Omega Products AD590L Installation Manual

User’s Guide
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.
w
2-Terminal IC
Temperature Transducer
FEATURES
Linear current output: 1 µA/K Wide temperature range: −55°C to +150°C Pr
obe-compatible ceramic sensor package 2-terminal device: voltage in/current out Laser trimmed to ±0.5°C calibration accuracy (AD590M) Excellent linearity: ±0.3°C over full range (AD590M) Wide power supply range: 4 V to 30 V
isolation from case
Sensor Low cost
GENERAL DESCRIPTION
e AD590 is a 2-terminal integrated circuit temperature tran
sducer that produces an output current proportional to
absolute temperature. For supply voltages between 4 V and
V, the device acts as a high impedance, constant current
30 regulator passing 1 µA/K. Laser trimming of the chip’s thin-film resistors is used to calibrate the device to 298.2 µA output at 298
.2 K (25°C).
e
AD590 should be used in any temperature-sensing application below 150°C in which conventional electrical temperature sensors are currently employed. e inherent low cost of a monolithic integrated circuit combined with the elimination of support circuitry makes the AD590 an attractive alternative for many temperature measurement situations. Linearization circuitry, precision voltage amplifiers, resistance measuring circuitry, and cold junction compensation are not needed in applying the AD590.
AD590
PIN CONFIGURATIONS
NC
1
2
V+
TOP VIEW
(Not to Scale)
V–
3
4
420-3
3 500
+
Fi
gure 1. 2-Lead CQFP Figure 2. 8-Lead SOIC
+
gure 3. 3-Pin TO-52
Fi
5 2 0-
3 35
0
NC
NC = NO CONNECT
PRODUCT HIGHLIGHTS
1. e AD590 is a calibrated, 2-terminal temperature sensor requiring only a dc voltage supply (4 V to 30 V). Costly transmitters, filters, lead wire compensation, and linearization ci
rcuits are all unnecessary in applying the device.
2. State-of-the-art laser trimming at the wafer level in conjunction with extensive final testing ensures that AD
590 units are easily interchangeable.
NC
8
7
NC
NC
6
5
NC
100
­33500
In addition to temperature measurement, applications include temperature compensation or correction of discrete components, biasing proportional to absolute temperature, flow rate measurement, level detection of fluids and anemometry. e
AD590 is available in chip form, making it suitable for hybrid circuits and fast temperature measurements in protected environments.
e AD590 is particularly useful in remote sensing applications. e
device is insensitive to voltage drops over long lines due to its high impedance current output. Any well-insulated twisted pair is sufficient for operation at hundreds of feet from the receiving circuitry. e output characteristics also make the
easy to multiplex: the current can be switched by a
AD590
3. Superior interface rejection occurs because the output is a current rather than a voltage. In addition, power requirements are low (1.5 mW @ 5 V @ 25°C). ese features make the AD590 easy to apply as a remote sensor.
4. e high output impedance (>10 MΩ) provides excellent rejection of supply voltage dri and ripple. For instance,
ging the power supply from 5 V to 10 V results in only
chan a 1 µA maximum current change, or 1°C equivalent error.
5. e AD590 is electrically durable: it withstands a forward voltage of up to 44 V and a reverse voltage of 20 V. e
refore, supply irregularities or pin reversal does not
damage the device.
CMOS multiplexer, or the supply voltage can be switched by a lo
gic gate output.
AD590
TABLE OF CONTENTS
Features.............................................................................................. 1
Ge
neral Description ......................................................................... 1
Explanation of Temperature Sensor Specifications ..................7
Calibration Error...........................................................................7
Configurations ...........................................................................1
Pin
Product Highlights ........................................................................... 1
Revision History ............................................................................... 2
Specifications..................................................................................... 3
AD590J
AD590L
Absolute Maximum Ratings............................................................ 5
ESD Caution.................................................................................. 5
Ge
Circuit Description....................................................................... 6
and AD590K Specifications ......................................... 3
and AD590M Specifications ....................................... 4
neral Description ......................................................................... 6
Error vs. Temperature: with Calibration Error Trimmed
Out...................................................................................................7
Error vs. Temperature: No User Trims .......................................7
Nonlinearity...................................................................................7
Voltage and ermal Environment Effects ...............................8
General Applications...................................................................... 10
Outline Dimensions....................................................................... 13
Page 2 of 16
AD590
SPECIFICATIONS
AD590J AND AD590K SPECIFICATIONS
25°C and VS = 5 V, unless otherwise noted.
Table 1.
