<?xml version="1.0" encoding="UTF-8"?><!DOCTYPE article  PUBLIC "-//NLM//DTD Journal Publishing DTD v3.0 20080202//EN" "http://dtd.nlm.nih.gov/publishing/3.0/journalpublishing3.dtd"><article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" dtd-version="3.0" xml:lang="en" article-type="research article"><front><journal-meta><journal-id journal-id-type="publisher-id">JEMAA</journal-id><journal-title-group><journal-title>Journal of Electromagnetic Analysis and Applications</journal-title></journal-title-group><issn pub-type="epub">1942-0730</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/jemaa.2016.81002</article-id><article-id pub-id-type="publisher-id">JEMAA-63209</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Engineering</subject><subject> Physics&amp;Mathematics</subject></subj-group></article-categories><title-group><article-title>
 
 
  Antenna Performance Improvement in Elliptical Array Using RMI Method of Mutual Coupling Compensation
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>luru</surname><given-names>Venkata Lakshmi Narayana Rao</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Nunna</surname><given-names>Bala Ankaiah</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Dharma</surname><given-names>Raj Cheruku</given-names></name><xref ref-type="aff" rid="aff3"><sup>3</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>Department of ECE, SSNCET, Ongole, India,</addr-line></aff><aff id="aff2"><addr-line>ECIL, Hyderabad, India,</addr-line></aff><aff id="aff3"><addr-line>Departement of ECE, GIT, GITAM University, Visakhapatnam, India</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>narayanaavlrao@gmail.com(LVLNR)</email>;<email>bala.nunna8@gmail.com(NBA)</email>;<email>dharmarajc@yahoo.com(DRC)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>22</day><month>01</month><year>2016</year></pub-date><volume>08</volume><issue>01</issue><fpage>8</fpage><lpage>21</lpage><history><date date-type="received"><day>4</day>	<month>December</month>	<year>2015</year></date><date date-type="rev-recd"><day>accepted</day>	<month>25</month>	<year>January</year>	</date><date date-type="accepted"><day>29</day>	<month>January</month>	<year>2016</year></date></history><permissions><copyright-statement>&#169; Copyright  2014 by authors and Scientific Research Publishing Inc. </copyright-statement><copyright-year>2014</copyright-year><license><license-p>This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/</license-p></license></permissions><abstract><p>
 
 
  The number of wireless electronic gadgets used in mobile communication, vehicle collision avoidance system, compact radars, etc. is extremely increasing at a rapid rate. Thus, the characteristics of the antennas involved in these gadgets are to be designed very stringently so as to avoid interferences &amp; coupling and to improve compatibility, susceptibility, etc. Compact smart antenna with improved performance is highly essential to meet this challenging scenario. Mutual coupling between various elements of an array is one of the main factors which can be considered for improvement of performance of the antenna. Influence of mutual coupling on performance of the antenna is considered in this paper and various techniques to minimize this effect are presented. Effect of mutual coupling on radiation characteristics of the antenna can be compensated employing various methods like Conventional Mutual Impedance (CMI), Receiving Mutual Impedance (RMI). Analysis is presented as comparison between the two methods for different number of elements in the array. Analysis is also presented for different geometries of the array like circular and elliptical for improved performance. The results show performance improvement in the proposed array for parameters like SNR and Speed of convergence.
