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Me 414

by: Caleb Turner

Me 414 Me 414

Caleb Turner
U of L

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This is the class book as well as hw that I believe we will be covering in this class
Mechanical Structure and Design
Jeff Bordon
Engineering, mechanical engineering
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E1FTOC 09/15/2010 11:10:55 Page 10 E1FFIRS09/09/2014:58:3Page 1 Theory and Design for Mechanical Measurements Fifth Edition Richard S. Figliola Clemson University Donald E. Beasley Clemson University John Wiley & Sons, Inc. E1FFIRS 09/09/2010 14:58:34 Page 2 ACQUISITIONS EDITOR Linda Ratts PRODUCTION EDITOR Anna Melhorn PRODUCTION SERVICES MANAGER Dorothy Sinclair SENIOR MEDIA EDITOR Tom Kulesa SENIOR MARKETING MANAGER Christopher Ruel SENIOR DESIGNER Wendy Lai This book was set in 10/12 Times Roman by Thomson Digital and printed and bound by RR Donnelley, The cover was printed by RR Donnelley. This book is printed on acid free paper. ▯ Founded in 1807, John Wiley & Sons, Inc. has been a valued source of knowledge and understanding for more than 200 years, helping people around the world meet their needs and fulfill their aspirations. Our company is built on a foundation of principles that include responsibility to the communities we serve and wherewe live and work. In 2008, we launched a Corporate Citizenship Initiative, a global effort to address the environmental, social, economic, and ethical challenges we face in our business. Among the issues we are addressing are carbon impact, paper specifications and procurement, ethical conduct within our business and among our vendors, and community and charitable support. For more information, please visit our website: Copyright # 2011 John Wiley & Sons, Inc. All rights reserved. No part of this publication may be reproduced, stored in a retrieval system or transmitted in any form or by any means, electronic, mechanical, photocopying, recording, scanning, or otherwise, except as permitted under Sections 107 or 108 of the 1976 United States Copyright Act, without either the prior written permission of the Publisher, or authorization through payment of the appropriate per-copy fee to the Copyright Clearance Center, Inc., 222 Rosewood Drive, Danvers, MA 01923, (978)750-8400, fax (978)750-4470 or on the web at Requests to the Publisher for permission should be addressed to the Permissions Department, John Wiley & Sons, Inc., 111 River Street, Hoboken, NJ 07030-5774, (201)748-6011, fax (201)748-6008, or online at Evaluation copies are provided to qualified academics and professionals for review purposes only, for use in their courses during the next academic year. These copies are licensed and may not be sold or transferred to a third party. Upon completion of the review period, please return the evaluation copy to Wiley. Return instructions and a free of charge return shipping label are available at go/returnlabel. Outside of the United States, please contact your local representative. Printed in the United States of America 10987654321 E1FPREF 09/14/2010 12:7:8 Page 3 Preface th We are pleased to offer this 5 edition of Theory and Design for Mechanical Measurements. This text provides a well-founded background in the theory of engineering measurements. Integrated throughout are the necessary elements for the design of measurement systems and measurement test plans, with an emphasis on the role of statistics and uncertainty analyses in design. The measurements field is very broad, but through careful selection of the topical coverage we establish the physical principles and practical techniques for many engineering applications while keeping page count and text cost manageable. Our aim is not to offer a manual for instrument construction and assembly. Instead, we develop the conceptual design framework for selecting and specifying equipment and test procedures and for interpreting test results, which we feel are necessary and common bases for the practice of test engineering. The text is appropriate for undergraduate and graduate level study in engineering, but is also suitably advanced and oriented to serve as a reference source for professional practitioners. The pedagogical approach invites independent study or use in related fields requiring an understanding of instrumentation and measurements. The organization of the text develops from our view that certain aspects of measurements can be generalized, such as test plan design, signal analysis and reconstruction, and measurement system response. Topics such as statistics and uncertainty analysis require a basic development of principles but are then best illustrated by integrating these topics throughout the text material. Other aspects are better treated in the context of the measurement of a specific physical quantity, such as strain or temperature. PEDAGOGICAL TOOLS TO AID LEARNING In this textbook:  Each chapter begins by defining a set of learning outcomes.  The text develops an intuitive understanding of measurement concepts with its focus on test system modeling, test plan design, and uncertainty analysis.  Each chapter includes carefully constructed example problems that illustrate new material and problems that build on prior material.  