In order to arrive at a three dimensional computer simulation of the electric arc, the electric railgun has been adopted as a simple model. The projectile representing the arc is a solid conductor moving between two parallel electrodes supplied by direct current. To accurately describe the problem, a three dimensional formulation that takes into account the eddy currents and the velocity, is required. Within the finite element method, a formulation based on a current vector potential is adopted because it enforces the conservation of the current which is here the origin of the force acting on the projectile. The results show the influence of the velocity on the eddy currents as well as on the Lorentz force. Eddy currents are mostly located in the rails near the contact. While in the magnetostatic case, the Lorentz force acting on the projectile is in good agreement with hand calculations of the loop effect, the current density is strongly affected by the velocity of the projectile.
[1]
O. C. Zienkiewicz,et al.
An ‘upwind’ finite element scheme for two‐dimensional convective transport equation
,
1977
.
[2]
Raffaele Martone,et al.
Unified approach to electromagnetic shape-inverse and mechanically coupled problems via a Lagrangian technique
,
1998
.
[3]
K. Preis,et al.
Computation of 3-D Current Driven Skin Effect Problems Using a Current Vector Potential
,
1992,
Digest of the Fifth Biennial IEEE Conference on Electromagnetic Field Computation.
[4]
Kuo-Ta Hsieh,et al.
A Lagrangian formulation for mechanically, thermally coupled electromagnetic diffusive processes with moving conductors
,
1995
.
[5]
A. Abri,et al.
A model for the current interruption of an electric arc
,
1984
.
[6]
Bok-Ki Kim,et al.
Implementing tri-potential approach in EMAP3D
,
1999
.