Abstract
The effect of the inlet liquid distribution on the operation of a trickle-bed reactor is experimentally investigated, and the observed phenomena are analyzed using a one-dimensional mathematical model with nonequilibrium approaches to describing phase transitions. The modeling shows that, if the fraction of the wetted surface at the reactor inlet is below unity, then, along a sufficiently long bed, there is always a stationary front of complete evaporation and complete conversion. The main conclusion within the framework of the considered one-dimensional model with separate evaporation (on completely wetted granules) and gas-phase hydrogenation (on dry granules) is that safe operation (the absence of a thermal explosion) can be ensured by complete suppression of the reaction in the gas phase.
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Abbreviations
- A:
-
absolute output, g/s
- c g :
-
specific heat of the gas mixture, J/(kg K)
- c ℓ :
-
specific heat of the liquid, J/(kg K)
- D:
-
reactor diameter, mm
- D AB :
-
binary diffusion coefficient of components A and B, m2 s
- D AH :
-
binary diffusion coefficient of components A and H, m2 s
- D 0 :
-
effective diffusion coefficient of the vapor of component A, m2 s
- d eq :
-
equivalent diameter of intergranular channels for the gas
- d p :
-
diameter of catalyst granules, m
- f:
-
surface fraction of the wetted catalyst
- G g :
-
gas mass flow rate per total cross section, kg/(m2 s)
- G ℓ :
-
liquid mass flow rate per total cross section, kg/(m2 s)
- ΔH evA , ΔH evB :
-
enthalpy changes in the phase transitions of α-methylstyrene and cumene, respectively, J/mol
- K:
-
liquid flow rate, g/s
- L:
-
length of the reactor or the catalyst bed, mm
- L tz :
-
trickling zone length, mm
- m H, m A, m B :
-
molar masses of hydrogen, α-methylstyrene, and cumene, respectively, kg/mol
- N A, N B :
-
phase transition rates of α-methylstyrene (A) and cumene (B), respectively, mol/(m2 s)
- N AB = N A + N B :
-
total phase transition rate, mol/(m2 s)
- P:
-
total pressure, N/m2
- P*A, P*B :
-
saturation vapor pressures of α-methylstyrene and cumene, respectively, N/m2
- Q:
-
heat of gas-phase hydrogenation, J/mol
- Q evA , Q evB :
-
heat of phase transitions for α-methylstyrene (A) and cumene (B), respectively, J/mol
- R:
-
gas constant, J/(mol K)
- S:
-
specific geometric surface area of the granular bed, m−1
- S sp :
-
specific mass surface area of the catalyst, m2/g
- T Ab = 438.5 K, T Ac = 654 K, P Ac = 33.6 bar, T Bb = 425.6 K, T Bc = 631 K, P Bc = 31.7 bar:
-
boiling points (subscript b) and critical temperatures and critical pressures (subscript c) for α-methylstyrene (A) and cumene (B)
- T i :
-
temperature (i = g, ℓ, s), °C
- T in :
-
temperature at the reactor inlet, °C
- U H, U A :
-
linear velocities of hydrogen and α-methylstyrene, respectively, cm/s
- W g :
-
gas-phase reaction rate, mol/(m2 s)
- X:
-
α-methylstyrene conversion, %
- x i :
-
mass fractions of components in the gas (i = A, B, H)
- x ℓi :
-
mass fractions of components in the liquid (i = A, B)
- y*A, y*B, y*H :
-
equilibrium mole fractions of components A, B, and H2, respectively, in the gas at the boundary with the liquid and the wetted granules
- y i :
-
mole fractions of components in the gas (i = A, B, H)
- y li :
-
mole fractions of components in the liquid (i = A, B)
- z:
-
coordinate along the catalyst bed length, mm
- αg :
-
heat-transfer coefficient between the gas and the catalyst surface, W/(m2 K)
- αSL :
-
heat-transfer coefficient between the dry and wetted surfaces of granules, W/(m2 K)
- βAH, β*:
-
mass-transfer coefficients between the gas and the wetted surface of granules, m/s
- βgS :
-
mass-transfer coefficient between the gas and the dry surface of granules, m/s
- γ:
-
porosity
- ɛ:
-
fraction of the evaporated liquid
- λg :
-
thermal conductivity of the gas mixture, W/(m K)
- λH, λA :
-
thermal conductivities of hydrogen and α-methylstyrene, respectively, W/(m K)
- λp :
-
thermal conductivity of catalyst granules, W/(m K)
- λS :
-
longitudinal thermal conductivity on dry granules, W/(m K)
- μ:
-
gas dynamic viscosity, kg/(m s)
- μl :
-
liquid viscosity, kg/(m s)
- ρl :
-
liquid density, kg/m3
- σ:
-
liquid surface tension, N/m
- ϕ:
-
liquid volume fraction in the intergranular space
- ϕ = ϕdyn + ϕstat :
-
liquid fraction in the free volume of the granular bed as the sum of dynamic and static components
- ω:
-
volume output, mol/(m3 s)
- Eo:
-
Eötvös number
- Ga:
-
Galo number
- Nu:
-
Nusselt number
- Pr:
-
Prandtl number for gas
- Re:
-
Reynolds number for the gas phase
- Sc:
-
Schmidt number
- Sh:
-
Sherwood number
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Original Russian Text © V.V. Kireenkov, A.B. Shigarov, N.A. Kuzin, A.A. Bocharov, V.A. Kirillov, 2006, published in Teoreticheskie Osnovy Khimicheskoi Tekhnologii, 2006, Vol. 40, No. 5, pp. 508–519.
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Kireenkov, V.V., Shigarov, A.B., Kuzin, N.A. et al. Effect of the nonuniformity of the inlet liquid distribution on the trickle-bed reactor output in an exothermic reaction accompanied by evaporation. Theor Found Chem Eng 40, 472–482 (2006). https://doi.org/10.1134/S0040579506050046
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DOI: https://doi.org/10.1134/S0040579506050046