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JP6283812B2 - Load measuring device and load measuring sensor - Google Patents
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JP6283812B2 - Load measuring device and load measuring sensor - Google Patents

Load measuring device and load measuring sensor Download PDF

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JP6283812B2
JP6283812B2 JP2015121519A JP2015121519A JP6283812B2 JP 6283812 B2 JP6283812 B2 JP 6283812B2 JP 2015121519 A JP2015121519 A JP 2015121519A JP 2015121519 A JP2015121519 A JP 2015121519A JP 6283812 B2 JP6283812 B2 JP 6283812B2
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佐 長田
佐 長田
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Description

本発明は、圧電体を用いた高感度のインピーダンス変化型の荷重測定装置に関するものである。例えば起き上がりの見守りや、脈拍数や呼吸数、血圧などの圧力や荷重・力の計測に適している。  The present invention relates to a highly sensitive impedance change type load measuring device using a piezoelectric body. For example, it is suitable for watching a rising, and measuring pressure, load and force such as pulse rate, respiration rate and blood pressure.

圧電体は、応力や力を受けると電荷が発生する。これを利用した圧電型の荷重や力センサとして利用されている。しかし、電荷が漏洩するため、静的感度を持たせるために工夫が必要である。  A piezoelectric body generates electric charges when subjected to stress or force. It is used as a piezoelectric load or force sensor using this. However, since charges leak, it is necessary to devise in order to provide static sensitivity.

振動型または共振型は、圧電体が応力を受けたときの共振周波数の変化を検出するもので静的な感度を有するが、ある特定の共振点の移動を追尾するため、検出回路は複雑となる。  The vibration type or resonance type detects a change in the resonance frequency when the piezoelectric body receives stress, and has a static sensitivity. However, since the movement of a specific resonance point is tracked, the detection circuit is complicated. Become.

これらの問題を解決するものとして、たとえば特許第4178600号に圧電体の共振点近傍で一定周波数かつ一定振幅の電流を与え、圧電体のインピーダンス変化を検出する荷重や力の測定を簡単な回路で実現する測定装置が提案されている。  In order to solve these problems, for example, in Patent No. 4178600, a current having a constant frequency and a constant amplitude is applied in the vicinity of the resonance point of the piezoelectric body, and a load or force measurement for detecting a change in impedance of the piezoelectric body is performed with a simple circuit. A measuring device to be realized has been proposed.

しかし、検出感度が小さく共振の尖鋭度Qを高くすると測定範囲が狭くなり、荷重や力の増減に対して十分な感度が得られないという欠点があった。また、素子の物性に起因する焦電効果に対する改善策が難しいなどの問題がある。  However, if the detection sensitivity is low and the resonance sharpness Q is increased, the measurement range becomes narrow, and there is a drawback that sufficient sensitivity cannot be obtained with respect to increase or decrease in load or force. In addition, there is a problem that it is difficult to improve the pyroelectric effect due to the physical properties of the element.

特許第4178600号Patent No. 4178600

長田 佐著 「圧電セラミックによる圧力センサ」 自動化技術、1982年Satoshi Nagata “Pressure Sensor Using Piezoelectric Ceramics” Automation Technology, 1982

大内英俊、長田 佐、河西敏雄共著「圧電素子を利用した力センサの静特性の改善」精密工学会誌、2001年  Hidetoshi Ouchi, Satoshi Nagata, Toshio Kawanishi, “Improvement of Static Characteristics of Force Sensors Using Piezoelectric Elements”, Journal of Precision Engineering, 2001

解決しようとする問題点は、ピエゾ効果には圧電効果と焦電効果がある。荷重や力の検出では、荷重や力の増減に対して圧電体自体のインピーダンスの変化が少なく、十分な感度が得られないという欠点があった。また、圧電素子の物性に起因する焦電効果に対する改善策が難しいなどの問題がある。  The problem to be solved is that the piezo effect includes a piezoelectric effect and a pyroelectric effect. In detecting the load or force, there is a drawback that the impedance of the piezoelectric body itself is small with respect to increase or decrease of the load or force, and sufficient sensitivity cannot be obtained. In addition, there is a problem that it is difficult to improve the pyroelectric effect due to the physical properties of the piezoelectric element.

