Halo antenna

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Typical halo antenna construction. The round tuning plates are tuned for resonance and omitted in some designs. The small box contains a small trimmer capacitor used to fine-tune the gamma match arm.
Connection diagram for a gamma matched halo antenna.

A halo antenna, or halo, is a  1 /2 wavelength dipole antenna, which has been bent into a circle with an electrical break directly opposite the feed point. The dipole ends are close, but do not meet, and may have an air capacitor between them to adjust the antenna's resonant frequency. If mounted horizontally, this antenna's radiation is approximately omnidirectional and horizontally polarized.

File:Halo geometry.png
A "folded dipole" type of halo. Gain along Y axis 1.2 dBi, gain along Z axis −1 dBi, gain along X axis −1.7 dBi. Fed at the center of the bottom conductor (at the red mark; feed-line not shown), supported at the center of the top conductor which is at ground potential for RF. This is similar to the original halo patent.[1]

Halo antennas vs. loop antennas

This section contrasts halo antennas with loop antennas which are electrically dissimilar, but can be confused as they all share the same circular shape.

Halo vs. large loops

Although also a resonant antenna, the halo antenna is distinct from the full-wave loop antenna, which is approximately double its size for the same operating frequency. In the case of the halo antenna, each half is about a quarter wavelength long and ends with a current node (zero current and peak voltage) at the break. On the other hand, the two semi-circles of a resonant loop, each being a half wavelength long, end with a voltage node (peak current and zero voltage) opposite the feedpoint, where the semi-circles are connected.

Self-resonant loops with a perimeter of one full wavelength have a radiation pattern which peaks perpendicular to the plane of the loop (along the Z-axis, in the diagram) but falls to zero within the plane of the loop, quite opposite the radiation pattern of a halo antenna. Thus, despite the superficial similarity, these two antenna types behave fundamentally differently.

Halo vs. small loops

A halo antenna is distinct from the small-loop antenna in size,[a] radiation resistance, and efficiency. Their radiation patterns are nearly the same. A halo antenna is a self-resonant antenna: Its feedpoint impedance is purely resistive at the design frequency. A small loop antenna, on the other hand, has lower radiation resistance[b] and is not self-resonant; it requires some form of impedance matching to counter the loop's reactance – in practice, this usually consists of a shunt capacitor.

The distribution of current along the two arms of a halo antenna is similar to the currents along the two arms (also a quarter wavelength long) of a half-wave dipole (see animation), being largest at the feedpoint and dropping to zero at the ends (the gap in the case of the halo). On the other hand, a small loop has a current which is approximately uniform and in‑phase along the conductor. The halo – again like the half-wave dipole – also has voltage peaks at the gap, whereas it is the larger current near the feedpoint most responsible for the radiation produced, with the antenna radiating slightly more towards the split in the loop.[citation needed] The small loop radiates nearly equally in all directions within the plane of the conductor.

Both the halo and small loops' radiation patterns are opposite that of the full-wave loop, being maximum in the plane of the loop, rather than perpendicular to it; halo antennas radiate only a small amount perpendicular to the loop plane, and small loops have no perpendicular radiation at all ("null").

Halos are most often oriented with the plane of the loop aligned horizontally, parallel to the ground, in order to effect an approximately omnidirectional radiation pattern in the horizontal plane. Small loops, on the other hand, are often oriented vertically, to take advantage of the small loop's "null" reception by pointing their "deaf" direction (perpendicular to the loop plane) towards a source of interference.

Mistaken understanding of the halo's gap

Although some writers consider the gap in the halo antenna's loop to distinguish it from a small loop antenna – since there is no DC connection between the two ends – that distinction is lost at RF: The close-bent high-voltage ends are connected capacitively, with a RF electrical connection completed through displacement current. Despite the reversal in voltage, the RF current across the gap is continuous (even though possibly momentarily zero).

The gap in the halo is electrically equivalent to the tuning capacitor on a small loop, although its stray capacitance is not nearly as large as needed for a magnetic loop: Capacitance is not needed since the halo antenna is already resonant, but since some small capacitive coupling is present anyway, the arms of the dipole are trimmed back from 97% of a quarter-wave each to restore resonance. Moreover, the halo ends are often cut even shorter, and the ends edged closer together to increase their mutual capacitance to compensate, to make the radiation pattern even more nearly omnidirectional. The altered pattern has the added improvement of even less wasteful vertical radiation[c] (for a halo mounted horizontally).

Modern vs. original halo designs

Early halo antennas[2] used two or more parallel loops, modeled after a 1943 patent[1] which was a folded dipole[3] bent into a circle.

The double loop design can be extended to multiple, stacked electrically parallel loops. Each additional loop increases the radiation resistance by the square of the number of turns, which broadens the SWR bandwidth, increases radiation efficiency, and to a point, helps with impedance matching.

More recent halo antennas have tended to use a single turn loop, fed with a one-armed gamma match.[d] The newer approach uses less material and reduces wind load, but has narrower bandwidth, may be mechanically less robust, and usually requires a current balun to inhibit feed-line radiation.