Each example makes use of a KNOWN, FIND, SOLVE approach as an organizational aid to a problem’s solution. This methodology for problem solutions helps new users to link words and concepts with symbols and equations. Many problems contain COMMENTS that expand on the solution, provide a proper context for application of the principle, or offer design application insight.  End-of-Chapter practice problems are included for each chapter to exercise new concepts.  Practice problems range from those focused on concept development, to building of advanced skills, to open-ended design applications.  With each chapter, we have added new practice problems but have substantially ‘‘refreshed’’ many problems from previous editions.  We provide a detailed Instructors Manual for instructors who have adopted the book. We have carefully reviewed the solutions in this edition to minimize typographical and arithmetical errors. The manual is available on-line at the Wiley Instructor’s website.  Answers to selected problems will be posted on the Wiley website.  Use of the software in problem solving allows in-depth exploration of key concepts that would be prohibitively time consuming otherwise. The text includes on-line access to interactive software of iii E1FPREF 09/14/2010 12:7:8 Page 4 iv Preface focused examples based on software using National Instruments Labview 1 for exploring some of the 1 text concepts, while retaining our previous efforts using Matlab The Labview programs are available as executables so they can be run directly without a Labview license. The software is available on both the Wiley Student and Instructor’s websites. TH NEW TO THIS 5 EDITION th With this 5 edition, we have new or expanded material on a number of topics. As highlights:  We introduce Monte Carlo simulation methods in Chapter 4 and tie their use with uncertainty estima- tions in Chapter 5.  Treatment of uncertainty analysis in Chapter 5 has been updated to include changes in test standards methodology relative to ASME PTC 19.1 Test Uncertainty and the International Standards Organization (ISO) Guide to Uncertainty in Measurements. These changes have been carried into the other chapters both in language and in example problems. Where we deviate from the methodology of the Standards, we do so for pedagogical reasons.  Discussion has been added on using rectangular (uniform) distributions in uncertainty estimation.  The treatment of non-symmetric uncertainty intervals and methods for treating correlated errors in Chapter 5 has been expanded and revisited in other chapters.  We have updated our symbol usage for closer consistency with the standards.  We have added a section presenting image acquisition and processing using digital techniques in Chapter 7.  We have changed our presentation of pressure transmission line effects to make better use of the lumped parameter methods of Chapter 3 that engineering students are familiar with, including discussion of the ideal elements of inertance, resistance, and compliance.  We have revised our treatment of Butterworth filters, including added coverage, in Chapter 6.  WehaveaddedanintroductiontotheanalysisofstraingaugedatatocomputeprincipalstressesinChapter11. SUGGESTED COURSE COVERAGE To aid in course preparation, Chapters 1 through 5 providean introduction to measurement theory with statistics and uncertainty analysis, Chapters 6 and 7 provide a broad treatment of analog and digital sampling methods, and Chapters 8 through 12 are instrumentation focused. Many users report to us that they use different course structures, so many that it makes a preferred order of topical presentation difficult to anticipate. To accommodate this, we have written the text in a manner that allows anyinstructortocustomizetheorderofmaterialpresentation.WhilethematerialofChapters4and5areintegrated throughout the text and should be taught in sequence, the other chapters tend to stand on their own. The text is flexible and can be used in a variety of course structures at both the undergraduate and graduate levels. For a complete measurements course, we recommend the study of Chapters 1 through 7 with use of the remaining chapters as appropriate. For a lab-course sequence, we recommend using chapters as they best illustrate the course exercises while building complete coverage over the several lab courses normally within a curriculum. The manner of the text allows it to be a resource for a lab-only course with minimal lecture. Over the years, we have used it in several forums, as well as professional development courses, and simply rearrange material and emphasis to suit the audience and objective. We express our sincerest appreciation to the students, teachers, and engineers who have used our earlier editions. We are indebted to the many who havewritten us with their constructive comments and encouragement. Richard S. Figliola Donald E. Beasley Clemson, South Carolina E1FTOC 09/15/2010 11:10:55 Page 5 Contents 1 Basic Concepts of Measurement Methods 1 1.1 Introduction 1 1.2 General Measurement System 2 1.3 Experimental Test Plan 6 1.4 Calibration 15 1.5 Standards 23 1.6 Presenting Data 30 1.7 Summary 31 References 31 Nomenclature 32 Problems 32 2 Static and Dynamic Characteristics of Signals 41 2.1 Introduction 41 2.2 Input/Output Signal Concepts 41 2.3 Signal Analysis 46 2.4 Signal Amplitude And Frequency 49 2.5 Fourier Transform and The Frequency Spectrum 63 2.6 Summary 71 References 71 Suggested Reading 