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Guest : A minor (but longwinded) correction to the above statement about 'signals' traveling in the field outside of a conductor.
But a very nice one Richard
A further elaboration on skin depth..
The equation is
delta=5033 sqr {p/uf}
delta is skin depth in cm
p is resistivity of conductor, ohms per centimeter cube
f is frequency hertz
u is magnetic permeability, =1 for air
for copper, it reduces to depth in cm = 6.62/sqr(f)
giving .85cm at 60 hz, as you correctly stated.
This equation, of course, is useful only for wire diameters greater than about 5 times the skin depth, and is in fact, a planar solution. For typical wires used for speakers, it is incorrect..when the exact solution for skin depth of small round conductors is used, this exponential solution is found to be off by a factor of three...giving too much skinning..
If I find myself in a situation where EMP warfare equations are needed, I'll revisit the Hawksford paper.
Cheers, John</font>