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WO2012144252A1 - Electrode structure for electric field communication - Google Patents

Electrode structure for electric field communication Download PDF

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Publication number
WO2012144252A1
WO2012144252A1 PCT/JP2012/052774 JP2012052774W WO2012144252A1 WO 2012144252 A1 WO2012144252 A1 WO 2012144252A1 JP 2012052774 W JP2012052774 W JP 2012052774W WO 2012144252 A1 WO2012144252 A1 WO 2012144252A1
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Prior art keywords
electrode
electric field
field communication
electrode structure
transmission medium
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French (fr)
Japanese (ja)
Inventor
四方 勝
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Alps Alpine Co Ltd
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Alps Electric Co Ltd
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    • HELECTRICITY
    • H04ELECTRIC COMMUNICATION TECHNIQUE
    • H04BTRANSMISSION
    • H04B13/00Transmission systems characterised by the medium used for transmission, not provided for in groups H04B3/00 - H04B11/00
    • H04B13/005Transmission systems in which the medium consists of the human body

Definitions

  • the present invention relates to an electrode structure for electric field communication applicable to electric field communication for transmitting and receiving information through a transmission medium such as a human body.
  • This electric field communication system includes a transmission medium such as a human body, a transmitter that generates an electric field corresponding to an information signal, and a receiver that detects a potential variation of the transmission medium and demodulates the information signal.
  • the transmitter electrode and the transmission medium, and the receiver electrode and the transmission medium are capacitively coupled, and communication is performed between the transmitter and the receiver by this capacitive coupling.
  • a parallel plate structure has been proposed as an electrode (electrode structure for electric field communication) of a transceiver used for electric field communication (see, for example, Patent Document 1).
  • This electrode structure for electric field communication has two flat conductors arranged substantially in parallel and an insulator arranged between them, and a ground potential is applied to one flat conductor and a signal potential is applied to the other flat conductor. Is to be given.
  • a transmission medium such as a human body comes close to a flat conductor to which a signal potential is applied, a potential fluctuation corresponding to the signal potential occurs in the transmission medium, and communication becomes possible.
  • the electric field between the flat conductors is very large, so even if a human body is close to the other flat conductor, almost no electric field is generated on the transmission medium side, and the potential fluctuation of the transmission medium occurs. Becomes extremely small.
  • the potential fluctuation of the transmission medium is reduced, the signal intensity received by the receiving electrode is also reduced, and communication errors frequently occur.
  • a communication error can be reduced by providing a matching circuit on the transmission side, in this case, the matching circuit increases the number of parts of the transmission side device and increases the manufacturing cost. Further, if the distance between the flat conductors is increased, it is expected that there is an effect that the loss to the COLD electrode side to which the ground potential is applied can be suppressed, but there is a problem that the electrode structure becomes large.
  • the present invention has been made in view of the above points, and an object of the present invention is to provide an electrode structure for electric field communication having good communication characteristics, which can prevent an increase in the number of parts and an increase in size of the electrode structure itself.
  • the electrode structure for electric field communication includes a first electrode connected to a fixed potential, and a second electrode arranged to face the first electrode and provided with a feeding point, and the second electrode
  • the second electrode In the electrode structure for electric field communication in which is an electrode adjacent to the transmission medium, the second electrode has the first electrode at a location away from the feeding point by a predetermined distance or more so that the electric resistance of the current path length is a predetermined value or more. It is connected to an electrode.
  • the second electrode is connected to the first electrode at a location that is a predetermined distance or more away from the feeding point so that the electric resistance of the current path length is a predetermined value or more, the number of parts is increased.
  • an electrode structure for electric field communication with good communication characteristics can be realized.
  • the first and second electrodes have a rectangular shape with the same outer region, and the feeding point of the second electrode is provided at the end of the first side of the square.
  • the first electrode may be connected to any part of the second side facing the first side or the entire second side.
  • each of the first and second electrodes has a structure in which one rectangular electrode is bent at an intermediate position in the longitudinal direction, and the first electrode and the first electrode are bent at a bent portion. Two electrodes may be connected.
  • the first electrode is constituted by a flat plate conductor extending in a region facing the second electrode, and the second electrode is constituted by a meander shape or other fine line pattern. May be.
  • the present invention it is possible to prevent an increase in the number of parts and prevent an increase in the size of the electrode structure itself, thereby providing an electrode structure for electric field communication with good communication characteristics.
  • FIG. 1 is a perspective view showing a configuration of an electrode structure for electric field communication according to Embodiment 1.
  • FIG. 1 is a plan view showing a configuration of an electric field communication electrode structure according to Embodiment 1.
  • FIG. It is a schematic diagram which shows a simulation model. It is a perspective view which shows the electrode structure (model B) for electric field communication of a parallel plate structure. It is a perspective view which shows the electrode structure (model C) for electric field communication of a parallel plate structure. It is a table
  • FIG. 1 is a schematic diagram showing a configuration example of an electric field communication system in which the electric field communication electrode structure according to the present embodiment is used.
  • the electric field communication system shown in FIG. 1 includes a transmitter 1 that modulates an information signal to generate an electric field corresponding to the information signal, and a transmission medium 2 such as a human body that transmits the information signal by the electric field generated by the transmitter 1. And a receiver 3 that demodulates an information signal by detecting a potential fluctuation that becomes an electric field propagating through the transmission medium 2.
  • the transmitter 1 may be a transceiver having a reception function
  • the receiver 3 may be a transceiver having a transmission function.
  • the present invention can be easily applied to two-way communication.
  • the transmitter 1 is a control unit 11 such as a computer that performs signal transmission control, a transmission unit 12 that modulates an information signal from the control unit 11 to generate an RF signal, and an RF signal from the transmission unit 12 And an electric field communication electrode structure 13 for generating an electric field.
  • the transmitter 12 and the electric field communication electrode structure 13 are connected via a coaxial cable L.
  • the control unit 11 is configured to supply the information signal in the intermediate frequency band to the transmission unit 12 and to supply the power supply potential Vdd and the ground GND that is a fixed potential.
  • the transmission unit 12 includes a modulation circuit (not shown) and the like, and is configured to be able to generate an RF signal by modulating an information signal (IF) from the control unit 11.
  • the transmitter 12 generates an RF signal and supplies the RF signal to the electric field communication electrode structure 13 through the coaxial cable L.
  • the electrode structure 13 for electric field communication includes a first electrode 131 to which a ground potential (GND) as a fixed potential is applied, a second electrode 132 to which an RF signal (signal potential) from the control unit 11 is fed, and a first electrode 131 and an insulator 133 interposed between the second electrode 132 and an electric field corresponding to the RF signal from the transmitter 12 can be generated.
  • GND ground potential
  • the transmission medium 2 is a medium having predetermined conductivity such as a human body.
  • an electrostatic capacity is generated between the second electrode 132 and the transmission medium 2, and the second electrode 132 and the transmission medium 2 Are capacitively coupled. For this reason, when an RF signal is supplied to the second electrode 132, the potential of the transmission medium 2 varies according to the signal potential of the RF signal.
  • the receiver 3 includes a first electrode 31 for forming a capacitance with the transmission medium 2 and a second electrode 32 disposed so as to oppose the first electrode 31.
  • a first electrode 31 for forming a capacitance with the transmission medium 2
  • a second electrode 32 disposed so as to oppose the first electrode 31.
  • an electrostatic capacitance is generated between the transmission medium 2 and the first electrode 31, and the transmission medium 2 and the first electrode 31 are capacitively coupled.
  • the potential of the transmission medium 2 fluctuates in accordance with the signal potential of the RF signal
  • the potential of the first electrode 31 that is capacitively coupled also fluctuates in the same manner. Therefore, the potential fluctuation of the first electrode 31 is detected and a demodulation circuit (not shown) is used. By demodulating, an information signal can be received.
  • FIG. 2 is a perspective view showing the configuration of the electrode structure 13 for electric field communication according to the present embodiment.
  • FIG. 3 is a plan view showing the configuration of the electric field communication electrode structure 13 according to the present embodiment.
  • 3A mainly shows a configuration of the first electrode 131
  • FIG. 3B mainly shows a configuration of the second electrode 132
  • FIG. 3C shows a cross section taken along the arrow AA in FIGS.
  • the electric field communication electrode structure 13 includes a first electrode 131 formed of a flat conductor, a second electrode 132 disposed so as to face the first electrode 131, and a first electrode 131.
  • the insulator 133 is disposed between the first electrode 131 and the second electrode 132.
  • the first electrode 131 is a flat electrode having a substantially rectangular planar shape, and is configured to be supplied with a ground potential (GND).
  • the potential applied to the first electrode 131 is not limited to the ground potential (GND) as long as it is a fixed potential.
  • the planar shape of the first electrode 131 is not limited to a substantially rectangular shape, and may be various shapes such as a substantially circular shape and a substantially polygonal shape.
  • the first electrode 131 is not limited to a so-called solid electrode, and may be formed in a desired pattern.
