Anyone who has used an oscilloscope will have come into contact with a probe. Usually, the oscilloscope we are talking about is used to measure voltage signals (there are also those that measure light or current , which are first converted into voltage measurements through corresponding sensors). The main function of the probe is to lead the voltage signal to be measured from the measurement point to the oscilloscope for measurement.
Most people pay more attention to the use of the oscilloscope itself, but ignore the selection of the probe. In fact, the probe is the intermediate link between the measured signal and the oscilloscope. If the signal is distorted at the probe, then no matter how good the oscilloscope is, it will be useless. In fact, the design of the probe is much more difficult than the oscilloscope, because the inside of the oscilloscope can be well shielded and does not need to be frequently disassembled. In addition to meeting the requirements of detection convenience, the probe must also ensure at least the same bandwidth as the oscilloscope, which is much more difficult. Therefore, when the earliest high-bandwidth real-time oscilloscope first appeared, there was no corresponding probe, and the probe came out after a while.
To choose a suitable probe, the first thing to do is to understand the impact of the probe on the test, which includes two parts: 1/the impact of the probe on the circuit under test; 2/the signal distortion caused by the probe. The ideal probe should have no impact on the circuit under test and no distortion on the signal. Unfortunately, no real probe can meet these two conditions at the same time, and usually some compromises need to be made between these two parameters.
In order to consider the impact of the probe on the measurement, we can usually simply equate the probe model to an R, L, C model, and analyze this model together with our circuit under test.
First, the probe itself has input
resistance
. Just like the principle of measuring
voltage
with a multimeter
, in order to minimize the impact on the measured
circuit
, the input resistance Rprobe of the probe itself is required to be as large as possible. However, since Rprobe cannot be infinite, it will produce voltage division with the measured circuit, and the actual measured voltage may not be the real voltage before the probe point, which is often encountered in the test of some
power supplies
or amplifier circuits. In order to avoid the influence of the probe resistance load, it is generally required that Rprobe is more than 10 times greater than Rsource and Rload. The input impedance of most probes is between tens of k ohms and tens of megohms.
Secondly, the probe itself has input capacitance . This capacitance is not deliberately added, but is the parasitic capacitance of the probe. This parasitic capacitance is also the most important factor affecting the bandwidth of the probe, because this capacitance will attenuate the high-frequency component and slow down the rising edge of the signal. Usually, the parasitic capacitance of high-bandwidth probes is relatively small. Ideally, Cprobe should be 0, but it is not possible in reality. Generally, the input capacitance of a passive probe is between 10pf and several hundred pf, and the input capacitance of an active probe with a higher bandwidth is generally between 0.2pf and several pf.
Secondly, the probe input will also be affected by inductance. The input resistance and capacitance of the probe are relatively easy to understand, but the inductance of the probe input is often overlooked, especially when measuring at high frequencies. Where does the inductance come from? We know that where there is a wire, there will be inductance. There must be a wire connecting the probe and the circuit under test, and the signal return must pass through the probe ground wire. Usually, the ground wire of a 1mm probe will have an inductance of about 1nH. The longer the signal and ground wires, the greater the inductance value. The parasitic inductance and parasitic capacitance of the probe form a resonant circuit. When the inductance value is too large, high-frequency resonance may occur under the excitation of the input signal, causing signal distortion. Therefore, the length of the signal and ground wires needs to be strictly controlled during high-frequency testing, otherwise ringing is likely to occur.
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