JP2010021617A - Electromagnetic wave output circuit and communication device for radio tag - Google Patents

Electromagnetic wave output circuit and communication device for radio tag Download PDF

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JP2010021617A
JP2010021617A JP2008177779A JP2008177779A JP2010021617A JP 2010021617 A JP2010021617 A JP 2010021617A JP 2008177779 A JP2008177779 A JP 2008177779A JP 2008177779 A JP2008177779 A JP 2008177779A JP 2010021617 A JP2010021617 A JP 2010021617A
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frequency
constant voltage
antenna
electromagnetic wave
electric field
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JP5140506B2 (en
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Katsumi Katakura
克己 片倉
Yuichi Iwakata
裕一 岩方
Ryuzo Noda
龍三 野田
Kazuaki Matsuo
和顕 松尾
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Lintec Corp
CDN Corp
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CDN Corp
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Abstract

<P>PROBLEM TO BE SOLVED: To generate an electric field of fixed strength to a fluctuation in a frequency under a fixed voltage, relating to the reader/writer device of a contactless IC tag utilizing electromagnetic waves. <P>SOLUTION: On a circuit between a variable frequency constant voltage oscillator 3 for generating an AC current which changes in a frequency range including a first frequency and a second frequency at a fixed voltage and an antenna 5 for generating the electromagnetic waves by the input of the AC current, a resistive element 4 is provided for making the electric field intensities of the output electromagnetic waves of the antenna equal or nearly equal to each other between at the first frequency and at the second frequency. A constant voltage control circuit 2 includes a level setting reference voltage source 21, a level detection circuit 22 and a comparator 23. <P>COPYRIGHT: (C)2010,JPO&INPIT

Description

本発明は、電磁波を利用した非接触ICタグのリーダライタ装置に係り、一定電圧下で周波数の変動に対して一定強度の電界を発生させる技術に関する。   The present invention relates to a reader / writer device for a non-contact IC tag using electromagnetic waves, and relates to a technique for generating an electric field having a constant intensity with respect to frequency fluctuations under a constant voltage.

電磁波を利用した非接触ICタグは、所定の共振周波数(例えば、13.56MHz)で動作するICチップ及びアンテナコイルを有しており、リーダライタ装置は、当該周波数の電磁波を送信するように構成されている。   A non-contact IC tag using electromagnetic waves has an IC chip and an antenna coil that operate at a predetermined resonance frequency (for example, 13.56 MHz), and the reader / writer device is configured to transmit electromagnetic waves of the frequency. Has been.

タグの使用態様によっては、複数の非接触ICタグが接近した状態、あるいは重なった状態で読み取り動作を行わなければならないことがある。このように接近した状態、あるいは重なった状態の非接触ICタグは、アンテナコイル同士の相互誘導作用によりインダクタンスが変化し、共振周波数が低下する。そのため、所定周波数の電磁波を受信しても、ICタグとして動作するために必要な電力を得ることができず、通信が不能になることがある。   Depending on how the tags are used, it may be necessary to perform a reading operation in a state where a plurality of non-contact IC tags are close to each other or overlapped. In the non-contact IC tag in the close state or the overlapped state as described above, the inductance changes due to the mutual induction action between the antenna coils, and the resonance frequency decreases. For this reason, even if an electromagnetic wave having a predetermined frequency is received, the power required to operate as an IC tag cannot be obtained, and communication may be disabled.

共振周波数が低下した非接触ICタグを読み取るためには、リーダライタ装置が、所定周波数よりも低い周波数の範囲も含めて、送信周波数を繰り返し変化(スイープ)させる方法が考えられる。このように、送信周波数を変化させれば、低下した周波数でも通常と同様に十分な電力を供給することができる。   In order to read a non-contact IC tag having a lowered resonance frequency, a method in which the reader / writer device repeatedly changes (sweeps) the transmission frequency including a frequency range lower than a predetermined frequency is conceivable. In this way, if the transmission frequency is changed, sufficient power can be supplied even at a lowered frequency as usual.

しかし、電波法で定められた所定の周波数(例えば、13.56MHz)で許容されている出力レベルを、所定の周波数以外の範囲で出力することは認められていない。従って、リーダライタ装置が、従来の出力レベルのまま送信周波数を変化させることは法的に許されない。   However, it is not permitted to output an output level permitted at a predetermined frequency (for example, 13.56 MHz) defined by the Radio Law in a range other than the predetermined frequency. Therefore, it is legally not allowed for the reader / writer device to change the transmission frequency with the conventional output level.

所定の周波数よりも低い周波数を含めた範囲で通信を行うためには、リーダライタ装置の出力レベルを微弱電波として許容される電界強度の範囲に抑えなければならない。図6に示すように、周波数が10kHz〜322MHzの範囲においては、3mの距離で500μV/mまでの低出力が許されているに過ぎないので、リーダライタ装置の出力を許容範囲の上限に近い出力レベルを維持するように制御することが望ましい。   In order to perform communication in a range including a frequency lower than a predetermined frequency, the output level of the reader / writer device must be suppressed to a range of electric field strength allowed as a weak radio wave. As shown in FIG. 6, in the frequency range of 10 kHz to 322 MHz, only a low output of up to 500 μV / m is allowed at a distance of 3 m, so the output of the reader / writer device is close to the upper limit of the allowable range. It is desirable to control to maintain the output level.

