Meets IEC 1000-4-2 Level 4 ESD Tests with
Two External 5k Resistors
■
Single Gain Set Resistor: G = 1 to 10,000
■
Gain Error: G = 10, 0.4% Max
■
Input Offset Voltage Drift: 0.3µV/°C Max
■
Gain Nonlinearity: G = 10, 20ppm Max
■
Input Offset Voltage: 40µV Max
■
Input Bias Current: 250pA Max
■
PSRR at AV =1: 103dB Min
■
CMRR at AV = 1: 90dB Min
■
Wide Supply Range: ±2.3V to ±18V
■
1kHz Voltage Noise: 10nV/√Hz
■
0.1Hz to 10Hz Noise: 0.28µV
■
Available in 8-Pin PDIP and SO Packages
P-P
U
APPLICATIOS
■
Bridge Amplifiers
■
Strain Gauge Amplifiers
■
Thermocouple Amplifiers
■
Differential to Single-Ended Converters
■
Differential Voltage to Current Converters
■
Data Acquisition
■
Battery-Powered and Portable Equipment
■
Medical Instrumentation
■
Scales
Precision Instrumentation Amplifier
DESCRIPTIO
U
March 2000
The LT®1168 is a micropower, precision instrumentation
amplifier that requires only one external resistor to set gains
of 1 to 10,000. The low voltage noise of 10nV/√Hz (at 1kHz)
is not compromised by low power dissipation (350µA typical
for ±15V supplies). The wide supply range of ±2.3V to ±18V
allows the LT1168 to fit into a wide variety of industrial as well
as battery-powered applications.
The high accuracy of the LT1168 is due to a 20ppm maximum
nonlinearity and 0.4% max gain error (G = 10). Previous
monolithic instrumentation amps cannot handle a 2k load
resistor whereas the nonlinearity of the LT1168 is specified
for loads as low as 2k. The LT1168 is laser trimmed for very
low input offset voltage (40µV max), drift (0.3µV/°C), high
CMRR (90dB, G = 1) and PSRR (103dB, G = 1). Low input
bias currents of 250pA max are achieved with the use of
superbeta processing. The output can handle capacitive
loads up to 1000pF in any gain configuration while the inputs
are ESD protected up to 13kV (human body). The LT1168
with two external 5k resistors passes the IEC 1000-4-2 level
4 specification.
The LT1168 is a pin-for-pin improved second source for the
AD620 and INA118. The LT1168, offered in 8-pin PDIP and
SO packages, requires significantly less PC board area than
discrete op amp resistor designs. These advantages make
the LT1168 the most cost effective solution for precision
instrumentation amplifier applications.
, LTC and LT are registered trademarks of Linear Technology Corporation.
TYPICAL APPLICATIO
5V
1
3.5k
3.5k
*See Theory of Operation section
3.5k
G = 200
3.5k
249Ω
3
8
R1
1
2
U
Single Supply* Pressure Monitor
+
LT1168
–
4
Information furnished by Linear Technology Corporation is believed to be accurate and reliable.
However, no responsibility is assumed for its use. Linear Technology Corporation makes no representation that the interconnection of its circuits as described herein will not infringe on existing patent rights.
BI TECHNOLOGIES
67-8-3 R40KQ, (0.02% RATIO MATCH)
7
5
40k
6
20k
3
+
40k
1/2
LT1112
2
–
REF
IN
1
AGND
LTC
ADC
®
1286
DIGITAL
DATA
OUTPUT
1168 TA01
Gain Nonlinearity
NONLINEARITY (100ppm/DIV)
G = 1000OUTPUT VOLTAGE (2V/DIV)
RL = 2K
V
= ±10V
OUT
1168 TA01a
1
LT1168
1
2
3
4
8
7
6
5
TOP VIEW
R
G
–IN
+IN
–V
S
R
G
+V
S
OUTPUT
REF
N8 PACKAGE
8-LEAD PDIP
S8 PACKAGE
8-LEAD PLASTIC SO
+
–
WW
W
U
ABSOLUTE MAXIMUM RATINGS
(Note 1)
Supply Voltage ...................................................... ±20V
G = 10 (Note 7)0.040.40.050.5%
G = 100 (Note 7)0.040.50.050.6%
G = 1000 (Note 7)0.080.50.080.6%
Gain Nonlinearity (Notes 7, 8)VO = ±10V, G = 126310ppm
V
= ±10V,G = 10 and 10010201525ppm
O
= ±10V, G = 100020402560ppm
V
O
VO = ±10V, G = 1, RL = 2k415520ppm
= ±10V,G = 10 and 100, RL = 2k20403060ppm
V
O
= ±10V, G = 1000, RL = 2k40755090ppm
V
O
V
OST
V
OSI
V
OSO
I
OS
I
B
e
n
i
n
R
IN
2
Total Input Referred Offset Voltage V
Input Offset VoltageG = 1000, VS = ±5V to ±15V15402060µV
Output Offset VoltageG = 1, VS = ±5V to ±15V4020050300µV
Input Offset Current90300100450pA
Input Bias Current4025080500pA
Input Noise Voltage, RTI0.1Hz to 10Hz, G = 12.002.00µV
Input Noise Voltage Density, RTIfO = 1kHz10151015nV/√Hz
Output Noise Voltage Density, RTI fO = 1kHz (Note 9)165220165220nV/√Hz
Input Noise CurrentfO = 0.1Hz to 10Hz55pA
Input Noise Current DensityfO = 10Hz7474fA/√Hz
Input ResistanceVIN = ±10V30010002001000GΩ
= V
OST
0.1Hz to 10Hz, G = 10000.280.28µV
TA = 25°C. VS = ±15V, VCM = 0V, RL = 10k unless otherwise noted.
