- Open Access
- Total Downloads : 421
- Authors : Ratna Kumari U, Prof. P. Mallikarjuna Rao, Prof. G. S. N. Raju
- Paper ID : IJERTV2IS120544
- Volume & Issue : Volume 02, Issue 12 (December 2013)
- Published (First Online): 17-12-2013
- ISSN (Online) : 2278-0181
- Publisher Name : IJERT
- License: This work is licensed under a Creative Commons Attribution 4.0 International License
Optimization of Radiation Patterns of Circular Antenna Arrays using Genetic Algorithm for Wireless Communications
*Ratna Kumari U, **Prof. P. Mallikarjuna Rao, **Prof. G. S. N. Raju
* Assistant Professor, Department of ECE, GIT, GITAM University, Visakhapatnam 45.
** Professors, Department of ECE, AU College of Engineering, Andhra University, Visakhapatnam-03.
Abstract
The circular arrays are extremely useful in direction finding, wide bandwidth HF communication systems, wrap – around shipborne communications, navigational aids, space craft communications, null steering systems for mobile communication applications, and wide bandwidth microwave direction finders. The presence of high side lobes causes electromagnetic interference in radar receivers due to nearby objects. Sometimes this interference is so high that it blocks the required echoes completely. Moreover, with the presence of high side lobes the radar systems are susceptible for jamming. In the present paper, an attempt is made to design circular antenna array with optimum low side lobe level and narrow beamwidth. Genetic algorithm is used in the present paper to optimize the radiation patterns of circular antenna array.
Keywords- Circular array, Genetic Algorithm, Narrow beam width.
Introduction:
Linear arrays [1-2] with narrow main beamwidth are used for point to point communications and high angular resolution radars. However, in the applications where angular symmetry in direction finding and 360 degrees scanning is required, they are not suitable. In view of these facts, efforts are made to design the circular arrays.
Circular array antenna [3-7] is an assembly of similar radiating elements electrically and geometrically in the form of a circle. The radiation pattern of circular antenna array with isotropic elements depends on the main parameters like the excitation current, excitation phase, and the spacing between the elements. In the array design process excitation currents, excitation phases, and inter element spacing are the three parameters that can be controlled to achieve the required objective.
Geometry of Circular antenna array ( CAA ) and Design equations:
The geometry of CAA is as shown in Fig.1
y
d3 d2
I2
I3
d
d
d4 I1
1
1
I
I
I4 x
N
d5 dN
I5 IN-1
I6
d6 dN-1
Fig 1. Circular Antenna Array
The array factor of this CAA is calculated as follows
Normalised field can be written as
=1
=1
, , =
Where
( 1 )
GA is Initially developed by John Holland, University of Michigan (1970s) , Based on the mechanics of biological evolution to understand processes in natural
systems and to design artificial systems
= 2 + 2 2 ( 2 ) For the far field the array field reduces to
retaining the robustness and adaptation properties of natural systems.
GA conceptually follows steps
, , =
cos ( )
inspired by the biological process of
(3)
=1
evolution. It follow the idea of survival of the fittest better and better solutions evolve from
Where n is the complex excitation
coefficient both amplitude and phase
= – ( 4 )
n is angular position of the nth element
previous generations until a near optimal solutions is obtained.
Terms related to GA:
Gene a single encoding of part of the solution space, i.e. either single bits or short
=1
=1
=
( 5 )
blocks of adjacent bits that encode an element of the candidate solution
=1
=1
= 2
( 6 )
Chromosome a string of genes that
In is excitation currents, n is excitation phases,
d is inter element spacing, k is the wave number,
N is no of elements and
is the angle of incidence.
Finally the array factor of CAA can be reduced and is given as
represents a solution
Population the number of chromosomes available to test
Selection A proportion of the existing population is selected to bread a new bread of generation. Parents with better fitness have better chances to produce offspring. There are three types of selection are there which
are popular rank, tournament and roulette
, , = =1 ( )
Genetic Algorithm:
( 7 )
wheel.
Crossover – a genetic operator that combines (mates) two individuals (parents) to produce
Genetic algorithm (GA) [8-12] is a global optimization technique which works on the mechanics of natural selection and genetics. It can be used to optimize the solution of any problem. GA is best suited if the objective function is discontinuous, highly non linear, high dimension, stochastic and has unreliable or undefined derivatives. It does not use any gradient information. It is most widely used technique in business, science and engineering areas.
two new individuals (Childs). The idea behind crossover is that the new chromosome may be better than both of the parents if it takes the best characteristics from each of the parents. There are 4 types of crossover single point, two point, uniform and real value.
Mutation – a genetic operator used to maintain genetic diversity from one generation of a population of chromosomes to the next. It is analogous to biological mutation. Mutation Probability determines how often the parts of a chromosome will be
mutated. Types of mutation are bit reversal and polynomial.
Fitness Function – A fitness function quantifies the optimality of a solution (chromosome) so that that particular solution may be ranked against all the other solutions.
