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Home Technical Index Site Map ARES/Traffic Scouts Photo Index Roster Repeaters 2m Nets HF Nets
Understanding Shortwave Radio Listening
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| Freq | Band | When |
|---|---|---|
| 1.8-2.0 | 160 M Ham | Late Night |
| 2.3-2.4 | 120 M Bc | Late Night |
| 3.2-3.4 | 90 M Bc | All Night |
| 3.5-4.0 | 80/75 M Ham | All night |
| 4.75-5.07 | 60 M Bc | All Night |
| 5.9-6.2 | 49 M Bc, P | All Night |
| 7.0-7.3 | 40 M Ham | Eve, Night, Morn |
| 7.1-7.4 | 41 M Bc (foreign) | Eve, Night, Morn |
| 9.4-9.9 | 31 M Bc, P | Morn, Day Eve |
| 10.1-10.15 | 30 M Ham | Morn, Day, Eve |
| 11.65-12.05 | 25 M Bc, P | All day |
| 13.6-13.8 | 21 M Bc, P | All day |
| 14.0-14.35 | 20 M Ham | All day |
| 15.1-15.6 | 19 M Bc, P | All day |
| 17.55-17.9 | 16 M Bc, P | All day |
| 21.0-21.45 | 15 M Ham | All day |
| 21.45-21.85 | 13 M Bc | Not used much |
| 25.67-26.1 | 11 M Bc | Not used much |
| 26.965-27.405 | 11 M CB | Lots of noise |
| 28.0-29.7 | 10 M Ham | All day, sometimes |
The shortwave spectrum is divided into bands. You need a basic familiarity with this to use a shortwave radio effectively. The shortwave spectrum is about 25 times larger than the AM broadcast band (.55 - 1.7), so you need to know what is where, and when.
The bands are called "Meter" bands and are identified by their approximate wavelength in meters.
Notice that 40 meter ham and 41 meter broadcast overlap. This is a big problem we are working to fix in the next international radio conference.
As you can see, the broadcast bands starting at 5.9, 7.1, 9.4, 11.65, 13.6, 15.1, 17.55 are the main place where most all your shortwave broadcast listening will be concentrated. Note, however, that some stations fall slightly outside of these ranges, so make sure to tune above and below them. Also, band edges, and broadcasters' frequencies, change from time to time. So, it pays to keep fresh frequency schedules. Search the internet for "shortwave shedule" and you'll find plenty. Locate one that you like, and that has fresh data. Shortwave listening magazines, and their web sites, are also good sources.
Most Amateur communications uses single-sideband. You need an SSB-equipped radio, or one with a "BFO" control, to receive them.
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Wavelength (feet) = 984 ÷ frequency (in megahertz).Example: Middle of FM-band, 98 megahertz,984 ÷ 98 = 10.04 feet.Example: Bottom of AM-band, 0.55 megahertz,984 ÷ 0.55 = 1,789 feet.No, radio waves don't really go "squiggling"through the air like a wave - we just draw themthat way on x-y (amplititude-time) graphs.
Section of wire, with electron concentrationalternately compressed and expanded.They are "jiggling" back and forth,
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Let's start here. Electricity, when flowing continuously in one direction is called direct current (DC). DC obeys the same rules as water in a pipe - flow is a function of pressure and resistance. More pressure and less resistance equals more flow. Congratulations - you just learned Ohm's Law.
Electricity, unlike water, can change its direction of flow very rapidly. Electricity that flows back and forth is called alternating current (AC). Utility power changes directions 120 times per second, AM-band radio about 2 million, FM-band radio about 200 million, and a microwave oven about 4 billion. Two changes, one forward and then one backward, are called one cycle or one Hertz. The number of cycles per second is called the frequency. The distance one cycle travels in one second is called the wavelength of that frequency. Since the speed is fixed (the speed of light), higher frequencies have shorter wavelengths, and lower frequencies have longer wavelengths.
Electricity travels down a wire at near the speed of light. At high frequencies, it becomes practical to shove extra electrons into one end of a wire then jerk them back out again long before the effect reaches the other end. The result of this is that, at such high frequencies, we don't need a closed loop to have a useful circuit - we can set up an electron oscillation in an open-ended conductor, much like a vibrating coil spring.
