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    RF Communication Lecture # 1

    Dr. Irfan Ahmed

    Introduction to RF Propagation

    By: Seybold J.S.

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    1.1 FREQUENCY DESIGNATIONS

    The electromagnetic spectrum is loosely divided into regions as

    shown in Table 1.1 [1].

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    During World War II, letters were used to designate various frequency bands, particularly

    those used for radar. These designations were classified at the time, but have found their

    way into mainstream use. The band identifiers may be used to refer to a nominal frequency

    range or specific frequency ranges. Table 1.2 shows the nominal band designations and

    the official radar band designations in Region 2 as determined by international

    agreement through the International Telecommunications Union (ITU).

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    ITU-Region MAP

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    1.2 MODES OF PROPAGATION

    For most RF propagation modeling, it is sufficient to visualize the electromagnetic wave

    by a ray (the Poynting vector) in the direction of propagation.

    In free space, electromagnetic waves are modeled as propagating outward from the

    source in all directions, resulting in a spherical wave front. Such a source is called an

    isotropic radiator and in the strictest sense, does not exist.

    As the distance from the source increases, the spherical wave (or phase) front converges

    to a planar wave front over any finite area of interest, which is how the propagation is

    modeled.

    The power density on the surface of an imaginary sphere surrounding the

    RF source can be expressed as

    where d is the diameter of the imaginary sphere, P is the total power at the source, and S is

    the power density on the surface of the sphere in watts/m2.

    P = EH

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    1.2.1 Line-of-Sight Propagation and the Radio Horizon

    When considering line-of-sight (LOS)

    propagation, it may be necessary toconsider the curvature of the earth

    (Figure 1.1). The curvature of the

    earth is a fundamental geometric

    limit on LOS propagation. In

    particular, if the distance between the

    transmitter and receiver is largecompared to the height of the

    antennas, then an LOS may not exist.

    The simplest model is to treat the

    earth as a sphere with a radius

    equivalent to the equatorial radius of

    the earth.

    where d is the distance to the radio horizon

    in miles and h is in feet

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    Example LOS

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    1.2.2 Non-LOS Propagation

    The mechanisms of non-LOS propagation vary considerably, based on

    the operating frequency. At VHF and UHF frequencies, indirect

    propagation is often used. Examples of indirect propagation are cell phones, pagers, and some

    military communications. An LOS may or may not exist for these

    systems.

    In the absence of an LOS path, diffraction, refraction, and/or multipath

    reflections are the dominant propagation modes Diffractionis the phenomenon of electromagnetic waves bending at

    the edge of a blockage, resulting in the shadow of the blockage being

    partially filled-in.

    Refractionis the bending of electromagnetic waves due to in-

    homogeniety in the medium.

    Multipathis the effect of reflections from multiple objects in the field

    of view, which can result in many different copies of the wave arriving

    at the receiver.

    The over-the-horizon propagation effects are loosely categorized as

    sky waves, tropospheric waves, and ground waves.

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    Sky waves are based on ionospheric reflection/refraction

    and are discussed presently. Tropospheric waves are those electromagnetic waves that

    propagate through and remain in the lower atmosphere.

    Ground waves include

    Surface waves, which follow the earths contour

    Space waves, which include direct, LOS propagation as

    well as ground-bounce propagation.

    1.2.2 Non-LOS Propagation contd.

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    1.2.2.1 Ind irect o r Obstructed Propagation

    Indirect propagation aptly describes terrestrial propagation

    where the LOS is obstructed

    In such cases, reflection from and diffraction around buildingsand foliage may provide enough signal strength

    HFfrequencies can penetrate buildings and heavy foliage quite

    easily

    Above UHF, indirect propagation becomes very inefficient and isseldom used

    When the features of the obstruction are large compared to the

    wavelength, the obstruction will tend to reflect or diffractthe wave

    rather than scatterit

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    1.2.2.2 Tropospheric Propagation

    The troposphere is the first (lowest) 10 km of the atmosphere,

    where weather effects exist.

