FEATURES
Single-Supply Operation: 2.7 V to 12 V
Wide Input Voltage Range
Rail-to-Rail Output Swing
Low Supply Current: 300 A/Amp
Wide Bandwidth: 3 MHz
Slew Rate: 0.5 V/s
Low Offset Voltage: 700 V
No Phase Reversal
APPLICATIONS
Industrial Process Control
Battery-Powered Instrumentation
Power Supply Control and Protection
Telecommunications
Remote Sensors
Low Voltage Strain Gage Amplifiers
DAC Output Amplifiers
GENERAL DESCRIPTION
The OP191, OP291, and OP491 are single, dual, and quad
micropower, single-supply, 3 MHz bandwidth amplifiers featuring rail-to-rail inputs and outputs. All are guaranteed to
operate from a +3 V single supply as well as ± 5 V dual supplies.
Fabricated on Analog Devices’ CBCMOS process, the OP191
family has a unique input stage that allows the input voltage to
safely extend 10 V beyond either supply without any phase inversion or latch-up. The output voltage swings to within millivolts
of the supplies and continues to sink or source current all the
way to the supplies.
Applications for these amplifiers include portable telecommunications equipment, power supply control and protection, and
interface for transducers with wide output ranges. Sensors
requiring a rail-to-rail input amplifier include Hall effect, piezo
electric, and resistive transducers.
The ability to swing rail-to-rail at both the input and output
enables designers to build multistage filters in single-supply
systems and to maintain high signal-to-noise ratios.
The OP191/OP291/OP491 are specified over the extended
industrial –40∞C to +125∞C temperature range. The OP191 single
and OP291 dual amplifiers are available in 8-lead plastic SOIC
surface-mount packages. The OP491 quad is available in 14-lead
PDIP, narrow 14-lead SOIC, and 14-lead TSSOP packages.
PIN CONFIGURATIONS
8-Lead Narrow-Body
SOIC
NC
–INA
+INA
1
2
OP191
3
–V
4
8
7
6
5
NC
+V
OUTA
NC
14-Lead Narrow-Body
SOIC
OP491
14
OUTD
13
–IND
12
+IND
11
–V
10
+INC
9
–INC
8
OUTC
OUTA
–INA
+INA
+V
+INB
–INB
OUTB
1
2
3
4
5
6
7
14-Lead TSSOP
8-Lead Narrow-Body
SOIC
OUTA
–INA
+INA
1
2
OP291
3
–V
4
8
7
6
5
+V
OUTB
–INB
+INB
14-Lead PDIP
OUTA
–INA
+INA
+V
+INB
–INB
OUTB
1
2
3
4
5
6
7
OP491
14
13
12
11
10
9
8
OUTD
–IND
+IND
–V
+INC
–INC
OUTC
REV. C
Information furnished by Analog Devices is believed to be accurate and
reliable. However, no responsibility is assumed by Analog Devices for its
use, nor for any infringements of patents or other rights of third parties that
may result from its use. No license is granted by implication or otherwise
under any patent or patent rights of Analog Devices. Trademarks and
registered trademarks are the property of their respective owners.
Lead Temperature Range (Soldering, 60 sec) . . . . . . . . 300∞C
ORDERING GUIDE
TemperaturePackagePackage
ModelRangeDescriptionOption
OP191GS–40ⴗC to +125ⴗC8-Lead SOICR-8
OP191GS-REEL–40ⴗC to +125ⴗC8-Lead SOICR-8
OP191GS-REEL7–40ⴗC to +125ⴗC8-Lead SOICR-8
OP291GS–40ⴗC to +125ⴗC8-Lead SOICR-8
OP291GS-REEL–40ⴗC to +125ⴗC8-Lead SOICR-8
OP291GS-REEL7–40ⴗC to +125ⴗC8-Lead SOICR-8
OP291GSZ
OP291GSZ-REEL
OP291GSZ-REEL7
*
*
*
–40ⴗC to +125ⴗC8-Lead SOICR-8
–40ⴗC to +125ⴗC8-Lead SOICR-8
–40ⴗC to +125ⴗC8-Lead SOICR-8
OP491GP–40ⴗC to +125ⴗC14-Lead PDIPN-14
OP491GS–40ⴗC to +125ⴗC14-Lead SOICR-14
OP491GS-REEL–40ⴗC to +125ⴗC14-Lead SOICR-14
OP491GS-REEL7–40ⴗC to +125ⴗC14-Lead SOICR-14
OP491GSZ
OP491GSZ-REEL
OP491GSZ-REEL7
*
*
*
–40ⴗC to +125ⴗC14-Lead SOICR-14
–40ⴗC to +125ⴗC14-Lead SOICR-14
–40ⴗC to +125ⴗC14-Lead SOICR-14
OP491GRU-REEL–40ⴗC to +125ⴗC14-Lead TSSOPRU-14
OP491GBCDIE form
Stresses above those listed under Absolute Maximum Ratings may cause perma-
nent damage to the device. This is a stress rating only and functional operation of
the device at these or any other conditions above those indicated in the operational
section of this specification is not implied. Exposure to absolute maximum rating
conditions for extended periods may affect device reliability.
2
Absolute maximum ratings apply to both DICE and packaged parts, unless
otherwise noted.
3
qJA is specified for the worst-case conditions; i.e., q
for PDIP packages; q
and SOIC packages.
is specified for device soldered in circuit board for TSSOP
ESD (electrostatic discharge) sensitive device. Electrostatic charges as high as 4000 V readily
accumulate on the human body and test equipment and can discharge without detection. Although the
WARNING!
OP191/OP291/OP491 features proprietary ESD protection circuitry, permanent damage may occur
on devices subjected to high energy electrostatic discharges. Therefore, proper ESD precautions are
recommended to avoid performance degradation or loss of functionality.
TPC 2. OP291 Input Offset Voltage
Drift Distribution, VS = 3 V
0
–0.2
VS = 3V
–0.4
–0.6
–0.8
–1.0
–1.2
–1.4
INPUT OFFSET CURRENT (nA)
–1.6
12525–4085
–1.8
VS = 3V
–40ⴗC < T
BASED ON 600 OP AMPS
1400
VCM = 0.1V
VCM = 2.9V
TEMPERATURE (ⴗC)
VCM = 3V
< +125ⴗC
A
VCM = 0V
85
7
64325
12525–40
TPC 3. Input Offset Voltage vs.