Advantages and disadvantages of a halo antennas

Like all antenna designs, the halo antenna is a compromise that sacrifices one desirable quality for another even more desirable quality – for example halos are small and moderately efficient, but only for a single frequency and a narrow band around it. The following sections discuss the advantages and disadvantages of halo antennas both for practical and theoretical issues.

Advantages

Car roof-mounted 6 meter halo antenna for mobile amateur radio (by WA8FJW). Note the triple-loop.
  • The halo, as a larger antenna, is more efficient than a small loop.
  • On the VHF bands and above, the physical diameter of a halo is small enough to be effectively used as a mobile antenna.
  • Towards the horizon, the pattern is omnidirectional to within 3 dB or less, and that can be evened out by making the loop slightly smaller and adding more capacitance between the element tips. Not only will that even out the gain, it will reduce the largely-wasted upward radiation.[c]
  • When fed with a gamma match, the radiating element of the halo is at DC ground, which tends to reduce static buildup.
  • Halos pick up less ignition noise from vehicles when mounted atop vehicle roofs than whip antennas.[4]
  • Halos may be stacked for additional gain. This reduces the high angle radiation, but has little or no effect on the shape of the radiation pattern in the plane of the antenna.[c]

Disadvantages

  • Radiation from horizontal halos has almost no vertical polarization component. One can expect a large signal loss when the other station uses vertical polarization.[4]
  • The halo antenna is structurally rigid; if attached to a vehicle, it may suffer damage from tree branches or other obstacles, unlike a whip antenna which bends and springs back.
  • A halo antenna is a resonant antenna, providing best performance only around one frequency. On the other hand, a small transmitting loop can be tuned over a 3:1 frequency range with a variable capacitor.[e]
  • For mobile use, the halo is rather conspicuous compared to the much more common vertical whip antenna, and may attract unwanted attention.
  • A halo antenna is not as efficient for skywave communications as a horizontal small loop, other things being equal, since more of its signal is sent upward instead of outward, wasting signal power "warming the clouds".

Notes

  1. ^ Note carefully that for all antenna types, for pattern and performance measurement antenna size is measured as a fraction (or multiple) of the length of waves passing through it; hence any one antenna's effective "size" changes with the frequency the attached radio is operating on.
  2. ^ Since the small antenna's radiation resistance is small, at most perhaps a few Ohms, power converted to radio waves can be dwarfed by power lost by heat, due to resistance in the conductor, which is at least a few Ohms. For better transmitting performance, larger antennas are always preferred, but at long wavelengths (lower MF and LF) the size of any resonant antenna (including halo antennas) is unfeasibly large, and small loops are nevertheless used as a least-worst option.
  3. ^ a b c High angle radiation is not useful for radio communications, except for near vertical incidence skywave (NVIS) or for signalling fast-orbiting spacecraft with a fixed antenna. For the special case of satellite communications, a radiation pattern that uniformly covers the entire sky is convenient. For local communications by NVIS, vertical radiation is necessary, but at the low frequencies for which the upward signal can be reflected back down, the long wavelengths make the sizes of half-wave loops cumbersome. Furthermore, the frequencies usable for NVIS change from day-to-day, and a half-wave loop cannot adapt to the needed change in wavelength.
  4. ^ A “one-armed” standard gamma match, providing an unbalanced feed, as opposed to a balanced “two-armed” ‘T’-match (a gamma match for each side of the feedpoint). Note that either type of feed can support a grounded halo, if the connection to the supporting mast is placed (as shown in the illustrations) at the electrically neutral center of the halo loop(s) and has a connection to ground through the mast. The use of an unbalanced gamma match is only a typical feature of modern halos; it is not essential to its design. There are other, less common methods of feeding halos that work just as well, or even better.
  5. ^ The feasible transmitting frequencies are those that make the small loop circumference between about 1/ 10 ~ 1 /3 wavelength (where [wavelength] = 299.79 meters/ [frequency in MHz] = 983.563 feet/ [frequency in MHz] ). The highest operating frequency is determined by the minimum capacitance of the variable capacitor; the lowest frequency by the maximum capacitance and by how much loss is acceptable, since the reduction in radiation resistance with smaller size will make the already marginal efficiency very low. A more often seen, but overly conservative range is  1 /8~ 1 /4 wavelength. For receiving shortwave and mediumwave, a much smaller loop antenna size range is quite practical, with the circumferences down to perhaps 1/ 16  wavelength or smaller. There is no such latitude with a halo antenna: It can only be (very nearly)  1 /2 wavelength.

References

  1. ^ a b US patent 2324462, Leeds, L.M. & Scheldorf, M.W., "High frequency antenna system", issued 1943-07-13, assigned to General Electric Company 
  2. ^ Stites, Francis H. (October 1947). "A halo for six meters". QST. p. 24.
  3. ^ "Folded dipole". Antenna Theory.
  4. ^ a b Tildon, Edward P. (December 1956). "Polarization effects in VHF mobile". QST. pp. 11–13.
  5. ^ Danzer, Paul (September 2004). "A 6 meter halo". QST Magazine. pp. 37–39.

External links

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