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JP2004053325A - Capacitive liquid density meter - Google Patents

Capacitive liquid density meter Download PDF

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Publication number
JP2004053325A
JP2004053325A JP2002208837A JP2002208837A JP2004053325A JP 2004053325 A JP2004053325 A JP 2004053325A JP 2002208837 A JP2002208837 A JP 2002208837A JP 2002208837 A JP2002208837 A JP 2002208837A JP 2004053325 A JP2004053325 A JP 2004053325A
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Prior art keywords
insulating liquid
capacitance
plate
density
curvature
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JP2002208837A
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Japanese (ja)
Inventor
Yoshiharu Kudo
工藤 芳春
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Japan Aviation Electronics Industry Ltd
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Japan Aviation Electronics Industry Ltd
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Abstract

【課題】絶縁性液体が流れる配管内に設置され、絶縁性液体の流速が高く、Re値が大きいときでも、電極板間におけるキャビテーションが抑制され、絶縁性液体の密度を高い精度で測定できる静電容量式液密度計の提供。
【解決手段】コンデンサ部1の正電極板2および負電極板3は、絶縁性液体の流線に平行な1つの平面における断面形が流線形である。絶縁性液体流入口の側(前縁21側)の断面の曲率は、絶縁性液体流出口の側(後縁22側)の断面の曲率よりも小さい。電極板の断面を流線形することにより、電極板2,3の表面で絶縁性液体の剥離が生じず、キャビテーションが抑止され、電極板間容量が絶縁性液体の密度に正確に対応し、電極板間容量の測定により絶縁性液体の密度が高い精度で測定される。
【選択図】   図1
An insulating liquid is provided in a pipe through which an insulating liquid flows. Even when the flow rate of the insulating liquid is high and the Re value is large, cavitation between electrode plates is suppressed, and the density of the insulating liquid can be measured with high accuracy. Provide capacitance type liquid density meter.
A positive electrode plate (2) and a negative electrode plate (3) of a capacitor section (1) have a streamlined cross section in one plane parallel to a streamline of an insulating liquid. The curvature of the cross section on the side of the insulating liquid inlet (front edge 21 side) is smaller than the curvature of the cross section on the side of the insulating liquid outlet (rear edge 22 side). By streamlining the cross section of the electrode plate, the insulating liquid does not peel off on the surfaces of the electrode plates 2 and 3, cavitation is suppressed, and the capacitance between the electrode plates accurately corresponds to the density of the insulating liquid. By measuring the capacitance between the plates, the density of the insulating liquid is measured with high accuracy.
