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Survey of Radio Propagation Models for Mobile Communication

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    Technical Seminar Presentation - 2004

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    Survey of Radio Propagation Models forMobile Communication

    Presented bySalini Patnaik

    Roll# EC200157231

    AtNIST,Berhampur

    Under the guidance of

    Mr. Rowdra Ghatak

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    High-tier

    Low-tier

    Satellite

    High Mobility Low MobilityWide Area

    Regional Area

    Local Area

    Different Communication System

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    INTRODUCTION:

    Various propagationmodels can actually address

    both problems.

    BAS E

    STATIONRADIO

    TOWER

    The objective here is to

    design a suitable receiver

    that

    will receive the transmitted

    signal, distorted due to themultipath and dispersion

    effects of the channel, and

    that will decode the

    transmitted signal.

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    DEFINITIONS AND TERMINOLOGIES

    Path Loss:

    Where Ptand P

    rthe transmitted and received power

    Power Delay Profile:

    Where h(t) = impulse response

    Time-Delay Spread

    Coherence Bandwidth: Bc=1/50 RMS

    Where BC = Coherence bandwidth

    RMS = RMS Delay

    r

    t

    PPlog10)dB(PL =

    =dt|)t(h|

    |)t(h|)t(P

    2

    2

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    TYPES OF FADING:

    Large-scale fading Frequency-selective fading Flat fading Fast fading and slow fading

    BASIC PROPAGATION MECHANISMS :

    Reflection

    Diffraction Scattering

    Transmissionthrough a

    dielectric slab

    TR

    1st Fresnel zone

    ObstructionDiffraction

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    OUTDOOR CASE

    OKUMURA et al MODEL

    L50

    (db) = LF

    +Amu

    (f,d)-G(hte) - G(h

    re)-G

    AREA

    Where

    L50

    is the median value of the propagation path loss

    LF

    is the free-space propagation loss

    Amu, is the median attenuation in the medium relative to free space at frequencyf

    dcorresponds to the distance between the base and the mobile unit.G(h

    te) and G(h

    re) are the gain factors for the BTS antenna and the MS antenna.

    hte

    and hre

    are the effective heights (in meters )of the BTS and the MS antennae.

    GAREA

    is the gain generated by the environment in which the system is operating.

    EMPIRICAL OR STATISTICAL MODELS FOR PATH LOSS

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    HATA MODEL

    L50 (urban)(dB) = 69.55 + 26.16log fc - 13.82 log hre -a(hre,)

    + (44.9 - 6.55 log hre)logd

    Where

    fcis the frequency (in MHz), which varies from 150 MHz to 1500MHz.

    hte

    and hre

    are the effective heights of the base-station and the mobile

    antennas (in meters), respectively.

    d is the distance from the base station to the mobile antenna,

    a(hre) is the correction factor for the effective antenna height of the mobile

    unit, which is a function of the size of the area of coverage.

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    88

    COST-231-Walfisch-lkegami Model

    Where

    L0

    represents the free-space loss.

    Lrts is the roof-top-to-street diffraction andscattering loss.

    Lmsd

    is the multi-screen diffraction loss.

    +>+++

    =0LLL

    0LLLLLL

    msdrts0

    msdrtsmsdrts0b

    for

    for

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    INDOOR CASE

    It can be affected by the layout in a building.

    When electromagnetic radiation is incident on a wall or

    a flow in an oblique fashion, less power will be

    transmitted through the wall than would occur at normal

    incidence .

    Transmitter

    Propagation in Indoor Case

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    1010

    SITE-SPECIFIC MODELS FOR PATH LOSS

    RAY-TRACING TECHNIQUE Technique based on Geometrical Optics (GO) Fermat principle and the principle of the local field are two

    basic concepts extensively used by the ray models . The Fermat principle states that a ray follows the shortest path

    from a source point to a field point. The principle of the local field states that the high-frequency

    rays produce reflection, refraction, and diffraction when

    hitting a surface.

    Two types of ray-tracing methods :Image methodBrute-force ray-tracing method

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    1111

    Image Method

    This method generates the images

    of a source at all planes These images then serve as

    secondary sources for thesubsequent points of reflections.

    It can only handle simpleenvironments.

    Ground reflections and rays overrooftops are neglected .

    A threshold must be set with

    respect to the number and order ofreflection and diffraction rays thatcan be considered.

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    1212

    Brute-Force Ray-Tracing Method

    This method considers a

    bundle of transmitted rays

    that may or may not reach

    the receiver.

    A finite sample of the

    possible directions of the

    propagation from the

    transmitter is chosen. A

    ray is launched for each

    such direction.

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    There are two kinds of methods to obtain the rays at the sourcepoint.

    2D ray tracing approach:At the source, rays are launched along

    different directions with the same sector angle, , in a plane . An intersection with a surface of an object is represented by a

    node in the tree. The incident ray is decomposed into an object-reflected ray and

    an object-penetrated ray . 3D ray tracing approach:The transmitter and receiver are

    modeled as point sources . In order to determine all possible rays that may leave the

    transmitter and arrive at the receiver in three dimensions, all

    possible angles of departure and arrival at the transmitter and

    receiver are considered.

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    1414

    Applicable when transmitting and receiving antennas are

    often inevitably installed close to structures with complex

    material .

    properties for which no asymptotic solutions are available.

    Advantages of the FDTD method are its accuracy. It also

    gives signal-coverage information throughout a given area

    Disadvantage of FDTD is that it requires large amounts of

    computer memory.

    FDTD modelFDTD model

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    1515

    Moment-Method Models

    Method of Moments(MOM) model is better when higher

    precision is required and when the size of the buildings is

    smaller.

    Due to limitations of computer memory and CPU time,the

    MOM is usually applied for analyzing objects that are tens of

    wavelengths in size.

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    1616

    Artificial Neural-Network Models

    Key feature of the neural network is the intrinsic parallelism,allowing for fast evaluation of the solutions .

    The inputs were the frequency, the heights of the antenna forthe base and mobile stations, respectively, and the distances

    between them. The output was the field strength. Multilayered ANN suffers from slow convergence and

    unpredictable solutions during learning . Radial-basis function (RBF) neural networks that have a

    linear-in-the parameters representation were proposed to

    overcome multilayered ANN problem.

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    1717

    Vector Parabolic-Equation Model As a parabolic version of Maxwells equations, it allows

    a full treatment of three-dimensional electromagnetic

    scattering . Fast Far-Field Approximation Model

    The method has been applied to gently undulating

    terrains and more hilly terrain. Waveguide Model

    In large metropolitan areas the city streets act as a type of

    wave-guiding structure for the propagating signal . the statistical propagation characteristics in such a

    Waveguide are expressed in terms of multiple ray fields

    approaching the observer.

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    1818

    Boltzmann Model

    It describes a physical system in terms of the motion of

    fictitious microscopic particles on a lattice . MODELS FOR SMALL SCALE FADING

    Ricean Distribution:

    Where

    ris the amplitude of the envelope of the received signal,

    2 2 is the predicted mean power of the multipath signalA denotes the peak amplitude of the dominant signal, and

    Io (Ar/ 2) is the modified Bessel function of the first kind

    Rayleigh Distribution:


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