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Hilmi ECE GMDSS Instructor 1 RADIO THEORY & PROPAGATION The magnetic field strength in the vicinity of a conductor is directly proportional to the magnitude of the current flowing through the conductor. Recall the discussion of alternating current above. A rotating generator produces current in the form of a sine wave. That is, the magnitude of the current varies as a function of the relative position of the rotating conductor and the stationary magnetic field used to induce the current. The current starts at zero, increases to a maximum as the rotor completes one quarter of its revolution, and falls to zero when the rotor completes one half of its revolution. The current then approaches a negative maximum; then it once again returns to zero. Radio Wave Terminology
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2 Propagation Modulation

Sep 07, 2015

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Propagation Modulation
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  • Hilmi ECE GMDSS Instructor1

    RADIO THEORY & PROPAGATION

    The magnetic field strength in the vicinity of a conductor is

    directly proportional to the magnitude of the current flowing

    through the conductor. Recall the discussion of alternating

    current above. A rotating generator produces current in the

    form of a sine wave. That is, the magnitude of the current

    varies as a function of the relative position of the rotating

    conductor and the stationary magnetic field used to induce

    the current. The current starts at zero, increases to a

    maximum as the rotor completes one quarter of its revolution,

    and falls to zero when the rotor completes one half of its

    revolution. The current then approaches a negative

    maximum; then it once again returns to zero.

    Radio Wave Terminology

  • Hilmi ECE GMDSS Instructor2

    RADIO THEORY & PROPAGATION

    This cycle can be represented by a sine function. The

    relationship between the current and the magnetic field

    strength induced in the conductor through which the current is

    flowing is shown in the diagram on the next page. Recall from

    the discussion above that this field strength is proportional to

    the magnitude of the current; that is, if the current is

    represented by a sine wave function, then so too will be the

    magnetic field strength resulting from that current. This

    characteristic shape of the field strength curve has led to the

    use of the term wave when referring to electromagnetic

    propagation. The maximum displacement of a peak from zero

    is called the amplitude. The forward side of any wave is called

    the wave front. For a nondirectional antenna, each wave

    proceeds out-ward as an expanding sphere (or hemisphere).

  • Hilmi ECE GMDSS Instructor3

    RADIO THEORY & PROPAGATION

    One cycle is a complete sequence of values, as from crest to

    crest. The distance traveled by the energy during one cycle is

    the wavelength, usually expressed in metric units (meters,

    centimeters, etc.). The number of cycles repeated during unit

    time (usually 1 second) is the frequency. This is given in hertz

    (cycles per second). A kilohertz (kHz) is 1,000 cycles per

    second. A megahertz (MHz) is 1,000,000 cycles per second.

    Wavelength and frequency are inversely proportional. The

    phase of a wave is the amount by which the cycle has

    progressed from a specified origin. For most purposes it is

    stated in circular measure, a complete cycle being considered

    360. Generally, the origin is not important, principal interest

    being the phase relative to that of some other wave.

  • Hilmi ECE GMDSS Instructor4

    RADIO THEORY & PROPAGATION

  • Hilmi ECE GMDSS Instructor5

    RADIO THEORY & PROPAGATION

    Units of Measuring Hertz

    We use the decimal system for simplicity and use the

    following designations in measuring the frequency:

    Hertz (Hz) 1 to 999 Hz

    Kilo Hertz (kHz) thousand 1,000 Hz

    Mega Hertz (MHz) million 1,000,000 Hz

    Giga Hertz (GHz) billion 1,000,000,000 Hz

    Examples: 2182.0 kHz is equal to 2,182,000 Hz

    156.8 MHz is equal to 156,800 kHz or

    156,800,000 Hz

  • Hilmi ECE GMDSS Instructor6

    RADIO THEORY & PROPAGATION

    Audio Frequencies (AF)

    The human ear responds to audio frequencies between

    20Hz and about 20kHz with the pitch of the note

    increasing with frequency.

    Above that, the human ear loses interest although other

    animals such as dogs and bats can hear higher

    frequencies. Human hearing becomes impaired with age

    and can be damaged by working in a noisy environment,

    the effect being to reduce the upper frequency limit.