  • the second electrode 132 is formed in a current path length (in this example, a meander shape) with an electrical resistance value equal to or greater than a predetermined value, and the RF from the transmitter 12 is fed to a feeding point a provided at one end of the current path length. The signal is fed. More specifically, the second electrode 132 is an outer region that is disposed away from the first electrode 131 in a direction (vertical direction) perpendicular to the main surface of the first electrode 131 so as to face the first electrode 131. Is formed of a conductor having a rectangular meander pattern substantially the same as that of the first electrode 131.
  • the meander pattern of the second electrode 132 is composed of a plurality of straight portions that are substantially parallel to the side e1 that forms the rectangle of the outer region, and a plurality of folded portions that connect adjacent straight portions to each other.
  • the first straight portion extending from the feeding point a is connected to the first folded portion at the end opposite to the feeding point a (side e2 side), and the first folded portion is connected to the first straight portion. It is connected to the adjacent second straight line portion.
  • the second straight line portion is connected to the second folded portion at the end on the feeding point a side (side e3 side), and the second folded portion is connected to the third straight line portion.
  • the meander pattern is configured by providing such a repeating pattern of straight and folded portions up to the vicinity of the side e4.
  • the electric resistance of the second electrode 132 can be made higher than that of the flat conductor by making the second electrode 132 a thin line pattern having a predetermined current path length.
  • the thin line pattern is not limited to the meander pattern, and other patterns such as a spiral pattern may be used.
  • the length of the thin line pattern serving as the current path length can be appropriately set according to a desired electric resistance value or the like.
  • the second electrode 132 is connected to the first electrode 131 at a predetermined distance (point or straight line) from the feeding point a. More specifically, the second electrode 132 is connected to the first electrode 131 in a region b near the end point on the opposite side to the feeding point a of the meander pattern. In other words, the second electrode 132 is connected to the first electrode 131 in the region b near the side e4 facing the side e1 on the feeding point a side. However, the first electrode 131 and the second electrode 132 may be connected at least at one point, and may not be connected in a region having a range such as the region b.
  • the second electrode 132 is configured by a thin line pattern having a predetermined current path length, and is connected to the first electrode 131 in the region b at a predetermined distance from the feeding point a.
  • the electrode structure 13 can be realized.
  • the first electrode 131 and the second electrode 132 are a substantially rectangular single electrode having a flat plate area constituting the first electrode 131 and a fine line pattern area constituting the second electrode 132. It is configured to be bent at an intermediate position in the longitudinal direction that becomes a boundary with the region. By bending the single electrode in this manner, an electrode structure in which the first electrode 131 and the second electrode 132 are connected in the region b can be realized. However, the separate first electrode 131 and second electrode 132 may be connected.
  • the insulator 133 is configured to insulate the first electrode 131 and the second electrode 132 and to keep the distance between the first electrode 131 and the second electrode 132 substantially constant. For example, when the thickness of the insulator 133 is 3 mm, the distance between the first electrode 131 and the second electrode 132 can be maintained at about 3 mm. Note that the insulator 133 may be omitted as long as the first electrode 131 and the second electrode 132 can be separated and insulated. For example, a spacer may be disposed under the second electrode 132 and insulation may be realized by air.
  • FIG. 4 is a schematic diagram showing a simulation model for confirming the communication characteristics of the electrode structure 13 for electric field communication.
  • Transmission medium 2 corresponding to a human body using electric field communication electrode structure 13 as an electrode (floor electrode) of transmitter 1, having an electric conductivity of 0.62 S / m, a relative dielectric constant of 162.5, and a height of 1.4 m.
  • a simulation was performed assuming that As shown in FIG. 4, the electrode structure of the receiver 3 is a parallel plate structure including a first electrode 31 made of a flat plate conductor and a second electrode 32 made of a flat plate conductor. Further, the distance between the first electrode 131 and the second electrode 132 of the electrode structure 13 for electric field communication was set to 3 mm (model A).
  • FIG. 5 is a perspective view showing a configuration of an electric field communication electrode structure 14a as a comparative example.
  • the electrode structure for electric field communication 14a is a parallel plate structure including a first electrode 141a made of a flat plate conductor and a second electrode 142a made of a flat plate conductor.
  • the distance between the first electrode 141a and the second electrode 142a was 3 mm (model B).
  • the first electrode 141a and the second electrode 142a are connected in the electric field communication electrode structure 14a having a parallel plate structure, the first electrode 141a and the second electrode 142a are not connected because communication is impossible.
  • FIG. 6 is a perspective view showing a configuration of an electrode structure for electric field communication 14b as a comparative example.
  • the electrode structure for electric field communication 14b is a parallel plate structure including a first electrode 141b made of a flat plate conductor and a second electrode 142b made of a flat plate conductor.
  • the distance between the first electrode 141b and the second electrode 142b was 100 mm (model C).
  • the first electrode 141b and the second electrode 142b are not connected.
  • the same simulation was performed using the electric field communication electrode structure in which the first electrode 131 and the second electrode 132 of the electric field communication electrode structure 13 are not connected. Except for the point that the first electrode 131 and the second electrode 132 are not connected, the configuration was the same as the electrode structure for electric field communication 13 (model D).
  • FIG. 7 is a table showing simulation results.
  • the impedance value is 15 ⁇ or more, and the transmission loss is the smallest among the models A to D.
  • the transmission loss is minimized in the model A because the first electrode 131 and the second electrode 132 are connected so that the electric resistance of the current path length is equal to or greater than a predetermined value.
  • model B with a parallel plate structure has a small impedance value of 0.37 ⁇ and a large transmission loss.
  • the impedance value is as high as 13.7 ⁇ , and the transmission loss is suppressed to some extent.
  • the electrical resistance component occupying the impedance value is sufficiently small.
  • the distance between the first electrode 141b and the second electrode 142b is as extremely large as 100 mm.
  • the impedance value is as high as 12.0, but the transmission loss is large.
  • the transmission loss of the model A is improved by about 8 dB.
  • the received electric field intensity received by the first electrode 31 of the receiver 3 in the model A is about 2.5 times that in the model B.
  • good communication characteristics can be realized by greatly increasing the received electric field strength.
  • Model C corresponding to the case where the electrode structure for electric field communication 14b is used can achieve a certain degree of communication characteristics.
  • the electrode structure for electric field communication is The problem that it will enlarge will arise.
  • the communication characteristics do not reach that of model A.
  • the model A using the electric field communication electrode structure 13 can achieve better communication characteristics than the model C, and the electric field communication electrode structure can be made thinner and smaller than the model C. .
  • model D The communication characteristics of model D are worse than model A. From comparison between model A and model D, it can be seen that a short circuit between the first electrode 131 and the second electrode 132 is necessary to improve the communication characteristics.
  • a parallel plate structure such as the electric field communication electrode structure 14a and the electric field communication electrode structure 14b
  • electric field communication cannot be performed even if the first electrode and the second electrode made of a flat plate conductor are connected. This is because the electric resistance of the flat conductor itself constituting the second electrode is extremely low, and when the first electrode and the second electrode are connected, the second electrode is strongly influenced by the first electrode and the electric field due to the RF signal is generated. This is thought to be due to almost no generation. That is, it is important to increase the electric resistance of the current path by configuring the second electrode with a fine line pattern or the like.
  • the electrical resistance of the current path is increased, but in this case, the transmission loss is not improved.
  • two flat electrodes are formed using a material such as a silver paste (conductive paste in which silver particles and resin are mixed) having a lower conductivity than copper used in ordinary printed circuit boards. Even if a parallel plate structure in which the two electrodes are short-circuited is used, the transmission loss is not improved. From this, by using a material with high conductivity (for example, a material having a conductivity of 10 5 (S / m) or more: copper, aluminum, silver, gold, and alloys thereof, etc.) and devising an electrode pattern, etc. It can be said that increasing the electrical resistance is important.
  • the electrode structure for electric field communication in which the second electrode 132 is connected to the first electrode 131 at a location b that is a predetermined distance or more away from the feeding point a so that the electric resistance of the current path length is a predetermined value or more. 13 (model A) shows that good communication characteristics can be realized even if the thickness is thin.
  • the first electrode and the second electrode are connected at a location away from the feeding point by a predetermined distance or more so that the electric resistance of the current path becomes a predetermined value or more.
  • this invention is not limited to description of the said embodiment, It can change suitably in the aspect in which the effect is exhibited, and can be implemented.
  • the electrical resistance is expressed as an electrical parameter of the current path, but it can also be expressed by an impedance including the electrical resistance.
  • the structures, methods, and the like described in the above embodiments can be combined as appropriate.
  • the present invention can be implemented with appropriate modifications without departing from the scope of the present invention.
  • the electrode structure for electric field communication of the present invention is useful as an electrode for a transmitter used in an electric field communication system, for example.

