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Chapter 5 Small-scale

Multi-path Propagation 10 0 -10

dB 

time or

Wireless Communication

Small-scale and Multipath

 Rapid fluctuation of the amplitude of a signal over a short period of time or travel distance  Fading is caused by multipath • Transmitted signal which arrive at the receiver at slightly different times  Effects: factors influencing small-scale fading • Rapid changes in signal strength over a small travel distance or time interval – Random frequency  varying Doppler shift – Speed of the mobile or speed of surrounding objects. • Time dispersion  Multipath delay : depends on of the signal.  Fading • No single line-of-sight (LOS): mobile antennas are below the height of surround structures • With LOS, multipath still occurs • Multipath  random distributed amplitude, phases and angles. • A mobile is stationary, the signal may fade due to movement of surrounding objects. • A receiver moving at high speed can pass through several fades in a small of time. • Doppler shift

Chapter 5 –Small-scale multipath propagation 1 Dr. Sheng-Chou Lin

Page 1 Communication

Multipath Fading

 Slow Fading •over large distances, due to gross changes in path •also called shadowing, log-normal fading  Fast Fading •over distances on the order of a wavelength •also called  Assumptions for above types: •many waves of roughly equal amplitude arrive •Rayleigh distributed amplitude •uniformly distributed phase •spatial angle of arrival •azimuth is uniformly distributed •elevation: PDF has mean of 0o, biased towards small angles, does not extend to infinity, and has no discontinuities  •there is a LOS or dominant path, producing fewer deep fades occurs in small cells

Chapter 5 –Small-scale multipath propagation 2 Dr. Sheng-Chou Lin

Wireless Communication Multipath Fading: Duration and Frequency

AT LEAST 18 dB C/I 10 0 -10 THRESHOLD FOR dB ESTIMATING n and t 

time or wavelength

for a Rayleigh signal 95% of the amplitude is above -10 dB V = vehicle speed, = carrier wavelength n = average number of level crossings at 10 dB below average power t = average fade duration at 10 dB below RMS power  n = 0.75V crossings/second and t = 0.132 seconds  V e.g. at 850 mHz and 15 miles per hour, n = 16 crossings/second, and t = 6 msec

Chapter 5 –Small-scale multipath propagation 3 Dr. Sheng-Chou Lin

Page 2 Wireless Communication

Multi-path Propagation Effects

Multi-path Propagation  Signal levels vary as user moves  Slow variations come from blockage and shadowing by large objects such as hills and buildings  Rapid Fading comes as signals received from many paths drift into and out of phase •phase cancellation occurs, causing rapid fades that are occasionally deep Rayleigh Fading

•the fades are roughly /2 apart: A  7 inches apart at 800 MHz. 10-15 dB 3 inches apart at 1900 MHz •called Rayleigh fading, after the statistical model that describes it t

Chapter 5 –Small-scale multipath propagation 4 Dr. Sheng-Chou Lin

Wireless Communication

Selective Diversity

. maximum amplitude A ...... path 1 ...... path 2

t

Use a to take advantage of uncorrelated fading Use the dominant instantaneous amplitude This eliminates most of the deep nulls

Chapter 5 –Small-scale multipath propagation 5 Dr. Sheng-Chou Lin

Page 3 Wireless Communication Space Diversity A Method for Combating Rayleigh Fading

D  Fortunately, Rayleigh fades are very short and last a small percentage of the time  Two antennas separated by several will not generally experience fades at the same time  “Space Diversity”can be obtained by using two receiving antennas Signal received by 1 and switching instant-by-instant to whichever is best

Signal received by  Required separation D for good Antenna 2 decorrelation is 10-20(BS) •12-24 ft. @ 800 MHz.

