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Summary mass transfer measurements

The remainder of this book is organized as follows. All bioreactors have common modes of operation, which are described in Chapter 2. General gas-liquid mass transfer considerations are then summarized in Chapter 3. Various hydrodynamic and gas-liquid mass transfer measure techniques are then outlined in Chapter 4, followed by a summary of multiphase flow modeling... [Pg.1]

In many practical applications, gas-liquid mass transfer plays a significant role in the overall chemical reaction rate. It is, therefore, necessary to know the values of effective interfacial area (aL) and the volumetric or intrinsic gas-liquid mass transfer coefficients such as kLah, kL, ktaL, kg, etc. As shown in Section IX, the effective interfacial area is measured by either physical e.g., photography, light reflection, or light scattering) or chemical methods. The liquid-side or gas-side mass-transfer coefficients are also measured by either physical (e.g., absorption or desorption of gas under unsteady-state conditions) or chemical methods. A summary of some of the experimental details and the correlations for aL and kLaL reported in the literature are given by Joshi et al. (1982). In most practical situations, kgaL does not play an important role. [Pg.17]

Knowledge of interfacial areas, drop size distributions, and dispersed phase coalescence rates is essential for accurate description and prediction of mass transfer and chemical reaction rates in liquid-liquid dispersions. In this section, a review of the experimental methods and techniques developed for describing and measuring interfacial area, drop size distributions, and coalescence rates will be given in addition, summaries of important results and correlations are presented. [Pg.221]

Data for such a direct comparison have been pubhshed elsewhere (13), along with a complete description of the tests. A summary of the results is shown in Figure 8, where the conversion efficiency for each of the square channel substrates is plotted against the conversion efficiency for each of the sinusoidal channel substrates, for the peirticular FTP test portion and for each of the three measured gases (HC, CO, and NOx). Here, only the latter part of the first test cycle (bag IB), all of the second cycle (bag 2), and only the latter part of the third test cycle (bag 3B) are included in the comparison. The slope of the best-fit fine to these data is 1.004 0.003, demonstrating that the test results are similar for the two structures, as the Heat Mass Transfer Factor predicts. [Pg.462]

In summary, the dimensionless molar density and temperature profiles are described by the incomplete gamma function. This conclusion is expected for high-shear no-slip interfaces in which the fluid velocity component parallel to the interface (i.e., Vx) varies linearly with independent variable y, measured normal to the solid-hquid interface, within a thin mass transfer boundary layer. [Pg.348]

A study of the condensation of several sublimable materials in a fluidized bed was reported by Ciborowski and Wronski (1962) and a summary of a study on heat and mass transfer processes in a fluidized bed desublimation unit was reported by Knuth and Weinspach (1976). The measurement and correlation of... [Pg.362]

An estimation of the mass transfer coefficients (Kq, Xl), the mass transfer area (fly), and the volume fractions of gas and liquid (ec, el) can be carried out with the correlation equations, which have been developed on the basis of hydrodynamical theories and dimension analysis. The constants incorporated into the equations have subsequently been determined on the basis of experimental data for a number of model systems (such as air-water, oxygen-water, etc.). The dependability of these correlation equations can thus be very different. Usually, the quality of the estimations falls somewhere around 10-30% of the actual values. The correlations presented in the literature should therefore be utilized with great caution, and the validity limitations should be carefully analyzed. However, these correlations are very useful, for example, when performing feasibility studies or planning one s own experimental measurements. A thorough summary of various correlation equations for gas-Kquid reactors is presented by Myllykangas [ 1 ]. Here we will only treat two common gas-Kquid reactors, namely, bubble columns and packed columns, operating in a countercurrent mode. [Pg.563]

In summary, it has to be mentioned that in many studies intrinsic viscosity, inherent viscosity and dilute solution viscosity (DSV) were used in order to monitor the increase of molar mass on monomer conversion. Unfortunately, only a few studies use GPC rather than viscosity measurements. For a few Nd-carboxylate-based catalyst systems linear dependencies of Mn on monomer conversion were established and proof in favor of requirement No. 2 linear increase of Mn with monomer conversion (no irreversible chain transfer) was provided. A more detailed analysis of the data, however, reveals deviations from linearity particularly at low monomer conversions (< 20%). These deviations are particularly pronounced for polymerizations with induction periods. Also the extrapolation of the straight lines to zero monomer conversion reveals intercepts on the Mn-axis. [Pg.120]

The threshold energy for the dissociative electron attachment process e" + SPg(g) = SF "(g) + F(g) has been measured directly by means of mass spectrometry ( .- ). In addition, mass spectrometric studies (5) have been reported on various electron transfer reactions which provide Independent estimates of the enthalpy for the above process. Presented below is a summary of the results derived from these measurements. Also included in the summary are results obtained from an electron-impact study ( ) of the process e + SFgCl(g) = SFg (g) + Cl(g). We assume that the fragment-ions are formed in each process with no excess or kinetic energies. As a result, the derived electron affinities represent lower limits to the true value. Other reported values of EA(SFg) include >1.465 eV (9), 3.2 eV (5) and 3.66 0.04 eV (10). The first two results are based on charge-transfer studies (5-9) while the latter value represents a direct measurement of EA using the magnetron technique (10). [Pg.1159]


See other pages where Summary mass transfer measurements is mentioned: [Pg.521]    [Pg.212]    [Pg.355]    [Pg.55]    [Pg.212]    [Pg.376]    [Pg.455]    [Pg.68]    [Pg.1208]    [Pg.42]   
See also in sourсe #XX -- [ Pg.66 ]




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