Analysis of Multiconductor Transmission LinesThe essential textbook for electrical engineering students and professionals-now in a valuable new edition The increasing use of high-speed digital technology requires that all electrical engineers have a working knowledge of transmission lines. However, because of the introduction of computer engineering courses into already-crowded four-year undergraduate programs, the transmission line courses in many electrical engineering programs have been relegated to a senior technical elective, if offered at all. Now, Analysis of Multiconductor Transmission Lines, Second Edition has been significantly updated and reorganized to fill the need for a structured course on transmission lines in a senior undergraduate- or graduate-level electrical engineering program. In this new edition, each broad analysis topic, e.g., per-unit-length parameters, frequency-domain analysis, time-domain analysis, and incident field excitation, now has a chapter concerning two-conductor lines followed immediately by a chapter on MTLs for that topic. This enables instructors to emphasize two-conductor lines or MTLs or both. In addition to the reorganization of the material, this Second Edition now contains important advancements in analysis methods that have developed since the previous edition, such as methods for achieving signal integrity (SI) in high-speed digital interconnects, the finite-difference, time-domain (FDTD) solution methods, and the time-domain to frequency-domain transformation (TDFD) method. Furthermore, the content of Chapters 8 and 9 on digital signal propagation and signal integrity application has been considerably expanded upon to reflect all of the vital information current and future designers of high-speed digital systems need to know. |
From inside the book
Page xiii
... Representation of the Lossy MTL with the Generalized Method of Characteristics 498 499 501 9.2.5 Model Order ... Representations 585 11.2 The Frequency - Domain Solution 586 11.2.1 Solution of the Transmission - Line Equations 586 xiv ...
... Representation of the Lossy MTL with the Generalized Method of Characteristics 498 499 501 9.2.5 Model Order ... Representations 585 11.2 The Frequency - Domain Solution 586 11.2.1 Solution of the Transmission - Line Equations 586 xiv ...
Page xv
... Representation with Lumped - Circuit Approximate Models 13.3 Representation via the Admittance or Impedance 2n - Port Parameters 13.4 Representation with the BLT Equations 686 691 692 693 696 699 699 712 13.5 Direct Time - Domain ...
... Representation with Lumped - Circuit Approximate Models 13.3 Representation via the Admittance or Impedance 2n - Port Parameters 13.4 Representation with the BLT Equations 686 691 692 693 696 699 699 712 13.5 Direct Time - Domain ...
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Contents
Introduction | 1 |
43 | 22 |
56 | 28 |
Problems | 61 |
References | 69 |
77 | 137 |
79 | 156 |
Rectangular Cross Section | 189 |
References | 399 |
Problems | 461 |
References | 467 |
Terminations in the FDTD Analysis | 490 |
Literal Symbolic Solutions for ThreeConductor Lines | 544 |
Problems | 575 |
CONTENTS | 592 |
Problems | 638 |
81 | 208 |
The TransmissionLine Equations for Multiconductor Lines | 215 |
FrequencyDomain Analysis of TwoConductor Lines | 240 |
1 | 260 |
Problems | 278 |
Problems | 338 |
Equations from the Integral Form of Maxwells Equations | 386 |
Common terms and phrases
ANALYSIS OF MULTICONDUCTOR approximate bound charge capacitance matrix chain-parameter matrix Chapter characteristic impedance charge distribution computed cross section crosstalk denoted determine diagonal dielectric domain electric field Electromagnetic Compatibility FDTD frequency frequency-domain FREQUENCY-DOMAIN ANALYSIS gives ground plane Hence homogeneous medium identical IEEE Transactions illustrated in Figure INCIDENT FIELD EXCITATION inhomogeneous input internal inductance ith conductor Laplace transform line length line voltages load voltage losses lossless line lossy lumped-Pi method mils MTL equations MULTICONDUCTOR LINES multiconductor transmission lines near-end crosstalk node obtained per-unit-length capacitance per-unit-length inductance PER-UNIT-LENGTH PARAMETERS permittivity pF/m phasor potential predictions printed circuit board propagation pulse reference conductor reflection coefficient resistance ribbon cable shown in Figure skin effect solution solved SPICE model Substituting surface TDFD time-domain transmission lines transmission-line equations transverse TWO-CONDUCTOR LINES vector voltages and currents Vs(t wave waveform wire zero