# Modeling Skin Effect

Depak Patel writes:

Why does high-frequency current flow only on the outer surface of a printed-circuit trace?

Magnetic fields cause the behavior you describe. The technical name for this property is
the *skin effect*. It happens in all conductors. If you really
like mathematics, the following section will help you to better understand *why* the skin effect happens. If not, this might be a
good time to step out for a cup of tea.

I'll start the discussion with a perfect coaxial cable. Figure 1
divides the center conductor of this cable into a series of three concentric rings with
radii *r*_{0}, *r*_{1},
and *r*_{2}. A lumped-element model of this simple
circuit demonstrates that high-frequency signal current flows only on ring 2.

(courtesy EDN)

At dc, the longitudinal-voltage drop per inch across each conductor *n* equals the current, *I*_{n}, times its resistance per inch.
You can express this relation in matrix terms by defining a square matrix, *R*, with these elements along the diagonal and 0 elsewhere:

Then, write *V*=*RI*, where *V* is a vector
representing the longitudinal voltage per inch across the ends of each conductor, *I *is a vector representing the currents, and
ρ is the resistivity of
the center conductor in units of ohm inches.

At high frequencies, the magnetic interactions between conductors become significant.
Figure 1 illustrates the pattern of magnetic fields
between the center conductor and shield. The magnetic lines of force (B-field) form
concentric circles around the conductive rings. The drawing plots the field intensity,
|*B*|, versus radial position, *r*,
assuming a positive signal current of 1A flowing in ring 0 with the return current
flowing in the shield. The field strength is zero within the interior of ring 0 and
zero outside the shield and varies with 1/*r* (Ampere's law) in
between. The exact field intensity for a current of 1A on conductor *m* is:

for *r*_{m}< *r* < *d*/2, where µ is the magnetic permeability of
the dielectric material (usually
3.192×10^{–8}
webers/amp-in.).

You calculate the mutual inductance per inch between conductors *n* and *m* (for *n* ≥ *m*) using Faraday's law as the integral of the magnetic-field
strength, *B _{m}*, taken
over the range from conductor

*n*(at radial position

*r*) and the shield (at radial position

_{n}*d*/2). Integrating 1/

*r*yields ln(

*r*) and the following matrix equation for mutual inductance:

To find values for *n* < *m*,
use symmetry: *L*_{n,m}=*L*_{m,n}.

The Laplace system equation for the whole coaxial circuit sums both resistive and
inductive terms as *V*=(*R*+ *sL*)*I*. The following is the
inductance matrix for an RG-58/U coaxial cable:

Now comes the main point of this article: The terms in the right-hand column of *L* are all the same. Why? Because ring 2 concentrates *all its flux* into the space between ring 2 and the shield.
Therefore, all other rings couple 100 percent to this flux.

The constancy of the right-hand column greatly simplifies the solution to the
system equation. To solve this equation, you must find a pattern of currents *I* such that (*R*+ *sL*)*I* generates the same longitudinal voltage across every ring. You need the same
voltage across every ring because the rings are all connected together at their ends.
If you operate at a frequency so high that the *R *term
becomes insignificant compared with *sL*, the solution
is simple. Just fill in the last element of *I*, leaving
all others zero. This solution peels off only the right-hand column of *L*, properly generating the same voltage for every ring.
This is one of the few matrix problems you can solve by inspection.

The simple solution says that at high frequencies, the signal current flows only on the
outer ring, as governed by matrix *L*. At dc, the current
distributes itself more evenly, according to matrix *R*. At
middle frequencies, you get a mixture of both effects. That's the nature of the
skin effect.

Continuous conductors behave in a similar manner, as if they were made from a continuum of infinitely thin rings. At higher and higher frequencies, the current squeezes more and more tightly against the surface of the conductor, progressively decreasing the useful current-carrying cross section of the conductor and raising its effective resistance.

You can view all of the mathematical details in the following completely-worked 40-ring example.

Don't have Mathcad? Then check out the PDF file that details the base file and shows all the calculations. After that, get yourself a mathematical spreadsheet program like Mathcad, MatLab, or Mathematica—such tools are invaluable.

Mathcad files — modelskineffect.zip

Just the PDF file — modelskineffect.pdf