AD592
REV.
–6–
V
T
AVG
(1mV/K)
AD592
+5V
333.3
(0.1%)
V
T
AVG
(10mV/K)
10k
(0.1%)
+15V
AD592
AD592
AD592
Figure 9. Average and Minimum Temperature
Connections
The circuit of Figure 10 demonstrates a method in which a
voltage output can be derived in a differential temperature
measurement.
R1
50k
10k
AD741
V
OUT
= (T
1
– T
2
) x
(10mV/
o
C)
10k
5M
–V
+V
AD592
AD592
Figure 10. Differential Measurements
R1 can be used to trim out the inherent offset between the two
devices. By increasing the gain resistor (10 k) temperature
measurements can be made with higher resolution. If the magni-
tude of V+ and V– is not the same, the difference in power con-
sumption between the two devices can cause a differential
self-heating error.
Cold junction compensation (CJC) used in thermocouple signal
conditioning can be implemented using an AD592 in the circuit
configuration of Figure 11. Expensive simulated ice baths or
hard to trim, inaccurate bridge circuits are no longer required.
AD OP07E
REFERENCE
JUNCTION
100k
10k
V
OUT
+7.5V
MEASURING
JUNCTION
1k
AD592
R
THERMOCOUPLE
TYPE
APPROX.
R VALUE
J
K
T
E
S
R
52
41
41
61
6
6
2.5V
AD1403
R
G1
R
G2
(1k)
Cu
Cu
Figure 11. Thermocouple Cold Junction Compensation
Response of the AD592 output to abrupt changes in ambient
temperature can be modeled by a single time constant
τ
expo-
nential function. Figure 8 shows typical response time plots for
several media of interest.
PERCENT OF FINAL TEMPERATURE
TIME – sec
100
80
60
50
40
30
20
10
90
70
A
B
C
D
E
F
0 20 40 60 80 100 120 140 160 180 200 220 240 260 280 300
A ALUMINUM BLOCK
B FLUORINERT LIQUID
C MOVING AIR (WITH HEAT SINK)
D MOVING AIR (WITHOUT HEAT SINK)
E STILL AIR (WITH HEAT SINK)
F STILL AIR (WITHOUT HEAT SINK)
Figure 8. Thermal Response Curves
The time constant, τ, is dependent on θ
JA
and the thermal ca-
pacities of the chip and the package. Table I lists the effective τ
(time to reach 63.2% of the final value) for several different
media. Copper printed circuit board connections where ne-
glected in the analysis, however, they will sink or conduct heat
directly through the AD592’s solder dipped Kovar leads. When
faster response is required a thermally conductive grease or glue
between the AD592 and the surface temperature being mea-
sured should be used. In free air applications a clip-on heat sink
will decrease output stabilization time by 10-20%.
MOUNTING CONSIDERATIONS
If the AD592 is thermally attached and properly protected, it
can be used in any temperature measuring situation where the
maximum range of temperatures encountered is between –25°C
and +105°C. Because plastic IC packaging technology is em-
ployed, excessive mechanical stress must be safeguarded against
when fastening the device with a clamp or screw-on heat tab.
Thermally conductive epoxy or glue is recommended under
typical mounting conditions. In wet or corrosive environments,
any electrically isolated metal or ceramic well can be used to
shield the AD592. Condensation at cold temperatures can cause
leakage current related errors and should be avoided by sealing
the device in nonconductive epoxy paint or dips.
APPLICATIONS
Connecting several AD592 devices in parallel adds the currents
through them and produces a reading proportional to the aver-
age temperature. Series AD592s will indicate the lowest tem-
perature because the coldest device limits the series current
flowing through the sensors. Both of these circuits are depicted
in Figure 9.
B
AD592
REV.
–7–
The circuit shown can be optimized for any ambient tempera-
ture range or thermocouple type by simply selecting the correct
value for the scaling resistor – R. The AD592 output (1 µA/K)
times R should approximate the line best fit to the thermocouple
curve (slope in V/°C) over the most likely ambient temperature
range. Additionally, the output sensitivity can be chosen by
selecting the resistors R
G1
and R
G2
for the desired noninverting
gain. The offset adjustment shown simply references the AD592
to °C. Note that the TC’s of the reference and the resistors are
the primary contributors to error. Temperature rejection of 40
to 1 can be easily achieved using the above technique.
Although the AD592 offers a noise immune current output, it is
not compatible with process control/industrial automation cur-
rent loop standards. Figure 12 is an example of a temperature to
4–20 mA transmitter for use with 40 V, 1 k systems.
In this circuit the 1 µA/K output of the AD592 is amplified to
1 mA/°C and offset so that 4 mA is equivalent to 17°C and
20 mA is equivalent to 33°C. Rt is trimmed for proper reading
at an intermediate reference temperature. With a suitable choice
of resistors, any temperature range within the operating limits of
the AD592 may be chosen.
