Tutorial 5 Principles of Transducers and Temperature Measurement

Similar documents
VISCOSITY OF BIO-DIESEL FUELS

Deflection of Electrons by Electric and Magnetic Fields

4a 4ab b (count number of places from first non-zero digit to

LSI/CSI LS7362 BRUSHLESS DC MOTOR COMMUTATOR/CONTROLLER DESCRIPTION:

Experiment MF Magnetic Force

Comparing Availability of Various Rack Power Redundancy Configurations

Discussion on Fuzzy Logic Operation of Impedance Control for Upper Limb Rehabilitation Robot 1,a Zhai Yan

Analytical Proof of Newton's Force Laws

Introduction to Fluid Mechanics

The LCOE is defined as the energy price ($ per unit of energy output) for which the Net Present Value of the investment is zero.

The Electric Potential, Electric Potential Energy and Energy Conservation. V = U/q 0. V = U/q 0 = -W/q 0 1V [Volt] =1 Nm/C

CLOSE RANGE PHOTOGRAMMETRY WITH CCD CAMERAS AND MATCHING METHODS - APPLIED TO THE FRACTURE SURFACE OF AN IRON BOLT

Questions & Answers Chapter 10 Software Reliability Prediction, Allocation and Demonstration Testing

How To Power A Clou Mpa Series Mixer

Comparing Availability of Various Rack Power Redundancy Configurations

AN IMPLEMENTATION OF BINARY AND FLOATING POINT CHROMOSOME REPRESENTATION IN GENETIC ALGORITHM

Experiment 6: Centripetal Force

ON THE (Q, R) POLICY IN PRODUCTION-INVENTORY SYSTEMS

Lecture 16: Color and Intensity. and he made him a coat of many colours. Genesis 37:3

Chapter 19: Electric Charges, Forces, and Fields ( ) ( 6 )( 6

[TO BE PUBLISHED IN THE GAZETTE OF INDIA, EXTRAORDINARY, PART-II, SECTION-3, SUB-SECTION (i)]

Forces & Magnetic Dipoles. r r τ = μ B r

Vector Calculus: Are you ready? Vectors in 2D and 3D Space: Review

Problem Set # 9 Solutions

CHAPTER 10 Aggregate Demand I

Episode 401: Newton s law of universal gravitation

Financing Terms in the EOQ Model

An Introduction to Omega

Magnetic Bearing with Radial Magnetized Permanent Magnets

PAN STABILITY TESTING OF DC CIRCUITS USING VARIATIONAL METHODS XVIII - SPETO pod patronatem. Summary

2 r2 θ = r2 t. (3.59) The equal area law is the statement that the term in parentheses,

SELF-INDUCTANCE AND INDUCTORS

YARN PROPERTIES MEASUREMENT: AN OPTICAL APPROACH

CA723, CA723C. Voltage Regulators Adjustable from 2V to 37V at Output Currents Up to 150mA without External Pass Transistors. Features.

FXA Candidates should be able to : Describe how a mass creates a gravitational field in the space around it.

Michal Szyper. "Inductance Measurement." Copyright 2000 CRC Press LLC. <

PHYSICS 111 HOMEWORK SOLUTION #13. May 1, 2013

Instituto Superior Técnico Av. Rovisco Pais, Lisboa virginia.infante@ist.utl.pt

Voltage ( = Electric Potential )

How many times have you seen something like this?

INDUSTRIAL VOLTAGE AMPLIFIER IC AM401 PRINCIPLE FUNCTION

est using the formula I = Prt, where I is the interest earned, P is the principal, r is the interest rate, and t is the time in years.

Chapter 3 Savings, Present Value and Ricardian Equivalence

Physics 235 Chapter 5. Chapter 5 Gravitation

A PID Tuning Method for Tracking Control of an Underactuated Gantry Crane

Voltage ( = Electric Potential )

N V V L. R a L I. Transformer Equation Notes

Determining solar characteristics using planetary data

AM26LS30 TIMING CHARACTERISTICS

STABILITY ANALYSIS IN MILLING BASED ON OPERATIONAL MODAL DATA 1. INTRODUCTION

Solution Derivations for Capa #8

Quantity Formula Meaning of variables. 5 C 1 32 F 5 degrees Fahrenheit, 1 bh A 5 area, b 5 base, h 5 height. P 5 2l 1 2w

Research on Risk Assessment of the Transformer Based on Life Cycle Cost

APPLICATIO S TYPICAL APPLICATIO. LM134 Series Constant Current Source and Temperature Sensor FEATURES DESCRIPTIO

An application of stochastic programming in solving capacity allocation and migration planning problem under uncertainty

CMOS 12-Bit Monolithic Multiplying DAC AD7541A

Lab #7: Energy Conservation

CRRC-1 Method #1: Standard Practice for Measuring Solar Reflectance of a Flat, Opaque, and Heterogeneous Surface Using a Portable Solar Reflectometer

DSP monitoring systems

Multiple choice questions [60 points]

Gravitation. AP Physics C

Measurement of Capacitance

Supplementary Material for EpiDiff

Skills Needed for Success in Calculus 1

Space Charge Accumulation in Polymeric. High Voltage DC Cable Systems

Gauss Law. Physics 231 Lecture 2-1

AP Physics Electromagnetic Wrap Up

Chapter 22. Outside a uniformly charged sphere, the field looks like that of a point charge at the center of the sphere.

