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Again, it s important, for completeness, to write the 0 and not just the j 4 The points for 3 j 0 and 0 j 4, and two others, are plotted on the RC plane in Fig 14-6 In practical circuits, all capacitors have some leakage resistance If the frequency goes to zero (pure dc), a tiny current always flows, because no capacitor has a perfect insulator between its plates In addition to this, all resistors have a little capacitive reactance because they occupy a finite physical space So there is no such thing as a mathematically perfect resistor, either The points 3 j0 and.

A circuit must be designed to have fo 9.00 MHz. You have a 33-pF fixed capacitor available. What size coil will be needed to get the desired resonant frequency Use the formula fo 0.159/(LC)1/2, and plug in the values. Convert the capacitance to microfarads: 33 pF 0.000033 F. Then just manipulate the numbers, using familiar rules of arithmetic, until the value of L is ferreted out : 9.00 0.159/(L 0.000033)1/2 9.002 0.1592/(0.000033 L) 81.0 0.0253/(0.000033 L) 81.0 0.000033 L 0.0253 0.00267 L 0.0253 L 0.0253/0.00267 9.48 H

Downloaded from Digital Engineering Library @ McGraw-Hill (www.digitalengineeringlibrary.com) Copyright 2004 The McGraw-Hill Companies. All rights reserved. Any use is subject to the Terms of Use as given at the website.

capacitive reactance (XC ) and resistance (R ). This is also known as the RC quarter-plane, or simply as the RC plane.

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Resonant devices 321 In practical circuits, variable inductors and/or variable capacitors are often placed in tuned circuits, so that small errors in the frequency can be compensated for. The most common approach is to design the circuit for a frequency slightly higher than fo, and to use a padder capacitor in parallel with the main capacitor (Fig. 17-13).

The 802.11 MAC layer, like CSMA/CD and token passing, presents the rules used to access the wireless medium. The primary services provided by the MAC layer are as follows:

0 j4 represent an ideal resistor and an ideal capacitor, respectively components that can be worked with in theory, but that you will never see in the real world. Sometimes, resistance and capacitive reactance are both placed in a circuit deliberately. Then you get impedances such as 2 j3 and 5 j5, both shown in Fig. 14-6. Remember that the values for X C are reactances, not the actual capacitances. If you raise or lower the frequency, the value of X C will change. A higher frequency causes X C to get smaller negatively (closer to zero). A lower frequency causes X C to get larger negatively (farther from zero, or lower down on the RC plane). If the frequency goes to zero, then the capacitive reactance drops off the bottom of the RC plane to negative infinity!

17-13 Padding capacitors (Cp) allow adjustment of resonant frequency in a series LC circuit (A) or a parallel LC circuit (B).

Recall from the last chapter that RL impedances can be represented as vectors. The same is true for RC impedances. In Fig. 14-6, four different complex impedance points are shown. Each point is represented by a certain distance to the right of the origin (0,j 0), and a certain displacement downward. The first of these is the resistance, R, and the second is the capacitive reactance, X C. The complex RC impedance is a two-dimensional quantity. Impedance points in the RC plane can be rendered as vectors, just as they can in the RL plane. Then the points become rays, each with a certain length and direction. The magnitude and direction for a vector, and the coordinates for the point, both uniquely define the same complex impedance. The length of the vector is the distance of the point from the origin, and the direction is the angle measured clockwise from the resistance (R ) line, and specified in negative degrees. The equivalent vectors, for the points in Fig. 14-6, are shown in Fig. 14-7.

While resonant circuits often consist of coils and capacitors in series or parallel, there are other kinds of hardware that exhibit resonance. Some of these are as follows.

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