Abstract
A batch cylindrical photocatalytic reactor, externally irradiated by 1–6 UV fluorescent lamps and containing a stirred slurry of polycrystalline TiO2, was modeled by coupling a modified Langmuir–Hinshelwood kinetics together with a two-dimensional light intensity field. The radiation field has been determined on the main assumptions of diffuse radiation, isotropic scattering and negligible backward reflected photon flow. The model has been applied to the photocatalytic oxidation of organic substrates which do not undergo homogeneous photochemical degradation. The model is characterized by the following four parameters: the kinetic constants of substrate adsorption, desorption and degradation and the exponent of the power law expressing the kinetics dependence on the light intensity. The model constants may be determined by applying a simple least-squares best fitting procedure.
Appendix A: Geometrical derivation of r1and r2as a function of θ, r0and R
The coordinate system used was indicated by (x, y) in Figure 6.

Geometric scheme referred to reactor and lamp (grey).
![[28]](/document/doi/10.1515/ijcre-2012-0049/asset/graphic/ijcre-2012-0049_eq28.png)
![[29]](/document/doi/10.1515/ijcre-2012-0049/asset/graphic/ijcre-2012-0049_eq29.png)
Substituting eq. [29] in eq. [28]:
![[30]](/document/doi/10.1515/ijcre-2012-0049/asset/graphic/ijcre-2012-0049_eq30.png)
Developing the square present in eq. [30] and substituting
ith
:
![[31]](/document/doi/10.1515/ijcre-2012-0049/asset/graphic/ijcre-2012-0049_eq31.png)
Substituting
with
in eq. [31]:
![[32]](/document/doi/10.1515/ijcre-2012-0049/asset/graphic/ijcre-2012-0049_eq32.png)
By solving eq. [32] with respect to
:
![[33]](/document/doi/10.1515/ijcre-2012-0049/asset/graphic/ijcre-2012-0049_eq33.png)
By considering the following equation coming from Pythagorean theorem applied to the down-right triangle and by applying eq. [29]:
![[34]](/document/doi/10.1515/ijcre-2012-0049/asset/graphic/ijcre-2012-0049_eq34.png)
By substituting eq. [33] in eq. [34]:
![[35]](/document/doi/10.1515/ijcre-2012-0049/asset/graphic/ijcre-2012-0049_eq35.png)
Finally:
![[36]](/document/doi/10.1515/ijcre-2012-0049/asset/graphic/ijcre-2012-0049_eq36.png)
whereas by applying the plus sign in eq. [33] one gets the relationship for r2:
![[37]](/document/doi/10.1515/ijcre-2012-0049/asset/graphic/ijcre-2012-0049_eq37.png)
Appendix B: Geometrical derivation of rII, rIII, rIV, rV, rVI, θ2, θ3, θ4, θ5 and θ6

Geometric scheme referred to lamp 1 reference system.
![[38]](/document/doi/10.1515/ijcre-2012-0049/asset/graphic/ijcre-2012-0049_eq38.png)
![[39]](/document/doi/10.1515/ijcre-2012-0049/asset/graphic/ijcre-2012-0049_eq39.png)
![[40]](/document/doi/10.1515/ijcre-2012-0049/asset/graphic/ijcre-2012-0049_eq40.png)
![[41]](/document/doi/10.1515/ijcre-2012-0049/asset/graphic/ijcre-2012-0049_eq41.png)
![[42]](/document/doi/10.1515/ijcre-2012-0049/asset/graphic/ijcre-2012-0049_eq42.png)
![[43]](/document/doi/10.1515/ijcre-2012-0049/asset/graphic/ijcre-2012-0049_eq43.png)
Notations
| A [m2] | catalyst surface area (specific surface area multiplied by weight) |
| b [dimensionless] | parameter defined by eq. [8] |
| Ccat [g m–3] | catalyst concentration |
| Ci [mmol m–3] | concentration of I-intermediate |
| CSub [mmol m–3] | substrate concentration |
| CSub,0 [mmol m–3] | substrate initial concentration |
| e [dimensionless] | Napierian extinction coefficient |
| I [W m–2] | light radiation flux coming from one lamp in the positive propagation direction |
| I0 [W m–2] | light radiation flux coming from one lamp at boundary medium (between light source and reacting suspension) |
| I0,r1 [W m–2] | light radiation flux coming from one lamp at boundary medium as a function of r1 |
| Iλ [W m–2] | local radiation intensity |
| J [W m–2] | radiation flux in the opposite propagation direction |
| k [m–1] | absorption coefficient |
| k* [m2 g–1] | absorption coefficient per unit concentration |
| k′ [mmol m–2 h–1] | absolute kinetic constant (not depending on light intensity) |
| k1″ [mmol m–2 h–1] = k′′θOx | L.-H. surface pseudo-first-order kinetic rate constant |
| k2″ [mmol m–2 h–1] | L.-H. second-order kinetic rate constant |
| kads [m3mmol–1] | substrate adsorption kinetic constant |
| kdes [m3mmol–1] | substrate desorption kinetic constant |
| KSub [m3mmol–1] | reagent equilibrium adsorption constant |
| Ki [m3mmol–1] | intermediate products equilibrium adsorption constant |
| kobs [m h–1] | observed pseudo-first-order disappearance rate |
| l [m] | light path length; coordinate along which propagation occurs |
| NSub [mmol] | phenol moles present in the liquid phase |
| r [m] | distance between light source and a reactant element, i.e. cylindrical radial coordinate |
| r0 [m] | smaller distance between light source and external reactor wall |
| r1 [m] = (r–l) | distance between light source 1 and circumference points nearer to the light source (see Figures 2 and 6) |
