Analog Devices AD625SD, AD625SCHIPS, AD625KN, AD625CD, AD625BD Datasheet

FUNCTIONAL BLOCK DIAGRAM

+

–

+

–

+

–

+

–

+

–

50

50

10k

10k

10k

10k

V

B

–INPUT

–GAIN

SENSE

+INPUT

–GAIN
DRIVE

+GAIN

SENSE

+GAIN
DRIVE

SENSE

OUTPUT

REFERENCE

AD625

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
which may result from its use. No license is granted by implication or
otherwise under any patent or patent rights of Analog Devices.

a

Programmable Gain

Instrumentation Amplifier

AD625

One Technology Way, P.O. Box 9106, Norwood, MA 02062-9106, U.S.A.
Tel: [phone] World Wide Web Site: http://www.analog.com
Fax: [phone] © Analog Devices, Inc., 2000

FEATURES
User Programmed Gains of 1 to 10,000
Low Gain Error: 0.02% Max
Low Gain TC: 5 ppm/C Max
Low Nonlinearity: 0.001% Max
Low Offset Voltage: 25 V
Low Noise 4 nV/√Hz (at 1 kHz) RTI
Gain Bandwidth Product: 25 MHz
16-Lead Ceramic or Plastic DIP Package,

20-Terminal LCC Package
Standard Military Drawing Available
MlL-Standard Parts Available
Low Cost

PRODUCT DESCRIPTION

The AD625 is a precision instrumentation amplifier specifically
designed to fulfill two major areas of application: 1) Circuits re­quiring nonstandard gains (i.e., gains not easily achievable with
devices such as the AD524 and AD624). 2) Circuits requiring a
low cost, precision software programmable gain amplifier.

For low noise, high CMRR, and low drift the AD625JN is the
most cost effective instrumentation amplifier solution available.
An additional three resistors allow the user to set any gain from
1 to 10,000. The error contribution of the AD625JN is less than

0.05% gain error and under 5 ppm/°C gain TC; performance
limitations are primarily determined by the external resistors.
Common-mode rejection is independent of the feedback resistor
matching.

A software programmable gain amplifier (SPGA) can be config­ured with the addition of a CMOS multiplexer (or other switch
network), and a suitable resistor network. Because the ON
resistance of the switches is removed from the signal path, an
AD625 based SPGA will deliver 12-bit precision, and can be
programmed for any set of gains between 1 and 10,000, with
completely user selected gain steps.

For the highest precision the AD625C offers an input offset
voltage drift of less than 0.25 µV/°C, output offset drift below
15 µV/°C, and a maximum nonlinearity of 0.001% at G = 1. All
grades exhibit excellent ac performance; a 25 MHz gain band­width product, 5 V/µs slew rate and 15 µs settling time.

The AD625 is available in three accuracy grades (A, B, C) for
industrial (–40°C to +85°C) temperature range, two grades (J,
K) for commercial (0°C to +70°C) temperature range, and one
(S) grade rated over the extended (–55°C to +125°C) tempera­ture range.

PRODUCT HIGHLIGHTS

1. The AD625 affords up to 16-bit precision for user selected
fixed gains from 1 to 10,000. Any gain in this range can be
programmed by 3 external resistors.

2. A 12-bit software programmable gain amplifier can be config­ured using the AD625, a CMOS multiplexer and a resistor
network. Unlike previous instrumentation amplifier designs,
the ON resistance of a CMOS switch does not affect the gain
accuracy.

3. The gain accuracy and gain temperature coefficient of the
amplifier circuit are primarily dependent on the user selected
external resistors.

4. The AD625 provides totally independent input and output
offset nulling terminals for high precision applications. This
minimizes the effects of offset voltage in gain-ranging
applications.

5. The proprietary design of the AD625 provides input voltage
noise of 4 nV/√Hz at 1 kHz.

6. External resistor matching is not required to maintain high
common-mode rejection.

AD625A/J/S AD625B/K AD625C

Model Min Typ Max Min Typ Max Min Typ Max Unit

GAIN

Gain Equation

2 R

F

R

G

+ 1

2 R

F

R

G

+ 1

2 R

F

R

G

+ 1

Gain Range 1 10,000 1 10,000 1 110,000
Gain Error

1

±.0350.05 ±0.020.03 ±0.010.02 %

Nonlinearity, Gain = 1-256 ±0.005 ± 0.002 ±0.001 %

Gain>256 ±0.01 ±0.008 ±0.005 %

Gain vs. Temp. Gain<1000

1

5 5 5 ppm/°C

GAIN SENSE INPUT

Gain Sense Current 300 500 150 250 50 100 nA

vs. Temperature 5 20 2 15 2 10 nA/°C

Gain Sense Offset Current 150 500 75 250 50 100 nA

vs. Temperature 2 15 1 10 2 10 nA/°C

VOLTAGE OFFSET (May be Nulled)

Input Offset Voltage 50 200 25 50 10 25 µV

vs. Temperature 1 2/2 0.25 0.50/1 0.1 0.25 µV/°C

Output Offset Voltage 4 5 2 3 1 2 mV

vs. Temperature 20 50/50 10 25/40 10 15 µV/°C

Offset Referred to the

Input vs. Supply

G = 1 70 75 75 85 80 90 dB
G = 10 85 95 90 100 95 105 dB
G = 100 95 100 105 110 110 120 dB
G = 1000 100 110 110 120 115 140 dB

INPUT CURRENT

Input Bias Current ±30



50 ±20



25 ±10



15 nA

vs. Temperature ±50 ±50 ± 50 pA/°C

Input Offset Current ±2



35 ±1



15 ±1



5 nA

vs. Temperature ±20 ±20 ± 20 pA/°C

INPUT

Input Impedance

Differential Resistance 1 1 1 GΩ
Differential Capacitance 4 4 4 pF
Common-Mode Resistance 1 1 1 GΩ
Common-Mode Capacitance 4 4 4 pF

Input Voltage Range

Differ. Input Linear (V

DL

)

2

±10 ±10 ± 10 V

Common-Mode Linear (V

CM

)

