Instrumentation & Measurement _____________________________________________________ _ AAiT Chapter 3 Transducers and Their Response 3.1 Transducer Instrument Society of America defines a sensor or transducer as a device which provides a usable output in response to a specified measured. Here the measured is a physical quantity and the output may be an electrical quantity, mechanical and- optical. Sensor An element that senses a variation in input energy to produce a variation in another or same form of energy is called a sensor. Transducer Transducer converts a specified measured into usable output using transduction principle. For example, a properly cut piezoelectric crystal can be called a sensor where as it becomes a transducer with appropriate electrodes and input/output mechanisms attached to it. So, the sensor is the primary element of a transducer. Transducers is a devices used to transform one kind of energy to another. When a transducer converts a measurable quantity (temperature, pressure, level, optical intensity, magnetic field, etc) to an electrical voltage or an electrical current we call it a sensor. Energy information conversion is the objective of a sensor. The information available in one energy form must be converted into the same or another energy form, with exactly the same information content as the originating energy form. The sensor or the sensing element is the first element in a measuring system and takes information about the variable being measured and transforms it into a more suitable form to be measured. Sensor is sometimes called a primary measuring element, it can be found simply as a mercury thermometer to measure the temperature. It may be embedded in the transducer to perform its function. That means the transducer consists of a primary element (sensor) plus a secondary _____________________________________________________________________________________ Compiled by Yidnekachew M. Page 1 of 9 Instrumentation & Measurement _____________________________________________________ _ AAiT element (signal conditioning circuit) that transforms the passive change or small voltage signal into active signal range that can be easily used in other chains of the control loop. A transducer can be defined as a device capable of converting energy from one form into another. Transducers can be found both at the input as well as at the output stage of a measuring system. The input transducer is called the sensor, because it senses the desired physical quantity and converts it into another energy form. The output transducer is called the actuator, because it converts the energy into a form to which another independent system can react, whether it is a biological system or a technical system. So, for a biological system the actuator can be a numerical display or a loudspeaker to which the visual or aural senses react respectively. For a technical system the actuator could be a recorder or a laser, producing holes in a ceramic material. The results can be interpreted by humans. Actuators are important in instrumentation. They allow the use of feedback at the source of the measurement. However we will pay little attention to them in this course. The study of using actuators and feedback belongs to a course in Control theory. 3.2 Types of Energy Form We can distinguish six different energy domains: (1) radiant, (2) mechanical, (3) thermal, (4) electrical, (5) magnetic and (6) chemical. If certain information is already available in the electrical domain it can be claimed that it requires no energy conversion, but in general there is 'shape' conversion left and this is just the domain which belongs to the field of electronics and electrical science and engineering. A good example of such a sensor only sensitive to electrical energy is the probe of an oscilloscope, with which a good adaptation to the signal source is realized. In the modifier stage we meet other examples of shape converters, for instance the A/D and D/A converters. Table 1.6 Energy types and corresponding measured _____________________________________________________________________________________ Compiled by Yidnekachew M. Page 2 of 9 Instrumentation & Measurement _____________________________________________________ _ Energy Measurands Length, area, volume, force, pressure, acceleration, torque, mass flow, acoustic intensity and so on. Temperature, heat flow, entropy, state of matter Charge, current, voltage, resistance, inductance, capacitance, dielectric constant, polarization, frequency, electric field, dipole moment, and so on. Field intensity, flux density, permeability, magnetic moment, and so on. Intensity, phase, refractive index, reflectance, transmittance, absorbance, wavelength, polarization, and so on. Concentration, composition, oxidation/reduction potential, Reaction rate, pH and the like. Mechanical Thermal Electrical Magnetic Radiant Chemical 3.3 AAiT Classification of transducers The transducers may be classified based on i. i. The physical effect employed ii. The physical quantity measured iii. The source of energy Classification based on physical effect The physical quantity applied as measurand (quantity to be measured) to the transducer causes some physical changes in its element. By this physical effect the transducer converts the physical quantity in to electrical quantity. For example, a change in temperature to be measured causes variation of resistance (physical change) in a copper wire (element) and this effect could, be used to convert temperature in to an electrical output, The physical effects commonly employed are a. b. c. d. e. Variation of resistance Variation. of inductance Variation of capacitance Piezo electric effect Magnetostrictive effect _____________________________________________________________________________________ Compiled by Yidnekachew M. Page 3 of 9 Instrumentation & Measurement _____________________________________________________ _ AAiT f. Elastic effect g. Hall effect a. Variation of resistance The resistance of a length of metallic wire is given by R= ρl a Where, R = Resistance in ohm. ρ =Resistivity (or specific resistance) of the material in ohm-m. l = length of wire in m. a = Area of cross-section in m2. As resistance is a function of ρ , l , a (i.e) R = f ( ρ , l , a ) , with any change in anyone of the physical quantities ρ , a or l due to variation in resistance, a variable resistance transducer can be designed to convert physical quantity. Some of the transducers based on this principle are potentiometer, strain gauge, resistance thermometer, carbon microphone, and photoconductive cell. • The resistance thermometer is based upon thermo resistive effect which is the change in electrical resistivity of a metal or semiconductor due to change in temperature co-efficient of resistivity. • Carbon microphone works on the principle of change in contact resistance due to applied pressure. • Photoconductive cell is based on photoconductive effect which is the change in electrical conductivity due, to incident light. • Potentiometer works on the principle of change in resistance due to linear or rotational motion. • Strain gauge works on the principle of change in resistance due to applied pressure. b. Variation of inductance _____________________________________________________________________________________ Compiled by Yidnekachew