Temperature, V
36
30
VS = 3V
24
18
12
6
0
–6
–12
–18
–24
INPUT BIAS CURRENT (nA)
–30
–36
0.30
0
INPUT COMMON-MODE VOLTAGE (V)
= 3 V
S
2.72.42.11.81.51.20.900.60
3.0
TPC 4. Input Bias Current vs.
Temperature, V
3.00
2.95
2.90
2.85
2.80
OUTPUT VOLTAGE SWING (V)
VS = 3V
2.75
–40
= 3 V
S
+VO @ RL = 100k⍀
+VO @ RL = 2k⍀
25
TEMPERATURE (ⴗC)
TPC 7. Output Voltage Swing vs.
Temperature, VS = 3 V
TPC 5. Input Offset Current vs.
Temperature, VS = 3 V
160
140
120
100
80
60
40
20
OPEN-LOOP GAIN (dB)
0
–20
85
125
–40
100
1k10k100k1M10M
FREQUENCY (Hz)
VS =3V
= 25ⴗC
T
A
0
45
90
135
180
225
270
TPC 8. Open-Loop Gain and Phase
vs. Frequency, VS = 3 V
TPC 6. Input Bias Current vs. Input
Common-Mode Voltage, VS = 3 V
1200
RL = 100k⍀,
= 2.9V
V
1000
800
600
400
PHASE SHIFT (ⴗC)
OPEN-LOOP GAIN (V/mV)
200
0
CM
RL = 100k⍀,
= 0.1V
V
CM
VS = 3V, VO = 0.3V/2.7V
TEMPERATURE (ⴗC)
85
TPC 9. Open-Loop Gain vs.
Temperature, VS = 3 V
12525–40
–6–
REV. C
OP191/OP291/OP491
50
40
30
20
10
0
–10
–20
–30
CLOSED-LOOP GAIN (dB)
–40
–50
1010010M1M100k10k1k
FREQUENCY (Hz)
VS = 3V
= 25ⴗC
T
A
TPC 10. Closed-Loop Gain vs.
Frequency, V
160
140
120
100
80
60
40
PSRR (dB)
20
0
–20
–40
100
1k10k100k1M10M
= 3 V
S
ⴙPSRR
–PSRR
FREQUENCY (Hz)
ⴞPSRR
= 3V
V
S
= 25ⴗC
T
A
160
140
120
100
80
60
40
CMRR (dB)
20
0
–20
–40
100
1k10k100k1M10M
FREQUENCY (Hz)
CMRR
=3V
V
S
= 25ⴗC
T
A
TPC 11. CMRR vs. Frequency,
V
= 3 V
S
113
112
111
110
PSRR (dB)
109
108
107
–40
25
TEMPERATURE (ⴗC)
VS = 3V
85
125
90
VS = 3V
89
88
87
CMRR (dB)
86
85
84
–40
25
TEMPERATURE (ⴗC)
85
125
TPC 12. CMRR vs. Temperature,
= 3 V
V
S
1.6
VS = 3V
1.4
1.2
1.0
0.8
0.6
SLEW RATE (V/s)
0.4
0.2
0
TEMPERATURE (ⴗC)
ⴙSR
–SR
25–40
85
125
TPC 13. PSRR vs. Frequency,
= 3 V
V
S
0.35
VS = 3V
0.30
0.25
0.20
0.15
0.10
SUPPLY CURRENT/AMPLIFIER (mA)
0.05
–40
25
TEMPERATURE (ⴗC)
85
TPC 16. Supply Current vs.
Temperature, V
= +3 V, +5 V, ±5 V
S
125
TPC 14. PSRR vs. Temperature,
VS = 3 V
2.8
2.6
2.4
2.2
2.0
1.8
1.6
1.4
MAXIMUM OUTPUT SWING (V)
1.2
1.0
0.50.1
FREQUENCY (kHz)
VIN = 2.8V p-p
V
= 3V
S
= 1
A
V
R
= 100k⍀
L
300
250200150100705030101.0
TPC 17. Maximum Output Swing vs.
Frequency, VS = 3 V
TPC 15. Slew Rate vs.
Temperature, VS = 3 V
MKR: 36.2 nV/冪Hz
100
90
10
0%
MKR:
0 Hz
1000 Hz
BW:
2.5kHz
15.0 Hz
TPC 18. Voltage Noise Density,
= +3 V to ±5 V, AVO = 1000
V
S
REV. C
–7–
OP191/OP291/OP491
70
VS = 5V
= 25ⴗC
T
A
60
BASED ON 600
OP AMPS
50
40
UNITS
30
20
10
0
–0.50
INPUT OFFSET VOLTAGE (mV)
0.300.10–0.10–0.30
0.50
TPC 19. OP291 Input Offset Voltage
Distribution, VS = 5 V
40
30
20
10
(nA)
B
I
–10
–20
–30
–40
= 5V
V
S
VCM = 5V
0
V
= 0V
CM
25–40
TEMPERATURE (ⴗC)
+I
B
–I
B
–I
B
+I
B
85
125
TPC 22. Input Bias Current vs.
Temperature, VS = 5 V
120
100
80
60
UNITS
40
20
0
1.0
0
INPUT OFFSET VOLTAGE (V/ⴗC)
VS = 5V
C < TA < +125ⴗC
–40
BASED ON 600 OP AMPS
6.05.04.03.02.0
TPC 20. OP291 Input Offset
Voltage Drift Distribution, VS = 5 V
1.6
1.4
1.2
1.0
0.8
0.6
0.4
0.2
INPUT OFFSET CURRENT (nA)
0
–0.2
VCM = 0V
VCM = 5V
25–40
TEMPERATURE (ⴗC)
VS = 5V
85
TPC 23. Input Offset Current vs.