If the length of the conductor is 1/2, 3/2, or other odd-multiple half-wavelengths long, the conductor is said to be resonant. The length of the wire is in agreement with the length of the wave, at this frequency of oscillation.
When electricity flows, it creates a magnetic field. If the direction of the electricity alternates, the polarity of the magnetic field does, too. It also creates an electrostatic field. A radio wave is simply energy which is alternating between a magnetic field and an electrostatic field. This effect can go on indefinately, while there is a source of energy to sustain it. The energy at a given point diminishes with distance, because the size of the field is growing (and diffusing) as it goes outward.
When a conductor is resonant, it will convert virtually all of the electrical power into radio waves, and thus, is an efficient antenna. (Some power is lost to resistance, but never mind.)
There is a reciprocal law about antennas - any antenna which transmits well can also receive well. When receiving, a radio wave passes across the antenna, inducing an alternating electrical current in it. Variations in the frequency and/or amplititude are called "modulation." A radio receiver then makes the modulation intelligible (hopefully).
Not all antennas are resonant. A long piece of wire, for example, will pick up a little of just about everything, and induce enough current to drive a receiver. Transmitting antennas, however, are almost always designed to be resonant on the particular frequency of the transmitter.
In antenna books, the antenna itself is frequently used as the x-axis of the graph. This antenna is called a half-wave dipole - it has two poles, and is one-half wave long at its design frequency. The sine graphs for voltage and current are shown sitting atop the antenna.
Cycle or Hertz - two changes of the polarity of energy, i.e., stop, forward, stop, reverse, stop.
Kilocycle or kiloHertz (kHz) - One kilocycle = one thousand cycles per second.
Megacycle or MegaHertz (MHz) - One megacycle = one million cycles per second.
Frequency - how frequent something repetitive happens. The frequency of alternating energy is usually expressed in cycles per second or Hertz.
Resonance - Input of alternating or pulsating energy timed to coincide with something's natural tendency to oscillate. Like pushing a child in a swing - you push at the right time, don't you? The swing and the child are a resonant pendulum, and you push forward just as the swing starts forward again. The resonance of a guitar string is determined by its length, weight, and tension. The resonance of a quartz crystal is useful as a stable time-base for electronic watches, computers, and radios. A particular length of wire or tubing is resonant at a particular frequency. Longer wires resonate at lower frequencies. Shorter, higher.
Wavelength - the distance energy travels, at the speed of light, during one complete cycle. Electricity in wire travels a tiny bit slower than light, therefore, a wavelength in wire is not exactly the same as a wavelength in free space (or air).
Bandwidth - how narrow or wide a range of frequencies a particular antenna design can cover efficiently. TV and scanner antennas have a wide bandwidth (hundreds of MHz). A CB antenna has a narrow bandwidth (0.5 MHz). Bandwidth is much more critical when transmitting than when receiving.
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Now that we know our antennas should be resonant, let's see how to make them resonant.
First, are we transmitting or receiving? Transmitting antennas are much more critical than receiving antennas, although a receiving antenna can transmit if it is resonant (or otherwise matched) and if it can handle the transmitter's output power. A transmitting antenna can also receive, and will do so particularly well on the frequency for which it was designed.
If you are running a low-power FM transmitter, or a CB or HAM station, you already know something about transmitting antennas. Amateur operators, in particular, must pass exam questions on antenna design and theory.
If we are operating a shortwave radio, we want it to quit fading out in the middle of our favorite shows.
Now that you are ready to get brilliant, learn rule #1 of antenna design: All antenna designs are a mixture of compromises. Just like boat hulls and airplane wings.
What we need to do, therefore, is identify our particular need and design an antenna which is optimized to fulfill that particular characteristic - whether it be directionality, gain, or bandwidth, or just all-around good performance.
I have been an antenna experimenter for over 25 years. My goal has always been to build cheap, simple antennas that work well. It's all in the numbers. I had a $25 multiband shortwave antenna in the attic which would outperform any commercially-made $150 antenna. I had a discone scanner antenna made of stainless steel welding rods which I built for about $3. I had a VHF yagi which would go five miles on ¼ watt, made of scrap TV antenna parts. The only antenna I have ever had to purchase is a satellite dish, because I can't build parabolic reflectors. I am currently running a 265-foot dipole fed with ladder-line and an antenna tuner. My next will be a 130-foot square horizontal loop. Having 5½ acres of trees helps!