    Tropospheric propagation consists of reflection (refraction) of RF

    from temperature and moisture layers in the atmosphere.

    Tropospheric propagation is less reliable than ionospheric

    This effect is sometimes called ducting, although technically

    ducting consists of an elevated channel or duct in the atmosphere.

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    1.2.2.3 Ionospheric Propagation

    The ionosphereis an ionized plasma around the earth that is essential to

    sky-wave propagation and provides the basis for nearly all HF

    communications beyond the horizon. It is also important in the study of satellite communications at higher

    frequencies since the signals must transverse the ionosphere, resulting in

    refraction, attenuation, depolarization, and dispersion due to frequency

    dependent group delay and scattering.

    HFcommunication relying on ionospheric propagation was once thebackbone of all long-distance communication.

    Over the last few decades, ionospheric propagation has become primarily

    the domain of shortwavebroadcasters and radio amateurs.

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    1.2.3 Propagation Effects as a Function of Frequency

    Very low frequency (VLF) band covers 330kHz

    The VLF band only permits narrow bandwidths to be used (theentire band is only 27kHz wide)

    The primarily mode of propagation in the VLF range is ground-

    wavepropagation

    VLF has been successfully used with underground antennas for

    submarinecommunication

    The low frequency dictates that large antennas are required to

    achieve a reasonable efficiency

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    1.2.3 Propagation Effects as a Function of Frequency contd

    The low-(LF) and medium-frequency (MF) bands, cover the range

    from 30kHz to 3MHz.

    Both bands use ground-wavepropagation and some sky wave. While the wavelengths are smaller than the VLF band, these bands

    still require very large antennas.

    These frequencies permit slightly greater bandwidth than

    the VLFband.

    Uses include broadcast AM radio and theWWVB time referencesignal that is broadcast at 60 kHz for automatic (atomic) clocks.

    WWVBis a NISTtime signalradio station near Fort Collins,

    Colorado.

    http://en.wikipedia.org/wiki/NISThttp://en.wikipedia.org/wiki/Time_signalhttp://en.wikipedia.org/wiki/Fort_Collins,_Coloradohttp://en.wikipedia.org/wiki/Fort_Collins,_Coloradohttp://en.wikipedia.org/wiki/Fort_Collins,_Coloradohttp://en.wikipedia.org/wiki/Fort_Collins,_Coloradohttp://en.wikipedia.org/wiki/Time_signalhttp://en.wikipedia.org/wiki/NIST
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    The high-frequency (HF), band covers 330MHz.

    Most HF communication is via sky wave. There are few remaining commercial

    uses due to unreliability, but HF sky waves were once the primary means of long-

    distance communication.

    One exception is international AM shortwave broadcasts, which still rely on

    ionospheric propagation to reach most of their listeners.

    The HF band includes citizens band (CB) radio at 27MHz.CB radio is an example

    of poor frequency reuse planning. While intended for short-range communication,

    CB signals are readily propagated via sky wave and can often be heard hundreds

    of miles away.

    The advantages of the HF band include inexpensiveand widely available

    equipment and reasonably sized antennas, which was likely the original

    reason for the CB frequency selection

    Several segments of the HF band are still used for amateur radio and for militaryground and over-the-horizon communication.

    1.2.3 Propagation Effects as a Function of Frequency contd

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    1.2.3 Propagation Effects as a Function of Frequency contd

    The very high frequency (VHF) and ultra-high frequency (UHF)cover frequencies

    from 30MHz to 3GHz .

    In these ranges, there is very little ionospheric propagation, which makes them

    ideal for frequency reuse.

    For the most part, VHF and UHF waves travel by LOS and ground-bounce

    propagation.

    VHF and UHF systems can employ moderately sized antennas, making these

    frequencies a good choice for mobile communications.

    Applications of these frequencies include broadcast FM radio, aircraft radio,cellular/PCS telephones, pagers, public service radio such as police and fire

    departments, and the Global Positioning System (GPS).

