JPH0454890B2 - - Google Patents
Info
- Publication number
- JPH0454890B2 JPH0454890B2 JP58090789A JP9078983A JPH0454890B2 JP H0454890 B2 JPH0454890 B2 JP H0454890B2 JP 58090789 A JP58090789 A JP 58090789A JP 9078983 A JP9078983 A JP 9078983A JP H0454890 B2 JPH0454890 B2 JP H0454890B2
- Authority
- JP
- Japan
- Prior art keywords
- output
- electrodes
- amplifier
- fluid
- flowing
- 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
Links
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01F—MEASURING VOLUME, VOLUME FLOW, MASS FLOW OR LIQUID LEVEL; METERING BY VOLUME
- G01F1/00—Measuring the volume flow or mass flow of fluid or fluent solid material wherein the fluid passes through a meter in a continuous flow
- G01F1/56—Measuring the volume flow or mass flow of fluid or fluent solid material wherein the fluid passes through a meter in a continuous flow by using electric or magnetic effects
- G01F1/58—Measuring the volume flow or mass flow of fluid or fluent solid material wherein the fluid passes through a meter in a continuous flow by using electric or magnetic effects by electromagnetic flowmeters
- G01F1/60—Circuits therefor
Landscapes
- Physics & Mathematics (AREA)
- Electromagnetism (AREA)
- Fluid Mechanics (AREA)
- General Physics & Mathematics (AREA)
- Measuring Volume Flow (AREA)
Description
【発明の詳細な説明】
〔発明の技術分野〕
本発明は、例えば各種化学プロセスにおいてパ
イプを通じて供給される水その他導電性を有する
各種原料流体の流量を測定する場合などに用いら
れる電磁流量計に関するのである。DETAILED DESCRIPTION OF THE INVENTION [Technical Field of the Invention] The present invention relates to an electromagnetic flowmeter used, for example, to measure the flow rate of water and other conductive raw material fluids supplied through pipes in various chemical processes. It is.
電磁流量計はフアラデーの法則を基本原理とし
て利用するもので、通常流量を測定する流れに直
交して交流磁界を発生させ、流れとこの磁界とに
直交して配置した対向電極間に生ずる電位差を増
幅して取り出している。流体の電気伝導率は一般
に余り大きいものではなく、従来、5μS/cm程度
の電気伝導度(1cm当たり200KΩ程度の抵抗)
の流体に対しても測定できるように、増幅器は高
入力インピーダンス(例えば300MΩ)、高利得の
ものが用いられる。このため、電極間を電流が全
く流れていない場合でも、例えば測定場所近くに
配電盤が設置されており、大電流を断続している
ような場合、そこから発生する電磁波によつて電
極間にノイズが生じ、信号として検出されること
がある。このような信号自体はわずかでも、通常
流量の積算も併せて行なわれることが普通である
ため、その場合わずかな信号でも積算すると大き
な値となつて表われ、プロセス制御上問題とな
る。
An electromagnetic flowmeter uses Faraday's law as its basic principle, and normally generates an alternating magnetic field perpendicular to the flow whose flow rate is to be measured, and calculates the potential difference generated between opposing electrodes placed perpendicular to the flow and this magnetic field. It is amplified and extracted. The electrical conductivity of fluids is generally not very high, and conventionally the electrical conductivity is about 5μS/cm (resistance of about 200KΩ per cm).
An amplifier with high input impedance (for example, 300 MΩ) and high gain is used so that measurements can be performed even on fluids such as Therefore, even if no current is flowing between the electrodes, for example, if a power distribution board is installed near the measurement location and is passing a large current intermittently, the electromagnetic waves generated from it may cause noise between the electrodes. may occur and be detected as a signal. Although such a signal itself is small, it is common that the normal flow rate is also integrated, so even if the signal is small, when integrated, it appears as a large value, which poses a problem in process control.
