Frank wrote:
. . . I agree with comments about adding a horizontal wire to the top of the vertical; it will probably be easier than a capacity hat. I am overloaded with work at the moment, but would like to attempt a model in a week or so when I have less work. Take a look also at a tee type arrangement. That is, a horizontal wire with the tip of the vertical connected at or near its center. It might have some advantages over connecting the wire's end to the vertical. But of course it might be more involved to construct. Roy Lewallen, W7EL |
Dan, KB0QIL wrote:
"From a practical perspective it would seem to me that building a 40 foot crnter loaded dipole and putting it in the sttic or on the roof would probably perform somewhat better." The roof or attic may be noisy receiving locations. The ionospheric spot which effectively reflects a high frequency signal to a point beyond the horizon is variable so that the received signal direction varies from the true bearing of the transmitter, The received signal elevation angle also varies from that predicted by the assumed layer height for any given path length, and may change from instant to instant. The differences between predicted and actual azimuth and elevation angles may at any momement be several degrees. These differences make high frequency direction finding complicated, but results may be good enough for some pracical purposes. Optimum vertical and horizontal angles are sought in directional antenna design but enough beamwidth is needed to accommodate the angular variations which occur. Over sea water, ground wave propagation is good and loss is low as compared with propagation over earth. Frequencies up to about 5 MHz are used for communications beyond the line of sight between ships and between ships and shore. These frequencies are also used for tropical broadcasting among islands. For ionospheric reflection to near spots beyond the line of sight, near vertical incidence reflections are used. The frequency must be below the maximum usable frequency for vertical incidence at the transmitting site. For ground wave propagation a vertical transmitting antenna is used. Horizontally polarized antennas are often used for sky wave signals because reflection from the ionosphere makes equal strength components, horizontally polarized and vertically polarized, from the incident wave, regardless of its initial polarization. Most disturbing noise is that generated within ground wave range of the receiving antenna. It is vertically polarized.There is no ground wave propagation of horizontally polarized waves. Thus, a horizontally polarized receiving antenna ignores much of the available noise. However, it receives as much signal from the sky wave as a vertically polarized antenna would. If a single antenna is to be used for both transmitting and receiving a shy wave, a forizontally polarized antenna may be the better choice due to its noise rejection. See "Radio Antenna Engineering" by Edmund A. Laport for details. Best regards, Richard Harrison, KB5WZI |
"Richard Harrison" wrote in message ... Dan, KB0QIL wrote: "From a practical perspective it would seem to me that building a 40 foot crnter loaded dipole and putting it in the sttic or on the roof would probably perform somewhat better." The roof or attic may be noisy receiving locations. The ionospheric spot which effectively reflects a high frequency signal to a point beyond the horizon is variable so that the received signal direction varies from the true bearing of the transmitter, The received signal elevation angle also varies from that predicted by the assumed layer height for any given path length, and may change from instant to instant. The differences between predicted and actual azimuth and elevation angles may at any momement be several degrees. These differences make high frequency direction finding complicated, but results may be good enough for some pracical purposes. Optimum vertical and horizontal angles are sought in directional antenna design but enough beamwidth is needed to accommodate the angular variations which occur. Over sea water, ground wave propagation is good and loss is low as compared with propagation over earth. Frequencies up to about 5 MHz are used for communications beyond the line of sight between ships and between ships and shore. These frequencies are also used for tropical broadcasting among islands. For ionospheric reflection to near spots beyond the line of sight, near vertical incidence reflections are used. The frequency must be below the maximum usable frequency for vertical incidence at the transmitting site. For ground wave propagation a vertical transmitting antenna is used. Horizontally polarized antennas are often used for sky wave signals because reflection from the ionosphere makes equal strength components, horizontally polarized and vertically polarized, from the incident wave, regardless of its initial polarization. Most disturbing noise is that generated within ground wave range of the receiving antenna. It