Numerical Analysis of Helical and Log-Periodic Antennas For

Total Page:16

File Type:pdf, Size:1020Kb

Numerical Analysis of Helical and Log-Periodic Antennas For NUMERICAL ANALYSIS OF HELICAL AND LOG-PERIODIC ANTENNAS FOR SHORT PULSE APPLICATIONS A THESIS IN Electrical Engineering Presented to the Faculty of the University of Missouri-Kansas City in partial fulfillment of the requirements for the degree MASTER OF SCIENCE by WALEED AL-SHAIKHLI B.S., University of Missouri – Kansas City, 2018 Kansas City, Missouri 2020 © 2020 WALEED AL-SHAIKHLI ALL RIGHTS RESERVED NUMERICAL ANALYSIS OF HELICAL AND LOG-PERIODIC ANTENNAS FOR SHORT PULSE APPLICATIONS Waleed K. Al-Shaikhli, Candidate for the Master of Science Degree University of Missouri – Kansas City, 2020 ABSTRACT The planar log-periodic (LP) and helical antennas are numerically studied as two antennas with a wide range of applications. The advantages of the LP antenna are the large adjustable bandwidth as a frequency independence radiator, its low profile, and that it can be made to be elliptically polarized. The main advantages of a helical antenna are its excellent power handling capability and tunable gain. The helical antenna is widely used in many UWB applications such as Radar, satellite communication, GPS, and other short-pulse applications. High far-field gain is essential to many applications, but a tradeoff between gain, and time- domain dispersion exists if the input of the helical antenna is to consist of short-pulses. To quantify the level of dispersion, the antennas considered in this work are modeled as linear systems, and their time-domain impulse response is calculated using CST Microwave time- domain and FEKO frequency-domain simulations of the structure. A comprehensive parametric study of the helical antenna is conducted in FEKO followed by a multigoal optimized design of an L band helical antenna to minimize pulse dispersion, size, and input impedance while maximizing far-field gain and pulse shape preservation. iii APPROVAL PAGE The faculty listed below, appointed by the Dean of the School of Computing and Engineering have examined a thesis titled “Numerical Analysis of Helical and Log-periodic Antennas for Short Pulse Applications,” presented by Waleed Al-Shaikhli, candidate for the Master of Science degree, and certify that in their opinion it is worthy of acceptance. Supervisory Committee Ahmed M. Hassan, Ph.D., Committee Chair Department of Computer Science & Electrical Engineering Deb Chatterjee, Ph.D. Department of Computer Science & Electrical Engineering Anthony Caruso, Ph.D. Department of Physics and Astronomy Mahrukh Khan, Ph.D. Department of Computer Science & Electrical Engineering iv TABLE OF CONTENTS ABSTRACT ................................................................................................................. iii LIST OF ILLUSTRATIONS ............................................................................................ viii LIST OF TABLES .......................................................................................................... xi LIST OF ABBREVIATIONS ............................................................................................xii ACKNOWLEDGMENTS............................................................................................... xiii 1. Antenna Introduction and Definitions ......................................................................... 1 Motivation for Work .................................................................................................................. 1 The Antenna Concept ................................................................................................................ 1 Antenna Figures-of-Merit .......................................................................................................... 2 Field Regions .............................................................................................................................. 8 Antennas in Short-Pulse Systems............................................................................................... 9 Friis transmission equation ...................................................................................................... 11 Survey of Antennas for Short Pulse Applications ..................................................................... 12 Summary.................................................................................................................................. 15 2. Performance Analysis for Short Pulse Applications ................................................... 16 UWB Signals ............................................................................................................................ 17 Frequency Domain Performance ............................................................................................. 19 Group Delay ............................................................................................................................. 21 Fidelity Factor .......................................................................................................................... 22 Time Domain Performance ...................................................................................................... 24 Summary.................................................................................................................................. 27 v 3. The Log Periodic Antenna ......................................................................................... 28 Frequency Independent antennas ........................................................................................... 28 The Planar Log-Periodic Antenna ............................................................................................ 29 Design of a Planar Log-Periodic for Short pulse-UWB Applications ........................................ 