Fringing Field In Microstrip Patch Antenna Radiation

08.08.2019
  1. Properties of a Basic Microstrip Patch. A microstrip or patch antenna is a lowprofile antenna that has a number of advantages over. Radiation Pattern. The patch's radiation at the fringing fields results in a certain farfield radiation pattern. This radiation pattern shows that the antenna radiates more power in a certain.
  2. Presents an analysis of the patch antenna. In this video: (1) Why the patch.

It is the fringing fields that are responsible for the radiation. Note that the fringing fields near the surface of the patch antenna are both in the +y direction. Hence, the fringing E-fields on the edge of the microstrip antenna add up in phase and produce the radiation of the microstrip antenna.

A microstrip or patch antenna is a low-profile antenna that has a number of advantages
over other antennas: it is lightweight, inexpensive, and electronics like LNA’s and
SSPA’s can be integrated with these antennas quite easily.
The distance between the patch and the ground plane – the
substrate or dielectric height h – determines the bandwidth.
A thicker substrate increases the gain to some extent, but may lead to undesired effects
like surface wave excitation
Making the ground plane larger also increases the gain but the diffraction at the edges makes it less of the count.
A half wave long patch operates in what we call thefundamental mode: the electric field
is zero at the center of the patch, maximum (positive) on one side, and minimum
(negative) on the opposite side. These minima and maxima continuously change side like
the phase of the RF signal.
Thesefield extensions are known as fringing fields and cause the patch to radiate.
Patchthe magnetic fields in patch antennas are always transverse to
their z-axis.
therefore the electric field in the z direction, and the magnetic field components in x and y directions.
In general, modes are designated as TMnmp. The ‘p’ value is mostly omitted because the
electric field variation is considered negligible in the z-axis since only a phase variation
exists in the z axis. So, TMnm represents the fieldvariations in the x and y directions.
The field variation in the y direction (impedance width direction) is negligible and m is 0.
The field has one minimum-to-maximum variation in the x direction (resonance length
direction and a half wave long), n is 1 in this case and we say that this patch operates in
the TM10 mode.

The resonant length (the x axis in Figure 2) determines the resonant frequency and is
about 位
d
/2 for a rectangular patch excited in its fundamental mode where 位
d
is the
wavelength in the PCB material.
Other parameters that have less influence on the resonant frequency include:
• Ground plane size
• Metal (copper) and dielectric thickness
• Patch (impedance) width

Impedance Matching

The feed position of a patch antenna excited in itsfundamental mode is typically located
in the center of the patch width direction (y axis)and somewhere along the patch
resonant length direction (x axis). The exact position along the resonant length is
determined by the electromagnetic field distribution in the patch. Looking at the current
Patch(magnetic field) and voltage (electric field) variation along the patch, the current has a
maximumat the center and a minimumnear the left and right edges, while the electric
field is zeroin the center and maximumnear the left and minimumnear the right edges.
Keep in mind that the field distribution constantlychanges in amplitude and sign. Figures
2 and 3below clarify


Fundamental Specifications Of Patch Antennas

Radiation Pattern

A patch antenna radiates power in certain directions and we say that the antenna has
directivity (usually expressed in dBi). If the antenna had a 100% radiation efficiency, all
directivity would be converted to gain. Typical half wave patches have efficiencies well

The rectangular patch excited in its fundamental mode has a maximum directivity in the
direction perpendicular to the patch (z-axis or broadside). The directivity decreases when
moving away from broadside towards lower elevations.
The 3 dB beamwidth is the width at which the gain of the beam decreases by 3 dB relative to the gain in broadside to either side of the main beam.

Antenna
So far, the directivity has been defined relative to an isotropic radiator and we use dBi.

Antenna Gain

Antennas do not have gain because they are passive structures. Antenna gain is defined as
antenna directivity times a factor representing theradiation efficiency. Radiation
efficiency is always lower than 100% so the antennagain is always lower than antenna
directivity. This efficiency quantifies the losses in the antenna and is defined as the ratio
of radiated power (Pr) to input power (Pi). The input power is transformed into radiated power, surface wave power and a small portion is dissipated due to conductor and dielectric losses.

