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IXR100

型号:

IXR100

描述:

孤立的,自供电,温度传感器调节的4-20mA两线制变送器[ Isolated, Self-Powered, Temperature Sensor Conditioning 4-20mA TWO-WIRE TRANSMITTER ]

品牌:

BB[ BURR-BROWN CORPORATION ]

页数:

14 页

PDF大小:

107 K

®
IXR100  
Isolated, Self-Powered,  
Temperature Sensor Conditioning  
4-20mA TWO-WIRE TRANSMITTER  
FEATURES  
APPLICATIONS  
1500Vrms ISOLATION  
INDUSTRIAL PROCESS CONTROL:  
All Types of Isolated Transmitters;  
Pt100 RTD  
TRUE TWO-WIRE OPERATION :  
Power and Signal on One Wire Pair  
Thermocouple Inputs  
Current Shunt (mV) Inputs  
RESISTANCE OR VOLTAGE INPUT  
DUAL MATCHED CURRENT SOURCES:  
400µA at 7V  
ISOLATED DUAL CURRENT SOURCES  
AUTOMATED MANUFACTURING  
POWER PLANT/ENERGY MONITORING  
GROUND LOOP ELIMINATION  
WIDE SUPPLY RANGE 12V TO 36V  
PT100 RTD LINEARIZATION  
DESCRIPTION  
The isolated two-wire transmitter allows signal trans-  
mission and device power to be supplied on a single  
wire-pair by modulating the power supply current  
with the isolated signal source. The transmitter is  
resistant to voltage drops from long runs and noise  
from motors, relays, actuators, switches, transformers  
and industrial equipment.  
The IXR100 is an isolated 2-wire transmitter featuring  
loop powered operation and resistive temperature  
sensor conditioning (excitation and linearization).  
It contains a DC/DC convertor, high accuracy instru-  
mentation amplifier with single resistor programmable  
span and linearization, and dual matched excitation  
current sources. This combination is ideally suited  
to a range of transducers such as thermocouples,  
RTDs, thermistors and strain gages. The small size  
makes it ideal for use in head mounted isolated tem-  
perature transmitters as well as rack and rail mounted  
equipment.  
It can be used by OEMs producing isolated transmitter  
modules or by data acquisition system manufacturers.  
The IXR100 is also useful for general purpose isolated  
current transmission where the elimination of ground  
loops is important.  
0.4mA  
Optional  
Offset  
Adjust  
0.4mA  
RO  
Pt100 NONLINEARITY CORRECTION  
USING IXR100  
4
1
2
4-20mA  
28  
+IR  
10  
R
+VIN  
+
11  
IR  
12  
4.4  
OR  
ORO  
VS  
Uncorrected  
6
RS  
RS  
IXR100  
VOUT  
+
RL  
RS  
7
3
18  
Com  
RLIN  
5
9
–VIN  
RLIN  
8
Corrected  
+0.1  
RLIN  
RTD  
RZ  
–0.1  
RCM  
–200  
850  
0.01µF  
Process Temperature (°C)  
International Airport Industrial Park  
Mailing Address: PO Box 11400  
Cable: BBRCORP  
Tucson, AZ 85734  
Street Address: 6730 S. Tucson Blvd.  
Tucson, AZ 85706  
Tel: (520) 746-1111 Twx: 910-952-1111  
Telex: 066-6491  
FAX: (520) 889-1510  
Immediate Product Info: (800) 548-6132  
©1992 Burr-Brown Corporation  
PDS-1141A  
Printed in U.S.A. August, 1993  
SPECIFICATIONS  
ELECTRICAL  
At VS = +24V, TA = +25°C, unless otherwise noted.  
IXR100  
TYP  
PARAMETER  
CONDITIONS  
MIN  
MAX  
UNITS  
OUTPUT AND LOAD CHARACTERISTICS  
Output Current  
Output Current Limit  
Loop Supply Voltage  
Load Resistance  
Linear Operating Region  
4
20  
36  
mA  
mA  
VDC  
32  
11.6  
RLOAD = (VS –11.6)/IO  
ZERO  
Initial Error(1)  
vs Temperature  
VIN = 0, RS = ∞  
300  
200  
µA  
ppm FSR/°C  
SPAN  
Output Current Equation  
Span Equation  
Untrimmed Error  
vs Temperature  
Nonlinearity : EMF Input  
: Pt100 Input  
R
S in , VIN in V  
IO = 4mA + [0.016 + (40/RS)] (VIN  
S = [0.016 + (40/RS)]  
)
A/V  
%
ppm/°C  
%FSR  
%FSR  
(1)  
–2.5  
0
100  
0.025  
Excluding TCR of RS  
50  
0.01  
0.1  
(2)  
(3)  
INPUT  
Voltage Range  
RS = ∞  
1
V
V
mV  
µV/°C  
dB  
Common-Mode Range  
Offset Voltage  
vs Temperature  
vs Supply  
V
IN+, VIN– with Respect to COM  
2
4
2.5  
5
0.5  
3
100  
CURRENT SOURCES  
Magnitude  
Accuracy  
vs Temperature  
Match  
vs Temperature  
0.4  
50  
25  
mA  
%
ppm/°C  
%
1
100  
0.5  
50  
ppm/°C  
DYNAMIC RESPONSE  
Settling Time  
To 0.1% of Span  
500  
ms  
TEMPERATURE RANGE  
Operating  
Storage  
–20  
–40  
+70  
+85  
°C  
°C  
ISOLATION  
Isolation Voltage  
VISO  
VISO  
1000 JP  
1500 KP  
Vrms  
Vrms  
NOTES: (1) Can be adjusted to zero. (2) End point span non-linearity. (3) End point, corrected span non-linearity with a Pt100 RTD input operated from –200°C to  
+850°C.  
