The XTR106 is a low cost, monolithic 4-20mA, twowire current transmitter designed for bridge sensors. It
provides complete bridge excitation (2.5V or 5V reference), instrumentation amplifier, sensor linearization,
and current output circuitry. Current for powering additional external input circuitry is available from the
V
pin.
REG
The instrumentation amplifier can be used over a wide
range of gain, accommodating a variety of input signal
types and sensors. Total unadjusted error of the complete current transmitter, including the linearized bridge,
is low enough to permit use without adjustment in many
applications. The XTR106 operates on loop power supply voltages down to 7.5V.
Linearization circuitry provides second-order correction
to the transfer function by controlling bridge excitation
voltage. It provides up to a 20:1 improvement in
nonlinearity, even with low cost transducers.
The XTR106 is available in 14-pin plastic DIP and
SO-14 surface-mount packages and is specified for the
–40°C to +85°C temperature range. Operation is from
–55°C to +125°C.
APPLICATIONS
● PRESSURE BRIDGE TRANSMITTER
● STRAIN GAGE TRANSMITTER
● TEMPERATURE BRIDGE TRANSMITTER
● INDUSTRIAL PROCESS CONTROL
● SCADA REMOTE DATA ACQUISITION
● REMOTE TRANSDUCERS
● WEIGHING SYSTEMS
● ACCELEROMETERS
2.0
1.5
1.0
0.5
Nonlinearity (%)
–0.5
5V
0
0mV
BRIDGE NONLINEARITY CORRECTION
V
5
REF
R
V
REF
+
G
USING XTR106
5mV
Bridge Output
(5.1V)
V
REG
2.5V
XTR106
Corrected
R
LIN
7.5V to 36V
Uncorrected
Bridge Output
4-20mA
10mV
V
PS
V
O
R
L
–
I
RET
International Airport Industrial Park • Mailing Address: PO Box 11400, Tucson, AZ 85734 • Street Address: 6730 S. Tucson Blvd., Tucson, AZ 85706 • Tel: (520) 746-1111 • Twx: 910-952-1111
✻ Specification same as XTR106P, XTR106U.
NOTES: (1) Describes accuracy of the 4mA low-scale offset current. Does not include input amplifier effects. Can be trimmed to zero. (2) Does not include initial
error or TCR of gain-setting resistor, R
measured with respect to I
®
pin. (6) See “Linearization” text for detailed explanation. VFS = full-scale VIN.
RET
. (3) Increasing the full-scale input range improves nonlinearity. (4) Does not include Zero Output initial error. (5) Voltage
G
XTR106
IO = VIN • (40/RG) + 4mA, VIN in Volts, RG in Ω
A
242830✻✻✻ mA
0.02✻µA/V
0.035✻µAp-p
S = 40/R
G
✻A/V
±10±50✻±100µV/V
1.13.5✻✻V
525✻50nA
±0.2±3✻±10nA
0.1 || 1✻GΩ || pF
0.6✻µVp-p
5.1✻V
See Typical Curves✻mA
R
= K
LIN
4B
• , K
LIN
1 – 2B
in Ω, B is nonlinearity relative to V
LIN
FS
Ω
FS
FS
2
Page 3
PIN CONFIGURATION
Top ViewDIP and SOIC
1
V
REG
–
2
V
IN
3
R
G
4
R
G
+
5
V
IN
6
I
RET
7
I
O
14
13
12
11
10
9
8
V
5
REF
2.5
V
REF
Lin Polarity
R
LIN
V+
B (Base)
E (Emitter)
ABSOLUTE MAXIMUM RATINGS
Power Supply, V+ (referenced to IO pin) .......................................... 40V
Input Voltage, V
Storage Temperature Range ........................................ –55°C to +125°C
Lead Temperature (soldering, 10s).............................................. +300 °C
Output Current Limit ............................................................... Continuous
Junction Temperature................................................................... +165 °C
NOTE: (1) Stresses above these ratings may cause permanent damage.
Exposure to absolute maximum conditions for extended periods may degrade
device reliability.
+
–
, VIN (referenced to I
IN
(1)
pin) ......................... 0V to V+
RET
ELECTROSTATIC
DISCHARGE SENSITIVITY
This integrated circuit can be damaged by ESD. Burr-Brown
recommends that all integrated circuits be handled with
appropriate precautions. Failure to observe proper handling
and installation procedures can cause damage.
