em analysis of aircraft in-cabin area

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    A STUDY OF METHODS FOR

    ELECTROMAGNETIC EVALUATION OF A

    LARGE AIRCRAFT IN-CABINENVIRONMENT

    SUBMITTED BY:- SOUMYA TEJAS

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    ABSTRACT

    Electromagnetic (EM) field mapping inside the aircraft cabin area is

    required for commercial applications for the passenger area (wireless

    communication, Wi Fi WLAN etc.)

    It is done using 3-D ray tracing. However, computations become highly

    complex due to the presence of passenger seats, partitions, flooring

    material, apertures etc. in the passenger area.

    A literature survey is done with focus on EM scattering, diffraction, and

    absorption mechanisms in a closed lossy cavity.

    Methods that make computations numerically efficient have been

    discussed.

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    ORGANIZATION PROFILE

    National Aerospace Laboratories

    NAL is a government organization under Council of Scientific and

    Industrial Research (CSIR) established in 1959 in Bangalore.

    It is a high technology oriented institution concentrating on

    advanced topics in aerospace and related disciplines.

    NAL has developed HANSA trainer aircraft and another light

    transport aircraft SARAS is undergoing flight testing.

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    RAY TRACING

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    Forms of Interaction of EM rays WithSurface

    Reflection Transmission (Refraction)

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    o Geometrical Optics (GO): It is suitable for direct and line-of-sight (LOS) path GO considers only direct and reflected paths

    o

    Physical Optics (PO): It also considers scattered field strengthso Physical Theory of Diffraction (PTD):

    It is an extension of PO It includes the consideration of edge currents

    o Geometrical Theory of Diffraction (GTD):

    It is an extension of GO GTD considers diffraction It tends to give erroneous results in shadowed regions

    o Uniform Theory of Diffraction (UTD): It is an improved version of GTD UTD considers multiple diffractions and scattering This theory tends to give good results for shadowed regions

    Theories for Interaction of EM raysWith Surface

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    PATH LOSS

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    Definition : Path loss is the power lost during transmission of

    electromagnetic radiation from transmitter to thereceiver.

    Models : Two categories of models are there for path loss models(i) Empirical(ii) Site-specific

    Empirical model : Considers only the parameters of the communication system Simple calculations Approximate results

    Site-Specific model : Considers details of the environment Complex calculations Accurate results

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    EMPIRICAL MODELS1. Okumura Model Applicable for:

    Frequencies from 150-1920 MHz Radio path length of 1 100 km

    Transmitter antenna height from30 1000 m

    Outdoor environment

    Model equation:

    L50(dB): median propagation path loss A mu : median attenuation relative to free spaceG: gain factors

    1. Hata Model Applicable for:

    Frequencies from 150 - 1500 MHz Radio path length of 1 100 km Receiver antenna height from 1 - 10

    m Outdoor environment

    Model equation:

    h re: receiver antenna effective heighth te: transmitter antenna effective height

    AREAretemu F GhGhGd f A LdB L +=++=

    retec hah f dBurban L

    d hte

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    EMPIRICAL MODELS1. Cost-231-Walfisch-Ikegami

    Model Applicable for:

    Frequencies from 800 2000MHz

    Transmitter antenna height 4 50m

    Receiver antenna height 1 3 m Urban environment

    Model equation:

    Lo: free space lossLrts : roof-top to street scattering and diffraction

    lossLmsd : multi-screen diffraction loss

    1. Dual Slope Method

    Applicable for: Line-of-sight (LOS) condition Outdoor environment

    Model equation:

    d brk : turning point or break-point distancen

    1: slope of best fit line before break-point

    n 2: slope of best fit line after break-point

    +>+++=

    msd rts

    msd rtsmsd rtsb L L L

    L L L L L L ++

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    EMPIRICAL MODELS1. Power/Distance Model

    Applicable only for indoor environment.

    Model equation:

    FAF: floor attenuation factor WAF: wall attenuation factord: radio-path lengthd o: reference radio-path length

    == +++= P

    p

    Q

    q pWAF q FAF d d nd PLd PL

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    SITE-SPECIFIC MODELS1. Ray-tracing technique2. Finite difference time domain (FDTD)

    3. Method of Moments4. Artificial Neural Networks (ANN)

    FDTD and MoM are numerical methods ANN includes usage of specifically trained neural networks

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    SMALL-SCALE FADING

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    MODELS:1. Ricean (Rice) Distribution

    This model is applicable only forLOS paths.

    Probability distribution function:

    r: amplitude of received signal envelope2 2: predicted mean power of multipath signal A: amplitude of dominant signalI0(.): Bessel function, first kind, zero order

    1. Rayleigh DistributionThis model is applicable only forNon-Line-of-Sight (NLOS) paths.

    Probability distribution function: