In an earlier paper (Rajan and Heideger, 1971), we reported measurements of mass transfer coefficients determined photographically for extraction from single drops during formation. The system employed was continuous phase resistance controlled, and yet the mass transfer was strongly affected by circulation within the drop, especially in the early formation period. The reported coefficients generally decayed to a nearly steady value long before the drop detached from the forming nozzle, consistent with the subsequent observation (Humphrey et al., 1974) that internal circulation during drop formation can effectively cease before drop detachment. All of the results were correlated as Cumulative mass transfer = const. (formation time)n in which n varied from 0.6 to 2.4 with variation in nozzle diameter and dispersed phase flow rate.No single correlation was obtained for either instantaneous or cumulative mass transfer, because of the large number of variables affecting the exchange between phases. However, in going back to that data, we have observed that the total formation time for any drop is a good correlating parameter for the average mass transfer coefficient integrated over the formation period. Although the linear infusion velocity of the dispersed phase fluid should obviously be important in establishing internal circulation, it appears that total formation time effectively incorporates that with nozzle size and dropdiameter to represent all of the observations. Figure 1 shows this result, in which even the measurements made at different continuous phase velocities are well correlated by a single line.
W. J. HEIDEGER and S. E. DUBOIS
University of WashhgtonSeattle, WA 98195Since circulation was obviously so important even in this continuous phase resistance system, we decided to make the comparable study for a system controlled by the dispersed phase resistance. Photographic measurements similar to those already reported were made, except that in the present study drops of water were formed in a stationary continuous organic phase consisting of 2-ethoxyethyl acetate. The organic was presaturated with water so that no m a s transfer occurred within the continuous phase. Thus m a s was transferred only from the interface into the forming drop and the total resistance to mass transfer at all times resided in the dispersed phase. Again, the instantaneous drop volume was determined by careful measurements on cine photographs and the mass transferred was evaluated by difference between infused volume and measured volume.
RESULTSAs in the previous study, the instantaneous mass transfer coefficients were generally high at the onset of drop formation, decreased rapidly early in the formation period, and then either held constant or increased only slightly until final detachment of the drop from the nozzle. Absolute magnitudes of the coefficients are different from those determined for the continuous phase but, since the system's physical properties (especially diffusivity, dispersed phase viscosity, and interfacia...