ところが、リーダライタ装置で用いているアンテナは数ターンのコイルアンテナであることが多いので、そのようなアンテナの特性によると、単純な構造のまま一定電圧で出力する電磁波の周波数を変更させた場合に、それに応じて出力レベルが変動してしまうことになる。具体的には、低周波数域よりも高周波数域において電界強度が低くなる。そのため、低下した共振周波数域における読取性能を考慮して低周波数域での許容範囲の上限の出力レベルを得るように電圧を設定すると、同じ電圧のままで高周波数域に周波数を高めたときに、許容範囲の上限に及ばない低いレベルの出力しかえられないことになり、所定の共振周波数における通常の通信時にICタグの動作に必要な電力を供給できないおそれが生じる。一方、所定の共振周波数における出力レベルを許容範囲の上限に合わせるように電圧を設定すると、低周波数域で法定の出力基準を超えてしまうことになる。   However, since the antenna used in the reader / writer device is often a coil antenna of several turns, according to the characteristics of such an antenna, the frequency of electromagnetic waves output at a constant voltage with a simple structure is changed. In addition, the output level fluctuates accordingly. Specifically, the electric field strength is lower in the high frequency range than in the low frequency range. Therefore, if the voltage is set to obtain the upper limit output level of the allowable range in the low frequency range in consideration of the reading performance in the lowered resonance frequency range, when the frequency is increased to the high frequency range while maintaining the same voltage Thus, only a low level output that does not reach the upper limit of the allowable range can be obtained, and there is a possibility that power necessary for the operation of the IC tag cannot be supplied during normal communication at a predetermined resonance frequency. On the other hand, if the voltage is set so that the output level at the predetermined resonance frequency matches the upper limit of the allowable range, the legal output standard will be exceeded in the low frequency range.

周波数を変更した場合の電界強度の変動を調整する方法として、周波数に応じて電圧を調節することが考えられる。つまり、高周波数域では電圧が高くなるように制御することにより、電界強度を一定に保つことができる。但し、周波数に応じて電圧を制御するためには、レベルモニターや可変ゲインアンプを備えた複雑かつ高価な構成となる。図7に、レベルモニターをCPUで監視し、可変ゲインアンプを制御する構成となっている比較例を示す。
特開2007−193785号公報 特開平10−145987号公報
As a method of adjusting the fluctuation of the electric field strength when the frequency is changed, it is conceivable to adjust the voltage according to the frequency. In other words, the electric field strength can be kept constant by controlling the voltage to be higher in the high frequency range. However, in order to control the voltage according to the frequency, a complicated and expensive configuration including a level monitor and a variable gain amplifier is required. FIG. 7 shows a comparative example in which the level monitor is monitored by the CPU and the variable gain amplifier is controlled.
JP 2007-193785 A Japanese Patent Laid-Open No. 10-145987

そこで、本発明は、このような問題を解決することを主な目的とし、出力する電磁波の周波数を変更させながらICタグと通信するリーダライタ装置において、一定電圧の電源によっても周波数域によらず一定の電界強度を得る制御を、単純かつ安価な回路構成により実現することを課題とする。   Therefore, the present invention mainly aims to solve such problems, and in a reader / writer device that communicates with an IC tag while changing the frequency of an electromagnetic wave to be output, regardless of the frequency range, even with a constant voltage power source. It is an object of the present invention to realize control for obtaining a constant electric field intensity with a simple and inexpensive circuit configuration.

本発明に係る電磁波出力回路は、以下の要素を有することを特徴とする。
(1)一定電圧で第一の周波数と第二の周波数を含む周波数範囲で変化する交流電流を発生させる可変周波数定電圧発振器
(2)交流電流の入力により、電磁波を発生させるアンテナ
(3)可変周波数定電圧発振器とアンテナの間の回路上に設けられた抵抗素子。
The electromagnetic wave output circuit according to the present invention has the following elements.
(1) A variable frequency constant voltage oscillator that generates an alternating current that varies in a frequency range including the first frequency and the second frequency at a constant voltage. (2) An antenna that generates an electromagnetic wave by the input of the alternating current. (3) Variable. A resistive element provided on the circuit between the frequency constant voltage oscillator and the antenna.

更に、前記抵抗素子は、前記可変周波数定電圧発振器が前記一定電圧で前記第一の周波数の交流電流を発生させたときの前記アンテナの出力電磁波の電界強度と、前記可変周波数定電圧発振器が前記一定電圧で前記第二の周波数の交流電流を発生させたときの前記アンテナの出力電磁波の電界強度とが同一あるいは略同一となる抵抗値を有することを特徴とする。   Further, the resistance element includes an electric field strength of an electromagnetic wave output from the antenna when the variable frequency constant voltage oscillator generates an alternating current of the first frequency at the constant voltage, and the variable frequency constant voltage oscillator It has a resistance value in which the electric field strength of the electromagnetic wave output from the antenna when the alternating current of the second frequency is generated at a constant voltage is the same or substantially the same.

