
Catalog excerpts

Probing Solutions PP066 High Bandwidth Passive Probe Technical Specifications Electrical Characteristics: Bandwidth Maximum Voltage: Cable Length: Transmission Line Probing The PP066 is a high-bandwidth passive probe designed for the use with the WaveMaster™ and other high-bandwidth oscilloscopes that have 50 Ω input termination.This very low capacitance probe provides an excellent solution for higher frequency applications, especially the probing of transmission lines with 20–100 Ω impedance. Flexibility Interchangeable attenuator tips provide the user a choice of input resistances and sensitivities.The probe cable connection is a standard SMA. PP066 probes are suited to a wide range of design applications including probing of analog and digital IC's commonly found in computer, communications, data storage, and other high-speed designs. Signal Integrity at High Bandwidth When measuring very high frequencies, use of a probe with low input capacitance is the key to preserving signal integrity. A 1 pf active probe, though nominally high impedance, loads a 1 GHz signal with 159 ohm capacitive reactance (X = 1/2π fC). The PP066 preserves high bandwidth content of signals, retaining proper signal shape even for very fast edges. The PP066 passive probe has lower circuit loading at high frequencies than an active probe. PROBING HIGH SPEED SIGNALS Accurately measuring digital waveforms with oscilloscopes becomes increasingly challenging as edge speeds become faster. Often, interconnecting the test circuit to the oscilloscope is the most difficult part of the problem. Designers frequently select an active probe as the tool of choice for this task. However, in many situations a lesser known type of passive probe can provide better performance at a lower cost. Probing any circuit for the purpose of making a measurement will change its operation. This is often the case when it comes to measuring waveforms with high frequency content. Extremely small parasitic elements added to the probe circuit can greatly distort the signal being measured. Probe loading is usually the most significant factor that contributes to waveform distortion. Any real life voltage signal can be diagrammed as a Thévenin equivalent model represented as an ideal voltage source with a series impedance between it and the test point where the probe is connected (see the figure on back). The impedance in the probe to ground forms a voltage divider, which attenuates the measured signal. If the impedances were purely resistive, this effect could be easily compensated for by applying a scalar multiplier to the measured waveform amplitude. However, the reactive portions of the circuit’s source impedance and the measurement probe create a frequency dependent attenuation that cannot be effectively corrected. As the frequency content of the signal being measured increases, even the most minute parasitic capacitance and inductance will impart significant attenuation, greatly distorting the appearance of the measured waveform. Consider an example where we probe a fast digital signal with a 1 ns transition time using a high-quality passive probe. The input impedance of these probes is generally 1 MΩ in parallel with about 10 pF. If the source impedance of the circuit being tested is 30 Ω , the 1 MΩ resistive component of the probe creates virtually no DC attenuation. However, the effect of the capacitance is significant. Using the basic rule to translate rise time into
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Sales and Service Throughout the World Corporate Headquarters 700 Chestnut Ridge Road Chestnut Ridge, NY 10977 USA http://www.lecroy.com LeCroy Sales Offices: Simplified model of probe loading effects frequency, 1 ns rise time corresponds to approximately 350 MHz. The capacitive reactance of 10 pF at 350 MHz is 45 Ω. So during the 1 ns transition, the impedance in the lower leg of the voltage divider would be 45 Ω rather than 1 MΩ, attenuating the signal by approximately 40%. Since we usually cannot tolerate measurements that include 40% or greater errors, an active probe is often used to...
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