is vertically polarized.There is no ground wave propagation of horizontally polarized waves. Thus, a horizontally polarized receiving antenna ignores much of the available noise. However, it receives as much signal from the sky wave as a vertically polarized antenna would. If a single antenna is to be used for both transmitting and receiving a shy wave, a forizontally polarized antenna may be the better choice due to its noise rejection. See "Radio Antenna Engineering" by Edmund A. Laport for details. Best regards, Richard Harrison, KB5WZI ================================ Richard, I am impressed by your logical descriptions and explanations of skywave and groundwave propagation. You are more than convincing. No doubt reinforced from practical experience. It all makes sense. Something much needed on these newsgroups. I notice you do not treat the works of so-called 'experts' as bibles but as a means of further study. ---- Reg, G4FGQ |
Roy,
Thanks. This might be feasible. The site would support 50 foot wire from the tip. At 500 watts what would the current in the horizontal leg be? In other words what is the minimum effective gage? What is the purpose of this leg? Is it capacitive or does it begin to look like something else. What are it directional characteristics? Dipoles nodes are perpendicular while long wire nodes are parallel. Dan Roy Lewallen wrote: Frank wrote: . . . I agree with comments about adding a horizontal wire to the top of the vertical; it will probably be easier than a capacity hat. I am overloaded with work at the moment, but would like to attempt a model in a week or so when I have less work. Take a look also at a tee type arrangement. That is, a horizontal wire with the tip of the vertical connected at or near its center. It might have some advantages over connecting the wire's end to the vertical. But of course it might be more involved to construct. Roy Lewallen, W7EL |
To determine the horizontal wire current, download the free EZNEC demo
from http://eznec.com. That's exactly the kind of thing it's good for. If you put a single horizontal wire out to make an L shape, the wire radiates a considerable amount. Being as low as it is, a lot of the power will be dissipated in the ground, and only a small fraction will be radiated at a low elevation angle. But if you connect to the center of a horizontal wire to make a T shape, the fields from the two halves of the horizontal wire will nearly cancel, so it'll radiate very little. Its main effect, like a capacitive top hat, will be to even out the current in your vertical wire, which will raise the radiation resistance and therefore the efficiency. EZNEC or a similar program will quickly show you the differences in field strength in various directions for the antenna as it is, and with either of the top loading configurations. Roy Lewallen, W7EL dansawyeror wrote: Roy, Thanks. This might be feasible. The site would support 50 foot wire from the tip. At 500 watts what would the current in the horizontal leg be? In other words what is the minimum effective gage? What is the purpose of this leg? Is it capacitive or does it begin to look like something else. What are it directional characteristics? Dipoles nodes are perpendicular while long wire nodes are parallel. Dan Roy Lewallen wrote: Frank wrote: . . . I agree with comments about adding a horizontal wire to the top of the vertical; it will probably be easier than a capacity hat. I am overloaded with work at the moment, but would like to attempt a model in a week or so when I have less work. Take a look also at a tee type arrangement. That is, a horizontal wire with the tip of the vertical connected at or near its center. It might have some advantages over connecting the wire's end to the vertical. But of course it might be more involved to construct. Roy Lewallen, W7EL |
There is no ground wave
propagation of horizontally polarized waves. Thus, a horizontally polarized receiving antenna ignores much of the available noise. There can be exceptions to this though. There is a horizontal "space wave" and it can cause all kinds of noise problems. In fact, I have had just as much noise problems with horizontal dipoles, as I have with verticals. Much of the local noise here is power line noise. The lines are horizontal in general, and do emit a horizontaly polarized space wave which can travel a fair piece. I've found at this qth, polarization and noise don't always follow the expected norms. I've had horizontal antennas that picked up horrible amounts of noise. But....On the bright side...it does verify that they are working... :/ Here in the cement jungle, I think noise can be about any polarization depending on the source. Some is vertical, but just as much is also horizontal. Of course, being vertical can follow a true ground wave type of propogation, I would expect vertical noise to travel farther than horizontal if you exceeded the direct line of sight. MK |
I think Roy is referring to a T configuration rather than an upside-down L.
