Propagation of radio waves is something that has intrigued me from the very first time I made a radio contact. In the past 25 years that I studied propagation, I gathered a lot of knowledge. I believe that I should share my knowledge so I wrote this article hoping that it can explain how radio wave propagation works.
1. Radio waves:
Radio waves are electromagnetic waves that propagate with a speed near 300,000 km/s. Electromagnetic waves have a frequency and wavelength. There are different type of waves, with high and low frequency. Even visible light is an electromagnetic wave, that has a very short wavelength. Your own eye is in fact an antenna, and you probably did not know!
You can calculate frequency or wavelength with these two formulas:
Frequency (MHz) = 300 / Wavelength (m).
For example a wavelength of 10m has the following frequency: 300 / 10 = 30 MHz.
Wavelength (m) = 300 / Frequency (MHz).
For example a frequency 28.495 MHz has the following wavelength: 300 / 28.495 = 10.528 m.
In the world of communication, different wavelengths or frequencies are divided into:
- LF (Low Frequency) = 0.03 – 0.3 MHz (1000 m to 10000 m band)
- MF (Middle Frequency) = 0,3 – 3 MHz (100 m to 1000 m band)
- HF (High Frequency) = 3 – 30 MHZ (10 m to 100 m band)
- VHF (Very High Frequency) = 30 – 300 MHz (1 m to 10 m band)
- UHF (Ultra High Frequency) = 300 – 3000 MHz (1 m to 10 cm band)
- SHF (Super High Frequency) = 3000 – 30000 MHz (10 cm to 1 cm band)
- EHF (Extremely High Frequency = 30000 – 300000 MHz (1 cm to 1 mm band)
By the way:
- 1000 Hz = 1 kHz
- 1000 kHz = 1 MHz
- 1000 MHz = 1 GHz
There are also differences in properties for these wavelengths. LF waves easily penetrate through dense materials like concrete, rock, soil, etc. They follow the curve of the Earth, which makes LF ideal for long distance ground wave communication over more than 1000 km. Submarines even use VLF (Very Low Frequency) radio waves, because they can even travel right through the Earth’s core!
The higher the frequency becomes, the less they bend along the Earth’s curve, and the less they can penetrate dense materials. 10 m band waves follow the Earth’s curve only little.
2. Earth’s atmosphere
Before we explain the physics of propagation, it is good to that the Earth’s atmosphere has a great influence on propagation:
The lowest part of the atmosphere is the troposphere. This part of the atmosphere holds for our weather. The troposphere ends at roughly 14 km under a small layer, the tropopause. Only the tops of large thunderstorm or supercell clouds (Cumulonimbus Incus) occasionally reach over 14 km, and some even push up the tropopause. The troposphere does not have great influence on HF propagation, but can sometimes extend normal ‘ground wave’ propagation, especially on the short HF wavelengths like 10 m and 12 m.
This part of the atmosphere does not influence HF propagation. The upper part of the stratosphere holds the ozone layer, which filters harmful ultraviolet (UV) radiation. The only clouds you find here are so called Noctilucent Iceclouds which are sometimes visible after midsummer sunsets.
The mesosphere harbours the so called D-layer. The most lower part of the ionosphere. The D-layer absorbs HF radiowaves, especially up to 10 MHz.
The ionosphere is very important for propagation of HF radiowaves. It harbours the so called E-layer, F1-layer and F2-layer. These layers emerge under influence of solar radiation.
3. Three types of propagation
We divide propagation in roughly three types:
3a. Ground waves
Ground waves are waves that propagate along the Earth’s surface. Your favourite station on FM for example uses ground waves. How far ground waves can travel depends on the height of the antenna. That is why commercial broadcast stations on FM use large towers or are located on the highest mountains. 10 m band radiowaves usually travel around 30-50 km on ground wave, with the antenna at an average height of 10 m. The less obstacles the radio wave encounters, the stronger the signal will be. Ground waves over large surfaces of water travel much further than ground waves in mountainous or rural areas. Once the ground wave cannot follow the Earth’s curve anymore, it travels into the sky and into space!