AD590J AD590K Parameter Min Typ Max Min Typ Max Unit
POWER SUPPLY Operating Voltage Range OUTPUT
Nominal Current Output @ 25°C (298.2K) 298.2 298.2 µA Nominal Temperature Coefficient 1 1 µA/K Calibration Error @ 25°C Absolute Error (Over Rated Performance Temperature Range)
Without External Calibration Adjustment With 25°C Calibration Error Set to Zero Nonlinearity For TO-52 and CQFP Packages For 8-Lead SOIC Package Repeatability
Long-Term Drift
2
3
Current Noise 40 40 Power Supply Rejection
4 V ≤ VS ≤ 5 V 0.5 0.5 µA/V 5 V ≤ VS ≤ 15 V 0.2 0.2 µV/V
15 V ≤ VS ≤ 30 V 0.1 0.1 µA/V Case Isolation to Either Lead 10 Effective Shunt Capacitance 100 100 pF Electrical Turn-On Time 20 20 µs Reverse Bias Leakage Current (Reverse Voltage = 10 V)
1
Specifications shown in boldface are tested on all production units at final electrical test. Results from those tests are used to calculate outgoing quality levels. All
minimum
2
Maximum deviation between +25°C readings after temperature cycling between −55°C and +150°C; guaranteed, not tested.
3
Conditions: constant 5 V, constant 125°C; guaranteed, not tested.
4
Leakage current doubles every 10°C.
and maximum specifications are guaranteed, although only those shown in boldface are tested on all production units.
1
4
30
±5.0
±10 ±3.0
±1.5 ±1.5
4
30 V
±2.5
±5.5 ±2.0
±0.8 ±1.0
°C
°C °C
°C
°C ±0.1 ±0.1 °C ±0.1 ±0.1 °C
pA/Hz
10
10
4
10 10 pA
10
Ω
Page 3 of 16
AD590
K°C
AD590L AND AD590M SPECIFICATIONS
25°C and VS = 5 V, unless otherwise noted.
Table 2.
AD590L AD590M Parameter Min Typ Max Min Typ Max Unit
POWER SUPPLY
Operating Voltage Range 4 30 4 30 V
OUTPUT
Nominal Current Output @ 25°C (298.2K) 298.2 298.2 µA Nominal Temperature Coefficient 1 1 µA/K Calibration Error @ 25°C ±1.0 ±0.5 °C Absolute Error (Over Rated Performance Temperature Range) °C
Without External Calibration Adjustment ±3.0 ±1.7 °C With ± 25°C Calibration Error Set to Zero ±1.6 ±1.0 °C Nonlinearity ±0.4 ±0.3 °C Repeatability Long-Term Drift
2
3
Current Noise 40 40 pA/√Hz Power Supply Rejection
4 V ≤ VS ≤ 5 V 0.5 0.5 µA/V 5 V ≤ VS ≤ 15 V 0.2 0.2 µA/V
15 V ≤ VS ≤ 30 V 0.1 0.1 µA/V Case Isolation to Either Lead 10 Effective Shunt Capacitance 100 100 pF Electrical Turn-On Time 20 20 µs Reverse Bias Leakage Current (Reverse Voltage = 10 V)
1
Specifications shown in boldface are tested on all production units at final electrical test. Results from those tests are used to calculate outgoing quality levels. All
minimum and maximum specifications are guaranteed, although only those shown in boldface are tested on all production units.
2
Maximum deviation between +25°C readings after temperature cycling between –55°C and +150°C; guaranteed, not tested.
3
Conditions: constant 5 V, constant 125°C; guaranteed, not tested.
4
Leakage current doubles every 10°C.
1
±0.1 ±0.1 °C ±0.1 ±0.1 °C
10
10
4
10 10 pA
10
Ω
+223°
°
°F
–50
°
–100° +100° +200° +300°
Figure 4. Temperature Scale Conversion Equations
+273°0°+298°
+32° +70° +212°
5 9
9
°F = °C + 32)
5
+25°
(
(
+323°
+50°
32)
+373°
+100°
+ 273.15°C = °F – K = °C
+423°
+150°
2 0 0
­3 3 5 00
+ 459.7R = °F
Page 4 of 16
AD590
ABSOLUTE MAXIMUM RATINGS
Table 3.
Parameter Rating
Forward Voltage ( E+ or E–) 44 V Reverse Voltage (E+ to E–) −20 V Breakdown Voltage (Case E+ or E–) ±200 V Rated Performance Temperature Range Storage Temperature Range Lead Temperature (Soldering, 10 sec) 300°C
1
The AD590 was used at −100°C and +200°C for short periods of
mea
surement with no physical damage to the device. However, the absolute
erro
rs specified apply to only the rated performance temperature range.
1
1
−55°C to +150°C
−65°C to +155°C
ESD CAUTION
ESD (electrostatic discharge) sensitive device. Electrostatic charges as high as 4000 V readily accumulate on the
human body and test equipment and can discharge without detection. Although this product features
proprietary ESD protection circuitry, permanent damage may occur on devices subjected to high energy
ctrostatic discharges. Therefore, proper ESD precautions are recommended to avoid performance
ele
ation or loss of functionality.
degrad
Stresses above those listed under Absolute Maximum Ratings may cause permanent damage to the device. is is a stress rating only and functional operation of the device at these or any other conditions above those indicated in the operational section of this specification is not implied. Exposure to absolute ma
ximum rating conditions for extended periods may affect
device reliability.