33 Size and Polarization improvement of a Planar Log-Periodic .................................................. 38 Summary.................................................................................................................................. 41 4. The Helical Antenna ................................................................................................. 42 Modes of Operation................................................................................................................. 43 Helical Antenna Applications ................................................................................................... 44 Antenna Validation .................................................................................................................. 45 Helical Antenna Literature Review .......................................................................................... 47 Summary.................................................................................................................................. 48 5. Design and Parametric Analysis of A Helical Antenna ................................................ 49 Antenna Design ....................................................................................................................... 49 Ground Plane Size .................................................................................................................... 53 Wire Diameter ......................................................................................................................... 55 Helix Turns ............................................................................................................................... 57 Dielectric Rod ........................................................................................................................... 62 Impedance Matching ............................................................................................................... 67 Summary.................................................................................................................................. 76 6. Helical Antenna Optimization ................................................................................... 77 vi Antenna Optimization ............................................................................................................. 77 Summary.................................................................................................................................. 84 7. Conclusion and Future Work..................................................................................... 85 References ............................................................................................................... 87 VITA ......................................................................................................................... 95 vii LIST OF ILLUSTRATIONS FIGURE PAGE Figure 1. Antenna 2D field pattern ........................................................................................... 2 Figure 2. Reflection, dielectric and ohmic losses ...................................................................... 7 Figure 3. Friis Equation ........................................................................................................... 11 Figure 4. Example of UWB signal in the (a) time-domain (b) and frequency domain ............ 18 Figure 5. Frequency-domain system link-level characterization [5] ...................................... 19 Figure 6. UWB system link-level characterization in the time-domain [5]. ............................ 24 Figure 7. Planar Log-periodic .................................................................................................. 30 Figure 8. 2-Arm Log-Periodic Antenna ...................................................................................
Recommended publications
  • Chapter 22 Fundamentalfundamental Propertiesproperties Ofof Antennasantennas
    ChapterChapter 22 FundamentalFundamental PropertiesProperties ofof AntennasAntennas ECE 5318/6352 Antenna Engineering Dr. Stuart Long 1 .. IEEEIEEE StandardsStandards . Definition of Terms for Antennas . IEEE Standard 145-1983 . IEEE Transactions on Antennas and Propagation Vol. AP-31, No. 6, Part II, Nov. 1983 2 ..RadiationRadiation PatternPattern (or(or AntennaAntenna Pattern)Pattern) “The spatial distribution of a quantity which characterizes the electromagnetic field generated by an antenna.” 3 ..DistributionDistribution cancan bebe aa . Mathematical function . Graphical representation . Collection of experimental data points 4 ..QuantityQuantity plottedplotted cancan bebe aa . Power flux density W [W/m²] . Radiation intensity U [W/sr] . Field strength E [V/m] . Directivity D 5 . GraphGraph cancan bebe . Polar or rectangular 6 . GraphGraph cancan bebe . Amplitude field |E| or power |E|² patterns (in linear scale) (in dB) 7 ..GraphGraph cancan bebe . 2-dimensional or 3-D most usually several 2-D “cuts” in principle planes 8 .. RadiationRadiation patternpattern cancan bebe . Isotropic Equal radiation in all directions (not physically realizable, but valuable for comparison purposes) . Directional Radiates (or receives) more effectively in some directions than in others . Omni-directional nondirectional in azimuth, directional in elevation 9 ..PrinciplePrinciple patternspatterns . E-plane . H-plane Plane defined by H-field and Plane defined by E-field and direction of maximum direction of maximum radiation radiation (usually coincide with principle planes of the coordinate system) 10 Coordinate System Fig. 2.1 Coordinate system for antenna analysis. 11 ..RadiationRadiation patternpattern lobeslobes . Major lobe (main beam) in direction of maximum radiation (may be more than one) . Minor lobe - any lobe but a major one . Side lobe - lobe adjacent to major one .
