This application is based on and claims priority from Japanese Patent Application No. 2017-002809 filed on Jan. 11, 2017.
The disclosure relates to a microstrip antenna.
In the related art, for a radar device to be mounted to a moving body such as an automobile, a microstrip antenna is used as an inexpensive and small-scaled antenna, for example. The microstrip antenna includes a plurality of stacked dielectric layers, conductor layers provided on lower surfaces of the respective dielectric layers, and an antenna provided on the uppermost dielectric layer of the plurality of dielectric layers (for example, refer to Patent Document 1).
Patent Document 1: Japanese Patent Application Publication No. 2014-165529A
However, in the microstrip antenna, an electromagnetic wave may be radiated from the conductor layer. In this case, an electromagnetic wave to be radiated from the antenna and the electromagnetic wave to be radiated from the conductor layer interfere with each other, so that directionality of the antenna is badly influenced.
It is therefore an object of an aspect of the present invention to provide a microstrip antenna capable of suppressing a bad influence on directionality of an antenna.
According to an aspect of the embodiments of the present invention, there is provided a microstrip antenna comprising: a plurality of stacked dielectric layers; an antenna provided on the uppermost dielectric layer of the plurality of dielectric layers; and conductor layers respectively provided on lower surfaces of the dielectric layers, the conductor layers having different dimensions in a plane direction thereof so that electromagnetic waves to be radiated from the conductor layers are cancelled with each other.
With the above configuration, the microstrip antenna can suppress a bad influence on the directionality of the antenna.
In the accompanying drawings:
Hereinafter, an illustrative embodiment of a microstrip antenna disclosed herein will be described in detail with reference to the accompanying drawings. In the meantime, the disclosure is not limited to the illustrative embodiment to be described later. Herein, a microstrip antenna configured to radiate an electromagnetic wave for target detection by a radar device to a surrounding in a wide angle is exemplified.
As shown in
Also, in
The first dielectric layer 21 and the second dielectric layer 22 are formed of fluorine resin, liquid crystal polymer, ceramic, Teflon (registered trademark) or the like, for example. Also, the antenna 3 is formed of copper, for example. The antenna 3 includes a plurality of radiation elements 31, and a power feeding line 32 configured to feed high-frequency power to each radiation element 31.
Also, as shown in
The microstrip antenna 1 is connected to an MIMIC (Monolithic Microwave Integrated Circuit), for example. When a microwave signal modulated and amplified is supplied from the MIMIC to the power feeding line 32, an electromagnetic wave is radiated from each radiation element 31.
At this time, in the microstrip antenna 1, a current (surface current) flows on a surface of the second conductor layer 42 due to an electric field that is formed between the radiation element 31 and the second conductor layer 42 of the antenna 3 when radiating the electromagnetic wave. Also, the electromagnetic wave propagates in the second dielectric layer 22.
The surface current and the propagating electromagnetic wave are transmitted to an end portion of the second conductor layer 42 and an end portion of the first conductor layer 41, and are diffracted at the end portions of the first conductor layer 41 and the second conductor layer 42, so that the radiation is generated from the end portions of the first conductor layer 41 and the second conductor layer 42. By the radiation from the end portions of the first conductor layer 41 and the second conductor layer 42, the directionality of the antenna is badly influenced.
Therefore, in the microstrip antenna 1, dimensions in a plane direction of the first conductor layer 41 and the second conductor layer 42 are made different so that the electromagnetic waves to be radiated from the first conductor layer 41 and the second conductor layer 42 are to be cancelled with each other.
For example, as shown in
The width d is determined by a simulation to be described later so that phases of the electromagnetic wave to be radiated from the first conductor layer 41 and the electromagnetic wave to be radiated from the second conductor layer 42 become antiphases with respect to each other and the electromagnetic waves to be radiated are thus to be cancelled with each other.
Thereby, the microstrip antenna 1 can suppress the bad influence on the directionality of the antenna 3, as compared to a microstrip antenna where a conductor layer and a dielectric layer of which planar shapes and dimensions in the plane direction are the same are sequentially stacked without considering the electromagnetic waves to be radiated.
In the below, operational effects of the microstrip antenna 1 in accordance with the illustrative embodiment are described, in contrast with the general microstrip antenna.
Also,
As shown in
In the microstrip antenna 100, an electromagnetic wave W101 to be radiated from the first conductor layer 141 and an electromagnetic wave W102 to be radiated from the second conductor layer 142 and an electromagnetic wave W to be radiated from the antenna 103 interfere with each other, so that the electromagnetic wave W changes from an ideal gain characteristic.
For this reason, a simulation result of the gain characteristic of the microstrip antenna 100 is as shown in
Also, d=0 [mm] in
As shown in
Therefore, in the microstrip antenna 1 of the illustrative embodiment, the dimensions in the plane direction of the first conductor layer 41 and the second conductor layer 42 are made different so that the electromagnetic waves to be radiated from the first conductor layer 41 and the second conductor layer 42 are to be cancelled with each other. Thereby, the change of the ideal gain characteristic of the electromagnetic wave W is suppressed.
When the dimension in the plane direction of the first conductor layer 41 is changed, a path length from the radiation element 31 to the end portion of the first conductor layer 41 changes. For this reason, it is possible to change the phase of the electromagnetic wave to be radiated from the first conductor layer 41 by changing the dimension in the plane direction of the first conductor layer 41.
By using the above principle, the gain characteristic of the microstrip antenna 1 is sequentially simulated by fixedly setting the dimension in the plane direction of the second conductor layer 42 and gradually increasing the dimension in the plane direction of the first conductor layer 41 from a state where it is the same as the dimension in the plane direction of the second conductor layer 42.
