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The field radiated by a small linear antenna is not distributed uniformly
in the direction perpendicular to the axis of the antenna. As in case of a
short dipole, the maximum radiation takes place in the direction right
angles to the axis of the dipole.
So this non-uniform radiation characteristics may be used for many
broadcast services. But such a characteristics are not preferred in point
to point communication.
In the point to point communication, it is desired to have most of the
energy radiated in one particular direction. That means it is desired to
have greater directivity in a desired direction particularly which is not
possible with single dipole antenna.
Hence to increase the field strength in the desired direction by using
group of antennas excited simultaneously. Such a group of antennas is
called array of antennas or simply antenna array.
Thus antenna array can be defined as the system of similar antennas
directed to get required high directivity in the desired direction. In
general, antenna array is the radiating system in which several antennas
are spaced properly so as to get greater field strength at a far distance
from the radiating system by combining radiations at point from all the
antennas in the system.
In general, the total field produced by the antenna array at a far distance
is the vector sum of the fields produced by the individual antennas of the
array. The individual element is generally called element of an antenna
array.
The antenna array is said to linear if the elements of the antenna array
are equally spaced along a straight line. The linear antenna array is said
to be uniform linear array if all the elements are fed with a current of
equal magnitude with progressive uniform phase shift along the line.
Antenna array is a radiating system in which individual array elements
contribute to obtain maximum field strength in the desired direction;
while cancelling the individual field strength in all other directions to get
maximum directivity in the desired direction.
Practically various forms of the antenna array are used as radiating
systems. Some of the practically used forms are as follows
1. Broadside Array
2. End fire Array
3. Collinear Array
4. Parasitic Array
Broadside Array
This form of the antenna array is one of the
most important practical forms used in
practice. The broadside array is the array of
antennas in which all the elements are placed
parallel to each other and the direction of
maximum radiation is always perpendicular to
the plane consisting elements.
A typical arrangement of a Broadside array is as shown in the Fig. A
broadside array consists number of identical antennas placed parallel to
each other along a straight line.
This straight line is perpendicular to the axis of individual antenna
known as axis of antenna array. Thus each element is perpendicular to
the axis of antenna array.
Broadside Array
All the individual antennas are spaced equally along the axis of antenna
array. The spacing between any two elements is denoted by 'd'. All the
elements are fed with currents with equal magnitude and same phase.
As the maximum radiation is directed in broadside direction i.e.
perpendicular to the line of axis of array, the radiation pattern for the
broadside array is bidirectional.
Thus we can define broadside array as the arrangement of antennas in
which maximum radiation is in the direction perpendicular to the axis of
array and plane containing the elements of array.
Consider two isotropic point sources spaced equally with respect to the
origin of the co-ordinate system as shown in the Fig. Assume that the
two point sources are with equal amplitude and phase.
Broadside Array
Consider that point P is far away from the origin. Let the distance of
point from origin be r.
The wave radiated by radiator A2 will reach point P as compared to that
radiated by radiator A1 This is due to the path difference that the wave
radiated radiator A, has to travel extra distance. Hence the path
difference is given by.
End Fire Array
The end fire array is very much similar to the broadside array from the
point of view of arrangement. But the main difference is in the direction
of maximum radiation. In broadside array, the direction of the
maximum radiation is perpendicular to the axis of array; while in the
end fire array, the direction of the maximum radiation is along the axis
of array.
Thus in the end fire array number of identical antennas are spaced
equally along a line. All the antennas are fed individually with currents
of equal magnitudes but their phases vary progressively along the line
to get entire arrangement unidirectional finally. i.e. maximum radiation
along the axis of array. Thus end fire array can be defined as an array
with direction of maximum radiation coincides with the direction of the
axis of array to get unidirectional radiation.
Collinear Array
As the name indicates, in the collinear array, the antennas are
arranged co-axially i.e. the antennas are arranged end to end along a
single line as shown in the Fig.
The individual elements in the
collinear array are fed with
currents equal in magnitude and
phase. This condition is similar to
the broadside array.
In collinear array the direction of maximum radiation is
perpendicular to the axis of array. So the, radiation pattern of
the collinear array and the broadside array is very much
similar but the radiation pattern of the collinear array has
circular symmetry with main lobe perpendicular everywhere
to the principle axis. Thus the collinear array is also called
omnidirectional array or broadcast array.
Collinear Array
The gain of the collinear array is maximum if the spacing between
the elements is of the order of 0.3λ to 0.5λ. But this small spacing
introduces constructional and feeding problems.
