The physical quantities, representative of monodisperse divided solids, are essentially their true density, i.e. ρs, and their diameter dp.
In the case of non-spherical particles, we define dp as the diameter of an equivalent sphere, having the same volume as that of the particle under consideration. We then introduce a sphericity factor Φs, defined as the ratio between the surface area of a sphere of the same volume as the particle, to its true external surface areaSp, i.e. :
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