Ab initio quantum chemistry is used to generate a three-dimensional reactive potential-energy surface for the collision of 1 S Al + ions with 1 ∑ g + H 2 molecules. This surface, in a tessellated and locally interpolated form, is used to generate forces for classical trajectory simulations of the 3.98 eV endothermic Al + + H 2 f AlH + + H reactions with initial conditions appropriate to a thermal H 2 sample and an Al + beam of specified center of mass collision kinetic energies in the 3-20 eV range. Our findings indicate that the reaction occurs not on (or near) the collinear path, which has no barrier above the reaction endothermicity, but via a near-C 2V insertive path which spontaneously breaks C 2V symmetry via second-order Jahn-Teller distortion to permit flux to evolve to AlH + + H products. The strong propensity to "avoid" the collinear path and to follow a higherenergy route is caused, at long range, by the ion-quadrupole interaction between Al + and H 2 and, at shorter range, by favorable overlap between the H 2 σ u and Al + 3p obitals. Examination of a large number of trajectories shows clearly that reactive collisions (1) lose much of their initial kinetic energy to the repulsive ionmolecule interfragment potential as the closed-shell Al + and H 2 approach, (2) transfer significant energy to the H-H stretching coordinate, thus weakening the H-H bond, (3) convert initial H 2 rotational motion as well as Al + to H 2 collisional angular momentum into rotational angular momentum of the HAlH + complex, "locking" the H 2 moiety into the insertive near-C 2V geometry about which twisting motion occurs, and (4) allow the Al + ion to form a new bond with whichever H atom is nearest it when the system crosses into regions of the energy surface where the H-Al-H asymmetric stretch mode becomes second-order JahnTeller unstable, thus allowing fragmentation into AlH + + H. These findings, combined with considerations of kinematic factors that distinguish among H 2 , D 2 , and HD, allow us to explain certain unusual threshold and isotope effects seen in the experimental reaction cross-section data on these reactions.