SM6EHY on PROPAGATION (below 10 MHz mainly)
After beeing active some few 10 years on especially 80 and 160-meters having used directional antennas one cannot neglect to comprehend something about the band behaviour or propagation towards distant locations.
Most of the papers written on this subject is made due to direct orders
from the BC-industry.
They had to know where their transmitters could be heard with reasonable
readability and for how long at dayhours mostly. A radio amateur is not
only interested in this phenomenon, rather is it how far out one can reach
at each time (evening or nighthours mostly) on a given band.
Using a non directional antenna one can only notice different signalstrengths
and cannot decide from which azimuth sector the particular signal is coming
from. Ofcourse one can hear from what country a station is coming from
but this does not indicate the azimuth direction for certain.
One can quite easily decide however if the signal travels trough an area
where the Aurora Boralis is active, due to the signal quality: Selective
fading and flutter are signs of auroral affection.
Communication parameters
Most commonly (nowdays) this is a matter associated with microwave
communication links. These parameters are (seen from the transmitter /
receiver all the way towards the ionsphere):
|
Transmitter |
Receiver |
|
Modulation type |
Demodulation |
|
Transmit bandwidth |
Demodulation bandwidth |
|
Power |
Sensitivity |
|
Feeder loss |
Feeder loss |
|
Antenna gain |
Antenna gain |
|
Clear view in direction |
Clear view in direction |
|
Fading, Multipath, Background |
Fading, Multipath, Statics, QRM, |
If You increase Your transmit power by a factor of 4, You will be heard
at twice the distance, when You are in the linear portion of the graph.
If You have gained enough number of dB's, for the path of interest, You
will notice that You will get out twice the distance for LESS than 4 times
(6 dB's) the power. The graph can be almost flat, meaning that You can
count with to increase Your distance twice by only increasing Your power
a fraction of a dB !
It is quite obvious that it is desireable to reach for this "super-conducting"-level.
In order to gain it, Your antenna radiation lobe has to be in the very
right spot, both in azimuth and in elevation. The specific installation
is more responsable than the antenna itself.
The transmit energy excites the atoms at the bouncing mass in such a way that they cause a chain reaction. If the transmit energy is high enough it seems like the electyrons are lifted one or more energy "levels". On very rare occations the transmit energy can set such a stress at the mass, that the reflection coefficient rather gets worse with increased level for a specific angle. The reflection starts at other angles, and a spread reflection takes place. Too much background energy from the sun has the same effect.
Read the A-index from WWV i Boulder; if under some 4 or over some 10, indicates disturbed conditions. The A-index is a 24 hours average, and the K-index is a 3 hour index. For the ionsphere layers to be best for low frequencies (some 2 to 10 MHz), the K-index has to be low (<2 ); the longer the better. It indicates that the bouncing mass is uniform enough in order to enhance bouncing. With values a bit higher, the upper HF-bands gets better, hence the uniform unit is in wavelengths.
As the activities of SM6EHY reveals, we have no less than 8 different
propagation modes on the 80m-band:
|
Propagation mode |
Takeoff angle |
Maximum occurance Duration |
Distance |
|
1. |
High |
Always |
No DX |
|
2. |
High |
Almost always |
No DX |
|
3. |
High and |
Nights / Twilight |
DX |
|
4. |
Mid high |
Depends upon DX location |
DX |
|
5. |
High |
Summer |
DX |
|
6. |
High and |
Both highly dependant upon |
DX |
|
7. |
High |
The dark half year |
DX |
|
8. |
High |
Depends upon DX location |
DX |
How to determine if the condx are good or bad ?
It is highly a matter of what You think of !
1 Is it the signalstrength
or the readability at one or both ends ?
2 Is it to be able to get
as far away as possible?
3 Is it to be able to talk
with Your friend in VE1 (N.Foundland)[in the European point of view]?
4 Is it the number of DX-stations
You can work per hour ?
1: Signalstrength: You have to decide
what time of night that is best, considering the equipment used at both
ends. If both stations are using DX-wise poor antennas (a simple InvVee
or a Dipole at some low height ; < 15 meters AGL) the maximum occurs
when both are in TWILIGHT or both are in darkness and have equal distance
to a twilight zone.
Readability: Not only to have the above in mind, but also consider
Local Noise (QRN=static crashes from thunderstorms nearby). For example
if You are located in the Mexican Gulf or in Indonesia You have some 15
times more statics than the guy up in Scandinavia. In a low noise area
it is common knollege that if You hear a station from a high noise area,
he must be at least S9+ before it is worth calling him, because he has
a local noise level of some S9... . Choose a low noise period or yet better
a special low noise reveiving antenna at the high noise end. The QST-magazine
has an article almost anually about this matter.
