This invention relates to transmitting and receiving signals, and more particularly to transmitting and receiving circular polarized radiation using a single feed.
Circularly polarized antennas are often desirable in many applications using ultra high frequency (UHF), microwave frequencies, and millimeter wave frequencies. A circularly polarized wave may be produced by radiating horizontally and vertically polarized waves ninety degrees out of phase. This is often accomplished with power dividers and ninety-degree phase shifters. However, these power divider and phase shifter components often complicate the design of circularly polarized antennas. Additionally, the extremely narrow bandwidth of prior circularly polarized antennas make them undesirable in many applications requiring moderate bandwidth. Many systems, such as military and commercial communications systems, could be improved with compact, low cost, rugged, conformable antennas. Such antennas could readily be utilized in aircraft and global positioning system receivers.
In some implementations, a microstrip antenna includes a dielectric substrate, a rectangular radiating plate, and a single feed connection. In these instances, the rectangular radiating plate is affixed to the dielectric substrate and having a center point, and the radiating patch defines a first aperture and a second aperture on opposite sides of the center point, each aperture having a center longitudinally aligned with the center point. The single feed connection is laterally offset from a point on a virtual line, wherein the virtual line is located between two opposite corners of the rectangular radiating patch and passes through the center point.
The details of one or more embodiments of the invention are set forth in the accompanying drawings and the description below. Other features, objects, and advantages of the invention will be apparent from the description and drawings, and from the claims.
Like reference symbols in the various drawings indicate like elements.
In the illustrated implementation, the CP microstrip antenna 100 includes a dielectric substrate 102 and a radiating patch 104. The radiating patch 104 is affixed to a top surface of the dielectric substrate 102. A transceiver 116 is connected to the radiating patch 104 at the feed connection 114. The transceiver 116 supplies (and receives), the radiating patch 104, RF power at a specific frequency. The radiating patch 104 generates a first mode at the specific frequency and a second mode orthogonal to the first at the specific frequency with a 90° phase shift compared to the first signal.
The radiating patch 104 includes apertures 106a and 106b that form channels to the dielectric substrate 102. As illustrated, the apertures 106a and 106b are circular but, with departing from the scope of the disclosure, may be other shapes as well (e.g., rectangular). In some implementations, the apertures 106a and 106b may have substantially the same dimensions. In the illustrated implementation, the aperture 106a is located between the left side and center point of the radiating patch 104, and the aperture 106b is located between the right side and center point of the radiating patch 104. The center of the aperture 106a may be longitudinally aligned with the center point 108 of the radiating patch 104, and the center of the aperture 106b may be longitudinally aligned with the center point 108 of the radiating patch 104. In some implementations, the center of the aperture 106a may be equidistant between the top side and the bottom side of the radiating patch 104. In some implementations, the center of the aperture 106b may be equidistant between the top side and the bottom side of the radiating patch 104.
The virtual line 110 extends from the top right corner, through the center point 108, and to the bottom left corner of the radiating patch 104. As previously mentioned, the virtual line 110 may be used to determine a point on the virtual line 110 where the measured rate loss in dB is at a minimum or otherwise below a predefined threshold. A lateral offset 112 may be determined from the point on the virtual line 110 where the axial ratio in dB is at a minimum or otherwise below a predefined threshold. In some implementations, the lateral offset 112 is substantially parallel to the top and bottom side of the radiating patch 104. As illustrated, the lateral offset 112 can determine a feed connection 114 for the transceiver 116. In some implementations, the connection for the transceiver 116 may be feed through the dielectric substrate 102.
In some aspects of operations, the feed connection 114 may be determined based on multiple measurements at different frequencies along the virtual line 110 followed by multiple measurements at different frequencies in a lateral direction away from the virtual line 110. For example, measurements over a frequency range may be made starting at the center point 108 and then along the virtual line 110 toward the upper right hand corner of the radiating patch 104. The measurements are analyzed to determine a point on the virtual line 110 where a frequency has the lowest value or a value below a predefined threshold for the measured return loss. In these implementations, measurements over the frequency range are then performed in a lateral direction starting from the point on the virtual line 110. The measurements are analyzed to determine a lateral offset where the frequency has the lowest value or a value below a predefined threshold for the axial ratio in dB. The single feed connection 114 is made using the later offset 112.
