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Multi hopping radio waves
Reflection loss can vary from zero to infinity; depending on the
material and angle of incidence. ==================================== Yes I know. That's obvious. But what I would like to know is a typical or average value, or a range of most likely expected values found in practice. Some experienced person must know! Needed to crudely ESTIMATE ionospheric multi-hop path loss. Ground reflection losses are a small proportion of the total path loss but not small enough to be neglected. Just a whole number of decibels per reflection will do please. --- Reg. |
Multi hopping radio waves
"Reg Edwards" wrote in message ... Reflection loss can vary from zero to infinity; depending on the material and angle of incidence. ==================================== Yes I know. That's obvious. But what I would like to know is a typical or average value, or a range of most likely expected values found in practice. Some experienced person must know! Needed to crudely ESTIMATE ionospheric multi-hop path loss. Ground reflection losses are a small proportion of the total path loss but not small enough to be neglected. Just a whole number of decibels per reflection will do please. --- Reg. Some approximate examples at 7 MHz with angles of incidence from 0 - 40 degrees: Sea Water 0.2 dB Rocky Ground 5 dB Average Gnd. 2 dB Frank |
Multi hopping radio waves
Thank you Richard, and the others, for digging out and presenting the
information from which I can deduce a ball-park figure. My original figure of 5 dB per hop for a ground reflection was slightly too high. It's nearer to 3.5 dB. I'm still thinking about it. But 4 dB is near enough. Not that it matters very much. I deduced 5 dB from my experience of signal strengths received from such places as the antipodes and the Western US states. It's not surprising hopping across just the North Atlantic results in zero dB loss. The excess path loss, over and above spreading loss, must be due to ground reflection losses. Just calculate backwards from received signal strength, path distance and the probable number of hops. It's easy to do this with dedicated computer programs. For very long distance paths assume that half the ground reflections are due to sea/ocean water and the other half is due to land masses and you won't go far wrong. Ground reflection losses at the transmitting and receiving sites can be ignored. Or such losses can be lumped together to constitute another complete hop. I needed the information to include in a simple program which predicts (approximately) path loss for multi-hop propagation. Program users cannot be expected to know incidence angles, ground conductivity and permittivity, Brewster angles etc, for every hop along a route. Some guesswork is needed on the part of the programmer to make a program useful. Despite your continuing abuse of the English language I know you are quite capable of understanding the foregoing waffle. I'm on South Eastern Australian Merlot tonight. Hic! I think the Chinese will be coming along shortly with their own high quality stuff. They are not just becoming adept with their high technology. Californian wine growers should look to their laurels. But no doubt you are all more immediately concerned with the price of oil, the gas in your tanks, and from where it may be obtained. Iraq and Iran for example. ---- Reg, G4FGQ |
Multi hopping radio waves
Roy Lewallen wrote:
Reg Edwards wrote: The amplitude and phase of a field after ground reflection depends on the polarization, and is quite different for horizontal and vertical. It of course also depends on ground conductivity and permittivity, frequency, and angle. The equations are simple, and can be found in Kraus and other references. Those equations are used by NEC for determination of the far field pattern. Roy Lewallen, W7EL =========================================== Yes! But what's the ball park, rule-of-thumb value in dB ? ---- Reg I dunno. What's the ball park, rule-of-thumb value of a resistor in ohms? Sumptin tween nuttin and everthin Roy Lewallen, W7EL |
Multi hopping radio waves
Frank wrote -
Some approximate examples at 7 MHz with angles of incidence from 0 - 40 degrees: Sea Water 0.2 dB Rocky Ground 5 dB Average Gnd. 2 dB ========================================= Thanks Frank, Your figures for 7 MHz are representative of HF. Nobody is particularly interested in MF, LF or VLF. They confirm my latest estimate of an average, between sea water and dry land, of roughly 3.5 dB per ground reflection. ---- Reg. |
Multi hopping radio waves
