JP2009124259A - Antenna unit - Google Patents

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Publication number
JP2009124259A
JP2009124259A JP2007293521A JP2007293521A JP2009124259A JP 2009124259 A JP2009124259 A JP 2009124259A JP 2007293521 A JP2007293521 A JP 2007293521A JP 2007293521 A JP2007293521 A JP 2007293521A JP 2009124259 A JP2009124259 A JP 2009124259A
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antenna
waveguide structure
substrate
radio wave
conductor
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JP5041416B2 (en
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Masayuki Sugano
真行 菅野
Yuzo Shibuya
裕三 渋谷
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Japan Radio Co Ltd
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Japan Radio Co Ltd
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Abstract

<P>PROBLEM TO BE SOLVED: To provide an antenna unit arranged to cancel a direct wave from a first antenna to a second antenna through a simple configuration. <P>SOLUTION: A transmission antenna 20, a reception antenna 30, and a waveguide structure 40 located between the transmission antenna 20 and the reception antenna 30 and inverting the phase of a radio wave propagating from the transmission antenna 20 to the reception antenna 30 are arranged on a substrate 10. The waveguide structure 40 is constituted of a conductor pattern 41 formed on the substrate 10, a side board 42 consisting of an array of a plurality of through-holes connecting the conductor pattern 41 and a ground conductor 11, and a ground conductor 44. <P>COPYRIGHT: (C)2009,JPO&INPIT

Description

本発明は、送信アンテナ等の第1アンテナから受信アンテナ等の第2アンテナへの直接波をキャンセルするアンテナ装置に関するものである。   The present invention relates to an antenna device that cancels a direct wave from a first antenna such as a transmission antenna to a second antenna such as a reception antenna.

例えば、距離計測装置では、図5(a)に示すように、送信アンテナから発射した送信電波Pxが被測定物で反射して受信アンテナに受信電波Prとして受信されたとき、その電波の送信から受信までの時間を計測するによって、被測定物までの距離を測定する。このような目的で使用するアンテナでは、送信と受信に使用するアンテナ間において、ある規定値を満足するアイソレーション値が必要となる。すなわち、図5(b)に示すように、送信アンテナから発射される電波Pxが直接波Pr’として受信アンテナで受信されると、距離が誤検出される。アイソレーション値は、送信アンテナから直接受信アンテナに伝搬される直接波Pr’の量を示す値であり、この値が大きいと、特に近距離の被測定物を検出する際に、誤差要因となる。   For example, in the distance measuring device, as shown in FIG. 5 (a), when the transmission radio wave Px emitted from the transmission antenna is reflected by the object to be measured and received by the reception antenna as the reception radio wave Pr, The distance to the object to be measured is measured by measuring the time until reception. An antenna used for such a purpose requires an isolation value that satisfies a specified value between the antennas used for transmission and reception. That is, as shown in FIG. 5B, when the radio wave Px emitted from the transmission antenna is received as the direct wave Pr ′ by the reception antenna, the distance is erroneously detected. The isolation value is a value that indicates the amount of the direct wave Pr ′ that is directly propagated from the transmitting antenna to the receiving antenna. If this value is large, it becomes an error factor particularly when detecting an object to be measured at a short distance. .

そこで、従来では、送信と受信それぞれのアンテナ間に電波吸収材を設ける(特許文献1)、送信と受信それぞれのアンテナ間の間隔を大きくする、送信アンテナについて受信アンテナの位置する方向のアンテナ指向性を低減する等の手法により、アイソレーション値を改善させていた。
特開2002−104070号公報
Therefore, conventionally, a radio wave absorber is provided between each antenna for transmission and reception (Patent Document 1), and the antenna directivity in the direction in which the reception antenna is positioned with respect to the transmission antenna is increased. The isolation value was improved by a technique such as reducing the above.
JP 2002-104070 A

ところが、電波吸収材を配置する手法やアンテナ間隔を大きくする手法は大きなスペースが必要となり小型アンテナには適用できず、また、アンテナ指向性を調整する手法は平面アンテナの場合には限界がある等の問題があった。   However, the method of arranging the electromagnetic wave absorber and the method of increasing the antenna interval require a large space and cannot be applied to a small antenna, and the method of adjusting the antenna directivity is limited in the case of a planar antenna. There was a problem.