12 V –

G

2

×V

D

(

)

12 V –

G

2

×V

D

(

)

12 V –

G

2

×V

D

(

)

Common-Mode Rejection Ratio dc to

60 Hz with 1 kΩ Source Imbalance

G = 1 70 75 75 85 80 90 dB
G = 10 90 95 90 105 100 115 dB
G = 100 100 105 105 115 110 125 dB
G = 1000 110 115 110 125 120 140 dB

OUTPUT RATING ± 10 V ±10 V ±10 V

@ 5 mA @ 5 mA @ 5 mA

DYNAMIC RESPONSE

Small Signal –3 dB

G = 1 (RF = 20 kΩ) 650 650 650 kHz
G = 10 400 400 400 kHz
G = 100 150 150 150 kHz
G = 1000 25 25 25 kHz

Slew Rate 5.0 5.0 5.0 V/µs
Settling Time to 0.01%, 20 V Step

G = 1 to 200 15 15 15 µs
G = 500 35 35 35 µs
G = 1000 75 75 75 µs

AD625–SPECIFICATIONS

(typical @ VS = 15 V, RL = 2 k and TA = + 25C, unless otherwise noted)

REV. D

–2–

AD625

AD625A/J/S AD625B/K AD625C

Model Min Typ Max Min Typ Max Min Typ Max Unit

NOISE

Voltage Noise, 1 kHz

R.T.I. 4 4 4 nV/√Hz
R.T.O. 75 75 75 nV/√Hz

R.T.I., 0.1 Hz to 10 Hz

G = 1 10 10 10 µV p-p
G = 10 1.0 1.0 1.0 µV p-p
G = 100 0.3 0.3 0.3 µV p-p
G = 1000 0.2 0.2 0.2 µV p-p

Current Noise

0.1 Hz to 10 Hz 60 60 60 pA p-p

SENSE INPUT

R

IN

10 10 10 kΩ

I

IN

30 30 30 µA
Voltage Range ± 10 ± 10 ±10 V
Gain to Output 1 ± 0.01 1 ± 0.01 1 ± 0.01 %

REFERENCE INPUT

R

IN

20 20 20 kΩ
I

IN

30 30 30 µA
Voltage Range ± 10 ± 10 ±10 V
Gain to Output 1 ± 0.01 1 ± 0.01 1 ± 0.01 %

TEMPERATURE RANGE

Specified Performance

J/K Grades 0 +70 0 +70 °C
A/B/C Grades –40 +85 –40 +85 –40 +85 °C
S Grade –55 +125 °C

Storage –65 +150 –65 +150 –65 +150 °C

POWER SUPPLY

Power Supply Range ±6 to ± 18 ±6 to ±18 ± 6 to ± 18 V
Quiescent Current 3.5 5 3.5 5 3.5 5 mA

NOTES

1

Gain Error and Gain TC are for the AD625 only. Resistor Network errors will add to the specified errors.

2

VDL is the maximum differential input voltage at G = 1 for specified nonlinearity. VDL at other gains = 10 V/G. VD = actual differential input voltage.
Example: G = 10, VD = 0.50; VCM = 12 V – (10/2 × 0.50 V) = 9.5 V.

Specifications subject to change without notice.
All min and max specifications are guaranteed. Specifications shown in boldface are tested on all production units at final electrical test. Results from those tests are

used to calculate outgoing quality levels.

REV. D

–3–

AD625

REV. D–4–

PIN CONNECTIONS

Ceramic DIP (D) and Plastic DIP (N) Packages

TOP VIEW

(Not to Scale)

NC = NO CONNECT

+INPUT –INPUT

AD625

+GAIN SENSE –GAIN SENSE

RTI NULL RTO NULL

RTI NULL RTO NULL

+GAIN DRIVE

–GAIN DRIVE

NC SENSE

REFERENCE V

OUT

–V

S

+V

S

10k 10k+V

S

–V

S

1

2

3

4

5

6

7

8

16

15

14

13

12

11

10

9

Leadless Chip Carrier (E) Package

20 19123

18

14

15

16

17

4

5

6

7

8

910111213

TOP VIEW

(Not to Scale)

AD625

RTI NULL

RTI NULL

NC

+GAIN DRIVE

NC

RTO NULL

RTO NULL

NC

–GAIN NULL

SENSE

NC = NO CONNECT

+INPUT

REFERENCE

–V

S

NC

+V

S

NC

+GAIN SENSE

–GAIN SENSE

V

OUT

–INPUT

ABSOLUTE MAXIMUM RATINGS*

Supply Voltage . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . ± 18 V

Internal Power Dissipation . . . . . . . . . . . . . . . . . . . . . . 450 mW

Input Voltage . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . ±V

S

Differential Input Voltage . . . . . . . . . . . . . . . . . . . . . . . . . ±V

S

Output Short Circuit Duration . . . . . . . . . . . . . . . . Indefinite

Storage Temperature Range (D, E) . . . . . . . . –65°C to +150°C

Storage Temperature Range (N) . . . . . . . . . . –65°C to +125°C

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 AD625 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.

WARNING!

ESD SENSITIVE DEVICE

ORDERING GUIDE

Model Temperature Range Package Description Package Option

AD625AD –40°C to +85°C 16-Lead Ceramic DIP D-16
AD625BD –40°C to +85°C 16-Lead Ceramic DIP D-16
AD625BD/+ –40°C to +85°C 16-Lead Ceramic DIP D-16
AD625CD –40°C to +85°C 16-Lead Ceramic DIP D-16
AD625SD –55°C to +125°C 16-Lead Ceramic DIP D-16
AD625SD/883B –55°C to +125°C 16-Lead Ceramic DIP D-16
AD625SE/883B –55°C to +125°C 20-Terminal Leadless Chip Carrier E-20A
AD625JN 0°C to +70°C 16-Lead Plastic DIP N-16
AD625KN 0°C to +70°C 16-Lead Plastic DIP N-16
AD625ACHIPS –40°C to +85°CDie
AD625SCHIPS –55°C to +125°CDie
5962-87719012A* –55°C to +125°C 20-Terminal Leadless Chip Carrier E-20A
5962-8771901EA* –55°C to +125°C 16-Lead Ceramic DIP D-16

*Standard Military Drawing Available

Operating Temperature Range

AD625J/K . . . . . . . . . . . . . . . . . . . . . . . . . . . . 0°C to +70°C

AD625A/B/C . . . . . . . . . . . . . . . . . . . . . . . . –40°C to +85°C

AD625S . . . . . . . . . . . . . . . . . . . . . . . . . . . –55°C to +125°C

Lead Temperature Range (Soldering 10 sec) . . . . . . . . +300°C

*Stresses above those listed under Absolute Maximum Ratings may cause perma-

nent damage to the device. This is a stress rating only; 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.

