02. radio propagation fundamentals

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  • 7/30/2019 02. Radio Propagation Fundamentals

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    Radio propagation fundamentals

    MODULE 2

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    Module 2 Radio propagation fundamentals

    Objectives

    After this module the participant shall be able to:-

    Understand basic radio propagation mechanisms

    Understand fading phenomena

    Calculate free space loss

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    Module Contents

    Propagation mechanisms

    Multipath And Fading

    Propagation Slope And Different Environments

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    Module Contents

    Propagation mechanisms

    Basics: deciBel (dB) Radio channel

    Reflections

    Diffractions

    Scattering

    Multipath And Fading

    Propagation Slope And Different Environments

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    deciBel (dB) Definition

    Power

    Voltages

    dB PP

    PlinP dB

    10 10

    0

    10log [ ].( )

    dBE

    E Elin

    E dB

    20 10020log [ ].

    ( )

    Plin.=Elin.

    / 2

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    deciBel (dB) Conversion

    Calculations in dB (deciBel)

    Logarithmic scale

    Always with respect to a reference dBW = dB above Watt

    dBm = dB above mWatt

    dBi = dB above isotropic

    dBd = dB above dipole

    dBmV/m = dB above mV/m

    Rule-of-thumb: +3dB = factor 2

    +7 dB = factor 5

    +10 dB = factor 10

    -3dB = factor 1/2

    -7 dB = factor 1/5

    -10 dB = factor 1/10

    -30 dBm = 1 mW-20 dBm = 10 mW

    -10 dBm = 100 mW-7 dBm = 200 mW-3 dBm = 500 mW0 dBm = 1 mW+3 dBm = 2 mW

    +7 dBm = 5 mW+10 dBm = 10 mW

    +13 dBm = 20 mW

    +20 dBm = 100mW

    +30 dBm = 1 W

    +40 dBm = 10W+50 dBm = 100W

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    Radio Channel Main Characteristics

    Linear

    In field strength Reciprocal

    UL & DL channel same (if in same frequency)

    Dispersive

    In time (echo, multipath propagation)

    In spectrum (wideband channel)

    amplitude

    delay time

    direct path

    echoes

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    Propagation Mechanisms (1/2)

    Free-space propagation

    Signal strength decreases exponentially with

    distance

    Reflection

    Specular reflection

    amplitude A a*A (a < 1)

    phase f - f

    polarisation material dependant

    phase shift

    Diffuse reflection

    amplitude A a *A (a < 1)

    phase f random phase

    polarisation random

    specular reflection

    diffuse reflection

    D

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    Propagation Mechanisms (2/2)

    Absorption

    Heavy amplitude attenuation Material dependant phase shifts

    Depolarisation

    Diffraction

    Wedge - model Knife edge

    Multiple knife edges

    A A - 5..30 dB

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    Scattering Macrocell

    Scattering local to mobile

    Causes fading

    Small delay and angle spreads

    Doppler spread causes time varying

    effects

    Scattering local to base station

    No additional Doppler spread

    Small delay spread

    Large angle spread

    Remote scattering

    Independent path fading

    No additional Doppler spread

    Large delay spread Large angle spread

    Scattering to mobile

    Scattering to base station

    Remote scattering

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    Scattering Microcell

    Many local scatterers: Large angle spread

    Low delay spread Medium or high Doppler spread

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    Module Contents

    Reflections, Diffractions And Scattering

    Multipath and Fading

    Delay Time dispersion

    Angle Angular Spread

    Frequency Doppler Spread

    Fading

    Slow & Fast

    Propagation Slope And Different Environments

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    Multipath propagation

    Radio signal propagates from A to B over multiple paths using different

    propagation mechanisms

    Multipath Propagation

    Received signal is a sum of multipath signals

    Different radio paths have different properties

    Distance Delay/Time Direction Angle

    Direction & Receiver/Transmitter Movement Frequency

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    Delay Time dispersion

    Multipath delays due to multipath propagation

    1 ms 300 m path difference

    WCDMA Rake receiver to combine multipath components

    Components with delay separation more than 1 chip (0.26 ms = 78 m) can beseparated and combined

    Standardized delay profiles in 3GPP specs: TU3 typical urban at 3 km/h (pedestrians)

    TU50 typical urban at 50 km/h (cars)

    HT100 hilly terrain (road vehicles, 100 km/h)

    RA250 rural area (highways, up to 250 km/h)

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    t

    P

    4.3.2.

    1.1.

    2.