    [Show full text]
  • Array Designs for Long-Distance Wireless Power Transmission: State
    INVITED PAPER Array Designs for Long-Distance Wireless Power Transmission: State-of-the-Art and Innovative Solutions A review of long-range WPT array techniques is provided with recent advances and future trends. Design techniques for transmitting antennas are developed for optimized array architectures, and synthesis issues of rectenna arrays are detailed with examples and discussions. By Andrea Massa, Member IEEE, Giacomo Oliveri, Member IEEE, Federico Viani, Member IEEE,andPaoloRocca,Member IEEE ABSTRACT | The concept of long-range wireless power trans- the state of the art for long-range wireless power transmis- mission (WPT) has been formulated shortly after the invention sion, highlighting the latest advances and innovative solutions of high power microwave amplifiers. The promise of WPT, as well as envisaging possible future trends of the research in energy transfer over large distances without the need to deploy this area. a wired electrical network, led to the development of landmark successful experiments, and provided the incentive for further KEYWORDS | Array antennas; solar power satellites; wireless research to increase the performances, efficiency, and robust- power transmission (WPT) ness of these technological solutions. In this framework, the key-role and challenges in designing transmitting and receiving antenna arrays able to guarantee high-efficiency power trans- I. INTRODUCTION fer and cost-effective deployment for the WPT system has been Long-range wireless power transmission (WPT) systems soon acknowledged. Nevertheless, owing to its intrinsic com- working in the radio-frequency (RF) range [1]–[5] are plexity, the design of WPT arrays is still an open research field currently gathering a considerable interest (Fig.
    [Show full text]
  • Improving Wireless LAN Antenna Gain and Coverage
    APPLICATION NOTE Improving Wireless LAN Antenna Gain and Coverage antenna, which can help mitigate interference between floors. The only drawback is that the longer antenna may be somewhat less aesthetic. Mounting a dipole antenna on a conductive ground plane has a similar effect as using a longer antenna. The elevation pattern is flattened, creating higher gain around the perimeter of the doughnut. Additionally, the ground plane mounted antennas pattern is maximized downward slightly (if the antenna is mounted beneath a ceiling ground plane). This is an ideal elevation pattern for a ceiling mounted antenna in a multi-story building. The ground plane has the effect of minimizing gain below and especially above Most of the antennas provided with Wi-Fi the antenna. access points, or purchased separately, are simple dipole antennas with an omni- Wi-Fi antennas may be classified as ground directional pattern. Omni-directional means plane dependent and ground plane that the gain is the same in a 360º circle independent. The ground plane dependent around the axis of the antenna. antenna must be mounted on a conductive, flat ground plane which is several However, the elevation gain pattern is wavelengths long and wide in order to different. In cross section, the elevation provide the rated gain and impedance pattern is that of a doughnut, with the match. The ground plane independent antenna axis running through the center of antenna does not need to be mounted on a the doughnut. In the absence of a ground ground plane to provide the rated gain and plane, the gain of the dipole is a maximum impedance match.
    [Show full text]
  • Model ATH33G50 Antenna, Standard Gain 33Ghz–50Ghz
    Model ATH33G50 Antenna, Standard Gain 33GHz–50GHz The Model ATH33G50 is a wide band, high gain, high power microwave horn antenna. With a minimum gain of 20dB over isotropic, the Model ATH33G50 supplies the high intensity fields necessary for RFI/EMI field testing within and beyond the confines of a shielded room. The Model ATH33G50 is extremely compact and light weight for ready mobility, yet is built tough enough for the extra demands of outdoor use and easily mounts on a rigid waveguide by the waveguide flange. Part of a family of microwave frequency antennas, the Model ATH33G50 provides the 33-50GHz response required for many often used test specifications. The Model ATH33G50 standard gain pyramidal horn antenna is electroformed to give precise dimensions and reproducible electrical characteristics. The Model ATH33G50 is used to measure gain for other antennas by comparing the signal level of a test antenna to the signal level of a test antenna to the standard gain horn and adding the difference to the calibrated gain of the standard gain horn at the test frequency. The Model ATH33G50 is also used as a reference source in dual-channel antenna test receivers and can be used as a pickup horn for radiation monitoring. SPECIFICATIONS FREQUENCY RANGE .................................................... 33-50GHz POWER INPUT (maximum) ............................................ 240 watts CW 2000 watts Peak POWER GAIN (over isotropic) ........................................ 20 ± 2dB VSWR Average ................................................................
