Wireless Channel Model
Wha Sook Jeon
Mobile Computing and Communication Lab.
Radio Channel (1)
Signal Fading
− large-scale component: Path Loss
− medium-scale slow varying component:
Shadowing
− small-scale fast varying component:
Multipath fading
Radio Channel (2)
LOS Path vs. NLOS Path
Path Loss & Shadowing
Path Loss
− caused by dissipation of the power radiated by the transmitter
− depends on the distance between transmitter and receiver
Shadowing
− caused by obstacles between the transmitter and receiver
that absorb power.
Multipath fading
short-term fluctuation of the received signal caused by multipath propagation
when mobile is moving
Fading becomes fast as a mobile moves faster
delay-power profile (delay spread)
Average power (dB)
Delay Narrowband
fading
Wideband fading
Rayleigh distribution
Channel Model
Simplified Pass Loss Model
Path loss as a function of distance:
−
sometimes simple model can captures the essence of signal propagation without resorting to complicated path loss models.−
Free-space, two-ray, Hata, COST extension to Hata are all of the same form−
K : constant which depends on antenna characteristics and the average channel attenuation■ Free space path gain at distance d0 assuming omni-directional antennas
■ Empirical measurements at d0
−
d0: reference distance■ generally valid only at d> d0
■ d0 : 1-10m (indoor), 10-100m (outdoor)
−
: path loss exponent■ at higher frequencies tend to be higher and at higher antenna heights tend to be lower
γ
= d
K d P
Pr t 0
γ
Empirical Path Loss Models
Piecewise Linear Model Indoor Attenuation Factors
− partition loss
− floor loss
− the building penetration loss
− It is difficult to find generic
models
Shadowing (1)
Statistical models
−
The transmitted signal experiences random variation due to blockage from objects in the signal path and changes in reflecting surfaces and scattering objects. Log-normal shadowing
−
Ratio of transmit-to-receive power is a random variable with a log-normal distribution−
Distribution of (the dB value of ) is Gaussian with mean and standard deviationt
r P
P / ψ =
−
−
= 2
2 10
2
) log
10 exp (
2
10 ln / ) 10
(
dB dB
dB
p
ψ ψ
ψ σ
µ ψ ψ
σ ψ π
ψdB
ψ
ψdB
µ
ψdB
σ
−
−
= 2
2
2
) exp (
2 ) 1
(
dB dB
dB
dB
p dB
ψ ψ
ψ σ
µ ψ
σ ψ π
Shadowing (2)
constant.
n attenuatio an
is where
, )
(d e αd α
s = −
∑
= i
t d
d
i dt
d
t e e
d
s( ) = −α∑ = −α
Justification for the Gaussian model as the distribution of
−
when shadowing is dominated by the attenuation from blocking object−
attenuation of a signal as traveling through an obstacle with depth d■
−
attenuation of a signal as it propagates through the region■
−
dt : Gussian r.v. (by the Central Limit Theorem)−
: Gussian r.v. Decorrelation distance :
−
the distance at which autocovariance equals 1/e of its maximum value−
on the order of the size of the blocking objects or clusters of objects )( log10s dt
ψdB
Combined Path Loss and Shadowing
Combined model
− average dB path loss: the path loss model
− shadow fading with mean of 0 dB: variations about the path loss
Simplified path loss with log-normal shadowing
−
− : ψ
dBa Guassian r.v. with mean zero and variance
dB t
r
d K d
P dB
P = − γ +ψ
0 10
10 10 log
log 10 ) (
ψdB
σ
Pr/Pt (dB)
log d Very slow Slow
10logK
γ
−10
Outage Probability
under the path loss and shadowing
− : the minimum received power level
− outage probability:
■
the probability that the received power at a given distance d falls below
■
■
for the combined path loss and shadowing (at slide 23)
P
minPmin
) , (Pmin d pout
) )
( ( )
,
(Pmin d p P d Pmin pout = r <
− + −
−
=
<
dB
d d K
P Q P
P d
P
p r t
σψ
γ log ( / ) 10
log 10 1 (
) )
(
( min min 10 10 0
Multipath
Multipath fading
−
Constructive and destructive addition of different multipath components introduced by a channel Time-varying channel impulse response
−
If a single pulse is transmitted over a multipath channel, the received signal appears as a pulse train−
A multipath channel is modeled by a channel impulse response. Characteristic of the multipath channel
−
time delay spread■ Time delay between the arrivals of the first received signal component and the last received component associated with a single transmitted pulse
−
time-varying nature due to moving Narrowband fading model
Wideband fading model
Example of Multipath
Multipath Component (1)
Nonresolvable components:
these are combined into a single component.