3b. Tropospheric skywaves
Sometimes ground waves travel further than theoretically possible. Distances up to 100 km and even more are possible on 10 m. This type of propagation is called Troposheric or ‘Tropo’. In the troposhere, there are different layers of air, with different temperatures and different humidities. When it’s windy, these layers of air mix together. But when it is not windy, different layers of air are present at different altitudes. When you are in the center of a high pressure area, weather is very quiet. In the morning, the air layer close to the ground is relatively cool and moist (sometimes it produces fog or mist!), while the area above it is relatively warm and dry. The change of temperature can be easily 10°C over 100 m, and is called an inversion. Now the cold layer of air is more dense than the warm layer of air. The sharp transition between cold and warm air, a temperature inversion, refracts radiowaves in VHF and UHF bands.
On some occasions there can be multiple inversions. Once a radio signal has been caught between two inversions, it can travel in between like travelling through a kind tunnel. This propagation mode is called tropospheric ducting. Ducting has only been reported on VHF and UHF.
Tropo is also observed along cold fronts, where there is a very sharp transition between cold dry and warm moist air. But even in violent atmospheres like hurricanes and typhoons.
Such inversions affects VHF and UHF bands most, but the higher HF bands like 10 m are also affected, however much less. On 10 m band contacts have been made over 350 km on a day with paths across stationary high pressure areas, and no reports of any ionospheric propagation at all on the same day.
3c. Ionospheric sky waves
Radio waves can travel far distances because they can be reflected to the Earth’s ionosphere. They call such a reflection a ‘hop’. The radio wave that is being reflected by the ionosphere can travel back to Earth. It bounces of the Earth’ s surface back up again into the ionosphere. There it will be reflected down and again. Multiple bounces and reflections are called ‘multi hop’ propagation.
4. The Ionosphere
The ionosphere is a thin layer of air. It is called ionosphere because it is formed by ions. Ions are charged particles that appear under the influence of solar radiation (ultraviolet and X-rays). These ions have the capability to bend or reflect a radiowave. That capability depends on the density of ions, the more ions the stronger the reflection. The maximum frequency that the ionosphere can reflect is called the MUF or Maximum Usable Frequency.
We read earlier that the ionosphere consists out of 4 layers:
- D-layer: only absorbs radiowaves, especially under 4-5 MHz. Appears very fast after sunrise, and disappears almost immediately during sunset.
- E-Layer: reflects radiowaves up to 5 MHz, radiowaves above 5 MHz are absorbed, but less than in the D-layer. Appears shortly after sunrise, and disappears shortly after sunset.
- F1-layer: reflects radiowaves up to 10 MHz. Appears shortly after sunrise and after sunset it merges with the F2-layer to become the F-layer.
- F2-layer: reflects radiowaves up to 50 MHz (occasionally MUF’s of 70 MHz have been reported). Appears after sunrise and disappears shortly and after sunset it merges with the F2-layer to become the F-layer. Is stronger in the winter than in the summer, due to seasonal effects.
As you can see the F2-layer is the most important one for us, it reflects our HF radiowaves along great distances, and at nighttime the F-layer does the same.
5. Solar Activity
You now know that the ionosphere appears under the influence of solar radiation, mainly Ultraviolet (UV) and X-ray. This solar radiation varies under the influence of:
5a. Sunspots and Solar Flux
sunspots are dark spots on the sun’s surface, and can be compared with the crater of an active volcano. They produce the intense radiation which causes ionization of the ionosphere. The index for this radiation is called the Solar Flux and is measured at 2800 MHz. The higher this Solar Flux, the higher the level of ionization. The lowest possible Solar Flux is 64 (no sunspot regions), and the highest numbers go well into 200. Conditions on 10 m band generally start to become interesting on all latitudes, when the solar flux index passes the 100 number.
Sunspots are classified by their magnetic complexity. The more complex the magnetic configuration, the more active they are producing lots of radiation and all kind of other events like solar flares and CME’s. Magnetic configuration is classified as:
Up to date Solar Flux can be found on the Spaceweather Canada website.