[Selection diagram] Fig. 1

Description

【0001】
【発明の属する技術分野】
本発明は、静電容量式液密度計に関し、特に流動する絶縁性液体の密度を測定する静電容量式液密度計に関する。
【0002】
【従来の技術】
図2は、LNG、LPG等の絶縁性液体の配管内に設置された静電容量式液密度計の構成を示す概念図である。本図は、配管16の軸に直交する面において配管16を切断した状態で示してある。本図では、配管16及び貫通フランジ15は、断面で現れているが、断面を表すハッチングは省略してある。断面にハッチングを入れると、符号の引出し線とハッチングとが錯綜し、図面が読み難くなるので、その錯綜を避けるために、本図では断面のハッチングを省略してある(図5(b)及び図1(b)の断面図においても同様の理由で断面のハッチングが省略してある)。
【0003】
図2に示されるように、静電容量式液密度計は、配管16の内部に挿入して設置されるコンデンサ部1と、温度センサ6と、コンデンサ部1および温度センサ6による計測値を外部に取り出すための電線7とを含む。これらの電線7は、貫通フランジ15とハーメチック・コネクタ9を介して、引出し電線8として外部に取り出されており、コンデンサ部1の静電容量および温度センサ6による検知温度を液密度測定用の信号処理部に伝達する。コンデンサ部1は、絶縁材でなる筐体内に納められた導体板10及び11と、これら導体板10及び11から櫛状に伸びる複数の電極板とを含んでなる。保持体12は、コンデンサ部1を吊るすような態様で、貫通フランジ15を支点としてコンデンサ部1を保持する保持手段である。
【0004】
密度測定対象はLNG、LPG等の絶縁性液体である。絶縁性液体は、配管16内を管軸方向に流れており、その一部分はコンデンサ部1の電極間隙を通り抜ける。コンデンサ1の電極間の誘電率は、温度が一定のとき、コンデンサ部1の電極間隙を通り抜ける絶縁性液体の密度に対応している。更に、その電極間の誘電率はコンデンサ1の静電容量に対応している。このように、絶縁性液体の温度が一定のとき、コンデンサ1の静電容量は絶縁性液体の密度に一意に対応しているので、電線7および引出し電線8を介してコンデンサ1の静電容量を取得した信号処理部は、絶縁性液体の密度と静電容量との既知の関係から絶縁性液体の密度を計算できる。絶縁性液体の密度と静電容量との関係は、絶縁性液体の温度をパラメータとするので、信号処理部は温度センサ6で検知した絶縁性液体の温度を用いて、コンデンサ1の静電容量に基づく絶縁性液体の密度を補正し、正確な絶縁性液体の密度を算出する。
【0005】
図4は、従来の静電容量式液密度計におけるコンデンサ部1の外観構造を示す斜視図である。また、図5(a)はそのコンデンサ部1の正面図、図5(b)は同図(a)のB−B線矢視断面図である。図において、2は正電極板、3は負電極、4aは上面板、4bは下面板、5は側面板をそれぞれ表す。また、符号101は絶縁性液体の流れる方向を表す。図5(a)は、絶縁性液体が流入する側からコンデンサ部1を見た図である。図5(b)において、正電極板2、負電極板3および側面板5は断面で現れている。但し、断面にはハッチングは省略してある。断面にハッチングを省略した理由は、図2について述べたところと同じである。正電極板2は、図2における導体板10から櫛状に伸びている。但し、正電極板2および導体板10は一体に形成してあり、両者の境界は具体的には現れない。また、負電極板3は、図2における導体板11から櫛状に伸びている。但し、正電極板3および導体板11は一体に形成してあり、両者の境界は具体的には現れない。
【0006】
図5(a)および(b)から明らかなように、正電極板2は単純な矩形板であり、正電極板2の広平面は矩形である。負電極板3も正電極板2と全く同じ形の矩形板である。このように、正電極板2および負電極板3は共に平行平板による電極板として形成されており、絶縁性液体は、流れ方向101に沿ってコンデンサ部1の流入口側より内部に入り、これらの相対向する正負の電極板間を通って流出口側より配管16内に出てゆく。正電極板2および負電極板3は矩形板であるから、正電極板2および負電極板3における流入口側の端面および流出口側の端面は、絶縁性液体の流線に対し直交する。このような絶縁性液体の流れ状態において、図2に示されるように、コンデンサ部1における正負両電極板間の容量と、温度センサ6による絶縁性液体の温度とが計測され、これらの計測値を引出し電線8を介して外部の信号処理部に伝達して処理することにより、該絶縁性液体の密度が測定される。
【0007】
【発明が解決しようとする課題】
図4及び図5を参照して以上に説明した従来例では、コンデンサ部において容量計測用として配置される正負の電極板が共に単純な平行平板により構成されている。このように、正負の電極板が共に単純な平行平板であると、配管内の絶縁性液体の流速の増加に伴なうRe数(レイノルズ数)の増大により、電極間隙において該絶縁性液体の正負両電極板からの剥離等に起因するキャビテーションが発生する。正負両電極板間の絶縁性液体にキャビテーションが発生すると、正負両電極板間の容量はキャビテーションの生じない状態のときより小さくなる。すると、前記信号処理部の演算で得られる液体密度が、実際の絶縁性液体の密度より小さく計測される。
