a Monolithic Thermocouple Amplifiers with Cold Junction Compensation AD594/AD595 FEATURES Pretrimmed for Type J (AD594) or Type K (AD595) Thermocouples Can Be Used with Type T Thermocouple Inputs Low Impedance Voltage Output: 10 mV/ⴗC Built-In Ice Point Compensation Wide Power Supply Range: +5 V to ⴞ15 V Low Power: <1 mW typical Thermocouple Failure Alarm Laser Wafer Trimmed to 1ⴗC Calibration Accuracy Setpoint Mode Operation Self-Contained Celsius Thermometer Operation High Impedance Differential Input Side-Brazed DIP or Low Cost Cerdip PRODUCT DESCRIPTION The AD594/AD595 is a complete instrumentation amplifier and thermocouple cold junction compensator on a monolithic chip. It combines an ice point reference with a precalibrated amplifier to produce a high level (10 mV/°C) output directly from a thermocouple signal. Pin-strapping options allow it to be used as a linear amplifier-compensator or as a switched output setpoint controller using either fixed or remote setpoint control. It can be used to amplify its compensation voltage directly, thereby converting it to a stand-alone Celsius transducer with a low impedance voltage output. FUNCTIONAL BLOCK DIAGRAM –IN 14 –ALM 13 +ALM 12 V+ 11 COMP 10 VO 9 FB 8 OVERLOAD DETECT AD594/AD595 +A ICE POINT COMP. –TC G G +TC 1 2 3 4 5 6 7 +IN +C +T COM –T –C V– are available at the package pins so that the circuit can be recalibrated for the thermocouple types by the addition of two or three resistors. These terminals also allow more precise calibration for both thermocouple and thermometer applications. The AD594/AD595 is available in two performance grades. The C and the A versions have calibration accuracies of ± 1°C and ± 3°C, respectively. Both are designed to be used from 0°C to +50°C, and are available in 14-pin, hermetically sealed, sidebrazed ceramic DIPs as well as low cost cerdip packages. PRODUCT HIGHLIGHTS The AD594/AD595 includes a thermocouple failure alarm that indicates if one or both thermocouple leads become open. The alarm output has a flexible format which includes TTL drive capability. 1. The AD594/AD595 provides cold junction compensation, amplification, and an output buffer in a single IC package. The AD594/AD595 can be powered from a single ended supply (including +5 V) and by including a negative supply, temperatures below 0°C can be measured. To minimize self-heating, an unloaded AD594/AD595 will typically operate with a total supply current 160 µA, but is also capable of delivering in excess of ± 5 mA to a load. 3. Flexible pinout provides for operation as a setpoint controller or a stand-alone temperature transducer calibrated in degrees Celsius. The AD594 is precalibrated by laser wafer trimming to match the characteristic of type J (iron-constantan) thermocouples and the AD595 is laser trimmed for type K (chromel-alumel) inputs. The temperature transducer voltages and gain control resistors 2. Compensation, zero, and scale factor are all precalibrated by laser wafer trimming (LWT) of each IC chip. 4. Operation at remote application sites is facilitated by low quiescent current and a wide supply voltage range +5 V to dual supplies spanning 30 V. 5. Differential input rejects common-mode noise voltage on the thermocouple leads. REV. C Information furnished by Analog Devices is believed to be accurate and reliable. However, no responsibility is assumed by Analog Devices for its use, nor for any infringements of patents or other rights of third parties which may result from its use. No license is granted by implication or otherwise under any patent or patent rights of Analog Devices. One Technology Way, P.O. Box 9106, Norwood, MA 02062-9106, U.S.A. Tel: 781/329-4700 World Wide Web Site: http://www.analog.com Fax: 781/326-8703 © Analog Devices, Inc., 1999 (@ +25ⴗC and VS = 5 V, Type J (AD594), Type K (AD595) Thermocouple, AD594/AD595–SPECIFICATIONS unless otherwise noted) Model AD594A Typ Max Min ABSOLUTE MAXIMUM RATING +VS to –V S Common-Mode Input Voltage Differential Input Voltage Alarm Voltages +ALM –ALM Operating Temperature Range Output Short Circuit to Common 36 +VS +VS –VS – 0.15 –VS –VS –VS –55 Indefinite –VS + 36 +VS +125 TEMPERATURE MEASUREMENT (Specified Temperature Range 0°C to +50°C) Calibration Error at +25°C1 Stability vs. Temperature 2 Gain Error Nominal Transfer Function AMPLIFIER CHARACTERISTICS Closed Loop Gain 3 Input Offset Voltage Input Bias Current Differential Input Range Common-Mode Range Common-Mode Sensitivity – RTO Power Supply Sensitivity – RTO Output Voltage Range Dual Supply Single Supply Usable Output Current4 3 dB Bandwidth ALARM CHARACTERISTICS VCE(SAT) at 2 mA Leakage Current Operating Voltage at – ALM Short Circuit Current POWER REQUIREMENTS Specified Performance Operating5 Quiescent Current (No Load) +VS –VS PACKAGE OPTION TO-116 (D-14) Cerdip (Q-14) AD594C Typ Max Min 36 +VS +VS –VS – 0.15 –VS –VS –VS –55 Indefinite –VS + 36 +VS +125 ⴞ3 ⴞ0.05 ⴞ1.5 10 193.4 (Temperature in °C) × 51.70 µV/°C 0.1 –10 +50 –VS – 0.15 –VS – 4 10 10 –VS + 2.5 0 ±5 15 +VS – 2 +VS – 2 193.4 (Temperature in °C) × 51.70 µV/°C 0.1 –VS –VS –55 Indefinite –VS + 36 +VS +125 –VS – 0.15 –VS – 4 10 10 –VS + 2.5 0 +VS – 2 –VS – 2 –VS + 2.5 0 ±5 15 0.3 ±5 15 20 AD594AD AD594AQ 160 100 AD594CD AD594CQ 300 AD595C Typ Max Units 36 +VS +VS Volts Volts Volts –VS + 36 +VS +125 Volts Volts °C ⴞ1 ⴞ0.025 ⴞ0.75 10 °C °C/°C % mV/°C –VS – 0.15 –VS –VS –VS –55 Indefinite 247.3 (Temperature in °C) × 40.44 µV/°C 0.1 –10 +50 –VS – 0.15 –VS – 4 10 10 –VS + 2.5 0 ±5 15 AD595AD AD595AQ ⴞ1 +VS – 4 20 +VS = 5, –VS = 0 +VS to –VS ≤ 30 160 100 +VS – 2 +VS – 2 0.3 ⴞ1 +VS – 4 20 +VS = 5, –VS = 0 +VS to –VS ≤ 30 300 +VS – 2 +VS + 2 0.3 ⴞ1 +VS – 4 20 Min ⴞ3 ⴞ0.05 ⴞ1.5 10 247.3 (Temperature in °C) × 40.44 µV/°C 0.1 –10 +50 –VS – 0.15 –VS – 4 10 10 ⴞ1 +VS – 4 160 100 36 +VS +VS –VS – 0.15 –VS ⴞ1 ⴞ0.025 ⴞ0.75 10 0.3 +VS = 5, –VS = 0 +VS to –VS ≤ 30 AD595A Typ Max Min +VS = 5, –VS = 0 +VS to –VS ≤ 30 300 160 100 µV µA mV Volts mV/V mV/V Volts Volts mA kHz Volts µA max Volts mA Volts Volts 300 µA µA AD595CD AD595CQ NOTES 1 Calibrated for minimum error at +25°C using a thermocouple sensitivity of 51.7 µV/°C. Since a J type thermocouple deviates from this straight line approximation, the AD594 will normally read 3.1 mV when the measuring junction is at 0°C. The AD595 will similarly read 2.7 mV at 0°C. 2 Defined as the slope of the line connecting the AD594/AD595 errors measured at 0°C and 50°C ambient temperature. 3 Pin 8 shorted to Pin 9. 4 Current Sink Capability in single supply configuration is limited to current drawn to ground through a 50 kΩ resistor at output voltages below 2.5 V. 5 –VS must not exceed –16.5 V. 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 min and max specifications are guaranteed, although only those shown in boldface are tested on all production units. Specifications subject to change without notice. compensated signal, the following transfer functions should be used to determine the actual output voltages: AD594 output = (Type J Voltage + 16 µV) × 193.4 AD595 output = (Type K Voltage + 11 µV) × 247.3 or conversely: Type J voltage = (AD594 output/193.4) – 16 µV Type K voltage = (AD595 output/247.3) – 11 µV INTERPRETING AD594/AD595 OUTPUT VOLTAGES To achieve a temperature proportional output of 10 mV/°C and accurately compensate for the reference junction over the rated operating range of the circuit, the AD594/AD595 is gain trimmed to match the transfer characteristic of J and K type thermocouples at 25°C. For a type J output in this temperature range the TC is 51.70 µV/°C, while for a type K it is 40.44 µV/°C. The resulting gain for the AD594 is 193.4 (10 mV/°C divided by 51.7 µV/°C) and for the AD595 is 247.3 (10 mV/°C divided by 40.44 µV/°C). In addition, an absolute accuracy trim induces an input offset to the output amplifier characteristic of 16 µV for the AD594 and 11 µV for the AD595. This offset arises because the AD594/ AD595 is trimmed for a 250 mV output while applying a 25°C thermocouple input. Because a thermocouple output voltage is nonlinear with respect to temperature, and the AD594/AD595 linearly amplifies the Table I lists the ideal AD594/AD595 output voltages as a function of Celsius temperature for type J and K ANSI standard