JPH0820391B2 - Constant current circuit for fluid resistance measurement - Google Patents
Constant current circuit for fluid resistance measurementInfo
- Publication number
- JPH0820391B2 JPH0820391B2 JP15832092A JP15832092A JPH0820391B2 JP H0820391 B2 JPH0820391 B2 JP H0820391B2 JP 15832092 A JP15832092 A JP 15832092A JP 15832092 A JP15832092 A JP 15832092A JP H0820391 B2 JPH0820391 B2 JP H0820391B2
- Authority
- JP
- Japan
- Prior art keywords
- electrode
- fluid
- resistance
- current
- main
- 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
- G03—PHOTOGRAPHY; CINEMATOGRAPHY; ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ELECTROGRAPHY; HOLOGRAPHY
- G03G—ELECTROGRAPHY; ELECTROPHOTOGRAPHY; MAGNETOGRAPHY
- G03G15/00—Apparatus for electrographic processes using a charge pattern
- G03G15/06—Apparatus for electrographic processes using a charge pattern for developing
- G03G15/10—Apparatus for electrographic processes using a charge pattern for developing using a liquid developer
- G03G15/104—Preparing, mixing, transporting or dispensing developer
- G03G15/105—Detection or control means for the toner concentration
Landscapes
- Investigating Or Analyzing Materials By The Use Of Electric Means (AREA)
- Measurement Of Resistance Or Impedance (AREA)
Description
【0001】[0001]
【産業上の利用分野】本発明は、流体中に混入している
固体粒子の濃度や気泡の量を測定したり、流体の導電率
を測定する流体抵抗測定用定電流回路に関するものであ
る。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a constant current circuit for measuring fluid resistance, which measures the concentration of solid particles and the amount of bubbles mixed in a fluid and the conductivity of the fluid.
【0002】[0002]
【従来の技術】従来の定電流回路は、例えば「リニアI
C回路技法」(オーム社)の19頁に示されているよう
に、ただ一つの電流検出抵抗手段から得られる電圧に基
づいて電流値の制御が行われていた。2. Description of the Related Art A conventional constant current circuit is, for example, a "linear I
As shown on page 19 of "C Circuit Technique" (Ohm Co.), the current value is controlled based on the voltage obtained from only one current detecting resistor means.
【0003】[0003]
【発明が解決しようとする課題】上記のようなただ一つ
の電流検出抵抗手段から得られる電圧に基づいて電流値
を制御するような定電流回路の構成方法を、第一の電極
1と第二の電極2からなる一対の主電極aと、主電極a
間の電位分布を一様にするため、主電極aの左右に第三
の電極3と第四の電極4とからなる一対の補助電極b・
bを近接状態に付設して構成した流体抵抗測定用電極体
cを、流体内に浸漬或いは流体の流路または液槽の内壁
に設置し、主電極a間に一定電流を流して主電極a間の
電位差により主電極a間の固液混合体または気液混合体
または気固液混合体の抵抗値を測定する流体抵抗測定用
定電流回路として採用すると、主電極a間の液体または
混相流体塊を含んだ流体の抵抗値に大きな誤差を生ずる
場合がある。A method for constructing a constant current circuit in which the current value is controlled based on the voltage obtained from only one current detecting resistance means as described above is used in the first electrode 1 and the second electrode. A pair of main electrodes a composed of the electrodes 2 of
In order to make the potential distribution between the electrodes uniform, a pair of auxiliary electrodes b, which are composed of a third electrode 3 and a fourth electrode 4 on the left and right of the main electrode a.
An electrode body c for measuring fluid resistance, which is formed by attaching b to the adjacent state, is immersed in the fluid, or is installed on the flow path of the fluid or on the inner wall of the liquid tank, and a constant current is passed between the main electrodes a to make the main electrode a When adopted as a constant current circuit for measuring fluid resistance, which measures the resistance value of the solid-liquid mixture or the gas-liquid mixture or the gas-solid mixture between the main electrodes a by the potential difference between them, the liquid or the multiphase fluid between the main electrodes a A large error may occur in the resistance value of the fluid containing lumps.
