Electromagnetic fields satisfying the condition B×(∇×B) = 0.
Abstract
It is proved that (1) electromagnetic fields with electric and magnetic components parallel to one another are solutions of Maxwell's equations; (2) the equationB∧(∇∧B)=0 (B is the magnetic field) is gauge and relativistically-invariant for systems of reference moving with velocityv/c=E∧B(1+v2/c2)/(E2+B2).
- Publication:
-
Astrophysics and Space Science
- Pub Date:
- April 1988
- DOI:
- Bibcode:
- 1988Ap&SS.143..113E
- Keywords:
-
- Astrophysics;
- Conservation Laws;
- Electromagnetic Fields;
- Magnetic Field Configurations;
- Maxwell Equation;
- Numerical Analysis;
- Plasma Physics;
- Physics (General);
- Magnetic Field;
- Electromagnetic Field;
- Magnetic Component;
- Plasma:Electromagnetic Fields