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Area for Bubbles Rising in a Vessel

Example 16 Interfacial Area for Bubbles Rising in a Vessel... [Pg.88]

Two complementai y reviews of this subject are by Shah et al. AIChE Journal, 28, 353-379 [1982]) and Deckwer (in de Lasa, ed.. Chemical Reactor Design andTechnology, Martinus Nijhoff, 1985, pp. 411-461). Useful comments are made by Doraiswamy and Sharma (Heterogeneous Reactions, Wiley, 1984). Charpentier (in Gianetto and Silveston, eds.. Multiphase Chemical Reactors, Hemisphere, 1986, pp. 104—151) emphasizes parameters of trickle bed and stirred tank reactors. Recommendations based on the literature are made for several design parameters namely, bubble diameter and velocity of rise, gas holdup, interfacial area, mass-transfer coefficients k a and /cl but not /cg, axial liquid-phase dispersion coefficient, and heat-transfer coefficient to the wall. The effect of vessel diameter on these parameters is insignificant when D > 0.15 m (0.49 ft), except for the dispersion coefficient. Application of these correlations is to (1) chlorination of toluene in the presence of FeCl,3 catalyst, (2) absorption of SO9 in aqueous potassium carbonate with arsenite catalyst, and (3) reaction of butene with sulfuric acid to butanol. [Pg.2115]

In these equations, a is the specific interfacial area for a significant degree of surface aeration (m2/m3), I is the agitator power per unit volume of vessel (W/m3), pL is the liquid density, o is the surface tension (N/m), us is the superficial gas velocity (m/s), u0 is the terminal bubble-rise velocity (m/s), N is the impeller speed (Hz), d, is the impeller diameter (m), dt is the tank diameter (m), pi is the liquid viscosity (Ns/m2) and d0 is the Sauter mean bubble diameter defined in Chapter 1, Section 1.2.4. [Pg.711]

This is the holdup as a volume fraction of fluid in the vessel. It is the volume of dispersed phase (e.g., gas) in the vessel divided by the total volume. This is a variable strongly affected by the mixing conditions. In Chapter 11 there are several correlations for this variable. Holdup (d>) times a gives total mass transfer surface area per unit vessel volume, which is often called a. Thus, one often sees correlations of kta versus mixing parameters. It should always be remembered that this value contains implicitly the holdup and the bubble size. One way to think of holdup is as the ratio of the superficial gas velocity to the bubble rise velocity. This comes from a simplistic picture of the motion of the gas phase ... [Pg.792]


See other pages where Area for Bubbles Rising in a Vessel is mentioned: [Pg.249]    [Pg.266]    [Pg.118]    [Pg.232]    [Pg.45]    [Pg.143]    [Pg.2135]    [Pg.1131]    [Pg.2121]    [Pg.118]    [Pg.363]    [Pg.46]   


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