eecs 380: wireless communications weeks 3-4: propagation
DESCRIPTION
EECS 380: Wireless Communications Weeks 3-4: Propagation. Michael L. Honig Department of EECS Northwestern University. October 2009. Why Study Radio Propagation?. To determine coverage Must determine path loss Function of Frequency Distance - PowerPoint PPT PresentationTRANSCRIPT
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N O R T H W E S T E R NU N I V E R S I T Y MSIT | Master of Science in Information TechnologyDepartment of EECS
EECS 380: Wireless CommunicationsWeeks 3-4: Propagation
Michael L. HonigDepartment of EECS
Northwestern University
October 2009
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N O R T H W E S T E R NU N I V E R S I T Y MSIT | Master of Science in Information TechnologyDepartment of EECS
Why Study Radio Propagation?• To determine coverage
• Must determine path loss– Function of
• Frequency• Distance• Terrain (office building, urban, hilly, rural, etc.)
Need “large-scale” models
Can we use the samechannels?
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N O R T H W E S T E R NU N I V E R S I T Y MSIT | Master of Science in Information TechnologyDepartment of EECS
Why Study Radio Propagation?
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N O R T H W E S T E R NU N I V E R S I T Y MSIT | Master of Science in Information TechnologyDepartment of EECS
Why Study Radio Propagation?• To enable robust communications (MODEM design)
• How can we guarantee reliable communications?• What data rate can we provide?• Must determine signal statistics:
– Probability of outage– Duration of outage
Need “small-scale” models
Received Power
time
Deep fades may cause an outage
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N O R T H W E S T E R NU N I V E R S I T Y MSIT | Master of Science in Information TechnologyDepartment of EECS
Will provide answers to…
• What are the major causes of attenuation and fading?• Why does the achievable data rate decrease with
mobility?• Why are wireless systems evolving to wider
bandwidths (spread spectrum and OFDM)?• Why does the accuracy of location tracking methods
increase with wider bandwidths?
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N O R T H W E S T E R NU N I V E R S I T Y MSIT | Master of Science in Information TechnologyDepartment of EECS
Propagation Key Words• Large-scale effects
– Path-loss exponent– Shadow fading
• Small-scale effects– Rayleigh fading– Doppler shift and Doppler spectrum– Coherence time / fast vs slow fading
• Narrowband vs wideband signals• Multipath delay spread and coherence bandwidth• Frequency-selective fading and frequency diversity
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N O R T H W E S T E R NU N I V E R S I T Y MSIT | Master of Science in Information TechnologyDepartment of EECS
Propagation Mechanisms:1. Free Space
reference distance d0=1
distance d
Reference power at reference distance d0 Path loss exponent=2
In dB: Pr = P0 (dB) – 20 log (d)
Pr (dB)
log (d)
slope = -20 dB per decade
P0
0
P0 = Gt Gr (/4)2
antenna gains wavelength
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N O R T H W E S T E R NU N I V E R S I T Y MSIT | Master of Science in Information TechnologyDepartment of EECS
Wavelength
• Wavelength >> size of object signal penetrates object.
• Wavelength << size of object signal is absorbed and/or reflected by object.
• Large-scale effects refers to propagation over distances of many wavelengths.
Small-scale effects refers to propagation over a distances of a fraction of a wavelength.
(meters) = c (speed of light) / frequency
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N O R T H W E S T E R NU N I V E R S I T Y MSIT | Master of Science in Information TechnologyDepartment of EECS
Dipole Antenna
cable from transmitter
wire (radiator)
802.11 dipole antenna
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N O R T H W E S T E R NU N I V E R S I T Y MSIT | Master of Science in Information TechnologyDepartment of EECS
Radiation Pattern: Dipole Antenna
Dipole axisDipole axis
Electromagnetic wave radiates outfrom the dipole axis.
Cross-section of doughnut pattern
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N O R T H W E S T E R NU N I V E R S I T Y MSIT | Master of Science in Information TechnologyDepartment of EECS
Antenna Gain Pattern
Dipole pattern (close to isotropic)
Red curve shows the antenna gain versusangle relative to an isotropic pattern (perfect circle) in dB.
Often referred to as dBi, dB “isotropic”.
-5 dB (factor of about 1/3) relative to isotropicpattern
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N O R T H W E S T E R NU N I V E R S I T Y MSIT | Master of Science in Information TechnologyDepartment of EECS
Antenna Gain Pattern
Dipole pattern (vertical) 90 degree sector
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N O R T H W E S T E R NU N I V E R S I T Y MSIT | Master of Science in Information TechnologyDepartment of EECS
Attenuation: Wireless vs. Wired
• Path loss ~ 13 dB / 100 meters or 130 dB / 1 km– Increases linearly with
distance
• Requires repeaters for long distances
• Path loss ~ 30 dB for the first meter + 20 dB / decade– 70 dB / 100 meters
(2 decades)– 90 dB / 1 km
(3 decades)– 130 dB / 100 km!– Increases as log (distance)
• Repeaters are infeasible for satellites
Short distance Wired has less path loss.Large distance Wireless has less path loss.
Unshielded Twisted Pair 1 GHz Radio (free space)
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N O R T H W E S T E R NU N I V E R S I T Y MSIT | Master of Science in Information TechnologyDepartment of EECS
Propagation Mechanisms
2. Reflection
3. Diffraction
4. Scattering
Incident E-M wave
reflected wave
transmitted waveLength of boundary >> wavelength
Hill
Signal loss dependson geometry
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N O R T H W E S T E R NU N I V E R S I T Y MSIT | Master of Science in Information TechnologyDepartment of EECS
Why Use > 500 MHz?