 
</p></abstract><kwd-group><kwd>Antenna Arrays</kwd><kwd> Elliptical (Oval) Arrays</kwd><kwd> Mutual Coupling</kwd><kwd> Compensation Methods</kwd><kwd> Beam Forming</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Wide spread application of wireless communication technology in daily life demands efficient and reliable signal transmission. Increased directivity, user capacity, battery life and source separation can be achieved by smart antenna to cope-up the demands. Smart antenna is popularly used in radar systems, wireless communications and in vehicle collision avoidance applications [<xref ref-type="bibr" rid="scirp.63209-ref1">1</xref>] . Antenna array is an integral part of smart antenna system. In smart antenna system, array of elements are designed to achieve required beam form for a given application.</p><p>A systematic arrangement of group of radiating elements is called an array. Size of the array and aperture proportionally increases with gain of the antenna [<xref ref-type="bibr" rid="scirp.63209-ref2">2</xref>] . Two methods to increase the aperture size of the array are to increase the number of elements and/or inter element spacing of the array [<xref ref-type="bibr" rid="scirp.63209-ref3">3</xref>] . Computational complexity increases with the number of elements. However, this leads to increase in grating lobes. Power efficiency reduces due to grating lobes [<xref ref-type="bibr" rid="scirp.63209-ref4">4</xref>] . A compromise between these two parameters can be achieved by reorienting the geometry and number of elements in the array.</p><p>Linear array is simple in structure and is limited to estimation of the elevation angle (one dimensional) of incoming signal only. In addition, the linear array can only estimate the range of azimuth angle limited by 180˚ (−90˚ &lt; θ &lt; 90˚) [<xref ref-type="bibr" rid="scirp.63209-ref5">5</xref>] . Hence the accuracy of Direction of Arrival (DOA) estimation is greatly affected when the incoming signal is within the range of end-fire array (70˚ &lt; |θ| &lt; 90˚).</p><p>The entire transmitted signal is equal to the sum and reradiated signal from the elements. Similarly, induced current on the antenna element reradiates electromagnetic field which would be received by the other neighboring elements in the array. Such mutual coupling effect is usually considered as a defect which degrades the performance of the array. Two types of coupling compensation methods: Conventional Mutual Impedance (CMI) and Receiving Mutual Impedance (RMI) methods are popular.</p></sec><sec id="s2"><title>2. The Mutual Coupling Analysis</title><p>For an antenna array with N elements, receiving an incoming signal, being a plane wave source, the received terminal voltage at the k<sub>th</sub> antenna element V<sub>k</sub> can be expressed as</p><disp-formula id="scirp.63209-formula533"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-9801661x6.png"  xlink:type="simple"/></disp-formula><p>U<sub>k</sub> = received voltage of k<sub>th</sub> antenna element by the plane wave source alone</p><p>W<sub>k</sub> = coupled voltage of the scattered fields from the other antenna elements in the array</p><p>The coupled voltage W<sub>k</sub> in (1) can be written as [<xref ref-type="bibr" rid="scirp.63209-ref6">6</xref>] -[<xref ref-type="bibr" rid="scirp.63209-ref8">8</xref>]</p><disp-formula id="scirp.63209-formula534"><label>(2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-9801661x7.png"  xlink:type="simple"/></disp-formula><p>where Z<sub>k</sub> is the receiving mutual impedance between the k<sub>th</sub> and the i<sub>th</sub> antenna elements and I<sub>i</sub> is the terminal current at the i<sub>th</sub> antenna element given by:</p><disp-formula id="scirp.63209-formula535"><graphic  xlink:href="http://html.scirp.org/file/2-9801661x8.png"  xlink:type="simple"/></disp-formula><p>with Z<sub>L</sub> being the terminal load impedance of the antenna elements. Putting (2) and (3) into (1), we have:</p><disp-formula id="scirp.63209-formula536"><label>(3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-9801661x9.png"  xlink:type="simple"/></disp-formula><p>The relationship between the uncoupled voltages U<sub>k</sub> and the received voltages (i.e., coupled voltages) V<sub>k</sub> can be written in a matrix equation as:</p><disp-formula id="scirp.63209-formula537"><label>(4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-9801661x10.png"  xlink:type="simple"/></disp-formula><sec id="s2_1"><title>2.1. Conventional Mutual Impedance Method</title><p>A circuit theory approach for reducing or compensating mutual coupling effect is discussed in this work. This method is called conventional mutual impedance method (CMI) [<xref ref-type="bibr" rid="scirp.63209-ref9">9</xref>] . Common mutual coupling can be easily measured directly or from S-parameters.