In the picture below you can see many sunspots, and just above the middle, the largest sunspot ever recorded in modern history. These sunspots are clustered together in so called sunspot regions. The active regions are assigned a number when they appear on the sun’s surface.
5b. Solar Wind
The solar wind is a constant stream of charged particles which flows form the sun into our solar system. Solar wind can reach speeds up to 1000 km per second.
5c. EGF (Earth’s Geomagnetic Field)
Our planet has a core that consists mainly of iron. The funny thing about iron is when you rotate its, it produces a magnetic field like in the picture below. This magnetic field protects the Earth from the charged particles from the solar wind. When solar wind speed is very low, the EGF is quiet, but when the solar wind’s speed is very high, the EGF becomes unsettled to active, and in some occasions we even talk about a solar wind storm. The EGF is very important for the production of a stable ionosphere. A quiet EGF means a stable ionosphere, with relative high MUF’s. An active or stormy EGF means unstable propagation with a relative low MUF.
The EGF is strongest around the equator and weakest on the north pole and south pole, as you can see in the picture below.
5d. Solar Flares
When groups of sunspots are active, they are likely to produces solar flares. These solar flares are like vulcanic eruptions with large flames shooting millions of kilometres into space, like in the pictures below. These solar flares produce a lot of radiation, like X-ray which causes the D-layer to grow stronger. Usually after a large solar flare, propagation blacks out, because of very high absorption of the D-layer. Solar Flares also cause and ejection of large masses of charged particles, which is called a Coronal Mass Ejection (CME). The strength of a solar flare is measured from C-class followed by a number, up to M-class and X-class. M-class and X-class flares are likely to produce a radio blackout. A-level means very low levels of X-ray radiation.
Now the chance for a solar flare, depends on the magnetic configuration of the sunspot group:
|Beta||Up to low M-class|
|Gamma||Up to low X-class|
|Delta||Up to extreme large X-class|
The magnetic configuration is very important. For example, a sunspot group or region with a 5 spot count in Delta-class can produce much more and bigger solar flares, than a 30 spot count group in Beta-class!
Solar Flares can even be heard on your own radio, especially the larger X-class flares, but also C-class flares that spit out lots of radiation. You can hear the level of background static rise for a short period, as the radiation reaches Earth.
5e. Coronal Holes
that is a a hole through the sun’s outer shell (the corona). Coronal holes are always there, and they always produces a stream of charged particles. When a coronal hole faces Earth, it’s stream is likely to hit the EGF within 1-5 days, and push solar wind speeds up to 600-700 km/s, bringing the K-index to active or storm levels. The black area in the picture below is a very large coronal hole.
5f. CME (Coronal Mass Ejection):
With every solar flare the sun spits out a vast cloud of charged particles. This coronal mass ejections can speed up the solar wind up to 1000 km/s. Coronal mass ejections are immense clouds of charged particles, which travel very fast. They usually follow a solar flare within 72 hours after the eruption (like lava which flows form a volcanic eruption). Very fast moving CME’s travel to Earth within 24 hours. A CME is likely to hit Earth when the sunspot region which produced the CME, is directed to Earth. When a full halo CME is reported, it is directed to Earth. A partial halo means it is directed partial to Earth.
Watch closely around 2003/10/28 when a series large full halo CME’s knocks out the SOHO satellites instruments. On 2003/11/04 (19:54 hours) you can see the largest CME ever seen, being ejected from the right side of the sun, a partial halo. A full halo would have sparked Aurora even at tropical latitudes.
5g. The 27-day cycle
While Earth needs 1 day to rotate around its axis, the Sun needs 27 days. That means that active sunspots that appear on certain days, are likely to return there 27 days later. It can be that the sunspots developed into more active regions in those 27 days, but it could also be that they decayed fully. But 27 days is a cycle that counts.
5h. The sunspot cycle
Solar activity is not on the same level constantly. It follows an average 11 year cycle, called the sunspot cycle or solar cycle. On the peak of this cycle, the number of sunspots can reach well over 100, with solar flux numbers reaching over 200. In between those peaks, solar activity can be very low, with not a single sunspot for months and Solar Fluxes under 70.