    [Show full text]
  • High Gain Isotropic Rectenna Erika Vandelle, Phi Long Doan, Do Hanh Ngan Bui, T.-P
    High gain isotropic rectenna Erika Vandelle, Phi Long Doan, Do Hanh Ngan Bui, T.-P. Vuong, Gustavo Ardila, Ke Wu, Simon Hemour To cite this version: Erika Vandelle, Phi Long Doan, Do Hanh Ngan Bui, T.-P. Vuong, Gustavo Ardila, et al.. High gain isotropic rectenna. 2017 IEEE Wireless Power Transfer Conference (WPTC), May 2017, Taipei, Taiwan. pp.54-57, 10.1109/WPT.2017.7953880. hal-01722690 HAL Id: hal-01722690 https://hal.archives-ouvertes.fr/hal-01722690 Submitted on 29 Aug 2018 HAL is a multi-disciplinary open access L’archive ouverte pluridisciplinaire HAL, est archive for the deposit and dissemination of sci- destinée au dépôt et à la diffusion de documents entific research documents, whether they are pub- scientifiques de niveau recherche, publiés ou non, lished or not. The documents may come from émanant des établissements d’enseignement et de teaching and research institutions in France or recherche français ou étrangers, des laboratoires abroad, or from public or private research centers. publics ou privés. High Gain Isotropic Rectenna E. Vandelle1, P. L. Doan1, D.H.N. Bui1, T.P. Vuong1, G. Ardila1, K. Wu2, S. Hemour3 1 Université Grenoble Alpes, CNRS, Grenoble INP*, IMEP–LAHC, Grenoble, France 2 Polytechnique Montréal, Poly-Grames, Montreal, Quebec, Canada 3 Université de Bordeaux, IMS Bordeaux, Bordeaux Aquitaine INP, Bordeaux, France *Institute of Engineering University of Grenoble Alpes {vandeler, buido, vuongt, ardilarg}@minatec.inpg.fr [email protected] [email protected] [email protected] Abstract— This paper introduces an original strategy to step up the capacity of ambient RF energy harvesters.
    [Show full text]
  • 25. Antennas II
    25. Antennas II Radiation patterns Beyond the Hertzian dipole - superposition Directivity and antenna gain More complicated antennas Impedance matching Reminder: Hertzian dipole The Hertzian dipole is a linear d << antenna which is much shorter than the free-space wavelength: V(t) Far field: jk0 r j t 00Id e ˆ Er,, t j sin 4 r Radiation resistance: 2 d 2 RZ rad 3 0 2 where Z 000 377 is the impedance of free space. R Radiation efficiency: rad (typically is small because d << ) RRrad Ohmic Radiation patterns Antennas do not radiate power equally in all directions. For a linear dipole, no power is radiated along the antenna’s axis ( = 0). 222 2 I 00Idsin 0 ˆ 330 30 Sr, 22 32 cr 0 300 60 We’ve seen this picture before… 270 90 Such polar plots of far-field power vs. angle 240 120 210 150 are known as ‘radiation patterns’. 180 Note that this picture is only a 2D slice of a 3D pattern. E-plane pattern: the 2D slice displaying the plane which contains the electric field vectors. H-plane pattern: the 2D slice displaying the plane which contains the magnetic field vectors. Radiation patterns – Hertzian dipole z y E-plane radiation pattern y x 3D cutaway view H-plane radiation pattern Beyond the Hertzian dipole: longer antennas All of the results we’ve derived so far apply only in the situation where the antenna is short, i.e., d << . That assumption allowed us to say that the current in the antenna was independent of position along the antenna, depending only on time: I(t) = I0 cos(t) no z dependence! For longer antennas, this is no longer true.
    [Show full text]
  • W5GI MYSTERY ANTENNA (Pdf)
    W5GI Mystery Antenna A multi-band wire antenna that performs exceptionally well even though it confounds antenna modeling software Article by W5GI ( SK ) The design of the Mystery antenna was inspired by an article written by James E. Taylor, W2OZH, in which he described a low profile collinear coaxial array. This antenna covers 80 to 6 meters with low feed point impedance and will work with most radios, with or without an antenna tuner. It is approximately 100 feet long, can handle the legal limit, and is easy and inexpensive to build. It’s similar to a G5RV but a much better performer especially on 20 meters. The W5GI Mystery antenna, erected at various heights and configurations, is currently being used by thousands of amateurs throughout the world. Feedback from users indicates that the antenna has met or exceeded all performance criteria. The “mystery”! part of the antenna comes from the fact that it is difficult, if not impossible, to model and explain why the antenna works as well as it does. The antenna is especially well suited to hams who are unable to erect towers and rotating arrays. All that’s needed is two vertical supports (trees work well) about 130 feet apart to permit installation of wire antennas at about 25 feet above ground. The W5GI Multi-band Mystery Antenna is a fundamentally a collinear antenna comprising three half waves in-phase on 20 meters with a half-wave 20 meter line transformer. It may sound and look like a G5RV but it is a substantially different antenna on 20 meters.
