At the liquid-solid interface, the energy of the liquid is different from the bulk resulting from surface tension due to the balance between the attraction between molecules to each other (cohesion) and the attraction to the surface (wetting). While capillary effects are well known and described at the air/liquid/solid interfaces, much less is known on the effects induced in the bulk close to the wall. The present experimental study reveals that nonnegligible interfacial effects can be revealed in the bulk of the liquid using the high wetting power of ceramics. Close to the wall, thermal measurements reveal a progressive temperature drop in the liquid (about 0.15°C). This zone extends up to several millimeters, creates a nonequilibrium/equilibrium interface within the liquid and is balanced at larger distances by a temperature increase. This localized effect is highlighted with strong wetting metal oxide surfaces as ceramics.Keywords: ceramic, wetting, long range interactions, liquid/solid interface.
IntroductionIn the bulk of the liquid, molecules are pulled in every direction by neighboring liquid molecules, resulting in a net force of zero. Close to a surface, the situation is different. The molecules at the boundary do not have other molecules on all sides of them and create some variation of internal pressure [1]. Thermal exchanges that take place in a liquid bulk close to an immersed wall or in between two walls are usually not explored, hardly modelled [2] and considered as restricted to very small length scales [3,4].Recently a submillimetre scale thermal study of liquids under flow has revealed that shearing liquids may induce a cooling effect at low shear rates in ordinary Newtonian liquids as water or low viscous polymer melts [5]. The detailed analysis of this non-equilibrium endothermic process indicates that the cooling is firstly generated at the walls and propagates in the fluid giving rise to the establishment of a thermal shear banding regime along the flow axis [5]. We report here on the situation where no external force is exerted on the liquid; i.e. the quiescent state. We examine the influence of a solid wall strongly interacting (total wetting) with the molecules of liquids as water, glycerol or alkanes on the thermal equilibrium. The liquid is observed in its quiescent bulk away from the liquid-air interface. We report on the identification of a slight temperature fall observed at the vicinity of a wetting wall followed by a slight temperature rise at larger distance from the wall. This situation is particularly observable when the liquid is in strong interaction with the wall (total wetting condition). The attraction energy exercised by the wetting surface to the liquid produces a pressure variation, in correlation with a slowing down of the molecules at the wall and correlatively creates a different thermodynamic equilibrium. The cooling zone is compensated away from the surface by a zone slightly warmer than the average temperature. These wall effects are induced in various d...