ABSOLUTE MAXIMUM RATINGS  
ELECTROSTATIC  
Power Supply (+VS –IOUT) .................................................................. 40V  
DISCHARGE SENSITIVITY  
Input Voltage (Com to VIN) .................................................................... 9V  
Storage Temperature Range ........................................... –40°C to +85°C  
Electrostatic discharge can cause damage ranging from  
Lead Temperature (soldering 10s) ................................................ +300°C  
performance degradation to complete device failure. Burr-  
Output Current Limit Duration ................................................. Continuous  
Power Dissipation ......................................................................... 500mW  
Brown Corporation recommends that this integrated circuit  
be handled and stored using appropriate ESD protection  
methods.  
PACKAGE INFORMATION  
PACKAGE DRAWING  
MODEL  
PACKAGE  
NUMBER(1)  
IXR100  
2-wire Transmitter  
901  
NOTE: (1) For detailed drawing and dimension table, please see end of data  
sheet, or Appendix D of Burr-Brown IC Data Book.  
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.  
®
2
IXR100  
PIN CONFIGURATION  
Top View  
IREF1  
VIN+  
VIN–  
IREF2  
Com  
RS1  
RS2  
RL1  
1
2
3
4
5
6
7
8
9
28 +VS  
27  
26  
25  
24  
23  
22  
21  
20  
19  
*
*
*
*
*
*
*
*
*
RL2  
OS1 10  
OS2 11  
OS3 12  
18 IOUT  
17  
16  
15  
*
*
*
*
*
13  
14  
* = No Pin  
DISCUSSION  
OF PERFORMANCE  
FUNCTIONAL DESCRIPTION  
The IXR100 comprises of several functions:  
• Sensor excitation  
The IXR100 makes the design of isolated two wire 4 to  
20mA transmitters easy and provides exceptional perfor-  
mance at very low cost. It combines several unique features  
not previously available in a single package. These include  
galvanic isolation, sensor excitation and linearization, excel-  
lent DC performance, and low zero and span drift. The  
IXR100 functions with voltages as low as 11.6V at the  
device. This allows operation with power supplies at or  
below 15V. When used with the RCV420 the complete 4 to  
20mA current loop requires only 13.1V. If series diode  
protection is desired the minimum loop supply voltage is  
still only about 13.7V. This is especially useful in systems  
where the available supplies are only 15V.  
• Internal voltage regulator  
• Input amplifier and V/I converter  
• Linearization circuit  
• DC/DC Converter  
SENSOR EXCITATION  
Sensor Excitation consists of two matched 0.4mA current  
sources. One is used to excite the resistive sensor and the  
other is used to excite the zero balance resistor RZ. When the  
linearity correction feature is used these current sources are  
modulated together so that three wire operation of a Pt100  
RTD is possible.  
BASIC CONNECTION  
The basic connection of the IXR100 is shown in Figure 1. A  
differential voltage applied between pins 2 and 3 will cause  
a current of 4 to 20mA to circulate in the two wire output  
loop pins 28 and 18. Pins 1 and 4 supply the current  
excitation for resistive sensors. Pins 6 and 7 are provided for  
the connection of an external span resistor which increases  
the gain. Pins 8 and 9 provide linearity correction. Pins 10,  
11 and 12 adjust the output offset current.  
INTERNAL VOLTAGE REGULATOR  
The circuitry within the IXR100 regulates the supply voltage  
to the DC/DC Converter, Input Amplifier, Linearization  
Amplifier and V/I Converter and removes the normal varia-  
tions in VS from these stages as the output spans from 4 to  
20mA.  
®
3
IXR100  
0.4mA  
0.4mA  
40  
RS  
IO = 4mA + (0.016 +  
) V  
IN  
Optional  
Offset  
Adjust  
VIN = IREF (RTD – RZ)  
RO  
4
1
2
4-20mA  
+IR  
10  
R
+VIN  
+
11  
IR  
12  
OR  
ORO  
VS  
28  
6
RS  
(2)  
RS  
IXR100  
VOUT  
+
RL  
RS  
7
3
18  
Com  
RLIN  
5
9
–VIN  
RLIN  
8
(3)  
RLIN  
(1)  
RTD  
RZ  
NOTES: (1) RZ = RTD resistance at the minimum process temperature.  