NUCLEAR MAGNETIC RESONANCE

ELECTRİC DRİVE SYSTEMS AND MATLAB APPLICATIONS

TL074 TL074A - TL074B

THERMAL ISOLATION TECHNIQUES FOR CURE MONITORING USING FBG OPTICAL SENSORS

A statistical development of fixed odds betting rules in soccer

12.1. FÖRSTER RESONANCE ENERGY TRANSFER

Hip Hop solutions of the 2N Body problem

Do Vibrations Make Sound?

Semipartial (Part) and Partial Correlation

Lesson 7 Gauss s Law and Electric Fields

Tracking/Fusion and Deghosting with Doppler Frequency from Two Passive Acoustic Sensors

Continuous Compounding and Annualization

Manual ultrasonic inspection of thin metal welds

Chapter 2 Mathematical Model of the Safety Factor and Control Problem Formulation

unit : mm With heat sink (see Pd Ta characteristics)

The Role of Gravity in Orbital Motion

Definitions. Optimization of online direct marketing efforts. Test 1: Two campaigns. Raw Results. Xavier Drèze André Bonfrer. Lucid.

NBER WORKING PAPER SERIES FISCAL ZONING AND SALES TAXES: DO HIGHER SALES TAXES LEAD TO MORE RETAILING AND LESS MANUFACTURING?

LM 358 Op Amp. If you have small signals and need a more useful reading we could amplify it using the op amp, this is commonly used in sensors.

Carter-Penrose diagrams and black holes

UC2842B/3B/4B/5B UC3842B/3B/4B/5B

i( t) L i( t) 56mH 1.1A t = τ ln 1 = ln 1 ln ms

Example Optimization Problems selected from Section 4.7

Transcription:

Tutoial 5 Pinciples of Tansuces an Tempeatue Measuement Chapte 5 Pinciples of Tansuces Example 5.1 (Johnson 26) A potentiometic isplacement senso is use to measue wokpiece motion fom to 1 cm. The esistance changes linealy ove this ange fom to 1 kω. Develop signal conitioning to povie a linea, - to 1-V output. 15V 25Ω 51Ω Senso 5.1V Op-Amp Figue 5.1 The key thing is to not lose the lineaity of the esistance vesus isplacement. We cannot put the vaying esistance in a ivie to pouce a vaying voltage because the voltage vaies nonlinealy with esistance. Remembe though that the output voltage of an inveting amplifie vaies linealy with the feeback esistance. Theefoe, let s put the senso in the feeback of a simple inveting amplifie. Then we woul have something like R 2 Vout = V in R1 We can now get i of the pesky negative by using Vin as a constant negative voltage, say 5.1 volts fom a zene ioe. Then we pick R 1 to give the esie output, 1 volts at 1 kω (1 cm), 1 1 = ( 5.1) so R 1 = 51 Ω R 1 Example 5.2 The following figue shows a capacitive isplacement senso esigne to monito small changes in wok-piece position. The two metal cylines ae sepaate by a plastic sheath/beaing of thickness 1 mm an ielectic constant at 1 khz of 2.5. If the aius of 2.5 cm, fin the sensitivity in pf/m as the uppe cyline slies in an out of the lowe cyline. What is the ange of capacity if h vaies fom 1. to 2. cm? ( ε = 8.854 pf/m) The capacity is given by the following equation A C =εε 1