LT1168AC/LT1168AILT1168C/LT1168I
+ V
OSO
/G
OSI
P-P
P-P
P-P
LT1168
ELECTRICAL CHARACTERISTICS
SYMBOL PARAMETERCONDITIONS (Note 6)MINTYPMAXMINTYPMAXUNITS
C
IN(DIFF)
C
IN(CM)
V
CM
CMRRCommon Mode1k Source Imbalance,
PSRRPower SupplyVS = ±2.3V to ±18V
I
S
V
OUT
I
OUT
BWBandwidthG = 1400400kHz
SRSlew RateG = 1, V
REFINReference Input Resistance6060kΩ
I
REFIN
V
REF
A
VREF
Differential Input CapacitancefO = 100kHz1.61.6pF
Common Mode InputfO = 100kHz1.61.6pF
Capacitance
Input Voltage RangeG = 1, Other Input Grounded
The ● denotes the specifications which apply over the –40°C ≤ TA ≤ 85°C temperature range. VS = ±15V, VCM = 0V, RL = 10k unless
otherwise noted. (Note 8)
LT1168AILT1168I
SYMBOL PARAMETERCONDITIONS (Note 6)MINTYPMAXMINTYPMAXUNITS
Gain ErrorG = 1●0.0140.040.0150.05%
G = 10 (Note 7)
G = 100 (Note 7)
G = 1000 (Note 7)
G
N
Gain NonlinearityVO = ±10V, G = 1●320525ppm
(Notes 7, 8)V
= ±10V, G = 10 and 100●10351540ppm
O
VO = ±10V, G = 1000
●0.6001.90.7002.0%
●0.6002.00.7002.1%
●0.6002.10.7002.2%
●307035100ppm
G/TGain vs TemperatureG < 1000 (Note 7)●100200100200ppm/°C
4
LT1168
ELECTRICAL CHARACTERISTICS
The ● denotes the specifications which apply over the –40°C ≤ TA ≤ 85°C temperature range. VS = ±15V, VCM = 0V, RL = 10k unless
otherwise noted. (Note 5)
LT1168AILT1168I
SYMBOL PARAMETERCONDITIONS (Note 6)MINTYPMAXMINTYPMAXUNITS
V
OST
V
OSI
V
OSIH
V
OSO
V
OSOH
V
OSI
V
OSO
I
OS
IOS/TInput Offset Current Drift●0.30.3pA/°C
I
B
IB/TInput Bias Current Drift●1.41.4pA/°C
V
CM
CMRRCommon Mode1k Source Imbalance,
PSRRPower SupplyVS = ±2.3V to ±18V
I
S
V
OUT
I
OUT
SRSlew Rate●0.220.410.220.42V/µs
V
REF
Note 1: Absolute Maximum Ratings are those values beyond which the life
of a device may be imparied.
Note 2: If the input voltage exceeds the supplies, the input current should
be limited to less than 20mA.
Note 3: A heat sink may be required to keep the junction temperature
below absolute maximum.
Note 4: The LT1168AC/LT1168C are guaranteed functional over the
operating temperature range of –40°C and 85°C.
Note 5: The LT1168AC/LT1168C are guaranteed to meet specified
performance from 0°C to 70°C. The LT1168AC/LT1168C are designed,
characterized and expected to meet specified performance from –40°C
and 85°C but are not tested or QA sampled at these temperatures. The
LT1168AI/LT1168I are guaranteed to meet specified performance from
–40°C to 85°C.
