Temperature Measurement
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Temperature Measurement S. Wang Juming Tang F. Younce Washington State University, Pullman, Washington, U.S.A. INTRODUCTION (e.g., epoxy, glass, stainless steel) and are in the form of beads, rods, probes, and disks. Sensors can be made as Temperature is a principle parameter that needs to be small as 0.1 mm in diameter to give short response time. monitoredandcontrolledinmostfoodprocessing Glass and stainless steel-sheathed probes between 2 mm operations such as heating, cooling, drying and storage. and 3 mm are widely used. In measurement, a thermistor is Temperature sensors have been developed based on connected to one leg of a Wheatstone bridge to yield a different temperature-dependent physical phenomena resolution as precise as 0.00058C.[3] Accuracy of a including thermal expansion, thermoelectricity, electrical thermistor sensor is often limited by the readout device resistance, and thermal radiation.[1,2] Temperature sensors with a resolution of only ^ 0.18C. Nonlinearity in used in agricultural and food industries and research vary electrical resistance output limits application of a from simple liquid-in-glass thermometers to sophisticated thermistor to relatively narrow temperature ranges (e.g., and state-of-art thermal imaging. This article focuses only within 1008C). Long-term output stability is another on temperature sensors that generate digital signals readily common problem of thermistor probes. used for on-line monitoring and automatic temperature The RTD uses metal materials (e.g., platinum) as the control purposes. The article focuses on the commonly sensing element. Electrical resistance in a metal changes in used temperature sensors, principles, precision, response a predictable manner with temperature. A general time, advantages, and limitations for agricultural and food relationship is used to convert electrical resistance R to engineering applications. temperature T: 2 3 RT ¼ R0ð1 þ aT þ bT þ cT þ ···Þ ð2Þ PRINCIPLES AND PROPERTIES where RT is the electrical resistance at temperature T, R0 is the electrical resistance at a reference temperature, Resistance Thermometers usually 08C, and a, b, and c are material constants. The number of terms used in Eq. 2 depends on the material used Resistance thermometers measure temperature of an in the sensor, the temperature range to be measured, and the object based on changes in electrical resistance of the accuracy required. In many cases, only constant, a, is used sensing element. Two types of resistance thermometers are to provide satisfactory accuracy over limited temperature commonly used: thermistors and resistance temperature ranges. Fig. 1 shows the temperature range and the output devices (RTD). resistance ratio of the three commonly used metals: A thermistor uses a semiconductor as the sensing platinum, nickel, and copper. The RTD has a small positive element. The electrical resistance of the semiconductor, 2 2 temperature resistance coefficient of 0.0039 VV 1 8C 1 made mostly from metallic oxides (e.g., NiO), decreases for a platinum RTD at 258C as compared with a high sharply as the temperature increases. Response follows the negative temperature resistance coefficient of about general relationship[3]: 20.045 for a thermistor with a b value of 4000. bð1=T21=T0Þ The most widely used RTD is a platinum resistance R ¼ R0 e ð1Þ sensor, which is measured to be 100 V and 139 V where R is the electrical resistance (V) at temperature T corresponding with 0 and 1008C, respectively. Lead wire (K), R0 is the electrical resistance at a reference resistance and changes in lead wire resistance with temperature, T0. b is a constant for specific materials (K) temperature may have significant effects on the resistance and is in the order of 4000. The reference temperature, T0, readings. In application, RTD resistance is transformed is generally taken as 298K (258C). into voltage and measured in a bridge circuit connected by The sensing elements of commercially available two, three, or four wires according to application thermistors are protected by noncorrosive materials objectives and the need to minimize the influence of lead Encyclopedia of Agricultural, Food, and Biological Engineering 987 DOI: 10.1081/E-EAFE 120006895 Copyright q 2003 by Marcel Dekker, Inc. All rights reserved. 