thermocouples, with the package and reference junction at 25°C. As is normally the case, these outputs are subject to calibration, gain and temperature sensitivity errors. Output values for intermediate temperatures can be interpolated, or calculated using the output equations and ANSI thermocouple voltage tables referred to zero degrees Celsius. Due to a slight variation in alloy content between ANSI type J and DIN FE-CUNI –2– REV. C AD594/AD595 Table I. Output Voltage vs. Thermocouple Temperature (Ambient +25°C, VS = –5 V, +15 V) Thermocouple Temperature °C Type J Voltage mV AD594 Output mV Type K Voltage mV AD595 Output mV –200 –180 –160 –140 –120 –7.890 –7.402 –6.821 –6.159 –5.426 –1523 –1428 –1316 –1188 –1046 –5.891 –5.550 –5.141 –4.669 –4.138 –1454 –1370 –1269 –1152 –1021 –100 –80 –60 –40 –20 –4.632 –3.785 –2.892 –1.960 –.995 –893 –729 –556 –376 –189 –3.553 –2.920 –2.243 –1.527 –.777 –10 0 10 20 25 –.501 0 .507 1.019 1.277 –94 3.1 101 200 250 30 40 50 60 80 1.536 2.058 2.585 3.115 4.186 100 120 140 160 180 Type J Voltage mV AD594 Output mV Type K Voltage mV AD595 Output mV 500 520 540 560 580 27.388 28.511 29.642 30.782 31.933 5300 5517 5736 5956 6179 20.640 21.493 22.346 23.198 24.050 5107 5318 5529 5740 5950 –876 –719 –552 –375 –189 600 620 640 660 680 33.096 34.273 35.464 36.671 37.893 6404 6632 6862 7095 7332 24.902 25.751 26.599 27.445 28.288 6161 6371 6581 6790 6998 –.392 0 .397 .798 1.000 –94 2.7 101 200 250 700 720 740 750 760 39.130 40.382 41.647 42.283 – 7571 7813 8058 8181 – 29.128 29.965 30.799 31.214 31.629 7206 7413 7619 7722 7825 300 401 503 606 813 1.203 1.611 2.022 2.436 3.266 300 401 503 605 810 780 800 820 840 860 – – – – – – – – – – 32.455 33.277 34.095 34.909 35.718 8029 8232 8434 8636 8836 5.268 6.359 7.457 8.560 9.667 1022 1233 1445 1659 1873 4.095 4.919 5.733 6.539 7.338 1015 1219 1420 1620 1817 880 900 920 940 960 – – – – – – – – – – 36.524 37.325 38.122 38.915 39.703 9035 9233 9430 9626 9821 200 220 240 260 280 10.777 11.887 12.998 14.108 15.217 2087 2302 2517 2732 2946 8.137 8.938 9.745 10.560 11.381 2015 2213 2413 2614 2817 980 1000 1020 1040 1060 – – – – – – – – – – 40.488 41.269 42.045 42.817 43.585 10015 10209 10400 10591 10781 300 320 340 360 380 16.325 17.432 18.537 19.640 20.743 3160 3374 3588 3801 4015 12.207 13.039 13.874 14.712 15.552 3022 3227 3434 3641 3849 1080 1100 1120 1140 1160 – – – – – – – – – – 44.439 45.108 45.863 46.612 47.356 10970 11158 11345 11530 11714 400 420 440 460 480 21.846 22.949 24.054 25.161 26.272 4228 4441 4655 4869 5084 16.395 17.241 18.088 18.938 19.788 4057 4266 4476 4686 4896 1180 1200 1220 1240 1250 – – – – – – – – – – 48.095 48.828 49.555 50.276 50.633 11897 12078 12258 12436 12524 thermocouples Table I should not be used in conjunction with European standard thermocouples. Instead the transfer function given previously and a DIN thermocouple table should be used. ANSI type K and DIN NICR-NI thermocouples are composed CONSTANTAN (ALUMEL) +5V 10mV/8C Thermocouple Temperature °C SINGLE AND DUAL SUPPLY CONNECTIONS The AD594/AD595 is a completely self-contained thermocouple conditioner. Using a single +5 V supply the interconnections shown in Figure 1 will provide a direct output from a type J thermocouple (AD594) or type K thermocouple (AD595) measuring from 0°C to +300°C. Figure 1. Basic Connection, Single Supply Operation Any convenient supply voltage from +5 V to +30 V may be used, with self-heating errors being minimized at lower supply levels. In the single supply configuration the +5 V supply connects to Pin 11 with the V– connection at Pin 7 strapped to power and signal common at Pin 4. The thermocouple wire inputs connect to Pins 1 and 14 either directly from the measuring point or through intervening connections of similar thermocouple wire type. When the alarm output at Pin 13 is not used it should be connected to common or –V. The precalibrated feedback network at Pin 8 is tied to the output at Pin 9 to provide a 10 mV/°C nominal temperature transfer characteristic. of identical alloys and exhibit similar behavior. The upper temperature limits in Table I are those recommended for type J and type K thermocouples by the majority of vendors. By using a wider ranging dual supply, as shown in Figure 2, the AD594/AD595 can be interfaced to thermocouples measuring both negative and extended positive temperatures. 