Page 5 of 16
AD590
(
GENERAL DESCRIPTION
e AD590H has 60 µ inches of gold plating on its Kovar leads and Kovar header. A resistance welder is used to seal the nickel cap to the header. e AD590 chip is eutectically mounted to the header and ultrasonically bonded to with 1 mil aluminum wire. Kovar composition: 53% iron nominal; 29% ± 1% nickel; 17% ± 1% co
balt; 0.65% manganese max; 0.20% silicon max;
0.10% aluminum max; 0.10% magnesium max; 0.10% zirconium max; 0.10%
e AD590F is
titanium max; and 0.06% carbon max.
a ceramic package with gold plating on its Kovar leads, Kovar lid, and chip cavity. Solder of 80/20 Au/Sn composition is used for the 1.5 mil thick solder ring under the li
d. e chip cavity has a nickel underlay between the metallization and the gold plating. e AD590 chip is eutectically mounted in the chip cavity at 410°C and ultrasonically bonded to with 1 mil aluminum wire. Note that the chip is in direct contact with the cer
amic base, not the metal lid. When using the AD590 in die form, the chip substrate must be kept electrically isolated (floating) for correct circuit operation.
66
MILS
V+
42MILS
PTAT current. In this figure, Q8 and Q11 are the transistors that produce the PTAT voltage. R5 and R6 convert the voltage to current. Q10, whose collector current tracks the collector currents in Q9 and Q11,
supplies all the bias and substrate leakage current for the rest of the circuit, forcing the total current to be PTAT. R5 and R6
are laser-trimmed on the wafer to calibrate the device at 25°C.
Figure 7 shows the typical V–I characteristic of the circuit at 25°C a
nd the temperature extremes.
Figure 6 is the schematic diagram of the AD590.
+
R1
R2
26
0
1040
Q2
Q1
Q7
SUBSTRATE
R6 82
0
Figure 6
Q5 Q3
C1
R3 5k
26pF
R4 11k
Q10Q9
CH
Q6
IP
Q12
R5
146
. Schematic Diagram
Q8
Q4
Q11
40
118
0
­33
500
V–
THE AD590 IS AVAILABLE IN LASER-TRIMMED CHIP FORM; CONSULT THE CHIP CATALOG FOR DETAILS
Fi
gure 5. Metallization Diagram
CIRCUIT DESCRIPTION
1
e AD590 uses a fundamental property of the silicon transistors from which it is made to realize its temperature pro
portional characteristic: if two identical transistors are operated at a constant ratio of collector current densities, r, then the difference in their base-emitter voltage is (kT/q)(In r). Because both k (Boltzman’s constant) and q (the charge of an electron) are constant, the resulting voltage is directly
portional to absolute temperature (PTAT).
pro
In the AD590, this PTAT voltage is converted to a PTAT current by low temperature coefficient thin-film resistors. e total current of the device is then forced to be a multiple of this
423
30 0
­3350
0
) A
298
µ
T U O
I
218
0 1 2
1
For a more detailed description, see M.P. Timko, “A Two-Terminal IC
Temperature Dec.
Transducer,” IEEE J. Solid State Circuits, Vol. SC-11, p. 784-788,
1976. Understanding the Specifications–AD590.
3 4
SUPPLY VOLTAGE (V)
. V–I Plot
Figure 7
+150°C
+25°C
–55°C
5 6 3
50 0-3
3 500
0
Page 6 of 16
AD590
(
V
EXPLANATION OF TEMPERATURE SENSOR SPECIFICAT
e way in which the AD590 is specified makes it easy to apply it in a wide variety of applications. It is important to understand the meaning of the various specifications and the effects of the suppl
y voltage and thermal environment on accuracy.
AD590 is a PTAT1 current regulator. at is, the output
e current is equal to a scale factor times the temperature of the sensor in degrees Kelvin. is scale factor is trimmed to 1 µA/K at the factory, by adjusting the indicated temperature (that is, the output current) to agree with the actual temperature. is is done with 5 V across the device at a temperature within a few de
grees of 25°C (298.2K). e device is then packaged and
tested for accuracy over temperature.
IONS
CALIBRATION ERROR
At final factory test, the difference between the indicated temperature and the actual temperature is called the calibration error. Since this is a scale factory error, its contribution to the total error of the device is PTAT. For example, the effect of the 1°C
specified maximum error of the AD590L varies from 0.73°C at
–55°C
to 1.42°C at 150°C.
calibration error would vary from the ideal over temperature.
