (\vec v' \times \vec w')}{\vec u' \cdot (\vec v' \times \vec w')} = 1.$$ So $\vec u \cdot \vec u' = \vec u'' \cdot \vec u'$. In general, if we had $\vec u'' = c \vec u$, then $\vec u'' \cdot \vec u'$ would be $c (\vec u \cdot \vec u')$, so in this case $c=1$ and therefore $\vec u'' = \vec u$.