13 14 12 11 10 9 8 OVERLOAD DETECT AD594/ AD595 +A G G +TC IRON (CHROMEL) 1 2 3 4 5 ICE POINT COMP. –TC 6 7 COMMON REV. C –3– AD594/AD595 The printed circuit board layout shown also provides for placement of optional alarm load resistors, recalibration resistors and a compensation capacitor to limit bandwidth. +5V TO +30V CONSTANTAN (ALUMEL) 14 13 12 11 9 10 8 OVERLOAD DETECT AD594/ AD595 G G +TC IRON (CHROMEL) 1 2 To ensure secure bonding the thermocouple wire should be cleaned to remove oxidation prior to soldering. Noncorrosive rosin flux is effective with iron, constantan, chromel and alumel and the following solders: 95% tin-5% antimony, 95% tin-5% silver or 90% tin-10% lead. +A 3 4 5 ICE POINT –TC COMP. 6 SPAN OF 5V TO 30V 7 FUNCTIONAL DESCRIPTION The AD594 behaves like two differential amplifiers. The outputs are summed and used to control a high gain amplifier, as shown in Figure 4. COMMON 0V TO –25V Figure 2. Dual Supply Operation –IN 14 With a negative supply the output can indicate negative temperatures and drive grounded loads or loads returned to positive voltages. Increasing the positive supply from 5 V to 15 V extends the output voltage range well beyond the 750°C temperature limit recommended for type J thermocouples (AD594) and the 1250°C for type K thermocouples (AD595). G +C –IN +ALM –ALM COMMON –T –C V– 8 VOUT +A ICE POINT COMP. –TC G 1 2 3 4 5 6 7 +IN +C +T COM –T –C V– In addition to the feedback signal, a cold junction compensation voltage is applied to the right-hand differential amplifier. The compensation is a differential voltage proportional to the Celsius temperature of the AD594/AD595. This signal disturbs the differential input so that the amplifier output must adjust to restore the input to equal the applied thermocouple voltage. COMP 7 FB 8 In normal operation the main amplifier output, at Pin 9, is connected to the feedback network, at Pin 8. Thermocouple signals applied to the floating input stage, at Pins 1 and 14, are amplified by gain G of the differential amplifier and are then further amplified by gain A in the main amplifier. The output of the main amplifier is fed back to a second differential stage in an inverting connection. The feedback signal is amplified by this stage and is also applied to the main amplifier input through a summing circuit. Because of the inversion, the amplifier causes the feedback to be driven to reduce this difference signal to a small value. The two differential amplifiers are made to match and have identical gains, G. As a result, the feedback signal that must be applied to the right-hand differential amplifier will precisely match the thermocouple input signal when the difference signal has been reduced to zero. The feedback network is trimmed so that the effective gain to the output, at Pins 8 and 9, results in a voltage of 10 mV/°C of thermocouple excitation. CONSTANTAN (ALUMEL) 14 VO 9 Figure 4. AD594/AD595 Block Diagram A method that provides for thermal equilibrium is the printed circuit board connection layout illustrated in Figure 3. 1 COMP 10 +TC The isothermal terminating connections of a pair of thermocouple wires forms an effective reference junction. This junction must be kept at the same temperature as the AD594/AD595 for the internal cold junction compensation to be effective. +IN V+ 11 AD594/AD595 THERMOCOUPLE CONNECTIONS +T +ALM 12 OVERLOAD DETECT Common-mode voltages on the thermocouple inputs must remain within the common-mode range of the AD594/AD595, with a return path provided for the bias currents. If the thermocouple is not remotely grounded, then the dotted line connections in Figures 1 and 2 are recommended. A resistor may be needed in this connection to assure that common-mode voltages induced in the thermocouple loop are not converted to normal mode. IRON (CHROMEL) –ALM 13 The compensation is applied through the gain scaling resistors so