TW201231937A - Electrostatic capacity-type displacement sensor and proportional control valve having electrostatic capacity-type displacement sensor - Google Patents

Electrostatic capacity-type displacement sensor and proportional control valve having electrostatic capacity-type displacement sensor Download PDF

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TW201231937A
TW201231937A TW100143543A TW100143543A TW201231937A TW 201231937 A TW201231937 A TW 201231937A TW 100143543 A TW100143543 A TW 100143543A TW 100143543 A TW100143543 A TW 100143543A TW 201231937 A TW201231937 A TW 201231937A
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Taiwan
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electrode
cylindrical
pair
sensor
displacement sensor
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TW100143543A
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Chinese (zh)
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Kazutoshi Itoh
Yasuhisa Hirose
Keiichi Nishikawa
Takahiro Minatani
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Ckd Corp
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    • GPHYSICS
    • G01MEASURING; TESTING
    • G01DMEASURING NOT SPECIALLY ADAPTED FOR A SPECIFIC VARIABLE; ARRANGEMENTS FOR MEASURING TWO OR MORE VARIABLES NOT COVERED IN A SINGLE OTHER SUBCLASS; TARIFF METERING APPARATUS; MEASURING OR TESTING NOT OTHERWISE PROVIDED FOR
    • G01D5/00Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable
    • G01D5/12Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable using electric or magnetic means
    • G01D5/14Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable using electric or magnetic means influencing the magnitude of a current or voltage
    • G01D5/24Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable using electric or magnetic means influencing the magnitude of a current or voltage by varying capacitance
    • G01D5/241Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable using electric or magnetic means influencing the magnitude of a current or voltage by varying capacitance by relative movement of capacitor electrodes

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  • Engineering & Computer Science (AREA)
  • Power Engineering (AREA)
  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Measurement Of Length, Angles, Or The Like Using Electric Or Magnetic Means (AREA)

Abstract

The present invention provides an electrostatic capacity-type displacement sensor for measuring linear displacement of a measurement subject. This electrostatic capacity-type displacement sensor comprises a first member having a cylinder electrode in the shape of a cylinder the central axis of which is parallel to a straight line, and a second member having a tubular outer electrode provided in a state electrically insulated from the cylinder electrode at the outer side of the cylinder electrode. The outer electrode has at least one pair of electrodes circumferentially separated from and facing one another, and the cylinder electrode is electrically insulated from the circuit connected to the outer electrode. The first and second members move relative to each other on the straight line with the displacement of the measurement subject, and the electrostatic capacity between the at least one pair of outer electrodes changes in accordance with this movement.

Description

201231937 六、發明說明: 【明戶斤屬名奸冷貝:^ j 發明領域 本發明係有關於一種靜電容式變位感測器,特別是有 關於一種利用因於電極之對向面積之變化所引起之靜電容 變化的變位感測器。 L· Jl 發明背景 在具有稱為流體控制閥或致動 0 π <詞·桎1線移 動之構成要件的裝置巾,有具有m彳量其變位之變位感 测器者。此種用途之變位感測器因測量對象之變位量大, 而可利用接觸式電位ϋ(專利文獻1}或差動變壓器式變位感 測器、或者利用諸如霍耳科之磁性體的非接觸式變位感 =m具有簡易之結構之靜電容式變位感測器 迄今亦利用於其他用途。 p容式變位感測器係利用因對向之電極之相對移動 =起之靜電容的變化,對測量對象之變錢行測量之感 ==測量對象之變位-般係檢測因對向之電極之對向面 ^:開距離之變動所叫之靜電容的變化。利用對向面 方式的靜電容式變位感測器(專利 由於如 第15圖所示,利用對向電 故具有爾靡量_。^面離財)之變化, 由於儘量料對向電極以點ϋ,在本方式中, 17圖之區域Zi解,^ 提高f敏度,故如第 一 巨離廿之誤差而引起之測量誤差顯 201231937 著。結果,產生了嚴密製造公差與測量靈敏度間之取捨的 問題。 另一方面,利用隔開距離變化之方式的靜電容式變位 感測器如第16圖所示,具有下述優點,前述優點係因與平 行於對向電極間之對向面之相對位置有關之誤差所引起的 測量誤差在線性上不致過大。然而,如第17圖所示,本方 式測量對象之變位d與靜電容(C= ε ><S/d)之關係為非線 性,而有在諸如區域Z2之大變位量(衝程)之區域中測量極 為困難的問題。 另一方面,亦提出非利用靜電容之變化的測量方式, 而是依據利用了電容耦合之對向電極間之通訊狀態而進行 測量之方式的感測器(專利文獻4、5),來作為利用靜電容之 感測器。在本方式中,在施加了相位相互不同之電壓的複 數對向電極此點上具有特徵,按照測量對象之變位,與複 數對向電極中之何者會產生最強電容耦合,而依此來進行 測量。由於本方式可以非接觸切換電路,故可在不對測量 對象之移動造成影響下進行測量。然而,本方式須在用以 切換電路之曲面上形成複雜之電極圖形,而亦具有配線或 電路複雜之問題。 先行技術文獻 專利文獻 專利文獻1 日本專利公開公報2010-152763號 專利文獻2 曰本專利公開公報平01-196011號 專利文獻3 曰本專利公開公報平03-123814號201231937 VI. INSTRUCTIONS: [Ming jin genus genius cold shell: ^ j FIELD OF THE INVENTION The present invention relates to a capacitive displacement sensor, in particular to a use of the change in the opposing area of the electrode A displacement sensor that causes a change in electrostatic capacitance. BACKGROUND OF THE INVENTION In a device towel having a component called a fluid control valve or actuating a movement of 0 π < word 桎 1 line, there is a displacement sensor having a displacement of m 彳. The displacement sensor for such a use can utilize a contact potential ϋ (Patent Document 1) or a differential transformer type displacement sensor, or a magnetic body such as a holster, because the displacement amount of the measurement object is large. The non-contact displacement sensor = m has a simple structure, and the capacitive displacement sensor has been used for other purposes. The p-type displacement sensor utilizes the relative movement of the opposite electrode. The change of the static capacitance, the measurement of the change of the measurement object == the displacement of the measurement object - the detection of the opposite direction of the opposite electrode ^: the change of the open distance is called the change of the electrostatic capacitance. The opposite-surface type of electrostatic capacitance type displacement sensor (the patent uses the opposite direction as shown in Fig. 15, which has the effect of the opposite direction), because the point of the counter electrode is as much as possible. ϋ In this method, the region of the figure 17 is solved by Z, and the sensitivity of f is improved. Therefore, the measurement error caused by the error of the first large deviation is 201231937. As a result, a strict manufacturing tolerance and measurement sensitivity are generated. The problem of trade-offs. On the other hand, the way to change the distance As shown in Fig. 16, the electrostatic capacitance type displacement sensor has the advantage that the measurement error caused by the error related to the relative position parallel to the opposing surface between the counter electrodes is linear. However, as shown in Fig. 17, the relationship between the displacement d of the measuring object and the electrostatic capacitance (C = ε >< S/d) is nonlinear, and there is a large change such as the region Z2. The extremely difficult problem is measured in the region of the bit amount (stroke). On the other hand, the measurement method that does not utilize the change of the electrostatic capacitance is proposed, but the measurement method based on the communication state between the counter electrodes using the capacitive coupling is also proposed. The sensor (Patent Documents 4 and 5) is used as a sensor using a static capacitance. In this embodiment, a plurality of counter electrodes having voltages different in phase from each other are applied to the point, and the object is measured. The displacement and the complex counter electrode produce the strongest capacitive coupling, and the measurement is performed accordingly. Since the method can be used for the non-contact switching circuit, the measurement can be performed without affecting the movement of the measuring object. However, this method requires a complicated electrode pattern to be formed on the curved surface for switching the circuit, and has a problem that the wiring or the circuit is complicated. PRIOR ART DOCUMENT Patent Document Patent Document 1 Japanese Patent Laid-Open Publication No. 2010-152763 Patent Document 2 Patent Publication No. 01-196011 Patent Document 3 曰 Patent Publication No. 03-123814

S 4 201231937 專利文獻4 日本專利公開公報平08-159704號 專利文獻5 日本專利公開公報平08-166204號 C發明内容3 發明概要 發明欲解決之課題 如此,迄今在利用靜電容之變化之方式的感測器中, 產生可測量之變位量與對向電極之組裝容許公差間之取捨 的問題。另一方面,利用電容耦合,以非接觸切換電路之 方式有在曲面上之複雜電極圖形的形成、配線或電路之複 雜化等問題。 本發明係為解決上述習知之課題之至少一部份而創作 者,目的在於提供一種利用靜電容,並以簡易之結構對測 量對象之變位進行測量的技術。 用以欲解決課題之手段 以下,就對解決上述課題有效之手段等,一面依需要, 顯示效果等,一面說明。 手段1. 一種靜電容式變位感測器,係對測量對象之直 線上之變位進行測量者,其包含有第1構件及第2構件,該 第1構件具有圓柱狀圓柱電極,該圓柱狀圓柱電極係具有平 行於前述直線之中心軸線;該第2構件係具有圓筒狀外側電 極,該圓筒狀外側電極係在前述圓柱電極之外側,以與前 述圓柱電極電性絕緣之狀態而設;前述外側電極具有於圓 周方向分割,且相對向之至少一對電極,前述圓柱電極從 連接於前述外側電極之電路電性絕緣,前述第1構件與前述 201231937 第構件隨著前述測量對象之變位,相對地在前述直線上移 動月IJ述至少-對之外側電極之相互間之靜電容因應前述 移動而變化。 手段1包含有外側電極,該外側電極具有在圓柱電極之 外側,以與圓柱電極電性絕緣之狀態而設,且靜電容隨著 測!對象之變位而變化之一對電極。靜電容之變化因外側 電極與圓桎電極隨著測量對象之變位而相對移動,因而使 外側電極與圓柱電極間之對向面積變化而產生。由於圓柱 電極與外側電極之對向面形周狀,圓柱電極與連接於 外側電極之電路電性絕緣,故即使圓柱電極與外側電極相 互H因對向面之隔開距離之變化而引起之靜電容的變 化仍可抵銷。 藉此可解決可測量之變位量與對向電極之組裝容 A差間之取捨的問題,而不須過度嚴密要求組裝容許 差即可擴大可測量之變位量。再者,由於圓柱電極即 1與外側電極之内面之位置關係亦不致變化,故適 ㈣之閥體或致動器之各種變位的測量。 ,一手^2.如手段1記載之靜電容式變位感測器,其中 述一料側電極係以包含前述測量對象之變位之方向的 面’均=地分割為二而相對向之一對電極。 較佳的八丨t藉發明人之解析與實驗而導出之外側電極: 柱電極^卜:^構她機發明人之實驗1 而方向之測量誤錢錄度分析, 而使對向面稽掸+ I。伯 θ 偏心方向具有外側電極相對於分害Japanese Patent Laid-Open Publication No. Hei 08-166204 C Patent Literature No. Hei 08-166204 C. SUMMARY OF THE INVENTION PROBLEMS TO BE SOLVED BY THE INVENTION The present invention has hitherto utilized a change in electrostatic capacitance. In the sensor, there is a problem of a trade-off between the measurable displacement amount and the assembly tolerance of the counter electrode. On the other hand, with capacitive coupling, in the form of a non-contact switching circuit, there are problems such as formation of a complicated electrode pattern on a curved surface, wiring or circuit recombination. The present invention has been made in order to solve at least a part of the above-mentioned problems, and an object of the invention is to provide a technique for measuring displacement of a measuring object by means of a simple capacitance using a static capacitance. Means for Solving the Problem The following is a description of the means for solving the above-mentioned problems, and the like, as needed, and the like. Means 1. A static capacitance type displacement sensor for measuring a displacement on a straight line of a measurement object, comprising: a first member and a second member, the first member having a cylindrical cylindrical electrode, the cylinder The cylindrical electrode has a central axis parallel to the straight line; the second member has a cylindrical outer electrode that is electrically insulated from the cylindrical electrode on the outer side of the cylindrical electrode. The outer electrode has a circumferential direction and is opposed to at least one pair of electrodes, wherein the cylindrical electrode is electrically insulated from a circuit connected to the outer electrode, and the first member and the 201231937 member are subjected to the measurement target. The displacement is relatively relatively long on the straight line. The electrostatic capacitance between the outer electrodes is changed in response to the aforementioned movement. The means 1 comprises an outer electrode which is provided on the outer side of the cylindrical electrode and is electrically insulated from the cylindrical electrode, and the electrostatic capacitance is measured! The displacement of the object changes one of the electrodes. The change in the electrostatic capacitance is caused by the relative displacement of the outer electrode and the round electrode with the displacement of the measuring object, thereby causing a change in the opposing area between the outer electrode and the cylindrical electrode. Since the cylindrical electrode and the outer electrode are circumferentially opposed to each other, the cylindrical electrode is electrically insulated from the circuit connected to the outer electrode, so even if the cylindrical electrode and the outer electrode are separated from each other by the distance between the opposing faces, the static electricity is caused. The change in capacity can still be offset. Thereby, the problem of the trade-off between the measurable displacement amount and the assembly tolerance A of the counter electrode can be solved, and the measurable displacement amount can be expanded without excessively demanding the assembly tolerance. Furthermore, since the positional relationship between the cylindrical electrode, i.e., the inner surface of the outer electrode, does not change, the measurement of various displacements of the valve body or actuator of (4) is suitable. The one-handed ^2. The electrostatic capacitance type displacement sensor according to the first aspect, wherein the one side electrode is divided into two by a plane including a direction of the displacement of the measuring object, and one of the opposite directions Electrode. The better gossip is derived from the inventor's analysis and experiment and the outer electrode is derived: the column electrode ^ Bu: ^ The invention of the inventor's experiment 1 and the measurement of the direction of the wrong money, and the opposite direction + I. The eccentric direction of the θ has an outer electrode relative to the damage