Temperature, VS = 5 V
125
7.0
0.15
0.10
0.05
(mV)
OS
V
–0.05
–0.10
0
–40
VCM = 0V
V
CM
25
TEMPERATURE (ⴗC)
= 5V
85
VS = 5V
125
TPC 21. Input Offset Voltage vs.
Temperature, VS = 5 V
36
30
VS = 5V
24
18
12
6
0
–6
–12
–18
INPUT BIAS CURRENT (nA)
–24
–30
–36
0
COMMON MODE INPUT VOLTAGE (V)
5
4321
TPC 24. Input Bias Current vs.
Common-Mode Input Voltage, VS = 5 V
5.00
4.95
4.90
4.85
= 2k⍀
R
4.80
OUTPUT VOLTAGE SWING (V)
4.75
VS = 5V
4.70
–40
L
25
TEMPERATURE (ⴗC)
RL = 100k⍀
85
TPC 25. Output Voltage Swing vs.
Temperature, VS = 5 V
125
160
140
120
100
80
60
40
20
OPEN-LOOP GAIN (dB)
0
–20
–40
100
1k10k100k1M10M
FREQUENCY (Hz)
VS = 5V
= 25ⴗC
T
A
0
45
90
135
180
225
270
TPC 26. Open-Loop Gain and Phase
vs. Frequency, V
= 5 V
S
140
120
RL = 100k⍀, VCM = 5V
100
80
60
40
PHASE SHIFT (ⴗC)
OPEN-LOOP GAIN (V/mV)
20
0
–40
RL = 2k⍀, VCM = 5V
RL = 2k⍀, VCM = 0V
RL = 100k⍀, VCM = 0V
25
TEMPERATURE (ⴗC)
TPC 27. Open-Loop Gain vs.
Temperature, V
= 5 V
S
VS = 5V
85
125
–8–
REV. C
OP191/OP291/OP491
50
40
30
20
10
0
–10
–20
–30
CLOSED-LOOP GAIN (dB)
–40
–50
1010010M1M100k10k1k
FREQUENCY (Hz)
VS = 5V
= 25ⴗC
T
A
TPC 28. Closed-Loop Gain vs.
Frequency, V
160
140
120
100
80
60
40
PSRR (dB)
20
0
–20
–40
100
= 5 V
S
ⴞPSRR
= 5V
V
S
= 25ⴗC
T
A
+PSRR
–PSRR
1k10k100k1M10M
FREQUENCY (Hz)
TPC 31. PSRR vs. Frequency,
VS = 5 V
160
140
120
100
80
60
40
CMRR (dB)
20
0
–20
–40
100
1k10k100k1M10M
FREQUENCY (Hz)
CMRR
= 5V
V
S
= 25ⴗC
T
A
TPC 29. CMRR vs. Frequency,
V
= 5 V
S
0.6
0.5
0.4
+SR
0.3
SR (V/s)
0.2
0.1
0
–40
–SR
25
TEMPERATURE (ⴗC)
85
VS = 5V
TPC 32. OP291 Slew Rate vs.
Temperature, VS = 5 V
125
96
VS = 5V
95
94
93
92
91
CMRR (dB)
90
89
88
87
86
–40
25
TEMPERATURE (ⴗC)
85
125
TPC 30. CMRR vs. Temperature,
VS = 5 V
0.50
VS = 5V
0.45
SR (V/s)
0.40
0.35
0.30
0.25
0.20
0.15
0.10
0.05
0
–40
+SR
–SR
25
TEMPERATURE (ⴗC)
85
TPC 33. OP491 Slew Rate vs.
Temperature, VS = 5 V
125
20
18
16
14
+ISC, VS = +3V
12
10
8
6
SHORT-CIRCUIT CURRENT (mA)
4
+ISC, VS = ⴞ5V
–ISC, VS = ⴞ5V
–ISC, VS = +3V
25–40
TEMPERATURE (ⴗC)
85
125
TPC 34. Short-Circuit Current vs.
Temperature, VS = +3 V, +5 V,±5V
80
70
60
50
40
30
VOLTAGE (V)
20
10
0
V
= 10V p-p @ 1kHz
IN
0
A
10k⍀
FREQUENCY (Hz)
10k⍀
VS = ⴞ5V
1k⍀
B
200015001000500
TPC 35. Channel Separation,
=±5 V
V
S
V
O
2500
5.0
4.5
4.0
3.5
3.0
2.5
2.0
1.5
1.0
MAXIMUM OUTPUT SWING (V)
0.5
0
0.5
0.1
FREQUENCY (kHz)
VIN = 4.8V p-p
VS = 5V
= 1
A
V
= 100k⍀
R
L
4 PARTS
250100 15050 7020030101.0
TPC 36. Maximum Output Swing
vs. Frequency, VS = 5 V
300
REV. C
–9–
OP191/OP291/OP491
5.00
–5.00
125
–4.85
–4.95
25
–4.90
–40
0
–4.80
–4.75
4.75
4.80
4.85
4.95
4.90
85
OUTPUT VOLTAGE SWING (V)
TEMPERATURE (ⴗC)
V
S
= ⴞ5V
RL = 100k⍀
R
L
= 2k⍀
RL = 100k⍀
RL = 2k⍀
10
9
8
7
6
5
4
3
2
MAXIMUM OUTPUT SWING (V)
1
0
0.5
0.1
FREQUENCY (kHz)
VIN = +9.8V p-p
VS = ⴞ5V
AV = +1
RL = 100k⍀
4 PARTS
(nA)
B
I
–10
–20
–30
–40
–50
50
40
30
20
10
0
–40
VS = ⴞ5V
VCM = +5V
VCM = –5V
25
TEMPERATURE (ⴗC)
85
+I
B
–I
B
–I
B
+I
B
125
0.15
0.10
VCM = –5V
0.05
0
–0.05
INPUT OFFSET VOLTAGE (mV)
–0.10
300
250100 15050 7020030101.0
–40
VCM = +5V
25
TEMPERATURE (ⴗC)
VS = ⴞ5V
85
125
TPC 37. Maximum Output Swing vs.
Frequency, VS=±5V
1.6
VS = ⴞ5V
1.4
1.2
1.0
0.8
0.6
0.4
0.2
INPUT OFFSET CURRENT (nA)
0
–0.2
25–40
TEMPERATURE (ⴗC)
VCM = –5V
VCM = +5V
85
125
TPC 40. Input Offset Current vs.