    [Show full text]
  • California State University, Northridge
    CALIFORNIA STATE UNIVERSITY, NORTHRIDGE Design of a 5.8 GHz Two-Stage Low Noise Amplifier A graduate project submitted in partial fulfillment of the requirements For the degree of Master of Science in Electrical Engineering By Yashika Parwath August 2020 The graduate project of Yashika Parwath is approved: Dr. John Valdovinos Date Dr. Jack Ou Date Dr. Brad Jackson, Chair Date California State University, Northridge ii Acknowledgement I would like to express my sincere gratitude to Dr. Brad Jackson for his unwavering support and mentorship that aided me to finish my master’s project. With his deep understanding of the subject and valuable inputs this design project has been quite a learning wheel expanding my knowledge horizons. I would also like to thank Dr. John Valdovinos and Dr. Jack Ou for being the esteemed members of the committee. iii Table of Contents Signature page ii Acknowledgement iii List of Figures v List of Tables vii Abstract viii Chapter 1: Introduction 1 1.1 Communication System 1 1.2 Low Noise Amplifier 2 1.3 Design Goals 2 Chapter 2: LNA Theory and Background 4 2.1 Introduction 4 2.2 Terminology 4 2.3 Design Procedure 10 Chapter 3: LNA Design Procedure 12 3.1 Transistor 12 3.2 S-Parameters 12 3.3 Stability 13 3.4 Noise and Noise Figure 16 3.5 Cascaded Noise Figure 16 3.6 Noise Circles 17 3.7 Unilateral Figure of Merit 18 3.8 Gain 20 Chapter 4: Source and Load Reflection Coefficient 23 4.1 Reflection Coefficient 23 4.2 Source Reflection Coefficient 24 4.3 Load Reflection Coefficient 26 Chapter 5: Impedance Matching
    [Show full text]
  • Analysis and Measurement of Horn Antennas for CMB Experiments
    Analysis and Measurement of Horn Antennas for CMB Experiments Ian Mc Auley (M.Sc. B.Sc.) A thesis submitted for the Degree of Doctor of Philosophy Maynooth University Department of Experimental Physics, Maynooth University, National University of Ireland Maynooth, Maynooth, Co. Kildare, Ireland. October 2015 Head of Department Professor J.A. Murphy Research Supervisor Professor J.A. Murphy Abstract In this thesis the author's work on the computational modelling and the experimental measurement of millimetre and sub-millimetre wave horn antennas for Cosmic Microwave Background (CMB) experiments is presented. This computational work particularly concerns the analysis of the multimode channels of the High Frequency Instrument (HFI) of the European Space Agency (ESA) Planck satellite using mode matching techniques to model their farfield beam patterns. To undertake this analysis the existing in-house software was upgraded to address issues associated with the stability of the simulations and to introduce additional functionality through the application of Single Value Decomposition in order to recover the true hybrid eigenfields for complex corrugated waveguide and horn structures. The farfield beam patterns of the two highest frequency channels of HFI (857 GHz and 545 GHz) were computed at a large number of spot frequencies across their operational bands in order to extract the broadband beams. The attributes of the multimode nature of these channels are discussed including the number of propagating modes as a function of frequency. A detailed analysis of the possible effects of manufacturing tolerances of the long corrugated triple horn structures on the farfield beam patterns of the 857 GHz horn antennas is described in the context of the higher than expected sidelobe levels detected in some of the 857 GHz channels during flight.
