Chapter 4. Antenna Synthesis

Slides:



Advertisements
Similar presentations
BEAM FORMING NETWORKS ( BFN’s ) EE 525 Antenna Engineering.
Advertisements

EMLAB 1 2. Radiation integral. EMLAB 2 EM radiation Constant velocity Constant acceleration Periodic motion Accelerating charges radiate E and H proportional.
Nonrecursive Digital Filters
1 EMLAB Antennas. 2 EMLAB Hertzian dipole antenna Heinrich Hertz ( )
Filtering Filtering is one of the most widely used complex signal processing operations The system implementing this operation is called a filter A filter.
Design and Analysis of RF and Microwave Systems IMPEDANCE TRANSFORMERS AND TAPERS Lecturers: Lluís Pradell Francesc.
Antennas: from Theory to Practice 5. Popular Antennas
Lecture VI Antennas & Propagation -1- Antennas & Propagation Mischa Dohler King’s College London Centre for Telecommunications Research.
1 EE 542 Antennas and Propagation for Wireless Communications Array Antennas.
ANTENNA ARRAYS A Short Review. Array Factor (1) Uniform, Linear Array Equally spaced elements along the z-axis Equally spaced elements along the z-axis.
Electric Dipole Radiation The image shows electric dipole radiation from a point electric dipole. The dipole moment vector is always vertical, and its.
9. Radiation & Antennas Applied EM by Ulaby, Michielssen and Ravaioli.
A Multilayered Broadband Reflect-Array Manuel Romero.
Antennas and Radiation
Antenna Types Dipole Folded Dipole Monopole
Lecture 8 Periodic Structures Image Parameter Method
SKA AA-Low Station Configurations and Trade-off Analysis Nima Razavi-Ghods, Ahmed El-Makadema AAVP 2011, ASTRON, Dwingeloo Dec
Filter Design Techniques
ANTENNA ARRAYS.
Analysis of Low Frequency Phased Array Stations Dr. Nima Razavi-Ghods Dr. Eloy de Lera Acedo Cambridge AAVP 2010, 09/12/10 1.
Find the local linear approximation of f(x) = e x at x = 0. Find the local quadratic approximation of f(x) = e x at x = 0.
Consider the following: Now, use the reciprocal function and tangent line to get an approximation. Lecture 31 – Approximating Functions
IIR Filter design (cf. Shenoi, 2006) The transfer function of the IIR filter is given by Its frequency responses are (where w is the normalized frequency.
Normal Curves and Sampling Distributions Chapter 7.
1 Lecture 3: March 6, 2007 Topic: 1. Frequency-Sampling Methods (Part I)
Pattern Diversity Compact Patch Antenna M. S. Ruiz Palacios, M. J. Martínez Silva Universidad de Guadalajara, Jalisco, México Abstract— Diversity is a.
The Fundamental Physics of Directive Beaming at Microwave and Optical Frequencies in Terms of Leaky Waves Saman Kabiri, Master’s Student Dept. of Electrical.
CST Array Wizard User‘s Guide
Antennas: from Theory to Practice 4. Antenna Basics
11/20/2015 Fourier Series Chapter /20/2015 Fourier Series Chapter 6 2.
Chapter 7 Finite Impulse Response(FIR) Filter Design
Chapter 9-10 Digital Filter Design. Objective - Determination of a realizable transfer function G(z) approximating a given frequency response specification.
Polynomial Functions and Models
Chapter 3 Antenna Types Part 1.
Chapter 3 Antenna Types Part 1.
CHAPTER 5 Digital Processing of Continuous- Time Signal Wangweilian School of Information Science and Technology Yunnan University.
EMLAB 1 초고주파 통신 project 2015 년 2 학기. EMLAB 2 Antenna pattern synthesis.
Variance Stabilizing Transformations. Variance is Related to Mean Usual Assumption in ANOVA and Regression is that the variance of each observation is.
Maclaurin and Taylor Polynomials Objective: Improve on the local linear approximation for higher order polynomials.
Fourier Approximation Related Matters Concerning Fourier Series.
Section 10.5 Fourier Series. Taylor Polynomials are a good approximation locally, but not necessarily globally We can use Fourier approximations –May.
Antenna Theory CONSTANTINE A. BALANIS Arizona State University
RADAR ANTENNA. Functions of Radar Antenna Transducer. Concentrates the radiated energy in one direction (Gain). Collects echo energy scattered back to.
Eeng360 1 Chapter 2 Linear Systems Topics:  Review of Linear Systems Linear Time-Invariant Systems Impulse Response Transfer Functions Distortionless.
ENE 429 Antenna and Transmission lines Theory Lecture 10 Antennas DATE: 18/09/06 22/09/06.
ANTENNA THEORY ANALYSIS AND DESIGN Linear Wire Antennas
Notes 17 ECE Microwave Engineering Multistage Transformers
Microwave Engineering Chapter 5.7 ~ 5.9
1/28 Antennas & RF Devices Lab. Seminar on Microwave and Optical Communication -Antenna Theory- Chapter 10. Traveling Wave and Broadband Antennas
Antenna Theory EC 544 Lecture#5. Chapter 5 Dolph – Tchebycheff Design Equal Side Lobes Equal Side Lobes.
Hanyang University 1/15 Antennas & RF Devices Lab. MODERN ANTENNA HANDBOOK by CONSTANTINE A.BALANIS ch. 5.6 ~5.6.5 Jeong Gu Ho.
College Algebra Chapter 6 Matrices and Determinants and Applications
IIR Filter design (cf. Shenoi, 2006)
ANTENNA THEORY by Constantine A. Balanis Chapter 4.5 – 4.7.2
Polynomial Functions Objectives: Identify Polynomials and their Degree
Seminar on Microwave and Optical Communication
Chapter 4 Antenna Arrays
Chapter 9 Power Series Copyright © 2011 Pearson Education, Inc. Publishing as Pearson Addison-Wesley.
Real Zeros Intro - Chapter 4.2.
Chapter 5 Z Transform.
Quantum Two.
Seminar on Microwave and Optical Communication
Numerical Analysis Lecture 16.
Network Analysis and Synthesis
Antenna Engineering EC 544
Microwave Engineering
Antenna Array Dr Jaikaran Singh Reference Book : Antenna by John D. Kraus (TMH)
Chapter 7 Finite Impulse Response(FIR) Filter Design
Paper review Yun-tae Park Antennas & RF Devices Lab.
Antenna Theory Chapter.2.6.1~2.7 Antennas
Presentation transcript:

Chapter 4. Antenna Synthesis 4.1 Basic principle for antenna synthesis 4.2 Line source synthesis (Fourier transform, woodward-lanson sampling) 4.3 Linear array synthesis (Fourier series, woodward-lanson sampling) 4.4 Low sidelobe synthesis (Dolph-Chebyshev, Taylor)

Synthesis Problems Given affordable SLL, No. of elements, how to synthesize? Ideal case: narrow beam, constant side-lobe envelope Approaches: Dolph-Chebyshev, Taylor Line Source…. Secret behind: to synthesize a polynomial like pattern….

Dolph-Chebyshev Linear Array The Chebyshev polynomials: Property used:

Chebyshev Polyminals

Symmetrically Excited Array , P odd , P even Property: is P-1 th polynomial of Let Choose appropriate to match the coefficients to those in Chebyshev polynomial, we obtain,

Chebyshev Polynomial Example

Synthesis Standards SLL=-20log R (dB) so Optimum spacing, Endfire: Broadside: Endfire: , where

Beamwidth and Directivity (broadside) In general, (endfire) , where An approximation for the broadside: Beambroadening factor: Directivity:

Example No.1 Five element array (P=5), -20dB Side-Lobe, Half-Wavelength Spaced Dolph-Chebyshev Array

Synthesized Array Factor

Example No.2 Optimum Spaced 10-Element, -30dB Side Lobe, Dolph-Chebyshev Endfire Array

Taylor Line Source Method Transform: where a is a constant and, So the pattern maximum is, For the side-lobe region: Main beam region:

Transformed Chebyshev Polynomial

Basic Properties of Zeros Zeros of the transformed function in the side-lobes are given by: For the main beam, Introduce A so that, and For large N,

Selection of Constant a a is selected so that the first zero location remains fixed as N increases, Then The pattern should have the following format,

Ideal Pattern Factor Normalizing the pattern to unity at x=0, (side lobes) (main beam)

Realistic Pattern Factor where In format of w,

Woodward-Lawson Equivalent for The source current is

Beamwidth and Directivity (ideal Taylor) (realistic Taylor)

Example A 10-Wavelength Taylor Line Source with –25 dB side lobes and

Pattern and Current Source