Combined Signal •5-10 ft. @ 1900 MHz.  Required separation D is (MS)

Chapter 5 –Small-scale multipath propagation 6 Dr. Sheng-Chou Lin

Wireless Communication

Space Diversity D Application Limitations

 Space Diversity can be applied only on the receiving end of a link.  Transmitting on two antennas would: •fail to produce diversity, since the two signals combine to produce only one value of signal level at a given Signal received point -- no diversity results. by Antenna 1 •produce objectionable nulls in the radiation at some angles Signal received  Therefore, space diversity is by Antenna 2 applied only on the “uplink”, i.e., reverse path Combined •there isn’t room for two sufficiently Signal separated antennas on a mobile or handheld

Chapter 5 –Small-scale multipath propagation 7 Dr. Sheng-Chou Lin

Page 4 Wireless Communication

Doppler Shift

 Doppler spreading increases the signal bandwidth •fd : moving toward, –moving away •fd = cos() (v/ )  Example: fc 1850 MHz, 60mile/hour (mph) •= c / fc = 3 × 108 / 1850 × 106 = 0.162 m •v = 60 mph = 26.82 m/s

•The mobile is moving toward the , fd = 26.82 / 0.162 = 1850.0 Hz

•The mobile is moving away the transmitter, fd = - 1850.0 Hz •fd = 0, as = 90  cos() = 0 v

D

Chapter 5 –Small-scale multipath propagation 8 Dr. Sheng-Chou Lin

Wireless Communication Impulse Response Model of a multipath Channel  The small-scale variations of a signal ; assumptions •The velocity may be assumed constant over a short time (or distance) interval. •The multipath channel is a band-limited band-pass channel •The variations caused by carrier is removed. (baseband). N-1

hb (t, ) = ai ( t, ) exp [ j2fc i ( t ) + i (t, )] (-i ( t )] I = 0 i (t, ) ai ( t, ) : real amp. and excess delay of A time-varying discrete-time impulse response for a multipath radio channel Ith multipath component at time t.

i (t, ) = 2fc I ( t ) + i (t, ) : the phase shift due to free space propagations of the Ith multipath component + additional phase shifts

i (t, ) : lumps together all the mechanisms for phase shifts of a single multipath component within the ith excess delay bin. Chapter 5 –Small-scale multipath propagation 9 Dr. Sheng-Chou Lin

Page 5 Wireless Communication

Impulse Reponses Model (time invariant)

 If the channel impulse response is assumed to be time invariant or is at WSS over a small-scale time or distance interval, then N-1

hb () =  ai exp [ ji ] (- i ) i = 0 x + i y 2  Power delay profile: the spatial of | hb (t, ) | over a local area. 2 P ( t ; ) = k | hb (t, ) |  base band ,K relates the transmitted power • average over a local area to provide a single time -invariant multipath power  make several local area measurement in different location  P ()

 Measurement : hb ( ) can be predicted by a probing pulse p( t ) p( t ) ( t - ) x2(t) = 1/2c(t)2

Chapter 5 –Small-scale multipath propagation 10 Dr. Sheng-Chou Lin

Wireless Communication

Bandwidth and Received power

 Wideband signal : a very narrow pulse, p( t ), does not fluctuate when a receiver is moved about a local area  The received power varies very little  Narrowband signal : the CW signal strength will vary at a rate governed by

the fluctuations of ai and i  large signal fluctuations (fading) occur

• ai varies little over local area Narrowband • I varies greatly due to changes in propagation distance • When the path amplitudes are uncorrelated, multipath phases Wideband are I.I.d over [ 0 , 2] • multipath is not resolved • fading due to the phase shifts of the many unresolved multipath components

– Ex: Tb = 10ns wideband signal and CW signal, fc = 4GHz

Chapter 5 –Small-scale multipath propagation 11 Dr. Sheng-Chou Lin

Page 6 Wireless Communication Bandpass and Baseband channel impulse response  Mobile radio channel as a function of time and space. • Channel impulse response = h(d, t), x(t) = transmitted signal • the received signal y(d,t) = x(t) h(d,t), d: position of the receiver • d = vt, v : assumed constant over a short time interval. • h(d, t)  h( t, ) , t : time due to motion, : multipath delay for a fixed t.  Bandpass channel  Complex baseband impulse response

Bandpass channel factor of 1/2 are due to the properties of the complex envelope y(t) 1 f -f f c  c f

Complex Baseband 2 ~y(t) f f ~ ~ ~ ~ ~ ~ y(t) = 1/2 x(t ) h(t ), x(t ) = c(t ), h(t ) = hb(t ), y(t ) = r(t ) Chapter 5 –Small-scale multipath propagation 12 Dr. Sheng-Chou Lin