    No problems are experienced unless the upper-frequency

    response falls to below 3kHz, which is the upper limit of

    human speech.

  • Hilmi ECE GMDSS Instructor7

    RADIO THEORY & PROPAGATION

    Electromagnetic Spectrum

    The entire range of electromagnetic radiation frequencies is

    called the electromagnetic spectrum. The frequency range

    suitable for radio transmission, the radio spectrum, extends

    from 10 kilohertz to 300,000 megahertz. It is divided into a

    number of bands, as shown in Table below.

    Below the radio spectrum, but overlapping it, is the audio

    frequency band, extending from 20 to 20,000 hertz. Above

    the radio spectrum are heat and infrared, the visible

    spectrum (light in its various colors), ultraviolet, X-rays,

    gamma rays, and cosmic rays. Waves shorter than 30

    centimeters are usually called microwaves.

  • Hilmi ECE GMDSS Instructor8

    RADIO THEORY & PROPAGATION

    Radio Frequency Spectrum

    ELF Extremely Low Frequency 300 Hz 3 kHz

    VLF Very Low Frequency 3 30 kHz Myriametric waves

    LF Low Frequency 30 300 kHz Kilometric waves

    MF Medium Frequency 300 3,000 kHz Hectometric waves

    HF High Frequency 3 MHz 30 MHz Decametric waves

    VHF Very High Frequency 30 300 MHz Metric waves

    UHF Ultra High Frequency 300 MHz 3 GHz Decimetrik waves

    SHF Super High Frequency 3 30 GHz Centimetric waves

    EHF Extremely High Frequency 30 300 GHz Millimetric wavesPlease Note: We do not use all of these frequencies in the Maritime Mobile

    Service, only a select portion of each

  • Hilmi ECE GMDSS Instructor9

    RADIO THEORY & PROPAGATION

  • Hilmi ECE GMDSS Instructor10

    RADIO THEORY & PROPAGATION

    Radio Wave Propagation

    This topic area deals with the path taken by a radio wave when

    it leaves the transmitting antenna. The main factor that

    determines the path taken by a radio wave is the frequency or

    wavelength of the transmission.

    Radio waves travel at the speed of light (300 x 106 meters per

    second). The relationship between the frequency and

    wavelength is expressed in the following formula:

    Frequency = Speed of Light Wavelength

  • Hilmi ECE GMDSS Instructor11

    RADIO THEORY & PROPAGATION

    This formula shows that the longer wavelength corresponds

    to lower frequencies.

    Such as a shorter wavelength corresponds to higher

    frequencies. We will be using this information later when we

    talk about antennas.

    Example: 150 MHz frequency is a 2 meter wavelength

    2 MHz frequency is a 150 meter wavelength

  • Hilmi ECE GMDSS Instructor12

    RADIO THEORY & PROPAGATION

    Radio communication is a wonderful thing. Via radio, we send

    messages at the speed of light over great distances.

    Messages can travel from one side of the earth to another, or

    to satellites orbiting a distant planet.

    By changing the frequency of transmission, our radio can

    communicate at different distances. Each frequency band has

    widely varying properties with respect to its range and

    behavior under different conditions. Knowing in advance what

    frequency to use in communicating with a distant station is the

    single most important part of learning to use your radio.

  • Hilmi ECE GMDSS Instructor13

    RADIO THEORY & PROPAGATION

    Approximate guide frequency bands and ranges (for 100 watt commercial services)

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    RADIO THEORY & PROPAGATION

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    RADIO THEORY & PROPAGATION

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    RADIO THEORY & PROPAGATION

  • Hilmi ECE GMDSS Instructor17

    RADIO THEORY & PROPAGATION

  • Hilmi ECE GMDSS Instructor18

    RADIO THEORY & PROPAGATION

    The three main modes of propagation of radio waves from

    transmitter (Tx) to receiver (Rx) in maritime radio

    communications are:

    Direct or Space Wave

    Ground Waves

    Sky Waves

  • Hilmi ECE GMDSS Instructor19

    RADIO THEORY & PROPAGATION

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    RADIO THEORY & PROPAGATION

  • Hilmi ECE GMDSS Instructor21

    RADIO THEORY & PROPAGATION

  • 22Hilmi ECE GMDSS Instructor

    Direct Wave Propagation

    Frequencies above 30 MHz use the Direct or Space Wave

    propagation. The radio waves leave the antenna in a

    straight line following a line of sight path. The radio

    waves do not follow the earths curvature, but will

    penetrate right through the ionosphere and out into space.

