
Power Magnetic Devices
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Discover a cutting-edge discussion of the design process for power magnetic devices
In the newly revised second edition of Power Magnetic Devices: A Multi-Objective Design Approach, accomplished engineer and author Dr. Scott D. Sudhoff delivers a thorough exploration of the design principles of power magnetic devices such as inductors, transformers, and rotating electric machinery using a systematic and consistent framework.
The book includes new chapters on converter and inverter magnetic components (including three-phase and common-mode inductors) and elaborates on characteristics of power electronics that are required knowledge in magnetics. New chapters on parasitic capacitance and finite element analysis have also been incorporated into the new edition. The work further includes:
* A thorough introduction to evolutionary computing-based optimization and magnetic analysis techniques
* Discussions of force and torque production, electromagnet design, and rotating electric machine design
* Full chapters on high-frequency effects such as skin- and proximity-effect losses, core losses and their characterization, thermal analysis, and parasitic capacitance
* Treatments of dc-dc converter design, as well as three-phase and common-mode inductor design for inverters
* An extensive open-source MATLAB code base, PowerPoint slides, and a solutions manual
Perfect for practicing power engineers and designers, Power Magnetic Devices will serve as an excellent textbook for advanced undergraduate and graduate courses in electromechanical and electromagnetic design.
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SCOTT D. SUDHOFF, PhD, is a Professor of Electrical and Computer Engineering at Purdue University. He served as Editor-in-Chief of IEEE???s Transactions on Energy Conversion and IEEE???s Power and Energy Technology Systems Journal. He is an IEEE Fellow, recipient of the Veinott award, and co-author of the Wiley-IEEE Press title Analysis of Electric Machinery and Drive Systems, Third Edition (2013). Dr. Sudhoff also holds patents in the areas of solid-state distribution transformers, stability of power-electronics based systems, and novel electric machine design concepts.
Content
Author Biography xiii
Preface xv
About the Companion Site xix
1 Optimization-Based Design 1
1.1 Design Approach 1
1.2 Mathematical Properties of Objective Functions 3
1.3 Single-Objective Optimization Using Newton's Method 5
1.4 Genetic Algorithms: Review of Biological Genetics 7
1.5 The Canonical Genetic Algorithm 10
1.6 Real-Coded Genetic Algorithms 15
1.7 Multi-Objective Optimization and the Pareto-Optimal Front 25
1.8 Multi-Objective Optimization Using Genetic Algorithms 27
1.9 Formulation of Fitness Functions for Design Problems 31
1.10 A Design Example 33
References 39
Problems 40
2 Magnetics and Magnetic Equivalent Circuits 43
2.1 Ampere's Law, Magnetomotive Force, and Kirchhoff's MMF Law for Magnetic Circuits 43
2.2 Magnetic Flux, Gauss's Law, and Kirchhoff's Flux Law for Magnetic Circuits 46
2.3 Magnetically Conductive Materials and Ohm's Law For Magnetic Circuits 48
2.4 Construction of the Magnetic Equivalent Circuit 56
2.5 Translation of Magnetic Circuits to Electric Circuits: Flux Linkage and Inductance 59
2.6 Representing Fringing Flux in Magnetic Circuits 64
2.7 Representing Leakage Flux in Magnetic Circuits 68
2.8 Numerical Solution of Nonlinear Magnetic Circuits 80
2.9 Permanent Magnet Materials and Their Magnetic Circuit Representation 95
2.10 Closing Remarks 98
References 98
Problems 99
3 Introduction to Inductor Design 103
3.1 Common Inductor Architectures 103
3.2 DC Coil Resistance 105
3.3 DC Inductor Design 108
3.4 Case Study 113
3.5 Closing Remarks 119
References 120
Problems 120
4 Force and Torque 123
4.1 Energy Storage in Electromechanical Devices 123
4.2 Calculation of Field Energy 125
4.3 Force from Field Energy 127
4.4 Co-Energy 128
4.5 Force from Co-Energy 132
4.6 Conditions for Conservative Fields 133