40  
(2) RS  
=
Ω.  
0.016/(VIN) – 0.016  
RCM  
(3) RLIN = 500to 1500or if linearization is not required.  
0.01µF  
FIGURE 1. Basic Connection for RTD.  
INPUT AMPLIFIER AND V/I CONVERTER  
DC/DC CONVERTER  
The Input Amplifier is an instrumentation amplifier whose  
gain is set by RS, it drives the V/I Converter to produce a 4  
to 20mA output current. The Input Amplifier has a common  
mode voltage range of 2 to 4V with respect to COM (pin 5).  
Normally this requirement is satisfied by returning the  
currents from the RTD and zero balance resistor RZ to COM  
through a common mode resistor RCM. For most applica-  
tions a single value of 3.9kmay be used. When used with  
RTDs having large values of resistance RCM must be chosen  
so that the inputs of the amplifier remain within its rated  
common mode range. RCM should be bypassed with a  
0.01µF or larger capacitor.  
The DC/DC Converter transfers power from the 2 wire  
current loop across the barrier to the circuitry used on the  
input side of the isolation barrier.  
PIN DESCRIPTIONS  
IREF1, IREF2  
These pins provide a matched pair of current sources for  
sensor excitation. These current sources provide excellent  
thermal tracking, and when the linearization feature is used,  
are modulated by an equal amount. Their nominal current  
value is 0.4mA and their compliance voltage is:  
VIN+ < VIREF < (Com + 7V)  
LINEARIZATION CIRCUIT  
The Linearity Correction Circuit is unique in several ways.  
A single external resistor will provide up to 50 times  
improvement in the basic RTD linearity. Terminal based  
non-linearity can be reduced to less than ±0.1% for all RTD  
temperature spans. The Linearization circuit also contains an  
instrumentation amplifier internally connected to the ±VIN  
pins. The gain of this stage is set by RLIN. The output  
controls the excitation current sources to produce an increas-  
ing excitation current as VIN increases. An important feature  
is that the Linearity Correction is made directly to the RTD  
output independent of the gain of the Input Amplifier. This  
provides minimal interaction between RS and RZ. This  
feature can be useful at the systems level by reducing data  
acquisition system processor overhead previously used to  
linearize sensor response in software/firmware.  
VREF  
IREF = 400µA +  
2RLIN  
+VIN, –VIN  
These are the inputs to both the input amplifier and the  
linearization amplifier. Because the IXR100 has been  
optimized for RTD applications, the two sets of inputs are  
internally connected.  
RS1, RS2  
The resistor connected across these terminals determines the  
gain of the IXR100. For normal 4-20mA outputs:  
40  
RS =  
(1)  
0.016/(VIN) – 0.016  
®
4
IXR100  
RL1, RL2  
The resistor connected between these terminals determines  
the gain of the linearization circuit and the amount of  
correction applied to the RTD. Its value may be determined  
in several ways. Two of which are shown as follows.  
1. Empirically by interactively adjusting RLIN, RS and RZ to  
achieve best fit 4 to 20mA output. RZ is used to set 4mA  
at minimum input, RS is adjusted for 12mA with a half  
span input, and RLIN is adjusted to give 20mA with a full  
span input. This may require a few iterations but is  
probably the most practical method for field calibration.  
RLIN will range between 500and 1500for 100Ω  
sensors (Pt100, D100, SAMA). Initially it may seem a  
little strange adjusting RS for 12mA and RLIN for 20mA.  
However, convergence is achieved much more quickly as  
the linearized curve passes through zero and has less  
effect at the mid span and the linearity trim resistor tends  
to adjust the transfer function more at the full span than  
the mid point.  
IXR100  
11  
(a)  
+
12  
10  
10kΩ  
±400µA adjust range  
2. Using Table I and linear interpolation for values of span  
not given in the table. This will yield very accurate results  
for the Pt100 sensor and acceptable results for D100 and  
SAMA sensors.  
IXR100  
ZERO ADJUST (OPTIONAL) OS1, OS2, OS3  
11  
(b)  
The IXR100 has provision for adjusting the output offset  
current as shown in Figure 2. In many applications the  
already low offset will not need to be known at all. This trim  
effects the V/I converter stage and does not introduce VOS  
drift errors that occur when the trim is performed at the input  
stage. If possible use RZ to trim sensor output error to zero  
and use the offset control to trim the output to 4mA when  
VIN = 0V. The offset adjustment can be made with a  
+
12  
10  
5kΩ  
5kΩ  
±40µA adjust range  
FIGURE 2. Basic Connection for Zero Adjust.  