    For VHF communications the range depends on the

    height of both the transmitting and receiving antennas.

    For a ship, with an antenna mounted at the top of the

    mast, communicating with another ship with a similar

    antenna is approximately about 25nm.

    RADIO THEORY & PROPAGATION

  • Hilmi ECE GMDSS Instructor23

    RADIO THEORY & PROPAGATION

    Communication from a coast station can produce a

    greater range because the coast station antenna is at a

    greater height. In the same respect, communication from

    a smaller vessel, or a hand held portable, will produce a

    shorter range of communication.

    Remember: frequency band for VHF is 156mHz to 164

    MHz, and is limited to 25 watts of output power.

  • Hilmi ECE GMDSS Instructor24

    RADIO THEORY & PROPAGATION

    Ground Wave Propagation

    The common mode of propagation for medium frequency (MF

    1605 kHz to 3800 kHz) is Ground Wave, also known as

    surface wave. Radio waves leave the antenna and follow the

    earths curvature. As they travel over the sea, or land, energy

    is gradually lost, in technical term the wave is attenuated. The

    further away from a transmitter you are, the weaker the signal

    becomes, until eventually communication is lost. As ships

    transmitters are typically limited to a power of 400 watts.

    Maximum range for these frequencies is 300 nm. This will

    depend on ships transmitter power, and antenna efficiency

    and can range from 150 to 300 nm. The higher the frequency

    the shorter the range of the ground wave.

  • Hilmi ECE GMDSS Instructor25

    RADIO THEORY & PROPAGATION

    Sky Wave Propagation

    This is where radio waves are beamed up from the antenna

    towards the ionosphere and are refracted back to the earth.

    This gives a maximum range of about 4000 nm. Greater

    ranges, giving worldwide coverage, are obtained by multi-

    hop transmissions. A radio wave leaves the antenna then is

    refracted by the ionosphere back to the earth, refracted

    back to up to the ionosphere, then back again and so on.

  • Hilmi ECE GMDSS Instructor26

  • Hilmi ECE GMDSS Instructor27

    RADIO THEORY & PROPAGATION

    The ionosphere is layers of ionized gases in the upper

    atmosphere, ranging from about 50 to 300 miles above the

    earths surface. The density of the gas present and the

    level of ultraviolet radiation from the sun determine the

    degree of ionization.

    Thus the density and width of the ionosphere depends on

    the time of day or night, and the season, winter or summer.

    During the day, there are normally four layers, known as the

    D, E, F1, and F2 layers. At night the D layer disappears

    and the two F layers combine into one, leaving just the E

    and F layer for propagation.

  • Hilmi ECE GMDSS Instructor28

    RADIO THEORY & PROPAGATION

  • 29Hilmi ECE GMDSS Instructor

    RADIO THEORY & PROPAGATIOND Layer : 20-500kHz,

    E Layer : 500-2.000kHz,

    F1 Layer : 1.500-30.000kHz,

    F2 Layer : 3.000-30.000kHz

  • Hilmi ECE GMDSS Instructor3030

  • 31Hilmi ECE GMDSS Instructor

    RADIO THEORY & PROPAGATION

  • Hilmi ECE GMDSS Instructor32

    RADIO THEORY & PROPAGATION

    As the radio wave enters the ionosphere it suffers both

    attenuation and refraction. This is also known as weakening

    and bending of the radio waves in more non-technical terms.

    Both of these two effects are greater the lower the frequency

    used. If refraction is sufficient the wave is returned to the earth.

    Thus lower frequencies are returned from lower heights giving

    shorter ranges. There is a minimum range over which a

    particular frequency can communicate by sky waves, this is

    known as the skip distance. The higher the frequency, the

    greater the skip distance. The distance between the end of the

    ground (surface) wave and the skip distance is known as dead

    space, and no communications on this frequency can reach this

    area.

