AE6PM 11/06/20071 Heard at Pacificon 2001-2007 Technical tidbits from selected presentations.

Slides:



Advertisements
Similar presentations
Note 2 Transmission Lines (Time Domain)
Advertisements

Feeders and Antennas.
Technician Licensing Class Supplement T4, Questions Only Amateur Radio Practices 2 Exam Questions, 2 Groups.
How they work How they are made
© 2008 The McGraw-Hill Companies 1 Principles of Electronic Communication Systems Third Edition Louis E. Frenzel, Jr.
WØINK February 2009 BALUNSPage 1 of 25 BALUNS BY VIRGIL LEENERTS WØINK ARRL Technical Specialist –
1 Chelmsford Amateur Radio Society Intermediate Licence Course Carl Thomson G3PEM Slide Set 9: v1.2, 31-May-2009 Antennas & Feeders Chelmsford Amateur.
Chapter 13 Transmission Lines
Chapter Fourteen: Transmission Lines
UNIVERSITI MALAYSIA PERLIS
Antennas.
Chapter 6 Antennas Antenna Basics
Antennas Lecture 9.
Key Points We have seen that the antenna theory is based on the radiation produced by the sources (charges, currents) on the surface of a conductor. When.
Folded Dipole Antenna BHAVIN V KAKANI IT-NU. Introduction A folded dipole is a half-wave dipole with an additional wire connecting its two ends. It’s.
Name: Mashhour jumah ID: Welcome. What is an antenna? An antenna is an electrical conductor or system of conductors used for transmission and.
Urban Legends from the world of Antennas Marc C. Tarplee Ph.D., N4UFP ARRL South Carolina Section Technical Coordinator.
Training materials for wireless trainers Antennas and Transmission Lines.
Two Bands from One Dipole Marc C. Tarplee Ph.D., N4UFP ARRL South Carolina Section Technical Coordinator.
Family Tree of Antennas David Conn VE3KL
Antennas and Propagation
G Practical MRI 1 – 26 th March 2015 G Practical MRI 1 Review of Circuits and Electronics.
Care Use and Feeding of a MFJ-259B Antenna Analyzer.
Lecture 2 Most basic facts from Electricity needed for understanding telecommunications Local transmission lines in the telephone system Decibels Signals.
General Licensing Class G9A – G9D Antennas Your organization and dates here.
ELECTRONIC COMMUNICATIONS A SYSTEMS APPROACH CHAPTER Copyright © 2014 by Pearson Education, Inc. All Rights Reserved Electronic Communications: A Systems.
1 ENE 429 Antenna and Transmission lines Theory Lecture 4 Transmission lines.
Lecture 4.  1.5 The terminated lossless transmission line What is a voltage reflection coefficient? Assume an incident wave ( ) generated from a source.
OBJECTIVES To become familiar with propagation of signals through lines Understand signal propagation at Radio frequencies Understand radio propagation.
Oct. 16, 2006 Midterm Next Class Assignment #4 is Marked
10/5/2015Antenna Presentation: Carp,Ontario1 Family Tree of Antennas David Conn VE3KL Acknowledgements Acknowledgements Doug Leach VE3XK Doug Leach VE3XK.
Transmission Line Theory
Trasmission lines.
10. Transmission Line 서강대학교 전자공학과 윤상원 교수
CHAPTER 4 TRANSMISSION LINES.
12 Transmission Lines.
TELECOMMUNICATIONS Dr. Hugh Blanton ENTC 4307/ENTC 5307.
Simple radio communications system. Electric field around elements.
SUBELEMENT G9 ANTENNAS AND FEEDLINES [4 Exam Questions–4 Groups]
G9 - Antennas 1 G9 – Antennas and Feedlines [4 exam questions - 4 groups] G9A - Antenna feed lines: characteristic impedance and attenuation; SWR calculation,
Yi HUANG Department of Electrical Engineering & Electronics
1.  Transmission lines or T-lines are used to guide propagation of EM waves at high frequencies.  Examples: › Transmitter and antenna › Connections.
ECE 4710: Lecture #37 1 Link Budget Analysis  BER baseband performance determined by signal to noise ratio ( S / N ) at input to detector (product, envelope,
Part I: Dipoles by Marc C. Tarplee Ph.D. N4UFP
A TECHNICAL BRIEFING FOR AMATEUR RADIO OPERATORS
ENE 490 Applied Communication Systems
Chapter 2 Transmission Line Theory (2.1 ~ 2.5) 전자파연구실 1.
1 “BUILDING QUICK TAPE ANTENNAS” Dr. Al Torres KP4AQI FEBRUARY 2015.
Practice Questions 2015 General License Course. How does antenna gain stated in dBi compare to gain stated in dBd for the same antenna? A. dBi gain figures.
Antenna Basics.
ANTENNA THEORY : Analysis and design Third edition
Antenna Matching Techniques
G9 - Antennas 1 G9 – Antennas and Feedlines [4 exam questions - 4 groups] G9A - Antenna feed lines: characteristic impedance and attenuation; SWR calculation,
Hanyang University 1/24 ANTENNA THEORY ANALYSIS AND DESIGN Chapter.2 Sungjoon YOON
HF Mobile Vertical Design By Larry Benson, N7GY Vertical Antenna Theory Base vs Center Loaded Efficiency/Installation Techniques Design Example. Program.
Chapter 7 Antennas Antennas Jim Siemons, AF6PU.
Lecture 2 Transmission Line Characteristics
TRANSMISSION LINES.
Subject Name: Microwave and Radar Subject Code: 10EC54
International Africa University Faculty of Engineering Eight Semester
20M Antenna.
Ham ANTENNAS: A practical introduction to The THEORY AND operation
Applied Electromagnetic Waves Notes 6 Transmission Lines (Time Domain)
What must be considered to determine the minimum current capacity needed for a transceiver power supply? A. Efficiency of the transmitter at full power.
Ferrite cores for transmitting chokes (baluns)
WELCOME.
Understanding Network Analysis
4th Week Seminar Sunryul Kim Antennas & RF Devices Lab.
ANTENNA’S MURRAY AMATEUR RADIO CLUB – KJ7HRI PRESENTS
Presentation transcript:

AE6PM 11/06/20071 Heard at Pacificon Technical tidbits from selected presentations

AE6PM 11/06/20072 Steve Stearns, K6OIK Pacificon 2001 Coaxial cable characteristic impedance Z o = 50Ω has no special significance For minimum lossZ o = 77Ω For maximum breakdown voltage Z o = 30Ω For minimum temperature rise Z o = 60Ω

AE6PM 11/06/20073 Steve Stearns, K6OIK Pacificon 2001 Round Open-Wire Transmission Line Impedance Formulas: Approximate, widely published, but accurate only for large spacings: s/d>3. Z 0 = 120 ln(2s/d) = 276 log 10 (2s/d) Exact, accurate for all spacings & impedances Z 0 = cosh -1 (s/d)

AE6PM 11/06/20074 Comment Yet another equation: Z 0 = 276 log 10 (s/d+ sqrt((s/d) 2 – 1) d = conductor diameter S = center-to-center spacing

AE6PM 11/06/20075 Steve Stearns, K6OIK Pacificon /2λ transmission line repeats the impedance of the load Z i = Z L 1/4λ transmission line repeats the reciprocal of the load Z Z i = Z o 2 /Z L

AE6PM 11/06/20076 Steve Stearns, K6OIK Pacificon /8λ transmission line always shows the impedance of the transmission line X L = Z o tan l for a short-circuited line less than 1/8λ in length ( l) 1/8λ = 45 o and tan 45 o = 1 The impedance at the antenna is almost never what is seen at the input end of the transmission line. - AE6PM -

