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AD8551ARMZ Datasheet(PDF) 14 Page - Analog Devices

Part # AD8551ARMZ
Description  Zero-Drift, Single-Supply, Rail-to-Rail Input/Output Operational Amplifiers
PDF  24 Pages
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Manufacturer  AD [Analog Devices]
Direct Link  http://www.analog.com
Logo AD - Analog Devices

AD8551ARMZ Datasheet(HTML) 14 Page - Analog Devices

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AD8551/AD8552/AD8554
Data Sheet
Rev. F | Page 14 of 24
FUNCTIONAL DESCRIPTION
The AD8551/AD8552/AD8554 are high precision, rail-to-rail
operational amplifiers that can be run from a single-supply voltage.
Their typical offset voltage of less than 1 μV allows these amplifiers
to be easily configured for high gains without risk of excessive
output voltage errors. The extremely small temperature drift of
5 nV/°C ensures a minimum of offset voltage error over its
entire temperature range of −40°C to +125°C, making the
AD8551/AD8552/AD8554 amplifiers ideal for a variety of
sensitive measurement applications in harsh operating
environments, such as underhood and braking/suspension
systems in automobiles.
The AD8551/AD8552/AD8554 are CMOS amplifiers and
achieve their high degree of precision through auto-zero
stabilization. This autocorrection topology allows the
AD8551/AD8552/AD8554 to maintain its low offset voltage
over a wide temperature range and over its operating lifetime.
AMPLIFIER ARCHITECTURE
Each AD8551/AD8552/AD8554 op amps consist of two
amplifiers, a main amplifier and a secondary amplifier, used
to correct the offset voltage of the main amplifier. Both consist
of a rail-to-rail input stage, allowing the input common-mode
voltage range to reach both supply rails. The input stage consists
of an NMOS differential pair operating concurrently with a
parallel PMOS differential pair. The outputs from the
differential input stages are combined in another gain stage
whose output is used to drive a rail-to-rail output stage.
The wide voltage swing of the amplifier is achieved by using two
output transistors in a common-source configuration. The output
voltage range is limited by the drain-to-source resistance of
these transistors. As the amplifier is required to source or sink
more output current, the rDS of these transistors increases, raising
the voltage drop across these transistors. Simply put, the output
voltage does not swing as close to the rail under heavy output
current conditions as it does with light output current. This is a
characteristic of all rail-to-rail output amplifiers. Figure 12 and
Figure 13 show how close the output voltage can get to the rails
with a given output current. The output of the AD8551/AD8552/
AD8554 is short-circuit protected to approximately 50 mA of
current.
The AD8551/AD8552/AD8554 amplifiers have exceptional gain,
yielding greater than 120 dB of open-loop gain with a load of 2 kΩ.
Because the output transistors are configured in a common-source
configuration, the gain of the output stage, and thus the open-
loop gain of the amplifier, is dependent on the load resistance.
Open-loop gain decreases with smaller load resistances. This is
another characteristic of rail-to-rail output amplifiers.
BASIC AUTO-ZERO AMPLIFIER THEORY
Autocorrection amplifiers are not a new technology. Various IC
implementations have been available for more than 15 years with
some improvements made over time. The AD8551/AD8552/
AD8554 design offers a number of significant performance
improvements over previous versions while attaining a very
substantial reduction in device cost. This section offers a simplified
explanation of how the AD8551/AD8552/AD8554 are able to
offer extremely low offset voltages and high open-loop gains.
As noted in the Amplifier Architecture section, each AD8551/
AD8552/AD8554 op amp contains two internal amplifiers. One
is used as the primary amplifier, the other as an autocorrection,
or nulling, amplifier. Each amplifier has an associated input
offset voltage that can be modeled as a dc voltage source in
series with the noninverting input. In Figure 50 and Figure 51
these are labeled as VOSX, where x denotes the amplifier
associated with the offset: A for the nulling amplifier and B for
the primary amplifier. The open-loop gain for the +IN and −IN
inputs of each amplifier is given as AX. Both amplifiers also have
a third voltage input with an associated open-loop gain of BX.
There are two modes of operation determined by the action of
two sets of switches in the amplifier: an auto-zero phase and an
amplification phase.
Auto-Zero Phase
In this phase, all φA switches are closed and all φB switches are
opened. Here, the nulling amplifier is taken out of the gain loop
by shorting its two inputs together. Of course, there is a degree
of offset voltage, shown as VOSA, inherent in the nulling amplifier
which maintains a potential difference between the +IN and
−IN inputs. The nulling amplifier feedback loop is closed through
φB2 and VOSA appears at the output of the nulling amp and on
CM1, an internal capacitor in the AD8551/AD8552/AD8554.
Mathematically, this is expressed in the time domain as
VOA[t] = AAVOSA[t] − BAVOA[t]
(1)
which can be expressed as

 
A
OSA
A
OA
B
t
V
A
t
V
1
(2)
This demonstrates that the offset voltage of the nulling amplifier
times a gain factor appears at the output of the nulling amplifier
and, thus, on the CM1 capacitor.
+
AB
BB
CM2
VIN+
VNB
CM1
VOA
–BA
VNA
ФB
ФA
AA
VOSA
ФB
ФA
VOUT
VIN–
Figure 50. Auto-Zero Phase of the AD8551/AD8552/AD8554



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