In April 2000 Solar Cycle 23 peaked with a smoothed sunspot number of 120. Cycle 24 started late 2007 and peaked at the end of 2013. It was much less intense than Cycle 23 and 22.
5i. The Earth’s seasons
As normal weather changes by the season propagation also does. Like with normal weather, temperatures at the equator remain at the same level during the year, but temperature differences between summer and winter increase as you go northwards or southwards. Same happens with propagation, but the other way around! The MUF of the F2 layer is higher in wintertime than in summertime. One cause is that more intense and longer sunshine in the summer gives the D-layer more strength to absorb HF waves. Due to other complex atmospheric influences, ions in the F2 layer tend do “dissolve” more quickly in the summer then in the winter. That allows winter MUF to reach higher levels than summer MUF.
6. Solar activity and the effects on HF propagation:
We have seen in Chapter 5 that X-ray and UV radiation make the ionosphere, and that charged particles influence the EGF. These factors strongly affect the ionization process and so propagation.
6a. Solar flares
Solar flares produce large amounts of X-ray radiation, causing radio blackouts, but can also intensify ionization in the F2-layer for a short period, with unstable and fast and deep QSB (fading).
6b. Coronal holes
Coronal holes produce streams of energized particles which “presses” the EGF down. The EGF is weakest around the poles, so stormy conditions are most noticeable around the polar areas. Large streams can enter Earth’s atmosphere on the poles, and collision with gases like oxygen, nitrogen, etc., produces the Northern Lights or Aurora.
Same as Coronal Holes only with a more intense effect. CME’s have caused satellites, power grids and communications on Earth to go dead because of the intense bombardments with charged particles. Back in the 90’s a giant CME caused a part of the North American power grid to go down. During such a CME the currents that flow through the atmosphere at high and polar latitudes exceed 1,000,000 (one million) Ampere!
7. Extraordinary propagation
Next to the ‘standard’ type propagation, there are also some very special types of propagation. Some predictable and some unpredictable. But some can be very spectacular.
7a. Sporadic-E (Es)
Every year around mid summer (May-August) and mid winter (December-January) short skip propagation turns up with distances form 500-1800 km. Remarkable about this propagation is that it can turn up in only 15 minutes, and disappear just as fast. Also signal levels can be very high. On the CB band (27 MHz or 11 m) for example, you can hear small stations from other areas between 500-1800 km with only 4 watts in FM with impressive signals. QSO’s with toy handhelds on the CB band have been made over more than 1000 km.
The layer in the ionosphere responsible for this is called the Es-layer (Es = sporadic-E). This layer floats at the same altitude as the normal E-layer, somewhere between 80-150 km. Scientists still do not know what makes the Es-layer appear and disappear, but it is surely not influenced by solar radiation.
We do know that Es is at it’s best during a sunspot minimum, because it turns op more regular with a quiet EGF. Studies on this type of propagation learned us, that Es shows up mostly in the late morning and early evening, but can show up at any time, even at night! The MUF of the Es-layer can reach upto the VHF band, with recorded QSO’s signals at 200 MHz! Amateurs in the 6 m (50 MHz) 4 m (70 MHz) and 2m (144 MHz) band use Es to cover distances well over 2000 km. In multihop occasions, even double that! I remember a summer holiday in Portugal, when we received Dutch FM stations in the 88-108 MHz VHF broadcast band!
Normally you would expect HF radio signals to be reflected forwards in the ionosphere, but there is a propagation mode where signals are being reflected back from the surface after a first hop. The modulation of the station you are hearing via backscatter, has a specific ‘sound’. It sounds hollow like talking through a tube and sometimes even a short echo can be heard. Backscatter signals are not very strong, usually not more than an S1 to S5. About 100 Watts and a directional antenna is needed to produce a readable backscatter signal. Backscatter is best on the higher HF bands like 15 m to 10 m, but can also be observed on 6 m (50 MHz).