本発明は、抵抗RとコイルLとコンデンサCの直列共振回路において、周波数が変化すると、リアクタンス分が変化する原理を用いた。周波数の変化に伴うリアクタンスXの変化は次の通りである。
直列共振回路において、共振周波数fからΔfに変化すると、

Figure 0006283812
となり、
電源電圧Eときの電流Iは(1)式となる。
Figure 0006283812
する。本発明は、この知見に基づいてなされている。The present invention uses the principle that in a series resonant circuit of a resistor R, a coil L, and a capacitor C, the reactance component changes as the frequency changes. The change in reactance X accompanying the change in frequency is as follows.
In the series resonance circuit, when the resonance frequency f 0 changes to Δf,
Figure 0006283812
And
Current I m when the power supply voltage E m is (1).
Figure 0006283812
To do. The present invention has been made based on this finding.

Figure 0006283812
ると図2の直列共振回路におけるEmとEsmは電源電圧Emより昇圧する。
Figure 0006283812
すなわち、(2)式より、PVDF圧電素子両端電圧Esmとコイル両端電圧Emは電源電圧Eと選択度Qの積となり電源電圧より昇圧するので、検出感度がQで任意に得られる。
Figure 0006283812
Then, E L m and Esm in the series resonance circuit of FIG. 2 are boosted from the power supply voltage Em.
Figure 0006283812
That is, equation (2), since the PVDF piezoelectric element voltage across Esm and the coil end voltage E L m is boosted from the power supply voltage is the product of the selectivity Q and the power supply voltage E m, the detection sensitivity can be obtained arbitrarily Q.

上述の如き知見に基づき、十分な感度を有するとともに、圧電素子の物性に起因する焦電効果に対する改善も実現し得る本発明の第1の態様は、
圧電材料を2枚の電極で挟んで形成した圧電素子を、複数個積層して形成するとともに、前記各圧電素子間のインピーダンス変化に基づき前記複数個の圧電素子に作用する荷重負荷を検出する荷重検出部と、
前記圧電素子をそれぞれ含み、交流電源により所定の共振周波数で駆動される複数の共振回路とを有するとともに、
前記共振回路は、共振周波数特性が、一つの共振回路の共振周波数特性の高周波側で、かつ他の共振回路の共振周波数特性の低周波側に交点を持ち、該交点が前記荷重負荷の基準点になるように形成したことを特徴とする。
本態様によれば、図4に基づき、後に詳細に説明するが、圧電素子に荷重負荷が作用することにより一方の共振周波数特性においては基準点(荷重負荷=0)にあった電圧が低下するとともに、他方の共振周波数特性においては基準点(荷重負荷=0)にあった電圧が上昇する。この結果、両者の相対的な差として検出される荷重負荷の検出値の感度を上昇させ、荷重負荷の検出値を高精度なものとすることができる。
本発明の第2の態様は、
第1の態様に記載する荷重測定装置において、
積層方向において隣接する2つの圧電素子のうち、前記積層方向で相対向する一方の前記電極間に絶縁層を挟んで形成した静電容量を前記共振回路の回路素子とすることを特徴とする。
本態様によれば、図3に基づき後に詳述するように、圧電素子の電極間の絶縁層を利用して共振回路の回路素子である静電容量を形成することができる。
本発明の第3の態様は、
第2の態様に記載する荷重測定装置において、
複数個の圧電素子は、絶縁層の上面に一方の電極、該電極の上面に前記圧電材料、該圧電材料の上面に他方の電極、該他方の電極の上面に他の絶縁層を順次積層して形成した同構成のものを複数個積層して形成したことを特徴とする。
本態様によれば、図3に基づき後に詳述するように、絶縁層、一方の電極、圧電材料、他方の電極、他の絶縁層をこの順序で積層したものを一ユニットとして、当該ユニットを順次積層するだけで第2の態様に記載する構造を形成することができる。
本発明の第4の態様は、
第1の態様に記載する荷重測定装置の2組を組合わせ、荷重負荷が作用する一方の荷重測定装置の電極の間のインピーダンスに基づく電圧と、前記荷重負荷の影響を受けることなく圧電素子の周囲温度に基づき他方の荷重測定装置の電極の間のインピーダンスに基づく電圧との差分に基づき前記荷重負荷の測定値の温度補正を行うようにしたことを特徴とする。
本態様によれば、図8に基づき後に詳述する、圧電材料の焦電効果による影響をキャンセルすることができる。
発明において、荷重検出は図3(a)に示すように、二つのPVDF圧電素子1とPVDF圧電素子2を上下に重ね合わせた一対とした。同図(b)は荷重測定センサの構成を略図で示した。絶縁膜ポリエステル薄膜コーティング面(8)をCs1とし、もう一方のポリエステル薄膜コーティング面(9)をCs2とすると電極(4)と電極(5)間の誘電体となる。その結果、合成静電量Cs1+Cs2=Csとなり、一対化することでPVDF圧電素子1に容量Csが付加された形となる。