ESD damage can range from subtle performance degradation
to complete device failure. Precision integrated circuits may
be more susceptible to damage because very small parametric
changes could cause the device not to meet its published
specifications.
PACKAGE/ORDERING INFORMATION
PACKAGESPECIFIED
DRAWINGTEMPERATUREPACKAGEORDERINGTRANSPORT
PRODUCTPACKAGENUMBER
XTR106P14-Pin DIP010–40°C to +85°CXTR106PXTR106PRails
XTR106PA14-Pin DIP010–40°C to +85°CXTR106PAXTR106PARails
XTR106USO-14 Surface Mount235–40°C to +85°CXTR106UXTR106URails
(1)
RANGEMARKINGNUMBER
"""""XTR106U/2K5Tape and Reel
XTR106UASO-14 Surface Mount235–40°C to +85°CXTR106UAXTR106UARails
"""""XTR106UA/2K5Tape and Reel
NOTES: (1) For detailed drawing and dimension table, please see end of data sheet, or Appendix C of Burr-Brown IC Data Book. (2) Models with a slash (/ ) are
available only in Tape and Reel in the quantities indicated (e.g., /2K5 indicates 2500 devices per reel). Ordering 2500 pieces of “XTR106U/2K5” will get a single
2500-piece Tape and Reel. For detailed Tape and Reel mechanical information, refer to Appendix B of Burr-Brown IC Data Book.
(2)
MEDIA
The information provided herein is believed to be reliable; however, BURR-BROWN assumes no responsibility for inaccuracies or omissions. BURR-BROWN assumes
no responsibility for the use of this information, and all use of such information shall be entirely at the user’s own risk. Prices and specifications are subject to change
without notice. No patent rights or licenses to any of the circuits described herein are implied or granted to any third party. BURR-BROWN does not authorize or warrant
any BURR-BROWN product for use in life support devices and/or systems.
3
XTR106
®
Page 4
FUNCTIONAL DIAGRAM
Lin
Polarity
V
REG
12
R
LIN
11
1
V+
10
14
V
5
REF
13
2.5
V
REF
5
+
V
IN
4
REF
Amp
Bandgap
V
REF
100µA
Lin
Amp
Current
Direction
Switch
5.1V
B
9
R
G
975
3
V
2
–
V
IN
I = 100µA +
IN
R
G
25
Ω
Ω
E
8
®
XTR106
6
I
RET
7
= 4mA + V
I
O
• ( )
IN
40
R
G
4
Page 5
TYPICAL PERFORMANCE CURVES
101k10010k100k1M
Frequency (Hz)
POWER SUPPLY REJECTION vs FREQUENCY
160
140
120
100
80
60
40
20
0
Power Supply Rejection (dB)
RG = 1kΩ
C
OUT
= 0
RG = 50Ω
At TA = +25°C, V+ = 24V, unless otherwise noted.
60
RG = 50Ω
50
40
30
RG = 1kΩ
C
C
OUT
C
OUT
connected
C
OUT
between V+ and I
20
TRANSCONDUCTANCE vs FREQUENCY
10
Transconductance (20 log mA/V)
R
= 250Ω
L
0
1001k10k100k1M
Frequency (Hz)
COMMON-MODE REJECTION vs FREQUENCY
110
100
90
80
70
RG = 1kΩ
RG = 50Ω
60
50
Common-Mode Rejection (dB)
40
30
101k10010k100k1M
Frequency (Hz)
= 0.01µF
= 0.01µF
OUT
= 0.033µF
STEP RESPONSE
C
= 0.01µF
RG = 1kΩ
OUT
20mA
O
RG = 50Ω
4mA/div
4mA
50µs/div
INPUT OFFSET VOLTAGE DRIFT
90
PRODUCTION DISTRIBUTION
80
70
60
50
40
30
Percent of Units (%)
20
10
0
0
0.25
0.5
0.75
1.0
Offset Voltage Drift (µV/°C)
INPUT OFFSET VOLTAGE CHANGE
Typical production
distribution of
packaged units.