本発明の目的は、簡単な構造で第1アンテナから第2アンテナへの直接波をキャンセルできるようにしたアンテナ装置を提供することである。   An object of the present invention is to provide an antenna device capable of canceling a direct wave from a first antenna to a second antenna with a simple structure.

上記目的を達成するために、請求項1にかかる発明は、第1アンテナと、第2アンテナと、前記第1アンテナと前記第2アンテナとの間に位置し前記第1アンテナから前記第2アンテナに伝搬する電波の位相を反転させる導波管構造体と、を備えることを特徴とする。
請求項2にかかる発明は、請求項1に記載のアンテナ装置において、裏面に接地導体が形成された基板上に、前記第1アンテナおよび前記第2アンテナをパッチアンテナ構造で形成するとともに、前記基板上に前記導波管構造体を形成してなり、前記導波管構造体は、前記基板上に形成した導体パターンと、該導体パターンと前記接地導体とを接続する列並びの複数のスルーホールからなる側板と、前記接地導体とからなることを特徴とする。
請求項3にかかる発明は、請求項2に記載のアンテナ装置において、前記導波管構造体を、前記基板上に積層した別の基板上に形成した導体パターンと、該導体パターンと前記接地導体とを接続する列並びの複数のスルーホールからなる側板と、前記接地導体とからなる導波管構造体に置き換えたことを特徴とする。
In order to achieve the above object, the invention according to claim 1 is the first antenna, the second antenna, the first antenna, and the second antenna located between the first antenna and the second antenna. And a waveguide structure for inverting the phase of the radio wave propagating to the antenna.
According to a second aspect of the present invention, in the antenna device according to the first aspect, the first antenna and the second antenna are formed in a patch antenna structure on a substrate having a ground conductor formed on a back surface, and the substrate The waveguide structure is formed thereon, and the waveguide structure includes a conductor pattern formed on the substrate, and a plurality of through holes arranged in a row connecting the conductor pattern and the ground conductor. It consists of the side plate which consists of, and the said ground conductor, It is characterized by the above-mentioned.
The invention according to claim 3 is the antenna device according to claim 2, wherein the waveguide structure is formed on another substrate laminated on the substrate, the conductor pattern and the ground conductor. And a waveguide structure made up of a side plate made of a plurality of through holes arranged in a row and the ground conductor.

本発明によれば、導波管構造体によって第1アンテナから第2アンテナに到達する直接波がキャンセルされるので、第1アンテナと第2アンテナとの間のアイソレーション値を、簡単な構造により、小さくできる。   According to the present invention, since the direct wave reaching the second antenna from the first antenna is canceled by the waveguide structure, the isolation value between the first antenna and the second antenna can be reduced with a simple structure. Can be small.

図1は本発明の1つの実施例のアンテナ装置を示す斜視図である。10は誘電体板11の裏面に接地導体12が設けられた基板、20は基板10の上面にパッチアンテナ構造で形成した送信アンテナ(第1アンテナ)、30は同様の受信アンテナ(第2アンテナ)、40は導波管構造体である。   FIG. 1 is a perspective view showing an antenna apparatus according to one embodiment of the present invention. 10 is a substrate on which the ground conductor 12 is provided on the back surface of the dielectric plate 11, 20 is a transmitting antenna (first antenna) formed with a patch antenna structure on the upper surface of the substrate 10, and 30 is a similar receiving antenna (second antenna). , 40 is a waveguide structure.

この導波管構造体40は、基板20に送信アンテナ20および受信アンテナ30の形成面と同じ面に形成された導電パターン41と、その導体パターン41と基板10の裏面の接地導体12とを接続するスルーホールで形成した側板42と、裏面の接地導体12とで囲まれた構造である。側板42を形成するスルーホールは、使用信号の波長に比べて決めて短いピッチで複数本を直線状に一列又は複数列並べて等価的に埋込金属平板となるよう構成されている。本実施例の導波管構造体40は、送信アンテナ20と受信アンテナ30との間において、導波路が誘電体板11で充填された2個の導波管が並列配置された構造となっている。   This waveguide structure 40 connects the conductive pattern 41 formed on the substrate 20 on the same surface as the transmitting antenna 20 and the receiving antenna 30, and the conductor pattern 41 and the ground conductor 12 on the back surface of the substrate 10. The structure is surrounded by a side plate 42 formed by through-holes and a ground conductor 12 on the back surface. The through holes that form the side plates 42 are configured to be equivalent to buried metal plates by arranging a plurality of lines in a straight line or a plurality of lines at a short pitch determined in comparison with the wavelength of the used signal. The waveguide structure 40 of the present embodiment has a structure in which two waveguides each having a waveguide filled with a dielectric plate 11 are arranged in parallel between the transmission antenna 20 and the reception antenna 30. Yes.

