Signal Integrity: Applied Electromagnetics and Professional by Samuel H. Russ

By Samuel H. Russ

This textbook teaches how one can layout operating platforms at very excessive frequencies. it truly is designed to introduce desktop engineers to the layout of super excessive pace electronic structures. Combining an intuitive, physics-based method of electromagnetics with a spotlight on fixing sensible difficulties, the writer offers techniques which are crucial for desktop and electric engineers at the present time. The e-book emphasizes an intuitive method of electromagnetics, after which makes use of this beginning to teach the reader how either actual phenomena could cause signs to propagate incorrectly; and the way to resolve in general encountered matters. Emphasis is put on actual difficulties that the writer has encountered in his specialist profession, integrating problem-solving thoughts and actual signal-integrity case stories during the presentation. scholars are challenged to contemplate handling advanced layout tasks and imposing profitable engineering and production approaches. every one bankruptcy contains workouts to check thoughts introduced.

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Signal Integrity: Applied Electromagnetics and Professional Practice

This textbook teaches tips to layout operating structures at very excessive frequencies. it truly is designed to introduce laptop engineers to the layout of tremendous excessive pace electronic structures. Combining an intuitive, physics-based method of electromagnetics with a spotlight on fixing real looking difficulties, the writer offers innovations which are crucial for desktop and electric engineers this present day.

Additional resources for Signal Integrity: Applied Electromagnetics and Professional Practice

Example text

So the resistor heats up to 55  C. What happens if the power dissipation goes up? It turns out that the temperature difference between the temperature of the resistor and the temperature of the ambient air is a linear function of power. The constant of linearity depends on the size and shape of the resistor, the packaging around it, and whether or not the air is moving. 5 W, with an ambient of 20  C, the temperature of the resistor might go up to 65  C. In other words, the temperature of the resistor above ambient might go from 30 to 45  C.

Specifically, since Z ¼RÀ 1 þ jωL jωC ð3:5Þ Z is minimized when 1 ¼ jωL jωC ð3:6Þ 1 ω ¼ pffiffiffiffiffiffi LC ð3:7Þ or This point is called the self-resonant frequency or SRF. Since most datasheets only give you the ESR of a capacitor and the SRF, one can calculate the ESL from the other parameters. Solving Eq. 7 for L, we get 34 3 Gates, Packaging, and Boards: Properties and Modeling Fig. 3 Model of a capacitor ESR ESL ¼ 1 1 ¼ 2 Cω Cð2πSRFÞ2 C ESL ð3:8Þ Armed with ESL, ESR, and capacitance C, one can then construct a detailed model of a capacitor (Fig.

So resistivity actually has units of ohms times area per length. It is important to keep the area and the length in the definition because they represent the cross-sectional area and length, respectively, of the resistor. Each material has its own value of resistivity. For example, the resistivity of silver (the most conductive metal) is 1:59 Â 10À8 Ω Á m. Copper, the most commonly used conductive material, weighs in at 1:68 Â 10À8 Ω Á m. So it turns out copper is almost as conductive as silver and much less expensive.

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