Polarization

The plane in which the electric field varies is also known as the polarization plane. The
basic patch covered so far is linearly polarized since the electric field varies in only one
direction. This polarization can be anything between vertical and horizontal depending on
the orientation of the patch. For optimum system performance, transmit and receive antennas must have the same polarization.
In a circularly polarized antenna, the electric field
varies in two orthogonal planes (x and y direction)with the same magnitude and a 90°
phase difference. The result is the simultaneous excitation of two modes, i.e. the TM10
mode (x direction) and the TM01 mode (y direction).One of the modes is excited with a

Microstrip Antenna Theory

90° phase delay with respect to the other mode. A circularly polarized antenna can either
be right-hand circular polarized (RHCP) or left-hand circular polarized (LHCP). The
antenna is RHCP when the phases are 0° and -90° forthe antenna in Figure 5when it
radiates towards the reader, and it is LHCP when the phases are 0° and +90°.








Microstrip Patch Antenna Design





A microstrip antenna array for a satellite television receiver.
Diagram of the feed structure of a microstrip antenna array.

In telecommunication, a microstrip antenna (also known as a printed antenna) usually means an antenna fabricated using microstrip techniques on a printed circuit board (PCB).[1] It is a kind of internal antenna. They are mostly used at microwavefrequencies. An individual microstrip antenna consists of a patch of metal foil of various shapes (a patch antenna) on the surface of a PCB (printed circuit board), with a metal foil ground plane on the other side of the board. Most microstrip antennas consist of multiple patches in a two-dimensional array. The antenna is usually connected to the transmitter or receiver through foil microstriptransmission lines. The radio frequency current is applied (or in receiving antennas the received signal is produced) between the antenna and ground plane. Microstrip antennas have become very popular in recent decades due to their thin planar profile which can be incorporated into the surfaces of consumer products, aircraft and missiles; their ease of fabrication using printed circuit techniques; the ease of integrating the antenna on the same board with the rest of the circuit, and the possibility of adding active devices such as microwave integrated circuits to the antenna itself to make active antennas.

Patch antenna[edit]

The most common type of microstrip antenna is the patch antenna. Antennas using patches as constitutive elements in an array are also possible. A patch antenna is a narrowband, wide-beam antenna fabricated by etching the antenna element pattern in metal trace bonded to an insulating dielectric substrate, such as a printed circuit board, with a continuous metal layer bonded to the opposite side of the substrate which forms a ground plane. Common microstrip antenna shapes are square, rectangular, circular and elliptical, but any continuous shape is possible. Some patch antennas do not use a dielectric substrate and instead are made of a metal patch mounted above a ground plane using dielectric spacers; the resulting structure is less rugged but has a wider bandwidth. Because such antennas have a very low profile, are mechanically rugged and can be shaped to conform to the curving skin of a vehicle, they are often mounted on the exterior of aircraft and spacecraft, or are incorporated into mobile radio communications devices.

Advantages[edit]

Microstrip antennas are relatively inexpensive to manufacture and design because of the simple 2-dimensional physical geometry. They are usually employed at UHF and higher frequencies because the size of the antenna is directly tied to the wavelength at the resonant frequency. A single patch antenna provides a maximum directive gain of around 6-9 dBi. It is relatively easy to print an array of patches on a single (large) substrate using lithographic techniques. Patch arrays can provide much higher gains than a single patch at little additional cost; matching and phase adjustment can be performed with printed microstrip feed structures, again in the same operations that form the radiating patches. The ability to create high gain arrays in a low-profile antenna is one reason that patch arrays are common on airplanes and in other military applications.

Such an array of patch antennas is an easy way to make a phased array of antennas with dynamic beamforming ability.[2]

An advantage inherent to patch antennas is the ability to have polarization diversity. Patch antennas can easily be designed to have vertical, horizontal, right hand circular (RHCP) or left hand circular (LHCP) polarizations, using multiple feed points, or a single feedpoint with asymmetric patch structures.[3] This unique property allows patch antennas to be used in many types of communications links that may have varied requirements.

