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All resistors have a little bit of capacitive reactance, just because they occupy physical space So there is no such thing as a mathematically pure resistance, either The points 3 j0 and 0 j4 are idealized Often, 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 XC are reactances, and not the actual capacitances They vary with the frequency in an RC circuit If you raise or lower the frequency, the value of XC will change A higher frequency causes XC to get smaller and smaller negatively (closer to zero) A lower frequency causes XC to get larger and larger negatively (farther from zero, or lower down on the RC plane).

Like all modern technologies, ATM has a well-developed protocol stack, shown in Figure 6-6, which clearly delineates the functional breakdown of the service. The stack consists of four layers: the Upper Services layer, the ATM Adaptation layer (AAL), the ATM layer, and the Physical layer. The Upper Services layer defines the nature of the actual services that ATM can provide. It identifies both constant and variable bit rate (VBR) services. Voice is an example of a constant bit rate service, while signaling, IP, and Frame Relay are examples of both connectionless and connection-oriented VBR services. The AAL has four general responsibilities:

If the frequency goes to zero, then the capacitive reactance drops off the bottom of the plane, out of sight In that case you have two oppositely charged plates or sets of plates, and no action..

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Zpri/Zsec = (Tpri/Tsec)2 = (4.00/1)2 = 4.00 2 = 16.0 We know that the secondary impedance, Zsec is 37.5 . Thus: Zpri = 16.0 Zsec = 16.0 37.5 = 600

If you work much with engineers, or if you plan to become one, you ll get familiar with the RC plane, just as you will with the RL plane. Recall from the last chapter that RL impedances can be represented as vectors. The same is true for RC impedances. In Fig. 14-6, there are four different impedance points. Each one is represented by a certain distance to the right of the origin (0,0), and a certain displacement downwards. The first of these is the resistance, R, and the second is the capacitive reactance, Xc. Therefore, the RC impedance is a two-dimensional quantity. Doesn t this look like a mirror-image reflection of RL impedances You could almost imagine that we re looking at an RL plane reflected in a pool of still water. This is, in fact, an excellent way to envision this situation. The impedance points in the RC plane can be rendered as vectors, just as this can be done 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 impedance value. 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 illustrated in Fig. 14-7.

Synchronization and recovery from errors Error-detection and correction Segmentation and reassembly of the data stream Multiplexing

In radio receivers and transmitters, transformers can be categorized generally by the method of construction used. Some have primary and secondary windings, just like utility and audio units. Others employ transmission-line sections. These are the two most common types of transformer found at radio frequencies.

Capacitance stores energy in the form of an electric field. When a current is driven through a capacitor, it takes a little time before the plates can fully charge to the full potential difference of the source voltage. When an ac voltage source is placed across a capacitor, the voltage in the capacitor lags the current in phase. Another way of saying this is that the current leads the voltage. The phase difference can range from zero, to a small part of a cycle, to a quarter of a cycle (90 degrees).

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.

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