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
Results 1-5 of 85
Page ix
... Homogeneous Media 171 5.2.1.1 n + 1 Wires 173 5.2.1.2 n Wires Above an Infinite , Perfectly Conducting Plane 173 5.2.1.3 n Wires Within a Perfectly Conducting Cylindrical Shield 174 5.2.2 Numerical Methods for the General Case 5.2.2.1 ...
... Homogeneous Media 171 5.2.1.1 n + 1 Wires 173 5.2.1.2 n Wires Above an Infinite , Perfectly Conducting Plane 173 5.2.1.3 n Wires Within a Perfectly Conducting Cylindrical Shield 174 5.2.2 Numerical Methods for the General Case 5.2.2.1 ...
Page x
... Homogeneous Media 7.2.2.2 Lossy Conductors in Lossy, Homogeneous Media 7.2.2.3 Perfect Conductors in Lossless, Inhomogeneous 292 293 Media 296 7.2.2.4 The General Case: Lossy Conductors in Lossy, Inhomogeneous Media 298 7.2.2.5 Cyclic ...
... Homogeneous Media 7.2.2.2 Lossy Conductors in Lossy, Homogeneous Media 7.2.2.3 Perfect Conductors in Lossless, Inhomogeneous 292 293 Media 296 7.2.2.4 The General Case: Lossy Conductors in Lossy, Inhomogeneous Media 298 7.2.2.5 Cyclic ...
Page xii
... Homogeneous Media 9.1.2.2 Lossless Lines in Inhomogeneous Media 9.1.2.3 Incorporating the Terminal Conditions via the SPICE Program 471 476 478 479 482 9.1.3 Lumped-Circuit Approximate Characterizations 9.1.4 The Time-Domain to ...
... Homogeneous Media 9.1.2.2 Lossless Lines in Inhomogeneous Media 9.1.2.3 Incorporating the Terminal Conditions via the SPICE Program 471 476 478 479 482 9.1.3 Lumped-Circuit Approximate Characterizations 9.1.4 The Time-Domain to ...
Page xiii
... Homogeneous Medium 548 10.1.1 Inductive and Capacitive Coupling 554 10.1.2 Common - Impedance Coupling 556 10.2 The Literal Time - Domain Solution for a Homogeneous Medium 558 10.2.1 Explicit Solution 560 10.2.2 Weakly Coupled Lines 562 ...
... Homogeneous Medium 548 10.1.1 Inductive and Capacitive Coupling 554 10.1.2 Common - Impedance Coupling 556 10.2 The Literal Time - Domain Solution for a Homogeneous Medium 558 10.2.1 Explicit Solution 560 10.2.2 Weakly Coupled Lines 562 ...
Page xiv
... Homogeneous Media 658 12.2.4 Lumped - Circuit Approximate Characterizations 12.2.5 Uniform Plane - Wave Excitation of the Line 660 660 12.3 The Time - Domain Solution 667 12.3.1 Decoupling the MTL Equations 668 12.3.2 A SPICE Equivalent ...
... Homogeneous Media 658 12.2.4 Lumped - Circuit Approximate Characterizations 12.2.5 Uniform Plane - Wave Excitation of the Line 660 660 12.3 The Time - Domain Solution 667 12.3.1 Decoupling the MTL Equations 668 12.3.2 A SPICE Equivalent ...
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