From charlesreid1

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* For a dipole antenna in free space, the radiation pattern is a figure-eight at right angles to the antenna
* For a dipole antenna in free space, the radiation pattern is a figure-eight at right angles to the antenna
* Antenna height affects horizontal (azimuthal) radiation pattern of a dipole by making antenna omnidirectional if low (less than 1/2 wavelength high)
* Antenna height affects horizontal (azimuthal) radiation pattern of a dipole by making antenna omnidirectional if low (less than 1/2 wavelength high)
* Radial wires of ground-mounted vertical should be placed on the Earth or buried a few inches below the ground
* As a 1/2 wavelength dipole antenna is lowered to less than 1/4 wavelength above ground, the feed-point impedance steadily decreases
* As a 1/2 wavelength dipole has its feed point moved from the center to the end, the feed-point impedance steadily increases (to several thousand Ohms)
* Horizontally polarized HF antenna has lower ground-reflection losses than a vertically polarized HF antena (advantage of horizontal polarization)
* The paproximate length for a 1/2 wavelength dipole antenna cut for 14.250 MHz is given by 492/f = 492/14.250 = 34.5 ft or approximately 32 feet
* The approximate length for a 1/2 wavelength dipole antenna cut for 3.550 MHz is 492/f = 492/3.550 = 131 feet
* The approximate length for a 1/4 wavelength vertical antenna cut for 28.5 MHz is 246/f = 246/28.5 = 8.6 feet or 8 feet
* Antenna gains in dBi compare to antenna gains in dBd as follows:
** dBi gain is 2.15 dB higher than dBd gain
** dBi = gain relative to isotropic antenna
** dBd = gain relative to dipole antenna


