Signal Loading For Non-Differential Input Signals; Probing Philosophy - R&S RT-ZD40 Mode D'emploi

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R&S
RT-ZD40
5.2.2

Signal Loading for Non-Differential Input Signals

As described in
chapter 4, "Characteristics of Differential
various types of input signals can be measured with a differential probe. Every
type of input signal has an associated input impedance.
● For differential input signals, the input impedance of the probe is the impe-
dance between its positive and negative signal sockets.
● For single-ended input signals, the input impedance is the impedance
between the positive or negative signal socket and the ground socket.
● For common mode input signals, the input impedance is the impedance
between the parallel connection of the positive and negative signal sockets
and the ground socket.
The equivalent circuit diagram in
ated input impedance. The
ance for several input signals.
Table 5-3: DC Input Resistance for Various Input Signals
Type of input signal
Input Resistance
This table shows that common mode signals suffer the highest loading. This char-
acteristic of all differential probes is particularly bothersome because common
mode signals frequently have a very high source resistance (e.g. 10 kΩ for con-
ventional fail-safe circuits). While the input resistance achieved for common mode
voltages with the R&S RT-ZD40 differential probe remains sufficiently high,
probes with lower input resistances can lead to unfavorable loading effects.
5.3

Probing Philosophy

The previous sections made clear that probes exert a load on the signal to be
measured and change its characteristic. The signal at the test point where the
probe makes contact (V
before the probe was connected (V
with all real probes – independent of type and manufacturer.
User Manual 1410.5363.02 ─ 03
figure 5-1
table 5-3
provides as an example the DC input resist-
Differential
1 MΩ
) is therefore different from the signal that was present
in
). This effect cannot be avoided and occurs
S
Measurement Principles
Probes",
can be used to determine the associ-
Single-ended
500 kΩ
Probing Philosophy
on page 28,
Common mode
250 kΩ
42

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