Antennas, to quote a friend, are one of life’s eternal mysteries. “All I’m totally certain of is that any antenna is better than no antenna and the antenna should preferably erected as high and be as long as is possible or desirable”. Here we will discuss the very basics of antennas. Remember that thought: these are just some introductory antenna basics. Each type of antenna will eventually have its own page. In particular I would commend everyone to read my page on earth dangers. I think it ought to be compulsory reading.
The basic antenna
The most basic antenna is called “a quarter wave vertical”, it is a quarter wavelength long and is a vertical radiator. Typical examples of this type would be seen installed on motor vehicles for two way communications. Technically the most basic antenna is an “isotropic radiator”. This is a mythical antenna which radiates in all directions as does the light from a lamp bulb. It is the standard against which we sometimes compare other antennas.
This type of antenna relies upon an “artificial ground” of either drooping radials or a car body to act as ground. Sometimes the antenna is worked against an actual ground – see later.
Depending upon how the antenna is orientated physically determines it’s polarisation. An antenna erected vertically is said to be “vertically polarised” while an antenna erected horizontally is said (not so surprising) to be “horizontally polarised”. Other specialised antennas exist with “cross polarisation”, having both vertical and horizontal components and we can have “circular polarisation”.
Note that when a signal is transmitted at one polarisation but received at a different polarisation there exists a great many decibels of loss.
This is quite significant and is often taken advantage of when TV channels and other services are allocated. If there is a chance of co-channel interference then the license will stipulate a different polarisation. Have you ever noticed vertical and horizontal TV antennas in some areas. Now you know why.
Technically, antenna impedance is the ratio at any given point in the antenna of voltage to current at that point. Depending upon height above ground, the influence of surrounding objects and other factors, our quarter wave antenna with a near perfect ground exhibits a nominal input impedance of around 36 ohms. A half wave dipole antenna is nominally 75 ohms while a half wave folded dipole antenna is nominally 300 ohms. The two previous examples indicate why we have 75 ohm coaxial cable and 300 ohm ribbon line for TV antennas.
A quarter wave antenna with drooping quarter wave radials exhibits a nominal 50 ohms impedance, one reason for the existence of 50 ohm coaxial cable.
The quarter wave vertical antenna
The quarter wave vertical antenna is usually the simplest to construct and erect although I know a great many people who would dispute that statement. In this context I am speaking of people (the majority) who have limited space to erect an antenna.
In figure 1 we have depicted a quarter wave vertical antenna with drooping radials which would be about 45 degrees from horizontal. These 45 degree drooping radials simulate an artificial ground and lead to an antenna impedance of about 50 ohms.
A quarter wave vertical antenna could also be erected directly on the ground and indeed many AM radio transmitting towers accomplish this especially where there is suitable marshy ground noted for good conductivity. An AM radio transmitting tower of a quarter wave length erected for say 810 Khz in the AM band would have a length of nearly 88 metres (288′) in height.
The formula for quarter wave is L = 71.25 metres / freq (mhz) and in feet L = 234 / freq (mhz). Note the variance from the standard wavelength formula of 300 / freq. This is because we allow for “velocity factor” of 5% and our wavelength formula becomes 285 / freq.
When a quarter wave antenna is erected and “worked” against a good rf ground (called a Marconi Antenna) the earth provides a “mirror” image of the missing half of the desired half wave antenna.
In figure 2 above where I have depicted the Marconi Antenna imagine a duplicate of the quarter wave antenna being in existence from the top of the ground and extending down the page. This is the mirror image.
Half wave dipole antenna
The half wave dipole antenna becomes quite common where space permits. It can be erected vertically but is more often than not erected horizontally for practical reasons. I gave quite a good example of its use in my paper on radio telescopes from my original site. I have reproduced it in figure 3 below.
Figure 3. – half wave dipole antenna
As with all antennas, the height above ground and proximity to other objects such as buildings, trees, guttering etc. play an important part. However, reality says we must live with what we can achieve in the real world notwithstanding what theory may say.
People erect half wave dipoles in attics constructed of fine gauge wire – far from ideal BUT they get reasonable results by living with less than the “ideal”. A lesson in life we should always remember in more ways than one.
The folded dipole antenna
The folded dipole antenna is probably only ever seen as a TV antenna. It exhibits an impedance of 300 ohms whereas a half wave dipole is 75 ohms and I’m certain someone will be alert enough to ask “why 75 ohms, if figure 3 above is 50 ohms?”.
Within the limits of my artistic skills I have depicted a folded dipole antenna below.
One powerful advantage of a folded dipole antenna is that is has a wide bandwidth, in fact a one octave bandwidth. This is the reason it was often used as a TV antenna for multi channel use. Folded dipole antennas were mainly used in conjuction with Yagi antennas.
The Yagi antenna
The Yagi antenna or more correctly, the Yagi – Uda antenna was developed by Japanese scientists in the 1930’s. It consists of a half wave dipole (sometimes a folded one, sometimes not), a rear “reflector” and may or may not have one or more forward “directors”. These are collectively referred to as the “elements”.
Figure 5. – the Yagi antenna
However in figure 6 below, which happens to be a photograph of a neighbour’s TV antenna, I can clearly point out details of a practical Yagi antenna.
This particular antenna has been optimised for dual band operation. It is designed to pick up both VHF and UHF transmissions. Because I live in a regional of NSW in Australia, TV antennas tend to be single channel types designed either for higher gain or better directivity. Different examples will be presented later.
