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JP4790684B2 - Antenna device - Google Patents
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JP4790684B2 - Antenna device - Google Patents

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JP4790684B2
JP4790684B2 JP2007261074A JP2007261074A JP4790684B2 JP 4790684 B2 JP4790684 B2 JP 4790684B2 JP 2007261074 A JP2007261074 A JP 2007261074A JP 2007261074 A JP2007261074 A JP 2007261074A JP 4790684 B2 JP4790684 B2 JP 4790684B2
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planar coil
antenna device
antenna
radiation
conductor
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JP2009094631A (en
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元珠 竇
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Alps Alpine Co Ltd
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Alps Electric Co Ltd
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    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01QANTENNAS, i.e. RADIO AERIALS
    • H01Q1/00Details of, or arrangements associated with, antennas
    • H01Q1/36Structural form of radiating elements, e.g. cone, spiral, umbrella; Particular materials used therewith
    • H01Q1/38Structural form of radiating elements, e.g. cone, spiral, umbrella; Particular materials used therewith formed by a conductive layer on an insulating support
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01QANTENNAS, i.e. RADIO AERIALS
    • H01Q1/00Details of, or arrangements associated with, antennas
    • H01Q1/12Supports; Mounting means
    • H01Q1/22Supports; Mounting means by structural association with other equipment or articles
    • H01Q1/24Supports; Mounting means by structural association with other equipment or articles with receiving set
    • H01Q1/241Supports; Mounting means by structural association with other equipment or articles with receiving set used in mobile communications, e.g. GSM
    • H01Q1/242Supports; Mounting means by structural association with other equipment or articles with receiving set used in mobile communications, e.g. GSM specially adapted for hand-held use
    • H01Q1/243Supports; Mounting means by structural association with other equipment or articles with receiving set used in mobile communications, e.g. GSM specially adapted for hand-held use with built-in antennas
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01QANTENNAS, i.e. RADIO AERIALS
    • H01Q1/00Details of, or arrangements associated with, antennas
    • H01Q1/36Structural form of radiating elements, e.g. cone, spiral, umbrella; Particular materials used therewith
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01QANTENNAS, i.e. RADIO AERIALS
    • H01Q21/00Antenna arrays or systems
    • H01Q21/29Combinations of different interacting antenna units for giving a desired directional characteristic
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01QANTENNAS, i.e. RADIO AERIALS
    • H01Q9/00Electrically-short antennas having dimensions not more than twice the operating wavelength and consisting of conductive active radiating elements
    • H01Q9/04Resonant antennas
    • H01Q9/16Resonant antennas with feed intermediate between the extremities of the antenna, e.g. centre-fed dipole
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01QANTENNAS, i.e. RADIO AERIALS
    • H01Q9/00Electrically-short antennas having dimensions not more than twice the operating wavelength and consisting of conductive active radiating elements
    • H01Q9/04Resonant antennas
    • H01Q9/16Resonant antennas with feed intermediate between the extremities of the antenna, e.g. centre-fed dipole
    • H01Q9/28Conical, cylindrical, cage, strip, gauze, or like elements having an extended radiating surface; Elements comprising two conical surfaces having collinear axes and adjacent apices and fed by two-conductor transmission lines

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  • Engineering & Computer Science (AREA)
  • Computer Networks & Wireless Communication (AREA)
  • Details Of Aerials (AREA)
  • Variable-Direction Aerials And Aerial Arrays (AREA)

Abstract

Provided is a dipole or monopole antenna device capable of realizing great miniaturization. In a dipole antenna device 1, a plurality of flat coils 3a and 3b, and 4a and 4b are connected in which conductors forms closed areas in the plan view in a magnetic field area in the vicinity of a power supply portion 2. Capacitors 5 and 6 as radiation conductors are connected to both ends of the antenna device 1, respectively. Resonant current radiation is performed from the capacitors 5 and 6 at the antenna ends, and magnetic field radiation is performed from flat foils 3a and 3b, and 4a and 4b in the vicinity of the power supply portion 2.

Description

本発明は、小型の無線通信機器等に使用可能なダイポール又はモノポール型のアンテナ装置に関する。   The present invention relates to a dipole or monopole antenna device that can be used in a small wireless communication device or the like.

一般的にアンテナの長さは波長に比べ、長い方が受信感度が上がるが、携帯電話等のアンテナ装置として用いる場合、アンテナ長を波長の長さと同一寸法にしたのでは大き過ぎて携帯性に優れないので、アンテナ長を短くすることが望まれる。   In general, the longer the antenna length, the higher the reception sensitivity compared to the wavelength. However, when the antenna is used as an antenna device for a mobile phone or the like, it is too large if the antenna length is the same as the wavelength length. Since it is not excellent, it is desirable to shorten the antenna length.

図10(a)は1/2波長ダイポールアンテナの模式図である。アンテナに高周波電流を供給すると、アンテナ線上に電流と電圧が分布する。アンテナの長さが1/2波長の整数倍のときアンテナが共振して効率よく電波が放射される(共振電流放射)。1/2波長ダイポールアンテナではアンテナの長さは1/2波長前後の長さが必要である。   FIG. 10A is a schematic diagram of a ½ wavelength dipole antenna. When a high frequency current is supplied to the antenna, current and voltage are distributed on the antenna line. When the length of the antenna is an integral multiple of ½ wavelength, the antenna resonates to efficiently radiate radio waves (resonant current radiation). In a half-wave dipole antenna, the length of the antenna needs to be about half a wavelength.