Based on the findings as described above, the first aspect of the present invention, which has sufficient sensitivity and can also improve the pyroelectric effect due to the physical properties of the piezoelectric element,
A plurality of piezoelectric elements formed by sandwiching a piezoelectric material between two electrodes, and a load for detecting a load applied to the plurality of piezoelectric elements based on a change in impedance between the piezoelectric elements. A detection unit;
Each of the piezoelectric elements includes a plurality of resonance circuits driven at a predetermined resonance frequency by an AC power source,
The resonance circuit has an intersection on the high frequency side of the resonance frequency characteristic of one resonance circuit and a low frequency side of the resonance frequency characteristic of another resonance circuit, and the intersection is a reference point of the load load. It is formed so that it becomes.
According to this aspect, as will be described in detail later with reference to FIG. 4, when a load is applied to the piezoelectric element, the voltage at the reference point (load load = 0) decreases in one resonance frequency characteristic. At the same time, in the other resonance frequency characteristic, the voltage at the reference point (load load = 0) increases. As a result, it is possible to increase the sensitivity of the detection value of the load load detected as a relative difference between the two and to make the detection value of the load load highly accurate.
The second aspect of the present invention is:
In the load measuring device described in the first aspect,
Of the two piezoelectric elements adjacent in the stacking direction, a capacitance formed by sandwiching an insulating layer between one of the electrodes facing each other in the stacking direction is used as a circuit element of the resonance circuit.
According to this aspect, as will be described in detail later with reference to FIG. 3, it is possible to form a capacitance that is a circuit element of the resonance circuit using an insulating layer between the electrodes of the piezoelectric element.
The third aspect of the present invention is:
In the load measuring device described in the second aspect,
The plurality of piezoelectric elements are formed by sequentially laminating one electrode on the upper surface of the insulating layer, the piezoelectric material on the upper surface of the electrode, the other electrode on the upper surface of the piezoelectric material, and the other insulating layer on the upper surface of the other electrode. It is characterized by being formed by laminating a plurality of the same structures formed in the above.
According to this aspect, as will be described in detail later with reference to FIG. 3, an insulating layer, one electrode, a piezoelectric material, the other electrode, and another insulating layer laminated in this order as a unit, The structure described in the second embodiment can be formed only by sequentially laminating.
The fourth aspect of the present invention is:
A combination of two sets of load measuring devices described in the first aspect, the voltage based on the impedance between the electrodes of one of the load measuring devices on which the load is applied, and the piezoelectric element without being affected by the load The temperature correction of the measurement value of the load load is performed based on the difference from the voltage based on the impedance between the electrodes of the other load measuring device based on the ambient temperature.
According to the present embodiment will be described in detail later based on FIG. 8, Ru can cancel the effect of the pyroelectric effect of the piezoelectric material.
In the present invention, as shown in FIG. 3 (a), the load is detected as a pair in which two PVDF piezoelectric elements 1 and PVDF piezoelectric elements 2 are vertically stacked. FIG. 2B schematically shows the configuration of the load measuring sensor. When the insulating film polyester thin film coating surface (8) is Cs1, and the other polyester thin film coating surface (9) is Cs2, a dielectric is formed between the electrodes (4) and (5). As a result, the combined electrostatic quantity Cs1 + Cs2 = Cs, and by forming a pair, the capacitor Cs is added to the PVDF piezoelectric element 1.






