LT1920CS8#TRPBF

7
LT1920
TYPICAL PERFOR A CE CHARACTERISTICS
UW
50µs/DIV
Large-Signal Transient Response
G = 1000
V
S
= ±15V
R
L
= 2k
C
L
= 60pF
5V/DIV
1167 G37
GAIN (dB)
1
1
SETTLING TIME (µs)
10
100
1000
10 100 1000
1920 G30
V
S
= ±15V
T
A
= 25°C
V
OUT
= 10V
1mV = 0.01%
Settling Time vs Gain
50µs/DIV
Small-Signal Transient Response
G = 1000
V
S
= ±15V
R
L
= 2k
C
L
= 60pF
20mV/DIV
1167 G38
Slew Rate vs Temperature
TEMPERATURE (°C)
–50 25
0.8
SLEW RATE (V/µs)
1.2
1.8
0
50
75
1920 G36
1.0
1.6
1.4
25
100
125
V
S
= ±15V
V
OUT
= ±10V
G = 1
+SLEW
SLEW
Settling Time vs Step Size
SETTLING TIME (µs)
2
OUTPUT STEP (V)
2
6
10
10
1920 G33
–2
–6
0
4
8
–4
–8
–10
4
6
8
311
5
7
9
12
0V
V
OUT
TO 0.1%
TO 0.1%
TO 0.01%
TO 0.01%
0V
V
OUT
V
S
= ±15
G = 1
T
A
= 25°C
C
L
= 30pF
R
L
= 1k
Output Voltage Swing
vs Load Current
OUTPUT CURRENT (mA)
OUTPUT VOLTAGE SWING (V) 
(REFERRED TO SUPPLY VOLTAGE)
+V
S
+V
S
– 0.5
+V
S
– 1.0
+V
S
– 1.5
+V
S
– 2.0
–V
S
+ 2.0
–V
S
+ 1.5
–V
S
+ 1.0
–V
S
+ 0.5
–V
S
0.01 1 10 100
1920 G39
0.1
V
S
= ±15V
85°C
25°C
–40°C
SOURCE
SINK
8
LT1920
with programmed gain. Therefore, the bandwidth does not
drop proportional to gain.
The input transistors Q1 and Q2 offer excellent matching,
which is inherent in NPN bipolar transistors, as well as
picoampere input bias current due to superbeta process-
ing. The collector currents in Q1 and Q2 are held constant
due to the feedback through the Q1-A1-R1 loop and
Q2-A2-R2 loop which in turn impresses the differential
input voltage across the external gain set resistor R
G
.
Since the current that flows through R
G
also flows through
R
1 and R2, the ratios provide a gained-up differential volt-
age, G = (R1 + R2)/R
G
, to the unity-gain difference
amplifier
A3. The common mode voltage is removed by A3, result-
ing in a single-ended output voltage referenced to the
voltage on the REF pin. The resulting gain equation is:
V
OUT
– V
REF
= G(V
IN
+
– V
IN
)
where:
G = (49.4k/R
G
) + 1
solving for the gain set resistor gives:
R
G
= 49.4k/(G – 1)
THEORY OF OPERATIO
U
The LT1920 is a modified version of the three op amp
instrumentation amplifier. Laser trimming and monolithic
construction allow tight matching and tracking of circuit
parameters over the specified temperature range. Refer to
the block diagram (Figure 1) to understand the following
circuit description. The collector currents in Q1 and Q2 are
trimmed to minimize offset voltage drift, thus assuring a
high level of performance. R1 and R2 are trimmed to an
absolute value of 24.7k to assure that the gain can be set
accurately (0.3% at G = 100) with only one external
resistor R
G
. The value of R
G
in parallel with R1 (R2)
determines the transconductance of the preamp stage. As
R
G
is reduced for larger programmed gains, the transcon-
ductance of the input preamp stage increases to that of the
input transistors Q1 and Q2. This increases the open-loop
gain when the programmed gain is increased, reducing
the input referred gain related errors and noise. The input
voltage noise at gains greater than 50 is determined only
by Q1 and Q2. At lower gains the noise of the difference
amplifier and preamp gain setting resistors increase the
noise. The gain bandwidth product is determined by C1,
C2 and the preamp transconductance which increases
BLOCK DIAGRAM
W
Q1
R
G
2
OUTPUT
6
REF
1920 F01
5
7
+
A1
+
A3
VB
R1
24.7k
R3
400
R4
400
C1
1
R
G
8
R7
10k
R8
10k
R5
10k
R6
10k
DIFFERENCE AMPLIFIER STAGEPREAMP STAGE
+IN
–IN
3
+
A2
VB
R2
24.7k
C2
V
+
V
V
V
+
V
Q2
V
V
+
4
V
Figure 1. Block Diagram
9
LT1920
Input and Output Offset Voltage
The offset voltage of the LT1920 has two components: the
output offset and the input offset. The total offset voltage
referred to the input (RTI) is found by dividing the output