You can string up a wire just about anywhere and get a good signal on shortwave. Fifty feet of very fine wire, strung along the ceiling on thumbtacks, will give you much more signal than the ridiculous telescopic whip that comes with portable radios. Telescopic antennas are extremely too short for shortwave frequencies!
There is one fundamental rule for receiving antennas: It must be at least ¼-wave long at the lowest frequency you plan to use. Thus, if your lowest regular listening is on 3315 kHz, your wire should be 70 feet long - minimum. Obviously, the 5-foot whip antenna on your shortwave is just a bit too short. For much better performance, it shoud be ½ wave long on your lowerst frequency (a Zepp). Multiwire dipoles are best of all. Avoid all "trap" antennas.
Let's design a decent longwire antenna for general shortwave listening. We will want to listen down to 2500 kHz (2.5 MHz), then analyze its performance.
The formula for determining the ½ wave length of wire is: 468 ÷ f (MHz) = feet.
In our example, 2.5 MHz is our lowest frequency, therefore: 468 ÷ 2.5 = 187.2 feet of wire. That's a lot! No room!
Let's say we'll design it for 5 MHz, and be willing to accept slightly reduced performance down to 2.5: 468 ÷ 5 = 93.6 feet of wire. We can handle that.
Longwires are usually strung up something like this:

This arrangement keeps constant tension on the wire while allowing the tree to sway without breaking the wire.
Electrical suppliers carry 500-foot rolls of #14 stranded THHN wire (about $35). Electricians frequently have scraps and partial rolls. Farm supply stores carry #17 aluminum fence wire (about $12 for ¼-mile roll). Wal-Mart carries 100-foot rolls of telephone house wiring (about $10) (solder all 4 strands together at both ends). Any wire will do -- but some will last longer than others. Stranded, insulated wire (#14 green THHN) is best.
This page details the installation of a relatively safe, good-performing, long-lasting shortwave antenna. The #1 rule is: Where you scrimp on quality is where it will break!
Yes, you can simply hang a wire out the window. But experience shows that a properly installed antenna that is mechanically and electrically sound, and a properly grounded radio, will consistently yield better performance and reliability. It really is worth the extra effort -- if you are a frequent, serious shortwave listener.
Wires should be insulated, stranded #18 - #14. A jack may be soldered on to plug into your radio. If the radio has no Ext. Ant. jack, solder an alligator clip to the antenna wire and clip it to the telescopic whip.
Usually, directly away from overhead power lines.
If the lines run across the back of your property, go up the back of the house, over the roof, to a tree in the front yard. If the lines run across the front of your property, go up the front (or side) of the house, over the roof, to a tree in the back yard. You can also run a wire along eaves and/or the top rail of a wooden privacy fence.
Run the longwire as far from, and as perpendicular to, the power lines as possible. This will help reduce noise. If you have buried power lines, run your antenna any way you like. In the USA, pointing your longwire northeast will help bring in European stations in the daytime, on the higher shortwave bands.



As previously stated, a ½ wave antenna radiates off of the sides, perpendicular to the wire. Longwire antennas radiate toward the far end of the wire. Let's look at what happens to the directivity pattern of our 94-foot wire.
As we dial up the frequency, the pattern of the antenna changes. The following diagrams show relative signal strength, looking down from the top. As the frequency goes up, the two lobes split into 4, then get stronger toward the far end of the wire. The patterns are like doughnuts circling the wire - thus, the patterns extend upward as well as long the ground.
In each case, the wire is fed from the left end. Increasing the frequency has the same effect on the pattern as lengthening the wire. The two side lobes squash and divide into four (at 1 wave), then the directivity shifts toward the far end of the wire. They then come together as one long lobe. This is the primary negative design characteristic of longwire antennas.
You should keep these patterns in mind when stringing up a single-wire antenna, so that, at your favorite frequencies, a lobe is pointing toward the right part of the world. Other (slightly more complex) antenna designs avoid this problem of changing directivity by using several antenna elements of different lengths, as we shall see on the following page.

It's important to note that the height of the antenna above ground also affects the pattern. Lower antennas have higher radiation angles - thus, more energy is wasted into the sky. It would be nice to be able to get our antenna ½ wave above ground at the lowest operating frequency. This would mean that our 100-foot long antenna should be 100 feet high, but alas, this is hardly practical -- unless you have some old pine or redweed trees on your property. The general rule of antenna height is: higher = better. Surprisingly, however, even the top wire of a fence will do quite well.