電圧の共振特性を合わせたPVDF圧電素子に上記の容量CをPVDF圧電素子1に付加したときの、一対の共振周波数特性を調べた結果を図4に示した。正弦波発生電源Eの周波数をわずか変化させながら、かつ一定振幅の電流をPVDF圧電素子1(1)とPVDF圧電素子2(2)に別途に与え、両端子間電圧Esmプロットした。図示したようにPVDF圧電素子1の方は僅かに共振点が低い方に移動した。Shows when the capacitance C S to a PVDF piezoelectric element combined resonance characteristic of voltage added to the PVDF piezoelectric element 1, the results of examining the pair of resonance frequency characteristics in FIG. Slightly varying the frequency of the sine wave generation source E m, and the constant amplitude current fed separately to the PVDF piezoelectric element 1 (1) and the PVDF piezoelectric element 2 (2), and the voltage Esm plotted between both terminals. As shown in the figure, the PVDF piezoelectric element 1 moved slightly toward the lower resonance point.

上記の、PVDF圧電素子1(1)とPVDF圧電素子2(2)を重ね合わせた一対で構成した荷重測定センサであり、それぞれの出力電圧はPVDF圧電素子1(1)の電極間電圧ESm1とVDF圧電素子2(2)の電極間電圧ESm2とする。The load measuring sensor is a load measuring sensor constituted by a pair of the PVDF piezoelectric element 1 (1) and the PVDF piezoelectric element 2 (2), and each output voltage is an inter-electrode voltage ESm of the PVDF piezoelectric element 1 (1). 1 and the interelectrode voltage E Sm 2 of the VDF piezoelectric element 2 (2).

図4のfS0で示す点は、一対のPVDF圧電素子の電極間電圧(ESm1=ESm2)が同じ電圧になるように、正弦波発生電源(13)の周波数を固定して設定した。The point indicated by f S0 in FIG. 4 is set by fixing the frequency of the sine wave generating power supply (13) so that the voltage between the electrodes (E Sm 1 = E Sm 2) of the pair of PVDF piezoelectric elements becomes the same voltage. did.

図面より、一対のPVDF圧電素子1(1)とPVDF圧電素子2(2)に、外力が加わると素子の電圧の周波数はわずかにfso+△fに移動する。PVDF圧電素子1(1)の端子間電圧Esm1は、周波数をfsoのときより低い値となる。同様に、PVDF圧電素子2(2)の端子間電圧Esm2は、周波数fs0のときより高い値となり差動出力電圧が得られる。






From the drawing, when an external force is applied to the pair of PVDF piezoelectric elements 1 (1) and PVDF piezoelectric elements 2 (2), the frequency of the voltage of the elements slightly moves to fso + Δf. The voltage Esm1 between terminals of the PVDF piezoelectric element 1 (1) is lower than when the frequency is fso. Similarly, the voltage between the terminals Esm2 of PVDF piezoelectric element 2 (2), Ru high as will the differential output voltage than when the frequency fs0 is obtained.






本発明の荷重測定センサは、荷重や力を加えると電圧の周波数の高い方に移動する振動型センサの原理を利用している。圧電素子の直列共振回路の選択度Qの利用により、検出感度が任意に設定できる。  The load measuring sensor of the present invention utilizes the principle of a vibration type sensor that moves to a higher voltage frequency when a load or force is applied. The detection sensitivity can be arbitrarily set by using the selectivity Q of the series resonance circuit of the piezoelectric element.

2つの圧電素子を重ね合わせた一対構成によって、生成した静電容量を利用すると両者に僅かの共振点の差異が生じた。一対の圧電素子に与える外力を増減するとそれに応じて周波数が移動し、これに対応して、両者の素子間電圧が増減するので、それぞれの端子間電圧は検出手段(14)で外力の増減が高感度で検出できる荷重測定センサが提供できる。  When the generated electrostatic capacity is used by a paired configuration in which two piezoelectric elements are superposed, a slight difference in resonance point occurs between them. When the external force applied to the pair of piezoelectric elements is increased or decreased, the frequency shifts accordingly, and accordingly, the voltage between both elements increases or decreases. Therefore, the voltage between the terminals is increased or decreased by the detecting means (14). A load measuring sensor capable of detecting with high sensitivity can be provided.