1.5
1.0
0.5
vs V
REG
VOS vs I
and V
CURRENTS
REF
REG
0
(µV)
–0.5
OS
∆ V
–1.0
–1.5
VOS vs I
REF
–2.0
–2.5
–1.0–0.500.51.01.52.02.5
1.25
1.5
1.75
2.0
2.25
2.5
2.75
3.0
5
Current (mA)
®
XTR106
Page 6
TYPICAL PERFORMANCE CURVES (CONT)
At TA = +25°C, V+ = 24V, unless otherwise noted.
2.5
UNDER-SCALE CURRENT vs TEMPERATURE
2.0
1.5
1.0
Under-Scale Current (mA)
0.5
V+ = 7.5V to 36V
0
–75–50–250255075100
Temperature (°C)
OVER-SCALE CURRENT vs TEMPERATURE
30
With External Transistor
29
28
V+ = 36V
27
26
Over-Scale Current (mA)
25
V+ = 24V
V+ = 7.5V
24
–75–50–250255075100
Temperature (°C)
125
125
4.0
UNDER-SCALE CURRENT vs I
REF
3.5
T
3.0
= –55°C
A
2.5
2.0
TA = +25°C
1.5
1.0
Under-Scale Current (mA)
TA = +125°C
0.5
0
00.51.01.52.02.5
+ I
REG
(mA)
I
REF
ZERO OUTPUT ERROR
3.0
REF
and V
CURRENTS
REG
vs V
2.5
2.0
I
ZERO
Error vs I
1.5
1.0
0.5
0
Zero Output Error (µA)
I
ZERO
Error vs I
–0.5
–1.0
–1–0.500.51.01.52.0
Current (mA)
+ I
REG
REG
REF
2.5
ZERO OUTPUT CURRENT ERROR
vs TEMPERATURE
4
2
0
–2
–4
–6
–8
Zero Output Current Error (µA)
–10
–12
–75–50–250255075100
Temperature (°C)
®
XTR106
125
ZERO OUTPUT DRIFT
70
60
PRODUCTION DISTRIBUTION
Typical production
distribution of
packaged units.
50
40
30
20
Percent of Units (%)
10
0
0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.05
0.15
0.25
0.35
0.45
0.55
0.65
0.75
0.85
0.9
Zero Output Drift (µA/°C)
6
Page 7
TYPICAL PERFORMANCE CURVES (CONT)
101001k10k100k1M
Frequency (Hz)
REFERENCE AC LINE REJECTION vs FREQUENCY
120
100
80
60
40
20
0
Line Rejection (dB)
V
REF
2.5
V
REF
5
At TA = +25°C, V+ = 24V, unless otherwise noted.
INPUT VOLTAGE, INPUT CURRENT, and ZERO
OUTPUT CURRENT NOISE DENSITY vs FREQUENCY
10k
Zero Output Noise
1k
Input Current Noise
100
Input Voltage Noise (nV/√Hz)
10
Input Voltage Noise
1101001k10k
Frequency (Hz)
V
5.6
OUTPUT VOLTAGE vs V
REG
OUTPUT CURRENT
REG
5.5
5.4
5.3
5.2
5.1
Output Current (V)
REG
5.0
V
4.9
TA = +125°C
TA = +25°C, –55°C
4.8
–1.0–0.500.51.01.52.02.5
Output Current (mA)
V
REG
100k
10k
1k
100
10
Input Current Noise (fA/√Hz)
10
8
6
4
2
0
Input Bias and Offset Current (nA)
Zero Output Current Noise (pA/√Hz)
–2
–75–50–250255075100125
REFERENCE TRANSIENT RESPONSE
50mV/div
500µA/div
INPUT BIAS and OFFSET CURRENT
vs TEMPERATURE
I
B
I
OS
Temperature (°C)
= 5V
V
REF
10µs/div
Output
Reference
1mA
0
V
5 vs V
REF
5.008
5.004
5.000
5 (V)
REF
V
4.996
4.992
4.988
–1.0–0.500.51.01.52.02.5
V
OUTPUT CURRENT
REG
T
= +25°C
A
T
= +125°C
A
T
= –55°C
A
Current (mA)
REG
®
7
XTR106
Page 8
TYPICAL PERFORMANCE CURVES (CONT)
–75–50–250255075100125
Temperature (°C)
REFERENCE VOLTAGE DEVIATION
vs TEMPERATURE
0.1
0
–0.1
–0.2
–0.3
–0.4
–0.5
Reference Voltage Deviation (%)
V
REF
= 5V
V
REF
= 2.5V
At TA = +25°C, V+ = 24V, unless otherwise noted.
