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                   The Wireless Channel (2)

                           Wireless Communication
Review
   What we discussed last lecture:
       The large-scale fading because of path loss
       The empirical path loss formulas
   Today, we will discuss about the small-scale fading
    and the statistical models represent it
Introduction
   The small-scale fading is usually called “fading”
   It is caused by multipath signal, so it is also called
    “multipath fading”
   Multipath signal causes constructive and destructive
    addition of the received signal
Introduction
   If a single pulse is transmitted in the multipath
    channel, it will yield a train of pulses with delay time


                               LOS
                                     Reflected components


   Delay spreadTd ): the time delay between the
                     (
    arrival of the first received signal component and the
    last received signal component associated with a
    single transmitted pulse
Introduction
   If the delay spread is small compared to the (1/BW),
    then there is little time spreading in the received
    signal
   If the delay spread is relatively large, there is little
    time spreading of the received signal, i.e. signal
    distortion
   Multipath channel is also time-varying that means
    either the transmitter or the receiver is moving
   It also causes the location of the reflectors will
    change over time
   We will limit the model to be narrowband fading, i.e.
    the BW is small compared to (1/delay spread)
Introduction
   Physical factors influencing fading:
       Multipath propagation
       Speed of the mobile
       Speed of surrounding objects
       The transmision bandwidth of the signal
Review of Doppler Shift
   The received signal may experience Doppler shift
                                                   v eff




   If the receiver is moving towards the transmitter, the
    Doppler freq is positive, otherwise it is negative
Example
   Consider a transmitter which radiates a carrier of
    1850 MHz. For a vehicle moving 26.82 mps,
    compute the received carrier frequency if the mobile
    is moving:
       Directly towards the transmitter
       Directly away from the transmitter
       In a direction which is perpendicular to the direction of
        arrival of the transmitted signal
Solution
   Carrier freq = 1850 MHz
                           3           8

   Wavelength =  fc  18501010  0.162m
                                           6
                            c

   Vehicle speed = 26.82 m/s
   Vehicle moving towards the transmitter means
    positive Doppler frequency
                                        26.82
               f  f c  f d  1850          cos 0  1850.00016MHz
                                        0.162
   Vehicle moving towards the transmitter means
    negative Doppler frequency
                                    26.82
              f  f c  f d  1850       cos 0  1849.999834MHz
                                    0.162
   Vehicle   is moving perpendicular means90         
                                       26.82
                f  f c  f d  1850        cos90  1850MHz
                                       0.162
Doppler Spread
   Doppler spread is given by
                     Ds : D2  D1
                fv                fv
 Where, D1          and D2  
                c                 c

   E.g. If the mobile is moving at 60 kph and f = 900
    MHz, the the Doppler spread is
                         fv   fv      fv
                   Ds         2
                         c   c        c
                          900 106 16.67
                      2                   100 Hz
                               3 108
Time-Varying Channel Impulse Response
   We have already known that the transmitted signal is
       s  t   u  t  e j 2 f t   u  t  cos  2 fct   u  t  sin  2 f ct 
                                 c




   Then, the received signal in multipath channel is



    n = 0 corresponds to the LOS path
    N(t) is the number of resolvable multipath
    components
                     is corresponding delay
           is Doppler phase shift
           is amplitude
Time-Varying Channel Impulse Response
   The n-th resolvable multipath component may
    correspond to the multipath associated with a single
    reflector or multiple reflectors clustered together
Time-Varying Channel Impulse Response
   If single reflector exists, the amplitude is based on
    the path loss and shadowing, its phase change
            n t  with  f  t 
    associated e j 2delay
                        c n
                                                and Doppler
    phaseshiftt of
    D   2 f D  dt
      N       N
          t


          1      2                     1  2  Bu1
    If reflector cluster exists, two multipath components
    with delay and            are resolvable if
   If t criteriat isnot satisfied, then it is nonresolvable
     u the 1   u   2 
    since
                                                    1   2
   The nonresolvable components are combined into a
    single multipath component with delay                      and
    an amplitude and phase corresponding to the sum of
    different components
Time-Varying Channel Impulse Response
   The amplitude of the summed signal will undergo
    fast variations due to the constructive and
    destructive combining of the nonresolvable multipath
    components
   Wideband channels have resolvable multipath
    components  the parameters change slowly
   Narrowband channels tend to have nonresolvable
    multipath components  the parameters change
    quickly
Time-Varying Channel Impulse Response
   We can simplifyr t  by letting
                   n t   2 fc n t   D
                                              n


