1 Overview
There are many types of probes, among which high-voltage differential probes are widely used in switching power supply applications. However, many engineers do not have a deep understanding of differential probes. There are also many differential probe manufacturers on the market, and their performance indicators vary, and even vary greatly, resulting in different measured waveforms, and engineers cannot see the correct waveform. This article will mainly explain what is a differential signal, the measurement of differential signals, the main indicators of high-voltage differential probes, advantages and disadvantages, and related usage tips, as well as the typical applications of high-voltage differential probes in switching power supplies.
2. What is differential signaling?
Before explaining differential probes, let's first understand differential signals. Differential signals are signals that reference each other, not the ground. For example, the voltage signal in the upper and lower switches (Q1, Q2) of the half-bridge in the switching power supply in Figure 1; the voltage signal in the multi-phase power system in Figure 2, the above signals are essentially "floating" above the ground.
3. Differential signal measurement method
The common measurement methods for differential signals are as follows:
1) Use two probes to measure, and then use the oscilloscope's math function to calculate, as shown in Figure 3
Using two probes to make two single-ended measurements is a common and least desirable approach to making differential measurements. By measuring the signal to ground (single-ended) and using the oscilloscope's math function (channel A signal minus channel B), the differential signal can be measured. This approach works well when the signal is low frequency and the signal amplitude is large enough to overcome any noise of concern. There are several potential problems with combining two single-ended measurements. One problem is that there are two separate long signal paths along each probe and through each oscilloscope channel. Any delay difference between these two paths will cause the two signals to be offset in time. On high-speed signals, this offset can cause significant amplitude and timing errors in the calculated differential signal. Another problem is that they do not provide adequate common-mode noise rejection. In real circuits , there are many sources of common-mode noise, such as noise caused by a nearby clock line on both signal lines, and noise from external sources such as fluorescence. As the frequency increases, the CMMR (common-mode rejection ratio) performance of single-ended measurements degrades rapidly. This can cause the signal to appear much noisier than it actually is if common-mode interference is retained.
2) Oscilloscope floating measurement
The most common wrong floating measurement method is the oscilloscope floating measurement method, which is to cut off the connection between the neutral line and the ground line by cutting off the ground line of the standard three-pin AC socket or using an AC isolation transformer. Float the oscilloscope from the protective ground line, as shown in Figure 4, to reduce the impact of the ground loop. This method is not feasible because the neutral line may be connected to the ground line somewhere in the building's wiring, which is an unsafe measurement method; in addition, it violates industrial health and safety regulations and the measurement results obtained are also poor. Moreover, when the oscilloscope is floating on the ground, a large parasitic capacitance will appear, and the floating measurement will be damaged by oscillation, and the measured waveform will be seriously distorted. There will be examples to demonstrate later. In short, oscilloscope floating measurement is easy to damage the device under test; damage the oscilloscope; bring potential harm to people; large measurement errors.
3) Differential measurement
The best solution for floating measurements is to use a differential probe with a high common-mode rejection ratio. Because there is no grounding problem at either input terminal, the differential operation of the two input signals is completed in the front-end amplifier of the probe, and the signal transmitted to the oscilloscope channel is a differential voltage. The oscilloscope can achieve safe floating measurements without removing the ground terminal of the three-wire plug, as shown in Figure 5.
4. Differential probe
Among the common differential probes, there is a type that is designed for low-voltage signals. This type of differential signal is more common in high-speed digital circuits. The common amplitude of the measured voltage of this type of differential probe is ±8V, and the bandwidth is generally above 1GHz. The other type is specifically designed for high-voltage measurement, with a measured voltage of up to KV. This type of differential signal is more common in switching power supply measurements. This type of differential probe is called a high-voltage differential probe. The measured voltage is generally at the KV level, and the bandwidth is more commonly in the range of 20MHz-100MHz.