REFERENCE VOLTAGE DRIFT
40
35
30
25
20
15
Percent of Units (%)
10
5
0
02468
PRODUCTION DISTRIBUTION
Typical production
distribution of
packaged units.
101214161820222426283032343638
Reference Voltage Drift (ppm/°C)
40
®
XTR106
8
Page 9
APPLICATIONS INFORMATION
Figure 1 shows the basic connection diagram for the XTR106.
The loop power supply, VPS, provides power for all circuitry. Output loop current is measured as a voltage across
the series load resistor, RL. A 0.01µF to 0.03µF supply
bypass capacitor connected between V+ and IO is recommended. For applications where fault and/or overload conditions might saturate the inputs, a 0.03µF capacitor is
recommended.
A 2.5V or 5V reference is available to excite a bridge sensor.
For 5V excitation, pin 14 (V
bridge as shown in Figure 1. For 2.5V excitation, connect
pin 13 (V
terminals of the bridge are connected to the instrumentation
amplifier inputs, VIN and VIN. A 0.01µF capacitor is shown
2.5) to pin 14 as shown in Figure 3b. The output
REF
+–
connected between the inputs and is recommended for high
impedance bridges (> 10kΩ). The resistor RG sets the gain
of the instrumentation amplifier as required by the full-scale
bridge voltage, VFS.
Lin Polarity and R
provide second-order linearization
LIN
correction to the bridge, achieving up to a 20:1 improvement
in linearity. Connections to Lin Polarity (pin 12) determine
the polarity of nonlinearity correction and should be connected either to I
nected to V
R
is chosen according to the equation in Figure 1 and is
LIN
REG
dependent on K
or V
RET
even if linearity correction is not desired.
(linearization constant) and the bridge’s
LIN
nonlinearity relative to VFS (see “Linearization” section).
5) should be connected to the
REF
. Lin Polarity should be con-
REG
The transfer function for the complete current transmitter is:
IO = 4mA + VIN • (40/RG)(1)
VIN in Volts, RG in Ohms
where VIN is the differential input voltage. As evident from
the transfer function, if no RG is used (RG = ∞), the gain is
zero and the output is simply the XTR106’s zero current.
A negative input voltage, VIN, will cause the output current
to be less than 4mA. Increasingly negative VIN will cause the
output current to limit at approximately 1.6mA. If current is
being sourced from the reference and/or V
, the current
REG
limit value may increase. Refer to the Typical Performance
Curves, “Under-Scale Current vs I
REF
+ I
REG
” and “Under-
Scale Current vs Temperature.”
Increasingly positive input voltage (greater than the full-
scale input, VFS) will produce increasing output current
according to the transfer function, up to the output current
limit of approximately 28mA. Refer to the Typical Performance Curve, “Over-Scale Current vs Temperature.”
The I
references and V
is the reference point for V
references. The I
pin is the return path for all current from the
RET
. I
REG
RET
also serves as a local ground and
RET
and the on-board voltage
REG
pin allows any current used in external
circuitry to be sensed by the XTR106 and to be included in
the output current without causing error. The input voltage
range of the XTR106 is referred to this pin.
5V
(5)
R
(5)
R
2
NOTES:
(1) Connect Lin Polarity (pin 12) to I
bridge nonlinearity or connect to V
nonlinearity. The R
V
section and Figure 3.
(2) Recommended for bridge impedances > 10kΩ
( 3)
1
Bridge
Sensor
if linearity correction is not desired. Refer to “Linearization”
REG
= K
LIN
•
R
LIN
R
+–
B
RET
pin and Lin Polarity pin must be connected to
LIN
4B
1 – 2B
REG
(K
For 2.5V excitation, connect
pin 13 to pin 14
V
5
REF
5
V
C
IN
(2)
0.01µF
(pin 6) to correct for positive
(pin 1) for negative bridge
in Ω)
LIN
4
R
(4)
R
G
3
R
V
2
PACKAGE
4-20 mA
R
L
(see text).
