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/content/aip/journal/adva/5/10/10.1063/1.4933238
1.
1.R. J. Zollweg, “Convection in vertical high-pressure mercury arcs,” J. Appl. Phys. 49(3), 10771091 (1978).
http://dx.doi.org/10.1063/1.325036
2.
2.J. Wendelstorf, “Two-temperature, two-dimensional modeling of cathode plasma interaction in electric arcs,” in Proc. ICPIG XXIV Int. Conf. Phenom. Ionized Gases, Warsaw, Poland, Jul. 11–16 (1999), Vol.2, pp. 227228.
3.
3.P. Flesch and M. Neiger, “Modeling of high-pressure discharge lamps including electrodes,” IEEE Trans. Plasma Sci. 27(1), 1819 (1999).
http://dx.doi.org/10.1109/27.763002
4.
4.E. Fischer, “Modeling of low-power high-pressure gas discharge lamps,” Philips J. Res. 42(1), 5885 (1987).
5.
5.L. M. Beks, M. Haverlag, and J. J. A. M. van der Mullen, “A model for additive transport in metal halide lamps containing mercury and dysprosium tri-iodide,” J. Phys. D, Appl. Phys. 41(12), 125209-1125209-9 (2008).
http://dx.doi.org/10.1088/0022-3727/41/12/125209
6.
6.K. Charrada and G. Zissis, “Spatio-temporal study of the deviations from thermal equilibrium in a high-pressure mercury plasma working under an ac power supply,” J. Phys. D, Appl. Phys. 33(8), 968976 (2000).
http://dx.doi.org/10.1088/0022-3727/33/8/313
7.
7.K. Charrada, G. Zissis, and M. Aubes, “Two-temperature, two dimensional fluid modelling of mercury plasma in high-pressure lamps,” J. Phys. D, Appl. Phys. 29(9), 24322438 (1996).
http://dx.doi.org/10.1088/0022-3727/29/9/030
8.
8.K. Charrada, G. Zissis, and M. Stambouli, “A study of the convective flow as a function of external parameters in high-pressure mercury lamps,” J. Phys. D, Appl. Phys. 29(3), 753760 (1996).
http://dx.doi.org/10.1088/0022-3727/29/3/036
9.
9.K. C. Paul, T. Takemura, T. Hiramoto, M. Yoshioka, and T. Igarashi, “Three-dimensional modeling of a direct current operated Hg-Ar lamp,” IEEE Trans. Plasma Sci. 34(2), 254262 (2006).
http://dx.doi.org/10.1109/TPS.2006.872188
10.
10.P. Y. Chang, W. Shyy, and J. T. Dakin, “A study of three-dimensional natural convection in high-pressure mercury lamps—I. Parametric variations with horizontal mounting,” Int. J. Heat Mass Transf. 33(3), 483493 (1990).
http://dx.doi.org/10.1016/0017-9310(90)90183-U
11.
11.W. Shyy and P. Y. Chang, “A study of three-dimensional natural convection in high-pressure mercury lamps—II. Wall temperature profiles and inclination angles,” Int. J. Heat Mass Transf. 33(3), 495506 (1990).
http://dx.doi.org/10.1016/0017-9310(90)90184-V
12.
12.M. Galvez, “3-D LTE modeling of HID lamps with electrode plasma interaction,” in Proc. Light Sour., Toulouse, France, 2004. Vol. 10, pp. 219220.
13.
13.M. B. Ben Hamida, H. Helali, Z. Araoud, and K. Charrada, “Contrast between the vertical and horizontal mercury discharge lamps,” Phys. Plasmas 18, 063506-1063506-7 (2011).
http://dx.doi.org/10.1063/1.3598447
14.
14.W. Shyy and P. Y. Chang, “Effects of convection and electric field on thermofluid transport in horizontal high-pressure mercury arcs,” J. Appl. Phys. 67(4), 17121719 (1990).
http://dx.doi.org/10.1063/1.346097
15.
15.D. K. McLain and R. J. Zollweg, “Convection in horizontal high-pressure mercury, mercury plus iodine, and metal halide additive arcs,” J. Appl. Phys. 52, 199 (1981).
http://dx.doi.org/10.1063/1.328475
16.
16.M. B. Ben Hamida and K. Charrada, “Application of a three-dimensional model for a study of the energy transfer of a high-pressure mercury horizontal lamp,” Phys. Plasmas 19, 063504-8 (2012).
http://dx.doi.org/10.1063/1.4728088
17.
17.P. Y. Chang and W. Shyy, “A study of three-dimensional natural convection in high-pressure mercury lamps—III. Arc centering by magnetic field,” Int. J. Heat Mass Transf. 35(8), 18571864 (1992).
http://dx.doi.org/10.1016/0017-9310(92)90189-Y
18.
18.Peggy Y. Chang and James T. Dakin, “Effects of rotation and magnetic field on a horizontal high-pressure Hg arc,” J. Appl. Phys. 69, 3763 (1991).
http://dx.doi.org/10.1063/1.348472
19.
19.C. Kenty, “On Convection Currents in High Pressure Mercury Arcs,” J. Appl. Phys. 9, 53 (1938).
http://dx.doi.org/10.1063/1.1710361
20.
20.P Flesch and M Neiger, J. Phys. D: Appl. Phys. 38, 3098 (2005).
http://dx.doi.org/10.1088/0022-3727/38/17/S12
21.
21.M S Benilov, M.D Cunha, and G.V Naidis, “Modelling interaction of multispecies plasmas with thermionic cathodes,” Plasma Sources Science and Technology 14, 517524 (2005).
http://dx.doi.org/10.1088/0963-0252/14/3/014
22.
22.Yan-Ming Li, “Effects of Plasma Rotation and Magnetic Fields on convection Flows in the Horizontal Burning High Intensity Discharge Lamps,” in Excerpt from the Proceedings of the COMSOL Multiphysics User’s Conference, Boston, 2005.
http://aip.metastore.ingenta.com/content/aip/journal/adva/5/10/10.1063/1.4933238
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/content/aip/journal/adva/5/10/10.1063/1.4933238
2015-10-09
2016-12-08

Abstract

The aim of this paper is to evaluate the magnitude of the external magnetic field to be applied to a horizontal mercury discharge lamp such that the Lorentz forces counterbalance buoyancy forces and the hot region of the arc remains centered inside the lamp with the variation of six parameters of the lamp such as the external temperature of the lamp, envelope thickness, convective loss, Interelectrodeslength, pressure and current supply pointing to the influence of the parameters to the compensating magnetic field value. To achieve this objective, a commercial numerical software “Comsol Multiphysics” is used to implement the model that solves the equations of mass, energy and momentum for laminar compressible flow combined with the Laplace equation for the plasma in a three dimensional.

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