that its effect on the main output is also 10 mV/°C. As a result, the compensation voltage adds to the effect of the thermocouple voltage a signal directly proportional to the difference between 0°C and the AD594/AD595 temperature. If the thermocouple reference junction is maintained at the AD594/AD595 temperature, the output of the AD594/AD595 will correspond to the reading that would have been obtained from amplification of a signal from a thermocouple referenced to an ice bath. V+ Figure 3. PCB Connections Here the AD594/AD595 package temperature and circuit board are thermally contacted in the copper printed circuit board tracks under Pins 1 and 14. The reference junction is now composed of a copper-constantan (or copper-alumel) connection and copper-iron (or copper-chromel) connection, both of which are at the same temperature as the AD594/AD595. –4– REV. C AD594/AD595 The AD594/AD595 also includes an input open circuit detector that switches on an alarm transistor. This transistor is actually a current-limited output buffer, but can be used up to the limit as a switch transistor for either pull-up or pull-down operation of external alarms. The ice point compensation network has voltages available with positive and negative temperature coefficients. These voltages may be used with external resistors to modify the ice point compensation and recalibrate the AD594/AD595 as described in the next column. The feedback resistor is separately pinned out so that its value can be padded with a series resistor, or replaced with an external resistor between Pins 5 and 9. External availability of the feedback resistor allows gain to be adjusted, and also permits the AD594/ AD595 to operate in a switching mode for setpoint operation. CAUTIONS: The temperature compensation terminals (+C and –C) at Pins 2 and 6 are provided to supply small calibration currents only. The AD594/AD595 may be permanently damaged if they are grounded or connected to a low impedance. The AD594/AD595 is internally frequency compensated for feedback ratios (corresponding to normal signal gain) of 75 or more. If a lower gain is desired, additional frequency compensation should be added in the form of a 300 pF capacitor from Pin 10 to the output at Pin 9. As shown in Figure 5 an additional 0.01 µF capacitor between Pins 10 and 11 is recommended. AD594/ AD595 VO 9 300pF COMP 10 0.01mF +V 11 Figure 5. Low Gain Frequency Compensation RECALIBRATION PRINCIPLES AND LIMITATIONS The ice point compensation network of the AD594/AD595 produces a differential signal which is zero at 0°C and corresponds to the output of an ice referenced thermocouple at the temperature of the chip. The positive TC output of the circuit is proportional to Kelvin temperature and appears as a voltage at +T. It is possible to decrease this signal by loading it with a resistor from +T to COM, or increase it with a pull-up resistor from +T to the larger positive TC voltage at +C. Note that adjustments to +T should be made by measuring the voltage which tracks it at –T. To avoid destabilizing the feedback amplifier the measuring instrument should be isolated by a few thousand ohms in series with the lead connected to –T. 1 +IN +T 3 this terminal can be produced with a resistor between –C and –T to balance an increase in +T, or a resistor from –T to COM to offset a decrease in +T. If the compensation is adjusted substantially to accommodate a different thermocouple type, its effect on the final output voltage will increase or decrease in proportion. To restore the nominal output to 10 mV/°C the gain may be adjusted to match the new compensation and thermocouple input characteristics. When reducing the compensation the resistance between –T and COM automatically increases the gain to within 0.5% of the correct value. If a smaller gain is required, however, the nominal 47 kΩ internal feedback resistor can be paralleled or replaced with an external resistor. Fine calibration adjustments will require temperature response measurements of individual devices to assure accuracy. Major reconfigurations for other thermocouple types can be