Circuit Note
CN-0122
Circuit Designs Using Analog Devices Products
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Devices Connected/Referenced
AD8271/AD8274 Difference Amplifier
ADA4627-1
High Speed JFET Input Operational
Amplifier
AD8599 Low Noise Operational Amplifier
High Speed Instrumentation Amplifier Using the AD8271 Difference Amplifier and
the ADA4627-1 JFET Input Op Amp
Rev.A
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CIRCUIT FUNCTION AND BENEFITS
A traditional method for building an instrumentation amplifier is
to use three op amps and seven resistors as shown in Figure 1.
This approach requires four precision matched resistors for a good
common-mode rejection ratio (CMRR). Errors in matching will
produce errors at the final output. An imbalance of one or two
picofarads on certain nodes will drastically degrade the high
frequency CMRR, a fact often overlooked.
This circuit uses a monolithic difference amplifier with laser
trimmed thin film resistors for the output amplifier, thereby
providing good dc and ac accuracy with fewer components
than the traditional approach.
CIRCUIT DESCRIPTION
This circuit utilizes the AD8271 difference amplifier and two
ADA4627-1 amplifiers, which have low noise, low drift, low
offset, and high speed. For high impedance sources, the
ADA4627-1 is an ideal choice for the input stage amplifiers due
to the extremely low input bias current of their JFET inputs.
The op amps selected for the input stage must also have low
offset voltage and low offset voltage drift with temperature. They
also need to have good drive characteristics. This allows the use
of low value resistors to minimize resistor thermal noise.
Headroom issues relating to the op amp must be considered in
this circuit for proper operation.
When working with any op amp having a gain-bandwidth
product greater than a few MHz, careful layout and bypassing
are essential. A typical decoupling network consists of a 1 µF
to 10 µF electrolytic capacitor in parallel with a 0.01 µF to
0.1 µF low inductance ceramic MLCC type.
For the lowest noise with low impedance sources only, low
voltage noise is important. The AD8599 has lower noise, lower
offset voltage drift, and lower supply current; but the input bias
currents are much higher, and the bandwidth will be lower than
that obtained with the ADA4627-1. The measured −3 dB points
–IN
+IN
10kΩ
10kΩ
10kΩ
10kΩ
ADA4627-1
ADA4627-1
R
G
20Ω
R
F1
R
F2
2kΩ
AD8271
OUT
2kΩ
V
S
= ±15V
08517-001
+V
S
+V
S
–V
S
+V
S
–V
S
–V
S
NOTES
1. 10kΩ THIN FILM TRIMMED RESISTOR
ARE INTERNAL TO THE AD8271.
Figure 1. In Amp with Gain = 201
(Simplified Schematic: Decoupling and All Connections Not Shown)
are 56.6 kHz and 87.6 kHz for the AD8599 and ADA4627-1,
respectively. (See Figure 2).
With high impedance sources, the input bias current and the
input noise current of a bipolar op amp can result in errors. The
bias current creates an I × R drop, which will be multiplied by
the overall circuit gain. This can result in several volts of offset
at the output. The input noise current is also multiplied by the
source impedances, creating an additional noise voltage. To
avoid this, a JFET input op amp, such as the ADA4627-1,
should be used. Even though the voltage noise is slightly higher
than the AD8599, the current noise is significantly lower,
resulting in lower overall noise when used with high impedance
sources.
As Figure 3 and Figure 4 show, the AD8599 is the proper choice
with low source impedances, and the ADA4627-1 is better with
higher source impedances. There is a trade-off: the input
capacitance of JFET op amps is higher than bipolar op amps, so
the RC time constant must be considered.