==Section 7.3: Yagi Antennas==
* Yagi antennas are cheap, effective
* Directional antennas have frontal lobes and side lobes
* Pointing antenna in direction shown by azimuthal map enables you to beam signal directly to other station
* HF signals can skew signal path by up to 15 degrees
* Minimize noise/interference by listening for best direction and using S-meter
* On crowded bands like 20 m, having directional antenna can reduce unwanted noise
* Dipole, ground plane, and rnaomd wire antenas use a single radiating element
* Yagis use more than one radiating elemetn - array antenna
* Main lobe/major lobe - direction of maximum field strength
* Two types of arrays: driven, and parasitic
** Driven array: all elements are connected to transmitter, and all are driven elements
** parasitic array: one or more elements are not connected to feed line, but influence radiation pattern of antenna
* Array pattern of radiation depends on constructive and destructive interference
* If 2 interfering waves are in phase, they reinforce each other
* If 2 interfering waves are out of phase, they cancel each other out
* For pair of dipoles, radiated fields add/subtract to create the radiated field/lobes/nulls
* In a parasitic array, antenna elements close together enough that energy from the driven element induces current in parasitic element
* Parasitic element will re-radiate power as if it were fed too
Yagi structure and function:
* Yagi is parasitic array with 1 driven element and 1 or more parasitic element
* Parasitic elements are arranged to create main lobe
* '''directors''' - elements placed in direction of maximum gain
* '''reflectors''' - elements placed in direction of minimum gain
* '''front-to-back ratio''' - ratio of signal strength at peak of major lobe to signal strenght in opposite direction
* Yagi driven element should be resonant dipole at approximately 1/2 wavelength long
* Reflector shoudl be 5% longer than driven element, placed 0.15 - 0.2 wavelengths behind driven element
* Signal from DE causes current to flow into RE
* Signal in RE is 180 degrees out of phase, so cancels signal in direction of reflected element
* Added length of RE is due to fact that there is incomplete cancellation
* Larger element creates additional phase shift due to inductive impedance
* Director element placed in front of DE increases forward gain
* Shorter element results in capacitive reactance, which subtracts some phase shift
Performance
* 2-Element Yagi (neglecting height above ground):
** Compared to isotropic antenna, gain of 7 dBi
* Compared to dipole, gain of 5 dBd
** Front to back ratio - 10-15 dB
* Three element Yagi:
** 9.7 dBi
** front to back ratio of 30-35 dB
* Additional reflectors make little difference, usually just 1
* Additional reflectors increases antenna gain
Yagi design tradeoffs
* Many things to optimize for: maximum gain, front to back ratio, SWR variation across bands, etc.
* Variables for Yagi design:
** Length and diameter of each element
** Placement of elements along boom
* Affect of elements:
** More directors increase gain
** Longer boom, for a given number of directors, increase gain, up to a certain maximum (then decreases again)
** Large diameter elements reduce SWR variation with frequency
** Placement of elements of tuning of elements affects gain and feed point impedance and SWR
Impedance matching:
* Yagis with desirable radiation patterns have impedances that don't match 50 Ohm coax
* Typical impedance is 20-25 Ohms, creating SR of 2:1
* To match impedances, can use gamma match
* ''Gamma match'' - short section of parallel conductor transmission line, uses driven element as one conductor
* Adjustable capacitor used to gamma match SWR to 1:1
* Gamma match advantage: driven element need not be insulated from boom
* Other techniques: beta match (hairpin), omega match, impedance transformers, transmission line stubs
* VHF/UHF Yagis, can make element diameters larger
===Section 7.3 Summary===
* An azimuthal projection map shows true bearings and distances from a particular location
* An HF antenna that minimizes interference is a directional antenna
* To increase the bandwidth of a Yagi, use larger diameter elements
* The approximate length of a Yagi driven element is 1/2 wavelength
* For a three-element, single-band Yagi, the director is the shortest element
* For a three-element, single-band Yagi, the reflector is the longest element
* On a Yagi, increasing boom length and adding directors increases gain
* On a Yagi, front-to-back ratio means the power radiated in maximum gain direction to power radiated in opposite direction
* ON a directive antenna, the main lobe is the direction of maximum radiated field strenght from antenna
* Gain of 2 three-element Yagis, horizontally polarized, spaced vertically 1/2 wwavelength apart, ocmpared with gain of 1 three-element Yagi, will be 3 dB higher
* A Yagi design variable to optimize forward gain, front to back ratio, or SWR bandwidth includes:
** Physical boom length
** Number of elements on boom
** Spacing of each element along boom
* The purpose of a Yagi gamma match is to match the LOW feed point impedance to 50Ohms
* Using a gamma match for impedance matching of Yagi to 50 Ohm feed line has advantage of not requiring elements to be insulated from boom
==Section 7.4: Loop Antennas==
Loop antennas enclose an area 1 wavelength or more in circumference
* Loops can be any shape, but can't be too narrow
** Quad lop: 4 sides, each 1/4 wavelength long
** Delta loop or triangular loop: 3 sides, each 1/3 wavelength long
* Direction of maximum signal is broadside to the loop
** Horizontally oriented loop good for vertical waves, local/regional contacts
** Vertically oriented loop good for singnals pointing to horizon: DX, etc.
* One wavelength loop acts like 2 dipoles end-to-end
* Feed point is point of maximum current, other point of max current is 1/2 wavelength from feedpoint
* Shorter/longer loops (non-integer multiples of wavelength) have higher feed point impedance
* Can use loops in arrays: Yagi concept, but with quad loops for elements, is quad antenna
* Driven element of quad antenna is 1 wavelength is circumference, so 1/4 wavelength on each side
* Quad/delta loop has reflectors 5% longer in circumference, directors that are 5% shorter in circumference
* Two-element quad/delta has same gain as three-element Yagi
* Yagi has better front-to-back ratio than quad/delta loop
* Quads have more restrictions/complexities on constructions
* Polarization of a horizontally oriented loop is always horizontal, regardless of feed point
* Polarization of vertical loop depends on feed point location
* Feed point at midpoint of bottom or top leads to horizontal polarization
* Feed point at vertical side results in vertical polarization
* Rotation/orientation (square or diamond) doesn't matter
===Section 7.4: Summary===
* The loops of a two-element quad antenna must be configured so the reflector element is 5% longer than the beam element, to use it as beam antenna
* Each side of a driven element of a quad antenna is 1/4 wavelength
* Forward gain of a 2-element quad antenna is about the same as a 3-element Yagi
* Each side of a reflector element of a quad antenna is more than 1/4 wavelength
* Gain of a two-elemetn delta loop is about the same as gain of two-element quad loop
* Each leg of a symmetrical delta loop antenna is approx. 1/3 wavelength


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Revision as of 06:43, 27 June 2016

Chapter 7: Antennas

Section 7.1: Antenna Basics

Review of terminology:

  • Elements - conducting portions of an antenna that radiate or receive signals
  • Polarization - orientation of electric field radiated by antenna
  • Feedpoint impedance - ratio of RF voltage to current at antenna feedpoint
  • Resonance - when feed point impedance is purely resistive, with no reactance
  • Radiation pattern - graph of signal strength in every direction
  • Azimuthal pattern - shows signal strength in horizontal directions (birds eye view)
  • Elevation pattern - shows signal strength in vertical directions (side view)
  • Lobes - regions in radiation pattern where signal is being radiated
  • Nulls - points at which radiation pattern is at a minimum
  • Isotropic antenna - radiates equally in every possible direction 9horizontal or vertical)
  • Omnidirectional antenna - radiates a signal of equal strength in every horizontal direction
  • Directional antenna - radiates preferentially in one or more directions
  • Gain - concentrating transmitted or received signals in a specific direction
  • dB - decibels, units of gain
    • dBi = gain with respect to isotropic antenna
    • dBd = gain with respect to dipole antenna

Section 7.2: Dipoles, Ground Waves, Random Wires

Dipoles

  • Dipole = 2 electrical polarities
  • Dipoles have a figure-8 radiation pattern, signal is strongest broadside to antenna
  • Actual ground installation changes radiation pattern
  • Half wave dipole - 1/2 wavelength total, feedpoint in center, each half of the dipole is 1/4 wavelength
  • Voltage: lowest at feedpoint, highest at ends
  • Current: highest at feedpoint, lowest at ends
  • Length of a dipole in feet: 492/f
  • Feedpoint impedance of center-fed, free-radiating dipole should be 72 Ohms
  • Becomes several THOUSAND Ohms when feedpoint is connected at the ends
  • Physical thickness of wire can electrically lengthen wire, meaning you need a shorter antenna
  • Height above ground affects resonant frequency
  • Insulation, nearby conductors, and method of insulation all affect resonant frequency and length of dipole
  • Start near free-space length, and use SWR/antenna tuner to trim dipole
  • Exam asks to approximate resonant length for dipole. Use 492/f - pick the closest value to that

Ground plane vertical antena:

  • Dipoleantenna, with missing half: ground plane acts as electric mirror
  • Ground plane consists of sheet of metal or ground radial wires
  • Often installed vertically, making them omnidirectional (good for VHF/UHF)
  • Base impedance is 35 Ohms (half of dipole)
  • Sloping ground radials down will increase impedance
  • Downward angle of 30-45 degrees will match 50 Ohm impedance of coax cable
  • Impedance increases as feed point moved further from the "center"
  • Start with half of the free-space 1/2 wavelength length: length in feet is 246/f
  • Example calculation: approximate length of 1/4 wave ground vertical antenna that is resonant at 28.5 MHz is:
    • Free space length = fsl = 246/f = 246/28.5 = 8.6 ft

Mobile HF antennas;

  • Mobile HF antennas are ground-plane antennas
  • Vertically oriented whip antennas - thin steel rod mounted atop vehicle surface
  • Full-size 1/4 wavelength whip not feasible below 10 m
  • Loading techniques used to physically shorten/electrically lengthen an antenna
  • Loaded antennas have reasonable impedanc, but inefficient
  • Screwdriver antenna: whip with adjustable loading coil at base

Random wires:

  • Feed point impedance and radiation patterns are totally unpredictable
  • May have lobes at multiple angles and multiple locations
  • Connected to transmitter output or to antenna tuner without feedline
  • Antenna, radio, station equipment are all part of the antenna system
  • May result in significant RF currents/voltages on station equipment
  • Can result in RF burns
  • If impedance can be matched, can give excellent results

Effect of height:

  • Feed point impedance and radiation pattern affected by antenna's physical height above ground
  • Presence of electrical image created in conducting ground below antenna affects performance
  • Image is electrically reversed
  • As antenna and image get closer, they start to short each other out
  • Close to ground level, feed point impedance is near zero
  • Above half wavelength, impedance varies. Goes through maxima and minima
  • Maxima at 1/4 wavelength, then 1 wavelength
  • Ground also affects radiation patterns: real radiation patterns composed of energy received by antenna, and energy reflected from ground
  • Direct and reflected signals take different times to travel, and may combine, cancel out, or anywhere in between
  • This leads to new lobes/nulls pattern
  • Depending on height, you can have most radiation going UP, or most radiation going out via side lobes

Polarization:

  • Polarization can affect amount of signal lost due to ground resistance
  • Radio waves reflected from ground: lower losses when polarization is parallel to ground
  • Radiation pattern consists of reflected waves combined with direct waves not reflected
  • Lower reflection loss means higher maximum signal strength
  • HF DX done with vertical antennas - lower losses at low angles (but at higher angles, still more effective than horizontally polarized)
  • Ground-mounted vertical: not polarized efficiently, but still generates stronger signals at lower angles of radiation from horizontally polarized antennas at lower heights
  • DX or HF bands use verticals, because horizontally polarized antennas require unreasonable hieghts