The currents will balance in the T so wire size is limited by physical considerations rather than electrical. This is just another form of a capacity hat. The net result is to raise the radiation resistance. "dansawyeror" wrote in message ... Roy, Thanks. This might be feasible. The site would support 50 foot wire from the tip. At 500 watts what would the current in the horizontal leg be? In other words what is the minimum effective gage? What is the purpose of this leg? Is it capacitive or does it begin to look like something else. What are it directional characteristics? Dipoles nodes are perpendicular while long wire nodes are parallel. Dan Roy Lewallen wrote: Frank wrote: . . . I agree with comments about adding a horizontal wire to the top of the vertical; it will probably be easier than a capacity hat. I am overloaded with work at the moment, but would like to attempt a model in a week or so when I have less work. Take a look also at a tee type arrangement. That is, a horizontal wire with the tip of the vertical connected at or near its center. It might have some advantages over connecting the wire's end to the vertical. But of course it might be more involved to construct. Roy Lewallen, W7EL |
Fred W4JLE wrote:
I think Roy is referring to a T configuration rather than an upside-down L. The currents will balance in the T so wire size is limited by physical considerations rather than electrical. This is just another form of a capacity hat. The net result is to raise the radiation resistance. In a tee type antenna, there will be considerable current at the junction of the horizontal and vertical wires. While it's unlikely that any wire strong enough to be used won't be able to handle the current from a heating standpoint, it is possible that using a wire on the small end of the range might result in noticeable loss. A quick run with a modeling program would show whether or not that might happen with a given set of dimensions. One thing I should mention. If the horizontal portion is higher than about 0.2 wavelength, MININEC-type ground can be used for modeling either a T or L. The vertical wire is connected directly to ground, and ground loss can be inserted at the base as a resistive load. If the horizontal wire is much less than 0.2 wavelength high, the MININEC-type ground can still be used with reasonable accuracy only for the T type antenna. For an L type antenna where the horizontal wire is less than 0.2 wavelength high, a model has to use the High Accuracy ground model, with the ground system modeled as radial wires just above the ground. Roy Lewallen, W7EL |
Mark Keith, NM5K wrote:
"I`ve had horizontal antennas that picked up horrible amounts of noise." Yes, the protectection comes from noise beyond the line of sight range but not so far away as to require aky wave propagation. Propagation is a function of frequency. Below 100 KHz, gtound waves are little affected by the earth`s attenuation and the sky wave is reflected with little loss by the ionosphere. Waves travel up to 600 miles with little perturbation from the time of day, season, or year, but at greater distances, low frequency reception is better at night and in the winter due to ionospheric changes affecting the reflected signal.. On a yearly basis, signal strength over long distances correspond with the 11-year sunspot cycle. Low frequency signal strength changes only slowly without rapid fades which characterize high frequency operation. At frequencies above 100 KHz but below 535 KHz, ground wave attenuation is greater than at frequencies below 100 KHz. Daytime ionospheric losses are very high. Daytime ground wave propagation is better at the lower end of this frequency range and over soil of higher conductivity. Signals may extend to several hundred miles, where noise levels in the receiving location are low. Nighttime transmission to distant points is possible due to ionospheric reflection. Dependable daytime reception in the 100 to 535 KHz range is bad due to lack of ionospheric propagation and high attenuation of the ground wave especially at the higher frequency end of this band over poorly conductive earth and during the summer months when there may be thunder storms producing static eithin ground wave range.. At frequencies between 535 KHz and 1600 KHz, only the ground wave is useful in the daytime beyond the line of sight, as the sky wave is completely absorbed. The higher the frequency in this range, and the poorer the earrth`s conductivity,, the greater the attenuation of the ground wave. High powered transmitters at the lower frequencies in this range reach 50 to 100 miles over high conductivity soil. This may be pessimistic. I listen 24 hours to 50 KW KKYX in San Antonio which is 200 miles to my west satisfactorily. It broadcasts on 680 KHz. My receivers are quite ordinary and use internal loop antennas. The earth is highly conductive but there is no sea water in the path. At night, other stations produce low frequency carrier beats with KKYX causing undesirable automatic volume control action. but KKYX`s sky wave is stronger than its groundwave and its reception is still acceptable.. Radio Havana is one of its competitors. I hear all about "El Comandante" at times. Sky wave goes far in the 535 to 1600 KHz band. During Hurricane Carla in the 1960`s I listened to Dan Rather describe the storm blow by blow on KTRH, Houston`s 50 KW outlet, from Tierra del Fuego where I was working, and listening on a Hitachi pocket transistor portable radio with its built in loop antenna. The path is about 6000 miles long but mostly over the ocean. KTRH transmits on 740 KHz from the banks of Cedar Bayou. They have a 4-tower directionnal array with a North-South bias. Reception was good in Tierra fel Fuego as it is nearly at the Antarctic Circle and there are no thunder storms