resistance entre chanel 1 et 2 oscilloscope | oscilloscope input resistance

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Understanding the input impedance of your oscilloscope is crucial for obtaining accurate and reliable measurements. This is particularly true when analyzing signals simultaneously on multiple channels, as the interaction between the oscilloscope's input impedance and the circuit under test can significantly affect the observed waveforms. This article delves into the intricacies of oscilloscope input impedance, specifically focusing on the implications of the resistance between channel 1 and channel 2, and how this impacts circuit analysis. We'll explore how this impedance affects measurements, how to account for it, and the best practices for minimizing its influence on your results.

Oscilloscope Input Impedance: A Foundation for Accurate Measurements

An oscilloscope's input impedance is the combined resistance, capacitance, and inductance presented by the input connector to the signal source. This impedance acts as a load on the circuit being measured. Ideally, the oscilloscope's input impedance should be infinitely high, meaning it draws no current from the circuit and doesn't affect its behavior. However, in reality, oscilloscopes have a finite input impedance, typically represented as a parallel combination of resistance and capacitance.

The most significant component of this impedance is the input resistance, usually denoted as Rin. This resistance is typically in the megaohm range (e.g., 1 MΩ) for most oscilloscopes. The input capacitance, Cin, is typically in the picofarad range (e.g., 10-20 pF). Both Rin and Cin influence the accuracy of measurements, particularly at higher frequencies where the capacitive component becomes more significant.

The Significance of the Resistance Between Channels

While the input impedance of individual channels is well-documented in the oscilloscope's specifications, the impedance between channels is less often explicitly stated. However, understanding this inter-channel impedance is crucial, especially when measuring differential signals or when the circuits under test have low impedance characteristics.

The resistance between channel 1 and channel 2 (let's denote it as R12) arises primarily from the internal circuitry of the oscilloscope. This resistance can influence measurements in several ways:

* Signal Attenuation: If a significant current flows between the channels due to a low impedance circuit under test, the voltage measured on each channel can be attenuated due to the voltage divider effect created by Rin and R12. This is especially problematic when measuring low-level signals.

* Signal Distortion: The capacitive coupling between channels can introduce frequency-dependent signal distortion. High-frequency components of the signal might be affected differently on each channel due to the capacitive coupling, leading to discrepancies in the measured waveforms.

* Ground Loops: If the circuit under test has multiple ground points, connecting the oscilloscope's probes to different points can create ground loops. These ground loops can introduce noise and distortion into the measurements, especially when the impedance between channels is low.

* Differential Measurements: When performing differential measurements (measuring the voltage difference between two points), the impedance between channels directly influences the accuracy of the measurement. A low inter-channel impedance can introduce significant errors in the differential voltage calculation.

Determining the Inter-Channel Resistance

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