FEATURES
Low Offset Voltage: 50 V max
Low Offset Voltage Drift: 0.5 V/ⴗC max
Very Low Bias Current
25ⴗC: 100 pA max
–55ⴗC to +125ⴗC: 450 pA max
Very High Open-Loop Gain: 2000 V/mV min
Low Supply Current (per Amplifier): 625 A max
Operates from ⴞ2 V to ⴞ20 V Supplies
High Common-Mode Rejection: 120 dB min
APPLICATIONS
Strain Gage and Bridge Amplifiers
High Stability Thermocouple Amplifiers
Instrumentation Amplifiers
Photo-Current Monitors
High Gain Linearity Amplifiers
Long-Term Integrators/Filters
Sample-and-Hold Amplifiers
Peak Detectors
Logarithmic Amplifiers
Battery-Powered Systems
Quad Operational Amplifier
OP497
PIN CONNECTIONS
16-Lead Wide Body SOIC
(S-Suffix)
OUT D
1
OUT A
–IN A
2
+
–
3
+IN A
V+
4
OP497
5
+IN B
–IN B
OUT B
NC
–
+
6
7
8
NC = NO CONNECT
14-Lead Plastic Dip
(P-Suffix)
14-Lead Ceramic Dip
(Y-Suffix)
16
–IN D
15
+
–
+IN D
14
V–
13
+IN C
12
–
+
11
10
9
–IN C
OUT C
NC
GENERAL DESCRIPTION
The OP497 is a quad op amp with precision performance in the
space-saving, industry standard 16-lead SOlC package. Its combination of exceptional precision with low power and extremely
low input bias current makes the quad OP497 useful in a wide
variety of applications.
Precision performance of the OP497 includes very low offset,
under 50 µV, and low drift, below 0.5 µV/°C. Open-loop gain
exceeds 2000 V/mV ensuring high linearity in every application.
Errors due to common-mode signals are eliminated by the OP497’s
common-mode rejection of over 120 dB. The OP497’s power
supply rejection of over 120 dB minimizes offset voltage changes
experienced in battery-powered systems. Supply current of the
OP497 is under 625 µA per amplifier, and it can operate with
supply voltages as low as ±2 V.
The OP497 utilizes a superbeta input stage with bias current cancellation to maintain picoamp bias currents at all temperatures.
This is in contrast to FET input op amps whose bias currents start
in the picoamp range at 25°C, but double for every 10°C rise in
temperature, to reach the nanoamp range above 85°C. Input bias
current of the OP497 is under 100 pA at 25°C and is under 450
pA over the military temperature range.
Combining precision, low power, and low bias current, the
OP497 is ideal for a number of applications, including instrumentation amplifiers, log amplifiers, photo-diode preamplifiers,
and long-term integrators. For a single device, see the OP97; for a
dual device, see the OP297.
OUT A
1
–IN A
2
+–+
+IN A
V+
+IN B
–IN B
OUT B
1000
100
INPUT CURRENT – PA
10
–75–50–250255075100125
–
3
4
OP497
5
–
+–+
6
7
TEMPERATURE – C
OUT D
14
–IN D
13
+IN D
12
V–
11
+IN C
10
–IN C
9
OUT C
8
VS = ⴞ15V
V
CM
–I
B
+I
B
I
OS
Input Bias, Offset Current vs. Temperature
= 0V
REV. D
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.
Absolute Maximum Ratings apply to both DICE and packaged parts, unless
otherwise noted.
2
For supply voltages less than ± 20 V, the absolute maximum input voltage is
equal to the supply voltage.
3
HIA is specified for worst-case mounting conditions, i.e., JA is specified for
device in socket for cerdip, P-DIP packages; JA is specified for device soldered
to printed circuit board for SOIC package.
ORDERING GUIDE
TemperaturePackagePackage
ModelRangeDescriptionOption
OP497AY* –55°C to +125°C 14-Lead CerdipQ-14
OP497CY* –55°C to +125°C 14-Lead CerdipQ-14
OP497FP–40°C to +85°C14-Lead Plastic DIP N-14
OP497FS–40°C to +85°C16-Lead SOICR-16
OP497GP–40°C to +85°C14-Lead Plastic DIP N-14
OP497GS–40°C to +85°C16-Lead SOICR-16
*Not for new design; obsolete April 2002.
