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the activation energy for the best-fitted model (FT-III-3)
was found to be 106.2 kJ mol−1 which is close to activa-
tion energies reported previously: 100 and 103 kJ mol−1
reported by Yang et al. [33] and Storch et al. [24], respec-
tively. Nevertheless, it was substantially lower than the
value of 142 kJ mol−1 reported by Reuel and Bartholomew
[34]. Reuel and Bartholomew’s value achieved at lower sig-
nificantly reactant partial pressure based on two data points,
while in this study it was based on thirty-one data points. It
suggested that the activation energy obtained for hydrocar-
bon formation for the diffusion interference is not signifi-
cant in the tests [35]. The presence of external mass-transfer
limitations could be discerned via measuring the apparent
activation energy with intraparticle diffusion limitations. A
control regime of external mass-transfer could lead to the
obvious energy activation of just a few kJ mol−1 [29].
Conclusion
An active silica-supported cobalt–iron nanocatalyst was pre-
pared by impregnation method and was tested for hydro-
genation of carbon monoxide to light olefins. The kinetic
experimental study was performed in a differential fixed-bed
micro-reactor by altering reaction pressure (4–16 bar), H2/
CO feed molar ratio (1–1.5) and space velocity (4500 h−1) at
the temperature range of 230–280 °C. Considering LHHW
adsorption theory in catalytic reactions, CO consumption rate
equations were defined by 6 mechanisms; consequently, 7
kinetic models were proposed. Essential kinetic data obtained
in the initial rate region illustrate that the enolic mechanism
with interaction between adsorption CO and separated adsorp-
tion hydrogen as the rate-controlling step provides the most
plausible kinetic model. The kinetic parameters estimated for
this kinetic model showed reasonable confidence intervals.
The OFAT method was applied to investigation of temperature
and pressure influence on the conversion of syngas into a wide
spectrum of hydrocarbons in FTS. The product distributions in
FT synthesis are strongly influenced by temperature and pres-
sure, and 260 °C and 8 bar are the optimum temperature and
pressure for obtaining C2–C3 light olefins hydrocarbons with
high selectivity. 106.2 kJ mol−1 was the activation energy for
the best-fitted model; this value of activation energy approves
that intraparticle mass transport is not significant.
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