SUPPLY VOLTAGE – V

INPUT VOLTAGE RANGE – V

20

0

15

10

5

0

5101520

25C

Figure 1. Input Voltage Range vs.
Supply Voltage, G = 1

FREQUENCY – Hz

CMRR – dM

–160

0

10 100 1k 10k 100k 10M

–140

–120

–100

–80

–60

–40

–20

0

G = 1000

G = 100

G = 10

G = 1

Figure 4. CMRR vs. Frequency
RTI, Zero to 1 k

Ω

Source Imbal-

ance

WARM-UP TIME – Minutes

V

OS

FROM FINAL VALUE – V

–1

0

0

1

2

3

4

5

6

7

1.0 2.0 3.0 4.0 5.0 6.0 7.0 8.0

Figure 7. Offset Voltage, RTI, Turn
On Drift

SUPPLY VOLTAGE – V

OUTPUT VOLTAGE SWING – V

20

0

15

10

5

0

5101520

Figure 2. Output Voltage Swing
vs. Supply Voltage

FREQUENCY – Hz

FULL POWER RESPONSE – V p-p

30

1k

20

10

0

10k 100k 1M

G = 500

G = 1, 100

G = 1000

G = 100

BANDWIDTH

LIMITED

Figure 5. Large Signal Frequency
Response

FREQUENCY – Hz

POWER SUPPLY REJECTION – dB

160

10

140

120

100

80

60

40

20

0

100 1k 10k 100k

–VS = –15V dc+

1V p-p SINEWAVE

G = 500

G = 100

G = 1

Figure 8. Negative PSRR vs.
Frequency

LOAD RESISTANCE – 

OUTPUT VOLTAGE SWING – V p-p

30

10

20

10

0

100 1k 10k

Figure 3. Output Voltage Swing
vs. Load Resistance

FREQUENCY – Hz

GAIN

100

1000

100

10

1

1k 10k 100k 1M 10M

Figure 6. Gain vs. Frequency

FREQUENCY – Hz

POWER SUPPLY REJECTION – dB

160

10

140

120

100

80

60

40

20

0

100 1k 10k 100k

+VS = +15V dc+

1V p-p SINEWAVE

G = 500

G = 100

G = 1

Figure 9. Positive PSRR vs.
Frequency

Typical Performance Characteristics–A

D625

REV. D

–5–

AD625

REV. D–6–

TEMPERATURE – C

INPUT CURRENT – nA

40

–125

30

20

10

0

–10

–20

–30

–40

–75 –25 25 75 125

Figure 10. Input Bias Current vs.
Temperature

SUPPLY VOLTAGE – V

AMPLIFIER QUIESCENT CURRENT – A

8.0

0

6.0

4.0

2.0

0

5101520

Figure 13. Quiescent Current vs.
Supply Voltage

Figure 16. Low Frequency Voltage
Noise, G = 1 (System Gain = 1000)

+V

S

–V

S

AD625

10V

V

OUT

Figure 11. Overrange and Gain
Switching Test Circuit (G = 8, G = 1)

FREQUENCY – Hz

VOLT NSD – nV/ Hz

1

1000

100

10

1

0.1
10 100 1k 10k 100k

G = 1

G = 10

G = 100, 1000

G = 1000

Figure 14. RTI Noise Spectral
Density vs. Gain

+V

S

–V

S

AD625

DUT

–V

S

1/2

+V

S

1/2

AD712

1F

1F

1F

16.2k

100

G = 1000

G = 1, 10, 100

1k

1.62M

9.09k

1.82k

16.2k

AD712

Figure 17. Noise Test Circuit

Figure 12. Gain Overrange Recovery

FREQUENCY – Hz

CURRENT NOISE SPECTRAL DENSITY – fA/ Hz

100k

1

10k

1k

100

10

10 100 1k 10k 100k

Figure 15. Input Current Noise

Figure 18. Low Frequency Voltage
Noise, G = 1000 (System
Gain = 100,000)

AD625

REV. D

–7–

Figure 19. Large Signal Pulse
Response and Settling Time, G = 1

Figure 22. Large Signal Pulse
Response and Settling Time, G = 10

SETTLING TIME – S

–12 TO 12

0

10 20 30 40 50 60 70

–8 TO 8

–4 TO 4

OUTPUT

STEP – V

4 TO –4

8 TO –8

12 TO –12

G = 1

G = 100

G = 1000

G = 1000

G = 100

G = 1

Figure 20. Settling Time to 0.01%

+V

S

–V

S

AD625

200

0.1%

500

0.1%

1k

0.1%

INPUT

20V p-p

100k

0.1%

10k1%1k

10T

10k

1%

V

OUT

Figure 23. Settling Time Test Circuit

Figure 21. Large Signal Pulse
Response and Settling Time, G = 100

Figure 24. Large Signal Pulse
Response and Settling Time,
G = 1000

AD625

REV. D–8–

THEORY OF OPERATION

The AD625 is a monolithic instrumentation amplifier based on
a modification of the classic three-op-amp approach. Monolithic
construction and laser-wafer-trimming allow the tight matching
and tracking of circuit components. This insures the high level
of performance inherent in this circuit architecture.

