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ASOC Restricted course Section A 📡 Aerials and Feeders

Common Transmitting and Receiving Aerials

Dipole, ground plane, vertical, Yagi, loop, long wire and the microwave dish - pattern, gain and where each one earns its place.

  • Lesson 23 of 36
  • 13 min read
  • Syllabus A(vii)

There is no best aerial, only the best aerial for a band, a space and a purpose. A rotatable Yagi is a magnificent thing on 20 m and an absurdity on a Mumbai balcony; a rubber duck is hopeless from indoors and exactly right clipped to your belt at a rally. This lesson goes through the aerials the syllabus names, and for each one asks the same four questions: what is it, what shape does it radiate, what does it feed at, and what does it buy you. The examiner asks about the Yagi more than all the others put together, so that section is the long one.

A flat concrete roof with a low parapet. A guyed vertical aerial is bolted to the parapet with a metal bracket; three guy wires run down to anchors. Coaxial cable leaves the feedpoint, runs down the wall and along the roof under cable clips, past a black plastic water tank on a raised plinth. Low-rise apartment blocks and palm trees fill the background.
A whole VU3 station's aerial system: one vertical, three guys, a bracket on the parapet and a coax run held down with clips. Nothing here costs much, and the cable management is doing as much work as the aerial.

Reading a radiation pattern before we start

A radiation pattern is a polar graph of relative field strength against direction: distance from the centre means signal strength that way, not distance in kilometres. Two slices are usually shown — the azimuth plan view looking down, and the elevation slice from the side. Choose an aerial in the gallery below and its pattern is drawn on the same grid every time, with the half-wave dipole left as a faint outline behind it so you can see what has been given up to gain what.

Radiation patterns same grid, six aerials

90° 180° 270°
Azimuth — the plan view, looking down on the aerial.
zenith 90° horizon horizon 0°
Elevation — a vertical slice, side view.

selected aerial half-wave dipole, for shape comparison

Typical gain
Front-to-back
Polarisation
Feed impedance

 

 

Every outline is plotted from the standard free-space expression for that aerial, as relative field strength on a linear scale. It shows the shape honestly; it is not a measured range plot, and no real aerial escapes the influence of the ground under it.

Keep one principle in mind while you play with it: an aerial makes no power. Every decibel of gain in one direction has been taken away from some other direction. The feed impedances quoted below matter because the feeder has to be matched to them, which is the subject of the next lesson.

The dipole family

Half-wave dipole

The reference against which everything else is measured, and the aerial most Indian amateurs start with. Two legs of wire totalling 142 ÷ f (MHz) metres, fed at the centre, about 73 Ω, pattern a figure of eight broadside to the wire with deep nulls off the ends, gain 0 dBd by definition. Cheap, predictable, and hard to beat for the money. The previous lesson covers its cutting and its current distribution.

Inverted V

The same dipole with its centre insulator hoisted to the top of a single mast and both legs sloping down to low anchor points, typically at an included angle of about 120 degrees. Its decisive advantage is mechanical: it needs only one high support instead of two, which on a small plot or a flat roof is often the difference between having an aerial and not having one. The sloping legs fill in the end nulls, so the pattern becomes more nearly omnidirectional, and they drop the feedpoint impedance conveniently towards 50 Ω.

Folded dipole

A half-wave dipole with a second conductor joined across both ends and spaced a few centimetres away, the feeder connecting to a break in the middle of one side only. The current now divides between two conductors, so for the same radiated power the feedpoint sees half the current at the same voltage — and impedance goes up four times:

4 × 73 Ω ≈ 300 Ω

Four times seventy-three ohms is about three hundred ohms.

That is a direct match to 300 Ω twin lead, which is why television aerials use it, but what matters more to an amateur is bandwidth: the fatter effective conductor keeps the SWR usable right across a wide band like 10 m instead of climbing at the edges. It is also a robust, DC-continuous loop, so static cannot build up on it in a dusty pre-monsoon wind. Both are why it is the standard driven element in a good Yagi.