   The received signal is then



   The received signal is obtained by convolving the
    baseband input signal with equivalent lowpass time-
    varying channel impulse response of the channel,
    and then upconverting the carrier frequency
Time-Varying Channel Impulse Response
   The c  , t  represents the equivalent lowpass
                                                t 
    response of the channel at time t to an impulse at
    time
Parameters of Mobile Multipath Channels
   Time dispersion parameters
   Coherence bandwidth
   Doppler spread and coherence time
Time Dispersion Parameters
   The time dispersive properties of wideband multipath
    channels are most commonly quantified by their
    mean excess delay and rms delay spread
   The mean excess delay:
                     a            2
                                    k k         P             k       k
                      k
                                                 k

                     a     k
                                     2
                                     k          P  
                                                      k
                                                                       k



   The rms delay spread is the square root of the
    second central moment of the power delay profile
                                                          
                                                               2
                                        2



                         a         2 2
                                     k k         P                k
                                                                               2
                                                                               k
                  2       k
                                                     k

                         a     k
                                         2
                                         k       P    k
                                                                           k
Time Dispersion Parameters
   The delays are measured relative to the first
                                    0
    detectable signal arriving at the receiver at
   The maximum excess delay (X dB) of the power
    delay profile is defined to be the time delay during
    which multipath energy falls to X dB below the
    maximum.
                                           X 0
    The maximum excess delay sometimescalled
    excessdelay spread, which can be expressed as
            X

    Where is the maximum delay at which a multipath
                        
    component is within0 X dB of the strongest arriving
    multipath signal and is the first arriving signal
Time Dispersion Parameters
Coherence Bandwidth
   Coherence bandwidth is a statistical measure of the
    range of frequencies over which the channel can be
    considered “flat”
   Flat fading is a channel which passes all spectral
    components with approximately equal gain and
    linear phase
   The coherence bandwidth can be expressed as
                            1   (above 90% correlation)
                       Bc 
                         50 

                              1
                      Bc           (above 50% correlation)
                             5 
Example
   Compute the mean excess delay, rms delay spread,
    and the maximum excess delay for the following
    power delay profile
   Estimate the 50% coherence bandwidth of the
    channel
Solution
   Using the definition of maximum excess delay (10
                     10 dB 4 s
    dB), it can be seenthat
   The mean excess delay:
             
                  1 5   0.11   0.1 2    0.01 0   4.38 s
                               0.01  0.1  0.1  1

   The second moment
                 1 5   0.11   0.1 2    0.01 0 
                         2               2               2            2

            2                                                            21.07  s 2
                               0.01  0.1  0.1  1
   The rms delay spread:
                            21.07   4.38   1.37  s
                                                             2



   The coherence bandwidth:
                                     1                1
                             Bc                               146kHz
                                    5          5 1.37  s 
Doppler Spread and Coherence Time
   Doppler spread has been discussed before
   The coherence time is related with Doppler spread
    (Doppler shift)
                          0.423
                     Tc 
                             v
Types of Small-Scale Fading
Flat Fading
   If the mobile radio channel has a constant gain and
    linear phase response over a bandwidth which is
    greater than the bandwidth of the transmitted
    signal, then the received signal will undergo flat
    fading
Flat Fading
   Flat fading channels are also known as amplitude
    varying channels
   It is also sometimes referred to as narrowband
    channels
   The most common amplitude distributions are:
    Rayleigh, Rician, and Nakagami
   Summarize: a signal undergoes flat fading if
                        B  B
                        s     c


                       Ts   
Frequency Selective Fading
   If the channel has a constant-gain and linear phase
    response over a bandwidth that is smaller than the
    bandwidth of transmitted signal, then the channel
    creates frequency selective fading on the received
    signal
Frequency Selective Fading
   The received signal includes multiple versions of the
    transmited waveform which are attenuated and
    delayed in time, and hence the received signal is
    distorted
   Frequency selective fading is due to time dispersion
    of the transmitted symbols within the channel
   Thus, the channel induces intersymbol interference
    (ISI)
   The modeling for this kind of channel is more difficult
    since each multipath signal must be modeled and
    channel must be considered to be a linear filter
   The common model: 2-ray Rayleigh fading
Frequency Selective Fading
   It is sometimes called wideband channels since the
    bandwidth of the signal is wider than the bandwidth
    of the channel impulse response
   Summarize: a signal undergoes frequency selective
    fading if
                         Bs  Bc