A preamp section (Q1–Q4) provides additional gain to A1 and
A2. Feedback from the outputs of A1 and A2 forces the collec­tor currents of Q1–Q4 to be constant, thereby, impressing the
input voltage across R

G

. This creates a differential voltage at the

outputs of A1 and A2 which is given by the gain (2R

F/RG

+ 1)
times the differential portion of the input voltage. The unity
gain subtracter, A3, removes any common-mode signal from the
output voltage yielding a single ended output, V

OUT

, referred to

the potential at the reference pin.

The value of R

G

is the determining factor of the transconduc-

tance of the input preamp stage. As R

G

is reduced for larger
gains the transconductance increases. This has three important
advantages. First, this approach allows the circuit to achieve a
very high open-loop gain of (3 × 10

8

at programmed gains ≥ 500)

thus reducing gain related errors. Second, the gain-bandwidth
product, which is determined by C3, C4, and the input trans­conductance, increases with gain, thereby, optimizing frequency
response. Third, the input voltage noise is reduced to a value
determined by the collector current of the input transistors
(4 nV/√Hz).

INPUT PROTECTION

Differential input amplifiers frequently encounter input voltages
outside of their linear range of operation. There are two consid­erations when applying input protection for the AD625; 1) that
continuous input current must be limited to less than 10 mA
and 2) that input voltages must not exceed either supply by
more than one diode drop (approximately 0.6 V @ 25°C).

Under differential overload conditions there is (R

G

+ 100) Ω in

series with two diode drops (approximately 1.2 V) between the
plus and minus inputs, in either direction. With no external protec­tion and R

G

very small (i.e., 40 Ω), the maximum overload

voltage the AD625 can withstand, continuously, is approximately
±2.5 V. Figure 26a shows the external components necessary to
protect the AD625 under all overload conditions at any gain.

V

B

+

–

GAIN

DRIVE

GAIN
DRIVE

R

FRF

R

G

50A50A

C3

C4

A1 A2

10k

10k

50

GAIN

SENSE

GAIN

SENSE

Q1, Q3 Q2, Q4

50

50A50A

10k

10k

–IN

+V

S

–V

S

+IN

SENSE

V

O

REF

Figure 25. Simplified Circuit of the AD625

The diodes to the supplies are only necessary if input voltages
outside of the range of the supplies are encountered. In higher
gain applications where differential voltages are small, back-to­back Zener diodes and smaller resistors, as shown in Figure
26b, provides adequate protection. Figure 26c shows low cost
FETs with a maximum ON resistance of 300 Ω configured to offer
input protection with minimal degradation to noise, (5.2 nV/√Hz
compared to normal noise performance of 4 nV/√Hz).

During differential overload conditions, excess current will flow
through the gain sense lines (Pins 2 and 15). This will have no
effect in fixed gain applications. However, if the AD625 is being
used in an SPGA application with a CMOS multiplexer, this
current should be taken into consideration. The current capa­bilities of the multiplexer may be the limiting factor in allowable
overflow current. The ON resistance of the switch should be
included as part of R

G

when calculating the necessary input

protection resistance.

AD625

+V

S

–V

S

R

F

R

G

R

F

FD333

FD333

FD333

FD333

–IN

+IN

1.4k

1.4k

V

OUT

Figure 26a. Input Protection Circuit

AD625

+V

S

–V

S

R

F

R

G

R

F

FD333

FD333

FD333

–IN

+IN

500

V

OUT

FD333

1N5837A

1N5837A

500

Figure 26b. Input Protection Circuit for G > 5

AD625

+V

S

–V

S

R

F

R

G

R

F

FD333

–IN

+IN

V

OUT

FD333

FD333

FD333

2k

2N5952

2k

2N5952

Figure 26c. Input Protection Circuit

AD625

REV. D

–9–

Any resistors in series with the inputs of the AD625 will degrade
the noise performance. For this reason the circuit in Figure 26b
should be used if the gains are all greater than 5. For gains less
than 5, either the circuit in Figure 26a or in Figure 26c can be
used. The two 1.4 kΩ resistors in Figure 26a will degrade the
noise performance to:

4 kTR

ext

+(4 nV/ Hz )2= 7.9 nV / Hz

RESISTOR PROGRAMMABLE GAIN AMPLIFIER

In the resistor-programmed mode (Figure 27), only three exter­nal resistors are needed to select any gain from 1 to 10,000.
Depending on the application, discrete components or a
pretrimmed network can be used. The gain accuracy and gain
TC are primarily determined by the external resistors since the
AD625C contributes less than 0.02% to gain error and under
5 ppm/°C gain TC. The gain sense current is insensitive to
common-mode voltage, making the CMRR of the resistor pro­grammed AD625 independent of the match of the two feedback
resistors, R

F

.

Selecting Resistor Values

As previously stated each RF provides feedback to the input
stage and sets the unity gain transconductance. These feedback
resistors are provided by the user. The AD625 is tested and
specified with a value of 20 kΩ for R

F

. Since the magnitude of

RTO errors increases with increasing feedback resistance, values
much above 20 kΩ are not recommended (values below 10 kΩ
for R

F

may lead to instability). Refer to the graph of RTO noise,
offset, drift, and bandwidth (Figure 28) when selecting the
feedback resistors. The gain resistor (R

G

) is determined by the

formula R

G

= 2 RF/(G – l).

+GAIN

SENSE

–GAIN
SENSE

+INPUT –INPUT

RTI NULL

RTI NULL

RTO
NULL

RTO
NULL

+V

S

+GAIN DRIVE –GAIN DRIVE

R

F

R

G

R

F

NC

REF

–V

S

V

OUT

+V

S

G = +1

2R

F

R

G

A1 A2

AD625

10k

10k 10k

10k

A3

1

2

3

4

5

6

7

8

16

15

14

13

12

11

10

9

Figure 27. AD625 in Fixed Gain Configuration

A list of standard resistors which can be used to set some com­mon gains is shown in Table I.

For single gain applications, only one offset null adjust is neces­sary; in these cases the RTI null should be used.