It depicts the closeness of a given solution to the desired result. Most functions are stochastic and designed so that a small proportion of less fit solutions are selected. This helps keep the diversity of the population large, preventing premature convergence on poor solutions.
The fitness function for the optimization is given as
Fitness=min(max(20*log AF)/AF)
Termination Termination of the algorithm can be done if a solution is found that satisfies minimum criteria or Fixed number of generations found or Allocated budget (computation, time/money) reached or the highest ranking solutions fitness has reached
GA parameters selected here are
Max number of iterations : 100 Population size 50
Mutation rate : 0.15
The process of GA is indicated as flow chart in the Fig.2.
Results
excitation and 12.8o with optimization. The results are tabulated in Table 1 for 20 elements CAA.
Figures [ 4 6 ] shows that the radiation patterns of 30, 40 and 60 elements CAA with uniform excitation and GA method. The corresponding sidelobe level and beam width comparison values are presented in tables 2 4.
Tables 5 and 6 indicate the optimized values of excitation currents, excitation phases and inter element spacing of the CAA with 20 elements and 30 elements by using GA method respectively.
Start
Generate random population of n chromosomes (suitable solutions for the problem)
Generate random population of n chromosomes (suitable solutions for the problem)
[Fitness] Evaluate the fitness f(x) of each chromosome x in the population [Fitness] Evaluate the fitness f(x) of each chromosome x in the population [Selection] Select to parent chromosomes from a population according to their fitness (the better fitness, the bigger chance to be selected) [Selection] Select two parent chromosomes from a population according to their fitness (the better fitness, the bigger chance to be selected) [Mutation] With a mutation probability mutate new offspring at each locus (position in chromosome). [Mutation] With a mutation probability mutate new offspring at each locus (position in chromosome).Radiation patterns for circular antenna array of 20, 30, 40 and 60 elements are numerically evaluated using the equations 1 to 7 with uniform excitation. The Genetic algorithm is applied to optimize the excitation currents, excitation phases and inter element spacing of circular antenna array. For 20 elements CAA the radiation patterns are numerically evaluated and they are presented in Fig 3. From the results it is observed that the sidelobe level is -7.9dB with uniform excitation and -10.16dB with
optimization which is reduced drastically. The beam width is 13.04o with uniform
[Accepting] Place new offspring in the new population and [Replace] Use new generated population for a further run of the algorithm [Accepting] Place new offspring in the new population and [Replace] Use new generated population for a further run of the algorithmCondition Satisfied
Best Solution
Best Solution
Stop
Fig 2. Flow chart of Genetic Algorithm
0 0
Uniform excitation Genetic Algorithm
-5 -5
Uniform excitation Genetic Algorithm
-10 -10
Gain [dB]
Gain [dB]
Gain [dB]
Gain [dB]
-15 -15
-20 -20
-25 -25
-30
-150 -100 -50 0 50 100 150
Phi deg
-30
-150 -100 -50 0 50 100 150
Phi deg
Fig 3. Radiation pattern of CAA for N=20
2 1st SLL |
0 Elements 2nd SLL |
Max SLL |
B.W |
|
Uniform |
-7.9 |
-10.45 |
-6.43 |
13.0o |
GA |
-10.16 |
-16.6 |
-10.5 |
12.8o |
Table 1. Comparison values for 20 elements CAA
Fig 5. Radiation pattern of CAA for N=40
4 1st SLL |
0 Elements 2nd SLL |
Max SLL |
B.W |
|
Uniform |
-7.9 |
-10.4 |
-7.9 |
7.2o |
GA |
-9.12 |
-12.6 |
-9.12 |
6.4o |
Table 5. Comparison values for 40 elements CAA
0 0
Uniform excitation Genetic Algorithm
-5 -5
Uniform excitation Genetic Algorithm
Gain [dB]
Gain [dB]
-10
-10
Gain [dB]
Gain [dB]
-15
-15
-20
-20
-25
-25