S 6 201231937 面之方向的相對之方向之含意。 a手段3_如手段!或2記載之靜電容式變位感測器,其中 MW構件具有用以連接於前述測量對象之連接部,前述 第2構件具有分別連接於前述至少一對之外側電極,且朝前 迷第2構件之外部貫穿前述第2構件之至少_對導電部。 手段3由於設有連接於與測量對象―同變位之第消 側從其内部貫穿至外部之電極,故可避免 對象之變位之配線的變形1此,不需考慮配線 之妓形之設計,並且,藉消除線 感測器之可靠度。 *之了動部份,亦可提高 述第==手段1記載之靜電容式變位感測器,其中前 =第前料㈣極與前㈣㈣極包圍之區 域,刚述區域以非壓縮性介電流體填滿。 手段4由於以外側電極及 縮性之介電流體填滿,故可增大靜^包圍之空間以非壓 利用各種介電流體作為非壓縮性而提高。可 指介電性優於導電性之流體。^電流體。介電流體係 手段5.如手段4記載之靜雷办 述第2構件更具有補償用電^變位感測器,其中前 於前述外側電極之外周方向if償用電容器具有配置 直徑相互不同之-_稍=述介電越而對向, 前述-對固定對向電==柱電極包圍之區域及以 電流體。 區域的連通孔,共有前述介 201231937 手段5包含有補償用電容器,該補償用電容器具有配置 於外側電極之外周方向,隔著介電流體對向,直徑相互不 同之一對固定對向電極。補償用電容器藉連通於以外側電 極與圓柱電極包圍之區域及以一對固定對向電極包夾之區 域的連通孔’共有前述介電流體。藉此,可不使測量對象 之變位方向之尺寸過大而安裝補償用電容器,可補償因介 電承數之變化引起之測量變位的誤差。 手段6_如手段1記載之靜電容式變位感測器,其中前 述第2構件具有麵㈣,該靜電容式變位感測器並設有以 與該兩者電H緣之狀態存纽錢㈣電極與前述感測 器體間,且在前述第1構件與前述第2構件相對移動之移動 範圍值蓋⑴述外側電極及前述圓柱電極兩者之金屬繁筒狀 遮蔽構件’前述筒狀遮蔽構件係電性接地。 手段6係第1構件與第2構件相對移動之期間,金屬製筒 狀遮蔽構件會覆蓋外側電極及圓柱電極兩者。因此,於檢 測靜電容之際,即使存在人接觸具有外側電極之第2構件之 感測器體等外在干擾主要·,亦可減少㈣外在干擾主 要原因所引起之影響。又,於外側電極或圓杈電極與感測 器體間產生之雜散電容,可藉由接地之筒狀遮蔽構件削 除。因此,可減低使靜電容之數值不穩定之主要原因,而 穩定地進行靜電容之檢測。 手段7·如手段6記載之靜電容式變位感測器,其中前 述第2構件具有分別連接於至少一對之前述外側電極,且朝 前述第2構件之外部貫穿前述第2構件之至少一對導電部,S 6 201231937 The meaning of the relative direction of the direction of the face. a means 3_ as means! Or a static capacitance type displacement sensor according to claim 2, wherein the MW member has a connection portion for connecting to the measurement target, and the second member has a connection to the at least one pair of outer electrodes, respectively, and the second forward The outside of the member penetrates at least the pair of conductive portions of the second member. Since the means 3 is provided with an electrode that is connected to the outside from the inside to the outside of the measurement object-co-located position, it is possible to avoid deformation of the wiring of the object displacement, and it is not necessary to consider the design of the wiring. And, by eliminating the reliability of the line sensor. * The moving part can also improve the static capacitance type displacement sensor described in the above == means 1, wherein the front = the front (four) pole and the front (four) (four) pole surrounded by the area, the area is non-compressive The dielectric fluid is filled. Since the means 4 is filled with the outer electrode and the dielectric fluid of the contraction, the space surrounded by the static electrode can be increased by the non-pressure using various dielectric fluids as the non-compressibility. It can refer to a fluid that is more dielectric than conductive. ^ Current body. The dielectric current system means 5. The second member of the static lightning system described in the fourth aspect further has a compensation electric displacement sensor, wherein the outer peripheral electrode of the outer electrode is provided with a different diameter from each other. _Slightly = the opposite of the dielectric, the aforementioned - for the fixed opposite power = = the area surrounded by the column electrode and the current body. In the communication hole of the region, the means 5 includes a compensation capacitor having a pair of opposite electrodes arranged in the outer circumferential direction of the outer electrode and opposed to each other with a diameter interposed therebetween. The compensating capacitor shares the dielectric fluid by communicating with a region surrounded by the outer electrode and the cylindrical electrode and a communicating hole of a region sandwiched by the pair of fixed counter electrodes. Thereby, the compensation capacitor can be mounted without making the size of the measurement object in the displacement direction too large, and the error of the measurement displacement due to the change in the dielectric load can be compensated. [6] The static capacitance type displacement sensor according to the first aspect, wherein the second member has a surface (four), and the static capacitance type displacement sensor is provided with a state of being in a state of being electrically H a movement range value cover (1) between the electrode (four) electrode and the sensor body, and a metal tubular shielding member of the outer electrode and the cylindrical electrode The shielding member is electrically grounded. In the means 6 when the first member and the second member move relative to each other, the metal cylindrical shielding member covers both the outer electrode and the cylindrical electrode. Therefore, when detecting the electrostatic capacitance, even if there is external disturbance such as a sensor body that contacts a second member having the outer electrode, the influence of (4) the main cause of external disturbance can be reduced. Further, the stray capacitance generated between the outer electrode or the round electrode and the sensor body can be removed by the cylindrical shield member that is grounded. Therefore, the main cause of the instability of the electrostatic capacitance can be reduced, and the detection of the electrostatic capacitance can be performed stably. The static capacitance type displacement sensor according to the sixth aspect, wherein the second member has at least one pair of the outer electrodes, and the outer member penetrates at least one of the second members toward the outer side of the second member For the conductive part,

S 8 201231937 件朝前物構件之外部貫穿前述第2構 “ %卩之—部份亦為前述筒__件所覆蓋, ::導電部及前述筒狀遮蔽構件中往前述第2構件之外 =的部份,安裝背面朝向電極側之電路基板,且於前 ㈣Γ基板之背面’形成有與形成於該電路基板之接地用 電路電性連接之金屬膜。 手段7係可以筒狀遮蔽構件與金屬膜包圍電極部份及 電^之。P伤’而可獲得更廣大之遮蔽效果。因此,可 錢少因外在干擾主要·㈣之影響,亦有助於雜散電 谷之刪減’而使靜電容之檢測更穩定化。 此外’若前述電路基板與第2構件隔開距離而安裝時, 即使導電部為突出至第2構件之外部之部份,亦可減少因外 在干擾主要原因5丨起之影響。又,於突出之導電部間產生 之雜散電容可藉由分別連接於接地之筒狀賴構件或金屬 膜刪減。因此,可抑制雜散電容之增加,即使採用使電路 基板隔=距離之結構,亦可在使靜電容穩定之狀態下檢測。 手U種比例控制閥,係控制介電流體之流動者, 其^ 3有Z載於手段4或5之靜電容式變位感測器及間本 體,該閥本體係具有作為連接於前述第嘴件之前述測量對 象的閥體’ β賴度因應前述直線上之前述閥體之變位而變化 者;又’前關本體具有將介電錢料至前舰域之流路。 由於手1又8利用控制對象之流體作為介電流體故可在 不設有用以使用介電流體之專錢路或儲存槽下,簡易地 使用介電流體。此外,在本說明書中,比例控制閥具有廣 201231937 義之含意,舉例言之,只要為可測量閥開度而反饋者即可, 例如亦包含控制混合比之混合閥。 此外,本發明不僅可以靜電容式變位感測器或真空控 制閥及其他比例控制閥具體實現化,例如亦可以具有靜電 容式變位感測器之圓筒、致動器、線軸閥之形式具體實現 化。 圖式簡單說明 第1圖係顯示第1實施形態之真空控制閥4 〇之閥全關狀 態之結構的截面圖。 第2圖係顯示第丨實施形態之真空控制閥4 〇之閥半開狀 態之結構的截面圖。 第3圖係顯示上升量感測器1〇〇之結構的截面圖。 第4圖係顯示上升量感測器1〇〇之端部的外觀圖。 第5圖係顯示上升量感測器1〇〇之結構的示意圖。 第6圖係顯示上升量感測以⑼之對向電極之結構的立 體圖。 第7圖係顯示上升量感測器⑽之靜電容的計算式。 第8圖係比較圓柱電極及外側電極之靜電容與理論值 而顯不之圖表。 第9圖係顯示因圓柱電極及外側電極之偏心而引起之 測量誤差的圖表。 △第10圖係顯示第i變形例之真空控制閥*之閥全關狀 態之結構的截面圖。 第11圖係顯示介電常數因應介電流體之溫度而變化之S 8 201231937 The outer part of the front member is penetrated through the second structure "%" is also covered by the above-mentioned tube, and the conductive portion and the cylindrical shielding member are outside the second member. a portion of the circuit board having the back surface facing the electrode side, and a metal film electrically connected to the grounding circuit formed on the circuit board on the front surface of the front (four) germanium substrate. The means 7 is a cylindrical shielding member and The metal film surrounds the electrode part and the electric circuit. P damage' can obtain a wider shielding effect. Therefore, the amount of money can be less due to external interference (4), and also contribute to the deletion of stray electricity valley. In addition, when the circuit board is mounted at a distance from the second member, even if the conductive portion protrudes to the outside of the second member, the external interference can be reduced. The cause of the cause is 5. The stray capacitance generated between the protruding conductive portions can be reduced by the cylindrical member or the metal film respectively connected to the ground. Therefore, the increase of the stray capacitance can be suppressed even if Separate the circuit board = The structure can also be detected in a state in which the static capacitance is stabilized. The U-type proportional control valve is used to control the flow of the dielectric fluid, and the Z 3 has a static capacitance type displacement of the means 4 or 5. a valve body having a valve body '''''''''''''''''''''''''''''''''''''''' The dielectric material is fed to the flow path of the front ship. Since the hand 1 and 8 use the fluid of the control object as the dielectric fluid, it can be easily used without the special money path or storage tank for using the dielectric fluid. In addition, in the present specification, the proportional control valve has the meaning of the broad 201231937. For example, as long as it is measurable for measuring the valve opening degree, for example, a mixing valve for controlling the mixing ratio is also included. The invention can not only realize the static capacitance type displacement sensor or the vacuum control valve and other proportional control valves, for example, the cylinder, the actuator and the spool valve of the static capacitance type displacement sensor can be realized. Chemical BRIEF DESCRIPTION OF THE DRAWINGS Fig. 1 is a cross-sectional view showing a configuration of a valve fully closed state of a vacuum control valve 4 of the first embodiment. Fig. 2 is a view showing a half-open state of a vacuum control valve 4 of the second embodiment. Fig. 3 is a cross-sectional view showing the structure of the amount of rise sensor 1 。. Fig. 4 is an external view showing the end of the amount of rise sensor 1 第. Fig. 5 shows the amount of rise sensing Fig. 6 is a perspective view showing the structure of the counter electrode of (9) for the amount of rise sensing. Fig. 7 is a graph showing the calculation formula of the electrostatic capacitance of the amount of rise sensor (10). Fig. 8 is a comparison The static capacitance of the cylindrical electrode and the outer electrode is not shown by the theoretical value. Fig. 9 is a graph showing the measurement error caused by the eccentricity of the cylindrical electrode and the outer electrode. ΔFig. 10 shows the vacuum of the i-th modification. A cross-sectional view of the structure of the valve fully closed state of the control valve*. Figure 11 shows the dielectric constant changes in response to the temperature of the dielectric fluid.