Total Input Referred Offset VoltageV
OST
= V
OSI
+ V
OSO
/G
Input Offset Voltage●207525100µV
Input Offset Voltage Hysteresis(Notes 7, 10)●3.03.0µV
Output Offset Voltage●180500200600µV
Output Offset Voltage Hysteresis (Notes 7, 10)●3030µV
Note 6: Typical parameters are defined as the 60% of the yield parameter
distribution.
Note 7: Does not include the tolerance of the external gain resistor RG.
Note 8: This parameter is measured in a high speed automatic tester that
does not measure the thermal effects with longer time constants. The
magnitude of these thermal effects are dependent on the package used,
heat sinking and air flow conditions.
Note 9: This parameter is not 100% tested.
Note 10: Hysteresis in offset voltage is created by package stress that
differs depending on whether the IC was previously at a higher or lower
temperature. Offset voltage hysteresis is always measured at 25°C, but
the IC is cycled to 85°C I-grade (or 70°C C-grade) or –40°C I-grade
(0°C C-grade) before successive measurement. 60% of the parts will
pass the typical limit on the data sheet.
5
LT1168
TIME (SEC)
0
NOISE VOLTAGE (2µV/DIV)
8
1168 G11
2
4
5
10
6
1
3
9
7
VS = ±15V
T
A
= 25°C
TIME (SEC)
0
NOISE CURRENT (5pA/DIV)
8
1168 G14
2
4
5
10
6
1
3
9
7
VS = ±15V
T
A
= 25°C
UW
TYPICAL PERFOR A CE CHARACTERISTICS
60
G = 1000
50
40
G = 100
30
20
G = 10
GAIN (dB)
10
0
G = 1
–10
–20
0.01
110010000.110
FREQUENCY (kHz)
0.1Hz to 10Hz Noise Voltage, RTI
G = 1000
VS = ±15V
= 25°C
T
A
VS = ±15V
T
= 25°C
A
LT1168 • G02
Voltage Noise Density vs
FrequencyGain vs Frequency
1000
1/f CORNER = 2Hz
GAIN = 1
100
1/f CORNER = 7Hz
GAIN = 10
10
1/f CORNER = 3Hz
VOLTAGE NOISE DENSITY (nV/√Hz)
1
1101001k10k100k
GAIN = 100, 1000
BW LIMIT
GAIN = 1000
FREQUENCY (Hz)
BW LIMIT
GAIN = 100
VS = ±15V
= 25°C
T
A
LT1168 • G01
0.1Hz to 10Hz Noise Voltage,
G = 1
Current Noise Density vs
Frequency0.1Hz to 10Hz Current Noise
1000
VS = ±15V
= 25°C
T
A
RS
NOISE VOLTAGE (0.2µV/DIV)
1
0
Short-Circuit Current vs TimeOvershoot vs Capacitive Load
50
40
30
20
10
0
–10
–20
OUTPUT CURRENT (mA)
–30
(SINK)(SOURCE)
–40
–50
0
TIME FROM OUTPUT SHORT TO GROUND (MINUTES)
2
3
VS = ±15V
5
4
TIME (SEC)
1
6
7
TA = –40°C
TA = 25°C
TA = 85°C
TA = 85°C
TA = 25°C
TA = –40°C
2
100
1
1/f CORNER = 55Hz
101001000
FREQUENCY (Hz)
1168 G13
CURRENT NOISE DENSITY (fA/√Hz)
8
10
9
1168 G12
10
Output Impedance vs Frequency
100
VS = ±15V
90
80
70
60
50
40
OVERSHOOT (%)
30
20
10
0
10
= ±50mV
V
OUT
=
∞
R
L
G = 1
G = 10
G = 100, 1000
100100010000
CAPACITIVE LOAD (pF)
1168 G16
3
1168 G15
OUTPUT IMPEDANCE (Ω)
1k
100
10
1
0.1
VS = ±15V
= 25°C
T
A
G = 1 TO 1000
1k
10k100k1M
FREQUENCY (Hz)
1168 G17
6
UW
TYPICAL PERFOR A CE CHARACTERISTICS
LT1168
10
VS = ±15
8
G = 1
= 25°C
T
A
6
= 30pF
C
L
R
= 1k
4
L
2
0
–2
OUTPUT STEP (V)
–4
–6
–8
–10
8 101214161820222426283032
TO 0.1%
TO 0.01%
0V
0V
TO 0.01%
TO 0.1%
SETTLING TIME (µs)
Falling Edge Settling Time
(0.10%)
0
(V)
–5
IN
V
–10
0
(V)
–5
OUT
V
–10
Settling Time vs GainSettling Time vs Step Size
1000
VS = ±15V
T
= 25°C
A
= 10V TO 0.01%
∆V
OUT
V
OUT
V
OUT
1168 G19
100
10
SETTLING TIME (µs)
1
1
101001000
GAIN
1168 G18
Capacitance
34
32
G = 1, RISING EDGE
30
28
G = 100, FALLING EDGE
26
G = 100,
24
RISING EDGE
22
SETTLING TIME (µs)
VS = ±15V
20
T
A
18
R
L
STEP SIZE = 10V
16
10
G = 1, FALLING EDGE
G = 10,
FALLING EDGE