ダイポール又はモノポールアンテナの電気長を変えずにアンテナを小型化するためには、等価容量C又は等価インダクタLを大きくして共振周波数を小さくすることが考えられる。しかし、等価容量Cを大きくするためにはアンテナ面積が大きくなるので好ましくない。また、チップインダクタを挿入することにより寸法を大きくすることなくインダクタLを大きくできるが、チップインダクタは放射しないのでアンテナ全体の効率が悪くなる。   In order to reduce the size of the antenna without changing the electrical length of the dipole or monopole antenna, it is conceivable to increase the equivalent capacitance C or the equivalent inductor L to reduce the resonance frequency. However, increasing the equivalent capacitance C is not preferable because the antenna area increases. Although the inductor L can be increased without increasing the size by inserting a chip inductor, the chip inductor does not radiate, so the efficiency of the entire antenna is deteriorated.

図10(b)はアンテナ線をミアンダラインで構成したダイポールアンテナの模式図である。アンテナ線をミアンダラインで構成することにより、アンテナの電気長を変えずに、アンテナの長さを1/8波長程度まで小型化することができる。但し、ミアンダラインの間隔を狭くするほどアンテナ長を短くできるが、ミアンダラインの間隔がある程度まで狭くなると段間結合容量の影響でミアンダラインによる小型化にも限界がある。   FIG.10 (b) is a schematic diagram of the dipole antenna which comprised the antenna line by the meander line. By configuring the antenna line with a meander line, the length of the antenna can be reduced to about 1/8 wavelength without changing the electrical length of the antenna. However, the antenna length can be shortened as the interval between the meander lines is reduced. However, when the interval between the meander lines is reduced to a certain extent, there is a limit to miniaturization by the meander line due to the influence of the interstage coupling capacitance.

また、ミアンダラインで構成したダイポールアンテナにおいて、アンテナ長を1/8波長からさらに短縮するアンテナ装置が提案されている(例えば、特許文献1参照)。特許文献1に開示されたアンテナ装置は、プリント基板とは別体に放射エレメントを設け、該放射エレメントの導体パターンをプリント基板より誘電率が大きい誘電体部材に形成するといったものである。これにより、誘電体部材の比誘電率による受信信号波長の短縮量が多くなるので、アンテナの小型化を図ることができる。
特開2006−319437号公報
In addition, an antenna device that further shortens the antenna length from 1/8 wavelength in a dipole antenna configured with meander lines has been proposed (see, for example, Patent Document 1). The antenna device disclosed in Patent Document 1 is such that a radiating element is provided separately from a printed board, and a conductive pattern of the radiating element is formed on a dielectric member having a dielectric constant larger than that of the printed board. As a result, the amount of shortening of the received signal wavelength due to the relative permittivity of the dielectric member increases, and the antenna can be downsized.
JP 2006-319437 A

しかしながら、特許文献1に記載されたアンテナ装置のように誘電体部材の比誘電率による受信信号波長の短縮量だけでは限界があり、アンテナ装置のさらなる小型化が望まれる。   However, like the antenna device described in Patent Document 1, there is a limit only by the amount of shortening of the received signal wavelength due to the relative permittivity of the dielectric member, and further downsizing of the antenna device is desired.

本発明は、かかる点に鑑みてなされたものであり、大幅な小型化を実現可能なダイポール又はモノポール型のアンテナ装置を提供することを目的とする。   The present invention has been made in view of this point, and an object of the present invention is to provide a dipole or monopole antenna device capable of realizing a significant reduction in size.

本発明のモノポール又はダイポール型のアンテナ装置は、給電点の近傍の磁場領域に当該給電点に接続され平面視で導体が中央部に開口部を有する閉領域を形成する平面コイルを備え、前記平面コイルは、フィルム基板の同一面において境界線を挟んで対向する第1及び第2の区域にそれぞれ形成された導体が、前記フィルム基板を前記境界線を中心に折り曲げることで重なり合い平面視で閉領域を形成したものであり、前記平面コイルによる磁力線放射を放射源としたことを特徴とする。 Monopole or dipole antenna device of the present invention includes a planar coil conductor in a plan view are connected to the feeding point to the magnetic field region near the feed point to form a closed region having an opening in a central portion, said The planar coil is formed by overlapping conductors formed in the first and second areas facing each other across the boundary line on the same surface of the film substrate so that the film substrate is folded around the boundary line and closed in plan view. A region is formed, and a magnetic field radiation by the planar coil is used as a radiation source.

この構成によれば、モノポール又はダイポール型のアンテナ装置でありながら平面コイルによる磁力線放射を放射源とした放射が行われる。しかも、磁場領域のインダクタ(平面コイル)が大きいため、アンテナ共振周波数が低くなり、アンテナ装置の小型化が図られる。   According to this configuration, although the antenna device is of a monopole or dipole type, radiation using magnetic field radiation by a planar coil as a radiation source is performed. Moreover, since the inductor (planar coil) in the magnetic field region is large, the antenna resonance frequency is lowered, and the antenna device can be downsized.