S 10 201231937 圖表。 第12圖係顯示第2變形例之真空控制閥4 0 b之閥全關狀 態之結構的截面圖。 第13圖係顯示第3變形例之介電流體控制閥4 0 c之結構 的部份截面圖。 第14(a)圖、第14(b)圖係顯示第2實施形態之線轴閥100 之感測器設置側的截面圖。 第15圖係顯示習知技術之對向電極之對向面積變化之 態樣的示意圖。 第16圖係顯示在習知技術中,對向電極之隔開距離變 化之態樣的示意圖。 第17圖係顯示習知技術之對向電極之隔開距離與靜電 容之關係的圖表。 I:實施方式】 用以實施發明之形態 第1實施形態 以下,一面參照圖式,一面說明具體實現本發明之第1 實施形態。在本實施形態中,具體實現在半導體裝置等製 造線所使用之真空控制閥40,並依據第1圖至第6圖進行說 明。 第1圖係顯示第1實施形態之真空控制閥40之閥全關狀 態之結構的截面圖。第2圖係顯示第1實施形態之真空控制 閥40之閥半開狀態之結構的截面圖。真空控制閥40包含有 閥本體41、開關閥30、致動器42及上升量感測器100。於閥 201231937 本^形成有連接真空容器(省略圖示)及真空 :物。流路轉有用以連私真空容器側之上游側流 路81'及用以連接於真空制之下游側流路82。 開關閱30具有開關上游側流_與下游側流路82間之 流路的功能 '及操作該流路之開度而調整電導之功能。開 關闊3〇具有提動閥體31、閥座32、彈性密封構件33、密封 滑動部之伸縮囊仏__藉由使提動_31抿接閥座 32,可以彈性密封構件33封閉上游側流路81與下游側流路 82之間。開關閥3〇可操作作為提動閥體31與閥座32間之距 離的上升虹⑽度)’而磐上游側流路81與下游側流路82 間之電導。提動閥體31之移動方向亦稱為軸線方向。上升 量L係可於轴線方向變位之量。 致動器42驅動提動閥體31,以操作上升量L。致動器42 具有致動器本體43、為絕緣體之樹脂製活塞49、連接活塞 49與提動閥體31之陶瓷製活塞桿44、賦與活塞49勢能之賦 與勢能彈簧46、支撐賦與勢能彈簧46之樹脂製圓筒蓋45〇。 活塞49於與形成於致動器本體43之内部之凹部4%間形成 圓筒室45。調壓閥(bellofram)49b係密封圓筒室45之構件, 裝設於活塞49之外周面與圓筒室45之内周面間之間隙。於 圓筒室45形成有用以從電動氣壓控制閥(省略圖示)供給作 動空氣之作動空氣流路47。 致動器42可藉由操作來自圖中未示之電動氣壓控制間 之作動空氣的供給壓,將提動閥體31控制至任意之位置。 提動閥體31之位置在施加於活塞49之作動空氣的載重與賦S 10 201231937 Chart. Fig. 12 is a cross-sectional view showing the structure of the valve fully closed state of the vacuum control valve 40b of the second modification. Fig. 13 is a partial cross-sectional view showing the structure of the dielectric fluid control valve 40c of the third modification. Figs. 14(a) and 14(b) are cross-sectional views showing the sensor installation side of the bobbin valve 100 of the second embodiment. Fig. 15 is a view showing a state in which the opposing area of the counter electrode of the prior art is changed. Fig. 16 is a view showing a state in which the distance between the opposing electrodes is changed in the prior art. Fig. 17 is a graph showing the relationship between the separation distance of the counter electrode and the electrostatic capacitance of the prior art. I. Embodiments for carrying out the invention. First Embodiment Hereinafter, a first embodiment of the present invention will be specifically described with reference to the drawings. In the present embodiment, the vacuum control valve 40 used in the manufacturing line of a semiconductor device or the like is specifically realized, and the description will be made based on Figs. 1 to 6 . Fig. 1 is a cross-sectional view showing the structure of the valve fully closed state of the vacuum control valve 40 of the first embodiment. Fig. 2 is a cross-sectional view showing the structure of the valve half-open state of the vacuum control valve 40 of the first embodiment. The vacuum control valve 40 includes a valve body 41, an on-off valve 30, an actuator 42, and a lift amount sensor 100. In the valve 201231937, a vacuum container (not shown) and a vacuum are formed. The flow path is used to connect the upstream side flow path 81' on the vacuum container side and the downstream side flow path 82 to be connected to the vacuum system. The switch 30 has a function of a flow path between the upstream side stream _ and the downstream side flow path 82 and a function of adjusting the conductance by operating the opening degree of the flow path. The switch valve body 31 has a poppet valve body 31, a valve seat 32, an elastic sealing member 33, and a bellows for sealing the sliding portion. By closing the valve seat 32 with the lifter_31, the elastic sealing member 33 can close the upstream side. The flow path 81 is between the flow path 81 and the downstream side flow path 82. The on-off valve 3A is operable to elevate the conductance between the upstream side flow path 81 and the downstream side flow path 82 as the rising rainbow (10) degrees of the distance between the valve body 31 and the valve seat 32. The direction of movement of the poppet valve body 31 is also referred to as the axial direction. The amount of rise L is an amount that can be displaced in the axial direction. The actuator 42 drives the poppet valve body 31 to operate the amount of lift L. The actuator 42 has an actuator body 43, a resin-made piston 49 as an insulator, a ceramic piston rod 44 connecting the piston 49 and the poppet valve body 31, a potential energy spring 46 for imparting potential energy to the piston 49, and a support The resin cylinder cover 45 is made of the potential spring 46. The piston 49 forms a cylindrical chamber 45 between the recess 4% formed inside the actuator body 43. A bellofram 49b is a member for sealing the cylindrical chamber 45, and is installed in a gap between the outer peripheral surface of the piston 49 and the inner peripheral surface of the cylindrical chamber 45. An operating air flow path 47 for supplying operating air from an electric air pressure control valve (not shown) is formed in the cylindrical chamber 45. The actuator 42 can control the poppet valve body 31 to an arbitrary position by operating the supply pressure of the actuating air from the electric air pressure control (not shown). The position of the poppet valve body 31 is the load and the load of the actuating air applied to the piston 49.

S 12 201231937 與勢能力平衡的位置為安定。這是因作動空氣於增大上升 里L之方向對活塞49施加載重,另一方面賦與勢能彈簧46 於縮小上升量L之方向對活塞49施加賦與勢能力之故。 第3圖係顯示第i實施形態之上升量感測器丨〇 〇之結構 的截面圖。第4圖係顯示第〖實施形態之上升量感測器1〇〇之 端部的外觀圖。第5圖係顯示第丨實施形態之上升量感測器 100之結構的示意圖。第6圖係顯示第丨實施形態之上升量感 測器100之對向電極之結構的立體圖。升量感測器1〇〇係 靜電容式變位感測器。 上升量感測器100係測量上升量L(參照第2圖)之感測 器。上升1感测器100包含有樹脂製之感測器本體60、具有 圓柱狀形狀之金屬製可動電極50、一對金屬製固定電極 、20、分別連接於一對固定電極1〇、2〇並貫穿感測器本 體6〇之-對端子71、72、密封端子71、72與感測器本體6〇 之連接之樹脂性密封部73。此外,一對固定電極1〇、2〇亦 稱為外側電極。可動電極50亦稱為圓柱電極。 "T動電極50在上升量感測器之内部,與上升量感測 器100之其他零件呈電性絕緣之狀態。具體言之,可動電極 50具有與樹脂製圓筒蓋45e滑動之滑動自,且裝設於樹脂製 活塞49與陶瓷製活塞桿44。此外,可動電極%只要在上升 量感測器100之内部為電性絕緣即可,亦可將例如樹脂製插 入構件等絕緣體裝設於活塞桿44等間,而與其他零件電性 絕緣。關於可動電極50電性絕緣之理由容後再述。 如第3圖及第4圖所示,感測器本體6〇以4根螺栓62裝設 13 201231937 於致動器42。於感’則器本體60形成有内腔面61。在内腔面 61,一對固定電極10、20以預定距離G隔開而裝設。預定距 離G可設定為不致於相對向之—對切斷端面15、25產生過度 之寄生電容(靜電容)的距離。寄生電容之容許量依據與檢測 對象之靜電容之比較而設定。此外,具有感測器本體6〇、 一對固定電極10、20及一對端子乃、π之組裝體亦稱為第2 構件。 如第5圖所示,於固定電極1〇之内部形成有端部壁面 11、對端部壁面11於垂直方向相連之圓柱狀圓柱壁面u、 對圓柱壁面12於垂直方向相連之外部端面13。於固定電極 2〇之内部形成有端部壁面21、對端部壁面21於垂直方向相 連之圓柱狀圓柱壁面22、對圓柱壁面册垂直方向相連: 外。P端面23。圓枉壁面12與圓柱壁面22配置於相對向之位 置”端壁面11、21共同形成圓柱狀内部空間Spl。 對固定電極10、20可例如以下般以機械加工製造。 可以下述—般之機械加工製造:首先以車床形成外形形 狀,接著,以臥式搪床形成端部壁面11、21及圓柱狀圓杈 壁面12、22 ’最後藉由切斷,形成切斷端面15、25。如此, 由於-對固定電極1G、2G可以機械加工形成外形,故可以 一般之步驟進行高精確度之製造。 圓枉狀内部空間Spl係可插入可動電極50之區域。可動 電極50以對一對固定電極1〇、20電性絕緣之狀態(非接觸狀 態)插入。可動電極5G以對E1定電極1G保持(5 1之隔開距離 之狀態插入。藉此,可動電極50構成具有對固定電極1〇可S 12 201231937 The position of balance with potential capacity is stability. This is because the moving air exerts a load on the piston 49 in the direction of increasing the rising L, and on the other hand, the potential energy spring 46 is biased to the piston 49 in the direction of decreasing the amount of rise L. Fig. 3 is a cross-sectional view showing the structure of the amount of rise sensor 丨〇 of the i-th embodiment. Fig. 4 is a view showing the appearance of the end portion of the lift amount sensor 1 of the first embodiment. Fig. 5 is a view showing the structure of the lift amount sensor 100 of the second embodiment. Fig. 6 is a perspective view showing the structure of the counter electrode of the amount-of-rising sensor 100 of the second embodiment. The up-and-down sensor 1 is a static capacitance type displacement sensor. The ascending amount sensor 100 is a sensor that measures the amount of rise L (refer to Fig. 2). The rise 1 sensor 100 includes a sensor body 60 made of resin, a metal movable electrode 50 having a cylindrical shape, a pair of metal fixed electrodes, 20, and a pair of fixed electrodes 1 and 2, respectively. A resinous sealing portion 73 that penetrates the sensor body 6 to the terminals 71, 72, the sealing terminals 71, 72, and the sensor body 6A. Further, a pair of fixed electrodes 1 〇, 2 〇 are also referred to as outer electrodes. The movable electrode 50 is also referred to as a cylindrical electrode. "T moving electrode 50 is electrically insulated from other parts of the rising amount sensor 100 inside the rising amount sensor. Specifically, the movable electrode 50 is slidably slidably fitted to the resin-made cylindrical cover 45e, and is attached to the resin-made piston 49 and the ceramic-made piston rod 44. In addition, the movable electrode may be electrically insulated from the inside of the lift sensor 100, and an insulator such as a resin insertion member may be mounted between the piston rod 44 or the like to be electrically insulated from other components. The reason why the movable electrode 50 is electrically insulated is described later. As shown in Figs. 3 and 4, the sensor body 6 is mounted on the actuator 42 by four bolts 62 13 201231937. The sensor body 60 is formed with an inner cavity surface 61. On the inner cavity surface 61, a pair of fixed electrodes 10, 20 are spaced apart by a predetermined distance G. The predetermined distance G can be set so as not to be relatively opposed to the excessive parasitic capacitance (static capacitance) of the cut end faces 15, 25. The allowable amount of parasitic capacitance is set in accordance with the comparison with the electrostatic capacitance of the object to be detected. Further, an assembly having a sensor body 6A, a pair of fixed electrodes 10, 20, and a pair of terminals, π is also referred to as a second member. As shown in Fig. 5, an end wall surface 11 is formed inside the fixed electrode 1A, a cylindrical cylindrical wall surface u which connects the end wall surface 11 in the vertical direction, and an outer end surface 13 which is connected to the cylindrical wall surface 12 in the vertical direction. An end wall surface 21 is formed inside the fixed electrode 2, and a cylindrical cylindrical wall surface 22 which is connected to the end wall surface 21 in the vertical direction is connected to the cylindrical wall sheet in the vertical direction: P end face 23. The cylindrical wall surface 12 and the cylindrical wall surface 22 are disposed at opposite positions, and the end wall surfaces 11 and 21 together form a cylindrical internal space Spl. The fixed electrodes 10 and 20 can be mechanically manufactured, for example, as follows. Processing and manufacturing: First, the outer shape is formed by a lathe, and then the end wall faces 11, 21 and the cylindrical circular wall faces 12, 22' are formed by a horizontal boring machine, and finally the cut end faces 15, 25 are formed by cutting. Since the fixed electrodes 1G and 2G can be machined to form an outer shape, high-precision manufacturing can be performed in a general procedure. The circular-shaped internal space Spl can be inserted into the region of the movable electrode 50. The movable electrode 50 is opposed to a pair of fixed electrodes 1〇, 20 electrically insulated state (non-contact state) is inserted. The movable electrode 5G is held in the state in which the E1 fixed electrode 1G is held (the distance of 5 1 is separated. Thereby, the movable electrode 50 is configured to have the pair of fixed electrodes 1) can