Displacement h Figue 5.2 The effective aea is the aea of the shae cylinical aea, which has a aius,, an height, h. Thus, A = 2πh, so the capacity can be expesse as h C= 2πKε The sensitivity with espect to the height, h, is efine by how C changes with h, that is, it is given by the eivative C = 2πKε h Substituting fo the given values, we get 2 C 2.5 1 m = 2π ( 2.5)( 8.85 pf/m) = 3475 pf / m 3 h 1 m Since the function is linea with espect to h, we fin the capacity ange as C min = (3475 pf/m)(1 2 m) = 34.75 pf to C max = (3475 pf/m)(2 1 2 m) = 69.5 pf. Example 5.3 An LVDT has a maximum coe motion of ± 1.5 cm with a lineaity of ±.3% ove that ange. The tansfe function is 23.8 mv/mm. If use to tack wok-piece motion fom 1.2 to + 1.4 cm, what is the expecte output voltage? What is the uncetainty in position etemination ue to nonlineaity? Using the known tansfe function, the output voltages can easily be foun, V( 1.2cm) = (23.8 mv/mm)( 12mm) = 285.6 mv an V(1.4cm) = (23.8 mv/mm)(14mm) = 333 mv The lineaity eviation shows up in eviations of the tansfe function. Thus, the tansfe fuction has an uncetainty of (±.3)(23.8mV/mm) = ±.714mV/mm This means that a measue voltage, V m (in mv), coul be intepete as a isplacement that anges fom Vm/23.73 to Vm/23.8 mm, which is appoximately ±.3%, as expecte. Thus, if the senso output was 33 mv, which is nominally 1.4 cm, the actual coe position coul ange fom 1.4329 to 1.3956 cm. Example 5.4 The level of ethyl alcohol is to be measue fom to 5 m using a capacitive system such as shown in the following figue. 2

C h Figue 5.3 The following specifications efine the system: fo ethyl alcohol: ε = 26 (fo ai, ε = 1) cyline sepaation: =.5 cm plate aea: A = 2πRL whee R = 5.75 cm = aveage aius, L = istance along cyline axis Fin the ange of capacity vaiation as the alcohol level vaies fom to 5 m. The capacity is given by A C =εε Theefoe all we nee to o is to fin the capacity fo the entie cyline with no alcohol an then multiply that by 26. A = 2πRL = 2π(.575m)(5m) = 1.86 m 2 Thus, fo ai, C = (1)(8.85 pf/m)(1.86m 2 /.5m) = 3196 pf.32 µf With the ethyl alcohol, the capacity becomes C = 26(.32 µf) =.832 µf The ange is.32 to.832 µf. Execise 5.1 The output voltage of a potentiomete-type esistance tansuce is to be measue by a ecoe having an input esistance of 2 kω. If the eo of measuement is not to excee 2% at 5% f.s., etemine esistance value of the potentiomete. [1.633kΩ] Execise 5.2 The following is a typical specification fo potentiomete-type esistance tansuce. Examine the specification an explain the meaning an significance of each item. Type wie-woun esistance isplacement potentiomete Teminal esistance 1kΩ Range -25mm Resolution.4% Powe ating.25w Maximum wipe cuent 15mA Themal ift.5% pe o C Life expectancy 1 8 cycles Execise 5.3 A linea vaiable iffeential tansfome is excite with a 1 Hz 6V peak-to-peak wavefom. The input coe motion is sinusoial at 1 Hz an has a isplacement amplitue of ± 3 3

mm. If the l.v..t sensitivity is 2 V/mm, aw the wavefoms of the excitation voltage, input isplacement an output voltage. Execise 5.4 The specifications fo the l.v..t in Execise 5.3 ae as follows: Lineaity:.4% Resolution: infinite Resiual voltage:.5% Dift bette than.1% pe o C Output impeance: 2.5kΩ Response time: 1ms Explain the meaning an significance of the specifications. See attache sheet fo an example fo LVDT specifications. Execise 5.5 (a) Descibe the pinciple of opeation an constuction etails of the piezoelectic (quatz) tansuce. (b) A quatz pessue tansuce has a sensitivity of 8 pc/ba. If, when the input pessue is 3 bas, an output voltage of 1 V is pouce, etemine the capacitance of the evice. [24 pf] Chapte 6 Tempeatue measuement Execise 6.1 Explain the pinciple of opeation of the themocouples. Execise 6.2 Explain the pinciple of opeation of the esistance tempeatue etectos. Execise 6.3 Explain the pinciple of opeation of the themistos. Execise 6.4 Explain the pinciple of opeation of the aiation pyometes. Execise 6.5 A type-k themocouple is expose to a tempeatue of 12 o C. If the inicato is use as the col junction an its tempeatue is 5 o C. Use the following figue to calculate the e.m.f inicate. [47mV] 8 7 Type E 6 5 Type K 4 3 2 1 Type T Type S 2 4 6 8 1 12 14 16 18 2 Figue 6.1 Themocouple chaacteistics (efeence o C) 4

