HF Mobile Vertical Design By Larry Benson, N7GY Vertical Antenna Theory Base vs Center Loaded Efficiency/Installation Techniques Design Example. Program.

Slides:



Advertisements
Similar presentations
Let’s Design An Antenna VK3PY
Advertisements

ENE 428 Microwave Engineering
How they work How they are made
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
1 Chelmsford Amateur Radio Society Advanced Licence Course Carl Thomson G3PEM Slide Set 14: v1.1, 22-Aug-2006 (5) Antennas Chelmsford Amateur Radio Society.
HF Vertical Antenna Ground Systems Some Experiments
EMLAB 1 4. Linear wire antenna. EMLAB 2 Simulation of dipole antennas.
Part II: Loops and Verticals
THE OFF CENTER-LOADED DIPOLE A PHYSICALLY SHORT 160 METER ANTENNA by NNN0IAD Introduction Many operators have never given 160 meters a try simply because.
Different Types of Antennas
Chapter Fourteen: Transmission Lines
Transmission Lines Demonstration High Frequency Electronics Course EE527 Andrew Rusek Oakland University Winter 2007 Demonstration is based on the materials.
Part I: Dipoles by Marc C. Tarplee Ph.D. N4UFP
18 October 2003By NNN0JQH1 Wide Band Folded Dipoles A comparison between Wide Band Folded Dipole (WBFD) and an Open Wire Fed Dipole (OWFD)
Antenna Types WB5CXC.
Limited Space and Mobile Antennas
Antennas.
Chapter 6 Antennas Antenna Basics
Ground Screen Replace / Compliment a Radial System
Joe Horanzy AA3JH April 4th, 2013 K3DN Presentation
K9MBQ COAX VERTICAL FOR 160 AND 80 METERS
End Fed Antennas End Fed Long Wires
Antenna Types Dipole Folded Dipole Monopole
CHAPTER 8 ANTENNAS.
General Licensing Class
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.
Basic (VHF) Radio Communications
rectangular waveguides x z y 0 a b 0 TE or H mode.
SUBELEMENT T9 Antennas and feed lines [2 Exam Questions - 2 Groups] 1Antennas & Feedlines 2014.
Transmission Lines No. 1  Seattle Pacific University Transmission Lines Kevin Bolding Electrical Engineering Seattle Pacific University.
Basic Wire Antennas Part I: Dipoles. Dipole Fundamentals A dipole is antenna composed of a single radiating element split into two sections, not necessarily.
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
Part I: Dipoles by Marc C. Tarplee Ph.D. N4UFP
ENE 428 Microwave Engineering
1 Chelmsford Amateur Radio Society Intermediate Licence Course Carl Thomson G3PEM Slide Set 9 Antennas & Feeders Chelmsford Amateur Radio Society Intermediate.
1 “BUILDING QUICK TAPE ANTENNAS” Dr. Al Torres KP4AQI FEBRUARY 2015.
1 A TECHNICAL BRIEFING FOR AMATEUR RADIO OPERATORS “VOLTAGE STANDING WAVE RATIOS (VSWR): WHY IT DOES NOT MEAN AS MUCH AS YOU THINK” PRESENTED TO: ARASWF.
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.
Moxon Beams Design & Building by WB5CXC 2006 Ham - Com.
Antenna Basics.
Basic Wire Antennas Part I: Dipoles.
Part I: Dipoles by Marc C. Tarplee Ph.D. N4UFP
End Fed Antenna Secrets Select, Install & Operate
End Fed Antenna Secrets Select, Install & Operate
Chapter 7 Antennas Antennas Jim Siemons, AF6PU.
4. Linear wire antenna.
Transmission Lines As Impedance Transformers
Antennas 10/18/2017.
Technician Licensing Class
Vertical Antenna Myths
Antennas with Loads and Traps – What are these things and why are they used in our antennas? By: Dave Brown K3CTN.
“So . . how does this J-Pole thingamabob work?”
Amateur Extra Q & A Study Pool
Technician Licensing Class
20M Antenna.
Ham ANTENNAS: A practical introduction to The THEORY AND operation
End Fed Antenna Secrets Select, Install & Operate
VE3KL Selecting a Portable HF Antenna
ENE 429 Antenna and Transmission lines Theory
Part I: Dipoles by Marc C. Tarplee Ph.D. N4UFP
ENE 429 Antenna and Transmission lines Theory
CHAPTER 8 ANTENNAS.
What is a beam antenna? A. An antenna built from aluminum I-beams
Ferrite cores for transmitting chokes (baluns)
WELCOME.
Presentation transcript:

HF Mobile Vertical Design By Larry Benson, N7GY Vertical Antenna Theory Base vs Center Loaded Efficiency/Installation Techniques Design Example. Program Demo July, 2002

Obtained from Worldradio Books

HF Mobile Vertical Design by Larry Benson N7GY Vertical Theory Fundamental Freq. of a ¼ wave vert. is the lowest freq. for which the reactance (j) is zero at the feedpoint. This is the resonant freq. ¼ = 3 x 10 8 m x ¼ -- > Free Space Freq. Physical length = Free Space x K This makes the physical length shorter than free space. Approximately 5% shorter due to capacitive and inductive effects of the conductor, end effects and proximity. Electrical length for ¼ wave antenna is defined as 90 .

When resonant, /4 vert. is just a resistor (no reactance, i.e. no  j): R t What value? R t = R R (Radiation Resistance) + Losses Radiation resistance, R R,, is proportional to the length and inversely proportional to the diameter of the antenna element.

