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Sampling Theory
   In many applications it is useful to represent a signal in terms
    of sample values taken at appropriately spaced intervals.
   The signal can be reconstructed from the sampled waveform
    by passing it through an ideal low pass filter.
   In order to ensure a faithful reconstruction, the original signal
    must be sampled at an appropriate rate as described in the
    sampling theorem.
     – A real-valued band-limited signal having no spectral
       components above a frequency of B Hz is determined
       uniquely by its values at uniform intervals spaced no
       greater1 than
             
             
                  
                  
              2B 
                         seconds apart.



          EE 541/451 Fall 2006
Sampling Block Diagram
   Consider a band-limited signal f(t) having no spectral
    component above B Hz.
   Let each rectangular sampling pulse have unit amplitudes,
    seconds in width and occurring at interval of T seconds.

               f(t)                    A/D       fs(t)
                                    conversion




                                      T



                                 Sampling
          EE 541/451 Fall 2006
Bandpass sampling theory
   2B sampling rate for signal from 2B to 3B
                                          X(f)



                             -3B -2B -B       B     2B 3B
                                          X(f-fs)



                             -3B -2B -B      B    2B 3B 4B 5B
                                          X(f+fs)



                -5B -4B -3B -2B -B             B    2B 3B
                                          Xs



                 -5B -4B -3B -2B -B            B    2B 3B 4B 5B
          EE 541/451 Fall 2006
Impulse Sampling


        Signal waveform                               Sampled waveform



                                              0
0
                                                  1                      201
    1                                201




                                   Impulse sampler



                       0
                           1                               201

            EE 541/451 Fall 2006
Impulse Sampling
           with increasing sampling time T

        Sampled waveform                       Sampled waveform



0                                      0
    1                            201       1                      201




        Sampled waveform                       Sampled waveform



0                                      0
    1                            201       1                      201




          EE 541/451 Fall 2006
Introduction
Let gδ (t ) denote the ideal sampled signal
                ∞
gδ ( t ) =    ∑ g (nT ) δ (t − nT )
             n = −∞
                         s         s    (3.1)

where Ts : sampling period
          f s = 1 Ts : sampling rate




  EE 541/451 Fall 2006
Math
From Table A6.3 we have
         ∞
g(t ) ∑δ (t − nTs ) ⇔
      n =−∞
                  ∞
         1                           m
G( f ) ∗
         Ts
                 ∑ δ( f −
                 m =−∞               Ts
                                        )
     ∞
=   ∑ f G( f
    m =−∞
             s        − mf s )
                          ∞
    gδ ( t ) ⇔ f s        ∑G ( f
                       m =−∞
                                      − mf s )                  (3.2)

or we may apply Fourier Transform on (3.1) to obtain
                      ∞
    Gδ ( f ) =     ∑ g (nT ) exp( − j 2π nf T )
                  n =−∞
                                 s                        s     (3.3)
                                            ∞
or Gδ ( f ) = f sG ( f ) + f s              ∑G ( f
                                        m =−∞
                                                     − mf s )   (3.5)
                                        m ≠0

If G ( f ) = 0 for f ≥ W and Ts = 1
                                      2W
                 ∞
                      n          jπ n f
    Gδ ( f ) = ∑ g (    ) exp( −        )                       (3.4)
               n =−∞ 2W           W
                   EE 541/451 Fall 2006
Math, cont.
With
1.G ( f ) = 0 for        f ≥W
2. f s = 2W
we find from Equation (3.5) that
          1
G( f ) =    Gδ ( f ) , − W < f < W                    (3.6)
         2W
Substituting (3.4) into (3.6) we may rewrite G ( f ) as
          1        ∞
                        n           jπnf
G( f ) =
         2W
                 ∑ 2W
                n = −∞
                        g( ) exp( −
                                     W
                                         ) , − W < f < W (3.7)

                                        n
g (t ) is uniquely determined by g (        ) for − ∞ < n < ∞
                                       2W
          n 
or  g (     )  contains all information of g (t )
    2W 
       EE 541/451 Fall 2006
Interpolation Formula
                                n 
To reconstruct g (t ) from  g (   )  , we may have
                            2W 
           ∞
g (t ) = ∫ G ( f ) exp( j 2πft )df
          −∞

                1       ∞
                               n         jπ n f
                        ∑ g ( 2W ) exp( − W ) exp( j 2π f t )df
          W
     =∫
          −W   2W      n = −∞
          ∞
               n   1                         n 
     = ∑ g(
                                 W

       n = −∞
                 )
              2W 2W    ∫−W exp  j 2π f (t − 2W )df (3.8)
                                                
