By Stephen H. Hall
ISBN10: 0470192356
ISBN13: 9780470192351
ISBN10: 0470423889
ISBN13: 9780470423882
ISBN10: 0470423897
ISBN13: 9780470423899
A synergistic method of sign integrity for highspeed electronic layout
This ebook is designed to supply modern readers with an realizing of the rising highspeed sign integrity matters which are growing roadblocks in electronic layout. Written through the main specialists at the topic, it leverages ideas and methods from nonrelated fields similar to utilized physics and microwave engineering and applies them to highspeed electronic design—creating the optimum mixture among idea and useful purposes.
Following an creation to the significance of sign integrity, bankruptcy assurance comprises:
 Electromagnetic basics for sign integrity

Transmission line basics

Crosstalk

Nonideal conductor types, together with floor roughness and frequencydependent inductance

Frequencydependent homes of dielectrics

Differential signaling

Mathematical specifications of actual channels

Sparameters for electronic engineers

Nonideal go back paths and through resonance

I/O circuits and types

Equalization

Modeling and budgeting of timing jitter and noise

process research utilizing reaction floor modeling
every one bankruptcy comprises many figures and diverse examples to aid readers relate the ideas to daily layout and concludes with difficulties for readers to check their figuring out of the cloth. complicated sign Integrity for HighSpeed electronic Designs is acceptable as a textbook for graduatelevel classes on sign integrity, for courses taught in for pro engineers, and as a reference for the highspeed electronic dressmaker.
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Extra resources for Advanced signal integrity for highspeed digital designs
Example text
Suppose that a wire contains electric charges of density ρ(C/m3 ) in a region and the charges have a velocity ν(m/s). The current density in the region is calculated as J = ρ ν A/m2 (218) the instantaneous rate of charge flow per unit crosssectional area at point P in space. , the cross section of the wire) is the sum of all the current density functions within the area of the surface times the surface area. This calculates the total number of vectors ( J ) passing though the crosssectional surface S of the wire, which is flux.
Floop = I2 I 1 µ0 2π C az dz × B ay + b A −az dz × D ay a From the righthand rule, the cross products are as follows: az × ay = −ax −az × ay = ax Therefore, the force is reduced to Floop = I2 I 1 µ0 1 1 −ax (B − C) + ax (D − A) 2π b a Since segments BC = DA, we can call this length d: Floop = ax I2 I 1 µ0 d 2π 1 1 − a b Therefore, the loop will be pushed away from the wire in the direction of ax . Note that the magnetic force has caused the wire loop to move. Since work is force × distance, it would be easy to conclude that the magnetic force has performed work.
To study the behavior of timeharmonic plane waves, it is necessary to rederive the wave equation from the timeharmonic form of Maxwell’s x Direction of propagation z y Figure 211 Plane wave propagating in the z direction. 1. Again, assume a sourcefree, linear, homogeneous medium: ∇ × (∇ × E) = −j ωµ(∇ × H ) The formula can be further simplified by using the following vector identity (Appendix A): ∇ × (∇ × E) = ∇(∇ · E) − ∇ 2 E Since we have assumed a sourcefree medium, the charge density is zero (ρ = 0) and Gauss’s law reduces to ∇ · E = 0, yielding ∇ 2 E + j 2 ω2 µεE = ∇ 2 E − ω2 µεE = 0 (238) Substituting γ 2 = ω2 µε yields ∇ 2E − γ 2E = 0 (239) which is the timeharmonic planewave equation for the electric field, where γ is known as the propagation constant.
Advanced signal integrity for highspeed digital designs by Stephen H. Hall
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