Resolvable components:
if the delay difference between two components significantly exceeds the inverse signal bandwidth
Multipath Component (2)
Doppler Shift
When the transmitter is
moving, the received signal has a Doppler shift
Doppler effect is on the order of 100 Hz for typical vehicle speed (75km/hr) and
frequencies (about 1GHz )
D D
D
f
v f t
π φ
λ θ φ
π
22 cos 1
=
∆ =
= ∆
Time-varying Channel Impulse Response
Equivalent lowpass time-varying channel impulse response at time t to an impulse at time :
−
N(t): the number of multipath components−
For the nth component■ : delay
■ : phase shift -
■ : Doppler phase shift
■ : amplitude
Time-invariant channel:
) (
) (
0
n j
N
n n
e n
c τ = α − φ δ τ −τ
∑
=τ
−
t ( , ) ( ) ( ) ( ) ( ( ))
0 t e t
t
c N t n j t n
n
n
δ τ τ
α
τ
=∑
= − φ −)
n(t τ
Dn
φ n
D n
c
n t πf τ t φ
φ ( )=2 ( )−
)
n(t α
)
n(t φ
Transmit & Receive Signal Models (1)
Complex baseband representation
− The transmitted or received signals are actually real sinusoids
− The complex representations are used to facilitate analysis
Transmitted signal
−
−
■
complex baseband signal with in-phase component s
I(t) and quadrature component s
Q(t)
{
( )}
( )cos(2 ) ( )sin(2 )Re )
(t u t e 2 s t f t s t f t
s = j πfct = I π c − Q π c
) ( )
( )
(t s t js t
u = I + Q
Transmit & Receive Signal Models (2)
Transmitted signal
−
Received signal
−
−
−
=
− −
=
− −
=
−
=
∑
∑ ∫
∫ ∑
∫
=
−
=
∞
∞
−
−
∞
∞ =
−
∞
∞
−
t f j N(t)
n
n t
j n
t f j N(t)
n
n t
j n
t f j -
N(t)
n
n t
j n
t f j
c n
c n
c n
c
e t t
u e
t
e d
t u t e
t
e d t
u t e
t
e d t
u t c t
r
π φ
π φ
π φ
π
τ α
τ τ τ
τ δ α
τ τ τ
τ δ α
τ τ τ
2 0
) (
2 0
) (
2 0
) (
2
)) ( (
) ( Re
) ( )) ( (
) ( Re
) ( )) ( (
) ( Re
) (
) , ( Re
) (
{
u t ej fct}
t
s( ) = Re ( ) 2π
−
=
∑
N t t e−j n t u t t ej fctt
r( ) Re ( )α ( ) φ ( ) ( τ ( )) 2π
Narrowband Fading Model
Narrowband Fading Model (1)
Narrowband fading assumption
− Delay spread:
− The LOS and all multipath components are typically nonresolvable.
Received Signal
−
−
In order to characterize the random scale factor caused by the multipath, u(t)=1
− Transmitted signal:
− Received signal:
Tm << 1B
i
i u t
t
u( −
τ
) ≈ ( ) for allτ
= −
∑
=( ) ( ) 02 ( )
) ( Re )
( j t
t N
n n t
f
j c n
e t e
t u t
r π α φ
channel
characteristic
{ }
e f tt
s( ) = Re j2πfct = cos2
π
ct
N( )
Narrowband Fading Model (2)
Received Signal
−
− in-phase component:
− quadrature component:
r
I(t) and r
Q(t) can be approximated as Gaussian random processes
− if N(t) is large, and and are independent for different components.
