Harmonic Balance Finite Element Method
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Harmonic Balance Finite Element Method

Applications in Nonlinear Electromagnetics and Power Systems

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eBook - ePub

Harmonic Balance Finite Element Method

Applications in Nonlinear Electromagnetics and Power Systems

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About This Book

The first book applying HBFEM to practical electronic nonlinear field and circuit problems • Examines and solves wide aspects of practical electrical and electronic nonlinear field and circuit problems presented by HBFEM
• Combines the latest research work with essential background knowledge, providing an all-encompassing reference for researchers, power engineers and students of applied electromagnetics analysis
• There are very few books dealing with the solution of nonlinear electric- power-related problems
• The contents are based on the authors' many years' research and industry experience; they approach the subject in a well-designed and logical way
• It is expected that HBFEM will become a more useful and practical technique over the next 5 years due to the HVDC power system, renewable energy system and Smart Grid, HF magnetic used in DC/DC converter, and Multi-pulse transformer for HVDC power supply
• HBFEM can provide effective and economic solutions to R&D product development
• Includes Matlab exercises

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1
Introduction to Harmonic Balance Finite Element Method (HBFEM)

1.1 Harmonic Problems in Power Systems

The harmonics problem in power systems is not a new problem. It has existed since the early 1900s – as long as AC power itself has been available. The earliest harmonic distortion issues were associated with third harmonic currents produced by saturated iron in machines and transformers, or so‐called ferromagnetic loads. Later, arcing loads, like lighting and electric arc furnaces, were also shown to produce harmonic distortion. The final type, electronic loads, burst onto the power scene in the 1970s and 1980s, and has represented the fastest growing category ever since [1].
Since power system harmonic distortion is mainly caused by non‐linear loads and power electronics used in the electrical power system [2, 3], the presence of non‐linear loads and the increasing number of distributed generation power systems in electrical grids contributes to changing the characteristics of voltage and current waveforms in power systems (which differ from pure sinusoidal constant amplitude signals). The impact of non‐linear loads and power electronics used in electrical power systems has been increasing during the last decade.
Such electrical loads, which introduce non‐sinusoidal current consumption patterns (current harmonics), can be found in power electronics [4], such as: DC/AC inverters; switch mode power supplies; rectification front‐ends in motor drives; electronic ballasts for discharge lamps; personal computers or electrical appliances; high‐voltage DC (HVDC) power systems; impulse transformers; magnetic induction devices; and various electric machines. In addition, the harmonics can be generated in distributed renewable energy systems, geomagnetic disturbances (GMDs) and geomagnetic induced currents (GICs) [5, 6].
Harmonics in power systems means the existence of signals, superimposed on the fundamental signal, whose frequencies are integer numbers of the fundamental frequency. The presence of harmonics in the voltage or current waveform leads to a distorted signal for the voltage or current, and the signal becomes non‐sinusoidal. Thus, the study of power system harmonics is an important subject for electrical engineers. Electricity supply authorities normally abrogate responsibility on harmonic matters by introducing standards or recommendations for the limitation of voltage harmonic levels at the points of common coupling between consumers.

1.1.1 Harmonic Phenomena in Power Systems

A better understanding of power system harmonic phenomena can be achieved by consideration of some fundamental concepts, especially the nature of non‐linear loads, and the interaction of harmonic currents and voltages within the power system. By definition, harmonic (or non‐linear) loads are those devices that naturally produce a non‐sinusoidal current when energized by a sinusoidal voltage source. As shown in Figure 1.1, each “waveform” represents the variation in instantaneous current over time for two different loads each energized from a sinusoidal voltage source. This pattern is repeated continuously, as long as the device is energized, creating a set of largely‐identical waveforms that adhere to a common time period. Both current waveforms were produced by turning on some type of load device. In the case of the current on the left, this device was probably an electric motor or resistance heater. The current on the right could have been produced by an electronic variable‐speed drive, for example. The devices could be single‐ or three‐phase, but only one phase current waveform is shown for illustration. The other phases would be similar.
Graphs displaying a sine wave or sinusoidal current (left) and a distorted waveform or non-sinusoidal current (right).
Figure 1.1 (a) Sine wave. (b) Distorted waveform or non‐sinusoidal
A French mathematician, Jean Fourier, discovered a special characteristic of periodic waveforms in the early 19th century. The method describing the non‐sinusoidal waveform is called its Fourier Series. The Fourier theorem breaks down a periodic wave into its component frequencies. Periodic waveforms are those waveforms comprised of identical values that repeat in the same time interval, as shown in Figure 1.2. Fourier discovered that periodic waveforms can be represented by a series of sinusoids summed together. The frequency of these sinusoids is an integer multiple of the frequency represented by the fundamental periodic waveform.
Graph of distorted current waveform with an arrow to a graph of equivalent harmonic components by Fourier series. Fundamental (60 Hz), 5th harmonic (300 Hz), and 7th harmonic (420 Hz) are indicated.
Figure 1.2 Distorted waveform and number of harmonics by Fourier series
The distorted (non‐linear) waveform, however, deserves further scrutiny. This waveform meets the continuous, periodic requirement established by Fourier. It can be described, therefore, by a series of sinusoids. This example waveform is represented by only three harmonic components, but some real‐world waveforms (square wave, for example) require hundreds of sinusoidal components to describe them fully. The magnitude of these sinusoids decreases with increasing frequency, often allowing the power engineer to ignore the effect of components above the 50th harmonic.

