We compute the billiards that emerge in the Belinskii-KhalatnikovLifshitz (BKL) limit for all pure supergravities in D = 4 spacetime dimensions, as well as for D = 4, N = 4 supergravities coupled to k (N = 4) Maxwell supermultiplets. We find that just as for the cases N = 0 and N = 8 investigated previously, these billiards can be identified with the fundamental Weyl chambers of hyperbolic KacMoody algebras. Hence, the dynamics is chaotic in the BKL limit. A new feature arises, however, which is that the relevant Kac-Moody algebra can be the Lorentzian extension of a twisted affine Kac-Moody algebra, while the N = 0 and N = 8 cases are untwisted. This occurs for N = 5, where one gets A , and for N = 3 and 2, for which one gets A (2)∧ 2 . An understanding of this property is provided by showing that the data relevant for determining the billiards are the restricted root system and the maximal split subalgebra of the finite-dimensional real symmetry algebra characterizing the toroidal reduction to D = 3 spacetime dimensions. To summarise: split symmetry controls chaos.