achieved without seriously compromising initial calibration accuracy, so long as the procedure is done at a fixed temperature using the factory calibration as a reference. It should be noted that intermediate recalibration conditions may require the use of a negative supply. EXAMPLE: TYPE E RECALIBRATION—AD594/AD595 Both the AD594 and AD595 can be configured to condition the output of a type E (chromel-constantan) thermocouple. Temperature characteristics of type E thermocouples differ less from type J, than from type K, therefore the AD594 is preferred for recalibration. While maintaining the device at a constant temperature follow the recalibration steps given here. First, measure the device temperature by tying both inputs to common (or a selected common-mode potential) and connecting FB to VO. The AD594 is now in the stand alone Celsius thermometer mode. For this example assume the ambient is 24°C and the initial output VO is 240 mV. Check the output at VO to verify that it corresponds to the temperature of the device. Next, measure the voltage –T at Pin 5 with a high impedance DVM (capacitance should be isolated by a few thousand ohms of resistance at the measured terminals). At 24°C the –T voltage will be about 8.3 mV. To adjust the compensation of an AD594 to a type E thermocouple a resistor, R1, should be connected between +T and +C, Pins 2 and 3, to raise the voltage at –T by the ratio of thermocouple sensitivities. The ratio for converting a type J device to a type E characteristic is: r (AD594) =(60.9 µV/°C)/(51.7 µV/°C)= 1.18 Thus, multiply the initial voltage measured at –T by r and experimentally determine the R1 value required to raise –T to that level. For the example the new –T voltage should be about 9.8 mV. The resistance value should be approximately 1.8 kΩ. Figure 6. Decreased Sensitivity Adjustment The zero differential point must now be shifted back to 0°C. This is accomplished by multiplying the original output voltage VO by r and adjusting the measured output voltage to this value by experimentally adding a resistor, R2, between –C and –T, Pins 5 and 6. The target output value in this case should be about 283 mV. The resistance value of R2 should be approximately 240 kΩ. Changing the positive TC half of the differential output of the compensation scheme shifts the zero point away from 0°C. The zero can be restored by adjusting the current flow into the negative input of the feedback amplifier, the –T pin. A current into Finally, the gain must be recalibrated such that the output VO indicates the device’s temperature once again. Do this by adding a third resistor, R3, between FB and –T, Pins 8 and 5. VO should now be back to the initial 240 mV reading. The resistance value 14 –IN AD594/ AD595 COM 4 8 FB 9 REV. C VO –T 5 –5– AD594/AD595 of R3 should be approximately 280 kΩ. The final connection diagram is shown in Figure 7. An approximate verification of the effectiveness of recalibration is to measure the differential gain to the output. For type E it should be 164.2. 1 +IN THERMAL ENVIRONMENT EFFECTS The inherent low power dissipation of the AD594/AD595 and the low thermal resistance of the package make self-heating errors almost negligible. For example, in still air the chip to ambient thermal resistance is about 80°C/watt (for the D package). At the nominal dissipation of 800 µW the self-heating in free air is less than 0.065°C. Submerged in fluorinert liquid (unstirred) the thermal resistance is about 40°C/watt, resulting in a selfheating error of about 0.032°C. COM 4 14 –IN +T 3 AD594/ AD595 R1 +C 2 SETPOINT CONTROLLER The AD594/AD595 can readily be connected as a setpoint controller as shown in Figure 9. –C 6 9 VO R2 –T 8 FB 5 HEATER DRIVER R3 CONSTANTAN HEATER (ALUMEL) Figure 7. Type E Recalibration When implementing a similar recalibration procedure for the AD595 the values for R1, R2, R3 and r will be approximately 650 Ω, 84 kΩ, 93 kΩ and 1.51, respectively. Power consumption will increase by about 50% when using the AD595 with type E inputs. SETPOINT VOLTAGE INPUT +5V 14 13 12 11 10 9 8 20MV (OPTIONAL) FOR HYSTERESIS OVERLOAD DETECT