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EE Expert Dennis Feucht
Power & Instrumentation Electronics

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Race Cars, Oscilloscopes, and Fully Differential Amplifiers Page 1 of 2
by Dennis Feucht

Semiconductor companies are now introducing fully differential amplifiers. These diff-amps are differential not only at their input, but also at the output, doubling their output range. These input and output circuits have closed paths not shared by other signals through a common ground node. This circuit (and hence signal) isolation improves signal integrity. By keeping both the input and the output circuits complete in themselves, the ground is only important for dc analysis and range determination. So what do these diff-amps have to do with race cars?

The "Race Track" in Electronics

State-of-the-art or "leading-edge" technology is often developed in adventurous settings. New automotive ideas, such as overhead cams and multi-port valving, are refined and characterized by applying them in demanding situations that have no significant effect on the company's present business. That setting is the race track, where technical concepts compete for performance advantages. The winning ideas go on to become integrated into products, where they then help compete for market share.

Where is the "race track" setting in electronics? Although the electronics industry lacks a glamorous event like the Indy 500, exciting developments occur in several branches of the field. For example, the Radiation Laboratory at MIT turned out some excellent results in the development of radar during WW II. Electronikers can admire, even to this day, the set of "Rad Lab" volumes from that era, containing a good, solid presentation of theory backed up by the electronics implemented. An earlier example: when Vladimir Zworykin developed television at RCA, this was an impressive breakthrough entirely unlike the incremental improvements of next-generation commodity products.

In the 1950s, the development of a laboratory-quality cathode-ray oscilloscope at Tektronix by Howard Vollum, Jack Murdock, Cliff Moulton, John Kobbe (to whom one Tek legend attributes the invention of the JK flip-flop), Bill Polits, and other highly creative engineers led to a most desirable technical environment for the motivated designer. With over 70% of the oscilloscope market—a market driven by technological advances—and with founders that were inventive engineers themselves, Tek was an engineering-driven company, an idea-advancing enterprise.

Although Tek and H-P are the outstanding examples of test and measurement (T&M) instrument companies, it is generally the case that high-performance T&M is the "race track" of the electronics industry. After all, one must be able to measure the behavior of circuits being developed, and test-equipment circuitry must be that much better to make the measurements. No wonder that interesting circuits are found in T&M equipment. And this leads to diff-amps.

Diff-Amps Found in Scopes

Oscilloscopes have used fully differential amplifiers for decades. (Why did it take so long for them to appear as commercial ICs?) Typical examples are found in vertical amplifiers. These scope subsystems amplify the probe voltage by precise gains before applying the amplified waveform to the vertical deflection plates of the CRT. And except for the first stage, which is driven by a ground-referenced probe, they are fully differential amplifiers, through and through. To demonstrate, let's look at part of the vertical amplifier of a Tek T935A 35 MHz scope—now obsolete, 1970s vintage, and low-cost. The input buffer amplifier stage, scanned from the manual, is shown below in Figure 1. (And by the way, the old Tek "instruction manuals" as they were called, contained schematics that were works of art, unparalleled by EDA CAD drawings of today—the price of progress!)

Figure 1
Figure 1 - Tek T935A 35 MHz Oscilloscope Input Buffer Amplifier

The very first stage consists of JFETs Q4222A and B. The probe waveform is input to the gate of Q4222B. A ×1 buffer amplifier is formed with the other JFET below it, with a near-zero offset voltage between the input and the output. This is accomplished by using matched JFETs, and using the lower one as a current source. Its gate is connected to the –8 V supply, and whatever VGS results from the drop across R4225 (the 20 W resistor in its source) corresponds to a drain current that flows through the JFET above it. The JFETs are matched, and the upper JFET will then have the same VGS. The corresponding lower terminal voltage across R4224, another 20 W resistor, is consequently the same as the input gate voltage. Some current from the upper JFET is gained as the base current of Q4232, but it is minor and the matching is quite good.

This amplifier drives a full diff-amp consisting of Q4232 and Q4234 at the second stage. Only the upper BJT (Q4232) is driven by the waveform to be amplified, while the lower input—at the base of Q4234—is ac-grounded to the scope-probe circuit ground, thus completing the return of the input circuit. Because vertical amplifiers (like all amplifiers) have an input offset error, the otherwise unused input is used for offset-error adjustment, which in oscilloscope language is dc balance. The word balance is a hint that oscilloscope amplifiers are heavily differential and that the two sides of the amplifier must be made to operate with the same dc conditions.

The output of stage 2 is also differential. This stage is only an emitter-follower, with no voltage gain, but it is needed to present a high input impedance to the JFET buffer while driving stage 3 with a low impedance. In other words, it presents a voltage source to the next stage. However, the input waveform is not yet differentially balanced at its differential output because the emitter-followers have no gain interaction between them and no splitting of the input waveform occurs between them. Stage 2 is differential only in that it has two inputs and two outputs. With no voltage gain, the input difference voltage is the output difference voltage.

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