上記モノポール又はダイポール型のアンテナ装置において、複数の平面コイルを接続することもでき、インダクタ(平面コイル)を大きくしてアンテナ共振周波数を低くすることができる。   In the monopole or dipole antenna device, a plurality of planar coils can be connected, and an inductor (planar coil) can be enlarged to lower the antenna resonance frequency.

また本発明は、上記モノポール又はダイポール型のアンテナ装置において、前記平面コイルに接続された他の放射導体を設け、前記他の放射導体による共振電流放射と前記平面コイルによる磁力線放射とを行うことを特徴とする。   According to the present invention, in the above monopole or dipole antenna device, another radiation conductor connected to the planar coil is provided, and resonance current radiation by the other radiation conductor and magnetic field radiation by the planar coil are performed. It is characterized by.

この構成によれば、モノポール又はダイポール型のアンテナ装置として他の放射導体から共振電流放射を行うことができると共に、給電部近傍の平面コイルからは磁力線放射を行うことができる。   According to this configuration, as a monopole or dipole type antenna device, it is possible to radiate resonance current from other radiation conductors, and it is possible to radiate magnetic field lines from a planar coil in the vicinity of the power feeding unit.

また本発明は、上記モノポール又はダイポール型のアンテナ装置において、前記平面コイルに可変容量素子を直列に接続し、前記可変容量素子にチューニング電圧を印加してアンテナ共振周波数を可変としたことを特徴とする。   In the monopole or dipole antenna device according to the present invention, a variable capacitance element is connected in series to the planar coil, and a tuning voltage is applied to the variable capacitance element to make the antenna resonance frequency variable. And

この構成によれば、可変容量素子にチューニング電圧を印加してアンテナ共振周波数を変えることができるので、受信帯域の広帯域化が可能である。   According to this configuration, the tuning voltage can be applied to the variable capacitance element to change the antenna resonance frequency, so that the reception band can be widened.

本発明によれば、アンテナ装置の大幅な小型化を実現することができる。   According to the present invention, the antenna device can be significantly reduced in size.

以下、本発明に係るアンテナ装置の実施の形態について図面を参照して詳細に説明する。
図1(a)(b)は本実施の形態に係るアンテナ装置の模式図であり、同図(a)はアンテナ装置を高開口平面コイルの開口方向から見た平面図、同図(b)はアンテナ装置を高開口平面コイルの側面方向から見た側面図である。
Embodiments of an antenna device according to the present invention will be described below in detail with reference to the drawings.
FIGS. 1A and 1B are schematic views of the antenna device according to the present embodiment. FIG. 1A is a plan view of the antenna device as viewed from the opening direction of the high aperture planar coil, and FIG. FIG. 3 is a side view of the antenna device viewed from the side surface direction of the high aperture planar coil.

本実施の形態に係るアンテナ装置1は、アンテナ中央部に配置した給電部2の一方の側(図中右側)に複数の高開口平面コイル3a,3bが直列に接続され、該給電部2の他方の側(図中左側)に複数の高開口平面コイル4a,4bが直列に接続され、ダイポール型アンテナを構成している。アンテナ装置1において電場領域に当たるアンテナ両端部に共振電流による電界放射のための放射導体5,6が接続されている。図1(a)(b)には給電部2の両側にそれぞれ2つの高開口平面コイル3a,3b及び4a,4bを接続した状態を模式的に示しているが、高開口平面コイルの接続数は所要のアンテナ感度を得られる接続数に設定する。   In the antenna device 1 according to the present embodiment, a plurality of high aperture planar coils 3a and 3b are connected in series on one side (right side in the figure) of a power feeding unit 2 arranged at the center of the antenna. A plurality of high aperture planar coils 4a and 4b are connected in series on the other side (left side in the figure) to form a dipole antenna. In the antenna device 1, radiation conductors 5 and 6 for electric field radiation due to a resonance current are connected to both ends of the antenna that hit the electric field region. FIGS. 1A and 1B schematically show a state in which two high-aperture planar coils 3a, 3b and 4a, 4b are connected to both sides of the power supply unit 2, respectively. Is set to the number of connections that can achieve the required antenna sensitivity.

高開口平面コイル3a,3b及び4a,4bは、磁場領域である給電部2の近傍に配置されている。図1(a)に示すように、高開口平面コイル3aはコイル中央が大きく開口した開口部7を有し、コイル開口方向からの平面視で導体が閉領域(7)を形成している。図1(b)に示すように、高開口平面コイル3aは平面視で導体が閉領域(7)を形成するために、導体同士の一部を上下方向に重ねるように配置している。なお、他の高開口平面コイル3b及び4a,4bも同様の構造を有している。   The high aperture planar coils 3a, 3b and 4a, 4b are arranged in the vicinity of the power feeding unit 2 that is a magnetic field region. As shown in FIG. 1A, the high opening planar coil 3a has an opening 7 having a large opening at the center of the coil, and the conductor forms a closed region (7) in plan view from the coil opening direction. As shown in FIG. 1B, the high-aperture planar coil 3a is arranged so that a part of the conductors overlap in the vertical direction so that the conductors form a closed region (7) in plan view. The other high opening planar coils 3b and 4a, 4b have the same structure.