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N O R T H W E S T E R NU N I V E R S I T Y MSIT | Master of Science in Information TechnologyDepartment of EECS
Why Use > 500 MHz?• There is more spectrum available above 500 MHz.• Lower frequencies require larger antennas
– Antenna dimension is on the order of awavelength = (speed of light/frequency) = 0.6 M @ 500 MHz
• Path loss increases with frequency for the first meter– 10’s of GHz: signals are confined locally– More than 60 GHz: attenuation is too large
(oxygen absorbs signal)
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N O R T H W E S T E R NU N I V E R S I T Y MSIT | Master of Science in Information TechnologyDepartment of EECS
700 MHz Auction• Broadcast TV channels 52-69 to be relocated in Feb. 2009.
– 6 MHz channels occupying 698 – 806 MHz
• Different bands were auctioned separately:– “A” and “B” bands: for exclusive use (like cellular bands)– “C” band (11 MHz): must support open handsets, software apps– “D” band (5 MHz): shared with public safety (has priority)
• Commenced January 24, 2008, ended in March
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N O R T H W E S T E R NU N I V E R S I T Y MSIT | Master of Science in Information TechnologyDepartment of EECS
Why all the Hubbub?• This band has excellent propagation characteristics for cellular
types of services (“beach-front property”).• Carriers must decide on technologies: 3G, LTE, WiMax,…• Rules for spectrum sharing can be redefined…
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N O R T H W E S T E R NU N I V E R S I T Y MSIT | Master of Science in Information TechnologyDepartment of EECS
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N O R T H W E S T E R NU N I V E R S I T Y MSIT | Master of Science in Information TechnologyDepartment of EECS
C Band Debate• Currently service providers in the U.S. do not allow any services,
applications, or handsets from unauthorized 3rd party vendors.
• Google asked the FCC to stipulate that whoever wins the spectrum must support open applications, open devices, open services, open networks (net neutrality for wireless).
• Verizon wants to maintain “walled-garden”.
• FCC stipulated open applications and devices, but not open services and networks: spectrum owner must allow devices or applications to connect to the network as long as they do not cause harm to the network
• Aggressive build-out requirements:– Significant coverage requirement in four years, which continues to
grow throughout the 10-year term of the license.
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N O R T H W E S T E R NU N I V E R S I T Y MSIT | Master of Science in Information TechnologyDepartment of EECS
Sold to…
• Verizon
• Other winners: AT&T (B block), Qualcomm (B, E blocks)
• Total revenue: $19.6 B– $9.6 B from Verizon, $6.6 B from AT&T
• Implications for open access, competition?
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N O R T H W E S T E R NU N I V E R S I T Y MSIT | Master of Science in Information TechnologyDepartment of EECS
D Band Rules
• Winner gets to use both D band and adjacent public service band (additional 12 MHz!), but service can be preempted by public safety in emergencies.
• Winner must build out public safety network:must provide service to 75% of the population in 4 years, 95% in 7 years, 99.3% in 10 years
• Minimum bid: $1.3 B; estimated cost to deploy network: $10-12 B
• Any takers? …
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N O R T H W E S T E R NU N I V E R S I T Y MSIT | Master of Science in Information TechnologyDepartment of EECS
D Band Rules
• Winner gets to use both D band and adjacent public service band (additional 12 MHz!), but service can be preempted by public safety in emergencies.
• Winner must build out public safety network:must provide service to 75% of the population in 4 years, 95% in 7 years, 99.3% in 10 years
• Minimum bid: $1.3 B; estimated cost to deploy network: $10-12 B
• Any takers? … Nope! Highest bid was well below reserve…
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N O R T H W E S T E R NU N I V E R S I T Y MSIT | Master of Science in Information TechnologyDepartment of EECS
Radio Channels
Troposcatter Microwave LOS
Mobile radio Indoor radio
T
T
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N O R T H W E S T E R NU N I V E R S I T Y MSIT | Master of Science in Information TechnologyDepartment of EECS
Two Signal Paths
s1(t)
s2(t)
Received signal r(t) = s1(t) + s2(t)
Suppose s1(t) = sin 2f t.Then s2(t) = h s1(t - ) = h sin 2f (t - )
attenuation(e.g., h could be ½)
delay(e.g., could be 1 microsec.)
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N O R T H W E S T E R NU N I V E R S I T Y MSIT | Master of Science in Information TechnologyDepartment of EECS
Sinusoid Addition (Constructive)
+ =
s1(t)
s2(t)
r(t)
Adding two sinusoids with the same frequency gives another sinusoid with the same frequency!
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N O R T H W E S T E R NU N I V E R S I T Y MSIT | Master of Science in Information TechnologyDepartment of EECS
Sinusoid Addition (Destructive)
+ =
Signal is faded.
s1(t)
s2(t)
r(t)
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N O R T H W E S T E R NU N I V E R S I T Y MSIT | Master of Science in Information TechnologyDepartment of EECS
Indoor Propagation Measurements
Hypothetical large indoor environment
Ceiling
Normalized received power vs. distance
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N O R T H W E S T E R NU N I V E R S I T Y MSIT | Master of Science in Information TechnologyDepartment of EECS
Power Attenuation
In dB: Pr = P0 (dB) – 10 n log (d)
reference distance d0=1
distance d
Reference power at reference distance d0Path loss exponent
Pr (dB)
log (d)
slope (n=2) = -20 dB per decadeP0
0
slope = -40(n=4)
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N O R T H W E S T E R NU N I V E R S I T Y MSIT | Master of Science in Information TechnologyDepartment of EECS
Path Loss Exponents
ENVIRONMENT PATH LOSS EXPONENT, n
Free space 2
Urban cellular radio 2.7 to 3.5
Shadowed urban cellular radio 3 to 5
In building line-of-site 1.6 to 1.8
Obstructed in building 4 to 6
Obstructed in factories 2 to 3
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N O R T H W E S T E R NU N I V E R S I T Y MSIT | Master of Science in Information TechnologyDepartment of EECS
Large-Scale Path Loss (Scatter Plot)
Ave
rage
Rec
eive
d P
ower
(dB
m)
Distance (meters)
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N O R T H W E S T E R NU N I V E R S I T Y MSIT | Master of Science in Information TechnologyDepartment of EECS
Shadow Fading
• Random variations in path loss as mobile moves around buildings, trees, etc.