本発明はこのような事情に鑑みなされたもの
で、その目的は、流体が流れていない場合には常
に出力を零として電極間のノイズにかかわらず積
算カウンタのカウントアツプも行なわないように
することが可能な電磁流量計を提供することにあ
る。
The present invention was developed in view of these circumstances, and its purpose is to always set the output to zero when no fluid is flowing, so that the integration counter does not count up regardless of noise between the electrodes. Our goal is to provide an electromagnetic flowmeter that is capable of
このような目的を達成するために、本発明は、
増幅器の前段に高インピーダンス素子を介して電
源を接続し、流体がなくなつて電極間が高インピ
ーダンスとなつてときに流れているときとは明確
に区別できる出力が増幅器に得られるようにする
とともに、上記出力が得られたことを判定する手
段と、その判定出力が得られたときに電磁流量計
としての出力を強制的に零にする手段とを設けた
ものである。以下、実施例を用いて本発明を詳細
に説明する。 In order to achieve such an objective, the present invention
A power supply is connected to the front stage of the amplifier via a high impedance element, so that the amplifier can obtain an output that can be clearly distinguished from when there is no fluid and the gap between the electrodes becomes high impedance. , means for determining whether the above output has been obtained, and means for forcibly reducing the output of the electromagnetic flowmeter to zero when the determined output is obtained. Hereinafter, the present invention will be explained in detail using Examples.
第1図は本発明の一実施例を示す回路図であ
る。図において、1は流体の流れる管路であり、
励磁コイル2により内部に流体の流通方向と直交
する磁界が形成されるとともに、当該磁界と直交
して相互に絶縁された対向電極3および4が設け
てあり、流速に応じて生ずる起電力が電極3,4
間に印加されるように構成してある。これら管路
1、励磁コイル2および電極3,4により検出器
5が構成される。6は定電流源、7は励磁回路で
あり、タイミング信号発生回路8から送出される
信号aによつて定電流源6を励磁コイル2に反転
接続し、励磁コイル2に矩形波の交番電流を供給
する。
FIG. 1 is a circuit diagram showing an embodiment of the present invention. In the figure, 1 is a pipe through which fluid flows;
A magnetic field perpendicular to the flow direction of the fluid is formed internally by the excitation coil 2, and opposing electrodes 3 and 4 are provided which are orthogonal to the magnetic field and are insulated from each other. 3,4
The configuration is such that the voltage is applied between the two. A detector 5 is constituted by the conduit 1, the excitation coil 2, and the electrodes 3 and 4. 6 is a constant current source, and 7 is an excitation circuit. The constant current source 6 is invertedly connected to the excitation coil 2 by the signal a sent from the timing signal generation circuit 8, and a square wave alternating current is applied to the excitation coil 2. supply
電極2および3は、それぞれ演算増幅器9およ
び10の非反転入力端子に接続してある。演算増
幅器9,10はいずれもその出力端子と反転入力
端子とを直接接続していわゆるボルテツジ・ホロ
ワを構成し、これら両演算増幅器9および10の
出力は抵抗器R1およびR2を介して演算増幅器1
1の反転入力端子および非反転入力端子に接続さ
れている。したがつて、通常管路1に流体が流れ
ている状態では、励磁コイル2に第2図aに示す
ような正・負の矩形波の励磁電流CLが流れ正
(+)・負(−)の励磁が交互に行なわれた場合、
演算増幅器9には同様の波形の出力が得られる。
一方、演算増幅器10は、インピーダンス変換が
目的で、その結果、演算増幅器11にも、同図b
に示すように同様の矩形波状の出力V1が得られ
る。この場合、演算増幅器11の出力電圧V1は、
演算増幅器9の出力をV2、演算増幅器10の出
力をV3とし、抵抗器R1,R2の抵抗値をそれぞれ
r1,r2、演算増幅器11の非反転入力端子と接地
端子間に接続した抵抗器R3の抵抗値r3、演算増幅
器11の反転入力端子と出力端子間に接続した抵
抗器R4の抵抗値をr4として、
V1=r1+r4/r2+r3・r3/r1・V3−r4/r1×V2
仮にr1=r2,r3=r4とすれば、
V=r4/r1(V3−V2) ……(1)
で表わされる。 Electrodes 2 and 3 are connected to non-inverting input terminals of operational amplifiers 9 and 10, respectively. Both operational amplifiers 9 and 10 have their output terminals directly connected to their inverting input terminals to form a so-called voltage follower, and the outputs of both operational amplifiers 9 and 10 are connected via resistors R1 and R2 . amplifier 1
It is connected to the inverting input terminal and the non-inverting input terminal of No. 1. Therefore, when fluid is normally flowing in the pipe line 1, an excitation current CL of positive and negative rectangular waves as shown in FIG. If the excitation of is performed alternately,
An output with a similar waveform is obtained from the operational amplifier 9.
