1989
DOI: 10.1002/aic.690350117
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Study of gas‐to‐liquid mass transfer by dynamic methods in trickle beds

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Cited by 5 publications
(2 citation statements)
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“…Midoux et al determined mass transfer parameters by chemical technique using organic liquids. Goenaga et al used dynamic methods to study gas-to-liquid mass transfer in trickle-bed reactors, indicating a strong dependence of mass transfer coefficient on gas flow rate, while Toppinen et al modeled mass transfer using both Stefan−Maxwell equations and the effective diffusivity method, extracting similar results. Iliuta and Thyrion 54 showed that, in the trickle-flow regime, volumetric liquid mass transfer coefficients obtained by physical and chemical absorption are close and axial dispersion is significant at low liquid velocities and high initial concentration of the liquid reactant.…”
Section: Introductionmentioning
confidence: 99%
“…Midoux et al determined mass transfer parameters by chemical technique using organic liquids. Goenaga et al used dynamic methods to study gas-to-liquid mass transfer in trickle-bed reactors, indicating a strong dependence of mass transfer coefficient on gas flow rate, while Toppinen et al modeled mass transfer using both Stefan−Maxwell equations and the effective diffusivity method, extracting similar results. Iliuta and Thyrion 54 showed that, in the trickle-flow regime, volumetric liquid mass transfer coefficients obtained by physical and chemical absorption are close and axial dispersion is significant at low liquid velocities and high initial concentration of the liquid reactant.…”
Section: Introductionmentioning
confidence: 99%
“…Conceptual Models for Nonaqueous − Aqueous Phase Mass Transfer. The two-resistance theory for mass transfer between two immiscible phases has been successfully used to describe gas−liquid mass transfer in trickle-bed reactors ( , ), volatilization from surface waters ( , ), and contaminant transfer between oil films and water ( , ). For transport across an oil or NAPL interface into the aqueous phase, the flux is where J i is the mass flux of species i into the aqueous phase; is the aqueous-side mass transfer coefficient; is the nonaqueous-side mass transfer coefficient; P i is the nonaqueous−aqueous phase partition coefficient; is the bulk nonaqueous phase concentration of species i ; and is the bulk aqueous phase concentration of species i .…”
Section: Introductionmentioning
confidence: 99%