)A
I
ACTUAL
µ
T UO
298.2
I
LIBRATION
CA ERROR
Figure 8 shows how an exaggerated
ACTUAL
TRANSFER
FUNCTION
IDEAL
TRANSFER
FUNCTION
+
5
Figur
+
AD590
+
R
0
10
= 1mV/K
V
T
950
e 9. One Temperature Trim
70 0
­3 3 5 0 0
ERROR VS. TEMPERATURE: WITH CALIBRATION ERROR
Each AD590 is tested for error over the temperature range with the calibration error trimmed out. is specification could also be called the variance from PTAT, because it is the maximum di PTAT multiplication of the actual current at 25°C. is error consists of a slope error and some curvature, mostly at the temperature extremes. temperature curve before and aer calibration error trimming.
TRIMMED OUT
fference between the actual current over temperature and a
Figure 10 shows a typical AD590K
2
)C °(
RORR
E
ETUL
0
O SBA
–2
BEFORE CA
LIBRATION
TRIM
CALIBRATION
ERROR
AFTER CA
LIBRATION
TRIM
–55 150
Figur
e 10. Effect to Scale Factor Trim on Accuracy
TEMPERATURE (°C)
8 00-
33 50 0
6 00-
335
298.2
TEMPERATURE (°K)
Figur
e 8. Calibration Error vs. Temperature
00
e calibration error is a primary contributor to the maximum total error in all AD590 grades. However, because it is a scale factor error, it is particularly easy to trim. Figure 9 shows the most elementary way of accomplishing this. To trim this circuit, the temperature of the AD590 is measured by a reference te
mperature sensor and R is trimmed so that V
= 1 mV/K at
T
that temperature. Note that when this error is trimmed out at one temperature, its effect is zero over the entire temperature range. In most applications, there is a current-to-voltage conversion resistor (or, as with a current input ADC, a reference) that can be trimmed for scale factor adjustment.
ERROR VS. TEMPERATURE: NO USER TRIMS
Using the AD590 by simply measuring the current, the total error is the variance from PTAT, described above, plus the effect of the calibration error over temperature. For example, the AD590L ma
3.02°C
ximum total error varies from 2.33°C at –55°C to
at 150°C. For simplicity, only the large figure is shown
on the specification page.
NONLINEARITY
Nonlinearity as it applies to the AD590 is the maximum deviation of current over temperature from a best-fit straight lin
e. e nonlinearity of the AD590 over the −55°C to +150°C range is superior to all conventional electrical temperature sensors such as thermocouples, RTDs, and thermistors. shows the nonlinearity of the typical AD590K from
1
T(°C) = T(K) − 273.2. Zero on the Kelvin scale is absolute zero; there is no
lower temperature.
Figure 11
Figure 10.
Page 7 of 16
AD590
V
R
A
1.6
)C°( RO
0.8
R RE ETULOS
0
0.8°C MAX
B A
–0
.8
.6
–1
5 150
–5
TEMPERATURE (°C)
gure 11. Nonlinearity
Fi
0.8°C MAX
0.8°C MAX
9 00
­3 3 5 00
Figure 12 shows a circuit in which the nonlinearity is the major contributor to error over temperature. e circuit is trimmed by adjusting R1 for a 0 V output with the AD590 at 0°C. R2 is then adjusted for 10 V output with the sensor at 100°C. Other pairs of temperatures can be used with this procedure as long as they are measured accurately by a reference sensor. Note that for 15 V output (150°C), the V+ of the op amp must be greater th
an 17 V. Also, note that V− should be at least −4 V; if V− is
ground, there is no voltage applied across the device.
15
AD581
2
) C°( E
R U T
E
0
P MET
–2
R1
2k
35.7k
27k
V–
e 12. 2-Temperature Trim
Figur
5 0 150100
–5
TEMPERATURE (°C)
Figure 13. Typical 2-Trim Accuracy
97.6k
AD590
R2
5k
30pF
AD707A
100mV/°C
= 100mV/°C
V
T
0 10-
33 500
11 0
­3 3 5 0 0
VOLTAGE AND THERMAL ENVIRONMENT EFFECTS
e power supply rejection specifications show the maximum ex
pected change in output current vs. input voltage changes.
e in
sensitivity of the output to input voltage allows the use of
un
regulated supplies. It also means that hundreds of ohms of resistance (such as a CMOS multiplexer) can be tolerated in series with the device.
It is important to note that using a supply voltage other than 5 V does not change the PTAT nature of the AD590. In other words, this change is equivalent to a calibration error and can be removed by the scale factor trim (see
e AD590
specifications are guaranteed for use in a low thermal resistance environment with 5 V across the sensor. Large changes in the thermal resistance of the sensor’s environment change the amount of self-heating and result in changes in the output, which are predictable but not necessarily desirable.
thermal environment in which the AD590 is used
e
termines two important characteristics: the effect of self-
de heating and the response of the sensor with time. Figure 14 is a model of the AD590 that demonstrates these characteristics.
