Abstract In the December 1988 issue of Tile Journal of Canadian Petroleum Technology, Koichi Takamura and Dean Wallace published a paper entitled "The physical chemistry of the hot water process"(1). The paper ‘describes a model for the hot water process based on the’ DLVO and lonizable Surface Group theories' 'that, according to the authors, can be used to maximize bitumen recovery from low grade oil sands. On page 100 the authors claim that 'It is known* * that monodisperse panicles in an unstirred suspension will coagulate if the potential energy barrier to coagulation, Vscb, is less than 20 to 100 kT because the Brownian motion of the particle provides sufficient energy to overcome the repulsion between them. In a stirred reactor, hydrodynamic forces tend to drive the particles together and a higher energy barrier is required to keep them dispersed.' Both sentences above warrant a comment.In colloidal dispersion slow coagulation can be observed for the stability ratio W< 104(2). W is defined as the ratio of rapid to slow coagulation rate constants (kr and ks respectively) and is related to the height and shape of the energy barrier with the following formula:Equation (Available In Full Paper)where the total interaction energy Φ is a function of the separation between the centres of the particles r, and 2R is the radius of ‘sphere of interaction’, which in the simplest model is assumed to be twice the radius of monodispersed, spherical particles R. A stability ratio of about 104 (which means that the coagulation rate is 10 000 times slower than it would have been if no energy barrier was present), for a typical barrier shape, corresponds to the maximum barrier height Φmax of about 15 kT. A barrier of 20 kT or more would thus characterize a stable system.For fine solid particles suspended in liquids, inertia effects can be neglected for Reynolds number (set on particle dimension) Re < 1(3). Under typical industrial conditions, the Reynolds number based on the dimension of the vessel (typically of an order of metres) may be as high as 100 000. However, the Reynolds number based on the particle dimension (of an order of µm) is of about 0.1. The flow, as seen by particles of that size, fulfills the creeping flow conditions, and inertia effects for those particles can be neglected. Therefore, although stirring increases the number of collisions between the particles the hydrodynamic forces cannot ‘drive the particles together’ across the energy barrier. The barrier height necessary for stabilization of the system does not depend on whether the suspension of fines is agitated or not. The barrier height of 400 kT units, assumed by the authors to be a critical value dividing stable from flocculating systems, is thus completely unrealistic. One can barely agree on a critical barrier height of 20 to 40 kT. Yet, even for a barrier of 40 kT, only one in 1017 particles has sufficiently high energy to pass across the barrier.