General/Chapter 8 Study Guide: Difference between revisions
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** F2 is highest layer, reaches highest point at noon | ** F2 is highest layer, reaches highest point at noon | ||
Reflection and absorption | |||
* Weak conduction of layers allows bending/refracting of waves | |||
* Layers of ionosphere can bend waves | |||
* Bending o waves depends on ionization level, and wave frequency | |||
* VHF/UHF waves hardly bent at all | |||
* HF waves bent, can be reflected back to Earth | |||
* Weaker bending requires lower takeoff angles, otherwise waves lost to space | |||
* '''Critical angle''' - angle above which all energy lost to space | |||
* '''Critical frequency''' - frequency above which all energy lost to space (if pointed straight up) | |||
* '''Ionosonde''' - device used for measuring reflection of radio waves by ionosphere | |||
* Absorption is the enemy of propagation | |||
* In D and E layers, waves pass through denser gas regions, absorbed as they are refracted | |||
* For HF bands, below 10 MHz, AM broadcast bands, the D layer completely absorbs radio waves | |||
* Absorption increases with sunlight, ionization, more UV, and lower frequencies | |||
Sky-wave and ground-wave propagation | |||
* Reflection by ionosphere is called '''hop''' | |||
* Signals received via waves bouncing off of ionosphere called '''sky-wave propagation''' | |||
* Propagation via ionosphere called '''skip''' | |||
** Skip via higher ionosphere layers travel further | |||
** F2 layer skip travels up to 2,500 miles | |||
** E layer skip travels up to 1,200 miles | |||
** Sky wave propagation can also skip over Earth's surface | |||
* Ocean's surface reflects radio waves (salt water) | |||
* Skip can also travel shorter distance as angle increased | |||
* Short skip can indicate there is larger skip available at lower frequencies | |||
** Short skip on 10 m indicates long skip on 6 m | |||
* Ionosphere has many variations in density, turbulent, rough | |||
* Variations can cause signals to take multiple paths | |||
* Multipath signals have echo/flutter | |||
* Ground wave signals attenuated more (ground not good conductor) | |||
* Higher frequency ground waves attenuated more | |||
* Ring-shaped region around station forms skip zone (further than maximum ground wave and shorter than minimum sky wave) | |||
* Stations in skip zone can't be contacted | |||
Long path/short path | |||
* Short path: shorter of great circle paths between two stations | |||
* Long path: travels long way around globe | |||
* If signal travels by both paths, short delay/echo | |||
* Round the world propagation: 1/7 second delay with own signal | |||
===Section 8.1 Summary=== | ===Section 8.1 Summary=== | ||
* When making a long path contact, antenna is pointed 180 degrees from short path heading | |||
* If sky wave signal arriving via short '''and''' long path, a well-defined echo will be heard | |||
* A good indicator of possible sky-wave propagation ('''long skip propagation''') on 6 m is, '''short skip skywave propagation''' on the 10 m band | |||
* Radio waves with frequencies below MUF and above LUF sent into ionosphere will be bent back to Earth | |||
* Approximate maximum distance covered by F2 layer skips is 2,500 miles | |||
* Approximate maximum distance covered by E layer skips is 1,200 miles | |||
* Ionospheric layer closest to surface of Earth is D layer | |||
* Earth's ionospheric layers reach maximum height where the sun is directly overhead | |||
* F2 region responsible for longest radio wave propagation because it is the highest ionospheric region | |||
* Critical angle in radio wave propagation refers to highest takeoff angle that will return the wave3 to Earth | |||
* Long distance communication on 40 m, 60 m, 80 m, 160 m, more difficult during day because the D layer absorbs these frequencies during the day | |||
* Ionospheric layer that absorbs most long skip signals during daylight, below 10 MHz, is D layer | |||
==Section 8.2: The Sun== | |||
Sunspots and cycles: | |||
* Sn generates UV rays, but a lot of variation over time | |||
* Variations caused by sunspots (cooler regions on Sun surface) | |||
* Sunspot number - number of sunspots present on solar disk | |||
* Sunspots vary over an 11 year period (sunspot cycle) | |||
* More sunspots lead to more UV radiation lead to more intense ionization | |||
* More ionization improves propagation on HF above 10 MHz, and into low VHF | |||
* Peak sunspot: bands like 10 m stay open into the evening, enabling long-distance contacts | |||
* High ionization increases absorption, takes a toll on 80 m and 160 m | |||
