JPH0810155B2 - Weight detector - Google Patents

Weight detector

Info

Publication number
JPH0810155B2
JPH0810155B2 JP63220959A JP22095988A JPH0810155B2 JP H0810155 B2 JPH0810155 B2 JP H0810155B2 JP 63220959 A JP63220959 A JP 63220959A JP 22095988 A JP22095988 A JP 22095988A JP H0810155 B2 JPH0810155 B2 JP H0810155B2
Authority
JP
Japan
Prior art keywords
detection
electrode
weight
mounting table
capacitance
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Expired - Lifetime
Application number
JP63220959A
Other languages
Japanese (ja)
Other versions
JPH0267925A (en
Inventor
茂樹 植田
誠 三原
正信 井上
謙三 黄地
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Panasonic Holdings Corp
Original Assignee
Matsushita Electric Industrial Co Ltd
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Matsushita Electric Industrial Co Ltd filed Critical Matsushita Electric Industrial Co Ltd
Priority to JP63220959A priority Critical patent/JPH0810155B2/en
Publication of JPH0267925A publication Critical patent/JPH0267925A/en
Publication of JPH0810155B2 publication Critical patent/JPH0810155B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

Links

Description

【発明の詳細な説明】 産業上の利用分野 本発明は静電容量の変化を利用して被測定物の重量を
検出する重量検出装置に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a weight detection device that detects the weight of an object to be measured by utilizing a change in capacitance.

従来の技術 電極を所定の間隙を保って対向させ、これに加えられ
た圧力を静電容量の変化として取り出す静電容量型圧力
センサは、すでに多数実用に供されている。
2. Description of the Related Art A large number of capacitance-type pressure sensors have been put to practical use, in which electrodes are opposed to each other with a predetermined gap therebetween and the pressure applied to the electrodes is taken out as a change in capacitance.

このようなセンサの容量値は、通常20〜50pF程度とご
くわずかなため、検出回路やセンサ自身の温度特性によ
り、大きな誤差が生じる。そこで温度による特性の変化
を如何に解決するかがこの種のセンサにおける重要な課
題であった。
Since the capacitance value of such a sensor is usually as small as about 20 to 50 pF, a large error occurs due to the temperature characteristics of the detection circuit and the sensor itself. Therefore, how to solve the change in characteristics due to temperature was an important issue in this type of sensor.

このため加えられた圧力に応じて容量値が鋭敏に変化
する検出電極を基板の中央部に設け、その外周部に加え
られた圧力によってはあまり容量値の変化しない基準電
極を配する静電容量型圧力センサが、一般に知られてい
る。
For this reason, a capacitance is provided in the center of the substrate where the capacitance value changes sharply according to the applied pressure, and a reference electrode whose capacitance value does not change much depending on the pressure applied to the outer periphery Mold pressure sensors are generally known.

特開昭58−198739号公報に記載の静電容量型圧力セン
サは、このようなセンサの一例であり、上記の二つの容
量を充放電し、これらを比較することで、センサおよび
回路の温度特性の低減を図ろうとしている。
The capacitance type pressure sensor described in Japanese Patent Laid-Open No. 58-198739 is an example of such a sensor. By charging and discharging the above two capacitors and comparing them, the temperature of the sensor and the circuit can be compared. We are trying to reduce the characteristics.

第6図はかかる静電容量型圧力センサの構成を表して
おり、(a)図は断面を、(b)図は2枚の基板を展開
した状態を示している。
FIG. 6 shows the configuration of such a capacitance type pressure sensor, FIG. 6 (a) shows a cross section, and FIG. 6 (b) shows a state in which two substrates are developed.

アルミナの基板1および2には二つの電極が印刷さ
れ、一定の間隙を保って対向するよう周縁をガラス3に
よって封止されている。このため中央の検出電極4は外
圧に対して鋭敏に変化し、一方外周の基準電極5はガラ
スに近接しているためにたわみにくく、外圧による圧力
変化が前者と比してごく少ない。
Two electrodes are printed on the substrates 1 and 2 made of alumina, and the peripheral edges thereof are sealed with glass 3 so as to face each other with a constant gap. Therefore, the detection electrode 4 in the center changes sharply with respect to the external pressure, while the reference electrode 5 on the outer periphery is close to the glass and is not easily bent, and the pressure change due to the external pressure is very small compared with the former.