71 Nomenclature 72 Problems 72 3 Measurement System Behavior 79 3.1 Introduction 79 3.2 General Model for a Measurement System 79 3.3 Special Cases of the General System Model 83 3.4 Transfer Functions 104 3.5 Phase Linearity 106 3.6 Multiple-Function Inputs 107 3.7 Coupled Systems 109 3.8 Summary 111 References 111 Nomenclature 111 Problems 112 v E1FTOC 09/15/2010 11:10:55 Page 6 vi Contents 4 Probability and Statistics 118 4.1 Introduction 118 4.2 Statistical Measurement Theory 119 4.3 Describing the Behavior of a Population 125 4.4 Statistics of Finite-Sized Data Sets 129 4.5 Chi-Squared Distribution 135 4.6 Regression Analysis 139 4.7 Data Outlier Detection 147 4.8 Number of Measurements Required 148 4.9 Monte Carlo Simulations 150 4.10 Summary 152 References 152 Nomenclature 153 Problems 153 5 Uncertainty Analysis 161 5.1 Introduction 161 5.2 Measurement Errors 162 5.3 Design-Stage Uncertainty Analysis 164 5.4 Identifying Error Sources 168 5.5 Systematic and Random Errors 170 5.6 Uncertainty Analysis: Error Propagation 172 5.7 Advanced-Stage Uncertainty Analysis 176 5.8 Multiple-Measurement Uncertainty Analysis 182 5.9 Correction for Correlated Errors 195 5.10 Nonsymmetrical Systematic Uncertainty Interval 197 5.11 Summary 198 References 199 Nomenclature 199 Problems 200 6 Analog Electrical Devices and Measurements 209 6.1 Introduction 209 6.2 Analog Devices: Current Measurements 210 6.3 Analog Devices: Voltage Measurements 214 6.4 Analog Devices: Resistance Measurements 219 6.5 Loading Errors and Impedance Matching 226 6.6 Analog Signal Conditioning: Amplifiers 230 6.7 Analog Signal Conditioning: Special-Purpose Circuits 234 6.8 Analog Signal Conditioning: Filters 239 6.9 Grounds, Shielding, and Connecting Wires 250 6.10 Summary 252 References 253 Nomenclature 253 Problems 254 E1FTOC 09/15/2010 11:10:55 Page 7 Contents vii 7 Sampling, Digital Devices, and Data Acquisition 260 7.1 Introduction 260 7.2 Sampling Concepts 261 7.3 Digital Devices: Bits and Words 269 7.4 Transmitting Digital Numbers: High and Low Signals 271 7.5 Voltage Measurements 271 7.6 Data-Acquisition Systems 283 7.7 Data-Acquisition System Components 284 7.8 Analog Input-Output Communication 288 7.9 Digital Input-Output Communication 293 7.10 Digital Image Acquisition and Processing 299 7.11 Summary 303 References 303 Suggested Reading 304 Nomenclature 304 Problems 305 8 Temperature Measurements 309 8.1 Introduction 309 8.2 Temperature Standards and Definition 310 8.3 Thermometry Based on Thermal Expansion 313 8.4 Electrical Resistance Thermometry 315 8.5 Thermoelectric Temperature Measurement 330 8.6 Radiative Temperature Measurements 351 8.7 Physical Errors in Temperature Measurement 356 8.8 Summary 365 References 365 Nomenclature 366 Problems 367 9 Pressure and Velocity Measurements 375 9.1 Introduction 375 9.2 Pressure Concepts 375 9.3 Pressure Reference Instruments 378 9.4 Pressure Transducers 386 9.5 Pressure Transducer Calibration 392 9.6 Pressure Measurements in Moving Fluids 396 9.7 Modeling Pressure and Fluid Systems 400 9.8 Design and Installation: Transmission Effects 401 9.9 Fluid Velocity Measuring Systems 405 9.10 Summary 415 References 416 Nomenclature 417 Problems 417 E1FTOC 09/15/2010 11:10:55 Page 8 viii Contents 10 Flow Measurements 423 10.1 Introduction 423 10.2 Historical Background 423 10.3 Flow Rate Concepts 424 10.4 Volume Flow Rate Through Velocity Determination 425 10.5 Pressure Differential Meters 427 10.6 Insertion Volume Flow Meters 446 10.7 Mass Flow Meters 454 10.8 Flow Meter Calibration and Standards 459 10.9 Estimating Standard Flow Rate 460 10.10 Summary 461 References 461 Nomenclature 462 Problems 462 11 Strain Measurement 466 11.1 Introduction 466 11.2 Stress and Strain 466 11.3 Resistance Strain Gauges 469 11.4 Strain Gauge Electrical Circuits 476 11.5 Practical Considerations for Strain Measurement 479 11.6 Apparent Strain and Temperature Compensation 482 11.7 Optical Strain Measuring Techniques 492 11.8 Summary 497 References 498 Nomenclature 498 Problems 499 12 Mechatronics: Sensors, Actuators, and Controls 504 12.1 Introduction 504 12.2 Sensors 504 12.3 Actuators 534 12.4 Controls 540 12.5 Summary 557 Nomenclature 558 References 558 Problems 559 E1FTOC 09/15/2010 11:10:55 Page 9 Contents ix Appendix A A Guide for Technical Writing 563 A Guide For Technical Writing 563 References 568 Appendix B Property Data and Conversion Factors 569 Appendix C Laplace Transform Basics 576 C.1 Final Value Theorem 577 C.2 Laplace Transform Pairs 577 References 577 Glossary 578 Index 585 E1FTOC 09/15/2010 11:10:55 Page 10 E1C01 09/14/201015:40:34 Page 1 Chapter 1 Basic Concepts of Measurement Methods 1.1 INTRODUCTION We make measurements every day. Consider the common measurements illustrated in Figure 1.1. We routinely read the temperature of an outdoor thermometer to choose appropriate clothing for the day. We expect to have exactly 10 gallons or lite rs of fuel added to our tank when that volume is indicated on a fuel pump. And we expect meas uring cups to yield correct quantities of ingredients in cooking. We put little thought into t he selection of instruments for these routine measurements. After all, the direct use of the d ata is clear to us, the type of instruments and techniques are familiar to us, and the outcome o f these measurements is not important enough to merit much attention to features