2015
DOI: 10.1016/j.ijheatmasstransfer.2014.11.090
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Three-dimensional calculation of a chemically reacting porous particle moving in a hot O 2 /CO 2 atmosphere

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Cited by 61 publications
(43 citation statements)
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“…Complete pore‐resolved simulations of all transport and reaction processes have so far only been performed for individual particles , . The reaction was implemented either under simplified macro kinetic approaches or under transient conditions .…”
Section: Classification Of Model Approachesmentioning
confidence: 99%
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“…Complete pore‐resolved simulations of all transport and reaction processes have so far only been performed for individual particles , . The reaction was implemented either under simplified macro kinetic approaches or under transient conditions .…”
Section: Classification Of Model Approachesmentioning
confidence: 99%
“…However, a coupled solution of all balances is not possible or only with very long computation time of up to months (e.g., , ). Furthermore, the complete solution of all balances is only possible for single particles , . The calculation of entire reactor geometries or transient processes has not been possible until today.…”
Section: Classification Of Model Approachesmentioning
confidence: 99%
“…, ) und iterativen Vorgehen verbunden. Zudem ist die vollständige Lösung aller Bilanzen nur für einzelne Partikel möglich , . Die Berechnung vollständiger Reaktorgeometrien bzw.…”
Section: Klassifizierung Der Modellansätzeunclassified
“…It should also be noted that the reaction C + 2H 2 is not included in the considerations because the rate of reaction is much lower than for other heterogeneous reactions. For further discussion on this issue we refer to Schulze et al and Richter …”
Section: Model Descriptionmentioning
confidence: 99%
“…Note here that in terms of ideal gas the word ‘incompressible’ does not mean constant density; see Equation . Porosity of the particles is not taken into account, thus the intraparticle diffusion is neglected. The particles consist of carbon only. In particular, the volatilization of the particles is neglected due to the steady‐state character of the model. The radiation of the gas phase is modelled using the P‐1 model due to its robustness and good performance when applied to char oxidation modelling The buoyancy effect is neglected. Transport properties of solid carbon are constant; their temperature dependence is negligible. Finally, the complete system of equations including the solved P1 radiation model takes the following form: ·false(ρufalse)=0 ·false(ρuufalse)=p+·false(truetrueτfalse) where ρ is the density, p is the pressure, and trueu is the velocity vector.…”
Section: Model Descriptionmentioning
confidence: 99%