Section 7.2 Summary

  • A capacitance hat on a mobile antenna is used to electrically lengthen/physically shorten an antenna
  • A corona ball on an HF mobile antenna reduces high voltage discharge from the tip of the antenna
  • A disadvantage of a shortened mobile antenna is a smaller bandwidth
  • A disadvantage of a directly-fed random-wire antenna is that you may experience RF burns if you touch it
  • To adjust the feedpoint impedance of a quarter wave ground plane vertical antenna, slope the radials downward
  • If a ground plane antenna's radials are changed from horizontal to downward, the feed point impedance increases (maximum angle makes them into a dipole, which has double the feed point impedance of a ground wave vertical antenna)
  • For a dipole antenna in free space, the radiation pattern is a figure-eight at right angles to the antenna
  • Antenna height affects horizontal (azimuthal) radiation pattern of a dipole by making antenna omnidirectional if low (less than 1/2 wavelength high)
  • Radial wires of ground-mounted vertical should be placed on the Earth or buried a few inches below the ground
  • As a 1/2 wavelength dipole antenna is lowered to less than 1/4 wavelength above ground, the feed-point impedance steadily decreases
  • As a 1/2 wavelength dipole has its feed point moved from the center to the end, the feed-point impedance steadily increases (to several thousand Ohms)
  • Horizontally polarized HF antenna has lower ground-reflection losses than a vertically polarized HF antena (advantage of horizontal polarization)
  • The paproximate length for a 1/2 wavelength dipole antenna cut for 14.250 MHz is given by 492/f = 492/14.250 = 34.5 ft or approximately 32 feet
  • The approximate length for a 1/2 wavelength dipole antenna cut for 3.550 MHz is 492/f = 492/3.550 = 131 feet
  • The approximate length for a 1/4 wavelength vertical antenna cut for 28.5 MHz is 246/f = 246/28.5 = 8.6 feet or 8 feet
  • Antenna gains in dBi compare to antenna gains in dBd as follows:
    • dBi gain is 2.15 dB higher than dBd gain
    • dBi = gain relative to isotropic antenna
    • dBd = gain relative to dipole antenna

Section 7.3: Yagi Antennas

  • Yagi antennas are cheap, effective
  • Directional antennas have frontal lobes and side lobes
  • Pointing antenna in direction shown by azimuthal map enables you to beam signal directly to other station
  • HF signals can skew signal path by up to 15 degrees
  • Minimize noise/interference by listening for best direction and using S-meter
  • On crowded bands like 20 m, having directional antenna can reduce unwanted noise
  • Dipole, ground plane, and rnaomd wire antenas use a single radiating element
  • Yagis use more than one radiating elemetn - array antenna
  • Main lobe/major lobe - direction of maximum field strength
  • Two types of arrays: driven, and parasitic
    • Driven array: all elements are connected to transmitter, and all are driven elements
    • parasitic array: one or more elements are not connected to feed line, but influence radiation pattern of antenna
  • Array pattern of radiation depends on constructive and destructive interference
  • If 2 interfering waves are in phase, they reinforce each other
  • If 2 interfering waves are out of phase, they cancel each other out
  • For pair of dipoles, radiated fields add/subtract to create the radiated field/lobes/nulls
  • In a parasitic array, antenna elements close together enough that energy from the driven element induces current in parasitic element
  • Parasitic element will re-radiate power as if it were fed too

Yagi structure and function:

  • Yagi is parasitic array with 1 driven element and 1 or more parasitic element
  • Parasitic elements are arranged to create main lobe
  • directors - elements placed in direction of maximum gain
  • reflectors - elements placed in direction of minimum gain
  • front-to-back ratio - ratio of signal strength at peak of major lobe to signal strenght in opposite direction
  • Yagi driven element should be resonant dipole at approximately 1/2 wavelength long
  • Reflector shoudl be 5% longer than driven element, placed 0.15 - 0.2 wavelengths behind driven element
  • Signal from DE causes current to flow into RE
  • Signal in RE is 180 degrees out of phase, so cancels signal in direction of reflected element
  • Added length of RE is due to fact that there is incomplete cancellation
  • Larger element creates additional phase shift due to inductive impedance
  • Director element placed in front of DE increases forward gain
  • Shorter element results in capacitive reactance, which subtracts some phase shift

Performance

  • 2-Element Yagi (neglecting height above ground):
    • Compared to isotropic antenna, gain of 7 dBi
  • Compared to dipole, gain of 5 dBd
    • Front to back ratio - 10-15 dB
  • Three element Yagi:
    • 9.7 dBi
    • front to back ratio of 30-35 dB
  • Additional reflectors make little difference, usually just 1
  • Additional reflectors increases antenna gain

