6. long distance links

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    Long-Distance Links

    Telecommunication Engineering

    www.ee.ui.ac.id/wasp

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    Propagation of Wave

    The propagation of electromagnetic waves is dependenton the frequency

    The propagation characteristics are the result of changesin the radio-wave velocity as a function ofaltitude andboundary conditions

    The wave velocity is dependent on air temperature, airdensity, and levels of air ionization

    Ionization (free electrons) of the rarified air at highaltitudes has a dominant effect on wave propagation in

    the MF and HF bands The ionization is caused by ultraviolet radiation from the

    sun, as well as cosmic rays

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    Propagation of Wave

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    Propagation of Wave

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    Propagation of Wave

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    Propagation of Wave

    The dominant ionized regions are D, E, F1, and F2 The D layer is located closest to the Earths surface at an

    altitude of about 45 or 55 miles

    For f > 300 kHz, it acts as a RF sponge to absorb(attenuate) the waves

    The attenuation is inversely proportional to frequencyand becomes small for frequencies above 4 MHz

    For f < 300 kHz, it provides refraction (bending) of RFwaves

    It is most pronounced during the daylight hours, withmaximum ionization when the sun is overhead, andalmost dissapears at night

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    Propagation of Wave

    The E layer has a height of 65 to 75 miles, has maximumionization around noon and disappears after sunset

    The F layer has a height of 90 to 250 miles

    It ionizes rapidly at sunrise, with its peak ionization in

    early afternoon and decay slowly after sunset The F region splits into two: F1 and F2 during the day and

    combines into one layer at night

    The F region is the most predominant medium in

    providing reflection of HF waves

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    Propagation of Wave

    Three dominant propagation characteristics: Ground wave

    Sky wave

    LOS

    Ground wave propagation is the dominant mode ofpropagation for frequencies < 2 MHz

    Here, the wave tends to follow the contour of the Earth

    because the diffraction of wave causes it to propagate

    along the surface of the Earth What is the lowest radio frequency that can be used?

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    Propagation of Wave

    For efficient radiation, the antenna needs to be longer

    than 1/10 of a wavelength For example, for signaling with a carrier frequency of 10

    kHz, the antenna length is minimum 3000 m

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    Propagation of Wave

    Sky wave propagation is the dominant mode ofpropagation in the 2 to 30 MHz frequency range

    Here, long-distance coverage is obtained by reflecting the

    wave at the ionosphere and at the Earths boundaries

    In the ionosphere the waves are refracted gradually in aninverted U shape because the index of refraction varies

    with altitude as the ionization density changes

    The refraction index of the ionosphere is given by

    2

    811

    Nn

    f refractive indexn

    3free electron density (electrons/m )N frequency (Hz)f

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    Propagation of Wave

    Typical N values range between 10^10 and 10^12

    depending on the time of day, season, sunspots In an ionized region because and outside the

    ionized region because

    1n 0N

    1n 0N

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    Propagation of Wave

    In the ionized region the waves will be bent according toSnells law

    The layer D is present during the day and absorbsfrequencies below 4 MHz

    Thats why in AM broadcast, the distant stations cannotbe heard during the day, but at night the layer disappearsand distant AM stations can be heard via sky wavepropagation

    Sky wave propagation is caused by reflection from the Flayer

    sin r in

    angle of incidencei angle of refractionr

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    Propagation of Wave

    LOS propagation is the dominant mode for frequenciesabove 30 MHz

    Here the electromagnetic wave propagates in a straight

    line

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    LOS Systems

    The LOS mode has the disadvantage that forcommunication between two terrestrial stations, the

    signal path has to be above the horizon

    Otherwise, the Earth will blockthe LOS path

    The antennas need to be placed on tall towers so thatthe receiver antenna can see the transmitting antenna

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    LOS Systems

    To the optical horizon, k (bending characteristic) = 1

    To the radio horizon, k =4/3

    The design of an LOS microwave linkinvolves 5 basic steps: Setting performance requirements

    Site selection and preparation of a path profile to determine antennatower heights

    Carrying out a path analysis (link budget) Physically running a path/site survey

    Installation of equipment and test of the system prior to cutting itover to carry traffic

    3 [ ][ ] 2.9

    2o

    h md km

    [ ] 2.9 2 [ ]rd km h m

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    Site Selection

    Select operational site where we will install and operate radioequipment

    Path profile of each link to determine the heights of radiotower to achieve LOS

    Steps to obtain path profile:

    Obtain good toplogical maps of the region Draw a straight line with a long straight edge connecting the two

    sites identified

    Follow along down the line identifying obstacles and their heights

    Calculate earth curvature (EC)

    Calculate the Fresnel zone clearance for each obstacle

    Add a value of additional height for vegetation and a growth factor

    Draw a straight line from left to right connecting the two highestobstacle locations on the profile

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    Site Selection

    To calculate the EC we must account for the radio raypath bending by using K-factor

    When K-factor is greater than 1, the ray beam bendstowards the earth

    Whne K-factor is less than 1, the ray beam bends awayfrom the earth

    The following formula applies

    where is the distance from the transmit site to theobstacle in question and is the distance from thatobstacle to the receive site

    1 20.078d d

    h mK

    1d

    2d

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    Site Selection

    How to find the K-factor?

    Fresnel zone clearance

    1 2

    [ ] 17.3d km d km

    R mF GHz D km

    1 2D d d

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    Link Budget

    A path analysis is carried out to dimension the link Establishing operating parameters such as transmitter

    power output, parabolic antenna aperture (diameter),

    receiver noise figure

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    Link Budget

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    Link Budget

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    Link Budget

    For operating frequencies up to about 10 GHz, path lossis synonymous with free-space path loss

    Free-space path loss is given by

    EIRP is calculated by adding decibel units: transmittedpower (in dBm or dBW), the transmission line losses in

    dB, and antenna gain in dBi

    Example: If a microwave transmitter has 1 W of power

    output, the waveguide loss is 3 dB and the antenna gain is

    34 dBi, the EIRP is

    [ ] 92.4 20log [ ] 20log [ ]PL dB F GHz D km

    .output trans lineEIRP dBW P dBW Loss dB G dBi

    0 3 34 31EIRP dBW dB dBi dBW

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    Link Budget

    Isotropic Receive Level (IRL) is the RF power levelimpinging on the receive antenna

    Receive signal level (RSL) is the power level at the input

    port if the first active stage in the receiver

    IRL dBW EIRP dBW PL dB

    . .rec ant trans lineRSL dBW IRL dBW G dB Loss dB

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    Link Budget

    Example: Suppose the IRL was -121 dBW, the receiveantenna gain was 31 dB, and the line losses were 5.6 dB.

    The RSL would be

    The thermal noise level of a receiver is a function of thereceiver noise figure and its bandwidth

    The thermal noise power level in a 1-Hz bandwidth of a

    perfect receiver operating at absolute zero is

    The thermal noise level of a perfect receiver operating at

    room temperature is

    121 31 5.6 95.6RSL dBW dB dB dBW

    228.6nP dBW Hz

    228.6 10log 290 204nP dBW Hz K dBW Hz

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    Link Budget

    We can convert noise figure to noise temperature inkelvins with the following formula

    The thermal noise power level of a device operating atroom temperature is

    Example: A microwave receiver has a noise figure of 8 dB

    and its bandwidth is 10 MHz. The thermal noise level is

    10log 1 290eNF dB T

    the effective noise temperature of a deviceeT

    204 10lognP dBW Hz NF dB BW Hz

    6204 8 10log 10 10 126nP dBW Hz dB dBW

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    Link Budget

    S/N is widely used in analog transmission systems as onemeasure of signal quality

    In digital systems the basic measure of transmission

    quality is BER

    In digital radio links, the ratio Eb/N0 is used as themeasure of signal quality

    Eb/N0 means energy per bit per noise spectral density

    ratio

    N0 is simply the thermal noise in 1 Hz of bandwidth or

    0 204N dBW Hz NF dB

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    Link Budget

    Example: Suppose a receiver has a noise figure of 2.1 dB,what is the thermal noise level in 1 Hz of bandwidth. The

    N0 is

    Eb is the signal energy per bit and defined as

    Example: The RSL into a certain receiver was -89 dBW

    and bit rate was 2.048 Mbps. The Eb value is

    Then, the formula for Eb/N0 is

    0 204 2.1 201.9N dBW Hz dB dBW Hz

    or 10logbE RSL dBm dBW bit rate

    689 10log 2.048 10 152.11bE dBW dBW

    0 10log 204bE N RSL dBW bit rate dBW NF dB