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1.1 About reactions

Delft University of Technology
Updated: 18 Oct 2026

The chemical reaction we’re interested in is acetylene semi-hydrogenation to ethylene:

C2H2+H2−>C2H4C2H2 + H2 -> C2H4

The problem is that the reaction doesn’t stop at ethylene, but it also produces ethane:

C2H2+2H2−>C2H6C2H2 + 2H2 -> C2H6

We want to maximize the production of ethylene and minimize the production of ethane.

And keep the total production high, besides the selectivity.

The ideal catalyst would be one that selectively hydrogenates acetylene to ethylene and then stops.

In reality, we can control the selectivity by adjusting the reaction conditions (temperature, pressure, residence time, etc.). This is grounded in x papers (the ones who talk about transients).

In this paper we’re interested in manipulating the reation through transient concentration profiles by pulsing the concentrations of reactants.

By modelling the reaction using a rate-equation model (grounded in the papers on microkinetic parameters) we can then use control theory to design optimal Input Profiles (in this case H2 and C2H2 concentrations over time).

By finding the optimal input profile we can then use it to control the reaction in a lab-scale setup (plug flow reactor). This is grounded in another set of papers.

To achieve this, we first need a model of the reaction.

The reaction network consists of adsorption, surface reaction, and desorption steps (using ∗* to denote an adsorbed species, with vacant site fraction θ∗=1−θH−θC2H2−θC2H4\theta_* = 1 - \theta_{\mathrm{H}} - \theta_{\mathrm{C_2H_2}} - \theta_{\mathrm{C_2H_4}}):

  1. Dissociative adsorption of H2\mathrm{H_2}:

    H2+2∗⇌2H∗\mathrm{H_2 + 2* \rightleftharpoons 2H*}

    R1=k1,adsPH2θ∗2−k1,desθH2R_1 = k_{1,\mathrm{ads}} P_{\mathrm{H_2}} \theta_*^2 - k_{1,\mathrm{des}} \theta_{\mathrm{H}}^2
  2. Molecular adsorption of C2H2\mathrm{C_2H_2}:

    C2H2+∗⇌C2H2∗\mathrm{C_2H_2 + * \rightleftharpoons C_2H_2*}

    R2=k2,adsPC2H2θ∗−k2,desθC2H2R_2 = k_{2,\mathrm{ads}} P_{\mathrm{C_2H_2}} \theta_* - k_{2,\mathrm{des}} \theta_{\mathrm{C_2H_2}}
  3. Surface hydrogenation to ethylene (reversible):

    C2H2∗+2H∗⇌C2H4∗+2∗\mathrm{C_2H_2* + 2H* \rightleftharpoons C_2H_4* + 2*}

    R3=k3,fwdθC2H2θH2−k3,revθC2H4θ∗2R_3 = k_{3,\mathrm{fwd}} \theta_{\mathrm{C_2H_2}} \theta_{\mathrm{H}}^2 - k_{3,\mathrm{rev}} \theta_{\mathrm{C_2H_4}} \theta_*^2
  4. Desorption of target product (ethylene):

    C2H4∗⇌C2H4+∗\mathrm{C_2H_4* \rightleftharpoons C_2H_4 + *}

    R4=k4,desθC2H4−k4,adsPC2H4θ∗R_4 = k_{4,\mathrm{des}} \theta_{\mathrm{C_2H_4}} - k_{4,\mathrm{ads}} P_{\mathrm{C_2H_4}} \theta_*
  5. Over-hydrogenation to ethane (direct desorption to gas phase, irreversible):

    C2H4∗+2H∗→C2H6(g)+3∗\mathrm{C_2H_4* + 2H* \rightarrow C_2H_6(g) + 3*}

    R5=k5θC2H4θH2R_5 = k_{5} \theta_{\mathrm{C_2H_4}} \theta_{\mathrm{H}}^2

Anyhow

We have the reaction. But it can only react on the catalyst surface, not in the gas phase.

So for our model we need to consider the gas-phase species, the adsorbed species and the catalyst surface as a whole.

We do this through the conservation laws. Paper 2008 Berger (1D dynamic axial model): \

∂Ci∂t=−usεb∂Ci∂z+Dax∂2Ci∂z2+ρs(1−εb)CtεbRi\frac{\partial C_i}{\partial t} = -\frac{u_s}{\varepsilon_b} \frac{\partial C_i}{\partial z} + D_{\mathrm{ax}} \frac{\partial^2 C_i}{\partial z^2} + \frac{\rho_s (1 - \varepsilon_b) C_t}{\varepsilon_b} R_i

It has accumulation (∂Ci/∂t\partial C_i/\partial t), convective transport (−usεb∂Ci∂z- \frac{u_s}{\varepsilon_b}\frac{\partial C_i}{\partial z}), axial dispersion (Dax∂2Ci∂z2D_{\mathrm{ax}}\frac{\partial^2 C_i}{\partial z^2}, negligible under plug-flow criteria Peax>100Pe_{\mathrm{ax}} > 100), and catalytic surface generation/consumption (RiR_i).

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