G = 10,
= 25°C
= 1k
301003001000
LOAD CAPACITANCE (pF)
RISING EDGE
1168 G25
Rising Edge Settling Time
(O.10%)
10
Settling Time (0.1%) vs Load
0.10
0.05
0
0.05
0.10
SETTLING (%)
(V)
IN
V
(V)
OUT
V
5
0
10
5
0
0.10
0.05
0
0.05
0.10
SETTLING (%)
5µs/DIV1168 G29
t = 0
TA = 25°C
= ±15V
V
S
= 2k
R
L
CL = 15pF
Settling Time (0.01%) vs Load
Capacitance
36
G = 100,
34
FALLING EDGE
32
G = 1, RISING EDGE
30
28
G = 10, FALLING EDGE
26
G = 10, RISING EDGE
24
SETTLING TIME (µs)
VS = ±15V
22
= 25°C
T
A
20
= 1k
R
L
STEP SIZE = 10V
18
10
301003001000
LOAD CAPACITANCE (pF)
G = 100,
RISING EDGE
G = 1,
FALLING
EDGE
1168 G26
5µs/DIV1168 G28
t = 0
TA = 25°C
= ±15V
V
S
= 2k
R
L
CL = 15pF
Undistorted Output Swing vs
Frequency
35
G = 10, 100, 1000
30
25
G = 1
20
15
10
5
PEAK-TO-PEAK OUTPUT SWING (V)
0
1
101001000
FREQUENCY (kHz)
VS = ±15V
= 25°C
T
A
1168 G31
7
LT1168
UW
TYPICAL PERFOR A CE CHARACTERISTICS
Output Voltage Swing vs
Load Current
+V
S
VS = ±15V
– 0.5
+V
S
– 1.0
+V
S
– 1.5
+V
S
– 2.0
+V
S
REFERRED TO
SUPPLY VOLTAGE
+V
– 2.5
S
+ 2.5
–V
S
+ 2.0
–V
S
+ 1.5
–V
S
(SINK)(SOURCE)
+ 1.0
–V
S
SWING (V)
–VS + 0.5
OUTPUT VOLTAGE
–V
S
0.01110100
0.1
OUTPUT CURRENT (mA)
Large-Signal Transient Response
5V/DIV
Large-Signal Transient Response
85°C
25°C
–40°C
5V/DIV
G = 1
= ±15V
V
S
RL = 2k
= 60pF
C
L
1168 G20
Small-Signal Transient Response
20mV/DIV
50µs/DIV
1168 G03
Small-Signal Transient Response
20mV/DIV
G = 1
= ±15V
V
S
= 2k
R
L
= 60pF
C
L
10µs/DIV
Large-Signal Transient Response
5V/DIV
1168 G04
G = 10
= ±15V
V
S
= 2k
R
L
= 60pF
C
L
50µs/DIV
Small-Signal Transient Response
20mV/DIV
G = 100
= ±15V
V
S
RL = 2k
= 60pF
C
L
10µs/DIV
1168 G05
1168 G08
G = 10
= ±15V
V
S
= 2k
R
L
= 60pF
C
L
10µs/DIV
Large-Signal Transient Response
5V/DIV
G = 1000
= ±15V
V
S
= 2k
R
L
CL = 60pF
200µs/DIV
1168 G06
1168 G09
G = 100
= ±15V
V
S
= 2k
R
L
= 60pF
C
L
50µs/DIV
1168 G07
Small-Signal Transient Response
20mV/DIV
G = 1000
= ±15V
V
S
= 2k
R
L
= 60pF
C
L
200µs/DIV
1168 G10
8
UW
TEMPERATURE
–75
–50 –25 02550 75 100 125
INPUT BIAS AND OFFSET CURRENT (pA)
1168 G30
500
400
300
200
100
0
–100
–200
–300
–400
–500
VS = ±15V
V
CM
= 0V
I
OS
I
B
TYPICAL PERFOR A CE CHARACTERISTICS
LT1168
Negative Power Supply Rejection
Ratio vs Frequency
160
140
120
100
80
60
40
V+ = 15V
20
T
0
NEGATIVE POWR SUPPLY REJECTION RATIO (dB)
0.11101001k10k100k
G = 100
G = 10
G = 1
= 25°C
A
G = 1000
FREQUENCY (Hz)
Warm-Up Drift
35
30
25
20
1168 G21
SO-8
Positive Power Supply Rejection
Ratio vs Frequency
160
140
120
100
80
60
40
20
0
POSITIVE POWR SUPPLY REJECTION RATIO (dB)
0.11101001k10k100k
V– = –15V
= 25°C
T
A
G = 100
G = 10
G = 1
G = 1000
FREQUENCY (Hz)
Common Mode Rejection Ratio vs
Frequency (1k Source Impedance)
160
140
120
100
COMMON MODE REJECTION RATIO (dB)
1168 G22
G = 1000
G = 100
G = 10
G = 1
80
60
40
VS = 15V
= 25°C
T
A
20
1k SOURCE IMBALANCE
0
0.11101001k10k100k
FREQUENCY (Hz)
Input Bias and Offset Current vs
Temperature
1168 G23
15
10
5
CHANGE IN OFFSET VOLTAGE (µV)
0
012345
BLOCK DIAGRAM
N-8
TIME AFTER POWER-ON (MINUTES)
W
+
V
R3
–IN
2
1
R
G
8
R
G
+IN
3
400Ω
–
V
+
V
R4
400Ω
–
V
1168 G24
VB
+
A1
–
C1
Q1
R1
24.7k
VB
+
A2
–
C2
Q2V
R2
24.7k
30k
30k
R5
R6
30k
–
A3
+
R7
DIFFERENCE AMPLIFIER STAGEPREAMP STAGE
R8
30k
Figure 1. Block Diagram
OUTPUT
6
–
V
REF
5
–
+
V
7
–
V
4
1168 F01
9
LT1168
THEORY OF OPERATIO
U