On the other hand, the purpose of the operational amplifier 10 is impedance conversion, and as a result, the operational amplifier 11 is also
A similar rectangular waveform output V 1 is obtained as shown in . In this case, the output voltage V 1 of the operational amplifier 11 is
The output of operational amplifier 9 is V 2 , the output of operational amplifier 10 is V 3 , and the resistance values of resistors R 1 and R 2 are respectively
r 1 , r 2 , the resistance value r 3 of the resistor R 3 connected between the non-inverting input terminal of the operational amplifier 11 and the ground terminal, and the resistance value of the resistor R 4 connected between the inverting input terminal and the output terminal of the operational amplifier 11 Assuming the resistance value is r 4 , V 1 = r 1 + r 4 / r 2 + r 3・r 3 / r 1・V 3 − r 4 / r 1 ×V 2. If r 1 = r 2 , r 3 = r 4 . Then, it is expressed as V=r 4 /r 1 (V 3 −V 2 ) (1).
サンプルホールド回路12は、演算増幅器11
の出力端子に接続され、タイミング信号発生回路
8から送出される第2図cに示すような一定周期
のサンプリング信号bに従つて、演算増幅器11
の出力電圧が定常値になつた時点で当該出力電圧
をサンプリングして保持し、その出力として、励
磁コイル2の励磁電流に比例し、かつ管路1を流
れる流体の流速に比例した信号が得られる。した
がつてこの信号を直流増幅器13によりさらに増
幅して流量出力OUTが得られる。この流量出力
OUTは、例えば電圧電流増幅器により4〜
20mAの電流に変換して計節計の入力信号とし、
流量の制御が行なわれる。 The sample hold circuit 12 includes an operational amplifier 11
The operational amplifier 11
When the output voltage reaches a steady value, the output voltage is sampled and held, and a signal proportional to the excitation current of the excitation coil 2 and proportional to the flow rate of the fluid flowing through the pipe line 1 is obtained as the output. It will be done. Therefore, this signal is further amplified by the DC amplifier 13 to obtain the flow rate output OUT. This flow rate output
OUT is set to 4 to 4 by a voltage current amplifier, for example.
Convert it to a 20mA current and use it as the input signal for the meter.
The flow rate is controlled.
上記構成において、管路1の内部を流れる流体
がほとんどなくなつて空の状態となつた場合、対
向電極3,4間はほとんど開放状態となるが、こ
のように電極間が高インピーダンスの状態となつ
たとき、従来の構成では初段演算増幅器9,10
の特性如何によつて出力がどちらに行くかは不明
であり、その場合、前述したように流体が流れて
ないにもかかわわらず、検出器に生ずるノイズを
拾つて積算カウンタがカウントアツプするなどの
問題を生ずる。 In the above configuration, when there is almost no fluid flowing inside the pipe line 1 and the pipe line 1 becomes empty, the space between the opposing electrodes 3 and 4 becomes almost open, but the space between the electrodes is in a high impedance state. In the conventional configuration, the first stage operational amplifiers 9 and 10
It is unknown which direction the output will go depending on the characteristics of the detector, and in that case, as mentioned above, even though no fluid is flowing, the noise generated in the detector will be picked up and the integration counter will count up. This will cause problems.