4.7 Magnetically Linear Systems 134
4.8 Torque 135
4.9 Calculating Force Using Magnetic Equivalent Circuits 135
References 139
Problems 139
5 Introduction to Electromagnet Design 141
5.1 Common Electromagnet Architectures 141
5.2 Magnetic, Electric, and Force Analysis of an Ei-Core Electromagnet 141
5.3 EI-Core Electromagnet Design 151
5.4 Case Study 155
References 162
Problems 163
6 Magnetic Core Loss and Material Characterization 165
6.1 Eddy Current Losses 165
6.2 Hysteresis Loss and the B-H Loop 172
6.3 Empirical Modeling of Core Loss 177
6.4 Magnetic Material Characterization 183
6.5 Measuring Anhysteretic Behavior 188
6.6 Characterizing Behavioral Loss Models 197
6.7 Time-Domain Loss Modeling: the Preisach Model 201
6.8 Time-Domain Loss Modeling: the Extended Jiles-Atherton Model 205
References 211
Problems 212
7 Transformer Design 215
7.1 Common Transformer Architectures 215
7.2 T-Equivalent Circuit Model 217
7.3 Steady-State Analysis 221
7.4 Transformer Performance Considerations 223
7.5 Core-Type Transformer Configuration 231
7.6 Core-Type Transformer MEC 238
7.7 Core Loss 244
7.8 Core-Type Transformer Design 245
7.9 Case Study 251
7.10 Closing Remarks 259
References 260
Problems 260
8 Distributed Windings and Rotating Electric Machinery 263
8.1 Describing Distributed Windings 263
8.2 Winding Functions 271
8.3 Air-Gap Magneto Motive Force 276
8.4 Rotating MMF 278
8.5 Flux Linkage and Inductance 280
8.6 Slot Effects and Carter's Coefficient 282
8.7 Leakage Inductance 284
8.8 Resistance 289
8.9 Introduction to Reference Frame Theory 290
8.10 Expressions for Torque 294
References 299
Problems 299
9 Introduction to Permanent Magnet AC Machine Design 303
9.1 Permanent Magnet Synchronous Machines 303
9.2 Operating Characteristics of PMAC Machines 305
9.3 Machine Geometry 312
9.4 Stator Winding 317
9.5 Material Parameters 320
9.6 Stator Currents and Control Philosophy 320
9.7 Radial Field Analysis 321
9.8 Lumped Parameters 326
9.9 Ferromagnetic Field Analysis 327
9.10 Formulation of Design Problem 332
9.11 Case Study 336
9.12 Extensions 344
References 345
Problems 346
10 Introduction to Thermal Equivalent Circuits 349
10.1 Heat Energy, Heat Flow, and the Heat Equation 349
10.2 Thermal Equivalent Circuit of One-Dimensional Heat Flow 352
10.3 Thermal Equivalent Circuit of a Cuboidal Region 358
10.4 Thermal Equivalent Circuit of a Cylindrical Region 361
10.5 Inhomogeneous Regions 367
10.6 Material Boundaries 373
10.7 Thermal Equivalent Circuit Networks 376
10.8 Case Study: Thermal Model of Electromagnet 380
References 396
Problems 397
11 Alternating Current Conductor Losses 399
11.1 Skin Effect in Strip Conductors 399
11.2 Skin Effect in Cylindrical Conductors 405
11.3 Proximity Effect in a Single Conductor 409
11.4 Independence of Skin and Proximity Effects 411
11.5 Proximity Effect in a Group of Conductors 413
11.6 Relating Mean-Squared Field and Leakage Permeance 416
11.7 Mean-Squared Field for Select Geometries 417
11.8 Conductor Losses in Rotating Machinery 422
11.9 Conductor Losses in a UI-Core Inductor 426
11.10 Closing Remarks 431
References 431
Problems 432
12 Parasitic Capacitance 433
12.1 Modeling Approach 433
12.2 Review of Electrostatics 434
12.3 Turn-to-Turn Capacitance 442
12.4 Coil-to-Core Capacitance 446
12.5 Layer-to-Layer Capacitance 449
12.6 Capacitance in Multi-Winding Systems 452
12.7 Measuring Capacitance 455
References 458
Problems 459
13 Buck Converter Design 461
13.1 Buck Converter Analysis 461
13.2 Semiconductors 469
13.3 Heat Sink 472
13.4 Capacitors 474
13.5 UI-Core Input Inductor 476
13.6 UI-Core Output Inductor 477
13.7 Operating Point Analysis 488
13.8 Design Paradigm 492
13.9 Case Study 495
13.10 Extensions 501
References 501
Problems 501
14 Three-Phase Inductor Design 503
14.1 System Description 503
14.2 Inductor Geometry 516
14.3 Magnetic Equivalent Circuit 518
14.4 Magnetic Analysis 529
14.5 Inductor Design Paradigm 533
14.6 Case Study 537
References 541
Problems 541
15 Common-Mode Inductor Design 543