そして両容量とも同一の基板内に近接して配されてい
るので、温度による影響はほぼ同様に受ける。従って両
者を比較すれば、温度の影響のみを取り除き、圧力情報
だけを得ることができる。
Since both capacitors are arranged close to each other on the same substrate, they are affected by temperature almost in the same manner. Therefore, by comparing the two, it is possible to remove only the influence of temperature and obtain only pressure information.

第7図はかかる従来の回路構成である。検出電極4の
容量Cpと基準電極5の容量Crとは、それぞれ抵抗R1,R2
に接続され、充放電回路が構成される。両容量はトラン
ジスタQ1,Q2によりオンオフされ、充放電を繰り返す。
その動作および各部の波形については、引用例に詳しい
ので省略するが、センサの容量をCp>Crに設定すれば、
電源電圧がVCCのとき、ローパスフィルタ6の出力電圧V
outは Vout=VCC(1−Cr/Cp) ……(1) となる。センサの温度特性はすでに述べたようにほぼ同
一であるから、温度に起因する容量の変化分ΔCr(ppm/
℃)およびΔCp(ppm/℃)は、(1−Cr/Cp)項により
相殺され、出力電圧Voutからセンサの温度特性を取り除
ける。
FIG. 7 shows such a conventional circuit configuration. The capacitance C p of the detection electrode 4 and the capacitance C r of the reference electrode 5 are the resistances R 1 and R 2 respectively.
And a charge / discharge circuit is configured. Both capacitors are turned on and off by the transistors Q 1 and Q 2 , and charging and discharging are repeated.
The operation and waveforms of each part are omitted because they are detailed in the cited example, but if the capacitance of the sensor is set to C p > C r ,
When the power supply voltage is V CC , the output voltage V of the low pass filter 6
out becomes V out = V CC (1-C r / C p ) ... (1). Since the temperature characteristics of the sensor are almost the same as already described, the change in capacitance due to temperature ΔC r (ppm /
C) and ΔC p (ppm / ° C.) are canceled by the (1-C r / C p ) term to remove the temperature characteristic of the sensor from the output voltage V out .

ただしこのときR1=R2であり、比較器7と8およびト
ランジスタQ1とQ2とは、温度特性の揃ったものを選別し
てペアにしなければならない。このような条件を守れ
ば、センサ以外の回路に起因する温度特性を取り除ける
という。
However, at this time, R 1 = R 2 , and the comparators 7 and 8 and the transistors Q 1 and Q 2 must be selected as a pair so as to have uniform temperature characteristics. If these conditions are observed, the temperature characteristics due to circuits other than the sensor can be removed.

発明が解決しようとする課題 ところが、このような従来の構成の静電容量型圧力セ
ンサを重量検出装置として利用したところ検出した重量
値が温度によって実用上無視できない程度にドリフトし
てしまうことがわかった。
The problem to be solved by the invention However, when the capacitance type pressure sensor having such a conventional configuration is used as a weight detection device, it is found that the detected weight value drifts to a practically nonnegligible temperature value. It was

この原因を追求してみると、センサの温度特性はごく
小さなものであったが、回路に起因する温度特性が比較
的大きく存在することが判明した。
In pursuit of this cause, it was found that the temperature characteristic of the sensor was extremely small, but the temperature characteristic due to the circuit was relatively large.

これは一般に発振回路の動作周波数fは、次式で表さ
れるが、この回路定数Kが温度特性を有するためである
と推測される。
This is generally because the operating frequency f of the oscillation circuit is expressed by the following equation, but it is presumed that this circuit constant K has a temperature characteristic.

f=K/RC ……(2) ただし K:回路定数 第8図はかかる動作周波数fの温度特性をある発振回
路で実測したものである。横軸の動作周波数fはCもし
くはRを変化させ、縦軸の温度特性Δfは次式によっ
た。
f = K / RC (2) However, K: Circuit constant FIG. 8 shows the temperature characteristics of the operating frequency f measured by an oscillator circuit. The operating frequency f on the horizontal axis changes C or R, and the temperature characteristic Δf on the vertical axis is obtained by the following equation.