【0004】即ち、主電極a間の流体または混相流体に
おいて部分的に周囲と導電率の異なる流体塊が存在する
場合、その流体塊の存在する位置により測定される抵抗
値が大幅に異なり、抵抗を測定する際の大きな誤差にな
る場合がある。このように主電極a間において導電率の
異なる流体塊の位置の違いにより、測定される抵抗値が
異なる理由を図3及び図4を用いて説明すると次のよう
になる。That is, when a fluid mass having a conductivity different from that of the surroundings partially exists in the fluid between the main electrodes a or in the multiphase fluid, the resistance value measured greatly varies depending on the position where the fluid mass exists, and the resistance is There may be a large error in measuring. The reason why the measured resistance value differs due to the difference in the positions of the fluid masses having different conductivity between the main electrodes a will be described below with reference to FIGS. 3 and 4.
【0005】図3及び図4は電極間を流れる電流の様子
を電気力線で表したものである。3 and 4 show the state of the current flowing between the electrodes by lines of electric force.
【0006】補助電極bの第三の電極3には主電極aの
第一の電極1と同じ電圧が供給され、補助電極bの第四
の電極4には主電極aの第二の電極2と同じ電圧が供給
される。The third electrode 3 of the auxiliary electrode b is supplied with the same voltage as that of the first electrode 1 of the main electrode a, and the fourth electrode 4 of the auxiliary electrode b is supplied with the second electrode 2 of the main electrode a. Is supplied with the same voltage as.
【0007】電流検出抵抗手段7を、たとえば主電極a
の第二の電極2の側に設定したとする。The current detecting resistor means 7 is connected to, for example, the main electrode a.
It is assumed that the second electrode 2 is set on the side of the second electrode 2.
【0008】図3に示すようにいま仮に、周囲の流体よ
り導電率の小さい流体塊が第一の電極1の表面の近くに
あるとする。この流体塊に妨げられるため第一の電極1
を通る電流は第二の電極を通る電流より小さい。As shown in FIG. 3, it is assumed that a fluid mass having a conductivity lower than that of the surrounding fluid is near the surface of the first electrode 1. The first electrode 1 because it is hindered by this fluid mass
The current passing through is less than the current passing through the second electrode.
【0009】逆に周囲の流体より導電率の小さい上記流
体塊が第二の電極の表面の近くにあるとすると、この流
体塊に妨げられるため、図4に示すように第二の電極2
を通る電流は第一の電極1を通る電流より小さい。しか
しいずれの場合も、電流検出抵抗手段7を通る電流が一
定値になるように制御が行われるので、周囲の流体より
導電率の小さい流体塊が第一の電極1の表面の近くにあ
る時には、主電極a間に印加される電圧が低いために抵
抗値はより小さく測定され、逆にそのような流体塊が第
二の電極2の表面の近くにある時は、主電極a間に印加
される電圧が高いために抵抗値はより大きな値として測
定される。On the contrary, if the fluid mass whose conductivity is smaller than that of the surrounding fluid is near the surface of the second electrode, the fluid mass hinders the fluid mass. Therefore, as shown in FIG.
The current passing through is smaller than the current passing through the first electrode 1. However, in both cases, control is performed so that the current passing through the current detection resistance means 7 becomes a constant value, so when a fluid mass having a conductivity lower than that of the surrounding fluid is near the surface of the first electrode 1. , The resistance value is measured smaller due to the lower voltage applied between the main electrodes a, and conversely when such a fluid mass is near the surface of the second electrode 2, it is applied between the main electrodes a. Due to the high voltage applied, the resistance value is measured as a larger value.
【0010】発明者は主電極a間の流体中に部分的に周
囲と導電率の異なる流体塊が存在する場合、その流体塊
の存在する位置の違いにはほとんど影響されことなく主
電極a間の抵抗値を測定できる方法を考案した。The inventor has found that when a fluid mass having a conductivity different from that of the surroundings partially exists in the fluid between the main electrodes a, there is almost no effect on the difference in the position where the fluid mass exists between the main electrodes a. I devised a method that can measure the resistance value of.
【0011】[0011]
【課題を解決するための手段】添付図面を参照して本発
明の要旨を説明する。The gist of the present invention will be described with reference to the accompanying drawings.
