On the anode potential fall in a vacuum arc: PIC simulation

The interaction of plasma generated by a vacuum arc with the anode surface was numerically simulated by using a particle-in-cell (PIC) method. It has been found that the anode potential fall remains negative even at high electron drift velocities. The plasma–anode-surface interaction has been analyzed for a ‘steady-state’ regime and for a ‘turbulent’ regime with microinstabilities developing in the plasma. For the steady-state regime, approximate formulas for the anode potential fall and energy flux have been derived from the simulation results. For the turbulent regime, naturally associated with high electron drift velocities, the negative anode fall voltage and the effective plasma electron temperature have been found to be larger than that for the steady-state regime.

[1]  Raymond L. Boxman,et al.  Handbook Of Vacuum Arc Science And Technology , 2015 .

[2]  H. Purwins,et al.  Synergetic aspects of gas-discharge: lateral patterns in dc systems with a high ohmic barrier , 2014 .

[3]  K. N. Ul’yanov,et al.  Generalized Bohm’s criterion and negative anode voltage fall in electric discharges , 2013 .

[4]  S. Jia,et al.  Three-Dimensional Time-Dependent Model and Simulation of High-Current Vacuum Arc in Commercial Axial Magnetic Fields Vacuum Interrupters , 2013, IEEE Transactions on Plasma Science.

[5]  Y. Londer,et al.  Model of Short Vacuum Arc at Collision Free Motion of Ions , 2013, IEEE Transactions on Plasma Science.

[6]  D. Shmelev Kinetic Model of Short Vacuum Arc With Hot Evaporating Anode , 2013, IEEE Transactions on Plasma Science.

[7]  Y. Londer,et al.  Theory of Anode Region of Short High-Current Vacuum Arc , 2013, IEEE Transactions on Plasma Science.

[8]  D. Shmelev,et al.  Kinetic Numerical Simulation of the Cathode Attachment Zone of Constricted High-Current Vacuum Arcs , 2013, IEEE Transactions on Plasma Science.

[9]  Y. Londer,et al.  Model of the short vacuum arc at collision free motion of ions , 2012, 2012 25th International Symposium on Discharges and Electrical Insulation in Vacuum (ISDEIV).

[10]  W. Lijun,et al.  Numerical simulation of high-current vacuum arc with consideration of anode vapor , 2012 .

[11]  P. Chapelle,et al.  On the numerical simulation of the diffuse arc in a vacuum interrupter , 2011 .

[12]  S. Shkol’nik Anode phenomena in arc discharges: a review , 2011 .

[13]  A. Anders Cathodic Arcs: From Fractal Spots to Energetic Condensation , 2008 .

[14]  D. Shmelev,et al.  Numerical simulation of high-current vacuum arcs in external magnetic fields taking into account essential anode evaporation , 2004, XXIst International Symposium on Discharges and Electrical Insulation in Vacuum, 2004. Proceedings. ISDEIV..

[15]  D. Shmelev,et al.  Numerical simulation of high-current vacuum arcs with an external axial magnetic field , 2003 .

[16]  B. Kadomtsev,et al.  Reviews of Plasma Physics , 2012 .

[17]  G. Mesyats,et al.  The cathode spot of a high-current vacuum arc as a multiecton phenomenon , 2000, Proceedings ISDEIV. 19th International Symposium on Discharges and Electrical Insulation in Vacuum (Cat. No.00CH37041).

[18]  G. A. Mesi︠a︡t︠s︡ Cathode phenomena in a vacuum discharge : the breakdown, the spark and the arc , 2000 .

[19]  W. Egli,et al.  Theoretical analysis of the current and energy flow to the anode in the diffuse vacuum arc , 1989 .

[20]  W. Lawson Particle simulation of bounded 1D Plasma Systems , 1989 .

[21]  S. Goldsmith,et al.  Model of the anode region in a uniform multi‐cathode‐spot vacuum arc , 1983 .

[22]  T. Takizuka,et al.  A binary collision model for plasma simulation with a particle code , 1977 .

[23]  O. Buneman,et al.  Dissipation of Currents in Ionized Media , 1959 .

[24]  Lewi Tonks,et al.  A General Theory of the Plasma of an Arc , 1929 .