Δf=(f20−fα)/〔f20×(α−20)〕……(3) ただし、 f20:20℃での周波数 fα:α℃での周波数 つまり第8図は、センサの温度特性が小さく抑えられ
ても、発振回路に温度特性が残留し、しかもそれはその
動作周波数に応じて現れ、周波数が高くなるほど温度特
性も大きくなる、ということを示している。
Δf = (f 20 -fα) / [f 20 × (α-20)] ... (3) where, f 20: Frequency at 20 ° C. f.alpha: Frequency ie Figure 8 at alpha ° C., the temperature of the sensor It is shown that even if the characteristic is suppressed to be small, the temperature characteristic remains in the oscillation circuit, which appears according to the operating frequency, and the higher the frequency, the larger the temperature characteristic.

さまざまな発振回路で実験を行ったが、温度特性直線
の勾配や正負の極性には変化が現れるものの、基本的に
はいずれの発振回路によっても動作周波数に依存する同
様の温度特性が確認された。
Experiments were carried out in various oscillator circuits, but basically the same temperature characteristics depending on the operating frequency were confirmed by any oscillator circuit, although the slope of the temperature characteristic line and the positive and negative polarities changed. .

この現象はセンサの容量を検出する手段として発振回
路を用いると、検出周波数と基準周波数が一致している
時、つまり検出容量と基準容量が一致している時には、
その温度特性は完全に消去されるが、その周波数がずれ
てくると、回路に起因する温度特性が現れてくる、とい
うことを示唆している。
This phenomenon occurs when an oscillation circuit is used as a means for detecting the capacitance of the sensor, when the detection frequency and the reference frequency match, that is, when the detection capacitance and the reference capacitance match.
The temperature characteristic is completely erased, but it is suggested that when the frequency shifts, the temperature characteristic due to the circuit appears.

しかるに引用した先行技術では、Cp>Crが満足されな
ければ動作しないので、使用する全領域に渡って、この
周波数のずれによる温度特性を覚悟しなければならな
い。
However, in the prior art cited above, if C p > C r is not satisfied, operation does not occur, and therefore temperature characteristics due to this frequency shift must be prepared over the entire range of use.

本発明はかかる回路に起因する温度特性の影響を軽微
に抑えようとするものである。
The present invention intends to suppress the influence of temperature characteristics caused by such a circuit to a slight extent.

課題を解決するための手段 本発明は、上記課題を解決するために、被測定物を載
置する載置台と、所定の間隙を設けて対向し、中央部に
検出電極を、その外周部に基準電極を有する一対の平板
より形成した静電容量型圧力センサと、前記検出電極お
よび基準電極の容量を読み出す検出手段と、演算手段を
有し、前記両電極の容量を切り換えて測定する制御部と
を備えている。
Means for Solving the Problems The present invention, in order to solve the above problems, a mounting table on which an object to be measured is mounted, is opposed to the mounting table with a predetermined gap, and a detection electrode is provided in the central portion and an outer peripheral portion thereof. A control unit having an electrostatic capacitance type pressure sensor formed of a pair of flat plates having a reference electrode, a detection means for reading the capacitances of the detection electrode and the reference electrode, and an arithmetic means, for switching and measuring the capacitances of the both electrodes. It has and.

作用 本発明の重量検出装置は、載置台と機械的に係合さ
れ、載置台上に載置される被測定物の重量により検出電
極の容量値が変化するよう構成され、載置台上に最大秤
量の略二分の一の重量の被測定物を載置した際に、検出
電極と基準電極の容量がほぼ一致するように電極形状が
設定される。そして制御部は検出電極および基準電極の
容量を切り換えながら検出手段を介して測定し、演算手
段を用いてその測定結果を演算処理し、その解をもとに
被測定物の重量を算出する。
Action The weight detection device of the present invention is configured to be mechanically engaged with the mounting table so that the capacitance value of the detection electrode changes depending on the weight of the object to be measured mounted on the mounting table. The electrode shape is set so that the capacitances of the detection electrode and the reference electrode are substantially the same when the object to be measured having a weight of approximately one half of the weight is placed. Then, the control unit performs measurement through the detection unit while switching the capacitances of the detection electrode and the reference electrode, arithmetically processes the measurement result using the arithmetic unit, and calculates the weight of the object to be measured based on the solution.

