Wireless and Mobile Networking Dr. Faramarz Hendessi I f h U i fT h Isfahan Univ. of Tech. Spring 2009
Lecture 15: Lecture 15:
Basic Principles
Fading Distribution and Models
١
Types of Small‐scale Fading Small-scale Fading (Based on Multipath Tİme Delay Spread)
Flat Fading
Frequency Selective Fading
1. BW Signal < BW of Channel 2. Delay Spread < Symbol Period
1. BW Signal > Bw of Channel 2. Delay Spread > Symbol Period
Small-scale Fading (Based on Doppler Spread)
Fast Fading 1. High Doppler Spread 2. Coherence Time < Symbol Period 3. Channel variations faster than baseband signal variations
Slow Fading 1. Low Doppler Spread 2. Coherence Time > Symbol Period 3. Channel variations smaller than baseband signal variations
Fading Distributions •
• •
٢
Describes how the received signal amplitude changes with time. – Remember that the received signal is combination of multiple signals arriving from different directions, phases and amplitudes. – With the received signal we mean the baseband signal, namely the With the received signal we mean the baseband signal namely the envelope of the received signal (i.e. r(t)). It is a statistical characterization of the multipath fading. Two distributions – Rayleigh Fading – Ricean Fading
Rayleigh Distributions •
Describes the received signal envelope distribution for channels, where all the components are non‐LOS: – i.e. there is no line‐of–sight (LOS) component.
Ricean Distributions •
٣
Describes the received signal envelope distribution for channels where one of the multipath components is LOS component. – i.e. there is one LOS component.
Rayleigh Fading
Rayleigh Fading
۴
Rayleigh Fading Distribution • The Rayleigh distribution is commonly used to describe the statistical time varying nature of the received envelope of a flat fading signal, or the envelope of an individual multipath the envelope of an individual multipath component. • The envelope of the sum of two quadrature Gaussian noise signals obeys a Rayleigh distribution. ⎧ r r 2
⎪ exp(− 2 ) p(r ) = ⎨σ 2 2σ ⎪0 r <0 ⎩
0≤ r ≤ ∞
• σ is the rms value of the received voltage before envelope detection, and σ2 is the time‐ average power of the received signal before envelope detection.
Rayleigh Fading Distribution • The probability that the envelope of the received signal does not exceed a specified value of R is given by the CDF: R
−
P(R) = Pr (r ≤ R) = ∫ p(r)dr =1− e ∞
0
rmean = E[ r ] = ∫ rp ( r ) dr = σ 0
rmedian
π
2
2σ 2
= 1.2533σ
1 = 1.177σ found by solving = 2
rrms = 2σ σ r2 = E [ r 2 ]− E 2 [ r ] =
∫
∞
0
r 2 p ( r ) dr −
• rpeak=σ and p(σ)=0.6065/σ
۵
R2
σ 2π 2
rmedian
∫ p (r )dr 0
= 0. 4292σ 2
Rayleigh PDF 0.7
0.6065/σ 0.6
mean = 1.2533σ median = 1.177σ
0.5
variance = 0.4292σ2
0.4
0.3
0.2
0.1
0 0
1 σ
22 σ
33 σ
4 4σ
5 5σ
A typical Rayleigh fading envelope at 900MHz.
۶
Ricean Distribution • •
When there is a stationary (non‐fading) LOS signal present, then the envelope distribution is Ricean. The Ricean distribution degenerates to Rayleigh when the dominant component fades away. p y
Ricean Fading Distribution •
•
When there is a dominant stationary signal component present, the small‐scale fading envelope distribution is Ricean. The effect of a dominant signal arriving with many weaker multipath signals gives rise to the Ricean distribution. The Ricean distribution degenerates to a Rayleigh distribution when th d i the dominant component fades away. t tf d ⎧ r ( r 2 + A2 ) Ar exp[ − ]I 0 ( 2 ) ⎪ p ( r ) = ⎨σ 2 2σ 2 σ ⎪0 r <0 ⎩
A≥0
•
The Ricean distribution is often described in terms of a parameter K which is defined as the ratio between the deterministic signal power and the variance of the multipath.
• •
K is known as the Ricean factor As A→0, A→0 K → ‐∞ dB, dB Ricean distribution degenerates to Rayleigh distribution. 2 K =
٧
0 ≤ r ≤ ∞,
A
2σ 2
CDF •
Cumulative distribution for three small‐scale fading measurements and their fit to Rayleigh, Ricean, and log‐normal distributions.
PDF • Probability density function of Ricean distributions: K=‐∞dB (Rayleigh) and K=6dB. For K>>1, the Ricean pdf is approximately Gaussian about the mean.