Wireless Communication

Complex Envelop of Bandpass System

1 x(t) htReh tej2fct , h th tjh t b b R I f

Immediate complex -fc fc 1 j2fct 2 ht hb te c.c term 2 c(t) 1 f xt ctej2fct c.c 2  1 ytxththxt d h(t)  f -fc f  2 c 1 h (t)  h c t de j2fct c.c b b   4  Cos(2fct )+ j sin(2fct ) f  0 2 1 r(t)= ½ (c(t)  h (t)  h ct e j2fcdej2fct c.c b 4 b  f 1 j2f t  1 c 1 ytRe  hbtcte  rt hbtct y(t) 2  2 f Chapter 5 –Small-scale multipath propagation 13 Dr. Sheng-Chou Lin

Page 7 Wireless Communication

Channel Baseband Complex Envelope

 Baseand impulse of a multipath channel N-1 Initial phase

hb ( t, ) = ai ( t, ) exp [ j2fc i ( t ) + i (t, ) ] (- i ( t )) I = 0 i (t, )  Time invariant baseand impulse h(t) Re[hb N-1

hb ( ) =  ai exp [ ji ] (- i ) i = 0 x + i y

• Power delay profile : the spatial 2 average of hb (t, )  over a local area ~ d ~ t. • To provide a single time-invariant multipath power delay profile P () d(t) • Maximum bandwidth that this model can accurately represent is equal to 1 / 2  t   Chapter 5 –Small-scale multipath propagation 14 Dr. Sheng-Chou Lin

Wireless Communication

Wideband Signal in Mutipath Channel

Tbb  A pulsed, transmitted RF signal 2 a1 x( t ) = Re { p( t ) exp [ j2fc( t ) ], T p t 2  T REP •  max bb a repetitive baseband pulse a  2 train with very narrow pulse width Tbb and period TREP  Wideband signal

• TREP >> max , max : maximum excess delay • Low-pass channel output r(t) hb (t) Instantaneous power delay profile N-1 a1 Measure at t ~ d r (t ) =  ai exp [ ji ] p(t - i ) 0 0 i = 0 a2 a3  To determine the received power at ai some time t  Complex Base Band 0     • The measured power if the multipath 1 2 3 i t   components are resolved Resolved N-1 average N-1 d d2 0 2 2 2 d PWB = |r (t0 ) | =  ak (t0 )  Ea, [PWB ]=  ak 1 k= 0 k= 0 Sum of powers received in each multipath bins  received f power does not fluctuate with d ~ ai , Chapter 5 –Small-scale multipath propagation 15 Dr. Sheng-Chou Lin

Page 8 Wireless Communication

Narrow Signal in Mutipath Channel

Tbb  A CW, transmitted RF signal a1

x( t ) = Re { p( t ) exp [ j2fc( t ) ], • The complex envelope is given by c(t) = 2 a2 • Instantaneous complex envelope of the received  signal N-1 r (t ) =  a exp [ j ( t, ) ] i i fading i = 0 Instantaneous envelope a1 + a2  Instantaneous power (Complex base band )

N-1 Measured at t0 ~ d0 2 2 Pcw = |r (t0 ) | = | ai exp [ ji ( t, ) ] |  i = 0 N-1 N-1 N 2 Ea,[Pcw ] =  ai + 2   r i, j cos(i - j ) i = 0 i = 0 j i d

• r i, j = Ea [ai aj ]: path amp. Correlation coefficient d0 d1 • Ea,[Pcw ]= Ea, [PWB ] as r i, j and/or cos(i - j ) =0

This can occur i are i.i.d over [0,2] or path amplitudes are uncorrelated f Chapter 5 –Small-scale multipath propagation 16 Dr. Sheng-Chou Lin

Wireless Communication

An Example (SMRCIM)

 This technique of quantizing the delay bins determines the time delay resolution of the channel model •Maximum bandwidth that the SMRCIM model (Simulation of Mobile Radio Channel Impulse-response Models) can accurately represent is equal to 1 / 2 (useful frequency span of the model)  Example: A discrete channel impulse response model, If number of multipath bins is 64, •urban radio cahannel with excess delays up to 100 s.

