AD595AQ

AD594/AD595
REV. C
–7–
ALARM CIRCUIT
In all applications of the AD594/AD595 the –ALM connection,
Pin 13, should be constrained so that it is not more positive
than (V+) – 4 V. This can be most easily achieved by connect-
ing Pin 13 to either common at Pin 4 or V– at Pin 7. For most
applications that use the alarm signal, Pin 13 will be grounded
and the signal will be taken from +ALM on Pin 12. A typical
application is shown in Figure 10.
In this configuration the alarm transistor will be off in normal
operation and the 20 k pull up will cause the +ALM output on
Pin 12 to go high. If one or both of the thermocouple leads are
interrupted, the +ALM pin will be driven low. As shown in Fig-
ure 10 this signal is compatible with the input of a TTL gate
which can be used as a buffer and/or inverter.
CONSTANTAN
(ALUMEL)
IRON
(CHROMEL)
+5V
ALARM
TTL GATE
20kV
ALARM OUT
GND
OVERLOAD
DETECT
G
–TC
+TC
1234567
13 12 11 10
AD594/
AD595
14
ICE
POINT
COMP.
+A
98
G
10mV/8C
Figure 10. Using the Alarm to Drive a TTL Gate
(“Grounded’’ Emitter Configuration)
Since the alarm is a high level output it may be used to directly
drive an LED or other indicator as shown in Figure 11.
CONSTANTAN
(ALUMEL)
IRON
(CHROMEL)
COMMON
LED
270V
V+
OVERLOAD
DETECT
G
–TC
+TC
123 4 5
67
13 12 11 10
AD594/
AD595
14
ICE
POINT
COMP.
+A
98
G
10mV/8C
Figure 11. Alarm Directly Drives LED
A 270 series resistor will limit current in the LED to 10 mA,
but may be omitted since the alarm output transistor is current
limited at about 20 mA. The transistor, however, will operate in
a high dissipation mode and the temperature of the circuit will
rise well above ambient. Note that the cold junction compensa-
tion will be affected whenever the alarm circuit is activated. The
time required for the chip to return to ambient temperature will
depend on the power dissipation of the alarm circuit, the nature
of the thermal path to the environment and the alarm duration.
The alarm can be used with both single and dual supplies. It
can be operated above or below ground. The collector and emit-
ter of the output transistor can be used in any normal switch
configuration. As an example a negative referenced load can be
driven from –ALM as shown in Figure 12.
CONSTANTAN
(ALUMEL)
IRON
(CHROMEL)
+10V
GND
ALARM
RELAY
–12V
OVERLOAD
DETECT
G
–TC
+TC
1234567
13 12 11 10
AD594/
AD595
14
ICE
POINT
COMP.
+A
98
G
10mV/8C
Figure 12. –ALM Driving A Negative Referenced Load
The collector (+ALM) should not be allowed to become more
positive than (V–) +36 V, however, it may be permitted to be
more positive than V+. The emitter voltage (–ALM) should be
constrained so that it does not become more positive than 4
volts below the V+ applied to the circuit.
Additionally, the AD594/AD595 can be configured to produce
an extreme upscale or downscale output in applications where
an extra signal line for an alarm is inappropriate. By tying either
of the thermocouple inputs to common most runaway control
conditions can be automatically avoided. A +IN to common
connection creates a downscale output if the thermocouple opens,
while connecting –IN to common provides an upscale output.
CELSIUS THERMOMETER
The AD594/AD595 may be configured as a stand-alone Celsius
thermometer as shown in Figure 13.
+5V TO +15V
OUTPUT
10mV/8C
GND
0 TO –15V
OVERLOAD
DETECT
G
–TC
+TC
123
4567
13 12 11 10
AD594/
AD595
14
ICE
POINT
COMP.
+A
98
G
Figure 13. AD594/AD595 as a Stand-Alone Celsius
Thermometer
Simply omit the thermocouple and connect the inputs (Pins 1
and 14) to common. The output now will reflect the compensa-
tion voltage and hence will indicate the AD594/AD595
temperature with a scale factor of 10 mV/°C. In this three termi-
nal, voltage output, temperature sensing mode, the AD594/
AD595 will operate over the full military –55°C to +125°C tem-
perature range.
AD594/AD595
REV. C
–8–
C731g–0–11/99
PRINTED IN U.S.A.
OUTLINE DIMENSIONS
Dimensions shown in inches and (mm).