For a military processed devices, please refer to the Standard
Microcircuit Drawing (SMD) available at www.dscc.dla.mil/
programs.milspec./default.asp.
SMD Part NumberADI Part Number
5962–9452101M2A*OP497BRC
5962–9452101MCAOP497BY
*Not for new designs; obsolete April 2002.
DICE CHARACTERISTICS
–
1/4
OP497
+
CHANNEL SEPARATION = 20 log
V
20V p–p @ 10Hz
1
2k⍀
50⍀
V
1
()
V /10000
2
50k⍀
–
1/4
OP497
+
V
2
Channel Separation Test Circuit
CAUTION
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 OP497 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.
REV. D
–3–
OP497
–Typical Performance Characteristics
(25ⴗC, Vs = 15 V, unless otherwise noted.)
50
40
30
20
PERCENTAGE OF UNITS
10
0
–80
–100
–20–40–60
INPUT OFFSET VOLTAGE – V
TA = 25ⴗC
= 15V
V
S
V
CM
0
TPC 1. Typical Distribution of
Input Offset Voltage
50
40
30
20
PERCENTAGE OF UNITS
10
0
0
0.1
TCVOS – V/ⴗC
VS = ⴞ15V
V
TPC 4. Typical Distribution of
TCV
OS
CM
= 0V
= 0V
50
40
30
20
PERCENTAGE OF UNITS
10
100
80604020
0
–80
–100
INPUT BIAS CURRENT – pA
–20–40–60
TA = 25ⴗC
= 15V
V
S
= 0V
V
CM
0
100
80604020
TPC 2. Typical Distribution of
Input Bias Current
1000
VS = ⴞ15V
= 0V
V
CM
100
–I
INPUT CURRENT – pA
10
0.8
0.70.60.50.40.30.2
–75 –50 –25 025 50 75 100 125
B
+I
I
OS
TEMPERATURE – ⴗC
B
TPC 5. Input Bias, Offset
Current vs. Temperature
60
TA = 25ⴗC
50
40
30
20
PERCENTAGE OF UNITS
10
0
0
10
INPUT OFFSET CURRENT – pA
V
S
V
CM
TPC 3. Typical Distribution of
Input Offset Current
70
TA = 25 C
= ⴞ15V
V
S
60
50
40
30
20
INPUT BIAS CURRENT – pA
10
0
–10
–15
COMMON-MODE VOLTAGE – Volts
0
–5
TPC 6. Input Bias Current vs.
Common-Mode Voltage
= 15V
= 0V
50403020
105
60
–I
B
+I
B
15
ⴞ3
ⴞ2
ⴞ1
DEVIATION FROM FINAL VALUE – V
0
0
TIME AFTER POWER APPLIED – Minutes
TA = 25ⴗC
V
V
TPC 7. Input Offset Voltage
Warm-Up Drift
= ⴞ15V
S
= 0V
CM
10000
BALANCED OR UNBALANCED
= 15V
V
S
= 0V
V
CM
1000
100
–55 C T 125 C
A
EFFECTIVE OFFSET VOLTAGE – V
10
10
51
432
100
SOURCE RESISTANCE – ⍀
10k
1k
T = +25 C
100k
A
1M
10M
TPC 8. Effective Offset Voltage
vs. Source Resistance
–4–
100
BALANCED OR UNBALANCED
= 15V
V
S
= 0V
V
CM
10
1
EFFECTIVE OFFSET VOLTAGE – V/ ⴗC
0.1
1001k10k 100k
SOURCE RESISTANCE – ⍀
TPC 9. Effective TCVOS vs.
