OP281/OP481
Rev. D | Page 13 of 20
APPLICATIONS
THEORY OF OPERATION
The OPx81 family of op amps is comprised of extremely low
powered, rail-to-rail output amplifiers, requiring less than 4 μA of
quiescent current per amplifier. Many other competitors’ devices
may be advertised as low supply current amplifiers but draw
significantly more current as the outputs of these devices are driven
to a supply rail. The supply current of the OPx81 remains under
4 μA even when the output is driven to either supply rail. Supply
currents should meet the specification as long as the inputs and
outputs remain within the range of the power supplies.
Figure 36 shows a simplified schematic of a single channel for
the OPx81. A bipolar differential pair is used in the input stage.
PNP transistors are used to allow the input stage to remain
linear with the common-mode range extending to ground. This
is an important consideration for single-supply applications.
The bipolar front end also contributes less noise than a MOS
front end with only nanoamps of bias currents. The output of
the op amp consists of a pair of CMOS transistors in a common
source configuration. This setup allows the output of the
amplifier to swing to within millivolts of either supply rail. The
headroom required by the output stage is limited by the amount
of current being driven into the load. The lower the output
current, the closer the output can go to either supply rail.
Figure 11, Figure 12, and Figure 13 show the output voltage
headroom vs. the load current. This behavior is typical of rail-
to-rail output amplifiers.
00291-036
+IN
–IN
V
EE
OUT
V
CC
Figure 36. Simplified Schematic of a Single OPx81 Channel
INPUT OVERVOLTAGE PROTECTION
The input stage to the OPx81 family of op amps consists of a
PNP differential pair. If the base voltage of either of these input
transistors drops to more than 0.6 V below the negative supply,
the input ESD protection diodes become forward-biased, and
large currents begin to flow. In addition to possibly damaging the
device, this creates a phase reversal effect at the output. To prevent
this, the input current should be limited to less than 0.5 mA.
This can be done by simply placing a resistor in series with the
input to the device. The size of the resistor should be proportional
to the lowest possible input signal excursion and can be found
using the following formula:
3
,
105.0
×
=
MININEE
VV
R
where:
V
EE
is the negative power supply for the amplifier.
V
IN, MIN
is the lowest input voltage excursion expected.
For example, a single channel of the OPx81 should be used with a
single-supply voltage of +5 V if the input signal may go as low as
−1 V. Because the amplifier is powered from a single supply, V
EE
is
the ground; therefore, the necessary series resistance should be 2 kΩ.
INPUT OFFSET VOLTAGE
The OPx81 family of op amps was designed for low offset
voltages (less than 1 mV).
00291-037
OP281
V
OUT
+3V
100k
100k
100k
+
100k
V
IN
= 1kHz AT
400mV p-p
–0.1V
–0.27V
Figure 37. Single OPx81 Channel Configured as a Difference Amplifier
Operating at V
CM
< 0 V
INPUT COMMON-MODE VOLTAGE RANGE
The OPx81 is rated with an input common-mode voltage range
from V
EE
to 1 V less than V
CC
. However, the op amp can operate
with a common-mode voltage that is slightly less than V
EE
.
Figure 37 shows a single OPx81 channel configured as a difference
amplifier with a single-supply voltage of 3 V. Negative dc voltages
are applied at both input terminals, creating a common-mode
voltage that is less than ground. A 400 mV p-p input signal is
then applied to the noninverting input. Figure 38 shows the
resulting input and output waves. Notice how the output of the
amplifier also drops slightly negative without distortion.
10
0%
100
90
0V
V
OUT
V
IN
0.1V
00291-038
0.2ms
Figure 38. Input and Output Signals with V
CM
< 0 V
OP281/OP481
Rev. D | Page 14 of 20
CAPACITIVE LOADING
Most low supply current amplifiers have difficulty driving
capacitive loads due to the higher currents required from the
output stage for such loads. Higher capacitance at the output
will increase the amount of overshoot and ringing in the amplifier’s
step response and may affect the stability of the device. However,
through careful design of the output stage and its high phase
margin, the OPx81 family can tolerate some degree of capacitive
loading. Figure 39 shows the step response of a single channel
with a 10 nF capacitor connected at the output. Notice that the
overshoot of the output does not exceed more than 10% with
such a load, even with a supply voltage of only 3 V.
10
0%
100
90
00291-039
Figure 39. Ringing and Overshoot of the Output of the Amplifier
MICROPOWER REFERENCE VOLTAGE GENERATOR
Many single-supply circuits are configured with the circuit biased
to half of the supply voltage. In these cases, a false ground reference
can be created by using a voltage divider buffered by an amplifier.
Figure 40 shows the schematic for such a circuit.
The two 1 MΩ resistors generate the reference voltage while
drawing only 1.5 μA of current from a 3 V supply. A capacitor
connected from the inverting terminal to the output of the op amp
provides compensation to allow a bypass capacitor to be
connected at the reference output. This bypass capacitor helps
to establish an ac ground for the reference output. The entire
reference generator draws less than 5 μA from a 3 V supply source.
OP281
10k
0.022µF
V
REF
1.5V TO 6V
1µF
1µF
1M
3V TO 12
V
100
1M
8
4
3
1
2
00291-040
Figure 40. Single Channel Configured as a Micropower Bias Voltage Generator
WINDOW COMPARATOR
The extremely low power supply current demands of the OPx81
family make it ideal for use in long-life battery-powered
applications such as a monitoring system. Figure 41 shows a
circuit that uses the OP281 as a window comparator.
