(i) Curl m - δet = C,

(ii) div e = lρ.

(iii) Curl E + δM/δt = 0,

(iv) Div M = 0.

(2) Further relations, which characterise the influence of existing matter for the most important case to which we limit ourselves i.e. for isotopic bodies;—they are comprised in the equations

(V) e = ε E, M = μm, C = σE.

where ε = dielectric constant, μ = magnetic permeability, σ = the conductivity of matter, all given as function of x, y, z, t; s is here the conduction current.

By employing a modified form of writing, I shall now cause a latent symmetry in these equations to appear. I put, as in the previous work,

x₁ = x, x₂ = y, x₃ = z, x₄ = it,

and write s₁, s₂, s₃, s₄ for Cx, Cy, Cz (√-1)ρ.