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RF 大牛Clayton R. Paul 经典论著Analysis of Multiconductor Transmission Lines.
如果你对PCB微带线，带状线上传输的RF信号特性，多层PCB的阻抗控制还缺乏理论认识，
这本书会带给你很多帮助，RF工程师经验很重要 但是理论基础更要扎实。
【文件名】:09729@52RD_Analysis of Multiconductor Transmission Lines.part1.rar
【格 式】:rar
【大 小】:4000K
【简 介】:
A printed circuit board (PCB) consists of a planar dielectric
board on which rectangular cross section conductors (lands) serve to interconnect
digital devices as well as analog devices. Crosstalk can be a significant functional
problem with these PCB’s as can the degradation of the intended signal transmission
through attenuation, time delay, and other effects. Signal degradation, time delay
and crosstalk can create significant functional problems in today’s high-speed
digital circuits so that it is important to understand and predict this effect. It has
been said that optical fibers will eliminate many of these problems associated with
metallic conductors such as crosstalk. Although this is true to a large degree, full
implementation of fiber optic transmision paths will occur well into the future because
of the present low cost and significant use of metallic-conductor lines.
【目 录】:
1 Introduction
1.1 Examples of Multiconductor Transmission-Line Structures
1.2 Properties of the Transverse ElectroMagnetic (TEM) Mode of
1.3 Derivation of the Transmission-Line Equations for
Propagation
Two-Conductor Lines
1.3.1 Derivation from the Integral Form of Maxwell’s Equation
1.3.2 Derivation from the Differential Form of Maxwell’s
1.3.3 Derivatipn from the Per-Unit-Length Equivalent Circuit
1.3.4 Properties of the Per-Unit-Length Parameters
Equations
1.4 Classification of Transmission Lines
1.5 Restrictions on the Applicability of the Transmission-Line
Equation Formulation
1.5.1 Higher-Order Modes
1.5.1,l The Infinite Parallel-Plate Transmission Line
1.5.1.2 The Coaxial Transmission Line
1.5.1.3 Two-Wire Lines
1.5.2 Transmission-Line Currents vs. Antenna Currents
References
Problems
2 The Mulliconductor Transmission-Line Equations
2.1 Derivation from the Integral Form of Maxwell’s Equations
2.2 Derivation from the Per-Unit-Length Equivalent Circuit
2.3 Summary of the MTL Equations
2.4 Properties of the Per-Unit-Length Parameter Matrices L, C, G
References
Problems
3 The Per-Unit-iength Parameters
3.1 Definitions of the Per-Unit-Length Parameter Matrices
L, c, G
3.1.1 The Per-Unit-Length Inductance Matrix, L
3.1.2 The Per-Unit-Length Capacitance Matrix, C
3.1.3 The Per-Unit-Length Conductance Matrix, G
3.1.4 The Generalized Capacitance Matrix, Q
3.2 Multiconductor Lines Having Conductors of Circular
Cylindrical Cross Section
3.2.1 Fundamental Subproblems for Wires
3.2.1.1 Magnetic Flux Due to a Filament of Current
3,2.1.2 Voltage Due to a Filament of Charge
3.2.1.3 The Method of Images
3.2.2.1 Two Wires
3.2.2.2 One Wire Above an Infinite, Perfectly Conducting
Plane
3.2.2.3 The Coaxial Cable
Homogeneous Media
3.2.3.1 (n + 1) Wires
3.2.3.2 n Wires Above an Infinite, Perfectly Conducting
Plane
3.2.3.3 n Wires Within a Perfectly Conducting Shield
3.2.4.1 Applications to Inhomogeneous Dielectric Media
3.2.2 Exact Solutions for Two-Conductor Wire Lines
3.2,3 Wide-Separation Approximations for Wires in