The LT1168 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 (0.6% at G = 100) with only one external
resistor RG. The value of RG in parallel with R1 (R2)
determines the transconductance of the preamp stage. As
RG is reduced for larger programmed gains, the transconductance 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
with programmed gain. Therefore, the bandwidth does not
drop proportionally with 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 processing. 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 RG.
Since the current that flows through RG also flows through
R
1 and R2, the ratios provide a gained-up differential volt-
age, G = (R1 + R2)/RG, to the unity-gain difference
amplifier
A3. The common mode voltage is removed by A3, resulting in a single-ended output voltage referenced to the
voltage on the REF pin. The resulting gain equation is:
The offset voltage of the LT1168 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 dominates, 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 30k
resistors around the difference amplifier. The output voltage of the LT1168 (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 6Ω resistance from the REF pin
to ground will not only increase the gain error by 0.02%
but will lower the CMRR to 80dB.
G = (49.4kΩ/RG) + 1
solving for the gain set resistor gives:
RG = 49.4kΩ/(G – 1)
Table 1 shows appropriate 1% resistor values for a variety
of gains.
10
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 later
THEORY OF OPERATIO
–
+
2
–IN
OUTPUT
+IN
1
8
10k
100Ω
100Ω
–10mV
1168 F02
V
–
V
+
10mV
5
6
LT1112
±10mV
ADJUSTMENT RANGE
R
G
3
–
+
LT1168
REF
LT1168
U
in this data sheet is an example that satisfies these
conditions. The resistance Rb 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 LT1168 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 require 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
front of this data sheet, Single Supply Pressure Monitor,
is an example.
Output Offset Trimming
The LT1168 is laser trimmed for low offset voltage so that
no external offset trimming is required for most applications. 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.
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 LT1168, 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 10kΩ 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.
Input Bias Current Return Path
The low input bias current of the LT1168 (250pA) and the
high input impedance (200GΩ) allow the use of high
impedance sources without introducing additional offset
voltage errors, even when the full common mode range is
–
THERMOCOUPLE
10k
+
LT1168
Figure 3. Providing an Input Common Mode Current Path
MICROPHONE,
HYDROPHONE,
ETC
200k
Figure 2. Optional Trimming of Output Offset Voltage
–
LT1168
+
200k
–
+
CENTER-TAP PROVIDES
BIAS CURRENT RETURN
LT1167
LT1168
1168 F03
11
LT1168
U
WUU
APPLICATIONS INFORMATION
The LT1168 is a low power precision instrumentation
amplifier that requires only one external resistor to accurately set the gain anywhere from 1 to 1000. The LT1168
is trimmed for critical DC parameters such as gain error
(0.04%, G = 10), input offset voltage (40µV, RTI), CMRR
(90dB min, G = 1) and PSRR (103dB min, G = 1). These
trims allow the amplifier to achieve very high DC accuracy.