S 14 201231937 :照二量二而對向面積變動之對向面的靜電容C1的電容 益。可動電極50以對固定電極聰持 電合 插入。葬此,可#乏&開距離之狀態 祕了動電極5〇構成具有對固定電極20可按昭上 升量L而對向面積變動之對向面的靜電容_電容器Γ 形成於固定電極10與可動電極5〇間之靜電° =由作為導體之可動電極5Q,與形成於可動電^ 定電極20間之靜電容C2的電容器串聯。另 :口 極H)與較電極20分別電性連接於端子71與端子 此,於一對端子71與端子72間產生作為靜電容C1之電容器 與靜電谷C2之電容器串聯的電容器之靜電容。 於内部空間Spl,為了增大檢測對象之靜電容以提高 SN比’㈣人有介電流體。介電流體係指介電性優於導電 性之流體,例如可利用非壓縮性氟系惰性流體。«惰性 流體具有優異之魏祕及熱雜。由於«惰性流體黏 度小’故具有可減低因隨著外側電極與圓柱電極之相對移 動之流動而引起的負荷之特徵。 於可動電極5〇形成有4個介電流體通過孔53(圖中僅顯 示3個)。介電流體通過孔„係於可動電極%在内部”spi 之内部移動之際,供封人_部空間Spl之介電流體流動之 貫穿孔。具體言之,上升量L增大時,介電流體通過4個介 電流體通過孔53,從内部空間Spl排出。另一方面,上升量 L縮小時’介電越通過4個介電流體制㈣,而被供給 至内部空間Spl。 如第1圖及第2圖所示,於可動電極5〇之内部形成有用 15 201231937 以貯存介電流體之貯存圓筒室55(參照第2圖)。於儲存圓筒 室55構造成裝設有貯存用活塞52,而使貯存圓筒室μ之内 容量為可變。於貯存圓筒室55連通有形成於活塞桿44之内 部之内部孔44h。於内部孔44h形成有在軸方向具有長軸之 長孔狀連通孔48h,而與排氣流路48連通,實現了貯存用舌 塞52之平順之移動。此外,可動電極5〇與貯存用活塞u 組裝體亦稱為第1構件。 土 之 第7圖顯示概念地表示上升量感測器1〇〇之靜電容▲ 算式。計算式F1係靜電容之定義式。計算式打係表示之= 動電極50與固定電極1〇間之對向面產生之靜電容的於y 式。此外,計算式!?2為了易理解說明,而微小化(離散彳十算 而將各部份作為平面來處理。 化), 靜電容ci係以介電常數ε與對向面積s之積除以s 距離dl之值而算出。對向面積S因應上升量L而變動。隔開 式F3係表示於可動電極50與固定電極20間之對向面十算 靜電容的計算式。靜電容C2係以介電常數£與對向生之 之積除以隔開距離d2之值而算出。對向面積s因應 而變動 計算式F4係用以算出串聯之2個靜電容^、C2 、 電容C的定義心上升量感測器丨湖用—對端子 之複合電容C之變化,測量上升量L。這是因複合電容^ 前述,為作為串聯靜電容C1之電容器與靜電容C2之 如 之電容器的複合電容c之故。 容器 計算式F4係將被2個固定電極1〇包失之可動電極$ 201231937 構造、串聯之2個靜電gC1、C2作為等姝電路。此等效電 路如前述係在以可動電極5 〇與上升量感測器10 0之其他零 件電性絕緣為前提下成立者。具體言之,設想一間早例係 可動電極50電性接地,固定電極2〇係接地側之電位時,由 於固定電極20與可動電極5〇間之靜電容C2失效,故形成為 不同之電路。惟,可動電極5〇不需一直為電性絕緣,至少 於測量時絕緣即可。 計算式F5係用以算出靜電容C1之電容器與靜電容C2 之電容器之複合電容c的計算式。2個隔開距離dl、d2以標 稱值(名目值)<5 n與上升量感測器1〇〇之製造公差而算出。製 造公差主要係作為可動電極50與固定電極1〇之組裝誤差之 偏心量<5。 標稱值占η係相對向之一對圓柱壁面12、22之内徑與可 動電極50之外形之差。即,作為組裝誤差之偏心量占不存 在時’相當於可動電極5〇與固定電極1〇之隔開距離之2倍或 可動電極50與固定電極20之隔開距離之2倍的值。 計算式F6係以標稱值5 η與偏心量5表示可動電極5〇 與固定電極10之隔開距離dl之式。隔開距離dl以標稱值占η 與偏心量5之和來算出。關於隔開距離dl,表示可動電極 50與固定電極1〇之偏心於隔開距離變大之方向產生。 另一方面,計算SF7係將可動電極5〇與固定電極2〇之 隔開距離d2以標稱值s n與偏心量5之差而算出。關於隔開 距離d2,由於固定電極2〇配置於隔著可動電極%,與固定 電極10對向之位置,故可動f極5G與©定電極2G之偏心^ 201231937 隔開距離變小之方向產生。 計算式F8係將以計算式別、F7算出之2個隔開距離d 1、 d2代入算出複合電容C之計算式F5之計算式。在計算式F8, 可知偏心量<5被抵銷,而可以標稱值$ η、對向面積S及介 電常數ε,算出複合電容C。即,可知,複合電容c在計算 上不受偏心量5影響。此種效果係如前述,因上升量感測 器100構造成可動電極50與感測器100之其他零件電性絕緣 而可奏效者。 第8圖係顯示按照可動電極50與一對固定電極1 〇、20之 上升量L之複合電容C的實測值之圖表。理論值係顯示為表 示上升量L與對向面積S之關係為線形之直線。這是因對向 面積S作為一對固定電極10、20之圓周方向之長度的總合與 上升量L之積,而決定其變動量之故。實測值顯示上升量[ 與複合電容C(靜電容)為線形。 如此,由於上升量感測器100於上升量匕與複合電容C 間具有線形性,故具有適合作為感測器之特性。再者,上 升量感測器100顯示理論上變位量無限制。這是因可動電極 50與一對固定電極10、20—面維持感測器之線形性,一面 於軸方向自由地延長在理論上為可行之故。 第9圖係顯示因可動電極50與一對固定電極1〇、2〇之偏 心引起之測量誤差(實測值)的圖表。此圖表係表示相對於偏 心量5之複合電容C的靈敏度分析之圖表。此圖表係就偏心 量<5不存在之狀態、偏心量5存在於距離G之間隙之方向之 狀態(切口側)及偏心量(5存在於與距離G之間隙之方向垂S 14 201231937 : The capacitance of the static capacitance C1 on the opposite side of the change in the area of the opposite direction. The movable electrode 50 is inserted into the fixed electrode. In this case, the state of the open electrode can be set to the fixed electrode 10, which has a static capacitance to the opposite surface of the fixed electrode 20 which can vary in the opposing area by the amount of rise L. The static electricity between the movable electrode 5 and the movable electrode 5 is connected in series with a capacitor of the movable electrode 5Q as a conductor and a capacitor C2 formed between the movable electrode 20. Further, the port H) and the counter electrode 20 are electrically connected to the terminal 71 and the terminal, respectively, and a static capacitance of a capacitor which is a capacitor of the capacitor C1 and a capacitor of the electrostatic valley C2 is generated between the pair of terminals 71 and 72. In the internal space Spl, in order to increase the electrostatic capacitance of the detection object to increase the SN ratio, the human has a dielectric fluid. The dielectric current system refers to a fluid having a dielectric property superior to that of conductivity, and for example, an incompressible fluorine-based inert fluid can be used. «Inert fluids have excellent mystery and heat. Since «the viscosity of the inert fluid is small", it is characterized in that the load due to the flow of the relative movement of the outer electrode and the cylindrical electrode can be reduced. Four dielectric fluid passage holes 53 are formed in the movable electrode 5 (only three are shown in the figure). When the dielectric fluid passes through the hole „ inside the movable electrode% inside the inside spi, the through hole for the flow of the dielectric body of the human space Spl is sealed. Specifically, when the amount of rise L is increased, the dielectric fluid passes through the holes 53 through the four dielectric bodies, and is discharged from the internal space Spl. On the other hand, when the amount of increase L is reduced, the dielectric is supplied to the internal space Spl as it passes through the four dielectric current systems (4). As shown in Fig. 1 and Fig. 2, a storage cylinder chamber 55 (see Fig. 2) for storing a dielectric fluid is formed inside the movable electrode 5A. The storage cylinder chamber 55 is configured to be provided with a storage piston 52 so that the capacity inside the storage cylinder chamber μ is variable. An inner hole 44h formed in the inner portion of the piston rod 44 is communicated with the storage cylinder chamber 55. The inner hole 44h is formed with a long hole-shaped communication hole 48h having a long axis in the axial direction, and communicates with the exhaust flow path 48, thereby achieving smooth movement of the storage tongue plug 52. Further, the movable electrode 5A and the storage piston u assembly are also referred to as a first member. Figure 7 of the soil shows the static capacitance ▲ formula conceptually representing the amount of rise sensor. The calculation formula F1 is a definition of static capacitance. The calculation type indicates that the static capacitance generated by the opposing surface between the movable electrode 50 and the fixed electrode 1 is in the y formula. In addition, the calculation formula!? 2 is easy to understand and the description is miniaturized (discrete 彳 ten counts and treat each part as a plane), and the static capacitance ci is divided by the product of the dielectric constant ε and the opposing area s. Calculated by the value of s distance dl. The opposing area S varies depending on the amount of rise L. The partition type F3 is a calculation formula for calculating the static capacitance of the opposing surface between the movable electrode 50 and the fixed electrode 20. The static capacitance C2 is calculated by dividing the product of the dielectric constant £ and the opposite direction by the value of the separation distance d2. The variation of the opposing area s is calculated. The calculation formula F4 is used to calculate the difference between the two capacitors ^, C2 and the capacitor C in series. The core rise amount sensor is used to measure the rise of the composite capacitor C of the terminal. . This is because the composite capacitor ^ is the composite capacitor c of the capacitor of the series capacitor C1 and the capacitor C2. Container The calculation formula F4 is an isoelectric circuit in which two static electricitys gC1 and C2 which are connected by the movable electrode $201231937 and are connected in series by the two fixed electrodes 1 . The equivalent circuit is established as described above on the premise that the movable electrode 5 is electrically insulated from the other components of the lift amount sensor 100. Specifically, it is assumed that an early movable electrode 50 is electrically grounded, and when the potential of the fixed electrode 2 is grounded, the static capacitance C2 between the fixed electrode 20 and the movable electrode 5 is disabled, so that a different circuit is formed. . However, the movable electrode 5〇 does not need to be always electrically insulated, and at least it can be insulated during measurement. The calculation formula F5 is a calculation formula for calculating the composite capacitance c of the capacitor of the capacitor C1 and the capacitor of the capacitor C2. The two separation distances d1 and d2 are calculated by the nominal value (name value) < 5 n and the manufacturing tolerance of the amount of rise sensor 1〇〇. The manufacturing tolerance is mainly the eccentric amount <5 as the assembly error of the movable electrode 50 and the fixed electrode 1〇. The nominal value is the difference between the inner diameter of one of the pair η relative pairs and the outer diameter of the cylindrical wall faces 12, 22 and the outer shape of the movable electrode 50. In other words, when the eccentricity of the assembly error is not present, the value corresponds to twice the distance between the movable electrode 5A and the fixed electrode 1A or twice the distance between the movable electrode 50 and the fixed electrode 20. The calculation formula F6 is expressed by the nominal value 5 η and the eccentric amount 5 indicating the distance dl between the movable electrode 5 〇 and the fixed electrode 10 . The separation distance dl is calculated by the sum of the nominal value η and the eccentricity amount 5. The separation distance d1 indicates that the eccentricity of the movable electrode 50 and the fixed electrode 1〇 is generated in a direction in which the separation distance becomes large. On the other hand, the calculation SF7 calculates the distance d2 between the movable electrode 5A and the fixed electrode 2A by the difference between the nominal value s n and the eccentric amount 5. In the separation distance d2, since the fixed electrode 2 is disposed at a position opposed to the fixed electrode 10 via the movable electrode %, the distance between the movable f pole 5G and the eccentricity of the fixed electrode 2G is reduced in the direction of the distance of 201231937. . The calculation formula F8 is substituted into the calculation formula of the calculation formula F5 of the composite capacitor C by the two separation distances d 1 and d2 calculated by the calculation formula and F7. In the calculation formula F8, it is understood that the eccentric amount <5 is offset, and the composite capacitor C can be calculated from the nominal value $η, the opposing area S, and the dielectric constant ε. That is, it can be seen that the composite capacitor c is not affected by the eccentricity amount 5 in calculation. This effect is as described above, since the rise amount sensor 100 is constructed such that the movable electrode 50 is electrically insulated from other parts of the sensor 100. Fig. 8 is a graph showing measured values of the composite capacitor C in accordance with the amount of rise L of the movable electrode 50 and the pair of fixed electrodes 1 and 20. The theoretical value is shown as a straight line indicating that the relationship between the amount of rise L and the area of the opposite direction S is linear. This is because the opposing area S is the product of the total length of the pair of fixed electrodes 10 and 20 in the circumferential direction and the amount of rise L, and the amount of change is determined. The measured value shows the amount of rise [and the composite capacitor C (static capacitance) is linear. As such, since the amount of rise sensor 100 has linearity between the amount of rise 匕 and the composite capacitor C, it has characteristics suitable as a sensor. Furthermore, the lift sensor 100 shows that there is no limit to the theoretical amount of displacement. This is because the movable electrode 50 and the pair of fixed electrodes 10, 20 are used to maintain the linearity of the sensor, and it is theoretically possible to freely extend in the axial direction. Fig. 9 is a graph showing measurement errors (measured values) due to the eccentricity of the movable electrode 50 and the pair of fixed electrodes 1 〇 and 2 。. This graph is a graph showing the sensitivity analysis of the composite capacitor C with respect to the eccentricity amount 5. This graph is a state in which the eccentricity amount <5 does not exist, the state in which the eccentric amount 5 exists in the direction of the gap G (the slit side), and the eccentric amount (5 exists in the direction of the gap with the distance G).

