And yet another approach ...
Again, we're going to show that if the three vectors $\mathbf{u}$, $\mathbf{v}$, $\mathbf{w}$ are not coplanar, then they span $\mathbb{R}^3$.
If $\mathbf{u} \cdot (\mathbf{v} × \mathbf{w}) \ne 0$, we can define three magic new vectors
$\tilde{\mathbf{u}}$, $\tilde{\mathbf{v}}$, $\tilde{\mathbf{w}}$ by the equations
$$
\tilde{\mathbf{u}} = \frac{\mathbf{v} × \mathbf{w}}{\mathbf{u} \cdot (\mathbf{v} × \mathbf{w})} \quad ; \quad
\tilde{\mathbf{v}} = \frac{\mathbf{w} × \mathbf{u}}{\mathbf{u} \cdot (\mathbf{v} × \mathbf{w})} \quad ; \quad
\tilde{\mathbf{w}} = \frac{\mathbf{u} × \mathbf{v}}{\mathbf{u} \cdot (\mathbf{v} × \mathbf{w})}
$$
These three vectors are called the dual vectors of $\mathbf{u}$, $\mathbf{v}$, $\mathbf{w}$, or the reciprocal vectors.
If $\mathbf{x}$ is any given vector, it is straightforward to verify that
$$
\mathbf{x} =
(\mathbf{x} \cdot \tilde{\mathbf{u}})\mathbf{u} +
(\mathbf{x} \cdot \tilde{\mathbf{v}})\mathbf{v} +
(\mathbf{x} \cdot \tilde{\mathbf{w}})\mathbf{w}
$$
This shows that $\mathbf{x}$ lies in the span of $\{\mathbf{u}, \mathbf{v}, \mathbf{w} \}$, and even gives you explicit formulae for the coefficients. This is cute, but it doesn't give you much insight into the geometry of the situation.
The last equation giving $\mathbf{x}$ is just a disguised statement of Cramer's rule, so this approach is strongly related to the previous one.