GARTHWILSON wrote:
For the few who aren't afraid of some heavy-ish math, Dr. Howard Johnson addresses losses and other characteristics due to skin effect in articles linked
here. Otherwise, don't worry about it. Skin depth of copper at 100MHz is about 250 microinches. Standard 1oz copper is .0014" thick, so the resistance of a narrow trace at 74AC edge speeds should be somewhere around five times what the DC resistance is; but five times the third-of-an-ohm number above is still piddly, for digital signal lines! Also, where there's no power plane, power-supply lines will be bypassed to ground right near each IC's V
DD pin, so skin effect won't really matter there either.
POC V1.1 is running on my desk at 14.1 MHz and when scoped, looks pretty clean. Signal traces are 6 mil and the board is four layers, with 1 ounce copper. The four-layer construction shows its value in the general quietness of the unit and the absence of ground bounce.
For most of us, transmission line effects should not be a problem—assuming construction is with tight wire-wrap or on a PCB with a reasonable layout. Many of our gadgets don't run all that fast and even the ones that do run fast aren't running fast enough for signal propagation time and all that that entails to cause any grief. More likely, trouble will arise from very fast signal edges, which are characteristic of the high-speed logic families.
Nevertheless, knowing some transmission line theory can help with physical design. In that regard, Dr. Johnson is considered an expert among experts and I highly recommend his material. Yes, it's technical and some of it may be math-intensive, but his expositions are written in a lucid style and are understandable. In other words, you won't need an advanced degree to learn something.