S 201231937 直的方向之狀態(無切口側)之3個狀態,比較實測值。在此 實驗例中,標稱值(5η為200μηι。 如此,發明人成功確認至少即使產生一般之製造公差 程度之偏心,亦不致對複合電容C造成影響。本實驗更具有 對相對於偏心方向之複合電容C之影響的靈敏度分析之意 義。本靈敏度分析係用以利用於外側電極之分割數增加之 必要性或決定分割形狀之最適當值者。 然而,由於根據本實驗,可確認若為一般之製造公差 程度,即使偏心產生於任一方向,亦幾乎不致對複合電容C 造成影響,故確認了分割數為2個便足夠。具體言之,例如 當切口側之偏心比無切口側之偏心對複合電容C造成較大 之影響時,為縮小真空控制閥40之測量值之個體差,亦需檢 討增加切口(距離G)之數或調整位置。然而,由於若為一般 之製造公差程度時,即使於任一方向產生偏差,亦幾乎不對 複合電容C造成影響,故從實用性之觀點確認了不需檢討。 根據上述解析及實驗,可知:以包含作為測量對象之 提動閥體31之變位之方向的平面,大致均等地分割為二而 相對向之一對電極係較佳之形態。這是因為以包含測量對 象之變位之方向的平面分割時,固定電極10側之電容器與 固定電極20側之電容器的電容比,由於不因測量對象移動 而受到影響,故可確保變位與複合電容C之關係之線形性之 故。這是因下述之故,即,若大致均等地分割為二而相對 向時,可使以固定電極10側之電容器與固定電極20側之電 容器之串聯形成的複合電容C為最大值。 19 201231937 本實施形態可發揮以下之效果。 (1) 上升量感測器10 0解決在靜電容式感測器可測量之 變位量(上升量L之最大值)與對向電極之組裝容許公差(偏 心量δ)之取捨問題,因此,具有作為感測器理想之線形特 性。 (2) 上升量感測器100具有作為圓柱電極之可動電極50 與作為外側電極之一對固定電極10、20之任一者皆可以一 般之機械加工實現精密之形狀與尺寸的形狀。 (3) 上升量感測器100由於對向電極以物理方式非接觸 地對向配置,故具有不易使歷時劣化產生之特徵。 此外,第1實施形態不限於上述内容,亦可如下般實施。 (1) 在上述實施形態中,外側電極以機械零件構成,但 亦可例如於形成於感測器本體60之内腔面61以金屬膜沉積 形成。若如此進行時,由於對向面積顯著地縮小,故可縮 小距離G,而使測量對象之對向面積增加。外側電極亦可令 感測器本體60為耐熱樹脂,於金屬電極之周圍注入樹脂, 以插入成型而製造為一體。再者,外側電極亦可以於内腔 面61嵌入金屬加壓零件之夾構造來製造。如此,外側電極 具有廣義之含意,只要為具有於圓周方向分割,且相對向 之至少一對電極者即可。 (2) 在上述實施形態中,構成為使用分割為二之一對外 側電極,亦可分割成例如3個以上。如此,可在本發明使用 之外側電極只要為構成圓筒狀且於圓周方向分割之一組外 側電極即可。惟,如上述分割為二之一對外側電極為最簡S 201231937 Three states of the straight direction (no slit side), comparing the measured values. In this experimental example, the nominal value (5η is 200μηι. Thus, the inventors succeeded in confirming that at least the eccentricity of the general manufacturing tolerance is not affected by the composite capacitor C. This experiment has more opposition to the eccentric direction. The significance of the sensitivity analysis of the influence of the composite capacitor C. The sensitivity analysis is used for the necessity of increasing the number of divisions of the outer electrode or determining the optimum value of the split shape. However, according to the experiment, it can be confirmed that The degree of manufacturing tolerance is such that even if the eccentricity is generated in either direction, the composite capacitor C is hardly affected, so it is confirmed that the number of divisions is two. Specifically, for example, when the eccentricity of the slit side is smaller than the eccentricity of the non-cut side In the case of a large influence on the composite capacitor C, in order to reduce the individual difference of the measured values of the vacuum control valve 40, it is also necessary to review the number of increments (distance G) or the adjustment position. However, since it is a general manufacturing tolerance level Even if there is a deviation in either direction, it hardly affects the composite capacitor C, so it is confirmed from the practical point of view that it is not necessary. According to the above analysis and experiment, it is understood that the plane including the direction of the displacement of the poppet valve body 31 as the measurement target is substantially equally divided into two, and is preferably in the form of a pair of counter electrode systems. When the plane is divided by the plane including the direction of the displacement of the measuring object, the capacitance ratio of the capacitor on the side of the fixed electrode 10 and the capacitor on the side of the fixed electrode 20 is not affected by the movement of the measuring object, so that the displacement and the composite capacitor C can be ensured. The linearity of the relationship is caused by the fact that the capacitors on the side of the fixed electrode 10 and the capacitor on the side of the fixed electrode 20 can be formed in series when they are substantially equally divided into two. The composite capacitor C has the maximum value. 19 201231937 This embodiment can achieve the following effects: (1) The amount of rise sensor 10 solves the amount of displacement (maximum amount of rise L) that can be measured in the capacitive sensor The assembly tolerance tolerance (eccentricity δ) of the counter electrode is a problem, and therefore has a linear characteristic as a sensor. (2) The rise amount sensor 100 has a cylindrical electrode The movable electrode 50 and any one of the fixed electrodes 10 and 20 as one of the outer electrodes can be mechanically machined to achieve a precise shape and size. (3) The rise amount sensor 100 is physically non-oriented due to the counter electrode The first embodiment is not limited to the above, and may be implemented as follows. (1) In the above embodiment, the outer electrode is made of a mechanical component, but For example, it may be formed by depositing a metal film on the inner cavity surface 61 formed on the sensor body 60. If this is done, since the opposing area is significantly reduced, the distance G can be reduced, and the opposing area of the measuring object can be increased. The outer electrode may also be such that the sensor body 60 is a heat-resistant resin, and a resin is injected around the metal electrode to be integrally molded by insert molding. Further, the outer electrode may be fabricated by inserting a sandwich structure of the metal pressurizing member on the inner cavity surface 61. As described above, the outer electrode has a broad meaning, and it is only required to have at least one pair of electrodes which are divided in the circumferential direction and opposed to each other. (2) In the above embodiment, the external electrode is divided into two, and may be divided into, for example, three or more. As described above, the outer electrode which can be used in the present invention may be formed into a cylindrical shape and divided into a group of outer electrodes in the circumferential direction. However, as described above, it is divided into two, and the outer electrode is the simplest.

S 20 201231937 易之結構,具有減少距離G,而實現對向面積之增大,亦可 藉由配線之刪減,使雜散電容減低之優點。 (3) 在上述實施形態中,圓柱電極(在實施例為可動電 極50)形成端部,但亦可如第1變形例(參照第10圖),將圓柱 電極設於可動部份之中間位置(例如圓柱構件51與活塞桿 44間)。在第1變形例中,於可動電極50a之端部以螺栓56裝 設有樹脂製圓柱構件51。圓柱構件係於形成有陰螺旋之插 入構件54之周圍注入樹脂而以插入成型構成之零件。貫穿 孔51h係用以按照圓柱構件51之移動,進行供氣排氣之孔。 本結構具有介電流體不需按照測量對象之變位而流動 之優點。如此,圓柱電極不需裝設於測量對象之端部,亦 可裝設於致動器42與閥本體41間或致動器42之内部。再 者,亦可為以一對測量對象夾持圓柱電極之結構。 (4) 在上述實施形態中,為使SN比較高,而利用了介 電流體,但介電流體未必為必須之結構。惟,使用介電流 體,並假設介電流體之大幅溫度變化時,宜補償因介電流 體之溫度變化而引起之介電常數之變化。具體言之,宜為 例如進行介電流體之溫度測量而補正之結構或後述之第2 變形例之結構。 第11圖係顯示介電常數因應介電流體之溫度而變化之 態樣的圖表。線E2係顯示介電流體之溫度與介電常數之關 係的線。介電常數係當例如介電流體之溫度從0度上升至 100度時,會下降變動量Ea。介電常數之變化當例如在溫度 〇度,進行靜電容與上升量之校正時,在溫度0度,會產生 21 201231937 因相當於變動量Ea之介電常數變化而引起之誤差。 如第12圖所示,第2變形例在外側電極之外部具有用以 補償因介電常數變化而引起之誤差的補償用電容器此點與 上述實施形態不同。補償用電容器係將共通之介電流體作 為介電體,且與一對固定對向電極91a、91b之固定對向電 極隔開距離固定之電容器。於固定對向電極91a、9 lb分別 電性連接有不同之端子(省略圖示)。 一對固定對向電極91a、9lb配置於一對固定電極10、 20之外周方向(外側),且裝設於被分割之一對感測器本體 60al、60a2間。一對固定對向電極91a、91b皆具有直徑相 互不同之環狀形狀,且共有中心軸線。一對固定對向電極 91a、91b間之空間通過連通孔92、93,連通於内部空間Spl。 藉此,介電流體可填滿内部空間Spl與固定對向電極91a、 91b間之空間。 補償用電容器以與外側電極或圓柱電極電性分離之狀 態裝備,而不致對端子71、72間之靜電容造成影響。由於 補償用電容器可藉由實測其靜電容而觀測介電常數,故可 使用所觀測之介電常數,測量變位量。藉此,可在不使測 量對象之變位方向之尺寸過大下,安裝補償用電容器,而 可補償因介電常數之變化而引起之測量變位的誤差。 (5)在上述實施形態十,利用與控制對象之流體不同之 流體作為介電流體,亦可如第3變形例(參照第13圖),利用 控制對象之流體作為介電流體。若如此進行時,可不設用 以使用介電流體之專用流路或儲存槽,而簡易地使用介電S 20 201231937 Easy structure, which has the advantage of reducing the distance G and increasing the opposing area, and also reducing the stray capacitance by eliminating the wiring. (3) In the above embodiment, the cylindrical electrode (in the embodiment, the movable electrode 50) is formed with an end portion. However, as in the first modification (see Fig. 10), the cylindrical electrode may be disposed in the middle of the movable portion. (for example, between the cylindrical member 51 and the piston rod 44). In the first modification, a resin cylindrical member 51 is attached to the end portion of the movable electrode 50a by a bolt 56. The cylindrical member is a member formed by inserting and molding a resin by injecting a resin around the insertion member 54 in which the female screw is formed. The through hole 51h is for performing a hole for supplying air and exhaust according to the movement of the cylindrical member 51. This structure has the advantage that the dielectric fluid does not need to flow in accordance with the displacement of the measuring object. Thus, the cylindrical electrode does not need to be installed at the end of the measuring object, and may be installed between the actuator 42 and the valve body 41 or inside the actuator 42. Further, it is also possible to adopt a structure in which a cylindrical electrode is sandwiched by a pair of measuring objects. (4) In the above embodiment, a dielectric fluid is used to make the SN relatively high, but the dielectric fluid is not necessarily required. However, when a dielectric fluid is used and a large temperature change of the dielectric fluid is assumed, it is desirable to compensate for the change in dielectric constant due to the temperature change of the dielectric fluid. Specifically, for example, a structure for correcting the temperature of the dielectric fluid or a structure of the second modification described later is preferable. Fig. 11 is a graph showing a state in which the dielectric constant changes in response to the temperature of the dielectric fluid. Line E2 is a line showing the relationship between the temperature of the dielectric fluid and the dielectric constant. The dielectric constant decreases when the temperature of the dielectric fluid rises from 0 to 100 degrees, for example. When the change in the dielectric constant is corrected for the electrostatic capacitance and the rising amount, for example, at a temperature of 0 degrees, an error caused by a change in the dielectric constant corresponding to the variation Ea is generated at 21 201231937. As shown in Fig. 12, the second modification differs from the above embodiment in that a compensation capacitor for compensating for an error due to a change in dielectric constant is provided outside the outer electrode. The capacitor for compensation is a capacitor in which a common dielectric current is used as a dielectric and is fixed to a fixed counter electrode of the pair of fixed counter electrodes 91a and 91b. Different terminals (not shown) are electrically connected to the fixed counter electrodes 91a and 91b, respectively. The pair of fixed counter electrodes 91a and 9lb are disposed in the outer circumferential direction (outer side) of the pair of fixed electrodes 10 and 20, and are disposed between the paired sensor bodies 60a1 and 60a2. Each of the pair of fixed counter electrodes 91a, 91b has an annular shape different in diameter from each other and shares a central axis. The space between the pair of fixed counter electrodes 91a, 91b is communicated with the internal space Sp1 through the communication holes 92, 93. Thereby, the dielectric fluid can fill the space between the internal space Spl and the fixed counter electrodes 91a, 91b. The compensating capacitor is equipped in a state of being electrically separated from the outer electrode or the cylindrical electrode without affecting the electrostatic capacitance between the terminals 71, 72. Since the compensation capacitor can observe the dielectric constant by measuring its electrostatic capacitance, the observed dielectric constant can be used to measure the displacement. Thereby, the compensation capacitor can be mounted without making the size of the measurement object in the displacement direction too large, and the error of the measurement displacement due to the change in the dielectric constant can be compensated. (5) In the tenth embodiment, a fluid different from the fluid to be controlled is used as the dielectric fluid, and the fluid to be controlled may be used as the dielectric fluid in the third modification (see Fig. 13). If this is done, it is not necessary to use a dedicated flow path or storage tank for the dielectric fluid, and the dielectric is simply used.