かかる構成、作用により、載置台上で無負荷から最大
秤量に至るまで、温度特性を極端に増大させることなく
重量を検出できる。
With such a configuration and operation, the weight can be detected on the mounting table from no load to the maximum weighing without extremely increasing the temperature characteristics.

実 施 例 以下、本発明に係わる重量検出装置を図面を参照して
説明する。
Example Hereinafter, a weight detection device according to the present invention will be described with reference to the drawings.

第2図は電子レンジの如き加熱装置の載置台に本発明
に係わる重量検出装置を装備した例を示しており、被加
熱物の初期重量や加熱中の重量変化を検出する。
FIG. 2 shows an example in which a weight detecting device according to the present invention is mounted on a mounting table of a heating device such as a microwave oven, and detects the initial weight of the object to be heated and the weight change during heating.

加熱室9には熱源10が結合され、載置台11上には被測
定物12が載置される。13はこの載置台11を回転駆動する
モータであり、被測定物12が熱源10により加熱される
際、加熱ムラを起こすことを改善する。
A heat source 10 is coupled to the heating chamber 9, and an object to be measured 12 is placed on a mounting table 11. Reference numeral 13 is a motor that drives the mounting table 11 to rotate, and improves the occurrence of uneven heating when the object 12 to be measured is heated by the heat source 10.

このモータ13の回転軸は、スラスト方向に自在に動
き、その先端を静電容量型圧力センサ14が支持するの
で、載置台11と被測定物12の重量は、静電容量型圧力セ
ンサ14に伝達される。
The rotating shaft of the motor 13 freely moves in the thrust direction, and the tip end thereof is supported by the capacitance type pressure sensor 14. Therefore, the weights of the mounting table 11 and the object 12 to be measured are stored in the capacitance type pressure sensor 14. Transmitted.

センサの構成は、第6図に示した従来のものと同一で
あり、すでに記述したのでここでは重複を避けて説明は
割愛する。
The structure of the sensor is the same as that of the conventional one shown in FIG. 6 and has already been described. Therefore, the description will be omitted here by avoiding duplication.

第3図は本発明に係わる重量検出装置のシステム構成
を示すブロック図の一実施例である。
FIG. 3 is an embodiment of a block diagram showing the system configuration of the weight detecting apparatus according to the present invention.

単一の検出手段は基準電極の容量値である基準容量Cr
と、検出電極の容量値である検出容量Cpおよび抵抗Rを
含むCR発振回路15により構成される。スイッチング手段
16は制御部17に内蔵された切換ゲート信号制御手段18に
よって制御され、基準容量Crと検出容量Cpとを切り換え
て発振回路15に接続し、発振周波数frおよびfpとして制
御部17内のカウンタ手段19に入力する。そしてカウンタ
手段19の出力は、それぞれRAM20の所定のアドレスに格
納され、演算手段21に転送されて除算処理を施され、比
rが求められる。
The single detection means is the reference capacitance C r, which is the capacitance value of the reference electrode.
And a CR oscillation circuit 15 including a detection capacitance C p which is the capacitance value of the detection electrode and a resistor R. Switching means
16 is controlled by a switching gate signal control means 18 incorporated in the control unit 17, switches between the reference capacitance C r and the detection capacitance C p and is connected to the oscillation circuit 15, and the control unit 17 sets the oscillation frequencies f r and f p. Input to the counter means 19 inside. Then, the output of the counter means 19 is stored in a predetermined address of the RAM 20, respectively, transferred to the arithmetic means 21 and subjected to division processing, and the ratio r is obtained.

次に第1図を用いて本発明の要点を説明する。第1図
は検出電極と基準電極との容量の関係を示す線図であ
る。横軸は載置台上に載置される被測定物の重量wを、
縦軸は検出手段たる発振回路の出力周波数およびその比
rを示す。w=wplなる点は、載置台のみを載置した状
態を、w=wmaxなる点は最大秤量を、それぞれ表してい
る。
Next, the essential points of the present invention will be described with reference to FIG. FIG. 1 is a diagram showing a capacitance relationship between a detection electrode and a reference electrode. The horizontal axis represents the weight w of the object to be measured placed on the mounting table,
The vertical axis represents the output frequency of the oscillation circuit as the detection means and the ratio r thereof. The point w = w pl represents the state where only the mounting table is mounted, and the point w = w max represents the maximum weighing amount.