like improved a ccuracy or alternative methods. But when the stakes become greater, the selection of measurement equipment and techniques and the interpre- tation of the measured data can demand considerable attention. Just contemplate how you might verify that a new engine is built as designed and meets the power and emissions performance specifications required. But first things first. The objective in any measurement is to answer a question. So we take measurements to establish the value or the tendency of some variable, the results of which are specifically targeted to answer our question. The information acquired is based on the output of the measurement device or system. There are important issues to be addressed to ensure that the output of the measurement device is a reliable indication of the true value of the measured variable. In addition, we must address the following important questions: 1. How can a measurement or test plan be devised so that the measurement provides the unambiguous information we seek? 2. How can a measurement system be used so that the engineer can easily interpret the measured data and be confident in their meaning? There are procedures that address these measurement questions. At the onset, we want to stress that the subject of this text is real-life oriented. Specifying a measurement system and measurement procedures represents an open-ended design problem whose outcome will not have one particular solution. That means there may be several approaches to solving a measurement problem, and some will be better than others. This text emphasizes accepted procedures for analyzing a measurement problem to assist in the selection of equipment, 1 E1C01 09/14/2010 15:40:34 Page 2 2 Chapter 1 Basic Concepts of Measurement Methods Figure 1.1 Common devices that involve measurements. methodology, and data analysis to meet the design objectives. Perhaps more than in any other technical field, the approach taken in measurement design and the outcome achieved will often depend on the attention and experience of the designer. Upon completion of this chapter, the reader will be able to ▯ identify the major components of a general measurement system, and state the function of each, ▯ develop an experimental test plan, ▯ distinguish between random and systematic errors, ▯ describe and define the various error types, ▯ define a standard and distinguish among primary, secondary, and transfer standards, and ▯ clearly delineate defined and derived dimensions in various unit systems. 1.2 GENERAL MEASUREMENT SYSTEM 1 A measurement is an act of assigning a specific value to a physical variable. That physical variable is the measured variable. A measurement system is a tool used for quantifying the measured variable. As such, a measurement system is used to extend the abilities of the human senses that, while they can detect and recognize different degrees of roughness, length, sound, color, and smell, are limited and relative; they are not very adept at assigning specific values to sensed variables. A system is composed of components that work together to accomplish a specific objective. We begin by describing the components that make up a measurement system, using specific examples. Then we will generalize to a model of the generic measurement system. 1 There are many new engineering measurement terms introduced. A glossary of the italicized terms is located in the back of the text for your reference. E1C01 09/14/2010 15:40:34 Page 3 1.2 General Measurement System 3 Cantilever and tip Sample surface Figure 1.2 Sensor stage of an atomic-force microscope. Sensor and Transducer An increasingly important area of scientific inquiry is the characteristics of matter at the nanoscale. Suppose we want to measure the profile of a surface at a nanometer scale. We discover that a small (very small) cantilever beam placed near the surface is deflected by atomic forces. Let’s assume for now that they are repulsive forces. If this cantilever is translated over the surface, the cantilever will deflect, indicating the height of the surface. This concept is illustrated in Figure 1.2; the device is called an atomic force microscope. The cantilever beam is a sensor, a physical element that employs some natural phenomenon, in this case deflection under the action of a force, to sense the variable being measured, in this case the height of the surface. So,wehaveasensortomeasureatthenanometerscale.Butwehavenomeansofgettinganoutput fromthesensorthatwecanrecord.Supposethattheuppersurfaceofthecantileverisreflective,andwe shinealaserontotheuppersurface,asshowninFigure1.3.Themovementofthecantileverwilldeflect the laser. Employing a number of light sensors, alsoshown in Figure 1.3,the deflectionof the laser can be sensed and that deflection corresponds to the height of the surface. Together the laser and the light sensors (photodiodes) form the transducer component of the measurement system. A transducer converts the sensed information into a detectable signal. The signal might be mechanical, electrical, optical, or may take any other form that can be meaningfully recorded. We should note that sensor selection, placement, and installation are particularly important to ensure that the sensor output accurately reflects the measurement objective. The familiar phrase Detector and feedback electronics Laser Photodiodes