更に、前記周波数範囲は、2〜14MHzであり、前記アンテナがループ状のコイルアンテナであることを特徴とする。   Furthermore, the frequency range is 2 to 14 MHz, and the antenna is a looped coil antenna.

更に、前記可変周波数定電圧発振器から発生される電圧を制御するための定電圧制御回路を有し、当該定電圧制御回路が電圧レベルを検出するレベル検出回路と、基準となる電圧を発生させるレベル設定基準電圧源と、電圧レベルを比較する比較器から構成されることを特徴とする。   And a constant voltage control circuit for controlling a voltage generated from the variable frequency constant voltage oscillator, a level detection circuit for detecting the voltage level by the constant voltage control circuit, and a level for generating a reference voltage. It comprises a set reference voltage source and a comparator for comparing voltage levels.

更に、本発明に係る無線タグ用通信装置は、電磁波出力回路と、無線タグに送信する情報を当該電磁波出力回路に入力する演算装置と、無線タグから返信された情報を受け取る受信回路を有することを特徴とする。   Furthermore, the wireless tag communication device according to the present invention includes an electromagnetic wave output circuit, an arithmetic device for inputting information to be transmitted to the wireless tag to the electromagnetic wave output circuit, and a receiving circuit for receiving information returned from the wireless tag. It is characterized by.

本発明によれば、アンテナに対して直列に抵抗を設けることにより、低周波数域における電流増加を抑えることにより、一定電圧源での駆動においても電界出力を一定化することができる。   According to the present invention, by providing a resistor in series with the antenna, it is possible to make the electric field output constant even in driving with a constant voltage source by suppressing an increase in current in a low frequency region.

特に無線タグ用通信装置として、複数のスイープされた周波数(例えば、2〜14MHzの周波数範囲)の一定の電界強度を有する電波を送信することができるので、重ねられた状態で共振周波数が低下した複数の無線タグを読み取ることができる。しかも出力する電波の電界強度を所望の値に制御することができるので、電波法等で定められた範囲において最大限の効果を発揮するように運用することができる。   In particular, as a wireless tag communication device, a radio wave having a constant electric field strength of a plurality of swept frequencies (for example, a frequency range of 2 to 14 MHz) can be transmitted, so that the resonance frequency is lowered in a superimposed state. A plurality of wireless tags can be read. In addition, since the electric field intensity of the output radio wave can be controlled to a desired value, it can be operated so as to exhibit the maximum effect within the range defined by the Radio Law.

実施の形態1.
図1は、本発明の電磁波出力回路の構成の一例を示す図である。電磁波出力回路は、可変周波数定電圧発振器3と、抵抗素子4、及びアンテナ5から構成され、さらに演算装置(CPU)1と、定電圧制御回路2を設けることが好ましい。本発明では、アンテナ5と可変周波数定電圧発振器3の間に所定抵抗値の抵抗素子4を設ける。このように、アンテナ5と直列に抵抗素子4を設けることにより、定電圧の交流電流が広い周波数域で変化しても、アンテナ5から出力される電界強度を一定に保つことができる。
Embodiment 1 FIG.
FIG. 1 is a diagram showing an example of the configuration of an electromagnetic wave output circuit of the present invention. The electromagnetic wave output circuit includes a variable frequency constant voltage oscillator 3, a resistance element 4, and an antenna 5, and further preferably includes an arithmetic unit (CPU) 1 and a constant voltage control circuit 2. In the present invention, a resistance element 4 having a predetermined resistance value is provided between the antenna 5 and the variable frequency constant voltage oscillator 3. Thus, by providing the resistance element 4 in series with the antenna 5, even if the constant voltage alternating current changes in a wide frequency range, the electric field intensity output from the antenna 5 can be kept constant.

可変周波数定電圧発振器3は、周波数が変化した場合でも一定の電圧の交流電流を発生させる発振器である。   The variable frequency constant voltage oscillator 3 is an oscillator that generates an alternating current having a constant voltage even when the frequency changes.

アンテナ5は、入力された電流により電磁波を発生させるアンテナであり、例えば八木アンテナ、ダイポールアンテナ、ループ状のコイルアンテナ等を例示することができる。その中でもコイルアンテナが好ましく、導電性の材料をらせん状に巻き回されたループ形状で構成され、巻き回数は出力する電磁波の周波数により適宜選択すればよい。コイルアンテナを構成する導電性の材料としては、金、銀、銅、アルミニウム、ニッケル等の金属からなる導線、箔膜、それら金属粒子を含む導電性ペーストなどを挙げることができる。前記導電性の材料を用いて、コイルアンテナを作成する方法としては、導線を用いる場合にはループ状に巻き返せばよく、箔膜を用いる場合には所望のループ状になるように余分な箔膜をエッチング処理により除去すればよく、導電性ペーストを用いる場合にはグラビア印刷、スクリーン印刷、フレキソ印刷、インクジェット印刷等によりループ状に印刷すればよい。   The antenna 5 is an antenna that generates an electromagnetic wave by an input current, and examples thereof include a Yagi antenna, a dipole antenna, and a looped coil antenna. Among these, a coil antenna is preferable, and it is configured in a loop shape in which a conductive material is spirally wound, and the number of windings may be appropriately selected depending on the frequency of the output electromagnetic wave. Examples of the conductive material constituting the coil antenna include a conductive wire made of a metal such as gold, silver, copper, aluminum, and nickel, a foil film, and a conductive paste containing these metal particles. As a method of creating a coil antenna using the conductive material, it is only necessary to wrap around a loop when using a conductive wire, and when using a foil film, an extra foil film is formed so as to form a desired loop. May be removed by etching, and when a conductive paste is used, it may be printed in a loop by gravure printing, screen printing, flexographic printing, ink jet printing, or the like.

演算装置(CPU)1は、スイープさせる周波数の値を可変周波数定電圧発振器3に与える。定電圧制御回路2は、可変周波数定電圧発振器3から出力される交流電圧を一定に保つための定電圧生成回路であり、レベル設定基準電圧源21とレベル検出回路22と比較器23からなる。レベル設定基準電圧源21は、電圧レベルを設定する際の基準となる電圧を生じさせる。レベル検出回路22は、可変周波数定電圧発振器3から出力される交流電流の電圧レベルを検出する回路である。比較器23は、レベル設定基準電圧源21から基準電圧レベルを入力し、レベル検出回路22より検出電圧レベルを入力し、両電圧レベルを比較し、可変周波数定電圧発振器3から出力された電圧が基準電圧と一致するように可変周波数定電圧発振器3を制御する。   The arithmetic unit (CPU) 1 gives a frequency value to be swept to the variable frequency constant voltage oscillator 3. The constant voltage control circuit 2 is a constant voltage generation circuit for keeping the AC voltage output from the variable frequency constant voltage oscillator 3 constant, and includes a level setting reference voltage source 21, a level detection circuit 22, and a comparator 23. The level setting reference voltage source 21 generates a voltage serving as a reference when setting the voltage level. The level detection circuit 22 is a circuit that detects the voltage level of the alternating current output from the variable frequency constant voltage oscillator 3. The comparator 23 receives the reference voltage level from the level setting reference voltage source 21, receives the detection voltage level from the level detection circuit 22, compares both voltage levels, and the voltage output from the variable frequency constant voltage oscillator 3 is obtained. The variable frequency constant voltage oscillator 3 is controlled so as to coincide with the reference voltage.

ここで、抵抗素子4を可変周波数定電圧発振器3とアンテナ5の間の回路上に設けることにより、一定電圧下で周波数の変化に対して電界強度を一定に保つ理論について説明する。   Here, a theory will be described in which the resistance element 4 is provided on a circuit between the variable frequency constant voltage oscillator 3 and the antenna 5 so that the electric field strength is kept constant with respect to a change in frequency under a constant voltage.

図2は、電磁場の位置関係を示す図である。コイルアンテナの中心を原点とし、コイルアンテナに垂直な軸方向にz軸を設け、z軸と直交する平面上に互いに直角をなすx軸とy軸を設ける。   FIG. 2 is a diagram showing the positional relationship of the electromagnetic field. The center of the coil antenna is the origin, the z-axis is provided in the axial direction perpendicular to the coil antenna, and the x-axis and the y-axis are perpendicular to each other on a plane orthogonal to the z-axis.

コイルアンテナのループ断面積をS[m2]で示し、アンテナ電流をI[A]で示す。 The loop cross-sectional area of the coil antenna is indicated by S [m 2 ], and the antenna current is indicated by I [A].

電界及び磁界を示す基準点は、原点からの距離r[m]、原点から基準点へのベクトルがz軸となす角θ、当該ベクトルのxy平面への垂線の足と原点の線分がy軸となす角φにより特定される。   A reference point indicating an electric field and a magnetic field has a distance r [m] from the origin, an angle θ formed by a vector from the origin to the reference point and the z-axis, a perpendicular leg of the vector to the xy plane, and a line segment of the origin at y It is specified by the angle φ formed with the axis.

以下に電界計算式を示す。   The electric field calculation formula is shown below.

Figure 2010021617
Figure 2010021617

ここで、E[V/m]は、r方向の磁界にZ0を乗じて求める電界である。
r[A/m]は、r方向の磁界である。
f[Hz]は、交流電流の周波数である。
0は、自由空間特性インピーダンスである。
Here, E [V / m] is an electric field obtained by multiplying the r-direction magnetic field by Z 0 .
H r [A / m] is a magnetic field in the r direction.
f [Hz] is the frequency of the alternating current.
Z 0 is a free space characteristic impedance.

以下に磁界計算式を示す。   The magnetic field calculation formula is shown below.

Figure 2010021617
Figure 2010021617

ここで、k(f)は、伝搬係数であり、jは、虚数である。   Here, k (f) is a propagation coefficient, and j is an imaginary number.

Figure 2010021617
Figure 2010021617

ここで、λ0(f)は、波長[m]である。 Here, λ 0 (f) is the wavelength [m].

Figure 2010021617
Figure 2010021617

ここで、c0は、真空中の光速度である。 Here, c 0 is the speed of light in vacuum.

基準点を固定して周波数の変化のみに着目すると、電界は周波数fと電流Iを変数とするE(f,I)としてとらえることができる。   Focusing only on the change in frequency with the reference point fixed, the electric field can be regarded as E (f, I) with the frequency f and current I as variables.

コイル特性を無視して、周波数が変化してもアンテナ電流Iを一定であると仮定すると、数1より周波数fが高くなると電界Eが高くなる傾向にある(高磁界化傾向、図3(イ)参照)。   Assuming that the antenna current I is constant even when the frequency changes, ignoring the coil characteristics, the electric field E tends to increase as the frequency f becomes higher than Equation 1 (the tendency to higher magnetic field, FIG. )reference).

しかし、抵抗を設けない従来の技術においては、実際には以下のアンテナ電流計算式(抵抗無し)に示すように、周波数fが高くなるとアンテナ電流Iは低くなる。   However, in the conventional technique in which no resistor is provided, the antenna current I actually decreases as the frequency f increases, as shown in the following antenna current calculation formula (no resistor).

Figure 2010021617
Figure 2010021617

Figure 2010021617
Figure 2010021617

ここで、Vrmsは、交流電流の実効電圧であり、ZL(f)は、アンテナのインピーダンスであり、Lは、アンテナのインダクタンスである。 Here, V rms is the effective voltage of the alternating current, Z L (f) is the impedance of the antenna, and L is the inductance of the antenna.

また、数1の電界計算式によると、電圧を一定にするとアンテナ電流Iが低くなると電界Eが低くなる傾向にある。つまり、数5を数1に代入すると周波数域が高くなると電界が低くなる傾向がある(低磁界化傾向、図3(ロ)参照)。   Further, according to the electric field calculation formula (1), when the voltage is constant, the electric field E tends to decrease as the antenna current I decreases. That is, if Equation 5 is substituted into Equation 1, the electric field tends to decrease as the frequency range increases (the tendency to lower the magnetic field, see FIG. 3B).

抵抗を設けない回路では、前述の高周波数域における高磁界化傾向と低磁界化傾向が相殺しつつも、低磁界化傾向の影響により全体としては低磁界化傾向を示す。   In a circuit without a resistor, the tendency to increase the magnetic field in the high frequency region and the tendency to decrease the magnetic field cancel each other, but the tendency to decrease the magnetic field as a whole is exhibited due to the influence of the decrease in magnetic field.

本発明では、低磁界化傾向を弱め、高磁界化傾向との相殺による磁界の一定化を図る。本発明で設ける抵抗Rは、低磁界化傾向を弱めるように作用する。   In the present invention, the tendency to lower the magnetic field is weakened, and the magnetic field is made constant by offsetting the tendency to increase the magnetic field. The resistor R provided in the present invention acts to weaken the tendency to lower the magnetic field.

本発明の構成の回路におけるアンテナ電流計算式(抵抗有り)を、以下に示す。   An antenna current calculation formula (with resistance) in the circuit having the configuration of the present invention is shown below.

Figure 2010021617
Figure 2010021617

Figure 2010021617
Figure 2010021617

この式によると、周波数fが高くなるとアンテナ電流Iが低くなり、高周波数域における低下電流化傾向は弱まる。その結果、高周波数域における低磁界化傾向も弱まることになる。   According to this equation, as the frequency f increases, the antenna current I decreases, and the tendency to decrease current in the high frequency region is weakened. As a result, the tendency to lower the magnetic field in the high frequency range is also weakened.

上述の傾向を検証する。ループ断面積S[m2]=0.000624、距離r[m]=3、角度θ[deg]=0、スイープさせる周波数f[MHz]=1.0,1.1,1.2,・・・,20.0、自由空間特性インピーダンスZ0[Ω]=376.73、真空中の光速度C0[m/sec]=2.998×108、アンテナ電圧Vrms[V]=2.263、アンテナのインダクタンスL[μH]=1として計算した電界強度Eの変化を図3(ロ)に示す。fs=1MHz(低周波数域の例)時の交流電流で、抵抗を設けない回路による電界強度Esが6236[μV/m]であり、同じくfs=20MHz(高周波数域の例)時の交流電流で、電界強度Eeが500[μV/m]となる。 Verify the above trends. Loop cross-sectional area S [m 2 ] = 0.000624, distance r [m] = 3, angle θ [deg] = 0, frequency to sweep f [MHz] = 1.0, 1.1, 1.2,. .., 20.0, free space characteristic impedance Z 0 [Ω] = 376.73, light velocity in vacuum C 0 [m / sec] = 2.998 × 10 8 , antenna voltage V rms [V] = 2 .263, the change in the electric field intensity E calculated with the antenna inductance L [μH] = 1 is shown in FIG. AC current at f s = 1 MHz (example in low frequency range), electric field strength E s by a circuit without a resistor is 6236 [μV / m], and f s = 20 MHz (example in high frequency range) Electric field strength E e is 500 [μV / m].

