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Effect of the nonuniformity of the inlet liquid distribution on the trickle-bed reactor output in an exothermic reaction accompanied by evaporation

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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 :

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 :

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 i :

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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