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Drops micron-size

Two effects are of predominant importance during drop formation. The primary goal of dispersing one phase into the other is to create a large interfacial area available for mass transfer. Subdivision into micron-size droplets will create enormous interfacial area. But one must also be concerned with the recovery of pure phases, and there is therefore an optimum drop size below which dispersion becomes undesirable. [Pg.54]

Dispersions may be classified into two types, based upon size range of the droplets formed. Turbulence creators (mixing impellers, mixing valves, eductors, orifice plates) will produce fine emulsions of micron-size droplets. Nozzles, perforated plates, bubble caps, tower packings, etc., can form discrete drops of relatively large size which will quickly settle through the continuous phase. [Pg.54]

Drops accelerated by an air stream may split, as described in Chapter 12. For drops which do not split, measured drag coefficients are larger than for rigid spheres under steady-state conditions (R2). The difference is probably associated more with shape deformations than with the history and added mass effects discussed above. For micron-size drops where there is no significant deformation, trajectories may be calculated using steady-state drag coefficients (SI). [Pg.305]

The levitation of a micron-sized particle provides the opportunity to examine the thermochemistry of the particle and phase transformations it may undergo with no interferences from foreign surfaces [42-44]. Moreover, since the diffusion times are small, the composition becomes uniform throughout the particle much more rapidly than it would in a bulk quantity of the particulate material. Applications of the EDB to systems other than those of environmental interest seem promising. Polymerization reactions in small drops can be followed by levitating a droplet of polymer precur-... [Pg.284]

More than a century ago, Pickering [2] and Ramsden [3] investigated paraffin-water emulsions contains solid particles such as iron oxide, silicon dioxide, barium sulfate, and kaolin and discovered that these micron-sized colloids generate a resistant film at the interface between the two immiscible phases, inhibiting the coalescence of the emulsion drops. These so-called Pickering emulsions are formed by the self-assembly of colloidal particles at fluid-fluid interfaces in two-phase liquid systems (Fig. 1). [Pg.41]

In Ref. 429, it was established that for micron-sized nondeformed droplets, the surfactant in the drop phase can slightly influence the velocity of film thinning [in contrast to the case of deformed drops, Fig. 15, described by Eq. (256)]. [Pg.390]

Theoretically, flocculation has been described using a kinetic model and using statistical thermodynamics. When two drops of millimeter size collide, one usually observes the formation of a planar film between them. For micron-size emulsions it is not clear whether such a deformation will occur, since on the one hand smaller drops possess higher capillary pressure which opposes their deformation, whereas on the other hand they undergo intensive Brownian motion giving rise to an additional force enhancing the deformation. Only a few studies were published where emulsion stability to flocculation was explained taking into... [Pg.23]

Figure 4.32 summarizes results from the SEM microscopy studies of the rice leaf along with water sessile drop data [97]. In terms of surface texture, rice leaf exhibits submillimeter groove structure with width at 200 pm and height 45 pm (Fig. 4.32c, d). Each groove is made of micron-size papillae array lining up in the direction of the groove, and the entire surface is covered with nano-size hairy plant wax (Fig. 4.32a). This hierarchical snrface stmctnre has resulted in a very... Figure 4.32 summarizes results from the SEM microscopy studies of the rice leaf along with water sessile drop data [97]. In terms of surface texture, rice leaf exhibits submillimeter groove structure with width at 200 pm and height 45 pm (Fig. 4.32c, d). Each groove is made of micron-size papillae array lining up in the direction of the groove, and the entire surface is covered with nano-size hairy plant wax (Fig. 4.32a). This hierarchical snrface stmctnre has resulted in a very...
The filter elements should remove particles of five microns, must be water-resistant, have a high flow rate capability with low pressure drop, possess high dirt-retention capacity, and be rupture-resistant. The clean pressure drop should not exceed five psig at 100 °F (38 °C). The elements must have a minimum collapse differential pressure of 50 psig. Pleated-paper elements are preferred—provided they meet these requirements. Usually, the pleated-paper element will yield the five psig clean drop when used in a filter that was sized to use depth-type elements. This result is due to the greater surface area of the pleated element, more than twice the area of a conventional stacked disc-type or other depth-type elements. [Pg.551]

Type Particle Size (Microns) Efficiency (%] ure Drop... [Pg.255]

For these units the usual particle size for removal is greater than 2 microns with a loading rate of greater than 0.1 grains/cu ft, with a collection efficiency of 99% . The pressure drop is very low for a range of gas velocity through the unit of 100-600 fl/min [40]. [Pg.280]


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See also in sourсe #XX -- [ Pg.85 ]




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Micronization

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