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Ghulam Mustafa Majal [email protected] KTH CCGEx The project aims to find methods for stimulating agglomeration of particles in the exhaust gases associated with internal combustion engines, by manipulation of hydrodynamic and acoustic fields. An understanding of the evolution of particulate characteristics (e.g. particle mass, particle number, size distribution) as traveling along the exhaust system components and connections with relevance to modern engines is needed. The enhancement of the aforementioned understanding will be developed with the usage of unsteady 3D CFD and possible experimental data from a parallel project. The flow is modelled using a Detached Eddy Simulation (DES) approach and the particle dynamics are modelled using a Lagrangian point force treatment. Introduction and Motivation : Modern internal combustion engines tend to form fine particles prone to penetrate through the human respiratory system and cause cardiovascular as well as neurological problems . This project aims at deriving predictive models for the manipulation of particles in the exhaust line through the use of forced pulsatile flow conditions and/or acoustic fields . Setup : 1 D models for particle agglomeration process have been developed to analyze the effect of different flow and geometrical parameters on particle agglomeration . The model considered an oscillating Stokesian flow in a corrugated pipe . Only the drag force acting on the particle has been considered . Later, the simulations were extended to 3 D flow calculations using the Detached Eddy Simulation (DES) approach and applying a Lagrangian point force to account for particle dynamics . Non - pulsatile flow inlet conditions and a monodisperse distribution of particles were considered . Simple particle advection was considered . Results : In the leftmost figures (normalized) particle displacement and velocity for grouping (upper panel) and non - grouping (lower panel) scenarios using the 1 D modelling are shown . For the 3 D flow modelling a uniform velocity is imposed at the inlet of the corrugated pipe geometry . Two different geometries were considered having the same inlet diameter ( ! "#$ ) and geometric wavelength ( % ) but different maximum diameter ( ! "&' ) . In the rightmost figures the normalized time - averaged streamwise velocity (left) and turbulent kinetic energy (right) are shown as predicted for the two different geometries (different ! "&' ) . The data is extracted along transversal radial lines located at different downstream positions in the corrugated pipe within the planes of maximum cross sectional area . A flow asymmetry is obvious as the ! "&' is increased . Summary and Conclusion : Tests have been carried out to understand the impact of the different non - dimensional parameters on particle grouping using a simple 1 D model . Conditions have been identified where particle agglomeration can occur in a corrugated pipe . 3 D flow scenarios have been studied for two geometries with the same inlet diameter and geometric wavelength but different maximum diameter ( ! "&' ) . A flow asymmetry and higher turbulent kinetic energy levels characterized the set - up with larger ! "&' . Future work will include understanding the flow instabilities developed as increasing the ! "&' diameter, along with studying the impact on particle - particle interactions and particle distribution along the geometry . Acknowledgement : This project is supervised by Mihai Mihaescu (KTH - Mechanics), Mats Åbom ( KTH - MWL), Lisa Prahl Wittberg (KTH - Mechanics), and Mikael Karlsson ( KTH - MWL) . The support received from the Swedish Energy Agency, Scania AB, Volvo GTT, BorgWarner, and Volvo Cars is highly appreciated . Part of simulations were performed on resources provided by the Swedish National Infrastructure for Computing (SNIC) at PDC Centre for High Performance Computing (PDC - HPC ) . Control of particle agglomeration with relevance to after-treatment gas processes

Ghulam Mustafa Majal - KTH · Ghulam Mustafa Majal KTH CCGEx [email protected] Theprojectaimstofindmethodsforstimulatingagglomerationofparticlesintheexhaustgasesassociatedwith

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Page 1: Ghulam Mustafa Majal - KTH · Ghulam Mustafa Majal KTH CCGEx gmmajal@kth.se Theprojectaimstofindmethodsforstimulatingagglomerationofparticlesintheexhaustgasesassociatedwith

Ghulam Mustafa Majal

[email protected] CCGEx

The project aims to find methods for stimulating agglomeration of particles in the exhaust gases associated withinternal combustion engines, by manipulation of hydrodynamic and acoustic fields. An understanding of the evolution ofparticulate characteristics (e.g. particle mass, particle number, size distribution) as traveling along the exhaust systemcomponents and connections with relevance to modern engines is needed. The enhancement of the aforementionedunderstanding will be developed with the usage of unsteady 3D CFD and possible experimental data from a parallelproject. The flow is modelled using a Detached Eddy Simulation (DES) approach and the particle dynamics are modelledusing a Lagrangian point force treatment.

Introduction and Motivation:Modern internal combustion engines tend to form fine particlesprone to penetrate through the human respiratory system andcause cardiovascular as well as neurological problems. This projectaims at deriving predictive models for the manipulation of particlesin the exhaust line through the use of forced pulsatile flowconditions and/or acoustic fields.

Setup:1D models for particle agglomeration process have been developedto analyze the effect of different flow and geometrical parameterson particle agglomeration. The model considered an oscillatingStokesian flow in a corrugated pipe. Only the drag force acting onthe particle has been considered. Later, the simulations wereextended to 3D flow calculations using the Detached EddySimulation (DES) approach and applying a Lagrangian point force toaccount for particle dynamics. Non-pulsatile flow inlet conditionsand a monodisperse distribution of particles were considered.Simple particle advection was considered.

Results:In the leftmost figures (normalized) particle displacement and velocity for grouping (upper panel) and non-grouping (lower panel) scenarios usingthe 1D modelling are shown. For the 3D flow modelling a uniform velocity is imposed at the inlet of the corrugated pipe geometry. Two differentgeometries were considered having the same inlet diameter (!"#$) and geometric wavelength (%) but different maximum diameter (!"&'). Inthe rightmost figures the normalized time-averaged streamwise velocity (left) and turbulent kinetic energy (right) are shown as predicted for thetwo different geometries (different !"&'). The data is extracted along transversal radial lines located at different downstream positions in thecorrugated pipe within the planes of maximum cross sectional area. A flow asymmetry is obvious as the !"&' is increased.

Summary and Conclusion:Tests have been carried out to understand the impact of the differentnon-dimensional parameters on particle grouping using a simple 1Dmodel. Conditions have been identified where particle agglomeration canoccur in a corrugated pipe. 3D flow scenarios have been studied for twogeometries with the same inlet diameter and geometric wavelength butdifferent maximum diameter (!"&' ). A flow asymmetry and higherturbulent kinetic energy levels characterized the set-up with larger !"&' .Future work will include understanding the flow instabilities developed asincreasing the !"&' diameter, along with studying the impact on particle-particle interactions and particle distribution along the geometry.

Acknowledgement:This project is supervised by Mihai Mihaescu (KTH-Mechanics),Mats Åbom (KTH-MWL), Lisa Prahl Wittberg (KTH-Mechanics), andMikael Karlsson (KTH-MWL).The support received from the Swedish Energy Agency, Scania AB,Volvo GTT, BorgWarner, and Volvo Cars is highly appreciated.Part of simulations were performed on resources provided by the Swedish National Infrastructure for Computing (SNIC) at PDC Centre for High Performance Computing (PDC-HPC).

Control of particle agglomeration with relevance to after-treatment

gas processes