    These bands are the region where satellite communication begins since the signals

    can penetrate the ionosphere with minimal loss.

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    1.2.3 Propagation Effects as a Function of Frequency contd

    The super-high-frequency (SHF) frequencies include 330GHz

    and use strictly LOS propagation.

    In this band, very small antennas can be employed, or, moretypically,moderately sized directional antennas with high gain

    Applications of the SHF band include satellite communications,

    direct broadcast satellite television, and point-to-point links.

    Precipitation and gaseous absorption can be an issue in these

    frequency ranges, particularly near the higher end of the range

    and at longer distances.

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    1.2.3 Propagation Effects as a Function of Frequency contd

    The extra-high-frequency (EHF) band covers 30300GHz and

    is often called millimeter wave.

    In this region, much greater bandwidths are available. Propagation is strictly LOS, and precipitation and gaseous

    absorption are a significant issue.

    The Atacama Large Millimeter/sub-millimeter Array(ALMA) is

    an astronomical interferometerof radio telescopesin the Atacama

    desertof northern Chile

    http://en.wikipedia.org/wiki/Astronomical_interferometerhttp://en.wikipedia.org/wiki/Radio_telescopehttp://en.wikipedia.org/wiki/Atacama_deserthttp://en.wikipedia.org/wiki/Atacama_deserthttp://en.wikipedia.org/wiki/Chilehttp://en.wikipedia.org/wiki/Chilehttp://en.wikipedia.org/wiki/Atacama_deserthttp://en.wikipedia.org/wiki/Atacama_deserthttp://en.wikipedia.org/wiki/Radio_telescopehttp://en.wikipedia.org/wiki/Astronomical_interferometer
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    1.3 WHY MODEL PROPAGATION?

    The goal of propagation modeling is often to determine the probability of

    satisfactory performance of a communication system or other system that is

    dependent upon EM wave propagation.

    If the modeling is too conservative, excessive costs may be incurred, whereas too

    liberalof modeling can result in unsatisfactory performance. Thus the fidelity of

    the modeling must fit the intended application.

    For communication planning, the modeling of the propagation channel is for the

    purpose of predicting the received signal strength at the end of the link.

    In addition to signal strength, there are other channel impairments that candegrade link performance. These impairments include

    delay spread

    (smearing in time) due to multipath

    rapid signal fading within a symbol (distortion of the signal spectrum).

    These effects must be considered by the equipment designer, but are notgenerally considered as part of communication link planning. Instead, it is

    assumed that the hardware has been adequately designed for the channel.

    In some cases this may not hold true and a communication link with sufficient

    receive signal strength may not perform well.

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    1.4 MODEL SELECTION AND APPLICATION

    The selection of the model to be used for a particular application often

    turns out to be as much art as it is science

    Corporate culture may dictate which models will be used for a given

    application Generally, it is a good idea to employ two or more independent models if

    they are available and use the results as bounds on the expected

    performance.

    The process of propagation modeling is necessarily a statistical one, and

    the results of a propagation analysis should be used accordingly

    There may be a temptation to shop different models until one is found

    that provides the desired answer. Needless to say, this can lead to

    disappointment

    Even so, it may be valuable for certain circumstances such as highlycompetitive marketing or proposal development

    It is important that the designer not be lulled into placing too much

    confidence in the results of a single model.

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    1.4.1 Model Sources

    Many situations of interest have relatively mature models based upon large

    amounts of empirical data collected specifically for the purpose of

    characterizing propagation for that application

    There are also a variety of proprietary models based on data collected for

    very specific applications

    For more widely accepted models, organizations like the International

    Telecommunications Union (ITU) provide recommendations for modeling

    various types of propagation impairments While these models may not always be the best suited for a particular

    application, their wide acceptance makes them valuable as a benchmark.

    There exist a number of commercially available propagation modeling

    software packages. Most of these packages employ standard modeling

    techniques.

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