• Modeled as an additional random variable:
Pr = P0 – 10 n log d + X
“log-normal” random variablestandard deviation
received power in dB
“normal” (Gaussian)probability distribution
For cellular: is about 8 dB
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N O R T H W E S T E R NU N I V E R S I T Y MSIT | Master of Science in Information TechnologyDepartment of EECS
Large-Scale Path Loss (Scatter Plot)
Most points are less thandB from the mean
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N O R T H W E S T E R NU N I V E R S I T Y MSIT | Master of Science in Information TechnologyDepartment of EECS
Empirical Path Loss Models• Propagation studies must take into account:
– Environment (rural, suburban, urban)– Building characteristics (high-rise, houses, shopping malls)– Vegetation density– Terrain (mountainous, hilly, flat)
• Okumura’s model (based on measurements in and around Tokyo)– Median path loss =
free-space loss + urban loss + antenna gains + corrections– Obtained from graphs– Additional corrections for street orientation, irregular terrain
• Numerous indoor propagation studies for 802.11
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N O R T H W E S T E R NU N I V E R S I T Y MSIT | Master of Science in Information TechnologyDepartment of EECS
SINR Measurements: 1xEV-DO
drive test plots
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N O R T H W E S T E R NU N I V E R S I T Y MSIT | Master of Science in Information TechnologyDepartment of EECS
Link Budget How much power is required to achieve target S/I?
• dBs add:
Target S/I (dB) + path loss (dB) + other losses (components) (dB) - antenna gains (dB)
Total Power needed at transmitter (dB)
• Actual power depends on noise level.– Given 1 microwatt noise power, if the transmit power is 60 dB above the noise level
then the transmit power is 1 Watt.
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N O R T H W E S T E R NU N I V E R S I T Y MSIT | Master of Science in Information TechnologyDepartment of EECS
Example
• Recall that dBm measures the signal power relative to 1 mW (milliwatt) = 0.001 Watt. To convert from S Watts to dBm, use S (dBm) = 10 log (S / 0.001)
• Transmitted power (dBm) = -30 + 40 = 10 dBm = 10 mW
• What if the received signal-to-noise ratio must be 5 dB, and the noise power is -45 dBm?
Transmitter Receiverwireless channel
40 dB attenuationReceived powermust be > -30 dBm
What is the requiredTransmit power?
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N O R T H W E S T E R NU N I V E R S I T Y MSIT | Master of Science in Information TechnologyDepartment of EECS
Urban Multipath
• No direct Line of Sight between mobile and base• Radio wave scatters off of buildings, cars, etc.• Severe multipath
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N O R T H W E S T E R NU N I V E R S I T Y MSIT | Master of Science in Information TechnologyDepartment of EECS
Narrowband vs. Wideband
• Narrowband means that the bandwidth of the transmitted signal is small (e.g., < 100 kHz for cellular). It therefore looks “almost” like a sinusoid.– Multipath changes the amplitude and phase.
• Wideband means that the transmitted signal has a large bandwidth (e.g., > 1 MHz for cellular).– Multipath causes “self-interference”.
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N O R T H W E S T E R NU N I V E R S I T Y MSIT | Master of Science in Information TechnologyDepartment of EECS
Narrowband FadingReceived signal r(t) = h1 s(t - 1 ) + h2 s(t - 2) + h3 s(t - 3 ) + …
attenuationfor path 1 (random) delay for path 1 (random)
If the transmitted signal is sinusoidal (narrowband), s(t) = sin 2f t,
then the received signal is also sinusoidal, but with a different(random) amplitude and (random) phase:
r(t) = A sin (2f t + )
A, depend on environment, location of transmitter/receiver
Transmitted s(t) Received r(t)
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N O R T H W E S T E R NU N I V E R S I T Y MSIT | Master of Science in Information TechnologyDepartment of EECS
Rayleigh FadingCan show:
A has a “Rayleigh” distribution has a “uniform” distribution
(all phase shifts are equally likely)
Probability (A < a) = 1 – e-a2/P0
where P0 is the average received power (averaged over different locations)
Ex: P0 =1, a=1: Pr(A<1) = 1 – e-1 = 0.63 (probability that signal is faded)
P0 = 1, a=0.1: Pr(A<0.1) = 1 – e-1/100 ≈ 0.01 (prob that signal is severely faded)
a
Prob(A < a)
11-e-a2/P0
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N O R T H W E S T E R NU N I V E R S I T Y MSIT | Master of Science in Information TechnologyDepartment of EECS
Small-Scale Fading
a = 0.1
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N O R T H W E S T E R NU N I V E R S I T Y MSIT | Master of Science in Information TechnologyDepartment of EECS
Small-Scale Fading
Fade rate depends on• Mobile speed• Speed of surrounding objects• Frequency
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N O R T H W E S T E R NU N I V E R S I T Y MSIT | Master of Science in Information TechnologyDepartment of EECS
Short- vs. Long-Term Fading
Long-term (large-scale) fading:• Distance attenuation
• Shadowing (blocked Line of Sight (LOS))
