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8/10/2019 2. Electronics - Ijecierd - Design of Dipole Arrays for the - Surendra Kumar (1)
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DESIGN OF DIPOLE ARRAYS FOR THE GENERATION OF MULTIPLE BEAMS
M SURENDRA KUMAR1
, A. GAYATRI2
& S. S. MADHAVI3
1Principal, KLR College of Engineering & Technology, Paloncha, Khammam, Telangana, India
2Assistant Professor, GITAM University, Visakhapatnam, Andhra Pradesh, India
3Associate Professor, KLR College of Engineering & Technology, Paloncha, Khammam, Telangana, India
ABSTRACT
A Dipole is a basic linear bi directional antenna available in different multiple of wave lengths like multiple of ,
/2 and /4 etc, Dipoles are very popularly used in variety of applications in wireless communications systems.
The works on the antennas for the generation of multiple beams are limited as reported in the literature. In view of this,in the present paper, desired numbers of multiple beams are generated from the arrays of dipole radiators and are compared
with the elements isotropic arrays. Taylors amplitude distribution is modified and is used for this paper. The design is
carried out for arrays of 20, 40 and 60 number of elements. The data on the patterns are generated and are useful in
wireless communication and Radar communication.
KEYWORDS:Dipole, Array Antennas, Multiple Beams, Taylors Amplitude Distribution, Radar Communication
INTRODUCTION
Wireless communication demands of spectral efficiency, antenna arrays increase the capacity of spectral
efficiency and the capacity depends mainly on the channel and the antenna characteristics. The capacity can be improved
by proper design of antenna elements and choosing appropriate array configuration and frequency bands [1].
A double-sided and center-feed of printed dipole antenna for dual-band WLAN applications was reported.
An advanced C-shaped parasitic strip with an asymmetric dipole composed for wireless communication system is reported
in the literature [2].
Propagation of electromagnetic (EM) waves above flat lossy ground for obvious applications in the area of
wireless communications reported by [3 - 4], because of the demands on the quality and capacity of the telecommunication
systems is increasing more and more, reconfigurable radiation patterns are desired. Several reconfigurable radiation pattern
antennas have been reported such as a three-layer switchable radiation pattern antenna based on the conventional Yagi
antenna, a hexagonal cylinder antenna with moderate gain, and a central circular patch with two paddle-shaped parasitic
patches. Among many types of reconfigurable antennas, planar structures [5 6] in particular have been extensively
investigated because of their attractive features such as simple structure, low profile, lightweight, and ease of fabrication
and integration. Printed monopole antennas for covering multiband have been reported and the designs occupy a relatively
larger space [7]. The length of the ground- arm of dipole antenna is larger than the signal-arm [8-9] it is beneficial to
enhance the antenna performance.
Optimization algorithms have also been widely used for different purposes in antenna array synthesis.
The uses of genetic algorithm (GA) procedures to optimize array characteristics can be found in [12-13], Direct analysis
International Journal of Electronics,
Communication & Instrumentation Engineering
Research and Development (IJECIERD)
ISSN(P): 2249-684X; ISSN(E): 2249-7951
Vol. 4, Issue 6, Dec 2014, 13-20
TJPRC Pvt. Ltd.
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14 M Surendra Kumar, A. Gayatri & S. S. Madhavi
Impact Factor (JCC): 4.9467 Index Copernicus Value (ICV): 3.0
approaches for radiating structures mounted on arbitrarily shaped platforms are typically based on either the method of
moments (MoM) [10-11], finite element methods (FEM) [14-15].
Taylors [16] reported a method of synthesis of line source for the generation of narrow beams. The same method
is extended to design amplitude distribution of line source required to produce specified number of multiple beams.
The method is further extended for the design of arrays of discrete radiators. The source positions of radiating elements in
the arrays are simply obtained from the sampled locations following the sampling theorem. Further, arrays of dipole
radiators are designed to realize the above mentioned multiple beams.
TAYLORS AMPLITUDE DISTRIBUTION AND RADIATION PATTERNS
The Taylor method is extended in the present work to produce multiple beams of desired number.
The method involves the determination of amplitude distribution for a specified multiple beams. The method of synthesis
is presented below.
(1)
Here n is an integer which divides the radiation pattern into uniform sidelobe region surrounding the main beam
and the region of decaying side lobes.
sinLu , L= array length. = angle measured from maximum radiation.
A = an adjustable real parameter having the property that cosh (A) is the side lobe ratio.
2)21n(2A
n
Using equation (1), the amplitude distribution of the array is found.
