VE3KL Presentation 4NEC2 Antenna Simulator by Arie Voors

Slides:



Advertisements
Similar presentations
Smith Chart Impedance measured at a point along a transmission line depends not only on what is connected to the line, but also on the properties of the.
Advertisements

Chapter 13 Transmission Lines
EMLAB 1 4. Linear wire antenna. EMLAB 2 Simulation of dipole antennas.
A NTENNA M ODELING FOR B EGINNERS Jonathan Woo W6GX June
Different Types of Antennas
Small 500 KHz Transmitting Antennas VE3KL 5/5/2015David Conn VE3KL1 Vertical 500 KHz Antenna….. Courtesy (Gunnar SM6BGP) Height = 30 metres R (antenna)
Ray Tracing A radio signal will typically encounter multiple objects and will be reflected, diffracted, or scattered These are called multipath signal.
Antennas.
Chapter 6 Antennas Antenna Basics
Helical Antennas Supervisor: Dr. Omar Saraereh Written By:
EZNEC Tutorial – Part III NPARC Presentation David Berkley, K2MUN And Barry Cohen, K2JV October 27, 2014.
EZNEC Tutorial – Part II NPARC Presentation David Berkley, K2MUN And Barry Cohen, K2JV October 13, 2014.
9. Radiation & Antennas Applied EM by Ulaby, Michielssen and Ravaioli.
Family Tree of Antennas David Conn VE3KL
Antenna Types Dipole Folded Dipole Monopole
CHAPTER 8 ANTENNAS.
Antenna Design Tools VE3KL
Chapter 4 Linear Wire Antennas ECE 5318/6352 Antenna Engineering
Antenna Modeling With 4NEC2
COMPUTED ENVELOPE LINEARITY OF SEVERAL FM BROADCAST ANTENNA ARRAYS J. Dane Jubera 2008 NAB Engineering Conference.
Efficient design of a C-band aperture-coupled stacked microstrip array using Nexxim and Designer Alberto Di Maria German Aerospace Centre (DLR) – Microwaves.
2M Moxon Antenna.
Antenna Modeling Presented by: Dave Woolf - K8RSP Bob Kenyon - K8LJ 12/06/2006.
Telecommunications JBCardenas © 1982 Com3 1Q1516 Antenna Design JBC © 198 v A2,2 Key design requirements 1.Provide the theoretical computations of shapes.
10/5/2015Antenna Presentation: Carp,Ontario1 Family Tree of Antennas David Conn VE3KL Acknowledgements Acknowledgements Doug Leach VE3XK Doug Leach VE3XK.
Wireless Technology Lab., Kyung Hee University S-band Patch Antenna Design for CINEMA Chungju Kim
Antennas: from Theory to Practice 4. Antenna Basics
Doc.: IEEE /0431r0 Submission April 2009 Alexander Maltsev, Intel CorporationSlide 1 Polarization Model for 60 GHz Date: Authors:
Modeling Signal Leakage Characteristics of Broadband Over Power Line (BPL) Using NEC With Experimental Verification Steve Cerwin WA5FRF Institute Scientist.
Part I: Dipoles by Marc C. Tarplee Ph.D. N4UFP
Helix Antenna Antenna and Microwave Laboratory In the name of God
Remcom Inc. 315 S. Allen St., Suite 416  State College, PA  USA Tel:  Fax:   ©
Telecommunications JBCardenas © 1982 Com3 3Q1415 Antenna Design JBC © 198 v A2,2 Additional data is in a separately provided Excel file. Key design requirements.
1 Antennas for Emergency Communications. Emergency Antennas VHF / UHF - FM HF – Voice, CW, or Digital 2.
ENE 429 Antenna and Transmission lines Theory
Notes 16 ECE 6340 Intermediate EM Waves Fall 2015
Telecommunications JBCardenas © 1982 Com3 4Q1516 Antenna Design JBC © 198 v A2,2 Key design requirements 1.Undertake the theoretical computations of shapes.
Antenna Basics.
ANTENNA THEORY : Analysis and design Third edition
Design of small directive antennas for IoT Habib Mariam Luvuezo Holldry July, 2017.
Antennas/Antenna Arrays
ANTENNA MEASUREMENTS Measurement of Radiation Pattern Gain
Antenna Design for Zigbee System
Designing a Circularly Polarized Antenna for EagleSat
4. Linear wire antenna.
Com3 2Q1617 Antenna Design Key design requirements
Antennas 10/18/2017.
Low-profile corrugated feeder horn antenna (Bull's Eye)
Vertical Antenna Myths
Amateur Extra Q & A Study Pool
Polarization in Nature, Technology and Radio
Ferrites VE3KL A spinning electron works like a gyroscope Gyro frequency tells all J Bo A method that you can use easily to evaluate your own noise environment.
Chapter 5. Polarization 第五章 極化 亞洲大學 資訊工程學系碩士班 呂克明教授 二○○六年十月十六日
The Lure of The Ladder Line G5RV Antenna VE3KL
Ham ANTENNAS: A practical introduction to The THEORY AND operation
VE3KL Selecting a Portable HF Antenna
Polarization in Nature, Technology and Radio
Announcements I should have exams back to you on Fri.
Antenna Design Tools VE3KL
CHAPTER 8 ANTENNAS.
Introduction to Antenna Modeling
Helical Antennas Supervisor: Dr. Omar Saraereh Written By:
Signals and Noise in Amateur Radio Systems
Family Tree of Antennas David Conn VE3KL
HF Signal Propagation Bill Leonard N0CU 1 June 2019
Antenna Theory Chapter.4.7.4~4.8.1 Antennas
Helical antenna It is a simple Broad band VHF and UHF antenna. The concept of Helical antenna is first introduced by J.D.Kraus. It consists of a helix.
ANTENNA’S MURRAY AMATEUR RADIO CLUB – KJ7HRI PRESENTS
Antenna Theory By CONSTANTINE A.BALANIS Ch1.4, 2.1~2.2.4 O Yeon Jeong.
SECTION 3 - Antenna Fundamentals
Presentation transcript:

VE3KL Presentation 4NEC2 Antenna Simulator by Arie Voors Based on the NEC2/4 Fortran Kernel Uses the classic Method of Moments Models radiating wires, loads, ground, sources…….more Four Editors with extensive Math capabilities Smith Charts Optimizer Extremely powerful graphics capabilities Free, users forum, updated frequently A method that you can use easily to evaluate your own noise environment A method that you can use to evaluate the quality of the ionosphere at any give time. Some methods to control received noise The Shannon Hartley limits 2/18/2019 David Conn VE3KL

Spherical Coordinate System Z θ Rx Antenna Elevation angle = 90 - θ Tx Antenna Y XY Horizontal Plane Z Vertical axis φ A method that you can use easily to evaluate your own noise environment A method that you can use to evaluate the quality of the ionosphere at any give time. Some methods to control received noise The Shannon Hartley limits X φ is the horizontal azimuth angle Θ is the angle measured from vertical 2/18/2019 David Conn VE3KL

Method of Moments A discrete numerical method Divide wires into many segments…25 per wavelength Apply Coulomb’s Law and match boundary conditions Solve large matricies EE Students usually solve the 3D Capacitor Problem 2/18/2019 David Conn VE3KL

3D Capacitor Example Divide plates into 14 segments Assume each plate has a point charge, ρi…not equal Apply a voltage V across the plates Write Coulombs Law for each charge > 14 by 14 Matrix Solve for charge by matrix inversion ρ1 ρ2 ρi V ρ14 Vj ρ1>ρ2 .. Charge piles up at edges 2/18/2019 David Conn VE3KL