You can bend the antenna wire around corners, but it's better if you do not. Try to keep most of the wire in a straight line.
The easy way to overcome undesirable directivity shift is to design a multi-band antenna. The simplest multi-band antenna for shortwave listening is the multi-wire. This may be a Zepp (end-fed) or a dipole (center-fed).
The theory is simple: if a ½ wave antenna is best, then we need several of them, at different lengths, tuned to the various shortwave bands. Since the ½ wave element is most efficient, the one whose length is nearest our current frequency will predominate, while the others are relatively inactive. The top wire is the longest, and we use it to suspend the lower, shorter ones.

Note that ½ wave antennas are also resonant at 1½ waves. This is called "third-harmonic" operation. Knowing this, international radio treaty makers long ago placed the shortwave broadcast bands at convenient locations. The result is that we can use 4 wires to pick up 8 shortwave bands with excellent efficiency. Below are the calculations for this antenna (frequencies shown are approximate band centers for the meter bands shown):
| Wire | Fundamental | 3rd Harmonic | Length |
|---|---|---|---|
| 1 | 3.25 MHz (90 meter) | 09.75 MHz (31 meter) | 468 ÷ 3.25 = 144' 0" |
| 2 | 3.95 MHz (75 meter) | 11.85 MHz (25 meter) | 468 ÷ 3.95 = 118' 6" |
| 3 | 5.10 MHz (60 meter) | 15.30 MHz (19 meter) | 468 ÷ 5.10 = 91' 9" |
| 4 | 5.90 MHz (49 meter) | 17.70 MHz (16 meter) | 468 ÷ 5.90 = 79' 3" |
The wires are spread 3-4 inches, held in place with simple Plexiglass spacers. Just cut a few pairs of the acrylic about 2 by 12 inches and run a few small bolts through them, pinching the wires between. Obviously, you stretch the whole mess out on the ground, assemble it, then pull it up with your rope and pulley.
The wires all join at the peak of the house and connect to the center wire of 50-ohm coax (RG-58). The shield of the coax connects to a wire which runs down to your ground rod. Solder and tape all connections to keep water out. Don't forget the lightning arrestor.
If you have a big tree about 170 feet away, this antenna will give fabulous results.
The next design is a center-fed multiwire dipole (below). The big advantage is, since the array is supported at the center, you can use lighter (cheaper) materials, since each span is only 72 feet long. Also, using two tall trees puts more of the antenna higher off of the ground.
The only way you that may further improve on this design is to raise it higher. If you have thousands of dollars laying around, you can string it across three 100-foot towers - and probably get a write-up in a national magazine.
Ok - enough dreaming. Let's get realistic here. We have no trees, and dozens of property association rules. We need a good shortwave antenna in the attic.

Indoor, or attic, antennas have several advantages: (1) no rain, no corrosion, no wind damage, (2) little possibility of lightning strike, (3) no problems with property association communists, and (4) no need for trees or other external supports.
It's possible to make a multiwire dipole out of 4 or 5 conductor TV antanna rotator cable. This type is a flat ribbon wire. Since it isn't very strong, it must be supported at frequent intervals. This means we can string it through our attic, diagonally, hanging it on the undersides of the rafters with bent nails.
Here comes the compromise: We will have to forego ½ wave operation on the lower bands. Below are the calculations for this antenna, which uses 5-conductor rotator ribbon wire (frequencies shown are approximate band centers for the meter bands shown):
| Wire | Fundamental | 3rd Harmonic | Overall Length | Per Leg |
|---|---|---|---|---|
| 1 (top) | 05.90 MHz (49 meter) | 17.70 MHz (16 meter) | 468 ÷ 05.90 = 79' 3" | 39' 6" |
| 2 | 07.20 MHz (41 meter) | 21.60 MHz (13 meter) | 468 ÷ 07.20 = 65' 0" | 32' 6" |
| 3 | 09.75 MHz (31 meter) | 29.25 MHz (10 meter) | 468 ÷ 09.75 = 48' 0" | 24' 0" |
| 4 | 11.85 MHz (25 meter) | 468 ÷ 11.85 = 39' 6" | 19' 9" | |
| 5 | 15.30 MHz (19 meter) | 468 ÷ 15.30 = 30' 6" | 15' 3" |
Since this is a dipole (center-fed), we need to buy ((79.25 + 30.5) ÷ 2) + 2 = about 55' 2" of ribbon (leaves an inch on each end for connection). We then measure, mark, cut, and peel it all apart to make the two halves of the dipole (notice that the center wire is cut twice - 7 feet is discarded) (cut each conductor by pushing a small screwdriver through it):

If you can't get in the attic, you can lay it on top of the roof. Bring the coax out through a ridge vent, if possible. Waterproof the connections. NOTE: If you don't want to build it, Radio Shack sells this type antenna for about $35 (+ coax).