</p><p>The relation between the terminal voltage and current can be given by</p><disp-formula id="scirp.63209-formula538"><label>(5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-9801661x11.png"  xlink:type="simple"/></disp-formula><p>Z<sub>L</sub> being impedance, relation between voltage and current is given by</p><disp-formula id="scirp.63209-formula539"><label>(6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-9801661x12.png"  xlink:type="simple"/></disp-formula><p>The relationship between the open-circuit voltages and terminal voltages can be written as</p><disp-formula id="scirp.63209-formula540"><label>(7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-9801661x13.png"  xlink:type="simple"/></disp-formula></sec><sec id="s2_2"><title>2.2. The Receiving Mutual Impedance</title><p>Another circuit theory approach for reducing or compensating mutual coupling effect is receiving mutual impedance method (RMI) [<xref ref-type="bibr" rid="scirp.63209-ref10">10</xref>] . The concept of receiving mutual impedance was suggested [<xref ref-type="bibr" rid="scirp.63209-ref11">11</xref>] as an alternative to the concept of conventional mutual impedance [<xref ref-type="bibr" rid="scirp.63209-ref12">12</xref>] . In fact, the need to handle mutual coupling problems differently in transmitting and receiving arrays has been noted before in mobile communications [<xref ref-type="bibr" rid="scirp.63209-ref13">13</xref>] and [<xref ref-type="bibr" rid="scirp.63209-ref14">14</xref>] . The basic difference between the receiving mutual impedance and the conventional mutual impedance lies in the fundamental causes of the coupling. In the conventional mutual impedance, the coupling is caused by the transmitting current distribution on an antenna while in the receiving mutual impedance; the coupling is caused by the receiving current distribution on an antenna.</p><p>The receiving mutual impedance between two antennas is the ratio of the coupled voltage across antenna1’s terminal load Z<sub>L</sub><sub>1</sub> (due to the receiving current distribution on antenna 2) to the terminal current through antenna 2’sterminal load Z<sub>L</sub><sub>2</sub> when the array is excited by an external plane wave source.</p><disp-formula id="scirp.63209-formula541"><label>(8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-9801661x14.png"  xlink:type="simple"/></disp-formula><p>i.e. Receiving mutual impedance with a receiving current on antenna 2 = coupled voltages across antenna 1’s terminal load/receiving current through antenna 2’s terminal load.</p><p>The definition of the receiving mutual impedance requires specifying a plane wave to excite the two antennas as shown in <xref ref-type="fig" rid="fig1">Figure 1</xref>. The coming direction of the plane wave is to be the same as the direction of the signal that the array is designed. In <xref ref-type="fig" rid="fig1">Figure 1</xref>, V<sub>1</sub> and V<sub>2</sub> are the received voltages across the terminal loads of antennas 1 and 2, respectively. The corresponding currents through the two antennas are I<sub>1</sub> and I<sub>2</sub>. In equation (1), U<sub>1</sub> is the received voltage across the terminal load of antennas 1 when antenna 1 is excited by the external plane wave source alone (with antenna 2 removed from the array). U<sub>1</sub> is also called the isolation voltage on antenna 1.</p></sec></sec><sec id="s3"><title>3. Geometry and Array Factor</title><p>Two different geometries of the array are considered for comparison in this paper viz., Circular and Elliptical (Oval).</p><sec id="s3_1"><title>3.1. Circular Array</title><p>In circular array it is assumed that N equally spaced isotropic elements are placed on X-Y plane along a circular ring. Let the radius be “a”. Circular array can able to scan 360˚ azimuthally. The geometry of N-element circular</p><fig id="fig1"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> Mutual impedance between antennas</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-9801661x15.png"/></fig><p>array antenna is shown in <xref ref-type="fig" rid="fig2">Figure 2</xref> [<xref ref-type="bibr" rid="scirp.63209-ref15">15</xref>] . The array factor is given by the equation [<xref ref-type="bibr" rid="scirp.63209-ref16">16</xref>]</p><disp-formula id="scirp.63209-formula542"><label>(9)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-9801661x16.png"  xlink:type="simple"/></disp-formula><p>where,</p><p>I<sub>n</sub> = amplitude of excitation</p><p>α<sub>n</sub> = phase of the n th element</p><p>θ = elevation angle from z axis.