Execise 6.6 Using the above figue, etemine (a) the sensitivity of the type-t themocouple in the ange of o C to 3 o C, (b) the sensitivities of the type-e an type-s themocouples in the ange of 4 o C to 1 o C. [.5mV/ o C] [.8mC/ o C] [.1mV/ o C] Execise 6.7 If the ynamic elationship between the measue tempeatue θ 2 an the efeence tempeatue θ 1 fo a themomete is given by θ 2 = k ( θ 1 θ 2) whee k =.2s -1 t etemine the time constant an static sensitivity fo the themomete. [5s] Execise 6.8 A mecuy themomete use to measue the tempeatue of a liqui has ynamics epesente by the following equation: Tm 1 1 CT + Tm = Ti t R T R T whee T m ( o C) is the tempeatue of mecuy, an T i ( o C) a change in the tempeatue of the liqui, R T an C T ae constant. Fin the time constant, sensitivity an the ynamic esponse of the themomete T m. using these numeical values: T i = 1 o C, R T = 131 o C/W, an C T =.56 J/ o C. Execise 6.9 An RTD has α =.5 / o C, R = 5 Ω an a issipation constant of P D = 3 mw/ o C at 2 o C. The RTD is use in a bige cicuit as shown in the following figue, with R 1 = R 2 = 5 Ω, an R 3 is a vaiable esisto use to null the bige. If the supply is 1 V an the RTD is place in an ice bath at o C: a) Fin the value of R 3 to null the bige [R 3 = 454.5 Ω]. Powe supply 1V R 1 V R 2 R 3 RTD Figue 6.2 RTD with a bige cicuit fo Execise 6.9 b) Fin the output voltage measue by a voltmete (R v = ) with the above value of R 3 if the tempeatue is 1 o C. Consie the effect of the self-heating an calculate the eo of the RTD at 1 o C. Hints: An RTD is a esistance, theefoe thee is an I 2 R powe issipate by the evice itself that causes a light heating effect, a self-heating. This may also cause an eoneous eaing o even upset the envionment in elicate measuement conition. Thus, the cuent though the RTD must be kept sufficiently low an constant to avoi self-heating. Typically, a issipation constant is povie in RTD specifications. This numbe elates the powe equie to aise the RTD 5

tempeatue by one egee of tempeatue. Thus, a 25-mW/ o C issipation constant shows that if I 2 R powe losses in the RTD equal 25 mw, the RTD will be heate by 1 o C. The issipation constant is usually specifie une two conitions: fee ai an a well-stie oil bath. This is because of the iffeence in capacity of the meium to cay heat away fom the evice. The self-heating tempeatue ise can be foun fom the powe issipate by the RTD, an the issipation constant fom: whee P T = P D T = tempeatue ise because of self-heating in o C P = powe issipate in the RTD fom the cicuit in W = issipation constant of the RTD in W/ o C P D Execise 6.1 (Themisto) A themisto is to monito oom tempeatue. It has a esistance of 3.5 kω at 2 o C with a slope of 1%/ o C. The issipation constant is P D = 5 mw/ o C. It is suppose to use the themisto in the ivie of the following figue to povie a voltage of 5. V at 2 o C. Evaluate the effects of selfheating [3. kω; V D = 4.6 V]. 1 V 3.5 kω Themisto R TH V D = 5 V Figue 6.3 Themisto in a ivie cicuit fo Execise 6.1 Execise 6.11 (Themocouples) Fin the emf fo a mateial with α = 5 µv/oc if the junction tempeatues ae 2 o C an 1 o C. Hint: The themoelectic effect is expesse by the following equation: T2 T1 ( ) ε= Q Q T A B whee ε = emf (also calle Seebeck emf) pouce in volts T 1, T 2 = junction tempeatues in K Q A, Q B = themal tanspot constants of the two metals This equation, which escibe the Seebect effect, shows that the emf pouce is popotional to the iffeence in tempeatue an, futhe, to the iffeence in the metallic themal tanspot 6

constants. Thus, if the metals ae the same, the emf is zeo, an if the tempeatue ae the same, the emf is zeo. In pactice, it is foun that the two constants, QA an QB, ae nealy inepenent of tempeatue an that an appoximate linea elationship exists as ε=α( T2 T1) whee α = constant in V/K T 1, T 2 = junction tempeatues in K Execise 6.12 A voltage of 23.72 mv is measue with a type K themocouple at a o C efeence. Fin the tempeatue of the measuement junction. [572.1 o C] Hints: use the attache sheet with the following intepolation equations: Tempeatue: TH T L TM = TL + ( VM VL) VH VL whee V M = measue voltage that lies between a highe voltage, V H, an a lowe voltage, V L, which ae in the tables. The tempeatues coesponing to these voltages ae T H an T L, espectively. Voltage: V = V V + V T T ( ) H L M L M L TH TL Execise 6.13 Fin the voltage of a type J themocouple with a o C efeence if the junction tempeatue is 172 o C. [ 7.18 o C] Execise 6.14 An RTD has α (2 o C) =.4 / o C. If R = 16 Ω at 2 o C, fin the esistance at 25 o C. 7