本発明では、一定電圧下で、低周波数域と高周波数域において同じ電界強度になるように抵抗を設ける。以下、その抵抗値を算出する手順について説明する。
(1)電界計算式に基づいて、一定電圧下の低周波数域と高周波数域の交流電流で、抵抗を設けない回路から同じ電界強度を得るための各周波数域でのアンテナ電流値を算出し、低周波数域から高周波数域へ移行した場合のアンテナ電流の変化比を求める。
(2)一定電圧下で、当該アンテナ電流の変化比となる、抵抗を設けた回路の全体インピーダンスの比を算出する。
(3)当該インピーダンス比を実現する抵抗値Rを算出する。
In the present invention, a resistor is provided so that the same electric field strength is obtained in a low frequency region and a high frequency region under a constant voltage. Hereinafter, a procedure for calculating the resistance value will be described.
(1) Based on the electric field calculation formula, calculate the antenna current value in each frequency range in order to obtain the same electric field strength from a circuit that does not provide resistance with alternating currents in the low frequency range and high frequency range under a constant voltage. Then, the change ratio of the antenna current when shifting from the low frequency range to the high frequency range is obtained.
(2) The ratio of the total impedance of the circuit provided with the resistance, which is the change ratio of the antenna current under a constant voltage, is calculated.
(3) A resistance value R that realizes the impedance ratio is calculated.

前述の条件で実際に算出した例を示す。
(1)fs=1MHz(低周波数域の例)時の交流電流で、抵抗を設けない回路による電界強度Esが500[μV/m]となる条件により、電界計算式とアンテナ電流計算式によりアンテナ電流値を算出するとIs=−0.36iとなる。また、fe=20MHz(高周波数域の例)時の交流電流で、同様に電界強度Eeが500[μV/m]となる条件により、アンテナ電流値を算出するとIe=−0.225iとなる。従って、1MHzから20MHzへ周波数を変化させた場合のアンテナ電流の変化比は、Is/Ie=1.603となる。
(2)以下の式に従って、インピーダンス比K=Ze/Zs=1.603となる。
An example of actual calculation under the above conditions will be shown.
(1) An electric field calculation formula and an antenna current calculation formula under the condition that the electric field strength E s is 500 [μV / m] by an AC current when f s = 1 MHz (an example in a low frequency range) without a resistor. If the antenna current value is calculated by the above, I s = −0.36i. Further, when the antenna current value is calculated under the condition that the electric field intensity E e is 500 [μV / m] with an alternating current at f e = 20 MHz (example in a high frequency range), I e = −0.225i It becomes. Therefore, when the frequency is changed from 1 MHz to 20 MHz, the change ratio of the antenna current is I s / I e = 1.603.
(2) according to the following formula, the impedance ratio K = Z e / Z s = 1.603.

Figure 2010021617
Figure 2010021617

(3)それぞれのインピーダンスを以下の式で算出する。 (3) Each impedance is calculated by the following formula.

Figure 2010021617
Figure 2010021617

以下の式に従って、抵抗値R=99.89となる。尚このとき、Zs=100.178、Ze=160.585となる。 According to the following formula, the resistance value R = 99.89. At this time, Z s = 100.178 and Z e = 160.585.

Figure 2010021617
Figure 2010021617

上述の手順で求めた抵抗値を用いて、電界強度が500[μV/m]に近づくようにアンテナ電圧を求めると、Vrms[V]=36.06となる。このアンテナ電圧による各電界強度を改めて算出すると、1MHzの交流電流で、抵抗を設けた回路による電界強度Esが499.92384となり、20MHzの交流電流で、抵抗を設けた回路による電界強度Esが500.07463となり、ほぼ一定となることが証明された。この周波数範囲での電界強度を図4に示す。電界強度の変化は、ごく微小であることがわかる。 When the antenna voltage is obtained so that the electric field strength approaches 500 [μV / m] using the resistance value obtained in the above procedure, V rms [V] = 36.06. When the electric field strength due to this antenna voltage is calculated again, the electric field strength E s by the circuit provided with the resistance becomes 499.992384 with an alternating current of 1 MHz, and the electric field strength E s by the circuit provided with the resistance with an alternating current of 20 MHz. Was 500.07463 and proved to be almost constant. The electric field strength in this frequency range is shown in FIG. It can be seen that the change in electric field strength is very small.

図5に本発明の無線タグ用通信装置の一例を示す。本発明の無線タグ用通信装置は、可変周波数定電圧発振器3と抵抗素子4とアンテナ5を有する電磁波出力回路と、演算装置(CPU)1と、受信回路6から構成される。さらに定電圧制御回路2を設けることが好ましい。   FIG. 5 shows an example of a wireless tag communication device of the present invention. The wireless tag communication device of the present invention includes an electromagnetic wave output circuit having a variable frequency constant voltage oscillator 3, a resistance element 4, and an antenna 5, an arithmetic unit (CPU) 1, and a receiving circuit 6. Furthermore, it is preferable to provide a constant voltage control circuit 2.