          ∞
               n sin( 2π Wt − nπ )
     = ∑ g(      )
       n = −∞ 2W    2π Wt − nπ
          ∞
                n
     = ∑ g(        ) sin c( 2Wt − n ) , - ∞ < t < ∞         (3.9)
       n = −∞  2W
(3.9) is an interpolation formula of g (t )
EE 541/451 Fall 2006
Interpolation

If the sampling is at exactly the Nyquist rate, then
                                       ∞
                                         t − nTs 
               g (t ) = ∑ g (nTs ) sin c
                                         T      
                        n = −∞               s   

        ∞
                          t − nTs 
                                           g (t )
g (t ) = ∑ g (nTs ) sin c
                          T      
         n = −∞               s   




 EE 541/451 Fall 2006
Practical Interpolation

Sinc-function interpolation is theoretically perfect but it
can never be done in practice because it requires samples
from the signal for all time. Therefore real interpolation
must make some compromises. Probably the simplest
realizable interpolation technique is what a DAC does.

                g (t )




   EE 541/451 Fall 2006
Sampling Theorem
Sampling Theorem for strictly band - limited signals
1.a signal which is limited to − W < f < W , can be completely
                    n 
  described by  g (   ) .
                2W 
                                                    n 
2.The signal can be completely recovered from  g (    )
                                                  2W 
  Nyquist rate = 2W
  Nyquist interval = 1
                       2W
When the signal is not band - limited (under sampling)
aliasing occurs .To avoid aliasing, we may limit the
signal bandwidth or have higher sampling rate.

   EE 541/451 Fall 2006
Under Sampling, Aliasing




EE 541/451 Fall 2006
Avoid Aliasing
   Band-limiting signals (by filtering) before sampling.
   Sampling at a rate that is greater than the Nyquist rate.




                            Anti-aliasing      A/D       fs(t)
       f(t)
                               filter       conversion


                                               T

                                            Sampling




              EE 541/451 Fall 2006
Anti-Aliasing




EE 541/451 Fall 2006
Aliasing
   2D example




         EE 541/451 Fall 2006
Example: Aliasing of Sinusoidal Signals

     Frequency of signals = 500 Hz, Sampling frequency = 2000Hz




   EE 541/451 Fall 2006
Example: Aliasing of Sinusoidal Signals

     Frequency of signals = 1100 Hz, Sampling frequency = 2000Hz




   EE 541/451 Fall 2006
Example: Aliasing of Sinusoidal Signals

     Frequency of signals = 1500 Hz, Sampling frequency = 2000Hz




   EE 541/451 Fall 2006
Example: Aliasing of Sinusoidal Signals

     Frequency of signals = 1800 Hz, Sampling frequency = 2000Hz




   EE 541/451 Fall 2006
Example: Aliasing of Sinusoidal Signals

     Frequency of signals = 2200 Hz, Sampling frequency = 2000Hz




   EE 541/451 Fall 2006
Natural sampling
                    (Sampling with rectangular waveform)

                                                                                Figure 6.7

              Signal waveform                                                                                        Sampled waveform



                                                                                                             0
0                                                                                                                1   201   401   601   801   1001   1201   1401   1601   1801   20
    1   201   401   601   801   1001   1201   1401   1601       1801    2001




                                                                         Natural sampler



                                                       0
                                                            1     201     401   601   801   1001 1201 1401 1601 1801 2001


                          EE 541/451 Fall 2006
Bandpass Sampling
         (a) variable sample rate
 (b) maximum sample rate without aliasing
(c) minimum sampling rate without aliasing




EE 541/451 Fall 2006
Bandpass Sampling
   A signal of bandwidth B, occupying the frequency range
    between fL and fL + B, can be uniquely reconstructed from the
    samples if sampled at a rate fS :
    fS >= 2 * (f2-f1)(1+M/N)
    where M=f2/(f2-f1))-N and N = floor(f2/(f2-f1)),
    B= f2-f1, f2=NB+MB.




          EE 541/451 Fall 2006
Bandpass Sampling Theorem




EE 541/451 Fall 2006
PAM, PWM, PPM, PCM




EE 541/451 Fall 2006
Time Division Multiplexing
   Entire spectrum is allocated for a channel (user) for a limited time.
   The user must not transmit until its
                                                        k1   k2    k3       k4    k5   k6
    next turn.
   Used in 2nd generation                             c
                                                                                 Frequency
                                                                                          f




                              t
   Advantages:                Time
     – Only one carrier in the medium at any given time
     – High throughput even for many users
      – Common TX component design, only one power amplifier
      – Flexible allocation of resources (multiple time slots).