【0012】第一の電極1と第二の電極2からなる一対
の主電極aと、この主電極aの左右に第三の電極3と第
四の電極4からなる一対の補助電極b・bを近接状態に
付設して構成した流体抵抗測定用電極体cを、流体中に
浸漬或いは流体の流路または液槽の内壁に設置し、主電
極a間に一定電流を流して主電極a間の電位差により主
電極間の流体または固液混合体または気液混合体または
気固液混合体の抵抗値を測定する流体抵抗測定用定電流
回路であって、主電極aの第一の電極1側と第二の電極
2側の夫々に電流検出抵抗手段7を設け、それぞれの電
流検出抵抗手段7から得られる二つの電圧を平均して得
た電圧に基づき電流値を制御することを特徴とする流体
抵抗測定用定電流回路に係るものである。A pair of main electrodes a consisting of the first electrode 1 and the second electrode 2, and a pair of auxiliary electrodes b and b consisting of a third electrode 3 and a fourth electrode 4 on the left and right of the main electrode a. A fluid resistance measuring electrode body c configured by being attached in close proximity is installed in the fluid or in the flow path of the fluid or on the inner wall of the liquid tank, and a constant current is applied between the main electrodes a to provide a space between the main electrodes a. A constant current circuit for measuring fluid resistance for measuring a resistance value of a fluid or solid-liquid mixture or a gas-liquid mixture or a gas-solid mixture between the main electrodes by the potential difference of the first electrode 1 of the main electrode a. Side and the second electrode 2 side are respectively provided with current detection resistance means 7, and the current value is controlled based on the voltage obtained by averaging two voltages obtained from the respective current detection resistance means 7. The present invention relates to a constant current circuit for measuring fluid resistance.
【0013】[0013]
【作用】主電極a間にあって周囲の流体と導電率の異な
る流体塊が第一の電極1と第二の電極2との丁度中間位
置にある場合は、第一の電極1を通過する電流と第二の
電極2を通過する電流の大きさは等しく主電極a間の抵
抗値は正しく測定される。When a fluid mass having a conductivity different from that of the surrounding fluid between the main electrodes a is located at an intermediate position between the first electrode 1 and the second electrode 2, a current passing through the first electrode 1 The magnitude of the current passing through the second electrode 2 is equal, and the resistance value between the main electrodes a is correctly measured.
【0014】いま仮に周囲の流体より導電率の小さい流
体塊が第一の電極1の表面の近くにあるとする。この時
には、中央にある時に比べて第一の電極1を通過する電
流は小さく第二の電極2を通過する電流は大きい。しか
し第一の電極1を通過する電流値と、第二の電極2を通
過する電流値とを平均した値は、中央にある時に比べて
あまり大きな違いはない。It is assumed that a fluid mass having a conductivity lower than that of the surrounding fluid is near the surface of the first electrode 1. At this time, the current passing through the first electrode 1 is smaller and the current passing through the second electrode 2 is larger than that at the center. However, the average value of the current value passing through the first electrode 1 and the current value passing through the second electrode 2 is not so different from that at the center.
【0015】逆にそのような周囲の流体より導電率の小
さい流体塊が第二の電極2の表面の近くにあるとする
と、その時は中央にある時に比べて、第一の電極1を通
過する電流は大きく第二の電極2を通過する電流は小さ
い。On the contrary, if a fluid mass having a conductivity lower than that of the surrounding fluid is near the surface of the second electrode 2, then it passes through the first electrode 1 at that time as compared to when it is at the center. The current is large and the current passing through the second electrode 2 is small.
【0016】しかし、第一の電極1を通過する電流値と
第二の電極2を通過する電流値とを平均した値は、中央
にある時に比べてあまり大きな違いはない。However, the average value of the current value passing through the first electrode 1 and the current value passing through the second electrode 2 is not so different from that at the center.
【0017】このように主電極aを構成する一対の電極
1,2の両方の側にそれぞれ電流検出抵抗手段7を設置
して、それぞれの電流検出抵抗手段7から得られる二つ
の電圧の平均値をもとに電流値の制御を行うことによ
り、主電極a間に周囲の流体と導電率の異なる流体塊が
存在する場合であっても、その位置の違いにほとんど影
響されることなく主電極a間の抵抗値が測定できる。As described above, the current detecting resistor means 7 is installed on both sides of the pair of electrodes 1 and 2 constituting the main electrode a, and the average value of the two voltages obtained from the respective current detecting resistor means 7 is set. By controlling the current value based on the above, even if there is a fluid mass having a conductivity different from that of the surrounding fluid between the main electrodes a, the main electrode is hardly affected by the difference in position. The resistance value between a can be measured.
