Do you have anything with a input anywhere close to 3.9 puff...?
Or are you employing a variant of Bait Theory...?
mnem
Ah, so that's what the 3.9pf marking onthe probe means....
I was thinking of using them on my TDS 694C. Neither the front panel nor the user manual state what the input capacitance is, but it's a 3GHz scope so presumably it should do it ?!
3.9pF is the capacitance of the probe, not the scope. They don't need to match. High bandwidth probes always have low capacitance. Capacitance attenuate the signal at high frequency, resistors at lower frequency. That's why you have a mix of both in oscilloscope probes. The passive probe is a frequency compensated voltage divider.
Erm, there still seems to be some confusion here. I'm sure you all know what you mean, and are trying to say the right thing, but please excuse me if offer up a little clarification "for the young players".
Scope probes come in two basic flavours: high impedance probes which nowadays are almost always designed to work with 1MΩ scope input impedance, and low impedance probes that are designed to work with scopes with a 50Ω input impedance. In both cases the probe's impedance is not just resistive, but is reactive too (this is also true for the scope input the probe plugs into). Probes have stray capacitance, but also
deliberate capacitance introduced to
compensate for both the strays and in the input capacitance of the scope and produce as flat a frequency response as the construction allows. The compensation is designed to be adjustable to provide wiggle room for the tolerances involved in all the probe and input components.
The Tek probe in question is a high impedance one.
In the case of that 3.9pF 10MΩ Tektronix probe, the 3.9pF figure given
is the input capacitance (I checked the datasheet for it) as seen by the DUT
but there is a small range of input capacitances
for the scope input that the probe is capable of being properly compensated for. For high impedance probes the input capacitance of the scope
does need to match (within some range) the capabilities of the probe. (The TPP1000 data sheet does not state this range. That is unusual, it's a normal part of a probe specification.) The unspecified scope input capacitance will
not be that 3.9pF figure; it's likely to be on the close order of about 20pF.
For low impedance probes matching is not really an issue because generally "
as low a capacitance as possible" is the target and the issue of of HF and LF response balancing is less of a problem as the impedance seen by the probe input is both lower and flatter. To get a flavour of this, let's look at the impedance curve for that TPP1000 10MΩ probe:
You can see that as we get to higher frequencies the input impedance is dominated by the reactance of that 3.9pF input capacitance. The reactance of 3.9pF at 100 MHz is 408Ω, and it is no coincidence that's the region that the probe impedance is in by the time we get to 100MHz. Now, for a probe with 50Ω resistive impedance the 400Ω in parallel to that has a fraction of the effect (about 44Ω total) compared to being in parallel with 10MΩ (calculated as 407Ω for completeness sake) - a reduction of 12% compared to a reduction of 99.996%.