SPAN T (°C)  
300 400  
995 1083 1131 1152 1159 1159 1154 1140  
TMIN (°C)  
50  
100  
200  
500  
600  
700  
800  
900 1000  
–200  
–150  
–100  
–50  
573  
745  
653  
855  
839  
1059 1158 1197 1206 1205 1196 1175 1151 1127  
983 1105 1228 1251 1249 1231 1207 1182 1156 1129  
1233 1284 1286 1262 1236 1208 1180 1152 1125 1097  
0
50  
100  
150  
1302 1287 1273 1229 1201 1173 1145 1117 1089  
1263 1249 1220 1192 1164 1136 1108 1081 1054  
1225 1211 1183 1155 1127 1100 1073 1046  
1188 1174 1146 1119 1091 1064 1038 1011  
200  
250  
300  
350  
1151 1137 1110 1083 1056 1030 1003  
1114 1101 1074 1048 1021 995  
969  
1079 1066 1039 1013 987  
962  
928  
1044 1031 1005 979  
954  
400  
450  
500  
550  
1009 996  
971  
938  
905  
873  
946  
913  
881  
849  
921  
888  
975  
942  
909  
963  
930  
897  
NOTES:(1)Linearinterpolationbetweentwohorizontal  
orverticalvaluesyieldsacceptablevalues. (2)Although  
not optimum, these values will also yield acceptable  
results with D100 and SAMA 100nominal sensors.  
(3) Double RLIN value for PT200.  
600  
650  
700  
750  
800  
877  
845  
814  
784  
754  
865  
834  
803  
773  
841  
810  
TABLE I. RLIN Values for Pt100 Sensor.  
®
5
IXR100  
potentiometer connected as shown in Figures 2a and 2b. The  
circuit shown in Figure 2a provides more range while the  
circuit in Figure 2b provides better resolution. Note, it is not  
recommended to use this adjusting procedure for zero eleva-  
tion or suppression. See the signal suppression and elevation  
section for the proper techniques.  
the effects of non-uniform fields existing in heterogeneous  
dielectric material during barrier degradation. In the case of  
void non-uniformities, electric field stress begins to ionize  
the void region before bridging the entire high voltage  
barrier.  
The transient conduction of charge during and after the  
ionization can be detected externally as a burst of  
0.01µs-0.1µs current pulses that repeat on each AC voltage  
cycle. The minimum AC barrier voltage that initiates partial  
discharge is defined as the “inception voltage”. Decreasing  
the barrier voltage to a lower level is required before partial  
discharge ceases and is defined as the “extinction voltage”.  
COM  
This is the return for the two excitation currents IREF1 and  
IREF2 and is the reference point for the inputs.  
VS, IOUT  
We have designed and characterized the package to yield an  
inception voltage in excess of 2400Vrms so that transient  
overvoltages below this level will not cause any damage.  
The extinction voltage is above 1500Vrms so that even  
overvoltage-induced partial discharge will cease once the  
barrier voltage is reduced to the rated level. Older high  
voltage test methods relied on applying a large enough  
overvoltage (above rating) to catastrophically break down  
marginal parts, but not so high as to damage good ones. Our  
new partial discharge testing gives us more confidence in  
barrier reliability than breakdown/no breakdown criteria.  
These are the connections for the current loop VS being the  
most positive connection. For correct operation these pins  
should have 11.6 to 36V between them.  
HIGH VOLTAGE TESTING  
Burr-Brown Corporation has adopted a partial discharge test  
criterion that conforms to the German VDE0884 Optocoupler  
Standards. This method requires the measurement of minute  
current pulses (< 5pC) while applying 2400rms, 60Hz high-  
voltage stress across every devices isolation barrier. No  
partial discharge may be initiated to pass this test. This  
criterion confirms transient overvoltage (1.6 x VRATED  
)
APPLYING THE IXR100  
protection without damage. Life-test results verify the ab-  
sence of failure under continuous rated voltage and maxi-  
mum temperature.  
The IXR100 has been designed primarily to correct  
nonlinearities inherent in RTD sensors. It may also be used  
in other applications where its excellent performance makes  
it superior to other devices available. Examples are shown in  
the Applications Section.  
This new test method represents the “state-of-the-art” for  
nondestructive high voltage reliability testing. It is based on  
Optional Input  
Filtering  
0.4mA  
0.4mA  
1
(1)  
R1  
4
3
7
TRANZORB  
28  
1N4148  
VS  
C1  
RS  
IXR100  
CBYPASS  
VOUT  
+
6
2
RL  
18  
R2(1)  
5
+
9
CBYPASS  
8
RLIN  
CBYPASS  
0.01µF  
RZ  
RTD  
= Transmitter Case  
3.9kΩ  
NOTE: (1) R1 and R2 should be made equal if used (±1% resistors are adequate).  
FIGURE 3. Transient and RFI Protection Circuit.  