Differential probes are mainly used for measuring floating ground systems. In power system testing, it is often required to measure the relative voltage difference between the live wire and the live wire, or between the live wire and the neutral (neutral) wire in the three-phase power supply. Many users directly use single-ended probes to measure the voltage at two points, which often causes the probe to burn out. This is because the "signal common line" terminal of most oscilloscopes is connected to the protective grounding system, usually called "grounding". The result of this is that all signals applied to the oscilloscope and provided by the oscilloscope have a common connection point. This common connection point is usually the oscilloscope case. The probe ground wire is connected to a test point by using the third conductor ground wire in the power cord of the AC power supply device. If a single-ended probe is used for measurement at this time, the ground wire of the single-ended probe is directly connected to the power supply line, and the result is bound to be a short circuit. In this case, we need a differential probe for floating ground measurement.
Three important indicators of differential probes:
Bandwidth (common): All probes have a bandwidth. The bandwidth of a probe is the bandwidth over which the probe response causes the output amplitude to drop to 70.7%.
(-3 dB) frequency, as shown in Figure 6. When selecting an oscilloscope and oscilloscope probe, it is important to realize that bandwidth affects measurement accuracy in many ways. In amplitude measurements, as the frequency of a sine wave approaches the bandwidth limit, the amplitude of the sine wave becomes increasingly attenuated. At the bandwidth limit, the amplitude of the sine wave is measured as 70.7% of the actual amplitude. Therefore, to achieve the greatest amplitude measurement accuracy, it is necessary to select an oscilloscope and probe with a bandwidth several times higher than the highest frequency waveform you plan to measure. The same applies to measuring waveform rise and fall times. Waveform transition edges, such as pulse and square wave edges, are composed of high-frequency components. Bandwidth limitations attenuate these high-frequency components, resulting in displayed transitions that are slower than the actual transition speed. To accurately measure rise and fall times, the measurement system used must have sufficient bandwidth to retain the high-frequency components that make up the rise and fall times of the waveform. Most commonly, when measuring the rise time of a system, the system's rise time should generally be 4-5 times faster than the rise time to be measured. In the field of switching power supplies, a bandwidth of 50MHz is generally sufficient.
CMRR (Common Mode Rejection Ratio): Common Mode Rejection Ratio (CMRR) is the ability of a differential probe to reject the common mode signal at two test points in a differential measurement. This is the key specification for differential probes and is given by the formula: CMRR = |Ad/Ac|. Where: Ad = voltage gain of the differential signal. Ac = voltage gain of the common mode signal. Ideally, Ad should be large and Ac should be equal to 0, so the CMRR is infinite. In practice, a CMRR of 10,000:1 is considered very good. This means that a 5 V common mode input signal will be rejected so that it appears as 0.5 mV at the output. Since CMRR decreases with increasing frequency, the frequency at which CMRR is specified is as important as the CMRR value. CMRR is particularly important when measuring the upper tube drive wave of a full-bridge or half-bridge circuit, which is also a difficulty for high voltage differential probes to measure such signals. As shown in Figure 1, the upper tube GS driving voltage is very small, but the common mode voltage is very high. When measuring the waveform at this point, the CMRR requirements for the differential probe are relatively high. There will be examples to demonstrate the analysis later.
Distortion: Distortion is any deviation in amplitude from the expected or ideal response of the input signal. In practice, distortion usually occurs immediately between fast waveform transitions, which manifests as the so-called "ringing". The two differential input lines of the differential probe are very long, usually about 50cm. If the differential probe is not designed well, the measured signal is prone to distortion. Differential probes from different manufacturers on the market may produce different results, and some may differ greatly. This indicator is one of the reasons.
Of course, the differential probe also has indicators such as input impedance, input capacitance, accuracy, and attenuation coefficient. There is not much difference among different manufacturers on the market, and generally there will be no problems, so I will not introduce them one by one here.
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Next article:Special Uses of Digital Oscilloscope
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