Now, now, you know exactly what I mean. Low-value power
resistors are well characterized as a resistance in series
with an inductance. They "become" primarily inductive
above f = R / 2pi L, where the inductive reactance exceeds
the resistance.
No. A good LCR meter will show the same value for series
inductance over a wide range of measuring frequencies (to
be sure of the measurements, I do a quick check to verify
that I'm measuring with a high enough frequency to get a
sizable phase shift from the inductance, e.g. 5MHz or more
if needed). --- Sorry, here's a missing datum, the 48nH
measurement was on a 3-ohm 5-watt KoolOhm resistor, so
f = 3 / 2pi*48nH = 13MHz. Oops, where'd 10MH come from?
That was from an earlier 66nH measurement, except after
re-zeroing the meter I got 48nH. There are just too many
numbers floating around.
L = R / 2pi f = 23nH, or 2x better than 48nH (another
measurement yielded 66nH, hence the 2x - 3x estimate).
The carbon is close to a piece of similarly-shaped wire.
The breakpoint frequency. It's convenient to say the part
acts primarily as a resistor until a 3dB point, afterwhich
it acts primarily an an inductor. Plot Z vs. frequency: a
straight line from DC to a breakpoint, then rising with f.
You know the drill, I assume.