• Variations of signal strength over distances on the order of a wavelength
Time (t)
Sig
nal S
treng
th (d
B)
T T
Short-term fading
Long-term fading
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N O R T H W E S T E R NU N I V E R S I T Y MSIT | Master of Science in Information TechnologyDepartment of EECS
Combined Fading and Attenuation
Time (mobile is moving away from base)
Received powerPr (dB)
distance attenuation
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N O R T H W E S T E R NU N I V E R S I T Y MSIT | Master of Science in Information TechnologyDepartment of EECS
Combined Fading and Attenuation
Time (mobile is moving away from base)
shadowing
Received powerPr (dB) distance attenuation
![Page 47: EECS 380: Wireless Communications Weeks 3-4: Propagation](https://reader036.vdocuments.mx/reader036/viewer/2022062521/5681684a550346895dde389e/html5/thumbnails/47.jpg)
N O R T H W E S T E R NU N I V E R S I T Y MSIT | Master of Science in Information TechnologyDepartment of EECS
Combined Fading and Attenuation
Time (mobile is moving away from base)
shadowing
Received powerPr (dB)
distance attenuation
Rayleigh fading
![Page 48: EECS 380: Wireless Communications Weeks 3-4: Propagation](https://reader036.vdocuments.mx/reader036/viewer/2022062521/5681684a550346895dde389e/html5/thumbnails/48.jpg)
N O R T H W E S T E R NU N I V E R S I T Y MSIT | Master of Science in Information TechnologyDepartment of EECS
Example Diagnostic Measurements: 1XEV-DO
drive test measurements
drive path
![Page 49: EECS 380: Wireless Communications Weeks 3-4: Propagation](https://reader036.vdocuments.mx/reader036/viewer/2022062521/5681684a550346895dde389e/html5/thumbnails/49.jpg)
N O R T H W E S T E R NU N I V E R S I T Y MSIT | Master of Science in Information TechnologyDepartment of EECS
Time Variations: Doppler Shift
Audio clip (train station)
![Page 50: EECS 380: Wireless Communications Weeks 3-4: Propagation](https://reader036.vdocuments.mx/reader036/viewer/2022062521/5681684a550346895dde389e/html5/thumbnails/50.jpg)
N O R T H W E S T E R NU N I V E R S I T Y MSIT | Master of Science in Information TechnologyDepartment of EECS
Time Variations: Doppler Shift
Propagation delay = distance d / speed of light c = vt/c
Received signal r(t) = sin 2f (t- vt/c) = sin 2(f – fv/c) t
velocity v
distance d = v t
transmittedsignal s(t)
receivedsignal r(t)
propagationdelay
received frequencyDoppler shift fd = -fv/c
delay increases
![Page 51: EECS 380: Wireless Communications Weeks 3-4: Propagation](https://reader036.vdocuments.mx/reader036/viewer/2022062521/5681684a550346895dde389e/html5/thumbnails/51.jpg)
N O R T H W E S T E R NU N I V E R S I T Y MSIT | Master of Science in Information TechnologyDepartment of EECS
Doppler Shift (Ex)Mobile moving away from base v > 0, Doppler shift < 0Mobile moving towards base v < 0, Doppler shift > 0
Carrier frequency f = 900 MHz, v = 60 miles/hour = 26.82 meters/sec
Mobile Base: fd = fv/c = (900 × 106) × 26.82 / (3 × 108) ≈ 80 Hzmeters/sec
![Page 52: EECS 380: Wireless Communications Weeks 3-4: Propagation](https://reader036.vdocuments.mx/reader036/viewer/2022062521/5681684a550346895dde389e/html5/thumbnails/52.jpg)
N O R T H W E S T E R NU N I V E R S I T Y MSIT | Master of Science in Information TechnologyDepartment of EECS
Doppler (Frequency) Shift
Frequency= 1/50 Frequency= 1/45
in phase out of phase
½ Doppler “cycle”
![Page 53: EECS 380: Wireless Communications Weeks 3-4: Propagation](https://reader036.vdocuments.mx/reader036/viewer/2022062521/5681684a550346895dde389e/html5/thumbnails/53.jpg)
N O R T H W E S T E R NU N I V E R S I T Y MSIT | Master of Science in Information TechnologyDepartment of EECS
Doppler Shift (Ex)Mobile moving away from base v > 0, Doppler shift < 0Mobile moving towards base v < 0, Doppler shift > 0
Carrier frequency f = 900 MHz, v = 60 miles/hour = 26.82 meters/sec
Mobile Base: fd = fv/c = (900 × 106) × 26.82 / (3 × 108) ≈ 80 Hz
Suppose the data rate is 9600 bits/sec, 80 Hz Doppler shift phase inversion every (9600/80)/2 = 60 bits!
As the data rate increases, Doppler shift becomes less significant, i.e., channel is stable over more transmitted bits.
IS-136 data rate: 48.6 kbps GSM data rate 270 kbps
![Page 54: EECS 380: Wireless Communications Weeks 3-4: Propagation](https://reader036.vdocuments.mx/reader036/viewer/2022062521/5681684a550346895dde389e/html5/thumbnails/54.jpg)
N O R T H W E S T E R NU N I V E R S I T Y MSIT | Master of Science in Information TechnologyDepartment of EECS
Application of Doppler Shift: Astronomy
Astronomy:used to determineRelative velocity ofDistant objects(e.g., stars, galaxies…)
“red shift”: objectis moving away
“blue shift” objectis moving closer
sun light spectrum spectrum of galaxy supercluster
Observed “spectral lines”(radiation is emittedat discrete frequencies)
![Page 55: EECS 380: Wireless Communications Weeks 3-4: Propagation](https://reader036.vdocuments.mx/reader036/viewer/2022062521/5681684a550346895dde389e/html5/thumbnails/55.jpg)
N O R T H W E S T E R NU N I V E R S I T Y MSIT | Master of Science in Information TechnologyDepartment of EECS
Application of Doppler Shift: Police Radar
Doppler shift can be used to compute relative speed.