【0008】
本発明の目的は、電極板間を流れる絶縁性液体にキャビテーションが発生するのを抑止して、高い精度で絶縁性液体の密度を測定できる静電容量式密度計の提供にある。
【0009】
【課題を解決するための手段】
前述の課題を解決するために本発明は次の手段を提供する。
【0010】
(1)複数の板状電極を互いにほぼ平行に配置してなるコンデンサを備え、該複数の電極の間隙に絶縁性液体を流したときにおける該コンデンサの静電容量に基づき該絶縁性液体の液密度を測定する静電容量式液密度計において、
前記板状電極における1つの断面が流線形をなすことを特徴とする静電容量式液密度計。
【0011】
(2)少なくとも2枚の板状の電極をほぼ平行に対面させてなる平行平板型のコンデンサを備え、該コンデンサが絶縁性液体に漬けられ、該電極間隙に該絶縁性液体が流されたときにおける該コンデンサの静電容量に基づき該絶縁性液体の密度を測定する静電容量式液密度計において、
前記絶縁性液体の流線に平行な1つの面における前記電極の断面形が流線形であることを特徴とする静電容量式液密度計。
【0012】
(3)対向する正負の電極板により構成されるコンデンサ部と温度センサとを備え、該コンデンサ部の正負の電極板間に絶縁性液体が流され、該温度センサが該絶縁性液体に漬けられ、該電極板間の静電容量と該温度センサによる検知温度とに基づき該絶縁性液体の密度を測定する静電容量式液密度計において、
前記電極板における2つの広平面は1つの仮想平面に関し対称な形を成し、該仮想平面に直交しかつ絶縁性液体流の流線に平行な断面における前記電極板の輪郭は前記絶縁性液体の流入側の端および流出側の端においてほぼ半円形をなし、該流入側の該端における該半円形の曲率を第1の曲率とし、該流出側の該端における該半円形の曲率を第2の曲率とするとき、該第1の曲率は該第2の曲率より小さい
ことを特徴とする静電容量式液密度計。
【0013】
【発明の実施の形態】
次に、本発明の実施の形態を挙げ、本発明を一層具体的に説明する。
【0014】
図1は、本発明の一実施の形態におけるコンデンサ部の外観構造を示す図である。図3は、図1の実施の形態における正電極板2の斜視図である。また、図2は、図1の実施の形態を絶縁性液体の配管16内に配置した状態を示す概念図である。図2は、図4及び図5の従来の静電容量式液密度計に関して既に説明した図であり、絶縁性液体の配管16内に配置するという使用の形態の点では、本発明の実施の形態と従来の静電容量式液密度計とで差はない。
【0015】
図1(a)は、絶縁性液体が流入する側から見たコンデンサ部1の正面図(絶縁性液体が流入する側、すなわち該絶縁性液体の川上側より見た図)であり、図1(b)は、図1(a)のAーA線矢視断面図である。なお、図1(b)では、正電極2、負電極3および側面板5は断面で現れているが、線の錯綜を避けるために断面のハッチングが省略してあることは前述のとおりでる。図3は正電極板2の斜視図であるが、負電極板3の斜視図も図3と同じに表れる。図1(a)と図5(a)との対比および図1(b)と図5(b)との対比で明らかなように、本発明の実施の形態と従来の静電容量式液密度計とは、正負の電極板2,3の断面形状において相違し、その他の点では両者の構造に差はない。
【0016】
正電極板2は、図1(b)の線B−Bに関し左右対称の形をなす板状体である。図1(b)および図3に示すように、その板状体の正電極板2は、線B−Bを通り、導体板10の上面(図1(a)において上面)に直交する面に関し対称な形の広平面2aおよび2bを有する。正電極板2は導体板10と一体であり、正電極板2の上面23と導体板10との境界面は具体的な面としては現れない。図1から明らかなように、正電極板2は、導体板10から櫛状に伸びている。負電極板3は正電極板2と同じ構造である。負電極板3は導体板11から櫛状に伸びており、負電極板3と導体板11とは一体である。
【0017】
図1(a)および(b)並びに図3から明らかなように、本発明の実施の形態における正電極板2および負電極板3は共に単純な平行平板ではなく、A−A線断面形は流線形をなしている。絶縁性液体流入口の側の断面形状(図3における前縁21部のA−A線断面形)の曲率は、絶縁性液体流出口の側の断面形状(図3における後縁22部のA−A線断面形)の曲率よりも小さい。このように、正負の電極板の断面形状を流線形とすることにより、絶縁性液体のRe値が大きいときも正負の電極板間におけるキャビテーションの発生が抑止される。正負の電極板間におけるキャビテーションの発生が抑止されることにより、絶縁性液体のRe値の大小に拘わらずコンデンサ部1の容量が絶縁性液体の密度に高い精度で対応するので、信号処理部で演算される絶縁性液体の密度の精度が著しく向上される。信号処理部は、温度センサ6により検知された絶縁性液体の温度に基づき、コンデンサ部1の容量から求めた絶縁性液体の密度を補正し、より高い精度で絶縁性液体の密度を演算する。
【0018】
【発明の効果】
以上に実施の形態を挙げ具体的に説明したように、本発明によれば、絶縁性液体の流線に平行な1つの平面における正負の電極板の断面形が流線形であるから、配管内の絶縁性液体の流速が高く、Re値が大きくても、電極板表面で絶縁性液体の剥離が起き難く、電極板表面におけるキャビテーションが抑止され、正負の電極板間の容量が絶縁性液体の密度に高い精度で対応し、その容量の計測により絶縁性液体の密度が高い精度で測定される静電容量式密度計を提供できる。