The LT1168 achieves low input bias current of just 250pA
(max) through the use of superbeta processing. The
output can handle capacitive loads up to 1000pF in any
gain configuration and the inputs are protected against
ESD strikes up to ±13kV (human body).
Input Protection
The LT1168 can safely handle up to ±20mA of input
current in an overload condition. Adding an external 5k
input resistor in series with each input allows DC input
fault voltage up to ±100V and improves the ESD immunity
to ±8kV (contact) and ±15kV (air discharge), which is the
IEC 1000-4-2 level 4 specification. If lower value input
resistors must be used, a clamp diode from the positive
supply to each input will maintain the IEC 1000-4-2
specification to level 4 for both air and contact discharge.
A 2N4393 drain/source to gate is a good low leakage diode
for use with 1k resistors, see Figure 4. The input resistors
should be carbon and not metal film or carbon film.
OPTIONAL FOR
< 20k
R
J1
2N4393
R
IN
R
IN
Figure 4. Input Protection
J2
2N4393
IN
V
CC
+
R
LT1168
G
–
REF
V
EE
OUT
1168 F04
these very small signals (on the order of microvolts or
millivolts) are sensors that can be a significant distance
from the signal conditioning circuit. Although these sensors may be connected to signal conditioning circuitry,
using shielded or unshielded twisted-pair cabling, the cabling may act as antennae, conveying very high frequency
interference directly into the input stage of the LT1168.
The amplitude and frequency of the interference can have
an adverse effect on an instrumentation amplifier’s input
stage by causing an unwanted DC shift in the amplifier’s
input offset voltage. This well known effect is called RFI
rectification and is produced when out-of-band interference is coupled (inductively, capacitively or via radiation)
and rectified by the instrumentation amplifier’s input transistors. These transistors act as high frequency signal
detectors, in the same way diodes were used as RF
envelope detectors in early radio designs. Regardless of
the type of interference or the method by which it is
coupled into the circuit, an out-of-band error signal appears in series with the instrumentation amplifier’s inputs.
To significantly reduce the effect of these out-of-band
signals on the input offset voltage of instrumentation
amplifiers, simple lowpass filters can be used at the
inputs. This filter should be located very close to the input
pins of the circuit. An effective filter configuration is
illustrated in Figure 5, where three capacitors have been
added to the inputs of the LT1168. Capacitors C
C
form lowpass filters with the external series resis-
XCM2
tors R
to any out-of-band signal appearing on each of
S1, 2
XCM1
and
the input traces. Capacitor CXD forms a filter to reduce any
unwanted signal that would appear across the input traces.
An added benefit to using CXD is that the circuit’s AC
common mode rejection is not degraded due to common
mode capacitive imbalance. The differential mode and
common mode time constants associated with the capacitors are:
t
DM(LPF)
= (2)(RS)(CXD)
RFI Reduction
In many industrial and data acquisition applications,
instrumentation amplifiers are used to accurately amplify
small signals in the presence of large common mode
voltages or high levels of noise. Typically, the sources of
12
t
CM(LPF)
= (R
S1, 2
)(C
XCM1, 2
)
Setting the time constants requires a knowledge of the
frequency, or frequencies of the interference. Once this
frequency is known, the common mode time constants
can be set followed by the differential mode time constant.
LT1168
U
WUU
APPLICATIONS INFORMATION
To avoid any possibility of inadvertently affecting the
signal to be processed, set the common mode time
constant an order of magnitude (or more) larger than the
differential mode time constant. Set the common mode
time constants such that they do not degrade the LT1168
inherent AC CMR. Then the differential mode time constant can be set for the bandwidth required for the application. Setting the differential mode time constant close to
the sensor’s BW also minimizes any noise pickup along
the leads. To avoid any possibility of common mode to
differential mode signal conversion, match the common
mode time constants to 1% or better. If the sensor is an
RTD or a resistive strain gauge, then the series resistors
R
can be omitted, if the sensor is in proximity to the
S1, 2
instrumentation amplifier.