It mostly occurs when the MUF of the ionospherer is well above 28 MHz, and the reflection from the ionosphere is strong. Working via back scatter allows you to work stations within the so called blind zone (the area which is too far away for ground waves and to nearby for ionospheric waves, usually between ± 50-500 km). To work backscatter, both stations need to point there antenna to more or less the same point about 1000-4000 km away. If for example a station from Belgium wants to work a station from England, they could point there antenna’s both in the direction of the Azores, or any other direction that produces the loudest signals.
Backscatter is a typical F2-layer propagation mode but is also observed with Es-layer propagation.
When a CME or Coronal Hole stream hits Earth’s atmosphere it cannot penetrate at equatorial regions, lower and middle latitudes. The Earth’s magnetic fieldlines are strong there. They push the energized particles towards the polar regions where the magnetic field is weaker. When they enter the polar atmosphere, they collide with the different gases there. You will see it as Northern Lights or Aurora, like neon gas in a tube is lighted up by bombarding the neon gas with charged particles. Now these Aurora ‘clouds’ are ionized extremely intense. They can reflect radiowaves up to the UHF band. These Aurora clouds do not float horizontally like the normal D-, E-, and F-layers do. Instead they are hanging more like curtains (like in the picture below). This allows you to work just like backscatter.
Because Aurora only appears around the polar regions, you need to direct your antenna to the North Pole or South Pole (whatever is nearest). The distance you can work via aurora ranges up to 2000 km. Working Aurora on HF means having needs a good set of ears. The very fast and strong QSB make the signal almost unreadable! Like someone is talking with a soar throat, or talking behind a blowing fan. Aurora works best on the higher HF bands.
You do need to be on the higher latitudes to work Aurora propagation. The higher latitude you are, the more often you can work Aurora. Aurora appears when the K-index hits 3-4 of you live near the magnetic North Pole or South Pole. But for locations like London in the UK and Berlin in Germany, the K-index needs to be 8 or for aurora to be visible. But when you see it, the sky seems like it is on fire!
7d. Meteor scatter
Meteor scatter is a remarkable propagation mode is meteor scatter. Meteors are tiny rocks, or dust particles that enter Earth’s atmosphere at a high altitude (±100 km) at very high speeds (> 5000 m/s). Because of these very high speeds, these meteors burn up because due to friction in Earth’s atmosphere. When disintegrating, the heat is so intense that ionization of the surrounding air takes place. Now this ionization can be so dense, that the ionized air can reflect radiowaves up to 500 MHz, but also the higher HF bands like 28 10 m and 12 m. The distances for meteor scatter can range from 400 – 1800 km for 10 m and 12 m, and the openings can last from a second up to a few minutes, with very strong QSB.
Meteor scatter takes place in annual periods of meteor showers. All have their own name. Here are some important dates for meteorshowers which appear annually:
Meteorshowers tend to peak in the late winter evening into the night and early summer evening into the early morning.
7e. TEP (trans Equatorial Propagation)
The Earth’s magnetic poles are not at the same location as the exact North Pole and South Pole, but are located about 1000 km from the real poles. Therefore the magnetic equator does not run straight like the normal equator.
On each side of the magnetic equator the intense sunshine and the Earth magnetic fieldlines cause extreme ionization there. As a result the F2-layer extends upwards in the atmosphere up to 500 km and higher. Because of this very high altitude and the high level of ionization, a TEP signal is reflected twice against the ionosphere and can take a signal with a single hop over 6000 km, into the VHF range, and in a single occasion even up to 500 MHz! You can see how the TEP mode can exist in the picture below.
TEP usually peaks between late afternoon and late evening. Signals tend to become stronger during the evening, but with more and sometimes extreme QSB.
7f. FAI (Field Aligned Irregularities)
Field Aligned Irregularities is the most unpredictable propagation mode. It appears at the same altitude as the E-layer, when ions are being driven together by the EGF, into a small cloud of ions (from several meters in length and width, up to several kilometers). At a certain point the density is high enough, to produce a MUF that reaches over 200 MHz. It can appear at every time of the day. Its appears as very short openings, with mostly strong signals. Usually the signals have strong QSB. FAI openings can last seconds up to minutes.
There is much more to explain about propagation, but I like to keep things not too technical. If you want to know more, Google is your best friend.
73 de PA9X Jean-Paul