Unit-IV-Pulse modulation & Digital
Modulation
   Staff: Dr. R.Kalidoss
                      Objective
1. To introduce the concepts of pulse modulation
2. To introduce and understand sampling theorems
3. To discuss about different types of pulse modulation
   techniques
              Pulse Modulation
• The process of changing the characteristics of
  pulse carrier in accordance with the modulating
  signal is called pulse modulation.
• The major points of difference between analog
  modulation and pulse modulation are; in analog
  modulation technique simple or complex
  sinusoidal signal is considered as a carrier
  signal, whereas in pulse modulation, carrier
  signals are periodic rectangular trains of pulse
  signals.
• Fig Carrier signal format in pulse modulation
         Types of Pulse modulation
• The various types of analog pulse modulation techniques
  based on these characteristics are:
      1. Pulse amplitude modulation (PAM)
      2. Pulse width modulation (PWM)
      3. Pulse position modulation (PPM)
• Types of Digital Pulse modulation:
      1. Pulse code modulation (PCM)
      2. Delta modulation
      3. Adaptive delta modulation
   Pulse amplitude modulation (PAM)
• The process of changing the amplitude of the pulse
  carrier signal in accordance with the modulating signal is
  called “Pulse Amplitude Modulation” (PAM) which is also
  referred to as "sampling process".
                 Fig: Model of a sampler
 Generation of PAM signals / Sampling
               operation
• PAM signals can be generated using electronic switches.
  The inputs for the electronic switches are continuous
  time modulating signal and train of periodic pulses.
  When the switch is closed, the corresponding instant
  message signals are arrived at the output side. The
  output is zero when the switch is open. Continuous time
  signals are converted into discrete-time signal due to this
  process. The output signals are sampled signals.
              Sampling operation
Input or
                                            x (t)
message signal = x (t)
                                                                 t
                          g(t)
Carrier signal = g(t)
                                                                 t
                           0     T 2T 3T 4T 5T 6T 7T 8T 9T
                                           xs (t)
Sampled signal = xs (t)
                                                             t
                        Mathematical representation
  Let x(t) be the modulating signal (continuous)
     g(t) be the carrier (pulse) signal and xs (t ) sampled signal.
  Now g(t) are periodic train of pulses. Any periodic signal can represent
    by Fourier series. Hence Fourier series representation of carrier
    signal g(t) is given by
          ∞
  ()
g t = ∑ Cn e          j 2πnf s t
                                                  (1)
       n = −∞
 where Cn is a n th Fourier coefficients and it can be expressed as,
                   fs
                   2
     Cn =
          1
                ∫ g (t )e − j 2πnf s t
                                                 (2)
          T        fs
               −
                   2
  The output of a electronic switch or sampler circuit is given as
     x s (t ) = x(t )g (t )                      (3)
  This expression describes the sampling operation in time domain.
  • The sampled signal in frequency domain can also be
    expressed by finding the Fourier transform of a signal xs (t )
     x(t ) →
            FT
               x( f )
          ∞
  ( )
 x f– = ∫x t e     ()
                  − j 2πft
                           dt            (4)
          −∞
  The frequency  domain signal of sampled signal can be
    obtained in a similar manner.
    x s (t ) →
              FT
                 xs ( f )
             ∞
   ( )
xs f = ∫ xs t e       ()
                       − j 2πf t
                                 dt               (5)
  Sub (3) in−(5),
              ∞ we get
             ∞
xs ( f ) =         (t )g (t )e   − j 2πf t
              ∫x                             dt   (6)
             −∞
  Sub value of g(t) from eq. (1) to eq. (6)
    ∞               ∞
=    ∫ x   (t )     ∑ Cn e
                           j 2πnf s t − j 2πf t
                                     e          dt
    −∞           n = −∞
                    ∞          ∞
             =    ∑ C ∫ x(t )e
                  n = −∞
                           n
                                         − j 2π ( f − nf s )
                                                           dt
                               −∞
From the definition of Fourier transform,
              ∞
              ∫ x (t )e − j 2π ( f − nf s )
                                            dt = X ( f − nf s )
             −∞
                                    ∞
                 xs ( f ) =     ∑ C X ( f − nf )
                                         n                     s
                                n = −∞                             (7)
Eq. (7) can be represented pictorially, as shown in figure. It shows
  sampling in time domain introducing periodicity in the frequency
  domain. i.e. the same band limited spectrum repeated for every
  sample interval.
• The conclusion drawn from the figure are:
1. Band limited signal x(t ) can be perfectly recovered at the
   receiver side only when the sampling frequency is
   fs ≥ 2 fh .
2. When sampling frequency does not satisfy the above
   condition, recovery of the original signal at the receiver
   side is not possible. Also the signals are also affected by
   adjacent samples. This effect is referred to as "Aliasing
   effect". Hence the condition for Aliasing : f s ≤ 2 f h .
In other words, for perfect reconstruction 1
                                                of sampling
    interval (Ts ), is always higher than 2T . i.e. rate of closer of
    electronic switch at the transmitter side must satisfy the
    condition of Nyquist interval.
  Sampling Theorem or Nyquist Criterion for
            sampling operation
A band limited signal x(t ) which has no frequency
  components above f h , can be completely specified by
  samples at a rate greater than or equal to 2 f h .
i.e.   fs ≥ 2 fh                      (8)
Perfect recovery of the signal is not possible at the receiver
  side, when the sampling interval at the transmitter side is
  not followed.
              Detection of PAM signal
• Just passing the spectrum of x s ( f ) to low pass filter may be done
  for reconstructing the signal. Low pass filter allows the spectrum
  from the band − f h to + f h and suppresses all other side bands.
  Fig. illustrates the detection circuit of PAM signal.
                Fig: Detection of PAM signal