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Last but not least, let us examine simple wire antennas which may be designed and used indoors, for little or no cost. Such are need by renters and apartment dwellers, and are always better than the way-too-short telescopic whip antenna.
The simplest antenna which will drastically increase the amount of signal power (compared to the telescopic whip) is merely a much longer monopole -- i.e., 40 to 80 feet of fine wire, thumbtacked to the ceiling and connected to the radio.
You will be amazed when comparing a signal on the telescopic whip and the fine ceiling wire. When connecting the wire, the signal meter will jump way up. You will be able to pick up weaker signals, and will have less problems with fading. It will also pick up a lot more static and noise from electrical devices in your house...
How much better is the full-sized, outdoor, multiwire dipole antenna? On the strong signals, no better. But on the weakest ones, considerably better. If you regularly seek out weak signals, try to get a multi-wire up outdoors -- and considering purchasing a nice antenna tuner and an active audio filter. Mainly, a large outdoor antenna will have a much better singal-to-noise ratio. It will pull in more radio signal than electrical interference.
Almost all indoor antennas (including those expensive "active" ones) will pull in lots of electrical noise, requiring you to go around and turn off TVs, VCRs, computers, dimmers, florescent lights, and ceiling fans -- before your favorite shortwave radio program comes on. Even worse, the electrical interference may come from street lights or even neighbors -- sources you cannot control. This is why you should put up as big an antenna as possible, to get the induced signal power over the noise level.
These are all the crazy "try it and see if it works" non-designed antennas. They usually work better than the telescopic radio antenna, but worse than the indoor longwire.
Like every other hobby, shortwave listening attracts sundry gadgets. Some of these are quite useful, some are not, and some are for specialty purposes only.
These connect between the antenna and the radio.
With an "active" antenna, the idea is to take the usual 5-foot telescopic whip and add a very sensitive amplifier -- thus adding another input stage to the radio, which is, presumably, more sensitive than the radio itself. The ads promise that they will work as well as a 60-foot longwire. Baloney! Modern portable shortwave radios, like Sony, Grundig, and Sangean, are as sensitive as any active antenna. Therefore, adding an active antenna will not improve anything. In other words, do active antenna makers have access to more sensitive transistors than the radio manufacturers?
However, if you do buy an active antenna, or preamplifier, make sure it has a "helical" filter, and relatively impressive "intermodulation suppression" specifications. This simply means that it will feed a relatively clean signal to the radio, not a jumbled bunch of amplified garbage from nearby stations.
A preamp is simply a way to make your existing antenna "active." Same as above. May be indicated for very old radios with poor sensitivity.
A prescaler is a sort of antenna tuning device. You tune your radio to the desired frequency, then you tune the prescaler to peak the signal. These are good devices for improving the selectivity and signal-to-noise ratio, and are particularly helpful of cheap radios. Most prescalers also include a preamp, but some are passive.
My recommendations: Ignore active antennas. Put up some wire. Ignore preamps. Get a modern radio which has all the preamp built-in that you'll ever need. Get a passive prescaler or random-wire tuner if needed. MFJ makes a nice collection of such things. Look for their ads in radio magazines, and order a catalog. www.mfjenterprises.com.
These process the audio (speaker) output in some desireable way. You must plug them in between the radio's speaker (earphone) jack, and an external speaker (or headphones) which you have to purchase separately.
Audio filters allow you to "narrow" the bandwidth of the audio -- like turning a "Tone" control way down, but with more sophisticated control. It is a nice add-on, if you listen to CW (morse code), or if you regularly get interference from stations on nearby frequencies (like 5 kHz away) from your favorite stations. You can filter out the "hetrodyne" squeal -- but they will not filter out electrical noise. Be not deceived!