【図面の簡単な説明】
【図1】本発明の一実施の形態におけるコンデンサ部の構造を示す図である。
【図2】静電容量式液密度計の配管内における配置状況を示す概念図である。
【図3】図1の実施の形態における正電極2を示す斜視図である。
【図4】従来の静電容量式密度計の外観を示す斜視図である。
【図5】従来の静電容量式密度計におけるコンデンサ部の構造を示す図である。
【符号の説明】
1  コンデンサ部
2  正電極板
2a,2b  正電極板の広平面
3  負電極板
4a  上面板
4b  下面板
5  側面板
6  温度センサ
7  電線
8  引出し電線
9  ハーメチック・コネクタ
10,11  導体板
12  保持体
15  貫通フランジ
16  配管
21  正電極板の前縁
22  正電極板の後縁
23  正電極板の上面
24  正電極板の下面
[0001]
TECHNICAL FIELD OF THE INVENTION
The present invention relates to a capacitance type liquid density meter, and more particularly to a capacitance type liquid density meter for measuring the density of a flowing insulating liquid.
[0002]
[Prior art]
FIG. 2 is a conceptual diagram showing a configuration of a capacitance type liquid density meter installed in a pipe of an insulating liquid such as LNG and LPG. This figure shows a state where the pipe 16 is cut on a plane perpendicular to the axis of the pipe 16. In this drawing, the pipe 16 and the through flange 15 appear in a cross section, but hatching indicating the cross section is omitted. If hatching is applied to the cross section, the lead line of the code and the hatching are complicated, and the drawing becomes difficult to read. Therefore, in order to avoid such complication, the hatching of the cross section is omitted in FIG. 5 (b) and FIG. In the cross-sectional view of FIG. 1B, hatching of the cross-section is omitted for the same reason.).
[0003]
As shown in FIG. 2, the capacitance type liquid density meter is configured such that the capacitor unit 1 inserted and installed in the pipe 16, the temperature sensor 6, and the measurement values obtained by the capacitor unit 1 and the temperature sensor 6 are externally provided. And an electric wire 7 for extraction. These electric wires 7 are taken out as electric wires 8 through the through flange 15 and the hermetic connector 9, and the capacitance of the capacitor section 1 and the temperature detected by the temperature sensor 6 are used as signals for liquid density measurement. Notify the processing unit. The capacitor unit 1 includes conductor plates 10 and 11 housed in a housing made of an insulating material, and a plurality of electrode plates extending in a comb shape from the conductor plates 10 and 11. The holding body 12 is holding means for holding the capacitor portion 1 with the through flange 15 as a fulcrum, in a manner in which the capacitor portion 1 is hung.
