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Investigation of the structure of two-phase flow model-media in bubble-column bioreactors
Authors:R Buchholz  I Adler  K Schügerl
Institution:(1) Institut für Technische Chemie der Technischen Universität Hannover, Callinstr. 3, D-3000 Hannover 1, Federal Republic of Germany
Abstract:Summary By applying photographic, electrical conductivity, and electrooptical methods, the transverse variation of bubble size and velocity, the local gas hold up, and the local specific gas/liquid interfacial area were estimated in a bench scale bubble-column bioreactor containing model cultivation media. The liquid velocity profile, the transverse turbulence intensity variations, and the turbulence energy dissipation scale were also measured by a hot film turbulence probe and constant temperature anemometer technique.A significant relationship was found between the two-phase flow fluid dynamical state and the transverse variation of the various properties.Symbols M mass - L length - T time - aprime gas/liquid interfacial area L2 - 
$$\frac{{a'}}{V}$$
specific gas/liquid interfacial area with regard to the bubbling layer volume L–1 - D transverse coordinate (measured from the wall of the column) L - d bubble diameter L - d mean bubble diameter L - de dynamic equilibrium (maximum stable) bubble diameter L - dp primary bubble diameter L - ds Sauter bubble diameter L - Esgr specific energy dissipation rate with regard to the volume of the liquid ML–1T–3 - EsgrVL energy dissipation rate ML2T–3 - 
$$E = \frac{{E\rho }}{\rho }$$
, since sgr=1 g/cm3, E has the same numerical value as Esgr. Therefore, the symbol E is used everywhere in the present paper for Esgr for simplicity and called energy dissipation rate (S.s–2=Stokes.s–2) L2T–3 - EG or 
$$\varepsilon _G $$
local relative gas holdup - f (r) cross correlation function - g acceleration of gravity LT–2 - h longitudinal distance from the aerator L - 
$$I = u'/\overline u $$
relative turbulence intensity - NO number of u andumacr crossings T–1 - nB bubble frequency T–1 - r distance between two points 1 and 2 of the cross correlation function L - t time - u instantaneous liquid velocity LT–1 - umacr mean liquid velocity LT–1 - 
$$\overline {u^2 } $$
mean square fluctuation velocity L2T–2 - 
$$u' = \sqrt {u^2 } $$
turbulence intensity LT–1 - wSG superficial gas velocity LT–1 - wSL superficial liquid velocity LT–1 - 
$$\varepsilon _G $$
or EG local relative gas holdup LT–1 - lambda energy dissipation scale L - ngr kinematic liquid viscosity L2T–1 - sgr liquid density M L–3 - delta surface tension M T–2 - tau dynamic turbulence pressure M L–1T–2 Indices p primary (at the aerator) - e equilibrium (far from the aerator)
Keywords:
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