1
TO-225
TO-220
TO-220
I
O
V
FS
O
+
V
PS
–
V
REG
V
2.5
REF
14
13
XTR106
6
11
R
LIN
V
(1)
Lin
Polarity
12
or
(4)
(5) R
accuracy of the bridge. See “Bridge Balance” text.
+
IN
G
G
–
IN
I
RET
(3)
R
LIN
7.5V to 36V
10
V+
9
B
Q
1
E
8
I
O
7
I = 4mA + V
O
(1)
= (VFS/400µA) •
G
where K
and R2 form bridge trim circuit to compensate for the initial
1
IN
= 9.905kΩ for 2.5V reference
LIN
= 6.645kΩ for 5V reference
K
LIN
B is the bridge nonlinearity relative to V
VFS is the full-scale input voltage
REG
V
1
REG
R
Possible choices for Q
C
OUT
0.01µF
40
• ( )
R
G
1 + 2B
1 – 2B
TYPE
2N4922
TIP29C
TIP31C
(V
FS
in V)
FIGURE 1. Basic Bridge Measurement Circuit with Linearization.
9
®
XTR106
Page 10
EXTERNAL TRANSISTOR
External pass transistor, Q1, conducts the majority of the
signal-dependent 4-20mA loop current. Using an external
transistor isolates the majority of the power dissipation from
the precision input and reference circuitry of the XTR106,
maintaining excellent accuracy.
Since the external transistor is inside a feedback loop its
characteristics are not critical. Requirements are: V
CEO
= 45V
min, β = 40 min and PD = 800mW. Power dissipation requirements may be lower if the loop power supply voltage is less
than 36V. Some possible choices for Q1 are listed in Figure 1.
The XTR106 can be operated without an external pass
transistor. Accuracy, however, will be somewhat degraded
due to the internal power dissipation. Operation without Q
is not recommended for extended temperature ranges. A
resistor (R = 3.3kΩ) connected between the I
pin and the
RET
E (emitter) pin may be needed for operation below 0°C
without Q1 to guarantee the full 20mA full-scale output,
especially with V+ near 7.5V.
The low operating voltage (7.5V) of the XTR106 allows
operation directly from personal computer power supplies
(12V ±5%). When used with the RCV420 Current Loop
Receiver (Figure 8), load resistor voltage drop is limited to 3V.
BRIDGE BALANCE
Figure 1 shows a bridge trim circuit (R1, R2). This adjustment can be used to compensate for the initial accuracy of
the bridge and/or to trim the offset voltage of the XTR106.
The values of R1 and R2 depend on the impedance of the
bridge, and the trim range required. This trim circuit places
an additional load on the V
load on V
Performance Curve, “Under-Scale Current vs I
1
The effective load of the trim circuit is nearly equal to R2.
does not affect zero output. See the Typical
REF
output. Be sure the additional
REF
An approximate value for R1 can be calculated:
5V • R
R1≈
4 • V
B
TRIM
where, RB is the resistance of the bridge.
V
is the desired ±voltage trim range (in V).
TRIM
Make R2 equal or lower in value to R1.
REF
+ I
REG
.”
(3)
10
V+
8
E
I
RET
XTR106
6
R
= 3.3kΩ
Q
I
O
7
0.01µF
For operation without external
transistor, connect a 3.3kΩ
resistor between pin 6 and
pin 8. See text for discussion
of performance.
FIGURE 2. Operation without External Transistor.
LOOP POWER SUPPLY
The voltage applied to the XTR106, V+, is measured with
respect to the IO connection, pin 7. V+ can range from 7.5V
to 36V. The loop supply voltage, VPS, will differ from the
voltage applied to the XTR106 according to the voltage drop
on the current sensing resistor, RL (plus any other voltage
drop in the line).
If a low loop supply voltage is used, RL (including the loop
wiring resistance) must be made a relatively low value to
assure that V+ remains 7.5V or greater for the maximum
loop current of 20mA:
RLmax =
(V+)–7.5V
20mA
–R
WIRING
(2)
It is recommended to design for V+ equal or greater than
7.5V with loop currents up to 30mA to allow for out-ofrange input conditions. V+ must be at least 8V if 5V sensor
excitation is used and if correcting for bridge nonlinearity
greater than +3%.
