Clean and surfactant laden water jets were injected into otherwise still air; and silicone oils of various viscosity grades were injected into clean water and aqueous surfactant solutions. The tubes used to form the jets have diameters from 200 to 800 microns and are long enough to assure fully developed flow at the capillary tip. Several non-ionic surfactants, all insoluble in silicone oils, were added in turn to the aqueous phase. It should be noted that our two series of experiments are quite different. In the first series, surfactant must diffuse from within the jet to the water-air interface. In the latter, surfactant must diffuse from within the surrounding matrix phase to the oil jet interface. However, surfactant transport to the interface always occurs within the aqueous phase.
Two distinct CCD cameras were used to image droplets. A low frame rate (1 fps), high resolution camera was used to measure breakup length and to quantify droplet population statistics. A high frame rate (5,000 fps), moderate resolution camera was employed to observe detailed breakup phenomena. An automated image processing algorithm was used to acquire droplet geometry and population statistics. To aid in data interpretation, interfacial tension and other relevant interfacial properties were acquired/estimated using both static and dynamic Pendant Drop techniques.
We will report the effect of surfactant concentration, jet discharge flow rate, oil phase viscosity and capillary diameter on jet breakup length; and on primary and satellite droplet size distributions and relative population size. The data will be interpreted with respect to the relevant physicochemical phenomena. We will also discuss our future plans in the context of what can realistically be accomplished in the short term.