2.6: Permeability
( \newcommand{\kernel}{\mathrm{null}\,}\)
Permeability describes the effect of material in determining the magnetic flux density. All else being equal, magnetic flux density increases in proportion to permeability.
To illustrate the concept, consider that a particle bearing charge q moving at velocity v gives rise to a magnetic flux density:
B(r)=μ qv4πR2׈R
where ˆR is the unit vector pointing from the charged particle to the field point r, R is this distance, and “×” is the cross product. Note that B increases with charge and speed, which makes sense since moving charge is the source of the magnetic field. Also note that B is inversely proportional to 4πR2, indicating that |B| decreases in proportion to the area of a sphere surrounding the charge, also known as the inverse square law. The remaining factor, μ, is the constant of proportionality that captures the effect of material. We refer to μ as the permeability of the material. Since B can be expressed in units of Wb/m2 and the units of v are m/s, we see that μ must have units of henries per meter (H/m). (To see this, note that 1 H ≜ 1 Wb/A.)
Permeability (μ, H/m) describes the effect of material in determining the magnetic flux density.
In free space, we find that the permeability μ=μ0 where:
μ0=4π×10−7 H/m
It is common practice to describe the permeability of materials in terms of their relative permeability:
μr≜μμ0
which gives the permeability relative to the minimum possible value; i.e., that of free space. Relative permeability for a few representative materials is given in Appendix A2.
Note that μr is approximately 1 for all but a small class of materials. These are known as magnetic materials, and may exhibit values of μr as large as ∼106. A commonly-encountered category of magnetic materials is ferromagnetic material, of which the best-known example is iron.