                         Ts   
Fast Fading
   In a fast fading channel, the channel impulse
    response changes rapidly within the symbol duration
   In other words, the coherence time of the channel is
    smaller than the symbol period of the transmitted
    signal
   This causes frequency dispersion (time selective
    fading) due to Doppler spread, which lead to signal
    distortion
   Signal distortion due to fast fading increases with
    increasing Doppler spread relative to the bandwidth
    of the transmitted T  T
                       signal
                        s    c
   Summarize: a signal undergoes fast fading if
                      Bs  BD
Slow Fading
   In a slow fading channel, the channel impulse
    response changes at a rate much slower than the
    transmitted signal
   The channel may be assumed to be static over one
    or several reciprocal bandwidth interval
   The Doppler spread of the channel is much less than
    the bandwidth of the baseband signal
   Summarize: a signal undergoes slow fading if
                       Ts  Tc

                        Bs  BD
Summary
Remarks
   When a channel is specified as a fast or slow fading
    channel, it does not specify whether the channel is flat
    fading or frequency selective
   Fast fading only deals with the rate of change of the
    channel due to motion
   In flat fading channel, we can approximate the impulse
    response to be simply delta function
   A flat fading, fast fading channel is a channel in which the
    amplitude of the delta function varies faster that the rate
    of the transmitted baseband signal
   A frequency selective, fast fading channel, the
    amplitudes, phases, and time delays of any one of the
    multipath components vary faster than the rate of change
    of the transmitted signal
Rayleigh Fading
   The Rayleigh distribution is commonly used to
    describe the statistical time varying nature of the
    received envelope of a flat fading signal
   Rayleigh distributed signal:
Rayleigh Fading
   The Rayleigh distribution has pdf



            the rms value of the received voltage signal before envelope detection
          2  the time-average power of the received signal before envelope detection

   The probability that the envelope of the received
    signal does not exceed a specified value R is
Rayleigh Fading
   The mean value of Rayleigh distribution is



   The variance of the Rayleigh distribution (represent
    the ac power)



   The median value is

   The median is often used in practice
Rayleigh Fading
   The corresponding Rayleigh pdf is
Level Crossing and Fading Statistics
   The level crossing rate (LCR) is defined as the
    expected rate at which the Rayleigh fading
    envelope, normalized to the local rms signal
    level, crosses a specified level in a positive-going
    direction
   The number of level crossing per second is given by
                        
                  N R   rp  R, r  dr  2 f D  e 
                                                           2
                                  
                        0


   Where     
              r
              p  is r 
                     time derivative of r(t) (the slope)
                  R,                                          
                                                               r
                      is the joint density function of r and
              atrR=RR
                    rms
Example
   For a Rayleigh fading signal, compute the positive-
    going level crossing   1 for
                         rate          when the maximum
    Doppler frequency is 20 Hz
   What is the maximum velocity of the mobile for this
    Doppler frequency if the carrier frequency is 900
    MHz?
Solution
   Use the equation for LCR
                NR  2  201 e1  18.44

   Use equation of Doppler frequency
               v  f D  20 1 3  6.66m / s
Level Crossing and Fading Statistics
   The average fade duration is defined as the average
    period of time for which the received signal is below
    a specified level R.
   For a Rayleigh fading signal, it is given by
                                     1
                                      Pr  r  R 
                                     NR

                                     1
                    Pr  r  R        i
                                     T i
                                     R

                                                        
                                  p  r  dr  1  exp   2   
                                     0

   So, the average fade duration can be expressed as
                                           2
                                          e 1
                               
                                          f D 2
Example
                                                  
    Find the average fade duration for threshold levels0.01
    when the Doppler frequency is 200 Hz

Solution
 Average fade duration is
                           0.012
                           e    1
                                    19.9 s
                       0.01 200 2
Rician Fading Distribution
   When there is a dominant stationary (nonfading)
    signal component present, such as line-of-sight
    propagation path, the small-scale fading envelope
    distribution is Rician
   Random multipath componnets arriving at different
    angles are superimposed on a stationary dominant
    signal                    2
                                r  A 
                                      2