offset by the programmed gain (G) and adding it to the
input offset. At high gains the input offset voltage domi-
nates, whereas at low gains the output offset voltage
dominates. The total offset voltage is:
Total input offset voltage (RTI)
= input offset + (output offset/G)
Total output offset voltage (RTO)
= (input offset • G) + output offset
Reference Terminal
The reference terminal is one end of one of the four 10k
resistors around the difference amplifier. The output volt-
age of the LT1920 (Pin 6) is referenced to the voltage on
the reference terminal (Pin 5). Resistance in series with
the REF pin must be minimized for best common mode
rejection. For example, a 2 resistance from the REF pin
to ground will not only increase the gain error by 0.02%
but will lower the CMRR to 80dB.
Single Supply Operation
For single supply operation, the REF pin can be at the same
potential as the negative supply (Pin 4) provided the
output of the instrumentation amplifier remains inside the
specified operating range and that one of the inputs is at
least 2.5V above ground. The barometer application on the
front page of this data sheet is an example that satisfies
these conditions. The resistance R
SET
from the bridge
transducer to ground sets the operating current for the
bridge and also has the effect of raising the input common
mode voltage. The output of the LT1920 is always inside
the specified range since the barometric pressure rarely
goes low enough to cause the output to rail (30.00 inches
of Hg corresponds to 3.000V). For applications that re-
quire the output to swing at or below the REF potential, the
voltage on the REF pin can be level shifted. An op amp is
used to buffer the voltage on the REF pin since a parasitic
series resistance will degrade the CMRR. The application
in the back of this data sheet, Four Digit Pressure Sensor,
is an example.
THEORY OF OPERATIO
U
Output Offset Trimming
The LT1920 is laser trimmed for low offset voltage so that
no external offset trimming is required for most applica-
tions. In the event that the offset needs to be adjusted, the
circuit in Figure 2 is an example of an optional offset adjust
circuit. The op amp buffer provides a low impedance to the
REF pin where resistance must be kept to minimum for
best CMRR and lowest gain error.
Input Bias Current Return Path
The low input bias current of the LT1920 (2nA) and the
high input impedance (200G) allow the use of high
impedance sources without introducing additional offset
voltage errors, even when the full common mode range is
required. However, a path must be provided for the input
bias currents of both inputs when a purely differential
signal is being amplified. Without this path the inputs will
float to either rail and exceed the input common mode
range of the LT1920, resulting in a saturated input stage.
Figure 3 shows three examples of an input bias current
path. The first example is of a purely differential signal
source with a 10k input current path to ground. Since the
impedance of the signal source is low, only one resistor is
needed. Two matching resistors are needed for higher
impedance signal sources as shown in the second
example. Balancing the input impedance improves both
common mode rejection and DC offset. The need for input
resistors is eliminated if a center tap is present as shown
in the third example.
+
2
–IN
OUTPUT
+IN
1
8
10k
100
100
–10mV
1920 F02
V
V
+
10mV
5
2
3
1
6
1/2
LT1112
±10mV
ADJUSTMENT RANGE
R
G
3
+
LT1920
REF
Figure 2. Optional Trimming of Output Offset Voltage

LT1920CS8#TRPBF

Mfr. #:
Manufacturer:
Analog Devices Inc.
Description:
Instrumentation Amplifiers 1x Res Gain Progmable, Prec Instr Amp
Lifecycle:
New from this manufacturer.
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