15.1 Common-Mode Voltage and Current 543
15.2 System Description 545
15.3 Common-Mode Equivalent Circuit 546
15.4 Common-Mode Inductor Specification 552
15.5 UR-Core Common-Mode Inductor 557
15.6 UR-Core Common-Mode Inductor Magnetic Analysis 562
15.7 Common-Mode Inductor Design Paradigm 564
15.8 Common-Mode Inductor Case Study 566
References 571
Problems 571
16 Finite Element Analysis 573
16.1 Maxwell's and Poisson's Equations 573
16.2 Finite Element Analysis Formulation 575
16.3 Finite Element Analysis Implementation 580
16.4 Closing Remarks 587
References 588
Problems 588
Appendix A Conductor Data and Wire Gauges 589
Appendix B Selected Ferrimagnetic Core Data 593
Appendix C Selected Magnetic Steel Data 595
Appendix D Selected Permanent Magnet Data 599
Appendix E Phasor Analysis 601
Appendix F Trigonometric Identities 607
Index 609
1
Optimization-Based Design
We will begin our study of power magnetic device design with a general consideration of the design process. A case will be made to approach the design process rather formally by converting the design problem into an optimization problem. Next, single-objective optimization is discussed, with particular emphasis on optimization using genetic algorithms (GAs). This is followed by a discussion of multi-objective optimization. Practical aspects of formulating design problems as optimization problems are then considered. The chapter concludes with a design example that focuses on a UI-core inductor.
1.1 Design Approach
It is appropriate to begin this work by considering the design process. Clearly, there are a myriad of different approaches by which components may be designed. For example, a possible manual design process is illustrated in Figure 1.1. In order to consider this process in a more concrete way, suppose that the component we are designing is an electromagnet and that we wish to design an electromagnet so that a certain set of specifications are met.
Using the design process in Figure 1.1, our first step would be to perform a detailed mathematical analysis of the device. Typically, when we analyze a device, our analysis predicts device performance (mass, loss, force) in terms of the device parameters (geometry, materials) rather than directly addressing the design problem by deriving expressions for what the device parameters should be in terms of the device specifications (allowed loss, required force). Therefore, we must manipulate our detailed analysis into a set of design equations that are used to calculate the design parameters as a function of device specifications. However, going from detailed analysis to design equations invariably requires numerous assumptions and approximations, even beyond the ones found in our original "detailed" analysis. As a result, we check our design, either against our original analysis or using some numerical tool such as a finite element analysis. Based on the results from the numerical analysis, we will revise the design and repeat the numerical analysis until specifications are met, at which point we have arrived at a final design. Of course, we often use a more involved design process; for example, another iteration of the design may be made based on physical prototypes.
The manual design process we have been considering involves an engineer in the iteration process. Variations of this process are successfully used ubiquitously throughout the engineering community. However, the process has some significant drawbacks. First, it requires a great deal of engineering time. Second, it requires a great deal of engineering experience. This experience comes into play in the development of the design equations, which often take the form of rules-of-thumb based at least partially on experience. Experience is also a factor in making changes to the design based on the numerical analysis. Finally, while the process has been very successful in yielding working designs, it may not lead to the best design.
Figure 1.1 A manual design process.
Figure 1.2 Optimization-based design process.