The apertures 106a and 106b have centers along the y-axis, and the feed, through the feed connection 114, is placed near the diagonal line connecting two opposite corners of the radiating patch 104. In particular, the feed is offset from the diagonal along the y axis. The feed applies an oscillating current to the radiating patch 104 and excites two degenerate modes, transverse magnetic TM10 and TM01. The apertures 106a and 106b do not appreciably affect the modal excitation of TM10 because the centers of the apertures 106a and 106b are placed at the line of vanishing electric field of TM10. In contrast, the apertures 106a and 106b strongly affect modal fields of TM01. The apertures 106a and 106b impose a boundary condition on the TM01 mode, and the phase of the new modal excitation becomes 90° out of phase with that of TM10.
Another condition for good CP radiation is that the magnitudes of the TM10 and TM01 modes have to be as close as possible each other. In order to adjust the relative magnitude of one mode over the other, the feed location is shifted. For example, as the feed moves along the y-axis with a fixed value of x, the magnitude of TM01 changes while that of the TM10 mode is relatively unchanged. As the feed moves toward increasing value of y, the magnitude of TM01 will increase relative to that of TM10.
The apertures 106a and 106b have to be large enough that the apertures 106a and 106b provide sufficient influence on the field excitation of TM01 to provide a phase shift of 90° for CP radiation. However, excessively large aperture size may not provide a 90° phase shifter because the 90° phase shift is based on a small-hole approximation. Also, perturbation from large apertures may change the resonant frequency of TM01, which can be detrimental to CP radiation. In order to increase the effect of the apertures 106a and 106b without any detrimental aspects of large aperture size, the apertures 106a and 106b may be symmetrically placed as illustrated. In these instances, the apertures 106a and 106b may influence the TM01 modal excitation substantially identically.
The closer the apertures 106a and 106b are to the edges of the radiating patch 104, the apertures 106a and 106b are typically more effective on the phase shift of the modal excitation of TM01. But as the apertures 106a and 106b approaches their respective patch edges, interaction between the apertures 106a and 106b and the patch edges increases and may reduce the quality of CP radiation. The ideal axial ratio is 1 (or 0 dB). The dB for CP may be defined to be 20 log (linear axial ratio). Typically, an acceptable axial ratio is 3 dB or 6 dB.
The measured return loss (RL) and the axial ratio (AR) as a function of frequency are shown in
The measured radiation patterns at the resonant frequency with an optimized AR of 0.25 dB are shown in
A number of embodiments of the invention have been described. Nevertheless, it will be understood that various modifications may be made without departing from the spirit and scope of the invention. For example, a rectangular patch slightly deviant from a square may show improved CP due to compensation of the shifted resonant frequency of first mode relative to that of the other when placing the apertures. A non-rectangular shape of the radiating patch such as a circular shape is one other variation. Another example is aperture shapes other than a circle. Accordingly, other embodiments are within the scope of the following claims.
| Number | Name | Date | Kind |
|---|---|---|---|
| 5461393 | Gordon | Oct 1995 | A |
| 5471221 | Nalbandian | Nov 1995 | A |
| 5515057 | Lennen | May 1996 | A |
| 5703601 | Nalbandian | Dec 1997 | A |
| 6157348 | Openlander | Dec 2000 | A |
| 6166692 | Nalbandian | Dec 2000 | A |
| 6232923 | Guinn | May 2001 | B1 |
| 20100194663 | Rothwell | Aug 2010 | A1 |
| 20150303576 | Latrach | Oct 2015 | A1 |
| 20160118720 | Kim | Apr 2016 | A1 |
| 20160261039 | Parsche | Sep 2016 | A1 |