Time Varying and Frequency Selective Radio Channel - KIT - IHE
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Transcript of Time Varying and Frequency Selective Radio Channel - KIT - IHE
www.ihe.kit.eduKIT – The Research University in the Helmholtz Association
INSTITUTE OF RADIO FREQUENCY ENGINEERING AND ELECTRONICS
Time Varying and Frequency Selective Radio ChannelAdvanced Radio Communication IProf. Dr.-Ing. Marwan Younis
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Small-Scale Fading & Large-Scal Fading
small-scale fading: receiver moving through a spatial interference pattern.large-scale fading: slow changes in the propagation environment.
3 Institute of Radio Frequency Engineering and Electronics
Multipath Effects
Multipath in the radio channel creates small-scale fading effects. This results in:
• rapid changes in signal strength over a small travel distanceor time interval
• frequency selectivity caused by multipath propagation delays• frequency modulation due to varying Doppler shifts on
different multipath signals
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Spatial and Temporal Variations
Consider a moving mobile station, a fixed base station and a staticenvironment, i.e. only the mobile receiver is moving. Then, the spatial
variations of the signal are seen as temporal variations by the receiver as it moves through the interference pattern
time or position
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and Electronics
Factors Influencing Small-Scale Fading
Channel Type:
• fixed-to-mobile
• line of sight (LOS) radio link
• satellite link
• stationary reception of TV/Radio
• …
Physical Factors:
• multipath propagation
• speed of the receiver
• speed of the surrounding objects
• signal bandwidth
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Advanced Radio Communication I
Small-Scale Fading
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Small-Scale Fading f(t)Larg-Scale Fading m(t)
The Components of Fading
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2-Dimensional Gaussian distribution for ℜ(#$) and ℑ(#$)
'ℑ(#$()
ℜ(#$()
#$)
*)
*$
#$
ℜ(#$)
'ℑ(#$)
Superposition of Multipath Signals
#$(
*(
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0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0 1 2 3 4 5 6 7 8 9 10 11 12 13 14
Ricean PDF with K=SRV=0 (Rayleigh)Ricean PDF with K=SRV=0.51Ricean PDF with K=SRV=5Ricean PDF with K=SRV=50 (≈Gauß)
prob
abilit
y de
nsity
func
tion
(PD
F) [1
/Vol
t]
Probability Density Funciton
magnitude of the open circuit voltage VR
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Advanced Radio Communication I
Large-Scale Fading (Log-Normal Fading)
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-230 -210 -190 -170 -150 -130 -110 -90 -70 -50
standard deviation in dB ≈ 26mean power in dBm ≈ -122
received power [dBm]
prob
abilit
y de
nsity
func
tion
(PD
F)
Log-Normal Fading
GSM1800 Coverage Simulation: Calculated Large-Scale PDF
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Question 1:Multi-Path creates small scale fading. What are the effects of fading?Question 2:Which physical factors (multipath, speed of Rx, movements of objects) are relevant for a satellite TV downlink?Question 3:What is the probability density function of the sum of a large number of independent random variables? Question 4:Which are the condition(s) to obtain a Rayleigh distribution for the magnitude of the Rx signal in a small-scale fading environment? Question 5:What does the Ricean factor K describe? Question 6:What probability density function describes large scale fading characterized
Questions
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Advanced Radio Communication I
Channel Transfer Function and Impulse Response
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Channel Transfer Function and Impulse Response
The channel, the input signal and the output signal are modeled as linear time variant. Then they are completely described in:• Time Domain (time variable t)• Frequency Domain (frequency variable f)
In the time domain the channel, the input signal and the output signal are realquantities. Further, there DC component must be 0.