AE6PM 11/06/20077 Steve Stearns, K6OIK Pacificon 2004/2005 For an exact half-wave dipole, l = λ/2: Z A = j41.52 Independent of wire diameter For a resonant dipole, l < λ/2: Z A = j0 Depends on wire diameter Resonance is just an impedance property Maximum gain for a dipole is 5.18 dbi at a length of 1.269λ

AE6PM 11/06/20078 Steve Stearns, K6OIK Pacificon 2006 QEX Sep/Oct 2001 is not the way to match. Forget conjugate match (which assures maximum power transfer). The important thing is to prevent reflections (which cause waveform distortion and degrade information transfer).

AE6PM 11/06/20079 Comment The QEX article in question is evidently: “A Flat Impedance Bandwidth for any Antenna” by Grant Bingeman, KM5KG

AE6PM 11/06/ Comment So which is the best? –Conjugate match (Maxwell) Maximum power transfer –Maximum SWR bandwidth (Bingeman) Maximum operating convenience –Minimum waveform distortion (Stearns) Maximum fidelity for digital modes

AE6PM 11/06/ Steve Stearns, K6OIK Pacificon 2006 A Dipole antenna differentiates the signal once A Loop antenna differentiates the signal twice Digital TV will require a discone antenna or a bow tie antenna or a ?

AE6PM 11/06/ Comment Conversation with Steve Stearn 10/19/07: –Yagi and log periodic antennas introduce phase distortion. –Bow tie and discone antennas do not introduce phase distortion. –Most digital modes are intolerant of signal distortion.

AE6PM 11/06/ Tom Schiller, N6BT Pacificon 2006 Round elements are more efficient than square or rectangular. Solid wire for radials is more efficient than stranded. Stainless steel is a very poor conductor (high resistivity). Galvanized wire is a very poor conductor (coating too thin: skin effect).

AE6PM 11/06/ Tom Schiller, N6BT Pacificon 2006 Maybe 12 dB improvement by silver plating stainless steel. Copper clad, not copper coated or copper plated (again, due to skin effect).

AE6PM 11/06/ Comment  =  (2  /  ) Where:  = skin depth  = resistivity of conductor  = angular frequency of current  = absolute magnetic permeability of conductor 1 MHz = 2.84 mils 10 MHz = mils 30 MHz = mils Zinc = ? Steel = ? Aluminum = ?

AE6PM 11/06/ Steve Stearns, K6OIK Pacificon 2007 RL db = -20 log |  | Errors correcting errors …. stuff happens: Return Loss in decibels is 20 times the logarithm of the Reflection Coefficient –WorldRadio, January 2007 p52 (wrong) Return Loss in decibels is 20 times the logarithm of the Voltage Reflection Coefficient –Correction in WorldRadio, March 2007 p52 (wrong) Return Loss is 20 times the reciprocal of the Reflection Coefficient –Correction in WorldRadio, June 2007 p52 (wrong)

AE6PM 11/06/ Comment Errors correcting errors …. The correct answer is: RL db = -20 log |  | Where  = reflection coefficient = E r /E f = I r /I f Ref: The ARRL Antenna Book, 21 st Edition, p24-8

AE6PM 11/06/ Articles by Steve Stearns “Mysteries of the Smith Chart: Transmission Lines, Impedance Matching, and Little Known Facts” “Antenna Impedance Models – Old and New” “New Results on Antenna Impedance Models and Matching”

AE6PM 11/06/ Articles by Jim Brown, K9YC “Understanding and Eliminating RF Interference” “Transmitting Chokes” “RFI, Ferrites, and Common Mode Chokes for Hams” “Measured Data For HF Ferrite Chokes” ….. and many more

AE6PM 11/06/ K6OIK’s Broadband Equivalent Circuit 98.4’ 5 MHz, thin wire dipole resonant at 4.8 MHz. See Pacificon presentation chart for component values.

AE6PM 11/06/ Accuracy of K6OIK’s Broadband Equivalent Circuit