2: First of all, get yourself a DX-edge
calculator or a computer model visulizing the grayline around the globe
(Miller projection). By means of this tool You will be able to determine
how far away You can reach. The poorer Your efficiency is at the low take
off angles, the closer to the exact sunrise/sunset-line You get.
You can use the grayline info to determine how efficient your antenna is
for Long Haul DX-ing.
The following figures regards 80 meters:
for a latitude close to the equator you can get some 40 minutes grayline-effect
for a good antenna. The poor antenna will only give you some 10 minutes.
At 57° you can get up to 2.5 hours (and even more...) and down to 30
minutes, not counting the 3 summer months when the entire (quite short)
night will give you a grayline-effect.
3: The signalstrength maximum occurs
when both have equal distance to midnight and a dark sky. The takeoff angle
is quite high, and You must use a high angle radiating antenna such as
an average dipole or a horisontal polarized loop, broadside to the other
stations great circle sector. Under severe conditions the Aurora can wipe
out a contact. Using a vertical with good efficiency at low angles will
often make a contact possible at these severe conditions.
If the readability is the mayor concern use a vertical antenna with
good and long radials in the other stations great circle sector. You can
count with to have a contact up to some 1.5 hour BEFORE sunset in VE1 and
some 1.5 hour after sunrise at Your end.
4: Here we encounter some more factors other
than pure wave propagation. We have to include what the usual operators
habits are like.
When in the evening hours are most of them active on the radio ?
What do they do around their sunset / sunrise ?
What do they do around their midnight ?
At sunset the operators usually; drive home from work; eats their dinner;
watch their television news; socializing with their family e t c.
At sunrise they either; sleeps; eats their breakfast; drives to work e
t c.
The operating experience tells that we are mostly active from some 2100
to 2300 hours local time. At this time we have high radiation angles active.
To be able to contact a stateside station for a station in Eu, the operating
time shall be chosen to be 2100 + 6 = 0300 CET.
SKEWED PATH
This phenomenon is not mentioned in many other papers (if any ?). The occurance
is maximized around the Spring / Autumn equinoxes and are generally active
when the usual direct path is closed. Most often this means that the Aurora
is active.
As can be seen in the table above, this path involves HIGH take off angles,
almost disregarding the distance. The actual bouncing from the ionsphere
takes place higher up above the earth than usual.
How come ? To explain the bouncing mass, we have
to recall that our mother Earth is bombarded by the Sun-storm of particles.
During daylight the height of the ionsphere is depressed towards ground,
and the opposite during the night, when the storm tends to drag it out
from earth.
See an example picture of one of the equinoxes here.
As can be seen we have an oval highly dark area, with a twilight area surrounding
it. In the middle of this dark oval we have a peak height of the ionsphere.
It is highly assumtious that even the highest take off angle signals will
sooner or later come close to the bouncing layer in a smaller angle than
necessary for to be totally reflected. The incoming bounce-angle is the
same as the outgoing angle, which means that on the other side of this
oval the signal will be reflected again down to earth, in order for some
station to hear it.
If the signal path is skewed within the night oval, it is also quite possible for the signal to be bouncing around in ovally shaped circles, with a certain height angle transfer for eatch turn. This means that the signal can be delayed up to a few seconds, before eventually dropping down to earth again.
Propagation analysis are made in almost every countries national magazine.
There is but one significant thing that is overlooked in ALL predictions.
It is the "common knowledge" every active Ham has.
The analysis programs; IONCAP, ICEPAC, Minimuf e t c are NOT dealt with
in view of the active Ham operator. These analyses are based upon the BC-industry;
Good antenna and POWER at the transmit end, and poor efficient antenna
whip at the receiving end. This way the prediction has little effect for
us, telling us when a band is open.
As the investigation of SM6EHY reveals, we have to take off some 70 dB
of attenuation in order to be able to see the actual openings we hear on
the bands.
That is due to that the amateur can rely upon some 6 dB signal to
noise (s/n)-ratio, and NOT 70 dB the programs ,by default, puts in; the
Rx-antenna is far better than the default used "whip" and the
Rx-bandwidth is much smaller.
When such attentuation is taken off, we can see the following over a given
path.
In a typical winter month, Gothenburg (Sweden) -
Delaware (USA) in sunspot minimum.
© Björn Waller, SM6EHY 1998, 1999