M. Page 4 of 9 Instrumentation & Measurement _____________________________________________________ _ AAiT The inductance of a coil is given by L=N L= dφ dt N 2 µo µ r A l where, L = inductance in henry N = No., of turns µo = absolute permeability µr = relative permeability A = area of cross section of the core l = length of magnetic path dφ = rate of change of magnetic flux. dt As L is a function, of N, µr , A, l , (i.e) L = f (N, µr ,A, l ), when anyone of these quantities changes, the inductance changes. This leads to the design of a variable inductance transducer. Some of the transducers based on variation of inductance are induction potentiometer, linear variable differential transformer (LVDT) and synchros. c. Variation of capacitance The capacitance between two conductor plates is given by C= ε oε r A d Where C = capacitance in farad ε o = absolute permittivity _____________________________________________________________________________________ Compiled by Yidnekachew M. Page 5 of 9 Instrumentation & Measurement _____________________________________________________ _ AAiT ε r = relative permittivity of the separating medium A = area of cross-section of the plates As C is a function of ε r , A, d i.e C = ( ε r , A, d ) when anyone of these quantities changes, the capacitance varies. This leads to the design of a variable capacitance transducer. d. Piezoelectric effect When a piezoelectric crystal like quartz or Rochelle salt is subjected to mechanical stress, an electric charge is generated. This is known as piezoelectric effect. The transducer based on this effect is piezoelectric transducer. e. Magnetostrictive effect When a magnetic material is subjected to mechanical stress, its permeability changes. This effect is magnetostrictive effect and the transducer based on this effect is magnetostrictive transducer. f. Elastic effect When an elastic member is subjected to mechanical stress it is deformed. The transducer based on this effect is called elastic transducer. g. Hall effect When a magnetic field is applied to a current carrying conductor at right angles to the direction of current, a transverse electric potential gradient is developed in the conductor. This effect is called as Hall effect and the transducer based on this effect is called as Hall effect transducer. ii. Classification based on physical quantity measured The transducers may be classified based on the physical quantity they measure as follows: • • • • • • • Temperature transducers → Transducers used to measure temperature Pressure transducers → To measure pressure Flow transducers → To measure flow Liquid level transducers → To measure liquid level Force/Torque transducers → To measure force & Torque Velocity/Speed transducers → To measure velocity & speed Humidity transducers → To measure humidity _____________________________________________________________________________________ Compiled by Yidnekachew M. Page 6 of 9 Instrumentation & Measurement _____________________________________________________ _ • • iii. AAiT Acceleration/vibration transducers → To measure acceleration & vibration Displacement transducers → To measure displacement Classification based on source of energy Transducers may be, classified based on source of energy into two types. • • Active transducer Passive transducer Passive transducer A component whose output energy is supplied entirely or almost entirely by its input signal is called a passive transducer. A passive transducer is the one which absorbs energy from the input medium and converts it directly into the output signal. Example A Thermocouple extracts heat energy from the input medium and converts it into electrical energy (voltage). Active Transducer An active transducer has an auxiliary source of power which supplies a major part of the output power while the input signal supplies only an insignificant portion (i.e) this transducer uses the energy it absorbs from the input medium as a control signal to transfer energy from the power supply to produce a proportional output. Example Strain gauge The energy extracted from the strained member is very small. The energy for the output signal is supplied by an external power source. Fig. 1.7 Active and passive transducers _____________________________________________________________________________________ Compiled by Yidnekachew M. Page 7 of 9 Instrumentation & Measurement _____________________________________________________ _ AAiT Selection of Transducers Transducers are used for the measurement of physical quantities. The selection of transducers for particular measurand is very important. The selection of transducers may be based on the following factors for effective measurement. 1. The physical quantity to be measured (measurand), 2. The range of input quantity, Based on physical quantity to be measured The correct type of transducer should be selected for measuring the physical quantity. The following table shows the physical quantity and the corresponding transducer types available. No. Physical quantity 1 Temperature 2 Pressure 3 Force (weight) 4 Torque 5 Density of liquids Transducers available Bimetallic element Fluid expansion systems i. Liquid-in-steel bulb thermometers ii. Liquid-in-glass thermometers iii. Vapour pre-ssure thermometers Thermoresistive elements i. Resistance Temperature detector (RTD) ii. Thermistor Thermocouple Linear-Quartz thermometer Pyrometry U-tube and ball type manometers Ring balance manometer Metallic diaphragms Capsules and bellows Bourdon tubes Membranes Spring balance Cantilever Diaphragms Pneumatic and hydraulic load cells Column and proving ring load cells Torsion bar Flat spiral springs Dynamometer Gyroscope Hydrometer Air bubbler system _____________________________________________________________________________________ Compiled by Yidnekachew M. Page 8 of 9 Instrumentation & Measurement _____________________________________________________ _ AAiT U-tube weighing system 3.4 6 Liquid level Float elements. Manometer system Diaphragms Container weight 7 Viscosity Capillary tube Concentric cylinder system 8 Flow rate of fluids 9 Displacement Pitot static tube Flow-obstruction elements Rotating vane system Rotameter float system Flapper nozzle system 10 Absolute displacement, Velocity and acceleration Vehicle attitude Seismic system Gyroscope Characteristics of Transducers The selection of most suitable transducer from commercially available instruments is very important in designing an Instrumentation system. For the proper selection of transducer, knowledge of the performance characteristics of them are essential. The performance characteristics can be classified into two namely i. ii. Static characteristics Dynamic characteristics Static characteristics are a set of performance criteria that give a meaningful description of the quality of measurement without becoming concerned with dynamic descriptions involving differential equations. Dynamic characteristics describe the quality of measurement when the measured quantities vary rapidly with time. Here the dynamic relations between the instrument input and output must be examined, generally by the use of differential equations. For further reading on this subtopic please read the additional material _____________________________________________________________________________________ Compiled by Yidnekachew M. Page 9 of 9