Dipole Antennas: The Simplest, Most Common AntennaAugust 2021
As it’s name suggests, in its basic form, a dipole antenna consists of two conductive elements, unlike a monopole antenna, which has a single conductive element.
The dipole’s identical conductive elements (usually rods or metal wires) sit on either end of the antenna. While separated by a strain insulator, the center-facing ends of these two antenna sections are connected to a feed line or coaxial (RF) cable, which carries current in both the conductors. These currents are equal in magnitude but opposite directions, linking the radiating fields within the cable, and causing the fields to cancel each other out.
The current is maximum and voltage is minimum at the center of the dipole antenna. In contrast, the current is minimum and voltage is maximum at the ends of the dipole antenna.
The radiation pattern is perpendicular to the conductor of the antenna. This means that the dipole antenna radiates energy out into the space, perpendicularly to its axis.
There are many kinds of dipoles, but in this post, we will only describe two variations. A half-wave dipole, also known as a doublet, or the Hertz antenna, is the most commonly used type of dipole antenna. The length of its conductive elements is approximately half of the maximum wavelength (λ/2, the distance between two consecutive maximum or minimum points) in free space at the frequency of operation. A half-wave dipole’s current distribution is that of a standing wave, approximately sinusoidal (having the form of a mathematical sine curve) along its length.
While dipoles can be used standalone low-gain antennas, they can also be incorporated as driven elements in antenna designs such as the Yagi antenna and driven arrays.
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