CONSTRUCTION of a THERMOCOUPLE THERMOMETER by Jim Roberts, Professor of Physics and Material Science the University of North Texas

Total Page:16

File Type:pdf, Size:1020Kb

CONSTRUCTION of a THERMOCOUPLE THERMOMETER by Jim Roberts, Professor of Physics and Material Science the University of North Texas SUPPORT MATERIALS EXploriNG SCIENCE COLLECT AND ANALYZE DATA USING THE CASIO FX-9750 AND EA-200 CONSTRUCTION OF A THERMOCOUPLE THERMOMETER By Jim Roberts, Professor of Physics and Material Science The University of North Texas OBJECTIVE: This experiment is designed to show you how to construct a thermocouple or a device made of two (couple) of dissimilar metals that can produce a voltage when heat is applied, to collect voltage data, to plot the results on a fx-9750G graphing calculator and make a thermometer using the results. INTRODUCTION There are two types of effects that arise when two dissimilar metals are brought in contact with each other and the temperature is changed at the junction. One effect produces an electrical potential (Seebeck effect) when heat is applied and the other effect is to cool the junction when a current is passed through the junction in the proper direction (Peltier effect). These two effects can be very useful. Since the voltage at the junction depends upon the temperature of the end points, we may generate a voltage by heating one junction while holding the other constant in temperature, a source of electromotive force. The other effect is to make a cooling device, a refrigerator, by passing a current through the junction in the proper direction. In figure 1 is shown a thermocouple. This is the structure of a commercial thermocouple that is capable of sensing temperature changes at the junction. A very practical usage of the thermocouple is to control the safety of gas delivering systems. This is done by allowing the voltage produced to control the valve that delivers gas to the burners. If the burner goes out, there is no heat to the thermocouple and the voltage drops to release the valve and close off the gas flow, thus preventing a potential explosion. All gas systems are now required, by law, to have such safety valves. The device shown in figure 1 can be produced by the use of two electrically dissimilar metals such as copper and iron or copper and constantan. When the device has been constructed, it can be calibrated to read voltage and convert this into a temperature scale. If the amplifier gain is high enough the voltage can be read using an EA-200 to collect the data points. When this has been completed, the data are transferred into the graphing calculator for processing and testing for linear behavior over the temperature range of interest. Figure 1. A thermocouple mounted into a finger and the thermocouple wires and junction exposed so it can be seen what is in the sensing probe. PROCEDURE Construct your thermal junction by twisting a copper and an iron or constantan wire together at the ends to form a closed loop. Cut the copper wire in two pieces at the center and clean the surface to make good electrical contact with the iron. The voltmeter mode of the EA-200 can now be used to measure any potential difference at the terminals. Figure 2. Schematic of the thermocouple set up for making a thermometer using the voltage generated by a thermocouple. The signal from the thermocouple was amplified to raise the voltage output and to match impedance to the EA-200 Data Collector/Analyzer. Place the thermocouple in a small test tube to isolate it from water. If the temperature of air is to be measured, the isolation test tube is not needed. The tube is to isolate the junction from electrical interaction with the water. Place the thermocouple in the tube in about 250 ml of water in a beaker and place the beaker on a hot plate. Connect the voltage probe to the terminals of the thermocouple to warm it over a range of temperatures. You can also change the temperature by using a hair dryer to blow hot air over the temperature probe and the thermocouple junction. Put the temperature probe in channel 2 with the voltage probe in channel 1. You are ready to collect temperature and voltage data so the thermocouple voltage can be calibrated to become temperature. 6 4 2 0 10.7 16.8 24.5 33.4 43.1 53.4 63.9 75.3 86.1 -2 -4 VOLTAGE -6 -8 -10 TEMPERATURE Figure 3. (Left) An Excel plot of voltage versus centigrade temperature for the thermocouple with a reference bath of ice and water to reference to 0 degrees centigrade. (Right) A picture of the fx-9750G calculator display window; the bold line is produced by equation 1 below. Usually the voltage produced by the thermocouple junction is linear over a reasonable range of temperatures. When the data has been transferred to the fx-9750G graphing calculator it is tested for linear behavior. When you finish the plot the statistics for a linear least squares routine can be analyzed to determine how well the data fit a linear response by the r2 value. If the data do not fit a linear response, the graphing calculator function for X2 is used. The number r2 should be very close to 1. The values change from +1…..