RTO OFFSET VOLTAGE DRIFT

6

5

4

3

2

1

60k50k40k30k20k10k

MULTIPLYING FACTOR

BANDWIDTH

1M

100k

10k

1 10 100 1k

FREQUENCY – Hz

10k

20k

50k

FEEDBACK RESISTANCE –  FEEDBACK RESISTANCE – 

RTO NOISE RTO OFFSET VOLTAGE

300

200

100

3

2

10k 20k 30k 40k 50k 60k 10k 20k 30k 40k 50k 60k

VOLTAGE NOISE – nV Hz

MULTIPLYING FACTOR

FEEDBACK RESISTANCE –  FEEDBACK RESISTANCE – 

Figure 28. RTO Noise, Offset, Drift and Bandwidth vs.
Feedback Resistance Normalized to 20 k

Ω

Table I. Common Gains Nominally Within 0.5% Error
Using Standard 1% Resistors

GAIN R

F

R

G

1 20 kΩ∞
2 19.6 kΩ 39.2 kΩ

5 20 kΩ 10 kΩ
10 20 kΩ 4.42 kΩ
20 20 kΩ 2.1 kΩ
50 19.6 kΩ 806 Ω

100 20 kΩ 402 Ω
200 20.5 kΩ 205 Ω
500 19.6 kΩ 78.7 Ω

1000 19.6 kΩ 39.2 Ω

4 20 kΩ 13.3 kΩ

8 19.6 kΩ 5.62 kΩ
16 20 kΩ 2.67 kΩ
32 19.6 kΩ 1.27 kΩ
64 20 kΩ 634 Ω

128 20 kΩ 316 Ω
256 19.6 kΩ 154 Ω
512 19.6 kΩ 76.8 Ω

1024 19.6 kΩ 38.3 Ω

SENSE TERMINAL

The sense terminal is the feedback point for the AD625 output
amplifier. Normally it is connected directly to the output. If
heavy load currents are to be drawn through long leads, voltage
drops through lead resistance can cause errors. In these in­stances the sense terminal can be wired to the load thus putting

AD625

REV. D–10–

the I × R drops “inside the loop” and virtually eliminating this
error source.

Typically, IC instrumentation amplifiers are rated for a full ±10
volt output swing into 2 kΩ. In some applications, however, the
need exists to drive more current into heavier loads. Figure 29
shows how a high-current booster may be connected “inside the
loop” of an instrumentation amplifier. By using an external
power boosting circuit, the power dissipated by the AD625 will
remain low, thereby, minimizing the errors induced by self­heating. The effects of nonlinearities, offset and gain inaccura­cies of the buffer are reduced by the loop gain of the AD625’s
output amplifier.

AD625

+V

S

–V

S

R

F

R

G

R

F

VIN+

V

IN

–

R

I

SENSE

REFERENCE

X1

Figure 29. AD625 /Instrumentation Amplifier with Output
Current Booster

REFERENCE TERMINAL

The reference terminal may be used to offset the output by up
to ±10 V. This is useful when the load is “floating” or does not
share a ground with the rest of the system. It also provides a
direct means of injecting a precise offset. However, it must be
remembered that the total output swing is ±10 volts, from
ground, to be shared between signal and reference offset.

The AD625 reference terminal must be presented with nearly
zero impedance. Any significant resistance, including those
caused by PC layouts or other connection techniques, will in­crease the gain of the noninverting signal path, thereby, upset­ting the common-mode rejection of the in-amp. Inadvertent
thermocouple connections created in the sense and reference
lines should also be avoided as they will directly affect the out­put offset voltage and output offset voltage drift.

In the AD625 a reference source resistance will unbalance the
CMR trim by the ratio of 10 kΩ/R

REF

. For example, if the refer-

ence source impedance is 1 Ω, CMR will be reduced to 80 dB
(10 kΩ/1 Ω = 80 dB). An operational amplifier may be used to
provide the low impedance reference point as shown in Figure

30. The input offset voltage characteristics of that amplifier will
add directly to the output offset voltage performance of the
instrumentation amplifier.

The circuit of Figure 30 also shows a CMOS DAC operating in
the bipolar mode and connected to the reference terminal to
provide software controllable offset adjustments. The total offset
range is equal to ±(V

REF

/2 × R5/R4), however, to be symmetri-

cal about 0 V R3 = 2 × R4.

The offset per bit is equal to the total offset range divided by 2

N

,

where N = number of bits of the DAC. The range of offset for
Figure 30 is ±120 mV, and the offset is incremented in steps of

0.9375 mV/LSB.

AD625

+V

S

–V

S

V

OUT

SENSE

AD7502

A

0

A

1

E

N

GND VDDV

SS

+IN

–IN

1/2

AD712

1/2

AD712

REFERENCE

V

REF

AD589 1.2V

V

S

39k

MSB

LSB

DATA

INPUTS

CS

WR

+V

S

AD7524

8-BIT DAC

R

FB

C

1

OUT 1
OUT 2

+V

S

R4

10k

R3

20k

5k

–V

S

R5

2k

0.01F

Figure 30. Software Controllable Offset

An instrumentation amplifier can be turned into a voltage-to­current converter by taking advantage of the sense and reference
terminals as shown in Figure 31.

AD625

R

F

R

G

R

F

VIN+

V

IN

–

SENSE

I

L

AD711

LOAD

+VX–

R1

Figure 31. Voltage-to-Current Converter

By establishing a reference at the “low” side of a current setting
resistor, an output current may be defined as a function of input
voltage, gain and the value of that resistor. Since only a small
current is demanded at the input of the buffer amplifier A1, the
forced current I

L

will largely flow through the load. Offset and
drift specifications of A2 must be added to the output offset and
drift specifications of the In-Amp.

INPUT AND OUTPUT OFFSET VOLTAGE

Offset voltage specifications are often considered a figure of
merit for instrumentation amplifiers. While initial offset may be
adjusted to zero, shifts in offset voltage due to temperature
variations will cause errors. Intelligent systems can often correct
for this factor with an autozero cycle, but this requires extra
circuitry.

AD625

REV. D

–11–

Offset voltage and offset voltage drift each have two compo­nents: input and output. Input offset is that component of offset
that is generated at the input stage. Measured at the output it is
directly proportional to gain, i.e., input offset as measured at the
output at G = 100 is 100 times greater than that measured at
G = 1. Output offset is generated at the output and is constant
for all gains.