</p><p>Circumference = 2πr</p><p>Area = πr<sup>2</sup></p><p>The radius of the array increases the directivity of uniform circular array and tends to a value N [<xref ref-type="bibr" rid="scirp.63209-ref17">17</xref>] .</p></sec><sec id="s3_2"><title>3.2. Elliptical Antenna Array</title><p>The geometry of the elliptical antenna array with origin as center is shown in <xref ref-type="fig" rid="fig3">Figure 3</xref> [<xref ref-type="bibr" rid="scirp.63209-ref18">18</xref>]</p><p>The array factor is given by equation (10) [<xref ref-type="bibr" rid="scirp.63209-ref19">19</xref>] .</p><disp-formula id="scirp.63209-formula543"><label>(10)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-9801661x17.png"  xlink:type="simple"/></disp-formula><p>I<sub>n</sub>=amplitude of excitation</p><p>α<sub>n</sub>=phase of the n th element</p><p>θ=elevation angle from z axis.</p><p>&#248;<sub>n</sub>=Azimuth angle measured from x axis for n-th element.</p><p>a, b=semi major and minor axises respectively.</p><p>e=eccentricity of elliptical array and is 0.5</p><disp-formula id="scirp.63209-formula544"><label>(11)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-9801661x18.png"  xlink:type="simple"/></disp-formula><p>θ<sub>0</sub> = 90˚, &#248;<sub>0</sub> = 0˚.</p><p>N=no of elements is 8 or 10.</p><disp-formula id="scirp.63209-formula545"><graphic  xlink:href="http://html.scirp.org/file/2-9801661x19.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.63209-formula546"><graphic  xlink:href="http://html.scirp.org/file/2-9801661x20.png"  xlink:type="simple"/></disp-formula><p>Comparisons of area of circular and elliptical arrays are given below in <xref ref-type="table" rid="table1">Table 1</xref>.</p></sec></sec><sec id="s4"><title>4. Results</title><sec id="s4_1"><title>4.1. Conventional Mutual Impedance Method of Compensation</title><p>The objective is to analyze the response of elliptical antenna array with modified LMS (Least Mean Square) algorithm which optimizes the weight factor for DOA (Direction of Arrival) estimation. Mutual coupling is minimized by the CMI method in this case.</p><p>Example 1: Eight (Dipole) Element Array using CMI</p><p>In this example, an 8-element array using CMI is optimized with uniform spacing between the elements. It is assumed that the angle of signal and interference be 90˚ and 180˚ respectively.</p><fig id="fig2"  position="float"><label><xref ref-type="fig" rid="fig2">Figure 2</xref></label><caption><title> Geometry of circular antenna in XY-plane</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-9801661x21.png"/></fig><fig id="fig3"  position="float"><label><xref ref-type="fig" rid="fig3">Figure 3</xref></label><caption><title> Geometry of ellipse in XY-plane</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-9801661x22.png"/></fig><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> Comparision of area of circular and ellptical arrays</title></caption><table><tbody><thead><tr><th align="center" valign="middle"  rowspan="2"  >Circumference (cm)</th><th align="center" valign="middle"  colspan="6"  >Circular and oval array area.</th></tr></thead><tr><td align="center" valign="middle" >Circular array radius r (cm)</td><td align="center" valign="middle" >Circular array area A (cm)</td><td align="center" valign="middle"  colspan="2"  >Oval array major radius a (cm)</td><td align="center" valign="middle" >Oval array minor radius b (cm)</td><td align="center" valign="middle" >Area (cm<sup>2</sup>)</td></tr><tr><td align="center" valign="middle" >1.00 1.50 2.00 3.00 4.00</td><td align="center" valign="middle" >0.16 0.24 0.32 0.48 0.64</td><td align="center" valign="middle"  colspan="2"  >0.08 0.18 0.32 0.72 1.27</td><td align="center" valign="middle" >0.20 0.30 0.40 0.62 0.84</td><td align="center" valign="middle" >0.10 0.15 0.21 0.31 0.42</td><td align="center" valign="middle" >0.07 0.15 0.27 0.60 1.07</td></tr><tr><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td></tr></tbody></table></table-wrap><p>It can be evident from <xref ref-type="fig" rid="fig4">Figure 4</xref> and <xref ref-type="fig" rid="fig5">Figure 5</xref>, that elliptical (oval) array with CMI method has reduced number of side lobes. Also, lower response of −20 dB observed in the interference direction, compared to circular antenna with −10 dB response.