Source Resistance
1M10M
100M
REV. D
OP497
1000
TA = 25ⴗC
= 2V TO 20V
V
S
100
CURRENT NOISE
VOLTAGE NOISE
10
VOLTAGE NOISE DENSITY – nV/ Hz
1
110100
FREQUENCY – Hz
TPC 10. Voltage Noise Density
vs. Frequency
100
80
GAIN
60
PHASE
40
20
0
OPEN-LOOP GAIN – dB
–20
–40
100
1k
FREQUENCY – Hz
TPC 13. Open-Loop Gain,
Phase vs. Frequency
VS = ⴞ15V
= 30pF
C
L
R
= 1M⍀
L
= 25ⴗC
T
A
1M100k10k
1000
10M
90
135
180
225
10
TA = 25ⴗC
= ⴞ2V TO ⴞ20V
V
S
1
10Hz
0.1
CURRENT NOISE DENSITY – fA / Hz
TOTAL NOISE DENSITY – V/ Hz
0.01
2
10
10310410510610
SOURCE RESISTANCE – ⍀
TPC 11. Total Noise Density vs.
1kHz
NOISE VOLTAGE – 100mV/DIV
7
TPC 12. 0.1 Hz to 10 Hz Noise Voltage
5mV
100
90
10
0%
02 4 6810
TIME – Secs
1s
VS = 15V
T
= 25ⴗC
A
Source Resistance
PHASE SHIFT – DEG
10000
1000
OPEN - LOOP GAIN – V/ MV
100
11020
TA = –55ⴗC
TA = +125ⴗC
VS = ⴞ15V
= ⴞ10V
V
O
LOAD RESISTANCE – k⍀
TA = +25C
TPC 14. Open-Loop Gain vs.
RL = 2k⍀
= ⴞ15V
V
S
= ⴞ10V
V
CN
TA= +125ⴗC
TA= +25ⴗC
T
= –55ⴗC
A
DIFFERENTIAL INPUT VOLTAGE – 10V/ DIV
OUTPUT VOLTAGE – V
15–10–151050–5
TPC 15. Open-Loop Gain Linearity
Load Resistance
COMMON - MODE REJECTION – dB
160
140
120
100
80
60
40
20
0
101
FREQUENCY – Hz
VS = ⴞ15V
T
TPC 16. Common-Mode
Rejection vs. Frequency
REV. D
= 25ⴗC
A
100k10k1k100
1M
POWER SUPPLY REJECTION – dB
160
140
120
100
–PSR
80
60
40
20
0
+PSR
101
FREQUENCY – Hz
VS = ⴞ15V
= 25ⴗC
T
A
TPC 17. Power Supply
Rejection vs. Frequency
–5–
35
30
25
p-p
20
15
10
OUTPUT SWING – V
5
1M
100k10k1k100
0
100
1k
FREQUENCY – Hz
10k
V
= ⴞ15V
S
= 25ⴗC
T
A
A
VCL
1%THD
= 10k⍀
R
L
= +1
100k
TPC 18. Maximum Output
Swing vs. Frequency
OP497
+V
S
–0.5
–1.0
–1.5
1.5
1.0
0.5
(REFERRED TO SUPPLY VOLTAGES)
INPUT COMMON-MODE VOLTAGE – Volts
–V
S
0
ⴞ5
SUPPLY VOLTAGE – V
TA = 25ⴗC
ⴞ15ⴞ10
ⴞ20
TPC 19. Input Common-Mode
Voltage Range vs. Supply Voltage
700
+125 C
600
+25
500
400
300
SUPPLY CURRENT (PER AMPLIFIER) – A
200
C
–55
C
ⴞ5
0
ⴞ10
SUPPLY VOLTAGE – V
NO LOAD
ⴞ15
ⴞ20
TPC 22. Supply Current
(per Amplifier) vs. Supply Voltage
35
VS = ⴞ15V
= 25ⴗC
T
A
30
= +1
A
VCL
1%THD
f
= 1kHz
25
p-p
O
20
15
10
OUTPUT SWING – V
5
0
10
100
LOAD RESISTANCE – ⍀
1k
TPC 20. Maximum Output Swing
vs. Load Resistance
1000
VS = 15V
= 25 C
T
A
100
10
0.1
0.01
0.001
1
10
1
AV = +1
10k1k100
TPC 23. Closed-Loop Output
Impedance vs. Frequency
10k
100k
+V
S
–0.5
–1.0
–1.5
1.5
1.0
OUTPUT VOLTAGE SWING – V
0.5
(REFERRED TO SUPPLY VOLTAGES)
–V
S
0
ⴞ5
ⴞ10
SUPPLY VOLTAGE – V
TA = 25ⴗC
= 10k⍀
R
L
ⴞ15
TPC 21. Output Voltage Swing vs.