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  • Computer Networks & Wireless Communication (AREA)
  • Signal Processing (AREA)
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Abstract

The purpose of the present invention is to provide an electrode structure for electric field communication having good communication characteristics and capable of preventing both an increase in the number of components and an increase in the size of the electrode structure itself. The electrode structure (13) for electric field communication has a first electrode (131) connected to a fixed potential and a second electrode (132) arranged so as to face the first electrode (131) and having a power supply point (a) disposed therein. The second electrode (132) becomes the electrode adjacent to a transmission medium. The electrode structure (13) for electric field communication is characterized by the second electrode (132) being connected to the first electrode (131) at a site (b) separated by at least a prescribed distance from the power supply point (a) such that the electrical resistance along the length of the current path is at least a prescribed value.

Description

電界通信用電極構造Electrode structure for electric field communication

 本発明は、人体などの伝送媒体を介して情報を送受信する電界通信に適用可能な電界通信用電極構造に関する。 The present invention relates to an electrode structure for electric field communication applicable to electric field communication for transmitting and receiving information through a transmission medium such as a human body.

 近年、人体などの媒体を介して情報を送受信する電界通信システムが提案されている。この電界通信システムは、人体等の伝送媒体と、情報信号に対応する電界を発生させる送信機と、伝送媒体の電位変動を検出して情報信号を復調する受信機とで構成されている。送信機電極と伝送媒体、及び受信機電極と伝送媒体とは容量結合されており、この容量結合によって送信機と受信機との間で通信が行われる。 In recent years, an electric field communication system for transmitting and receiving information via a medium such as a human body has been proposed. This electric field communication system includes a transmission medium such as a human body, a transmitter that generates an electric field corresponding to an information signal, and a receiver that detects a potential variation of the transmission medium and demodulates the information signal. The transmitter electrode and the transmission medium, and the receiver electrode and the transmission medium are capacitively coupled, and communication is performed between the transmitter and the receiver by this capacitive coupling.

 電界通信に用いられる送受信機の電極(電界通信用電極構造)として、平行平板構造のものが提案されている(例えば、特許文献1参照)。この電界通信用電極構造は、略平行に配置された2つ平板導体と、その間に配置された絶縁体とを有し、一方の平板導体に接地電位が与えられ、他方の平板導体に信号電位が与えられるようになっている。信号電位が与えられる平板導体に人体などの伝送媒体が近接すると、伝送媒体には信号電位に応じた電位変動が生じて通信可能になる。 A parallel plate structure has been proposed as an electrode (electrode structure for electric field communication) of a transceiver used for electric field communication (see, for example, Patent Document 1). This electrode structure for electric field communication has two flat conductors arranged substantially in parallel and an insulator arranged between them, and a ground potential is applied to one flat conductor and a signal potential is applied to the other flat conductor. Is to be given. When a transmission medium such as a human body comes close to a flat conductor to which a signal potential is applied, a potential fluctuation corresponding to the signal potential occurs in the transmission medium, and communication becomes possible.

特開2007-174570号公報JP 2007-174570 A

 ところで、上述した平行平板構造の電極では平板導体間の電界が非常に大きいため、他方の平板導体に人体が近接しても、伝送媒体側への電界が殆ど発生せず、伝送媒体の電位変動は極めて小さくなってしまう。伝送媒体の電位変動が小さくなると受信側の電極が受ける信号強度も小さくなり、通信エラーが頻発する。送信側に整合回路を設けることで通信エラーを低減可能だが、この場合、整合回路によって送信側装置の部品点数が増大して製造コストが増大してしまう。また、平板導体間の間隔を大きくすれば、接地電位が与えられるCOLD電極側への損失を抑制できる効果があると期待されるが、それでは電極構造が大型化する問題がある。 By the way, in the parallel plate electrode described above, the electric field between the flat conductors is very large, so even if a human body is close to the other flat conductor, almost no electric field is generated on the transmission medium side, and the potential fluctuation of the transmission medium occurs. Becomes extremely small. When the potential fluctuation of the transmission medium is reduced, the signal intensity received by the receiving electrode is also reduced, and communication errors frequently occur. Although a communication error can be reduced by providing a matching circuit on the transmission side, in this case, the matching circuit increases the number of parts of the transmission side device and increases the manufacturing cost. Further, if the distance between the flat conductors is increased, it is expected that there is an effect that the loss to the COLD electrode side to which the ground potential is applied can be suppressed, but there is a problem that the electrode structure becomes large.

