Electrical Characteristics of Nonthermal Gliding Arc Discharge Reactor in Argon and Nitrogen Gases

Gliding arc discharge (GAD) has the properties of both thermal and nonthermal plasma conditions. GAD plasma in the atmospheric pressure with argon/nitrogen and its characteristics are described. Some experimental results about alternating current gliding arc plasma generator have been obtained. It seems that the current density strongly depends on the gas type, and increased with increasing discharge current and gas flow rate. In addition, the discharge current of GAD in nitrogen gas (N2) is greater than one in argon gas (Ar) because of N2 needs more breakdown voltage than Ar. The intensity of GAD increased with increasing the gas flow rate. The oscillograms of discharge current in each case of Ar and N2 were obtained. The electron temperatures of Ar and N2 plasma were calculated to be 22 800 and 8400 K, respectively. The characteristics of both Ar and N2 gases in atmospheric pressure, such as current density, electron density with flow rates (5, 10, 20, and 40) standard cubic foot per hour, were investigated and all experimental results were classified. An experimental study was carried out through using of GAD device for medical treatment by exposing three human blood samples of leukemia to the nonthermal GAD plasma for different periods.

[1]  Y. Ju,et al.  Characteristics of Gliding Arc and Its Application in Combustion Enhancement , 2008 .

[2]  A. Fridman,et al.  Gliding arc gas discharge , 1999 .

[3]  E. Nasser Fundamentals of gaseous ionization and plasma electronics , 1971 .

[4]  H. Sugimura,et al.  Excitation states of titanium and nitrogen gas in an electron beam evaporation sustained arc , 1999 .

[5]  Ahmed Addou,et al.  Density and Rotational Temperature Measurements of the OH° and NO° Radicals Produced by a Gliding Arc in Humid Air , 2002 .

[6]  K. Cen,et al.  Plasma chemical degradation of phenol in solution by gas–liquid gliding arc discharge , 2005 .

[7]  W. Marsden I and J , 2012 .

[8]  Aaas News,et al.  Book Reviews , 1893, Buffalo Medical and Surgical Journal.

[9]  F. Catoire,et al.  Double ionization of argon by electron impact: use of the approximate 6C model , 2006 .

[10]  A. Fridman,et al.  Gliding arc discharges as a source of intermediate plasma for methane partial oxidation , 2005, IEEE Transactions on Plasma Science.

[11]  M. Talaat Electrostatic field calculation in air gaps with a transverse layer of dielectric barrier , 2014 .

[12]  Alexander Gutsol,et al.  A non-equilibrium plasma source: magnetically stabilized gliding arc discharge: I. Design and diagnostics , 2010 .

[13]  D. Graves,et al.  Nonthermal atmospheric rf plasma in one-dimensional spherical coordinates: Asymmetric sheath structure and the discharge mechanism , 2007 .

[14]  Alexander Gutsol,et al.  A non-equilibrium plasma source: magnetically stabilized gliding arc discharge: II. Electrical characterization , 2010 .

[15]  L. K. Jha,et al.  Electron impact single and double ionization of argon , 2006 .

[16]  Radu Burlica,et al.  Formation of reactive species in gliding arc discharges with liquid water , 2006 .

[17]  Iu. P. Raizer Gas Discharge Physics , 1991 .

[18]  R. Bartnikas Engineering Dielectrics: Volume III Electrical Insulating Liquids , 1994 .

[19]  D. A. Gerdeman,et al.  Arc Plasma Technology in Materials Science , 1972 .

[20]  P. Bruggeman,et al.  An introduction to nonequilibrium plasmas at atmospheric pressure , 2012 .

[21]  Kevin Barraclough,et al.  I and i , 2001, BMJ : British Medical Journal.