Supply Voltage
35
30
25
20
15
VS = ⴞ15V
OUTPUT SHORTED
TO GROUND
SHORT CIRCUIT CURRENT – mA
–15
–20
–25
–30
–35
TA = +125 C
0
1
TIME FROM OUTPUT SHORT – Mins
= –55 C
T
A
TA = +25 C
TA = +125 C
= +25 C
T
A
TA = –55 C
2
3
TPC 24. Short-Circuit Current vs.
Time Temperature
ⴞ20
4
70
VS = ⴞ15V
= 25 C
T
A
60
= +1
A
VCL
= 100mV p–p
V
OUT
50
40
30
OVERSHOOT – %
20
10
0
10
100
LOAD CAPACITANCE – pF
1k
TPC 25. Small-Signal Overshoot
vs. Capacitance Load
10k
–IN
+IN
2.5k⍀
2.5k⍀
TPC 26. Simplified Schematic Showing One Amplifier
V+
V
OUT
V–
–6–
REV. D
APPLICATIONS INFORMATION
1/4
OP497
UNITY GAIN FOLLOWERNONINVERTING AMPLIFIER
INVERTING AMPLIFIER
B
8
A
1
MINI-DIP
BOTTOM VIEW
–
+
–
+
–
+
1/4
OP497
1/4
OP497
Extremely low bias current over the full military temperature range
makes the OP497 attractive for use in sample-and-hold amplifiers,
peak detectors, and log amplifiers that must operate over a wide
temperature range. Balancing input resistances is not necessary
with the OP497. Offset voltage and TCV
are degraded only
OS
minimally by high source resistance, even when unbalanced.
The input pins of the OP497 are protected against large differential voltage by back-to-back diodes and current-limiting resistors.
Common-mode voltages at the inputs are not restricted, and may
vary over the full range of the supply voltages used.
The OP497 requires very little operating headroom about the
supply rails, and is specified for operation with supplies as low
as ±2 V. Typically, the common-mode range extends to within
1 V of either rail. The output typically swings to within 1 V of
the rails when using a 10 kΩ load.
AC PERFORMANCE
The OP497’s ac characteristics are highly stable over its full
operating temperature range. Unity-gain small-signal response is
shown in Figure 1. Extremely tolerant of capacitive loading on
the output, the OP497 displays excellent response even with
1000 pF loads (Figure 2).
100
90
OP497
100
90
10
0%
50
2V
Figure 3. Large-Signal Transient Response (A
GUARDING AND SHIELDING
To maintain the extremely high input impedances of the OP497,
care must be taken in circuit board layout and manufacturing.
Board surfaces must be kept scrupulously clean and free of moisture. Conformal coating is recommended to provide a humidity
barrier. Even a clean PC board can have 100 pA of leakage currents
between adjacent traces, so guard rings should be used around
the inputs. Guard traces are operated at a voltage close to that
on the inputs, as shown in Figure 4, so that leakage currents
become minimal. In noninverting applications, the guard ring
should be connected to the common-mode voltage at the inverting input. In inverting applications, both inputs remain at ground,
so the guard trace should be grounded. Guard traces should be
on both sides of the circuit board.
s
= 1)
VCL
10
0%
20mV
Figure 1. Small-Signal Transient Response
(C
= 100 pF, A
LOAD
100
90
10
0%
20MV
Figure 2. Small-Signal Transient Response
(C
REV. D
= 1000 pF, A
LOAD
VCL
= 1)
VCL
5
= 1)
5s
Figure 4. Guard Ring Layout and Connections
s
–7–
OP497
OPEN-LOOP GAIN LINEARITY
The OP497 has both an extremely high gain of 2000 V/mv minimum and constant gain linearity. This enhances the precision of
the OP497 and provides for very high accuracy in high closed-loop
gain applications. Figure 5 illustrates the typical open-loop gain
linearity of the OP 497 over the military temperature range.