図1は直列共振回路の周波数変化と電流の関係を示した説明図である。FIG. 1 is an explanatory diagram showing the relationship between the frequency change of the series resonant circuit and the current. 図2は圧電素子の等価回路を示した説明図である。FIG. 2 is an explanatory diagram showing an equivalent circuit of the piezoelectric element. 図3はPVDF圧電素子の構成を示した説明図である。FIG. 3 is an explanatory diagram showing the configuration of the PVDF piezoelectric element. 図4は測定原理を示した説明図である。FIG. 4 is an explanatory diagram showing the measurement principle. 図5は荷重測定センサの構成を示した説明図である。FIG. 5 is an explanatory diagram showing the configuration of the load measuring sensor. 図6は荷量測定センサの等価回路を示した説明図である。FIG. 6 is an explanatory diagram showing an equivalent circuit of the load measuring sensor. 図7は出力―荷重特性を示した。(実施例1)FIG. 7 shows the output-load characteristics. Example 1 図8は温度補正回路のブロック線図を示した。(実施例2)FIG. 8 shows a block diagram of the temperature correction circuit. (Example 2)

荷重測定センサは高分子圧電材料からなり、外力を受けるPVDF圧電素子である。高分子圧電材料としては、ポリフッ化ビニリデン(PVDF)、ポリフッ化ビニル、ポリフッ化ビニリデンおよび/またはポリフッ化ビニルを主成分とする共重合体、奇数ナイロン、ポリ尿素、ビニリデンシシアナイドを主成分とする共重合体、ポリウレタン、アクリロニトリル系共重合体、およびポリ塩化ビニールの中から選択された材料などを採用できる。  The load measuring sensor is a PVDF piezoelectric element made of a polymer piezoelectric material and receiving an external force. Polymer piezoelectric materials include polyvinylidene fluoride (PVDF), polyvinyl fluoride, polyvinylidene fluoride and / or copolymers based on polyvinyl fluoride, odd-number nylon, polyurea, and vinylidene cycyanide as main components. A material selected from a copolymer, polyurethane, acrylonitrile copolymer, and polyvinyl chloride can be used.

本発明の実施形態の荷重測定センサの構成を図5に示す。回路は抵抗(11)とコイル(12)と荷重測定センサとして高分子圧電材料を用いた直列共振回路である。
共振周波数を合わせた圧電素子2つを上下に重ね合わせ固定して、一対の荷重センサとした。圧電素子間の出力電圧を検出手段(14)により荷重の大きさを検出した。
素子の電極表面はポリエステル薄膜(8)、(9)で絶縁されているので、2つの素子の電極同士は接触しない構成である。
The configuration of the load measuring sensor according to the embodiment of the present invention is shown in FIG. The circuit is a series resonant circuit using a resistor (11), a coil (12), and a polymer piezoelectric material as a load measuring sensor.
Two piezoelectric elements having the same resonance frequency were stacked one above the other and fixed to form a pair of load sensors. The magnitude of the load was detected by the detection means (14) for the output voltage between the piezoelectric elements.
Since the electrode surface of the element is insulated by the polyester thin films (8) and (9), the electrodes of the two elements are not in contact with each other.

圧電素子の電圧の共振周波数を合わせた二つのPVDF圧電素子のポリエステル薄膜コーティング面(8)をCS1とし、もう一方のポリエステル薄膜コーティング面(9)をCS2とすると電極(4)と電極(5)間ではポリエステル薄膜コーティング面が誘電体となり、静電容量 CS1+CS2=Cが生成され、容量CはPVDF圧電素子1に付加し、2つの圧電素子の共振周波数に僅かに差異を生じさせた荷重測定センサである。When the polyester thin film coating surface (8) of two PVDF piezoelectric elements having the resonance frequency of the piezoelectric element voltage is C S1 and the other polyester thin film coating surface (9) is C S2 , the electrode (4) and the electrode ( Between 5), the polyester thin film coating surface becomes a dielectric, and a capacitance C S1 + C S2 = C S is generated. The capacitance C S is added to the PVDF piezoelectric element 1, and the resonance frequency of the two piezoelectric elements is slightly different. This is a load measuring sensor that causes

