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Investigation of the structure of two-phase flow model-media in bubble-column bioreactors

II. Transverse variation of local properties when coalescence-suppressing media are used

  • Biotechnology
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European journal of applied microbiology and biotechnology Aims and scope Submit manuscript

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.

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Abbreviations

M:

mass

L:

length

T:

time

a′:

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

Eσ:

specific energy dissipation rate with regard to the volume of the liquid ML−1T−3

EσVL :

energy dissipation rate ML2T−3

\(E = \frac{{E\rho }}{\rho }\) :

, since σ=1 g/cm3, E has the same numerical value as Eσ. Therefore, the symbol E is used everywhere in the present paper for Eσ 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 andū 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

ū:

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

λ:

energy dissipation scale L

ν:

kinematic liquid viscosity L2T−1

σ:

liquid density M L−3

δ:

surface tension M T−2

τ:

dynamic turbulence pressure M L−1T−2

p:

primary (at the aerator)

e:

equilibrium (far from the aerator)

References

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Buchholz, R., Adler, I. & Schügerl, K. Investigation of the structure of two-phase flow model-media in bubble-column bioreactors. European J. Appl. Microbiol. Biotechnol. 7, 241–249 (1979). https://doi.org/10.1007/BF00498018

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  • DOI: https://doi.org/10.1007/BF00498018

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