To overcome this difficulty, the elements of the array are operated
with their ends very close to each other by connecting ends by an
insulator.
The power gain of the collinear array does not increase in proportion
with number of elements. For example, for 2-element array power
gain is 1.9dB, for 4-element array it is not equal to twice
of the power gain for 2-element array but it is simply equal to 4.3 dB
But practically 2-element collinear array is used as it allows
multiband operation. It generally known as two half waves in phase.
Parasitic Array
In order to overcome feeding problems of the antenna, sometimes,
the elements of the array are fed through the radiation from the
nearby element.
The array of antennas in which the parasitic elements get the power
through electromagnetic coupling with driven element which is in
proximity with the parasitic element is known as parasitic array.
The simplest form of the parasitic array consists one driven element
and one parasitic element. In multielement parasitic array, there may
be one or more driving elements and also one or more parasitic
elements. So in general the multielement parasitic array is the
array with at least one driven element and one or more parasitic
elements.
Parasitic Array
The common example of the parasitic array with linear half wave
dipoles as elements of array is Yagi-Uda array or simply Yagi antenna.
The amplitude and the phase of the current induced in the parasitic
element depends on the spacing between the driven element and
parasitic element.
To make the radiation pattern unidirectional, the relative phases of
the currents are changed by adjusting the spacing between the
elements. This is called tuning of array.
For a spacing between the driven and parasitic element equal to λ/4
and phase difference of radian, unidirectional radiation pattern is
obtained.
2

Array of Point Sources
The array of point sources is nothing but the array of an isotropic
radiators occupying zero volume.
Let us consider the array of two isotropic point sources, with a
distance of separation 'd' between them. The polarization of two
isotropic point sources is assumed to be the same.
To derive different expressions following conditions can be applied to
the antenna array
i) Two point sources with currents of equal magnitudes and with
same phase.
ii) Two point sources with currents of equal magnitude but with
opposite phase.
iii) Two point sources with currents of unequal magnitudes and with
opposite phase.
Phased Array
Consider a three element array as shown in the Fig. The element
of array is considered as λ/2 dipole. All the cables used are of same
length. All the three cables are brought together at common feed
point.
Here mechanical switches are used. Such switch is installed one at
each antenna and one at a common feed point. All Feed point switch
the switches are ganged together.
To receiver Thus by operating switch,
the beam can be shifted to any phase
shift.
Phased Array
To make operation reliable and at elements and feed point
simple, the ganged mechanical switch is replaced by PIN dipole which
acts as electronic switch. But for precision in results, the number of
cables should be minimized.
Phased Array
In many applications phase shifter is used instead of controlling
phase by switching cables. It can be achieved by using ferrite device.
The conducting wires are wrapped around the phase shifter.
The current flowing through these wires controls the magnetic
field within ferrite and then the magnetic field in the ferrite controls
the phase shift.
The phased array for specialized functional utility are recognized by
different names such as frequency scanning array, retroarray and
adoptive array.
The array in which the phase change is controlled by varying the
frequency is called frequency scanning array. This is found to be the
simplest phased array as at each element separate phase control is
not necessary.
Phased Array
A simple transmission line fed frequency scanning array as shown in
the Fig
Each element of the scanning array is fed by a transmission line via
directional coupler. Note that the directional couplers are fixed in
position, while the beam scanning is done with a frequency change.
To avoid reflections and to obtain pure form of the travelling wave,
the transmission line is properly terminated of the load.
The main advantage of the frequency
scanning array is that there are no
moving parts and no switches and
phase shifters are required.
Phased Array
The array which automatically reflects an incoming signal back to the
source is called retroarray. It acts as a retroreflector similar to the
passive square corner reflector.
That means the wave incident on the array is received and
transmitted back in the same direction.
In other words, each element of the retroarray reradiates signal
which is actually the conjugate of the received one. Simplest form of
the retroarray is the Van Atta array as shown in the Fig. in which 8
identical λ/2 dipole elements are used, with pairs formed between
elements 1 and 8, 2 and 7, 3 and 6, 4 and 5 using cables of equal
length.
If the wave arrives at angle φ say then it gets transmitted in the same
direction.
Phased Array
An array which automatically turn the maximum beam in the desired
direction while turn the null in the undesired direction is called
adoptive array.