®
6
IXR100  
RFI AND TRANSIENT SUPPRESSION  
INPUT BANDWIDTH LIMITING  
Radio frequency interference and transients are a common  
occurrence in 4-20mA loops, especially when long wiring  
lengths are involved. RFI usually appears as a temporary  
change in output and results from rectification of the radio  
signal by one or more stages in the amplifier. For sensors  
which are closely coupled to the IXR100 and are contained  
in a common metal housing, the usual entry for RFI is via the  
4-20mA loop wiring. Coaxial bypass capacitors may be used  
with great effectiveness to bring these leads into the trans-  
ducer housing while suppressing the RFI. Values of 100 to  
1000pF are generally recommended. For sensors remote  
from the IXR100, coaxial capacitors can also be used to  
filter the excitation and signal leads. Additional low-pass  
filtering at the IXR100 input helps suppress RFI. The easiest  
way to do this is with the optional differential RC filter  
shown in Figure 4. Typical values for R1 and R2 are  
100-1000, and for C1 are 100-1000pF.  
Filtering at the input to the IXR100 is recommended where  
possible and can be done as shown in Figure 4. C1 connected  
to pins 3 and 4 will reduce the bandwidth with a f–3dB  
frequency given by:  
f–3dB = 0.159/(R1 + R2 + RTD + RZ) (C1 + 3pF)  
This method has the disadvantage of having f–3dB vary with  
R1, R2, RTD, and RZ may require large values of R1, and R2.  
R1 and R2 should be matched to prevent zero errors due to  
input bias current.  
SIGNAL SUPPRESSION AND ELEVATION  
In some applications it is desired to have suppressed zero  
range (span elevation) or elevated zero range (span suppres-  
sion). This is easily accomplished with the IXR100 by using  
the current sources to create the suppression/elevation  
voltage. The basic concept is shown in Figure 5. In this  
example the sensor voltage is derived from RT (a thermistor,  
RTD or other variable resistance element) excited by one of  
the 0.4mA current sources. The other current source is used  
to create the elevated zero range voltage. Figures 6a, 6b, 6c  
and 6d show some of the possible circuit variations. These  
circuits have the desirable feature of noninteractive span and  
suppression/elevation adjustments.  
Transient suppression for negative voltages can be provided  
by the reverse-polarity protection diodes discussed later.  
However, positive transients cannot be handled by these  
diodes and do frequently occur in field-mounted loops. A  
shunt zener diode is of some help, but most zener diodes  
suffer from limited current-handling capacity and slow turn-  
on. Both of these characteristics can lead to device failure  
before the zener conducts. One type of zener, called the  
TRANZORB and available from General Semiconductor  
Industries, is especially effective in protecting against high-  
energy transients such as those induced by lightning or  
motor contactors. Choose a TRANZORB with a voltage  
rating close to, but exceeding, the maximum VS which the  
IXR100 will see. In combination, the coaxial bypass capaci-  
tors and TRANZORB provide a very high level of protec-  
tion against transients and RFI.  
NOTE: Use of the optional offset null (pins 10, 11, and 12)  
for elevation or suppression is not recommended. This trim  
technique is used only to trim the IXR100’s output offset  
current.  
MAJOR POINTS TO CONSIDER  
WHEN USING THE IXR100  
1. The leads to RS and RLIN should be kept as short as  
possible to reduce noise pick-up and parasitic resistance.  
If the linearity correction feature is not desired, the RLIN  
pins are left open.  
2. +VS should be bypassed with a 0.01µF capacitor as close  
to the unit as possible (pins 18 to 28).  
0.4mA  
0.4mA  
1
R1(1)  
4
3
7
3. Always keep the input voltages within their range of  
linear operation, +2V to +4V (±VIN measured with  
respect to pin 5).  
20  
RS  
C1  
IXR100  
Span Adjust  
6
2
15  
(1)  
R2  
5
+
9
10  
Elevated  
Zero  
Suppressed  
8
Zero  
RLIN  
Range  
5
0
Range  
0.01µF  
RZ  
RTD  
3.9kΩ  
+
0
NOTE: (1) R1 and R2 should be made equal if used.  
VIN  
Figure 4. Optional Bandwidth-Limiting Circuitry.  
Figure 5. Elevation and Suppression Graph.  
®
7
IXR100  
0.4mA  
0.4mA  
0.4 mA  
0.4mA  
VIN  
+
VIN  
+
+
+
e'2  
RT  
+
V4  
R4  
e'2  
RT  
+
V4  
R4  
0.8mA  
0.8mA  
V
IN = (e'2 +V4)  
VIN = (e'2 –V4)  
V4 = 0.4mA X R4  
e'2 = 0.4mA X RT  
V4 = 0.4mA X R4  
e'2 = 0.4mA X RT  
(b) Suppressed Zero Range  
(a) Elevated Zero Range  
0.8mA  
VIN  
+
0.8mA  
e'2  
VIN  
+
+
+
V4  
R4  
+
+
V4  
R4  
e'2  
0.8mA  
0.8mA  
VIN = (e'2 –V4)  
V
IN = (e'2 +V4)  
V4 = 0.8mA X R4  
V4 = 0.8mA X R4  
(c) Elevated Zero Range  
(d) Suppressed Zero Range  
FIGURE 6. Elevation and Suppression Circuits.  