Temperature, VS=±5V
70
60
50
40
30
20
10
0
OPEN-LOOP GAIN (dB)
–10
–20
–30
1k
10k10M1M100k
FREQUENCY (Hz)
VS = ⴞ5V
= 25ⴗC
T
A
0
45
90
135
180
225
270
TPC 38. Input Offset Voltage vs.
Temperature, V
36
VS = ⴞ5V
24
12
0
–12
INPUT BIAS CURRENT (nA)
–24
–36
COMMON-MODE INPUT VOLTAGE (V)
S
–1–2–3–4–5
=±5V
0
TPC 41. Input Bias Current vs.
Common-Mode Voltage, VS=±5V
200
180
160
140
120
100
80
65
40
OPEN-LOOP GAIN (V/mV)
PHASE SHIFT (ⴗC)
25
0
–40
RL = 100k⍀
RL = 2k⍀
25
TEMPERATURE (ⴗC)
85
VS = ⴞ5V
TPC 39. Input Bias Current vs.
Temperature, V
5
4321
= ±5 V
S
TPC 42. Output Voltage Swing vs.
Temperature, VS=±5V
125
50
40
30
20
10
0
–10
–20
–30
CLOSED-LOOP GAIN (dB)
–40
–50
1010010M1M100k10k1k
FREQUENCY (Hz)
V
S
T
A
= ⴞ5V
= 25ⴗC
TPC 43. Open-Loop Gain and Phase
vs. Frequency, V
= ±5 V
S
TPC 44. Open-Loop Gain vs.
Temperature, VS=±5V
–10–
TPC 45. Closed-Loop Gain vs.
Frequency, V
=±5V
S
REV. C
OP191/OP291/OP491
160
100
60
–40
1k10k100k1M10M
80
100
120
140
–20
0
20
40
+PSRR
–PSRR
ⴞPSRR
V
S
= ⴞ5V
T
A
= 25ⴗC
PSRR (dB)
FREQUENCY (Hz)
160
140
120
100
80
60
40
CMRR (dB)
20
0
–20
–40
100
1k10k100k1M10M
FREQUENCY (Hz)
CMRR
= ⴞ5V
V
S
= 25ⴗC
T
A
TPC 46. CMRR vs. Frequency,
VS=±5V
115
110
105
100
PSRR (dB)
95
90
–40
VS = ⴞ5V
OP291
25
TEMPERATURE (ⴗC)
OP491
85
TPC 49. OP291/OP491 PSRR vs.
Temperature, VS=±5V
125
102
VS = ⴞ5V
101
100
99
98
97
CMRR (dB)
96
95
94
93
92
–40
25
TEMPERATURE (ⴗC)
85
125
TPC 47. CMRR vs. Temperature,
VS=±5V
0.7
VS = ⴞ5V
0.6
0.5
0.4
s)
0.3
SR (V/
0.2
0.1
0
–40
+SR
–SR
25
TEMPERATURE (ⴗC)
85
125
TPC 50. Slew Rate vs. Temperature,
VS=±5V
TPC 48. PSRR vs. Frequency,
=±5V
V
S
1000
900
800
700
600
(⍀)
500
OUT
400
Z
300
200
100
0
1001k10M1M100k10k
A
= 10
VCL
FREQUENCY (Hz)
A
VCL
= 100
VS = 3V
TA = 25ⴗC
A
VCL
= 1
TPC 51. Output Impedance vs.
Frequency
100
90
INPUT
OUTPUT
10
0%
TPC 52. Large Signal Transient
Response, V
REV. C
1.00V
500mV
= 3 V
S
2.00s
VS = 3V
R
= 200k⍀
L
100mV
OUTPUT
–11–
2.00V
100
90
INPUT
VS = ⴞ5V
10
0%
R
A
2.00s
TPC 53. Large Signal Transient
Response, VS = ±5 V
= 200k⍀
L
= +1V/V
V
100mV1.00V
OP191/OP291/OP491
FUNCTIONAL DESCRIPTION
The OP191/OP291/OP491 are single-supply, micropower
amplifiers featuring rail-to-rail inputs and outputs. In order to
achieve wide input and output ranges, these amplifiers employ
unique input and output stages. As the simplified schematic
(Figure 2) shows, the input stage is comprised of two differential
pairs, a PNP pair and an NPN pair. These two stages do not
work in parallel. Instead, only one or the other stage is on for
any given input signal level. The PNP stage (transistors Q1 and
Q2) is required to ensure that the amplifier remains in the linear
region when the input voltage approaches and reaches the
negative rail. On the other hand, the NPN stage (transistors
Q5 and Q6) is needed for input voltages up to and including the
positive rail.
For the majority of the input common-mode range, the PNP
stage is active, as is evidenced by examining the graph of Input
Bias Current vs. Common-Mode Voltage. Notice that the bias
current switches direction at approximately 1.2 V to 1.3 V below
the positive rail. At voltages below this, the bias current flows
out of the OP291, indicating a PNP input stage. Above this
voltage, however, the bias current enters the device, revealing the
NPN stage. The actual mechanism within the amplifier for
switching between the input stages is comprised of the transistors
Q3, Q4, and Q7. As the input common-mode voltage increases,
the emitters of Q1 and Q2 follow that voltage plus a diode drop.
Eventually the emitters of Q1 and Q2 are high enough to turn
on Q3, which diverts the 8 mA of tail current away from the
PNP input stage, turning it off. Instead, the current is mirrored
through Q4 and Q7 to activate the NPN input stage.
Notice that the input stage includes 5 kW series resistors and
differential diodes, a common practice in bipolar amplifiers to
protect the input transistors from large differential voltages.
These diodes turn on whenever the differential voltage
exceeds approximately 0.6 V. In this condition, current flows
between the input pins, limited only by the two 5 kW resistors.
This characteristic is important in circuits where the amplifier
may be operated open-loop, such as a comparator. Evaluate
each circuit carefully to make sure that the increase in current
does not affect the performance.