上記より、2つの圧電素子を一対にした荷重測定センサは、外部から荷重や力を同時に受けることとなる。外力が加わると共振特性により、図6に示す素子間電圧Esm2は増加し、もう一方の素子間電圧Esm1は減少するので差動出力電圧の荷重測定センサが提供できる。なお、コイルの両端の電圧振幅を取り出しても良い。From the above, the load measuring sensor in which two piezoelectric elements are paired receives a load and a force from the outside at the same time. When an external force is applied, the inter-element voltage Esm2 shown in FIG. 6 increases and the other inter-element voltage Esm1 decreases due to the resonance characteristics, so that a differential output voltage load measuring sensor can be provided. The voltage amplitude at both ends of the coil may be taken out.

図4に示すように、PVDF圧電素子1(1)のΔfの時の端子間電圧Esm1とPVD圧電素子2(2)のΔfの端子間電圧Esm2が同電位になるように、正弦波発生電源(13)周波数を可変して図中のfS0点に固定して設定した。As shown in FIG. 4, a sinusoidal wave so that the voltage between terminals Esm1 at the time of Δf 1 of the PVDF piezoelectric element 1 (1) and the voltage between the terminals Esm2 at the Δf 2 of the PVD piezoelectric element 2 (2) are the same potential. The frequency of the generated power source (13) was varied and fixed at the fSO point in the figure.

圧電素子の出力電圧の周波数の急峻化により、PVDF圧電素子1(1)とPVDF圧電素子2(2)に、外力が加わると周波数はわずか(fS0+Δf(図4参照)に移動する。PVDF圧電素子1(1)の端子間電圧Esmは、周波数をfS0のときのより低い値となる。同様に、PVDF圧電素子2(2)の端子間電圧Esmは、周波数をfS0のときのより高い値となる。荷重測定センサの出力電圧は差動出力電圧が得られる。したがって、本発明によれば荷重や力が高感度での測定できる。Due to the steepness of the frequency of the output voltage of the piezoelectric element, when an external force is applied to the PVDF piezoelectric element 1 (1) and the PVDF piezoelectric element 2 (2), the frequency slightly shifts (f S0 + Δf (see FIG. 4)). The inter-terminal voltage Esm of the piezoelectric element 1 (1) has a lower value when the frequency is f S0 Similarly, the inter-terminal voltage Esm of the PVDF piezoelectric element 2 (2) is the same as that when the frequency is f S0 . Since the output voltage of the load measuring sensor is a differential output voltage, the load and force can be measured with high sensitivity according to the present invention.

図6は、本発明の1実施例の等価回路図であって、PVDF圧電素子(厚さ:28μm、電極寸法:10×15mm)を2枚上下に重ね一対にして、抵抗(50Ω)11とコイル(1.5mH)12を直列接続した直列共振回路に、PVDF圧電素子の共振点近傍の一定周波数fS0(約164kHz、2Vp−p)、振幅一定の電圧を正弦波発生電源13で印加した。FIG. 6 is an equivalent circuit diagram of an embodiment of the present invention, in which two PVDF piezoelectric elements (thickness: 28 μm, electrode dimensions: 10 × 15 mm) are stacked one above the other to form a resistor (50Ω) 11 A constant frequency f S0 (about 164 kHz, 2 Vp-p) near the resonance point of the PVDF piezoelectric element and a constant amplitude voltage were applied to a series resonance circuit in which a coil (1.5 mH) 12 was connected in series by a sine wave generation power source 13. .

上記検出部の出力電圧ESm1と出力電圧ESm2の差動出力電圧を、検出手段14で荷重の大きさの計測をした。The differential output voltage of the output voltage E Sm 1 and the output voltage E Sm 2 of the detection unit was measured for the magnitude of the load by the detection means 14.