988 Temperature Measurement Fig. 1 Resistance–temperature relationship for platinum, nickel, and copper. wire resistance. The RTD can be applied to measure solid, junction is maintained at a known reference temperature liquid, and gas substances at temperatures between 2200 (Tref) while the other is positioned for temperature and 8008C. A major problem with RTD sensors is the measurement. The temperature to be measured (T)is relatively slow response time due to the protective sheath converted from thermoelectric voltage V according to: (ceramic, glass, or stainless steel). Sensor accuracy of the order of 0.28C can be reached with careful calibration in V T ¼ Tref þ ð3Þ specific temperature ranges. a Thermocouples where V is the measured voltage in the thermocouple circuit and a is the voltage/temperature proportionality constant 21 When two dissimilar metals are joined at two points (V 8C ). Voltage can be measured with a potentiometer or (Fig. 2), a thermocouple circuit is formed. When these two a high-impedance solid-state digital voltmeter. The value of junctions are at different temperatures, an electromotive constant a depends on the type of wires used to make the force (emf) develops, causing an electric current to flow thermocouple. Theoretically, for precision work the through the circuit. The magnitude of this emf is reference junctions should be kept in a triple-point-of proportional to the temperature difference between the water apparatus that maintains a fixed temperature of ^ two junctions. This physical phenomenon, referred to as 0.01 0.00058C. In reality, the reference temperature, Tref, thermoelectricity, was discovered by T. J. Seebeck in can be room temperature, measured with a thermistor in 1821. The thermoelectricity is used for temperature most computer-based data acquisition systems. measurement in thermocouple systems, in which one Different pairs of metals are used for thermocouple types commercially labeled as types S (platinum/plati- num–10% rhodium), R (platinum/platinum–13% rho- dium), B (platinum–30% rhodium/platinum–6% rhodium), J (iron/constantan), T (copper/constantan), K (chrome/aluminum), and E (chromel/constantan). Typical characteristics of these thermocouples are shown in Fig. 3.[3] Thermocouples give relatively low voltage outputs (e.g., 0.04 mV 8C21 for type T). Type E Fig. 2 Thermocouple circuit to measure temperature (T) with thermocouples have the highest voltage output per degree the cold junction (Tref) from the output voltage (V). among all commonly used thermocouple types, but type E Temperature Measurement 989 Fig. 3 Typical voltage–temperature relationship for common thermocouple materials when the reference temperature is 08C. thermocouples are not suited for reducing, sulfurous, Gaynor[5] is: vacuum, and low-oxygen environments. Types T and J are 2 commonly used in industrial applications, because of their L 2 1 1 Ts ¼ þ 2273:15 ð4Þ resistance to corrosion and harsh environments. For 1612 t1 t2 example, type J can be used between 2150 and 7608Cin both oxidizing and reducing environments, while type T where L is the distance between the transducers (m), t1 and can be used between 2200 and 3508C. The upper t2 are the travel times in each direction (sec). This sensor temperature limit for type T is due to oxidation of copper has a high sampling rate of up to 50 times per second. at temperatures greater than 3508C. The measurement precision may reach 0.4% after careful The temperature-sensitive element in thermocouples calibration. can be made very small to provide a response time of only a few seconds.[4] Thermocouples can be used to Radiation Thermometer detect the transient temperature in a solid, liquid, and gas, with an accuracy of ^0.25% of reading for types Radiation thermometers (often referred to radiometer, R and S, and ^0.5% reading for type T over a radiation pyrometer, or optic pyrometer) operate using measurement range of 1008C. Generally, thermocouples electromagnetic radiation in the visible spectrum cannot be used in electromagnetic fields, because the metallic elements may interact with the electro- magnetic field. Sonic Thermometer The basic principle of a sonic thermometer is the measurement of the time of an ultrasound pulse traveling between two transducers (Fig. 4). It is well known that the speed of sound increases when the air moves in the same direction as the sound. This pair of transducers (a, b) act alternately as transmitters and receivers, exchanging high- frequency ultrasound pulses. This speed of sound in air is used for rapid calculation of air temperature. The output of Fig. 4 Sonic anemometer (v, air speed; L, the distance between [11] the sonic temperature (Ts, 8C) according to Kaimal and transducers a and b). (From Ref. .) 990 Temperature Measurement (0.3 mm–0.72 mm) and a portion of the infrared region A Fabry-Perot interferometer (FPI) consists of two (0.72 mm–40mm). A radiation thermometer may use parallel reflective surfaces that form a cavity resonator. either a thermal detector or photon detectors as its sensing The space separating these two surfaces, also called the element. Thermal detectors are blackened elements FPI cavity (1–2 wavelengths deep), varies with tempera- designed to absorb incoming radiation