  • 33Hilmi ECE GMDSS Instructor

    RADIO THEORY & PROPAGATION

  • Hilmi ECE GMDSS Instructor34

    RADIO THEORY & PROPAGATION

    As a general rule, the greater the distance over which the

    communication is to take place the higher the frequency you

    should use. Where the signals can be heard on two bands,

    the higher one should be used to minimize attenuation. One

    could use tables, like the ones in the next chapter, which are a

    rough guide to the ranges that different frequencies can

    achieve at different times.

    Although the HF band covers the frequency range from 3 to 30

    MHz, only small sections have been allocated to different

    services. The marine service has been allocated bands of

    frequencies around 4 MHz, 6 MHz, 8 MHz, 12/13MHz, 16/17

    MHz, and 22 MHz.

  • Hilmi ECE GMDSS Instructor35

    RADIO THEORY & PROPAGATION

    The combination of the 12/13 and the 16/17 MHz bands are

    typically known as the 12 and 16 MHz bands, since this is

    where the ship transmits. The maximum limit on HF output

    power is 1500 watts or 1.5 kW.

  • Hilmi ECE GMDSS Instructor36

    RADIO THEORY & PROPAGATION

    Mode of Radio Emissions

    The World Administrative Radio Conference held in 1979

    assigned each emission a classification that uses a three-

    character identification. These settings determine how the

    modulation of the signal is to be done. If the radio were set

    on the wrong mode, it would not be able to properly receive

    the communication.

  • Hilmi ECE GMDSS Instructor37

    On the nomenclature

    RADIO THEORY & PROPAGATION

  • 38Hilmi ECE GMDSS Instructor

    Classification

    The class of emission is a set of characteristics conforming to

    below.

    Emissions shall be classified and symbolized according to their

    basic characteristics.

    The basic characteristics (see Sub-Section IIA) are:

    1) first symbol type of modulation of the main carrier;

    2) second symbol nature of signal(s) modulating the main

    carrier;

    3) third symbol type of information to be transmitted.

    RADIO THEORY & PROPAGATION

  • 39Hilmi ECE GMDSS Instructor

    Modulation used only for short periods and for incidental

    purposes (such as, in many cases, for identification or calling)

    may be ignored provided that the necessary bandwidth as

    indicated is not thereby increased.

    RADIO THEORY & PROPAGATION

  • 40Hilmi ECE GMDSS Instructor

    RADIO THEORY & PROPAGATION

  • 41Hilmi ECE GMDSS Instructor

    RADIO THEORY & PROPAGATION

  • 42Hilmi ECE GMDSS Instructor

    RADIO THEORY & PROPAGATION

  • Hilmi ECE GMDSS Instructor43

    RADIO THEORY & PROPAGATION

    A few examples of the different modes of emission classification

    that are used in the Maritime Mobile Service are:

    A1A Continuous Wave (Morse Code)

    F1B Radio telex & Navtex assignments along with DSC for VHF

    F3E Frequency Modulation (Voice in VHF)

    H3E Single Sideband full carrier (permitted on 2182 only)

    (a.k.a. AM)

    J3E Single Sideband (SSB) Suppressed Carrier (typical voice

    SSB frequencies)(USB)

    J2B DSC for MF/HF bands

  • Hilmi ECE GMDSS Instructor44

    F3E : VHF Radio Telephone (Frequency modulation)

    G3E : VHF Radio Telephone (Phase modulation-simplex chann.)

    G1B : Satellite EPIRB

    G2B : VHF DSC (1200 Baud)

    G2B : VHF DSC EPIRB

    H3E : Below of 1605kHz (and 2182kHz Watch receiver)

    J3E : MF-HF/SSB (above of 1605kHz)

    J2B : NBDP (Radio telex-MF/HF DSC-NAVTEX-Amplitute Mod.)

    F1B : NBDP (Radio telex-MF/HF DSC-NAVTEX-freq.Mod.)