?
T
JC
J
P
C
CH
e 14. Thermal Circuit Model
Figur
As an example, for the TO-52 package, θJC is the thermal resistance between the chip and the case, about 26°C/W. θ the thermal resistance between the case and the surroundings and is determined by the characteristics of the thermal connection. Power source P represents the power dissipated on the chip. e rise of the junction temperature, T ambient temperature, T
T
TA = P(θJC + θCA) (1)
J
A
, is
Table 4 gives the sum of θJC and θCA for several common thermal media for both the H and F packages. e heat sink use
d was a common clip-on. Using Equation 1, the temperature rise of an AD590 H package in a stirred bath at 25°C, when driven with a 5 V supply, is 0.06°C. However, for the same conditions in still air, the temperature rise is 0.72°C. For a given supply voltage, the temperature rise varies with the current and is PTAT. erefore, if an application circuit is trimmed with the sensor in the same thermal environment in which it is used, the scale factor trim compensates for this effect over the entire temperature range.
Figure 10).
T
?
CA
C
C
C
+
T
A
2 1 0
-33500
CA
, above the
J
is
Page 8 of 16
AD590
Table 4. ermal Resistance
θ
+ θCA
JC
(°C/
Watt)
τ (sec)
1
Medium H F H F
Aluminum Block 30 10 0.6 0.1 Stirred Oil Moving Air
2
3
42 60 1.4 0.6
With Heat Sink 45 5.0 – Without Heat Sink 115 190 13.5 10.0 Still Air With Heat Sink 191 108 – Without Heat Sink 480 650 60 30
1
τ is dependent upon velocity of oil; average of several velocities listed above.
2
Air velocity @ 9 ft/sec.
3
The time constant is defined as the time required to reach 63.2% of an
in
stantaneous temperature change.
e time response of the AD590 to a step change in temperature is determined by the thermal resistances and the thermal capacities of the chip, C about 0.04 Ws/°C for the AD590. C
, and the case, CC. CCH is
CH
varies with the measured
C
medium, because it includes anything that is in direct thermal contact with the case. e single time constant exponential curve of response, T (t). se
Figure 15 is usually sufficient to describe the time
Table 4 shows the effective time constant, τ, for
veral media.
T
FINAL
E RUTAREP
M ET
DESNES
T
INITIAL
T(t) = T
INITIAL
τ
Figur
e 15. Time Response Curve
+ (T
FINAL
TIME
– T
INITIAL
4
τ
) × (1 – e
–t/τ
)
310-33500
Page 9 of 16
AD590
V
A
(
V
+
V
GENERAL APPLICATIONS
Figure 16 demonstrates the use of a low cost digital panel meter for the display of temperature on either the Kelvin, Celsius, or Fahrenheit scales. For Kelvin temperature, Pin 9, Pin 4, and Pin
2 are grounded; for Fahrenheit temperature, Pin 4 and Pin 2
are le open.
5
OFFSET
9
4
2
LIBRATION
CA
GAIN SCALING
OFFSET SCALING
410
-3 3
5 00
D590
+
Figure 16.
6
5
8
AD2040
3
GND
Variable Scale Display
e above configuration yields a 3-digit display with 1°C or 1°F resolution, in addition to an absolute accuracy of ±2.0°C over the −55°C to +125°C temperature range, if a one-temperature
libration is performed on an AD590K, AD590L, or AD590M.
ca
Connecting several AD590 units in series, as shown in
Figure 17, allows the minimum of all the sensed temperatures to be indicated. In contrast, using the sensors in parallel yields the average of the sensed temperatures.
15
+
10
k
0.1%)
AD590
– +
AD590
– +
AD590
+ MIN
V
T
e 17. Series and Parallel Connection
Figur
+
333
(0.1%)
.3
5V
+
+
AD590
+
AVG
V
T
510-335
0 0
e circuit in Figure 18 demonstrates one method by which di
fferential temperature measurements can be made. R1 and R2 can be used to trim the output of the op amp to indicate a desi
red temperature difference. For example, the inherent offset between the two devices can be trimmed in. If V+ and V− are radi
cally different, then the difference in internal dissipation causes a differential internal temperature rise. is effect can be used to measure the ambient thermal resistance seen by the sensors in applications such as fluid-level detectors or anemometry.