重量wが重くなるほど、基板のたわみは大きくなり、
電極間の距離が小さくなるので、容量値は次式から逆に
大きくなる。
The heavier the weight w, the greater the deflection of the substrate,
Since the distance between the electrodes becomes smaller, the capacitance value becomes larger from the following equation.

C=εS/d ……(4) ただし ε:空気中の誘電率 C:電極間容量 S:電極面積 d:電極間距離 周波数fは(2)式から求められるので、重量wが増
すと周波数fは逆に低くなっていく。
C = εS / d (4) where ε: Permittivity in air C: Interelectrode capacitance S: Electrode area d: Electrode distance Frequency f is calculated from equation (2), so if weight w increases, frequency On the contrary, f becomes lower.

ここで両者の比rを求めると、 となる。検出回路として単一の発振回路を用いているた
め、回路定数Kはfr,fpともに同一であり、また抵抗R
も共通なのて、周波数の比rを算出すれば、それは検出
容量Cpと基準容量Crの比と一致することになる。よって
かかる比rを求めれば、センサの温度特性を相殺でき
る。
Here, if the ratio r of both is calculated, Becomes Since a single oscillator circuit is used as the detection circuit, the circuit constant K is the same for both f r and f p , and the resistance R
Since the frequency ratio r is calculated, it is the same as the ratio between the detection capacitance C p and the reference capacitance C r . Therefore, the temperature characteristic of the sensor can be canceled by obtaining the ratio r.

ここでさらに基準容量Crと検出容量Cpとをwpl〜wmax
の間に、すなわち載置台上に最大秤量より軽い、ある重
量wzの被測定物が置かれたときに一致させると、当然の
ことながらふたつのときに一致させると、当然のことな
がらふたつの周波数frとfpとは、w=wz点で交差するこ
とになる。
Here, the reference capacity C r and the detection capacity C p are further calculated as w pl to w max.
Between, i.e., when a measured object of a certain weight w z , which is lighter than the maximum weight, is placed on the mounting table, it is natural that if the two objects are matched at two times, naturally, the two The frequencies f r and f p will intersect at the point w = w z .

従ってw=wz点で比rは1となる。すでに説明したよ
うに、動作周波数が一致する場合には、回路に起因する
温度特性は完全に消去できる。つまり比r=1となるwz
点での温度特性は原理上、ゼロとなる。
Therefore, the ratio r becomes 1 at the point of w = w z . As described above, when the operating frequencies are the same, the temperature characteristic caused by the circuit can be completely eliminated. That is, w z where the ratio r = 1
In principle, the temperature characteristic at the point is zero.

この比rと重量wの関係から、重量wは高次の近似
式、例えば下記のような二次式を演算すれば得られるこ
とがわかる。
From the relationship between the ratio r and the weight w, it can be seen that the weight w can be obtained by calculating a high-order approximation formula, for example, the following quadratic formula.

w=ar2+br+c ……(5) ただし、a、b、c:定数 以上のようにふたつの周波数frとfpの比rを求め、か
つCrとCpをw=wz点で一致させることで、センサの温度
特性が取り除け、さらに回路の温度特性も消去できる。
w = ar 2 + br + c (5) However, a, b, c: constants As described above, the ratio r between the two frequencies f r and f p is obtained, and C r and C p are calculated at w = w z point. By making them coincident, the temperature characteristic of the sensor can be removed and the temperature characteristic of the circuit can be erased.

wzは例えば次のように選べば、検出重量範囲の全域
で、温度特性を極端に大きくすることなく重量を検出す
ることができる。
If w z is selected as follows, for example, the weight can be detected in the entire detection weight range without extremely increasing the temperature characteristic.

wz=(wpl+wmax)/2 ……(6) 第4図はかかるシステムの具体的な回路構成の一実施
例を示す。制御部17はマイコン1により形成され、切換
ゲート信号制御手段として出力E0が、内蔵カウンタ手段
の入力端子としてTCが設けられている。
w z = (w pl + w max ) / 2 (6) FIG. 4 shows an example of a concrete circuit configuration of such a system. The control unit 17 is formed by the microcomputer 1, and is provided with an output E 0 as a switching gate signal control means and a TC as an input terminal of a built-in counter means.

