Today, when I was doing a performance test experiment of a solid-state relay (SSR), I gave a square wave to the control end of the SSR and used an oscilloscope to observe the output signal. It should be a good square wave. However, when the oscilloscope selected an input impedance of 1MΩ, the waveform displayed on the oscilloscope screen was very strange. When the input impedance of the oscilloscope was switched to 50Ω, the observed waveform was a good square wave.
This is a bit strange. When an oscilloscope collects voltage signals, shouldn't the larger the input impedance, the better? I checked some information, but I still don't fully understand it, so I'll post it here.
Ideally, testing the instrument under test should not affect its normal operation, and the measured value should be the same as when the test instrument is not connected. When connecting the instrument for measurement, the impact of impedance on the measurement accuracy must be considered. In order to ensure that the maximum power can be transmitted between the instruments, the impedance should be matched. If the impedance is a pure resistor, the input impedance should be equal to the output impedance. If the impedance contains reactance The components should make the input impedance of the load conjugate with the output impedance of the source, so that the maximum power can be transmitted.
The impedance value of impedance matching is usually consistent with the characteristic impedance value of the transmission line used. For RF systems, 50Ω impedance is generally used. For high-impedance instruments, due to the existence of equivalent parallel capacitance, as the frequency increases, the parallel combination impedance gradually decreases, which will form a load on the circuit under test. For example, with a 1MΩ input impedance, when the frequency reaches 100MHz, the equivalent impedance is only about 100Ω. Therefore, high-bandwidth oscilloscopes generally use 50Ω input impedance, which can ensure the matching of the oscilloscope and the source end. However, when using a 50Ω input impedance, it must be considered that the load effect of the 50Ω input impedance is more obvious. At this time, it is best to use a low-capacitance active probe.
Keywords:Oscilloscope
Reference address:Impedance selection for oscilloscopes
This is a bit strange. When an oscilloscope collects voltage signals, shouldn't the larger the input impedance, the better? I checked some information, but I still don't fully understand it, so I'll post it here.
In the power supply noise test, there is still controversy over the selection of oscilloscope channel input impedance. The oscilloscope channel has
three options: DC50/DC1M/AC1M (for high-end oscilloscopes, there may be only one option: DC50). Some engineers believe that 1M ohm input impedance should be used, while others believe that 50 ohm input impedance is more appropriate. In the test, we found that if a probe with 1x attenuation is used for testing, when the oscilloscope channel input is 1M ohm, the power supply noise measured is usually greater than the 50 ohm input impedance. The reason is that after the high-frequency power supply noise is transmitted from the coaxial cable to the oscilloscope channel, when the oscilloscope input impedance is 50 ohms, the characteristic impedance of the coaxial cable of 50 ohms is completely matched with the channel, and there is no reflection; when the channel input impedance is 1M ohms, it is equivalent to high impedance. According to the transmission line theory, the power supply noise is reflected, which causes the 1M ohm input impedance to be higher than the 50 ohm of the tested power supply noise. Therefore, it is recommended to use a 50 ohm input impedance to measure small power supply noise.
three options: DC50/DC1M/AC1M (for high-end oscilloscopes, there may be only one option: DC50). Some engineers believe that 1M ohm input impedance should be used, while others believe that 50 ohm input impedance is more appropriate. In the test, we found that if a probe with 1x attenuation is used for testing, when the oscilloscope channel input is 1M ohm, the power supply noise measured is usually greater than the 50 ohm input impedance. The reason is that after the high-frequency power supply noise is transmitted from the coaxial cable to the oscilloscope channel, when the oscilloscope input impedance is 50 ohms, the characteristic impedance of the coaxial cable of 50 ohms is completely matched with the channel, and there is no reflection; when the channel input impedance is 1M ohms, it is equivalent to high impedance. According to the transmission line theory, the power supply noise is reflected, which causes the 1M ohm input impedance to be higher than the 50 ohm of the tested power supply noise. Therefore, it is recommended to use a 50 ohm input impedance to measure small power supply noise.
The impedance matching of the probe refers to the impedance matching between the probe and the oscilloscope circuit, which is mainly the capacitance effect. When the impedance does not match, the signal will be reflected at the interface between the probe and the oscilloscope, thus generating oscillation. The higher the frequency waveform, the more obvious the performance.
There is a signal point on the oscilloscope for calibrating the square wave waveform output. Connect the probe to it and level the square wave. Generally, we think that the impedance of the probe is matched. Of course, other such matches are not complete. But generally, the maximum bandwidth of the passive probe is 5~6 Mbps, which is enough. When it comes to active probes, 50 ohms are generally used, so the impedance matching problem is easy to solve. Ideally, testing the instrument under test should not affect its normal operation, and the measured value should be the same as when the test instrument is not connected. When connecting the instrument for measurement, the impact of impedance on the measurement accuracy must be considered. In order to ensure that the maximum power can be transmitted between the instruments, the impedance should be matched. If the impedance is a pure resistor, the input impedance should be equal to the output impedance. If the impedance contains reactance The components should make the input impedance of the load conjugate with the output impedance of the source, so that the maximum power can be transmitted.
The impedance value of impedance matching is usually consistent with the characteristic impedance value of the transmission line used. For RF systems, 50Ω impedance is generally used. For high-impedance instruments, due to the existence of equivalent parallel capacitance, as the frequency increases, the parallel combination impedance gradually decreases, which will form a load on the circuit under test. For example, with a 1MΩ input impedance, when the frequency reaches 100MHz, the equivalent impedance is only about 100Ω. Therefore, high-bandwidth oscilloscopes generally use 50Ω input impedance, which can ensure the matching of the oscilloscope and the source end. However, when using a 50Ω input impedance, it must be considered that the load effect of the 50Ω input impedance is more obvious. At this time, it is best to use a low-capacitance active probe.
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