+
C
R
XCM1
S1
0.001µF
1.6k
+
IN
C
XD
0.1µF
R
S2
1.6k
–
IN
C
XCM2
0.001µF
EXTERNAL RFI
FILTER
R
G
V
+
LT1168
V
OUT
–
–
V
f
–3dB
≈ 500Hz
1168 F05
Nerve Impulse Amplifier
The LT1168’s low current noise makes it ideal for EMG
monitors that have high source impedances. Demonstrating the LT1168’s ability to amplify low level signals, the
circuit in Figure 6 takes advantage of the amplifier’s high
gain and low noise operation. This circuit amplifies the low
level nerve impulse signals received from a patient at
Pins␣ 2 and 3. RG and the parallel combination of R3 and R4
set a gain of ten. The potential on LT1112’s Pin 1 creates
a ground for the common mode signal. C1 was chosen to
maintain the stability of the patient ground. The LT1168’s
high CMRR ensures that the desired differential signal is
amplified and unwanted common mode signals are attenuated. Since the DC portion of the signal is not important, R6 and C2 make up a 0.3Hz highpass filter. The AC
signal at LT1112’s Pin 5 is amplified by a gain of 101 set
by R7/R8 +1. The parallel combination of C3 and R7 form
a lowpass filter that decreases this gain at frequencies
above 1kHz. The ability to operate at ±3V on 350µA of
supply current makes the LT1168 ideal for battery-powered applications. Total supply current for this application
is 1.05mA. Proper safeguards, such as isolation, must be
added to this circuit to protect the patient from possible
harm.
Figure 5. Adding a Simple RC Filter at the Inputs to an
Instrumentation Amplifier is Effective in Reducing Rectification
of High Frequency Out-of-Band Signals
3V
3
8
1
2
+
–
7
LT1168
G = 10
4
–3V
+IN
PATIENT
GND
–IN
PATIENT/CIRCUIT
PROTECTION/ISOLATION
C1
0.01µF
R2
1M
R1
12k
–
1
1/2
LT1112
+
R3
30k
R
G
6k
R4
30k
2
3
AV = 101
POLE AT 1kHz
Figure 6. Nerve Impulse Amplifier
0.3Hz
HIGHPASS
C2
0.47µF
6
R6
5
1M
R8
100Ω
3V
5
6
+
LT1112
–
1/2
–3V
C3
15nF
8
7
4
R7
10k
OUTPUT
1V/mV
1168 F06
13
LT1168
U
WUU
APPLICATIONS INFORMATION
Low IB Favors High Impedance Bridges, Lowers
Dissipation
The LT1168’s low supply current, low supply voltage
operation and low input bias currents allow it to fit nicely
into battery-powered applications. Low overall power
dissipation necessitates using higher impedance bridges.
The single supply pressure monitor application, Figure␣ 7,
shows the LT1168 connected to the differential output of
BI TECHNOLOGIES
(0.02% RATIO MATCH)
7
5
3.5k
3.5k
5V
1
3.5k
G = 200
249Ω
3.5k
3
+
8
LT1168
1
2
–
4
a 3.5k bridge. The picoampere input bias currents keep the
error caused by offset current to a negligible level. The
LT1112 level shifts the LT1168’s reference pin and the
ADC’s analog ground pins above ground. The LT1168’s
and LT1112’s combined power dissipation is still less than
the bridge’s. This circuit’s total supply current is just
2.2mA.
67-8-3 R40KQ
40k
6
20k
+
40k
1/2
LT1112
–
REF
IN
LTC
AGND
ADC
®
1286
DIGITAL
DATA
OUTPUT
U
TYPICAL APPLICATIONS
R5
392k
LT1634CCZ-1.25
2
1
R4
50k
R3
50k
3
2
R8
100k
+
1/2
LT1490
–
Figure 7. Single Supply Pressure Monitor
Single Supply Barometer
V
S
LUCAS NOVA SENOR
1
4
2
6
R7
50k
NPC-1220-015-A-3L
5k
5k
R
7
5k
5k
SET
5
1
–
R2
12Ω
3
+
0.6% ACCURACY AT 25°C
1.7% ACCURACY AT 0°C TO 60°C
= 8V TO 30V
V
S
8
4
R6
1k
5
+
1/2
LT1490
6
–
R1
825Ω
1168 TA05
V
S
–
2
1
8
+
3
LT1168
G = 60
7
6
5
4
VOLTS
2.800
3.000
3.200
TO
4-DIGIT
DVM
INCHES Hg
28.00
30.00
32.00
1168 TA03
14
U
TYPICAL APPLICATIONS
LT1168
AC Coupled Instrumentation Amplifier
392k
LT1634CCZ-1.25
R8
3
+
2
1
1/4
LT1114
2
–
0.6% ACCURACY AT ROOM TEMP
1.7% ACCURACY AT 0°C TO 60°C
VOLTS
INCHES Hg
2.800
3.000
3.200
–IN
+IN
9V
4
11
28.00
30.00
32.00
2
1
R
G
8
3
1
4
R9
1k
2
6
–
LT1168
REF
+
5
1
4-Digit Pressure Sensor
LUCAS NOVA SENOR
NPC-1220-015A-3L
–
5k
5k
R
5k
5k
+
SET
5
6
C1
0.1µF
1/2
LT1124
1
3
825Ω
12Ω
OUTPUT
R1
1M
–
2
=
(2π)(R1)(C1)
= 1.59Hz
9V
7
4
14
1
1168 TA02
5
6
10
9
R5
100k
+
LT1114
–
1/4
R6
50k
C1
1µF
TO
4-DIGIT
DVM
8
R7
180k
1168 TA04
f
2
1
8
3
+
LT1114
–
–3dB
–
LT1168
G = 60
+
1/4
R4
100k
+
3
R1
R2
12
13
R3
51k
PACKAGE DESCRIPTIO
0.300 – 0.325
(7.620 – 8.255)
0.009 – 0.015
(0.229 – 0.381)
+0.035
0.325
–0.015
+0.889
8.255
()
–0.381
*THESE DIMENSIONS DO NOT INCLUDE MOLD FLASH OR PROTRUSIONS.
