Magnetic Reconnection - Harvard
... otherwise (i.e. under ideal conditions with j /σ negligible) the z-component of equation (3) would require Ez = 0 at the neutral point, such that E0 would have to vanish. Another important property of the present geometry (shown in figure 1) is that ∂By /∂x > ∂Bx /∂y or jz > 0. Therefore, E · j = E0 ...
... otherwise (i.e. under ideal conditions with j /σ negligible) the z-component of equation (3) would require Ez = 0 at the neutral point, such that E0 would have to vanish. Another important property of the present geometry (shown in figure 1) is that ∂By /∂x > ∂Bx /∂y or jz > 0. Therefore, E · j = E0 ...
J. Opt. A: Pure Appl. Opt.11
... and there are some misconceptions about it. Here I attempt to clarify the situation and dispel the misconceptions. Many of the arguments are general, but for simplicity I restrict myself to monochromatic waves in free space. For scalar waves, a natural definition of the direction of the current in f ...
... and there are some misconceptions about it. Here I attempt to clarify the situation and dispel the misconceptions. Many of the arguments are general, but for simplicity I restrict myself to monochromatic waves in free space. For scalar waves, a natural definition of the direction of the current in f ...
