TWI696838B - Insulation measuring apparatus and insulation measuring method - Google Patents
Insulation measuring apparatus and insulation measuring method Download PDFInfo
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- TWI696838B TWI696838B TW108106303A TW108106303A TWI696838B TW I696838 B TWI696838 B TW I696838B TW 108106303 A TW108106303 A TW 108106303A TW 108106303 A TW108106303 A TW 108106303A TW I696838 B TWI696838 B TW I696838B
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- G—PHYSICS
- G01—MEASURING; TESTING
- G01R—MEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
- G01R31/00—Arrangements for testing electric properties; Arrangements for locating electric faults; Arrangements for electrical testing characterised by what is being tested not provided for elsewhere
- G01R31/50—Testing of electric apparatus, lines, cables or components for short-circuits, continuity, leakage current or incorrect line connections
- G01R31/52—Testing for short-circuits, leakage current or ground faults
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- G—PHYSICS
- G01—MEASURING; TESTING
- G01R—MEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
- G01R27/00—Arrangements for measuring resistance, reactance, impedance, or electric characteristics derived therefrom
- G01R27/02—Measuring real or complex resistance, reactance, impedance, or other two-pole characteristics derived therefrom, e.g. time constant
- G01R27/16—Measuring impedance of element or network through which a current is passing from another source, e.g. cable, power line
- G01R27/18—Measuring resistance to earth, i.e. line to ground
Abstract
本發明係提供一種絕緣測量裝置及絕緣測量方法,其係能夠確實地去除檢測時的誤差因子,並精確度良好地求得真正的電阻分量洩漏電流。絕緣測量裝置(10A)係測量從電源(1)連接於三相電動機(2)之三相配線TRS的電阻分量洩漏電流。其係具備:各匯流排(11),其係分別接通三相配線TRS;ZCT(12),其係具有貫通孔(12a),以絕緣的方式固定支撐各匯流排(11)並使各匯流排(11)貫通貫通孔(12a),且檢測將流過各匯流排(11)的各貫通電流所合成之零相電流;CT(13),其係檢測流過至少一個匯流排(11)的貫通電流;及控制部(14),其係使用在CT(13)所檢測之至少一個貫通電流,來修正經檢測之前述零相電流,並測量電阻分量洩漏電流。 The invention provides an insulation measurement device and an insulation measurement method, which can surely remove the error factor during detection and accurately obtain the true resistance component leakage current with good accuracy. The insulation measuring device (10A) measures the leakage current of the resistance component of the three-phase wiring TRS connected to the three-phase motor (2) from the power source (1). The system is equipped with: each bus bar (11), which is respectively connected to the three-phase wiring TRS; ZCT (12), which has a through hole (12a), fixedly supporting each bus bar (11) in an insulated manner and making each The bus bar (11) penetrates the through hole (12a), and detects the zero-phase current synthesized by the through currents flowing through the bus bars (11); CT (13), which detects at least one bus bar (11) ) Through current; and the control part (14), which uses at least one through current detected in CT (13) to correct the detected zero-phase current and measure the resistance component leakage current.
Description
本發明係關於一種絕緣測量裝置及絕緣測量方法,其係測量從電源連接到三相電動機之三相配線的電阻分量洩漏電流。 The present invention relates to an insulation measurement device and an insulation measurement method, which measure the leakage current of a resistance component of a three-phase wiring connected from a power source to a three-phase motor.
一直以來,舉例來說,在朝向電動機的配線中,因為感應器之絕緣電阻劣化會產生洩漏電流,而廣泛地利用零相比流器(ZCT:Zero-phase-sequence Current Transformer)作為檢測感應器。 For example, in the wiring to the motor, leakage current is generated due to deterioration of the insulation resistance of the inductor, and a zero-phase-sequence current transformer (ZCT) is widely used as a detection sensor .
零相比流器(ZCT)係藉由將交流三相分的電線共同通過比流器來檢測將三相分的貫通電流所合成之零相電流者。 The zero-phase current transformer (ZCT) detects the zero-phase current synthesized by the through currents of the three phases by passing the AC three-phase wires together through the current transformer.
此處,因為零相比流器(ZCT)係將貫通電流作為一次繞組,且將零相比流器(ZCT)內部的線圈作為二次繞組的變壓器,故因應繞組比的電流輸出到零相比流器(ZCT)的二次側。因此,若將三相分的貫通電流共同通過零相比流器(ZCT),則將三相分的貫通電流所合成之零相電流流向二次側。此時,因為三相交流在每相中具有相同的大小並且每個具有120°的相位差,故將三相交流的三相分的貫通電流所合成之零相電流為零。換言之,在普通的狀態下,零相比流器(ZCT)的二次側並未有電流流動。 Here, since the zero-phase current transformer (ZCT) uses the through current as the primary winding and the coil inside the zero-phase current transformer (ZCT) is used as the secondary winding transformer, the current corresponding to the winding ratio is output to the zero-phase Current secondary (ZCT) secondary side. Therefore, if the three-phase through currents are passed through the zero-phase current transformer (ZCT) together, the zero-phase current combined with the three-phase through currents flows to the secondary side. At this time, since the three-phase AC has the same magnitude in each phase and each has a phase difference of 120°, the zero-phase current synthesized by the through currents of the three phases of the three-phase AC is zero. In other words, in a normal state, no current flows on the secondary side of the ZCT.
另一方面,零相電流在零相比流器(ZCT)的二次側流動係指,當三相電流的平衡被破壞時,即為電流從三相電線之一個電線流向地面時的狀態,換言之,即為洩漏電流產生之時。結果,藉由使用零相比流器(ZCT),能夠檢測三相的相配線中的何者係成為規定的絕緣電阻以下。 On the other hand, the zero-phase current flowing on the secondary side of the zero-phase current transformer (ZCT) refers to the state when the balance of the three-phase current is broken, that is, the current flows from one of the three-phase wires to the ground, In other words, it is when the leakage current occurs. As a result, by using a zero-phase current transformer (ZCT), it can be detected which of the three-phase phase wiring is below a predetermined insulation resistance.
就此種技術而言,可舉出例如專利文獻1所揭示之接地電壓靈敏度試驗方法。
For such a technique, for example, the ground voltage sensitivity test method disclosed in
在專利文獻1所揭示之接地電壓靈敏度試驗方法中,其所使用之接地電壓靈敏度試驗裝置100係如圖9所示,具備:零相比流器101、接地方向繼電器102、電壓測量部103、變壓器T、殘留電壓消去裝置104、電源105、測量試驗器106、電壓檢測器107。
In the ground voltage sensitivity test method disclosed in
在此接地電壓靈敏度試驗方法中,在電壓測量部103測量殘流電壓,即測量洩漏電壓,且在產生殘流電壓時,將殘留電壓消去裝置104連接至電源105,並將殘留電壓消去裝置104的輸出端子y1、y2與電壓測量部103的輸出端子y1、y2連接,使用相位調整器104a調整相位,且使用電壓調整器104b調整電壓,以使出現在電壓檢測器107的殘流電壓成為零。
In this ground voltage sensitivity test method, the
藉此,因為電壓測量部103的殘留電壓呈現被去除的狀態,故能夠測量不受殘留電壓影響之正確的接地電壓。
Thereby, since the residual voltage of the
[先前技術文獻] [Prior Technical Literature]
[專利文獻] [Patent Literature]
[專利文獻1]日本國公開專利公報「特開平4-48273號(1998年9月8日公開)」 [Patent Document 1] Japanese Patent Laid-Open Publication No. 4-48273 (published on September 8, 1998)
[專利文獻2]日本國公開專利公報「特開2010-25743號(2010年2月4日公開)」 [Patent Document 2] Japanese Published Patent Gazette "Japanese Patent Laid-Open No. 2010-25743 (published on February 4, 2010)"
然而,在習知專利文獻1所揭示之接地電壓靈敏度試驗方法中,係在電動機(motor)未劣化的前提下,藉由使含有殘留電流之零相電流的值成為零,來修正殘留電流(專利文獻1中的殘流電壓)。然而,即使在初期狀態中電動機僅些微劣化的情況下,亦成為含有初期誤差的狀態。又,若朝配電線的零相比流器101的貫通位置及貫通電流產生變化,則因為修正值的相位及大小產生變化,而有需要再度修正的問題。
However, in the ground voltage sensitivity test method disclosed in the
針對此等問題,於以下進行詳述。 These issues will be described in detail below.