* Bottom on sunspot cycle: low HF bands have good propagation and higher bands (20 MHz) stay open | |||
* 20 m (14 MHz) supports daytime communication during the day | |||
* Sun rotates every 28 days, so spots change nad move | |||
* Propagation conditions can repeat themselves every 28 days | |||
* Strong daily/seasonal variations in HF propagation | |||
* Seasonal variation: summer, higher illumination, higher absorption, shifts HF activity to nighttime | |||
* Propagation around equinoxes (March/September) can be interesting | |||
Band: 160 m / 80 m / 60 m | |||
* Daytime: local and regional contacts, 100-200 miles | |||
* Nighttime: local to long distance, best near sunset/sunrise | |||
Band: 40 m / 30 m | |||
* Daytime: local and regional contacts, 300-400 miles | |||
* Nighttime: short and medium range to worldwide communications | |||
Band: 20 m / 17 m | |||
* Daytime: regional to long distance, open at sunrise, closing at nighttime | |||
* Nighttime: Open to west at night, may be open 24 hours | |||
Band: 15 m / 12 m / 10 m | |||
* Daytime: primarily long distance, 1,000+ miles | |||
* Nighttime: 10 m used for local communications 24 hours a day | |||
Measuring solar activity: | |||
* Solar activity critical to propagation and communication | |||
* Monitored 24/7 throughout world | |||
* Use of data, experience, and software allows for predicting propagation and being alerted to sudden propagation changes | |||
* '''SFI''' - solar flux index - amount of 2800 MHz radio energy coming from sun | |||
* Easier to measure than solar UV, and correlates with it | |||
* Higher levels of SFI indicate higher solar activity and better HF propagation above 10 MHz | |||
* '''K index''' - values from 0 to 9, represent short-term stability of Earth's magnetic field, updated every 3 hours at NIST in Boulder CO | |||
* Steady K values indicate a short term stable geomagnetic field; higher K values indicate short-term disturbances in geomagnetic field, disrupting HF communication | |||
* '''A index''' - time-averaged K values; A index ranges from 0 to 400, 0 = stable, 400 = greatly disturbed | |||
* Index values and other space weather data from NIST: spaceweather.com, WWV, WWVH | |||
Assessing propagation | |||
* Software tools for predicting propagation | |||
* MUF/LUF = maximum/lowest usable frequency | |||
* MUF/LUF depend on path between 2 points, time of day, time of year, conditions, etc. | |||
* MUF = highest frequency at which propagation exists between 2 points | |||
* Waves at or below the MUF reflected back to eart | |||
* Waves above MUF will, at some point during the journey, penetrate ionosphere and leave Earht | |||
* LUF = lowest frequency at which propagation between 2 points exist | |||
* Waves below LUF completely absorbed by ionosphere | |||
* If MUF < LUF, no propagation path exists via skywave | |||
* Check band conditions using beacons - Northern California DX Foundation | |||
* Many beacons between 28.190 and 28.225 MHz | |||
* Reverse Beacon Network - automated receivers reporting SS for signals on HF bands | |||
Solar disturbances | |||
* Common events on Sun that affect hF propagation | |||
* Measured by solar observatories | |||
* '''Solar flare''' - large eruption of energy/solar material, magnetic field disruptions occurring on surface of Sun | |||
* '''Coronal hole''' - weak area in Sun's corona (outer layer), plasma (ionized gases/particles) escape and stream into space at high velocities | |||
* '''Coronal mass ejection''' - ejection of large amount of material from corona | |||
Sudden ionospheric disturbances | |||
* UV, x-ray radiation from solar flare travels at speed of light | |||
* 8 minutes from Sun to Earth | |||
* Radiation hits ionosphere, raises ionization of D layer and other layers | |||
* Dramatic increase in absorption, radio blackout | |||
* '''Sudden ionospheric disturbance''' - radio blackout due to solar flare | |||
* Blackouts last seconds to hours | |||
* Lower bands affected more strongly | |||
* Only day side of Earth affected | |||
Geomagnetic disturbances | |||
* Solar wind - stream of charged particles | |||
* Interaction between solar wind and Earth's magnetic field creates '''magnetosphere''' | |||
* Charged particles from coronal holes/coronal mass ejections can take 20-40 hours to reach earth | |||
* Charged particles can affect/become trapped in Earth's magnetosphere, create disturbances | |||
* Charged particles depositing in magnetosphere increase ionization of E layer | |||
* Geomagnetic storm, auroral displays | |||
* Changes in geomagnetic field disrupt upper ionosphere layers, some HF paths passing near poles are completely wiped out | |||