–= N / N = 100/ 64 =1.5625 s –1 / 2 = 1/ (2(1.5625 s)) = 0.32 MHz DELAY SPREAD FUNCTION •microcellular channels with excess delays < 4 s.

–= N / N = 4/ 64 =62.5 ns –1 / 2 = 1/ (2(62.5s)) = 8 MHz •indoor channels with excess delays < 500ns -9 –= N / N = 500 10 / 64 =7.8125 ns  –1 / 2 = 1/ (2(7.8125 ns)) = 64 MHz N = Chapter 5 –Small-scale multipath propagation 17 Dr. Sheng-Chou Lin

Page 9 Wireless Communication

An Example (Narrow band v.s.Wideband)

 A mobile traveling at a velocity of 10 m/s, two multipath components, fc = 1000MHz, The first path with 0 = 0 and power = - 70dBm, Second path with 1 = 1s and power = -73dBm. Mobile moves directly towards the first path and away from the second.

•0 = 0, 1 = 0, = c / f = 0.3m second •P0 = -70dBm = 100pW, P1 = -73dBm = 50pW  complex •at t =0, the narrow instantaneous power = r(t)2 first =100pW exp(0)+ 50pW exp(0)2 = 291 pW

• at t = 0.1s, 0 = 2d / = 2vt / = 210 0.1 / 0.3 = 20.94 rad = 2.09 rad= 120  – 1 = -120 , since mobile moves away from the second component. – r(t)2 = 100pW exp(j120)+ 50pW exp(-j120)2 = 79.3 pW t = 0 2 • at t = 0.3s, 0 = 360= 0, 1 = -360= 0= r(t)= 291 pW • at t = 0.4s, r(t)2 = 79.3 pW, at t = 0.5s, r(t)2 = 79.3 pW. • The average narrowband received power = (2)(291)+(4)(79.3)/6 = 149 pW t = 0.1 • The average wideband received power = P0 + P1 = 100+50 = 150 pw – PW,B PN,B, The wideband signal power remains constant over the same interval

Chapter 5 –Small-scale multipath propagation 18 Dr. Sheng-Chou Lin

Wireless Communication

Delay Profile

 Measured multipath power delay profiles •900 MHz cellular in San Francisco •Inside a grocery store at 4GHz

Chapter 5 –Small-scale multipath propagation 19 Dr. Sheng-Chou Lin

Page 10 Wireless Communication

Time Dispersion Parameters

 Power delay profile •Mean excess delay •RMS delay spread •Excess delay spread

Mean excess delay

2  ak k  P( k ) k k  k = a 2  k  P( k ) k k RMS deplay spread a 2 2 2  k k  P( k ) k 2 k 2 2 k =  - ( ) Where   =  2  ak  P( k ) k k • In outdoor mobile: RMS ~ s • In indoor mobile: RMS ~ ns

Chapter 5 –Small-scale multipath propagation 20 Dr. Sheng-Chou Lin

Wireless Communication

An Example

Maximum excess delay ( xdB ): •time delay during which multipath energy falls to X dB below the maximum.

•I.e. x - 0 , where 0 is the first arriving signal, x is the maximum delay at which a multipath component X dB of the strongest arriving component (which does not necessarily arrive at 0 ) 2 Threshold level: , , depend on the choice of threshold 2 •noise threshold , , ,  Pr() 0dB

Example: -10dB 1 = 4.38 sec Bc = -20dB 5  -30dB 2 = 21.07 sec = 146 kHz   = 1.37 sec 0 1 2 5  ( s)

Chapter 5 –Small-scale multipath propagation 21 Dr. Sheng-Chou Lin

Page 11 Wireless Communication

Typical measured RMS delay spread

• Outdoor mobile channel : RMS is on the order of s • Indoor radio channel : RMS is on the order of ns

Chapter 5 –Small-scale multipath propagation 22 Dr. Sheng-Chou Lin

Wireless Communication

Coherence Bandwidth

 Relation derived from RMS delay spread

•BW Bc , the channel can be considered as “flat” •Flat channel: a channel which passes all spectral components with equal gain and linear phase •Two frequency components have a strong potential for amplitude correlation over the range of frequencies.