+
AD590L
#2
+
AD590L
#1
Figure 19 is an example of a cold junction compensation circuit for a Type J thermocouple using the AD590 to monitor the reference junction temperature. is circuit replaces an ice-bath as
the thermocouple reference for ambient temperatures between 15°C and 35°C. e circuit is calibrated by adjusting R for a proper meter reading with the measuring junction at a known reference temperature and the circuit near 25°C. Using components with the TCs as specified in ac
curacy is within ±0.5°C for circuit temperatures between 15°C
and 35°C. Other thermocouple types can be accommodated with different resistor values. Note that the TCs of the voltage reference and the resistors are the primary contributors to error.
7.5
AD580
+
V
OUT
Figure 19. Cold Junction Compensation Circuit for Type J Thermocouple
V
R3
10
k
R4 k
AD707A
+
R1
R2
k
50
Fi
5M
10
V–
gure 18. Differential Measurements
Figure 19, compensation
REFERENCE
TION
JUNC
+
AD590
C
52.3
8.66k
1k
R
T
U
+
METER
RESISTORS ARE 1%, 50ppm/°C
(T1 – T2) × (10mV/°C)
IRON
+
MEASURING
JUNC
61 0
-33
50 0
CONSTANTAN
TION
T
7 1 0-
3 35
00
Page 10 of 16
AD590
V
4m
m
20m
V
F
V
A
Figure 20 is an example of a current transmitter designed to be used with 40 V, 1 kΩ systems; it uses its full current range of 4 to 20 mA for a narrow span of measured temperatures. In this ex
ample, the 1 µA/K output of the AD590 is amplified to
/°C and offset so that 4 mA is equivalent to 17°C and
1 mA 20 mA is e
quivalent to 33°C. R
is trimmed for proper reading
T
at an intermediate reference temperature. With a suitable choice of resistors, any temperature range within the operating limits of the AD590 can be chosen.
+
+
12
0.01µF
A = 17°C
A = 25°C A = 33°C
AD590
AD581
V
OUT
+
10
k
35.7k
5k
12.7k
10
R
T
30pF
AD707A
+
5k500
8 1 0-
3 3 5
V–
00
Figure 20. 4 to 20 mA Current Transmitter
Figure 21 is an example of a variable temperature control circuit
hermostat) using the AD590. R
(t
gh and low limits for R
hi
SET
and RL are selected to set the
H
. R
could be a simple pot, a
SET
calibrated multiturn pot, or a switched resistive divider. Powering the AD590 from the 10 V reference isolates the AD590 from supply variations while maintaining a reasonable voltage (~7 V) ac
ross it. Capacitor C1 is oen needed to filter extraneous noise
from remote sensors. R
is determined by the β of the power
B
transistor and the current requirements of the load.
+
AD581
V+
OUT
V–
10
V
R
H
AD590
R
SET
R
L
gure 21. Simple Temperature Control Circuit
Fi
+
2
3
+
C1
10
k
7
LM311
4
R
1
GND
HEATING
B
ELEMENTS
91 0
­33500
20p
1.25k
–15V
DAC OUT
BIT 1 BIT 8
BIT 2 BIT 7
BIT 3 BIT 6
BIT 4 BIT 5
6.98k
1k, 15T
+
AD590
–15V
1408/1508
3
LM311
2
–15V
6.8k
MC
+5V +5V
8
1
4
Figure 22. DAC
REF
+5V
1.15k
200, 15T
+5V
+2.5V
200
1k
OUTPUT HIGH­TEMPERATURE ABOVE SETPOINT
7
OUTPUT LOW­TEMPERATURE BELOW SETPOINT
5.1M
Setpoint
AD580
02 0
-33
5 0 0
e voltage compliance and the reverse blocking characteristic of the AD590 allow it to be powered directly from 5 V CMOS
gic. is permits easy multiplexing, switching, or pulsing for
lo min
imum internal heat dissipation. In
Figure 23, any AD590 connected to a logic high passes a signal current through the current measuring circuitry, while those connected to a logic zero pass insignificant current. e outputs used to drive the AD590s can
be employed for other purposes, but the additional
capacitance due to the AD590 should be taken into account.
5
+
D590
CMOS
GATES
+
+
gure 23. AD590 Driven from CMOS Logic
Fi
+
1k (0.1%)
1 2 0-33
5 0
Figure 22 shows that the AD590 can be configured with an 8-bit DAC to produce a digitally controlled setpoint. is particular circuit operates from 0°C (all inputs high) to 51.0°C (all inputs low) in 0.2°C steps. e comparator is shown with 1.0°C hysteresis, which is usually necessary to guard-band for extraneous noise. Omitting the 5.1 MΩ resistor results in no hysteresis.
Page 11 of 16
AD590
V
CMOS analog multiplexers can also be used to switch AD590 current. Due to the AD590’s current mode, the resistance of such
switches is unimportant as long as 4 V is maintained across the transducer. the principle demonstrated in CMOS
multiplexer. e resulting circuit can select 1 to 80
Figure 24 shows a circuit that combines
Figure 23 with an 8-channel
sensors over only 18 wires with a 7-bit binary word.