[0004]
The density measurement target is an insulating liquid such as LNG and LPG. The insulating liquid flows in the pipe 16 in the pipe axis direction, and a part of the liquid passes through the electrode gap of the capacitor unit 1. The dielectric constant between the electrodes of the capacitor 1 corresponds to the density of the insulating liquid passing through the electrode gap of the capacitor unit 1 when the temperature is constant. Further, the dielectric constant between the electrodes corresponds to the capacitance of the capacitor 1. Thus, when the temperature of the insulating liquid is constant, the capacitance of the capacitor 1 uniquely corresponds to the density of the insulating liquid. Can obtain the density of the insulating liquid from the known relationship between the density of the insulating liquid and the capacitance. Since the relationship between the density of the insulating liquid and the capacitance is based on the temperature of the insulating liquid as a parameter, the signal processing unit uses the temperature of the insulating liquid detected by the temperature sensor 6 to determine the capacitance of the capacitor 1. The density of the insulating liquid is corrected based on the above, and the accurate density of the insulating liquid is calculated.
[0005]
FIG. 4 is a perspective view showing the external structure of the capacitor unit 1 in the conventional capacitance type liquid density meter. FIG. 5A is a front view of the capacitor unit 1, and FIG. 5B is a sectional view taken along line BB of FIG. In the figure, 2 is a positive electrode plate, 3 is a negative electrode, 4a is an upper plate, 4b is a lower plate, and 5 is a side plate. Reference numeral 101 indicates the direction in which the insulating liquid flows. FIG. 5A is a view of the capacitor section 1 viewed from the side where the insulating liquid flows. In FIG. 5B, the positive electrode plate 2, the negative electrode plate 3, and the side plate 5 appear in a cross section. However, hatching is omitted in the cross section. The reason why the hatching is omitted in the cross section is the same as that described with reference to FIG. The positive electrode plate 2 extends in a comb shape from the conductor plate 10 in FIG. However, the positive electrode plate 2 and the conductor plate 10 are formed integrally, and the boundary between them does not appear specifically. The negative electrode plate 3 extends in a comb shape from the conductor plate 11 in FIG. However, the positive electrode plate 3 and the conductor plate 11 are formed integrally, and the boundary between them does not appear specifically.
[0006]
As is clear from FIGS. 5A and 5B, the positive electrode plate 2 is a simple rectangular plate, and the wide plane of the positive electrode plate 2 is rectangular. The negative electrode plate 3 is also a rectangular plate having exactly the same shape as the positive electrode plate 2. As described above, both the positive electrode plate 2 and the negative electrode plate 3 are formed as parallel plate electrode plates, and the insulating liquid enters inside from the inlet side of the capacitor unit 1 along the flow direction 101. And exits into the pipe 16 from the outflow side through the space between the opposite positive and negative electrode plates. Since the positive electrode plate 2 and the negative electrode plate 3 are rectangular plates, the end faces of the positive electrode plate 2 and the negative electrode plate 3 on the inflow side and the outflow side are orthogonal to the stream lines of the insulating liquid. In such a flow state of the insulating liquid, as shown in FIG. 2, the capacitance between the positive and negative electrode plates in the capacitor section 1 and the temperature of the insulating liquid by the temperature sensor 6 are measured. Is transmitted to an external signal processing unit via the lead wire 8 and processed, whereby the density of the insulating liquid is measured.