</p><p><xref ref-type="fig" rid="fig6">Figure 6</xref> and <xref ref-type="fig" rid="fig7">Figure 7</xref> compare the output noise in circular and elliptical antennas. Elliptical antenna has noise power which is less by 0.5 dB (negligible noise) for the iterations 10 to 100, whereas the circular antenna has considerable noise at low iteration rates below 20 for minimum of 0.5 dB. Hence it can be concluded that convergence is fast in elliptical array antenna than in circular for low noise.</p><p>Example 2: Ten (Dipole) Element Array using CMI</p><p>In this example, a 10-element array using CMI is optimized with uniform spacing between the elements. It is assumed that the angle of signal and interference be 90˚ and 180˚ respectively.</p><p>In <xref ref-type="fig" rid="fig8">Figure 8</xref>, iterations vs. SNR in circular array with 10-elements (uniform spacing between elements) using RMI Method is presented. <xref ref-type="fig" rid="fig9">Figure 9</xref> is similar plot for Elliptical array. The elliptical antenna leads with better SNR than circular antenna for iterations below 20. Circular antenna has −10 dB SNR and elliptical antenna has −2 dB which confirms the faster convergence of elliptical array.</p><p><xref ref-type="fig" rid="fig1">Figure 1</xref>0 shows circular array with CMI Method and without CMI Method which has deeper nulls if compensation is not applied. But elliptical array performance is good with null points covered by peaks as shown in <xref ref-type="fig" rid="fig1">Figure 1</xref>1.</p><fig id="fig4"  position="float"><label><xref ref-type="fig" rid="fig4">Figure 4</xref></label><caption><title> Circular array using CMI Method</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-9801661x23.png"/></fig><fig id="fig5"  position="float"><label><xref ref-type="fig" rid="fig5">Figure 5</xref></label><caption><title> Elliptical (oval) array with CMI Method</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-9801661x24.png"/></fig><fig id="fig6"  position="float"><label><xref ref-type="fig" rid="fig6">Figure 6</xref></label><caption><title> Iterations vs. output noise in circular array with CMIMethod</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-9801661x25.png"/></fig><p>In CMI compensation both 8 &amp; 10 element arrays of circular and elliptical arrays are compared. Elliptical arrays show better in pattern generation, SNR and convergence speed. Advantage of elliptical antenna compared to circular antenna is its low area for same number of elements.</p><fig id="fig7"  position="float"><label><xref ref-type="fig" rid="fig7">Figure 7</xref></label><caption><title> Iterations vs. output noise in Elliptical(oval) array using CMI Method</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-9801661x26.png"/></fig><fig id="fig8"  position="float"><label><xref ref-type="fig" rid="fig8">Figure 8</xref></label><caption><title> Iterations vs. SNR in circular array with CMI Method</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-9801661x27.png"/></fig><fig id="fig9"  position="float"><label><xref ref-type="fig" rid="fig9">Figure 9</xref></label><caption><title> Iterations vs. output SNR in Elliptical array using CMI Method</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-9801661x28.png"/></fig><fig id="fig10"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref>0</label><caption><title> Circular array with and without CMI Method</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-9801661x29.png"/></fig><fig id="fig11"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref>1</label><caption><title> Elliptical array with and without CMI Method</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-9801661x30.png"/></fig></sec><sec id="s4_2"><title>4.2. The Receiving Mutual Impedance Method of Compensation</title><p>In this RMI Method, the source and noise are assumed to be 90˚ and 180˚ of azimuth directions respectively. A modified LMS algorithm is used to optimize the weight factor for DOA estimation.</p><p>Example 3: Eight (Dipole) Element Array using RMI</p><p>In this example, an 8-element Circular array is optimized with uniform spacing between the elements.</p><p>The best amplitude value determined by the optimized technique is shown in <xref ref-type="fig" rid="fig1">Figure 1</xref>2. From <xref ref-type="fig" rid="fig1">Figure 1</xref>3 it can be noted that the output noise power sustains minimum with the number of iterations above 10.