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Boreskov Institute of Catalysis of the Siberian Branch of Russian ...

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OP-II-9MODELLING OF DIESEL PARTICULATE FILTRATIONIN WALL-FLOW TRAPSS. Bensaid, D.L. Marchisio, D. Fino, G. Saracco, V. SpecchiaDipartimento di Scienza dei Materiali e Ingegneria Chimica - Politecnico di Torino,Corso Duca degli Abruzzi 24, 10129 Turin – ITALYTel./Fax: 011.564.4710/4699; corresponding author: e-mail: debora.fino@polito.itNowadays, soot emissions from Diesel engines can be reduced by physically trapping <strong>the</strong>particles with on-board diesel particulate filters (DPFs). The investigation <strong>of</strong> soot filtration viaDPFs, and <strong>the</strong>ir regeneration, can be split into four sub-problems: i) <strong>the</strong> computation <strong>of</strong> <strong>the</strong>multi-phase flow field inside <strong>the</strong> DPF; ii) <strong>the</strong> description <strong>of</strong> <strong>the</strong> evolution <strong>of</strong> <strong>the</strong> filtercharacteristics as soot is deposited and filtered; iii) <strong>the</strong> formation <strong>of</strong> a soot cake in <strong>the</strong> DPFchannels; iv) <strong>the</strong> modeling <strong>of</strong> regeneration dynamics. Hence, <strong>the</strong> aim <strong>of</strong> this work is todevelop a ma<strong>the</strong>matical model able to accurately describe each <strong>of</strong> <strong>the</strong>se four mentioned steps.Two and three dimensional CFD simulations <strong>of</strong> <strong>the</strong> multiphase flow inside <strong>the</strong> filterchannels are carried out by resorting to an Eulerian-Eulerian approach. The interactionbetween <strong>the</strong> main phase and <strong>the</strong> soot particles is taken into account through <strong>the</strong> drag force,calculated according to Schiller and Naumann [1]. The influence <strong>of</strong> Brownian forces on <strong>the</strong>drag force via <strong>the</strong> Stokes-Cunningham coefficient, and on particles trajectories in <strong>the</strong>channels, is proven to be negligible.Fig. 1 shows <strong>the</strong> gas and soot velocity axial pr<strong>of</strong>iles inside <strong>the</strong> DPF channels at <strong>the</strong>beginning <strong>of</strong> filtration (Fig 1-a), and <strong>the</strong> evolution <strong>of</strong> <strong>the</strong> gas velocity across <strong>the</strong> filter wallwith respect to <strong>the</strong> total amount <strong>of</strong> collected soot (Fig. 1-b). The accumulation <strong>of</strong> sootparticles into <strong>the</strong> filter pores modifies its characteristics: <strong>the</strong> porosity and <strong>the</strong> permeability <strong>of</strong><strong>the</strong> filter decrease until a maximum value <strong>of</strong> deposited soot volume fraction is reached into<strong>the</strong> porous media, thus making <strong>the</strong>se regions impermeable to <strong>the</strong> dispersed phase and entailing<strong>the</strong> formation <strong>of</strong> a soot layer onto <strong>the</strong> filter surface. A parameter <strong>of</strong> major importance inparticle interstitial filtration is <strong>the</strong> local efficiency, namely <strong>the</strong> probability <strong>of</strong> successfulcollections <strong>of</strong> soot particles onto fictitious spherical collectors constituting <strong>the</strong> channel walls,largely due to deposition from Brownian motions and interception. In <strong>the</strong> evaluation <strong>of</strong> <strong>the</strong>efficiency, calculated as indicated in literature [2], <strong>the</strong> size <strong>of</strong> <strong>the</strong> soot particles has a strongimpact. In <strong>the</strong> light <strong>of</strong> this consideration, our Eulerian-Eulerian approach is particularlyinteresting because it can be easily coupled with a population balance equation (PBE) for <strong>the</strong>description <strong>of</strong> poly-disperse solid-gas flows, resulting in a much lower computational timewhen compared with alternative Lagrangian-Eulerian approaches. The real soot distribution90

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