It is a classic result in geometry that $\mathbb S^1$, $\mathbb S^3$ and $\mathbb S^7$ are parallelizable: they admit a globally defined flat connection (Cartan & Schouten, 1926). Moreover, these are the only parallelizable spheres (Adams Theorem, 1959).We explore the extension of these results for different spacetime signatures and give explicit formulas for the connections for $H^{2,1}$ and $H^{1,2}$ in three dimensions, and for $H^{4,3}$ and $H^{3,4}$ in dimension seven.