10
0
3
1
14
2
2
SE
ROW
LECT
11 12 13 10
16
4028
CMOS
-TO-
BCD
DECIMAL
DECODER
8
+
22
e i
nhibit input on the multiplexer turns all sensors off for
min
imum dissipation while idling.
Figure 25 demonstrates a method of multiplexing the AD590 in the 2-trim mode (see
Figure 12 and Figure 13). Additional AD590s and their associated resistors can be added to multiplex up to eight channels of ±0.5°C absolute accuracy over the temperature range of −55°C to +125°C. e high temperature restriction of
+
+
12
125°C is 150°C can
02
due to the output range of the op amps; output to
be achieved by using a 20 V supply for the op amp.
+
+
+
21
+
01
11
+
+
AD590
00
10
20
COLUMN
SELECT
INHIBIT
AD581
+15V
+
9
10
11
6
V
OUT
10V
16
LOGIC LEVEL
INTERFACE
7 8
35.7k
35.7k
2k
2k
BINARY TO 1-OF-8 DECODER
gure 24. Matrix Multiplexer
Fi
5k
97.6k
5k
97.6k
S1
S2
DECODER/
S8
AD7501
+15V
–15V
TTL/DTL TO CMOS
INTERFACE
DR
15
IVER
0131142
27
51 CMOS ANALOG
40
MULTIPLEXER
10k 10mV/°C
V+
AD707A
–15V
k
10mV/°C
22 0-3
35 0
0
+
+
AD590L
–5V TO –15V
AD590L
gure 25. 8-Channel Multiplexer
Fi
EN
BINARY
CHANNEL
SELECT
3 2 0
­3 3 5 00
Page 12 of 16
AD590
OUTLINE DIMENSIONS
0.030 (0.76)
0.019 (0.48)
0.017 (0.43)
0.015 (0.38)
0.055 (1.40)
0.050 (1.27)
0.045 (1.14)
TYP
0.500 (12.69) MIN
0.0065 (0.17)
0.0050 (0.13)
0.0045 (0.12)
Figure 26. 2-Lead Ceramic Flat Package [CQFP]
Dimensions shown in inches and (millimeters)
POSITIVE LEAD INDICATOR
0.240 (6.10)
0.230 (5.84)
0.220 (5.59)
(F-2)
0.210 (5.34)
0.200 (5.08)
0.190 (4.83)
4.00 (0.1574)
3.80 (0.1497)
0.093 (2.36)
0.081 (2.06)
0.050 (1.27)
0.041 (1.04)
0.015 (0.38) TYP
5.00 (0.1968)
4.80 (0.1890)
8 5
6.20 (0.2440)
5.80 (0.2284)
41
0.500 (12.70)
0.150 (3.81)
0.115 (2.92)
)59.4( 591.0
)2
)
)13.5( 902.0
4
5
8
.
.
4
5(
( 87
03
1
2
.
.0
0
0.030 (0.76) MAX
CONTROLLING DIMENSIONS ARE IN INCHES; MILLIMETER DIMENSIONS (IN PARENTHESES) ARE ROUNDED-OFF INCH EQUIVALENTS FOR REFERENCE ONLY AND ARE NOT APPROPRIATE FOR USE IN DESIGN.
MIN
0.250 (6.35) MIN
0.050 (1.27) MAX
0.019 (0.48)
0.016 (0.41)
0.021 (0.53) MAX
BASE & SEATING PLANE
0.100 (2.54)
T.P.
0.050 (1.27) T.P.
2
0.050 (1.27)
T.P.
45° T.P.
0.048 (1.22)
0.028 (0.71)
0.046 (1.17)
0.036 (0.91)
3
1
Figure 27. 3-Pin Metal Header Package [TO-52]
(H-03)
Dimensions shown in inches and (millimeters)
1.27 (0.0500) BSC
0.25 (0.0098)
0.10 (0.0040)
COPLANARITY
0.10
CONTROLLING DIMENSIONS ARE IN MILLIMETERS; INCH DIMENSIONS (IN PARENTHESES) ARE ROUNDED-OFF MILLIMETER EQUIVALENTS FOR REFERENCE ONLY AND ARE NOT APPROPRIATE FOR USE IN DESIGN.
SEATING
PLANE
COMPLIANT TO JEDEC STANDARDS MS-012-AA
Fi
gure 28. 8-Lead Standard Small Outline Package [SOIC]
mensions shown in millimeters and (inches)
Di
1.75 (0.0688)
1.35 (0.0532)
0.51 (0.0201)
0.31 (0.0122)
rrow Body
Na
(R-8)
0.25 (0.0098)
0.17 (0.0067)
0.50 (0.0196)
0.25 (0.0099)
1.27 (0.0500)
0.40 (0.0157)
× 45°
Page 13 of 16
AD590
NOTES:
Page 14 of 16
AD590
NOTES:
Page 15 of 16
AD590
NOTES:
Page 16 of 16
WARRANTY/DISCLAIMER
OMEGA ENGINEERING, INC. warrants this unit to be free of defects in materials and workmanship for a period of 13 months from date of purchase. OMEGA’s WARRANTY adds an additional one (1) month grace period to the normal one (1) year product warranty to cover handling and shipping time. This ensures that OMEGA’s customers receive maximum coverage on each product.