− when for small N(t) each ray has a Rayleigh distributed envelope and uniform phase
− r
I(t) and r
Q(t) are independent Gaussian process with the same autocorrelation , a mean of zero, and a crosscorrelation of zero
) ( cos ) ( )
(
) (
0
t t
t
r n
t N
n n
I
∑
α φ=
=
t f t
r t f t
r t
r( ) = I( )cos2π c + Q( )sin2π c
) ( sin ) ( )
(
) (
0
t t
t
r n
t N
n n
Q
∑
α φ=
=
)
n(t
α φn(t)
Autocorrelation and Cross Correlation (1)
Assumption
− There is no dominant LOS component
− The amplitude, multipath delay and Doppler frequency shift are changing slowly enough to be considered constant over the time interval of interest
■
− is uniform distributed on [-
■π , π ]
■ this is reasonable because is large and hence can go through a 360o rotation for a small change
The received signal r(t) is zero-mean Gaussian process
−
−
n
n D
n D n
n
n(t) ≈α ,τ (t) ≈τ , f (t) ≈ f α
)
n(t φ
t f f
t c n Dn
n π τ π
φ ( ) = 2 −2
0 )]
( cos E[
] [ E )]
( [
E r t =
∑
n n t =n
I α φ
fc
τn
) 0 )]
( ) ( [ E
( rI t rQ t = 0
)]
( E[sin ]
[ E )]
( [
E r t =
∑
α φ t =Autocorrelation and Cross Correlation (2)
Autocorrelation
−
■
■
− A uniform scattering environment assumption
■ The channel consists of many scatters densely packed with respect to angle
− Each component has the same received
■power:
−
N n
n n θ π
θ = ∆ =2
N Pr
n] 2
[
E α2 =
) sin(2
) ( )
2 cos(
) ( )]
( ) ( [ E )
( t r t r t t A t f t A , t f t
Ar r c r r c
Q I
I ∆ ∆ − ∆ ∆
=
∆ +
=
∆ π π
∆
=
∆ +
=
∆
∑
n nn I
I r
t t v
t r t r t
AI θ
λ
α 2π cos cos
] [ E 5 . 0 )]
( ) ( [ E )
( 2
∆
−
=
∆ +
=
∆
∑
n nn Q
I r
r
t t v
t r t r t
AI Q θ
λ
α 2π cos sin
] [ E 5 . 0 )]
( ) ( [ E )
( 2
,
θ λ θ
π
π
∆
∆ ∆
=
∆
∑
=
t n v t P
A
N
n r
rI 2 cos
2 cos )
(
1
v
Autocorrelation and Cross Correlation (3)
) 2
cos(
) ( )
( t A t f t
A ∆ = ∆ π ∆
) 2
(
2 cos 2 cos
) (
0 2 0
t f J
P
t d v t P
A
D r
r rI
∆
=
∆
=
∆
∫
π
θ λ θ
π π
π
0
2 cos 2 sin
)
( 2
, 0
=
∆
=
∆t Pπ
∫
π πλv t θ dθAr r r
Q I
0
, ∆ →
∞
→
θ
N
λ 4 . 0
4 .