Cantilever and tip Sample surface Figure 1.3 Atomic-force microscope with sensor and transducer stages. E1C01 09/14/2010 15:40:34 Page 4 4 Chapter 1 Basic Concepts of Measurement Methods associated with hot days, ‘‘100 F in the shade’’ implies a specific sensor placement. Accordingly, the interpretation of all information passed through and indicated by the system depends on what is actually sensed by the sensor. For example, the interpretation of the output of a medical thermometer depends on where its sensor is placed. Output Stage The goal of a measurement system is to convert the sensed information into a form that can be easily quantified. Consider a familiar example, the liquid-in-glass bulb thermometer. The liquid contained within the bulb on the common bulb th ermometer of Figure 1.4 exchanges energy with its surroundings until the two are in thermal equilibrium. At that point they are at the same temperature. This energy exchange is the input signal to this measurement system. The phenome- non of thermal expansion of the liquid results in its movement up and down the stem, forming an output signal from which we determine temperature. The liquid in the bulb acts as the sensor. By forcing the expanding liquid into a narrow cap illary, this measurement system transforms thermal information into a mecha nical displacement. Hence, the bulb’s internal capillary design acts as a transducer. The output stage indicates or records the value measured. This might be a simple readout display, a marked scale, or even a recording device such as a computer disk drive. The readout scale of the bulb thermometer in Figure 1.4 serves as the output stage of that measurement system. It is worth noting that the term ‘‘transducer’’ is also often used in reference to a packaged device, which may contain a sensor, transducer, and even some signal conditioning elements. While such terminology is not true to our presentation, the context in which the term is used prevents ambiguity. 0 7 60 Output stage 0 40 Display scale 0 3 Stem 20 Bulb Sensor–transducer stage Figure 1.4 Components of bulb thermometer equivalent to sensor, transducer, and output Sensor stages. E1C01 09/14/2010 15:40:34 Page 5 1.2 General Measurement System 5 General Template for a Measurement System A general template for a measurement system is illustrated in Figure 1.5. Basically such a system consists of part or all of four general stages: (1) sensor–transducer stage, (2) signal-conditioning stage, (3) output stage, and (4) feedback-control stage. These stages form the bridge between the input to the measurement system and the system output, a quantity that is used to infer the value of the physical variable measured. We discuss later how the relationship between the input informa- tion, as acquired by the sensor, and the system outputis established by a calibration. We have already discussed the sensor–transducer stage, so let’s move on to the signal-conditioning stage. The signal-conditioning stage takes the transducer signal and modifies it to a desired magnitude. This optional intermediate stage might be used to perform tasks such as increasing the magnitude of the signal by amplification, removing portions of the signal through some filtering technique, or providing mechanical or optical linkage between the transducer and the output stage. Forexample, the translational displacement of a mechanic’s caliper (sensor) is often converted into a rotational displacement of a pointer. This stage can consist of one or more devices, which are often connected in series. For example, the diameter of the thermometer capillary relative to the bulb volume (see Fig. 1.4) determines how far up the stem the liquid moves with increasing temperature. It ‘‘conditions’’ the signal by amplifying the liquid displacement. In those measurement systems involved in process control, a fourth stage, the feedback-control stage, contains a controller that interprets the measured signal and makes a decision regarding the control of the process. This decision results in a signal that changes the process parameter that affects the magnitude of the sensed variable. In simple controllers, this decision is based on the magnitude of the signal of the sensed variable, usually whether it exceeds some high or low set point, avalue set by the system operator. Forexample, a simple measurement system with control stage is a household furnace thermostat. The operator fixes the set point for temperature on the thermostat display, and the furnace is activated as the local temperature at the thermostat, as determined by the Calibration Signal conditioning stage Signal Transducer Output Sensor stage stage stage path Process Control signal Control stage Figure 1.5 Components of a general measurement system. E1C01 09/14/2010 15:40:34 Page 6 6 Chapter 1 Basic Concepts of Measurement Methods sensor within the device, rises or falls above or below the set point. In a more sophisticated controller, a signal from a measurement system can be used as an input to an ‘‘expert system’’ controller that, through an artificial intelligence algorithm, determines the optimum set conditions for the process. Mechatronics deals with the interfacing of mechanical and electrical components with microprocessors, controllers, and measurements. Wewill discuss some features of mechatronic systems in detail in Chapter 12. 