Rectangular patch[edit]

The most commonly employed microstrip antenna is a rectangular patch which looks like a truncated microstrip transmission line. It is approximately of one-half wavelength long. When air is used as the dielectric substrate, the length of the rectangular microstrip antenna is approximately one-half of a free-space wavelength. As the antenna is loaded with a dielectric as its substrate, the length of the antenna decreases as the relative dielectric constant of the substrate increases. The resonant length of the antenna is slightly shorter because of the extended electric 'fringing fields' which increase the electrical length of the antenna slightly. An early model of the microstrip antenna is a section of microstrip transmission line with equivalent loads on either end to represent the radiation loss.

Specifications[edit]

Applications Of Microstrip Patch Antenna

The dielectric loading of a microstrip antenna affects both its radiation pattern and impedance bandwidth. As the dielectric constant of the substrate increases, the antenna bandwidth decreases which increases the Q factor of the antenna and therefore decreases the impedance bandwidth. This relationship did not immediately follow when using the transmission line model of the antenna, but is apparent when using the cavity model which was introduced in the late 1970s by Lo et al.[4] The radiation from a rectangular microstrip antenna may be understood as a pair of equivalent slots. These slots act as an array and have the highest directivity when the antenna has an air dielectric and decreases as the antenna is loaded by material with increasing relative dielectric constant.

The half-wave rectangular microstrip antenna has a virtual shorting plane along its center. This may be replaced with a physical shorting plane to create a quarter-wavelength microstrip antenna. This is sometimes called a half-patch. The antenna only has a single radiation edge (equivalent slot) which lowers the directivity/gain of the antenna. The impedance bandwidth is slightly lower than a half-wavelength full patch as the coupling between radiating edges has been eliminated.

Other types[edit]

Another type of patch antenna is the planar inverted-F antenna (PIFA).The PIFA is common in cellular phones (mobile phones) with built-in antennas.[5][6]The antenna is resonant at a quarter-wavelength (thus reducing the required space needed on the phone), and also typically has good SAR properties.This antenna resembles an inverted F, which explains the PIFA name. The PIFA is popular because it has a low profile and an omnidirectional pattern.[7]These antennas are derived from a quarter-wave half-patch antenna. The shorting plane of the half-patch is reduced in length which decreases the resonance frequency.[8]Often PIFA antennas have multiple branches to resonate at the various cellular bands. On some phones, grounded parasitic elements are used to enhance the radiation bandwidth characteristics.

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The folded inverted conformal antenna (FICA)[9] has some advantages with respect to the PIFA, because it allows a better volume reuse.

References[edit]

  1. ^Lee, Kai Fong,; Luk, Kwai Man (2011). Microstrip Patch Antennas. World Scientific. pp. 8–12. ISBN184816453X.CS1 maint: extra punctuation (link)
  2. ^'Welcome to antennas 101'by Louis E. Frenzel, 'Electronic Design' 2008
  3. ^Bancroft, R. Microstrip and Printed Antenna Design Noble Publishing 2004, chapter 2-3
  4. ^Lo, Y.T., Solomon D. andRichards, W.F. 'Theory and Experiment on Microstrip Antennas,' IEEE Transactions on Antennas and Propagation, AP-27, 1979 pp. 137-149.
  5. ^'PIFA - The Planar Inverted-F Antenna'.
  6. ^Iulian Rosu.'PIFA – Planar Inverted F Antenna'.
  7. ^Taga, T. Tsunekawa, K. and Saski, A., 'Antennas for Detachable Mobile Radio Units,' Review of the ECL, NTT, Japan, Vol. 35, No.1, January 1987, pp. 59-65.
  8. ^'Inverted-F Antenna (IFA)'at antenna-theory.com
  9. ^Di Nallo, C.; Faraone, A., 'Multiband internal antenna for mobile phones,' Electronics Letters , vol.41, no.9, pp. 514-515, 28 April 2005

External links[edit]

  • Microstrip Antennas antenna-theory.com
  • Microstrip Antenna Tutorial EM Talk
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