也就是說,洩漏電流(Io)包含兩個成分:可正常流動的電容分量洩漏電流(Ioc)與成為火災及事故之原因的電阻分量洩漏電流(Ior)。電阻分量洩漏電流(Ior)係伴隨絕緣劣化漸漸上昇,在成為規定的絕緣電阻以下時,引起絕緣破壞,而使電動機被破壞。為了此測量電阻分量洩漏電流(Ior),廣泛地使用分離兩個成分的方法,即被稱為Ior方法。 In other words, the leakage current (Io) includes two components: a capacitance component leakage current (Ioc) that can flow normally and a resistance component leakage current (Ior) that causes fire and accidents. The resistance component leakage current (Ior) gradually rises with the deterioration of the insulation, and when it falls below a predetermined insulation resistance, the insulation is broken and the motor is broken. For this measurement of the resistance component leakage current (Ior), a method of separating two components is widely used, which is called an Ior method.
在Ior方法中,如圖10所示,在電壓取得部測量絕緣電阻,即施加至三相配線的電壓(S101)。接著,在零相比流器(ZCT)測定零相電流(S102)。之後,將零相電流分離成電容分量洩漏電流(Ioc)與電阻分量洩漏電流(Ior)(S103)。最後,從電阻分量洩漏電流(Ior)與電壓演算出絕緣電阻值(S104)。 In the Ior method, as shown in FIG. 10, the insulation resistance, that is, the voltage applied to the three-phase wiring is measured in the voltage acquisition unit (S101). Next, the zero-phase current is measured in the zero-phase current transformer (ZCT) (S102). After that, the zero-phase current is separated into a capacitance component leakage current (Ioc) and a resistance component leakage current (Ior) (S103). Finally, the insulation resistance value is calculated from the resistance component leakage current (Ior) and the voltage (S104).
此處,為了讓使用者及早得知絕緣劣化,有必要測量例如在10MΩ左右的絕緣電阻流動之微小的電阻分量洩漏電流(Ior)。在200V系之電動機的情況下,相當於10MΩ的電阻分量洩漏電流(Ior)係20μA左右。又,如前述般,因為零相比流器(ZCT)係將三相配線的貫通電流作為一次繞組,且將零相比流器(ZCT)內部的線圈作為二次繞組的變壓器,故因應繞組比的電流輸出到零相比流器(ZCT)的二次側。因為輸出至零相比流器(ZCT)二次側的零相電流通常係1/1000左右,故有必要成為nA等級的測量精確度。結果,因為被輸出至零相比流器(ZCT)二次側的零相電流亦受到周圍環境之感應雜訊的影響,故在零相比流器(ZCT)的線圈、二次側輸出線及電流測量電路需要足夠的金屬遮蔽。 Here, in order to let the user know the deterioration of the insulation as early as possible, it is necessary to measure a small resistance component leakage current (Ior) flowing, for example, with an insulation resistance of about 10 MΩ. In the case of a 200V motor, the resistance component leakage current (Ior) corresponding to 10 MΩ is about 20 μA. In addition, as described above, the zero-phase current transformer (ZCT) uses the through current of the three-phase wiring as the primary winding and the coil inside the zero-phase current transformer (ZCT) as the secondary winding transformer. The current of the ratio is output to the secondary side of the ZCT (ZCT). Since the zero-phase current output to the secondary side of the zero-phase current transformer (ZCT) is usually about 1/1000, it is necessary to have nA-level measurement accuracy. As a result, the zero-phase current output to the secondary side of the zero-phase current transformer (ZCT) is also affected by the induced noise in the surrounding environment. And the current measurement circuit needs sufficient metal shielding.
又,電動機的驅動電流係根據電動機容量而不同,在一般的低壓電動機的300kW高容量產品之情況下,大約成為600A左右的流動。因此,因為其係能夠測量從600A的一次電流至nA等級的二次電流之非常嚴苛的測量系統,有必要採取措施消除周圍雜訊的對策。 In addition, the drive current of the motor differs according to the capacity of the motor, and in the case of a 300 kW high-capacity product of a general low-voltage motor, it flows about 600 A. Therefore, because it is a very strict measurement system capable of measuring a primary current of 600A to a secondary current of nA level, it is necessary to take measures to eliminate surrounding noise.
又,不僅周圍雜訊,零相比流器(ZCT)的測量精確度亦成為問題。零相比流器(ZCT)在二次側測量零相電流時,產生稱為殘留電流的誤差電流。此稱為殘留電流的誤差電流,其產生係因為根據構成零相比流器(ZCT)之鐵芯的製造不均勻性或線圈的繞組不均勻性等的構造不均勻性,而不能精確地遮斷由貫通電流所產生的磁束。因為零相比流器(ZCT)係測量三相配線的洩漏電流,即三相配線之不平衡的分量,故構造不均勻性之不平衡的分量係成為誤差。就此種構造不均勻性而言,舉例來說,因為殘餘電流的大小及相位 差可能根據三相配線及零相比流器(ZCT)之間的位置關係而改變,故難以識別誤差因子。 Moreover, not only the surrounding noise, but also the measurement accuracy of the zero-phase current transformer (ZCT) becomes a problem. When the zero-phase current transformer (ZCT) measures the zero-phase current on the secondary side, an error current called residual current is generated. This is called the residual current error current, which is due to the structural non-uniformity such as the manufacturing unevenness of the iron core constituting the zero-phase current transformer (ZCT) or the winding unevenness of the coil, which cannot be accurately masked Cut off the magnetic flux generated by the through current. Because the zero-phase current transformer (ZCT) measures the leakage current of the three-phase wiring, that is, the unbalanced component of the three-phase wiring, the unbalanced component of the structural unevenness becomes an error. In terms of this structural non-uniformity, for example, because of the magnitude and phase of the residual current The difference may change according to the positional relationship between the three-phase wiring and the zero-phase current transformer (ZCT), so it is difficult to identify the error factor.
因為針對原本測量所必須之絕緣電阻10MΩ時的電阻分量洩漏電流(Ior)而包含誤差的殘留電流係非常大,故無法測量微小的電阻分量洩漏電流(Ior),且因為在充分地進行絕緣劣化後,超過10MΩ而變得可測量。若充分地進行絕緣劣化,則在引起絕緣破壞為止的時間變得不充裕,使用者必須緊急地進行維修,而無法有計畫地保全。 The residual current including the error for the resistance component leakage current (Ior) when the insulation resistance required for the original measurement is 10 MΩ is very large, so it is impossible to measure the small resistance component leakage current (Ior), and because the insulation is sufficiently deteriorated After that, it becomes measurable beyond 10MΩ. If the insulation is sufficiently deteriorated, the time until the insulation is broken becomes insufficient, and the user must perform urgent repairs without being able to maintain it in a planned manner.