The output stage of the OP191 family uses a PNP and an NPN
transistor as do most output stages; however, the output transistors, Q32 and Q33, are actually connected with their collectors to the output pin to achieve the rail-to-rail output swing. As
the output voltage approaches either the positive or negative
rail, these transistors begin to saturate. Thus, the final limit on
output voltage is the saturation voltage of these transistors,
which is about 50 mV. The output stage does have inherent gain
arising from the collectors and any external load impedance.
Because of this, the open-loop gain of the amplifier is dependent
on the load resistance.
Input Overvoltage Protection
As with any semiconductor device, whenever the condition
exists for the input to exceed either supply voltage, attention
needs to be paid to the input overvoltage characteristic. When
an overvoltage occurs, the amplifier could be damaged depending on the voltage level and the magnitude of the fault current.
Figure 3 shows the characteristics for the OP191 family. This
graph was generated with the power supplies at ground and a
curve tracer connected to the input. As can be seen, when the
input voltage exceeds either supply by more than 0.6 V, internal
PN junctions energize, allowing current to flow from the input
to the supplies. As described above, the OP291/OP491 does
have 5 kW resistors in series with each input, which helps limit
the current. Calculating the slope of the current versus voltage
in the graph confirms the 5 kW resistor.
+IN
5k⍀
Q1 Q2
8A
Q4
Q3
5k⍀
–IN
Q5
Q6
Q8
Q9
Q7
Q10
Q11
Q12
Q13Q15
Figure 2. Simplified Schematic
Q14
Q16
Q17
Q18Q19
Q20
Q21
Q22
Q25
Q23
Q24
Q27
Q28
Q26
Q29
Q30
Q31
10pF
Q32
Q33
V
OUT
–12–
REV. C
I
IN
2mA
1mA
–5V–10V10V5V
–1mA
–2mA
V
IN
Figure 3. Input Overvoltage Characteristics
This input current is not inherently damaging to the device as
long as it is limited to 5 mA or less. In the case shown, for an
input of 10 V over the supply, the current is limited to 1.8 mA.
If the voltage is large enough to cause more than 5 mA of current
to flow, then an external series resistor should be added. The size
of this resistor is calculated by dividing the maximum overvoltage
by 5 mA and subtracting the internal 5 kW resistor. For example,
if the input voltage could reach 100 V, the external resistor
should be (100 V/5 mA) – 5 k = 15 kW. This resistance should
be placed in series with either or both inputs if they are subjected
to the overvoltages. For more information on general overvoltage
characteristics of amplifiers, refer to the 1993 System ApplicationsGuide, available from the Analog Devices Literature Center.
Output Voltage Phase Reversal
Some operational amplifiers designed for single-supply operation exhibit an output voltage phase reversal when their inputs
are driven beyond their useful common-mode range. Typically
for single-supply bipolar op amps, the negative supply determines the lower limit of their common-mode range. With these
devices, external clamping diodes with the anode connected to
OP191/OP291/OP491
ground and the cathode to the inputs prevent input signal excursions from exceeding the device’s negative supply (i.e., GND),
preventing a condition that could cause the output voltage to
change phase. JFET input amplifiers may also exhibit phase
reversal, and, if so, a series input resistor is usually required to
prevent it.
The OP191 family is free from reasonable input voltage range
restrictions due to its novel input structure. In fact, the input
signal can exceed the supply voltage by a significant amount
without causing damage to the device. As illustrated in Figure 4,
the OP191 family can safely handle a 20 V p-p input signal on
± 5 V supplies without exhibiting any sign of output voltage
phase reversal or other anomalous behavior. Thus no external
clamping diodes are required.
Overdrive Recovery
The overdrive recovery time of an operational amplifier is the
time required for the output voltage to recover to its linear region
from a saturated condition. This recovery time is important in
applications where the amplifier must recover quickly after a
large transient event, such as a comparator. The circuit shown
in Figure 5 was used to evaluate the OP191 family’s overload
recovery time. The OP191 family takes approximately 8 ms to
recover from positive saturation and approximately 6.5 ms to
recover from negative saturation.
R1
9k⍀
V
IN
10V STEP
10k⍀
V
= ⴞ5V
S
Figure 5. Overdrive Recovery Time Test Circuit
3
1/2
1
OP291
2
R2
R3
10k⍀
V
OUT
20V p-p
REV. C
5s
+5V
V
IN
3
OP291
2
–5V
8
1/2
4
V
1
OUT
100
90
(2.5V/DIV)
IN
V
10
0%
TIME (200s/DIV)
100
90
(2V/DIV)
OUT
V
10
0%
20mV
TIME (200s/DIV)
5
20mV
s
Figure 4. Output Voltage Phase Reversal Behavior
–13–
OP191/OP291/OP491
APPLICATIONS
Single 3 V Supply, Instrumentation Amplifier
The OP291’s low supply current and low voltage operation make
it ideal for battery-powered applications, such as the instrumentation amplifier shown in Figure 6. The circuit uses the classic
two op amp instrumentation amplifier topology, with four resistors
to set the gain. The equation is simply that of a noninverting
amplifier as shown in the figure. The two resistors labeled R1
should be closely matched to each other as well as both resistors
labeled R2 to ensure good common-mode rejection performance.
Resistor networks ensure the closest matching as well as matched
drifts for good temperature stability. Capacitor C1 is included
to limit the bandwidth and, therefore, the noise in sensitive
applications. The value of this capacitor should be adjusted
depending on the desired closed-loop bandwidth of the instrumentation amplifier. The RC combination creates a pole at a
frequency equal to 1/(2p ¥ R1C1). If AC-CMRR is critical,
then a matched capacitor to C1 should be included across the
second resistor labeled R1.
3V
5
8
V
IN
3
1/2
1
OP291
R1R2R2
2
V
= (1 + ––– ) V
OUT
R1
IN
R2
OP291
6
1/2
4
R1
C1
100pF
V
7
OUT
Figure 6. Single 3 V Supply Instrumentation Amplifier
Because the OP291 accepts rail-to-rail inputs, the input commonmode range includes both ground and the positive supply of
3V. Furthermore, the rail-to-rail output range ensures the widest signal range possible and maximizes the dynamic range of
the system. Also, with its low supply current of 300 mA/device,
this circuit consumes a quiescent current of only 600 mA yet still
exhibits a gain bandwidth of 3 MHz.