For 40 meters (7.2mhz), /4 = 33.3 feet! (399.68”) using ½ inch diam. conductor. Too long for vehicle! Let’s use 8 ½ft (102in) vertical. This is short on 40meters. This would look like this: R t -jXc We must tune it with an inductor because a short antenna is capacitive and a long antenna is inductive. NO perfect inductor. Can’t use superconductors yet! Wouldn’t want to anyway. Q too high. An inductor has losses: A. DC (small) B. AC (skin effects & proximity) Q is Freq. sensitive. Measured in Q = X L R AC

Grounded Verticals R G = 0 if perfect ground, but hard to come by. Would need solid copper surface wavelengths long. Typical is 120 radials minimum of 1/4 long. Soil conductivity & path is the problem.

Radiation resistance for a 1/4 vertical, ½ in diam. over perfect ground at 7.2 mhz is about 32 . How about on a vehicle? Example: A 102 in. whip on 7.2mhz (1/16 ), Rad. Resistance is about 4  ! R G =  for vehicle, but for a ground mounted vertical R G = . Tune by inductor, capacity hat & or make longer. 13 ½ feet is the limit.

Two cases explored: Base Loaded H = 102 in. (2.59m), F = 7.2mhz > = m Electrical height = (360  ) 2.59m =  m A =  = degree-amps 2 R R = (11.198) 2 = 1.52  for Base loaded.

Center Loaded H1 + H2 = H, I 1 = I 0 cos =.98 I 0 H1 = H2 = 51” (1.295m) G1 = G2 =  A = (1+.98) (.98) = degree-amps 2 2 R R = (16.56) 2 = 3.33  for center-loaded.

What does the coax on a vehicle see at the feedpoint for antenna impedance? Radiation Resistance? Will it see 3.3  ? 52  ? Remember the ground resistance? R G = 5  Where is this seen? Coax will see R R + R G Is this all? Not yet done. Remember the coil. Is it lossless? >> NO!

Calculate the Inductance for each case: Base Loaded -jX A = -j Z 0 where Z = 138log 2H Tan G V 2 H = ave. height above ground H = = 60A = ave. radius of element 2 G V = elec. Height of ant. A =.862 = Z 0 = 138log2(60) =  G V =  + 5% for end effects = 23.5  -jX A –j = -j , (X L = 2  FL) L = = uh Tan23.5  2  (7.2 x 10 6 ) Calculate the losses for coil. Not easy! If Q = X L and I measure coil Q = 250, R T Then R C = = 3.09  250

Center Loaded X L0 = jZ 0 (cotan G 1 – tan G 2 ), G 1 = G 2 = 23.5  =  2 jX L0 = j (cotan11.75  - tan11.75  ) = , L = 34.21uh Calculate the coil losses: If Q is 250, then R C =  = 6.19  250

So the antenna impedance is R T = R R + R G + R C Base Loaded antenna impedance is 1.5  + 5   = 9.59 , SWR = 52 = Center Loaded ant. impedance is 3.33  + 5   = 14.52, SWR = 52 = Don’t jump to conclusions regarding the SWR just yet. We will discuss this later.

Which is more efficient? BASE Loaded: 1.52 x 100 = 15.8% Center Loaded: 3.33 x 100 = 22.9% We have some control over the coil Q and a little control over the ground losses, but not much over the Rad. Resistance unless we add length or change antenna design.

Minimizing Losses R G is a function of: 1. Car A. Size and shape B. Height off ground 2. Soil losses at frequency 3. Position of antenna on vehicle if using same exact antenna. 4. Grounding methods in car My truck R G is around 5 , but varies over the ground it rides on. Salt flats = 4  To minimize ground losses: 1. Large gage ground strap to back of rig! 2. Additional ground straps A. Underneath vehicle, body to frame. B. Matching point, short leads 3. Conductive compound at screws & regular cleaning.

R C Losses Better Coil Methods 1. Larger diameter coil 2. Use optimum gage of wire 3. Optimum wire turns spacing/coil shape/size 4. Minimal coil form material, low dielectric constant

Capacity Hat 1. Circular is best for pattern, but straight wire works well too. 2. Placement on element (not too close to coil, at least a diam.) Can be used to tune the antenna to other bands like 18mhz from 21mhz or 24mhz from 28mhz.

Placement of antenna on Vehicle: 1.Bumper > Least desirable 2.Fender > better location 3.Top > Best location for signal strength but hard to do. Ground losses are effected. Example: Bumper = 6  ground loss Fender or hood = 4  Top = 2.5 

ANTENNA PLACEMENT at 7.2mhz Ant. A (104”) IN = 39uH Ht = 46” Rg = 5 ohms Rr = 4 ohms Eff. = 25.6% Ant. A (102”) IN = 39uH Ht = 18” Rg = 7 ohms Rr = 3.9 ohms Eff. = 22.3% Ant. B (132”) IN = 34uH Ht = 18” Rg = 7 ohms Rr = 6.7 ohms Eff. = 35.3%

Corona Need round smooth conductive bead or ball at high voltage end of antenna. Cause is ionization of the air at high voltage point of antenna. This lengthens the antenna and de-tunes it. Also causes static noise in receiver.

Diameter of radiating element Larger diameter of radiating element will give lower DC losses and gives the added benefit of more bandwidth and longer effective length.

This broadband “UnUn” will match your antenna’s low impedance (16  ). The author recommends to put a small cap across to help with the match above 8mhz. Use a variable to find value.

Example of Antenna design

HF Mobil Vertical Program Demo 1.Quarter wave for frequency section 2.Auto Optimize placement 3.Changes to efficiency (Placement of coil, diam., Q) 4.Radiation Resistance vs Antenna Impedance 5.SWR – Low SWR when losses are high 6.Less Bandwidth (with high Q coils) 7.Coil Section Demo a. Optimum Wire Gage b. Shape factor c. Length of coil vs form length 8. Coil Q design helps 9.Interactive screens between Antenna & Coil Sections 10. Printing