there. It is too cold. Groundwave extends hundreds of miles from KTRH, but not 6000 miles. My reception was shy wave using several hops.. Broadcast transmitters concentrate energy along the horizon so low elevation angles are favored.. This works well for sky wave DX, especially over the ocean. Sky wave attenuation in the 535 to 1600 KHz band is about the same throughout the band, so nighttime coverage of broadcast stations in this range is almost independent of frequency, while daytime ground waves favor the lower frequencies. When I was a kid, I had a crystal set fixed tuned to KTRH which directly drove a loudspeaker, if I could find a sensitive spot on the galena. I lived almost in sight of the station. At frequencies between 1600 KHz and 30 MHz, the ground wave attenuates so rapidly as to be usseless except over very short distances. Propagation is either line of sight or via ionospheric reflection or via tropospheric scattering. Frequencies above 30 MHz are often used for scattering ao that extremely high gain antennas are practical. Scatterihg often uses brute force to extend the range of signals beyond the line of sight. Most long-distance short-wave communications result from ionnospheric reflection. In the frequency range of 1600 KHz to 30 MH, a band of frequencies can almost always be found that provides communications by sky wave over a path between two points on earth. The maximum usable frequency depends on the distance between the points and ionospheric conditions. The minimum usable frequency depends on ionospheric conditions, effective radiated power, and the noise level at the receiver. Losses in the ionosphere increase with wavelength, so the frequency which gives the best signal is usually the maximum usable frequency. For communocations reliability, the maximum usable frequency is often discounted by 15% to provide an "Optimum Working Frequency". Daytime DX requires a high frequency. Shorter paths require lower frequencies. Typically 10 to 29 MHz during the day and 5 to 10 MHz, at night, are best for transmission over transoceanic distances (thousands of miles). Rember the Zenith portable? The best frequencies are usually higher during the day for long paths than they are at night Optimum frequency increases with the length of the path up to the maximum distance for one-hop transmission, about 1200 to 2400 miles. Low elevation-angle radiation such as 5 to 15 degrees is usually most desirable. Radiation below an angle of about 3.5 degrees may be absorbed by the earth near the transmitting antenna and wasted. Frequencies above 30 MHz are usually not reflected by the ionosphere and provide only sporadic sky wave communications. Best regards, Richard Harrison, KB5WZI |
Now that is interesting, Roy. I was going to put up a 160 m inverted L this
summer. I am limited to only being able to go up about 45 feet, so I would need about another 90 feet horizontal. Are you suggesting that it might be a better arrangement to go up the 45' and then put up the top "T"? If so, roughly how long should the top part of the T be (each side of center) to get me to 160? I'm guessing it may not be accomplished without some base loading...and that is what took me to the Inverted L in the first place...direct coax feed, albeit not a particularly good low angle radiator. I am prepared to put down a radial field...but I want to stick with a simple vertical wire, either extended horizontally as an Inverted L or as you suggest, a T, if it can be done. I have about 100' either side of center available to construct the top part of the T. In either case, the top loading wires will need to be somewhat of the inverted v construction, as I don't have 45' high supports for each end. Thanks for any thoughts you might have. I need to get something done before winter! 73, ....hasan, N0AN "Roy Lewallen" wrote in message ... To determine the horizontal wire current, download the free EZNEC demo from http://eznec.com. That's exactly the kind of thing it's good for. If you put a single horizontal wire out to make an L shape, the wire radiates a considerable amount. Being as low as it is, a lot of the power will be dissipated in the ground, and only a small fraction will be radiated at a low elevation angle. But if you connect to the center of a horizontal wire to make a T shape, the fields from the two halves of the horizontal wire will nearly cancel, so it'll radiate very little. Its main effect, like a capacitive top hat, will be to even out the current in your vertical wire, which will raise the radiation resistance and therefore the efficiency. EZNEC or a similar program will quickly show you the differences in field strength in various directions for the antenna as it is, and with either of the top loading configurations. Roy Lewallen, W7EL dansawyeror wrote: Roy, Thanks. This might be feasible. The site would support 50 foot wire from the tip. At 500 watts what would the current in the horizontal leg be? In other words what is the minimum effective gage? What is the purpose of this leg? Is it capacitive or does it begin to look like something else. What are it directional characteristics? Dipoles nodes are perpendicular while long wire nodes are parallel. Dan Roy Lewallen wrote: Frank wrote: . . . I agree with comments about adding a horizontal wire to the top of the vertical; it will probably be easier than a capacity hat. I am overloaded with work at the moment, but would like to attempt a model in a week or so when I have less work. Take a look also at a tee type arrangement. That is, a horizontal wire with the tip of the vertical connected at or near its center. It might have some advantages over connecting the wire's end to the vertical. But of course it might be more involved to construct. Roy Lewallen, W7EL |
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