</p><p>It can be evident that from <xref ref-type="fig" rid="fig1">Figure 1</xref>3 elliptical array with RMI Method has reduced side lobes and peaks compared with circular array with RMI Method in <xref ref-type="fig" rid="fig1">Figure 1</xref>2. Elliptical antenna has lower response in the interference direction than circular antenna.</p><p><xref ref-type="fig" rid="fig1">Figure 1</xref>4 and <xref ref-type="fig" rid="fig1">Figure 1</xref>5 compare the output noise in circular and elliptical arrays. Elliptical antenna has negligible noise throughout the iterations from 10 to 100 below 0.5 dB, whereas the circular antenna has noise slightly more than that of elliptical antenna. Also below 10 iterations makes much difference in both antenna output noise. Convergence is faster in elliptical antenna.</p><p>Example 4: Ten (Dipole) Element Array using RMI</p><p>In this example, a 10-element array with uniform spacing between the elements is optimized using RMI. As per the <xref ref-type="fig" rid="fig1">Figure 1</xref>6 &amp; <xref ref-type="fig" rid="fig1">Figure 1</xref>7 for Iterations vs. SNR in circular and elliptical arrays (no of elements 10) using</p><fig id="fig12"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref>2</label><caption><title> Circular array with RMI Method</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-9801661x31.png"/></fig><fig id="fig13"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref>3</label><caption><title> Elliptical (oval) array with RMI Method</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-9801661x32.png"/></fig><fig id="fig14"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref>4</label><caption><title> Iterations vs. output noise in circular array with RMI Method</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-9801661x33.png"/></fig><fig id="fig15"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref>5</label><caption><title> Iterations vs output noise in Elliptical (oval) array using RMI Method</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-9801661x34.png"/></fig><fig id="fig16"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref>6</label><caption><title> Iterations vs. SNR in circular array with RMI Method</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-9801661x35.png"/></fig><fig id="fig17"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref>7</label><caption><title> Iterations vs. output SNR in Elliptical array using RMI Method</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-9801661x36.png"/></fig><p>RMI Method, the elliptical antenna has better SNR below 20 iterations. Hence convergence is faster in elliptical antenna. For the iterations below 10, circular array has minimum of −12 db SNR.</p><p><xref ref-type="fig" rid="fig1">Figure 1</xref>8 and <xref ref-type="fig" rid="fig1">Figure 1</xref>9 presents the comparison between the patterns generated with RMI and without RMI method for circular array and elliptical antennas. Elliptical antenna beam minimized lobe in 120˚ to 240˚, azimuth angle compared to circular antenna.</p><p>Example 5: Sixteen (Dipole) Element Array using RMI</p><p>In this example, an 16-element Circular &amp; Elliptical arrays are optimized with uniform spacing between the elements. Simulations are shown in <xref ref-type="fig" rid="fig2">Figure 2</xref>0 &amp; <xref ref-type="fig" rid="fig2">Figure 2</xref>1. It observed that from <xref ref-type="fig" rid="fig2">Figure 2</xref>1 Elliptical (oval) array with RMI Method has reduced side lobes and peaks compared with circular array. Elliptical antenna has peak at −28 dB in the interference direction as circular antenna has −21 dB</p><p>In RMI compensation along with 8 &amp; 10 element arrays of circular and elliptical arrays, 16-element arrays are also compared. Elliptical arrays shows better in pattern generation, SNR. Convergence speed is more improved. Geometrical advantage of compact size for elliptical antenna with same number of elements as in circular antenna is sustained.</p><p>More over RMI sanctions receiving current distribution on an antenna compared to CMI mode of compensation. It is additional advantage to recommend the RMI in elliptical arrays so that DOA estimation depends on Direction of receiving signal strength.</p><p>Example 6: Sixteen (Dipole) Element Array with non linear spacing using RMI</p><p><xref ref-type="fig" rid="fig2">Figure 2</xref>2 and <xref ref-type="fig" rid="fig2">Figure 2</xref>3 compares the output of 16-element circular &amp; elliptical antenna with non linear spacing. Elliptical antenna has lower response at 210˚, 270˚ and 330˚ Azimuth direction, whereas the circular antenna has response better than that of elliptical antenna. Also, side lobes are more in circular antenna.