By Stephen H. Hall
A synergistic method of sign integrity for high-speed electronic layout
This publication is designed to supply modern readers with an figuring out of the rising high-speed sign integrity matters which are growing roadblocks in electronic layout. Written by way of the key specialists at the topic, it leverages suggestions and strategies from non-related fields corresponding to utilized physics and microwave engineering and applies them to high-speed electronic design—creating the optimum blend among concept and useful functions.
Following an advent to the significance of sign integrity, bankruptcy insurance contains:
- Electromagnetic basics for sign integrity
Transmission line basics
Non-ideal conductor versions, together with floor roughness and frequency-dependent inductance
Frequency-dependent homes of dielectrics
Mathematical necessities of actual channels
S-parameters for electronic engineers
Non-ideal go back paths and through resonance
I/O circuits and versions
Modeling and budgeting of timing jitter and noise
procedure research utilizing reaction floor modeling
each one bankruptcy comprises many figures and various examples to aid readers relate the options to daily layout and concludes with difficulties for readers to check their figuring out of the cloth. complex sign Integrity for High-Speed electronic Designs is acceptable 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 dressmaker.
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Extra resources for Advanced signal integrity for high-speed digital designs
Like poles will repel each other, and unlike poles will attract. Each “electromagnet” has its own north and south B B l dl B (a) (b) Figure 2-15 (a) Magnetic field generated by a loop of current; (b) elemental current loop analogous to an electric charge. 43 MAGNETOSTATICS poles. It is interesting to note that the fundamental source of the magnetic field is the moving charge Q that constitutes the steady-state current. Subsequently, when l1 is moved into the proximity of l0 , the force induced between the two electromagnets is caused by the charge (Q) of l1 moving in the magnetic field of l0 and is described by the Lorenz force law: Fm = Q(ν × B) (2-78a) A charge moving in the presence of both an electric and a magnetic field produces a force calculated as Fm = Q(E + ν × B) (2-78b) The implications of (2-78) are that the force is perpendicular to both the velocity ν of the charge q and the magnetic field B.
The stored energy is potential energy because it depends on the position of the charges within the field. The concept of scalar electric potential , which will now be derived, provides a metric to describe the work or energy required to move charges from one point to another inside an electrostatic field. The discussion above describes how an electric field is produced when two charges are brought into the vicinity of each other. If we assume that one charge (Q) is stationary and the other charge (q) is moved toward the stationary charge from point a to point b, the work can be calculated as force × distance.
This is achieved by expressing the current in terms of an area ratio: 2π 2πrBφ πr 2 Bφ r dφ = =i 2 µ0 µ0 πa 0 iµ0 r Bφ(ra) Bf(r >a) Bf(r >a) Bf(r >a) Bf(r