General/Chapter 8 Study Guide
From charlesreid1
Contents
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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General Class Ham License Notes from studying for my General Class ham license.
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 |