1.3 EXPERIMENTAL TEST PLAN An experimental test serves to answer a question, so the test should be designed and executed to answer that question and that question alone. This is not so easy to do. Let’s consider an example. Suppose you want to design a test to answer the question, ‘‘What is the fuel use of my new car?’’ What might be your test plan? In a test plan, you identify thevariables that you will measure, but you also need to look closely at other variables that will influence the result. Two important variables to measure would be distance and fuel volume consumption. Obviously, the accuracy of the odometer will affect the distance measurement, and the way you fill your tank will affect your estimate of the fuel volume. But what other variables might influence your results? If your intended question is to estimate the average fuel usage to expect over the course of ownership, then the driving route you choose would play a big role in the results and is a variable. Only highway driving will impose a different trend on the results than only city driving, so if you do both you might want to randomize your route by using various types of driving conditions. If more than one driver uses the car, then the driver becomes a variable because each individual drives somewhat differently. Certainly weather and road conditions influence the results, and you might want to consider this in your plan. Sowe see that the utility of the measured data is very much impacted by variables beyond the primary ones measured. In developing your test, the question you propose to answer will be a factor in developing your test plan, and you should be careful in defining that question so as to meet your objective. Imagine how your test conduct would need to be different if you were interested instead in providing values used to advertise the expected average fuel use of a model of car. Also, you need to consider just how good an answer you need. Is 2 liters per 100 kilometers or 1 mile per gallon close enough? If not, then the test might require much tighter controls. Lastly, as a concomitant check, you might compare your answer with information provided by the manufacturer or independent agency to make sure your answer seems reasonable. Interestingly, this one example contains all the same elements of any sophisticated test. If you can conceptualize the factors influencing this test and how you will plan around them, then you are on track to handle almost any test. Before we move into the details of measurements, we focus here on some important concepts germane to all measurements and tests. Experimental design involves itself with developing a measurement test plan. A test plan draws from the following three steps: 2 1. Parameter design plan. Determine the test objective and identify the process variables and parameters and a means for their control. Ask: ‘‘What question am I trying to answer? What needs to be measured?’’ ‘‘What variables and parameters will affect my results?’’ 2 These three strategies are similar to the bases for certain design methods used in engineering system design (1). E1C01 09/14/2010 15:40:34 Page 7 1.3 Experimental Test Plan 7 2. System and tolerance design plan. Select a measurement te chnique, equipment, and test procedure based on some preconceived tolerance limits for error. 3 Ask: ‘‘In what ways can I do the measurement and how good do the results need to be to answer my question?’’ 3. Data reduction design plan. Plan how to analyze, present, and use the anticipated data. Ask: ‘‘How will I interpret the resulting data? How will I use the data to answer my question? How good is my answer? Does my answer make sense?’’ Going through all three steps in the test plan before any measurements are taken is a useful habit for a successful engineer. Often, step 3 wil l force you to reconsider steps 1 and 2! In this section, we focus on the concepts related to ste p 1 but will discuss and stress all three throughout the text. Variables Once we define the question that we want the test to answer, the next step is to identify the relevant process parameters and variables. Variables are entities that influence the test. In addition to the targeted measured variable, there may be other variables pertinent to the measured process that will affect the outcome. All known process variables should be evaluated for any possible cause-and- effect relationships. If a change in one variable will not affect the value of some other variable, the two are considered independent of each other. Avariable that can be changed independently of other variables is known as an independent variable. Avariable that is affected by changes in one or more other variables is known as a dependent variable. Normally, thevariable that we measure depends on the value of the variables that control the process. Avariable may be continuous, in that its value is able to change in a continuous manner, such as stress under a changing load or temperature in a room, or it may be discrete in that it takes on discrete values or can be quantified in a discrete way, such as the value of the role of dice or a test run by a single operator. The control of variables is important. Avariable is controlled if it can be held at a constant value or at some prescribed condition during a measurement. Complete control of a variable would imply that it can be