Department of Electronics and Communication Engineering, R.V.R & J.C. College of Engineering, Chowdavaram, Guntur-522019, A.P, India.
ABSTRACTArray antennas are essential in communication technology because they can produce focused beams of electromagnetic radiation that can be precisely shaped and directed for various applications. These antennas typically generate a radiation pattern with a primary lobe, the main beam, accompanied by smaller minor lobes. The size and distribution of these lobes depend on the array's design and configuration. For large array antennas, the main beam becomes extremely narrow, enabling precise point-to-point communication over long distances. This precision is especially beneficial for applications requiring accurate targeting or transmission to specific locations. However, achieving such optimized performance requires careful design and engineering. This study, builds on Woodward's amplitude control method, initially developed for generating sector beams, to create ramp patterns with unique applications in antenna engineering. By adjusting the amplitudes of the signals fed into each element of the array, the researchers can shape the resulting radiation pattern to meet specific requirements. The paper provides detailed analysis and computational data demonstrating the effectiveness of this approach in achieving the desired beam patterns. These results offer valuable insights into antenna design and optimization, potentially advancements in wireless communication, radar systems, and satellite communication.
Keywords:Array Antennas, Communication, radiation pattern, lobes, Beam, performance, Ramp patterns, computational data, Wireless Communication.
1. INTRODUCTION
The line source antenna is characterized by its lengthy, narrow, and straight design. In this type of antenna, the directional properties are determined by variations in the field or current strength along its longitudinal axis. These variations are continuous, distinguishing line source antennas from discrete element arrays, although large arrays can sometimes be treated as continuous distributions for analytical purposes.
Here are the key points about the line source antenna:
In summary, the line source antenna's performance is predominantly determined by the careful design of the space factor, while the element factor plays a less significant role in enhancing directivity. The aim is to optimize the space factor to achieve the desired radiation pattern characteristics.
Array antennas are preferred as they provide flexibility in design, outstanding gain and high directivity. The array antennas are designed to produce radiation pattern which consists of nulls in particular directions and to produce narrow beams in the desired directions. A collection of beam shapes [1-7] are generated by these array antennas and are effective in numerous applications. Standard beam shapes are narrow/pencil, sector, cosecant, ramp, and stair-step etc. The narrow beams [8,9] are widely used for point-to-point communications including high resolution radars. Ramp patterns [10-18] have the applications to those of pencil beams. It is possible to generate enhanced/optimized beams from well-engineered array antennas. Optimization is achieved by using amplitude [7], spatial [8], and phase [9] distributions or their combinations. In the current research work, an amplitude distribution function is designed by using Woodward technique for the creation of ramp patterns.
2. SYNTHESIS OF AMPLITUDE DISTRIBUTION FOR DESIRED RADIATION BEAM SHAPES
The radiation pattern exhibited by a line source with a length of 1 can be described as follows
if A(x) is represented by Fourier series
then radiation pattern is given by
&
where u=k cosθ
It is obvious from the above expression; the design problem is reduced to the determination of the constant an which results any given pattern over a given region. The coefficients an are chosen such that the approximate pattern EN(k cos θ) at the points given by
The coefficient an are now obtained from
if an is changed
then amplitude distribution
Positive Ramp pattern is defined by
where u0= 0.4
Figure 1: Amplitude Distribution function for Ramp pattern.
Figure 2: Normalized Radiation Ramp pattern ( 2 L / λ = 20 )
Figure 3: Normalized Radiation Ramp pattern ( 2 L / λ = 50 )
Figure 4: Normalized Radiation Ramp pattern ( 2 L / λ = 100 )
Figure 5: Normalized Radiation Ramp pattern ( 2 L / λ = 200 )
3. RESULTS AND CONCLUSIONS
This study demonstrates the feasibility of using line source antenna with amplitude control to generate ramp patterns. The amplitude distribution functions for generating ramp patterns have been thoroughly evaluated and are now presented in Figure 1. The resultant radiation patterns are presented in Figures (2-5). The patterns presented in the present work are to be very close to the desired patterns when the array consists of a large number of elements. The provision of independent adjustment of the coefficients near a discontinuity is especially valuable.
ACKNOWLEDGEMENTS
Author expresses his deep sense of gratitude and indebtedness to my beloved Prof. Late A. Sudhakar and the Management of RVR&JC college of Engineering Guntur for their support for this work.
REFERENCES