"Reg Edwards" wrote in message ... Frank wrote - Some approximate examples at 7 MHz with angles of incidence from 0 - 40 degrees: Sea Water 0.2 dB Rocky Ground 5 dB Average Gnd. 2 dB ========================================= Thanks Frank, Your figures for 7 MHz are representative of HF. Nobody is particularly interested in MF, LF or VLF. They confirm my latest estimate of an average, between sea water and dry land, of roughly 3.5 dB per ground reflection. ---- Reg. No problem Reg. I did the computations recently trying to estimate the path loss, on 7 MHz, from the west coast to Europe via the long path. The various ground losses from all kinds of ground, including polar ice, and fresh water, are all fairly low. The real problem was to estimate the losses due to the incidence with the diffuse, conductive, ionospheric plasmas, and also to consider the possibility that some inonospheric ducting occurs. So far I have not attempted to estimate these losses, but they must be very high, since only considering ground incidence produces unrealistically low path losses. Frank |
Multi hopping radio waves
Dear Group:
The use of one number is crude and suitable only if one has imbibed enough grain alcohol or one does not care about Lord K's admonition or both. The preferred scheme is to model the expected virtual heights at each ionospheric reflection (note that the apparent TOA (angles) involved are not likely to be the same at each of these reflections) and then to use the angles involved to note the expected incidence angle of the intermediate "ground" reflection. The coordinates of the expected "ground" reflection areas are calculated and note is taken as to whether those areas are predominately salt-water, ice, or neither. A heuristic algorithm is applied that depends on type of "ground" and that weakly depends on the expected incidence angle. The result is a statistically significant reflection loss. [Some iteration is needed, which computers are very good at doing.] It is important to note that the apparent TOA of the major mode between two points is unlikely to be the same at both ends of the path because the virtual height is unlikely to be the same near both ends. For HF paths greater than something like 12 or 14 Mm predictions become more complex. In all cases of multiple hops (real DX), the TOA at which the gain of the antennas is effective varies between about 12 degrees and 2 degrees. If one wishes a simple predictor, one could find it in a paper published in the UK in the transactions on a conference on HF propagation in the 80s (as I recall) by a BBC engineer (IEE was the publisher). The entire computer code is given in the paper. It uses a simple heuristic model that was found by the BBC to give satisfactory results over the paths that their World Service used. Note that the BBC used paths that did not include much of the polar regions. To digress: The worst path to a DXCC entity from the Upper Midwest is over the magnetic pole to VU4. 100 watt transmitters, ice reflections, heavy absorption, and roughly 10 db more noise at the far end make the need for power and high antennas almost necessary. 73 Mac N8TT -- J. Mc Laughlin; Michigan U.S.A. Home: "Richard Harrison" wrote in message ... snip It could be right for some reflections. E.A. Laport was Chief Engineer of RCA International when he wrote "Radio Antenna Engineering". On page 236 Fig. 3.17 shows the effect of ground conductivity on maximum field strength from a horizontal dipole antenna versus its height in vavelengths. Optimum height would be about 0,50 wavelength to most concentrate energy at a certain vertical angle, 30-degrees according to the RAF Signal Manual quoted by Laport. 30-degrees might hop 1000 kilometers. At the antenna earth reflection point, frequencies between 2 and 16 MHz are reduced to 95% of their prereflection field strengths by ordinary soil from a dipole at 1/2-wavelength height. A reduction to 70.7% of prereflection strength would represent a 3 dB power loss. So no harm done yet by the reflection from an antenna over good soil. Lower antenna height and poorer soil would attenuate more. The angle at which rhe signal strikes the earth in subsequent reflections should be the same as the first reflection from the antenna. Conductivity and dielectric constant at subsequent earth reflection points are what they are. Shortwave broadcasters use vertically stacked horizontal elements to concentrate the vertical beam to avoid multipath interference. They also prefer targets reached on the first reflection from the ionosphere.. Best regards, Richard Harrison, KB5WZI |
Multi hopping radio waves
Mac, N8TT wrote:
"Note that the BBC used paths that did not include much of the polar regions." That`s an indication that they knew something about broadcasting. There must be a better way somewhere that doesn`t involve a path near a polar region. A broadcaster must advertise his programs well in advance. He can`t find a band that`s open and tailor his emissions to it. He must fire up on schedule with the right program at the designated time and direction regardless of conditions. All is planned long ahead of time. One of the most usless toys we had was a backscatter ionospheric sounder. It worked well but we had no immediate need for the information it provided. We were locked in our schedules for months in advance and today`s ionospheric conditions were short-term indeed. Best regards, Richard Harrison, KB5WZI |
Multi hopping radio waves
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