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By Stephen H. Hall

A synergistic method of sign integrity for high-speed electronic layout

This booklet is designed to supply modern readers with an knowing of the rising high-speed sign integrity concerns which are developing roadblocks in electronic layout. Written through the major specialists at the topic, it leverages options and strategies from non-related fields corresponding to utilized physics and microwave engineering and applies them to high-speed electronic design—creating the optimum mixture among conception and sensible functions.

Following an advent to the significance of sign integrity, bankruptcy assurance comprises:

  • Electromagnetic basics for sign integrity
  • Transmission line basics

  • Crosstalk

  • Non-ideal conductor types, together with floor roughness and frequency-dependent inductance

  • Frequency-dependent homes of dielectrics

  • Differential signaling

  • Mathematical specifications of actual channels

  • S-parameters for electronic engineers

  • Non-ideal go back paths and through resonance

  • I/O circuits and versions

  • Equalization

  • Modeling and budgeting of timing jitter and noise

  • process research utilizing reaction floor modeling

every one bankruptcy comprises many figures and various examples to assist readers relate the techniques to daily layout and concludes with difficulties for readers to check their figuring out of the fabric. complex sign Integrity for High-Speed electronic Designs is appropriate as a textbook for graduate-level classes on sign integrity, for courses taught in for pro engineers, and as a reference for the high-speed electronic fashion designer.

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Extra resources for Advanced signal integrity for high-speed digital designs

Example text

However, if the work is not being done by the magnetic field, what is doing the work? The answer is demonstrated in the following example. Example 2-4 Consider a long wire carrying current I1 in the presence of a rigid rectangular loop carrying current I2 , as shown in Figure 2-16. The long wire will generate a magnetic field as calculated in Example 2-2: B1 = I 1 µ0 2πr Calculate the magnetic force. B F F l2 x C F y z b F A D a F1 l1 Figure 2-16 Forces generated on a wire loop in the vicinity of a magnetic field generated from a wire.

Note that the time dependence of the electric field (∂D/∂t) has been eliminated because we are considering only a dc flow. Amp`ere’s law tells us that a steady-state current J will induce a magnetic field H that circulates around the wire. As described in Example 2-2, the direction of the circulation can be determined using the right-hand rule. If the thumb points in the direction of the current flow, the fingers of the right hand will curl around in the direction of the magnetic field. Subsequently, it is easy to imagine the form of the magnetic field from a single loop of current in our electromagnet, as shown in Figure 2-15a.

4 Propagation of Time-Harmonic Plane Waves As will be demonstrated in subsequent chapters, the propagation of time-harmonic plane waves is of particular importance for the study of transmission-line or other guided-wave structures. 3. A plane wave is defined so that propagation occurs in only one direction (z) and the fields do not vary with time in the x- and y-directions. If the fields were observed at an instant in time, they would be constant in the x –y plane for any given point z and would change for different values of z or t.

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