上記検出手段によって荷重を加えたときの出力電圧の関係を、出力電圧―荷重特性を図7に示す。加えた荷重に応じて出力電圧が直線的に変化し荷重測定装置として良好な結果が得られた。FIG. 7 shows the relationship between the output voltage and the output voltage-load characteristic when a load is applied by the detecting means. The output voltage changed linearly according to the applied load, and good results were obtained as a load measuring device.

圧電素子の物性に起因する焦電性は、温度を変えたとき外力を与えない状態で自発分極により、無荷重状態でも電圧が素子間に発生する。とくに、高感度が必要な微弱な荷重や力の測定において、焦電効果の影響は無視できない。In the pyroelectric property resulting from the physical properties of the piezoelectric element, a voltage is generated between the elements even in a no-load state due to spontaneous polarization without applying an external force when the temperature is changed. In particular, the influence of the pyroelectric effect cannot be ignored in measuring weak loads and forces that require high sensitivity.

図8に実施例2の、温度補正のブロック線図を示す。一対構成のセンサを2組によるもので、温度検出に荷重測定センサを利用した実施例を示す。PVDF圧電素子(厚さ:28μm、電極寸法:10×15mm)1とPVDF圧電素子(厚さ:28μm、電極寸法:10×15mm)2を2枚上下に重ね一対にした。抵抗(50Ω)11とコイル(1.5mH)12の直列共振回路に、PVDF圧電素子の共振点近傍の一定周波数fS0(約164kHz)、一定振幅の電圧の正弦波発生電源13で圧電素子を励振した。FIG. 8 is a block diagram of temperature correction according to the second embodiment. An embodiment in which two pairs of sensors are used and a load measuring sensor is used for temperature detection will be described. Two PVDF piezoelectric elements (thickness: 28 μm, electrode dimensions: 10 × 15 mm) 1 and PVDF piezoelectric elements (thickness: 28 μm, electrode dimensions: 10 × 15 mm) 2 were stacked one above the other to form a pair. A piezoelectric element is connected to a series resonant circuit of a resistor (50Ω) 11 and a coil (1.5 mH) 12 with a sine wave generation power supply 13 having a constant frequency f S0 (about 164 kHz) and a constant amplitude voltage near the resonance point of the PVDF piezoelectric element. Excited.

図に示すように、荷重測定センサ出力電圧(A)と温度検出センサ出力電圧(C)は温度補正増幅器(E)入力であり、荷重測定センサ出力電圧(B)と温度検出センサ出力電圧(D)を温度補正増幅器(F)入力として、演算すると温度補正が行われ後、出力電圧は増幅回路(G)により荷重の大きさを検出した実施例である。なお、温度検出センサは荷重や力のダミーとして用いた。図には示していないが、約20度から40度の範囲までの増幅回路(G)の出力電圧の変化は数mV以内であることを確認した。  As shown in the figure, the load measurement sensor output voltage (A) and the temperature detection sensor output voltage (C) are inputs to the temperature correction amplifier (E), and the load measurement sensor output voltage (B) and the temperature detection sensor output voltage (D) ) As an input to the temperature correction amplifier (F), the temperature is corrected by calculation and the output voltage is an embodiment in which the magnitude of the load is detected by the amplifier circuit (G). The temperature detection sensor was used as a load or force dummy. Although not shown in the figure, it was confirmed that the change in the output voltage of the amplifier circuit (G) within the range of about 20 degrees to 40 degrees was within several mV.

本荷重測定装置は、介護・医療監視用として起き上がり、胎児心拍モニター、無呼吸モニター、脈拍モニター、体圧分布センサ、血圧モニター、体温モニターなどに用いても好適である。  This load measuring apparatus is suitable for use in nursing and medical monitoring, and for fetal heart rate monitor, apnea monitor, pulse monitor, body pressure distribution sensor, blood pressure monitor, body temperature monitor and the like.

