Antenna Array Tutorial for dummies making of.pdf

Principles of antenna arrays

1. Array Antenna
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Antenna Array
Chapter 3

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Introduction
•Usually the radiation patterns of single-element antennas are
relatively wide. i.e., they have relatively low directivity (gain).
•In long distance communications, antennas with high
directivity are often required. Such antennas are possible to
construct by enlarging the dimensions of the radiating
aperture (maximum size much larger than λ).
•This approach however may lead to the appearance of multiple
side lobes. Besides, the antenna is usually large and difficult to
fabricate.

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Introduction cont.
•Another way to increase the electrical size of an antenna is to
construct it as an assembly of radiating elements in a proper
electrical and geometrical configuration –as known as
antenna array.
•Usually, the array elements are identical.
•This is not necessary but it is practical and simpler for design
and fabrication.
•The individual elements may be of any type (wire dipoles,
loops, apertures, etc.)

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Five basic methods
•To control the overall antenna pattern:
a)the geometrical configuration of the overall array (linear, circular,
spherical, rectangular, etc.)
b)the relative placement of the elements.
c)the excitation amplitude of the individual elements.
d)the excitation phase of each element.
e)the individual pattern of each element.

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Radiation Pattern
•Radiationpatternofarrayantennais
calledanArrayFactor(AF).
•Arrayfactorcanbeexpressedusing
thisformula:)
2
sin(
)
2
sin(


N
N
AF=
Where :
N = Total Element
k = 2π/ λ
is the polar angle
is the difference of phase between
any two successive elements
forming thearray.

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Array Antenna
•At the end of the chapter, you should able:
–What is the array antenna application
–What is array factor and how to determine it
–What is the radiation pattern for array antenna look like

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Radiation pattern for vertical plane
(a)Single halfwavedipole
(b) two-elemen array
(c) Three element array.
(a)Single halfwave dipole
(b) two-elemen array
(c) Three element array.

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Why An Array of Antenna?
•Single element is relatively wide and low gain (directivity)
•To have very high gain and long distance antenna, this can be accomplished
by increasing the electrical size of the antenna
•Enlarge dimensions of the antenna without increasing the size of individual
elements is to form an assembly of radiating elements in an electrical and
geometrical configuration
•This new antenna, formed by multielements, is referred to as an array
•Most cases, the elements of an array are identical
•The total field is determined by the vector addition of the fields radiated by
the individual elements

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Antenna Array Application
•An array is widely used as a base-station antenna for mobile
communication
•Each four-element array is used to cover an angular sector of
120
o

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Antenna Array Application
•Yagi-Uda array is used to TV and Amerteur radio application
•Log periodic antenna is used for TV with wider bandwidth
YagiUda
Log periodic

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Examples of antenna arrays
•Four-elementmicrostripantenna array (phased array).

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•Cell-tower Antenna Array. These Antenna Arrays are typically
used in groups of 3 (2 receive antennas and 1 transmit
antenna)

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Array Theory
•Configuration of individual radiating elements that are
arranged in space and can be used to produce a directional
radiation pattern
•Allows shaping of radiation pattern
–Narrow beam
–Low sidelobe
–Higher gain & directivity
•Arrays usually employ identical antenna elements

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Advantages of using antenna arrays
Antenna arrays are becoming increasingly important in wireless
communications.
1.They can provide the capability of a steerable beam (radiation
direction change) as in smart antennas.
2.They can provide a high gain (array gain) by using simple
antenna elements.
3.They provide a diversity gain in multipath signal reception.
4.They enable array signal processing.

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Far-Field Expression of An Antenna Array

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Uniform Liner Arrays (ULAs)

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Two element array
•Let us assume, that two infinitesimal horizontal dipole antennas positioned along the z-axis as depict
in figure below.
•The total field of the array is determined by the vector addition of the fields radiated by the
individual elements.
•The electric field pattern in the y-z plane for one element is given by:

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The far-field approximation
•The far field approximation of this two element array can be
illustrated as in figure below:

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Derivation Array Factor (1)

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Derivation Array Factor (2)

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Pattern Multiplication (1)

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Pattern Multiplication (2)
•The concept of pattern multiplication valid for arrays with any
number of identical elements.
•So each array has its own array factor (AF).
•The total pattern, therefore, can be controlled via the single-
element pattern or via the AF of an array can be obtained by
replacing the actual elements with isotropic sources.
•The AF, in general, depends on:
–Number of elements.
–Relative excitation (magnitudes and phases).
–Spacing between the elements.

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N-element Linear Array with Uniform
Amplitude and Spacing

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As we aim at obtaining the normalized AF, we will neglecting the
phase factor, which gives

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Typical Radiation Pattern

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Direction of Maximum Radiation

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•An array is said to be End-fire array if the main beam is along
the axis of the array.
•An array is said to be Broadside array if the main beam is
perpendicular to the axis of the array.
•There are two end-fire directions for an array but the
broadside is a plane perpendicular to the array axis (see Fig
below)

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Directions of Nulls

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Terminology
Antenna–structureordeviceusedtocollectorradiateelectromagneticwaves
Array–assemblyofantennaelementswithdimensions,spacing,andilluminationsequencesuchthatthe
fieldsoftheindividualelementscombinetoproduceamaximumintensityinaparticulardirection
andminimumintensitiesinotherdirections
Beamwidth–theanglebetweenthehalf-power(3-dB)pointsofthemainlobe,whenreferencedtothepeak
effectiveradiatedpowerofthemainlobe
Directivity–theratiooftheradiationintensityinagivendirectionfromtheantennatotheradiationintensity
averagedoveralldirections
Effectivearea–thefunctionalequivalentareafromwhichanantennadirectedtowardthesourceofthe
receivedsignalgathersorabsorbstheenergyofanincidentelectromagneticwave
Efficiency–ratioofthetotalradiatedpowertothetotalinputpower
Farfield–regionwherewavefrontisconsideredplanar
Gain–ratioofthepowerattheinputofaloss-freeisotropicantennatothepowersuppliedtotheinputof
thegivenantennatoproduce,inagivendirection,thesamefieldstrengthatthesamedistance
Isotropic–radiatesequallyinalldirections
Mainlobe–thelobecontainingthemaximumpower
Null– azoneinwhichtheeffectiveradiatedpowerisataminimumrelativetothemaximumeffective
radiationpowerofthemainlobe
Radiationpattern–variationofthefieldintensityofanantennaasanangularfunctionwithrespecttotheaxis
Radiationresistance–resistancethat,ifinsertedinplaceoftheantenna,wouldconsumethatsameamountof
powerthatisradiatedbytheantenna
Sidelobe–alobeinanydirectionotherthanthemainlobe

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Tutorial for Array Antenna (1)
A three elements array of isotropic sources has the phase and
the magnitude relationship as shown in figure below. The
spacing between the elements is d =
λ
2
.
(i) Find the array factor
(ii) Find the nulls
z
y
-1
-j
+1
#2
#1
#3
d
d

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Tutorial for Array Antenna (2)
four isotropic sources with spacing d between them are placed
along the z-axis as shown in figure below. Assuming that the
amplitudes of elements #1 and #2 are +1 and the amplitudes of
elements #3 and #4 are -1, find the,
(i)The array factor.
(ii)The nulls when d= λ/2
#4
y
-1
-j
+1
#2
#1
#3
d
d
-j
z
d/2
d/2