</p><p>Lobes between 180˚ - 240˚ &amp; 300˚ - 330˚ are smoothening and shaped compared to circular array in elliptical antenna.</p><p>However, below 180˚ of angle uniform spaced array is seems to be performing better.</p></sec></sec><sec id="s5"><title>5. Conclusions</title><p>The simulations categorically show that CMI compensation method applied to elliptical array with 8 &amp; 10 elements has better response in pattern generation, convergence speed and SNR compared with circular array. Compactness of elliptical antenna compared to circular antenna for the same number of elements is additional geometrical advantage.</p><p>Using RMI compensation method, a comparison is made for 8, 10 and 16 element array in circular as well as elliptical array. Elliptical arrays show better performance in pattern generation, SNR. Convergence speed is better compared to CMI method of compensation. Moreover, receiving current distribution on an antenna for RMI</p><fig id="fig18"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref>8</label><caption><title> Circular array with and without RMI Method</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-9801661x37.png"/></fig><fig id="fig19"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref>9</label><caption><title> Elliptical array with and without RMI Method</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-9801661x38.png"/></fig><fig id="fig20"  position="float"><label><xref ref-type="fig" rid="fig2">Figure 2</xref>0</label><caption><title> 16-Element Circular Dipole Antenna array with signal and inter- ference at 90˚and 180˚</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-9801661x39.png"/></fig><fig id="fig21"  position="float"><label><xref ref-type="fig" rid="fig2">Figure 2</xref>1</label><caption><title> 16-Element elliptical (oval) Dipole Antenna array with signal and interference at 90˚ and 180˚</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-9801661x40.png"/></fig><fig id="fig22"  position="float"><label><xref ref-type="fig" rid="fig2">Figure 2</xref>2</label><caption><title> 16-Element Circular Dipole Antenna array with non-uniform signal and interference at 90˚ and 180˚</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-9801661x41.png"/></fig><fig id="fig23"  position="float"><label><xref ref-type="fig" rid="fig2">Figure 2</xref>3</label><caption><title> 16-Element Elliptical (oval) Dipole Antenna array with non-uniform signal and interference at 90˚ and 180˚</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-9801661x42.png"/></fig><p>method is better compared to CMI mode of compensation. It is additional advantage to recommend the RMI in elliptical arrays because DOA estimation depends on Direction of receiving signal strength.</p><p>Also, the simulation of non uniform spaced elements array in either circular or elliptical patterns confirms that below 180 degrees of angle, uniform spaced array performance is better. Hence, it can be concluded that elliptical array of uniform spaced elements with RMI compensation method of mutual coupling has the best performance in a smart antenna.</p></sec><sec id="s6"><title>Cite this paper</title><p>Aluru Venkata Lakshmi NarayanaRao,Nunna BalaAnkaiah,Dharma RajCheruku, (2016) Antenna Performance Improvement in Elliptical Array Using RMI Method of Mutual Coupling Compensation. Journal of Electromagnetic Analysis and Applications,08,8-21. doi: 10.4236/jemaa.2016.81002</p></sec></body><back><ref-list><title>References</title><ref id="scirp.63209-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Okamoto, G.T. (2002) Smart Antenna Systems and Wireless LANs. Kluwer Academic, Santa Clara.</mixed-citation></ref><ref id="scirp.63209-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">Haupt, R.L. (2010) Antenna Arrays: A Computational Approach. John Wiley and Sons, Hoboken, New Jersey. http://dx.doi.org/10.1002/9780470937464</mixed-citation></ref><ref id="scirp.63209-ref3"><label>3</label><mixed-citation publication-type="other" xlink:type="simple">Fenn, A.J. (2008) Adaptive Antennas and Phased Arrays for Radar and Communications. Artech House Publishers, Massachusetts Institute of Technology, Norwood, MA.