held to an exact prescribed value. Such complete control of a variable is not usually possible. We use the adjective ‘‘controlled’’ to refer to a variable that can be held as prescribed, at least in a nominal sense. The cause-and-effect relationship between the independent variables and the dependent variable is found by controlling the values of the independent variables while measuring the dependent variable. Variables that are not or cannot be controlled during measurement butthat affect thevalue of the variable measured are called extraneous variables. Their influence can confuse the clear relation between cause and effect in a measurement. Would not the driving style affect the fuel consumption of a car? Then unless controlled, this influence will affect the result. Extraneous variables can introduce differences in repeated measurements of the same measured variable taken under seemingly identical operating conditions. They can also impose a false trend onto the behavior of that variable. The effects due to extraneous variables can take the form of signals superimposed onto the measured signal with such forms as noise and drift. 3 The tolerance design plan strategy used in this text draws on uncertainty analysis, a form of sensitivity analysis. Sensitivity methods are common in design optimization. E1C01 09/14/2010 15:40:34 Page 8 8 Chapter 1 Basic Concepts of Measurement Methods Boiling point results 215 214 Boiling region 213 212 212.5 211 212.1 210 211.6 209 Test 1 (30.2 in. Hg) Temperature ºF Test 2 (29.7 in. Hg) 208 Test 3 (30.0 in. Hg) 207 206 205 1 2 3 4 5 6 7 Time (min) Figure 1.6 Results of a boiling point test for water. Consider a thermodynamics experiment to establish the boiling point of water. The apparatus for measuring the boiling point might yield the results shown in Figure 1.6 for three test runs conducted on separate days. Notice the different outcome for each test. Why should the data from three seemingly identical tests show such different results? Suppose we determine that the measurement system accuracy accounts for only 0.1 ▯F of the test data scatter. So another plausible contributing factor is the effect of an extraneous variable. Indeed, a close examination of the test data shows a measured variation in the barometric pressure, which would affect the boiling temperature. The pressure variation is consistent with the trend seen in the boiling point data. Because the local barometric pressure was not controlled (i.e., it was not held fixed between the tests), the pressure acted as an extraneous variable adding to the differences in outcomes between the test runs. Control important variables or be prepared to solve a puzzle! Parameters In this text, we define a parameter as a functional grouping of variables. For example, a moment of inertia or a Reynolds number has its value determined from the values of a grouping of variables. A parameter that has an effect on the behavior of the measured variable is called a control parameter. Available methods for establishing control parameters based on known process variables include similarity and dimensional analysis techniques and physical laws (2–4). A parameter is controlled if its value can be maintained during a set of measurements. As an example, the flow rate, Q, developed by a fan depends on rotational speed, n, and the diameter, d, of the fan. A control parameter for this group of three variables, found by similarity methods, is the fan flow coefficient, C ¼ Q=nd . For a given fan, d is fixed (and therefore 1 controlled), and if speed is somehow controlled, the fan flow rate associated with that speed can be measured and the flow coefficient can be determined. E1C01 09/14/2010 15:40:34 Page 9 1.3 Experimental Test Plan 9 Noise and Interference Just how extraneous variables affect measured data can be delineated into noise and interference. Noise is a random variation of the value of the measured signal as a consequence of the variation of the extraneous variables. Noise increases data scatter. Interference imposes undesirable determi- nistic trends on the measured value. Any uncontrolled influence that causes the signal or test outcome to behave in a manner different from its true behavior is interference. A common interference in electrical instru ments comes from an AC power source and is seen as a sinusoidal wave superimposed onto the measured signal path. Hum and acoustic feedback in public address and audio systems are ready examples of interference effects that are superimposed onto a desirable signal. Sometime s the interference is obvious. But if the period of the interference is longer than the period over which the measurement is made, the false trend may go unnoticed. So we want either to cont rol the source of interference or to break up its trend. Consider the effects of noise and interference on the signal, yð tÞ¼ 2 þ sin2pt. As shown in Figure 1.7, noise adds to the scatter of the signal. Through statistical techniques and other means, we can sift through the noise to get at the desirable signal information. But interference imposes a trend onto the signal. The measurement plan should be devised to break up such trends so that they appear as random variations in the data set. Although this will increase the scatter in the measured values of a data set, noise can be handled by statistics. It is far more important