[0007]
[Problems to be solved by the invention]
In the conventional example described above with reference to FIGS. 4 and 5, both the positive and negative electrode plates arranged for measuring the capacitance in the capacitor section are each formed of a simple parallel flat plate. As described above, when both the positive and negative electrode plates are simple parallel flat plates, the Re number (Reynolds number) increases with an increase in the flow rate of the insulating liquid in the pipe, so that the insulating liquid flows in the electrode gap. Cavitation occurs due to separation from the positive and negative electrode plates and the like. When cavitation occurs in the insulating liquid between the positive and negative electrode plates, the capacitance between the positive and negative electrode plates becomes smaller than when no cavitation occurs. Then, the liquid density obtained by the operation of the signal processing unit is measured to be smaller than the actual density of the insulating liquid.
[0008]
An object of the present invention is to provide a capacitance type densitometer capable of suppressing the occurrence of cavitation in an insulating liquid flowing between electrode plates and measuring the density of the insulating liquid with high accuracy.
[0009]
[Means for Solving the Problems]
The present invention provides the following means to solve the above-mentioned problems.
[0010]
(1) A capacitor having a plurality of plate-like electrodes arranged substantially in parallel with each other, and a liquid of the insulating liquid based on the capacitance of the capacitor when the insulating liquid flows in a gap between the plurality of electrodes. In a capacitance type liquid density meter that measures density,
A capacitance-type liquid density meter, wherein one section of the plate-like electrode forms a streamline.
[0011]
(2) When a parallel plate type capacitor having at least two plate-like electrodes facing each other substantially in parallel is provided, the capacitor is immersed in an insulating liquid, and the insulating liquid flows through the electrode gap. In a capacitance type liquid density meter that measures the density of the insulating liquid based on the capacitance of the capacitor in,
A capacitance type liquid density meter, wherein a cross-sectional shape of the electrode on one surface parallel to a streamline of the insulating liquid is streamlined.
[0012]
(3) A capacitor portion including a positive and negative electrode plate and a temperature sensor are provided, and an insulating liquid is flown between the positive and negative electrode plates of the capacitor portion, and the temperature sensor is immersed in the insulating liquid. In a capacitance-type liquid density meter that measures the density of the insulating liquid based on the capacitance between the electrode plates and the temperature detected by the temperature sensor,
The two wide planes of the electrode plate are symmetrical with respect to one virtual plane, and the contour of the electrode plate in a cross section orthogonal to the virtual plane and parallel to the streamline of the insulating liquid flow is the insulating liquid. Are substantially semicircular at the inflow side end and the outflow side end, the semicircular curvature at the inflow side end is the first curvature, and the semicircular curvature at the outflow side end is the first curvature. When the curvature is 2, the first curvature is smaller than the second curvature.
[0013]
BEST MODE FOR CARRYING OUT THE INVENTION
Next, the present invention will be described more specifically with reference to embodiments of the present invention.
[0014]
FIG. 1 is a diagram illustrating an external structure of a capacitor unit according to an embodiment of the present invention. FIG. 3 is a perspective view of the positive electrode plate 2 in the embodiment of FIG. FIG. 2 is a conceptual diagram showing a state in which the embodiment of FIG. 1 is arranged in a pipe 16 of an insulating liquid. FIG. 2 is a diagram already described with respect to the conventional capacitance type liquid density meter shown in FIGS. 4 and 5, and in terms of the form of use of the present invention in which the insulating liquid is disposed in the piping 16, the embodiment of the present invention is not shown. There is no difference between the form and the conventional capacitance type liquid density meter.
[0015]
FIG. 1A is a front view of the capacitor section 1 as viewed from the side where the insulating liquid flows (a side where the insulating liquid flows, that is, a view as viewed from the upstream side of the insulating liquid). FIG. 2B is a sectional view taken along line AA of FIG. In FIG. 1B, the positive electrode 2, the negative electrode 3, and the side plate 5 appear in a cross section, but hatching in the cross section is omitted as described above in order to avoid complicated lines. FIG. 3 is a perspective view of the positive electrode plate 2, but a perspective view of the negative electrode plate 3 appears in the same manner as FIG. As is clear from the comparison between FIG. 1A and FIG. 5A and the comparison between FIG. 1B and FIG. 5B, the embodiment of the present invention and the conventional capacitance type liquid density It differs from the meter in the cross-sectional shapes of the positive and negative electrode plates 2 and 3, and there is no difference between the structures in other respects.