如前述般,因為殘留電流係包含起因於零相比流器(ZCT)構造上的不均勻性之誤差,故根據三相配線的貫通位置,殘留電流的大小及相位產生變化。又,具有以下問題點:電動機之由電動機容量所驅動的電流產生變化,且因應此電流大小,殘留電流的大小亦產生變化。 As described above, since the residual current includes an error due to non-uniformity in the structure of the zero-phase current transformer (ZCT), the magnitude and phase of the residual current vary depending on the penetration position of the three-phase wiring. In addition, there is a problem that the current of the motor driven by the capacity of the motor changes, and the magnitude of the residual current also changes according to the magnitude of the current.
又,就作為採用將電容分量洩漏電流(Ioc)與電阻分量洩漏電流(Ior)兩個成分分離之Ior方法的習知技術而言,舉例來說,專利文獻2所揭示之絕緣測量裝置係習知的。然而,即使在專利文獻2所揭示之絕緣測量裝置中,亦無法進行至包含此種多種誤差之殘留電流的解析。
In addition, as a conventional technique that uses the Ior method that separates the two components of the capacitance component leakage current (Ioc) and the resistance component leakage current (Ior), for example, the insulation measurement device disclosed in
本揭示的一態樣係有鑑於習知的問題點所完成者,其目的係提供一種絕緣測量裝置及絕緣測量方法,前述絕緣測量裝置及絕緣測量方法係能夠確實地去除檢測時的誤差因子,並精確度良好地求得真正的電阻分量洩漏電流。 An aspect of the present disclosure is accomplished in view of the conventional problems, and its object is to provide an insulation measurement device and an insulation measurement method. The aforementioned insulation measurement device and insulation measurement method can reliably remove the error factor during detection. And the leakage current of the real resistance component is obtained with good accuracy.
本發明人們藉由調查三相電動機的殘留電流(基於誤差的電流)的產生因子,並使用導電部件固定零相比流器與朝向三相電動機之三相配線的貫通位置,發現殘留電流的相位與大小未產生變化,進行完成本揭示的絕緣測量裝置及絕緣測量方法。 The inventors found out the phase of the residual current by investigating the generation factor of the residual current (current based on error) of the three-phase motor and fixing the penetration position of the zero-phase current transformer and the three-phase wiring toward the three-phase motor using conductive members If there is no change in the size, the insulation measurement device and the insulation measurement method of the present disclosure are completed.
本揭示的絕緣測量裝置及絕緣測量方法之一具體態樣係如下所述。 One specific aspect of the insulation measurement device and insulation measurement method of the present disclosure is as follows.
為了解決上述課題,本揭示一態樣的絕緣測量裝置,係測量從電源連接到三相電動機之三相配線的電阻分量洩漏電流,其係包含:各導電部件,其係分別接通前述三相配線;零相比流器,其係具有貫通孔,以絕緣的方式固定支撐各前述導電部件並使各前述導電部件貫通前述貫通孔,且檢測將流過各前述導電部件的各前述貫通電流所合成之零相電流;貫通電流比流器,其係檢測流過至少一個前述導電部件的貫通電流;及控制部,其係使用在前述貫通電流比流器所檢測之至少一個前述貫通電流,來修正經檢測之前述零相電流,並測量前述電阻分量洩漏電流。 In order to solve the above-mentioned problems, the disclosed insulation measurement device measures the leakage current of the resistance component of the three-phase wiring connected from the power supply to the three-phase motor, which includes: each conductive component, which is connected to the three-phase Wiring; a zero-phase current transformer, which has through-holes, fixedly supports each of the conductive members in an insulated manner and allows each of the conductive members to pass through the through-holes, and detects each of the through-currents that will flow through each of the conductive members Synthesized zero-phase current; a penetrating current comparator, which detects penetrating current flowing through at least one of the conductive members; and a control unit, which uses at least one penetrating current detected by the penetrating current comparator, to Correct the detected zero-phase current and measure the resistance component leakage current.
為了解決上述課題,本揭示一態樣的絕緣測量方法,係測量從電源連接到三相電動機之三相配線的電阻分量洩漏電流,其係包含:設置步驟,其係設置分別接通前述三相配線的各導電部件;零相電流檢測步驟,其係在零相比流器,以絕緣的方式固定支撐各前述導電部件並使各前述導電部件貫通前述貫通孔,且檢測將流過各前述導電部件的各貫通電流所合成之零相電流;貫通電流檢測步驟,其係在貫通電流比流器,檢測流過至少一個前述導電部件的貫通電流;及測量步驟,其係使用在前述貫通電流比流器所檢測之至少 一個前述貫通電流,來修正經檢測之前述零相電流,並測量前述電阻分量洩漏電流。 In order to solve the above-mentioned problems, the present invention discloses an aspect of the insulation measurement method, which measures the leakage current of the resistance component of the three-phase wiring connected from the power supply to the three-phase motor. Each conductive member of the wiring; a zero-phase current detection step, which is a zero-phase current transformer, which supports and supports each of the conductive members in an insulated manner and allows each of the conductive members to pass through the through holes, and detects that each of the conductive members will flow The zero-phase current synthesized by the penetrating currents of the components; the penetrating current detection step, which is a penetrating current ratio detector, which detects the penetrating current flowing through at least one of the conductive members; and the measuring step, which is used at the penetrating current ratio At least One of the aforementioned through currents corrects the detected zero-phase current and measures the leakage current of the resistance component.
根據本揭示的一態樣,能夠產生以下效果:提供一種絕緣測量裝置及絕緣測量方法,前述絕緣測量裝置及絕緣測量方法係能夠確實地去除檢測時的誤差因子,並精確度良好地求得真正的電阻分量洩漏電流。 According to one aspect of the present disclosure, the following effect can be produced: an insulation measurement device and an insulation measurement method can be provided. The insulation measurement device and the insulation measurement method can surely remove the error factor during detection, and can accurately find the true Leakage current of the resistance component.