 本発明はかかる点に鑑みてなされたものであり、部品点数の増大を防止すると共に電極構造自体の大型化も防止でき、通信特性の良い電界通信用電極構造を提供することを目的とする。 The present invention has been made in view of the above points, and an object of the present invention is to provide an electrode structure for electric field communication having good communication characteristics, which can prevent an increase in the number of parts and an increase in size of the electrode structure itself.

 本発明の電界通信用電極構造は、固定電位に接続される第1電極と、前記第1電極と対向するように配置され給電点が設けられた第2電極とを有し、前記第2電極が伝送媒体の近接する電極となる電界通信用電極構造において、前記第2電極は、電流経路長の電気抵抗が所定値以上となるように前記給電点から所定距離以上離れた箇所で前記第1電極と接続されることを特徴とする。 The electrode structure for electric field communication according to the present invention includes a first electrode connected to a fixed potential, and a second electrode arranged to face the first electrode and provided with a feeding point, and the second electrode In the electrode structure for electric field communication in which is an electrode adjacent to the transmission medium, the second electrode has the first electrode at a location away from the feeding point by a predetermined distance or more so that the electric resistance of the current path length is a predetermined value or more. It is connected to an electrode.

 この構成によれば、第2電極は、電流経路長の電気抵抗が所定値以上となるように給電点から所定距離以上離れた箇所において第1電極と接続されているため、部品点数の増大を防止すると共に電極構造自体の大型化も防止でき、通信特性の良い電界通信用電極構造を実現できる。 According to this configuration, since the second electrode is connected to the first electrode at a location that is a predetermined distance or more away from the feeding point so that the electric resistance of the current path length is a predetermined value or more, the number of parts is increased. In addition to preventing the increase in size of the electrode structure itself, an electrode structure for electric field communication with good communication characteristics can be realized.

 本発明の電界通信用電極構造において、前記第1及び第2電極は外形領域が同じサイズの方形状をなしており、前記第2電極の給電点が方形の第1辺の端部に設けられ、前記第1辺と対向する第2辺上のいずれかの箇所又は第2辺全体で前記第1電極と接続されていても良い。 In the electrode structure for electric field communication according to the present invention, the first and second electrodes have a rectangular shape with the same outer region, and the feeding point of the second electrode is provided at the end of the first side of the square. The first electrode may be connected to any part of the second side facing the first side or the entire second side.

 本発明の電界通信用電極構造において、前記第1及び第2電極は、長方形状の1枚電極を長手方向の中間位置で折り曲げた構造を有し、折り曲げ部位にて前記第1電極と前記第2電極とを接続していても良い。 In the electrode structure for electric field communication according to the present invention, each of the first and second electrodes has a structure in which one rectangular electrode is bent at an intermediate position in the longitudinal direction, and the first electrode and the first electrode are bent at a bent portion. Two electrodes may be connected.

 本発明の電界通信用電極構造において、前記第1電極は、前記第2電極との対向領域に延在する平面平板導体で構成され、前記第2電極は、ミアンダ形状又はその他の細線パターンで構成されていても良い。 In the electrode structure for electric field communication according to the present invention, the first electrode is constituted by a flat plate conductor extending in a region facing the second electrode, and the second electrode is constituted by a meander shape or other fine line pattern. May be.

 本発明によれば、部品点数の増大を防止すると共に電極構造自体の大型化も防止でき、通信特性の良い電界通信用電極構造を提供することができる。 According to the present invention, it is possible to prevent an increase in the number of parts and prevent an increase in the size of the electrode structure itself, thereby providing an electrode structure for electric field communication with good communication characteristics.

実施の形態1に係る電界通信用電極構造が用いられる電界通信システムの構成例を示す模式図である。It is a schematic diagram which shows the structural example of the electric field communication system in which the electrode structure for electric field communication which concerns on Embodiment 1 is used. 実施の形態1に係る電界通信用電極構造の構成を示す斜視図である。1 is a perspective view showing a configuration of an electrode structure for electric field communication according to Embodiment 1. FIG. 実施の形態1に係る電界通信用電極構造の構成を示す平面図である。1 is a plan view showing a configuration of an electric field communication electrode structure according to Embodiment 1. FIG. シミュレーションモデルを示す模式図である。It is a schematic diagram which shows a simulation model. 平行平板構造の電界通信用電極構造(モデルB)を示す斜視図である。It is a perspective view which shows the electrode structure (model B) for electric field communication of a parallel plate structure. 平行平板構造の電界通信用電極構造(モデルC)を示す斜視図である。It is a perspective view which shows the electrode structure (model C) for electric field communication of a parallel plate structure. シミュレーション結果を示す表である。It is a table | surface which shows a simulation result.

 以下、図面を参照して、本発明の電界通信用電極構造の構成について説明する。 Hereinafter, the configuration of the electrode structure for electric field communication according to the present invention will be described with reference to the drawings.

(実施の形態1)
 図1は、本実施の形態に係る電界通信用電極構造が用いられる電界通信システムの構成例を示す模式図である。図1に示される電界通信システムは、情報信号を変調して情報信号に対応する電界を発生する送信機1と、送信機1が発生する電界によって情報信号を伝送する人体などの伝送媒体2と、伝送媒体2を伝搬する電界となる電位変動を検出して情報信号を復調する受信機3とを備える。なお、送信機1は受信機能を備える送受信機であっても良く、受信機3は送信機能を備える送受信機であっても良い。ここでは、説明を簡略化するために一方向通信のみ説明するが、双方向通信にも容易に適用可能である。
(Embodiment 1)
FIG. 1 is a schematic diagram showing a configuration example of an electric field communication system in which the electric field communication electrode structure according to the present embodiment is used. The electric field communication system shown in FIG. 1 includes a transmitter 1 that modulates an information signal to generate an electric field corresponding to the information signal, and a transmission medium 2 such as a human body that transmits the information signal by the electric field generated by the transmitter 1. And a receiver 3 that demodulates an information signal by detecting a potential fluctuation that becomes an electric field propagating through the transmission medium 2. The transmitter 1 may be a transceiver having a reception function, and the receiver 3 may be a transceiver having a transmission function. Here, in order to simplify the description, only one-way communication will be described, but the present invention can be easily applied to two-way communication.

