الرحيـــــِ ِم َّ الر ْح َم ِن َّ ِـــــم هللا ِ ِب ْس Temperature Measurements Principles Measuring Devices Applications Definition of Temperature • An expression for the kinetic energy of vibrating atoms and molecules of matter. • Can be measured by various secondary phenomena, e.g., – – – – – change of volume or pressure, electrical resistance, electromagnetic force, electron surface charge, or emission of electromagnetic radiation. 12 Oct. 2015 BME 353 - Biomedical Measurements and Instrumentation 2 Direct and Indirect • Many engineering applications require direct measurement of temperature. – – – – Synthetic fuel research, solar energy conversion and new engine development are a few of these disciplines. All industries place new emphasis on energy efficiency. Hence, the fundamental measurement of temperature assumes new importance. • Temperature also effects measurement of most physical variables and it must be measured for compensation purposes as well. 12 Oct. 2015 BME 353 - Biomedical Measurements and Instrumentation 3 Temperature Scale • Celsius, divide the difference between the freezing and boiling points of water into 100° • Fahrenheit which divide the difference between the freezing and boiling points of water into 180° • °C = (5 /9) (°F - 32), and °F = (9 /5) °C + 32. • The thermodynamic scale begins at absolute zero, or 0 Kelvin, the point at which all atoms cease vibrating and no kinetic energy is dissipated. • 0 K = –273.15° C = –459.67° F. – The official Kelvin scale does not carry a degree sign. The units are expressed in “kelvins,” not degrees Kelvin. 12 Oct. 2015 BME 353 - Biomedical Measurements and Instrumentation 4 Reference Temperatures • No temperature divider or adder • We must rely upon temperatures established by physical phenomena which are easily observed and consistent in nature. • The International Temperature Scale (ITS) establishes seventeen fixed points and corresponding temperatures. Examples: – the triple-point (the temperature and pressure at which solid, liquid, and gas phases of a given substance are all present simultaneously in varying amounts) of water = 0.01C, – triple-point of hydrogen = -259.3467C, and – freezing point of silver = 961.78C. 12 Oct. 2015 BME 353 - Biomedical Measurements and Instrumentation 5 Heat Gain and Heat Loss • Heat gain: – – – – Environment Metabolism Hot food Shivering 12 Oct. 2015 • Heat loss: – – – – Convection Conduction Evaporation IR radiation BME 353 - Biomedical Measurements and Instrumentation 6 Temperature measuring devices • Temperature can be measured via a diverse array of sensors. All of them infer temperature by sensing some change in a physical characteristic. • In the chemical process industries, the most commonly used temperature sensors are thermocouples, resistive devices and infrared devices. 12 Oct. 2015 • thermocouples, • resistance temperature devices – RTD’s and – Thermistors • • • • • infrared radiators, I.C. sensors, bimetallic devices, liquid expansion devices, change-of-state devices. BME 353 - Biomedical Measurements and Instrumentation 7 Thermocouples Metal A Metal A Metal B + VAB - Metal A Metal B VAB = Seebeck voltage • Two strips or wires made of different metals and joined at one end. • Changes in temperature at that junction induce changes in the emf between the other ends. • As temperature goes up, this output emf of the thermocouple rises, though not necessarily linearly. VAB = T, where , the Seebeck coefficient, is the constant of proportionality. For real world thermocouples, is not constant but varies with temperature. 12 Oct. 2015 BME 353 - Biomedical Measurements and Instrumentation 8 Peltier effect • If a voltage is applied, then there will be temperature change at the junction. This is called the Peltier effect and can be used for heating and cooling (refrigeration). 12 Oct. 2015 BME 353 - Biomedical Measurements and Instrumentation 9 Equation of a thermocouple • The output voltage “V” of a simple thermocouple (with a reference temperature T0 = 0C = 32F) is: 1 1 2 V AT BT CT 3 2 3 volts, where T is the temperature of the measuring junction in C, A, B, and C are constants that depend upon the thermocouple material. The sensitivity V 2 S A BT CT T 12 Oct. 2015 volt/C BME 353 - Biomedical Measurements and Instrumentation 10 Characteristics of thermocouples 80 E 60 Millivolts K J 40 20 T R S 0 500 1000 1500 2000 Temperature, C 12 Oct. 2015 Type of Metals + E Chromel vs Constantan J Iron vs Constantan K Chromel vs Alumel R Platinum vs Platinum 13% Rhodium S Platinum vs Platinum 10% Rhodium T Copper vs Constantan Constantan is a metal alloy with %60 copper and %40 nickel BME 353 - Biomedical Measurements and Instrumentation 11 12 Oct. 2015 BME 353 - Biomedical Measurements and Instrumentation 12 Resistance Temperature Devices – fine platinum wire wrapped around a mandrel and covered with a protective