1:電源 1: power supply
2:三相電動機 2: three-phase motor
3:三相電動機 3: three-phase motor
10A,10B:絕緣測量裝置 10A, 10B: Insulation measuring device
11:匯流排(導電部件) 11: busbar (conductive parts)
12:零相比流器(ZCT) 12: ZCT (ZCT)
12a,13a:貫通孔 12a, 13a: through hole
13:貫通電流比流器(CT) 13: through current ratio (CT)
23a,23b,23c:貫通電流比流器(CT) 23a, 23b, 23c: through current comparator (CT)
14:控制部 14: Control Department
14a:測量零相電流取得部(第一測量零相電流取得部) 14a: Measurement zero-phase current acquisition section (first measurement zero-phase current acquisition section)
14b:修正部(第一修正部) 14b: Correction section (first correction section)
14c:電壓取得部(第一電壓取得部) 14c: Voltage acquisition unit (first voltage acquisition unit)
14d:演算部(第一演算部) 14d: Calculation Department (First Calculation Department)
24:控制部 24: Control Department
24a:測量零相電流取得部(第二測量零相電流取得部) 24a: Measurement zero-phase current acquisition section (second measurement zero-phase current acquisition section)
24b:修正部(第二修正部) 24b: Correction section (second correction section)
24c:電壓取得部(第二電壓取得部) 24c: Voltage acquisition unit (second voltage acquisition unit)
24d:演算部(第二演算部) 24d: Calculation Department (Second Calculation Department)
IR1:第一殘留電流 I R1 : first residual current
IR2:第二殘留電流 I R2 : second residual current
IT1:第一貫通電流 I T1 : first through current
IT2:第二貫通電流 I T2 : second through current
IT3:第三貫通電流 I T3 : third through current
TRS:三相配線 TRS: three-phase wiring
α,β:常數 α, β: constant
γ,δ:不平衡係數 γ, δ: unbalance coefficient
101:零相比流器 101: zero-phase current transformer
102:接地方向繼電器 102: Ground direction relay
103:電壓測量部 103: Voltage measurement section
104:殘留電壓消去裝置 104: Residual voltage elimination device
104a:相位調整器 104a: phase adjuster
104b:電壓調整器 104b: voltage regulator
105:電源 105: power supply
106:測量試驗器 106: Measuring tester
107:電壓檢測器 107: Voltage detector
[圖1]係表示本揭示實施形態1之絕緣測量裝置的整體構成之立體圖。
[Fig. 1] A perspective view showing the overall configuration of an insulation measurement device according to
[圖2]係表示前述絕緣測量裝置在工廠出貨時的修正方法的流程圖。 [Fig. 2] A flowchart showing a correction method of the aforementioned insulation measurement device when it is shipped from the factory.
[圖3]係表示用於導入前述絕緣測量裝置的修正訊息的概念之圖。 [Fig. 3] A diagram showing the concept of introducing a correction message for the aforementioned insulation measurement device.
[圖4]係表示前述絕緣測量裝置之使用者使用時的修正方法的流程圖。 FIG. 4 is a flowchart showing a correction method when the user of the insulation measurement device is used.
[圖5](a)係從前述絕緣測量裝置之測量後零相電流來修正殘留電流,以求得真正的零相電流的向量圖;(b)係表示沒有殘留電流修正時的零相電流的向量圖。 [Figure 5] (a) is a vector diagram of the residual current corrected from the zero-phase current measured by the aforementioned insulation measuring device to obtain the true zero-phase current; (b) is the zero-phase current without residual current correction Vector illustration.
[圖6]係本揭示實施形態2之絕緣測量裝置的整體構成之立體圖。
6 is a perspective view of the overall configuration of an insulation measurement device according to
[圖7]係表示用於導入前述絕緣測量裝置的不平衡狀態的修正訊息的概念之圖。 7 is a diagram showing the concept of introducing a correction message for the imbalance state of the insulation measurement device.
[圖8](a)係用於算出作為前述絕緣測量裝置的不平衡狀態的修正訊息γ之圖;(b)係用於算出作為不平衡狀態的修正訊息δ之圖。 [FIG. 8] (a) is a graph used to calculate the correction message γ as the unbalanced state of the insulation measurement device; (b) is a graph used to calculate the correction message δ as the unbalanced state.
[圖9]係表示習知的接地電壓靈敏度試驗裝置的構成之電路圖。 9 is a circuit diagram showing the structure of a conventional ground voltage sensitivity test device.
[圖10]係表示在習知絕緣測量裝置中,沒有進行修正時的測量流程之流程圖。 FIG. 10 is a flowchart showing a measurement flow when no correction is performed in the conventional insulation measurement device.
以下,基於圖式,說明本揭示一方面的實施形態(以下,亦表示為「本實施形態」)。 Hereinafter, an embodiment of one aspect of the present disclosure will be described based on the drawings (hereinafter, also referred to as "this embodiment").
(適用例) (Application example)
首先,基於圖1,針對本揭示所適用之一例進行說明。圖1係表示本揭示一態樣之絕緣測量裝置10A的整體構成之立體圖。
First, based on FIG. 1, an example to which the present disclosure is applied will be described. FIG. 1 is a perspective view showing the overall configuration of an
如圖1所示,本揭示一態樣的絕緣測量裝置10A係測量從電源1連接於三相電動機2之三相配線TRS的電阻分量洩漏電流(Ior)。接著,其係具備:各匯流排(Busbar)11.11.11,其係分別接通三相配線TRS;零相比流器(ZCT)12,其係具有貫通孔12a,以絕緣的方式固定支撐各匯流排11.11.11並使各匯流排11.11.11貫通貫通孔12a,且檢測將流過各匯流排11.11.11的各貫通電流所合成之零相電流;貫通電流比流器(CT)13,其係檢測流過至少一個匯流排11.11.11的貫通電流;及控制部14,其係使用在貫通電流比流器(CT)13所檢測之至少一個貫通電流,來修正經檢測之前述零相電流,並測量電阻分量洩漏電流(Ior)。
As shown in FIG. 1, the
又,本揭示一態樣的絕緣測量方法,係測量從電源連接到三相電動機之三相配線的電阻分量洩漏電流,其係包含:設置步驟,其係設置分別接通三相配線TRS的各匯流排11.11.11;零相電流檢測步驟,其係在零相比流器(ZCT)12,以絕緣的方式固定支撐各匯流排11.11.11並使各匯流排11.11.11
貫通貫通孔12a,且檢測將流過各匯流排11.11.11的各貫通電流所合成之零相電流;貫通電流檢測步驟,其係在貫通電流比流器(CT)13,檢測流過至少一個匯流排11.11.11的貫通電流;及測量步驟,其係使用在貫通電流比流器(CT)13所檢測之至少一個貫通電流,來修正經檢測之零相電流,並測量電阻分量洩漏電流(Ior)。又,匯流排11係具有作為本揭示之導電部件的功能。
Moreover, the insulation measurement method of the present disclosure measures the leakage current of the resistance component of the three-phase wiring connected from the power supply to the three-phase motor, which includes: a setting step, which sets each of the three-phase wiring TRS Busbar 11.11.11; Zero-phase current detection step, which is a zero-phase current transformer (ZCT) 12, which supports each busbar 11.11.11 in an insulated manner and makes each busbar 11.11. 11
The through-
藉此,因為直接檢測朝三相電動機2之電源線的零相電流,故能夠測量僅顯示三相電動機2的絕緣劣化狀態之電阻分量洩漏電流(Ior)。
By this, since the zero-phase current toward the power supply line of the three-
又,匯流排11.11.11具有導電性,各匯流排11.11.11係以絕緣的方式固定支撐於ZCT12的貫通孔12a並貫通貫通孔12a。因此,因為三相電動機2的電源線的位置固定在ZCT12的貫通孔12a內,所以殘留電流的相位及大小不會改變。結果,可以消除誤差因子,且前述誤差因子係指根據ZCT12的貫通孔12a中的各三相配線TRS的貫通位置而改變殘留電流的大小和相位。因此,可以修正殘留電流,並且可以測量nA等級的微小電阻分量洩漏電流(Ior)。
In addition, the bus bar 11.11.11 has conductivity, and each bus bar 11.11.11 is fixedly supported by the through
又,在本揭示一態樣的絕緣測量裝置10A中,還具備控制部14,其係使用在貫通電流比流器(CT)13所檢測之至少一個貫通電流,來修正經檢測之零相電流,並測量電阻分量洩漏電流。
In addition, the
藉此,因為使用在貫通電流比流器(CT)13所檢測之至少一個貫通電流,來修正測量零相電流,故能夠排除基於三相電動機2之電動機容量的誤差因子。又,因為在控制部14測量電阻分量洩漏電流(Ior),故能夠在修正測量零相電流後,求得真正的電阻分量洩漏電流(Ior)。
With this, since at least one penetration current detected by the penetration current transformer (CT) 13 is used to correct and measure the zero-phase current, an error factor based on the motor capacity of the three-
因此,能夠提供一種絕緣測量裝置10A及絕緣測量方法,其係能夠確實地去除檢測時的誤差因子,並精確度良好地求得真正的電阻分量洩
漏電流(Ior)。更甚者,因為能夠及早發現三相電動機2的絕緣劣化,故能夠有計畫地保全。
Therefore, it is possible to provide an
[實施形態1] [Embodiment 1]
基於圖1~圖5,針對本揭示的實施形態進行說明,則如下所述。 The embodiment of the present disclosure will be described based on FIGS. 1 to 5 as follows.