</mixed-citation></ref><ref id="scirp.63209-ref4"><label>4</label><mixed-citation publication-type="other" xlink:type="simple">Balanis, C.A. (2008) Modern Antenna Handbook. John Wiley and Sons, Hoboken, New Jersey, 135. http://dx.doi.org/10.1002/9780470294154</mixed-citation></ref><ref id="scirp.63209-ref5"><label>5</label><mixed-citation publication-type="other" xlink:type="simple">Ioannidis, P. and Balanis, C.A. (2005) Uniform Circular Arrays for Smart Antennas. IEEE Antennas and Propagation Magazine, 47, 192-206. http://dx.doi.org/10.1109/MAP.2005.1589932</mixed-citation></ref><ref id="scirp.63209-ref6"><label>6</label><mixed-citation publication-type="other" xlink:type="simple">Arrival Estimation for Antenna Arrays. Morgan &amp; Claypool, Arizona State University, Tempe, AZ.</mixed-citation></ref><ref id="scirp.63209-ref7"><label>7</label><mixed-citation publication-type="other" xlink:type="simple">Lui, H.-S. Hui, H. T. and Leong, M. S. (2008) Investigation of Direction-of-Arrival Estimation Using Uniform Linear Arrays with Different Antenna Separations and Array Apertures. Presented at the Asia Pacific Microwave Conference.</mixed-citation></ref><ref id="scirp.63209-ref8"><label>8</label><mixed-citation publication-type="other" xlink:type="simple">Balanis, C.A. (1997) Antenna Theory: Analysis and Design. Wiley, New York.</mixed-citation></ref><ref id="scirp.63209-ref9"><label>9</label><mixed-citation publication-type="book" xlink:type="simple">Collin, R.E. and Zucker, F.J., Eds. (1968) Antenna Theory. McGraw-Hill, New York.</mixed-citation></ref><ref id="scirp.63209-ref10"><label>10</label><mixed-citation publication-type="other" xlink:type="simple">Balanis, C.A. and Ioannides, P.I. (2007) Introduction to Smart Antenna. Morgan and Claypool, Arizona.</mixed-citation></ref><ref id="scirp.63209-ref11"><label>11</label><mixed-citation publication-type="other" xlink:type="simple">Singh, H., Sneha, H.L. and Jha, R.M. (2013) Mutual Coupling in Phased Arrays: A Review. International Journal of Antennas and Propagation, 2013, Article ID: 348123.</mixed-citation></ref><ref id="scirp.63209-ref12"><label>12</label><mixed-citation publication-type="other" xlink:type="simple">Hopkins, G.D., Ratner, J., Traille, A. and Tripp V. (2007) Aperture Efficiency of Amplitude, Weighting Distributions for Array Antennas. 2007 IEEE Aerospace Conference, Big Sky, 3-10 March 2007, 1-9. http://dx.doi.org/10.1109/aero.2007.352856</mixed-citation></ref><ref id="scirp.63209-ref13"><label>13</label><mixed-citation publication-type="other" xlink:type="simple">Cao, W.Q., Xiang, Y., Zhang, B.N., Liu, A.J., Yu, T.B. and Guo, D.S. (2011) A Low-Cost Compact Patch Antenna with Beam Steering Based on CSRR Loaded Ground. IEEE Antennas and Wireless Propagation Letters, 10, 1520-1523. http://dx.doi.org/10.1109/LAWP.2011.2181316</mixed-citation></ref><ref id="scirp.63209-ref14"><label>14</label><mixed-citation publication-type="other" xlink:type="simple">Chan, S.C. and Chen, H.H. (2006) Uniform Concentric Circular Arrays with Frequency Invariant Characteristics— Theory, Design, Adaptive Beam Forming and DOA Estimation. IEEE Transactions on Signal Processing, January 2007, 165-177.</mixed-citation></ref><ref id="scirp.63209-ref15"><label>15</label><mixed-citation publication-type="other" xlink:type="simple">Tvrdik, J., Pavliska, V. and Habiballa, H (2008) Stochastic Self-Adaptive Algorithms for Global Optimization— MATLAB and C++ Library. http://www1.osu.cz/home/habibal/optimization/index.html</mixed-citation></ref><ref id="scirp.63209-ref16"><label>16</label><mixed-citation publication-type="other" xlink:type="simple">Ammula, V., Rao, S.M. and Wentworth, S.M. (2010) Dual Excited Planar Circular Array Antennas for Direction Agile Applications. 42nd Southeastern Symposium on System Theory, Tyler, 7-9 March 2010, 138-142. http://dx.doi.org/10.1109/ssst.2010.5442853</mixed-citation></ref><ref id="scirp.63209-ref17"><label>17</label><mixed-citation publication-type="other" xlink:type="simple">Ahmidi, N., Neyestanak, A. and Dawes, R. (2008) Elliptical Array Antenna Design Based on Particle Swarm Method Using Fuzzy Decision Rules. 24th Biennial Symposium on Communications, Kingston, 24-26 June 2008, 352-355. http://dx.doi.org/10.1109/BSC.2008.4563274</mixed-citation></ref><ref id="scirp.63209-ref18"><label>18</label><mixed-citation publication-type="other" xlink:type="simple">Chou, J.Y.-L. (2002) An Investigation on the Impact of Antenna Array Geometry on Beam Forming User Capacity. Master of Science (Engineering), Queen’s University, Kingston.</mixed-citation></ref><ref id="scirp.63209-ref19"><label>19</label><mixed-citation publication-type="other" xlink:type="simple">Ioannidis, P. and Balanis, C.A. (2005) Uniform Circular Arrays for Smart Antennas. IEEE Antennas and Propagation Magazine, 47, 192-206. http://dx.doi.org/10.1109/MAP.2005.1589932</mixed-citation></ref></ref-list></back></article>