Abstract
Gas–liquid volumetric mass transfer coefficient “\({\mathrm{k}}_{\mathrm{L}}\mathrm{a}\)” for \({\mathrm{CH}}_{4}\), \({\mathrm{CO}}_{2}\), and \(\mathrm{Ar}\) were experimentally measured at different conditions in a mimicked Fischer–Tropsch (FT) slurry bubble column reactor by using a non-invasive gaseous tracer technique and the axial dispersion model. Results validate the square root relation, between \({\mathrm{k}}_{\mathrm{L}}\mathrm{a}\) and diffusivity “\({\mathrm{D}}_{\mathrm{g}}\)”, that can be used to predict \({\mathrm{k}}_{\mathrm{L}}\mathrm{a}\) for different species with \({\mathrm{k}}_{\mathrm{L}}\mathrm{a}\) values available in the literature. Additionally, Higbie’s penetration theory was adopted along with bubble dynamics parameters estimation to develop a correlation for predicting \({\mathrm{k}}_{\mathrm{L}}\mathrm{a}\) at wide range of conditions. Current results were used to tune and modify the developed correlation. Predictions of the modified correlation were found to be in line with the findings of previous studies and hence can used to predict \({\mathrm{k}}_{\mathrm{L}}\mathrm{a}\) for different gases including the syngas (i.e., \({\mathrm{H}}_{2}\) and \(\mathrm{CO}\)) at conditions close to FT conditions.
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Abbreviations
- \({\mathrm{k}}_{\mathrm{L}}\mathrm{a}\) :
-
Volumetric mass transfer coefficient, s−1
- \({\mathrm{k}}_{\mathrm{L}}{\mathrm{a}}^{\mathrm{o}}\) :
-
Reference volumetric mass transfer coefficient, s−1
- \({\mathrm{k}}_{\mathrm{L}}{\mathrm{a}}^{\mathrm{estimated}}\) :
-
Volumetric mass transfer coefficient estimated from correlation, s−1
- \({\mathrm{k}}_{\mathrm{L}}{\mathrm{a}}^{\mathrm{exp}}\) :
-
Experimental volumetric mass transfer coefficient, s−1
- \(t\) :
-
Time, s
- \({\mathrm{C}}_{\mathrm{in}}\) :
-
Normalized tracer concentration, mol/m3
- \({\mathrm{C}}_{\mathrm{g},\mathrm{in}}\) :
-
Inlet gas concentration, mol/m3
- \({\mathrm{C}}_{\mathrm{g}}\) :
-
Tracer gas concentration obtained by the detector at the exit, mol/m3
- \({\mathrm{C}}_{\mathrm{inj}}\) :
-
Tracer gas concentration after injection, mol/m3
- \({\mathrm{D}}_{\mathrm{g}}\) :
-
Gas diffusivity, m2/s
- \({{\mathrm{D}}_{\mathrm{g}}}^{\mathrm{o}}\) :
-
Reference gas diffusivity, m2/s
- \({\mathrm{D}}_{\mathrm{L}}\) :
-
Liquid diffusivity, m2/s
- \(\mathrm{H}\) :
-
Henry’s constant, dimensionless
- \({\mathrm{u}}_{\mathrm{g}}\) :
-
Superficial gas velocity, m/s
- \({\mathrm{n}}_{\mathrm{data}}\) :
-
Number of data points
- \({\mathrm{t}}_{\mathrm{e}}\) :
-
Exposure time, s
- \({\mathrm{d}}_{\mathrm{bm}}\) :
-
Geometric mean bubble diameter, m
- \({\mathrm{d}}_{\mathrm{bs}}\) :
-
Sauter mean diameter, m
- \({\mathrm{u}}_{\mathrm{bt}}\) :
-
Terminal bubble rise velocity, m/s
- \(g\) :
-
Acceleration gravity, m2/s
- \(a\) :
-
Interfacial area, m2
- \({\mathrm{d}}_{\mathrm{c}}\) :
-
Column diameter, m
- \({\upvarepsilon }_{\mathrm{L}}\) :
-
Liquid holdup, m3/m3
- \({\upvarepsilon }_{\mathrm{g}}\) :
-
Gas holdup, m3/m3
- \(\uptau\) :
-
Residence time, s
- \({\uprho }_{\mathrm{s}}\) :
-
Solid (catalyst) density, kg/m3
- \({\uprho }_{\mathrm{g}}\) :
-
Gas density, kg/m3
- \({\uprho }_{\mathrm{L}}\) :
-
Liquid density, kg/m3
- \({\upmu }_{\mathrm{L}}\) :
-
Liquid viscosity, Pa
- \(\sigma\) :
-
Surface tension, N/m
- \(\Phi\) :
-
Proportionality constant or arbitrary correction
- FT:
-
Fischer-Tropsch
- SBCRs:
-
Slurry bubble column reactors
- BCRs:
-
Bubble column reactors
- PPH:
-
Perforated plate with huge holes
- SCFM:
-
Standard cubic feet meter
- ADM:
-
Axial dispersion model
- TCD:
-
Thermal conductivity detector
- AARE:
-
Average absolute relative error
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Acknowledgements
The authors are grateful for financial support of the High-Pressure Slurry Bubble Column (HPSBC) Consortium by ConocoPhillips (USA), EniTecnologie (Italy), Sasol (South Africa), and Statoil (Norway).
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This work was conducted in the Chemical Reaction Engineering Laboratory (CREL), Department of Chemical Engineering, Washington University St. Louis, MO, USA.
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Han, L., Taha, M.M., Kamalanathan, P. et al. Experimentation and correlation development of mass transfer in a mimicked Fischer–Tropsch slurry bubble column reactor. Heat Mass Transfer 58, 1133–1143 (2022). https://doi.org/10.1007/s00231-021-03169-9
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DOI: https://doi.org/10.1007/s00231-021-03169-9