®
XTR106
LINEARIZATION
Many bridge sensors are inherently nonlinear. With the
addition of one external resistor, it is possible to compensate
for parabolic nonlinearity resulting in up to 20:1 improvement over an uncompensated bridge output.
Linearity correction is accomplished by varying the bridge
excitation voltage. Signal-dependent variation of the bridge
excitation voltage adds a second-order term to the overall
transfer function (including the bridge). This can be tailored
to correct for bridge sensor nonlinearity.
Either positive or negative bridge non-linearity errors can be
compensated by proper connection of the Lin Polarity pin.
To correct for positive bridge nonlinearity (upward bowing),
Lin Polarity (pin 12) should be connected to I
shown in Figure 3a. This causes V
to increase with bridge
REF
(pin 6) as
RET
output which compensates for a positive bow in the bridge
response. To correct negative nonlinearity (downward bowing), connect Lin Polarity to V
3b. This causes V
to decrease with bridge output. The Lin
REF
(pin 1) as shown in Figure
REG
Polarity pin is a high impedance node.
If no linearity correction is desired, both the R
Polarity pins should be connected to V
REG
LIN
(Figure 3c). This
results in a constant reference voltage independent of input
signal. R
or Lin Polarity pins should not be left open
LIN
or connected to another potential.
R
is the external linearization resistor and is connected
LIN
between pin 11 and pin 1 (V
3b. To determine the value of R
) as shown in Figures 3a and
REG
, the nonlinearity of the
LIN
bridge sensor with constant excitation voltage must be
known. The XTR106’s linearity circuitry can only compensate for the parabolic-shaped portions of a sensor’s
nonlinearity. Optimum correction occurs when maximum
deviation from linear output occurs at mid-scale (see Figure
4). Sensors with nonlinearity curves similar to that shown in
10
and Lin
Page 11
Figure 4, but not peaking exactly at mid-scale can be
substantially improved. A sensor with a “S-shaped”
nonlinearity curve (equal positive and negative nonlinearity)
cannot be improved with the XTR106’s correction circuitry.
The value of R
in Figure 3. R
K
, which differs for the 2.5V reference and 5V reference.
LIN
is chosen according to Equation 4 shown
LIN
is dependent on a linearization factor,
LIN
The sensor’s nonlinearity term, B (relative to full scale), is
positive or negative depending on the direction of the bow.
V
REG
V
5
REF
5V
R
R
2
1
+–
3a. Connection for Positive Bridge Nonlinearity, V
V
2.5
REF
2.5V
R
R
2
1
+–
3b. Connection for Negative Bridge Nonlinearity, V
V
5
REF
5V
R
R
2
1
+–
3c. Connection if no linearity correction is desired, V
5
4
R
G
3
2
V
REF
5
4
R
G
3
2
I
RET
5
4
R
G
3
2
I
RET
V
2.5
REF
14
13
+
XTR106
–
6
I
RET
= 5V
REF
V
5
14
13
+
XTR106
–
6
= 2.5V
REF
V
V
2.5
REF
14
13
+
XTR106
–
6
= 5V
REF
1
Lin
12
Polarity
REG
1
Lin
12
Polarity
REG
1
Lin
12
Polarity
R
LIN
11
R
LIN
11
R
LIN
11
A maximum ±5% non-linearity can be corrected when the
5V reference is used. Sensor nonlinearity of +5%/–2.5% can
be corrected with 2.5V excitation. The trim circuit shown in
Figure 3d can be used for bridges with unknown bridge
nonlinearity polarity.
Gain is affected by the varying excitation voltage used to
correct bridge nonlinearity. The corrected value of the gain
resistor is calculated from Equation 5 given in Figure 3.
