I've done calculations, just ouf of curiosity, instead of staying on a gut
feel :
For a 10us, 10kA pulse and a standard 35um copper, considering that the
process is strictly adiabatic for such a low pulse duration, we have a 37cm
wide for a 10K temp rise and a *huge* asumption : uniform current density.
Not too bad.
Using a 105um, your 3us pulse, and a 40K rise that gives a small 1cm wide.
That's, of course for a *single* pulse.
I'll be more concerned about mechanical stress : this kind of current is the
one that violently "shakes" the wires when power installations fails
short-circuited. The pulse length is much longer though, but also the wire
mass, so...
Plugging the numbers into I. M. Onderdonk's equation, we get a
required cross-sectional area of only 100 circular mils for actual
melting of the copper at 25°C ambient and a 5usec 10kA pulse. That's
73 square miles, and with 1-oz copper (0.0014" (?)) then the width
would be 52 mils. If that's the actual requirement, and if the
equation holds up, then a 125 mil trace on 1-oz copper ought to do it
with some margin. BTW, lightning damage is interesting, I've seen it
damage components without touching relatively narrow traces, unlike
shorts to the mains, which tend to vaporize as much of the trace as
the juice can arc over.
For those FAQ on designing a crude fuse to be etched into the copper
of a PCB, the equation ought to be sufficient, at least to get to the
testing point.
BTW, Onderdonk's work on determining fusing current is referenced in
ASTM "F855-97e1 Standard Specifications for Temporary Protective
Grounds to Be Used on De-energized Electric Power Lines and
Equipment".
You can also find some *steady-state* fusing currents for various
metal wires on my page at
http://www.speff.com. I'll add the Onderdonk
equation when I get a chance.
Best regards,
Spehro Pefhany