0 ⇒ ∆ =
=
∆t v t
fD
Antenna spacing of 0.4λ:
the signal decorrelates over a distance of 0.4λ
π θ
θ π θ
d e j e
x
Jn n 2 jxcos jn 2 0
) 1
( =
∫
Power Spectral Density
)]
2 ( [
) (
)]
( )
( [
25 . ) (
0
π
Dτ
r
c r
c r
r
f PJ
f S
f f
S f
f S f
S
I
I I
= F
+ +
−
=
f
c+f
Df
cS
r(f)
f
c-f
DEnvelope and Power Distributions without LOS
Signal envelope
−
− r
Iand r
Qare Gaussian random variables with mean zero and variance
− z(t) is Rayleigh distributed
■
Power
−
− The received signal power is exponentially distributed with mean
■
σ2
) ( )
( )
( )
( t r t r
2t r
2t
z = =
I+
Q0
, )
( 2
2
2
2 ≥
= z e− z
z p
z Z
σ σ
1
− x2 2
) ( )
( t r t
z =
2σ 2
Signal Envelope over Channel having a LOS
Signal envelope
− The received signal equals the superposition of a LOS component and a complex Gaussian component
−
The signal envelopez(t) has a Rician distribution.
Average received power
−
− Fading parameter :
■ K = 0: Rayleigh fading
■ K = ∞: no fading (only a LOS component)
■ the smaller K, the severer fading 0
, )
( 2 0 2
) ( 2
2 2 2
≥
=
− +
zs z I
z e z
p
s z
Z σ σ σ
2 2
0
2
( ) = + 2 σ
= ∫
∞x p x dx s
P
r ZLOS component power
NLOS component power
* I0: the modified Bessel function
2 2
2σ K = s
Nakagami Fading Channel
Nakagami fading distribution
− More general fading distribution whose parameters (m) can be adjusted to fit a variety of empirical measurements
−
m = 1: Rayleigh fading−
m = ∞: no fading−
: approximately Rician fading 5. 0
, )
( ) 2
(
2
1
2 ≥
= Γ − e− m
P m
z z m
p Pr
mz m
r m m Z
) 1 2
( ) 1
( + 2 +
= K K
m
Wideband Fading
Intersymbol Interference
Narrowband fading:
delay spread
-
There is little interference with a subsequentlytransmitted pulse
.
Wideband fading:
- The resolvable multipath components interfere with subsequently transmitted pulses:
τ
1 τ2 Bu2 1
1 −
τ
>>τ
T Tm >>
T Tm <<
Two multipath components with delay and are resolvable
if
Autocorrelation: Time Domain
Equivalent lowpass time-varying channel impulse response at time t to an impulse at time
−
: a complex zero-mean Gaussian random process The statistical characterization of is determined by its autocorrelation function
For the WSS channel, the autocorrelation is independent of t.
−
For the WSS channel with uncorrelated scattering
−
The channel response associated with a multipath component of delay is uncorrelated with the response associated with a component of adifferent delay because they are caused by different scatters.
−
)) ( (
) ( )
,
( ( )
) (
0
t e
t t
c j t n
t N
n n
n δ τ τ
α
τ = − φ −
∑
=−
τ
t) , ( t c
τ
)]
, ( ) , ( E[
) , , ,
( 1 2 t t c* 1 t c 2 t t
Ac τ τ ∆ = τ τ +∆
)]
, ( ) , ( E[
) , ,
( 1 2 t c* 1 t c 2 t t
Ac τ τ ∆ = τ τ +∆
τ
1 12
τ
τ
≠) , ( )
( ) , ( )]
, ( ) , (
E[c* τ1 t c τ2 t +∆t = Ac τ1 ∆t δ τ1 −τ2 = Ac τ ∆t
) (
τ
=τ
2 =τ
1Autocorrelation: Frequency Domain
Characteristics of the time-varying multipath channel at time t
−
in time domain:−
in frequency domain:■ A complex zero-mean Gaussian process
■ is completely characterized by its autocorrelation.
