1.6 Constitutive Relations
The electromagnetic properties of rocks (σ, ε, and μ) are expressed by the constitutive relations from the previous section:
J = σE, | (1.6.1) |
D = εE, | (1.6.2) |
and
B = μH. |
(1.6.3) |
In the most general cases σ, ε, and μ are complex tensors which are functions of angular frequency ω=2πf, the field strengths, position r, temperature T, pressure P, and composition. For example,
σ = σ(ω, E, r, T, P). | (1.6.4) |
In geophysics we usually normalize ε and μ by the free space values ε0 and μ0, and define the dielectric constant, K and relative magnetic permeability, Km as
K = ε/ε0 | (1.6.5) |
and
Km = μ/μ0 , | (1.6.6) |
respectively. Furthermore, for purely traditional reasons in geophysics the conductivity is usually expressed by its reciprocal, the resistivity, ρ,
ρ = 1/σ. | (1.6.7) |