Modelling of near corona wire electrohydrodynamic flow in a wire-plate electrostatic precipitator
The modelling of the flow velocity fields for near corona wire electrohydrodynamic (EHD) flow was performed. The steady, two-dimensional Navier-Stokes equations have been computed for a wire-to-plate type electrostatic precipitator (ESP). The numerical simulation used Phoenics (Version 3.5.1) CFD co...
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Published in: | CEIDP '05. 2005 Annual Report Conference on Electrical Insulation and Dielectric Phenomena, 2005 pp. 478 - 481 |
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2005
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Abstract | The modelling of the flow velocity fields for near corona wire electrohydrodynamic (EHD) flow was performed. The steady, two-dimensional Navier-Stokes equations have been computed for a wire-to-plate type electrostatic precipitator (ESP). The numerical simulation used Phoenics (Version 3.5.1) CFD code coupled with Poisson's and ion transport equations, and electric body force in momentum equation which were developed in this study. The Chen-Kim modified k-/spl epsiv/ turbulent model was used to obtain a quantitative image of the resulting mean flow field and the downstream wake flow of rear wire for EHD flow. The flow velocity field pattern showed a strong EHD secondary flow clearly visible in the downstream regions of the corona wire in spite of low Reynolds number for the electrode (Re/sub cw/=12.4). The secondary flow vortices are caused by the EHD also when discharge current is increased. |
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AbstractList | The modelling of the flow velocity fields for near corona wire electrohydrodynamic (EHD) flow was performed. The steady, two-dimensional Navier-Stokes equations have been computed for a wire-to-plate type electrostatic precipitator (ESP). The numerical simulation used Phoenics (Version 3.5.1) CFD code coupled with Poisson's and ion transport equations, and electric body force in momentum equation which were developed in this study. The Chen-Kim modified k-/spl epsiv/ turbulent model was used to obtain a quantitative image of the resulting mean flow field and the downstream wake flow of rear wire for EHD flow. The flow velocity field pattern showed a strong EHD secondary flow clearly visible in the downstream regions of the corona wire in spite of low Reynolds number for the electrode (Re/sub cw/=12.4). The secondary flow vortices are caused by the EHD also when discharge current is increased. |
Author | Chun, Y.N. Chang, J.-S. Brocilo, D. Berezin, A.A. Mizeraczyk, J. |
Author_xml | – sequence: 1 givenname: Y.N. surname: Chun fullname: Chun, Y.N. organization: Dept. of Eng. Phys., McMaster Univ., Hamilton, Ont., Canada – sequence: 2 givenname: A.A. surname: Berezin fullname: Berezin, A.A. organization: Dept. of Eng. Phys., McMaster Univ., Hamilton, Ont., Canada – sequence: 3 givenname: D. surname: Brocilo fullname: Brocilo, D. organization: Dept. of Eng. Phys., McMaster Univ., Hamilton, Ont., Canada – sequence: 4 givenname: J. surname: Mizeraczyk fullname: Mizeraczyk, J. – sequence: 5 givenname: J.-S. surname: Chang fullname: Chang, J.-S. |
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Snippet | The modelling of the flow velocity fields for near corona wire electrohydrodynamic (EHD) flow was performed. The steady, two-dimensional Navier-Stokes... |
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StartPage | 478 |
SubjectTerms | Computational fluid dynamics Corona Electrodes Electrohydrodynamics Electrostatic precipitators Fluid flow Numerical simulation Physics Poisson equations Wire |
Title | Modelling of near corona wire electrohydrodynamic flow in a wire-plate electrostatic precipitator |
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