If you get an audio filter, make sure it covers what you want to do, like shortwave broadcast clean-up, or single-sideband, or CW (morse code) copy. Each of these requires different types of filtering. Some units have it all in one box, and of course, cost more. Ask an Amateur (Ham) radio operator -- we Hams read the radio magazines and keep up with these things.
These connect to the speaker output of the radio, and usually to the serial input of a computer. They are used to receive and decode CW, radioteletype (many varieties), and weather fax transmissions.
My recommendations: The cheap ones ($100) are garbage, so don't waste your money. The better ones which cost several thousand dollars work very well. You need to have a real need-to-know (like surveillance work) to justify the expense. Even then, most of the signals are encrypted, and it's illegal to intercept them.
Lots of “digital” modes can now be demodulated (and transmitted, if you have the license) using only a computer with a sound card and the appropriate software. See my web article Getting Started in Digital Modes for info and many links.
This relatively small, strange-looking antenna may be used outdoors or in the attic, and is suitable for VHF and UHF transmitting and receiving. It has all these "way cool" features:
This antenna is excellent for scanners, FM-band micro-broadcasters, VHF/UHF business, law enforcement, GMRS, FRS, TV (7 and above), and VHF/UHF ham bands. It will do all of the above without ever taking it down to retune it. Just build it right (strong and weatherproof), put it up on a well-guyed mast, then use it for everything above shortwave.
These plans use dimensions which will set the lower cutoff frequency below 88 MHz, so that it may be used for FM micro-broadcasting. For cutoff to include:
Lowest Band: Cutoff: "L=":
Eliminating the lower bands simply makes a smaller antenna, which is easier and cheaper to build and support. The antenna has a considerable surface area and wind load, therefore should be placed upon a well-guyed mast. The guys may attach immediately below the skirt of the antenna, without any need for insulators.
Ideally, the discone should be made of copper or aircraft aluminum ("Alclad") sheet metal, but a heavy screen (¼-inch galvanized hardware cloth) will work as well, with lower wind loading and less cost.
Before erecting the discone, test it with a ohmmeter. The center-to-shield of the coax should not be shorted. The shield to cone (skirt) should show short (0 ohms) and center-to-disc should of course show short.
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It's a pretty good idea to plan and graph any proposed erection which could fall into power lines -- as opposed to killing yourself like several people per year do. This is easy to do using graph paper or a computer drawing program with a grid.
In the following example, a 40-foot aluminum tower will be anchored to a tilting base plate, bolted to a concrete pad, then attached to the house gable at 13 feet, then guyed near the top (39 feet) with one set of three 3/16" braided steel cables with turnbuckles. Up to 20 feet of 1½" heavy-wall steel mast pipe (commercial fence-post stock) will stand atop the tower, giving a height of 60 feet. The upper pipe mast will be guyed with three regular 7-strand galvanized guy wires.
Positioning the power line at the proper height and distance, then drawing an arc, will show where the tower must be placed, and the maximum height at that location, that will clear the lines.
To further eliminate the possibility of a line strike, the tower may be guyed with an additional safety cable extending away from the power lines. This will ensure that the top pole would topple before the tower, thus reducing the arc of fall to 40 feet. This failure mode assumes tornadic wind conditions. If it would take tornadic winds to topple the tower, the same would topple the power lines and poles! Thus, well-anchored steel cables, rated at over 2500 pounds working tensile, will totally prevent a power line strike.
Most electrocutions occur during tower erection. When pulling up an assembled tower or pole, at the very least a safety rope should be tied to the top, extending perpendicular, away from the power lines, tied securely to a tree trunk. If the tower falls during erection, the safety line will swing it down parallel to the power lines. Never try to man-handle a tower into position without safety lines !! One extra helper is ten times better!
No antenna, pole, mast, or tower should ever be raised alone, nor by unsupervised children.
Well, that’s all for now, folks! I hope this article has been helpful. If you wish to continue learning antenna theory and construction, obtain a few good books on the subject. I recommend you start with The ARRL Antenna Book.
73, de KV5R
Please see my new articles on KV5R.COM, too!
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Copyright (c) 2002, 2007 by Harold Melton, KV5R. All Rights Reserved. |
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