                           r             Ar  by
    The Rician distribution isI 0given for  A  0, r  0 
                 p r   2 e 2
                                  2

                                          2
                                          
                      0 for  r  0 
Rician Fading Distribution
   The Rician distribution is described in terms of a
    parameter K
                               A2
                           K
                              2 2
                                        A2
                      K  dB   10 log 2
                                       2

   As K  0 we have Rayleigh fading
   As K   we have no fading, channel has no
    multipath, only LOS component
Rician Fading Distribution
   The Rician pdf is
Conclusions
   Small-scale fading is variation of signal strength over
    distances of the order of the carrier wavelength
   It is due to constructive and destructive interference
    of multipath
   Key parameters:
                Doppler spread  coherence time
                Delay spread  coherence bandwidth
   Statistical small-scale fading: Rayleigh fading and
    Rician fading  flat fading

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3. the-wireless-channel-2

  • 1. www.ee.ui.ac.id/wasp The Wireless Channel (2) Wireless Communication
  • 2. Review  What we discussed last lecture:  The large-scale fading because of path loss  The empirical path loss formulas  Today, we will discuss about the small-scale fading and the statistical models represent it
  • 3. Introduction  The small-scale fading is usually called “fading”  It is caused by multipath signal, so it is also called “multipath fading”  Multipath signal causes constructive and destructive addition of the received signal
  • 4. Introduction  If a single pulse is transmitted in the multipath channel, it will yield a train of pulses with delay time LOS Reflected components  Delay spreadTd ): the time delay between the ( arrival of the first received signal component and the last received signal component associated with a single transmitted pulse
  • 5. Introduction  If the delay spread is small compared to the (1/BW), then there is little time spreading in the received signal  If the delay spread is relatively large, there is little time spreading of the received signal, i.e. signal distortion  Multipath channel is also time-varying that means either the transmitter or the receiver is moving  It also causes the location of the reflectors will change over time  We will limit the model to be narrowband fading, i.e. the BW is small compared to (1/delay spread)
  • 6. Introduction  Physical factors influencing fading:  Multipath propagation  Speed of the mobile  Speed of surrounding objects  The transmision bandwidth of the signal
  • 7. Review of Doppler Shift  The received signal may experience Doppler shift v eff  If the receiver is moving towards the transmitter, the Doppler freq is positive, otherwise it is negative
  • 8. Example  Consider a transmitter which radiates a carrier of 1850 MHz. For a vehicle moving 26.82 mps, compute the received carrier frequency if the mobile is moving:  Directly towards the transmitter  Directly away from the transmitter  In a direction which is perpendicular to the direction of arrival of the transmitted signal
  • 9. Solution  Carrier freq = 1850 MHz 3 8  Wavelength =  fc  18501010  0.162m  6 c  Vehicle speed = 26.82 m/s  Vehicle moving towards the transmitter means positive Doppler frequency 26.82 f  f c  f d  1850  cos 0  1850.00016MHz 0.162  Vehicle moving towards the transmitter means negative Doppler frequency 26.82 f  f c  f d  1850  cos 0  1849.999834MHz 0.162  Vehicle is moving perpendicular means90  26.82 f  f c  f d  1850  cos90  1850MHz 0.162
  • 10. Doppler Spread  Doppler spread is given by Ds : D2  D1 fv fv  Where, D1   and D2   c c  E.g. If the mobile is moving at 60 kph and f = 900 MHz, the the Doppler spread is  fv   fv  fv Ds         2  c   c  c 900 106 16.67 2  100 Hz 3 108
  • 11. Time-Varying Channel Impulse Response  We have already known that the transmitted signal is s  t   u  t  e j 2 f t   u  t  cos  2 fct   u  t  sin  2 f ct  c  Then, the received signal in multipath channel is n = 0 corresponds to the LOS path N(t) is the number of resolvable multipath components is corresponding delay is Doppler phase shift is amplitude
  • 12. Time-Varying Channel Impulse Response  The n-th resolvable multipath component may correspond to the multipath associated with a single reflector or multiple reflectors clustered together