Verticals

Quarter-wave ground plane

A single quarter-wave radiator standing on a ground plane — either real earth with buried radials, or three or four quarter-wave wires at the base of a mast-mounted one. The ground supplies the mirror image of the missing half, so it behaves as half a dipole and feeds at about 36 Ω with horizontal radials, rising towards 50 Ω when they are sloped down. The pattern is a circle in azimuth — omnidirectional, with no nulls to exploit — and low in elevation, which makes a vertical a good DX aerial and a poor one for local work on 40 m. On a vehicle the bodywork is the ground plane, which is why a mag-mount in the middle of the roof beats one on the boot lid. The whole thing lives or dies by its radials: two rusty ones make a heater, a dozen good ones make a DX machine.

The 5/8 wave vertical

Stretch the radiator to five-eighths of a wavelength and the vertical pattern is squashed further down towards the horizon, giving roughly 3 dB over a quarter-wave. Five-eighths of a wavelength is not a resonant length, so the feedpoint is strongly reactive and a loading coil at the base is needed to cancel that out before the feeder sees anything usable. This is the standard 2 m mobile and base whip in India: a 5/8 on 145 MHz is about 1.3 m of stainless steel, it clears every rooftop water tank in the neighbourhood, and its low angle is exactly what you want for reaching a repeater 40 km away.

The Yagi-Uda array

Invented at Tohoku University by Uda and published in English by Yagi, this is the directional aerial everyone recognises from a rooftop television installation. Only one element is connected to the feeder — the driven element, usually a dipole or folded dipole. The rest are parasitic: they carry current only because the driven element induces it in them, and their length sets the phase of that current.

boom reflector 0.55 λ driven 0.5 λ feeder director 1 0.45 λ director 2 beam back
A four-element Yagi seen from above. The reflector is about 5% longer than the driven element and sits behind it; the directors are shorter and sit in front. Only the driven element is connected to the feeder. The beam fires towards the directors.
ElementLengthPositionBehaves as
Reflector≈ 0.55 λ — longerBehind the driven elementInductive; it pushes energy forward
Driven element≈ 0.5 λFed by the transmitterResonant
Director(s)≈ 0.45 λ — shorterIn frontCapacitive; they pull energy along

Element spacing is usually 0.15 to 0.25 wavelengths, and a Yagi normally has exactly one reflector — a second one adds almost nothing — but as many directors as the boom will hold. Two figures describe how well it works: gain, its advantage over a dipole in the forward direction, and front-to-back ratio, how much weaker it is behind than in front. Both improve as elements are added, but what really buys gain is boom length: cramming more elements onto a short boom gains you very little. As a rough guide, three elements give around 5 dBd and a doubling of boom length is worth roughly another 2.5 dB, with diminishing returns all the way.

Why does it have gain at all? Not because it radiates more power — it cannot. It concentrates the radiated power into one direction. That is the examiner's own phrasing and it is the whole explanation, and it also explains the front-to-back ratio: the energy in the forward lobe is the energy missing from the back.

Cubical quad

A quad element is a full-wavelength loop of wire bent into a square on a fibreglass or bamboo spreader, so each of the four sides is a quarter wavelength. Like a Yagi it uses one driven loop with a parasitic reflector behind it, and directors may be added. It gives gain comparable to a Yagi with one more element, at a lower angle of radiation for the same mast height — the classic reason for choosing a quad on a crowded plot. It is lighter than a Yagi, but presents far more surface to the wind and is fussier to keep in one piece through a monsoon.

Loops

The full-wave loop above is a transmitting aerial. A small receiving loop is a different animal: a few turns of wire much smaller than a wavelength, often tuned with a capacitor. It responds chiefly to the magnetic component of the wave, which makes it far less sensitive to the electrical noise that saturates an Indian urban street — switch-mode chargers, LED drivers, unshielded cables. Its pattern is a figure of eight with very sharp nulls through the plane of the loop, so rotating it can null a single interfering source almost completely. That null, not gain, is the point: it is the classic direction-finding aerial, and with poor gain it stays a receiving aerial rather than a transmitting one.

Long wire and end-fed half wave

A long wire means a wire genuinely long compared with the wavelength — one wavelength or more, not merely a long piece of wire. Fed at one end against an earth or counterpoise through an ATU, it works on many bands at once, which is its whole appeal to someone who cannot put up several dipoles. The price is a pattern that breaks into multiple lobes, sharper and less predictable as the wire lengthens, and an earth that must be good or the losses are severe. Two long wires in a horizontal V, fed at the apex, make a V-antenna, which fires along the bisector and is genuinely directional.