The input offset and drift are multiplied by the gain, while the
output terms are independent of gain, therefore, input errors
dominate at high gains and output errors dominate at low gains.
The output offset voltage (and drift) is normally specified at
G = 1 (where input effects are insignificant), while input offset
(and drift) is given at a high gain (where output effects are negli­gible). All input-related parameters are specified referred to the
input (RTI) which is to say that the effect on the output is “G”
times larger. Offset voltage vs. power supply is also specified as
an RTI error.

By separating these errors, one can evaluate the total error inde­pendent of the gain. For a given gain, both errors can be com­bined to give a total error referred to the input (RTI) or output
(RTO) by the following formula:

Total Error RTI = input error + (output error/gain)
Total Error RTO = (Gain × input error) + output error

The AD625 provides for both input and output offset voltage
adjustment. This simplifies nulling in very high precision appli­cations and minimizes offset voltage effects in switched gain
applications. In such applications the input offset is adjusted
first at the highest programmed gain, then the output offset is
adjusted at G = 1. If only a single null is desired, the input offset
null should be used. The most additional drift when using only
the input offset null is 0.9 µV/°C, RTO.

COMMON-MODE REJECTION

Common-mode rejection is a measure of the change in output
voltage when both inputs are changed by equal amounts. These
specifications are usually given for a full-range input voltage
change and a specified source imbalance.

In an instrumentation amplifier, degradation of common-mode
rejection is caused by a differential phase shift due to differences

in distributed stray capacitances. In many applications shielded
cables are used to minimize noise. This technique can create

AD625

+V

S

–V

S

R

F

R

G

R

F

SENSE

REFERENCE

AD711

V

OUT

+INPUT

–INPUT

100

Figure 32. Common-Mode Shield Driver

common-mode rejection errors unless the shield is properly
driven. Figures 32 and 33 show active data guards which are
configured to improve ac common-mode rejection by “boot­strapping” the capacitances of the input cabling, thus minimiz­ing differential phase shift.

AD625

+V

S

–V

S

R

F

R

G

R

F

AD712

100

100

V

OUT

SENSE

REFERENCE

–INPUT

+INPUT

–V

S

Figure 33. Differential Shield Driver

GROUNDING

In order to isolate low level analog signals from a noisy digital
environment, many data-acquisition components have two or
more ground pins. These grounds must eventually be tied to­gether at one point. It would be convenient to use a single
ground line, however, current through ground wires and pc runs
of the circuit card can cause hundreds of millivolts of error.
Therefore, separate ground returns should be provided to mini­mize the current flow from the sensitive points to the system
ground (see Figure 34). Since the AD625 output voltage is
developed with respect to the potential on the reference termi­nal, it can solve many grounding problems.

AD625

AD7502

–VS+V

S

–V

S

+V

S

AD583

SAMPLE

AND

HOLD

HOLD

CAP

–VS+V

S

INPUT

SIGNAL

STATUS

ANALOG

OUT

–V

S

+V

S

DIGITAL

COMMON

V

LOGIC

ANALOG POWER

GROUND

AD574A

A/D

CONVERTER

Figure 34. Basic Grounding Practice for a Data Acquisition System

AD625

REV. D–12–

GROUND RETURNS FOR BIAS CURRENTS

Input bias currents are those currents necessary to bias the input
transistors of a dc amplifier. There must be a direct return path
for these currents, otherwise they will charge external capaci­tances, causing the output to drift uncontrollably or saturate.
Therefore, when amplifying “floating” input sources such as
transformers, or ac-coupled sources, there must be a dc path
from each input to ground as shown in Figure 35.

AD625

+V

S

–V

S

R

F

R

G

R

F

V

OUT

LOAD

TO POWER

SUPPLY

GROUND

SENSE

REFERENCE

Figure 35a. Ground Returns for Bias Currents with
Transformer Coupled Inputs

AD625

+V

S

–V

S

R

F

R

G

R

F

V

OUT

LOAD

TO POWER

SUPPLY

GROUND

SENSE

REFERENCE

Figure 35b. Ground Returns for Bias Currents with
Thermocouple Input

AD625

+V

S

–V

S

R

F

R

G

R

F

V

OUT

LOAD

TO POWER

SUPPLY

GROUND

SENSE

REFERENCE

100k 100k

Figure 35c. Ground Returns for Bias Currents with AC
Coupled Inputs

AUTOZERO CIRCUITS

In many applications it is necessary to maintain high accuracy.
At room temperature, offset effects can be nulled by the use of
offset trimpots. Over the operating temperature range, however,
offset nulling becomes a problem. For these applications the
autozero circuit of Figure 36 provides a hardware solution.

OTHER CONSIDERATIONS

One of the more overlooked problems in designing ultralow­drift dc amplifiers is thermocouple induced offset. In a circuit
comprised of two dissimilar conductors (i.e., copper, kovar), a
current flows when the two junctions are at different tempera­tures. When this circuit is broken, a voltage known as the
“Seebeck” or thermocouple emf can be measured. Standard IC
lead material (kovar) and copper form a thermocouple with a

high thermoelectric potential (about 35 µV°C). This means that
care must be taken to insure that all connections (especially
those in the input circuit of the AD625) remain isothermal. This
includes the input leads (1, 16) and the gain sense lines (2, 15).
These pins were chosen for symmetry, helping to desensitize the
input circuit to thermal gradients. In addition, the user should
also avoid air currents over the circuitry since slowly fluctuating

AD625

+V

S

–V

S

AD7502

GND VDDV

SS

15 16

13

14

V

DD

V

SS

GND

AD7510DIKD

A1 A2 A3 A4

200s

ZERO PULSE

AD711

+

V

IN

–

0.1F LOW
LEAKAGE

1k

12

11

9

10

V

OUT

Figure 36. Auto-Zero Circuit

thermocouple voltages will appear as “flicker” noise. In SPGA
applications relay contacts and CMOS mux leads are both
potential sources of additional thermocouple errors.