(構成例) (Configuration example)
針對本實施形態的絕緣測量裝置10A的整體構成,基於圖1進行說明。圖1係表示本揭示實施形態之絕緣測量裝置的整體構成之立體圖。
The overall configuration of the
如圖1所示,本實施形態的絕緣測量裝置10A係測量從電源1連接於三相電動機2之三相配線TRS的絕緣電阻值者。又,電源1亦可為逆變器(Inverter)的二次側。
As shown in FIG. 1, the
絕緣測量裝置10A係具備:作為導電部件的3個匯流排(Busbar)11.11.11,其係分別接通三相配線TRS;零相比流器12(以下稱為ZCT12),其係在具有貫通孔12a的同時,以絕緣的方式固定支撐3個匯流排11.11.11並使3個匯流排11.11.11貫通貫通孔12a,且測量被含於流過各匯流排11.11.11的貫通電流之洩漏電流;貫通電流比流器13(以下稱為CT13),其係測量流過3個匯流排11.11.11中的至少一個之貫通電流的大小。
The
匯流排11係由板狀的金屬板而成,且具有導電性及剛性。各匯流排11.11.11在貫通ZCT12的貫通孔12a的內部時,各匯流排11.11.11之間及貫通孔12a與匯流排11.11.11之間,係絕緣的。具體而言,此等之間係裝設有圖未示的絕緣材,且藉由絕緣材,以使各匯流排11.11.11不在貫通孔12a內部移
動的方式,進行固定支撐。又,在本實施形態中,雖然匯流排11較佳係具有剛性,但不必然需具有剛性,只要能夠以絕緣材固定並支撐即可。
The
各匯流排11.11.11的一端係連接於朝向電源1的三相配線TRS,另一方面,另一端係連接於朝向三相電動機2的三相配線TRS。
One end of each bus bar 11.11.11 is connected to the three-phase wiring TRS toward the
ZCT12係具有圖未示的線圈,其係將在各匯流排11.11.11流動的貫通電流作為一次繞組,並將ZCT12內部的線圈作為二次繞組,且作為變壓器而產生功能者,又,因應繞組比的電流輸出到作為ZCT12的二次側之後述的控制部14。
The ZCT12 series has a coil not shown in the figure, which uses the through current flowing through each bus bar 11.11.11 as the primary winding, and the coil inside the ZCT12 as the secondary winding, and functions as a transformer, and, The current according to the winding ratio is output to the
CT13係於中央部具有貫通孔13a,而成為貫通型電流器。在本實施形態中,以使CT13的貫通孔13a貫通3個匯流排11.11.11中的任何一個的方式,來設置貫通孔13a。CT13係測定流動於3個中的一個匯流排11之貫通電流的電流值。在本實施形態中,雖然CT13設置於匯流排11的三相電動機2之側,但並非僅限於此,亦能夠設置於匯流排11的電源1之側。
CT13 has a through-
在本實施形態的絕緣測量裝置10A中,例如在ZCT12的上側設置控制部14。控制部14係設置於由遮蔽電及磁的遮蔽部件而成之殼體的內部。以遮蔽部件構成殼體的理由為,藉由使用遮蔽部件覆蓋控制部14,能夠從微小的雜訊隔離控制部14。藉此,能夠減少感應雜訊的誤差,成為能夠進行nA等級之微小電流測量者。
In the
控制部14係如圖1所示,其包含:作為第一測量零相電流取得部的測量零相電流取得部14a;作為第一修正部的修正部14b;作為第一電壓取得部的電壓取得部14c;作為第一演算部的演算部14d。
As shown in FIG. 1, the
測量零相電流取得部14a係從由ZCT12檢測之零相電流,來測量該零相電流的大小及相位,以求得測量零相電流。修正部14b係求得在工廠出貨時之對應於任意貫通電流的殘留電流修正值。修正部14b還演算對應於在CT13檢測到的貫通電流之電流對應修正值,並使用針對測量零相電流的該電流對應修正值,來修正測量零相電流並求得修正後的零相電流。此修正後的零相電流係顯示接近真正的零相電流。電壓取得部14c係測量至少一個匯流排11的相配線間電壓之大小及相位,並取得作為導電部件電壓的匯流排電壓。演算部14d係以CPU構成,並藉由真正的零相電流與匯流排電壓,並演算出電阻分量洩漏電流(Ior)及絕緣電阻值。演算結果係能夠被儲存於圖未示的儲存部。
The measured zero-phase
針對使用具備前述構成的絕緣測量裝置10A,並求得在三相配線TRS中是否存在洩漏電流及求得三相配線TRS的絕緣電阻值之控制動作,基於圖2~圖5的(a)、(b)進行說明。圖2係表示本實施形態之絕緣測量裝置10A在工廠出貨時的修正方法的流程圖。圖3係表示用於導入修正訊息的概念之圖。圖4係表示本實施形態之絕緣測量裝置10A之使用者使用時的修正方法的流程圖。圖5的(a)係從絕緣測量裝置10A之測量後零相電流來修正殘留電流,以求得真正的零相電流的向量(vector)圖。圖5的(b)係表示沒有進行殘留電流修正時的零相電流的向量圖。
The control operation using the
如圖2及圖3所示,在本實施形態的絕緣測量裝置10A中,在工廠出貨時求得對應於流過匯流排電壓之任意貫通電流的殘留電流修正值。也就是說,流過匯流排11‧11‧11之貫通電流的大小及殘留電流的大小係具有線性變化的特性。因此,預先準備對應於任意貫通電流的殘留電流修正值作為修正式。
As shown in FIGS. 2 and 3, in the
具體而言,對應於任意貫通電流的殘留電流修正值之修正式能夠以貫通電流的一次式表示。藉此,根據第一貫通電流流過匯流排11時的第一殘留電流以及第二貫通電流流過匯流排11時的第二殘留電流,能夠求得修正式的斜率及截距。結果,可以獲得對應於任意貫通電流的殘留電流修正值。
Specifically, the correction formula corresponding to the correction value of the residual current of an arbitrary penetration current can be expressed as a linear expression of the penetration current. With this, the slope and intercept of the correction formula can be obtained from the first residual current when the first penetration current flows through the
具體之對應於任意貫通電流的殘留電流修正值之算出方法,係如下所述。 Specifically, the method of calculating the residual current correction value corresponding to any through current is as follows.