    [Show full text]
  • Circuit and Method for Balun Compensation
    Europaisches Patentamt J European Patent Office © Publication number: 0 644 605 A1 Office europeen des brevets EUROPEAN PATENT APPLICATION © Application number: 94112882.9 int. CI 6: H01P 5/10 @ Date of filing: 18.08.94 © Priority: 22.09.93 US 124875 © Applicant: MOTOROLA, INC. 1303 East Algonquin Road @ Date of publication of application: Schaumburg, IL 60196 (US) 22.03.95 Bulletin 95/12 @ Inventor: Kaltenecker, Robert S. © Designated Contracting States: 2719 S. Estrella Circle DE FR GB Mesa, Arizona 85202 (US) Inventor: Pfizenmayer, Henry L. 3318 E. Turquiose Avenue Phoenix, Arizona 85028 (US) Inventor: Wernett, Frederick C. 492 Kweo Trail Flagstaff, Arizona 86001 (US) © Representative: Hudson, Peter David et al Motorola European Intellectual Property Midpoint Alencon Link Basingstoke, Hampshire RG21 1PL (GB) © Circuit and method for balun compensation. 10 © A novel circuit and method for providing am- 14 plitude and phase compensation for a balun in order P1 P2 7o,Eo | Ox to provide first and second voltage signals that are 12 1 16 balanced has been provided. The compensation is I rrm < ^ achieved by an amplitude and phase com- adding P3 pensation circuit such as a transmission line (14) or 1 mm 18 o inductive (20) and capacitive (22) lumped elements CO in series with one of the ports of the balun on the balanced side. The and amplitude phase compensa- FIG. 1 tion circuit includes a characteristic impedance CO pa- rameter (Zo) and an electrical length parameter (Eo) that are optimized such that the amplitude difference between first and second voltage signals is mini- mized, while the magnitude of the phase difference between first and second voltage signals is maxi- mized.
    [Show full text]
  • Open Bradley Sherman Spring 2014.Pdf
    THE PENNSYLVANIA STATE UNIVERSITY SCHREYER HONORS COLLEGE DEPARTMENT OF ELECTRICAL ENGINEERING HIGH FREQUENCY ANTENNA COUPLING STUDY BRADLEY SHERMAN SPRING 2014 A thesis submitted in partial fulfillment of the requirements for a baccalaureate degree in Electrical Engineering with honors in Electrical Engineering Reviewed and approved* by the following: James K. Breakall Professor of Electrical Engineering Thesis Supervisor John D. Mitchell Professor of Electrical Engineering Honors Adviser Keith A. Lysiak Senior Research Associate Thesis Reader * Signatures are on file in the Schreyer Honors College. i ABSTRACT The objective of this project was to develop a methodology to accurately predict antenna coupling through the use of numerical electromagnetic modeling. A high-frequency (HF) ionospheric sounder is being developed for HF propagation studies. This sounder requires high power transmissions on one antenna while receiving on another antenna. In order to minimize the coupling of high power energy back into the receiver, the transmit and receive antenna coupling must be minimized. The results of this research effort have shown that the current antenna setup can be improved by choosing a co-polarization setup and changing the frequency to 6.78 MHz. Rotating the receive antenna so that it runs parallel to the receive antenna decreases the antenna coupling by 8 dB. Typically the cross-polarization created by putting two antennas perpendicular to each other would decrease the antenna coupling dramatically, but that does not work if the feeds are along the perpendicular access. Attaining the ideal perpendicular setup is not possible in this case due to space restrictions. ii TABLE OF CONTENTS List of Figures .........................................................................................................................
    [Show full text]
  • Arrays: the Two-Element Array
    LECTURE 13: LINEAR ARRAY THEORY - PART I (Linear arrays: the two-element array. N-element array with uniform amplitude and spacing. Broad-side array. End-fire array. Phased array.) 1. Introduction Usually the radiation patterns of single-element antennas are relatively wide, i.e., they have relatively low directivity. In long distance communications, antennas with high directivity are often required. Such antennas are possible to construct by enlarging the dimensions of the radiating aperture (size much larger than ). This approach, however, may lead to the appearance of multiple side lobes. Besides, the antenna is usually large and difficult to fabricate. Another way to increase the electrical size of an antenna is to construct it as an assembly of radiating elements in a proper electrical and geometrical configuration – antenna array. Usually, the array elements are identical. This is not necessary but it is practical and simpler for design and fabrication. The individual elements may be of any type (wire dipoles, loops, apertures, etc.) The total field of an array is a vector superposition of the fields radiated by the individual elements. To provide very directive pattern, it is necessary that the partial fields (generated by the individual elements) interfere constructively in the desired direction and interfere destructively in the remaining space. There are six factors that impact the overall antenna pattern: a) the shape of the array (linear, circular, spherical, rectangular, etc.), b) the size of the array, c) the relative placement of the elements, d) the excitation amplitude of the individual elements, e) the excitation phase of each element, f) the individual pattern of each element.
    [Show full text]