RL = 10k⍀
= ⴞ15V
V
S
= 0V
V
CM
DIFFERENTIAL INPUT VOLTAGE – 10µV/ DIV
T
= +125 C
A
= +25C
T
A
= –55 C
T
A
OUTPUT VOLTAGE – Volts
15–10–151050–5
Figure 5. Open-Loop Linearity of the OP497
APPLICATIONS
Precision Absolute Value Amplifier
The circuit of Figure 6 is a precision absolute value amplifier
with an input impedance of 30 MΩ. The high gain and low
TCV
of the OP497 ensure accurate operation with microvolt
OS
input signals. In this circuit, the input always appears as a common-mode signal to the op amps. The CMR of the OP497
exceeds 120 dB, yielding an error of less than 2 ppm.
+15V
PRECISION CURRENT PUMP
Maximum output current of the precision current pump shown
in Figure 7 is ±10 mA. Voltage compliance is ±10 V with ±15 V
supplies. Output impedance of the current transmitter exceeds
3 MΩ with linearity better than 16 bits.
R3
2
3
R4
10k⍀
10k⍀
1/4
OP497
7
1
+15V
8
1/4
OP497
–15V
4
R5
10k⍀
I
OUT
ⴞ10mA
5
6
R1
10k⍀
–
R2
V
IN
10k⍀
+
V
V
IN
I
OUT
IN
= = = 10mA/ V
R5
100⍀
Figure 7. Precision Current Pump
PRECISION POSITIVE PEAK DETECTOR
In Figure 8, the CH must be of polystyrene, Teflon*, or polyethylene to minimize dielectric absorption and leakage. The droop
rate is determined by the size of CH and the bias current of the
OP497.
1k⍀
+15V
2
1/4
OP497
1k⍀
V
IN
3
1
RESET
1N4148
C
H
1k⍀
2N930
1k⍀
6
OP497
5
1/4
4
–15V
0.1F
8
0.1F
7
V
OUT
C2
0.1F
C1
30pF
8
2
1/4
–15V
4
C3
0.1F
1
OP497
3
V
IN
1k⍀
D1
1N4148
D2
1N4148
R1
R2
2k⍀
6
5
R3
1k⍀
1/4
OP497
0V < V < 10V
Figure 6. Precision Absolute Value Amplifier
*Teflon is a registered trademark of the Dupont Company.
Figure 8. Precision Positive Peak Detector
SIMPLE BRIDGE CONDITIONING AMPLIFIER
7
OUT
Figure 9 shows a simple bridge conditioning amplifier using
the OP497. The transfer function is:
VV
=
OUTREF
RRRR
∆
R
+
F
∆
The REF43 provides an accurate and stable reference voltage
for the bridge. To maintain the highest circuit accuracy, R
F
should be 0.1% or better with a low temperature coefficient.
–8–
REV. D
+5V
1
2
3
6
7
5
C1
100pF
V+
2
3
8
1
4
V–
V
IN
I
IN
C2
100pF
6
5
7
V
OUT
I
O
9
8
10
Q1
Q3
Q2
14
12
Q4
13
–15V
I
REF
MAT-04E
R1
133k⍀
R2
33k⍀
R3
50k⍀
R4
50k⍀
1/4
OP497
1/4
OP497
1
2
3
6
7
5
C1
100pF
V+
2
3
8
1
4
V–
6
5
7
V
OUT
I
O
9
8
10
Q1
Q3
Q2
14
12
Q4
13
–15V
I
REF
MAT-04E
I
IN
V
IN
R1
33k⍀
R2
33k⍀
R5
2k⍀
R3
50k⍀
R4
50k⍀
C2
100pF
1/4
OP497
1/4
OP497
2
REF43
4
V
REF
2.5 V
6
R
R
R + ⌬R
R
+5V
6
8
1/4
OP497
5
7
4
–5V
V
2
3
OUT
R
1/4
OP497
= V
F
1
( )
REF
R + ⌬R
⌬R
V
OUT
R
F
R
Figure 9. A Simple Bridge Conditioning Amplifier Using
the OP497
OP497
NONLINEAR CIRCUITS
Due to its low input bias currents, the OP497 is an ideal log
amplifier in nonlinear circuits such as the square and square
root circuits shown in Figures 10 and 11. Using the squaring
circuit of Figure 10 as an example, the analysis begins by writing a
voltage-loop equation across transistors Q1, Q2, Q3, and Q4.