 送信機1は、信号の送信制御を行うコンピュータなどの制御部11と、制御部11からの情報信号を変調してRF信号を生成する送信部12と、送信部12からのRF信号に応じた電界を発生する電界通信用電極構造13とを備える。送信部12と電界通信用電極構造13との間は同軸ケーブルLを介して接続する。制御部11は、送信部12に中間周波数帯域の情報信号を供給すると共に、電源電位Vddと固定電位となるグランドGNDとを供給するように構成されている。送信部12は、不図示の変調回路などを含み、制御部11からの情報信号(IF)を変調してRF信号を生成可能に構成されている。送信部12は、RF信号を生成し同軸ケーブルLを介して電界通信用電極構造13に供給する。電界通信用電極構造13は、固定電位となる接地電位(GND)が与えられる第1電極131と、制御部11からのRF信号(信号電位)が給電される第2電極132と、第1電極131と第2電極132との間に介在させた絶縁体133とを含んで構成されており、送信部12からのRF信号に対応する電界を発生可能になっている。 The transmitter 1 is a control unit 11 such as a computer that performs signal transmission control, a transmission unit 12 that modulates an information signal from the control unit 11 to generate an RF signal, and an RF signal from the transmission unit 12 And an electric field communication electrode structure 13 for generating an electric field. The transmitter 12 and the electric field communication electrode structure 13 are connected via a coaxial cable L. The control unit 11 is configured to supply the information signal in the intermediate frequency band to the transmission unit 12 and to supply the power supply potential Vdd and the ground GND that is a fixed potential. The transmission unit 12 includes a modulation circuit (not shown) and the like, and is configured to be able to generate an RF signal by modulating an information signal (IF) from the control unit 11. The transmitter 12 generates an RF signal and supplies the RF signal to the electric field communication electrode structure 13 through the coaxial cable L. The electrode structure 13 for electric field communication includes a first electrode 131 to which a ground potential (GND) as a fixed potential is applied, a second electrode 132 to which an RF signal (signal potential) from the control unit 11 is fed, and a first electrode 131 and an insulator 133 interposed between the second electrode 132 and an electric field corresponding to the RF signal from the transmitter 12 can be generated.

 伝送媒体2は、人体などの所定の導電性を有する媒体である。伝送媒体2が電界通信用電極構造13の第2電極132に近接(又は接触)すると、第2電極132と伝送媒体2との間に静電容量が生じ、第2電極132と伝送媒体2とは容量結合する。このため、第2電極132にRF信号が給電されると、伝送媒体2の電位はRF信号の信号電位に応じて変動する。 The transmission medium 2 is a medium having predetermined conductivity such as a human body. When the transmission medium 2 approaches (or comes into contact with) the second electrode 132 of the electrode structure 13 for electric field communication, an electrostatic capacity is generated between the second electrode 132 and the transmission medium 2, and the second electrode 132 and the transmission medium 2 Are capacitively coupled. For this reason, when an RF signal is supplied to the second electrode 132, the potential of the transmission medium 2 varies according to the signal potential of the RF signal.

 受信機3は、伝送媒体2との間で静電容量を形成するための第1電極31、及びこれに対抗するように配置された第2電極32を含んで構成されている。第1電極31が伝送媒体2と近接(又は接触)すると、伝送媒体2と第1電極31との間に静電容量が生じ、伝送媒体2と第1電極31とは容量結合する。伝送媒体2の電位がRF信号の信号電位に応じて変動すると容量結合する第1電極31の電位も同様に変動するため、第1電極31の電位変動を検出して不図示の復調回路などで復調することで、情報信号を受信できる。 The receiver 3 includes a first electrode 31 for forming a capacitance with the transmission medium 2 and a second electrode 32 disposed so as to oppose the first electrode 31. When the first electrode 31 approaches (or comes into contact with) the transmission medium 2, an electrostatic capacitance is generated between the transmission medium 2 and the first electrode 31, and the transmission medium 2 and the first electrode 31 are capacitively coupled. When the potential of the transmission medium 2 fluctuates in accordance with the signal potential of the RF signal, the potential of the first electrode 31 that is capacitively coupled also fluctuates in the same manner. Therefore, the potential fluctuation of the first electrode 31 is detected and a demodulation circuit (not shown) is used. By demodulating, an information signal can be received.

 図2は、本実施の形態に係る電界通信用電極構造13の構成を示す斜視図である。図3は、本実施の形態に係る電界通信用電極構造13の構成を示す平面図である。図3Aは主に第1電極131の構成を示し、図3Bは主に第2電極132の構成を示し、図3Cは図3A、BのAA矢視断面を示す。図1~図3に示されるように、電界通信用電極構造13は、平板導体で構成された第1電極131と、第1電極131と対向するように配置された第2電極132と、第1電極131と第2電極132との間に配置された絶縁体133とで構成されている。 FIG. 2 is a perspective view showing the configuration of the electrode structure 13 for electric field communication according to the present embodiment. FIG. 3 is a plan view showing the configuration of the electric field communication electrode structure 13 according to the present embodiment. 3A mainly shows a configuration of the first electrode 131, FIG. 3B mainly shows a configuration of the second electrode 132, and FIG. 3C shows a cross section taken along the arrow AA in FIGS. As shown in FIGS. 1 to 3, the electric field communication electrode structure 13 includes a first electrode 131 formed of a flat conductor, a second electrode 132 disposed so as to face the first electrode 131, and a first electrode 131. The insulator 133 is disposed between the first electrode 131 and the second electrode 132.

 第1電極131は平面形状が略長方形の平板状電極であり、接地電位(GND)が与えられるように構成されている。第1電極131に与えられる電位は、固定電位であれば接地電位(GND)に限られない。第1電極131の平面形状は略長方形に限られず、略円形、略多角形などの各種形状とすることができる。また、第1電極131はいわゆるベタ電極に限らず、所望のパターンで形成されても良い。 The first electrode 131 is a flat electrode having a substantially rectangular planar shape, and is configured to be supplied with a ground potential (GND). The potential applied to the first electrode 131 is not limited to the ground potential (GND) as long as it is a fixed potential. The planar shape of the first electrode 131 is not limited to a substantially rectangular shape, and may be various shapes such as a substantially circular shape and a substantially polygonal shape. The first electrode 131 is not limited to a so-called solid electrode, and may be formed in a desired pattern.

 第2電極132は、電気抵抗値が所定値以上となる電流経路長に形成(本例ではミアンダ形状)されており、電流経路長の一端に設けられた給電点aに送信部12からのRF信号が給電されるようになっている。より具体的には、第2電極132は、第1電極131と対向するよう第1電極131の主表面に垂直な方向(上下方向)に第1電極131から離間して配置された、外形領域の形状が第1電極131と略同じ長方形状のミアンダパターンの導体で構成されている。 The second electrode 132 is formed in a current path length (in this example, a meander shape) with an electrical resistance value equal to or greater than a predetermined value, and the RF from the transmitter 12 is fed to a feeding point a provided at one end of the current path length. The signal is fed. More specifically, the second electrode 132 is an outer region that is disposed away from the first electrode 131 in a direction (vertical direction) perpendicular to the main surface of the first electrode 131 so as to face the first electrode 131. Is formed of a conductor having a rectangular meander pattern substantially the same as that of the first electrode 131.

