AD620AR Analog Devices Inc, AD620AR Datasheet - Page 13

• Manufacturer Part Number: AD620AR
• Description: IC AMP INST LP LN 18MA 8SOIC
• Manufacturer: Analog Devices Inc

Specifications of AD620AR

• Slew Rate: 1.2 V/µs
• Rohs Status: RoHS non-compliant
• Design Resources: Low Cost Programmable Gain Instrumentation Amplifier Circuit Using ADG1611 and AD620 (CN0146)
• Amplifier Type: Instrumentation
• Number Of Circuits: 1
• -3db Bandwidth: 1MHz
• Current - Input Bias: 500pA
• Voltage - Input Offset: 30µV
• Current - Supply: 900µA
• Current - Output / Channel: 18mA
• Voltage - Supply, Single/dual (±): 4.6 V ~ 36 V, ±2.3 V ~ 18 V
• Operating Temperature: -40°C ~ 85°C
• Mounting Type: Surface Mount
• Package / Case: 8-SOIC (3.9mm Width)
• No. Of Amplifiers: 1
• Bandwidth: 120kHz
• Supply Current: 1.3mA
• Amplifier Case Style: SOIC
• No. Of Pins: 8
• Operating Temperature Range: -40°C To +85°C
• Programmable Gain Max: 10000
• Output Type: -
• Gain Bandwidth Product: -
• Lead Free Status / RoHS Status: Contains lead / RoHS non-compliant

THEORY OF OPERATION
– IN
The AD620 is a monolithic instrumentation amplifier based on
a modification of the classic three op amp approach. Absolute
value trimming allows the user to program gain accurately
(to 0.15% at G = 100) with only one resistor. Monolithic
construction and laser wafer trimming allow the tight matching
and tracking of circuit components, thus ensuring the high level
of performance inherent in this circuit.
400Ω
R3
I1
Q1
Figure 38. Simplified Schematic of AD620
20µA
C1
SENSE
GAIN
A1
R1
R
–V
V
G
B
S
R2
SENSE
GAIN
A2
20µA
C2
Q2
I2
10kΩ
10kΩ
400Ω
R4
10kΩ
A3
10kΩ
+IN
OUTPUT
REF
Rev. G | Page 13 of 20
The input transistors Q1 and Q2 provide a single differential-
pair bipolar input for high precision (Figure 38), yet offer 10×
lower input bias current thanks to Superϐeta processing.
Feedback through the Q1-A1-R1 loop and the Q2-A2-R2 loop
maintains constant collector current of the input devices Q1
and Q2, thereby impressing the input voltage across the external
gain setting resistor R
inputs to the A1/A2 outputs given by G = (R1 + R2)/R
unity-gain subtractor, A3, removes any common-mode signal,
yielding a single-ended output referred to the REF pin potential.
The value of R
preamp stage. As R
transconductance increases asymptotically to that of the input
transistors. This has three important advantages: (a) Open-loop
gain is boosted for increasing programmed gain, thus reducing
gain related errors. (b) The gain-bandwidth product
(determined by C1 and C2 and the preamp transconductance)
increases with programmed gain, thus optimizing frequency
response. (c) The input voltage noise is reduced to a value of
9 nV/√Hz, determined mainly by the collector current and base
resistance of the input devices.
The internal gain resistors, R1 and R2, are trimmed to an
absolute value of 24.7 kΩ, allowing the gain to be programmed
accurately with a single external resistor.
The gain equation is then
Make vs. Buy: a Typical Bridge Application Error Budget
The AD620 offers improved performance over “homebrew”
three op amp IA designs, along with smaller size, fewer
components, and 10× lower supply current. In the typical
application, shown in Figure 39, a gain of 100 is required to
amplify a bridge output of 20 mV full-scale over the industrial
temperature range of −40°C to +85°C. Table 3 shows how to
calculate the effect various error sources have on circuit
accuracy.
G
R
G
=
=
49
49
R
4 .
G
4 .
G
k
G
−
Ω
k
1
also determines the transconductance of the
Ω
+
G
1
is reduced for larger gains, the
G
. This creates a differential gain from the
G
AD620
+ 1. The