![Page 56: EECS 380: Wireless Communications Weeks 3-4: Propagation](https://reader036.vdocuments.mx/reader036/viewer/2022062521/5681684a550346895dde389e/html5/thumbnails/56.jpg)
N O R T H W E S T E R NU N I V E R S I T Y MSIT | Master of Science in Information TechnologyDepartment of EECS
Scattering: Doppler Spectrum
distance d = v t
transmittedsignal s(t)
• Received signal is the sum of all scattered waves
• Doppler shift for each path depends on angle (vf cos c )
• Typically assume that the received energy is the same from all directions (uniform scattering)
receivedsignal ??
freq.
power
frequency of s(t)
![Page 57: EECS 380: Wireless Communications Weeks 3-4: Propagation](https://reader036.vdocuments.mx/reader036/viewer/2022062521/5681684a550346895dde389e/html5/thumbnails/57.jpg)
N O R T H W E S T E R NU N I V E R S I T Y MSIT | Master of Science in Information TechnologyDepartment of EECS
Scattering: Doppler Spectrum
distance d = v t
transmittedsignal s(t)
frequency
power
frequency of s(t) frequency
power
frequency of s(t) + Doppler shift fd
Doppler shift fd
2fd
Doppler Spectrum(shows relative strengths of Doppler shifts)
![Page 58: EECS 380: Wireless Communications Weeks 3-4: Propagation](https://reader036.vdocuments.mx/reader036/viewer/2022062521/5681684a550346895dde389e/html5/thumbnails/58.jpg)
N O R T H W E S T E R NU N I V E R S I T Y MSIT | Master of Science in Information TechnologyDepartment of EECS
Scattering: Doppler Spectrum
distance d = v t
transmittedsignal s(t)
frequency
power
frequency of s(t)
power
frequency of s(t) + Doppler shift fd
Doppler spectrum
2fd
![Page 59: EECS 380: Wireless Communications Weeks 3-4: Propagation](https://reader036.vdocuments.mx/reader036/viewer/2022062521/5681684a550346895dde389e/html5/thumbnails/59.jpg)
N O R T H W E S T E R NU N I V E R S I T Y MSIT | Master of Science in Information TechnologyDepartment of EECS
Rayleigh Fading
phase shiftdeep fade
Received waveform Amplitude (dB)
![Page 60: EECS 380: Wireless Communications Weeks 3-4: Propagation](https://reader036.vdocuments.mx/reader036/viewer/2022062521/5681684a550346895dde389e/html5/thumbnails/60.jpg)
N O R T H W E S T E R NU N I V E R S I T Y MSIT | Master of Science in Information TechnologyDepartment of EECS
Channel Coherence Time
Coherence Time: Amplitude and phase are nearly constant.
• Rate of time variations depends on Doppler shift: (velocity X carrier frequency)/(speed of light)
• Coherence Time varies as 1/(Doppler shift).
![Page 61: EECS 380: Wireless Communications Weeks 3-4: Propagation](https://reader036.vdocuments.mx/reader036/viewer/2022062521/5681684a550346895dde389e/html5/thumbnails/61.jpg)
N O R T H W E S T E R NU N I V E R S I T Y MSIT | Master of Science in Information TechnologyDepartment of EECS
Fast vs. Slow Fading
Fast fading: channel changes every few symbols. Coherence timeis less than roughly 100 symbols.
Slow fading: Coherence timelasts more than a few 100 symbols.
timetime
rece
ived
am
plitu
de
transmitted bits
![Page 62: EECS 380: Wireless Communications Weeks 3-4: Propagation](https://reader036.vdocuments.mx/reader036/viewer/2022062521/5681684a550346895dde389e/html5/thumbnails/62.jpg)
N O R T H W E S T E R NU N I V E R S I T Y MSIT | Master of Science in Information TechnologyDepartment of EECS
Fade Rate (Ex)• fc = 900 MHz, v = 60 miles/hour
Doppler shift ≈ 80 Hz.Coherence time is roughly 1/80, or 10 msec
• Data rate (voice): 10 kbps or 0.1 msec/bit 100 bits within a coherence time (fast fading)
• GSM data rate: 270 kbps about 3000 bits within a coherence time (slow fading)
![Page 63: EECS 380: Wireless Communications Weeks 3-4: Propagation](https://reader036.vdocuments.mx/reader036/viewer/2022062521/5681684a550346895dde389e/html5/thumbnails/63.jpg)
N O R T H W E S T E R NU N I V E R S I T Y MSIT | Master of Science in Information TechnologyDepartment of EECS
Channel Characterizations:Time vs. Frequency
• Frequency-domain description
• Time-domain description
Multipathchannel
input s(t) is a sinusoid“narrowband” signal
Amplitude attenuation,Delay (phase shift)
Multipathchannel
input s(t) is an impulse (very short pulse)“wideband” signal(Note: an impulse has zero duration and infinite bandwidth!)
time t
s(t)time t
r(t)
multipath components
![Page 64: EECS 380: Wireless Communications Weeks 3-4: Propagation](https://reader036.vdocuments.mx/reader036/viewer/2022062521/5681684a550346895dde389e/html5/thumbnails/64.jpg)
N O R T H W E S T E R NU N I V E R S I T Y MSIT | Master of Science in Information TechnologyDepartment of EECS
Pulse Width vs. Bandwidth
frequency
Powerbandwidth = 1/T
frequency
Powerbandwidth = 1/T
time
signal pulse
time
signal pulse
T
T
Narrowband
Wideband
![Page 65: EECS 380: Wireless Communications Weeks 3-4: Propagation](https://reader036.vdocuments.mx/reader036/viewer/2022062521/5681684a550346895dde389e/html5/thumbnails/65.jpg)
N O R T H W E S T E R NU N I V E R S I T Y MSIT | Master of Science in Information TechnologyDepartment of EECS
Power-Delay Profile
delay spread
Received power vs. time in response to a transmitted short pulse.
For cellular systems (outdoors), the delay spread is typically afew microseconds.