MOLD FLASH OR PROTRUSIONS SHALL NOT EXCEED 0.010 INCH (0.254mm)
0.065
(1.651)
TYP
U
Dimensions in inches (millimeters) unless otherwise noted.
N8 Package
8-Lead PDIP (Narrow 0.300)
(LTC DWG # 05-08-1510)
0.045 – 0.065
(1.143 – 1.651)
0.100
(2.54)
BSC
0.130 ± 0.005
(3.302 ± 0.127)
0.125
(3.175)
MIN
0.018 ± 0.003
(0.457 ± 0.076)
0.020
(0.508)
MIN
0.255 ± 0.015*
(6.477 ± 0.381)
0.400*
(10.160)
876
1234
MAX
5
N8 1098
15
LT1168
TYPICAL APPLICATIO
Programmable Audio HPF/LPF with “Pop-Less” Switching
R3
8k
314
+15V
8
2
–
1/2 LT1462
3
V
+
IN
–15V
1
4
215
TOTAL SUPPLY CURRENT < 400µA
PACKAGE DESCRIPTIO
U
+15V
7
3
+
R2
4k
P
1
116
LTC201
12 13
+15VNC–15V
P
2
89
5
4
R1
4k
611
710
GAIN SET
C1
100µF
8
1
2
5
6
LT1168
–
–15V
+
1/2 LT1462
–
6
5
4
7
U
Dimensions in inches (millimeters) unless otherwise noted.
HPF
LPF
—010 < 0.8V
P
1
P
0111 > 2.4V
2
POLE 100 200 400Hz
1168 TA06
S8 Package
8-Lead Plastic Small Outline (Narrow 0.150)
0.010 – 0.020
(0.254 – 0.508)
0.008 – 0.010
(0.203 – 0.254)
*
DIMENSION DOES NOT INCLUDE MOLD FLASH. MOLD FLASH
SHALL NOT EXCEED 0.006" (0.152mm) PER SIDE
**
DIMENSION DOES NOT INCLUDE INTERLEAD FLASH. INTERLEAD
FLASH SHALL NOT EXCEED 0.010" (0.254mm) PER SIDE
× 45°
0.016 – 0.050
(0.406 – 1.270)
0.053 – 0.069
(1.346 – 1.752)
0°– 8° TYP
0.014 – 0.019
(0.355 – 0.483)
TYP
(LTC DWG # 05-08-1610)
0.004 – 0.010
(0.101 – 0.254)
0.050
(1.270)
BSC
0.228 – 0.244
(5.791 – 6.197)
0.189 – 0.197*
(4.801 – 5.004)
7
8
1
2
5
6
3
4
RELATED PARTS
PART NUMBERDESCRIPTIONCOMMENTS
LTC1100Precision Chopper-Stabilized Instrumentation AmplifierG = 10 or 100, VOS = 10µV, IB = 50pA
LT1101Precision, Micropower, Single Supply Instrumentation AmplifierG = 10 or 100, IS = 105µA
LT1102High Speed, JFET Instrumentation AmplifierG = 10 or 100, Slew Rate = 30V/µs
LT1167Single Resistor Programmable Precision Instrumentation AmplifierLower Noise than LT1168, eN = 7.5nV/√Hz
0.150 – 0.157**
(3.810 – 3.988)
SO8 1298
16
Linear Technology Corporation
1630 McCarthy Blvd., Milpitas, CA 95035-7417
(408) 432-1900 ● FAX: (408) 434-0507
●
www.linear-tech.com
1168i LT/TP 0300 4K • PRINTED IN USA
LINEAR TECHNOLOGY CORPORATION 1998
Loading...
+ hidden pages
You need points to download manuals.
1 point = 1 manual.
You can buy points or you can get point for every manual you upload.