mobile antennas v1

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    Basic Antenna Theory and

    Concepts

    1

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    Introduction

    Antenna or aerial is a transducer

    antennas convert electromagnetic waves into electrical

    currents and vice versa

    An antenna is an electrical conductor or system of

    conductors

    Transmission - radiates electromagnetic energy into

    space Reception - collects electromagnetic energy from space

    Antenna application

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    Introduction

    Two important points:

    Antennas are passive devices

    Antennas are reciprocal devices

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    Antenna Definition

    An antenna is a circuit element thatprovides a transition from a guided

    wave on a transmission line to a freespace wave and it provides for thecollection of electromagnetic energy.

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    Antenna Definition-contd

    In transmit systems the RF signal isgenerated, amplified, modulated and

    applied to the antenna In receive systems the antenna collects

    electromagnetic waves that arecutting through the antenna andinduce alternating currents that areused by the receiver

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    Reciprocity

    An antenna ability to transfer energy form

    the atmosphere to its receiver with the same

    efficiency with which it transfers energyfrom the transmitter into the atmosphere

    Antenna characteristics are essentially the

    same regardless of whether an antenna issending or receiving electromagnetic energy

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    Simple Antennas

    Isotropic antenna (idealized)

    Radiates power equally in all directions

    it has zero size

    efficient

    used as reference antenna i.e. gain and directionality of

    other antennas are compared with isotropic antenna

    isotropic antenna cannot be built and tested but itscharacteristics are simple and easy to derive

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    Simple Antennas..

    Dipole antennas

    has two parts: two wires pointed in opposite directions

    arranged either horizontally or vertically, with one end

    of each wire connected to the device and the other endhanging free in space.

    Half-wave dipole antenna (or Hertz antenna)

    Quarter-wave vertical antenna (or Marconi antenna)

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    Length of half wave dipole antenna

    Typically the length of a half-wave dipole is95% of one-half the wavelength measured infree space

    Assumption: antenna conductor diameter ismuch less than the length of the antenna.

    The free space wavelength is given by

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    Length of half wave dipole antenna

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    Problem 1

    Calculate the length of a half-wavedipole for an operating frequency of200MHz

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    Dipole Antenna

    Hertz antennas are not found at frequenciesbelow 2MHz because of the physical sizeneeded of the antenna to represent a half-

    wave Vertical Antennas or marconi are used for

    frequencies under 2 MHz. It uses aconducting path to ground that acts as

    wavelength portion the antenna above theground. The above ground structurerepresents a /4 wavelength

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    Antenna Characteristics

    Radiation Pattern: The radiation pattern or antennapattern describes the relative strength of the radiated field

    in various directions from the antenna, at a constant

    distance. The radiation pattern is a reception pattern as well, since it

    also describes the receiving properties of the antenna.

    The radiation pattern is three-dimensional, but usually the

    measured radiation patterns are a two-dimensional slice of

    the three-dimensional pattern, in the horizontal or vertical

    planes.

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    Radiation Pattern... Horizontal Plane Vertical Plane

    Angle of Elevation: Vertical

    angle measured upward fromthe ground

    Representation of radiationpattern

    The three dimensionalrepresentation

    Two dimensional horizontal andvertical plane representation

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    3dimensional representation

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    2-dimensional pattern

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    2-dimensional pattern

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    Far-field and Near-field

    Near-field region: the observer close to theantenna

    Far-field region: an observer must be farenough away from the antenna that any localcapacitive or inductive coupling is negligible

    Radiation patterns are valid only in the far-

    field region;

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    Comparison of different antennas

    Reference antennas : isotropic or half-wave dipoleantennas are used

    The gain of the antenna may be expresses indecibels with respect to a half wavelength dipole or

    isotropic antenna dBdgain of an antenna expressed in decibels with

    respect to a half wave dipole antenna dBi gain of an antenna expressed in decibels with

    respect to a half wave isotropic antenna

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    Comparison of different antennas

    Since the gain of a dipole is 2.14 dBi, the gainof any antenna in dBd is 2.14 dB less than thegain of the same antenna expressed in dBi.

    That is,

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    Problem 2

    Two antennas have gains of 5.3 dBi and4.5 dBd, respectively. Which hasgreater gain?

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    Antenna Gain

    Antenna gain

    Power output, in a particular

    direction, compared to that

    produced in any direction by a

    perfect omnidirectional

    antenna (isotropic antenna)

    Antenna gain is themeasure in dB how much

    more power an antenna willradiate in a certain directionwith respect to that whichwould be radiated by a

    reference antenna

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    Antenna Gain

    Effective area

    Related to physical size and shape of antenna

    Relationship between antenna gain and effective area

    G = antenna gain

    Ae= effective area f = carrier frequency

    c = speed of light ( 3 108m/s)

    = carrier wavelength

    2

    2

    2

    44

    cAfAG ee

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    Directivity

    Sometimes the term directivity is used.

    This is not quite the same as gain. Directivity is thegain calculated assuming a lossless antenna. Real

    antennas have losses, and gain is simply thedirectivity multiplied by the efficiency of theantenna, that is:

    G =D

    where

    D = directivity, as a ratio (not in dB)

    G = gain, as a ratio (not in dB)

    = efficiency

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    Directivity

    When an antenna is used for transmitting, the totalpower emitted by the antenna is less than thatdelivered to it by the feedline.

    the efficiency as = Pr / Pt

    where = antenna efficiencyPr = radiated powerPt = power supplied to the antenna

    The figure of 2.14 dBi we have been using for thegain of a lossless dipole is also the directivity for anydipole.

    To find the gain of a real (lossy) dipole, it isnecessary first to convert the decibel directivity to apower ratio, then to multiply by the efficiency.

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    Problem 3

    A dipole antenna has an efficiency of85%. Calculate its gain in decibels.

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    Solution

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    Beamwidth

    Beamwidthis the angular separation ofthe half-power points of the radiatedpattern

    half-power pointsare also the points atwhich the power density is 3 dB less than it isat its maximum point.

    Half-wave dipole has a beamwidth of about78 in one plane and 360 in the other.

    Many antennas are much more directionalthan this, with a narrow beam in both planes.

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    beamwidth

    antenna

    A

    Power 3dB down

    from maximum

    point A

    Max power

    2 dipole

    Beamwidth of Directional Antenn

    Radiated energy is

    focused in a specific

    direction

    R di ti tt f

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    Radiation pattern ofunidirectional antenna

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    Major and Minor lobes

    Polar Plot

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    Major and Minor lobes

    The main beam(or main lobeor major lobe) is the regionaround the direction of maximum radiation (usually theregion that is within 3 dB of the peak of the main beam).

    The sidelobesare smaller beams that are away from the

    main beam. These sidelobes are usually radiation inundesired directions which can never be completelyeliminated.

    The sidelobe level (or sidelobe ratio) is an importantparameter used to characterize radiation patterns. It is themaximum value of the sidelobes away from the main beamand is expressed in Decibels.

    One sidelobe is called backlobe. This is the portion ofradiation pattern that is directed opposing the main beam

    direction.

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    Home work

    Polar plot

    Rectangular plot

    what is sidelobe ratio?

    what is front to back ratio?