図2はアンテナ装置1の給電部2及び高開口平面コイル3a,3b及び4a,4bを抜き出した斜視図である。本実施の形態では、平面視で導体が閉領域を形成するように導体を矩形状に四回りさせている。給電部2に対して接続部11を介して高開口平面コイル3aの一端部12が接続されている。高開口平面コイル3aは、給電部2側の一端部12が上下方向において一番高い位置となり、当該一端部12から導体13が同じ高さで矩形状に一回りしている(一回り目の矩形導体13)。一端部12を始点にして矩形に一回りした一回り目の矩形導体13の他端部は一端部12の少し手前で一段下がり、そこから二回り目の矩形導体14が一回り目の矩形導体13の下側を平面視で略同一の位置を矩形状に一回りしている。二回り目の矩形導体14は、一端部12側から見て反対側の辺が一回り目の矩形導体13よりも1ライン分だけ内側を通っていると共に、次段の高開口平面コイル3bとの接続導体15と重なる場所では一段高くなって干渉を避ける構造となっている。また、二回り目の矩形導体14は一回りして戻ってきた一端部12側の辺が一回り目の矩形導体13よりも1ライン分だけ内側を通っている。三回り目の導体16は再び一回り目の矩形導体13と同じ高さに戻り、一回り目及び二回り目の矩形導体13、14よりも1ライン分だけ内側を通り矩形状に一回りしている。そして、四回り目の半矩形導体17が次段の高開口平面コイル3bと近接した場所で二回り目の矩形導体14の形成位置より下まで立下り、そこまで延出している接続導体15の端部に接続している。   FIG. 2 is a perspective view of the antenna device 1 extracted from the feeding portion 2 and the high-aperture planar coils 3a, 3b and 4a, 4b. In the present embodiment, the conductor is rotated four times in a rectangular shape so that the conductor forms a closed region in plan view. One end portion 12 of the high opening planar coil 3 a is connected to the power feeding portion 2 via the connection portion 11. In the high-aperture planar coil 3a, the one end portion 12 on the power feeding unit 2 side is the highest position in the vertical direction, and the conductor 13 goes around in a rectangular shape at the same height from the one end portion 12 (the first turn) Rectangular conductor 13). The other end portion of the first round rectangular conductor 13 that goes round in a rectangle starting from the one end portion 12 is lowered by one step slightly before the one end portion 12, and then the second round rectangular conductor 14 becomes the first round rectangular conductor. The lower side of 13 is rotated around substantially the same position in a rectangular shape in plan view. The second rectangular conductor 14 has a side opposite to the first rectangular conductor 13 as viewed from the one end portion 12 side, and passes through the inner side by one line, and the next-stage high opening planar coil 3b. In a place overlapping with the connection conductor 15, the structure is higher by one step to avoid interference. Further, the second rectangular conductor 14 is turned around one end 12 and passes through the inner side by one line from the first rectangular conductor 13. The third conductor 16 returns to the same height as the first rectangular conductor 13 and passes one line inside the first and second rectangular conductors 13 and 14 and goes around in a rectangular shape. ing. The fourth half-rectangular conductor 17 falls below the position where the second round rectangular conductor 14 is formed at a location close to the next-stage high-aperture planar coil 3b, and the connecting conductor 15 extending there Connected to the end.

このように、一繋がりの矩形導体13,14,16及び半矩形導体17を上下方向に一部重ねて配置することで、高開口平面コイル3aの中央部には大きな開口部7が形成されている。他の高開口平面コイル3bも同様に構成されている。   In this way, by arranging the continuous rectangular conductors 13, 14, 16 and the semi-rectangular conductor 17 so as to partially overlap in the vertical direction, a large opening 7 is formed at the center of the high opening planar coil 3 a. Yes. The other high opening planar coil 3b is similarly configured.

以上のように構成されたアンテナ装置1では、図3に示すように共振電流放射と磁力線放射との異なる放射モードにて放射が行われる。給電部2に高周波電流を供給すると、ダイポールアンテナとして動作し、複数の高開口平面コイル3a等及び高開口平面コイル4a等からなるアンテナ線上に電流と電圧が分布し、中央の給電部2で電流が最大となると共に電圧が最小となり、給電部2から最も離れたアンテナ端部で電流が最小となると共に電界が最大となる。給電部2に供給される高周波電流がアンテナ装置1の共振周波数と一致する場合は、図3に示すように、アンテナ端部の放射導体(5,6及び給電部2から離れて磁場の弱い領域に配置された高開口平面コイル)での共振電流放射(共振電流による放射)が最も強くなる。共振電流放射の方向はアンテナ装置1の長手方向となる。   In the antenna device 1 configured as described above, radiation is performed in different radiation modes of resonance current radiation and magnetic field radiation as shown in FIG. When a high-frequency current is supplied to the power feeding unit 2, it operates as a dipole antenna, and current and voltage are distributed on an antenna line composed of a plurality of high aperture planar coils 3 a and the like and a high aperture planar coil 4 a and the like. Is maximized and the voltage is minimized, and the current is minimized and the electric field is maximized at the end of the antenna farthest from the feeding unit 2. When the high-frequency current supplied to the power feeding unit 2 matches the resonance frequency of the antenna device 1, as shown in FIG. 3, the radiation conductors 5 and 6 at the end of the antenna are separated from the power feeding unit 2 and have a weak magnetic field. Resonance current radiation (radiation by resonance current) in the high-aperture planar coil arranged at the maximum is the strongest. The direction of resonance current radiation is the longitudinal direction of the antenna device 1.