S 22 201231937 第3變形例係將本發明應用於 動之比例控制閥的線軸閥4 〇 c之 '作為控制介電流體之流 44a '套筒57及可動電極5此 例。線軸閥40c具有線軸 58,以固緊構件59裝設於線軸^動電極5此藉由絕緣構件 絕緣構件58在線軸閥4〇c之内邛絕这。由於可動電極5〇1)藉由 金屬材料作為線軸44a之材料,粂故亦可使用為導體之 在本說明書中,比例控㈣具^^4之選擇項目廣。此外, 可測量閥開度而反饋者即可,例f義之含意’例如只要為 合閥。 彳如亦包含控制混合比之混 第3變形例之線軸閥恢在第 .^ , τ 顯不綠釉44a最接 近疋電極1G、2G側之狀態°在此狀態下,介電流體之流 路從形成於_4&之作為流路的凹部他,透過套筒57之 開口部57h之連通,連接於流路之下游之開口部咖。此流 路當線轴44a離開固定電極1()、2()側_,便失去凹部44油與 開口部57h之連通而為封閉。一對固定對向電極91。、训之 端部面向此流路。 一對固定對向電極91c、91d裝設於形成於第3變形例之 感測器本體60b之凹部91e。於一對固定對向電極91c、91d 間存在介電流體可流入之間隔,由於流入與固定電極1〇、 20與可動電極5〇b間之介電流體相同之介電流體,故與第2 變形例同樣地,可利用作為補償用電容器。固定對向電極 91c、91d具有介電流體可不停滯地流入其間之優點,及僅 於感測器本體60b形成凹部9le ’便可裝備補償用電容器之 23 201231937 優點。 ⑹在上述實施形態中 動,作亦可爐m 圓柱電極側與測量對象-同移 勁仁亦了構造成外側電極 亦可構造成兩者移動。在本發;;^象—同㈣’或者’ 側電極隨著測量對象之變 為®柱電極及外 , ㈣地移動,至少一對外側 電極相互間之靜電容因肋移㈣化者即可。 門之(1 在上述實施形態中,舉了真空控制之閥體或線軸 由之移動量為測量對象之例來說明,但可應用於例 如具有稱从合閥之其他種類之閥或稱為致動器之以直線 狀變位(移動)之要件的機械零件。 第2實施形態 接著,一面參照圖式,-面說明具體實現本發明之第2 實施形態。在本實施形態中,具體實現在半導體裝置等製 造線使用之線軸閥。 第14圖係顯示第2實施形態之線軸閥之感測器設置側 之截面圖’(a)、(b)分別顯示線軸配置於不同之位置之狀 態。首先,依據第14(a)圖,說明線軸閥。 線軸閥200包含有閥本體部201、檢測線軸位置之感測 器部221。閥本體部201具有閥體202,該閥體2〇2為以不鏽 鋼等金屬材料形成之筒狀,且具有垂直相交於中心軸線之 截面形成圓形之中空部。於閥體202設有連通於該中空部之 流入口 203及流出口 204。 於閥體202之中空部設有套筒205。套筒205亦與閥體 202相同,為以不鏽鋼等金屬材料形成之筒狀。在套筒205,S 22 201231937 The third modification is an example in which the present invention is applied to the spool valve 4 〇 c of the proportional proportional control valve as the flow 44a of the control dielectric fluid 44a and the movable electrode 5. The bobbin valve 40c has a bobbin 58, which is attached to the bobbin movable electrode 5 by the fastening member 59. This is eliminated by the insulating member insulating member 58 in the bobbin case 4c. Since the movable electrode 5〇1) is made of a metal material as the material of the bobbin 44a, it can also be used as a conductor. In the present specification, the proportional control (four) has a wide selection of items. In addition, the valve opening degree can be measured and the feedback can be made, for example, the meaning of the meaning 'for example, as long as the valve is closed. For example, the spool valve of the third modified example of controlling the mixing ratio is restored to the state of the first, τ, and the green glaze 44a is closest to the side of the 疋 electrode 1G, 2G. In this state, the flow path of the dielectric fluid From the recess formed as a flow path in _4&, it is connected to the opening portion downstream of the flow path through the communication of the opening 57h of the sleeve 57. When the spool 44a is separated from the fixed electrode 1 () and the 2 () side, the flow of the recess 44 oil and the opening 57h are lost. A pair of fixed counter electrodes 91. The end of the training is oriented to this flow. The pair of fixed counter electrodes 91c and 91d are attached to the concave portion 91e formed in the sensor body 60b of the third modification. Between the pair of fixed counter electrodes 91c and 91d, there is a gap in which the dielectric fluid can flow in, and the dielectric fluid is the same as the dielectric fluid flowing between the fixed electrodes 1 and 20 and the movable electrode 5〇b. Similarly, the modification can be utilized as a compensation capacitor. The fixed counter electrodes 91c, 91d have the advantage that the dielectric fluid can flow in without stopping, and the capacitor body can be equipped with the compensation capacitor only when the concave portion 9e' is formed in the sensor body 60b. (6) In the above embodiment, the cylindrical electrode side of the furnace m and the measuring object may be moved to the same side as the outer electrode. In the present invention; ^^--(4)' or 'side electrode as the measuring object becomes the column electrode and (4) the ground moves, at least the pair of outer electrodes can be moved by the ribs (four) . (1) In the above embodiment, the valve body or the bobbin of the vacuum control is described as an example of the measurement target, but it can be applied to, for example, a valve of another type having a valve. In the second embodiment, the second embodiment of the present invention will be specifically described with reference to the drawings, and the second embodiment of the present invention will be specifically described. A spool valve used in a manufacturing line such as a semiconductor device. Fig. 14 is a cross-sectional view showing the sensor installation side of the spool valve of the second embodiment, (a) and (b) showing states in which the bobbins are disposed at different positions. First, the spool valve will be described based on Fig. 14(a). The spool valve 200 includes a valve body portion 201 and a sensor portion 221 for detecting the position of the bobbin. The valve body portion 201 has a valve body 202, and the valve body 2〇2 is The tubular body formed of a metal material such as stainless steel has a hollow portion having a circular cross section perpendicular to the central axis. The valve body 202 is provided with an inflow port 203 and an outflow port 204 communicating with the hollow portion. Hollow part A sleeve 205. The sleeve 205 is also the same as the valve body 202, a cylindrical shape and formed of a metal material such as stainless steel. In the sleeve 205,

S 24 201231937 於設有前述閥體202之流入口 203及流出口 204之位置設置 流通環狀溝2〇6a、206b及流通孔2〇7a、207b,透過該流通 環狀溝2〇6a、206b及流通孔207a、207b,與套筒205之中空 部連通。 套筒205之中空部形成圓筒,於此收容有線軸211。線 軸211其軸線與圓筒之轴線一致,滑動部212以對圓筒内面 滑動之狀態,可沿圓筒之軸線移動之方式而設。此外,使 線軸211移動之致動器(省略圖示)可適宜使用如第1實施形 態之氣壓式裝置或使用螺線管之裝置等眾所皆知之技術。 於線軸211除了形成有於圓筒内面滑動之前述滑動部 212 ’尚形成有環狀凹部213。如圖所示,令線軸211配置於 與感測器部221相反之側之移動端的狀態為第丨位置。在此位 置’以線軸211之滑動部212,堵住套筒205之流通孔207b。 因此,供給至流入口 203之流體不致從流出口 2〇4流出。 另一方面,令線軸211從前述第1位置移動,而配置於 感測器部221侧之移動端之狀態為第2位置。第14(b)圖顯示 此狀態。如圖所示,對應於流入口 203之流通環狀溝2〇6a、 對應於流出口 204之流通環狀溝206b透過流通孔2〇7a、2〇7b 及環狀凹部213而連通。因此,供給至流入口 2〇3之流體從 流出口 204流出。 返回第14(a)圖’前述感測器部221設於閥本體部2〇1之 一端側。感測器部221具有延長前述閥體2〇2而形成筒狀之 感測器體222。感測器體222之開口端部以形成平板狀之堵 塞構件223堵塞。堵塞構件223以氧化紹等具有電絕緣性之 25 201231937 材料形成。 感測器體222之中空部(堵塞構件223與套筒205之端部 間之空間)作為感測器設置空間224,於此設有由與上述第1 實施形態之上升量感測器100相同之結構構成之感測器。亦 即,作為外側電極之一對固定電極225、226設於封閉構件 223。又’作為圓柱電極之可動電極227於線軸211之端部以 絕緣構件214介在其間之狀態安裝。 在感測器設置空間224内,存在從套筒2〇5與線轴211間 漏出之控制對象之流體’此流體具有作為介電流體之功 月&。k者線轴211之移動’如第14(b)圖所示,可動電極2 2 7 進入以一對固定電極225、226形成之圓柱狀内部空間Sp2。 此時’透過形成於線軸211之貫穿孔215,内部空間Sp2内之 流體往相反側流通。藉此可動電極227之進入,可動電極227 與固定電極225、226之對向面積變動。藉由把握因此面積 變動所引起之靜電容之變化,可檢測線軸211之位置。 再度返回第14(a)圖’於一對固定電極225、226設有分 別作為導電部之電極端子225a、226a。電極端子225a、226a 貫穿堵塞構件223,於線軸211之移動方向延伸,而露出至 感測器設置空間224外。於電極端子225a、226a之突出端部 安裝有作為電路基板之感測器基板231。感測器基板231以 氧化鋁或合成樹脂等具有電絕緣性之材料形成。感測器基 板231在感測器設置空間224外,配置成從堵塞構件223拉開 距離,且與該線軸211之移動方向約略垂直相交之狀態,背 面(非形成電路面)並與堵塞構件223對向。S 24 201231937 The circulation annular grooves 2〇6a and 206b and the flow holes 2〇7a and 207b are provided at positions where the inlet port 203 and the outlet port 204 of the valve body 202 are provided, and are passed through the circulation annular grooves 2〇6a and 206b. The flow holes 207a and 207b communicate with the hollow portion of the sleeve 205. The hollow portion of the sleeve 205 forms a cylinder, and the wired shaft 211 is accommodated therein. The axis 211 has its axis aligned with the axis of the cylinder, and the sliding portion 212 is slidable in the state of the inner surface of the cylinder so as to be movable along the axis of the cylinder. Further, as the actuator (not shown) for moving the bobbin 211, a well-known technique such as a pneumatic device of the first embodiment or a device using a solenoid can be suitably used. The bobbin 211 is formed with an annular recessed portion 213 in addition to the sliding portion 212' which is formed to slide on the inner surface of the cylinder. As shown in the figure, the state in which the bobbin 211 is disposed on the side opposite to the sensor portion 221 is the second position. At this position, the sliding portion 212 of the bobbin 211 blocks the flow hole 207b of the sleeve 205. Therefore, the fluid supplied to the inflow port 203 does not flow out from the outflow port 2〇4. On the other hand, the bobbin 211 is moved from the first position, and the state of the moving end disposed on the side of the sensor unit 221 is the second position. Figure 14(b) shows this status. As shown in the figure, the circulation annular groove 2〇6a corresponding to the inflow port 203 and the circulation annular groove 206b corresponding to the outflow port 204 communicate with each other through the flow holes 2〇7a and 2〇7b and the annular recessed portion 213. Therefore, the fluid supplied to the inflow port 2〇3 flows out from the outflow port 204. Returning to Fig. 14(a), the sensor unit 221 is provided on one end side of the valve body portion 2〇1. The sensor unit 221 has a sensor body 222 that extends the valve body 2〇2 to form a cylindrical shape. The open end of the sensor body 222 is blocked by a plug member 223 which is formed in a flat shape. The clogging member 223 is formed of a material having electrical insulation such as oxidized. The hollow portion of the sensor body 222 (the space between the blocking member 223 and the end portion of the sleeve 205) serves as the sensor installation space 224, and is provided in the same manner as the lift amount sensor 100 of the first embodiment. The sensor of the structure. That is, the fixed electrodes 225 and 226 are provided as one of the outer electrodes to the closing member 223. Further, the movable electrode 227 as a cylindrical electrode is attached to the end portion of the bobbin 211 with the insulating member 214 interposed therebetween. In the sensor installation space 224, there is a fluid of a controlled object leaking from between the sleeve 2〇5 and the bobbin 211. This fluid has a function as a dielectric fluid. k Movement of the bobbin 211 As shown in Fig. 14(b), the movable electrode 2 2 7 enters the cylindrical internal space Sp2 formed by the pair of fixed electrodes 225 and 226. At this time, the fluid in the internal space Sp2 flows through the through hole 215 formed in the bobbin 211 to the opposite side. Thereby, the movable electrode 227 enters, and the opposing area of the movable electrode 227 and the fixed electrodes 225 and 226 fluctuates. The position of the bobbin 211 can be detected by grasping the change in electrostatic capacitance caused by the change in area. Returning to Fig. 14(a) again, the pair of fixed electrodes 225 and 226 are provided with electrode terminals 225a and 226a which are respectively conductive portions. The electrode terminals 225a, 226a extend through the blocking member 223 and extend in the moving direction of the bobbin 211 to be exposed outside the sensor installation space 224. A sensor substrate 231 as a circuit board is attached to the protruding end portions of the electrode terminals 225a and 226a. The sensor substrate 231 is formed of a material having electrical insulation such as alumina or synthetic resin. The sensor substrate 231 is disposed outside the sensor installation space 224, and is disposed to be apart from the blocking member 223, and is approximately perpendicularly intersected with the moving direction of the bobbin 211, and the back surface (not formed circuit surface) and the blocking member 223 Opposite.