[0016]
The positive electrode plate 2 is a plate-like body that is symmetrical with respect to the line BB in FIG. 1B. As shown in FIG. 1B and FIG. 3, the positive electrode plate 2 of the plate-like body passes through a line BB and is perpendicular to the upper surface of the conductor plate 10 (the upper surface in FIG. 1A). It has wide planes 2a and 2b of symmetric shape. The positive electrode plate 2 is integral with the conductor plate 10, and a boundary surface between the upper surface 23 of the positive electrode plate 2 and the conductor plate 10 does not appear as a specific surface. As is clear from FIG. 1, the positive electrode plate 2 extends in a comb shape from the conductor plate 10. The negative electrode plate 3 has the same structure as the positive electrode plate 2. The negative electrode plate 3 extends in a comb shape from the conductive plate 11, and the negative electrode plate 3 and the conductive plate 11 are integrated.
[0017]
As is clear from FIGS. 1A and 1B and FIG. 3, both the positive electrode plate 2 and the negative electrode plate 3 in the embodiment of the present invention are not simple parallel flat plates, and the cross-sectional shape along the line AA is It is streamlined. The curvature of the cross-sectional shape on the side of the insulating liquid inlet (the cross-sectional shape taken along line AA of the front edge 21 in FIG. 3) is determined by the cross-sectional shape on the side of the insulating liquid outlet (A of the rear edge 22 in FIG. 3). -A line cross section). By making the cross-sectional shape of the positive and negative electrode plates streamlined, the occurrence of cavitation between the positive and negative electrode plates is suppressed even when the Re value of the insulating liquid is large. Since the occurrence of cavitation between the positive and negative electrode plates is suppressed, the capacitance of the capacitor unit 1 accurately corresponds to the density of the insulating liquid regardless of the magnitude of the Re value of the insulating liquid. The accuracy of the calculated density of the insulating liquid is significantly improved. The signal processing unit corrects the density of the insulating liquid obtained from the capacity of the capacitor unit 1 based on the temperature of the insulating liquid detected by the temperature sensor 6, and calculates the density of the insulating liquid with higher accuracy.
[0018]
【The invention's effect】
As described above in detail with reference to the embodiment, according to the present invention, the cross-sectional shape of the positive and negative electrode plates in one plane parallel to the streamline of the insulating liquid is streamlined. Even if the flow rate of the insulating liquid is high and the Re value is large, peeling of the insulating liquid hardly occurs on the electrode plate surface, cavitation on the electrode plate surface is suppressed, and the capacity between the positive and negative electrode plates is It is possible to provide a capacitance type densitometer capable of responding to the density with high precision and measuring the density of the insulating liquid with high precision by measuring the capacitance.
[Brief description of the drawings]
FIG. 1 is a diagram showing a structure of a capacitor unit according to an embodiment of the present invention.
FIG. 2 is a conceptual diagram showing an arrangement state of a capacitance type liquid density meter in a pipe.
FIG. 3 is a perspective view showing a positive electrode 2 in the embodiment of FIG.
FIG. 4 is a perspective view showing an appearance of a conventional capacitance type density meter.
FIG. 5 is a diagram showing a structure of a capacitor unit in a conventional capacitance type density meter.