4. The maximum input signal level (VIN) is 1V with RS  
important if the receiving equipment has particularly low  
resistance or uses higher voltage supplies. In general, the  
series diode is recommended unless 12V operation is  
necessary. In either case a 1N4148 diode is suitable.  
open and is less as RS decreases in value.  
5. Always return the current references to COM (pin 5)  
through an appropriate value of RCM to keep VCM within  
its operating range. Also, operate the current sources  
within their rated compliance voltage:  
8. Use a layout which minimizes parasitic inductance and  
capacitance, especially in high gain.  
VIN + ≤ VIREF (Com + 7V)  
RECOMMENDED HANDLING  
PROCEDURES FOR INTEGRATED CIRCUITS  
6. Always choose RL, (including line resistance) so that the  
voltage between pins 18 and 28 (+VS) remains within the  
11.6V to 36V range as the output changes between 4mA  
and 20mA.  
All semiconductor devices are vulnerable, in varying  
degrees, to damage from the discharge of electrostatic  
energy. Such damage can cause performance degradation or  
failure, either immediate or latent. As a general practice, we  
recommend the following handling procedures to reduce the  
risk of electrostatic damage.  
7. It is recommended that a reverse polarity protection diode  
be used. This will prevent damage to the IXR100 caused  
by a transient or long-term reverse bias between pins 18  
and 28. This diode can be connected in either of the two  
positions shown in Figure 7, but each connection has its  
trade-off. The series-connected diode will add to the  
minimum voltage at which the IXR100 will operate but  
offers loop and device protection against both reverse  
connections and transients. The reverse-biased diode in  
parallel with the IXR100 preserves 11.6V minimum  
operation and offers device protection, but could allow  
excessive current flow in the receiving instrument if the  
field leads are accidently reversed. This is particularly  
1. Remove static-generating materials, such as untreated  
plastic, from all areas where microcircuits are handled.  
2. Ground all operators, equipment, and work stations.  
3. Transport and ship microcircuits, or products incorporat-  
ing microcircuits, in static-free, shielded containers.  
4. Connect together all leads of each device by means of a  
conductive material, when the device is not connected  
into a circuit.  
®
8
IXR100  
5. Control relative humidity to as high a value as practical  
(50% recommended).  
equally, so that use of the linearity correction does not affect  
the cancellation. This action is true so long as the three wires  
are of the same length and gauge. Because most RTD leads  
are twisted and bundled, this requirement is usually met with  
no difficulty. Care must be taken that intermediate connec-  
tions such as screw terminals do not violate this assumption  
by introducing unequal line resistances.  
RTD APPLICATIONS  
The IXR100 has been designed with RTD applications  
specifically in mind. The following information provides  
additional information for those applications.  
RTD ZERO ELEVATION AND SUPPRESSION  
The IXR100 may be operated in zero-elevated and zero-  
suppressed ranges by simply offsetting RZ. It may also be  
used in increase-decrease applications by interchanging the  
physical locations of the RTD and RZ as shown in Figure 8.  
Use the same values of RZ, RLIN and RS. Again, because the  
current sources are matched and are modulated equally, this  
connection has no effect on IXR100 performance, especially  
in three-wire applications.  
TWO- AND THREE-WIRE CONNECTIONS  
The IXR100 performs well with two-wire and three-wire  
RTD connections commonly encountered in industrial moni-  
toring and control.  
In two-wire applications, the voltage drop between the RTD  
and the IXR100 can be nulled by proper adjustment of RZ,  
but care must be taken that this voltage drop does not vary  
with ambient conditions. Such variation will appear as an  
apparent variation in the RTD resistance and therefore as a  
change in measured temperature. Also, the linearity correc-  
tion will interpret this change as a variation and attempt to  
linearize both the actual RTD signal and the resistance  
changes in the signal lines. For these reasons, the line  
resistance between the RTD and the IXR100 should be  
minimized by keeping line lengths short and/or using large-  
gauge wires. This limitation does not apply for three-wire  
connections.  
OPEN CIRCUIT DETECTION  
In some applications of the IXR100, the RTD will be located  
remotely. In these cases, it is possible for open circuits to  
develop. The IXR100 responds in the following manner to  
breaks in each lead. The following connections refer to the  
RTD connections shown in Figure 7.  
(1)  
TERMINAL OPEN  
IOUT  
1
2
3
32mA  
3.6mA  
32mA  
In three-wire applications, shown in Figure 7, the RTD and  
RZ lead arrangements set up a pseudo-Kelvin connection to  
the RTD. This occurs because the currents through the three  
wires are set up in opposing directions and cancel IR drops  
in the RTD leads. The current sources are both modulated  
NOTE: (1) Approximate value.  