1 PVDF圧電素子1
2 PVDF圧電素子2
3 PVDF圧電素子2の電極
4 PVDF圧電素子2の電極
5 PVDF圧電素子1の電極
6 PVDF圧電素子1の電極
7 PVDF圧電素子2のアクリルコーティング面
8 PVDF圧電素子2のポリエステル薄膜面
9 PVDF圧電素子1のポリエステル薄膜面
10 PVDF圧電素子1のアクリルコーティング面
11 抵抗
12 コイル
13 正弦波発生定電流電源
14 検出手段
1 PVDF piezoelectric element 1
2 PVDF piezoelectric element 2
DESCRIPTION OF SYMBOLS 3 Electrode of PVDF piezoelectric element 2 Electrode of PVDF piezoelectric element 2 Electrode of PVDF piezoelectric element 1 Electrode of PVDF piezoelectric element 1 Acrylic coating surface 8 of PVDF piezoelectric element 2 Polyester thin film surface 9 of PVDF piezoelectric element 2 PVDF piezoelectric element 1 Polyester thin film surface 10 Acrylic coating surface of PVDF piezoelectric element 1 Resistance 12 Coil 13 Sine wave generation constant current power supply 14 Detection means

Claims (4)

圧電材料を2枚の電極で挟んで形成した圧電素子を、複数個積層して形成するとともに、前記各圧電素子間のインピーダンス変化に基づき前記複数個の圧電素子に作用する荷重負荷を検出する荷重検出部と、
前記圧電素子をそれぞれ含み、交流電源により所定の共振周波数で駆動される複数の共振回路とを有するとともに、
前記共振回路は、共振周波数特性が、一つの共振回路の共振周波数特性の高周波側で、かつ他の共振回路の共振周波数特性の低周波側に交点を持ち、該交点が前記荷重負荷の基準点になるように形成したことを特徴とする荷重測定装置。
A plurality of piezoelectric elements formed by sandwiching a piezoelectric material between two electrodes, and a load for detecting a load applied to the plurality of piezoelectric elements based on a change in impedance between the piezoelectric elements. A detection unit;
Each of the piezoelectric elements includes a plurality of resonance circuits driven at a predetermined resonance frequency by an AC power source,
The resonance circuit has an intersection on the high frequency side of the resonance frequency characteristic of one resonance circuit and a low frequency side of the resonance frequency characteristic of another resonance circuit, and the intersection is a reference point of the load load. A load measuring device formed so as to become.
請求項1に記載する荷重測定装置において、
積層方向において隣接する2つの圧電素子のうち、前記積層方向で相対向する一方の前記電極間に絶縁層を挟んで形成した静電容量を前記共振回路の回路素子とすることを特徴とする荷重測定装置。
In the load measuring device according to claim 1,
Of the two piezoelectric elements adjacent in the stacking direction, a load formed by sandwiching an insulating layer between one of the electrodes facing each other in the stacking direction is a circuit element of the resonance circuit measuring device.
請求項2に記載する荷重測定装置において、
複数個の圧電素子は、絶縁層の上面に一方の電極、該電極の上面に前記圧電材料、該圧電材料の上面に他方の電極、該他方の電極の上面に他の絶縁層を順次積層して形成した同構成のものを複数個積層して形成したことを特徴とする荷重測定装置。
In the load measuring device according to claim 2,
The plurality of piezoelectric elements are formed by sequentially laminating one electrode on the upper surface of the insulating layer, the piezoelectric material on the upper surface of the electrode, the other electrode on the upper surface of the piezoelectric material, and the other insulating layer on the upper surface of the other electrode. A load measuring device formed by laminating a plurality of components having the same structure.
請求項1に記載する荷重測定装置の2組を組合わせ、荷重負荷が作用する一方の荷重測定装置の電極の間のインピーダンスに基づく電圧と、前記荷重負荷の影響を受けることなく圧電素子の周囲温度に基づき他方の荷重測定装置の電極の間のインピーダンスに基づく電圧との差分に基づき前記荷重負荷の測定値の温度補正を行うようにしたことを特徴とする荷重測定装置。 A combination of two sets of the load measuring device according to claim 1, a voltage based on an impedance between electrodes of one load measuring device on which a load load acts, and a surrounding of the piezoelectric element without being affected by the load load load measurement equipment being characterized in that to perform the temperature compensation of the measured value of the applied load based on the difference between the voltage based on the impedance between the electrode of the other of the load measuring device based on the temperature.
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US10905334B2 (en) 2015-08-31 2021-02-02 Koninklijke Philips N.V. Electroactive polymer sensors and sensing methods
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