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A 2D Gas-Solid Fluidized Bed

In a gas-fluidized bed (with diameter D=2.0 mD = 2.0~\mathrm{m} and expanded bed height L=3.0 mL = 3.0~\mathrm{m}), heterogeneously catalyzed chemical reactions take place involving the species AA, BB, and CC. The reaction scheme and associated kinetics are as follows:

AKr,1BKr,2C,rA=Kr,1cA,rB=Kr,1cAKr,2cB,rC=Kr,2cB.A \overset{K_{r,1}}{\rightarrow} B \overset{K_{r,2}}{\rightarrow} C, \quad r_{A} = -K_{r,1} c_{A}, \quad r_{B} = K_{r,1} c_{A} - K_{r,2} c_{B}, \quad r_{C} = K_{r,2} c_{B}.

The catalyst material consists of Geldart A type particles with a particle size of 50 μm50~\mathrm{\mu m} and a particle density of 1500 kg m31500~\mathrm{kg~m^{-3}}. Additional data are given in Table 1. In the extended Kunii and Levenspiel fine-particle model, the radial gas (bubble) velocity profile is taken into account as well as the radial gas dispersion. For the radial profile of the bubble rise velocity, we assume a parabolic profile given by:

U0(r)=2U0[1(rR)2],U_{0}(r) = 2 \langle U_{0} \rangle \left[ 1 - \left( \frac{r}{R} \right)^{2} \right],

where U0\langle U_{0} \rangle is the average bubble rise velocity. This expression approximately accounts for the fact that the preferential pathway of the bubbles is located in the central part of the gas-fluidized bed. Due to the relatively high value of the average superficial gas velocity, the axial gas dispersion can be neglected. Moreover, it can be assumed that the reactor is isothermal. The bubble-to-cloud mass transfer coefficients KbcK_{bc} and the cloud-to-emulsion mass transfer coefficients KceK_{ce} can be taken as the same for the components AA, BB, and CC (see Table 1).

Table 1: Additional Data

ParameterValue
Average bubble rise velocity U0\langle U_{0} \rangle0.50 m s10.50~\mathrm{m~s^{-1}}
Reaction rate constant Kr,1K_{r,1}0.080 s10.080~\mathrm{s^{-1}}
Reaction rate constant Kr,2K_{r,2}0.010 s10.010~\mathrm{s^{-1}}
Bubble-to-cloud mass transfer coefficient KbcK_{bc}2.5 s12.5~\mathrm{s^{-1}}
Cloud-to-emulsion mass transfer coefficient KceK_{ce}1.5 s11.5~\mathrm{s^{-1}}
Radial gas dispersion coefficient Di,rD_{i,r} (i = A, B, C)0.01 m2 s10.01~\mathrm{m^{2}~s^{-1}}
Bubble phase solids holdup parameter γb\gamma_{b}0.005 ()0.005~(-)
Cloud phase solids holdup parameter γc\gamma_{c}0.200 ()0.200~(-)
Emulsion phase solids holdup parameter γe\gamma_{e}5.000 ()5.000~(-)
Inlet concentration of species AA5.0 mol m35.0~\mathrm{mol~m^{-3}}
Inlet concentration of species BB0.0 mol m30.0~\mathrm{mol~m^{-3}}
Inlet concentration of species CC0.0 mol m30.0~\mathrm{mol~m^{-3}}

Questions:

  1. Formulate the steady-state model equations and the associated boundary conditions according to the extended Kunii and Levenspiel Fine Particle Model, taking into account the radial profile of bubble rise velocity and the radial gas dispersion.

  2. Implement the formulated model equations in Python.

  3. Compute the steady-state concentration profiles at the outlet of the gas-fluidized bed using the implemented Python model. Inspect the computed concentration profiles carefully and explain the qualitative shape of these profiles. Use 100 radial grid points and 200 axial grid points.

  4. Compute the degree of chemical conversion of species AA and the selectivity towards the desired product BB. Carefully account for the radial gas (bubble) velocity profiles.

  5. Consider the case where the bubble rise velocity is uniform and radial gas dispersion can be neglected (assuming uniform inlet conditions). Solve the resulting Ordinary Differential Equations (ODEs) and compute the degree of chemical conversion of species AA and the selectivity towards the desired product BB.

Note that all numerical implementations should be consistent with the provided equations and parameter values.