Yagi design tradeoffs

  • Many things to optimize for: maximum gain, front to back ratio, SWR variation across bands, etc.
  • Variables for Yagi design:
    • Length and diameter of each element
    • Placement of elements along boom
  • Affect of elements:
    • More directors increase gain
    • Longer boom, for a given number of directors, increase gain, up to a certain maximum (then decreases again)
    • Large diameter elements reduce SWR variation with frequency
    • Placement of elements of tuning of elements affects gain and feed point impedance and SWR

Impedance matching:

  • Yagis with desirable radiation patterns have impedances that don't match 50 Ohm coax
  • Typical impedance is 20-25 Ohms, creating SR of 2:1
  • To match impedances, can use gamma match
  • Gamma match - short section of parallel conductor transmission line, uses driven element as one conductor
  • Adjustable capacitor used to gamma match SWR to 1:1
  • Gamma match advantage: driven element need not be insulated from boom
  • Other techniques: beta match (hairpin), omega match, impedance transformers, transmission line stubs
  • VHF/UHF Yagis, can make element diameters larger

Section 7.3 Summary

  • An azimuthal projection map shows true bearings and distances from a particular location
  • An HF antenna that minimizes interference is a directional antenna
  • To increase the bandwidth of a Yagi, use larger diameter elements
* The approximate length of a Yagi driven element is 1/2 wavelength
  • For a three-element, single-band Yagi, the director is the shortest element
  • For a three-element, single-band Yagi, the reflector is the longest element
  • On a Yagi, increasing boom length and adding directors increases gain
  • On a Yagi, front-to-back ratio means the power radiated in maximum gain direction to power radiated in opposite direction
  • ON a directive antenna, the main lobe is the direction of maximum radiated field strenght from antenna
  • Gain of 2 three-element Yagis, horizontally polarized, spaced vertically 1/2 wwavelength apart, ocmpared with gain of 1 three-element Yagi, will be 3 dB higher
  • A Yagi design variable to optimize forward gain, front to back ratio, or SWR bandwidth includes:
    • Physical boom length
    • Number of elements on boom
    • Spacing of each element along boom
  • The purpose of a Yagi gamma match is to match the LOW feed point impedance to 50Ohms
  • Using a gamma match for impedance matching of Yagi to 50 Ohm feed line has advantage of not requiring elements to be insulated from boom

Section 7.4: Loop Antennas

Loop antennas enclose an area 1 wavelength or more in circumference

  • Loops can be any shape, but can't be too narrow
    • Quad lop: 4 sides, each 1/4 wavelength long
    • Delta loop or triangular loop: 3 sides, each 1/3 wavelength long
  • Direction of maximum signal is broadside to the loop
    • Horizontally oriented loop good for vertical waves, local/regional contacts
    • Vertically oriented loop good for singnals pointing to horizon: DX, etc.
  • One wavelength loop acts like 2 dipoles end-to-end
  • Feed point is point of maximum current, other point of max current is 1/2 wavelength from feedpoint
  • Shorter/longer loops (non-integer multiples of wavelength) have higher feed point impedance
  • Can use loops in arrays: Yagi concept, but with quad loops for elements, is quad antenna
  • Driven element of quad antenna is 1 wavelength is circumference, so 1/4 wavelength on each side
  • Quad/delta loop has reflectors 5% longer in circumference, directors that are 5% shorter in circumference
  • Two-element quad/delta has same gain as three-element Yagi
  • Yagi has better front-to-back ratio than quad/delta loop
  • Quads have more restrictions/complexities on constructions
  • Polarization of a horizontally oriented loop is always horizontal, regardless of feed point
  • Polarization of vertical loop depends on feed point location
  • Feed point at midpoint of bottom or top leads to horizontal polarization
  • Feed point at vertical side results in vertical polarization
  • Rotation/orientation (square or diamond) doesn't matter

Section 7.4: Summary

  • The loops of a two-element quad antenna must be configured so the reflector element is 5% longer than the beam element, to use it as beam antenna
  • Each side of a driven element of a quad antenna is 1/4 wavelength
  • Forward gain of a 2-element quad antenna is about the same as a 3-element Yagi
  • Each side of a reflector element of a quad antenna is more than 1/4 wavelength
  • Gain of a two-elemetn delta loop is about the same as gain of two-element quad loop
  • Each leg of a symmetrical delta loop antenna is approx. 1/3 wavelength

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