“…Now let us apply Equation (10a) for the case of a ¼ s, b ¼ l, c ¼ v, that is, for the solid particle at a liquid=vapor interface, by taking into account the Young equation: Equation (10b) was used to derive equations for penetration=infiltration of liquids into porous solids of different morphologies: solids with capillaries of different shapes, [31][32][33] solids made of closely packed equal spheres, [34,35] solids made of cylindrical fibers, [36][37][38] solids with irregular porous structure, [39][40][41][42] being the extension of the Carman equation [43,[44][45][46][47][48][49][50][51][52] ). Now, let us apply Equation (10b) to the classical problem of capillary rise.…”