                 EE 541/451 Fall 2006
Time Division Multiplexing
   Disadvantages
    – Synchronization
    – Requires terminal to support a much higher data rate than the
      user information rate therefore possible problems with
      intersymbol-interference.


   Application: GSM
           GSM handsets transmit data at a rate of 270
            kbit/s in a 200 kHz channel using GMSK
            modulation.
           Each frequency channel is assigned 8 users, each
            having a basic data rate of around 13 kbit/s


       EE 541/451 Fall 2006

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Sampling

  • 1. Sampling Theory  In many applications it is useful to represent a signal in terms of sample values taken at appropriately spaced intervals.  The signal can be reconstructed from the sampled waveform by passing it through an ideal low pass filter.  In order to ensure a faithful reconstruction, the original signal must be sampled at an appropriate rate as described in the sampling theorem. – A real-valued band-limited signal having no spectral components above a frequency of B Hz is determined uniquely by its values at uniform intervals spaced no greater1 than      2B  seconds apart. EE 541/451 Fall 2006
  • 2. Sampling Block Diagram  Consider a band-limited signal f(t) having no spectral component above B Hz.  Let each rectangular sampling pulse have unit amplitudes, seconds in width and occurring at interval of T seconds. f(t) A/D fs(t) conversion T Sampling EE 541/451 Fall 2006
  • 3. Bandpass sampling theory  2B sampling rate for signal from 2B to 3B X(f) -3B -2B -B B 2B 3B X(f-fs) -3B -2B -B B 2B 3B 4B 5B X(f+fs) -5B -4B -3B -2B -B B 2B 3B Xs -5B -4B -3B -2B -B B 2B 3B 4B 5B EE 541/451 Fall 2006
  • 4. Impulse Sampling Signal waveform Sampled waveform 0 0 1 201 1 201 Impulse sampler 0 1 201 EE 541/451 Fall 2006
  • 5. Impulse Sampling with increasing sampling time T Sampled waveform Sampled waveform 0 0 1 201 1 201 Sampled waveform Sampled waveform 0 0 1 201 1 201 EE 541/451 Fall 2006
  • 6. Introduction Let gδ (t ) denote the ideal sampled signal ∞ gδ ( t ) = ∑ g (nT ) δ (t − nT ) n = −∞ s s (3.1) where Ts : sampling period f s = 1 Ts : sampling rate EE 541/451 Fall 2006
  • 7. Math From Table A6.3 we have ∞ g(t ) ∑δ (t − nTs ) ⇔ n =−∞ ∞ 1 m G( f ) ∗ Ts ∑ δ( f − m =−∞ Ts ) ∞ = ∑ f G( f m =−∞ s − mf s ) ∞ gδ ( t ) ⇔ f s ∑G ( f m =−∞ − mf s ) (3.2) or we may apply Fourier Transform on (3.1) to obtain ∞ Gδ ( f ) = ∑ g (nT ) exp( − j 2π nf T ) n =−∞ s s (3.3) ∞ or Gδ ( f ) = f sG ( f ) + f s ∑G ( f m =−∞ − mf s ) (3.5) m ≠0 If G ( f ) = 0 for f ≥ W and Ts = 1 2W ∞ n jπ n f Gδ ( f ) = ∑ g ( ) exp( − ) (3.4) n =−∞ 2W W EE 541/451 Fall 2006
  • 8. Math, cont. With 1.G ( f ) = 0 for f ≥W 2. f s = 2W we find from Equation (3.5) that 1 G( f ) = Gδ ( f ) , − W < f < W (3.6) 2W Substituting (3.4) into (3.6) we may rewrite G ( f ) as 1 ∞ n jπnf G( f ) = 2W ∑ 2W n = −∞ g( ) exp( − W ) , − W < f < W (3.7) n g (t ) is uniquely determined by g ( ) for − ∞ < n < ∞ 2W  n  or  g ( )  contains all information of g (t )  2W  EE 541/451 Fall 2006
  • 9. Interpolation Formula  n  To reconstruct g (t ) from  g ( )  , we may have  2W  ∞ g (t ) = ∫ G ( f ) exp( j 2πft )df −∞ 1 ∞ n jπ n f ∑ g ( 2W ) exp( − W ) exp( j 2π f t )df W =∫ −W 2W n = −∞ ∞ n 1  n  = ∑ g( W n = −∞ ) 2W 2W ∫−W exp  j 2π f (t − 2W )df (3.8)   ∞ n sin( 2π Wt − nπ ) = ∑ g( ) n = −∞ 2W 2π Wt − nπ ∞ n = ∑ g( ) sin c( 2Wt − n ) , - ∞ < t < ∞ (3.9) n = −∞ 2W (3.9) is an interpolation formula of g (t ) EE 541/451 Fall 2006