to eliminate false trends in the data set. With this discussion in mind, recall the boiling point example earlier. Barometric pressure caused interference in each individual test. The barometric pressure did not change over the conduct of any one test. But we could discern the effect only because we showed the results of several tests taken over a period for which the value of this uncontrolled variable did change. This is a form of randomization in that as barometric pressure changed between tests, its effect was entered into the data set. Randomization methods are available that can be easily incorporated into the measurement 6 Signal: y(t) = 2 + sin (2πt) 5 Signal + interference 4 3 Signal + noise Signal y(t) 2 1 0 Figure 1.7 Effects of noise and 0.0 0.5 1.0 1.5 2.0 interference superimposed on Time (s) the signal y(t) ¼ 2 þ sin 2pt. E1C01 09/14/2010 15:40:34 Page 10 10 Chapter 1 Basic Concepts of Measurement Methods plan and will minimize or eliminate interference trends. Several methods are discussed in the paragraphs that follow. Random Tests Recall our car fuel-usage example in which the question is: ‘‘What fuel usage should I expect from this car?’’ Let y be the fuel use, which depends on x , fael volume consumption, and x , distabce traveled. We determine y by varying these two variables (that is, we drive the car). But the test result can be affected by discrete extraneous variables such as the route, driver, weather, and road conditions. For example, driving only on interstate highways would impose a false (untypical) trend on our intended average fuel estimate, so we could drive on different types of roads to break up this trend. This approach introduces a random test strategy. In general, consider the situation in which the dependent variable, y, is a function of several independent variables, x a, xb,....Howe,the measurement of y can also be influenced by several extraneous variables, z , where j ¼ 1, 2, . . . , such that y ¼ fx ▯ ▯ ;x ;...; z . To find the j a b j dependence of y on the independent variables, they are varied in a controlled manner. Although the influence of the z j variables on these tests cannot be eliminated, the possibility of their introducing a false trend on y can be minimized by a proper test strategy. Randomization is one such strategy. Randomization We define a random test by a measurement matrix that sets a random order to the change in thevalue of the independentvariable applied. The effect of the random order on the results of the testis termed randomization. Trends normally introduced by the coupling of a relatively slow and uncontrolled variation in the extraneous variables with a sequential application in values of the independent variable applied will be broken up. This type of plan is effective for the local control of extraneous variables that change in a continuous manner. Consider Examples 1.1 and 1.2. Discrete extraneous variables are treated a little differently. The use of different instruments, different test operators, and different test operating conditions are examples of discrete extraneous variablesthatcanaffecttheoutcomeofameasurement.Randomizingatestmatrixtominimizediscrete influencescanbedoneefficientlythroughtheuseofexperimentaldesignusingrandomblocks.Ablock consists of a data set of the measured variable in which the controlled variable is varied but the extraneous variable is fixed. The extraneous variable is varied between blocks. This enables some amount of local control over the discrete extraneous variable. In the fuel-usage example, we might consider several blocks, each comprised of a different driver (extraneous variable) driving similar routes, and averaging the results. In the example of Figure 1.6, if we cannot control the barometric pressure in the test, then the imposed strategy of using several tests (blocks) under different values of barometric pressure breaks up the interference effect found in a single test. Many strategies for randomized blocks exist, as do advanced statistical methods for data analysis (5–8). In any event, a randomtestisusefultoassesstheinfluenceofanuncontrolledvariable.ConsiderExamples1.3and1.4. Example 1.1 In the pressure calibration system shown in Figure 1.8, a sensor–transducer is exposed to a known pressure, p. The transducer, powered by an external supply, converts the sensed signal into a voltage that is measured by a voltmeter. The measurement approach is to control the applied E1C01 09/14/2010 15:40:34 Page 11 1.3 Experimental Test Plan 11 Extraneous x variables Open to atmosphere Power Pressure source p,∀, T transducer Voltmeter Piston Cylinder Figure 1.8 Pressure calibration system. pressure by the measured displace mentofapistonthatisusedtoc ompress a gas contained within the piston-cylinder chamber. The gas chosen closely obeys the ideal gas law. Hence, piston displacement, x, which sets the chamber volume, 8¼ (x ▯ area), is easily related to chamber pressure. Identify the independent and depend ent variables in the calibration and possible extraneous variables. KNOWN Pressure calibration system of Figure 1.8. FIND Independent, dependent, and extraneous variables. SOLUTION The control parameter for this problem can be formed from the ideal gas law: p8/T ¼ constant, where T is the gas temperature. An independent variable in the cali


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