如圖2及圖3所示,首先,使用流過匯流排11的第一貫通電流IT1測量第一殘留電流IR1的大小及相位(S1),接著,使用流過匯流排11的第二貫通電流IT2測量第二殘留電流IR2的大小(S2)。具體而言,通過三相配線TRS及匯流排11.11.11,從圖1所示之電源1供給第一貫通電流IT1至三相電動機2,並使用CT13測量第一殘留電流IR1的大小及相位。又,通過三相配線TRS及匯流排11.11.11,從圖1所示之電源1供給第二貫通電流IT2至三相電動機2,並使用CT13測量第二殘留電流IR2的大小。又,在本實施形態中,以使各匯流排11.11.11不在ZCT12的貫通孔12a內部移動的方式,進行固定支撐。因此,在第一貫通電流IT1及第二貫通電流IT2流過各匯流排11.11.11時,第一殘留電流IR1與第二殘留電流IR2的相位並未變化,彼此互為相同。因此,僅針對第一殘留電流IR1或第二殘留電流IR2,進行相位的測定即可。因此,在本實施例中,例如,僅測量第一殘留電流IR1的相位。
As shown in FIGS. 2 and 3, first, the first through current I T1 flowing through the
藉此,從圖3所示之圖來看,作為殘留電流修正值,能夠導入下述(式1)的關係式,並求得具體的常數α及常數β。 From this, from the graph shown in FIG. 3, as the residual current correction value, the following relational expression (Equation 1) can be introduced, and specific constant α and constant β can be obtained.
殘留電流IR=α*貫通電流IT+β……(式1)。 Residual current I R = α* through current I T + β (Equation 1).
結果,對於實際貫通電流的殘留電流修正值,即電流對應修正值係能夠以(式2)表示。 As a result, the residual current correction value for the actual through current, that is, the current corresponding correction value can be expressed by (Expression 2).
殘留電流修正值=-(α*貫通電流+β)……(式2)。 Residual current correction value =-(α * through current + β) ... (Equation 2).
(式2)的貫通電流係使用者實際測定時所能得到的貫通電流。又,在(式2)加上負號係因為殘留電流修正值=-(殘留電流IR),且針對經測量之零相電流的修正係在負號側作動。此等演算係修正部14B進行。 The penetrating current of (Equation 2) is the penetrating current available to the user when actually measured. In addition, a negative sign is added to (Equation 2) because the residual current correction value =-(residual current I R ), and the correction for the measured zero-phase current is operated on the negative sign side. These calculations are performed by the correction unit 14B.
又,圖3所示之殘留電流係顯示,在第一貫通電流IT1流過匯流排11時,因應此第一貫通電流IT1而產生第一殘留電流IR1;又,在第二貫通電流IT2流過匯流排11時,因應此第二貫通電流IT2而產生第二殘留電流IR2。又,第一貫通電流IT1的大小較佳係為所使用之三相電動機2的最小電動機容量的貫通電流,同時,第二貫通電流IT2的大小較佳係為所使用之三相電動機2的最大電動機容量的貫通電流。
In addition, the residual current shown in FIG. 3 shows that when the first through current I T1 flows through the
結果,如圖2所示,經算出之殘留電流IR的修正訊息(α,β)係被保持在演算部14d的儲存部(S3)。
As a result, as shown in FIG amended message calculating the residual current I R in the (α, β) is kept in a storage-based portion (S3) of calculating
如圖4所示,另一方面,購入此絕緣測量裝置10A的使用者在使用時,首先,在CT13求得貫通電流(S11)。具體而言,通過三相配線TRS及匯流排11.11.11,從圖1所示之電源1供給第三貫通電流IT3至三相電動機2。藉此,在CT13及修正部14b測量第三貫通電流IT3的大小。接著,使用修正部14b,從求得之第三貫通電流IT3(式1),來決定電流對應修正值,即對應於第三貫通電流IT3的殘留電流修正值(S12)。
As shown in FIG. 4, on the other hand, when a user who purchases this
接著,在電壓取得部14c測量關於匯流排11.11.11的施加到絕緣電阻之相配線間電壓及相位的同時(S13),在ZCT12及測量零相電流取得部14a測量零相電流及相位(S14)。
Next, while the
此處,如圖5的(a)所示,經測量之零相電流係在包含電容分量洩漏電流(Ioc)與電阻分量洩漏電流(Ior)的同時,還包含殘留電流的誤差。因此,於經測量之零相電流向量合成殘留電流修正值。藉此,求得真正的零相電流(S15)。 Here, as shown in (a) of FIG. 5, the measured zero-phase current includes the capacitance component leakage current (Ioc) and the resistance component leakage current (Ior) as well as the residual current error. Therefore, the residual current correction value is synthesized from the measured zero-phase current vector. With this, the true zero-phase current is obtained (S15).
接著,如圖4及圖5的(a)所示,將真正的零相電流分離成電容分量洩漏電流(Ioc)與電阻分量洩漏電流(Ior)(S16)。在進行分離的情況下,藉由經測量之零相電流的相位及施加到絕緣電阻的電壓的相位之間的相位差,分離成電容分量洩漏電流(Ioc)和電阻分量洩漏電流(Ior)。 Next, as shown in (a) of FIGS. 4 and 5, the true zero-phase current is separated into a capacitance component leakage current (Ioc) and a resistance component leakage current (Ior) (S16). In the case of separation, by the phase difference between the measured phase of the zero-phase current and the phase of the voltage applied to the insulation resistance, it is separated into a capacitance component leakage current (Ioc) and a resistance component leakage current (Ior).
接著,在演算部14d,根據電阻分量洩漏電流(Ior)及施加到由電壓取得部14c所取得之絕緣電阻的相配線間電壓,來演算絕緣電阻值(S17)。通過將施加到由電壓取得部14c所取得之絕緣電阻的電壓,除以電阻分量洩漏電流(Ior),能夠求得絕緣電阻值。
Next, the
又,在未進行如此之修正的情況下,如圖5的(b)所示,因為基於經測量之零相電流,來算出電阻分量洩漏電流(Ior),故變得算出包含殘留電流的誤差之電阻分量洩漏電流(Ior)。 Also, without such correction, as shown in (b) of FIG. 5, since the resistance component leakage current (Ior) is calculated based on the measured zero-phase current, an error including residual current is calculated The leakage current of the resistance component (Ior).