XTR106
V
Lin
Polarity
I
RET
6
R
X
100kΩ
Open RX for negative bridge nonlinearity
for positive bridge nonlinearity
Open R
Y
3d. On-Board Resistor Circuit for Unknown Bridge Nonlinearity Polarity
EQUATIONS
Linearization Resistor:
R
= K
LIN
4B
•
LIN
1– 2B
Gain-Set Resistor:
V
1 + 2B
FS
RG=
400µA
•
1– 2B
Adjusted Excitation Voltage at Full-Scale Output:
V
where, K
= V
REF ( Adj)
REF (Initial)
is the linearization factor (in Ω)
LIN
K
= 9905Ω for the 2.5V reference
LIN
K
= 6645Ω for the 5V reference
LIN
B is the sensor nonlinearity relative to V
(for –2.5% nonlinearity, B = –0.025)
V
is the full-scale bridge output without
FS
linearization (in V)
•
1 + 2B
1– 2B
Example:
Calculate R
2.5% downward bow nonlinearity relative to V
if the input common-mode range is valid.
V
REF
For a 2.5% downward bow, B = –0.025
(Lin Polarity pin connected to V
For V
R
LIN
RG=
VCM=
which falls within the 1.1V to 3.5V input common-mode range.
and the resulting RG for a bridge sensor with
LIN
= 2.5V and VFS = 50mV
= 2.5V, K
REF
(9905Ω) (4)(–0.025)
=
1– (2) (–0.025)
0.05 V
400µA
V
REF ( Adj)
2
= 9905Ω
LIN
1 + ( 2) ( –0. 025)
•
1 – ( 2 ) ( –0. 025 )
1
=
• 2. 5 V •
2
REG
1
12
R
Y
15kΩ
(in Ω)
(in Ω)
(in V)
)
REG
= 943Ω
= 113 Ω
1 + (2 ) ( –0 . 025)
1 – ( 2 ) ( –0. 025 )
FS
and determine
FS
= 1.13V
(4)
(5)
(6)
FIGURE 3. Connections and Equations to Correct Positive and Negative Bridge Nonlinearity.
11
®
XTR106
Page 12
When using linearity correction, care should be taken to
insure that the sensor’s output common-mode voltage remains within the XTR106’s allowable input range of 1.1V to
3.5V. Equation 6 in Figure 3 can be used to calculate the
XTR106’s new excitation voltage. The common-mode voltage of the bridge output is simply half this value if no
common-mode resistor is used (refer to the example in
Figure 3). Exceeding the common-mode range may yield
unpredicatable results.
For high precision applications (errors < 1%), a two-step
calibration process can be employed. First, the nonlinearity
of the sensor bridge is measured with the initial gain resistor
and R
the resulting sensor nonlinearity, B, values for RG and R
LIN
= 0 (R
pin connected directly to V
LIN
REG
). Using
LIN
are calculated using Equations 4 and 5 from Figure 3. A
second calibration measurement is then taken to adjust RG to
account for the offsets and mismatches in the linearization.
UNDER-SCALE CURRENT
The total current being drawn from the V
REF
and V
REG
voltage sources, as well as temperature, affect the XTR106’s
under-scale current value (see the Typical Performance
Curve, “Under-Scale Current vs I
REF
+ I
). This should be
REG
considered when choosing the bridge resistance and excitation voltage, especially for transducers operating over a
wide temperature range (see the Typical Performance Curve,
“Under-Scale Current vs Temperature”).
LOW IMPEDANCE BRIDGES
The XTR106’s two available excitation voltages (2.5V and
5V) allow the use of a wide variety of bridge values. Bridge
impedances as low as 1kΩ can be used without any additional circuitry. Lower impedance bridges can be used with
the XTR106 by adding a series resistance to limit excitation
current to ≤ 2.5mA (Figure 5). Resistance should be added
Shown connected to correct positive
bridge nonlinearity. For negative bridge
nonlinearity, see Figure 3b.
12
Page 13
to the upper and lower sides of the bridge to keep the bridge
output within the 1.1V to 3.5V common-mode input range.
Bridge output is reduced so a preamplifier as shown may be
needed to reduce offset voltage and drift.
OTHER SENSOR TYPES
The XTR106 can be used with a wide variety of inputs. Its
high input impedance instrumentation amplifier is versatile
and can be configured for differential input voltages from
millivolts to a maximum of 2.4V full scale. The linear range
of the inputs is from 1.1V to 3.5V, referenced to the I
RET
terminal, pin 6. The linearization feature of the XTR106 can
be used with any sensor whose output is ratiometric with an
excitation voltage.