A question may arise about other instrumentation amplifier
topologies for single-supply applications. For example, a variation
on this topology adds a fifth resistor between the two inverting
inputs of the op amps for gain setting. While that topology works
well in dual-supply applications, it is inherently inappropriate
for single-supply circuits. The same could be said for the traditional
three op amp instrumentation amplifier. In both cases, the circuits simply cannot work in single-supply situations unless a
false ground between the supplies is created.
Single-Supply RTD Amplifier
The circuit in Figure 7 uses three op amps of the OP491 to
develop a bridge configuration for an RTD amplifier that operates from a single 5 V supply. The circuit takes advantage of the
OP491’s wide output swing range to generate a high bridge
excitation voltage of 3.9 V. In fact, because of the rail-to-rail
output swing, this circuit works with supplies as low as 4.0 V.
Amplifier A1 servos the bridge to create a constant excitation
current in conjunction with the AD589, a 1.235 V precision
reference. The op amp maintains the reference voltage across
the parallel combination of the 6.19 kW and 2.55 MW resistors,
which generates a 200 mA current source. This current splits
evenly and flows through both halves of the bridge. Thus, 100 mA
flows through the RTD to generate an output voltage based on
its resistance. A 3-wire RTD is used to balance the line resistance in both 100 W legs of the bridge to improve accuracy.
100⍀
RTD
2.55M⍀
6.19k⍀
AD589
26.7k⍀
200⍀
10 TURNS
26.7k⍀
OP491
37.4k⍀
5V
100⍀
1/4
A1
1/4
OP491
365⍀365⍀
100k⍀
ALL RESISTORS 1% OR BETTER
A2
GAIN = 274
OP491
5V
1/4
100k⍀
0.01pF
A3
V
OUT
Figure 7. Single-Supply RTD Amplifier
Amplifiers A2 and A3 are configured in the two op amp IA
discussed above. Their resistors are chosen to produce a gain of
274, such that each 1∞C increase in temperature results in a
10 mV change in the output voltage, for ease of measurement.
A 0.01 mF capacitor is included in parallel with the 100 kW
resistor on amplifier A3 to filter out any unwanted noise from
this high gain circuit. This particular RC combination creates a
pole at 1.6 kHz.
–14–
REV. C
OP191/OP291/OP491
A 2.5 V Reference from a 3 V Supply
In many single-supply applications, the need for a 2.5 V reference
often arises. Many commercially available monolithic 2.5 V
references require a minimum operating supply voltage of 4 V.
The problem is exacerbated when the minimum operating system supply voltage is 3 V. The circuit illustrated in Figure 8 is
an example of a 2.5 V reference that operates from a single 3 V
supply. The circuit takes advantage of the OP291’s rail-to-rail
input and output voltage ranges to amplify an AD589’s 1.235 V
output to 2.5 V. The OP291’s low TCV
of 1 mV/∞C helps
OS
maintain an output voltage temperature coefficient of less than
200 ppm/∞C. The circuit’s overall temperature coefficient is
dominated by R2 and R3’s temperature coefficient. Lower temperature coefficient resistors are recommended. The entire
circuit draws less than 420 mA from a 3 V supply at 25∞C.
Figure 8. A 2.5 V Reference that Operates on a
Single 3 V Supply
5 V Only, 12-Bit DAC Swings Rail-to-Rail
The OP191 family is ideal for use with a CMOS DAC to generate
a digitally controlled voltage with a wide output range. Figure 9
shows the DAC8043 used in conjunction with the AD589 to
generate a voltage output from 0 V to 1.23 V. The DAC is operated in voltage switching mode, where the reference is connected
to the current output, I
the V
pin. This topology is inherently noninverting as opposed
REF
, and the output voltage is taken from
OUT
to the classic current output mode, which is inverting and, therefore, unsuitable for single supply.
5V
8
V
DD
DAC8043
I
OUT
GND CLK SR1
4765
V
DIGITAL
CONTROL
R
REF
LD
2
FB
1
5V
8
3
1/2
OP291
2
1
4
V
OUT
D
= –––– (5V)
4096
17.8k⍀
1.23V
AD589
R1
3
The OP291 serves two functions. First, it is required to buffer
the high output impedance of the DAC’s V
pin, which is on
REF
the order of 10 kW. The op amp provides a low impedance output
to drive any following circuitry. Second, the op amp amplifies
the output signal to provide a rail-to-rail output swing. In this
particular case, the gain is set to 4.1 to generate a 5.0 V output
when the DAC is at full scale. If other output voltage ranges are
needed, such as 0 V to 4.095 V, the gain can easily be adjusted
by altering the value of the resistors.
A High-Side Current Monitor
In the design of power supply control circuits, a great deal of
design effort is focused on ensuring a pass transistor’s long-term
reliability over a wide range of load current conditions. As a
result, monitoring and limiting device power dissipation is of
prime importance in these designs. The circuit illustrated in
Figure 10 is an example of a 5 V, single-supply, high-side
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. This design uses
an OP291’s rail-to-rail input voltage range to sense the voltage
drop across a 0.1 W current shunt. A p-channel MOSFET
used as the feedback element in the circuit converts the op
amp’s differential input voltage into a current. This current is
then applied to R2 to generate a voltage that is a linear representation of the load current. The transfer equation for the
current monitor is given by
Monitor Output = R2
Ê
¥
Á
Ë
R
SENSE
R1
ˆ
I
¥
L
˜
¯
For the element values shown, the monitor output’s transfer
characteristic is 2.5 V/A.