一方、給電部2の近傍では高開口平面コイル3a、3b及び高開口平面コイル4a、4bにより強い磁場領域が形成されており、高開口平面コイル3a等及び高開口平面コイル4a等が発生させた磁界によって図3に示すように、磁力線放射が行われる。給電部2に供給される高周波電流がアンテナ装置1の共振周波数と一致する場合に最大の共振電流が流れるので、その時の磁力線放射が最大となる。   On the other hand, a strong magnetic field region is formed by the high aperture planar coils 3a and 3b and the high aperture planar coils 4a and 4b in the vicinity of the power feeding unit 2, and the high aperture planar coil 3a and the high aperture planar coil 4a and the like are generated. As shown in FIG. 3, magnetic field radiation is performed by the magnetic field. Since the maximum resonance current flows when the high-frequency current supplied to the power feeding unit 2 matches the resonance frequency of the antenna device 1, the magnetic field line radiation at that time becomes maximum.

また、本実施の形態では、Qの低い放射しやすいインダクタンス(L)を高開口平面コイル3a等及び高開口平面コイル4a等で構成している。給電部2の近傍は磁場領域であり、そこに大きなインダクタンス(L)が配置されるので、アンテナ装置1の共振周波数が低くなる効果がある。   Further, in the present embodiment, an inductance (L) having a low Q that is easy to radiate is constituted by the high aperture planar coil 3a and the like and the high aperture planar coil 4a and the like. The vicinity of the power feeding unit 2 is a magnetic field region, and a large inductance (L) is disposed there, which has an effect of reducing the resonance frequency of the antenna device 1.

図4は本実施の形態に係るアンテナ装置1の小型化効果を検証したアンテナ共振周波数のシミュレーション結果を示す図である。アンテナ長LはL=150mmに設定している。本実施の形態に示すようにアンテナ線を高開口平面コイル3a等及び高開口平面コイル4a等で構成した場合、アンテナ共振周波数は200MHz付近であった。一方、図10(a)のように直線状の1/2波長の導体で構成した場合のアンテナ共振周波数は1000MHz付近であり、図10(b)のようにミアンダラインで構成した場合のアンテナ共振周波数は500MHz付近である。   FIG. 4 is a diagram showing a simulation result of the antenna resonance frequency that verifies the miniaturization effect of the antenna device 1 according to the present embodiment. The antenna length L is set to L = 150 mm. As shown in the present embodiment, when the antenna wire is composed of the high aperture planar coil 3a and the like and the high aperture planar coil 4a and the like, the antenna resonance frequency is around 200 MHz. On the other hand, the antenna resonance frequency in the case of a linear half-wave conductor as shown in FIG. 10A is around 1000 MHz, and the antenna resonance in the case of a meander line as shown in FIG. 10B. The frequency is around 500 MHz.

このように、本実施の形態によるアンテナ装置1の共振周波数はミアンダラインで構成した場合の1/2以下になっているので、アンテナ長はミアンダラインで構成した場合の1/2以下まで短縮することができることになる。よって、特許文献1のように誘電体部材の比誘電率による受信信号波長の短縮効果を利用する場合に比べて、大幅な小型化効果を奏することができる。   As described above, since the resonance frequency of the antenna device 1 according to the present embodiment is ½ or less of that of the meander line, the antenna length is reduced to ½ or less of that of the meander line. Will be able to. Therefore, compared with the case of using the shortening effect of the received signal wavelength due to the relative permittivity of the dielectric member as in Patent Document 1, it is possible to achieve a significant downsizing effect.

次に、アンテナ共振周波数を可変にしたアンテナ装置の変形例を説明する。
図5は共振周波数を可変にしたアンテナ装置の模式図である。同図に示すアンテナ装置20は、基本的な構成は上記した図1(a)(b)に示すアンテナ装置1と同一構成を有しており、同一部分には同一符号を付して説明の重複を避ける。
Next, a modification of the antenna device in which the antenna resonance frequency is made variable will be described.
FIG. 5 is a schematic diagram of an antenna device with a variable resonance frequency. The antenna device 20 shown in the figure has the same basic configuration as the antenna device 1 shown in FIGS. 1A and 1B described above, and the same parts are denoted by the same reference numerals. Avoid duplication.

アンテナ装置20では、高開口平面コイル3a(4a)と高開口平面コイル3b(4b)との間に可変容量素子としてバラクタダイオード21a,22aをそれぞれ直列に接続している。バラクタダイオード21a,22aの各カソードを抵抗R3,R4を介してグランドに接続し、各アノードに抵抗R1,R2を介してチューニング電圧VTを印加するように構成している。その他の構成はアンテナ装置1と同様である。   In the antenna device 20, varactor diodes 21a and 22a are connected in series as variable capacitance elements between the high aperture planar coil 3a (4a) and the high aperture planar coil 3b (4b), respectively. Each cathode of the varactor diodes 21a and 22a is connected to the ground via resistors R3 and R4, and a tuning voltage VT is applied to each anode via resistors R1 and R2. Other configurations are the same as those of the antenna device 1.