The adoptive array adjust itself in the desired direction with
awareness of its environment. In modern adoptive arrays, the output
of each element in the array is sampled, digitized and then
processed using computers. Such arrays are commonly called smart
antennas.

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Antenna Arrays.pdf

  • 1. The field radiated by a small linear antenna is not distributed uniformly in the direction perpendicular to the axis of the antenna. As in case of a short dipole, the maximum radiation takes place in the direction right angles to the axis of the dipole. So this non-uniform radiation characteristics may be used for many broadcast services. But such a characteristics are not preferred in point to point communication. In the point to point communication, it is desired to have most of the energy radiated in one particular direction. That means it is desired to have greater directivity in a desired direction particularly which is not possible with single dipole antenna. Hence to increase the field strength in the desired direction by using group of antennas excited simultaneously. Such a group of antennas is called array of antennas or simply antenna array.
  • 2. Thus antenna array can be defined as the system of similar antennas directed to get required high directivity in the desired direction. In general, antenna array is the radiating system in which several antennas are spaced properly so as to get greater field strength at a far distance from the radiating system by combining radiations at point from all the antennas in the system. In general, the total field produced by the antenna array at a far distance is the vector sum of the fields produced by the individual antennas of the array. The individual element is generally called element of an antenna array. The antenna array is said to linear if the elements of the antenna array are equally spaced along a straight line. The linear antenna array is said to be uniform linear array if all the elements are fed with a current of equal magnitude with progressive uniform phase shift along the line.
  • 3.
  • 4. Antenna array is a radiating system in which individual array elements contribute to obtain maximum field strength in the desired direction; while cancelling the individual field strength in all other directions to get maximum directivity in the desired direction. Practically various forms of the antenna array are used as radiating systems. Some of the practically used forms are as follows 1. Broadside Array 2. End fire Array 3. Collinear Array 4. Parasitic Array
  • 5. Broadside Array This form of the antenna array is one of the most important practical forms used in practice. The broadside array is the array of antennas in which all the elements are placed parallel to each other and the direction of maximum radiation is always perpendicular to the plane consisting elements. A typical arrangement of a Broadside array is as shown in the Fig. A broadside array consists number of identical antennas placed parallel to each other along a straight line. This straight line is perpendicular to the axis of individual antenna known as axis of antenna array. Thus each element is perpendicular to the axis of antenna array.
  • 6. Broadside Array All the individual antennas are spaced equally along the axis of antenna array. The spacing between any two elements is denoted by 'd'. All the elements are fed with currents with equal magnitude and same phase. As the maximum radiation is directed in broadside direction i.e. perpendicular to the line of axis of array, the radiation pattern for the broadside array is bidirectional. Thus we can define broadside array as the arrangement of antennas in which maximum radiation is in the direction perpendicular to the axis of array and plane containing the elements of array. Consider two isotropic point sources spaced equally with respect to the origin of the co-ordinate system as shown in the Fig. Assume that the two point sources are with equal amplitude and phase.
  • 7. Broadside Array Consider that point P is far away from the origin. Let the distance of point from origin be r. The wave radiated by radiator A2 will reach point P as compared to that radiated by radiator A1 This is due to the path difference that the wave radiated radiator A, has to travel extra distance. Hence the path difference is given by.
  • 8. End Fire Array The end fire array is very much similar to the broadside array from the point of view of arrangement. But the main difference is in the direction of maximum radiation. In broadside array, the direction of the maximum radiation is perpendicular to the axis of array; while in the end fire array, the direction of the maximum radiation is along the axis of array. Thus in the end fire array number of identical antennas are spaced equally along a line. All the antennas are fed individually with currents of equal magnitudes but their phases vary progressively along the line to get entire arrangement unidirectional finally. i.e. maximum radiation along the axis of array. Thus end fire array can be defined as an array with direction of maximum radiation coincides with the direction of the axis of array to get unidirectional radiation.
  • 9. Collinear Array As the name indicates, in the collinear array, the antennas are arranged co-axially i.e. the antennas are arranged end to end along a single line as shown in the Fig. The individual elements in the collinear array are fed with currents equal in magnitude and phase. This condition is similar to the broadside array. In collinear array the direction of maximum radiation is perpendicular to the axis of array. So the, radiation pattern of the collinear array and the broadside array is very much similar but the radiation pattern of the collinear array has circular symmetry with main lobe perpendicular everywhere to the principle axis. Thus the collinear array is also called omnidirectional array or broadcast array.