An end-fed half wave is a different idea: exactly half a wavelength of wire, fed at a voltage maximum, so the feedpoint impedance is several thousand ohms instead of 73. A step-down transformer at the feedpoint — a 49:1 is common — brings that down to something coax can carry. It needs no radial field, only a short counterpoise, which is why it has become the favourite portable and balcony aerial.

Parabolic dish

At microwave frequencies a reflector many wavelengths across can be used, and a parabola focuses everything arriving parallel to its axis onto a single feed point. Gain depends on how many wavelengths wide the aperture is:

G ∝ (π D ÷ λ)² — gain rises with the area of the dish and with the square of the frequency

Gain is proportional to the aperture measured in wavelengths, squared.

Double the diameter and the gain goes up four times, or 6 dB. Keep the dish and double the frequency and the gain also goes up four times, because the same metal is now twice as many wavelengths across. That relationship is why dishes are practical only at SHF and above: a dish with useful gain on HF would be hundreds of metres across.

Helical

A helix wound on a supporting cylinder in front of a ground-plane reflector, with a circumference of roughly one wavelength, radiates along its axis with circular polarisation — the E field rotates as the wave travels. That makes it indifferent to the orientation of the far-end aerial, exactly what satellite work needs when the spacecraft is tumbling. It is broadband and easy to build, and both ends must use the same hand of rotation: right-hand circular does not talk to left-hand circular.

Whips and the rubber duck

A whip is a vertical rod, usually a quarter wave, used where nothing larger will fit — on a vehicle, or a rooftop with no room for radials. For HF it is almost always shortened and brought back to resonance with a loading coil, and it works, after a fashion.

The rubber duck on your handheld takes that idea to its limit. A quarter wave on 2 m is about 49 cm and nobody will carry that on their belt, so the duck is a heavily shortened, coil-loaded aerial a fraction of the length: low radiation resistance, unchanged loss resistance, and several decibels thrown away against a full-size whip. The loss is not theoretical. Clip a full-length telescopic whip to the same handheld, or run a few metres of coax to a 5/8 on the terrace, and stations that were unreadable become comfortable copy. If you buy one accessory for a new handheld, buy an aerial.

The artificial aerial — the one you must own

A dummy load, which the rules call an artificial aerial, is a non-inductive resistor of 50 Ω in a housing that can get rid of the heat. It presents the transmitter with a perfect match while radiating essentially nothing, so you can tune up, measure power, test a repair or demonstrate a rig without putting a signal on the air. It is the only “aerial” the licence conditions actually oblige you to have.

All of them at a glance

AerialPatternTypical gainFeed ZWhere it earns its place
Half-wave dipoleFigure of eight, broadside0 dBd73 ΩThe first aerial, and the reference for all gain figures
Inverted VNearly omnidirectional≈ 0 dBd≈ 50 ΩOnly one high support needed — the small-plot dipole
Folded dipoleSame as a dipole0 dBd≈ 300 ΩWide bandwidth; matches 300 Ω ribbon; Yagi driven element
Quarter-wave ground planeOmnidirectional, low angle≈ −1 dBd36 Ω, or 50 Ω with sloping radialsDX and all-round coverage with no rotator
5/8 wave verticalOmnidirectional, lower angle still≈ 3 dB over a quarter-waveNeeds a base loading coilThe standard 2 m mobile and base whip
Yagi-UdaOne forward lobe, small back lobe5 dBd upwards with element countMatched to 50 Ω at the driven elementGain and front-to-back where you can rotate it
Cubical quadLike a YagiSimilar to a Yagi with one more element≈ 50–100 ΩLow angle from a low mast
Small receiving loopFigure of eight with very sharp nullsNegativeTuned, matched locallyLow-noise receiving and direction finding
Long wireMultiple lobesModest, unpredictableHigh; needs an ATUMany bands from one wire and one earth
End-fed half waveLike a dipole≈ 0 dBdSeveral kΩ, via a 49:1 transformerPortable and balcony work; no radial field
Parabolic dishVery narrow pencil beamTens of dBSet by the feedMicrowave only — SHF and above
HelicalAxial beam, circular polarisation10–15 dBi typicalBroadband, near 140 ΩSatellites and any tumbling far end
Rubber duckRoughly omnidirectional, poorSeveral dB below a quarter-wave whipMatched by its loading coilPortability, and nothing else
Dummy loadNone — it must not radiate50 Ω resistiveTesting, tuning, and the licence conditions

Practice

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