 第2電極132のミアンダパターンは、外形領域の長方形を構成する辺e1に略平行な複数の直線部と、隣接する直線部同士を互いに接続する複数の折り返し部とで構成されている。給電点aから伸びる第1の直線部は、給電点aと反対側(辺e2側)の端において第1の折り返し部と接続されており、当該第1の折り返し部は第1の直線部に隣接する第2の直線部と接続されている。さらに、この第2の直線部は、給電点a側(辺e3側)の端において第2の折り返し部と接続されており、第2の折り返し部は第3の直線部と接続されている。ミアンダパターンは、このような直線部と折り返し部との繰り返しパターンが辺e4付近まで設けられることにより構成されている。 The meander pattern of the second electrode 132 is composed of a plurality of straight portions that are substantially parallel to the side e1 that forms the rectangle of the outer region, and a plurality of folded portions that connect adjacent straight portions to each other. The first straight portion extending from the feeding point a is connected to the first folded portion at the end opposite to the feeding point a (side e2 side), and the first folded portion is connected to the first straight portion. It is connected to the adjacent second straight line portion. Further, the second straight line portion is connected to the second folded portion at the end on the feeding point a side (side e3 side), and the second folded portion is connected to the third straight line portion. The meander pattern is configured by providing such a repeating pattern of straight and folded portions up to the vicinity of the side e4.

 上述したミアンダパターンのように、第2電極132を所定の電流経路長の細線パターンとすることで、第2電極132の電気抵抗を平板導体の場合より高くすることができる。細線パターンはミアンダパターンに限られず、スパイラルパターンなどの他のパターンを用いても良い。電流経路長となる細線パターンの長さは、所望の電気抵抗値などに応じて適宜設定できる。 As in the meander pattern described above, the electric resistance of the second electrode 132 can be made higher than that of the flat conductor by making the second electrode 132 a thin line pattern having a predetermined current path length. The thin line pattern is not limited to the meander pattern, and other patterns such as a spiral pattern may be used. The length of the thin line pattern serving as the current path length can be appropriately set according to a desired electric resistance value or the like.

 第2電極132は、給電点aから所定距離の箇所(点又は直線)において第1電極131と接続している。より具体的には、第2電極132は、ミアンダパターンの給電点aと反対側の端点付近の領域bにおいて第1電極131と接続している。言い換えれば、第2電極132は、給電点a側の辺e1に対向する辺e4付近の領域bにおいて第1電極131と接続している。ただし、第1電極131と第2電極132とは少なくとも1点において接続していれば良く、領域bのように範囲を持った領域で接続されていなくても良い。また、第1電極131との接続点の位置は、給電点aから接続点までの電気抵抗値が所定値以上となるように給電点aから離れていれば、給電点aと反対側の端点付近に限られない。ただし、接続点と給電点aとが近い場合、電流経路の電気抵抗が小さくなり伝送損失は大きくなってしまう。このため、接続点の位置及び電流経路の電気抵抗の値は、伝送損失が許容範囲内になるように設定する。このように、第2電極132が所定の電流経路長の細線パターンで構成され、かつ給電点aから所定距離の領域bにおいて第1電極131と接続していることで、通信特性の良い電界通信用電極構造13を実現できる。 The second electrode 132 is connected to the first electrode 131 at a predetermined distance (point or straight line) from the feeding point a. More specifically, the second electrode 132 is connected to the first electrode 131 in a region b near the end point on the opposite side to the feeding point a of the meander pattern. In other words, the second electrode 132 is connected to the first electrode 131 in the region b near the side e4 facing the side e1 on the feeding point a side. However, the first electrode 131 and the second electrode 132 may be connected at least at one point, and may not be connected in a region having a range such as the region b. Further, if the position of the connection point with the first electrode 131 is far from the power supply point a so that the electrical resistance value from the power supply point a to the connection point is not less than a predetermined value, the end point on the side opposite to the power supply point a It is not limited to the vicinity. However, when the connection point is close to the feeding point a, the electrical resistance of the current path is reduced and the transmission loss is increased. For this reason, the position of the connection point and the value of the electric resistance of the current path are set so that the transmission loss is within an allowable range. In this way, the second electrode 132 is configured by a thin line pattern having a predetermined current path length, and is connected to the first electrode 131 in the region b at a predetermined distance from the feeding point a. The electrode structure 13 can be realized.

 第1電極131と第2電極132とは、第1電極131を構成する平板領域と、第2電極132を構成する細線パターン領域とを有する略長方形状の一枚電極を、平板領域と細線パターン領域との境界となる長手方向の中間位置で折り曲げて構成されている。このように一枚電極を折り曲げることで、第1電極131と第2電極132とが領域bにおいて接続された電極構造を実現できる。ただし、別体の第1電極131と第2電極132とを接続しても良い。 The first electrode 131 and the second electrode 132 are a substantially rectangular single electrode having a flat plate area constituting the first electrode 131 and a fine line pattern area constituting the second electrode 132. It is configured to be bent at an intermediate position in the longitudinal direction that becomes a boundary with the region. By bending the single electrode in this manner, an electrode structure in which the first electrode 131 and the second electrode 132 are connected in the region b can be realized. However, the separate first electrode 131 and second electrode 132 may be connected.

 絶縁体133は、第1電極131と第2電極132とを絶縁すると共に、第1電極131と第2電極132との間隔が略一定に保たれるように構成されている。例えば、絶縁体133の厚みを3mmとした場合、第1電極131と第2電極132との間隔を約3mmに保つことができる。なお、第1電極131と第2電極132とを離間して絶縁可能であれば、絶縁体133は省略しても良い。例えば、第2電極132の下部にスペーサを配置し、空気によって絶縁を実現しても良い。 The insulator 133 is configured to insulate the first electrode 131 and the second electrode 132 and to keep the distance between the first electrode 131 and the second electrode 132 substantially constant. For example, when the thickness of the insulator 133 is 3 mm, the distance between the first electrode 131 and the second electrode 132 can be maintained at about 3 mm. Note that the insulator 133 may be omitted as long as the first electrode 131 and the second electrode 132 can be separated and insulated. For example, a spacer may be disposed under the second electrode 132 and insulation may be realized by air.

 図4は、電界通信用電極構造13の通信特性を確認するためのシミュレーションモデルを示す模式図である。送信機1の電極(床電極)として電界通信用電極構造13を用い、導電率が0.62S/m、比誘電率が162.5、高さが1.4mの人体に相当する伝送媒体2を想定してシミュレーションを行った。図4に示されるように、受信機3の電極構造は、平板導体でなる第1電極31と平板導体でなる第2電極32による平行平板構造とした。また、電界通信用電極構造13の第1電極131と第2電極132との間隔は3mmとした(モデルA)。 FIG. 4 is a schematic diagram showing a simulation model for confirming the communication characteristics of the electrode structure 13 for electric field communication. Transmission medium 2 corresponding to a human body using electric field communication electrode structure 13 as an electrode (floor electrode) of transmitter 1, having an electric conductivity of 0.62 S / m, a relative dielectric constant of 162.5, and a height of 1.4 m. A simulation was performed assuming that As shown in FIG. 4, the electrode structure of the receiver 3 is a parallel plate structure including a first electrode 31 made of a flat plate conductor and a second electrode 32 made of a flat plate conductor. Further, the distance between the first electrode 131 and the second electrode 132 of the electrode structure 13 for electric field communication was set to 3 mm (model A).

