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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 marketa market driven by technological advancesand 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 scopenow 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 todaythe price of progress!)
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 inputat the base of Q4234is 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.
Power and Instrumentation Electronics Archive
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