【0018】[0018]
【実施例】図1及び図2は本発明の原理を示す基本的な
構成を図示した構成図で、符号5は差動増幅器、6は増
幅器、8は抵抗器、9は抵抗器である。DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS FIGS. 1 and 2 are block diagrams showing the basic configuration of the present invention. Reference numeral 5 is a differential amplifier, 6 is an amplifier, 8 is a resistor, and 9 is a resistor.
【0019】符号10は流体抵抗値を測定する水槽であ
り、この水槽10を内寸で縦20cm,横60cm,深さ45
cmのアクリル製樹脂板で成形し、この水槽10の横側板の
内壁中央部に対向状態に幅15cm,高さ46cm,厚さ1
mmのステンレス板で構成した第一の電極1と第一の電極
2とを対設し、この第一の電極1と第二の電極2の左右
に2mmの間隔を置いて幅15cm,高さ46cm,厚さ1mm
のステンレス板で構成した第三の電極3と第四の電極4
を配置し、図1に示すように電気的に接続して電極を構
成する。水槽10内に適量の水を満たし、測定試験のた
め、導電率の異なる流体塊の代替え品として、導電率が
零の縦5cm,横6cm,高さ20cmのプラスチックの角柱
11(導電率は零の流体塊とみなす。)を水槽10の底面に
垂直に立設する。水深は12.8cmであり、水の導電率
は122μs/cmであった。Reference numeral 10 is a water tank for measuring the fluid resistance value. The water tank 10 has internal dimensions of 20 cm in length, 60 cm in width, and 45 in depth.
Molded with an acrylic resin plate of cm, width 15 cm, height 46 cm, thickness 1 facing the center of the inner wall of the side plate of this water tank 10.
A first electrode 1 and a second electrode 2 made of a stainless steel plate having a width of 15 mm and a height of 15 cm with a distance of 2 mm between the first electrode 1 and the second electrode 2 are provided. 46 cm, thickness 1 mm
Third electrode 3 and fourth electrode 4 composed of the stainless steel plate
Are arranged and electrically connected as shown in FIG. 1 to form an electrode. Filling the water tank 10 with an appropriate amount of water, for measurement test, as a substitute for fluid lumps with different conductivity, a plastic prism with a vertical conductivity of 5 cm, width 6 cm, and height 20 cm.
11 (considered as a fluid mass having a conductivity of zero) is erected vertically on the bottom surface of the water tank 10. The water depth was 12.8 cm and the water conductivity was 122 μs / cm.
【0020】主電極aの二枚の対向する電極板1,2の
それぞれの中央を結ぶ直線に沿って、プラスチックの角
柱11の位置を変えながら(第二の電極2からプラスチッ
ク角柱11の表面までの間隔を図5のようにdとする。)
抵抗値を測定した。主電極a間に流す電流は5kHzの正
弦波交流で、電流値は0.5mAとした。While changing the position of the plastic prism 11 along the straight line connecting the centers of the two opposing electrode plates 1 and 2 of the main electrode a (from the second electrode 2 to the surface of the plastic prism 11) The distance between them is d as shown in FIG. 5.)
The resistance value was measured. The current flowing between the main electrodes a was a 5 kHz sinusoidal alternating current, and the current value was 0.5 mA.
【0021】抵抗値の測定結果を図6に示す。縦軸は主
電極a間の抵抗値[kΩ]であり、図に示すようにプラ
スチックの角柱11の位置による抵抗値の違いは僅かでほ
ぼ一定の値が得られた。FIG. 6 shows the measurement result of the resistance value. The vertical axis represents the resistance value [kΩ] between the main electrodes a, and as shown in the figure, the difference in the resistance value depending on the position of the plastic prism 11 was slight and a substantially constant value was obtained.