The base emitter junction of an input transistor can rectify out
of band signals (i.e., RF interference). When amplifying small
signals, these rectified voltages act as small dc offset errors. The
AD625 allows direct access to the input transistors’ bases and
emitters enabling the user to apply some first order filtering to
these unwanted signals. In Figure 37, the RC time constant
should be chosen for desired attenuation of the interfering signals.
In the case of a resistive transducer, the capacitance alone work­ing against the internal resistance of the transducer may suffice.

+GAIN SENSE

+IN

–IN

RTI NULL

RTI NULL

RTO
NULL

RTO
NULL

+V

+GAIN DRIVE

–GAIN DRIVE

R

F

R

G

R

F

NC

REF

–V

S

V

OUT

+V

S

A1 A2

AD625

10k

10k 10k

10k

A3

1

2

3

4

5

6

7

8

16

15

14

13

12

11

10

9

FILTER

CAP

R R

FILTER

CAP

CC

–GAIN SENSE

+IN

SENSE

V

OUT

–IN

Figure 37. Circuit to Attenuate RF Interference

AD625

REV. D

–13–

–

V

IN

+

12-BIT

DAS

10k

10k

AD625

10k

10k

V

S

–INPUT

–GAIN

SENSE

–GAIN
DRIVE

+GAIN
DRIVE

+GAIN

SENSE

+INPUT

20k

15.6k

3.9k

975k

650k

975k

3.9k

20k

15.6k

C

S

C

S

I

S

I

S

I

OUT

I

OUT

C

OUT

C

OUT

R

ON

R

ON

C

S-OUT

C

S-OUT

Figure 39. SPGA with Multiplexer Error Sources

Figure 39 shows a complete SPGA feeding a 12-bit DAS with a
0 V–10 V input range. This configuration was used in the error
budget analysis shown in Table II. The gain used for the RTI
calculations is set at 16. As the gain is changed, the ON resis­tance of the multiplexer and the feedback resistance will change,
which will slightly alter the values in the table.

Table II. Errors Induced by Multiplexer to an SPGA

Induced Specifications Voltage Offset
Error AD625C AD7520KN Calculation Induced RTI

RTI Offset Gain Sense Switch 40 nA × 170 Ω = 6.8 µV
Voltage Offset Resistance 6.8 µV

Current 170 Ω
40 nA

RTI Offset Gain Sense Differential 60 nA × 6.8 Ω = 0.41 µV
Voltage Current Switch 0.41 µV

60 nA Resistance

6.8 Ω

RTO Offset Feedback Differential 2 (0.2 nA × 20 kΩ) 0.5 µV
Voltage Resistance Leakage = 8 µV/16

20 kΩ

1

Current (IS)

2

+0.2 nA
–0.2 nA

RTO Offset Feedback Differential 2 (1 nA × 20 kΩ) 2.5 µV
Voltage Resistance Leakage = 40 µV/16

20 kΩ

1

Current
(I

OUT

)

2

+1 nA
–1 nA

Total error induced by a typical CMOS multiplexer
to an SPGA at +25°C 10.21 A

NOTES

1

The resistor for this calculation is the user-provided feedback resistance (RF).

20 kΩ is recommended value (see Resistor Programmable Gain Amplifier section).

2

The leakage currents (IS and I

OUT

) will induce an offset voltage, however, the offset
will be determined by the difference between the leakages of each “half’’ of the
differential multiplexer. The differential leakage current is multiplied by the
feedback resistance (see Note 1), to determine offset voltage. Because differential
leakage current is not a parameter specified on multiplexer data sheets, the most
extreme difference (one most positive and one most negative) was used for the
calculations in Table II. Typical performance will be much better.

**The frequency response and settling will be affected by the ON resistance and

internal capacitance of the multiplexer. Figure 40 shows the settling time vs.
ON resistance at different gain settings for an AD625 based SPGA.

**Switch resistance and leakage current errors can be reduced by using relays.

These capacitances may also be incorporated as part of the
external input protection circuit (see section on Input Protec­tion). As a general practice every effort should be made to
match the extraneous capacitance at Pins 15 and 2, and Pins 1
and 16, to preserve high ac CMR.

SOFTWARE PROGRAMMABLE GAIN AMPLIFIER

An SPGA provides the ability to externally program precision
gains from digital inputs. Historically, the problem in systems
requiring electronic switching of gains has been the ON resis­tance (R

ON

) of the multiplexer, which appears in series with the

gain setting resistor R

G

. This can result in substantial gain errors
and gain drifts. The AD625 eliminates this problem by making
the gain drive and gain sense pins available (Pins 2, 15, 5, 12;
see Figure 39). Consequently the multiplexer’s ON resistance is
removed from the signal current path. This transforms the ON
resistance error into a small nullable offset error. To clarify this
point, an error budget analysis has been performed in Table II
based on the SPGA configuration shown in Figure 39.

+GAIN

SENSE

+INPUT

–INPUT

RTI NULL

RTI NULL

+V

S

+GAIN DRIVE –GAIN DRIVE

NC

REF

–V

S

V

OUT

+V

S

A1 A2

AD625

10k

10k 10k

10k

A3

1

2

3

4

5

6

7

8

16

15

14

13

12

11

10

9

–GAIN
SENSE

TTL/DTL TO CMOS LEVEL TRANSLATOR

DECODER/DRIVER

3.9k 975 650 975 3.9k

15.6k 15.6k20k 20k

AD7502

A0

A1

E

N

V

SS

V

DD

GND

–V

S

RTO NULL

RTO NULL

Figure 38. SPGA in a Gain of 16

Figure 38 shows an AD625 based SPGA with possible gains of
1, 4, 16, 64. R

G

equals the resistance between the gain sense

lines (Pins 2 and 15) of the AD625. In Figure 38, R

G

equals

the sum of the two 975 Ω resistors and the 650 Ω resistor, or
2600 Ω. R

F

equals the resistance between the gain sense and the

gain drive pins (Pins 12 and 15, or Pins 2 and 5), that is R

F

equals the 15.6 kΩ resistor plus the 3.9 kΩ resistor, or 19.5 kΩ.
The gain, therefore equals:

2R

F

R

G

+1 =

2(19.5kΩ)

(2.6 kΩ)

+1 =16

As the switches of the differential multiplexer proceed synchro­nously, R

G

and RF change, resulting in the various programmed

gain settings.