  • 10. Interpolation If the sampling is at exactly the Nyquist rate, then ∞  t − nTs  g (t ) = ∑ g (nTs ) sin c  T   n = −∞  s  ∞  t − nTs  g (t ) g (t ) = ∑ g (nTs ) sin c  T   n = −∞  s  EE 541/451 Fall 2006
  • 11. Practical Interpolation Sinc-function interpolation is theoretically perfect but it can never be done in practice because it requires samples from the signal for all time. Therefore real interpolation must make some compromises. Probably the simplest realizable interpolation technique is what a DAC does. g (t ) EE 541/451 Fall 2006
  • 12. Sampling Theorem Sampling Theorem for strictly band - limited signals 1.a signal which is limited to − W < f < W , can be completely  n  described by  g ( ) .  2W   n  2.The signal can be completely recovered from  g ( )  2W  Nyquist rate = 2W Nyquist interval = 1 2W When the signal is not band - limited (under sampling) aliasing occurs .To avoid aliasing, we may limit the signal bandwidth or have higher sampling rate. EE 541/451 Fall 2006
  • 13. Under Sampling, Aliasing EE 541/451 Fall 2006
  • 14. Avoid Aliasing  Band-limiting signals (by filtering) before sampling.  Sampling at a rate that is greater than the Nyquist rate. Anti-aliasing A/D fs(t) f(t) filter conversion T Sampling EE 541/451 Fall 2006
  • 16. Aliasing  2D example EE 541/451 Fall 2006
  • 17. Example: Aliasing of Sinusoidal Signals Frequency of signals = 500 Hz, Sampling frequency = 2000Hz EE 541/451 Fall 2006
  • 18. Example: Aliasing of Sinusoidal Signals Frequency of signals = 1100 Hz, Sampling frequency = 2000Hz EE 541/451 Fall 2006
  • 19. Example: Aliasing of Sinusoidal Signals Frequency of signals = 1500 Hz, Sampling frequency = 2000Hz EE 541/451 Fall 2006
  • 20. Example: Aliasing of Sinusoidal Signals Frequency of signals = 1800 Hz, Sampling frequency = 2000Hz EE 541/451 Fall 2006
  • 21. Example: Aliasing of Sinusoidal Signals Frequency of signals = 2200 Hz, Sampling frequency = 2000Hz EE 541/451 Fall 2006
  • 22. Natural sampling (Sampling with rectangular waveform) Figure 6.7 Signal waveform Sampled waveform 0 0 1 201 401 601 801 1001 1201 1401 1601 1801 20 1 201 401 601 801 1001 1201 1401 1601 1801 2001 Natural sampler 0 1 201 401 601 801 1001 1201 1401 1601 1801 2001 EE 541/451 Fall 2006
  • 23. Bandpass Sampling (a) variable sample rate (b) maximum sample rate without aliasing (c) minimum sampling rate without aliasing EE 541/451 Fall 2006
  • 24. Bandpass Sampling  A signal of bandwidth B, occupying the frequency range between fL and fL + B, can be uniquely reconstructed from the samples if sampled at a rate fS : fS >= 2 * (f2-f1)(1+M/N) where M=f2/(f2-f1))-N and N = floor(f2/(f2-f1)), B= f2-f1, f2=NB+MB. EE 541/451 Fall 2006
  • 25. Bandpass Sampling Theorem EE 541/451 Fall 2006
  • 26. PAM, PWM, PPM, PCM EE 541/451 Fall 2006
  • 27. Time Division Multiplexing  Entire spectrum is allocated for a channel (user) for a limited time.  The user must not transmit until its k1 k2 k3 k4 k5 k6 next turn.  Used in 2nd generation c Frequency f t  Advantages: Time – Only one carrier in the medium at any given time – High throughput even for many users – Common TX component design, only one power amplifier – Flexible allocation of resources (multiple time slots). EE 541/451 Fall 2006
  • 28. Time Division Multiplexing  Disadvantages – Synchronization – Requires terminal to support a much higher data rate than the user information rate therefore possible problems with intersymbol-interference.  Application: GSM  GSM handsets transmit data at a rate of 270 kbit/s in a 200 kHz channel using GMSK modulation.  Each frequency channel is assigned 8 users, each having a basic data rate of around 13 kbit/s EE 541/451 Fall 2006