-1. If the number is +1 the data has a perfectly linear response and the data are well correlated to a linear fit. If the value is -1 the data and a linear response are dis-correlated and the data have the greatest departure from a linear response. The data in figure 1 were fit by equation 1 as given below: T = -7.0592V + 33.524 (1) 2.4 2.3 2.2 2.1 2 1.9 VOLTAGE 1.8 1.7 1.6 1.5 14.8 19.1 23 28 33.6 39.5 46 52.7 59 64.9 TEMPERATURE (C) Figure 4. (Left) An Excel plot of the amplified voltage versus centigrade temperature for the thermocouple with a reference bath of ice and water to reference to 0 degrees centigrade. (Right) A picture of the fx-9750G calculator display for the same experiment. Note the curvature is more pronounced and the data fit a quadratic model. This effect is due to the nonlinear property of the amplifier. The pictures were taken with a QV-7000-SX digital camera. T = -104.849V2+331.175V -196.23 (2) The thermocouple can be used to measure temperature by making a voltage measurement and converting to centigrade temperature by using equation 1. The voltage depends on the gain of the amplifier so each unit must be calibrated for the amplifier used in the measurement. The thermocouples used were obtained from a hardware store and produce up to 30 millivolts when heated with a blue gas flame. They serve as safety devices in conventional hot water heaters. SUMMARY The temperature sensor needs to be calibrated against a reference. This may be ice and water at standard pressure or by use of a reference voltage against which the instrument is calibrated. Both procedures were tested in this experiment. The type thermocouple chosen must be one that will produce sufficient voltage to activate the meter used to measure the output voltage. Of an amplifier is used, any nonlinear response must be considered for the instrument to be accurate. QUESTIONS 1. Can you save money by taking the energy from the Sun and converting it into electricity by using a thermocouple? Discuss the costs involved in providing such energy, if you answered yes to the question. 2. In the thermocouple part of this experiment you learned about converting heat to electricity. Discuss how this may be done efficiently by using the Sun's energy. Recall that focusing the rays of the Sun will multiply the heat energy falling on a given area. 3. The apparatus shown in figure 1 of this exercise is a pyrometer or a device for determining temperature. Discuss how you think this thing works. 4. One of the properties of nature is that if one process works, the reverse is true. That is, the generator of electricity produces electricity when a magnet is moved in a coil of wire. (The generator rule.) The inverse of this is that a current through a wire will cause a magnet to move. (The motor rule.) Since heating the thermocouple junction produces a voltage, might a current through the junction cool it? Look up the Seebeck Effect and the Peltier Effect on the internet and discuss these in the light of the “two faces of scientific processes”. 5. How many thermocouples of the composition studied above will need to be placed in series to light a 120 volt light bulb? 6. Since the energy from the Sun can be used to heat the thermocouple to produce electricity in the day time, discuss how we can store this electrical energy to be used when the Sun is not shining. 7. The reference junction of the thermocouple system needs to be kept at a fixed temperature to provide a reference for the second junction. Describe how the fact that the temperature of the soil at the surface of the Earth relative to a few feet below the surface is several degrees higher can be used to provide a temperature change that can drive the thermocouple system. 8. Based on what you learned about the voltage potential, how much voltage can be produced by the temperature difference found at a depth of one meter relative to the surface temperature. Determine the temperature difference by using a temperature probe and the EA-200 Data Collector/Analyzer. STUDYING VOLTAGE GENERATION BY THE FORCE OF GRAVITY By Jim Roberts, Professor of Physics and Material Science The University of North Texas OBJECTIVE: This activity is designed to see how we can generate electricity using gravity, to collect data with a Data Collector/Analyzer and display the data on a fx-9750G graphing calculator and to quantify the results.