そこで、本実施例では演算増幅器9の非反転入
力端子に抵抗器R5を介して電圧+Vを発生する
電源を接続するとともに、演算増幅器10の非反
転入力端子に抵抗器R6を介して電圧−Vを発生
する電源を接続してある。抵抗器R5およびR6の
抵抗値r5,r6は、いずれも、通常管路1を流体が
流れている状態で、電極3,4間の抵抗値が多く
の流体の場合100KΩ以内であるのに対して精度
上、十分に無視できるようにたとえば100MΩ程
度の十分に高い値とする。これにより、流体が流
れなくなつて電極3,4間が開放状態となつたと
き、演算増幅器9の出力には上記電源電圧+Vが
ほとんどそのまま生じ、演算増幅器10の出力に
は−Vがほとんどそのまま表われる。したがつ
て、抵抗器R1〜R4の抵抗値などの回路定数を適
当に選択すれば、例えば(1)式においてr1=2r4と
すれば、上述したように電極3,4間が開放状態
となつたときに演算増幅器11の出力はほぼ−V
へ振れ、第2図bに示すように通常流体の流れて
いる場合の出力に対して明確に区別することがで
きる。 Therefore, in this embodiment, a power supply that generates a voltage +V is connected to the non-inverting input terminal of the operational amplifier 9 through the resistor R5 , and a voltage is connected to the non-inverting input terminal of the operational amplifier 10 through the resistor R6 . A power supply that generates -V is connected. The resistance values r 5 and r 6 of the resistors R 5 and R 6 are both within 100KΩ when the fluid is flowing through the pipe 1 and the resistance value between the electrodes 3 and 4 is often within 100KΩ. However, in terms of accuracy, it is set to a sufficiently high value, for example, about 100 MΩ, so that it can be ignored. As a result, when the fluid stops flowing and the electrodes 3 and 4 are in an open state, the above power supply voltage +V is generated almost unchanged at the output of the operational amplifier 9, and -V is generated almost unchanged at the output of the operational amplifier 10. appear. Therefore, if the circuit constants such as the resistance values of the resistors R 1 to R 4 are appropriately selected, for example, if r 1 = 2r 4 in equation (1), the distance between electrodes 3 and 4 will be reduced as described above. When it is in the open state, the output of the operational amplifier 11 is approximately -V
It can be clearly distinguished from the output when the fluid is flowing normally, as shown in FIG. 2b.
本実施例ではさらに、演算増幅器11の出力を
入力とし、これを基準電圧V0と比較する、演算
増幅器からなる比較器14と、この比較器14の
出力を受けて動作するスイツチ回路15とを備え
ている。 The present embodiment further includes a comparator 14 formed of an operational amplifier that receives the output of the operational amplifier 11 and compares it with a reference voltage V 0 , and a switch circuit 15 that operates in response to the output of the comparator 14. We are prepared.
ここで、比較器14の基準電圧V0は、−Vより
もわずかに高い電圧に設定してあり、演算増幅器
11の出力V3が−Vへ振れた場合比較器14の
出力V4は第2図dに示すように正側へ振れる。
スイツチ回路15は、演算増幅器11の出力端子
とサンプルホールド回路12との間に接続された
ノーマリオフ形のアナログスイツチSW1およびサ
ンプルホールド回路12と接地端子間に接続され
たノーマリオフ形のアナログスイツチSW2からな
り、比較器14の出力はアナログスイツチSW1の
制御信号として送出されるとともに、インバータ
16により反転されてアナログスイツチSW2の制
御信号として送出される。したがつて、上述した
ように比較器14から流体が流れなくなつたこと
を示す正の判定出力が送出された場合、スイツチ
SW1が開放するとともにスイツチSW2が閉成し、
その結果サンプルオールド回路12の入力は検出
器5による検出出力にかかわらず零電位となる。 Here, the reference voltage V 0 of the comparator 14 is set to a voltage slightly higher than -V, and when the output V 3 of the operational amplifier 11 swings to -V, the output V 4 of the comparator 14 is set to the voltage slightly higher than -V. It swings to the positive side as shown in Figure 2 d.
The switch circuit 15 includes a normally-off analog switch SW 1 connected between the output terminal of the operational amplifier 11 and the sample-hold circuit 12, and a normally-off analog switch SW 2 connected between the sample-hold circuit 12 and the ground terminal . The output of the comparator 14 is sent out as a control signal for the analog switch SW1 , and is also inverted by the inverter 16 and sent out as a control signal for the analog switch SW2 . Therefore, as described above, if the comparator 14 sends out a positive judgment output indicating that fluid has stopped flowing, the switch
SW 1 opens and switch SW 2 closes,
As a result, the input of the sample old circuit 12 becomes zero potential regardless of the detection output from the detector 5.