An alternate design process is illustrated in Figure 1.2. Therein, an optimization-based design process is shown. In this case, the process is not illustrated in a sequential manner as in Figure 1.1, but rather in an organizational manner. The process again starts with a detailed analysis of the device or component. However, unlike the manual design process, in the optimization-based process, the detailed analysis is not used to formulate design equations. Instead, the detailed analysis is used to calculate design metrics such as mass, cost, and loss. The detailed analysis is also used to check constraints such as achieving some minimum acceptable level of performance. The metrics and constraints are combined into an objective or fitness function. This function is defined so that its optimization results in optimization of the design metrics subject to all design constraints being met.
At the outermost level of this design process, an optimization engine will select the parameters of the design (geometry, materials, etc.) so as to maximize the objective function. In terms of computational algorithm, Figure 1.2 depicts an optimization engine at the outer level. This engine operates on an objective function that is calculated based on the detailed analysis.
There are several advantages of this approach. First, it is unnecessary to formulate design equations. This is beneficial in that it reduces the number of approximations and assumptions made and reduces the amount of design experience needed for a good design. Second, the design is formally optimized with regard to the design metrics, potentially leading to better designs, at least in terms of the design metrics. Third, since the engineer is out of the optimization loop, less engineering time is generally required. There are some disadvantages of the procedure. First, the process can be numerically intense and require significant computing time, sometimes on the order of hours and, in extreme cases, days. Fortunately, computer time is significantly less expensive than engineering time. Second, the quality of the result depends upon the quality of the detailed analysis. In this regard, design experience is still valuable, though not as critical as in the manual design approach.
In order to utilize the optimization-based design process, it is clearly necessary to be able to optimize mathematical functions. For design purposes, we will be optimizing the objective function, which we will also refer to as a fitness function. Optimization is a broad subject, which has been the subject of a strong and sustained interest of a host of researchers over the years. The purpose of this chapter is to introduce the subject to an extent sufficient to enable the reader to utilize an optimization-based design process for power magnetic devices. More thorough study of optimization methods will serve every engineer well; for a good textbook devoted to the subject the reader is referred to Chong and Zak [1].
1.2 Mathematical Properties of Objective Functions
Before discussing optimization algorithms, it is appropriate to discuss some properties of objective functions that are relevant to their optimization, as these properties determine the effectiveness of one optimization approach relative to another.
As we proceed to do this, note that throughout this work, scalar variables are normally in italic font (for example, x) while vector and matrices are bold nonitalic (for example, x). Functions of all dimensionalities are denoted by nonitalic nonbold font (for example, x(?)). Brackets in equations are associated with iteration number in iterative methods.
In considering the properties of the objective function, it is appropriate to begin by defining our parameter vector, which will be denoted as x. The domain of x is referred to as the search space and will be denoted O, which is to say we require x ? O. The elements of parameter vector x will include those variables of a design that we are free to select. In general, some elements of x will be discrete in nature while others will be continuous. An example of a discrete element might be one that designates a material type from a list of available materials. A geometrical parameter such as the length of a motor would be an example of an element that can be selected from a continuous range. If all members of the parameter vector are discrete, the search space is described as being discrete. If all members of the search space are continuous (in the set of real numbers), the search space is said to be continuous. If the elements of x include both discrete and continuous elements, the search space is said to be mixed. It is assumed that the function that we wish to optimize is denoted f(x). We will assume that f(x) returns a vector of dimension m of real numbers, that is, f(x) ? Rm, where m is the number of objectives we are considering. For most of this chapter, we will merely consider f(x) to be a mathematical function for which we wish to identify the optimizer of; however, in Section 1.9, and in the rest of this book for that matter, we will focus on how to construct f(x) so as to serve as an instrument of engineering design.
For this section, let us focus on the case where all elements of x are real numbers so that x ? Rn, where Rn denotes the set of real numbers of dimension n and where the number of objectives is one (that is, m = 1) so that f(x) is a scalar function of a vector argument. Finally, let us suppose we wish to minimize f(x). A point x* is said to be the global minimizer of f over O provided that
(1.2-1)where ? is read as "for all" and O\{x*} denotes the set O less the point x*. If the = is replaced by <, then x* is referred to as the strict global minimizer.
As stated previously, the function f(x) can have properties that make it easier or more difficult to find the global minimizer. Some of these properties are depicted in Figure 1.3. An example of a feature that makes it...
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