 比較例として、電界通信用電極構造13とは異なる構造の電界通信用電極構造(床電極)を用いて同様のシミュレーションを行った。図5は、比較例である電界通信用電極構造14aの構成を示す斜視図である。電界通信用電極構造14aは、平板導体でなる第1電極141aと平板導体でなる第2電極142aによる平行平板構造である。第1電極141aと第2電極142aとの間隔は3mmとした(モデルB)。なお、平行平板構造の電界通信用電極構造14aにおいて第1電極141aと第2電極142aとを接続した場合は通信不能となるため、第1電極141aと第2電極142aとは接続していない。 As a comparative example, a similar simulation was performed using an electric field communication electrode structure (floor electrode) having a structure different from that of the electric field communication electrode structure 13. FIG. 5 is a perspective view showing a configuration of an electric field communication electrode structure 14a as a comparative example. The electrode structure for electric field communication 14a is a parallel plate structure including a first electrode 141a made of a flat plate conductor and a second electrode 142a made of a flat plate conductor. The distance between the first electrode 141a and the second electrode 142a was 3 mm (model B). In addition, when the first electrode 141a and the second electrode 142a are connected in the electric field communication electrode structure 14a having a parallel plate structure, the first electrode 141a and the second electrode 142a are not connected because communication is impossible.

 図6は、比較例である電界通信用電極構造14bの構成を示す斜視図である。電界通信用電極構造14bは、平板導体でなる第1電極141bと平板導体でなる第2電極142bによる平行平板構造である。第1電極141bと第2電極142bとの間隔は100mmとした(モデルC)。電界通信用電極構造14bについても同様に、第1電極141bと第2電極142bとは接続していない。 FIG. 6 is a perspective view showing a configuration of an electrode structure for electric field communication 14b as a comparative example. The electrode structure for electric field communication 14b is a parallel plate structure including a first electrode 141b made of a flat plate conductor and a second electrode 142b made of a flat plate conductor. The distance between the first electrode 141b and the second electrode 142b was 100 mm (model C). Similarly, in the electric field communication electrode structure 14b, the first electrode 141b and the second electrode 142b are not connected.

 また、電界通信用電極構造13の第1電極131と第2電極132とが接続されていない構造の電界通信用電極構造を用いて同様のシミュレーションを行った。第1電極131と第2電極132とが接続されていない点以外は、電界通信用電極構造13と同様とした(モデルD)。 Further, the same simulation was performed using the electric field communication electrode structure in which the first electrode 131 and the second electrode 132 of the electric field communication electrode structure 13 are not connected. Except for the point that the first electrode 131 and the second electrode 132 are not connected, the configuration was the same as the electrode structure for electric field communication 13 (model D).

 図7は、シミュレーション結果を示す表である。図7において、伝送損失(SパラメータのS21)の欄の数値が大きくなるほど伝送損失は小さいことを示す。図7に示されるように、本実施の形態の電界通信用電極構造13に相当するモデルAでは、インピーダンス値は15Ω以上となり、伝送損失もモデルA~D中で最小となる。モデルAにおいて伝送損失が最小となるのは、電流経路長の電気抵抗が所定値以上となるように第1電極131と第2電極132とが接続されているためである。 FIG. 7 is a table showing simulation results. In FIG. 7, the larger the value in the column of transmission loss (S parameter S21), the smaller the transmission loss. As shown in FIG. 7, in the model A corresponding to the electric field communication electrode structure 13 of the present embodiment, the impedance value is 15Ω or more, and the transmission loss is the smallest among the models A to D. The transmission loss is minimized in the model A because the first electrode 131 and the second electrode 132 are connected so that the electric resistance of the current path length is equal to or greater than a predetermined value.

 一方、平行平板構造のモデルBでは、インピーダンス値が0.37Ωと小さく、伝送損失も大きい。平行平板構造のモデルCでは、インピーダンス値が13.7Ωと高く、伝送損失はある程度抑制されている。ただし、インピーダンス値に占める電気抵抗成分は十分に小さい。また、第1電極141bと第2電極142bとの間隔は100mmと極めて大きくなっている。第1電極と第2電極とが接続されていないモデルDでは、インピーダンス値は12.0と高いが、伝送損失は大きい。 On the other hand, model B with a parallel plate structure has a small impedance value of 0.37Ω and a large transmission loss. In the model C of the parallel plate structure, the impedance value is as high as 13.7Ω, and the transmission loss is suppressed to some extent. However, the electrical resistance component occupying the impedance value is sufficiently small. Further, the distance between the first electrode 141b and the second electrode 142b is as extremely large as 100 mm. In model D in which the first electrode and the second electrode are not connected, the impedance value is as high as 12.0, but the transmission loss is large.

 電界通信用電極構造13を用いる場合に相当するモデルAと、一般的な電界通信用電極構造14aを用いる場合に相当するモデルBとを比較すると、モデルAでは伝送損失が約8dB向上している。これは、モデルAにおいて受信機3の第1電極31が受ける受信電界強度がモデルBの場合の約2.5倍になることを意味している。このように受信電界強度が大幅に高められることで良好な通信特性を実現できる。 Comparing model A corresponding to the case of using the electric field communication electrode structure 13 and model B corresponding to the case of using the general electric field communication electrode structure 14a, the transmission loss of the model A is improved by about 8 dB. . This means that the received electric field intensity received by the first electrode 31 of the receiver 3 in the model A is about 2.5 times that in the model B. Thus, good communication characteristics can be realized by greatly increasing the received electric field strength.

 電界通信用電極構造14bを用いる場合に相当するモデルCはある程度の通信特性を実現できているが、第1電極141bと第2電極142bとの間隔が大きい(100mm)ため電界通信用電極構造が大型化してしまうという問題を生じる。また、通信特性もモデルAには及ばない。つまり、電界通信用電極構造13を用いるモデルAはモデルCと比較しても良好な通信特性を実現できるうえ、モデルCと比較して電界通信用電極構造の薄型化・小型化が可能である。 Model C corresponding to the case where the electrode structure for electric field communication 14b is used can achieve a certain degree of communication characteristics. However, since the distance between the first electrode 141b and the second electrode 142b is large (100 mm), the electrode structure for electric field communication is The problem that it will enlarge will arise. Also, the communication characteristics do not reach that of model A. In other words, the model A using the electric field communication electrode structure 13 can achieve better communication characteristics than the model C, and the electric field communication electrode structure can be made thinner and smaller than the model C. .

 モデルDの通信特性はモデルAと比較して悪い。モデルAとモデルDとの比較から、通信特性の改善のためには、第1電極131と第2電極132との短絡が必要であると分かる。ただし、電界通信用電極構造14aや電界通信用電極構造14bのような平行平板構造において、平板導体でなる第1電極と第2電極とを接続しても電界通信を行うことはできない。これは、第2電極を構成する平板導体自体の電気抵抗が極めて低く、第1電極と第2電極とを接続した場合、第2電極が第1電極の影響を強く受けてRF信号による電界を殆ど発生できなくなってしまうためと考えられる。すなわち、第2電極を細線パターンなどで構成することで、電流経路の電気抵抗を高めておくことが重要である。 The communication characteristics of model D are worse than model A. From comparison between model A and model D, it can be seen that a short circuit between the first electrode 131 and the second electrode 132 is necessary to improve the communication characteristics. However, in a parallel plate structure such as the electric field communication electrode structure 14a and the electric field communication electrode structure 14b, electric field communication cannot be performed even if the first electrode and the second electrode made of a flat plate conductor are connected. This is because the electric resistance of the flat conductor itself constituting the second electrode is extremely low, and when the first electrode and the second electrode are connected, the second electrode is strongly influenced by the first electrode and the electric field due to the RF signal is generated. This is thought to be due to almost no generation. That is, it is important to increase the electric resistance of the current path by configuring the second electrode with a fine line pattern or the like.