Figure 1: Line Source Geometry
RADIATION PATTERN OF A DIPLOE
Figure 2: Radiation from Dipole Antenna
8/10/2019 2. Electronics - Ijecierd - Design of Dipole Arrays for the - Surendra Kumar (1)
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Design of Dipole Arrays for the Generation of Multiple Beams 15
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The vector potential [17] at a point P due to the current element I dz is given by,
(2)
Here d is the distance from the current element to the point P. the total vector potential at P due to all current
elements is given by
(3)
=
It is of interest here to consider radiation fields, d in the denominator can be approximated to r. but in the
numerator, d is the phase term and it is given by
For a half wave dipole,
(4)
But we have
(5)
From equation (4) and (5), we have
(6)
The magnitude of E for the radiation field is
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16 M Surendra Kumar, A. Gayatri & S. S. Madhavi
Impact Factor (JCC): 4.9467 Index Copernicus Value (ICV): 3.0
(7)
Electric field as a function in free space for a dipole of length of 2H is given by
The amplitude of is
(8)
PATTERN MULTIPLICATION
Pattern multiplication is defined that resultant pattern is equal to the array factor multiplied with the element
pattern i.e,
E()resultant= Element Pattern Array Factor
RESULTS
Expression (1) represents the structure of the desired patterns. The number of required multiple beams of the line
source is controlled by n and the parameter A. For the specified patterns containing multiple lobes 4, the amplitude is
numerically computed for a normalized line source of length 2. The resultant radiation patterns of arrays of dipoles are
presented by using pattern multiplication. The resultant distribution for multiple lobes 4 is represented (3-8) for both small
and large arrays for number of elements N= 20, 40 and 60 are presented. A large number of results are presented toindicate the valuation of the sidelobe structure, beamwidth etc.
-1 -0.8 -0.6 -0.4 -0.2 0 0.2 0.4 0.6 0.8 10
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1
x
A(x)
Figure 3: Amplitude Distribution of Four Multiple Beam Dipole Array of 20 Elements
8/10/2019 2. Electronics - Ijecierd - Design of Dipole Arrays for the - Surendra Kumar (1)
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Design of Dipole Arrays for the Generation of Multiple Beams 17
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-80 -60 -40 -20 0 20 40 60 80-50
-45
-40
-35
-30
-25
-20
-15
-10
-5
0
theta in degrees
IE(u)Iin
dB
Array of Dipoles
Array of isotropic elements
Figure 4: Four Multiple Beam Patterns from an Array of 20 Elements
-1 -0.8 -0.6 -0.4 -0.2 0 0.2 0.4 0.6 0.8 10
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1
x
A(x)
Figure 5: Amplitude Distribution of Four Multiple Beam Dipole Array of 40 Elements
-80 -60 -40 -20 0 20 40 60 80-50
-45
-40
-35
-30
-25
-20
-15
-10
-5
0
theta in degrees
IE(u)Iin
dB
Array of Dipoles
Array of isotropic elements
Figure 6: Four Multiple Beam Patterns from an Array of 40 Elements
-1 -0.8 -0.6 -0.4 -0.2 0 0.2 0.4 0.6 0.8 10
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1
x
A(x)
Figure 7: Amplitude Distribution of Four Multiple Beam Dipole Array of 60 Elements
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18 M Surendra Kumar, A. Gayatri & S. S. Madhavi
Impact Factor (JCC): 4.9467 Index Copernicus Value (ICV): 3.0
Figure 8: Four Multiple Beam Patterns from an Array of 60 Elements
CONCLUSIONS
It is evident from the amplitude distributions presented that the elements at the ends of array are highly excited
and the centre elements are thinly excited. However, in the realized patterns the multiple beams of equal heights are at the
centre. Moreover, the specified numbers of multiple beams are characterized by small beam width for large arrays and high
beam width for small arrays. As discussed in the introduction, Taylors reported an excellent method for the design of line
source to produce optimal pencil beams. In the present work this method is extended for discrete arrays to produce
specified number of multiple beams for both isotropic and array of dipoles. The patterns are obtained with good agreement.
The present approach is suitable for the arrays of any type of non isotropic elements.
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AUTHOR'S DETAILS
A. Gayatri received her B. Tech from JNTU University, Hyderabad and M. Tech, from JNTU University,
Kakinada. She has 10 years of teaching experience. She published 04 technical papers in National and International
conferences. Her fields of interest are Antennas and wave propagation, Microwave engineering and Radar Engineering.
Presently she is working as an Asst. prof, in GITAM UNIVERSITY Visakhapatnam. INDIA.
Dr. M. Surendra Kumar received his B. Tech from Nagarjuna University and M. Tech, Ph. D from Andhra
University. He has 17 years of teaching experience. He published 21 technical papers in National and International
conferences and journals. His fields of interest are Antennas and wave propagation, Microwave engineering and Radar
Engineering. Presently he is working as a Principal in K L R College of Engineering & Technology-Paloncha, Khammam-
Dist, INDIA.
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20 M Surendra Kumar, A. Gayatri & S. S. Madhavi
Impact Factor (JCC): 4.9467 Index Copernicus Value (ICV): 3.0
S. S. Madhavireceived her degree from Andhra University, M. Tech, from JNTU Kakinada. She has 11 Years of
Teaching Experience; She published 4 technical papers in National and International Conferences. Presently She is
Working as an Assoc. professor In K L R College of Engineering & Technology-Paloncha, Khammamt, INDIA.