ここで、側板42の相互間隔をL1、導電パターン41の送信アンテナ20と受信アンテナ30の並びに並行な辺の長さをL2、誘電体板11の厚さをL3とする。L1は導波管構造体40の導波管幅、L2は導波管長、L3は導波管高さとなる。そして、λ0を自由空間の波長、λgを導波管構造体40の管内波長とするとき、L1の値を
λg=2×λ0 (1)
なるように決定する。
Here, the interval between the side plates 42 is L1, the length of the parallel sides of the transmitting antenna 20 and the receiving antenna 30 of the conductive pattern 41 is L2, and the thickness of the dielectric plate 11 is L3. L1 is the waveguide width of the waveguide structure 40, L2 is the waveguide length, and L3 is the waveguide height. Then, when λ0 is the free space wavelength and λg is the in-tube wavelength of the waveguide structure 40, the value of L1 is λg = 2 × λ0 (1)
Decide to be.

図3に誘電体板11(比誘電率=2.2)のL1/λ0の変化に対するλg/λ0の変化の特性を示す。この図3において、L1/λ0=0.37に設定すれば、λg/λ0=2となるので、
L1=0.37×λ0 (2)
に設定する。これにより、式(1)のλg=2×λ0となるようにL1の値が設定される。なお、L2の値は、
L2=λ0 (3)
となるように設定する。
FIG. 3 shows the characteristic of the change in λg / λ0 with respect to the change in L1 / λ0 of the dielectric plate 11 (relative dielectric constant = 2.2). In FIG. 3, if L1 / λ0 = 0.37, then λg / λ0 = 2.
L1 = 0.37 × λ0 (2)
Set to. As a result, the value of L1 is set so that λg = 2 × λ0 in equation (1). The value of L2 is
L2 = λ0 (3)
Set to be.

このように設定すると、図2に示すように、送信アンテナ10から発射され自由空間を伝搬する電波F1の位相は、導波管構造体40の入口40Aから出口40Bまでの間(=L2)で考えると、
(λ0)×2π/λ0=2π (4)
のように変化する。
With this setting, as shown in FIG. 2, the phase of the radio wave F1 emitted from the transmitting antenna 10 and propagating through the free space is between the entrance 40A and the exit 40B of the waveguide structure 40 (= L2). If you think about it,
(Λ0) × 2π / λ0 = 2π (4)
It changes as follows.

一方、導波管構造体40の内部を伝搬する電波F2の位相は、
(λ0)×2π/λg=(λ0)×2π/2×λ0=π (5)
のように変化する。したがって、導波管構造体40の出口40Bにおける自由空間を伝搬する電波F1と導波管構造体40を伝搬する電波F2との位相差はπ(逆相)となる。
On the other hand, the phase of the radio wave F2 propagating inside the waveguide structure 40 is
(Λ0) × 2π / λg = (λ0) × 2π / 2 × λ0 = π (5)
It changes as follows. Therefore, the phase difference between the radio wave F1 propagating through the free space at the outlet 40B of the waveguide structure 40 and the radio wave F2 propagating through the waveguide structure 40 is π (reverse phase).

次に、導波管構造体40の導波管高さL3を適宜設定することで、導波管構造体40の内部を伝搬する電波F2の振幅を、導波管構造体40の入口40Aから出口40Bまで間(=L2)の自由空間を伝搬する電波F1の振幅と同じに設定する。   Next, by appropriately setting the waveguide height L3 of the waveguide structure 40, the amplitude of the radio wave F2 propagating through the waveguide structure 40 is changed from the entrance 40A of the waveguide structure 40. It is set to be the same as the amplitude of the radio wave F1 propagating in the free space between the exit 40B (= L2).