Recommended publications
  • Seebeck and Peltier Effects V
    Seebeck and Peltier Effects Introduction Thermal energy is usually a byproduct of other forms of energy such as chemical energy, mechanical energy, and electrical energy. The process in which electrical energy is transformed into thermal energy is called Joule heating. This is what causes wires to heat up when current runs through them, and is the basis for electric stoves, toasters, etc. Electron diffusion e e T2 e e e e e e T2<T1 e e e e e e e e cold hot I - + V Figure 1: Electrons diffuse from the hot to cold side of the metal (Thompson EMF) or semiconductor leaving holes on the cold side. I. Seebeck Effect (1821) When two ends of a conductor are held at different temperatures electrons at the hot junction at higher thermal velocities diffuse to the cold junction. Seebeck discovered that making one end of a metal bar hotter or colder than the other produced an EMF between the two ends. He experimented with junctions (simple mechanical connections) made between different conducting materials. He found that if he created a temperature difference between two electrically connected junctions (e.g., heating one of the junctions and cooling the other) the wire connecting the two junctions would cause a compass needle to deflect. He thought that he had discovered a way to transform thermal energy into a magnetic field. Later it was shown that a the electron diffusion current produced the magnetic field in the circuit a changing emf V ( Lenz’s Law). The magnitude of the emf V produced between the two junctions depends on the material and on the temperature ΔT12 through the linear relationship defining the Seebeck coefficient S for the material.
    [Show full text]
  • Practical Temperature Measurements
    Reference Temperatures We cannot build a temperature divider as we can a Metal A voltage divider, nor can we add temperatures as we + would add lengths to measure distance. We must rely eAB upon temperatures established by physical phenomena – which are easily observed and consistent in nature. The Metal B International Practical Temperature Scale (IPTS) is based on such phenomena. Revised in 1968, it eAB = SEEBECK VOLTAGE establishes eleven reference temperatures. Figure 3 eAB = Seebeck Voltage Since we have only these fixed temperatures to use All dissimilar metalFigures exhibit t3his effect. The most as a reference, we must use instruments to interpolate common combinations of two metals are listed in between them. But accurately interpolating between Appendix B of this application note, along with their these temperatures can require some fairly exotic important characteristics. For small changes in transducers, many of which are too complicated or temperature the Seebeck voltage is linearly proportional expensive to use in a practical situation. We shall limit to temperature: our discussion to the four most common temperature transducers: thermocouples, resistance-temperature ∆eAB = α∆T detector’s (RTD’s), thermistors, and integrated Where α, the Seebeck coefficient, is the constant of circuit sensors. proportionality. Measuring Thermocouple Voltage - We can’t measure the Seebeck voltage directly because we must IPTS-68 REFERENCE TEMPERATURES first connect a voltmeter to the thermocouple, and the 0 EQUILIBRIUM POINT K C voltmeter leads themselves create a new Triple Point of Hydrogen 13.81 -259.34 thermoelectric circuit. Liquid/Vapor Phase of Hydrogen 17.042 -256.108 at 25/76 Std.
    [Show full text]
  • Type T Thermocouple Copper-Constantan Temperature Vs Millivolt Table Degree C
    Technical Information Data Bulletin Type T Thermocouple Copper­Constantan T Extension Grade Temperature vs Millivolt Table Thermocouple Grade E + Copper Reference Junction 32°F + Copper M Temperature Range Maximum Thermocouple Grade Maximum Useful Temperature Range: Temperature Range P Thermocouple Grade: ­328 to 662°F –454 to 752°F ­ Consrantan ­200 to 350°C –270 to 400°C ­ Consrantan E Extension Grade: ­76 to 212°F Accuracy: Standard: 1.0°C or 0.75% ­60 to 100°C Special: 0.5°C or 0.4% R Recommended Applications: A Mild Oxidizing,Reducing Vacuum or Inert Environments. Good Where Moisture Is Present. Low Temperature Applications. T Temp0­1­2­3­4­5­6­7­8­9 U ­450 ­6.2544 ­6.2553 ­6.2562 ­6.2569 ­6.2575 ­440 ­6.2399 ­6.2417 ­6.2434 ­6.2451 ­6.2467 ­6.2482 ­6.2496 ­6.2509 ­6.2522 ­6.2533 R ­430 ­6.2174 ­6.2199 ­6.2225 ­6.2249 ­6.2273 ­6.2296 ­6.2318 ­6.2339 ­6.2360 ­6.2380 ­420 ­6.1873 ­6.1907 ­6.1939 ­6.1971 ­6.2002 ­6.2033 ­6.2062 ­6.2091 ­6.2119 ­6.2147 E ­410 ­6.1498 ­6.1539 ­6.1579 ­6.1619 ­6.1657 ­6.1695 ­6.1732 ­6.1769 ­6.1804 ­6.1839 ­400 ­6.1050 ­6.1098 ­6.1145 ­6.1192 ­6.1238 ­6.1283 ­6.1328 ­6.1372 ­6.1415 ­6.1457 ­390 ­6.0530 ­6.0585 ­6.0640 ­6.0693 ­6.0746 ­6.0799 ­6.0850 ­6.0901 ­6.0951 ­6.1001 & ­380 ­5.9945 ­6.0006 ­6.0067 ­6.0127 ­6.0187 ­6.0245 ­6.0304 ­6.0361 ­6.0418 ­6.0475 ­370 ­5.9299 ­5.9366 ­5.9433 ­5.9499 ­5.9564 ­5.9629 ­5.9694 ­5.9757 ­5.9820 ­5.9883 ­360 ­5.8598 ­5.8671 ­5.8743 ­5.8814 ­5.8885 ­5.8955 ­5.9025 ­5.9094 ­5.9163 ­5.9231 P ­350 ­5.7847 ­5.7924 ­5.8001 ­5.8077 ­5.8153 ­5.8228 ­5.8303 ­5.8378 ­5.8452
    [Show full text]
  • Introduction to Thermocouples and Thermocouple Assemblies
    Introduction to Thermocouples and Thermocouple Assemblies What is a thermocouple? relatively rugged, they are very often thermocouple junction is detached from A thermocouple is a sensor for used in industry. The following criteria the probe wall. Response time is measuring temperature. It consists of are used in selecting a thermocouple: slower than the grounded style, but the two dissimilar metals, joined together at • Temperature range ungrounded offers electrical isolation of one end, which produce a small unique • Chemical resistance of the 1 GΩ at 500 Vdc for diameters voltage at a given temperature. This thermocouple or sheath material ≥ 0.15 mm and 500 MΩ at 50 Vdc for voltage is measured and interpreted by • Abrasion and vibration resistance < 0.15 mm diameters. The a thermocouple thermometer. • Installation requirements (may thermocouple in the exposed junction need to be compatible with existing style protrudes out of the tip of the What are the different equipment; existing holes may sheath and is exposed to the thermocouple types? determine probe diameter). surrounding environment. This type Thermocouples are available in different offers the best response time, but is combinations of metals or ‘calibrations.’ How do I know which junction type limited in use to dry, noncorrosive and The four most common calibrations are to choose? (also see diagrams) nonpressurized applications. J, K, T and E. There are high temperature Sheathed thermocouple probes are calibrations R, S, C and GB. Each available with one of three junction What is ‘response time’? calibration has a different temperature types: grounded, ungrounded or A time constant has been defined range and environment, although the exposed.
    [Show full text]
  • Thermocouple Standards Platinum / Platinum Rhodium
    Thermocouple Standards 0 to 1600°C Platinum / Platinum Rhodium Type R & S Standard Thermocouple, Model 1600, Premium grade wire, gas tight assembly, g Type R and Type S No intermediate junctions. g Gas Tight Assembly g Premium Grade Wire The Isothermal range of Thermocouple Standards are the result of many years development. The type R and S standards will cover the range from 0°C to 1600°C. The measuring assembly comprises a 7mm x 300mm or 600mm gas tight 99.7% recrystallized alumina sheath inside which is a 2.5mm diameter twin bore tube holding the thermocouple. The inner 2.5mm assembly is removable since some calibration laboratories will only accept fine bore tubed thermocouples and some applications require fine bore tubing. The covered noble metal thermocouple wire connects the Also available without the physical cold junction - Specify No Cold Junction (NCJ). measuring sheath to the reference sheath which is a 4.5mm x 250mm stainless steel sheath suitable for Model 1600 referencing in a 0°C reference system. Two thermo electrically free multistrand copper wires (teflon coated) Hot Sheath connect the thermocouple to the voltage measuring device. Temperature Range 0°C to 1600°C (R or S) Emf Vs Temperature According to relevant document The thermocouple material is continuous from the hot or measuring junction to the cold, or referencing junction. Response Time 5 minutes Hot Junction see diagram Calibration Dimensions The 1600 is supplied with a certificate giving the error Connecting Cable see diagram between the ideal value and the actual emf of the thermo- couple at the gold point.
