.net pdf 417

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range of values employed in analog systems Although digital systems are as susceptible to noise impairment as their analog counterparts, the discrete nature of their binary signaling makes it relatively easy to separate the noise from the transmitted signal In digital carrier systems, only three valid signal values are used: one positive, one negative, and zero Anything else is construed to be noise It is therefore a trivial exercise for digital repeaters to discern what is desirable and what is not, thus eliminating the problem of cumulative noise The role of the regenerator, as shown is Figure 3-71, is to receive a weak, noisy digital signal, remove the noise, reconstruct the original signal, and amplify it before transmitting the signal onto the next segment of the transmission facility For this reason, repeaters are also called regenerators, because that is precisely the function they perform.

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It s important to remember that you must use units of volts, amperes, and ohms in order for Ohm s Law to work right. If you use volts, milliamperes, and ohms or kilovolts, microamperes, and megohms you cannot expect to get the right answers. If the initial quantities are given in units other than volts, amperes, and ohms, you must convert to these units, then calculate. After that, you can convert the units back again to whatever you like. For example, if you get 13,500,000 ohms as a calculated resistance, you might prefer to say that it s 13.5 megohms.

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One observation: it is estimated that as much as 60 percent of the cost of building a transmission facility lies in the regenerator sections of the span For this reason, optical networking, discussed a bit later, has various benefits, not the least of which is the capability to reduce the number of regenerators required on long transmission spans In a typical network, these regenerators must be placed approximately every 6,000 feet along a span, which means that a considerable expense is involved when providing regeneration along a long-haul network Digital signals, often called square waves, comprise a rich mixture of signal frequencies Not to bring too much physics into the discussion, we must at least mention the Fourier series, which describes the makeup of a digital signal The Fourier series is a mathematical representation of the behavior of waveforms Among other things, it notes the following fact.

1. 6. 11. 16. b a c d 2. 7. 12. 17. d b a b 3. 8. 13. 18. a c d c 4. 9. 14. 19. b d a a 5. 10. 15. 20. c b c a

The first way to use Ohm s Law is to find current values in dc circuits. In order to find the current, you must know the voltage and the resistance, or be able to deduce them. Refer to the schematic diagram of Fig. 4-7. It consists of a variable dc generator, a voltmeter, some wire, an ammeter, and a calibrated, wide-range potentiometer. Component values have been left out of this diagram, so it s not a wiring diagram. But

If we start with a fundamental signal, such as that shown in Figure 3-72, and mathematically add to it its odd harmonics (a harmonic is defined as a wave with a frequency that is a whole-number multiple of another wave), we see a rather remarkable thing happening The waveform gets steeper on the sides and flatter on top As we add more and more of the odd harmonics (which, after all, are infinite), the wave begins to look like the typical square wave Now, of course, there is no such thing as a true square wave For our purposes, though, we ll accept the fact..

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70 Basic dc circuits values can be assigned for the purpose of creating sample Ohm s Law problems. While calculating the current in the following problems, it is necessary to mentally cover up the meter.

Suppose that the dc generator (Fig. 4-7) produces 10 V, and that the potentiometer is set to a value of 10 . Then what is the current This is easily solved by the formula I E/R. Just plug in the values for E and R; they are both 10, because the units were given in volts and ohms. Then I 10/10 1 A.

1. 6. 11. 16. a c c d 2. 7. 12. 17. b d b b 3. 8. 13. 18. b c d a 4. 9. 14. 19. c d c b 5. 10. 15. 20. d b c c

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