Autocorrelation of−
−
the WSS channel:−
) , ( t c
τ
τ τ t e πτd c
t f
C
∫
−∞∞ j f= ( , ) − 2
) , (
) , (f t C
) , (f t C
)]
, ( ) , ( E[
) , , ,
( f1 f2 t t C* f1 t C f2 t t
AC ∆ = +∆
)]
, ( ) , ( E[
) , ,
(f1 f2 t C* f1 t C f2 t t
AC ∆ = +∆
[ ]
) , (
) ,
( ) , ( E
) ,
( )
, ( E
) , , (
) ( 2
2 1 2
2 2
1
*
2 2
- 2 1 2
- 1
* 2
1
1 2
2 2 1
1
2 2 1
1
d e
t A
d d e
e t t c t c
d e
t t c d
e t c
t f f A
f f j c
f j f j
f j f
j C
∆
=
∆ +
=
+∆
=
∆
∞
−
∞ −
∞
−
−
∞ −
∞
−
∞
∞
−
∞ −
∞
∞
∞
∫
∫
∫ ∫
∫
∫
τ τ
τ τ τ
τ
τ τ
τ τ
τ π
τ π τ
π
τ π τ
π
Power Delay Profile
Power delay profile
−
− Average power associated with a given multipath delay
Delay spread
− Average delay spread:
− rms delay spread:
− the delay associated with a given multipath component is weighted by its relative power
The delay spread of the channel is roughly by the time delay T where
− : the system experiences significant ISI
− : ISI can be negligible
) 0 when
) , ( ( )]
, ( ) , ( E[
)
( = c* t c t A ∆t ∆t =
Ac τ τ τ c τ
τ
∫
∫
∞
∞
=
0 0
) (
) (
τ τ
τ τ µ τ
d A
d A
c c Tm
∫
∫
∞∞ −
=
0 0
2
) (
) ( )
(
τ τ
τ τ µ
σ τ
d A
d A
c
c T
T
m m
Relative power
T Ac(τ) ≈ 0 for τ ≥
) 10 (
m
m s T
T
s T
T <<σ <σ
) 10 (
m
m s T
T
s T
T >>σ > σ
Coherence Bandwidth (1)
−
describes the autocorrelation of the time-varying multipath channel in frequency domain (coherence)
Coherence bandwidth of the channel−
−
By the Fourier transform relationship between
Flat fading and frequency selective fading−
signal bandwidth: B−
Flat fading:■
−
Frequency selective fading:c C
c A f f B
B such that (∆ ) ≈0 for all∆ ≥ )]
, (
) , ( E[
)
( f C* f t C f f t
AC ∆ = +∆
) ( and )
( c τ
C f A
A ∆ T f
f A T
Ac( ) 0 for , then C( ) 0 for 1
if τ ≈ τ > ∆ ≈ ∆ >
Tm
c k
B ≈ 1T = σ
Bc
B <<
ISI negligible
1
1 >> ≈ ⇒
≈ c Tm
s B B
T σ
⇒
≈
<<
≈ σ c
B B >>
Coherence Bandwidth (2)
Coherence Time and Doppler Power Spectrum (1)
Time variation of the channel which arise from transmitter or receiver motion cause a Doppler shift
−
describe the autocorrelation of the channel at a frequency over the time (channel coherence over the time) Coherence time
−
Doppler power spectrum
−
−
ρ : Doppler shift−
Sc(ρ): the PSD of the received signal as a function of ρ
Doppler Spread: B)]
, ( ) , ( E[
)
( t C* f t C f t t
AC ∆ = +∆
c C
c A t t T
T such that (∆ ) ≈0 for ∆ ≥
t d e
t A
SC =
∫
−∞∞ C ∆ j t ∆∆
− πρ
ρ) ( ) 2
(
Coherence Time and Doppler Power Spectrum (2)
Relationship between the coherence time and the Doppler spread−
By the Fourier transform relationship between
If the transmitter and reflector are stationary and the receiver is moving with velocity v−
−
Remind that in the narrowband fading model the signal decorrelates over the time of 0.4/fD−
In general,
In summary,c C
c
C t t T S T
A ( ) 0 for , then ( ) 0 for 1
if ∆ ≈ ∆ > ρ ≈ ρ>
) ( and )
( C ρ
C t S
A ∆
c
D T
B ≈ 1
D
D v f
B ≤ λ = Maximum Doppler shift
).
( of shape on the
depends where
, C ρ
c
D k T k S
B ≈
D c
T
c T B
B
m
1
1 , ≈
≈ σ