AD594/ AD595 +A G G +TC Note that during this procedure it is crucial to maintain the AD594/AD595 at a stable temperature because it is used as the temperature reference. Contact with fingers or any tools not at ambient temperature will quickly produce errors. Radiational heating from a change in lighting or approach of a soldering iron must also be guarded against. IRON (CHROMEL) TEMPERATURE CONTROLLED REGION 1 2 3 4 5 ICE POINT –TC COMP. 6 7 COMMON Figure 9. Setpoint Controller The thermocouple is used to sense the unknown temperature and provide a thermal EMF to the input of the AD594/AD595. The signal is cold junction compensated, amplified to 10 mV/°C and compared to an external setpoint voltage applied by the user to the feedback at Pin 8. Table I lists the correspondence between setpoint voltage and temperature, accounting for the nonlinearity of the measurement thermocouple. If the setpoint temperature range is within the operating range (–55°C to +125°C) of the AD594/AD595, the chip can be used as the transducer for the circuit by shorting the inputs together and utilizing the nominal calibration of 10 mV/°C. This is the centigrade thermometer configuration as shown in Figure 13. USING TYPE T THERMOCOUPLES WITH THE AD595 Because of the similarity of thermal EMFs in the 0°C to +50°C range between type K and type T thermocouples, the AD595 can be directly used with both types of inputs. Within this ambient temperature range the AD595 should exhibit no more than an additional 0.2°C output calibration error when used with type T inputs. The error arises because the ice point compensator is trimmed to type K characteristics at 25°C. To calculate the AD595 output values over the recommended –200°C to +350°C range for type T thermocouples, simply use the ANSI thermocouple voltages referred to 0°C and the output equation given on page 2 for the AD595. Because of the relatively large nonlinearities associated with type T thermocouples the output will deviate widely from the nominal 10 mV/°C. However, cold junction compensation over the rated 0°C to +50°C ambient will remain accurate. In operation if the setpoint voltage is above the voltage corresponding to the temperature being measured the output swings low to approximately zero volts. Conversely, when the temperature rises above the setpoint voltage the output switches to the positive limit of about 4 volts with a +5 V supply. Figure 9 shows the setpoint comparator configuration complete with a heater element driver circuit being controlled by the AD594/ AD595 toggled output. Hysteresis can be introduced by injecting a current into the positive input of the feedback amplifier when the output is toggled high. With an AD594 about 200 nA into the +T terminal provides 1°C of hysteresis. When using a single 5 V supply with an AD594, a 20 MΩ resistor from VO to +T will supply the 200 nA of current when the output is forced high (about 4 V). To widen the hysteresis band decrease the resistance connected from VO to +T. STABILITY OVER TEMPERATURE Each AD594/AD595 is tested for error over temperature with the measuring thermocouple at 0°C. The combined effects of cold junction compensation error, amplifier offset drift and gain error determine the stability of the AD594/AD595 output over the rated ambient temperature range. Figure 8 shows an AD594/ AD595 drift error envelope. The slope of this figure has units of °C/°C. +0.68C DRIFT ERROR LOW = > T < SETPOINT HIGH = > T > SETPOINT TEMPERATURE COMPARATOR OUT 0 258C –0.68C 508C TEMPERATURE OF AD594C/AD595C Figure 8. Drift Error vs. Temperature –6– REV. C AD594/AD595 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 connecting 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. The alarm can be used with both single and dual supplies. It can be operated above or below ground. The collector and emitter 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. +10V CONSTANTAN (ALUMEL) 14 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 Figure 10 this signal is compatible with the input of a TTL gate which can be used as a buffer and/or inverter. 