以上のように構成されたアンテナ装置20では、高開口平面コイル3a等及び高開口平面コイル4a等とバラクタダイオード21a,22aとで共振回路を形成する。高開口平面コイル3a、4aのインダクタ値をL1、高開口平面コイル3b、4bのインダクタ値をL2とし、バラクタダイオード21a,22aの容量をCとする。アンテナ装置20の共振周波数Foは、次の通りとなる。
Fo=1/2π((CTTL・(L1+L2)))1/2
なお、CTTLはアンテンのTotal等価容量であり、Cの値に直結している。
したがって、バラクタダイオード21a,22aの容量Cを可変させることで共振周波数Foがシフトする。
In the antenna device 20 configured as described above, a resonant circuit is formed by the high aperture planar coil 3a and the like, the high aperture planar coil 4a and the like, and the varactor diodes 21a and 22a. High opening flat coil 3a, the inductor value of 4a L1, high opening flat coils 3b, 4b of the inductor value and L2, to the varactor diode 21a, a capacity 22a and C T. The resonance frequency Fo of the antenna device 20 is as follows.
Fo = 1 / 2π ((C TTL · (L1 + L2))) 1/2
Incidentally, C TTL is Total equivalent capacitance of the saddle, it is directly linked to the value of C T.
Accordingly, the varactor diode 21a, the resonant frequency Fo by varying the capacitance C T of 22a shifts.

このようなアンテナ装置20によれば、共振電流放射と磁力線放射の放射源として小型化可能であると共に、共振周波数Foを可変することができるので受信周波数を広帯域化でき、テレビジョン放送のような広帯域の信号を受信可能になる。   According to the antenna device 20 as described above, it can be miniaturized as a radiation source for resonance current radiation and magnetic field radiation, and the resonance frequency Fo can be varied, so that the reception frequency can be widened. A wideband signal can be received.

図6は平面コイルの形状を変えたアンテナ装置の変形例を示す図であり、給電部及びそこに接続された平面コイルを拡大して示す図である。平面コイル3a,4aは、所定の太さを有する線状の導体18が平面内で外側から内側に向けて矩形状に3回転し、導体18の中央端部を矩形状に巻かれた導体の下を通して次の平面コイル3b,4bの一端部に接続している。平面コイル3a,4aと次段の平面コイル3b,4bとの間にバラクタダイオード21a,22aを直列接続している。   FIG. 6 is a view showing a modification of the antenna device in which the shape of the planar coil is changed, and is an enlarged view showing the power feeding unit and the planar coil connected thereto. The planar coils 3a and 4a are conductors in which a linear conductor 18 having a predetermined thickness is rotated three times in a rectangular shape from the outside to the inside in a plane, and the central end of the conductor 18 is wound in a rectangular shape. It is connected to one end of the next planar coils 3b and 4b through the bottom. Varactor diodes 21a and 22a are connected in series between the planar coils 3a and 4a and the subsequent planar coils 3b and 4b.

このような平面コイルを用いてアンテナ装置を構成した場合も、導体18が平面視で閉領域を形成するので、共振電流放射と磁力線放射との異なる放射モードにて放射が行われる。そして、Qの低い放射しやすいインダクタンス(L)を平面コイルで構成しているので、磁場領域に大きなインダクタンス(L)が配置され、アンテナ装置の共振周波数を低くしてアンテナ長の小型化を図ることができる。
なお、アンテナ装置において、平面視で閉領域を形成して磁力線放射の放射源となる高開口平面コイルの製造方法及びコイル形状について説明する。
Even when an antenna device is configured using such a planar coil, since the conductor 18 forms a closed region in plan view, radiation is performed in different radiation modes of resonance current radiation and magnetic field radiation. Since the inductance (L) having a low Q that is easy to radiate is formed by a planar coil, a large inductance (L) is arranged in the magnetic field region, and the resonance frequency of the antenna device is lowered to reduce the antenna length. be able to.
In the antenna device, a manufacturing method and a coil shape of a high-aperture planar coil that forms a closed region in a plan view and serves as a radiation source for magnetic field radiation will be described.

図7(a)に示すように、絶縁性の可撓性フィルムからなるフィルム基板31の上半分の領域32に折り曲げ線上の一辺が開放した矩形状の導体パターン34a〜34dを所定間隔で形成する。また、フィルム基板31の下半分の領域33に折り曲げ線上の一辺の中間部が開放した矩形状の導体パターン35a〜35dを上側の導体パターン34a〜34dに対して略半周期ずらして所定間隔で形成する。   As shown in FIG. 7A, rectangular conductor patterns 34a to 34d with one side on the folding line opened are formed at predetermined intervals in the upper half region 32 of the film substrate 31 made of an insulating flexible film. . In addition, rectangular conductor patterns 35a to 35d having an intermediate portion on one side of the folding line opened in the lower half region 33 of the film substrate 31 are formed at predetermined intervals with a substantially half cycle shift with respect to the upper conductor patterns 34a to 34d. To do.