![Page 66: EECS 380: Wireless Communications Weeks 3-4: Propagation](https://reader036.vdocuments.mx/reader036/viewer/2022062521/5681684a550346895dde389e/html5/thumbnails/66.jpg)
N O R T H W E S T E R NU N I V E R S I T Y MSIT | Master of Science in Information TechnologyDepartment of EECS
Two-Ray Impulse Response
direct path (path 1)
reflection (path 2)
time t
s(t)
time t
r(t) reflection is attenuated
![Page 67: EECS 380: Wireless Communications Weeks 3-4: Propagation](https://reader036.vdocuments.mx/reader036/viewer/2022062521/5681684a550346895dde389e/html5/thumbnails/67.jpg)
N O R T H W E S T E R NU N I V E R S I T Y MSIT | Master of Science in Information TechnologyDepartment of EECS
Two-Ray Impulse Response
direct path (path 1)
reflection (path 2)
= [(length of path 2) – (length of path 1)]/c
time t
s(t)
time t
r(t) reflection is attenuated
![Page 68: EECS 380: Wireless Communications Weeks 3-4: Propagation](https://reader036.vdocuments.mx/reader036/viewer/2022062521/5681684a550346895dde389e/html5/thumbnails/68.jpg)
N O R T H W E S T E R NU N I V E R S I T Y MSIT | Master of Science in Information TechnologyDepartment of EECS
Urban Multipath
time t time t
s(t)r(t)
time t
r(t)different locationfor receiver
Spacing and attenuation of multipath components depend onlocation and environment.
![Page 69: EECS 380: Wireless Communications Weeks 3-4: Propagation](https://reader036.vdocuments.mx/reader036/viewer/2022062521/5681684a550346895dde389e/html5/thumbnails/69.jpg)
N O R T H W E S T E R NU N I V E R S I T Y MSIT | Master of Science in Information TechnologyDepartment of EECS
Delay Spread and Intersymbol Interference
Multipathchanneltime t
s(t)
time t
r(t)
Multipathchannel
r(t)
Time between pulses is >> delay spread, therefore the receivedpulses do not interfere.
Time between pulses is < delay spread, which causesintersymbol interference. The rate at which symbols can betransmitted without intersymbol interference is 1 / delay spread.
s(t)time t
![Page 70: EECS 380: Wireless Communications Weeks 3-4: Propagation](https://reader036.vdocuments.mx/reader036/viewer/2022062521/5681684a550346895dde389e/html5/thumbnails/70.jpg)
N O R T H W E S T E R NU N I V E R S I T Y MSIT | Master of Science in Information TechnologyDepartment of EECS
Coherence Bandwidth
frequency
channelgain
The channel gain is approximately constant within a coherence bandwidth Bc. Frequencies f1 and f2 fade independently if | f1 – f2 | >> Bc.
If the signal bandwidth < coherence bandwidth Bc, then the channel is called flat fading, and the transmitted signal is regarded as narrowband.
If the signal bandwidth > Bc, then the channel is called frequency-selective and the signal is regarded as wideband.
coherence bandwidth Bc
f1 f2
Frequencies far outside the coherencebandwidth are affected differently by multipath.
![Page 71: EECS 380: Wireless Communications Weeks 3-4: Propagation](https://reader036.vdocuments.mx/reader036/viewer/2022062521/5681684a550346895dde389e/html5/thumbnails/71.jpg)
N O R T H W E S T E R NU N I V E R S I T Y MSIT | Master of Science in Information TechnologyDepartment of EECS
Coherence Bandwidth and Diversity
frequency
channelgain
Frequency-selective fading: different parts of the signal (in frequency)are affected differently by fading.
coherence bandwidth Bc
f1 f2
Frequencies far outside the coherencebandwidth are affected differently by multipath.
signal power(wideband)
![Page 72: EECS 380: Wireless Communications Weeks 3-4: Propagation](https://reader036.vdocuments.mx/reader036/viewer/2022062521/5681684a550346895dde389e/html5/thumbnails/72.jpg)
N O R T H W E S T E R NU N I V E R S I T Y MSIT | Master of Science in Information TechnologyDepartment of EECS
Coherence Bandwidth and Diversity
frequency
channelgain
Frequency-selective fading: different parts of the signal (in frequency)are affected differently by fading.
Wideband signals exploit frequency diversity. Spreading power across many coherence bands reduces the chances of severe fading.
Wideband signals are distorted by the channel fading (distortion causesIntersymbol interference).
coherence bandwidth Bc
f1 f2
Frequencies far outside the coherencebandwidth are affected differently by multipath.
signal power(wideband)
![Page 73: EECS 380: Wireless Communications Weeks 3-4: Propagation](https://reader036.vdocuments.mx/reader036/viewer/2022062521/5681684a550346895dde389e/html5/thumbnails/73.jpg)
N O R T H W E S T E R NU N I V E R S I T Y MSIT | Master of Science in Information TechnologyDepartment of EECS
Narrowband Signal
frequency
channelgain
Flat fading: the narrowband signal fades uniformly, hence does not benefit from frequency diversity.
coherence bandwidth Bc
f1 f2
Frequencies far outside the coherencebandwidth are affected differently by multipath.
signal power(narrowband)
For the cellular band, Bc is around 100 to 300 kHz.How does this compare with the bandwidth of cellular systems?
![Page 74: EECS 380: Wireless Communications Weeks 3-4: Propagation](https://reader036.vdocuments.mx/reader036/viewer/2022062521/5681684a550346895dde389e/html5/thumbnails/74.jpg)
N O R T H W E S T E R NU N I V E R S I T Y MSIT | Master of Science in Information TechnologyDepartment of EECS
Coherence Bandwidth and Delay Spread
delay spread
frequency
channelgain
coherence bandwidth Bc
Coherence bandwidth is inversely proportional to delay spread:Bc ≈ 1/
frequency
channelgain
coherence bandwidth Bc
delay spread
![Page 75: EECS 380: Wireless Communications Weeks 3-4: Propagation](https://reader036.vdocuments.mx/reader036/viewer/2022062521/5681684a550346895dde389e/html5/thumbnails/75.jpg)
N O R T H W E S T E R NU N I V E R S I T Y MSIT | Master of Science in Information TechnologyDepartment of EECS
Pulse Width vs. Bandwidth
frequency
Powerbandwidth = 1/T
frequency
Powerbandwidth = 1/T
time
signal pulse
time
signal pulse
T
T
Narrowband
Wideband
![Page 76: EECS 380: Wireless Communications Weeks 3-4: Propagation](https://reader036.vdocuments.mx/reader036/viewer/2022062521/5681684a550346895dde389e/html5/thumbnails/76.jpg)
N O R T H W E S T E R NU N I V E R S I T Y MSIT | Master of Science in Information TechnologyDepartment of EECS
Bandwidth and Multipath Resolution
direct path (path 1)
reflection (path 2)
signal pulse
Narrow bandwidth low resolutionReceiver cannot distinguish the two paths.