R
MONITOR
OUTPUT
5V
100⍀
3N163
2.49k⍀
M1
R2
SENSE
0.1⍀
R1
S
G
D
I
L
3
1/2
OP291
2
5V
5V
8
1
4
Figure 10. A High-Side Load Current Monitor
232⍀1%32.4k⍀
1%
R2
R3
R4
100k⍀
1%
Figure 9. 5 V Only, 12-Bit DAC Swings Rail-to-Rail
REV. C
–15–
OP191/OP291/OP491
A 3 V, Cold Junction Compensated Thermocouple Amplifier
The OP291’s low supply operation makes it ideal for 3 V batterypowered applications such as the thermocouple amplifier shown
in Figure 11. The K-type thermocouple terminates in an
isothermal block where the junctions’ ambient temperature is
continuously monitored using a simple 1N914 diode. The diode
corrects the thermal EMF generated in the junctions by feeding
a small voltage, scaled by the 1.5 MW and 475 W resistors, to
the op amp.
To calibrate this circuit, immerse the thermocouple measuring
junction in a 0∞C ice bath and adjust the 500 W potentiometer to
0V out. Next, immerse the thermocouple in a 250∞C temperature bath or oven and adjust the scale adjust potentiometer for
an output voltage of 2.50 V. Within this temperature range,
the K-type thermocouple is accurate to within ± 3∞C without
linearization.
1.235V
24.9k⍀
1%
2.1k⍀
1%
10k⍀
24.3k⍀
1%
4.99k⍀
500⍀
10 TURN
ZERO
ADJUST
1%
3.0V
2
OP291
3
SCALE
ADJUST
1.33M⍀ 20k⍀
8
1
0V = 0ⴗC
4
3V = 300ⴗC
V
OUT
ISOTHERMAL
BLOCK
ALUMEL
AL
CR
CHROMEL
K-TYPE
THERMOCOUPLE
40.7V/ⴗC
1N914
AD589
7.15k⍀
1.5M⍀
1%
COLD
JUNCTIONS
11.2mV
475⍀
1%
1%
Figure 11. A 3 V, Cold-Junction Compensated
Thermocouple Amplifier
Single-Supply, Direct Access Arrangement for Modems
An important building block in modems is the telephone line
interface. In the circuit shown in Figure 12, a direct access
arrangement is used for transmitting and receiving data from the
telephone line. Amplifier A1 is the receiving amplifier, and
amplifiers A2 and A3 are the transmitters. The fourth amplifier,
A4, generates a pseudo ground halfway between the supply
voltage and ground. This pseudo ground is needed for the
ac-coupled bipolar input signals.
The transmit signal, TXA, is inverted by A2 and then reinverted
by A3 to provide a differential drive to the transformer, where
each amplifier supplies half the drive signal. This is needed
because of the smaller swings associated with a single supply as
opposed to a dual supply. Amplifier A1 provides some gain for
the received signal, and it also removes the transmit signal present
at the transformer from the receive signal. To do this, the drive
signal from A2 is also fed to the noninverting input of A1 to
cancel the transmit signal from the transformer.
390pF
37.4k⍀
20k⍀, 1%
20k⍀, 1%
475⍀, 1%
0.033F
5.1V TO 6.2V
ZENER 5
100k⍀
10F0.1F
T1
1:1
RXA
TXA
0.1F
0.1F
20k⍀, 1%
14
0.0047F
10
9
750pF
6
5
1
A4
A1
1/4
OP491
3.3k⍀
1/4
OP491
37.4k⍀, 1%
20k⍀ 1%
20k⍀ 1%
1/4
OP491
4
1/4
OP491
11
13
12
A2
8
A3
7
3V OR 5V
2
3
100k⍀
Figure 12. Single-Supply Direct Access Arrangement
for Modems
The OP491’s bandwidth of 3 MHz and rail-to-rail output swings
ensure that it can provide the largest possible drive to the transformer at the frequency of transmission.
3 V, 50 Hz/60 Hz Active Notch Filter with False Ground
To process ac signals in a single-supply system, it is often best
to use a false-ground biasing scheme. A circuit that uses this
approach is illustrated in Figure 13. In this circuit, a false-ground
circuit biases an active notch filter used to reject 50 Hz/60 Hz
power line interference in portable patient monitoring equipment. Notch filters are quite commonly used to reject power
line frequency interference that often obscures low frequency
physiological signals, such as heart rates, blood pressure readings,
EEGs, and EKGs. This notch filter effectively squelches 60 Hz
pickup at a filter Q of 0.75. Substituting 3.16 kW resistors for
the 2.67 kW resistors in the twin-T section (R1 through R5)
configures the active filter to reject 50 Hz interference.
–16–
REV. C
OP191/OP291/OP491
R2
2.67k⍀
V
1F
IN
C4
2
3
R6
100k⍀
3V
R9
1M⍀
3V
11
1/4
OP491
4
R10
1M⍀
9
10
1
A1
R11
100k⍀
1/4
OP491
R1
2.67k⍀
(1Fⴛ2)
C5
0.01F
A3
R3
2.67k⍀
C3
2F
8
C1
1F
R12
499⍀
C2
1F
R4
2.67k⍀
R5
1.33k⍀
(2.67k⍀
C6
1.5V
1F
5
1/4
OP491
6
A2
2)
R8
1k⍀
R7
1k⍀
V
OUT
7
Figure 13. A 3 V Single-Supply, 50 Hz/60 Hz Active Notch
Filter with False Ground
Amplifier A3 is the heart of the false ground bias circuit. It
simply buffers the voltage developed by R9 and R10 and is the
reference for the active notch filter. Since the OP491 exhibits a
rail-to-rail input common-mode range, R9 and R10 are chosen
to split the 3 V supply symmetrically. An in-the-loop compensation scheme used around the OP491 allows the op amp to
drive C6, a 1 mF capacitor, without oscillation. C6 maintains a
low impedance ac ground over the operating frequency range of
the filter.
The filter section uses a pair of OP491s in a twin-T configuration whose frequency selectivity is very sensitive to the relative
matching of the capacitors and resistors in the twin-T section.
Mylar is the material of choice for the capacitors, and the relative matching of the capacitors and resistors determines the
filter’s pass-band symmetry. Using 1% resistors and 5% capacitors produces satisfactory results.
Single-Supply, Half-Wave and Full-Wave Rectifiers
An OP191 family configured as a voltage follower operating on
a single supply can be used as a simple half-wave rectifier in
low frequency (<2 kHz) applications. A full-wave rectifier can
be configured with a pair of OP291s as illustrated in Figure 14.