次に、折り曲げ線を中心にしてフィルム基板31を折り曲げることにより、図7(b)に示すように矩形状の導体の閉領域36a〜36gが所定の間隔で連続する複数の平面コイルが形成される。   Next, by bending the film substrate 31 around the fold line, a plurality of planar coils in which closed regions 36a to 36g of rectangular conductors continue at a predetermined interval as shown in FIG. 7B are formed. The

図8(a)(b)は導体による真円状の閉領域が形成される平面コイルの製造方法を例示している。図8(a)に示すように、フィルム基板31の上半分の領域32に折り曲げ線上の直線部が開放した長円状の導体パターン37a〜37cを所定間隔で形成する。また、フィルム基板31の下半分の領域33に折り曲げ線上の直線部が開放した長円状の導体パターン38a、38bを上側の導体パターン37a〜37cに対して略半周期ずらして所定間隔で形成する。   8A and 8B illustrate a method for manufacturing a planar coil in which a perfect circular closed region is formed by a conductor. As shown in FIG. 8A, oval conductor patterns 37 a to 37 c in which straight portions on the folding line are opened are formed at predetermined intervals in the upper half region 32 of the film substrate 31. Further, in the lower half region 33 of the film substrate 31, the ellipsoidal conductor patterns 38a and 38b whose straight lines on the folding line are opened are formed at predetermined intervals with a substantially half cycle shift with respect to the upper conductor patterns 37a to 37c. .

次に、折り曲げ線を中心にしてフィルム基板31を折り曲げることにより、図8(b)に示すように長円状の導体パターン37a〜37c及び導体パターン38a、38bの曲線部が重なり合い円形の閉領域39a〜39dが所定の間隔で連続する複数の平面コイルが形成される。   Next, by bending the film substrate 31 around the fold line, the curved portions of the ellipsoidal conductor patterns 37a to 37c and the conductor patterns 38a and 38b overlap with each other as shown in FIG. A plurality of planar coils in which 39a to 39d are continuous at a predetermined interval are formed.

図9(a)(b)は導体による半円状の閉領域が形成される平面コイルの製造方法を例示している。図9(a)に示すように、フィルム基板31の上半分の領域32に折り曲げ線上の一辺が開放した矩形状の導体パターン34a〜34dを所定間隔で形成する。また、フィルム基板31の下半分の領域33に折り曲げ線上の直線部が開放した長円状の導体パターン41a〜41dを上側の導体パターン34a〜34dに対して略半周期ずらして所定間隔で形成する。   9A and 9B illustrate a method for manufacturing a planar coil in which a semicircular closed region is formed by a conductor. As shown in FIG. 9A, rectangular conductor patterns 34a to 34d having one side on the folding line opened in the upper half region 32 of the film substrate 31 are formed at predetermined intervals. In addition, in the lower half region 33 of the film substrate 31, the oval conductor patterns 41a to 41d whose straight lines on the folding line are opened are formed at predetermined intervals with a substantially half cycle shift with respect to the upper conductor patterns 34a to 34d. .

次に、折り曲げ線を中心にしてフィルム基板31を折り曲げることにより、図9(b)に示すように矩形状の導体パターン34a〜34d及び長円状の導体パターン41a〜41dの曲線部が重なり会い半円形の閉領域42a〜42gが所定の間隔で連続する複数の平面コイルが形成される。   Next, by bending the film substrate 31 around the bend line, the curved portions of the rectangular conductor patterns 34a to 34d and the oval conductor patterns 41a to 41d overlap each other as shown in FIG. 9B. A plurality of planar coils in which semicircular closed regions 42a to 42g are continuous at a predetermined interval are formed.

以上の説明ではダイポール型アンテナを例に説明したが、モノポール型アンテナであっても同様に適用可能である。   In the above description, a dipole antenna has been described as an example, but a monopole antenna can be similarly applied.

本発明は、ダイポール又はモノポール型のアンテナ装置に適用可能である。   The present invention is applicable to a dipole or monopole antenna device.