S 26 201231937 於感測器基板231形成有將靜電容之檢測信號輸出至 外部之輸出電路等。一對電極端子225a、226a與形成於此感 測器基板231之電路電性連接。於感測器基板23丨設有連接器 232’於連接器232連接有設於電配線之端部之配線側連接器 (省略圖示)。藉此連接,可透過電配線,將信號輸出至外部。 感測器基板231及堵塞構件223以感測器蓋233覆蓋。 又,於堵塞構件223設置熱阻器234,該熱阻器234之檢測部 配置於内部空間Sp2内。熱阻器234與形成於感測器基板231 之電路電性連接,而可將以此熱阻器234所檢測出之填充流 體(介電流體)之溫度信號輸出至外部。依據此檢測溫度,進 行介電常數ε之溫度補償。當然,溫度補償亦可如上述第i 實施形態之第2變形例或第3變形例般,採用設置補償用電 容器之結構。 此外,在此第2實施形態中,具有感測器體222、一對 固定電極225、226及一對電極端子225a、226a之組裝體亦 稱為第2構件。又,以可動電極227、絕緣構件214及線轴211 構成之組裝體亦稱為第1構件。 在此’在採用了上述結構之感測器部221中,因人接觸 閥本體部201或感測器體222等外在干擾主要原因,所檢測 之靜電容之數值會大幅變動,而有產生偏差之虞。又,雜 散電容之存在亦為招致靜電容之數值之不穩定化之主要原 因。因此,有無法穩定地進行靜電容之檢測之弊端。 是故,在此第2實施形態中,於感測器部221之感測器 設置空間224設有筒狀遮蔽構件241。筒狀遮蔽構件241以 27 201231937 (鐵、錄及始之合金)或不鏽鋼等金屬材料形成。筒狀遮蔽構 件241其—端側懸掛支撐於堵塞構件223,且於感測器體222 與固定電極225、226間,以與該等任一者皆非接觸之狀態 "在其間。亦即,於筒狀遮蔽構件241之外側設有感測器體 222 ’於内側設有一對固定電極225、226,筒狀遮蔽構件241 呈與感測器體222或固定電極225、226電性絕緣之狀態。 筒狀遮蔽構件241之一端貫穿堵塞構件223,而突出至 感測器設置空間224外。筒狀遮蔽構件241之突出端部使用 螺絲或銷等固定構件,安裝於感測器基板231。因此,感測 器基板231支撐於筒狀遮蔽構件241。又’電極端子225a、 226a之突出部份之一部份以筒狀遮蔽構件241、感測器基板 231及堵塞構件223包圍。 另一方面,筒狀遮蔽構件241之與前述感測器基板231 相反之側之端部形成為延伸至感測器設置空間224之内 部。更具體來看,如第14(a)圖所示,筒狀遮蔽構件241具有 在諸電極之對向面積最小之第丨位置,可完全覆蓋從内部空 間Sp2露出至外部之狀態之可動電極227的長度。 接著’在感測器基板231,與堵塞構材223對向之背面, 至少於與筒狀遮蔽構件241之連接部份及其内側區域,以沉 積專形成有薄膜狀金属膜242。金屬膜242與形成於感測器 基板231之接地用電路電性連接,該接地用電路藉由連接器 232 ’與接地用配線連接。前述筒狀遮蔽構件mi以與此金 屬膜242接觸之狀態而設。因此,筒狀遮蔽構件241亦接地。 准,金屬膜242分別與電極端子225a、226a、連接來自熱阻 28 201231937 器234之配線之部份電性絕緣。 藉著具有以上之結構’根據此弟2實施形態之線軸閱 200’除了第1實施形態之上升量感測器1〇〇具有之效果,尚 可獲得以下之效果。 即’固定電極225、226及可動電極227以筒狀遮蔽構件 241覆蓋。又,延伸而出至感測器設置空間224外之電極端 子225a、226a之一部份也以筒狀遮蔽構件241與金屬膜242 覆蓋。因此,於檢測靜電容之際,即使存在人接觸閥本體 部201、感測器體222或感測器蓋233等外在干擾主要原因, 亦可抑制因此種外在干擾主要原因所引起之影響。 又’於固定電極225、226及可動電極227與感測器體222 間、電極端子225a、226a間分別產生之雜散電容藉由分別 連接於接地之筒狀遮蔽構件241或金屬膜242之介在其間而 刪減。因此,由於雜散電容減少,故可減低使靜電容之數 值不穩定之主要原因。藉此,可穩定地進行靜電容之檢測, 而可獲得可耐實用化之性能。 此外,以上述第1實施形態之另一形態說明之内容亦可 應用於此第2實施形態之線轴閥2〇〇。 舉例§之,在此實施形態中,將控制對象之流體利用 作為介電流體,此點以第丨實施形態之第3變形例(參照第13 圖)。兒明。與此相反,此第2實施形態之變形例亦可將與控 制對象之流體不同之流體利用作為介電流體。此時,為防 止控制對象之流體之漏出’彳將閥體2〇2與套筒2〇5間密 封,亦可應用上述之其他形態(1)〜(3)、(6)及⑺。 29 201231937 此外,亦可採用非使感測器基板231與堵塞構件223拉 開距離之狀態,而採用使其抵接堵塞構件223之狀態而設之 結構。又,關於形成於感測器基板231之背面之金屬膜242, 亦可省略此,但在使靜電容之檢測穩定之方面,宜採用形 成有金屬膜242之本實施形態之結構。 I:圖式簡單說明3 第1圖係顯示第1實施形態之真空控制閥40之閥全關狀 態之結構的截面圖。 第2圖係顯示第1實施形態之真空控制閥40之閥半開狀 態之結構的截面圖。 第3圖係顯示上升量感測器100之結構的截面圖。 第4圖係顯示上升量感測器100之端部的外觀圖。 第5圖係顯示上升量感測器100之結構的示意圖。 第6圖係顯示上升量感測器10 0之對向電極之結構的立 體圖。 第7圖係顯示上升量感測器100之靜電容的計算式。 第8圖係比較圓柱電極及外側電極之靜電容與理論值 而顯示之圖表。 第9圖係顯示因圓柱電極及外側電極之偏心而引起之 測量誤差的圖表。 第10圖係顯示第1變形例之真空控制閥4 0 a之閥全關狀 態之結構的截面圖。 第11圖係顯示介電常數因應介電流體之溫度而變化之 圖表。S 26 201231937 An output circuit or the like for outputting a detection signal of a static capacitance to the outside is formed on the sensor substrate 231. The pair of electrode terminals 225a, 226a are electrically connected to a circuit formed on the sensor substrate 231. A connector 232' is provided on the sensor substrate 23, and a wiring side connector (not shown) provided at an end portion of the electric wiring is connected to the connector 232. By this connection, the signal can be output to the outside through the electric wiring. The sensor substrate 231 and the blocking member 223 are covered by the sensor cover 233. Further, a heat resistor 234 is provided in the clogging member 223, and the detecting portion of the heat resistor 234 is disposed in the internal space Sp2. The thermistor 234 is electrically connected to the circuit formed on the sensor substrate 231, and the temperature signal of the filling fluid (dielectric body) detected by the thermistor 234 can be output to the outside. Based on this detected temperature, temperature compensation of the dielectric constant ε is performed. As a matter of course, the temperature compensation may be such that the compensation capacitor is provided as in the second modification or the third modification of the above-described first embodiment. Further, in the second embodiment, the assembly including the sensor body 222, the pair of fixed electrodes 225 and 226, and the pair of electrode terminals 225a and 226a is also referred to as a second member. Further, the assembly including the movable electrode 227, the insulating member 214, and the bobbin 211 is also referred to as a first member. Here, in the sensor unit 221 having the above configuration, the value of the detected electrostatic capacitance greatly changes due to the external interference of the human body such as the valve body portion 201 or the sensor body 222, and is generated. The difference between the deviations. Moreover, the presence of stray capacitance is also the main cause of the destabilization of the value of the electrostatic capacitance. Therefore, there is a drawback that the detection of the electrostatic capacitance cannot be performed stably. Therefore, in the second embodiment, the cylindrical shielding member 241 is provided in the sensor installation space 224 of the sensor unit 221 . The cylindrical shielding member 241 is formed of a metal material such as 27 201231937 (iron, alloy and alloy) or stainless steel. The cylindrical shielding member 241 is suspended from the blocking member 223 at the end side, and is in a state of being non-contact with any of the sensor body 222 and the fixed electrodes 225, 226. That is, the sensor body 222' is disposed on the outer side of the cylindrical shielding member 241, and a pair of fixed electrodes 225 and 226 are disposed on the inner side. The cylindrical shielding member 241 is electrically connected to the sensor body 222 or the fixed electrodes 225 and 226. The state of insulation. One end of the cylindrical shielding member 241 penetrates the blocking member 223 and protrudes out of the sensor setting space 224. The protruding end portion of the cylindrical shielding member 241 is attached to the sensor substrate 231 by using a fixing member such as a screw or a pin. Therefore, the sensor substrate 231 is supported by the cylindrical shielding member 241. Further, one of the protruding portions of the electrode terminals 225a and 226a is surrounded by the cylindrical shielding member 241, the sensor substrate 231, and the blocking member 223. On the other hand, the end portion of the cylindrical shielding member 241 opposite to the aforementioned sensor substrate 231 is formed to extend to the inside of the sensor installation space 224. More specifically, as shown in Fig. 14(a), the cylindrical shielding member 241 has the second position at which the opposing areas of the electrodes are the smallest, and the movable electrode 227 which can completely cover the state exposed from the internal space Sp2 to the outside can be completely covered. length. Next, on the sensor substrate 231, a film-like metal film 242 is formed by deposition on at least the portion on the back surface opposite to the clogging member 223 and at least the portion to be joined to the cylindrical shielding member 241 and the inner region thereof. The metal film 242 is electrically connected to a grounding circuit formed on the sensor substrate 231, and the grounding circuit is connected to the grounding wiring by the connector 232'. The cylindrical shield member mi is provided in contact with the metal film 242. Therefore, the cylindrical shielding member 241 is also grounded. The metal film 242 is electrically insulated from the electrode terminals 225a, 226a and the portion of the wiring from the thermal resistance 28 201231937 234, respectively. In addition to the above-described configuration, the following results can be obtained in addition to the effect of the amount of rise sensor 〇〇 of the first embodiment. That is, the fixed electrodes 225 and 226 and the movable electrode 227 are covered by the cylindrical shielding member 241. Further, a part of the electrode terminals 225a, 226a extending out of the sensor installation space 224 is also covered by the cylindrical shielding member 241 and the metal film 242. Therefore, when the static capacitance is detected, even if there is a cause of external interference such as the valve body portion 201, the sensor body 222, or the sensor cover 233, the influence of the external disturbance may be suppressed. . Further, the stray capacitance generated between the fixed electrodes 225 and 226 and the movable electrode 227 and the sensor body 222 and between the electrode terminals 225a and 226a is respectively connected to the grounded cylindrical shielding member 241 or the metal film 242. In the meantime, it was cut. Therefore, since the stray capacitance is reduced, the main cause of the instability of the electrostatic capacitance value can be reduced. Thereby, the static capacitance can be stably detected, and the performance that can withstand practical use can be obtained. Further, the content described in another aspect of the first embodiment described above can be applied to the spool valve 2 of the second embodiment. For example, in this embodiment, the fluid to be controlled is used as a dielectric fluid, and this is a third modification of the third embodiment (see Fig. 13). Children. On the contrary, in the modification of the second embodiment, a fluid different from the fluid to be controlled may be used as the dielectric fluid. At this time, in order to prevent the leakage of the fluid to be controlled, the seal body 2〇2 and the sleeve 2〇5 are sealed, and the other forms (1) to (3), (6) and (7) described above can be applied. In addition, in a state in which the sensor substrate 231 and the clogging member 223 are not separated from each other, a configuration in which the clogging member 223 is brought into contact with the clogging member 223 may be employed. Further, the metal film 242 formed on the back surface of the sensor substrate 231 may be omitted. However, in order to stabilize the detection of the electrostatic capacitance, the structure of the embodiment in which the metal film 242 is formed is preferably used. I. BRIEF DESCRIPTION OF THE DRAWINGS Fig. 1 is a cross-sectional view showing the structure of the valve fully closed state of the vacuum control valve 40 of the first embodiment. Fig. 2 is a cross-sectional view showing the structure of the valve half-open state of the vacuum control valve 40 of the first embodiment. FIG. 3 is a cross-sectional view showing the structure of the amount of rise sensor 100. Fig. 4 is a view showing the appearance of the end portion of the amount of rise sensor 100. FIG. 5 is a schematic view showing the structure of the lift amount sensor 100. Fig. 6 is a perspective view showing the structure of the counter electrode of the rising amount sensor 100. Fig. 7 is a graph showing the calculation formula of the electrostatic capacitance of the rise amount sensor 100. Fig. 8 is a graph showing the comparison of the electrostatic capacitance of the cylindrical electrode and the outer electrode with the theoretical value. Fig. 9 is a graph showing measurement errors due to eccentricity of the cylindrical electrode and the outer electrode. Fig. 10 is a cross-sectional view showing the structure of the valve fully closed state of the vacuum control valve 40 a of the first modification. Figure 11 is a graph showing the change in dielectric constant in response to the temperature of the dielectric fluid.