3.2.4 Numerical Methods for the General Case
3.2.5 Computed Resufts: Ribbon Cables
Cross Section
3.3.1 Method of Moments (MOM) Techniques
3.3 Multiconductor Lines Having Conductors of Rectangular
3.3.1.1 Applications to Printed Circuit Boards
3.3.1.2 Computed Results: Printed Circuit Boards
3.3.2 Finite Difference Techniques
3.3.3 Finite Element Techniques
3.4 Miscellaneous Additional Techniques
3.4.1 Conformal Mapping Techniques
3.4.2 Spectral-Domain Techniques
3.5 Shielded Lines
3.6 Incorporation of Losses; Calculation of R, L,, and G
3.6.1 Calculation of the Per-Unit-Length Conductance Matrix,
3.6.2 Representation of Conductor Losses
G
3.6.2.1 Surface Impedance of Plane Conductors
3.6.2.2 Resistance and Internal Inductance of Wires
3.6.2.3 Internal Impedance of Rectangular Cross Section
3.6.2.4 Approximate Representation of Conductor
References
Problems
Conductors
Internal Impedances in the Frequency Domain
4 Frequency-Domain Analysis
4.1 The MTL Equations for Sinusoidal Steady-State Excitation
4.2 Solutions for Two-Conductor Lines
4.3 General Solution for an (n + 1)-Conductor Line
4.3.1 Analogy of the MTL Equations to the State-Variable
4.3.2 Decoupling the MTL Equations by Similarity
4.3.3 Characterizing the Line as a 2n Port with the Chain
4.3.4 Properties of the Chain Parameter Matrix
4.3.5 Incorporating the Terminal Conditions
Equations
Transformations
Parameter Matrix
4.3.5.1 The Generalized Th6venin Equivalent
4.3.5.2 The Generalized Norton Equivalent
4.3.5.3 Mixed Representations
4.3.6 Approximating Nonuniform Lines
4.4.1 Perfect Conductors in Homogeneous Media
4.4.2 Lossy Conductors in Homogeneous Media
4.4.3 Perfect Conductors in Inhomogeneous Media
4.4.4 The General Case: Lossy Conductors in Lossy
Inhomogeneous Media
4.4.5 Cyclic Symmetric Structures
4.5 Lumped-Circuit Iterative Approximate Characterizations
4.6 AI ternative 2n-Port Characterizations
4.7 Power and the Reflection Coefficient Matrix
4.8 Computed Results
4.8.1 Ribbon Cables
4.8.2 Printed Circuit Boards
References
Problems
5 Time-Domain Analysis
5.1 Two-Conductor Lossless Lines
5.1.1 Graphical Solutions
5.1.2 The Method of Characteristics (Branin’s Method)
5.1.3 The Bergeron Diagram
5.2.1 Decoupling the MTL Equations
5.2 Multiconductor Lossless Lines
5.2.1.1 Lossless Lines in Homogeneous Media
52.1.2 Lossless Lines in Inhomogeneous Media
5.2.1.3 Incorporating the Terminal Conditions via the
SPICE Program
5.2.2 Extension of Branin’s Method to Lossless
5.2.3 Time-Domain to Frequency-Domain Transformations
5.2.4 Lumped-Circuit Iterative Approximate
Characterizations
5.2.5 Finite Difference-Time Domain (FDTD) Methods
5.2.6 Computed Results
Multiconductor Lines in Homogeneous Media
5.2.6.1 Ribbon Cable
5.2.6.2 Printed Circuit Board
5.3.1 Two-Conductor Lossy Lines
5.3 Incorporation of Losses
5.3.1.1 Lumped-Circuit Approximate Characterizations
5.3.1.2 Time-Domain to Frequency-Domain
5.3.1.3 Finite Difference-Time Domain (FDTD)
5.3.1.4 Direct Solution via Inversion of the Laplace
5.3.1.5 TimaDomain Characterization of the Line as
Transformations
Methods
Transform
a Two Port
5.3,2 Multiconductor Lines
5.3.3 Computed Results
5.3.3.1 Ribbon Cable
5.3.3.2 Printed Circuit Board
References
Problems
6 Literal (Symbolic) Solutions for Three-Conductor Lines
