ABSTRACT

The surfaces of most practical materials are heterogeneous (different functional groups, chemical non-uniformity, contaminations, mixtures of different solids, etc) and they are not ideally smooth. Therefore, a material may have different contact angles at local microspots. The averaging of contact angles on the micro­ spots results in an “effective contact angle” for the material. The wetting force, capillary pressure, capillary rise, wicking rate, liquid partitioning between layers, wetting-rewetting, etc. are proportional to cosine of the effective contact angle, 0.