This directional wire beam antenna - also known as the "4DX" antenna - was originally designed in 2017 by father and son team LZ1AQ and LZ1ABC, and subsequently further developed by Kev VK6LW and Ed DD5LP. This designer allows you to create such an antenna, for one or more bands: the antenna consists of four separate sloping wires making up an array of two angled inverted-vee dipoles, the apexes of which are arranged very close to each other at the center.
Each half of the array is a full-sized single-band dipole, or multiband linked dipole, antenna: to achieve directionality, one of the dipoles is loaded capacitively at the apex, effectively shortening its' legs electrically. This dipole then becomes a "director" for the other, "driver", dipole, and the array radiates preferentially in that direction. By arranging switchable capacitors and feed-point positions on each pair of arms of the array, the antenna can very quickly be made to radiate in any one of four different directions. Gains of 9dBi or greater can be achieved, and F/B ratios of 12dB or greater are possible, depending on height, apex-angle and frequency. Read more...
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Dipoles-beam antenna designer
portable-antennas.com
Antenna feed-point: ⬥
Arrow shows direction of main beam
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Here you can generate plots of
radiation patterns,
VSWR chart, antenna currents diagram and Smith chart for your antenna over a
choice of ground types. By changing the physical dimensions of the antenna, and refreshing these plots, you can learn a lot about
how such antennas will perform in the field.
Please note that
radiation patterns are here modelled over flat ground -
when the antenna is erected on a hill-top or mountain summit, the surrounding sloping ground will generally cause angles in
the elevation radiation pattern to be lowered in the direction of the
slope: the steeper the slope, the lower the effective elevation take-off angle will be, and the better the chances of making
long-distance contacts.
Read more...
| Choose antenna section: | |
| Check harmonics?: |
kHz
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Choose ground type of
land in the vicinity of the antenna: |
Conductivity:
S/m
Dielectric const.:
F/m
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| View radiation patterns: |
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| Choose type: | |
| Set ref. elevation angle: |
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| Set ref. azimuth angle: |
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| View VSWR chart: | |
| Effect of coax on VSWR: |
Coax length:
Type:
Effect of coax- and system-losses on VSWRWhen a coaxial cable is used to connect the antenna to a transmitter, the cable introduces signal loss, the magnitude of which can vary strongly with both frequency and antenna feed-point impedance. The main blue VSWR curve for this antenna is calculated at the antenna feed-point. The optional green curve represents the VSWR "seen" at the transmitter after losses in the coaxial cable are taken into account. At frequencies of antenna resonance, the blue and green curves usually coincide closely, since the coax contributes little additional attenuation at those frequencies. At frequencies away from resonance, however — often those corresponding to WARC bands — the feed-point impedance may become highly mismatched, producing very high VSWR values in the blue curve while the green curve shows substantially lower values. This reduction in VSWR at the transmitter occurs because signal losses in the coaxial cable attenuate both the forward and reflected waves. As a result, the reflected signal returning to the transmitter is weaker, causing the transmitter-end VSWR to appear lower than the actual feed-point VSWR. This effect can make some bands appear more "usable" from the transmitter's perspective, even though the antenna system may still be operating inefficiently at those frequencies. The green curve represents the "flattening" of the VSWR caused by the coax. Additional losses elsewhere in the system can further reduce the transmitter-end VSWR - these may include:
The magnitude of such losses, and their effect on actual radiated RF power, can only be estimated reliably through careful analysis of a particular antenna setup. In every-day portable operations, such losses can only be roughly estimated; however, comparisons can be made between commercially-produced EFHW and OCFD antennas for amateur radio use, and carefully-configured NEC models of those same antennas. Useful estimates can then be made of the efficiency of the commercial products by comparing their published VSWR curves, and the VSWR curves produced from the models. Improved transmitter-end VSWR therefore does not necessarily imply improved radiation efficiency: in some cases, a significant proportion of the transmitted power may simply be lost: dissipated as heat within the antenna system. Read more... |
| View currents diagram | |
| View Smith chart: |
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Antenna gains at 0° elevation: |
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| Feed-point impedance: | |
| Estimated bandwidth: | |