検出手段15はオペアンプののこぎり波発生回路と波形
整形回路の組み合わせで形成されている。スイッチング
手段16はアナログスイッチによって構成されているが、
これは他の半導体スイッチング手段でも、またリレーで
も実現できる。
The detection means 15 is formed by a combination of a sawtooth wave generation circuit of an operational amplifier and a waveform shaping circuit. The switching means 16 is composed of an analog switch,
This can be achieved with other semiconductor switching means as well as with relays.

22は電圧変換および波形整形をするレベルシフト回路
であり、必要に応じて適宜付加すればよい。
Reference numeral 22 denotes a level shift circuit that performs voltage conversion and waveform shaping, and may be added as needed.

例えば、アナログスイッチはμPC4066、オペアンプは
TL082、マイコンはMB88515で実現できるが、これに相当
する機能を有するものであれば利用できるのは言うまで
もない。
For example, analog switch is μPC4066, operational amplifier is
The TL082 and the microcomputer can be realized by MB88515, but it goes without saying that they can be used as long as they have a function equivalent to this.

第5図はかかるマイコンの制御プログラムを示すフロ
ーチャートである。
FIG. 5 is a flowchart showing a control program of the microcomputer.

重量の測定がスタートされると、まずゲート信号E0
Hレベルに転じられる(a)。そして若干のディレイ時
間が適宜挿入された(b)後、TC端子に接続される内蔵
カウンタが起動され(c)、基準周波数frの測定が開始
される。
When the weight measurement is started, the gate signal E 0 is first changed to the H level (a). And after a slight delay time is appropriately inserted (b), built-in counter which is connected to the TC terminal is started (c), the measurement of the reference frequency f r is started.

そしてカウンタのゲート時間、例えば1秒、がタイマ
割り込みなどを用いて管理され(d)、この所定時間が
経過すると、カウンタが停止される(e)。かかる計数
結果frはRAMの所定アドレスに転送され、記憶される
(f)。
Then, the gate time of the counter, for example, 1 second, is managed using a timer interrupt or the like (d), and when this predetermined time has elapsed, the counter is stopped (e). The counting result fr is transferred to a predetermined address of the RAM and stored (f).

次いでゲート信号E0がLレベルの転じられ(g)、以
下frとまったく同様の手順でfpの測定が行われる(h)
〜(l)。
Then the gate signal E 0 is turned the L level (g), the measurement of the f p is carried out in exactly the same procedure as below f r (h)
~ (L).

かかる処理を経て、RAMに記憶されたfrとfpは次に除
算処理をされてrがまず算出され(m)、ついで比rを
もとに重量wが二次近似式で算出される(n)。
After such processing, f r and f p stored in the RAM are then subjected to division processing to calculate r first (m), and then the weight w is calculated by the quadratic approximation formula based on the ratio r. (N).

以上の手順により求められた重量wは、既述したよう
にセンサの温度特性を相殺できる。
The weight w obtained by the above procedure can cancel the temperature characteristic of the sensor as described above.

発明の効果 以上のように本発明の重量検出装置は、従来のように
Cp>Crの状態で使用する、という制約がなく、回路の温
度特性がゼロになるCp=Crなる点を有効に利用でき、ゼ
ロ負荷と最大秤量の間の被測定物を載置した時にこれら
を一致させることで、検出重量範囲全般に渡って温度特
性を最小に抑えることができた。
As described above, the weight detecting device of the present invention is
There is no restriction that it is used in the condition of C p > C r, and the point where C p = C r at which the temperature characteristic of the circuit becomes zero can be effectively used, and the measured object between zero load and maximum weighing can be mounted. By matching them when placed, the temperature characteristics could be minimized over the entire detection weight range.