4NEC2 Super Graphics Helix Antenna Vertically Oriented 2/18/2019 A method that you can use easily to evaluate your own noise environment A method that you can use to evaluate the quality of the ionosphere at any give time. Some methods to control received noise The Shannon Hartley limits 2/18/2019 David Conn VE3KL

3D VE3XK 50 MHz Stack 50 MHz OMNI Source Side Along X Axis Right Hand Circular Polarization Shown A method that you can use easily to evaluate your own noise environment A method that you can use to evaluate the quality of the ionosphere at any give time. Some methods to control received noise The Shannon Hartley limits 2/18/2019 David Conn VE3KL

2D VE3XK 50 MHz Stack 50 MHz OMNI Source Side Along X Axis Total Gain Shown A method that you can use easily to evaluate your own noise environment A method that you can use to evaluate the quality of the ionosphere at any give time. Some methods to control received noise The Shannon Hartley limits 2/18/2019 David Conn VE3KL

4NEC2 3D Near Field 2/18/2019 David Conn VE3KL A method that you can use easily to evaluate your own noise environment A method that you can use to evaluate the quality of the ionosphere at any give time. Some methods to control received noise The Shannon Hartley limits 2/18/2019 David Conn VE3KL

4NEC2 Advanced Far Field Map θ High Gain A method that you can use easily to evaluate your own noise environment A method that you can use to evaluate the quality of the ionosphere at any give time. Some methods to control received noise The Shannon Hartley limits φ 2/18/2019 David Conn VE3KL

4NEC2 Far Field Traditional Plot Several Views Vertical, Horizontal, Total Circular Polarization RHC, LHC, Total A method that you can use easily to evaluate your own noise environment A method that you can use to evaluate the quality of the ionosphere at any give time. Some methods to control received noise The Shannon Hartley limits 2/18/2019 David Conn VE3KL

4NEC2 Several Views of Frequency Response A method that you can use easily to evaluate your own noise environment A method that you can use to evaluate the quality of the ionosphere at any give time. Some methods to control received noise The Shannon Hartley limits 2/18/2019 David Conn VE3KL

4NEC2 Smith Chart 2/18/2019 David Conn VE3KL A method that you can use easily to evaluate your own noise environment A method that you can use to evaluate the quality of the ionosphere at any give time. Some methods to control received noise The Shannon Hartley limits 2/18/2019 David Conn VE3KL

Matching 2/18/2019 David Conn VE3KL A method that you can use easily to evaluate your own noise environment A method that you can use to evaluate the quality of the ionosphere at any give time. Some methods to control received noise The Shannon Hartley limits 2/18/2019 David Conn VE3KL

4NEC2..The Big Gun (Optimization) Optimize (Tune) a 2 metre dipole to 6 metres Adjust reactance to zero Vary Length A method that you can use easily to evaluate your own noise environment A method that you can use to evaluate the quality of the ionosphere at any give time. Some methods to control received noise The Shannon Hartley limits Results L= 2.8 metres Xin = -0.13 Ohms 2/18/2019 David Conn VE3KL

Optimization Issues An extremely complex and active field of study Local minimum vs. global minimum .. Optimizer gets trapped Poorly defined problem by the user .. Optimizer loops forever Type of Objective function minimum .. for science and math people good enough .. for engineers constrained values .. for engineers Can be difficult for beginners Example: An optimizer might set the antenna length to infinity! A method that you can use easily to evaluate your own noise environment A method that you can use to evaluate the quality of the ionosphere at any give time. Some methods to control received noise The Shannon Hartley limits 2/18/2019 David Conn VE3KL

Using the Editors Define the wires and axis Define the Voltage Sources Define the Ground Type if any Define R,L,C, Transmission Line components 2/18/2019 David Conn VE3KL

4NEC2 Graphical Editor for Beginners A method that you can use easily to evaluate your own noise environment A method that you can use to evaluate the quality of the ionosphere at any give time. Some methods to control received noise The Shannon Hartley limits 2/18/2019 David Conn VE3KL