| r2 [m] | distance between light source 1 and circumference points farer from the light source (see Figures 2 and 7) |
| rII, rIII, rIV, rV, rVI [m] | distance between light source II, III, IV, V, VI and circumference points nearer to the light source (see Appendix B) |
| rSub [mmol m–2 h–1] | volumetric averaged surface reaction rate |
| R [m] | reactor radius |
| R∞ [dimensionless] | diffuse reflectance |
| s [m–1] | scattering coefficient |
| s* [m2 g–1] | scattering coefficient per unit concentration |
| S [m2] | cross-sectional area of the photoreactor |
| t [h] | reaction time |
| V [m3] | reaction volume |
| α [dimensionless] | parameter varying from 0.5 to 1 (present as an exponent in eq. [18]) |
| θ [rad] | cylindrical angular coordinate referred to lamp 1 |
| θ2, θ3, θ4, θ5, θ6[rad] | cylindrical angular coordinate referred to lamp 2, 3, 4, 5, 6 |
| θ* [dimensionless] | fractional site coverage |
| θ0 [rad] | boundary cylindrical angular to be considered |
| θOx [dimensionless] | oxygen fractional site coverage |
| θSub [dimensionless] | reagent fractional site coverage |
| λ [m] | radiation wavelength |
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©2013 by Walter de Gruyter Berlin / Boston
Artikel in diesem Heft
- Masthead
- Masthead
- Editorial
- In Honor of Alberto E. Cassano: Researcher, Engineer, and Academic
- Articles
- From Ideal Reactor Concepts to Reality: The Novel Drum Reactor for Photocatalytic Wastewater Treatment
- Synthesis, Characterization, and Comparison of Sol–Gel TiO2 Immobilized Photocatalysts
- Determination of Kinetic Parameter in a Unified Kinetic Model for the Photodegradation of Phenol by Using Nonlinear Regression and the Genetic Algorithm
- Mass Transfer and Conservation from a Finite Source to an Infinite Media
- Modelling and Simulation of Gas–liquid Hydrodynamics in a Rectangular Air-lift Reactor
- Two-Dimensional Modeling of an Externally Irradiated Slurry Photoreactor
- Role of Aspect Ratio and Joule Heating within the Fluid Region Near a Cylindrical Electrode in Electrokinetic Remediation: A Numerical Solution based on the Boundary Layer Model
- Solar Water Disinfection Using NF-codoped TiO2 Photocatalysis: Estimation of Scaling-up Parameters
- A Simple and Semi-Empirical Model to Predict THMs Generation in Water Facilities Including pH Effects
- On the Standardization of the Photocatalytic Gas/Solid Tests
- Microalgae Technology: A Patent Survey
- Influence of Physical and Optical Parameters on 2,4-Dichlorophenol Degradation
- Factors Capable of Modifying the Response of Pseudomonas aeruginosa to the Inactivation Induced by Heterogeneous Photocatalysis
- Enhanced Antibacterial Activity of CeO2 Nanoparticles by Surfactants
- Determination of Photochemical, Electrochemical and Photoelectrochemical Efficiencies in a Photoelectrocatalytic Reactor
- Correlations between Molecular Descriptors from Various Volatile Organic Compounds and Photocatalytic Oxidation Kinetic Constants
- Role of Joule Heating in Electro-Assisted Processes: A Boundary Layer Approach for Rectangular Electrodes
Artikel in diesem Heft
- Masthead
- Masthead
- Editorial
- In Honor of Alberto E. Cassano: Researcher, Engineer, and Academic
- Articles
- From Ideal Reactor Concepts to Reality: The Novel Drum Reactor for Photocatalytic Wastewater Treatment
- Synthesis, Characterization, and Comparison of Sol–Gel TiO2 Immobilized Photocatalysts
- Determination of Kinetic Parameter in a Unified Kinetic Model for the Photodegradation of Phenol by Using Nonlinear Regression and the Genetic Algorithm
- Mass Transfer and Conservation from a Finite Source to an Infinite Media
- Modelling and Simulation of Gas–liquid Hydrodynamics in a Rectangular Air-lift Reactor
- Two-Dimensional Modeling of an Externally Irradiated Slurry Photoreactor
- Role of Aspect Ratio and Joule Heating within the Fluid Region Near a Cylindrical Electrode in Electrokinetic Remediation: A Numerical Solution based on the Boundary Layer Model
- Solar Water Disinfection Using NF-codoped TiO2 Photocatalysis: Estimation of Scaling-up Parameters
- A Simple and Semi-Empirical Model to Predict THMs Generation in Water Facilities Including pH Effects
- On the Standardization of the Photocatalytic Gas/Solid Tests
- Microalgae Technology: A Patent Survey
- Influence of Physical and Optical Parameters on 2,4-Dichlorophenol Degradation
- Factors Capable of Modifying the Response of Pseudomonas aeruginosa to the Inactivation Induced by Heterogeneous Photocatalysis
- Enhanced Antibacterial Activity of CeO2 Nanoparticles by Surfactants
- Determination of Photochemical, Electrochemical and Photoelectrochemical Efficiencies in a Photoelectrocatalytic Reactor
- Correlations between Molecular Descriptors from Various Volatile Organic Compounds and Photocatalytic Oxidation Kinetic Constants
- Role of Joule Heating in Electro-Assisted Processes: A Boundary Layer Approach for Rectangular Electrodes