13 12 11 10 9 8 AD594/ AD595 +A G G +TC IRON (CHROMEL) 1 2 3 4 5 ICE POINT –TC COMP. 6 7 +5V 20kV 13 14 12 11 9 10 GND ALARM TTL GATE ALARM OUT CONSTANTAN (ALUMEL) 10mV/8C OVERLOAD DETECT ALARM RELAY 10mV/8C 8 –12V OVERLOAD DETECT AD594/ AD595 Figure 12. –ALM Driving A Negative Referenced Load +A G G +TC IRON (CHROMEL) 1 2 3 4 5 ICE POINT –TC COMP. 6 7 GND 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. V+ LED CONSTANTAN (ALUMEL) 13 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 270V 14 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. 10mV/8C 12 11 10 9 8 The AD594/AD595 may be configured as a stand-alone Celsius thermometer as shown in Figure 13. OVERLOAD DETECT AD594/ AD595 14 G G +TC IRON (CHROMEL) 1 2 +5V TO +15V +A 3 4 5 12 11 9 8 AD594/ AD595 +A 7 G G COMMON +TC Figure 11. Alarm Directly Drives LED A 270 Ω 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 compensation 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. REV. C 10 OVERLOAD DETECT ICE POINT –TC COMP. 6 13 OUTPUT 10mV/8C 1 2 3 4 5 ICE POINT –TC COMP. 6 7 GND 0 TO –15V 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 compensation voltage and hence will indicate the AD594/AD595 temperature with a scale factor of 10 mV/°C. In this three terminal, voltage output, temperature sensing mode, the AD594/ AD595 will operate over the full military –55°C to +125°C temperature range. –7– AD594/AD595 and to arrange its output voltage so that it corresponds to a thermocouple referred to 0°C. This voltage is simply added to the thermocouple voltage and the sum then corresponds to the standard voltage tabulated for an ice-point referenced thermocouple. Thermocouples are economical and rugged; they have reasonably good long-term stability. Because of their small size, they respond quickly and are good choices where fast response is important. They function over temperature ranges from cryogenics to jet-engine exhaust and have reasonable linearity and accuracy. V1' Because the number of free electrons in a piece of metal depends 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 temperature, as shown in Figure 14. The resulting voltage depends on the temperatures, T1 and T2, in a repeatable way. Cu CONSTANTAN V1' = V1 FOR PROPERLY SCALED V3' = f(T3) V1 C731g–0–11/99 THERMOCOUPLE BASICS Cu CuNi– V2 T3 V3' T1 V1 IRON Cu CONSTANTAN Figure 15. Substitution of Measured Reference Temperature for Ice Point Reference Cu CONSTANTAN T2 T1 The temperature sensitivity of silicon integrated circuit transistors is quite predictable and repeatable. This sensitivity is exploited in the AD594/AD595 to produce a temperature related voltage to compensate the reference of “cold” junction of a thermocouple as shown in Figure 16. IRON ICE POINT REFERENCE UNKNOWN TEMPERATURE 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 characterized 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. T3 CONSTANTAN T1 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 thermocouple 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 Cu IRON Cu Figure 16. Connecting Isothermal Junctions Since the compensation is at the reference junction temperature, it is often convenient to form the reference “junction” by connecting directly to the circuit wiring. So long as these connections and the compensation are at the same temperature no error will result. OUTLINE DIMENSIONS Dimensions shown in inches and (mm). Cerdip (Q) Package 0.77 ±0.015 (19.55 ±0.39) 0.430 (10.92) 0.040 (1.02) R 14 8 0.265 0.290 ±0.010 (6.73) (7.37 ±0.25) 1 14 8 0.260 ±0.020 (6.6 ±0.51) 0.310 (7.87) 7 1 PIN 1 0.31 ±0.01 (7.87 ±0.25) 0.700 ±0.010 (17.78 ±0.25) 0.035 ±0.010 (0.89 ±0.25) ( 7 PIN 1 0.095 (2.41) 0.085 (2.16) 0.125 (3.18) MIN 0.047 ±0.007 +0.003 0.100 (1.19 ±0.18) 0.017 –0.002 (2.54) BSC 0.43 +0.08 –0.05 PRINTED IN U.S.A. TO-116 (D) Package 0.180 ±0.030 (4.57 ±0.76) 0.035 ±0.010 (0.889 ±0.254) 0.032 (0.812) 0.30 (7.62) REF 0.018 (0.457) 0.600 (15.24) BSC ( –8– 0.148 ±0.015 (3.76 ±0.38) 0.180 ±0.030 (4.57 ±0.76) 0.125 3.175) MIN 0.01 ±0.002 (0.25 ±0.05) 0.300 (7.62) REF SEATING PLANE 0.100 (2.54) BSC 15° 0° 0.010 ±0.001 (0.254 ±0.025) REV. C