4NEC2 NEC Editor to Describe the Antenna Note the use of Math Functions A method that you can use easily to evaluate your own noise environment A method that you can use to evaluate the quality of the ionosphere at any give time. Some methods to control received noise The Shannon Hartley limits 2/18/2019 David Conn VE3KL

Simple Text Editor 'VE3XK OMNI 6 metres..stack SY height=3 'height in metres SY Freq=50.0 'freq in MHz SY B=0.3556 'metres SY C=0.8128 'metres SY D=0.29845 'metres SY rad=3.17e-3 'metres SY spacingWave=0.5 'spacing in wavelengths SY spacing=spacingWave*300/freq 'spacing in metres GW 1 21 -B 0 height B 0.00 heigh height+spacing rad GW 8 21 B C height+spacing B-D C Best for Computer Defined Antennas A method that you can use easily to evaluate your own noise environment A method that you can use to evaluate the quality of the ionosphere at any give time. Some methods to control received noise The Shannon Hartley limits 2/18/2019 David Conn VE3KL

A New Windows Menu Type Editor Menu Bar on top allows user to define files rapidly Geometry Menu Open in this example 2/18/2019 David Conn VE3KL

Editing Big Antennas..500 Segments Complex Geometry Use VB.Net or C#.net to drive the editors. 4NEC2 Text Editor VB.net Program Skew Planar Antenna 2/18/2019 David Conn VE3KL

Examples “Simple” 2m Dipole Free Space X Axis Horizontal Plane Theta = 90 degrees Horizontally Polarized No Vertical Component (No surprises Here!) 2/18/2019 David Conn VE3KL

Examples “Simple” 2m Dipole Free Space X Axis Horizontal Plane Theta = 90 degrees Horizontally Polarized No Vertical Component (No surprises Here!) 2/18/2019 David Conn VE3KL

Examples..Simple 2m Dipole X Axis Horizontal Plane BLUE :Vertical E Field RED: Horizontal E Field Green: Total Field Theta = 45 degrees (Is it OK to say that a dipole is Horizontally Polarized?) 2/18/2019 David Conn VE3KL

50 MHz Horizontal OMNI Geometry Source side on X axis Horizontally Mounted Geometry Window 2/18/2019 David Conn VE3KL

50 MHz Horizontal OMNI Pattern Horizontal Plane Showing Circular Polarization Blue RHCP RED LHCP Green Total Nearly Omni Directional Circular Polarization on X axis Linear Polarization on Y axis Note the Red/Blue Cardioids θ = 55 Degrees 2/18/2019 David Conn VE3KL

50 MHz Vertical OMNI Pattern Height = 3 metres Vertical Plane Linearly Polarized Takeoff angle 30 deg Max Gain = 7.15 dBi θ = 90 Degrees 2/18/2019 David Conn VE3KL

50 MHz OMNI Stack Same Orientation as Single Element Height = 3 metres Spacing = 0.5 wavelengths 2/18/2019 David Conn VE3KL

50 MHz OMNI Stack Vertical Plane Same Orientation as Single Element Height = 3 metres Spacing = 0.5 wavelengths Gain Increased to 9.29 dBi Take off angle now 15 degrees Some high angle side lobes. 2/18/2019 David Conn VE3KL

50 MHz OMNI Stack Horizontal Plane Same Orientation as Single Element Height = 3 metres Spacing = 0.5 wavelengths Circularly Polarized along the X axis Θ = 73 degrees 2/18/2019 David Conn VE3KL

Summary Uses NEC2 or NEC4 Engine Contains an Optimizer Outstanding Graphics capability Uses four different editors Many features not covered in this talk Fundamental Wave Reflection Talk Available A method that you can use easily to evaluate your own noise environment A method that you can use to evaluate the quality of the ionosphere at any give time. Some methods to control received noise The Shannon Hartley limits 73 Dave VE3KL 2/18/2019 David Conn VE3KL