coating (also abbreviated PRTD). – most stable temp trans. • Film RTD – a platinum or metal-glass slurry film is deposited or screened onto a small flat ceramic substrate, etched with a lasertrimming system, and sealed – device size itself is small, which means it can respond quickly to step changes in temperature. • Film RTD’s are less stable 12 Oct. 2015 • Thermistors – NTC – PTC • most sensitive temperature transducer V or T • RTD’s R = R0[1 + (T – T0)] • platinum, nickel, or ni alloys Thermistor RTD Thermocouple Temperature, C BME 353 - Biomedical Measurements and Instrumentation 13 Equation of a thermistor Steinhart-Hart equation: a simpler equation: 1 A B(ln R) C (ln R) 3 T T 1 C (ln R ) A R R0e 12 Oct. 2015 ( T0 T TT0 BME 353 - Biomedical Measurements and Instrumentation ) 14 The Self-Heating Problem 100 0 slope Voltage, V 10 - slope 1.0 + slope 0.1 0.10 1.0 10.0 100.0 Current, mA 12 Oct. 2015 BME 353 - Biomedical Measurements and Instrumentation 15 Integrated Circuit (I.C.) Sensors + + 1 A/K To DVM Current sensor 12 Oct. 2015 10 mV/K 1 M To DVM Voltage sensor BME 353 - Biomedical Measurements and Instrumentation 16 RTD T Self powered Simple Rugged Inexpensive Wide variety of physical forms Wide temperature range Non-linear Low voltage Reference required Least stable Least sensitive 12 Oct. 2015 Resistance Voltage Disadvantages Advantages Temperature I.C. Sensor R R Resistance V Thermistor Temperature Most stable Most accurate More linear than thermocouple T Temperature High output Fast Two-wire ohmic measurement Expensive Non-linear Slow Limited temperature range Current source Fragile required Small resistance Current source change required Four-wireBME 353 - Biomedical Self-heating Measurements and Instrumentation measurement T Voltage or current Thermocouple V or I Temperature Most linear Highest output Inexpensive T < 250C Power supply required Self-heating Limited configurations 17 T Bimetallic Devices Metal A Metal B 12 Oct. 2015 BME 353 - Biomedical Measurements and Instrumentation 18 Fluid-Expansion Devices • Types: Safety bulb 50 – the mercury type: an environmental hazard, so there are regulations governing the shipment of devices that contain it. – the organic-liquid type. – gas instead of liquid type • No electric power, do not pose explosion hazards, and are stable even after repeated cycling. • On the other hand, – they do not generate data that are easily recorded or transmitted, and – they cannot make spot or point 12 Oct.measurements. 2015 BME 353 - Biomedical Measurements and Instrumentation Capillary tube Stem 0 Temperature sensing bulb 19 Chemical (Change-of-State) Sensors • Change-of-state temperature sensors – labels, pellets, crayons,lacquers or liquid crystals whose appearance changes when a certain temperature is reached. – They are used, for instance, with steam traps – when a trap exceeds a certain temperature, a white dot on a sensor label attached to the trap will turn black. – Response time typically takes minutes, so these devices often do not respond to transient temperature changes, and accuracy is lower than other types of sensors. – the change in state is irreversible, except in the case of liquid-crystal displays. – Even so, change-of-state sensors can be handy when one needs confirmation that the temperature of a piece of equipment or a material has not exceeded a certain level, for instance for technical or legal reasons, during product shipment 12 Oct. 2015 BME 353 - Biomedical Measurements and Instrumentation 20 Radiation Detectors (IR Sensors) 12 Oct. 2015 BME 353 - Biomedical Measurements and Instrumentation 21 100% 0.00312 0.003 80 60 0.002 40 0.001 20 T = 300 K 5 10 15 20 25 % Total power Spectral radient emittance, W-cm-2·mm-1 m= 9.66 m Spectral radiant emittance versus wavelength for a blackbody at 300 K on the left vertical axis; percentage of total energy on the right vertical axis. 12 Oct. 2015 BME 353 - Biomedical Measurements and Instrumentation 22 Fused silica 100 Sapphire Arsenic trisulfide Thallium bromide iodine 50 10 0 1 10 100 Wavelength, m Spectral transmission for a number of optical materials. 12 Oct. 2015 BME 353 - Biomedical Measurements and Instrumentation 23 All thermal detectors 100 Indium antimonide (InSb) (photovoltaic) 60 Lead sulfide (PbS) 20 0 1 2 3 4 5 6 7 8 Wavelength, m Spectral sensitivity of photon and thermal detectors. 12 Oct. 2015 BME 353 - Biomedical Measurements and Instrumentation 24 Shutter Ear IR Ambient sensor Micro processor Ta Tb MUX A/D Amp. Sensor Waveguide Window Shutter switch Digital display The infrared thermometer opens a shutter to expose the sensor to radiation from the tympanic membrane. 12 Oct. 2015 BME 353 - Biomedical Measurements and Instrumentation 25 Details of the fiber/sensor arrangement for the GaAs semiconductor temperature probe. 12 Oct. 2015 BME 353 - Biomedical Measurements and Instrumentation 26