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You need to test, we're here to help.
Showing posts with label transfer function. Show all posts
Showing posts with label transfer function. Show all posts

01 November 2018

How Equalization Works in 10x Passive Probes

The adjustable equalization circuit on the oscilloscope end of the coaxial cable compensates for the 10x passive probe's inherent low-pass filter characteristics
Figure 1: The adjustable equalization circuit on the oscilloscope
end of the coaxial cable compensates for the 10x passive
probe's inherent low-pass filter characteristics
We've been discussing 10x passive probes and their inner workings; our last post covered all the ways in which a 10x passive probe is apt to be a liability. They'd be basically unusable for any measurements at all but for one attribute: their equalization circuit (Figure 1). Without it, the 10x passive probe makes a pretty good low-pass filter, but the equalization circuit counters that with a high-pass filter to balance things out.

10 October 2018

Putting Probes in Perspective

Probe, cable, and oscilloscope form a system that makes or breaks the accuracy of signal acquisitions
Figure 1: Probe, cable, and oscilloscope form a system
that makes or breaks the accuracy of signal acquisitions
Few aspects of using an oscilloscope are as important as the probe: after all, the probe forms both the mechanical and electrical interfaces between the device under test (DUT) and the oscilloscope itself. To feed a signal into an oscilloscope, we're limited to a coaxial connection. Thus, we need a geometry transformer that picks up the signal of interest from the DUT and transfers it to the oscilloscope's coaxial connection.

23 February 2018

Transmission Lines (Part II): More on Bandwidth vs. Rise Time

In the frequency domain (right), a near-ideal square wave displays predictable 1/f amplitude dropoff
Figure 1: In the frequency domain (right), a near-ideal
square wave displays predictable 1/f amplitude dropoff
We began this series about transmission lines by thinking about some pertinent principles and relationships that can help form our thinking about the topic. In particular, we'd covered the relationship between bandwidth and rise time and why we have this rule of thumb that says that bandwidth can be estimated using 0.35/10-90% rise time.

22 May 2014

The Effects of Passive Probe Ground Leads

Teledyne LeCroy's PP108, a representative passive probe
Figure 1: Teledyne LeCroy's PP108,
a representative passive probe
When you open the box containing your shiny new oscilloscope, one of the items you'll likely find inside is a set of basic 10:1 passive probes (Figure 1). Those probes have a ground lead that you'll want to use when you make measurements. Your probe has a bandwidth specification that's probably somewhere between a few hundred megahertz to 1 GHz; that spec was obtained at the factory with a specialized test jig having a specific ground inductance and source impedance. Now, the way in which you connect your ground lead can have a big impact on the real-world bandwidth and response of the probe.