* Auroras are glow of bases ionized by incoming charged particles | |||
* Conductive sheets that glow also reflect radio waves above 20 MHz | |||
* Auroral propagation strongest on 6 and 2 m, modulates signas with hiss or buzz | |||
===Section 8.2 Summary=== | |||
* Significance of sunspot number with with respect to HF propagation is, '''higher''' sunspot number indicates '''better''' propagation at '''higher''' frequencies | |||
* Sudden ionospheric disturbance in daytime affects ionospheric propagation of HF waves by disrupting signals on '''lower''' frequencies '''more than''' signals on '''higher''' frequencies | |||
* Increased UV/x-ray from solar flares take '''8 minutes''' to reach earth | |||
* For long distance communication during periods of low solar activity, the '''least reliable''' bands are 15 m, 12 m, 10 m | |||
* Solar flux index is measure of solar radiation at 10.7 cm wavelength (2.4 GHz) | |||
* Geomagnetic storms are temporary disturbances in Earth's magnetosphere | |||
* For 20 m band, worldwide propagation supported at any point in solar cycle | |||
* A geomagnetic storm can degrade '''high-latitude''' HF propagation (near the poles) | |||
* A high sunspot number enhances long-distance communication on the upper HF and lower VHF bands | |||
* HF propagation conditions vary on a 28-day cycle due to the sun's rotation on its axis | |||
* The typical sunspot cycle is 11 years | |||
* The K-index indicates the '''short-term''' stability of the Earth's geomagnetic field | |||
* The A-index indicates the '''long-term''' stability of the Earth's magnetic field | |||
* Charged particles escaping from coronal holes affect radio communications by causing an HF blackout (HF communications are disturbed) (due to higher absorption) | |||
* Charged particles from coronal mass ejections affecting radio propagation take 20-40 hours to reach Earth | |||
* Periods of high geomagnetic activity benefit radio propagation by creating conductive sheets that reflect VHF signals | |||
* When selecting a frequency for lowest attenuation on HF, select a frequency just below the MUF (best frequency for low attenuation) | |||
* To determine if MUF is high enough to support skip propagation between two distant stations for 14-30 MHz, use '''beacons''' (NC DX F beacon network) | |||
* Radio waves with frequencies below the MUF and above the LUF, when sent into the ionosphere, are bent back to the Earth's surface | |||
* Radio waves with frequencies below the LUF are completely absorbed | |||
* LUF = lowest usable frequency for communicating between 2 points | |||
* MUF = maximum usable frequency for communicating between 2 points | |||
* When LUF exceeds MUF, there is no HF radio frequency that supports sky wave communications over the path | |||
* Factors that affect the MUF include all of the following: | |||
** Path distance and location | |||
** Time of day and season | |||
** Solar radiation and ionospheric disturbances | |||
==Section 8.3: Scatter Modes== | |||
* HF signals via scatter are weaker than HF signals via sky-wave propagation (reflection is not efficient) | |||
* Scatter may make a signal arrive from multiple paths, causing fluttering sound or wavering sound | |||
* Waves close to MUF can be reflected by mountains and ocean, and can return back to transmitter (backscatter) | |||
* Waves can also be scattered within ionosphere inside skip zone (if too distant for ground wave and too high a frequency for short hop skywave) | |||
* scatter or backscatter can fill in this skip zone | |||
NVIS | |||
* below critical frequency, ionosphere reflects waves arriving at any angle (including vertical) | |||
* critical frequency is always above 5 MHz, often above 7 MHz (40 m) | |||
* For HF signals below that critical frequency, reflected signals are scattered over a wide area | |||
* This scatter mode is called NIVS, near vertical incidence skywave | |||
* Critical frequency increases with solar illumination | |||
* Antenna should be 1/8 to 1/4 wavelength high | |||
* Skip will be good over 200-300 miles | |||
===Section 8.3 Summary=== | |||
* A characteristic of HF scatter signals is a wavering sound | |||
* HF scatter signals sound distorted because they are arriving via multiple paths | |||
* HF signals arriving via scatter in skip zone are weak because only a small part of the signal energy is scattered into the skip zone | |||
* Radio wave propagation that works for stations too close for ground wave propagation and too far for sky wave propagation is '''scatter propagation''' | |||
* On HF bands, indication of signal received via scatter propagation is a signal being heard above a max. usable frequency | |||