以上、演算増幅器9および10の前段にそれぞ
れ抵抗器R5およびR6を介して+V、−Vの電源を
接続し、流体が流れなくなつたときに演算増幅器
11の出力V3はほぼ−Vとなるようにした場合
を例に説明したが、本発明はこれに限定されるも
のではなく、演算増幅器9の前段、あるいは演算
増幅器10の前段のいずれか一方にのみ高インピ
ーダンス素子を接続してもよく、また、流体が流
れなくなつた場合に、通常流体が流れている場合
に対して明確に区別できるような出力が演算増幅
器11に得られればよい。 As described above, +V and -V power supplies are connected to the front stages of operational amplifiers 9 and 10 through resistors R5 and R6 , respectively, and when fluid stops flowing, the output V3 of operational amplifier 11 is approximately -V. Although the present invention is not limited to this example, it is possible to connect a high impedance element only to either the front stage of the operational amplifier 9 or the front stage of the operational amplifier 10. Furthermore, it is only necessary that the operational amplifier 11 obtains an output that can clearly distinguish when the fluid stops flowing from when the fluid normally flows.
なお、上述した実施例では演算増幅器11の出
力が流体がなくなつて電極間が高インピーダンス
となつたときの出力にほぼ等しくなつたことを判
定する手段として、上記流体がなくなつて電極間
が高インピーダンスとなつたときの出力にほぼ等
しい基準電圧を設定した演算増幅器からなる比較
器14を用いたが、本発明はこれに限定されるも
のではない。例えば近年プロセス制御においては
コンピユータが用いられることが多いが、上記判
定はこのコンピユータを利用してソフト的に行な
つてもよいことはいうまでもない。また、スイツ
チ回路15に限らず、上記判定出力が得られた場
合、流量出力OUTを強制的に零とする手段であ
れば、どのような構成のものを用いてもよいこと
はもちろんである。 In the above-described embodiment, as a means for determining that the output of the operational amplifier 11 has become approximately equal to the output when the fluid has disappeared and the gap between the electrodes has become high impedance, Although the comparator 14 is made of an operational amplifier and has a reference voltage set to be approximately equal to the output when the impedance becomes high, the present invention is not limited thereto. For example, in recent years, computers have often been used in process control, and it goes without saying that the above-mentioned determination may be performed using software using this computer. Moreover, it is needless to say that the switch circuit 15 is not limited to the switch circuit 15, and any structure may be used as long as it is a means for forcibly reducing the flow rate output OUT to zero when the above judgment output is obtained.
以上説明したように、本発明によれば増幅器の
前段に高インピーダンス素子を介して電源を接続
し、流体がなくなつて電極間が高インピーダンス
となつたときに流れているときとは明確に区別で
きる出力が増幅器に得られるようにするととも
に、当該出力が得られたことを判定する手段と、
その判定出力が得られたときに電磁流量計の出力
を強制的に零にする手段とを設けたことにより、
流体がないときには電極間のノイズの有無にかか
わらず常に出力は零となり、積算カウンタのカウ
ントアツプも行なわれず、正確な測定が行なえ、
プロセス制御上もきわめて有用である。
As explained above, according to the present invention, a power supply is connected to the front stage of the amplifier via a high impedance element, and when the fluid is gone and the impedance between the electrodes becomes high, it is clearly distinguished from when the fluid is flowing. means for causing the amplifier to obtain an output that can be obtained, and for determining that the output has been obtained;
By providing a means for forcibly reducing the output of the electromagnetic flowmeter to zero when the judgment output is obtained,
When there is no fluid, the output is always zero regardless of the presence or absence of noise between the electrodes, and the integration counter does not count up, allowing accurate measurements.
It is also extremely useful for process control.
第1図は本発明の一実施例と示す回路図、第2
図はその動作を説明するためのタイミングチヤー
トである。
1…流体が流れる管路、2…励磁コイル、3,
4…対向電極、9,10,11…演算増幅器、1
4…判定手段としての比較器、15…出力を零に
する手段としてのスイツチ回路、R5,R6…高抵
抗の抵抗器、+V,−V…電源電圧。
Figure 1 is a circuit diagram showing one embodiment of the present invention, Figure 2 is a circuit diagram showing an embodiment of the present invention.