Figure 6. – a practical Yagi TV antenna
The next three much longer elements form a “phased array” for the VHF band. I am unsure of the function of the three remaining smaller elements, information is quite scant here but one would certainly be a UHF “reflector”. Likely the other two also fulfill this function also.
Note: This is a horizontally polarised antenna and is orientated roughly NNW, 315 degrees.
You will notice the effect of very strong storms from the sea have had in bending the second larger elements. In my locality storms are a problem but not as much as roosting parrots such as large sulphur crested cockatoos.
UHF Yagi antenna
In the photograph in figure 7 below you can see a classic UHF Yagi antenna. It has a total of nineteen “elements” comprising seventeen “directors”, a fancy folded dipole with a “low-noise mast head amplifier” and a “reflector”.
Figure 7. – a vertically polarised UHF Yagi antenna
This is the very same antenna I was suggesting to be used in the radio telescope array I depicted in figure 5 above.
Stacked half wave dipoles or a collinear array
To the left of the photograph are the “reflectors” and to the right are the four vertically stacked half wave dipoles. The wires connecting each half wave dipole are done in a “phased way”. This comprises a collinear antenna array and is so arranged for improved gain.
Note this antenna is horizontally polarised.
The loop antenna comes in an amazing number of configurations. It is a “small space” antenna and although extremely inefficient is capable of surprising results. In receiving applications the loop antenna works on the principle of the “differences” in voltages induced by the current flowing in the sides of the antenna. As you might imagine these difference voltages can be extremely minute in amplitude and any loop antenna usually requires an associated amplifier capable of at least 25 dB power gain following it.
One example of a shielded loop antenna is taken from my tutorial on mobius winding techniques is shown in figure 9 below.
This is the general loop antenna which has one interesting characteristic. It responds well to signals arriving in one direction, either from the left hand side of your computer screen or the right hand side of your computer screen for the loop shown in figure 9 (b) above. Signals from either your face or from behind your monitor would produce equal signal currents from both sides of the loop and consequently produce no difference voltage output.
Technically speaking, a loop antenna responds to the magnetic field rather than the electric field.
Rather than being omnidirectional (as a whip antenna would be) the loop antenna responds to the cosine of the angle between its face and the direction of arrival of the electromagnetic wave. This actually produces a figure eight pattern, which for receiving presents no probems. The addition of a small whip antenna in conjuction with proper phasing allows the direction ambiguity to be resolved and we have an antenna relatively ideal for direction finding.
The most common loop antenna you will encounter is the loopstick antenna [in the U.K. it is referred to as a “ferrite rod antenna”] built into portable receivers. In figure 10 below is the AM and shortwave loopstick antenna in a Sanyo model RP2127 MW / SW receiver (it’s old).
Figure 10. – AM and shortwave loopstick antenna
As an experiment you might, if you have a loopstick antenna radio available, tune to a weak station and rotate the radio around 360 degrees. You should notice two points 180 degrees apart where the signals seem to be the strongest and similarly notice two other points 180 degrees apart where the signals seem to be the weakest – these are called “nulls”. This is the aid to “Radio Direction Finding – RDF”.
Using the Small Loop Antenna
Joseph J. Carr, Universal Radio Research
Small loop antennas have an overall wire length < 0.15 λ. They exhibit deep nulls perpendicular to the plane of the loop, and broad maxima off the ends of the loop. The pattern of these small loop antennas is a variant of the classic “Figure-8” pattern. Although the loop has less gain than a dipole, the radiation pattern and small size make the antenna quite useful for certain situations…
A novel Bicycle Rim Wheel Loop Antenna for 20 metres
Now here’s a real novel idea using a junked bike wheel. Real amateur creativity. Bicycle Rim Antenna for 20 Metres by VK2ZAY, a fellow Australian so it has to be good [G].
The K9AY Terminated Loop — A Compact, Directional Receiving Antenna
Wish you had enough room for an effective low-band receiving antenna? You do! This four-direction system fits in a 30-foot circle!
By Gary Breed, K9AY
Low-band operators are always looking for ways to improve their hearing. As a low-band fan, I was impressed with the EWE antenna developed by Floyd Koontz, WA2WVL. [1, 2] Koontz shows us how to build a compact, directional antenna—a design that quickly became very popular. But when I sat down at the computer to figure out the best way to install my own EWEs, a surprising new design emerged from my modeling experiments…
Terminated Tilted Folded Dipole
Now here is a little gem. The terminated tilted folded dipole is bound to give a “rush of blood to the head” of any avid DX’er (that means long distance -dx- receive / transmit enthusiast).
The terminated tilted folded dipole is somewhat similar to the half wave folded dipole in figure 4 above yet the claims for its performance are quite astonishing. The terminated tilted folded dipole is claimed to have a bandwidth of something like 5 or 6 to one, been extensively tested and adopted by the US Navy, easy to construct from readily available materials and, has a feedpoint impedance of around 300 ohms.
Figure 11. – Terminated Tilted Folded Dipole
Each leg “A” = [ 2 X pi ( 15.25 / Fo )] and;
Distance “B” = [ 2 X pi ( 0.915 / Fo )]
where in both instances 2 X pi = 6.28 and Fo is in Mhz.
There seems to be some debate about the exact formula, my friend L. B. Cebik (see next) says:
Conclusion on antenna basics
The reason there has been emphasis on TV antennas is simply because nearly everyone can look at examples in their own locality for comparison. At TV frequencies the physical dimensions are such I can offer practical examples with photographs.
The same basic principles apply at HF and LF although physical sizes tend to be totally impractical.