AD625

REV. D–14–

GAIN

1000

1

SETTLING TIME – s

800

400

200

100

80

40

20

10

8

4

2

1

4 16 64 256 1024 4096

R

ON

= 1k

R

ON

= 500

R

ON

= 200

RON = 0

Figure 40. Time to 0.01% of a 20 V Step Input for
SPGA with AD625

DETERMINING SPGA RESISTOR NETWORK VALUES

The individual resistors in the gain network can be calculated
sequentially using the formula given below. The equation deter­mines the resistors as labeled in Figure 41. The feedback resis­tors and the gain setting resistors are interactive, therefore; the
formula must be a series where the present term is dependent on
the preceding term(s). The formula

RkR

G

G

G

R

F

i

F

j

j

i

i

F

+

=

=

=

=

=

∑

1

0

1

1

0

0

20 1

1

0

( – )( – )Ω

can be used to calculate the necessary feedback resistors for any
set of gains. This formula yields a network with a total resistance
of 40 kΩ. A dummy variable (j) serves as a counter to keep a
running total of the preceding feedback resistors. To illustrate
how the formula can be applied, an example similar to the
calculation used for the resistor network in Figure 38 is exam­ined below.

1) Unity gain is treated as a separate case. It is implemented

with separate 20 kΩ feedback resistors as shown in Figure 41.
It is then ignored in further calculations.

2) Before making any calculations it is advised to draw a resistor
network similar to the network in Figure 41. The network
will have (2 × M) + 1 resistors, where M = number of gains.
For Figure 38 M = 3 (4, 16, 64), therefore, the resistor string
will have seven resistors (plus the two 20 kΩ “side” resistors
for unity gain).

3) Begin all calculations with G

0

= 1 and R

F

0

= 0.

R

F

1

= (20 kΩ – R

F

0

) (1–1/4): R

F

0

= 0 ∴ R

F

1

= 15 kΩ

R

F

2

= [20 kΩ – (R

F

0

+ R

F

1

)] (1–4/16):

R

F

0

+ R

F

1

= 15 kΩ ∴ R

F

2

= 3.75 kΩ

R

F

3

= [20 kΩ – (R

F

0

+ R

F

1

+ R

F

2

)] (1–16/64):

R

F

0

+ R

F

1

+ R

F

2

= 18.75 kΩ ∴ R

F

3

= 937.5 Ω

4) The center resistor (R

G

of the highest gain setting), is deter-

mined last. Its value is the remaining resistance of the 40 kΩ
string, and can be calculated with the equation:

Rk R

GF

j

j

M

=

=

∑

( – )40 2

0

Ω

RG = 40 kΩ – 2 (R

F

0

+ R

F

1

+ R

F

2

+

R

F

3

)

40 k

Ω

– 39.375 kΩ = 625

Ω

5) If different resistor values are desired, all the resistors in the
network can be scaled by some convenient factor. However,
raising the impedance will increase the RTO errors, lowering
the total network resistance below 20 kΩ can result in ampli­fier instability. More information on this phenomenon is
given in the RPGA section of the data sheet. The scale factor
will not affect the unity gain feedback resistors. The resistor
network in Figure 38 has a scaling factor of 650/625 = 1.04,
if this factor is used on R

F

1

, R

F

2

, R

F

3

, and RG, then the resis-

tor values will match exactly.

6) Round off errors can be cumulative, therefore, it is advised to
carry as many significant digits as possible until all the values
have been calculated.

AD75xx

TO GAIN SENSE

(PIN 2)

20k RF

1

20k

RF

2

RFNRFGRF

N

RF

2

TO GAIN SENSE

(PIN 15)

TO GAIN DRIVE

(PIN 5)

TO GAIN DRIVE

(PIN 12)

CONNECT IF UNITY

GAIN IS DESIRED

CONNECT IF UNITY

GAIN IS DESIRED

Figure 41. Resistors for a Gain Setting Network

AD625

REV. D

–15–

–15–

OUTLINE DIMENSIONS

Dimensions shown in inches and (mm).

16-Lead Plastic DIP (N-16)

16

18

9

PIN 1

0.755 (19.18)

0.745 (18.93)

0.26 (6.61)

0.24 (6.1)

SEATING
PLANE

0.17 (4.32)
MAX

0.02 (0.508)

0.015 (0.381)

0.175 (4.45)

0.12 (3.05)

0.065 (1.66)

0.045 (1.15)

0.015 (2.67)

0.095 (2.42)

0.14 (3.56)

0.12 (3.05)

0.012 (0.305)

0.008 (0.203)

0.306 (7.78)

0.294 (7.47)

20-Terminal Leadless Chip Carrier (E-20A)

1

20

4

9

8

13

19

14

3

18

BOTTOM

VIEW

0.040  45°
(1.02  45°)

REF 3 PLCS

0.050
(1.27)

0.350 0.008
(8.89 0.20)

SQ

0.082 0.018

(2.085 0.455)

0.20  45°

(0.51  45°)

REF

0.025 0.003

(0.635 0.075)

16-Lead Ceramic DIP (D-16)

16

1

8

9

PIN 1

0.800 0.010

20.32 0.254

0.265
(6.73)

0.290 0.010

(7.37 0.254)

0.430

(10.922)

0.040R

0.310 0.01
.874 0.254)

SEATING
PLANE

0.095 (2.41)

0.180 0.03
(4.57 0.762)

0.125 (3.175)
MIN

0.035 0.01
(0.889 0.254)

0.047 0.007
(1.19 0.18)

0.100 (254)
BSC

0.017

+0.003
–0.002

0.43

+0.076
–0.05

0.700 (17.78) BSC

0.085 (2.159)

0.010 0.002
(0.254 0.05)

0.300
(7.62)

REF

C00780c–0–6/00 (rev. D)

PRINTED IN U.S.A.