A1
R1
R2
3V
OP281-A
V
IN
2k
5.1k
3V
3
V
V
OUT
Q1
5.1k
V
H
D1
10k
A2
R3
R4
3V
3V
V
L
D2
OP281-B
00291-041
Figure 41. Using the OP281 as a Window Comparator
The threshold limits for the window are set by V
H
and V
L
,
provided that V
H
> V
L
. The output of the first OP281 (A1) will
stay at the negative rail, in this case ground, as long as the input
voltage is less than V
H
. Similarly, the output of the second
OP281 (A2) will stay at ground as long the input voltage is
higher than V
L
. As long as V
IN
remains between V
L
and V
H
, the
outputs of both op amps will be 0 V. With no current flowing in
either D1 or D2, the base of Q1 will stay at ground, putting the
transistor in cutoff and forcing V
OUT
to the positive supply rail.
If the input voltage rises above V
H
, the output of A2 stays at
ground, but the output of A1 goes to the positive rail and D1
conducts current. This creates a base voltage that turns on Q1
and drives V
OUT
low. The same condition occurs if V
IN
falls
below V
L
with A2’s output going high and D2 conducting
current. Therefore, V
OUT
is high if the input voltage is between
V
L
and V
H
, but low if the input voltage moves outside of that range.
The R1 and R2 voltage divider sets the upper window voltage,
and the R3 and R4 voltage divider sets the lower voltage for the
window. For the window comparator to function properly, V
H
must be a greater voltage than V
L
.
R4R3
R4
V
R2R1
R2
V
L
H
+
=
+
=
The 2 kΩ resistor connects the input voltage of the input
terminals to the op amps. This protects the OP281 from
possible excess current flowing into the input stages of the
devices. D1 and D2 are small-signal switching diodes (1N4446
or equivalent), and Q1 is a 2N2222 or an equivalent NPN
transistor.
OP281/OP481
Rev. D | Page 15 of 20
LOW-SIDE CURRENT MONITOR
In the design of power-supply control circuits, a great deal of
design effort is focused on ensuring the long-term reliability of
a pass transistor over a wide range of load current conditions.
As a result, monitoring and limiting device power dissipation is
of primary importance in these designs. Figure 42 shows an
example of a 5 V, single-supply current monitor that can be
incorporated into the design of a voltage regulator with fold-
back current limiting or a high current power supply with
crowbar protection. The design capitalizes on the OPx81’s
common-mode range extending to ground. Current is
monitored in the power-supply return path, where a 0.1 Ω
shunt resistor, R
SENSE
, creates a very small voltage drop. The
voltage at the inverting terminal becomes equal to the voltage at
the noninverting terminal through the feedback of Q1, which is
a 2N2222 or an equivalent NPN transistor. This makes the
voltage drop across R1 equal to the voltage drop across R
SENSE
.
Therefore, the current through Q1 becomes directly
proportional to the current through R
SENSE
, and the output
voltage is given by the following equation:
××=
L
SENSECC
OUT
IR
R
R
VV
1
2
The voltage drop across R2 increases as I
L
increases; therefore,
V
OUT
decreases if a higher supply current is sensed. For the
element values shown, the V
OUT
transfer characteristic is
−2.5 V/A, decreasing from V
CC
.
00291-042
RETURN TO
GROUND
V
CC
V
CC
R2
2.49k
V
OUT
R1
100
0.1
R
SENSE
Q1
SINGLE
CHANNEL
OPx81
Figure 42. Low-Side Load Current Monitor
LOW VOLTAGE HALF-WAVE AND FULL-WAVE
RECTIFIERS
Because of its quick overdrive recovery time, an OP281 can be
configured as a full-wave rectifier for low frequency (<500 Hz)
applications. Figure 43 shows the schematic.
00291-043
3V
OP281-A
V
IN
= 2V p-p
2k
3V
OP281-B
A2
R1
100k
R2
100k
FULL-WAVE
RECTIFIED
OUTPUT
HALF-WAVE
RECTIFIED
OUTPUT
A1
Figure 43. Single-Supply Full-Wave and Half-Wave Rectifiers Using an OP281
10
0%
100
90
00291-044
SCALE
0.1V/DIV
SCALE
0.1ms/DIV
Figure 44. Full-Wave Rectified Signal
Amplifier A1 is used as a voltage follower that tracks the input
voltage only when it is greater than 0 V. This provides a half-
wave rectification of the input signal to the noninverting
terminal of Amplifier A2. When A1’s output is following the
input, the inverting terminal of A2 also follows the input from
the virtual ground between the inverting and noninverting
terminals of A2. With no potential difference across R1, no
current flows through either R1 or R2; therefore, the output of
A2 also follows the input. When the input voltage goes below
0 V, the noninverting terminal of A2 becomes 0 V. This makes
A2 work as an inverting amplifier with a gain of 1 and provides
a full-wave rectified version of the input signal. A 2 kΩ resistor
in series with A1s noninverting input protects the device when
the input signal becomes less than ground.
BATTERY-POWERED TELEPHONE HEADSET
AMPLIFIER
Figure 45 shows how the OP281 can be used as a two-way
amplifier in a telephone headset. One side of the OP281 can be
used as an amplifier for the microphone, and the other side can
be used to drive the speaker. A typical telephone headset uses a
600 Ω speaker and an electret microphone that requires a
supply voltage and a biasing resistor.

OP281GSZ-REEL

Mfr. #:
Manufacturer:
Analog Devices Inc.
Description:
Operational Amplifiers - Op Amps 5V DUAL RRO 4uA IC 2.7-12V
Lifecycle:
New from this manufacturer.
Delivery:
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