    A1A : Mors (Radio-telgraphy)

    F1C/F3C: FAX (weather fax)

    A3E : 121,5MHz, 123,1MHz (VHF AERO)

    P0N : SART

    Frequently Used in modulations modes of emission

    classification in GMDSS

  • Hilmi ECE GMDSS Instructor45

    RADIO THEORY & PROPAGATION

    Most communication on MF & HF now use single-sideband

    (SSB) techniques for both speech and NBDP/telex

    transmissions. In a double-sideband transmission more than

    two thirds of the output power of the transmitter is contained in

    the carrier, which contains no useful signal information. Also,

    the upper and lower sidebands contain the same information.

    By eliminating the duplicated information in the lower sideband,

    along with the carrier, the transmitter efficiency is greatly

    increased. In effect, the space taken up within the frequency

    band is reduced and so more stations can have the ability to

    transmit.

  • Hilmi ECE GMDSS Instructor46

    RADIO THEORY & PROPAGATION

    A narrower bandwidth for the transmitted signal means less

    noise and interference is apparent at the receiver, resulting in

    a relatively smaller masking effect on the wanted

    transmission.

    Also, the same power is used more efficiently. The net effect

    is that, for the same transmitter power, the effective range of

    a transmission will be greatly extended by using a narrow-

    bandwidth method of modulation such as SSB.

  • Hilmi ECE GMDSS Instructor47

    RADIO THEORY & PROPAGATION

    Necessary bandwidth

    The necessary bandwidth, determined in accordance with the

    formulae and examples, shall be expressed by three numerals

    and one letter.

    The letter occupies the position of the decimal point and

    represents the unit of bandwidth. The first character shall be

    neither zero nor K, M or G.

    between 0.001 and 999 Hz shall be expressed in Hz (letter H);

    between 1.00 and 999 kHz shall be expressed in kHz (letter K);

    between 1.00 and 999 MHz shall be expressed in MHz (letter M);

    between 1.00 and 999 GHz shall be expressed in GHz (letter G).

  • Hilmi ECE GMDSS Instructor48

    RADIO THEORY & PROPAGATION

  • Hilmi ECE GMDSS Instructor49

    RADIO THEORY & PROPAGATION

    Single Sideband, SSB Modulation

    Single sideband modulation is a form of amplitude

    modulation. As the name implies, single sideband, SSB uses

    only one sideband for a given audio path to provide the final

    signal.

    Single sideband modulation, SSB, provides a considerably

    more efficient form of communication when compared to

    ordinary amplitude modulation. It is far more efficient in terms

    of the radio spectrum used, and also the power used to

    transmit the signal.

    In view of its advantages single sideband modulation has

    been widely used for many years, providing effective

    communications, as well as forms being used for some

    analogue television signals, and some other applications.

  • Hilmi ECE GMDSS Instructor50

    RADIO THEORY & PROPAGATION

    Single sideband

    modulation basics single

    sideband modulation can

    be viewed as an

    amplitude modulation

    signal with elements

    removed or reduced. In

    order to see how single

    sideband is created, it is

    necessary to use an

    amplitude modulated

    signal as the starting

    point.

  • 51Hilmi ECE GMDSS Instructor

    RADIO THEORY & PROPAGATION

  • Hilmi ECE GMDSS Instructor52

    RADIO THEORY & PROPAGATION

    From this it can be seen that the signal has two

    sidebands, each the mirror of the other, and the carrier.

    To improve the efficient of the signal, both in terms of the

    power and spectrum usage, it is possible to remove the

    carrier, or at least reduce it, and remove one sideband -

    one is the mirror image of the other.

    A single sideband signal therefore consists of a single

    sideband, and often no carrier, although the various

    variants of single sideband are detailed below.

  • 53Hilmi ECE GMDSS Instructor

    It can be seen that either the upper sideband or lower

    sideband can be used. There is no advantage between

    using either the upper or lower sideband. The main

    criterion is to use the same sideband as used by other

    users for the given frequency band and application. The

    upper sideband is more commonly used for professional

    applications.