次に本発明の無線タグ用通信装置の操作について説明する。出力する電圧と周波数と無線タグに送信する情報を、演算装置(CPU)1から可変周波数定電圧発振器3に入力する。可変周波数定電圧発振器3から、無線タグに送信する情報を伴った入力された電圧と周波数を有する電流が発生され、抵抗素子4を介して、アンテナ5に電流が送られる。アンテナ5に電流が流れると、無線タグに送信する情報を伴った一定の電界強度を有する電波が無線タグに向けて発信される。無線タグから返信された情報を伴った電波をアンテナ5で受けて、受信回路6で受信する。受信回路6から受信した情報を演算装置(CPU)1に入力し、演算装置(CPU)1で無線タグから返信された情報を判断し、記録して管理する。次に可変周波数定電圧発振器3に入力する周波数をスイープさせて同様に操作する。その場合でもアンテナから発振される電界強度は周波数をスイープさせる前とほぼ同様の強度に抑えることができる。   Next, the operation of the wireless tag communication device of the present invention will be described. The voltage to be output, the frequency, and the information to be transmitted to the wireless tag are input from the arithmetic unit (CPU) 1 to the variable frequency constant voltage oscillator 3. The variable frequency constant voltage oscillator 3 generates a current having an input voltage and frequency accompanied by information to be transmitted to the wireless tag, and the current is sent to the antenna 5 through the resistance element 4. When a current flows through the antenna 5, a radio wave having a certain electric field strength accompanied by information to be transmitted to the wireless tag is transmitted toward the wireless tag. A radio wave accompanied by information returned from the wireless tag is received by the antenna 5 and received by the receiving circuit 6. Information received from the receiving circuit 6 is input to the arithmetic unit (CPU) 1, and the information returned from the wireless tag is judged by the arithmetic unit (CPU) 1, recorded and managed. Next, the same operation is performed by sweeping the frequency input to the variable frequency constant voltage oscillator 3. Even in this case, the electric field intensity oscillated from the antenna can be suppressed to substantially the same intensity as before the frequency is swept.

本発明の無線タグ用通信装置は、複数のスイープされた周波数(例えば、2〜14MHzの周波数範囲)において一定の電界強度を有する電波を送信することができるので、重ねられた状態で共振周波数が低下した複数の無線タグを読み取ることができる。しかも出力する電波の電界強度を所望の値に制御することができるので、電波法等で定められた範囲において最大限の効果を発揮するように運用することができる。   The wireless tag communication device of the present invention can transmit a radio wave having a constant electric field strength at a plurality of swept frequencies (for example, a frequency range of 2 to 14 MHz). A plurality of lowered wireless tags can be read. In addition, since the electric field intensity of the output radio wave can be controlled to a desired value, it can be operated so as to exhibit the maximum effect within the range defined by the Radio Law.

本発明の電磁波出力回路の構成を示す図である。It is a figure which shows the structure of the electromagnetic wave output circuit of this invention. 電磁場の位置関係を示す図である。It is a figure which shows the positional relationship of an electromagnetic field. (イ)抵抗を設けない回路で、一定電流の交流電流の周波数を変化させた場合の電界強度の変化と(ロ)抵抗を設けない回路で、一定電圧の交流電流の周波数を変化させた場合の電界強度の変化を示す図である。(B) Changes in the electric field strength when the frequency of the alternating current with a constant current is changed in a circuit without a resistor, and (b) When the frequency of the alternating current with a constant voltage is changed in a circuit without a resistor It is a figure which shows the change of the electric field strength. 本発明の電磁波出力回路で、一定電圧の交流電流の周波数を変化させた場合の電界強度の変化を示す図である。It is a figure which shows the change of the electric field strength at the time of changing the frequency of the alternating current of a fixed voltage in the electromagnetic wave output circuit of this invention. 本発明の無線タグ用通信装置の一例を示す図である。It is a figure which shows an example of the communication apparatus for radio | wireless tags of this invention. 交信距離3mにおける微弱電波の規格を示す図である。It is a figure which shows the standard of the weak radio wave in communication distance 3m. 比較構成例を示す図である。It is a figure which shows the comparative structural example.

符号の説明Explanation of symbols

1 演算装置(CPU)、2 定電圧制御回路、3 可変周波数定電圧発振器、4 抵抗素子、5 コイルアンテナ、6 受信回路、21 レベル設定基準電圧源、22 レベル検出回路、23 比較器。   1 arithmetic unit (CPU), 2 constant voltage control circuit, 3 variable frequency constant voltage oscillator, 4 resistance element, 5 coil antenna, 6 receiving circuit, 21 level setting reference voltage source, 22 level detection circuit, 23 comparator.