AD592
AD581
35.7k
10mV/
o
C
10k
12.7k
5k 500
+20V
–20V
V
T
10
C
R
T
5k
1mA/
o
C
208
17°C 4mA
33°C 20µA
Figure 12. Temperature to 4–20 mA Current Transmitter
Reading temperature with an AD592 in a microprocessor based
system can be implemented with the circuit shown in Figure 13.
AD1403
950
9k
1k
100
+5V
AD592
SPAN
TRIM
CENTER
POINT
TRIM
FORMAT
BPO/UPO
200
µP CONTROL
GND
V
IN
HI
V
I
HI
N
V
I
LO
N
V
I
LO
N
8 BITS
OUT
AD670
ADCPORT
R/W CS CE
V
CC
Figure 13. Temperature to Digital Output
By using a differential input A/D converter and choosing the
current to voltage conversion resistor correctly, any range of
temperatures (up to the 130°C span the AD592 is rated for)
centered at any point can be measured using a minimal number
of components. In this configuration the system will resolve up
to 1°C.
A variable temperature controlling thermostat can easily be built
using the AD592 in the circuit of Figure 14.
AD592
10k
R
HYST
R
PULL-UP
+15V
COMPARATOR
(OPTIONAL)
C
R
HIGH
62.7k
R
SET
10k
C
TEMP > SETPOINT
OUTPUT HIGH
TEMP < SETPOINT
OUTPUT LOW
R
LOW
27.3k
AD581
Figure 14. Variable Temperature Thermostat
R
HIGH
and R
LOW
determine the limits of temperature controlled
by the potentiometer R
SET
. The circuit shown operates over the
full temperature range (–25°C to +105°C) the AD592 is rated
for. The reference maintains a constant set point voltage and
insures that approximately 7 V appears across the sensor. If it is
necessary to guardband for extraneous noise hysteresis can be
added by tying a resistor from the output to the ungrounded
end of R
LOW.
Multiple remote temperatures can be measured using several
AD592s with a CMOS multiplexer or a series of 5 V logic gates
because of the device’s current-mode output and supply-voltage
compliance range. The on-resistance of a FET switch or output
impedance of a gate will not affect the accuracy, as long as 4 V
is maintained across the transducer. MUXs and logic driving
circuits should be chosen to minimize leakage current related
errors. Figure 15 illustrates a locally controlled MUX switching
the signal current from several remote AD592s. CMOS or TTL
gates can also be used to switch the AD592 supply voltages,
with the multiplexed signal being transmitted over a single
twisted pair to the load.
AD7501
D
E
C
O
D
E
R
/
D
R
I
V
E
R
T
8
T
2
T
1
REMOTE
AD592s
S1
S2
S8
E
N
TTL DTL TO
CMOS I/O
CHANNEL
SELECT
+15V –15V
V
OUT
10k
Figure 15. Remote Temperature Multiplexing
B
AD592
REV.
–8–
To minimize the number of MUXs required when a large num-
ber of AD592s are being used, the circuit can be configured in a
matrix. That is, a decoder can be used to switch the supply volt-
age to a column of AD592s while a MUX is used to control
which row of sensors are being measured. The maximum num-
ber of AD592s which can be used is the product of the number
of channels of the decoder and MUX.
An example circuit controlling 80 AD592s is shown in Figure
16. A 7-bit digital word is all that is required to select one of
the sensors. The enable input of the multiplexer turns all the
sensors off for minimum dissipation while idling.
+15V
COLUMN
SELECT
4028 BCD TO DECIMAL DECODER
ROW
SELECT
E
N
+15V
–15V
80 – AD592s
10k
V
OUT
AD7501
8-CHANNEL MUX
Figure 16. Matrix Multiplexer
To convert the AD592 output to °C or °F a single inexpensive
reference and op amp can be used as shown in Figure 17. Al-
though this circuit is similar to the two temperature trim circuit
shown in Figure 6, two important differences exist. First, the
gain resistor is fixed alleviating the need for an elevated tem-
perature trim. Acceptable accuracy can be achieved by choosing
an inexpensive resistor with the correct tolerance. Second, the
AD592 calibration error can be trimmed out at a known conve-
nient temperature (i.e., room temperature) with a single pot ad-
justment. This step is independent of the gain selection.
R
R
OFFSET
/R
GAIN
AD741
V
OUT
= 100mV/(
o
C OR
o
F)
+5V
AD1403
V–
o
C
o
F
9.1k
9.8k
100k
180k
R
GAIN
R
OFFSET
AD592
R
CAL
2.5V
R
GAIN
R
OFFSET
Figure 17. Celsius or Fahrenheit Thermometer
B

AD592ANZ

Mfr. #:
Manufacturer:
Analog Devices Inc.
Description:
Board Mount Temperature Sensors Crnt Outpt-Prec IC TEMP Transduce
Lifecycle:
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