VIn
T
1
I
IN
+
I
S
1
VIn
T
2
I
IN
I
S
=
2
VInI
T
3
I
O
+
I
S
3
VIn
T
4
I
REF
I
S
4
All the transistors of the MAT04 are precisely matched and at
the same temperature, so the I
2InIInIInIIn II
=+= ×
INOREFOREF
and VT terms cancel, giving:
S
()
Exponentiating both sides of thick equation leads to:
2
I
()
I
IN
=
O
I
REF
Op amp A2 forms a current-to-voltage converter which gives
V
= R2 × IO. Substituting (VIN/R1) for IIN and the above
OUT
equation for I
, yields:
O
V
OUT
R2
=
I
REF
2
V
IN
R1
Figure 10. Squaring Amplifier
A similar analysis made for the square-root circuit of Figure 11
leads to its transfer function:
VI
()( )
INREF
R1
In these circuits, I
VR2
=
OUT
is a function of the negative power sup-
REF
ply. To maintain accuracy, the negative supply should be well
regulated. For applications where very high accuracy is required,
a voltage reference may be used to set I
. An important con-
REF
sideration for the squaring circuit is that a sufficiently large
input voltage can force the output beyond the operating range
of the output op amp. Resistor R4 can be changed to scale I
REF
,
or Rl and R2 can be varied to keep the output voltage within
the usable range.
REV. D
Unadjusted accuracy of the square-root circuit is better than
0.1% over an input voltage range of 100 mV to 10 V. For a
similar input voltage range, the accuracy of the squaring circuit
is better than 0.5%.
–9–
Figure 11. Square-Root Amplifier
OP497
OP497 SPICE MACRO-MODEL
Figure 12 and Table I show the node and net list for a SPICE
macro-model of the OP497. The model is a simplified version of
the actual device and simulates important dc parameters such as
, IOS, IB, AVO, CMR, VO, and ISY. AC parameters such as slew
V
OS
rate, gain and phase response, and CMR change with frequency
are also simulated by the model.
–IN
+IN
2
1
R
IN2
C
IN
R
IN1
1516
ECM
ⴞ
I
OS
CCM
RCM1
RCM2
8
7
ENZ
R1
D1D2
R2
– +
E
OS
CNZ
RNZ1
1718
ⴞ
RNZ2
9
G2
The model uses typical parameters for the OP497. The poles and
zeros in the model were determined from the actual open and
closed-loop gain and phase response of the OP497. In this way,
the model presents an accurate ac representation of the actual
device. The model assumes an ambient temperature of 25°C.
99
ⴞ
V1
R3R4
C2
56
Q1 Q2
1011
R6R5
I
1
50
19
R10
C5
G1
98
ⴞ
E
REF
G2
13
D3
12
C3
R7
D4
14
ⴞ
V2
20
C5
R15
98
99
25 26
G4G5
D8D7
D5
23
24
D6
D10
50
V3
– +
V4
G6
R18
– +
22
G7
R19
L1
V
O
27
R16
I
SY
20
21
R17
D9
Figure 12. OP497 Macro Model
–10–
REV. D
Table I. OP497 SPICE Net-List
OP497
* Node assignments
*noninverting input
*inverting input
*positive supply
*negative supply
*output
*
*SUBCKT OP497 129950 27
*
* INPUT STAGE AND POLE AT 6 MHz
*