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TECHNICAL INFORMATION
INDEX
IPS also has an excellent page of facts and educational material which can found at http://www.ips.gov.au/Main.php?CatID=8 Frequency ranges & their use
Wave propagation
Ground conductivitySince the surface wave front is in contact with the ground, it will lose some energy into the ground. The amount of energy lost depends on the conductivity of the earth at any given point. If the ground is a good conductor, part of the energy will be returned to the other wave fronts. If it is a bad conductor, much of the energy will be lost into the ground. Below is a list comparing the different type of terrain.
* city areas and jungle are particularly bad for surface propagation due to the absorption of the radio waves by buildings and foliage The ionosphereThe ionosphere is the region of upper atmosphere (approx. 50 - 500km
above the earth's surface) where the air is ionised by solar radiation
(mainly ultraviolet). The composition of the ionosphere changes with height,
and each of the atmospheric gases is ionised by a different part of the
solar spectrum. This creates 'layers' of ionisation at different heights.
There are usually three identifiable layers, those being E layer in the
E region, and the F1 and F2 layers in the F region. When the sun sets,
the ions and electrons in the lower layers recombine, but the F region
collisions are less frequent and some ionisation remains all night.
Tilting effectSince some of the surface wave energy is lost into the ground, the wave is retarded at points to the ground, causing the whole wave front to tilt forward. This retarding effect becomes less noticeable with increasing height above ground. Poor conducting surfaces cause high loss, greater tilt, and total absorption of energy. The angle of tilt also varies with frequency - as frequency increases, the angle of the tilt increases. The table below shows angles of tilt over good (sea water) and poor (dry ground) conducting surfaces for a range of frequencies
DuctingDucting occurs when cool winds from the ocean blow across the land. This
creates a band (or duct) of cool air trapped between two layers of warm
air. Once radio signals (typically in the VHF and UHF bands) enter this
duct, they effectively 'bounce' inside the duct, with some of the signal
penetrating the top and bottom of the duct on each bounce. This anomaly
can greatly extend the range of communications. For UHF, ducting can extend
the range from 40km to over 400km. However, severe atmospheric disturbances,
such as tropical cyclones, destroy ducting by disrupting the temperature
inversion. Wavelength equations and lengthsWavelength (l) = velocity (V) / frequency (F) The length of a half wavelength dipole antenna is ½ l = 142.5 / F(MHz) Thus one element of the dipole is a quarter wavelength ¼ l = 71.25 / F(MHz)
Clark mast anchor alternativesOccasionally you will come across a situation where it is impossible to hammer the Clark mast anchor pickets into the ground, such as when the only high point around is a solid rock outcrop. This happened to us at a search we attended in September 2011, and below are some photos of the alternative anchor system employed by the responding team. Luckily there were some small shrubs that were growing in the cracks in the outcrop, and their root system was strong enough to support the mast. The spacing between the 3 sets of guys had to be adjusted from the standard 120° however the final setup proved to be suitable for the task. |
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