-30
-150 -100 -50 0 50 100 150
Phi deg
-30
-150 -100 -50 0 50 100 150
Phi deg
Fig 4. Radiation pattern of CAA for N=30
30 Elements |
||||
1st SLL |
2nd SLL |
Max SLL |
B.W |
|
Uniform |
-7.9 |
-10.77 |
-7.9 |
9.8o |
GA |
-12.79 |
-17.01 |
-12.79 |
8.4o |
Table 2. Comparison values for 30 elements CAA
Fig 6. Radiation pattern of CAA for N=60
60 Elements |
||||
1st SLL |
2nd SLL |
Max SLL |
B.W |
|
Uniform |
-8.02 |
-10.6 |
-8.02 |
4.8o |
GA |
-9.994 |
-18.6 |
-9.994 |
4.2o |
Table 4. Comparison values for 60 elements CAA
0.9247 |
0.2125 |
0.4607 |
0.8306 |
0.3224 |
4.0161 |
0.5671 |
0.2533 |
8.2696 |
0.4353 |
0.7678 |
1.2995 |
0.3945 |
0.5608 |
19.8883 |
0.8243 |
0.2314 |
1.5941 |
0.2722 |
0.8620 |
35.1230 |
0.7145 |
0.7741 |
37.0777 |
0.8400 |
0.3224 |
4.0152 |
0.8275 |
0.8463 |
34.1680 |
0.3537 |
0.5733 |
3.5770 |
0.9718 |
0.4792 |
47.5533 |
0.9624 |
0.4322 |
14.5522 |
0.8588 |
0.4792 |
68.8886 |
Excitation currents |
Spacing |
Excitation angle |
0.7427 |
0.3349 |
-60.1147 |
0.9875 |
0.5075 |
-50.6781 |
0.9906 |
0.6518 |
-36.1766 |
0.7082 |
0.7490 |
-30.6017 |
0.9467 |
0.7208 |
-4.3831 |
0.9467 |
0.2973 |
-0.4698 |
0.8180 |
0.4102 |
-1.4553 |
0.9498 |
0.6235 |
-10.8977 |
0.9467 |
0.3255 |
-10.9550 |
0.8243 |
0.5890 |
-0.6474 |
0.9875 |
0.3600 |
2.7445 |
0.6894 |
0.3035 |
10.2789 |
0.8275 |
0.2816 |
17.1028 |
0.9780 |
0.7302 |
8.2391 |
0.8808 |
0.4290 |
25.0440 |
0.7992 |
0.2910 |
25.6972 |
0.8463 |
0.6675 |
38.6174 |
0.8996 |
0.2439 |
6.3197 |
0.8463 |
0.2753 |
46.2377 |
0.9341 |
0.269 |
59.3069 |
Excitation currents |
Spacing |
Excitation angle |
0.7427 |
0.3349 |
-60.1147 |
0.9875 |
0.5075 |
-50.6781 |
0.9906 |
0.6518 |
-36.1766 |
0.7082 |
0.7490 |
-30.6017 |
0.9467 |
0.7208 |
-4.3831 |
0.9467 |
0.2973 |
-0.4698 |
0.8180 |
0.4102 |
-1.4553 |
0.9498 |
0.6235 |
-10.8977 |
0.9467 |
0.3255 |
-10.9550 |
0.8243 |
0.5890 |
-0.6474 |
0.9875 |
0.3600 |
2.7445 |
0.6894 |
0.3035 |
10.2789 |
0.8275 |
0.2816 |
17.1028 |
0.9780 |
0.7302 |
8.2391 |
0.8808 |
0.4290 |
25.0440 |
0.7992 |
0.2910 |
25.6972 |
0.8463 |
0.6675 |
38.6174 |
0.8996 |
0.2439 |
6.3197 |
0.8463 |
0.2753 |
46.2377 |
0.9341 |
0.269 |
59.3069 |
Table 6 Excitation currents, inter element spacing and excitation angle after optimization for 30 elements
Table 5 Excitation currents, inter element spacing and excitation angle after optimization for 20 elements
Conclusions:
Excitation currents |
Spacing |
Excitation angle |
0.9624 |
0.5482 |
-2.0161 |
0.5671 |
0.2220 |
-38.2676 |
0.9969 |
0.3537 |
-38.8868 |
0.9122 |
0.9341 |
-1.1220 |
0.8212 |
0.8996 |
-2.2040 |
0.3600 |
0.8212 |
-34.2247 |
0.3788 |
0.8714 |
-18.9556 |
0.6549 |
0.9780 |
-5.7950 |
0.4573 |
0.7176 |
-13.1427 |
0.8902 |
0.2471 |
-11.5858 |
0.3537 |
0.2690 |
-7.8791 |
0.9404 |
0.3004 |
-7.3715 |
0.7835 |
0.5263 |
-10.2108 |
0.5984 |
0.2094 |
-6.9733 |
0.9310 |
0.2345 |
-1.7556 |
0.9906 |
0.2282 |
0.3586 |
Excitation currents |
Spacing |
Excitation angle |
0.9624 |
0.5482 |
-2.0161 |
0.5671 |
0.2220 |
-38.2676 |
0.9969 |
0.3537 |
-38.8868 |
0.9122 |
0.9341 |
-1.1220 |
0.8212 |
0.8996 |
-2.2040 |
0.3600 |
0.8212 |
-34.2247 |
0.3788 |
0.8714 |
-18.9556 |
0.6549 |
0.9780 |
-5.7950 |
0.4573 |
0.7176 |
-13.1427 |
0.8902 |
0.2471 |
-11.5858 |
0.3537 |
0.2690 |
-7.8791 |
0.9404 |
0.3004 |
-7.3715 |
0.7835 |
0.5263 |
-10.2108 |
0.5984 |
0.2094 |
-6.9733 |
0.9310 |
0.2345 |
-1.7556 |
0.9906 |
0.2282 |
0.3586 |
It is evident from the radiation patterns that application of genetic algorithm is very helpful in reducing the sidelobe levels. The Genetic algorithm is found to be simple, accurate and fast and the patterns are converged after 50 iterations. It is also found from the results that the beam widths are narrowed when compared to the uniform excitation patterns and such beams are very useful in direction finding applications.
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