    [Show full text]
  • Specifications Overview Compatible Thermocouple Sensors Connecting
    HOBO® U12 J, K, S, T Thermocouple Data Logger (Part # U12-014) Inside this package: Thank you for purchasing a HOBO data logger. With proper care, it will give you years of accurate and reliable • HOBO U12 J, K, S, T measurements. Thermocouple Data Logger The HOBO U12 J, K, S, T Thermocouple data logger has a • Mounting kit with magnet, 12-bit resolution and can record up to 43,000 measurements hook-and-loop tape, tie- or events. The logger accepts J, K, S, and T type wrap mount, tie wrap, and thermocouple sensors, sold separately. The logger uses a two screws. direct USB interface for launching and data readout by a Doc # 13412-B, MAN-U12014 computer. Onset Computer Corporation An Onset software starter kit is required for logger operation. Visit www.onsetcomp.com for compatible software. Specifications Overview J type: 0 to 750 °C (32° to 1382°F) The U12 Thermocouple logger has two temperature channels. K type: 0 to 1250 °C (32° to 2282°F) Channel 1 is for a user-attached thermocouple. Channel 2 is the Measurement S type: -50 to 1760 °C (-58° to 3200°F) logger’s internal temperature, which is used for cold-junction range T type: -200 to 100 °C (-328° to 212°F) compensation of the thermocouple output. The logger can also Internal temperature: 0° to 50°C (32° to record the logger’s battery voltage (Channel 3) if selected. The 122°F) number of channels selected determines the maximum J type: ±2.5°C or 0.5% of reading, deployment time at a given sample interval.
    [Show full text]
  • In-Situ Measurement and Numerical Simulation of Linear
    IN-SITU MEASUREMENT AND NUMERICAL SIMULATION OF LINEAR FRICTION WELDING OF Ti-6Al-4V Dissertation Presented in Partial Fulfillment of the Requirements for the Degree Doctor of Philosophy in the Graduate School of The Ohio State University By Kaiwen Zhang Graduate Program in Welding Engineering The Ohio State University 2020 Dissertation Committee Dr. Wei Zhang, advisor Dr. David H. Phillips Dr. Avraham Benatar Dr. Vadim Utkin Copyrighted by Kaiwen Zhang 2020 1 Abstract Traditional fusion welding of advanced structural alloys typically involves several concerns associated with melting and solidification. For example, defects from molten metal solidification may act as crack initiation sites. Segregation of alloying elements during solidification may change weld metal’s local chemistry, making it prone to corrosion. Moreover, the high heat input required to generate the molten weld pool can introduce distortion on cooling. Linear friction welding (LFW) is a solid-state joining process which can produce high-integrity welds between either similar or dissimilar materials, while eliminating solidification defects and reducing distortion. Currently the linear friction welding process is most widely used in the aerospace industry for the fabrication of integrated compressor blades to disks (BLISKs) made of titanium alloys. In addition, there is an interest in applying LFW to manufacture low-cost titanium alloy hardware in other applications. In particular, LFW has been shown capable of producing net-shape titanium pre-forms, which could lead to significant cost reduction in machining and raw material usage. Applications of LFW beyond manufacturing of BLISKs are still limited as developing and quantifying robust processing parameters for high-quality joints can be costly and time consuming.
