Following work by Slater and Bunker, the unimolecular rate constant versus collision frequency, k uni (ω,E), is expressed as a convolution of unimolecular lifetime and collisional deactivation probabilities. This allows incorporation of nonexponential, intrinsically non-RRKM, populations of dissociating molecules versus time, N(t)/N(0), in the expression for k uni (ω,E). Previous work using this approach is reviewed. In the work presented here, the biexponentialand f 1 + f 2 = 1. With these two constraints, there are two adjustable parameters in the biexponential N(t)/N(0) to represent intrinsic non-RRKM dynamics. The rate constant k 1 is larger than k(E) and k 2 is smaller. This biexponential gives k uni (ω,E) rate constants that are lower than the RRKM prediction, except at the high and low pressure limits. The deviation from the RRKM prediction increases as f 1 is made smaller and k 1 made larger. Of considerable interest is the finding that, if the collision frequency ω for the RRKM plot of k uni (ω,E) versus ω is multiplied by an energy transfer efficiency factor β c , the RRKM k uni (ω,E) versus ω plot may be scaled to match those for the intrinsic non-RRKM, biexponential N(t)/N(0), plots. This analysis identifies the importance of determining accurate collisional intermolecular energy transfer (IET) efficiencies.