* Antenna type most effective for skip communication on 40 m during day is horizontal dipole 1/8 to 1/4 wavelength above ground | |||
* NVIS propagation is short distance HF propagation using high elevation angles | |||
=Flags= | =Flags= | ||
{{GeneralFlag}} | {{GeneralFlag}} | ||
Latest revision as of 17:33, 15 July 2016
Section 8.1: Ionosphere
- Atmosphere gets thinner as you go further away
- At 30 miles in altitude, gets thin enough that UV rays can knock electrons away from molecules
- Gas is ionized by loss of electron, positively charged ion, negative free electron
- Ion + electron respond to voltage, like electrons in conductor
- Atmospheric layer - ionosphere - becomes weak conductor
- Ionosphere extends to 300 miles above surface of Earth
Regions:
- ISS orbits 200 miles above Earht
- Ionosphere arranged into multiple layers (D, E, F layers)
- D layer - 30-60 miles, only present when illuminated by sun
- E layer - 60-70 miles, similar to D region, lasts longer after sunset
- F layer - 100-300 miles, least dens,e partially ionized at night
- F1 layer/F2 layer - split during day, recombine at night
- Height of regions vary with season, TOD, latitude, solar activity
- F2 is highest layer, reaches highest point at noon
Reflection and absorption
- Weak conduction of layers allows bending/refracting of waves
- Layers of ionosphere can bend waves
- Bending o waves depends on ionization level, and wave frequency
- VHF/UHF waves hardly bent at all
- HF waves bent, can be reflected back to Earth
- Weaker bending requires lower takeoff angles, otherwise waves lost to space
- Critical angle - angle above which all energy lost to space
- Critical frequency - frequency above which all energy lost to space (if pointed straight up)
- Ionosonde - device used for measuring reflection of radio waves by ionosphere
- Absorption is the enemy of propagation
- In D and E layers, waves pass through denser gas regions, absorbed as they are refracted
- For HF bands, below 10 MHz, AM broadcast bands, the D layer completely absorbs radio waves
- Absorption increases with sunlight, ionization, more UV, and lower frequencies
Sky-wave and ground-wave propagation
- Reflection by ionosphere is called hop
- Signals received via waves bouncing off of ionosphere called sky-wave propagation
- Propagation via ionosphere called skip
- Skip via higher ionosphere layers travel further
- F2 layer skip travels up to 2,500 miles
- E layer skip travels up to 1,200 miles
- Sky wave propagation can also skip over Earth's surface
- Ocean's surface reflects radio waves (salt water)
- Skip can also travel shorter distance as angle increased
- Short skip can indicate there is larger skip available at lower frequencies
- Short skip on 10 m indicates long skip on 6 m
- Ionosphere has many variations in density, turbulent, rough
- Variations can cause signals to take multiple paths
- Multipath signals have echo/flutter
- Ground wave signals attenuated more (ground not good conductor)
- Higher frequency ground waves attenuated more
- Ring-shaped region around station forms skip zone (further than maximum ground wave and shorter than minimum sky wave)
- Stations in skip zone can't be contacted
Long path/short path
- Short path: shorter of great circle paths between two stations
- Long path: travels long way around globe
- If signal travels by both paths, short delay/echo
- Round the world propagation: 1/7 second delay with own signal
Section 8.1 Summary
- When making a long path contact, antenna is pointed 180 degrees from short path heading
- If sky wave signal arriving via short and long path, a well-defined echo will be heard
- A good indicator of possible sky-wave propagation (long skip propagation) on 6 m is, short skip skywave propagation on the 10 m band
- Radio waves with frequencies below MUF and above LUF sent into ionosphere will be bent back to Earth
- Approximate maximum distance covered by F2 layer skips is 2,500 miles
- Approximate maximum distance covered by E layer skips is 1,200 miles
- Ionospheric layer closest to surface of Earth is D layer
- Earth's ionospheric layers reach maximum height where the sun is directly overhead
- F2 region responsible for longest radio wave propagation because it is the highest ionospheric region
- Critical angle in radio wave propagation refers to highest takeoff angle that will return the wave3 to Earth
- Long distance communication on 40 m, 60 m, 80 m, 160 m, more difficult during day because the D layer absorbs these frequencies during the day
- Ionospheric layer that absorbs most long skip signals during daylight, below 10 MHz, is D layer
Section 8.2: The Sun
Sunspots and cycles:
- Sn generates UV rays, but a lot of variation over time
- Variations caused by sunspots (cooler regions on Sun surface)
- Sunspot number - number of sunspots present on solar disk
- Sunspots vary over an 11 year period (sunspot cycle)
- More sunspots lead to more UV radiation lead to more intense ionization
- More ionization improves propagation on HF above 10 MHz, and into low VHF
- Peak sunspot: bands like 10 m stay open into the evening, enabling long-distance contacts
- High ionization increases absorption, takes a toll on 80 m and 160 m
- Bottom on sunspot cycle: low HF bands have good propagation and higher bands (20 MHz) stay open
- 20 m (14 MHz) supports daytime communication during the day
- Sun rotates every 28 days, so spots change nad move
- Propagation conditions can repeat themselves every 28 days
- Strong daily/seasonal variations in HF propagation
- Seasonal variation: summer, higher illumination, higher absorption, shifts HF activity to nighttime
- Propagation around equinoxes (March/September) can be interesting
Band: 160 m / 80 m / 60 m
- Daytime: local and regional contacts, 100-200 miles
- Nighttime: local to long distance, best near sunset/sunrise
Band: 40 m / 30 m
- Daytime: local and regional contacts, 300-400 miles
- Nighttime: short and medium range to worldwide communications
Band: 20 m / 17 m
- Daytime: regional to long distance, open at sunrise, closing at nighttime
- Nighttime: Open to west at night, may be open 24 hours
Band: 15 m / 12 m / 10 m
- Daytime: primarily long distance, 1,000+ miles
- Nighttime: 10 m used for local communications 24 hours a day
Measuring solar activity:
- Solar activity critical to propagation and communication
- Monitored 24/7 throughout world
- Use of data, experience, and software allows for predicting propagation and being alerted to sudden propagation changes
- SFI - solar flux index - amount of 2800 MHz radio energy coming from sun
- Easier to measure than solar UV, and correlates with it
- Higher levels of SFI indicate higher solar activity and better HF propagation above 10 MHz
- K index - values from 0 to 9, represent short-term stability of Earth's magnetic field, updated every 3 hours at NIST in Boulder CO
- Steady K values indicate a short term stable geomagnetic field; higher K values indicate short-term disturbances in geomagnetic field, disrupting HF communication
- A index - time-averaged K values; A index ranges from 0 to 400, 0 = stable, 400 = greatly disturbed
- Index values and other space weather data from NIST: spaceweather.com, WWV, WWVH
Assessing propagation
- Software tools for predicting propagation
- MUF/LUF = maximum/lowest usable frequency
- MUF/LUF depend on path between 2 points, time of day, time of year, conditions, etc.
- MUF = highest frequency at which propagation exists between 2 points
- Waves at or below the MUF reflected back to eart
- Waves above MUF will, at some point during the journey, penetrate ionosphere and leave Earht
- LUF = lowest frequency at which propagation between 2 points exist
- Waves below LUF completely absorbed by ionosphere
- If MUF < LUF, no propagation path exists via skywave
- Check band conditions using beacons - Northern California DX Foundation
- Many beacons between 28.190 and 28.225 MHz
- Reverse Beacon Network - automated receivers reporting SS for signals on HF bands
Solar disturbances
- Common events on Sun that affect hF propagation
- Measured by solar observatories
- Solar flare - large eruption of energy/solar material, magnetic field disruptions occurring on surface of Sun
- Coronal hole - weak area in Sun's corona (outer layer), plasma (ionized gases/particles) escape and stream into space at high velocities
- Coronal mass ejection - ejection of large amount of material from corona
Sudden ionospheric disturbances
- UV, x-ray radiation from solar flare travels at speed of light
- 8 minutes from Sun to Earth
- Radiation hits ionosphere, raises ionization of D layer and other layers
- Dramatic increase in absorption, radio blackout
- Sudden ionospheric disturbance - radio blackout due to solar flare
- Blackouts last seconds to hours
- Lower bands affected more strongly
- Only day side of Earth affected
Geomagnetic disturbances
- Solar wind - stream of charged particles
- Interaction between solar wind and Earth's magnetic field creates magnetosphere
- Charged particles from coronal holes/coronal mass ejections can take 20-40 hours to reach earth
- Charged particles can affect/become trapped in Earth's magnetosphere, create disturbances
- Charged particles depositing in magnetosphere increase ionization of E layer
- Geomagnetic storm, auroral displays