 Relation between Frequency correlation function and Bc 1 •correlation function > 0.9  B  c CR > 0.5 50 1 CR > 0.9 •correlation function > 0.5  Bc  5

 Ex: = 1.37 sec, Bc 1/ 5= 146 kHz •AMP BW = 30k  no equalizer required. •GSM 200 k equalizer required

Chapter 5 –Small-scale multipath propagation 23 Dr. Sheng-Chou Lin

Page 12 Wireless Communication

Signal BW v.s. Coherent Bandwidth



t f T BW > Bc Freq. Selective channel Narrowband Channel 1 Bc  BW  1/T 

t f BW B Flat channel Wideband Channel c

Chapter 5 –Small-scale multipath propagation 24 Dr. Sheng-Chou Lin

Wireless Communication

Flat and Frequency-selective Fading

2-ray multipath channel (point-point)

i

Flat fading Frequency-selective fading

Chapter 5 –Small-scale multipath propagation 25 Dr. Sheng-Chou Lin

Page 13 Wireless Delay Spread, A Phenomenological Model

DELAY SPREAD FUNCTION | H(f) |

TRANSMITTER RECEIVER CHANNEL  TRANSFER FUNCTION

• The delay spread of a channel d is the RMS value of the channel impulse response (delay spread function) • In a mobile environment, the delay spread function is constantly changing (i.e., |h(f)| is a nonlinear time-varying filter) • The channel transfer function |h(f)| has a lowpass characteristic with multiple delays (time dispersion) • The delay spread represents the time it takes most of the energy from the transmitter to propagate (at c = 3e+8 m/s) to the receiver • can be considered the group delay of the channel model |h(f)| • For in-building propagation, = 0.1 s; for urban propagation = 3s

Chapter 5 –Small-scale multipath propagation 26 Dr. Sheng-Chou Lin

Wireless Communication Bandwidth, Frequency Diversity Gain and Delay Spread

 The channel coherence bandwidth BC can be computed from the delay spread d of a channel: 1 B = C 2

 If a signal has a bandwidth b greater than BC , then the signal has frequency components that fade independently. the signal has a frequency diversity gain, G G = 1+B , B : Bandwidth of signal

 Signals with bandwidths greater than BC are more resistant to channel fading effects

 EXAMPLES:

•Compute the coherence bandwidth of a channel with = 3s (Bc = 53 khz) •Show there is no frequency diversity gain for amps.(AMPS = 30 khz < 53 khz) •Compute the frequency diversity gain for CDMA. ( g = 1 + 1.25 x 3 = 4.75) Chapter 5 –Small-scale multipath propagation 27 Dr. Sheng-Chou Lin

Page 14 Wireless Communication

INTERSYMBOL INTERFERENCE (ISI) AND DELAY SPREAD

 To avoid isi in the standstill (nonfading) case, the maximum data rate RB is related to the delay spread d of the channel 1 R = B 

 To avoid ISI in mobile environments (fading case), the maximum data rate R is given by: B 1 R = B 2

 EXAMPLE: • You are interested in buying a wireless modem from a vendor for indoor data transmission at rates less than 300 kbits/sec. • the vendor insists that you buy modems equipped with equalizers which doubles the price.

• is this necessary? no. assume a fading case with = 0.5s, then RB = 318 kbits/sec

Chapter 5 –Small-scale multipath propagation 28 Dr. Sheng-Chou Lin

Wireless Communication

Doppler Spread

 To describe time varying nature of the channel in a small-scale region.

•Doppler spread BD : a measure of the spectral boarding channel caused by the time rate of change of the channel.

•Doppler spectrum : components in the range fc-fd to fc-fd.