    =>

    f1

    f1

    f1

    f1

    BTS

    1st floor

    2nd floor

    3rd floor

    4th floor

    Delay Spread

    Multipath

    propagation

    Channel impulse

    response

    Delayed components in DAS

    (Distributed antenna systems)

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    Delay Spread

    Typical values

    Environment Delay Spread (ms)

    Macrocellular, urban 0.5-3

    Macrocellular, suburban 0.5

    Macrocellular, rural 0.1-0.2

    Macrocellular, HT 3-10

    Microcellular < 0.1

    Indoor 0.01...0.1

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    Angle Angular Spread

    Angular spread arises due to multipath, both from local scatterers near the

    mobile and near the base station and remote scatterers

    Angular spread is a function of base station location, distance and environment

    Angular Spread has an effect mainly on the performance of diversity reception

    and adaptive antennas

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    Macrocellular Environment

    = Macrocell Coverage Area

    Microcellular Environment

    = Microcell Coverage Area

    Microcell Antenna

    Macrocell Antenna

    a

    Angular Spread

    5 - 10 degrees in macrocellular environment

    >> 10 degrees in microcellular environment

    < 360 degrees in indoor environment

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    Frequency Doppler Spread

    With a moving transmitter or receiver, the frequency observed by the receiver will

    change (Doppler effect)

    Rise if the distance on the radio path is decreasing

    Fall if the distance in the radio path is increasing

    The difference between the highest and the lowest frequency shift is called

    Doppler spread

    fc

    vvfd

    v: Speed of receiver (m/s)c: Speed of light (3*10^8 m/s)

    f: Frequency (Hz)

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    Fading

    Fading describes the variation of the total pathloss ( signal level) when

    receiver/transmitter moves in the cell coverage area

    Fading is commonly categorised to two categories based on the phenomena

    causing it

    Slow fading: Caused by shadowing because of obstacles

    Fast fading: Caused by multipath propagation

    Time-selective fading: Short delay + Doppler

    Frequency-selective fading: Long delay

    Space-selective fading: Large angle

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    time

    power

    2 sec 4 sec 6 sec

    +20 dB

    meanvalue

    - 20 dB

    lognormal

    fading

    Rayleighfading

    Fading Slow & Fast

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    Slow Fading Gaussian Distribution

    Measurement campaigns have shown that slow fading follows Gaussian

    distribution

    Received signal strength in dB scale (e.g. dBm, dBW)

    Gaussian distribution is described by mean value m, standard deviation 68% of values are within m

    95% of values are within m 2

    Gaussian distribution used in planning margin calculations

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    Slow Fading Gaussian Distribution

    d

    Normal / Gaussian Distribution

    Standard Deviation, = 7 dB

    0.00000

    0.01000

    0.02000

    0.03000

    0.04000

    0.05000

    0.06000

    0.07000

    -25 -20 -15 -10 -5 0 5 10 15 20 25

    Normal / Gaussian Distribution

    22

    1

    m

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    Fast Fading

    Different signal paths interfere and affect the received signal

    Rice Fading the dominant (usually LOS) path exist

    Rayleigh Fading no dominant path exist

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    Fast Fading Rayleigh Distribution

    It can be theretically shown that fast fading follows Rayleigh Distribution when

    there is no single dominant multipath component

    Applicable to fast fading in obstructed paths

    Valid for signal level in linear scale (e.g. mW, W)

    +10

    0

    -10

    -20

    -300 1 2 3 4 5 m

    level (dB)

    920 MHz

    v = 20 km/h

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    Fast Fading Rician Distribution

    Fast fading follows Rician distribution when there is a dominant multipath

    component, for example line-of-sight component combined with in-direct

    components

    Sliding transition between Gaussian and Rayleigh

    Rice-factor K = r/A: direct / indirect signal energy

    K = 0 RayleighK >>1 Gaussian

    K = 0(Rayleigh)

    K = 1

    K = 5

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    Module Contents

    Reflections, Diffractions And Scattering

    Multipath And Fading

    Propagation Slope And Different Environments

    Free Space Loss

    Received power with antenna gain

    Propagation slope

    F S L

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    Free Space Loss

    Free space loss proportional to 1/d2

    Simplified case: isotropic antenna

    Which part of total radiated power is found within surfaceA?

    Power density S = P/A = P/ 4 d2

    Received power within surfaceA : P = P/A * A Received power reduces with square of distance

    d

    SurfaceA = 4 * d2

    assume surface

    A= 1m

    2

    2d

    4d

    A = 4*AA = 16*A

    A

    d

    R i d ith t i

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    Received power with antenna gain

    Power density at the receiving end

    Effective receiver antenna area

    Received power

    Reff GA

    4

    2

    s

    s

    Gd

    P

    S 24

    P

    PG G

    d

    r

    s

    s r

    4

    2

    Ps

    As

    Gs

    Pr

    Ar

    Gr

    d

    SAP effr

    P ti l

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    Propagation slope

    The received power equation can be formulated as

    Where

    C is a constant

    is the slope factor

    Free space = 2

    Practical propagation = 2.5 ... 5

    2

    4

    C

    dCGGPP rssr

    M d l 2 R di P ti F d t l

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    Module 2 Radio Propagation Fundamentals

    Summary

    Radio signal propagates with multiple propagation

    mechanisms

    Radio signal strength varies between locations Fading

    Fading is caused by shadowing and multipath propagation

    Received radio signal power attenuates with increasing

    distance Propagation slope