【0022】[0022]
【発明の効果】図5に示すように、第一の電極と第二の
電極との間の水中にプラスチックの角柱がある時の抵抗
値を測定してみると、図6のようにプラスチックの角柱
の位置にはほとんど関係なくほぼ一定の値が得られてい
ることがわかる。本発明の効果をより明らかにするため
に上記の測定と同様にして、第二の電極側にのみ電流検
出抵抗手段を設置した従来の方法による定電流回路で測
定した結果を図7に示す。電流検出抵抗手段の数がただ
ひとつであることを除き、それ以外のすべての条件を図
5の測定の場合に使用した回路と同じにして測定した結
果である。プラスチックの角柱の位置により測定値が大
幅に異なることがわかる。As shown in FIG. 5, when the resistance value of the plastic prism in the water between the first electrode and the second electrode is measured, the resistance value of the plastic is as shown in FIG. It can be seen that almost constant values are obtained regardless of the position of the prism. In order to further clarify the effect of the present invention, FIG. 7 shows the result of measurement by a constant current circuit according to the conventional method in which the current detecting resistor means is installed only on the second electrode side, in the same manner as the above measurement. It is the result of measurement under the same conditions as those of the circuit used in the measurement of FIG. 5, except that the number of current detection resistance means is only one. It can be seen that the measured values vary greatly depending on the position of the plastic prism.
【0023】このように、本発明の定電流回路による流
体抵抗測定方法により、流体中に局部的に導電率の異な
る流体塊が含まれている場合でも従来の方法に比較して
より正確な抵抗値の測定が可能である。As described above, according to the fluid resistance measuring method by the constant current circuit of the present invention, even if the fluid contains fluid lumps having different conductivity locally, the resistance is more accurate as compared with the conventional method. The value can be measured.
【図1】本実施例の原理を示す基本的な構成を図示した
構成図である。FIG. 1 is a configuration diagram illustrating a basic configuration showing the principle of the present embodiment.
【図2】本実施例の水槽に付設した主電極と補助電極の
設置位置を示す平面図である。FIG. 2 is a plan view showing installation positions of a main electrode and an auxiliary electrode attached to the water tank of this embodiment.
【図3】本実施例の水槽の電極間を流れる電流の状態を
概念的に図示した平面図である。FIG. 3 is a plan view conceptually showing the state of current flowing between the electrodes of the water tank of this embodiment.
【図4】本実施例の水槽の電極間を流れる電流の状態を
概念的に図示した平面図である。FIG. 4 is a plan view conceptually showing the state of current flowing between the electrodes of the water tank of this embodiment.
【図5】本実施例の測定試験の説明用平面図である。FIG. 5 is a plan view for explaining the measurement test of the present embodiment.
【図6】本実施例の測定結果を示すグラフである。FIG. 6 is a graph showing the measurement results of this example.
【図7】本実施例の比較試験(従来の回路で実測した)
の測定結果を示すグラフである。FIG. 7: Comparative test of this embodiment (measured by a conventional circuit)
It is a graph which shows the measurement result of.
1 第一の電極 2 第二の電極 3 第三の電極 4 第四の電極 7 電流検出抵抗手段 a 主電極 b 補助電極 c 流体抵抗測定用電極体 DESCRIPTION OF SYMBOLS 1 1st electrode 2 2nd electrode 3 3rd electrode 4 4th electrode 7 Current detection resistance means a Main electrode b Auxiliary electrode c Fluid resistance measurement electrode body
Claims (1)
主電極と、この主電極の左右に第三の電極と第四の電極
からなる一対の補助電極を近接状態に付設して構成した
流体抵抗測定用電極体を、流体中に浸漬或いは流体の流
路または液槽の内壁に設置し、主電極間に一定電流を流
して主電極間の電位差により主電極間の流体または固液
混合体または気液混合体または気固液混合体の抵抗値を
測定する流体抵抗測定用定電流回路であって、主電極の
第一の電極側と第二の電極側の夫々に電流検出抵抗手段
を設け、それぞれの電流検出抵抗手段から得られる二つ
の電圧を平均して得た電圧に基づき電流値を制御するこ
とを特徴とする流体抵抗測定用定電流回路。1. A pair of main electrodes composed of a first electrode and a second electrode, and a pair of auxiliary electrodes composed of a third electrode and a fourth electrode, which are provided in proximity to the left and right of the main electrode. The configured fluid resistance measuring electrode body is immersed in the fluid or installed in the flow path of the fluid or on the inner wall of the liquid tank, and a constant current is applied between the main electrodes to cause the potential difference between the main electrodes to cause fluid or solid A constant current circuit for measuring fluid resistance, which measures the resistance value of a liquid mixture, a gas-liquid mixture, or a gas-solid mixture, in which current is detected on the first electrode side and the second electrode side of the main electrode, respectively. A constant current circuit for measuring fluid resistance, characterized in that a resistance means is provided and a current value is controlled based on a voltage obtained by averaging two voltages obtained from the respective current detection resistance means.