•Effect of Doppler spread are negligible, as BWsignal BD t T  Coherence time TC is the time domain c dual of Doppler •To characterize time varying nature

•Tc 1/ fm under Rayleigh fading

•Ts Tc  channel will change during the transmission of the baseband message  •Time correlation function > 0.5,

 Tc 9 / 16fm , fm: the max. Doppler shift Chapter 5 –Small-scale multipath propagation 29 Dr. Sheng-Chou Lin

Page 15 Wireless Communication

A thumb rule

 A popular rule of thumb for modern digital communications is

9 0.423 T = = C 2 16 fm fm

• Tc 1/ fm suggests a time duration during Rayleigh fading

• Tc 9 / 16fm is often too restrictive

• Definition of coherence time : two signals arriving with a time separation > Tc are affected differently by the channel.

 Example: A vehicle, speed = 60 mile/per hour, fc = 900 MHz

• Tc = 9 / 16fm = 2.22ms

• If a digital transmission is used, max. symbol rate Rc = 1/ Tc = 454bps. –Distortion could result from multipath time delay spread = • Using the practical rule, Tc = 0.423/fm 6.77ms , max. symbol rate Rc = 1/ Tc = 150bps

Chapter 5 –Small-scale multipath propagation 30 Dr. Sheng-Chou Lin

Wireless Communication

An Example

 Small-scale propagation measurements •Determine the proper spatial sampling interval •consecutive samples are highly correlated in time

•fc = 1900 MHz and v = 50m/s.

•For correlation, the sampling time is Tc /2. Use the smallest Tc for conservative design.

–Tc 9 / 16fm = 9/16 v = 565 s  Tc /2 = 282.5 s •How many samples is required over 10m travel distance.

–Spatial sampling interval: x = vTc /2 = 50 565 s /2 = 1.41 cm

–Required samples = Nx = 10 / x =708 samples •How long would it take to make these measurements –d / v = 10m/50 = 0.2 seccond

•The Doppler spread BD = fm = vfc / c = 316.66 Hz

Chapter 5 –Small-scale multipath propagation 31 Dr. Sheng-Chou Lin

Page 16 Wireless Communication

Types of small-scale fading

 Depending on the relation Small-Scale fading between the signal and (based on multipath time delay spread) channel parameters, different transmitted signals will undergo Flat Fading Frequency selective Fading different types of fading 1. BW of signal < BW of channel 1. BW of signal > BW of channel 2. Delay spread < Symbol period 2. Delay spread > Symbol period

•Signal parameters: Small-Scale fading Bandwidth, symbol period (based on Doppler spread) •Channel parameters: RMS delay spread, Doppler spread Fast Fading Slow Fading 1. High Doppler spread 1. Low Doppler spread 2. Coherence time < Symbol period 2. Coherence time > Symbol period 3. Channel variations faster than 3. Channel variations slower than baseband signal variations baseband signal variations

Chapter 5 –Small-scale multipath propagation 32 Dr. Sheng-Chou Lin

Wireless Communication Types of fading

l T

o s b

f m o y Flat Slow Flat Fast d S

o Fading Fading i g

 Type of fading experienced r n i e t t P i

by a signal as a function of l m o  s

b 

n Frequency Selective Frequency Selective m a y r Slow Fading Fast Fading •Signal parameters: S T Ts Tc –Symbol period (Ts ) Transmitted Symbol Period –Baseband signal B

s

bandwidth ( B ) d s n a h t b d e •Channel parameters: i

s Frequency Selective Frequency Selective w a d b

Fast Fading Slow Fading n d –RMS delay spread () a e b t

t l B i c Coherent BW ( B ) a m c n s g

i Flat Fast Flat Slow n s –Doppler spread ( B ) a D r Fading Fading Coherent Time ( T ) T c Bs BD Transmitted baseband signal bandwidth Chapter 5 –Small-scale multipath propagation 33 Dr. Sheng-Chou Lin

Page 17 Wireless Communication

Rayleigh Distribution

 To describe statistical time varying nature of the received envelope • A flat fading signal • An individual multipath component • The envelope of the two quadrature Gaussian noise

x + i y r = x2 + y2

Zero-mean Gaussian dist. with 2

r r 2 exp ( ) , 0 r  P(r) = 2 22 0 , r 0 Rayleigh fading beams : rms before envelope 2 : time-average power before x, y envelope t

Chapter 5 –Small-scale multipath propagation 34 Dr. Sheng-Chou Lin

Wireless Communication

Rayleigh Distribution Parameters

 Cumulative distribution function (CDF)