  • 10. Collinear Array The gain of the collinear array is maximum if the spacing between the elements is of the order of 0.3λ to 0.5λ. But this small spacing introduces constructional and feeding problems. To overcome this difficulty, the elements of the array are operated with their ends very close to each other by connecting ends by an insulator. The power gain of the collinear array does not increase in proportion with number of elements. For example, for 2-element array power gain is 1.9dB, for 4-element array it is not equal to twice of the power gain for 2-element array but it is simply equal to 4.3 dB But practically 2-element collinear array is used as it allows multiband operation. It generally known as two half waves in phase.
  • 11. Parasitic Array In order to overcome feeding problems of the antenna, sometimes, the elements of the array are fed through the radiation from the nearby element. The array of antennas in which the parasitic elements get the power through electromagnetic coupling with driven element which is in proximity with the parasitic element is known as parasitic array. The simplest form of the parasitic array consists one driven element and one parasitic element. In multielement parasitic array, there may be one or more driving elements and also one or more parasitic elements. So in general the multielement parasitic array is the array with at least one driven element and one or more parasitic elements.
  • 12. Parasitic Array The common example of the parasitic array with linear half wave dipoles as elements of array is Yagi-Uda array or simply Yagi antenna. The amplitude and the phase of the current induced in the parasitic element depends on the spacing between the driven element and parasitic element. To make the radiation pattern unidirectional, the relative phases of the currents are changed by adjusting the spacing between the elements. This is called tuning of array. For a spacing between the driven and parasitic element equal to λ/4 and phase difference of radian, unidirectional radiation pattern is obtained. 2 
  • 13. Array of Point Sources The array of point sources is nothing but the array of an isotropic radiators occupying zero volume. Let us consider the array of two isotropic point sources, with a distance of separation 'd' between them. The polarization of two isotropic point sources is assumed to be the same. To derive different expressions following conditions can be applied to the antenna array i) Two point sources with currents of equal magnitudes and with same phase. ii) Two point sources with currents of equal magnitude but with opposite phase. iii) Two point sources with currents of unequal magnitudes and with opposite phase.
  • 14. Phased Array Consider a three element array as shown in the Fig. The element of array is considered as λ/2 dipole. All the cables used are of same length. All the three cables are brought together at common feed point. Here mechanical switches are used. Such switch is installed one at each antenna and one at a common feed point. All Feed point switch the switches are ganged together. To receiver Thus by operating switch, the beam can be shifted to any phase shift.
  • 15. Phased Array To make operation reliable and at elements and feed point simple, the ganged mechanical switch is replaced by PIN dipole which acts as electronic switch. But for precision in results, the number of cables should be minimized.
  • 16. Phased Array In many applications phase shifter is used instead of controlling phase by switching cables. It can be achieved by using ferrite device. The conducting wires are wrapped around the phase shifter. The current flowing through these wires controls the magnetic field within ferrite and then the magnetic field in the ferrite controls the phase shift. The phased array for specialized functional utility are recognized by different names such as frequency scanning array, retroarray and adoptive array. The array in which the phase change is controlled by varying the frequency is called frequency scanning array. This is found to be the simplest phased array as at each element separate phase control is not necessary.
  • 17. Phased Array A simple transmission line fed frequency scanning array as shown in the Fig Each element of the scanning array is fed by a transmission line via directional coupler. Note that the directional couplers are fixed in position, while the beam scanning is done with a frequency change. To avoid reflections and to obtain pure form of the travelling wave, the transmission line is properly terminated of the load. The main advantage of the frequency scanning array is that there are no moving parts and no switches and phase shifters are required.
  • 18. Phased Array The array which automatically reflects an incoming signal back to the source is called retroarray. It acts as a retroreflector similar to the passive square corner reflector. That means the wave incident on the array is received and transmitted back in the same direction. In other words, each element of the retroarray reradiates signal which is actually the conjugate of the received one. Simplest form of the retroarray is the Van Atta array as shown in the Fig. in which 8 identical λ/2 dipole elements are used, with pairs formed between elements 1 and 8, 2 and 7, 3 and 6, 4 and 5 using cables of equal length. If the wave arrives at angle φ say then it gets transmitted in the same direction.
  • 19. Phased Array An array which automatically turn the maximum beam in the desired direction while turn the null in the undesired direction is called adoptive array. The adoptive array adjust itself in the desired direction with awareness of its environment. In modern adoptive arrays, the output of each element in the array is sampled, digitized and then processed using computers. Such arrays are commonly called smart antennas.