Page 140 - Fundamentals of Communications Systems
P. 140

4.16  Chapter Four

                       the output bandpass signal will have the frequency domain representation of
                                                2
                                        Y c (f ) = √ [δ(f − (f c + f m ) + δ(f + (f c + f m )]  (4.31)
                                                 2
                       The complex envelopes of the input and output signals are
                                   x z (t) = exp[ j 2π f m t] + exp[ j 6π f m t]  y z (t) = 2 exp[ j 2π f m t]  (4.32)
                       consequently it makes sense to have

                                                          2 | f |≤ 2 f m
                                                 H z (f ) =                               (4.33)
                                                          0 elsewhere
                       and H c (f ) = H z (f − f c ) + H (− f − f c ).
                                               ∗
                                               z
                         Equations (4.27) and (4.14) combined with the convolution theorem of the
                       Fourier transform produce an expression for the Fourier transform of y c (t)
                       given as
                                                   1
                             Y c (f ) = X c (f )H c (f ) = √ [X z (f − f c ) + X (− f − f c )][H z (f − f c )
                                                                    ∗
                                                                    z
                                                    2
                                         ∗
                                     + H (− f − f c )]
                                         z
                       Since both X z (f ) and H z (f ) only take nonzero values in [−B T /2, B T /2], the
                       cross terms in this expression will be zero and Y c (f ) is given by
                                    1
                            Y c (f ) = √ [X z (f − f c )H z (f − f c ) + X (− f − f c )H (− f − f c )]  (4.34)
                                                               ∗
                                                                           ∗
                                                                          z
                                                               z
                                     2
                       Since y c (t) will also be a bandpass signal, it will also have a complex baseband
                       representation. A comparison of Eq. (4.34) with Eq. (4.14) demonstrates the
                       Fourier transform of the complex envelope of y c (t), y z (t), is given as
                                                  Y z (f ) = X z (f )H z (f )
                       Linear system theory produces the desired form
                                                 ∞

                                        y z (t) =  x z (τ)h z (t − τ)dτ = x z (t) ∗ h z (t)  (4.35)
                                                −∞
                       EXAMPLE 4.8
                       (Example 4.1 cont.) The input signal and Fourier transform are
                            x z (t) = 2 cos(2π f m t) + j sin(2π f m t)  X z (f ) = 1.5δ(f − f m ) + 0.5δ(f + f m )
                       Assume a bandpass filter with
                                                                  ⎧   f
                                                                  ⎪ j    −f m ≤ f ≤ f m
                                                                     f m
                                                                  ⎪
                                                                  ⎪
                                    2 −2 f m ≤ f ≤ 2 f m          ⎨  j   f m ≤ f ≤ 2 f m
                          H I (f ) =                     H Q (f ) =                       (4.36)
                                    0 elsewhere                   ⎪− j   −2 f m ≤ f ≤−f m
                                                                  ⎪
                                                                  ⎪
                                                                    0    elsewhere
                                                                  ⎩
   135   136   137   138   139   140   141   142   143   144   145