これにより、導波管構造体40の入口40Aから出口40Bまでの間(=L2)の自由空間を伝搬する電波F1と導波管構造体40の内部を伝搬する電波F2が互いにキャンセルされることになり、送信アンテナ20から受信アンテナ30への直接波をキャンセルすることができる。   Thereby, the radio wave F1 propagating through the free space between the inlet 40A and the outlet 40B of the waveguide structure 40 (= L2) and the radio wave F2 propagating through the inside of the waveguide structure 40 are cancelled. Thus, the direct wave from the transmitting antenna 20 to the receiving antenna 30 can be canceled.

図4は送信アンテナ20と受信アンテナ30の間のアイソレーション特性を示す図であり、導波管構造体40が無いとき(従来例)に比べて、導波管構造体40を設けたとき(本実施例)は、送信する電波の周波数f0において、−80dBという必要十分なアイソレーション値が得られている。   FIG. 4 is a diagram showing the isolation characteristics between the transmitting antenna 20 and the receiving antenna 30, when the waveguide structure 40 is provided compared to when the waveguide structure 40 is not provided (conventional example) ( In this embodiment, a necessary and sufficient isolation value of −80 dB is obtained at the frequency f0 of the radio wave to be transmitted.

なお、上記実施例では、λ0だけ隔たった出口40Bのポイントで電波F1とF2がキャンセルされる場合について説明したが、これに限られるものではなく、キャンセルポイントは多数あるので、導波管構造体40の数値L1,L2,L3の組み合わせは多数ある。また、導波管構造体40の導波管高さL3を基板10の誘電体板11の厚さによって設定するので、一枚構造の基板のみでは、導波管構造体40内を通過する電波F2の振幅を外部を通過する電波F1の振幅に合わせることが困難になることもある。しかし、この場合は、導波管構造体40の部分において、積層基板構造を採用することにより、所望の導波管高さL3を実現することができる。   In the above-described embodiment, the case where the radio waves F1 and F2 are canceled at the point of the exit 40B separated by λ0 has been described. There are many combinations of 40 numerical values L1, L2, and L3. Further, since the waveguide height L3 of the waveguide structure 40 is set by the thickness of the dielectric plate 11 of the substrate 10, the radio wave passing through the waveguide structure 40 can be obtained only with a single-layer substrate. It may be difficult to match the amplitude of F2 to the amplitude of the radio wave F1 passing outside. However, in this case, a desired waveguide height L3 can be realized by adopting a laminated substrate structure in the waveguide structure 40 portion.

本発明の1つの実施例のアンテナ装置の斜視図である。It is a perspective view of the antenna apparatus of one Example of this invention. 同実施例のアンテナ装置の作用説明図である。It is operation | movement explanatory drawing of the antenna apparatus of the Example. 導波管構造体内でのL1/λ0に対するλg/λ0の特性図である。FIG. 6 is a characteristic diagram of λg / λ0 with respect to L1 / λ0 in the waveguide structure. 本実施例と従来例のアイソレーション特性図である。It is an isolation characteristic figure of a present Example and a prior art example. 送信アンテナと受信アンテナを使用した距離測定の説明図である。It is explanatory drawing of distance measurement using a transmitting antenna and a receiving antenna.

符号の説明Explanation of symbols

10:基板、11:誘電体板、12:接地導体
20:送信アンテナ
30:受信アンテナ
40:導波管構造体、41:導体パターン、42:側板
40A:導波管構造体の入口、40B:導波管構造体の出口、F1:自由空間伝搬の電波、F2:導波管構造体内伝搬の電波
DESCRIPTION OF SYMBOLS 10: Board | substrate, 11: Dielectric board, 12: Grounding conductor 20: Transmitting antenna 30: Reception antenna 40: Waveguide structure, 41: Conductor pattern, 42: Side plate 40A: Entrance of waveguide structure, 40B: Exit of waveguide structure, F1: radio wave propagating in free space, F2: radio wave propagating in the waveguide structure

Claims (3)