    [Show full text]
  • PFA Insulated Thermocouple Grade Wire
    Thermocouple Grade Wire Single Pair - PFA Insulated A range of PFA insulated single pair Thermocouple Grade Wire available from stock for immediate delivery TC for Temperature Sensing, Measurement and Control PFA Thermocouple Grade Wire PFA Insulated Twisted Pair / PFA Insulated Bonded ‘Bell Wire’ -100°F to +480°F PFA is ideal for higher temperature applications up to 480°F. It is also excellent for cryogenic temperatures down to -100°F Withstands attack from virtually all known chemicals, oils and fluids. All our PFA wire are made in extruded form and are therefore gas, steam and water tight which makes them most suitable for applications such as autoclaves or sterilizers Twisted pair construction with either solid PFA Twisted Pair PFA Twisted Pair PFA Bonded ‘Bell Wire’ or stranded conductors in a range of sizes. One pair of solid conductors One pair of stranded conductors One pair of solid conductors. Ideal for making simple thermocouples PFA insulated. Pair twisted. PFA insulated. Pair twisted. Pair laid flat and PFA sheathed. Oval, bonded construction. Bonded ‘bell wire’ for autoclave applications Stock Number B10 B11 B12 B53 B54 B16 Wire Type (number of strands x AWG) Solid Solid Solid 7x26 7x32 Solid Total Wire Size - AWG (S = Stranded) 32 28 24 26S 24S 24 Total Area (mm2 ) 0.03 0.07 0.2 0.124 0.22 0.2 Insulation PFA PFA PFA CONDUCTORS Number of Pairs 1 1 1 Conductor Configuration Twisted Twisted Parallel PAIRS Shielded No No No Insulation — — — Continuous Insulation -100 to +480 -100 to +480 -100 to +480 Rating (°F) Short Term +570 +570 +570 Color Coding Yes Yes Yes Abrasion Resistance Good Good Good Physical Moisture Resistance Properties Very Good Very Good Very Good OVERALL Typical Weight (lbs/1000ft) (excluding reel) 7 7 7 7 7 7 Diameter under Armor (inches) — — — Diameter over Armor (inches) — — — Overall Diameter† (inches) 0.08” 0.08” 0.08” 0.059” 0.12” 0.037”x0.077” Notes Rejects electromagnetic Rejects electromagnetic Gas, steam and water interference.
    [Show full text]
  • Room Temperature Seebeck Coefficient Measurement of Metals and Semiconductors
    Room Temperature Seebeck Coefficient Measurement of Metals and Semiconductors by Novela Auparay As part of requirement for the degree of Bachelor Science in Physics Oregon State University June 11, 2013 Abstract When two dissimilar metals are connected with different temperature in each end of the joints, an electrical potential is induced by the flow of excited electrons from the hot joint to the cold joint. The ratio of the induced potential to the difference in temperature of between both joints is called Seebeck coefficient. Semiconductors are known to have high Seebeck coefficient values(∼ 200-300 µV/K). Unlike semiconductors, metals have low Seebeck coefficient (∼ 0-3 µV/K). Seebeck coefficient of metals, such as aluminum and niobium, and semiconductor, such as tin sulfide is measured at room temperature. These measurements show that our system is capable to measure Seebeck coefficient in range of (∼ 0-300 µV/K). The error in the system is measured to be ±0:14 µV/K. Acknowledgements I would like to thank Dr. Janet Tate for giving me the opportunity to work in her lab. I would like to thank her for her endless support and patience in helping me complete this project. I would like to thank Jason Francis who made the samples and wrote the program used in this project. I would like to thank the department of human resources of Papua, Indonesia for giving me the opportunity to study at Oregon State University. I would like to thank Corinne Manogue and Mary Bridget Kustusch for all the support they gave me along the way.
