J
John Woodgate
- Jan 1, 1970
- 0
I read in sci.electronics.design that Paul Burridge
[email protected]>) about 'Field Strength Meter (LTspice)', on Sun, 28 Dec
2003:
There ISN'T really a knee. It only appears that there is because of the
way the I/V curve is plotted. If you plot log(I) against V you get
nearly a straight line, with nothing unusual happening at V = 0.6 to 0.7
V.
At low signal levels, a diode detector (or any rectifying junction) has
a *square law* transfer characteristic. If you put a voltage-doubler
diode rectifier (the two-diode circuit you've been shown by me and Jim)
at the *input* of an op-amp d.c. amplifier with your meter at the op-amp
output (through a series resistor), you'd have a working circuit.
[email protected]>) about 'Field Strength Meter (LTspice)', on Sun, 28 Dec
2003:
ISTR somewhere that this *is* the preferred way of doing it. Saves on
RF transistors if nothing else! However one assumes at least *some*
degree of RF pre-amplification is needed to get a potentially very
weak signal beyond the knee of the diode characteristic.
There ISN'T really a knee. It only appears that there is because of the
way the I/V curve is plotted. If you plot log(I) against V you get
nearly a straight line, with nothing unusual happening at V = 0.6 to 0.7
V.
At low signal levels, a diode detector (or any rectifying junction) has
a *square law* transfer characteristic. If you put a voltage-doubler
diode rectifier (the two-diode circuit you've been shown by me and Jim)
at the *input* of an op-amp d.c. amplifier with your meter at the op-amp
output (through a series resistor), you'd have a working circuit.