Claims (5)

以下の要素を有することを特徴とする電磁波出力回路
(1)一定電圧で第一の周波数と第二の周波数を含む周波数範囲で変化する交流電流を発生させる可変周波数定電圧発振器
(2)交流電流の入力により、電磁波を発生させるアンテナ
(3)可変周波数定電圧発振器とアンテナの間の回路上に設けられた抵抗素子
An electromagnetic wave output circuit characterized by having the following elements: (1) A variable frequency constant voltage oscillator that generates an alternating current changing at a constant voltage in a frequency range including the first frequency and the second frequency (2) an alternating current (3) A resistance element provided on a circuit between the variable frequency constant voltage oscillator and the antenna.
前記抵抗素子は、前記可変周波数定電圧発振器が前記一定電圧で前記第一の周波数の交流電流を発生させたときの前記アンテナの出力電磁波の電界強度と、前記可変周波数定電圧発振器が前記一定電圧で前記第二の周波数の交流電流を発生させたときの前記アンテナの出力電磁波の電界強度とが同一あるいは略同一となる抵抗値を有することを特徴とする請求項1に記載の電磁波出力回路。   The resistance element includes an electric field strength of an output electromagnetic wave of the antenna when the variable frequency constant voltage oscillator generates an alternating current of the first frequency at the constant voltage, and the variable frequency constant voltage oscillator includes the constant voltage. 2. The electromagnetic wave output circuit according to claim 1, wherein the electromagnetic wave output circuit has a resistance value that is the same or substantially the same as an electric field intensity of the output electromagnetic wave of the antenna when the alternating current of the second frequency is generated. 前記周波数範囲は、2〜14MHzであり、前記アンテナがループ状のコイルアンテナであることを特徴とする請求項1又は2に記載の電磁波出力回路。   The electromagnetic wave output circuit according to claim 1, wherein the frequency range is 2 to 14 MHz, and the antenna is a loop-shaped coil antenna. 前記可変周波数定電圧発振器から発生される電圧を制御するための定電圧制御回路を有し、当該定電圧制御回路が電圧レベルを検出するレベル検出回路と、基準となる電圧を発生させるレベル設定基準電圧源と、電圧レベルを比較する比較器から構成されることを特徴とする請求項1乃至3のいずれか1項に記載の電磁波出力回路。   A constant voltage control circuit for controlling a voltage generated from the variable frequency constant voltage oscillator; a level detection circuit for detecting a voltage level by the constant voltage control circuit; and a level setting reference for generating a reference voltage 4. The electromagnetic wave output circuit according to claim 1, comprising a voltage source and a comparator for comparing voltage levels. 5. 請求項1乃至4のいずれか1項に記載の電磁波出力回路と、無線タグに送信する情報を当該電磁波出力回路に入力する演算装置と、無線タグから返信された情報を受け取る受信回路を有する無線タグ用通信装置。   5. A wireless circuit comprising: the electromagnetic wave output circuit according to claim 1; an arithmetic unit that inputs information to be transmitted to the wireless tag to the electromagnetic wave output circuit; and a receiving circuit that receives information returned from the wireless tag. Tag communication device.
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Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP5995022B1 (en) * 2015-09-10 2016-09-21 パナソニックIpマネジメント株式会社 Wireless power transmission system and power transmission device

Citations (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2004348496A (en) * 2003-05-23 2004-12-09 Hitachi Ltd Communication system
JP2005020295A (en) * 2003-06-25 2005-01-20 Nippon Telegr & Teleph Corp <Ntt> Transceiver
JP2005191961A (en) * 2003-12-25 2005-07-14 Sharp Corp Noncontact ic card, electronic information apparatus, portable electronic information apparatus, open-type system, method for controling electric power consumption, control program, and readable recording medium
WO2008105477A1 (en) * 2007-02-27 2008-09-04 Kyocera Corporation Portable electronic device and magnetic antenna circuit
JP2009111483A (en) * 2007-10-26 2009-05-21 Sony Corp Non-contact data carrier, reader/writer apparatus, and non-contact data carrier system

Patent Citations (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2004348496A (en) * 2003-05-23 2004-12-09 Hitachi Ltd Communication system
JP2005020295A (en) * 2003-06-25 2005-01-20 Nippon Telegr & Teleph Corp <Ntt> Transceiver
JP2005191961A (en) * 2003-12-25 2005-07-14 Sharp Corp Noncontact ic card, electronic information apparatus, portable electronic information apparatus, open-type system, method for controling electric power consumption, control program, and readable recording medium
WO2008105477A1 (en) * 2007-02-27 2008-09-04 Kyocera Corporation Portable electronic device and magnetic antenna circuit
JP2009111483A (en) * 2007-10-26 2009-05-21 Sony Corp Non-contact data carrier, reader/writer apparatus, and non-contact data carrier system

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP5995022B1 (en) * 2015-09-10 2016-09-21 パナソニックIpマネジメント株式会社 Wireless power transmission system and power transmission device
WO2017042987A1 (en) * 2015-09-10 2017-03-16 パナソニックIpマネジメント株式会社 Wireless power transmission system and power transmission device
CN106797140A (en) * 2015-09-10 2017-05-31 松下知识产权经营株式会社 Wireless power transmission system and power transmission device
CN106797140B (en) * 2015-09-10 2021-06-01 松下知识产权经营株式会社 Wireless power transmission system and power transmission device

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