A planar inverted-F antenna (PIFA) is used for wireless circuitry implemented in
microstrip. The microstrip format is the format of choice for modern
RF electronics. It can be used to implement required
distributed-element RF components such as
filters, while at the same time being economical because the same mass production methods are used as for
printed circuit boards. A printed inverted-F antenna can be implemented in the classic inverted-F shape, usually to one side of the circuit board where the
ground plane has been removed from underneath the antenna. However, another approach is a modified
patch antenna, the
shorted patch antenna. In this approach, one edge of the patch, or some intermediate point, is grounded with grounding pins or
vias through to the ground plane. This works on the same principle as an inverted-F; viewed sideways, the F shape can be seen, it is just that the antenna element is very wide in the horizontal plane. The shorted patch antenna has a wider
bandwidth than the thin line type due to the greater radiation area. Like the thin line type, the shorted patch antenna can be printed on the same
printed circuit board as the rest of the circuitry. However, they are commonly printed on to their own board, or on to a
dielectric fixed to the main board. This is done so that the antenna, which can be suspended and effectively be in air dielectric, is a greater distance from the ground plane than it would otherwise be, or the dielectric used is a more suitable material for
RF performance. The term
PIFA is reserved by many authors (e.g. Sánchez-Hernández) for the shorted patch antenna where the antenna element is wide with the ground plane underneath. The thin line type of inverted-F antennas with the ground plane to one side like A and B in the diagram are just called
IFA even if they are in planar format. An author may even call an IFA of this type a
printed inverted-F antenna but still reserve
PIFA for the shorted patch type (e.g. Hall and Wang.) A common configuration for a shorted patch antenna is to place the shorting pin as close to one corner as possible with the feed pin relatively close to the shorting pin. In this configuration, the
resonant frequency is given approximately by, : f_0 = \frac {c} {4 (w + b) \sqrt \varepsilon_\mathrm r} :where :
f0 is the resonant frequency :
w,
b are the width and breadth of the patch :
c is the speed of light :εr is the
dielectric constant of the substrate. This formula only holds if the antenna is not affected by nearby dielectrics, such as the casing of the device. Another variation that may be encountered is the meandered inverted-F antenna (MIFA). Where there is insufficient board space to extend an antenna to the full required length, the antenna may be meandered to reduce its height while retaining its designed electrical length. This can be compared to the spiralling of an antenna as found in the
rubber ducky antenna. Inverted-F antennas have narrow bandwidths. A wider bandwidth can be achieved by lengthening the antenna, which increases its
radiation resistance. Another solution is to place two antennas in close proximity. This works because
coupled resonators have a bandwidth wider than the bandwidth of either resonator on its own. Most of the techniques for producing
multi-band antennas are also effective at broadening bandwidth. ==Multi-band antennas==