TO-116 (D) Package
0.100
(2.54)
BSC
0.700 ±0.010
(17.78 ±0.25)
0.180 ±0.030
(4.57 ±0.76)
0.085 (2.16)
0.035 ±0.010
(0.89 ±0.25)
0.047 ±0.007
(1.19 ±0.18)
0.017
+0.003
–0.002
0.43
+0.08
–0.05
(
(
0.125
(3.18)
MIN
0.31 ±0.01
(7.87 ±0.25)
0.01 ±0.002
(0.25 ±0.05)
0.095 (2.41)
0.30 (7.62) REF
0.430 (10.92)
14
1
7
8
0.040
(1.02) R
PIN 1
0.265
(6.73)
0.290 ±0.010
(7.37 ±0.25)
Cerdip (Q) Package
14
1
7
8
PIN 1
0.77 ±0.015
(19.55 ±0.39)
0.310
(7.87)
0.260 ±0.020
(6.6 ±0.51)
SEATING
PLANE
0.100
(2.54)
BSC
0.035 ±0.010
(0.889 ±0.254)
0.180 ±0.030
(4.57 ±0.76)
0.125
3.175)
MIN
0.032
(0.812)
15°
0°
0.300 (7.62)
REF
0.148 ±0.015
(3.76 ±0.38)
0.010 ±0.001
(0.254 ±0.025)
0.018
(0.457)
0.600 (15.24)
BSC
THERMOCOUPLE BASICS
Thermocouples are economical and rugged; they have reason-
ably good long-term stability. Because of their small size, they
respond quickly and are good choices where fast response is im-
portant. They function over temperature ranges from cryogenics
to jet-engine exhaust and have reasonable linearity and accuracy.
Because the number of free electrons in a piece of metal de-
pends on both temperature and composition of the metal, two
pieces of dissimilar metal in isothermal and contact will exhibit
a potential difference that is a repeatable function of tempera-
ture, as shown in Figure 14. The resulting voltage depends on
the temperatures, T1 and T2, in a repeatable way.
CONSTANTAN
IRON
UNKNOWN
TEMPERATURE
ICE POINT
REFERENCE
T1
T2
CONSTANTAN
Cu Cu
V1
Figure 14. Thermocouple Voltage with 0
°
C Reference
Since the thermocouple is basically a differential rather than
absolute measuring device, a know reference temperature is
required for one of the junctions if the temperature of the other
is to be inferred from the output voltage. Thermocouples made
of specially selected materials have been exhaustively character-
ized in terms of voltage versus temperature compared to primary
temperature standards. Most notably the water-ice point of 0°C
is used for tables of standard thermocouple performance.
An alternative measurement technique, illustrated in Figure 15,
is used in most practical applications where accuracy requirements
do not warrant maintenance of primary standards. The reference
junction temperature is allowed to change with the environment
of the measurement system, but it is carefully measured by some
type of absolute thermometer. A measurement of the thermo-
couple voltage combined with a knowledge of the reference
temperature can be used to calculate the measurement junction
temperature. Usual practice, however, is to use a convenient
thermoelectric method to measure the reference temperature
and to arrange its output voltage so that it corresponds to a ther-
mocouple referred to 0°C. This voltage is simply added to the
thermocouple voltage and the sum then corresponds to the stan-
dard voltage tabulated for an ice-point referenced thermocouple.
CONSTANTAN
IRON
T1
V1
CuNi–
Cu
Cu
T3
V
1
'
= V
1
FOR PROPERLY
SCALED V
3
'
= f(T
3
)
V3
'
V1
'
V2
Figure 15. Substitution of Measured Reference
Temperature for Ice Point Reference
The temperature sensitivity of silicon integrated circuit transis-
tors is quite predictable and repeatable. This sensitivity is
exploited in the AD594/AD595 to produce a temperature re-
lated voltage to compensate the reference of “cold” junction of a
thermocouple as shown in Figure 16.
Cu
CONSTANTAN
IRON
T1
Cu
T3
Figure 16. Connecting Isothermal Junctions
Since the compensation is at the reference junction temperature,
it is often convenient to form the reference “junction” by connect-
ing directly to the circuit wiring. So long as these connections
and the compensation are at the same temperature no error will
result.

AD595AQ

Mfr. #:
Manufacturer:
Analog Devices Inc.
Description:
Board Mount Temperature Sensors THERMOCOUPLE AMP IC
Lifecycle:
New from this manufacturer.
Delivery:
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