Propagation Analysis Software
Skywave
Trigonometry
Author: R.J.Edwards G4FGQ © 17th February 2004
For given one-hop
ground path distance and height of reflecting layer this program
calculates radio path distances and the radio-path elevation angle.
The remainder of the program assists with appreciation
of how radio waves propagate via the ionosphere and
how losses are crudely proportioned. Greatest loss occurs due to dispersion
(spreading out) of waves in space. Then come ground absorption and reflection
losses which increase rapidly for small elevation angles. Under calm conditions
only a moderate loss occurs due to absorption in the ionosphere. Under
disturbed conditions ionospheric loss is subject to great variability.
The program crudely assumes "average" conditions.
For simplicity MUF, Maximum Useable Frequency, is disregarded.
This depends on the angle of incidence between the radio path and the reflecting
layer. It is influenced by the Sun's elevation angle, on seasonal variations,
etc.
It frequently occurs that two paths are simultaneously
available between transmitter and receivers each path using a different
number of hops. This causes the resulting signal to fade, perhaps flutter
and become distorted - multi-path distortion.
- Dispersion, spreading loss between transmitter and receiver assumes
both antennas are dipoles.
- Receiver input volts assumes antenna and the 50-ohm receiver are impedance-matched.
- Transmitter power output = 100 watts CW
- Antenna radiating efficiency = 100%
- Receiver S-meter is calibrated according to the de-facto standard.
- The midpoint of a hop decides whether a hop is in daylight or darkness.
- Layer heights are assumed to be the same for both hops.
- Remember: Signal strength can vary by 15 dB or more depending on conditions.
The Following
Notes are not Directly Connected with the Program, but may be of Interest.
Fcrit, critical frequency is the frequency at which the wave penetrates
a layer at vertical incidence without reflection. As elevation angle decreases
so does the angle of incidence - and the MUF increases according to the
relationship MUF = Fcrit/Sin(Angle-of-incidence). So highest MUFs occur
at low angles and at long distances. If frequency increases above MUF propagation
loss rapidly increases.
Lowest useful frequency occurs when a lower-height reflecting
layer intervenes between ground and a desired reflecting layer. The D-layer,
at 70 km, rapidly absorbs radio waves in daylight below about 3-4 MHz to
screen all other layers. So the amateur 160 meter band is of no use in
daylight except on groundwaves up about 80-100 miles. Frequencies above
5 MHz are unaffected by the D-layer.
Run this Program from
the Web or Download and Run it from Your Computer
This program is self-contained and ready to use. It does not require
installation. Click this link TwoHops then
click Open to run from the web or Save to save the program
to your hard drive. If you save it to your hard drive, double-click the
file name from Windows Explorer (Right-click Start then left-click
Explore to start Windows Explorer) and it will run.
Also see: Sky Trig
This page was last modified: Mon, 01 Feb 2010 22:36:55 GMT
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