[Explanation of symbols]
DESCRIPTION OF SYMBOLS 1 Capacitor part 2 Positive electrode plate 2a, 2b Wide plane of positive electrode plate 3 Negative electrode plate 4a Upper plate 4b Lower plate 5 Side plate 6 Temperature sensor 7 Electric wire 8 Leader wire 9 Hermetic connector 10, 11 Conductor plate 12 Holder 15 Through flange 16 Piping 21 Front edge of positive electrode plate 22 Rear edge of positive electrode plate 23 Upper surface of positive electrode plate 24 Lower surface of positive electrode plate

Claims (3)

複数の板状電極を互いにほぼ平行に配置してなるコンデンサを備え、該複数の電極の間隙に絶縁性液体を流したときにおける該コンデンサの静電容量に基づき該絶縁性液体の液密度を測定する静電容量式液密度計において、
前記板状電極における1つの断面が流線形をなすことを特徴とする静電容量式液密度計。
A capacitor having a plurality of plate-like electrodes arranged substantially parallel to each other is provided, and the liquid density of the insulating liquid is measured based on the capacitance of the capacitor when the insulating liquid flows in the gap between the plurality of electrodes. In the capacitance type liquid density meter,
A capacitance-type liquid density meter, wherein one section of the plate-like electrode forms a streamline.
少なくとも2枚の板状の電極をほぼ平行に対面させてなる平行平板型のコンデンサを備え、該コンデンサが絶縁性液体に漬けられ、該電極間隙に該絶縁性液体が流されたときにおける該コンデンサの静電容量に基づき該絶縁性液体の密度を測定する静電容量式液密度計において、
前記絶縁性液体の流線に平行な1つの面における前記電極の断面形が流線形であることを特徴とする静電容量式液密度計。
A parallel plate type capacitor having at least two plate-like electrodes facing each other substantially parallel to each other, the capacitor being immersed in an insulating liquid, and flowing when the insulating liquid flows through the electrode gap. In a capacitance-type liquid density meter that measures the density of the insulating liquid based on the capacitance of,
A capacitance type liquid density meter, wherein a cross-sectional shape of the electrode on one surface parallel to a streamline of the insulating liquid is streamlined.
対向する正負の電極板により構成されるコンデンサ部と温度センサとを備え、該コンデンサ部の正負の電極板間に絶縁性液体が流され、該温度センサが該絶縁性液体に漬けられ、該電極板間の静電容量と該温度センサによる検知温度とに基づき該絶縁性液体の密度を測定する静電容量式液密度計において、
前記電極板における2つの広平面は1つの仮想平面に関し対称な形を成し、該仮想平面に直交しかつ絶縁性液体流の流線に平行な断面における前記電極板の輪郭は前記絶縁性液体の流入側の端および流出側の端においてほぼ半円形をなし、該流入側の該端における該半円形の曲率を第1の曲率とし、該流出側の該端における該半円形の曲率を第2の曲率とするとき、該第1の曲率は該第2の曲率より小さい
ことを特徴とする静電容量式液密度計。
A capacitor portion composed of opposing positive and negative electrode plates and a temperature sensor; an insulating liquid flowing between the positive and negative electrode plates of the capacitor portion; the temperature sensor being immersed in the insulating liquid; In a capacitance liquid density meter that measures the density of the insulating liquid based on the capacitance between the plates and the temperature detected by the temperature sensor,
The two wide planes of the electrode plate are symmetrical with respect to one virtual plane, and the contour of the electrode plate in a cross section orthogonal to the virtual plane and parallel to the streamline of the insulating liquid flow is the insulating liquid. Are substantially semicircular at the inflow side end and the outflow side end, the semicircular curvature at the inflow side end is the first curvature, and the semicircular curvature at the outflow side end is the first curvature. When the curvature is 2, the first curvature is smaller than the second curvature.
JP2002208837A 2002-07-17 2002-07-17 Capacitive liquid density meter Withdrawn JP2004053325A (en)

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Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2009049119A3 (en) * 2007-10-12 2009-07-23 Hydro Aire Inc Flow meter

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2009049119A3 (en) * 2007-10-12 2009-07-23 Hydro Aire Inc Flow meter
JP2011501129A (en) * 2007-10-12 2011-01-06 ハイドロ エアー インコーポレイテッド Flowmeter
US7983856B2 (en) 2007-10-12 2011-07-19 Eldec Corporation Flow meter
US8255175B2 (en) 2007-10-12 2012-08-28 Eldec Corporation Flow meter

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