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Basic Concepts of Communication Systems



                                                        Basic Concepts of Communication Systems  5


                       Amplitude




                       0                                                       Time

                              1/f             Period = 1/f         1/f
                      Figure 1.2. Characteristics of a basic sine wave.

                          Amplitude  Wave 1
                                    Wave 1
                      A A 1 1

                       0                Time


                                    Wave 2
                         Amplitude  Wave 2
                      A 2
                      A 2
                       0                Time

                             A
                             A 1 + A 21 + A 2
                      Figure  1.3. Two in-phase
                      waves will add constructively.

                      number of cycles per second that the wave undergoes (i.e., the number of times
                      it oscillates per second), which is expressed in units of hertz (Hz). A hertz refers
                      to a complete cycle of the wave. The period (generally represented by the sym-
                      bol T) is the inverse of the frequency, that is, period   T   1/f. The term phase
                      (designated by the symbol φ) describes the position of the waveform relative to
                      time 0, as illustrated in Fig. 1.3. This is measured in degrees or radians (rad):
                      180°   π rad.
                        If the crests and troughs of two identical waves occur at the same time, they
                      are said to be in phase. Similarly, if two points on a wave are separated by whole
                      measurements of time or of wavelength, they also are said to be in phase. For
                      example, wave 1 and wave 2 in Fig. 1.3 are in phase. Let wave 1 have an ampli-
                      tude A 1 and let wave 2 have an amplitude A 2 . If these two waves are added, the
                      amplitude A of the resulting wave will be the sum: A   A 1   A 2 . This effect is
                      known as constructive interference.
                        Figure 1.4 illustrates some phase shifts of a wave relative to time 0. When two
                      waves differ slightly in their relative positions, they are said to be out of phase.
                      As an illustration, the wave shown in Fig. 1.4c is 180° (π rad) out of phase
                      with the wave shown in Fig. 1.4a. If these two waves are identical and have
                      the same amplitudes, then when they are superimposed, they cancel each
                      other out, which is known as  destructive interference. These concepts are of


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