If the unit malfunctions, it must be returned to the factory for evaluation. OMEGA’s Customer Servic Department will issue an Authorized Return (AR) number immediately upon phone or written request Upon examination by OMEGA, if the unit is charge. OMEGA’s WARRANTY does not
found to be defective, it will be repaired or replaced at no
apply to defects resulting from any action of the purchaser, including but not limited to mishandling, improper interfacing, operation outside of design limits, improper repair, having been or current,
or unauthorized modification. This WARRANTY is VOID if the unit shows evidence of
tampered with or shows evidence of having been damaged as a result of excessive corrosion;
heat, moisture or vibration; improper specification; misapplication; misuse or other operating conditions outside of OMEGA’s control. Components in which wear is not warranted, include but are not limited to contact points, fuses, and triacs.
OMEGA is pleased to offer suggestions on the use of its various products. However, OMEGA neither assumes responsibility for any omissions or errors nor assumes liability for any damages that result from the use of its products in accordance with information provided by OMEGA, either verbal or written. OMEGA warrants only that the parts manufactured by the company will be as specified and free of defects. OMEGA MAKES NO OTHER WARRANTIES OR REPRESENTATIONS OF ANY TITLE, AND
ALL IMPLIED WARRANTIES INCLUDING ANY WARRANTY OF MERCHANTABILITY
KIND WHATSOEVER, EXPRESSED OR IMPLIED, EXCEPT THAT OF
AND FITNESS FOR A PARTICULAR PURPOSE ARE HEREBY DISCLAIMED. LIMITATION OF LIABILITY: The remedies of purchaser set forth herein are exclusive, and the total liability of OMEGA with respect to this order, whether based on contract, warranty, negligence, indemnification, strict liability or otherwise, shall not exceed the purchase price of the co mponent upo n whi ch liabilit y is based. In no event shal l OME GA be lia ble for consequential, incidental or special damages.
CONDITIONS: Equipment sold by OMEGA is not intended to be used, nor shall it be used: (1) as a “Basic Component” under 10 CFR 21 (NRC), used in or with any nuclear installation or activity; or (2) in medical applications or used on humans. Should any Product(s) be used in or with any nuclear installation or activity, medical as set forth in our basic WARRANTY/DISCLAIMER language, OMEGA
and hold OMEGA harmless from any liability or damage whatsoever arising out of the use of the
application, used on humans, or misused in any way, OMEGA assumes no responsibility
and, additionally, purchaser will indemnify
Product(s) in such a manner.
e
.
RETURN REQUESTS/INQUIRIES
Direct all warranty and repair requests/inquiries to the OMEGA Customer Service Department. BEFORE RETURNING ANY PRODUCT(S) TO OMEGA, PURCHASER MUST OBTAIN AN AUTHORIZED RETUR (AR) NU M B ER FROM OM E G A’S CUSTOME R S ERV I CE DEPARTME N T ( IN ORDER T O AV OID PROCESSING DELAYS). The assigned AR number should then be marked on the outside of the retur package and on any correspondence.
The purchaser is responsible for shipping charges, freight, insurance and proper packaging to preven breakage in transit.
FOR WARRANT following information available BEFORE contacting OMEGA
1. Purchase Order number under which the produc was PURCHASED,
2. Model and serial number of the product unde warranty, an
3. Repair instructions and/or specific problems relative to the product.
OMEGA’s policy is to make running changes, not model changes, whenever an improvement is possible. This affords our customers the latest in technology and engineering.
OMEGA is a registered trademark of OMEGA ENGINEERING, INC © Copyright 2008 OMEGA ENGINEERING, INC. All rights reserved. This document may not be copied, photocopied,
reproduced, translated, or reduced to any electronic medium or machine-readable form, in whole or in part, without th prior written consent of OMEGA ENGINEERING, INC
Y RETURNS, please have the
:
d
FOR NON-WARRANTY REPAIRS,
consult OMEGA for current repair charges. Have the following information available BEFORE contacting OMEGA
t
1. Purchase Order number to cover the COST
of the repair,
r
2. Model and serial number of the product, an
3. Repair instructions and/or specific problems
.
relative to the product.
.
d
N
n
t
:
e
Where Do I Find Everything I Need for
Process Measurement and Control?
OMEGA…Of Course!
Shop online at omega.com
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