signal pulse
Wide bandwidth high resolutionReceiver can clearly distinguish two paths.
multipath components are resolvable
(delay spread)
T
T < T >
![Page 77: EECS 380: Wireless Communications Weeks 3-4: Propagation](https://reader036.vdocuments.mx/reader036/viewer/2022062521/5681684a550346895dde389e/html5/thumbnails/77.jpg)
N O R T H W E S T E R NU N I V E R S I T Y MSIT | Master of Science in Information TechnologyDepartment of EECS
Bandwidth and Multipath Resolution
direct path (path 1)
reflection (path 2)
signal pulse
Wide bandwidth high resolutionReceiver can clearly distinguish two paths.
multipath components are resolvable
The receiver can easily distinguish the two paths provided that they are separated by much morethan the pulse width . Since the signal bandwidthB ≈ 1/, this implies B >> 1/or B >> Bc ..
![Page 78: EECS 380: Wireless Communications Weeks 3-4: Propagation](https://reader036.vdocuments.mx/reader036/viewer/2022062521/5681684a550346895dde389e/html5/thumbnails/78.jpg)
N O R T H W E S T E R NU N I V E R S I T Y MSIT | Master of Science in Information TechnologyDepartment of EECS
Multipath Resolution and Diversity
direct path (path 1)
reflection (path 2)
signal pulse
Wide bandwidth high resolutionReceiver can clearly distinguish two paths.
multipath components are resolvable
Each path may undergo independent fading (i.e., due to Doppler). If one path is faded, the receiver may be able to detect the other path.
In the frequency domain, this corresponds to independent fading in different coherence bands.
![Page 79: EECS 380: Wireless Communications Weeks 3-4: Propagation](https://reader036.vdocuments.mx/reader036/viewer/2022062521/5681684a550346895dde389e/html5/thumbnails/79.jpg)
N O R T H W E S T E R NU N I V E R S I T Y MSIT | Master of Science in Information TechnologyDepartment of EECS
Fading Experienced by Wireless Systems
Standard Flat/Freq.-Sel. Fast/Slow
AMPS Flat FastIS-136 Flat FastGSM F-S SlowIS-95 (CDMA) F-S Fast3G F-S Slow to Fast
(depends on rate)802.11 F-S SlowBluetooth F-S Slow
![Page 80: EECS 380: Wireless Communications Weeks 3-4: Propagation](https://reader036.vdocuments.mx/reader036/viewer/2022062521/5681684a550346895dde389e/html5/thumbnails/80.jpg)
N O R T H W E S T E R NU N I V E R S I T Y MSIT | Master of Science in Information TechnologyDepartment of EECS
Radar Pulse Bandwidth
time t
r(t)
s(t)
delay = 2 x distance/c
reflection
time t
r(t)
s(t)
delay
Narrow bandwidth pulseHigh bandwidth pulse
![Page 81: EECS 380: Wireless Communications Weeks 3-4: Propagation](https://reader036.vdocuments.mx/reader036/viewer/2022062521/5681684a550346895dde389e/html5/thumbnails/81.jpg)
N O R T H W E S T E R NU N I V E R S I T Y MSIT | Master of Science in Information TechnologyDepartment of EECS
Bandwidth and Resolution
time t
r(t)
s(t)
delay = 2 x distance/c
The resolution of the delay measurement is roughly the width of the pulse.
Low bandwidth wide pulse low resolutionHigh bandwidth narrow pulse high resolution
If the delay measurement changes by 1 microsec, the distance erroris c x 10-6/2 = 150 meters!
reflection
![Page 82: EECS 380: Wireless Communications Weeks 3-4: Propagation](https://reader036.vdocuments.mx/reader036/viewer/2022062521/5681684a550346895dde389e/html5/thumbnails/82.jpg)
N O R T H W E S T E R NU N I V E R S I T Y MSIT | Master of Science in Information TechnologyDepartment of EECS
Propagation and Handoff
ReceivedSignal Strength (RSS)
from left BST
from right BST
unacceptable(call is dropped)
time
![Page 83: EECS 380: Wireless Communications Weeks 3-4: Propagation](https://reader036.vdocuments.mx/reader036/viewer/2022062521/5681684a550346895dde389e/html5/thumbnails/83.jpg)
N O R T H W E S T E R NU N I V E R S I T Y MSIT | Master of Science in Information TechnologyDepartment of EECS
Propagation and Handoff
ReceivedSignal Strength (RSS)
from left BST
from right BST
unacceptable(call is dropped)
time
with handoffhandoff threshold
![Page 84: EECS 380: Wireless Communications Weeks 3-4: Propagation](https://reader036.vdocuments.mx/reader036/viewer/2022062521/5681684a550346895dde389e/html5/thumbnails/84.jpg)
N O R T H W E S T E R NU N I V E R S I T Y MSIT | Master of Science in Information TechnologyDepartment of EECS
Propagation and Handoff
ReceivedSignal Strength (RSS)
from left BST
from right BST
unacceptable(call is dropped)
time
with handoffhandoff threshold
time needed for handoff
RSS margin
![Page 85: EECS 380: Wireless Communications Weeks 3-4: Propagation](https://reader036.vdocuments.mx/reader036/viewer/2022062521/5681684a550346895dde389e/html5/thumbnails/85.jpg)
N O R T H W E S T E R NU N I V E R S I T Y MSIT | Master of Science in Information TechnologyDepartment of EECS
Propagation and Handoff
ReceivedSignal Strength (RSS)
from left BST
from right BST
unacceptable(call is dropped)
time
handoff threshold
time needed for handoff
RSS margin
![Page 86: EECS 380: Wireless Communications Weeks 3-4: Propagation](https://reader036.vdocuments.mx/reader036/viewer/2022062521/5681684a550346895dde389e/html5/thumbnails/86.jpg)
N O R T H W E S T E R NU N I V E R S I T Y MSIT | Master of Science in Information TechnologyDepartment of EECS
Handoff Threshold
ReceivedSignal Strength (RSS)
from left BST
from right BST
unacceptable(call is dropped)
time
handoff threshold
time needed for handoff
RSS margin
• Handoff threshold too high too many handoffs (ping pong)• Handoff threshold too low dropped calls are likely• Threshold should depend on slope on vehicle speed (Doppler).