r(τ ) = h(τ )∗ s(τ )
output channel input
R( f ) = H ( f ) ⋅S( f )
output channel input
t
convolution
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spectrum of equivalent baseband signal
real partimaginary part
C(Δf )
f
real partimaginary part
+f0-f0
spectrum of bandpass signal for positive frequencies
spectrum of bandpass signal for negative frequencies
H ( f ) for f > 0H ( f ) for f < 0
Bandpass and Equivalent Baseband Signals
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Channel Transfer Function and Impulse Response
The channel, the input signal and the output signal are modeled as linear time variant. Then they are completely described in:• Time Domain (time variable t)• Frequency Domain (frequency variable f)
Since all signals are band-limited (bandpass) the equivalent (complex) basebandrepresentation can be used (known as low-pass or complex envelope)
bandpass
equivalent baseband
€
r(τ) = h(τ )∗ s(τ)
v(τ) =12c(τ )∗ x(τ)
time domain
output channel input
€
R( f ) = H( f ) ⋅ S( f )
V (Δf ) =12C(Δf ) ⋅ X(Δf )
frequency domain
output channel input
t
t
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Channel Transfer Function and Impulse Response
H ( f ) R( f )S( f )
C(Δf ) V (Δf )X(Δf )
bandpass
equivalent baseband
h(τ ) = c(τ ) cos 2π f0τ +∠c(τ )( )
H ( f ) = 12C( f − f0 )+
12C*(− f − f0 )
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time
dom
ain
sign
al
time t in millisecond
Bandpass Signal and its Complex Envelope
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Characterization of the Frequency-Selective Channel
– Time Domain –
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and Electronics
Band-Limited Impulse Response Function
0.0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1.0
1.1
1.2
1.3
50 52 54 56 58 60 62 64 66 68 70
not bandlimited
ideal filter of bandwidth B=500kHzm
agnitude o
f equiv
ale
nt baseband r
esponse
time delay parameter t [µs]
Gaussian filter, B(-20dB)=500kHz
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Normalized Power Delay Profile
-35
-30
-25
-20
-15
-10
-5
0
50 52 54 56 58 60 62 64 66 68 70norm
aliz
ed p
ower
del
ay p
rofil
e [d
B]
time delay parameter ! [#$]
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Frequency-Selective Channel
The radio channel can be characterized:• in the time domain by the impulse response• in the frequency domain by the channel transfer function
In the time domain, the characterization is based on the powerdelay profile (PDP) function which describes the relative receivedpower as a function of the delay.
In order to compare different channels, parameters whichquantify the channel are utilized. The mean excess delay and theRMS delay spread are parameters determined directly from thePDP
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Characterization of the Frequency-Selective Channel
– Frequency Domain –
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BB Transfer Function and Correlation Bandwidth
normalized frequency ACF
1
0.37
|ACFf1(Df)|
B corr1
B corr2
B corr3
equivalent baseband transfer function
|C1( f)|
|ACFf2(Df)|
|C3( f)|
|C2( f)|
|ACFf3(Df)|
Δf
Bcorr2Bcorr3
Bcorr1 f
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Frequency-Selective Channel
In the frequency domain, the characterization is based on thefrequency autocorrelation function (ACF) which describes overwhich frequencies the channel is flat.
In order to compare different channels, parameters whichquantify the channel are utilized. The coherence or correlationbandwidth is a parameters determined directly from thefrequency ACF
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Relating the Channel to the Signal
normalized frequency ACFbaseband transfer function
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Characterization of the Time-Variant Channel
– Time Domain –
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Signal Envelope and Coherence Time
normalized temporal ACFtime-varying envelope
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Characterization of the Time-Variant Channel
In the time domain, the characterization is based on the temporalautocorrelation function (ACF) which describes how fast thechannel changes in time.
In order to compare different channels, parameters whichquantify the channel are utilized. The coherence or correlationtime is a parameters determined directly from the temporal ACF
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Characterization of the Time-Variant Channel
– Frequency Domain –
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Power Spectral Density (power Doppler Spectrum)
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Characterization of the Time-Variant Channel
In the frequency domain, the characterization is based on thePower Spectral Density (PSD) or power Doppler spectrum(function) which is the received power spectrum for a puresinusoidal transmitted signal.
In order to compare different channels, parameters whichquantify the channel are utilized. The Doppler spread is ameasure of the spectral broadening.
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Signal Envelope and Coherence Time
normalized temporal ACFtime-varying envelope
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Geometry for Multipath Wave Propagation
last scattering center formultipath signal i
αvR,i
receiver positionat time t
receiver position
at time t=0
vR t
Δs =| vR| cos(αvR,i) t
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Jakes Doppler Spectrum
-202468
10121416
-303691215182124
-250-200-150-100 -50 0 50 100 150 200 250
Jakes spectrum (linear)Jakes spectrum (in dB)
norm
aliz
ed J
akes
spe
ctru
m (l
inea
r)norm
alized Jakes spectrum [dB]
doppler frequency [Hz]