The figure is a timing chart for explaining its operation. 1... Pipe line through which fluid flows, 2... Excitation coil, 3,
4... Counter electrode, 9, 10, 11... Operational amplifier, 1
4...Comparator as determination means, 15...Switch circuit as means for zeroing the output, R5 , R6 ...High resistance resistors, +V, -V...Power supply voltage.
Claims (1)
ルと、流れを挾んで上記交流磁界に直交する方向
に対向する電極と、この電極間の電位差を増幅す
る増幅器とを備えた電磁流量計において、上記増
幅器の前段に、電極間を流れる流体の抵抗よりも
十分に高いインピーダンスを有する高インピーダ
ンス素子を介して電源を接続し、この電源の電圧
を、流体がなくなつて電極間が高インピーダンス
となつたときに増幅器の出力として電極間を流体
が流れている間の出力と明確に区別できる程度の
出力が得られる値にするとともに、上記増幅器の
出力が上記電極間を流体がほとんど流れなくなつ
たときの出力にほぼ等しくなつたことを判定して
判定出力を送出する判定手段と、この判定手段か
ら判定出力が得られたときに電磁流量計としての
出力を強制的に零とする手段とを設けたことを特
徴とする電磁流量計。 2 判定手段として、電極間を流体がほとんど流
れなくなつたときの増幅器の出力にほぼ等しい基
準電圧を有し増幅器の出力を入力とする比較器を
設け、出力を強制的に零とする手段として、上記
比較器の出力によつて、出力端子と増幅器の出力
とを接続する接点を解放して出力端子と接地端子
とを接続する接点を閉成するスイツチ回路を設け
たことを特徴とする特許請求の範囲第1項記載の
電磁流量計。[Claims] 1. An excitation coil that forms an alternating current magnetic field perpendicular to the flow, electrodes facing each other in a direction perpendicular to the alternating current magnetic field across the flow, and an amplifier that amplifies the potential difference between the electrodes. In an electromagnetic flowmeter, a power source is connected to the front stage of the amplifier via a high impedance element having an impedance sufficiently higher than the resistance of the fluid flowing between the electrodes, and the voltage of this power source is applied to the voltage between the electrodes when the fluid runs out. When the impedance becomes high, the output of the amplifier is set to a value that can be clearly distinguished from the output when fluid is flowing between the electrodes, and the output of the amplifier is set to a value that can be clearly distinguished from the output when fluid is flowing between the electrodes. A determination means that determines that the output is almost equal to the output when there is almost no flow and sends out a determination output, and a determination means that forcibly makes the output of the electromagnetic flowmeter zero when the determination output is obtained from this determination means. An electromagnetic flowmeter characterized by comprising means for: 2. As a means of determination, a comparator is provided which has a reference voltage approximately equal to the output of the amplifier when almost no fluid flows between the electrodes, and whose input is the output of the amplifier, and as a means of forcing the output to zero. , a patent characterized in that a switch circuit is provided for opening a contact connecting the output terminal and the output of the amplifier and closing a contact connecting the output terminal and the ground terminal by the output of the comparator. An electromagnetic flowmeter according to claim 1.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP9078983A JPS59217114A (en) | 1983-05-25 | 1983-05-25 | Electromagnetic flowmeter |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP9078983A JPS59217114A (en) | 1983-05-25 | 1983-05-25 | Electromagnetic flowmeter |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS59217114A JPS59217114A (en) | 1984-12-07 |
| JPH0454890B2 true JPH0454890B2 (en) | 1992-09-01 |
Family
ID=14008355
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP9078983A Granted JPS59217114A (en) | 1983-05-25 | 1983-05-25 | Electromagnetic flowmeter |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS59217114A (en) |
Family Cites Families (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5742812A (en) * | 1980-08-28 | 1982-03-10 | Yokogawa Hokushin Electric Corp | Electromagnetic flowmeter with water-unfilling state detecting function |
| JPS5779714U (en) * | 1980-10-31 | 1982-05-17 |
-
1983
- 1983-05-25 JP JP9078983A patent/JPS59217114A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS59217114A (en) | 1984-12-07 |
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