٨
Rice time series
Nakagami Model • Nakagami Model p(r ) =
2m m r 2 m−1 exp( p(− Γ(m)Ω m
m 2 r ) Ω
• r: envelope amplitude • Ω=: time‐averaged power of received signal • m: the inverse of normalized variance of r2
– Get Rayleigh when m=1 G tR l i h h 1
٩
Small‐scale fading mechanism
• Assume signals arrive from all angles in the horizontal plane 0<α<360 • Signal amplitudes are equal, independent of α • Assume further that there is no multipath delay: (flat fading assumption) • Doppler shifts fn =
v
λ
cos a n
Small‐scale fading: effect of Doppler in a multipath environment • fm, the largest Doppler shift
S bbEz ( f ) =
١٠
⎛ f ⎞ 1 ⎟⎟ k 1 − ⎜⎜ 8πf m ⎝ 2 fm ⎠
2
Carrier Doppler spectrum
• Spectrum Empirical investigations show results that deviate from this model Power Model Power goes to infinity at fc+/‐fm
Baseband Spectrum Doppler Faded Signal
• Cause baseband spectrum has a maximum frequency of 2fm
١١
Simulating Doppler/Small‐scale fading
Simulating Doppler fading • Procedure in page 222
١٢
Level Crossing Rate (LCR) Threshold (R)
LCR is defined as the expected rate at which the Rayleigh fading envelope, normalized to the local rms signal level, crosses a specified threshold level R in a positive going direction. It is given by:
NR = 2π fmρe−ρ
2
where
ρ = R / rrms
(specfied envelopevaluenormalized torms)
NR : crossingspersecond
Average Fade Duration Defined as the average period of time for which the received signal is below a specified level R. For Rayleigh distributed fading signal, it is given by:
τ=
(
2 1 1 Pr[r ≤ R] = 1− e−ρ NR NR
eρ −1 R τ= , ρ= rrms ρfm 2π 2
Example 5.7, 5.8, 5.9
١٣
)
Fading Model: Gilbert‐Elliot Model Fade Period Signal Amplitude Threshold
Time t
Bad
Good
(Fade)
(Non-fade)
Gilbert‐Elliot Model 1/AFD Bad
Good (Non-fade) (Non fade)
((Fade))
1/ANFD
The channel is modeled as a Two-State Markov Chain. Each state duration is memory-less and exponentially distributed. The rate going from Good to Bad state is: 1/AFD (AFD: Avg Fade Duration The rate going from Bad to Good state is: 1/ANFD (ANFD: Avg Non-Fade Duration)
١۴
Simulating 2‐ray multipath
• a1 and a2 are independent Rayleigh fading • φ1 and φ2 are uniformly distributed over [0 2π) [0,2π)
Simulating multipath with Doppler‐induced Rayleigh fading
EE 542/452 Spring 2008
١۵
Saleh and Valenzuela Indoor Model •
•
Measured same‐floor indoor characteristics – Found that, with a fixed receiver, indoor channel is very slowly time‐varying – RMS delay spread: mean 25ns, max 50ns – Maximal delay spread 100ns‐200ns – With no LOS, path loss varied over 60dB range and obeyed log distance power law, 3 > n > 4 Model assumes a structure and models correlated multipath components.
• Multipath model – Multipath components arrive in clusters, follow Poisson distribution. Clusters relate to building structures. g – Within cluster, individual components also follow Poisson distribution. Cluster components relate to reflecting objects near the TX or RX. – Amplitudes of components are independent Rayleigh variables, decay exponentially with cluster delay and with intra‐cluster delay
SIRCIM and SMRCIM indoor/outdoor Models •
These models were developed by Rappaport and seidel SIRCIM is a computer program , that generates small scale indoor channel response measurements.
•
The most salient feature of the model is that it produces multipath channel conditions that are very realistic since they are based on real world measurements and may thus be used for meaningful system design in factories and office buildings
•
These programs are very useful and poplar and are used in over 100 institutions. Model can measure individual multipath fading and small scale receiver spacing. Multipath delay inside the building was found to be 40ns to 800ns. Mean multipath delay ranged from 30‐300 ns. Arriving multipath component has a Gaussian distribution. Average number of multipath components range from 9 to 36
• • • • •
١۶
SIRCIM and SMRCIM indoor/outdoor Models
• SIRCIM Model
– Based on measurements at 1300MHz in 5 factory and other buildings factory and other buildings – Model power‐delay profile as a piecewise function ⎧ TK TK < 110ns ⎪ 1− 367 ⎪⎪ T −110 PR (TK , S1 ) = ⎨0.65− K 110ns < TK < 200ns 360 ⎪ ⎪0.22- TK − 200 200ns < T < 500ns K ⎪⎩ 1360
T ⎧ 0.55 + K TK < 100ns ⎪ 667 PR (TK , S2 ) = ⎨ T −100 ⎪0.08+ 0.62exp( K ) 100ns < TK < 500ns 75 ⎩
١٧