![Page 87: EECS 380: Wireless Communications Weeks 3-4: Propagation](https://reader036.vdocuments.mx/reader036/viewer/2022062521/5681684a550346895dde389e/html5/thumbnails/87.jpg)
N O R T H W E S T E R NU N I V E R S I T Y MSIT | Master of Science in Information TechnologyDepartment of EECS
Handoff Measurements (3G)• Mobile maintains a list of neighbor cells to monitor.• Mobile periodically measures signal strength from BST pilot
signals.• Mobile sends measurements to network to request handoff.• Handoff decision is made by network.
B
AD
C
![Page 88: EECS 380: Wireless Communications Weeks 3-4: Propagation](https://reader036.vdocuments.mx/reader036/viewer/2022062521/5681684a550346895dde389e/html5/thumbnails/88.jpg)
N O R T H W E S T E R NU N I V E R S I T Y MSIT | Master of Science in Information TechnologyDepartment of EECS
Handoff Measurements (3G)• Mobile maintains a list of neighbor cells to monitor.• Mobile periodically measures signal strength from BST pilot
signals.• Mobile sends measurements to network to request handoff.• Handoff decision is made by network.
B
AD
CPilot signals(transmittedcontinuously)
![Page 89: EECS 380: Wireless Communications Weeks 3-4: Propagation](https://reader036.vdocuments.mx/reader036/viewer/2022062521/5681684a550346895dde389e/html5/thumbnails/89.jpg)
N O R T H W E S T E R NU N I V E R S I T Y MSIT | Master of Science in Information TechnologyDepartment of EECS
Handoff Measurements (3G)• Mobile maintains a list of neighbor cells to monitor.• Mobile periodically measures signal strength from BST pilot
signals.• Mobile sends measurements to network to request handoff.• Handoff decision is made by network.
B
AD
C
active link request handoff
![Page 90: EECS 380: Wireless Communications Weeks 3-4: Propagation](https://reader036.vdocuments.mx/reader036/viewer/2022062521/5681684a550346895dde389e/html5/thumbnails/90.jpg)
N O R T H W E S T E R NU N I V E R S I T Y MSIT | Master of Science in Information TechnologyDepartment of EECS
Handoff Measurements (3G)• Mobile maintains a list of neighbor cells to monitor.• Mobile periodically measures signal strength from BST pilot
signals.• Mobile sends measurements to network to request handoff.• Handoff decision is made by network.
B
AD
C
link is broken
network activates link
![Page 91: EECS 380: Wireless Communications Weeks 3-4: Propagation](https://reader036.vdocuments.mx/reader036/viewer/2022062521/5681684a550346895dde389e/html5/thumbnails/91.jpg)
N O R T H W E S T E R NU N I V E R S I T Y MSIT | Master of Science in Information TechnologyDepartment of EECS
Handoff Decision
• Depends on RSS, time to execute handoff, hysteresis, and dwell (duration of RSS)– Proprietary methods– Handoff may also be initiated for balancing traffic.
• 1G (AMPS): Network Controlled Handoff (NCHO)– Handoff is based on measurements at BS, supervised by MSC.
• 2G, GPRS: Mobile Assisted Handoff (MAHO)– Handoff relies on measurements at mobile– Enables faster handoff
• Mobile data, WLANs (802.11): Mobile Controlled Handoff (MCHO)– Handoff controlled by mobile
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N O R T H W E S T E R NU N I V E R S I T Y MSIT | Master of Science in Information TechnologyDepartment of EECS
Soft Handoff (CDMA) ”Make before break”
MSC
BSC BSC
MSC
BSC BSC
MSC
BSC BSC
Hard Handoff (TDMA)
MSC
BSC BSC
MSC
BSC BSC
MSC
BSC BSC
BEFORE DURING AFTER
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N O R T H W E S T E R NU N I V E R S I T Y MSIT | Master of Science in Information TechnologyDepartment of EECS
Types of Small-Scale Fading
Small-Scale FadingBased on multipath time delay spread
Flat Fading1. BW of signal < BW of channel2. Delay spread < Symbol period
Frequency Selective Fading1. BW of signal > BW of channel2. Delay spread > Symbol period
Small-Scale FadingBased on Doppler spread
Fast Fading1. High Doppler spread2. Coherence time < Symbol period3. Channel variations faster than base- band signal variations
Slow Fading1. Low Doppler spread2. Coherence time > Symbol period3. Channel variations slower than base- band signal variations
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N O R T H W E S T E R NU N I V E R S I T Y MSIT | Master of Science in Information TechnologyDepartment of EECS
Types of Small-Scale Signal Fading as a Function ofSymbol Period and Signal Bandwidth
Ts
delay spread
Tc (coherence time)
TsFlat Fast
FadingFlat SlowFading
Frequency-Selective Slow Fading
Frequency-Selective Fast Fading
Symbol PeriodRelative to delay spread
BsBd = fd (Doppler shift)
Bs
Flat Fast Fading
Flat SlowFading
Frequency Selective Slow Fading
Frequency Selective Fast Fading
Bc
Symbol Period relative to coherence time.
Signal BWrelative to channel BW
coherence BW
Signal bandwidth relative to Doppler shift