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09_200256_CH09/Bergren   4/17/03  11:24 AM  Page 234
                             234 CHAPTER NINE
                                 Frequency Shift Keying (FSK) sets
                                                 M1n2     A     sin 1vn     t     u2
                                 where A is the fixed amplitude, vn is one of n different frequencies, and u is the
                                 fixed phase. In the simplest form, n   2, and the waveform M looks like a sine
                                 wave that slows down in frequency whenever the data is zero (v   freq0 or freq1).
                                 Phase Shift Keying (PSK) sets

                                                 M1n2     A     sin 1v     t     un2


                                 where A is the fixed amplitude, v is the fixed frequency, and un is one of n dif-
                                 ferent phases. In the simplest form, n equals 2, and the waveform M looks like a
                                 sine wave that inverts vertically whenever the data is zero (u   0 or 180 degrees).

                               Each modulation method has a corresponding demodulation method. Each modula-
                             tion method also has a mathematical structure that shows the probability of making
                             errors given a specific S/N ratio. We won’t go into the math here since it involves both
                             calculus and probability functions with Gaussian distributions. For further reading on
                             this, please see the following web site and PDF file:
                                 www.sss-mag.com/ebn0.html
                                 www.elec.mq.edu.au/ cl/files_pdf/elec321/lect_ber.pdf
                               What comes out of the calculations are called Eb/No curves (pronounced “ebb no”).
                             They look like the following figure, which shows a bit error rate (BER) versus an
                             Eb/No curve for a specific modulation scheme (see Figure 9-5).
                               Remember, Eb/No is the ratio of the energy in a single bit to the energy density of
                             the noise. A few observations about this graph:
                                 The better the S/N ratio (the higher the Eb/No), the lower the error rate (BER). It
                                 stands to reason that a better signal will work more effectively in the channel.
                                 The Shannon limit is shown as a box. The top of the box is formed at a BER of
                                 0.50. Even a monkey can get a data bit right half the time! The vertical edge of the
                                 box is at an Eb/No of 0.69, the lower limit of the digital transmission we derived
                                 earlier. No meaningful transmission can take place with an Eb/No that low; the
                                 channel capacity falls to zero.
                                 This graph shows the BER we can expect in the face of various Eb/No values in
                                 the channel. Adjustments can be made. If the channel has a fixed No value that
                                 cannot be altered, an engineer can only try to increase Eb, perhaps by increasing
                                 the signal power pumped into the channel.
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