6.1 Frequency-Domain Solution
6.1.1 Inductive and Capacitive Coupling
6.1.2 Common-Impedance Coupling
6.2 Time-Domain Solution
6.2.1 Explicit Solution
6.2.2 Weakly Coupled Lines
6.2.3 Inductive and Capacitive Coupling
6.2.4 Common-Impedance Coupling
6.3.1 A Three-Wire Ribbon Cable
6.3.2 A Three-Conductor Printed Circuit Board
References
Problems
6.3 Computed Results
7 Incident-Field Excitation of the Line
7.1 Derivation of the MTL Equations for Incident-Field
Excitation
7.1.1 Equivalence of Source Representations
7.2.1 Solution of the MTL Equations
7.2.1.1 Simplified Forms of the Excitations
7.2.2 Incorporation of the Terminal Conditions
7.2.2.1 Lossless Lines in Homogeneous Media
7.2.3 Lumped-Circuit Iterative Approximate
Characterizations
7.2.4 Uniform Plane-Wave Excitation of the Line
7.2.5 Two-Conductor Lines
7.2 Frequency-Domain Solutions
7.2.5.1 Uniform Plane-Wave Excitation of the Line
7.2.5.2 Special Cases
7.2.5.3 One Conductor Above a Ground Plane
7.2.5.4 Electrically Short Lines
7.2.6.1 Comparison with Predictions of the Method of
7.2.6.2 A Three-Wire Line in an Incident Uniform
7.2.6 Computed Results
Moments Codes
Plane Wave
7.3.1 Two-Conductor Lossless Lines
7.3 Time-Domain Solutions
7.3.1.1 The General Solution via the Method of
Characteristics
7.3.1.2 The General Solution via the Frequency
7.3.1.3 Uniform Plane-Wave Excitation of the Line
7.3.1.4 Electrically Short Lines
7.3.1.5 A SPICE Equivalent Circuit
7.3.1.6 Computed Results
7.3.2,l Decoupling the MTL Equations
7.3.2.2 A SPICE Equivalent Circuit
7.3.2.3 Lumped-Circuit Iterative Approximate
7.3.2.4 Time-Domain to Frequency-Domain
7.3.2.5 Finite Difference-Time Domain Methods
7.3.2.6 Computed Results
References
Problems
Domain
7.3.2 Multiconductor Lines
Characterizations
Transformations
8 Transmission-line Networks
8.1 Representation with the SPICE Model
8.2 Representation with Lumped-Circuit Iterative Models
8.3 Representation via the Admittance or Impedance Parameters
8.4 Representation with the BLT Equations
8.5 Direct Time-Domain Solutions in terms of Traveling Waves
References
Problems
Publications by the Author Concerning Transmission lines
Appendix A Description of Computer Software
A.l Programs for Calculation of the Per-Unit-Length
Parameters
A.1.1 Wide-Separation Approximations for Wires:
A.1.2 Ribbon Cables: RIBBON.FOR
A. 1.3 Printed Circuit Boards: PCB.FOR,
A.1.4 Coupled Microstrip Structures: MSTRP.FOR,
WIDESEP.FOR
PCBGALFOR
MSTRPGAL.FOR
A.2 Frequency-Domain Analysis
A.3 Time-Domain Analysis
A.3.1 Time-Domain to Frequency-Domain
A.3.2 Branin's Method Extended to Multiconductor
A.3.3 Finite Difference-Time Domain Method:
A.3.4 Finite Difference-Time Domain Method:
Transforma tion : TIMEFREQ.FOR
Lines: BRANIN.FOR
FINDIF.FOR
FDTDLOSS.FOR
A.4 SPICE/PSPICE Subcircuit Generation Programs
A.4.1 General Solution, Lossless Lines:
A.4.2 Lumped-pi Circuit, Lossless Lines:
A.4.3 Inductive-Capacitive Coupling Model:
SPICEMTL.FOR
SPICELPLFOR
SPICELC.FOR
AS Incident Field Excitation
A.5.1 Frequency-Domain Program: 1NCIDENT.FOR
A.5.2 SPICE/PSPICE Subcircuit Model:
A53 Finite DiKerence-Time Domain (FDTD)
References
SPICEINC.FOR
Model: FDTDINCFOR
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