R
Robert Baer
- Jan 1, 1970
- 0
Fred said:Takes forever to converge.
I softened the analysis a bit by making the pulse risetime 20ns, similar
to your HP3312A, but it's still excruciatingly slow.
How sure are you of the resistor model? Have you considered making it a
uniform RC line (U) model? I'll try that in a while, it might converge
faster.
There's a pole at around 67 Hz that needs addressing.
I added 3 feet of RG179, which i have a model for, which is similar to
RG175, for which I don't. The inevitable quarter-wave spikes appear at
around 46MHz, et seq. 60 ohms in series with each end of the coax tames
this, and we now have a 3dB rolloff around 70MHz, making risetime about
5ns. That's why resistive cable is used in commercial probes.
I'd do what Tektronix do, and do all compensation at the 'scope end.
Bear in mind that Tek's 40kV probes used to run their HV resistor in an
atmosphere of Fluorcarbon 114 vapor, which needed topping up from time to
time. I don't know what they use these days in HV probes, but I doubt it's
FC.
Try this, it's your circuit with 3 feet of coax. Do an .ac analysis, with
and without the 60 ohm resistors.
I see you made Cs, capacitance from floating shields, a lot larger =
8pf instead of my wild guesstimate of 0.1pf.
Those floating shields allow defined and predictable capacitive
coupling across the resistors; the capacitance from them to "outer
space" ground seems to be undefinable: coax capacitance runs
(log(D/d))^-1 and with a theoretically infinite D (or very large D in
reality),the capacitance is rather close to zero.
I picked 0.1pf as an estimate to that "zero"; seems you picked a huge
8pf.
*
I did not know of that uniform RC line (U) model; it would be an
excellent choice; better than the pi-pad scheme.
Values can easily be calculated on basis of resistor diameter,
dielectric material and floating shield diameter.
Seems that an eXplicit shield around the floating shield makes for
more trouble.