  • 13. Time-Varying Channel Impulse Response  If single reflector exists, the amplitude is based on the path loss and shadowing, its phase change  n t  with  f  t  associated e j 2delay c n and Doppler phaseshiftt of D   2 f D  dt N N t  1 2 1  2  Bu1 If reflector cluster exists, two multipath components with delay and are resolvable if  If t criteriat isnot satisfied, then it is nonresolvable u the 1   u   2  since   1   2  The nonresolvable components are combined into a single multipath component with delay and an amplitude and phase corresponding to the sum of different components
  • 14. Time-Varying Channel Impulse Response  The amplitude of the summed signal will undergo fast variations due to the constructive and destructive combining of the nonresolvable multipath components  Wideband channels have resolvable multipath components  the parameters change slowly  Narrowband channels tend to have nonresolvable multipath components  the parameters change quickly
  • 15. Time-Varying Channel Impulse Response  We can simplifyr t  by letting n t   2 fc n t   D n  The received signal is then  The received signal is obtained by convolving the baseband input signal with equivalent lowpass time- varying channel impulse response of the channel, and then upconverting the carrier frequency
  • 16. Time-Varying Channel Impulse Response  The c  , t  represents the equivalent lowpass t  response of the channel at time t to an impulse at time
  • 17. Parameters of Mobile Multipath Channels  Time dispersion parameters  Coherence bandwidth  Doppler spread and coherence time
  • 18. Time Dispersion Parameters  The time dispersive properties of wideband multipath channels are most commonly quantified by their mean excess delay and rms delay spread  The mean excess delay: a  2 k k  P   k k  k  k a k 2 k  P   k k  The rms delay spread is the square root of the second central moment of the power delay profile  2      2 a  2 2 k k  P   k 2 k 2  k  k a k 2 k  P   k k
  • 19. Time Dispersion Parameters  The delays are measured relative to the first  0 detectable signal arriving at the receiver at  The maximum excess delay (X dB) of the power delay profile is defined to be the time delay during which multipath energy falls to X dB below the maximum.   X 0 The maximum excess delay sometimescalled excessdelay spread, which can be expressed as X Where is the maximum delay at which a multipath  component is within0 X dB of the strongest arriving multipath signal and is the first arriving signal
  • 21. Coherence Bandwidth  Coherence bandwidth is a statistical measure of the range of frequencies over which the channel can be considered “flat”  Flat fading is a channel which passes all spectral components with approximately equal gain and linear phase  The coherence bandwidth can be expressed as 1 (above 90% correlation) Bc  50  1 Bc  (above 50% correlation) 5 
  • 22. Example  Compute the mean excess delay, rms delay spread, and the maximum excess delay for the following power delay profile  Estimate the 50% coherence bandwidth of the channel
  • 23. Solution  Using the definition of maximum excess delay (10  10 dB 4 s dB), it can be seenthat  The mean excess delay:  1 5   0.11   0.1 2    0.01 0   4.38 s  0.01  0.1  0.1  1  The second moment 1 5   0.11   0.1 2    0.01 0  2 2 2 2 2   21.07  s 2  0.01  0.1  0.1  1  The rms delay spread:    21.07   4.38   1.37  s 2  The coherence bandwidth: 1 1 Bc    146kHz 5  5 1.37  s 
  • 24. Doppler Spread and Coherence Time  Doppler spread has been discussed before  The coherence time is related with Doppler spread (Doppler shift) 0.423 Tc  v
  • 26. Flat Fading  If the mobile radio channel has a constant gain and linear phase response over a bandwidth which is greater than the bandwidth of the transmitted signal, then the received signal will undergo flat fading
  • 27. Flat Fading  Flat fading channels are also known as amplitude varying channels  It is also sometimes referred to as narrowband channels  The most common amplitude distributions are: Rayleigh, Rician, and Nakagami  Summarize: a signal undergoes flat fading if B  B s c Ts   
  • 28. Frequency Selective Fading  If the channel has a constant-gain and linear phase response over a bandwidth that is smaller than the bandwidth of transmitted signal, then the channel creates frequency selective fading on the received signal
  • 29. Frequency Selective Fading  The received signal includes multiple versions of the transmited waveform which are attenuated and delayed in time, and hence the received signal is distorted  Frequency selective fading is due to time dispersion of the transmitted symbols within the channel  Thus, the channel induces intersymbol interference (ISI)  The modeling for this kind of channel is more difficult since each multipath signal must be modeled and channel must be considered to be a linear filter  The common model: 2-ray Rayleigh fading
  • 30. Frequency Selective Fading  It is sometimes called wideband channels since the bandwidth of the signal is wider than the bandwidth of the channel impulse response  Summarize: a signal undergoes frequency selective fading if Bs  Bc Ts   