R2 P( R ) = P ( r R) = 1- exp ( ) r 22

 Mean value of Rayleigh distribution  rmean = E [ r ] = r p( r ) dr = / 2 = 1.2533  0  Variance of Rayleigh distribution

E [ r 2 ] = E [ x 2 ] + E [ y 2 ] = 2 2 1.2533 

2 2 2 2 2 r = E [ r ] –(E [ r ]) = 2  - (/2) = 0.4292  rms of the envelope = square root of the mean square = E [ r 2 ] = 2 

Chapter 5 –Small-scale multipath propagation 35 Dr. Sheng-Chou Lin

Page 18 Wireless Communication

Ricean Fading Distribution

 There is a dominant stationary (nonfading) signal component

•line-of-sight ( LOS ) Rayleigh •small-scale fading envelope distribution is Ricean •Ricean  Rayleigh as LOS fades away

r ( r 2 +A2 ) Ar exp ( ) I0 ( 2 ) ,A 0, 0 r P(r) = 2 22   , r 0 0

A : peak amplitude of LOS Random multipath LOS I0 ( ) : Modified Bessel function of the first kind of zero-order K = A2 / ( 2 2 ) : describe Ricean distribution K (dB) = 10 log [ A2 / ( 2 2 ) ] dB

• A  0, K  dB, Ricean  Rayleigh

Chapter 5 –Small-scale multipath propagation 36 Dr. Sheng-Chou Lin

Wireless Communication

Clarke’s Model for Flat Fading

 Assumptions •A fixed transmitter with a vertically polarized antenna •The field on the mobile antenna comprises of N azimuthal plane waves with –arbitrary carrier phases z –arbitrary azimuthal angles of arrival vertically polarized y –each having equal average amplitude in absence of a direct LOS experience similar attenuation over small-scale distances   Vertically polarized plane waves at BS x N Azimuthal plane Ez = E0 Cn cos ( 2fct + n ) n =1

• Doppler shift is very small Tc( t ) and Ts( t ): Gaussian • The phase angles uniformly distributed on [0, 2] Random processes 2 2 Ez = Tc( t ) cos ( 2fct ) + Ts( t ) sin( 2fct ) r ( t ) = Tc ( t ) + Ts ( t ) 2 2 2 2 2  Rayleigh distribution = p (r) Tc = Tc = Ez  = E0 / 2 =  Chapter 5 –Small-scale multipath propagation 37 Dr. Sheng-Chou Lin

Page 19 Wireless Communication Spectral-Shape with Doppler-spread

 Spectral analysis for Clark’s model •Total received power z vertically polarized

2 y

Pr = AG() p() d 0 G() = Antenna Azimuthal gain pattern  x A : average received power w.r.t an Azimuthal plane isotropic antenna y p() = incoming power of the angle 

•instantaneous freq. Of the received signal (CW, freq.= fc) component arriving at an angle  v f () = f = cos() + f = f cos() + f  df = d-sinf  c m c m

fm : maximum Doppler shift, an even function  f () = f (-) •The received power with frequency S( f ) df = A [ G() p() + G(-) p(-)] d Chapter 5 –Small-scale multipath propagation 38 Dr. Sheng-Chou Lin

Wireless Communication Doppler power spread

0º 180º  Doppler power spectrum (unmodulated CW carrier) -1 = cos [ ( f-fc )/ fm ]

2  sin = 1-[( f-fc )/ fm ] •For the case, vertical /4 Antenna G() =1.5 and p() = 1/2over [0, 2] 1.5 SEz( f ) = f 2 m 1-[( f-fc )/ fm ]  A Baseband power 1 K 2 SbbEz( f ) = 1- ( f / 2fm ] 8fm K[ ] : complete elliptical integral of the first kind • not intuitive

Chapter 5 –Small-scale multipath propagation 39 Dr. Sheng-Chou Lin

Page 20 Wireless Communication

Two-Rayleigh Fading Model

 To consider multipath time delay spread as well as fading

hb ( t ) = 1 exp [ j1 ] ( t ) + 2 exp [ j2 ] ( t - )