(a)本実施の形態に係るアンテナ装置の模式図であり、高開口平面コイルの開口方向から見た平面図、(b)アンテナ装置を高開口平面コイルの側面方向から見た側面図(A) It is the schematic diagram of the antenna apparatus which concerns on this Embodiment, and the top view seen from the opening direction of the high opening planar coil, (b) The side view which looked at the antenna apparatus from the side direction of the high opening planar coil 本実施の形態に係るアンテナ装置の給電部及び高開口平面コイルを抜き出した斜視図The perspective view which extracted the electric power feeding part and high opening planar coil of the antenna device which concerns on this Embodiment 本実施の形態に係るアンテナ装置の共振電流放射及び磁力線放射を示す図The figure which shows the resonance current radiation | emission and magnetic field radiation | emission of the antenna apparatus which concerns on this Embodiment 本実施の形態に係るアンテナ装置の小型化効果を検証した共振周波数のシミュレーション結果を示す図The figure which shows the simulation result of the resonant frequency which verified the miniaturization effect of the antenna device which concerns on this Embodiment 共振周波数を可変にしたアンテナ装置の模式図Schematic diagram of antenna device with variable resonance frequency 平面コイルの形状を変えたアンテナ装置の変形例を示す図The figure which shows the modification of the antenna device which changed the shape of the plane coil (a)矩形状の高開口平面コイルの製造方法において折り曲げ前の状態を示す平面図、(b)折り曲げ後の状態を示す平面図(A) The top view which shows the state before bending in the manufacturing method of a rectangular high opening planar coil, (b) The top view which shows the state after bending (a)円形の高開口平面コイルの製造方法において折り曲げ前の状態を示す平面図、(b)折り曲げ後の状態を示す平面図(A) The top view which shows the state before bending in the manufacturing method of a circular high opening planar coil, (b) The top view which shows the state after bending (a)半円形の高開口平面コイルの製造方法において折り曲げ前の状態を示す平面図、(b)折り曲げ後の状態を示す平面図(A) The top view which shows the state before bending in the manufacturing method of a semicircle high opening planar coil, (b) The top view which shows the state after bending (a)ダイポールアンテナの模式図、(b)ミアンダ型のダイポールアンテナの模式図(A) Schematic diagram of dipole antenna, (b) Schematic diagram of meander-type dipole antenna

符号の説明Explanation of symbols

1…アンテナ装置、2…給電部、3a,3b,4a,4b…高開口平面コイル、5,6…コンデンサ、11…接続部、12…高開口平面コイル一端部、13…矩形導体(一回り目)、14…矩形導体(二回り目)、15…接続導体、16…矩形導体(三回り目)、17…半矩形導体(四回り目)、21a,22a…バラクタダイオード、31…フィルム基板、32…上半分の領域、33…下半分の領域、34a〜34d…導体パターン(上側)、35a〜35d…導体パターン(下側)
DESCRIPTION OF SYMBOLS 1 ... Antenna apparatus, 2 ... Feeding part, 3a, 3b, 4a, 4b ... High opening planar coil, 5, 6 ... Capacitor, 11 ... Connection part, 12 ... One end part of high opening planar coil, 13 ... Rectangular conductor (one round 14) Rectangular conductor (second turn), 15 ... Connection conductor, 16 ... Rectangular conductor (third turn), 17 ... Semi-rectangular conductor (fourth turn), 21a, 22a ... Varactor diode, 31 ... Film substrate 32 ... Upper half region, 33 ... Lower half region, 34a-34d ... Conductor pattern (upper side), 35a-35d ... Conductor pattern (lower side)

Claims (4)

給電点の近傍の磁場領域に当該給電点に接続され平面視で導体が中央部に開口部を有する閉領域を形成する平面コイルを備え、前記平面コイルは、フィルム基板の同一面において境界線を挟んで対向する第1及び第2の区域にそれぞれ形成された導体が、前記フィルム基板を前記境界線を中心に折り曲げることで重なり合い平面視で閉領域を形成したものであり、前記平面コイルによる磁力線放射を放射源としたことを特徴とするモノポール又はダイポール型のアンテナ装置。 The planar coil includes a planar coil connected to the feeding point in the vicinity of the feeding point and forming a closed region in which the conductor has an opening in the center in plan view, and the planar coil has a boundary line on the same surface of the film substrate. The conductors formed respectively in the first and second areas facing each other are formed by folding the film substrate around the boundary line to form a closed region in plan view, and the magnetic field lines generated by the planar coil A monopole or dipole antenna device characterized in that radiation is used as a radiation source. 前記平面コイルが複数接続されていることを特徴とする請求項1記載のモノポール又はダイポール型のアンテナ装置。   The monopole or dipole antenna device according to claim 1, wherein a plurality of the planar coils are connected. 前記平面コイルに接続された他の放射導体を設け、
前記他の放射導体による共振電流放射と前記平面コイルによる磁力線放射とを行うことを特徴とする請求項1または請求項2に記載のモノポール又はダイポール型のアンテナ装置。
Providing another radiation conductor connected to the planar coil;
3. The monopole or dipole antenna device according to claim 1 , wherein resonance current radiation by the other radiation conductor and magnetic field radiation by the planar coil are performed.
前記平面コイルに可変容量素子を直列に接続し、前記可変容量素子にチューニング電圧を印加してアンテナ共振周波数を可変としたことを特徴とする請求項1から請求項3のいずれかに記載のモノポール又はダイポール型のアンテナ装置。 The monolithic capacitor according to any one of claims 1 to 3 , wherein a variable capacitance element is connected in series to the planar coil, and a tuning voltage is applied to the variable capacitance element to change an antenna resonance frequency. Pole or dipole antenna device.
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GB201300513D0 (en) * 2013-01-11 2013-02-27 Roke Manor Research A dipole antenna
JP7170319B2 (en) * 2019-02-21 2022-11-14 国立大学法人京都工芸繊維大学 antenna device
JP7574665B2 (en) * 2021-01-26 2024-10-29 Toppanホールディングス株式会社 Antenna and contactless data transmitter and receiver
CN113889763A (en) * 2021-11-08 2022-01-04 山东炎一智能科技有限公司 FPC antenna and electronic device
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