    [Show full text]
  • Thermocouple Introduction and Theory
    Reference Temperatures We cannot build a temperature divider as we can a Metal A voltage divider, nor can we add temperatures as we + would add lengths to measure distance. We must rely eAB upon temperatures established by physical phenomena – which are easily observed and consistent in nature. The Metal B International Practical Temperature Scale (IPTS) is based on such phenomena. Revised in 1968, it eAB = SEEBECK VOLTAGE establishes eleven reference temperatures. Figure 3 Since we have only these fixed temperatures to use All dissimilar metals exhibit this effect. The most as a reference, we must use instruments to interpolate common combinations of two metals are listed in between them. But accurately interpolating between Appendix B of this application note, along with their these temperatures can require some fairly exotic important characteristics. For small changes in transducers, many of which are too complicated or temperature the Seebeck voltage is linearly proportional expensive to use in a practical situation. We shall limit to temperature: our discussion to the four most common temperature ∆ α∆ transducers: thermocouples, resistance-temperature eAB = T detector’s (RTD’s), thermistors, and integrated Where α, the Seebeck coefficient, is the constant of circuit sensors. proportionality. Measuring Thermocouple Voltage - We can’t measure the Seebeck voltage directly because we must IPTS-68 REFERENCE TEMPERATURES first connect a voltmeter to the thermocouple, and the 0 EQUILIBRIUM POINT K C voltmeter leads themselves create a
    [Show full text]
  • Thermocouple Temperature Measurement
    Acromag, Incorporated 30765 S Wixom Rd, PO Box 437, Wixom, MI 48393-7037 USA Tel: 248-295-0880 • Fax: 248-624-9234 • www.acromag.com CRITERIA FOR TEMPERATURE SENSOR SELECTION OF T/C AND RTD SENSOR TYPES The Basics of Temperature Measurement Using Thermocouples Part 1 of 3 Copyright © Acromag, Inc. April 2011 8500-911-A10M000 Trademarks are the property of their respective owners. CRITERIA FOR TEMPERATURE SENSOR SELECTION OF T/C AND RTD SENSOR TYPES Part 1 of 3: The Basics of Temperature Measurement Using Thermocouples Background Temperature reigns as the most often measured process parameter in industry. While temperature measurement utilizes sensors of many forms, the actual measurement of temperature is accomplished via only five basic sensor types: Thermocouple (T/C), Resistance Temperature Detector (RTD), Thermistor, Infrared Detector, and via semiconductor or integrated circuit (IC) temperature sensors. Of these five common types, the thermistor is perhaps the most commonly applied for general purpose applications. Semiconductor sensors dominate most printed circuit board or board level sensing applications. Infrared is used for non-contact line-of-sight measurement. But for industrial applications that typically employ remote sensing, thermocouples and RTD’s reign as the most popular sensor types. Most industrial applications require that a temperature be measured remotely, and that this signal be transmitted some distance. An industrial transmitter is commonly used to amplify, isolate, and convert the low-level sensor signal to a high level signal suitable for monitoring or retransmission. With respect to these transmitters, your choice of sensor type is generally limited to T/C, or RTD.
    [Show full text]
  • How to Maximize Temperature Measurement Accuracy
    technicalNOTE How to Maximize Temperature Measurement Accuracy INTRODUCTION Thermocouples are the most versatile and widely used devices for temperature measurements. They are inexpensive, reliable, rugged, and can be used over a wide temperature range. These sensors require cold junction compensation and complex linearization algorithms to achieve good accuracy. The output voltage of thermocouples is very small (tenths of mV) and hence require high gain amplifiers before being fed to the ADC. Any errors and non-linearity in these areas of signal conditioning and amplification will lead to inaccurate measurements. Most test engineers are careful about the measurement errors caused by thermocouples, but not always about the measurement system. Measurement systems are calibrated regularly (typically once per year) at ambient room temperatures and are expected to perform throughout the year with the same accuracies. What if the measurement system is placed where the temperature is not at ambient room temperature? Is the measured data accurate? This application note focuses on this lesser known and important aspect called “Self-Calibration”. Measurement instruments will be highly accurate only when they are compensated for conditions like gain drifting, aging and temperature variations. PRIMARY SOURCES OF ERRORS WITH THERMOCOUPLE MEASUREMENTS Let us look at the Primary Error Sources. They can be broadly categorized as: 1) Errors due to the measurement system 2) Errors due to the thermocouple CJC Errors: CJC error is one of the single largest contributors to overall accuracy. CJC is responsible for compensating the voltage difference as cold junction is not maintained at an ideal zero temperature. WWW.VTIINSTRUMENTS.COM RELIABLE DATA FIRST TIME EVERY TIME technicalNOTE The overall CJC error includes: DID YOU KNOW? The EX10xxA family 1.
    [Show full text]