1
3
7
4
D1  
+VS  
28  
1N4148  
4-20mA  
VOUT  
VIN  
+
0.4mA  
0.4mA  
RS  
IXR100  
6
2
+
RL  
18  
5
+
9
8
1
RLIN  
RZ  
2
RTD  
RCM = 3.9kΩ  
3
Three-wire Connection  
0.01µF  
FIGURE 7. Basic 3-Wire RTD Connection for Increase-Increase Action.  
9
®
IXR100  
1
3
7
4
D1  
+VS  
28  
1N4148  
4-20mA  
VOUT  
VIN  
+
0.4mA  
0.4mA  
RS  
IXR100  
6
2
+
RL  
18  
5
+
9
8
1
RLIN  
RZ  
2
RTD  
RCM = 3.9kΩ  
3
Three-wire Connection  
0.01µF  
FIGURE 8. Basic 3-Wire RTD Connection for Increase-Decrease Action.  
From Equation (1), RS = 48.5. Span adjustment (calibra-  
tion) is accomplished by trimming RS.  
OTHER APPLICATIONS  
In instances where the linearization capability of the IXR100  
is not required, it can still provide improved performance in  
several applications. Its small size, wide compliance  
voltage, low zero and span drift, high PSRR, high CMRR  
and excellent linearity makes the IXR100 ideal for a variety  
of other isolated two-wire transmitter applications. It can be  
used by OEMs producing different types of isolated trans-  
ducer transmitter modules and by data acquisition systems  
manufacturers who gather transducer data. Current mode  
transmission greatly reduces noise interference. The two-  
wire nature of the device allows economical signal condi-  
tioning at the transducer. Thus, the IXR100 is, in general,  
very suitable for a wide variety of applications. Some  
examples, including an isolated non-linearized Pt100 case,  
follow.  
In order to make the lower range limit of 25°C correspond  
to the output lower range limit at 4mA, the input circuitry  
shown in Figure 9 is used. VIN must be 0V at 25°C and RZ  
is chosen to be equal to the RTD resistance at 25°C, or  
109.73. Computing RCM and checking CMV:  
At +25°C, VIN+ = 43.9mV  
At +150°C, VIN+ = 62.9mV  
Since both VIN+ and VZ are small relative to the desired 2V  
common-mode voltage, they may be ignored in computing  
RCM as long as the CMV is met.  
RCM = 3V/0.8mA = 3.75kΩ  
VIN+ min = 3V + 0.0439V  
VIN+ max = 3V + 0.0629V  
VIN– = 3V + 0.0439V  
EXAMPLE 1  
Pt100 RTD without linearization shown in Figure 9.  
EXAMPLE 2  
Given a process with temperature limits of +25°C and  
+150°C, configure the IXR100 to measure the temperature  
with a Pt100 RTD which produces 109.73at 25°C and  
157.31at 150°C (obtained from standard RTD tables).  
Transmit 4mA for +25°C and 20mA for +150°C. The  
change in resistance of the RTD is 47.6. When excited  
with a 0.4mA current source VIN is 0.4mA x 47.6=  
19mV.  
Thermocouple shown in Figure 10.  
Given a process with temperature (Tl) limits of 0°C and  
+1000°C, configure the IXR100 to measure the temperature  
with a Type J thermocouple that produces a 58mV change  
for 1000°C change. Use a semiconductor diode for a cold  
junction compensation to make the measurement relative to  
0°C. This is accomplished by supplying a compensating  
voltage, equal to that normally produced by the thermo-  
couple with its “cold junction” (T2) at ambient. At +25°C  
this is 1.28mV (from thermocouple tables with reference  
junction at 0°C). Typically, at T2 = +25°C, VD = 0.6V and  
40  
RS =  
(1)  
0.016/(VIN) – 0.016  
®
10  
IXR100  
VD/T = –2mV/°C. R5 and R6 form a voltage divider for  
the diode voltage VD. The divider values are selected so that  
the gradient VD/T equals the gradient of the thermo-  
couple at the reference temperature. At +25°C this is  
approximately –52µV/°C (obtained from standard thermo-  
couple table); therefore,  
VD(25°C) = 600mV  
VIN(25°C) = 600mV (100/3740) = 16.0mV  
VIN = VIN+ – VIN– = VTC + V4 – VIN–  
With VIN = 0 and VTC = –1.28mV,  
V4 = VIN+ – VTC  
VTC/T = (VD/T)(R6/(R5 + R6))  
(2)  
V4 = 16.0mV – (–1.28mV)  
0.4mA (R4) = 17.28mV  
–52µV/°C = (–2000µV/°C)(R6/(R5+R6))  
R5 is chosen as 3.74kto be much larger than the resistance  
of the diode. Solving for R6 yields 100.  
R4 = 43.2Ω  
Transmit 4mA for Tl = 0°C and 20mA for Tl = +1000°C.  