S 30 201231937 第12圖係顯示第2變形例之真空控制閥4 0 b之閥全關狀 態之結構的截面圖。 第13圖係顯示第3變形例之介電流體控制閥4 0 c之結構 的部份截面圖。 第14(a)圖、第14(b)圖係顯示第2實施形態之線軸閥100 之感測器設置側的截面圖。 第15圖係顯示習知技術之對向電極之對向面積變化之 態樣的示意圖。 第16圖係顯示在習知技術中,對向電極之隔開距離變 化之態樣的示意圖。 第17圖係顯示習知技術之對向電極之隔開距離與靜電 容之關係的圖表。 【主要元件符號說明】 10,20,225,226...固定電極 40c,200··.線轴閥 11,21...端部壁面 41...閥本體 12,22…圓柱壁面 42...致動器 13,23...外部端面 43...致動器本體 15,25...切斷端面 43ah...開口部 30...開關閥 44...活塞桿 31...提動閥體 44a...線軸 32…閥座 44h...内部孔 33...彈性密封構件 44ah,45h,91e...凹部 37...伸縮囊 45...圓筒室 40,40a.··真空控制閥 45c...圓筒蓋 31 201231937 46.. .賦與勢能彈簧 47.. .作動空氣流路 48.. .排氣流路 48h...連通孔 49.. .活塞 49b...調壓閥 50,50a,50b,227·.·可動電極 51.. .圓柱構件 51h...貫穿孔 52.. .貯存用活塞 53.. .介電流體通過孔 54.. .插入材 55.. .貯存圓筒室 56.. .螺栓 57,205···套筒 57h...開口部 58,214...絕緣構件 59.. .固緊構件 60,60al,60a2,60b...感測器 本體 61.. .内腔面 62.. .螺栓 71,72...端子 73.. .密封部 80.. .流路 81.. .上游側流路 82.. .下游側流路 91a-91d...固定對向電極 92,93...連通孔 100—L升量感測器 201.. .閥本體部 202.. .閥體 203.. .流入口 204.. .流出口 206a,206b...流通環狀溝 207a,207b...流通孔 211.. .線軸 212.. .滑動部 213.. .環狀凹部 215.. .貫穿孔 221.. .感測器部 222.. ..感測器體 223.. .堵塞構件 224.. .感測器設置空間 225a,226a...電極端子 231.. .感測器基板 232.. .連接器 233.. .感測器蓋S 30 201231937 Fig. 12 is a cross-sectional view showing the structure of the valve fully closed state of the vacuum control valve 40b of the second modification. Fig. 13 is a partial cross-sectional view showing the structure of the dielectric fluid control valve 40c of the third modification. Figs. 14(a) and 14(b) are cross-sectional views showing the sensor installation side of the bobbin valve 100 of the second embodiment. Fig. 15 is a view showing a state in which the opposing area of the counter electrode of the prior art is changed. Fig. 16 is a view showing a state in which the distance between the opposing electrodes is changed in the prior art. Fig. 17 is a graph showing the relationship between the separation distance of the counter electrode and the electrostatic capacitance of the prior art. [Description of main component symbols] 10, 20, 225, 226... fixed electrode 40c, 200··. spool valve 11, 21... end wall surface 41... valve body 12, 22... cylindrical wall surface 42. .. actuators 13, 23... external end face 43... actuator body 15, 25... cut end face 43ah... opening 30... switch valve 44... piston rod 31. Lifting valve body 44a... spool 32... valve seat 44h... internal hole 33... elastic sealing member 44ah, 45h, 91e... recess 37... bellows 45... cylinder chamber 40, 40a.·· Vacuum control valve 45c...Cylinder cover 31 201231937 46.. . Assignment of potential energy spring 47.. Actuating air flow path 48.. Exhaust flow path 48h... communication hole 49. . . piston 49b...pressure regulating valve 50, 50a, 50b, 227 ·. movable electrode 51.. cylindrical member 51h... through hole 52.. storage piston 53.. dielectric fluid through hole 54.. . Insert material 55.. Storage cylinder chamber 56.. bolt 57, 205 · · sleeve 57h... opening portion 58, 214... insulating member 59.. fastening member 60, 60al, 60a2, 60b... sensor body 61.. lumen surface 62.. bolt 71, 72... terminal 73.. seal 80.. flow path 81.. upstream flow Road 82.. The downstream side flow paths 91a-91d... fixed counter electrodes 92, 93... communication holes 100-L lift sensor 201.. valve body portion 202.. valve body 203.. . The outflow ports 206a, 206b... flow through the annular grooves 207a, 207b... the flow holes 211.. the bobbin 212.. the sliding portion 213.. the annular recess 215.. the through hole 221.. Sensor portion 222... sensor body 223.. blocking member 224.. sensor setting space 225a, 226a... electrode terminal 231.. sensor substrate 232.. connector 233.. .Sensor cover

S 32 201231937 234...熱阻器 G. · _ 241...筒狀遮蔽構件 1L/... 242...金屬膜 Spl C...複合電容 δ\ Cl,C2...靜電容 預定距離 上升量 ,Sp2·.·内部空間 ,<52...隔開距離 33S 32 201231937 234...Thermistor G. · _ 241...Cylinder shielding member 1L/... 242...Metal film Spl C...Composite capacitor δ\ Cl, C2...Static capacitor The predetermined distance rise amount, Sp2·.·internal space, <52...separation distance 33

Claims (1)

201231937 七、申請專利範圍: 1. 一種靜電容式變位感測器,係對測量對象之直線上之變 位進行測量者,其包含有: 第1構件,係具有圓柱狀圓柱電極,該圓柱狀圓柱 電極具有平行於前述直線之中心軸線;及 第2構件,係具有圓筒狀外側電極,該圓筒狀外側 電極係在前述圓柱電極之外側,以與前述圓柱電極電性 絕緣之狀態而設; 前述外側電極具有於圓周方向分割,且相對向之至 少一對電極, 前述圓柱電極與連接於前述外側電極之電路電性 絕緣, 前述第1構件與前述第2構件隨著前述測量對象之 變位,相對地在前述直線上移動,前述至少一對之外側 電極之相互間之靜電容因應前述移動而變化。 2. 如申請專利範圍第1項之靜電容式變位感測器,其中前 述一對外側電極係以包含前述測量對象之變位之方向 的平面,均等地分割為二而相對向之一對電極。 3. 如申請專利範圍第1或2項之靜電容式變位感測器,其中 前述第1構件具有用以連接於前述測量對象之連接部, 前述第2構件具有分別連接於前述至少一對之外側電 極,且朝前述第2構件之外部貫穿前述第2構件之至少一 對導電部。 4. 如申請專利範圍第1項之靜電容式變位感測器,其中前 S 34 201231937 述第2構件密封以前述外側電極與前述圓柱電極包圍之 區域,前述區域以非壓縮性介電流體填滿。 5. 如申請專利範圍第4項之靜電容式變位感測器,其中前 述第2構件更具有補償用電容器,該補償用電容器具有 配置於前述外側電極之外周方向,隔著前述介電流體而 對向,直徑相互不同之一對固定對向電極, 前述補償用電容器藉由連通於以前述外側電極與 前述圓柱電極包圍之區域及以前述一對固定對向電極 包爽之區域的連通孔,共有前述介電流體。 6. 如申請專利範圍第1項之靜電容式變位感測器,其中前 述第2構件具有感測器體(sensor body), 該靜電容式變位感測器並設有以與該兩者電性絕緣 之狀態存在於前述外側電極與前述感測器體間,且在前 述第1構件與前述第2構件相對移動之移動範圍覆蓋前述 外側電極及前述圓柱電極兩者之金屬製筒狀遮蔽構件, 前述筒狀遮蔽構件係電性接地。 7. 如申請專利範圍第6項之靜電容式變位感測器,其中前述 第2構件具有分別連接於至少一對之前述外側電極,且朝 前述第2構件之外部貫穿前述第2構件之至少一對導電 部, 前述筒狀遮蔽構件朝前述第2構件之外部貫穿前述 第2構件,前述導電部之一部份亦為前述筒狀遮蔽構件 所覆蓋, 在前述導電部及前述筒狀遮蔽構件中往前述第2構 35 201231937 件之外部貫穿的部份,安裝背面朝向電極側之電路基 板,且於前述電路基板之背面,形成有與形成於該電路 基板之接地用電路電性連接的金屬膜。 8. —種比例控制閥,係控制介電流體之流動者,其包含有: 記載於申請專利範圍第4或5項之靜電容式變位感 測器;及 閥本體,係具有作為連接於前述第1構件之前述測 量對象的閥體,閥開度因應前述直線上之前述閥體之變 位而變化者; 又,前述閥本體具有將介電流體引導至前述區域之 流路。 S 36201231937 VII. Patent application scope: 1. A static capacitance type displacement sensor which measures the displacement of a measuring object on a straight line, and includes: a first member having a cylindrical cylindrical electrode, the cylinder The cylindrical electrode has a central axis parallel to the straight line; and the second member has a cylindrical outer electrode that is electrically insulated from the cylindrical electrode on the outer side of the cylindrical electrode. The outer electrode has a circumferential direction and is opposite to at least one pair of electrodes, and the cylindrical electrode is electrically insulated from a circuit connected to the outer electrode, and the first member and the second member follow the measurement target. The displacement is relatively moved on the straight line, and the electrostatic capacitance between the at least one pair of outer electrodes changes according to the aforementioned movement. 2. The electrostatic capacitance type displacement sensor according to claim 1, wherein the pair of outer electrodes are equally divided into two and opposite ones in a plane including a direction of displacement of the measuring object. electrode. 3. The capacitive displacement sensor according to claim 1 or 2, wherein the first member has a connection portion for connecting to the measurement object, and the second member has a connection to the at least one pair The outer electrode penetrates at least a pair of conductive portions of the second member toward the outside of the second member. 4. The electrostatic capacitance type displacement sensor according to claim 1, wherein the second member seals the region surrounded by the outer electrode and the cylindrical electrode, and the region is an incompressible dielectric fluid. Fill up. 5. The static capacitance type displacement sensor according to claim 4, wherein the second member further includes a compensation capacitor, wherein the compensation capacitor has a dielectric element disposed in a circumferential direction of the outer electrode In the opposite direction, one pair of mutually different diameters is fixed to the opposite electrode, and the compensation capacitor is connected to a region surrounded by the outer electrode and the cylindrical electrode and a communication hole in a region where the pair of fixed counter electrodes are cooled , the aforementioned dielectric fluid. 6. The capacitive displacement sensor of claim 1, wherein the second member has a sensor body, and the capacitive displacement sensor is provided with a state in which the electrical insulation is present between the outer electrode and the sensor body, and a metal cylinder that covers both the outer electrode and the cylindrical electrode in a range in which the first member and the second member move relative to each other The shielding member is electrically grounded to the cylindrical shielding member. 7. The capacitive displacement sensor according to claim 6, wherein the second member has at least one pair of the outer electrodes, and penetrates the second member toward the outside of the second member. At least one pair of conductive portions, the cylindrical shielding member penetrating the second member toward the outside of the second member, and one of the conductive portions is covered by the tubular shielding member, and the conductive portion and the tubular shielding a circuit board having a back surface facing the electrode side is mounted on a portion of the member that penetrates the outside of the second structure 35 201231937, and a ground connection circuit formed on the circuit board is electrically connected to the back surface of the circuit board. Metal film. 8. A proportional control valve for controlling a flow of a dielectric fluid, comprising: a capacitive displacement sensor as described in claim 4 or 5; and a valve body having a connection In the valve body to be measured of the first member, the valve opening degree is changed in accordance with the displacement of the valve body on the straight line; and the valve body has a flow path for guiding the dielectric fluid to the region. S 36
TW100143543A 2010-12-28 2011-11-28 Electrostatic capacity-type displacement sensor and proportional control valve having electrostatic capacity-type displacement sensor TW201231937A (en)

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CN105352422A (en) * 2015-11-17 2016-02-24 中国航空工业集团公司北京航空精密机械研究所 Capacitive displacement sensor used for electro-hydraulic servo valve
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CN105352422A (en) * 2015-11-17 2016-02-24 中国航空工业集团公司北京航空精密机械研究所 Capacitive displacement sensor used for electro-hydraulic servo valve
CN106771361A (en) * 2016-12-15 2017-05-31 西安邮电大学 Double-capacitor micro-mechanical acceleration transducer and the temperature self-compensation system based on it
CN106771361B (en) * 2016-12-15 2023-04-25 西安邮电大学 Double-capacitance type micro-mechanical acceleration sensor and temperature self-compensation system based on same
US10622996B1 (en) 2019-03-29 2020-04-14 Industrial Technology Research Institute Adjustable sensing capacitance microelectromechanical system (MEMS) apparatus

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