The circuit works in the following way. When the input signal is
above 0 V, the output of amplifier A1 follows the input signal.
Since the noninverting input of amplifier A2 is connected to
A1’s output, op amp loop control forces the A2’s inverting input
to the same potential. The result is that both terminals of R1 are
equipotential; i.e., no current flows. Since there is no current
flow in R1, the same condition exists upon R2; thus, the output
of the circuit tracks the input signal. When the input signal is
below 0 V, the output voltage of A1 is forced to 0 V. This condition now forces A2 to operate as an inverting voltage follower
because the noninverting terminal of A2 is at 0 V as well. The
output voltage at V
A is then a full-wave rectified version of
OUT
the input signal. If needed, a buffered, half-wave rectified version
of the input signal is available at V
R1
100k⍀
5V
V
IN
3
100
90
10
0%
OP291
2
1/2
1V
8
4
A1
500mV
1
500mV
TIME (200s/DIV)
2V p-p
<2kHz
(1V/DIV)
V
(0.5V/DIV)
V
(0.5V/DIV)
OUT
OUT
V
IN
B
A
OUT
6
OP291
5
B.
R2
100k⍀
1/2
200s
A2
V
A
OUT
7
FULL-WAVE
RECTIFIED
OUTPUT
V
B
OUT
HALF-WAVE
RECTIFIED
OUTPUT
Figure 14. Single-Supply, Half-Wave and Full-Wave
Rectifiers Using an OP291
REV. C
–17–
OP191/OP291/OP491
* OP491 SPICE Macro-modelREV. C, 5/94
*ARG/ADI
*
* Copyright 1994 by Analog Devices, Inc.
*
* Refer to “README.DOC” file for License Statement. Use of
* this model indicates your acceptance of the
terms and provisions in the License Statement.
*
* Node assignments
*noninverting input
*inverting input
*positive supply
*negative supply
*output
*
.SUBCKT OP491129950 45
*
* INPUT STAGE
*
I19978.06E-6
Q1647QP
Q2537QP
D1399DX
D2499DX
D334DX
D443DX
R1385E3
R2425E3
R35506.4654E3
R46506.4654E3
EOS 81POLY(1) (16,39) –0.08E-3 1
IOS 3450E-12
GB1 398(21,98) 50E-9
GB2 498(21,98) 50E-9
CIN 121E-12
*
* 1ST GAIN STAGE
*
EREF 980(39,0)1
G1989(6,5)31.667E-6
R79981E6
EC1 9910POLY(1) (99,39) –0.52 1
EC2 1150POLY(1) (39,50) –0.52 1
D5910DX
D6119DX
*
* 2ND GAIN STAGE AND DOMINANT POLE AT 1.25 Hz
*
G29812(9,39)8E-6
R81298276.311E6
C2129816E-12
D71213DX
D81412DX
V199130.58
V214500.58
*
* COMMON-MODE STAGE
*
ECM 1598POLY(2) (1,39) (2,39) 0 0.5 0.5
R915161E6
CONTROLLING DIMENSIONS ARE IN INCHES; MILLIMETER DIMENSIONS
(IN PARENTHESES) ARE ROUNDED-OFF INCH EQUIVALENTS FOR
REFERENCE ONLY AND ARE NOT APPROPRIATE FOR USE IN DESIGN
COMPLIANT TO JEDEC STANDARDS MO-095-AB
4.50
4.40
4.30
14
8
71
6.40
BSC
PIN 1
5.10
5.00
4.90
0.65
BSC
SEATING
PLANE
0.15
0.05
0.30
0.19
1.20
MAX
1.05
1.00
0.80
0.20
0.09
8ⴗ
0ⴗ
0.75
0.60
0.45
COMPLIANT TO JEDEC STANDARDS MO-153AB-1
COPLANARITY
0.10
OP191/OP291/OP491
8-Lead Standard Small Outline Package [SOIC]
Narrow Body
[S-Suffix]
(R-8)
Dimensions shown in millimeters and (inches)
5.00 (0.1968)
4.80 (0.1890)
4.00 (0.1574)
3.80 (0.1497)
0.25 (0.0098)
0.10 (0.0040)
COPLANARITY
0.10
CONTROLLING DIMENSIONS ARE IN MILLIMETERS; INCH DIMENSIONS
(IN PARENTHESES) ARE ROUNDED-OFF MILLIMETER EQUIVALENTS FOR
REFERENCE ONLY AND ARE NOT APPROPRIATE FOR USE IN DESIGN
85
1.27 (0.0500)
SEATING
PLANE
COMPLIANT TO JEDEC STANDARDS MS-012AA
BSC
6.20 (0.2440)
5.80 (0.2284)
41
1.75 (0.0688)
1.35 (0.0532)
0.51 (0.0201)
0.31 (0.0122)
0.25 (0.0098)
0.17 (0.0067)
0.50 (0.0196)
0.25 (0.0099)
8ⴗ
0ⴗ
1.27 (0.0500)
0.40 (0.0157)
14-Lead Standard Small Outline Package [SOIC]
Narrow Body
[S-Suffix]
(R-14)
Dimensions shown in millimeters and (inches)
14-Lead Plastic Dual In-Line Package [PDIP]
[P-Suffix]
(N-14)
Dimensions shown in inches and (millimeters)
ⴛ 45ⴗ
14-Lead Thin Shrink Small Outline Package [TSSOP]
(RU-14)
Dimensions shown in millimeters
8.75 (0.3445)
8.55 (0.3366)
8
6.20 (0.2441)
7
5.80 (0.2283)
1.75 (0.0689)
1.35 (0.0531)
SEATING
PLANE
0.25 (0.0098)
0.17 (0.0067)
4.00 (0.1575)
3.80 (0.1496)
0.25 (0.0098)
0.10 (0.0039)
COPLANARITY
CONTROLLING DIMENSIONS ARE IN MILLIMETERS; INCH DIMENSIONS
(IN PARENTHESES) ARE ROUNDED-OFF MILLIMETER EQUIVALENTS FOR
REFERENCE ONLY AND ARE NOT APPROPRIATE FOR USE IN DESIGN