如此一來,本實施形態的絕緣測量裝置10A係測量通過三相配線TRS從電源1連接的三相電動機2的電阻分量洩漏電流(Ior)。其係具備:作為導電部件的各匯流排11.11.11,其係分別接通三相配線TRS;零相比流器(ZCT)12,其係具有貫通孔12a,以絕緣的方式固定支撐各匯流排11.11.11並使
各匯流排11.11.11貫通貫通孔12a,且檢測將流過各匯流排11.11.11的各貫通電流所合成之零相電流;貫通電流比流器(CT)13,其係檢測流過至少一個匯流排11.11.11之貫通電流;及控制部14,其係使用在CT13所檢測之至少一個貫通電流,來修正經檢測之前述零相電流,並測量電阻分量洩漏電流(Ior)。
In this way, the
又,本實施形態的絕緣測量方法,係測量通過三相配線TRS從電源1連接的三相配線TRS的電阻分量洩漏電流(Ior)。其係包含:設置步驟,其係設置作為分別接通三相配線TRS的各導電部件之匯流排11.11.11;零相電流檢測步驟,其係在零相比流器(ZCT)12,以絕緣的方式固定支撐各匯流排11.11.11並使各匯流排11.11.11貫通貫通孔12a,且檢測將流過各匯流排11.11.11的各貫通電流所合成之零相電流;貫通電流檢測步驟,其係在貫通電流比流器(CT)13,檢測流過至少一個匯流排11.11.11的貫通電流;及測量步驟,其係使用在CT13所檢測之至少一個貫通電流,來修正經檢測之零相電流,並測量電阻分量洩漏電流(Ior)。
In addition, the insulation measurement method of this embodiment measures the resistance component leakage current (Ior) of the three-phase wiring TRS connected from the
藉此,因為能夠直接檢測朝三相電動機2之電源線的零相電流,故能夠測量僅顯示三相電動機2的絕緣劣化狀態之電阻分量洩漏電流(Ior)。
By this, since the zero-phase current toward the power supply line of the three-
又,匯流排11.11.11具有導電性,各匯流排11.11.11係以絕緣的方式固定支撐於ZCT12的貫通孔12a並貫通貫通孔12a。因此,因為三相電動機2的電源線的位置固定在ZCT12的貫通孔12a內,所以殘留電流的相位及大小不會改變。結果,可以消除誤差因子,且前述誤差因子係指根據ZCT12的貫通孔12a中的各三相配線TRS的貫通位置而改變殘留電流的大小和相位。因此,可以修正殘留電流,並且可以測量nA等級的微小電阻分量洩漏電流(Ior)。
In addition, the bus bar 11.11.11 has conductivity, and each bus bar 11.11.11 is fixedly supported by the through
又,在本實施形態的絕緣測量裝置10A中,還具備控制部14,其係使用在CT13所檢測之至少一個貫通電流,來修正經檢測之零相電流,並測量電阻分量洩漏電流(Ior)。
In addition, the
藉此,因為使用在CT13所檢測之至少一個貫通電流,來修正測量零相電流,故能夠排除基於三相電動機2之電動機容量的誤差因子。又,因為在控制部14測量電阻分量洩漏電流(Ior),故能夠在修正測量零相電流後,求得真正的電阻分量洩漏電流(Ior)。
By this, since at least one through current detected by CT13 is used to correct the measured zero-phase current, an error factor based on the motor capacity of the three-
因此,能夠提供一種絕緣測量裝置10A及絕緣測量方法,其係能夠確實地去除檢測時的誤差因子,並精確度良好地求得真正的電阻分量洩漏電流(Ior)。更甚者,因為能夠及早發現三相電動機2的絕緣劣化,故能夠有計畫地保全。
Therefore, it is possible to provide an
又,在本實施形態的絕緣測量裝置10A中,匯流排11具有剛性。藉此,在ZCT12的貫通孔12a的內部固定支撐各匯流排11.11.11的情況下,能夠使用簡單的支撐部件並使匯流排11.11.11不容易移動。
In addition, in the
又,在本實施形態的絕緣測量裝置10A中,控制部14係具備:作為第一測量零相電流取得部的測量零相電流取得部14a,其係從由ZCT12所檢測之零相電流,來測量該零相電流的大小及相位,以求得測量零相電流;作為第一修正部的修正部14b,其係在預先求得對應任意貫通電流之殘留電流修正值的同時,演算出因應在CT13檢測之貫通電流的電流對應修正值,並對於測量零相電流使用該電流對應修正值,來修正測量零相電流並求得修正後的零相電流;作為第一電壓取得部的電壓取得部14c,其係測量匯流排11.11.11的至少一個的相配線間電壓之大小及相位,並取得作為導電部件電壓的匯流排電壓;
作為第一演算部的演算部14d,其係藉由修正後的零相電流與匯流排電壓,演算出電阻分量洩漏電流(Ior)。
In addition, in the
藉此,測量零相電流取得部14a係從由ZCT12所檢測之零相電流,來測量該零相電流的大小及相位,並求得測量零相電流。又,修正部14b係使用對應於任意貫通電流的殘留電流修正值,演算出因應在CT13所檢測之貫通電流的電流對應修正值,並對於測量零相電流使用該電流對應修正值,修正測量零相電流,且求得作為修正後零相電流之真正的零相電流。
With this, the measured zero-phase
接著,電壓取得部14c係測量匯流排11.11.11的至少一個的相配線間電壓之大小及相位,並取得匯流排電壓。演算部14d係藉由真正的零相電流與匯流排電壓,演算出電阻分量洩漏電流(Ior)。
Next, the
結果,具體來說,能夠提供一種絕緣測量裝置10A,其係能夠確實地去除檢測時的誤差因子,並精確度良好地求得真正的電阻分量洩漏電流(Ior)。
As a result, specifically, it is possible to provide an
又,在本實施形態的絕緣測量裝置10A中,修正部14b係從第一殘留電流IR1與第二殘留電流IR2,來預先求得對應任意貫通電流之殘留電流修正值,其中,第一殘留電流IR1係包含誤差,其係因應第一貫通電流IT1流過匯流排11.11.11時之在CT13所檢測的該第一貫通電流IT1的大小;第二殘留電流IR2係包含誤差,其係因應第二貫通電流IT2流過匯流排11.11.11時之在CT13所檢測的該第二貫通電流IT2的大小。
In addition, in the
具體而言,因為對應於任意貫通電流之殘留電流修正值的修正式係能夠以貫通電流的一次式來表示,藉由第一貫通電流IT1流動時的第一殘留 電流IR1與第二貫通電流IT2流動時的第二殘留電流IR2,能夠求得修正式的斜率及截距。結果,能夠求得對應於任意貫通電流的殘留電流修正值。 Specifically, since the correction formula corresponding to the correction value of the residual current of any penetration current can be expressed as a linear expression of the penetration current, the first residual current I R1 and the second penetration when the first penetration current I T1 flows When the current I T2 flows, the second residual current I R2 can obtain the slope and intercept of the correction formula. As a result, the residual current correction value corresponding to any through current can be obtained.
因此,因為能夠使用修正式,來決定由貫通電流的大小而變化之殘留電流的修正值,能夠省去使用者修正的時間,且能夠提供具有便利性的絕緣測量裝置10A。
Therefore, since the correction formula can be used to determine the correction value of the residual current that changes according to the magnitude of the through current, it is possible to save time for the user to correct, and it is possible to provide a convenient
又,在本實施形態的絕緣測量裝置10A中,控制部14係設置於由遮蔽電及磁的遮蔽材料而成之殼體的內部。藉此,藉由使用由遮蔽材料而成之殼體覆蓋控制部14,能夠從微小的雜訊隔離控制部14。藉此,能夠減少感應雜訊的誤差,成為能夠進行nA等級之微小電流測量者。
In addition, in the
[實施形態2] [Embodiment 2]
若基於圖6~圖8,針對本發明的其他實施形態進行說明,則如下所述。又,在本實施形態進行說明以外的構成,係與前述實施形態1相同。又,為了方便說明,針對與前述實施形態1的圖式所示之部件具有相同功能的部件,賦予相同符號,並省略其說明。 Based on FIGS. 6 to 8, another embodiment of the present invention will be described as follows. In addition, the configuration other than that described in the present embodiment is the same as that of the aforementioned first embodiment. In addition, for convenience of explanation, components having the same functions as those shown in the drawings in the first embodiment are given the same symbols, and their descriptions are omitted.