SAMPLE ERROR CALCULATION
ERROR ANALYSIS
Table I shows how to calculate the effect various error
sources have on circuit accuracy. A sample error calculation
for a typical bridge sensor measurement circuit is shown
(5kΩ bridge, V
= 5V, VFS = 50mV) is provided. The
REF
results reveal the XTR106’s excellent accuracy, in this case
1.2% unadjusted. Adjusting gain and offset errors improves
circuit accuracy to 0.33%. Note that these are worst-case
errors; guaranteed maximum values were used in the calculations and all errors were assumed to be positive (additive).
The XTR106 achieves performance which is difficult to
obtain with discrete circuitry and requires less board space.
Bridge Impedance (RB)5kΩFull Scale Input (VFS)50mV
Ambient Temperature Range (∆T
Supply Voltage Change (∆V+)5VCommon-Mode Voltage Change (∆CM)25mV (= V
NOTE (1): All errors are min/max and referred to input, unless otherwise stated.
TOTAL ERROR:118033340
1.18% 0.33%
TABLE I. Error Calculation.
13
®
XTR106
Page 14
REVERSE-VOLTAGE PROTECTION
The XTR106’s low compliance rating (7.5V) permits the
use of various voltage protection methods without compromising operating range. Figure 6 shows a diode bridge
circuit which allows normal operation even when the voltage connection lines are reversed. The bridge causes a two
diode drop (approximately 1.4V) loss in loop supply voltage. This results in a compliance voltage of approximately
9V—satisfactory for most applications. A diode can be
inserted in series with the loop supply voltage and the V+
pin as shown in Figure 8 to protect against reverse output
connection lines with only a 0.7V loss in loop supply
voltage.
OVER-VOLTAGE SURGE PROTECTION
Remote connections to current transmitters can sometimes be
subjected to voltage surges. It is prudent to limit the maximum
surge voltage applied to the XTR106 to as low as practical.
Various zener diode and surge clamping diodes are specially
designed for this purpose. Select a clamp diode with as low a
voltage rating as possible for best protection. For example, a
36V protection diode will assure proper transmitter operation
at normal loop voltages, yet will provide an appropriate level
of protection against voltage surges. Characterization tests on
three production lots showed no damage to the XTR106 with
loop supply voltages up to 65V.
Most surge protection zener diodes have a diode characteristic in the forward direction that will conduct excessive
current, possibly damaging receiving-side circuitry if the
loop connections are reversed. If a surge protection diode is
used, a series diode or diode bridge should be used for
protection against reversed connections.
RADIO FREQUENCY INTERFERENCE
The long wire lengths of current loops invite radio frequency interference. RF can be rectified by the sensitive
input circuitry of the XTR106 causing errors. This generally
appears as an unstable output current that varies with the
position of loop supply or input wiring.
If the bridge sensor is remotely located, the interference may
enter at the input terminals. For integrated transmitter assemblies with short connection to the sensor, the interference more likely comes from the current loop connections.
Bypass capacitors on the input reduce or eliminate this input
interference. Connect these bypass capacitors to the I
RET
terminal as shown in Figure 6. Although the dc voltage at
the I
terminal is not equal to 0V (at the loop supply, VPS)
RET
this circuit point can be considered the transmitter’s “ground.”
The 0.01µF capacitor connected between V+ and IO may
help minimize output interference.
V
5
5V
R
+–
B
Bridge
Sensor
REF
R
G
0.01µF0.01µF
V
2.5
REF
14
5
4
3
2
13
+
V
IN
R
G
XTR106
R
G
–
V
IN
I
RET
6
10
V+
9
B
E
8
I
O
7
NOTE: (1) Zener Diode 36V: 1N4753A or Motorola
P6KE39A. Use lower voltage zener diodes with loop
power supply voltages less than 30V for increased
protection. See “Over-Voltage Surge Protection.”
0.01µF
Q
1
FIGURE 6. Reverse Voltage Operation and Over-Voltage Surge Protection.
R
L
must be
PS
V
PS
Maximum V
less than minimum
voltage rating of zener
diode.
(1)
D
1
1N4148
Diodes
The diode bridge causes
a 1.4V loss in loop supply
voltage.