•1 , 2 : independent and Rayleigh distributed •1 , 2 : independent and uniformly distributed over distributed •: time delay between two rays •To create a wide range of frequency selective fading effects by varying 

1st Rayleigh fading neam 2nd Rayleigh fading neam Rayleigh fading beam

 Chapter 5 –Small-scale multipath propagation 40 Dr. Sheng-Chou Lin

Wireless Communication

Simulation of Flat Fading Model

 Quadrature  Quadrature Amplitude modulation • RF Doppler filter  Two indep. Gaussian low-pass noise • Baseband Doppler filter for in-phase and quadrature fading  Spectral filter  Accurate time domain of Doppler fading  IFFT at the last stage

Construct negative components of the noise source

Chapter 5 –Small-scale multipath propagation 41 Dr. Sheng-Chou Lin

Page 21 Wireless Communication

Simulation of frequency-selective Fading

 To produce both flat and frequency-selective fading effects • Several Rayleigh fading simulators • Variable gains • Time delays

 Rayleigh  Ricean •Add a single freq. Component dominant in amplitude within Doppler fading spectrum

Chapter 5 –Small-scale multipath propagation 42 Dr. Sheng-Chou Lin

Wireless Communication

Small-scale multipath measurements

 Measurements • Direct RF pulse system • sliding correlator – Narrow BW  wideband • Frequency Domain – FFT, IFFT

Chapter 5 –Small-scale multipath propagation 43 Dr. Sheng-Chou Lin

Page 22 Wireless Communication

Digital Modulation under flat fading

 Performance in slow, flat fading channels in AWGN

•Binary modulation •Rayleigh fading •To average the error probability in AWGN over the possible ranges of signal strength due to fading

2 • = [ Eb/ No]  is the average value of signal-to- noise ratio, has a Rayleigh distribution •Mean SNR is significantly larger than that required Fading v.s. nonfading when operating over a nonfading channel (~20- 50dB)

Chapter 5 –Small-scale multipath propagation 44 Dr. Sheng-Chou Lin

Wireless Communication Level Crossing Rate (LCR)

 Level Crossing Rate (LCR): the rate at which the Rayleigh fading envelope, normalized to RMS level (2 ), crosses a specified level.

•NR : the number of level crossings per second ( r = R )  2 NR rpR,rdr 2fm e 10 0 0 -10 R fm : the maximum Doppler frequency r: time derivative of r(t) dB pR,r: joint density function ofr andr at r = R 1 sec.

= R / Rrms : the value of the specified NR R normalized to RMS amplitude of • Few crossings at both high and low levels fading envelope • Maximum at = 2  Example: For a Rayleigh fading signal, = 1, maximum Doppler freq. fm= 20Hz, fc = 900 MHz. -1 •NR = 2(20) 1e = 18.44 crossings per second

• f d,max = v /  v = 20 (1/3) = 6.66 ms = 24 km/hr Chapter 5 –Small-scale multipath propagation 45 Dr. Sheng-Chou Lin

Page 23 Wireless Communication

Average fade duration

 Average fade duration: average period of time for which the received signal a specified R. For a Rayleigh fading signal

2 1 e  - 1 10 = Pr [ r R ] = N f 2 0 R m R 2 • Pr [ r R ] = 1- exp(  ) : probability that the received signal less than R = the fading time in one second.

• Helps determine the most likely NR number of signaling bits that may be 1 sec. lost during a fade Pr [ r R ] = fading time in 1 sec.

 Example: Threshold level = 0.707, Doppler freq. = fm = 20Hz, Binary digital modulation with bit duration of 50 bps, bit error occurs for 0.1 2 • The average fade duration = (e 0.707 -1) / (0.707)20 2= 18.3 ms • bit period = 1/50 = 20ms  the signal undergoes than fast Rayleigh fading

• for =0.1, = 0.002 s = 20ms  one bit will be lost during a fade, NR = 4.96  the total number of bits in error is 5/sec.  BER = 5/50 = 0.1

Chapter 5 –Small-scale multipath propagation 46 Dr. Sheng-Chou Lin

Wireless Communication

Lesson 5 Complete

Chapter 5 –Small-scale multipath propagation 47 Dr. Sheng-Chou Lin

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