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Droplet size regime

Numerical Results. We have evaluated case 21 in more detail. The droplet size regime considered ranges from 100 im to 1,000 fim. The curves including and excluding the convective mass and heat transfer have been marked in the figures with ventilation and no ventilation , respectively. The droplets consist initially of pure ammonia ammonia then vaporizes and water vapor condenses onto the droplet surface. [Pg.626]

In the breakup regimes, a droplet may undergo secondary breakup when the breakup time is reached. The droplet size distribution after bag or multimode breakup may follow the Simmons root-normal distribution pattern 264 with MMD/SMD equal to 1.1,... [Pg.181]

Table 4.11a. Correlations for Mean and Maximum Droplet Sizes Generated by Smooth Flat Vaneless Disks in Direct Droplet Formation Regime... Table 4.11a. Correlations for Mean and Maximum Droplet Sizes Generated by Smooth Flat Vaneless Disks in Direct Droplet Formation Regime...
Table 4.12. Correlations for Mean Droplet Size Generated by Vaneless Disks in Three Droplet Formation Regimes... Table 4.12. Correlations for Mean Droplet Size Generated by Vaneless Disks in Three Droplet Formation Regimes...
In both the Direct Droplet and Ligament regimes, the mean droplet size is inversely proportional to the rotational speed co and the square root of the electrode or disk diameter dp ... [Pg.295]

This approximate relationship is similar to those for centrifugal atomization of normal liquids in both Direct Droplet and Ligament regimes. However, it is uncertain how accurately the model for K developed for normal liquid atomization could be applied to the estimation of droplet sizes of liquid metals Tombergl486 derived a semi-empirical correlation for rotating disk atomization or REP of liquid metals with the proportionality between the mean droplet size, rotational speed, and electrode or disk diameter similar to the above equation. Tornberg also presented the values of the constants in the correlation for some given operation conditions and material properties. [Pg.295]

To test the reliability of the previous method, the authors compared it to an independent measurement of oj. They thus propose an extended version of the previous mean-fleld model, valid at any stage of the coalescence regime, even in presence of broad droplet size distributions. It is obtained by considering that the variation of the total number of coalescence events is proportional to the total surface area per unit volume developed by the droplets of different sizes. The total number of drops and total surface are replaced by summations over all the granulometric size intervals ... [Pg.155]

This equation reflects the possibility to measure [3,0] and Dg, both diameters being directly deduced from the experimental droplet size distributions. Of course, this procedure is to be applied at long times, that is, in the regime governed by coalescence ( >j > D ). In Fig. 5.7, it appears that CO exhibits a regular decrease with time. [Pg.156]

R. Although expressions for this parameter exist, they are derived by a hybrid of molecular mechanical and thermodynamic arguments which are not at present known to be consistent as droplet size decreases (8). An analysis of the size limitation of the validity of these arguments has, to our knowledge, never been attempted. Here we evaluate these expressions and others which are thought to be only asymptotically correct. Ve conclude, from the consistency of these apparently independent approaches, that the surface of tension, and, therefore, the surface tension, can be defined with sufficient certainty in the size regime of the critical embryo of classical nucleation theory. [Pg.18]

Based mainly on the analytical results for single particle motion in impinging streams, Tamir derived a number of expressions for the two parameters for various flow regimes in the two cases with and without chemical reaction, in which the parameters such as the droplet size, the motion times of a particle in the accelerating and decelerating stages, particle to gas velocity ratio at the outlet of the accelerating tube, etc. were involved (see Eqs. 11.2 to 11.25 in Ref. [5]). [Pg.156]

This is simply improved methods to form droplets from a needle. The goal is to produce small droplets/microcapsules with low size dispersion (less than 10%) with a good level of production. To avoid broad size dispersion, the liquid flow must be in the laminar regime (avoiding turbulence), thus a relatively low flow rate is required compared to spraying (see below). In most cases, energy is required to reduce the droplet size (from a few millimeters with simple needle). This has led to the following systems. [Pg.27]

Colloid mill. This type of mill is used extensively in the food industry. A colloid mill is a conical rotator that turns in a stator of the same shape, leaving a very narrow gap between rotor and stator. The liquid is introduced from the top, and flows through the narrow gap. Due to the high rotation rate, and the small size of the gap, the shear forces are very intense, and small droplet sizes can be realized. The regime the mill operates at depends on the viscosity of the mixture. When the mixture is highly viscous, the flow will be laminar. The transition towards turbulent flow is given by the Reynolds number, which characterizes the flow ... [Pg.315]

Again, by assuming that We will be around unity, one can have an estimate of the droplet size obtained The transition in the turbulent regime from viscous-dominated break-up to inertia-dominated break-up, takes place when the droplets are larger than (Walstra 2003) ... [Pg.321]

Figure 15.18. Droplet size as a function of the flow rate of oil through the micro-channel. At lower flow rates, the droplet size is independent of the flow rate (regime 1), while from a certain critical flow rate, the droplets become larger (regime 2) (Dekkers 2003). Figure 15.18. Droplet size as a function of the flow rate of oil through the micro-channel. At lower flow rates, the droplet size is independent of the flow rate (regime 1), while from a certain critical flow rate, the droplets become larger (regime 2) (Dekkers 2003).
On the other hand, the fact that ultrasonic velocity is independent of droplet size In the low and high frequency limits allows droplet concentrations to be determined without prior knowledge of the droplet size distribution from ultrasonic velocity measurements. Whether measurements are to be made In the low- or high-frequency regime depends on the size of the droplets and the range of frequencies which can be measured using available ultrasonic equipment (typically 0.1-100 MHz). [Pg.372]

In bounded flow other relationships hold for example, if the smallest dimension of the part of the apparatus in which the droplets are disrapted (e.g., a slit) is comparable to the droplet size, the flow will always be laminar. A different regime prevails, however, if the droplets are injected directly through a narrow capillary into the continuous phase (injection regime), namely membrane emulsification. [Pg.176]


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See also in sourсe #XX -- [ Pg.294 ]




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