 なお、第2電極に導電率が低い材料を用いる場合も電流経路の電気抵抗は高まるが、この場合、伝送損失は改善されない。例えば、通常のプリント基板等に使用される銅に比べて導電率が低い銀ペースト(銀粒子と樹脂とを混合させた導電性のペースト)などの材料を用いて平板状の2つの電極を形成し、この2つの電極を短絡させた平行平板構造を用いても、伝送損失は改善されない。このことから、導電率が高い材料(例えば、導電率が10(S/m)以上の材料:銅、アルミニウム、銀、金、及びその合金など)を用い、電極パターンなどを工夫することで電気抵抗を高めることが重要であるといえる。 Note that, when a material with low conductivity is used for the second electrode, the electrical resistance of the current path is increased, but in this case, the transmission loss is not improved. For example, two flat electrodes are formed using a material such as a silver paste (conductive paste in which silver particles and resin are mixed) having a lower conductivity than copper used in ordinary printed circuit boards. Even if a parallel plate structure in which the two electrodes are short-circuited is used, the transmission loss is not improved. From this, by using a material with high conductivity (for example, a material having a conductivity of 10 5 (S / m) or more: copper, aluminum, silver, gold, and alloys thereof, etc.) and devising an electrode pattern, etc. It can be said that increasing the electrical resistance is important.

 以上の結果から、第2電極132が、電流経路長の電気抵抗が所定値以上となるように給電点aから所定距離以上離れた箇所bで第1電極131と接続された電界通信用電極構造13(モデルA)では、薄型にしても良好な通信特性を実現できることが分かる。 From the above results, the electrode structure for electric field communication in which the second electrode 132 is connected to the first electrode 131 at a location b that is a predetermined distance or more away from the feeding point a so that the electric resistance of the current path length is a predetermined value or more. 13 (model A) shows that good communication characteristics can be realized even if the thickness is thin.

 以上説明したように、本発明の電界通信用電極構造は、電流経路の電気抵抗が所定値以上となるように給電点から所定距離以上離れた箇所において第1電極と第2電極とが接続することで、通信特性の良い電界通信用電極構造を実現した。 As described above, in the electrode structure for electric field communication according to the present invention, the first electrode and the second electrode are connected at a location away from the feeding point by a predetermined distance or more so that the electric resistance of the current path becomes a predetermined value or more. As a result, an electrode structure for electric field communication with good communication characteristics was realized.

 なお、本発明は上記実施の形態の記載に限定されず、その効果が発揮される態様で適宜変更して実施することができる。例えば、上記実施の形態では、電流経路の電気的パラメータとして電気抵抗を用いて表現しているが、電気抵抗を含めたインピーダンスで表現することもできる。また、上記実施の形態に示す構成、方法などは、適宜組み合わせて実施可能である。その他、本発明は、本発明の範囲を逸脱しないよう適宜変更して実施できる。 In addition, this invention is not limited to description of the said embodiment, It can change suitably in the aspect in which the effect is exhibited, and can be implemented. For example, in the above-described embodiment, the electrical resistance is expressed as an electrical parameter of the current path, but it can also be expressed by an impedance including the electrical resistance. In addition, the structures, methods, and the like described in the above embodiments can be combined as appropriate. In addition, the present invention can be implemented with appropriate modifications without departing from the scope of the present invention.

 本発明の電界通信用電極構造は、例えば、電界通信システムに用いられる送信機用の電極として有用である。 The electrode structure for electric field communication of the present invention is useful as an electrode for a transmitter used in an electric field communication system, for example.

 本出願は、2011年4月19日出願の特願2011-093050に基づく。この内容は、全てここに含めておく。 This application is based on Japanese Patent Application No. 2011-093050 filed on Apr. 19, 2011. All this content is included here.

Claims (4)

 固定電位に接続される第1電極と、前記第1電極と対向するように配置され給電点が設けられた第2電極とを有し、前記第2電極が伝送媒体の近接する電極となる電界通信用電極構造において、
 前記第2電極は、電流経路長の電気抵抗が所定値以上となるように前記給電点から所定距離以上離れた箇所で前記第1電極と接続されることを特徴とする電界通信用電極構造。
An electric field having a first electrode connected to a fixed potential and a second electrode disposed opposite to the first electrode and provided with a feeding point, the second electrode being an electrode adjacent to the transmission medium In the communication electrode structure,
The electrode structure for electric field communication, wherein the second electrode is connected to the first electrode at a position separated from the feeding point by a predetermined distance or more so that an electric resistance of a current path length becomes a predetermined value or more.
 前記第1及び第2電極は外形領域が同じサイズの方形状をなしており、前記第2電極の給電点が方形の第1辺の端部に設けられ、前記第1辺と対向する第2辺上のいずれかの箇所又は第2辺全体で前記第1電極と接続されていることを特徴とする請求項1記載の電界通信用電極構造。 The first and second electrodes have a rectangular shape with the same outer region, and a feeding point of the second electrode is provided at an end of the first side of the square, and a second facing the first side. 2. The electrode structure for electric field communication according to claim 1, wherein the electrode structure is connected to the first electrode at any location on the side or the entire second side.  前記第1及び第2電極は、長方形状の1枚電極を長手方向の中間位置で折り曲げた構造を有し、折り曲げ部位にて前記第1電極と前記第2電極とを接続していることを特徴とする請求項1又は請求項2記載の電界通信用電極構造。 The first and second electrodes have a structure in which one rectangular electrode is bent at an intermediate position in the longitudinal direction, and the first electrode and the second electrode are connected at a bent portion. 3. The electrode structure for electric field communication according to claim 1, wherein the electrode structure is for electric field communication.  前記第1電極は、前記第2電極との対向領域に延在する平面平板導体で構成され、
 前記第2電極は、ミアンダ形状又はその他の細線パターンで構成されている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電界通信用電極構造。
The first electrode is composed of a flat plate conductor extending in a region facing the second electrode,
4. The electrode structure for electric field communication according to claim 1, wherein the second electrode is formed in a meander shape or other fine line pattern. 5.
PCT/JP2012/052774 2011-04-19 2012-02-07 Electrode structure for electric field communication Ceased WO2012144252A1 (en)

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JP2015037202A (en) * 2013-08-12 2015-02-23 日本信号株式会社 Fixator for electric field communication

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WO2009145142A1 (en) * 2008-05-27 2009-12-03 アルプス電気株式会社 Data communication system
JP2010074606A (en) * 2008-09-19 2010-04-02 Nippon Telegr & Teleph Corp <Ntt> Transmission line structure
JP2010177767A (en) * 2009-01-27 2010-08-12 Nippon Telegr & Teleph Corp <Ntt> Electrode adjustment system

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* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2009145142A1 (en) * 2008-05-27 2009-12-03 アルプス電気株式会社 Data communication system
JP2010074606A (en) * 2008-09-19 2010-04-02 Nippon Telegr & Teleph Corp <Ntt> Transmission line structure
JP2010177767A (en) * 2009-01-27 2010-08-12 Nippon Telegr & Teleph Corp <Ntt> Electrode adjustment system

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* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2015037202A (en) * 2013-08-12 2015-02-23 日本信号株式会社 Fixator for electric field communication

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