    RADIO THEORY & PROPAGATION

  • Hilmi ECE GMDSS Instructor5454

    SINGLE SIDE BAND

    WINDOW

    FREQUENCY

    LSB USB

    DSB (AM) MODULATION

    1.4 kHz1.4 kHz

    SSB

    -2.8 kHz +2.8 kHz

  • Hilmi ECE GMDSS Instructor5555

    WINDOW

    FREQUENCY

    LSB USB

    1.4 kHz1.4 kHz

    -1,4 kHz +1,4 kHz2.8 kHz

    Example:

    2635kHz (assigned 2636.4kHz) and

    2638kHz (assigned 2639.4kHz) freqeucies

  • 56Hilmi ECE GMDSS Instructor

    Frequency Allacotions

    Regions and Areas

    For the allocation of frequencies the world has been

    divided into three Regions' as shown on the following

    map and described in below.

    RADIO THEORY & PROPAGATION

  • Hilmi ECE GMDSS Instructor57

    For the allocations of frequencies the world has been divided into

    three Regions as shown on the map

  • Frequencies vs. Channels

    In order to make radio communications more user

    friendly, the ITU has started assigning both simplex and

    duplex frequencies to predetermined channels. In the

    past all communications had to be set for both the

    transmitting and receiving frequencies, including on VHF

    radios.

    Hilmi ECE GMDSS Instructor58

    RADIO THEORY & PROPAGATION

  • The ITU agreed and started assigning channels to frequencies.

    Such as 156.8 MHz is assigned to channel 16.

    On the modern VHF radios, there are setting for US and

    International channels. These settings are for the need of the

    two different sets of channel to frequency assignments. Many

    of them are identical between the US and International, but

    some are different. The difference is that the US uses more

    simplex frequencies for communicating with CRSs and VTS

    stations, where International settings are use more duplex

    operations in these areas.

    Hilmi ECE GMDSS Instructor59

    RADIO THEORY & PROPAGATION

  • With the introduction of GMDSS and MF/HF communications

    for mariners who may not be as familiar with all the different

    frequencies and the different bands of the MF/HF system, it

    is the goal if the ITU to improve the system to make it

    friendlier like the VHF system. The goal was to be able to

    use a channel number to reference the correct frequency.

    Some manufactures had units that had the capability of

    programming frequently used frequencies in to memory and

    assign a quick reference number.

    Hilmi ECE GMDSS Instructor60

    RADIO THEORY & PROPAGATION

  • When looking in the different publications, the frequency list

    is typically broken into three columns. The first column is

    the Ship Receive or the Shore Transmit (either way it is

    expressed, it is the receive frequency you would have to

    program in). The third column is the Ship Transmit or Shore

    Receive.

    The middle column is typically the ITU channel.

    Hilmi ECE GMDSS Instructor61

    RADIO THEORY & PROPAGATION

  • Hilmi ECE GMDSS Instructor62

    RADIO THEORY & PROPAGATION

  • Hilmi ECE GMDSS Instructor63

    RADIO THEORY & PROPAGATION

  • Hilmi ECE GMDSS Instructor64

    WAVELENGTH-TO-FREQUENCY CONVERSIONS

    Radio waves are often referred to by their wavelength in

    meters rather than by frequency. For example, most people

    have heard commercial radio stations make announcements

    similar to the following: "Station WXYZ operating on 240

    meters..." To tune receiving equipment that is calibrated by

    frequency to such a station, you must first convert the

    designated wavelength to its equivalent frequency. As

    discussed earlier, a radio wave travels 300,000,000 meters a

    second (speed of light); therefore, radio wave of 1 hertz would

    have traveled a distance (or wavelength) of 300,000,000

    meters. Obviously then, if the frequency of the wave is

    increased to 2 hertz, the wavelength will be cut in half

    to150,000,000 meters. This illustrates the principle that the

    HIGHER THE FREQUENCY, the SHORTERTHE

    WAVELENGTH.

    RADIO THEORY & PROPAGATION

  • Wavelength-to-frequency

    conversions of radio waves

    are really quite simple

    because wavelength and

    frequency are reciprocals:

    Either one divided into the

    velocity of a radio wave

    yields the other.

    Remember, the formula for

    wavelength is:

    Hilmi ECE GMDSS Instructor65

    RADIO THEORY & PROPAGATION

    The wavelength in meters divided into 300,000,000 yields

    the frequency of a radio wave in hertz. Likewise, the

    wavelength divided into 300,000 yields

    the frequency of a radio wave in kilohertz, and the wavelength

    divided into 300 yields the frequency in megahertz.