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP15832092A JPH0820391B2 (en) | 1992-06-17 | 1992-06-17 | Constant current circuit for fluid resistance measurement |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP15832092A JPH0820391B2 (en) | 1992-06-17 | 1992-06-17 | Constant current circuit for fluid resistance measurement |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH0627069A JPH0627069A (en) | 1994-02-04 |
| JPH0820391B2 true JPH0820391B2 (en) | 1996-03-04 |
Family
ID=15669064
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP15832092A Expired - Lifetime JPH0820391B2 (en) | 1992-06-17 | 1992-06-17 | Constant current circuit for fluid resistance measurement |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0820391B2 (en) |
Families Citing this family (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US7838574B2 (en) | 2006-10-20 | 2010-11-23 | Hewlett-Packard Development Company, L.P. | Dispersed pigments |
| US7812067B2 (en) | 2006-10-20 | 2010-10-12 | Hewlett-Packard Development Company, L.P. | Binders for pigmented ink formulations |
| US7675298B2 (en) | 2007-06-15 | 2010-03-09 | Hewlett-Packard Development Company, L.P. | Determining fluid characteristics |
| JP2010107487A (en) * | 2008-11-01 | 2010-05-13 | Tokyo Institute Of Technology | Device and method for measuring multiphase flow |
-
1992
- 1992-06-17 JP JP15832092A patent/JPH0820391B2/en not_active Expired - Lifetime
Also Published As
| Publication number | Publication date |
|---|---|
| JPH0627069A (en) | 1994-02-04 |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| US5503026A (en) | Method and apparatus for determining a volume flow | |
| US4780663A (en) | Gauge for measuring the conductance of a liquid present between two electrodes | |
| US6563306B2 (en) | Method and apparatus for detecting displacement of a magnet moved in response to variation of a physical characteristic of a fluid | |
| US7490513B2 (en) | Method for sensing levels of conductive liquids | |
| US4751466A (en) | Instrument for on-line measurement of the absolute electrical conductivity of a liquid | |
| US20100082271A1 (en) | Fluid level and concentration sensor | |
| CN100590396C (en) | Measuring device and conductivity measuring device, measuring element and method for determining the flow of an electrically conductive liquid | |
| US7117750B2 (en) | Method for operating a magnetoinductive flowmeter | |
| CN101769770A (en) | Method for operating a flow measuring device | |
| JPH0820391B2 (en) | Constant current circuit for fluid resistance measurement | |
| US7946184B2 (en) | Electromagnetic flowmeter having temperature measurement value for correcting electrical conductivity value | |
| EP4165378B1 (en) | Flow meter for measuring flow velocity in oil continuous flows | |
| JPS6379016A (en) | Liquid level measuring apparatus | |
| US20090266176A1 (en) | Magneto-inductive flow measuring device | |
| CN113286986A (en) | Capacitive sensor for detecting the level of a medium | |
| US20080148810A1 (en) | Device For Determining the Level of a Fluid | |
| JP3015616B2 (en) | Electromagnetic flow meter | |
| JPH116755A (en) | Interface detection switch | |
| Pauli et al. | Electrodiffusional direction-specific probe for measuring local velocity of aerated aqueous systems | |
| US20250377327A1 (en) | Measurement of characteristics of a fluid | |
| KR20030073617A (en) | Flow meter for open channel and thereof flow measuring method by using principle of electromagnetic induction | |
| JPH0419453Y2 (en) | ||
| JP3210094B2 (en) | Capacitor and fluid sensor using the same | |
| SU501279A1 (en) | Electromagnetic Flow Sensor | |
| JP2602110Y2 (en) | Apparatus for measuring solid fraction of snow-water mixture |