第1アンテナと、第2アンテナと、前記第1アンテナと前記第2アンテナとの間に位置し前記第1アンテナから前記第2アンテナに伝搬する電波の位相を反転させる導波管構造体と、を備えることを特徴とするアンテナ装置。   A first antenna, a second antenna, a waveguide structure positioned between the first antenna and the second antenna and inverting the phase of a radio wave propagating from the first antenna to the second antenna; An antenna device comprising: 請求項1に記載のアンテナ装置において、
裏面に接地導体が形成された基板上に、前記第1アンテナおよび前記第2アンテナをパッチアンテナ構造で形成するとともに、前記基板上に前記導波管構造体を形成してなり、
前記導波管構造体は、前記基板上に形成した導体パターンと、該導体パターンと前記接地導体とを接続する列並びの複数のスルーホールからなる側板と、前記接地導体とからなることを特徴とするアンテナ装置。
The antenna device according to claim 1,
Forming the first antenna and the second antenna in a patch antenna structure on a substrate having a ground conductor formed on the back surface, and forming the waveguide structure on the substrate;
The waveguide structure includes a conductor pattern formed on the substrate, a side plate formed of a plurality of through holes arranged in a row connecting the conductor pattern and the ground conductor, and the ground conductor. An antenna device.
請求項2に記載のアンテナ装置において、
前記導波管構造体を、前記基板上に積層した別の基板上に形成した導体パターンと、該導体パターンと前記接地導体とを接続する列並びの複数のスルーホールからなる側板と、前記接地導体とからなる導波管構造体に置き換えたことを特徴とするアンテナ装置。
The antenna device according to claim 2, wherein
A conductor pattern formed on another substrate laminated on the substrate; a side plate comprising a plurality of through holes arranged in a row connecting the conductor pattern and the ground conductor; and the ground An antenna device characterized by being replaced with a waveguide structure made of a conductor.
JP2007293521A 2007-11-12 2007-11-12 Antenna device Active JP5041416B2 (en)

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Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2012070253A (en) * 2010-09-24 2012-04-05 Toshiba Corp Wireless apparatus
WO2012043442A1 (en) * 2010-09-29 2012-04-05 三菱重工業株式会社 Antenna device
JP2017216587A (en) * 2016-05-31 2017-12-07 パナソニックIpマネジメント株式会社 Dielectric substrate circuit board and antenna device
JP2018046440A (en) * 2016-09-15 2018-03-22 京セラ株式会社 Antenna substrate

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Publication number Priority date Publication date Assignee Title
JPH11274818A (en) * 1998-03-20 1999-10-08 Fujitsu Ltd High frequency circuit device
JP2001102861A (en) * 1999-09-29 2001-04-13 Kyocera Corp Laminated opening plane array antenna
JP2001284950A (en) * 2000-03-31 2001-10-12 Alps Electric Co Ltd Primary radiator
JP2005244317A (en) * 2004-02-24 2005-09-08 Ntt Docomo Inc Microstrip antenna
JP2005249659A (en) * 2004-03-05 2005-09-15 Mitsubishi Electric Corp Transmission antenna and reception antenna for radar system

Patent Citations (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH11274818A (en) * 1998-03-20 1999-10-08 Fujitsu Ltd High frequency circuit device
JP2001102861A (en) * 1999-09-29 2001-04-13 Kyocera Corp Laminated opening plane array antenna
JP2001284950A (en) * 2000-03-31 2001-10-12 Alps Electric Co Ltd Primary radiator
JP2005244317A (en) * 2004-02-24 2005-09-08 Ntt Docomo Inc Microstrip antenna
JP2005249659A (en) * 2004-03-05 2005-09-15 Mitsubishi Electric Corp Transmission antenna and reception antenna for radar system

Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2012070253A (en) * 2010-09-24 2012-04-05 Toshiba Corp Wireless apparatus
WO2012043442A1 (en) * 2010-09-29 2012-04-05 三菱重工業株式会社 Antenna device
JP2012073853A (en) * 2010-09-29 2012-04-12 Mitsubishi Heavy Ind Ltd Antenna device
JP2017216587A (en) * 2016-05-31 2017-12-07 パナソニックIpマネジメント株式会社 Dielectric substrate circuit board and antenna device
JP2018046440A (en) * 2016-09-15 2018-03-22 京セラ株式会社 Antenna substrate

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