- Changes in geomagnetic field disrupt upper ionosphere layers, some HF paths passing near poles are completely wiped out
- Auroras are glow of bases ionized by incoming charged particles
- Conductive sheets that glow also reflect radio waves above 20 MHz
- Auroral propagation strongest on 6 and 2 m, modulates signas with hiss or buzz
Section 8.2 Summary
- Significance of sunspot number with with respect to HF propagation is, higher sunspot number indicates better propagation at higher frequencies
- Sudden ionospheric disturbance in daytime affects ionospheric propagation of HF waves by disrupting signals on lower frequencies more than signals on higher frequencies
- Increased UV/x-ray from solar flares take 8 minutes to reach earth
- For long distance communication during periods of low solar activity, the least reliable bands are 15 m, 12 m, 10 m
- Solar flux index is measure of solar radiation at 10.7 cm wavelength (2.4 GHz)
- Geomagnetic storms are temporary disturbances in Earth's magnetosphere
- For 20 m band, worldwide propagation supported at any point in solar cycle
- A geomagnetic storm can degrade high-latitude HF propagation (near the poles)
- A high sunspot number enhances long-distance communication on the upper HF and lower VHF bands
- HF propagation conditions vary on a 28-day cycle due to the sun's rotation on its axis
- The typical sunspot cycle is 11 years
- The K-index indicates the short-term stability of the Earth's geomagnetic field
- The A-index indicates the long-term stability of the Earth's magnetic field
- Charged particles escaping from coronal holes affect radio communications by causing an HF blackout (HF communications are disturbed) (due to higher absorption)
- Charged particles from coronal mass ejections affecting radio propagation take 20-40 hours to reach Earth
- Periods of high geomagnetic activity benefit radio propagation by creating conductive sheets that reflect VHF signals
- When selecting a frequency for lowest attenuation on HF, select a frequency just below the MUF (best frequency for low attenuation)
- To determine if MUF is high enough to support skip propagation between two distant stations for 14-30 MHz, use beacons (NC DX F beacon network)
- Radio waves with frequencies below the MUF and above the LUF, when sent into the ionosphere, are bent back to the Earth's surface
- Radio waves with frequencies below the LUF are completely absorbed
- LUF = lowest usable frequency for communicating between 2 points
- MUF = maximum usable frequency for communicating between 2 points
- When LUF exceeds MUF, there is no HF radio frequency that supports sky wave communications over the path
- Factors that affect the MUF include all of the following:
- Path distance and location
- Time of day and season
- Solar radiation and ionospheric disturbances
Section 8.3: Scatter Modes
- HF signals via scatter are weaker than HF signals via sky-wave propagation (reflection is not efficient)
- Scatter may make a signal arrive from multiple paths, causing fluttering sound or wavering sound
- Waves close to MUF can be reflected by mountains and ocean, and can return back to transmitter (backscatter)
- Waves can also be scattered within ionosphere inside skip zone (if too distant for ground wave and too high a frequency for short hop skywave)
- scatter or backscatter can fill in this skip zone
NVIS
- below critical frequency, ionosphere reflects waves arriving at any angle (including vertical)
- critical frequency is always above 5 MHz, often above 7 MHz (40 m)
- For HF signals below that critical frequency, reflected signals are scattered over a wide area
- This scatter mode is called NIVS, near vertical incidence skywave
- Critical frequency increases with solar illumination
- Antenna should be 1/8 to 1/4 wavelength high
- Skip will be good over 200-300 miles
Section 8.3 Summary
- A characteristic of HF scatter signals is a wavering sound
- HF scatter signals sound distorted because they are arriving via multiple paths
- HF signals arriving via scatter in skip zone are weak because only a small part of the signal energy is scattered into the skip zone
- Radio wave propagation that works for stations too close for ground wave propagation and too far for sky wave propagation is scatter propagation
- On HF bands, indication of signal received via scatter propagation is a signal being heard above a max. usable frequency
- Antenna type most effective for skip communication on 40 m during day is horizontal dipole 1/8 to 1/4 wavelength above ground
- NVIS propagation is short distance HF propagation using high elevation angles
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