In the meantime, a horizontal axis in
As shown in
Also, as shown in
Also, as shown in
Like this, when the width d is gradually increased, the gain characteristic of the microstrip antenna 1 periodically approaches to the ideal gain characteristic due to the change of the phase of the electromagnetic wave to be radiated from the first conductor layer 41. For this reason, for the microstrip antenna 1, d1 [mm] is adopted as the width d from the simulation result, in which the gain characteristic is most close to the ideal gain characteristic, of the plurality of simulation results.
Thereby, as shown in
Meanwhile, in the microstrip antenna 1, when a frequency of the electromagnetic wave to be radiated from the antenna 3 is changed, wavelengths of the electromagnetic waves to be radiated from the first conductor layer 41 and the second conductor layer 42 are changed. Specifically, when the frequency of the electromagnetic wave to be radiated from the antenna 3 becomes higher, the wavelengths of the electromagnetic waves to be radiated from the first conductor layer 41 and the second conductor layer 42 are shortened. Also, when the frequency of the electromagnetic wave to be radiated from the antenna 3 becomes lower, the wavelengths of the electromagnetic waves to be radiated from the first conductor layer 41 and the second conductor layer 42 are lengthened.
For this reason, the width d, which is a difference between the dimensions in the plane direction of the first conductor layer 41 and the second conductor layer 42, is determined on the basis of the frequency of the electromagnetic wave to be radiated from the antenna 3. For example, in case that the optimal width d at any frequency of the electromagnetic wave W to be radiated from the antenna 3 is the width d1 [mm], when a frequency of the electromagnetic wave W is set higher than any frequency, the optimal width d is made shorter than the width d1 [mm], in correspondence to the frequency of the electromagnetic wave W.
Thereby, even when the frequency of the electromagnetic wave W to be radiated from the antenna 3 is changed, the microstrip antenna 1 can suppress the change of the ideal gain characteristic of the electromagnetic wave W.
Also, in the microstrip antenna 1, a phase difference between the electromagnetic waves to be radiated from the first dielectric layer 21 and the second dielectric layer 22 is also changed due to a thickness of the first dielectric layer 21 or the second dielectric layer 22. For this reason, the width d, which is a difference of the dimensions in the plane direction of the first conductor layer 41 and the second conductor layer 42, is determined on the basis of the thickness of the first dielectric layer 21 or the second dielectric layer 22.
For example, when the optimal width d of the microstrip antenna 1 shown in
Thereby, even the microstrip antenna of which the thickness of the first dielectric layer is different from the microstrip antenna 1 shown in
In the meantime, the configuration of the microstrip antenna 1 shown in
As shown in
Like this, in the microstrip antenna 1a, the dimension in the plane direction of the first conductor layer 41 provided on the lower surface of the first dielectric layer 21 is smaller than the dimension in the plane direction of the second conductor layer 42a provided on the upper surface of the first dielectric layer 21.
Specifically, in the microstrip antenna 1a, each side end surface of the second conductor layer 42a is made to more protrude outward in the horizontal direction than each side end surface of the first conductor layer 41 by a width dx. The width dx is determined by a simulation similar to the above-described simulation.
That is, regarding the width dx, a width at which the electromagnetic wave to be radiated from the first conductor layer 41 and the electromagnetic wave to be radiated from the second conductor layer 42a are to be cancelled with each other is determined by a simulation. Thereby, the microstrip antenna 1a can suppress the change of the ideal gain characteristic of the electromagnetic wave to be radiated from the antenna 3.
In the meantime, as described above, the microstrip antenna 1 of the illustrative embodiment can be applied to a receiving antenna of the radar device, too. When the microstrip antenna 1 is applied to a receiving antenna of the radar device, a part of the electromagnetic wave to be originally received may be incident to the first conductor layer 41 and the second conductor layer 42. The first conductor layer 41 and the second conductor layer 42 radiate the incident electromagnetic wave, as described above.
Even in this case, the electromagnetic waves to be radiated from the first conductor layer 41 and the second conductor layer 42 are cancelled with each other, so that the microstrip antenna 1 can suppress the change of the ideal gain characteristic of the electromagnetic wave to be radiated from the antenna 3 and the bad influence on the directionality of the antenna 3.
Meanwhile, in the illustrative embodiment, the length of the conductor layer is adjusted in correspondence to the frequency of the electromagnetic wave, the thickness of the dielectric and the like. However, the length of the conductor layer may also be adjusted on the basis of parameters (for example, a dielectric constant of the dielectric, and the like other than the frequency and the thickness.
Also, in the illustrative embodiment, the conductor layer has a square shape, as seen from above. However, the planar shape of the conductor layer is not limited thereto. For example, the planar shape of the conductor layer may be a rectangular shape or may be a polygonal shape except for the tetragonal shape. Also, a shape of an end edge of the conductor layer as seen from above may be a wave shape or a serration shape.
Like this, even though the conductor layer has any planar shape, when the dimensions in the plane direction of the upper conductor layer and the lower conductor layer are adjusted to be different from each other so that the electromagnetic waves to be radiated from the conductor layers are to be cancelled with each other, the microstrip antenna can suppress the change of the ideal gain characteristic of the electromagnetic wave to be radiated from the antenna.
The additional effects and modified embodiments can be easily conceived by one skilled in the art. For this reason, the wider aspect of the disclosure is not limited to the specific details and representative illustrative embodiment described in the above. Therefore, a variety of changes can be made without departing from the spirit or scope of the general disclosure defined by the claims and equivalents thereto.
Number | Date | Country | Kind |
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2017-002809 | Jan 2017 | JP | national |
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2014-165529 | Sep 2014 | JP |
Number | Date | Country | |
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20180198198 A1 | Jul 2018 | US |