また比rには、従来のように電源電圧VCC項がないの
で、電源の温度特性の影響も受けない。さらに検出容量
Cpと基準容量Crの検出に用いられる抵抗Rおよび発振回
路15は、まったく同じものであるから、従来のように温
度特性の揃ったものをペアにする手間もない。
Further, since the ratio r does not have the power supply voltage V CC term as in the conventional case, it is not affected by the temperature characteristic of the power supply. Further detection capacity
Since the resistance R and the oscillation circuit 15 used to detect C p and the reference capacitance C r are exactly the same, there is no need to pair those having the same temperature characteristics as in the conventional case.

さらに発振回路の出力周波数は、そのままカウンタに
入力でき、従来のようにローパスフィルタで直流電圧に
変換する必要がなく、ために回路構成が簡素かつ低廉で
すむ。
Furthermore, the output frequency of the oscillator circuit can be input to the counter as it is, and it is not necessary to convert it to DC voltage with a low-pass filter as in the past, so the circuit configuration is simple and inexpensive.

【図面の簡単な説明】[Brief description of drawings]

第1図は本発明に係わる重量と各周波数およびその比を
示す線図、第2図は本発明に係わる重量検出装置の構成
の一実施例を示す断面図、第3図は同ブロック図、第4
図は本発明の一具体例を示す回路図、第5図は制御プロ
グラムの構造を示すフローチャート、第6図(a)は静
電容量型センサの断面図、第6図(b)は同展開図、第
7図は従来例の回路図、第8図は検出回路として発振回
路を利用したときの回路の動作周波数による温度特性図
である。 4……検出電極、5……基準電極、11……載置台、15…
…検出手段、16……スイッチング手段、17……制御部、
19……カウンタ手段、21……演算手段。
FIG. 1 is a diagram showing the weight and each frequency and its ratio according to the present invention, FIG. 2 is a sectional view showing an embodiment of the configuration of the weight detecting device according to the present invention, and FIG. 3 is a block diagram thereof. Fourth
FIG. 6 is a circuit diagram showing a specific example of the present invention, FIG. 5 is a flow chart showing the structure of a control program, FIG. 6 (a) is a sectional view of a capacitance type sensor, and FIG. 6 (b) is the same development. FIG. 7 is a circuit diagram of a conventional example, and FIG. 8 is a temperature characteristic diagram according to the operating frequency of the circuit when an oscillation circuit is used as the detection circuit. 4 ... Detection electrode, 5 ... Reference electrode, 11 ... Mounting table, 15 ...
… Detecting means, 16 …… Switching means, 17 …… Control section,
19 ... Counter means, 21 ... Calculation means.

───────────────────────────────────────────────────── フロントページの続き (72)発明者 黄地 謙三 大阪府門真市大字門真1006番地 松下電器 産業株式会社内 (56)参考文献 特開 昭58−198739(JP,A) 特開 昭61−40517(JP,A) ─────────────────────────────────────────────────── ─── Continuation of the front page (72) Inventor Kenzo Ochi 1006 Kadoma, Kadoma City, Osaka Prefecture Matsushita Electric Industrial Co., Ltd. (56) Reference JP-A-58-198739 (JP, A) JP-A-61- 40517 (JP, A)

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】被測定物を載置する載置台と、所定の間隙
を設けて対向し、中央部に検出電極を、その外周部に基
準電極を有する一対の平板より形成した静電容量型圧力
センサと、前記検出電極および基準電極の容量を読み出
す検出手段と、前記検出手段を介して前記検出電極およ
び基準電極の容量を切り換えて測定する制御部とより成
り、前記静電容量型圧力センサは前記載置台と機械的に
係合され、前記載置台上に載置される被測定物の重量に
より前記検出電極の容量値が変化するよう構成し、前記
載置台上に最大秤量の略二分の一の被測定物を載置した
際に、前記検出電極と前記基準電極の容量がほぼ一致す
るように電極形状を設定するとともに、前記制御部は演
算手段を有し、検出された前記検出電極および前記基準
電極の容量値を前記演算手段を用いて比を求め、その比
に基づいて前記載置台上に載置された被測定物の重量を
算出するよう構成した重量検出装置。
1. A capacitance type which is formed of a pair of flat plates facing a mounting table on which an object to be measured is placed with a predetermined gap, a detection electrode in the center, and a reference electrode in the outer periphery. The electrostatic capacitance type pressure sensor comprises a pressure sensor, a detection unit for reading out the capacitances of the detection electrode and the reference electrode, and a control unit for switching and measuring the capacitances of the detection electrode and the reference electrode via the detection unit. Is mechanically engaged with the mounting table, and is configured so that the capacitance value of the detection electrode changes depending on the weight of the object to be measured mounted on the mounting table, and approximately half of the maximum weighing amount on the mounting table. When one object to be measured is placed, the electrode shape is set so that the capacities of the detection electrode and the reference electrode are substantially equal to each other, and the control unit has a calculation means, and the detected detection The capacitance value of the electrode and the reference electrode Determine the specific by using an arithmetic unit, the weight detection apparatus configured to calculate the weight of the object that is placed on the mounting table on the basis of the ratio.
JP63220959A 1988-09-02 1988-09-02 Weight detector Expired - Lifetime JPH0810155B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP63220959A JPH0810155B2 (en) 1988-09-02 1988-09-02 Weight detector

