A finite volume method for electrostatic three species negative corona discharge simulations with application to externally charged powder bells

[1]  E. Warburg.  Ueber die Spitzenentladung , 1899 .

[2]  Julja Finkelstein-Cukier.  Über die Spitzenentladung , 1923 .

[3]  E. Kuffel.  Electron Attachment Coefficients in Oxygen, Dry Air, Humid Air and Water Vapour , 1959 .

[4]  R Coelho,et al.  Properties of the tip-plane configuration , 1971 .

[5]  R. S. Sigmond.  Simple approximate treatment of unipolar space‐charge‐dominated coronas: The Warburg law and the saturation current , 1982 .

[6]  R. S. Sigmond.  The unipolar corona space charge flow problem , 1986 .

[7]  J. Hoburg,et al.  Donor cell-finite element descriptions of wire-duct precipitator fields, charges and efficiencies , 1988, Conference Record of the 1988 IEEE Industry Applications Society Annual Meeting.

[8]  B. P. Leonard,et al.  Beyond first‐order upwinding: The ultra‐sharp alternative for non‐oscillatory steady‐state simulation of convection , 1990 .

[9]  B. P. Leonard,et al.  The ULTIMATE conservative difference scheme applied to unsteady one-dimensional advection , 1991 .

[10]  F. Pontiga,et al.  Spatial distribution of electrons and ions in a negative corona discharge , 1996, Proceedings of Conference on Electrical Insulation and Dielectric Phenomena - CEIDP '96.

[11]  J. Jones.  A theoretical explanation of the laws of Warburg and Sigmond , 1997, Proceedings of the Royal Society of London. Series A: Mathematical, Physical and Engineering Sciences.

[12]  Electrical and chemical model of negative corona in oxygen at atmospheric pressure , 1997 .

[13]  H. Brunet,et al.  EXPERIMENTAL STUDY OF THE EFFECTIVE SECONDARY EMISSION COEFFICIENT FOR RARE GASES AND COPPER ELECTRODES , 1998 .

[14]  Mohammad R. Madani,et al.  Current density distribution measurement of negative point-to-plane corona discharge , 1998, IEEE Trans. Instrum. Meas..

[15]  A. J. Schwab,et al.  Numerical solution of nonstationary charge coupled problems , 1999 .

[16]  R. I. Issa,et al.  A Method for Capturing Sharp Fluid Interfaces on Arbitrary Meshes , 1999 .

[17]  F. Peek.  Dielectric Phenomena in High Voltage Engineering , 2002 .

[18]  J. Domnick,et al.  On the simulation of space charge in electrostatic powder coating with a corona spray gun , 2003 .

[19]  P. Atten,et al.  Simulation of corona discharge in point–plane configuration , 2004 .

[20]  George E. Georghiou,et al.  Numerical modelling of atmospheric pressure gas discharges leading to plasma production , 2005 .

[21]  K. Adamiak,et al.  Corona discharge in the hyperbolic point-plane configuration: direct ionization criterion versus an approximate formulations , 2005, IEEE Transactions on Dielectrics and Electrical Insulation.

[22]  G. Raju.  Gaseous Electronics: Theory and Practice , 2005 .

[23]  Joachim Domnick,et al.  The Simulation of Electrostatic Spray Painting Process with High‐Speed Rotary Bell Atomizers. Part II: External Charging , 2006 .

[24]  K. Adamiak,et al.  A multi-species DC stationary model for negative corona discharge in oxygen; point-plane configuration , 2007 .

[25]  K. Adamiak,et al.  FEM–FCT-Based Dynamic Simulation of Corona Discharge in Point–Plane Configuration , 2010, IEEE Transactions on Industry Applications.

[26]  Robert Rundqvist,et al.  Comparison Between Different Immersed Boundary Conditions for Simulation of Complex Fluid Flows , 2011 .

[27]  Johan S. Carlson,et al.  Simulation of Electrostatic Rotary Bell Spray Painting in Automotive PAint Shops , 2012 .

[28]  Incorporation of the Corona Current into a Numerical 3D Model of the Electrostatic Coating Process , 2012 .