Note: VlN = VIN+ – VIN– indicates that Tl is relative to T2.  
The input full scale span is 58mV. RS is found from  
Equation (1) and equals 153.9.  
THERMOCOUPLE BURN-OUT INDICATION  
In process control applications it is desirable to detect when  
a thermocouple has burned out. This is typically done by  
forcing the two-wire transmitter current to the upper or  
lower limit when the thermocouple impedance goes very  
high. The circuits of Figures 10, 11 and 12 inherently have  
down scale indication. When the impedance of the thermo-  
couple gets very large (open) the bias current flowing into  
the + input (large impedance) will cause IO to go to its lower  
range limit value (about 3.6mA). If up scale indication is  
desired, the circuit of Figure 13 should be used. When the TC  
opens, the output will go to its upper range limit value (about  
32mA or higher).  
R4 is chosen to make the output 4mA at TTC = 0°C (VTC  
1.28mV) and TD = 25°C (VD = 0.6V).  
=
VTC will be –1.28mV when TTC = 0°C and the reference  
junction is at +25°C. V4 must be computed for TD = +25°C  
to make VIN = 0V.  
1
3
7
4
D1  
0.4mA 0.4mA  
+VS  
28  
1N4148  
4-20mA  
VIN  
+
RS  
IXR100  
VOUT  
6
2
+
RL  
18  
5
+
RZ  
RTD  
RCM  
0.01µF  
FIGURE 9. Pt100 RTD Without Linearization.  
®
11  
IXR100  
0.4mA  
0.4mA  
R5  
1
3.74kΩ  
1N4148  
4
3
+
+VS  
VD  
28  
7
+
VIN–  
RS  
IXR100  
R6  
100Ω  
153.9Ω  
6
18  
Thermocouple  
TTC  
2
5
+
IOUT  
+
+
0.01µF  
VTC  
VIN+  
+
V
4
R4  
43.2Ω  
3.9kΩ  
Temperature T2 = TD  
Temperature T1  
FIGURE 10. Thermocouple Input Circuit with Two Temperature Regions and Diode (D) Cold Junction Compensation.  
0.4mA  
0.4mA  
This circuit has down  
scale burn-out indication.  
3.9kΩ  
1
4
3
7
D1  
Type J  
+
+VS  
28  
1N4148  
4-20mA  
VOUT  
Zero Adjust  
RS  
100Ω  
IXR100  
50Ω  
6
2
+
RL  
18  
5
+
3.9kΩ  
0.01µF  
FIGURE 11. Thermocouple Input with Diode Cold Junction Compensation and Down Scale Burn-out Indication.  
®
12  
IXR100  
This circuit has down  
scale burn-out indication.  
0.4mA  
Type J  
0.4mA  
1
4
3
7
D1  
+VS  
28  
1N4148  
+
4-20mA  
VOUT  
RTD  
100Ω  
50Ω  
RS  
IXR100  
51Ω  
Zero  
Adjust  
6
2
+
RL  
18  
5
+
3.9kΩ  
0.01µF  
FIGURE 12. Thermocouple Input with RTD Cold Junction Compensation and Down Scale Burn-out Indication.  
This circuit has up  
scale burn-out indication.  
Type J  
0.4mA  
0.4mA  
1
4
+
D1  
3
7
+VS  
28  
1N4148  
4-20mA  
VOUT  
51Ω  
50Ω  
RS  
IXR100  
RTD  
100Ω  
Zero  
Adjust  
6
2
+
RL  
18  
5
+
Zero  
3.9kΩ  
0.01µF  
FIGURE 13. Thermocouple Input with RTD Cold Junction Compensation and Up Scale Burn-out Indication.  
RLIN  
14V to 38V  
1
4
8
1N4148  
2
7
9
+
+VS  
16  
28  
0.4mA  
0.4mA  
1µF  
+
RS  
IXR100  
10  
11  
3
2
6
3
12  
18  
15  
5
RCV420  
VOUT  
0 - 5V  
14  
RTD  
RZ  
13  
3.9kΩ  
5
4
1µF  
+
0.01µF  
–VS  
FIGURE 14. Isolated 4-20mA Instrument Loop.  
®
13  
IXR100  
+VS  
REF200  
100µA  
–V  
S
1
4
IR  
2
OPA177  
V
IN  
R3  
19.5kΩ  
VS  
IXR100  
IIN  
4-20mA  
0.01µF  
400Ω  
R1  
R2  
100Ω  
3
IO  
0-20mA  
COM  
R
R1  
IO = IIN(I + 2 ) + IR(R1 + R2 + R3)/R1 = 1.25IIN – 5mA(1)  
NOTE: (1) Other conversions are readily achievable by changing the  
R1, R2, and R3 ratios (see Burr-Brown Application Bulletin AB-031).  
FIGURE 15. 4-20mA to 0-20mA Output Converter.  
®
14  
IXR100  
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