1.1.2 Sources and Problems of Harmonics in Power Systems

Harmonic sources generated in power systems can be divided into two categories: established and known; and new and future. Table 1.1 presents sources and problems of harmonics. Harmonic problems in power systems can be traced to a number of factors [3], such as: (a) the substantial increase of non‐linear loads resulting from new technologies such as silicon‐controlled rectifiers (SCRs), power transistors, and microprocessor controls, which create load‐generated harmonics throughout the system; and (b) a change in equipment design philosophy.
Table 1.1 Sources and problems of harmonics
Established and known New and future
Tooth ripple or ripples in the voltage waveform of rotating machines. Energy conservation measures, such as those for improved motor efficiency and load‐matching, which employ power semiconductor devices and switching for their operation. These devices often produce irregular voltage and current waveforms that are rich in harmonics.
Variations in air‐gap reluctance over synchronous machine pole pitch. Motor control devices, such as speed controls for traction.
Flux distortion in the synchronous machine from sudden load changes. High‐voltage direct current power conversion and transmission.
Non‐sinusoidal distribution of the flux in the air gap of synchronous machines. Interconnection of wind and solar power converters with distribution systems.
Transformer magnetizing currents. Static var compensators which have largely replaced synchronous condensers as continuously variable‐var sources.
Network non‐linearities from loads such as rectifiers, inverters, welders, arc furnaces, voltage controllers, frequency converters, etc. The development and potential use of electric vehicles that require a significant amount of power rectification for battery charging.
N/A The potential use of direct energy conversion devices, such as magneto‐hydrodynamics, storage batteries, and fuel cells that require DC/AC power converters.
N/A Cyclo‐converters used for low‐speed high‐torque machines.
N/A Pulse‐burst‐modulated heating elements for large furnaces.
In the past, equipment designs tended to be under‐rated or over‐designed. Nowadays, in order to be competitive, power devices and equipment are more critically designed and, in the case of iron‐core devices, their operating points are more focused on non‐linear regions. Operation in these regions results in a sharp rise in harmonics.

1.1.3 Total Harmonic Distortion (THD)

The reduced impedance at the peak voltage results in a large, sudden rise in current flow until the impedance is suddenly increased, resulting in a sudden drop in current. Because the voltage and current waveforms are no longer related, they are said to be “non‐linear”. These non‐sinusoidal current pulses introduce unanticipated reflective currents back into the power distribution system, and the currents operate at frequencies other than the fundamental 50/60 Hz. Ideally, voltage and current waveforms are perfect sinusoids. However, because of the increased non‐linear load and power electronic devices based on switch mode power supplies and motor drives, these waveforms quite often become distorted. This deviation from a perfect sine wave can be represented by harmonics – sinusoidal components having a frequency that is an integral multiple of the fundamental frequency, as shown in Figure 1.3. Thus, a non‐sinusoidal wave has distort...

Table of contents

  1. Cover
  2. Title Page
  3. Table of Contents
  4. Preface
  5. About the Companion Website
  6. 1 Introduction to Harmonic Balance Finite Element Method (HBFEM)
  7. 2 Nonlinear Electromagnetic Field and Its Harmonic Problems
  8. 3 Harmonic Balance Methods Used in Computational Electromagnetics
  9. 4 HBFEM for Nonlinear Magnetic Field Problems
  10. 5 Advanced Numerical Approach using HBFEM
  11. 6 HBFEM and Its Future Applications
  12. Appendix
  13. Index
  14. End User License Agreement