  • 31. Fast Fading  In a fast fading channel, the channel impulse response changes rapidly within the symbol duration  In other words, the coherence time of the channel is smaller than the symbol period of the transmitted signal  This causes frequency dispersion (time selective fading) due to Doppler spread, which lead to signal distortion  Signal distortion due to fast fading increases with increasing Doppler spread relative to the bandwidth of the transmitted T  T signal s c  Summarize: a signal undergoes fast fading if Bs  BD
  • 32. Slow Fading  In a slow fading channel, the channel impulse response changes at a rate much slower than the transmitted signal  The channel may be assumed to be static over one or several reciprocal bandwidth interval  The Doppler spread of the channel is much less than the bandwidth of the baseband signal  Summarize: a signal undergoes slow fading if Ts  Tc Bs  BD
  • 34. Remarks  When a channel is specified as a fast or slow fading channel, it does not specify whether the channel is flat fading or frequency selective  Fast fading only deals with the rate of change of the channel due to motion  In flat fading channel, we can approximate the impulse response to be simply delta function  A flat fading, fast fading channel is a channel in which the amplitude of the delta function varies faster that the rate of the transmitted baseband signal  A frequency selective, fast fading channel, the amplitudes, phases, and time delays of any one of the multipath components vary faster than the rate of change of the transmitted signal
  • 35. Rayleigh Fading  The Rayleigh distribution is commonly used to describe the statistical time varying nature of the received envelope of a flat fading signal  Rayleigh distributed signal:
  • 36. Rayleigh Fading  The Rayleigh distribution has pdf   the rms value of the received voltage signal before envelope detection  2  the time-average power of the received signal before envelope detection  The probability that the envelope of the received signal does not exceed a specified value R is
  • 37. Rayleigh Fading  The mean value of Rayleigh distribution is  The variance of the Rayleigh distribution (represent the ac power)  The median value is  The median is often used in practice
  • 38. Rayleigh Fading  The corresponding Rayleigh pdf is
  • 39. Level Crossing and Fading Statistics  The level crossing rate (LCR) is defined as the expected rate at which the Rayleigh fading envelope, normalized to the local rms signal level, crosses a specified level in a positive-going direction  The number of level crossing per second is given by  N R   rp  R, r  dr  2 f D  e  2    0  Where  r p  is r  time derivative of r(t) (the slope) R,   r is the joint density function of r and atrR=RR  rms
  • 40. Example  For a Rayleigh fading signal, compute the positive- going level crossing   1 for rate when the maximum Doppler frequency is 20 Hz  What is the maximum velocity of the mobile for this Doppler frequency if the carrier frequency is 900 MHz?
  • 41. Solution  Use the equation for LCR NR  2  201 e1  18.44  Use equation of Doppler frequency v  f D  20 1 3  6.66m / s
  • 42. Level Crossing and Fading Statistics  The average fade duration is defined as the average period of time for which the received signal is below a specified level R.  For a Rayleigh fading signal, it is given by 1  Pr  r  R  NR 1 Pr  r  R    i T i R    p  r  dr  1  exp   2  0  So, the average fade duration can be expressed as 2 e 1   f D 2
  • 43. Example   Find the average fade duration for threshold levels0.01 when the Doppler frequency is 200 Hz Solution  Average fade duration is 0.012 e 1   19.9 s  0.01 200 2
  • 44. Rician Fading Distribution  When there is a dominant stationary (nonfading) signal component present, such as line-of-sight propagation path, the small-scale fading envelope distribution is Rician  Random multipath componnets arriving at different angles are superimposed on a stationary dominant signal 2 r  A  2 r   Ar  by The Rician distribution isI 0given for  A  0, r  0   p r   2 e 2 2  2     0 for  r  0 
  • 45. Rician Fading Distribution  The Rician distribution is described in terms of a parameter K A2 K 2 2 A2 K  dB   10 log 2 2  As K  0 we have Rayleigh fading  As K   we have no fading, channel has no multipath, only LOS component
  • 46. Rician Fading Distribution  The Rician pdf is
  • 47. Conclusions  Small-scale fading is variation of signal strength over distances of the order of the carrier wavelength  It is due to constructive and destructive interference of multipath  Key parameters: Doppler spread  coherence time Delay spread  coherence bandwidth  Statistical small-scale fading: Rayleigh fading and Rician fading  flat fading