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP63220959A JPH0810155B2 (en) 1988-09-02 1988-09-02 Weight detector

Publications (2)

Publication Number Publication Date
JPH0267925A JPH0267925A (en) 1990-03-07
JPH0810155B2 true JPH0810155B2 (en) 1996-01-31

Family

ID=16759237

Family Applications (1)

Application Number Title Priority Date Filing Date
JP63220959A Expired - Lifetime JPH0810155B2 (en) 1988-09-02 1988-09-02 Weight detector

Country Status (1)

Country Link
JP (1) JPH0810155B2 (en)

Family Cites Families (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS58198739A (en) * 1982-05-14 1983-11-18 Matsushita Electric Ind Co Ltd Electrostatic capacity type pressure sensor
JPS59198739A (en) * 1983-04-26 1984-11-10 Nec Corp Chipcarrier
JPS6140517A (en) * 1984-08-01 1986-02-26 Tanita Seisakusho:Kk Electrostatic capacity type digital electronic balance

Also Published As

Publication number Publication date
JPH0267925A (en) 1990-03-07

Similar Documents

Publication Publication Date Title
JP3139305B2 (en) Capacitive acceleration sensor
JP3579908B2 (en) Capacitive proximity sensor
JP3233791B2 (en) Differential capacitance inverting integrator and capacitance change amount detecting device using the same
JPH06242159A (en) Electrostatic capacity measuring device
JPS6375919A (en) Coordinate input device
EP0104243A1 (en) Capacitance manometer with digital output
JPH0810155B2 (en) Weight detector
JPH0810156B2 (en) Weight detector
JP3044938B2 (en) Capacitive displacement sensor
JPH0943078A (en) Capacitance detection circuit of capacitance-type sensor
JPH0823514B2 (en) Pressure detector
JPS5840125B2 (en) Seidenyouriyou - Chiyokuryuden Atsuhen Kansouchi
JP2606376B2 (en) Weight detector
JP3119386B2 (en) measuring device
JP2729321B2 (en) Capacitance type measuring instrument
JP2729322B2 (en) Capacitance type measuring instrument
JP2705128B2 (en) Electronic thermo-hygrometer and electronic hygrometer
JPH0518990A (en) Capacitance type dynamic quantity detector
SU735927A1 (en) Level meter
SU1767451A1 (en) Metering transducer with capacity sensor
JPS61292731A (en) Coordinate detector
JPH09257620A (en) Device for measuring displacement
JPS60203864A (en) Detector
SU851285A1 (en) Device for measuring material dielectric parameters
SU1149447A1 (en) Device for measuring significant values of harmonics of arc current of three-phase electric-arc furnace

Legal Events

Date Code Title Description
FPAY Renewal fee payment (event date is renewal date of database)

Free format text: PAYMENT UNTIL: 20080131

Year of fee payment: 12

FPAY Renewal fee payment (event date is renewal date of database)

Free format text: PAYMENT UNTIL: 20090131

Year of fee payment: 13

EXPY Cancellation because of completion of term
FPAY Renewal fee payment (event date is renewal date of database)

Free format text: PAYMENT UNTIL: 20090131

Year of fee payment: 13