General/Chapter 7 Study Guide
From charlesreid1
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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Chapter 2: Procedures and Practices: General/Chapter 2 Study Guide Chapter 3: Rules and Regulations: General/Chapter 3 Study Guide Chapter 4: Components and Circuits: General/Chapter 4 Study Guide Chapter 5: Radio Signals and Equipment: General/Chapter 5 Study Guide Chapter 6: Digital Modes: General/Chapter 6 Study Guide Chapter 7: Antennas: General/Chapter 7 Study Guide Chapter 8: Propagation: General/Chapter 8 Study Guide Chapter 9: Electrical and RF Safety: General/Chapter 9 Study Guide Flags · Template:GeneralFlag · e |