本實施形態的絕緣測量裝置10B除了包含前述實施形態1的絕緣測量裝置10A之外,如圖6所示,還包含以下的差異點:3個匯流排11.11.11係分別設於CT 23a.23b.23c。
The
針對本實施形態絕緣測量裝置10B的整體構成,基於圖6進行說明。圖6係本實施形態之絕緣測量裝置10B的整體構成之立體圖。
The overall configuration of the
如圖6所示,本實施形態的絕緣測量裝置10B係將3個匯流排11.11.11分別設於CT 23a.23b.23c。又,CT 23a.23b.23c係和實施形態1的CT13相同的部件。
As shown in FIG. 6, the
如圖6所示,於控制部24係設置:作為第二測量零相電流取得部的測量零相電流取得部24a;作為第二修正部的修正部24b;作為第二電壓取得部的電壓取得部24c;作為第二演算部的演算部24d。
As shown in FIG. 6, the
測量零相電流取得部24a係從由ZCT12檢測之零相電流,來測量該零相電流的大小及相位,以求得測量零相電流。修正部24b使用對應於任意貫通電流之殘留電流修正值,並演算出因應在CT 13.13.13所檢測之流過各匯流排11.11.11的貫通電流的電流對應修正值,並使用針對測量零相電流的該電流對應修正值,來修正測量零相電流並求得修正後的零相電流。電壓取得部24c係測量匯流排11.11.11之至少一個的相配線間電壓之大小及相位,並取得匯流排電壓。演算部24d係藉由真正的零相電流與至少一個匯流排電壓,並演算出電阻分量洩漏電流(Ior)。
The measured zero-phase
針對使用具備前述構成的絕緣測量裝置10B,並求得在三相配線TRS中是否存在洩漏電流及求得三相配線TRS的絕緣電阻值之控制動作,基於圖7及圖8的(a)、(b)進行說明。圖7係表示用於導入絕緣測量裝置10B的不平衡狀態的修正訊息的概念之圖。圖8的(a)係用於算出作為絕緣測量裝置10B的不平衡狀態的修正訊息γ之圖。圖8的(b)係用於算出作為不平衡狀態的修正訊息δ之圖。
For the control operation using the
首先,在本實施形態的絕緣測量裝置10B中,在工廠等,假定有因為電源環境惡化,而產生電流不平衡,且貫通電流在三相配線TRS的各相
產生變化之情形。也就是說,一般而言,雖然三相配線TRS的貫通電流係相同,但在設置於工廠等的三相電動機3中,三相配線TRS的貫通電流係有互為不同的情形。結果,根據在各相的貫通電流之電流不平衡,使殘留電流的修正值產生變化。
First, in the
因此,在本實施形態的絕緣測量裝置10B中,設置3個CT 23a.23b.23c,以分別檢測流過各匯流排11‧11‧11之貫通電流。接著,在各CT 23a.23b.23c,藉由測量各相的貫通電流,能夠不斷地監測貫通電流的不平衡狀態。因此,能夠進行配合電流不平衡的修正。
Therefore, in the
針對本實施形態之絕緣測量裝置10B所測量之零相電流的修正方法,於以下進行說明。
The correction method of the zero-phase current measured by the
如圖7所示,在絕緣測量裝置10B中,於工廠出貨時進行修正的情況下,使用第一貫通電流IT1測量第一殘留電流IR1的大小,並使用第二貫通電流IT2測量第二殘留電流IR2的大小。具體而言,通過三相配線TRS及各匯流排11.11.11,從圖6所示之電源1供給第一貫通電流IT1至三相電動機3,並使用CT23a.23b.23c中的任一者及修正部24b,測量第一殘留電流IR1的大小。又,通過三相配線TRS及各匯流排11.11.11,從圖6所示之電源1供給第二貫通電流IT2至三相電動機2,並使用CT 23a.23b.23c中的任一者及修正部24b,測量第二殘留電流IR2的大小。
As shown in FIG. 7, in the
又,在工廠出貨時,因為未發生不平衡狀態,故可使第一貫通電流IT1及第二貫通電流IT2在一個匯流排11流動。結果,此處理與前述實施形態1中的處理相同。
In addition, at the time of factory shipment, since an unbalanced state does not occur, the first through current I T1 and the second through current I T2 can flow in one
藉此,如前述圖3所示,作為一般的殘留電流修正值,能夠獲得實施形態1所示之以下的(式1)。
With this, as shown in FIG. 3 described above, as a general residual current correction value, the following (Equation 1) shown in
殘留電流IR=α*貫通電流IT+β……(式1) Residual current I R =α*Through current I T +β……(Equation 1)
接著,藉由(式1),並藉由第一貫通電流IT1、第一殘留電流IR1、第二貫通電流IT2及第二殘留電流IR2,能夠求得具體的常數α及常數β。演算部24d係進行此演算。 Next, by (Equation 1), and by the first through current I T1 , the first residual current I R1 , the second through current I T2 and the second residual current I R2 , specific constants α and β can be obtained . The calculation part 24d performs this calculation.
此處,因為合計存在著3個CT 23a.23b.23c,藉由(式1),如圖7所示,作為個別的殘留電流修正值,即電流對應修正值,獲得下述(式3)的關係式:殘留電流修正值=-(α’*貫通電流+β’)……(式3)。
Here, because there are 3
此時,α’與β’能夠作為下述(式4)及(式5)表示:α’=α*γ(不平衡係數)……(式4);β’=β*δ(不平衡係數)……(式5)。 At this time, α'and β'can be expressed as (Equation 4) and (Equation 5) as follows: α'=α*γ (unbalance coefficient)... (Equation 4); β'=β*δ (unbalance Coefficient) (Equation 5).
此等不平衡係數γ‧δ係能夠藉由圖8的(a)所示之不平衡係數γ算出表格及圖8的(b)所示之不平衡係數δ算出表格來求得。 These unbalance coefficients γ•δ can be obtained from the unbalance coefficient γ calculation table shown in FIG. 8(a) and the unbalance coefficient δ calculation table shown in FIG. 8(b).
具體而言,於圖8的(a)的縱軸顯示,S相配線的貫通電流是否為三相配線TRS中R相配線的0.7倍、0.8倍、0.9倍、1.0倍、1.1倍、1.2倍、1.3倍中的任一者;於圖8的(a)的橫軸顯示,T相配線的貫通電流是否為三相配線TRS中R相配線的0.7倍、0.8倍、0.9倍、1.0倍、1.1倍、1.2倍、1.3倍中的任一者。接著,不平衡係數γ顯示在彼此的交點。 Specifically, the vertical axis of (a) of FIG. 8 shows whether the penetration current of the S-phase wiring is 0.7 times, 0.8 times, 0.9 times, 1.0 times, 1.1 times, 1.2 times of the R-phase wiring in the three-phase wiring TRS , Any of 1.3 times; the horizontal axis in (a) of FIG. 8 shows whether the penetrating current of the T-phase wiring is 0.7 times, 0.8 times, 0.9 times, 1.0 times of the R-phase wiring in the three-phase wiring TRS Any of 1.1 times, 1.2 times, and 1.3 times. Next, the imbalance coefficient γ is shown at the intersection of each other.
藉此,舉例來說,在S相配線的貫通電流為R相配線的0.8倍,且T相配線的貫通電流為R相配線的0.9倍時,不平衡係數γ為0.9。結果,α’=α*γ(不平衡係數)=0.9*α。 Thus, for example, when the penetration current of the S-phase wiring is 0.8 times that of the R-phase wiring and the penetration current of the T-phase wiring is 0.9 times that of the R-phase wiring, the unbalance coefficient γ is 0.9. As a result, α'=α*γ (unbalance coefficient)=0.9*α.
又,於圖8的(b)的縱軸顯示,S相配線的貫通電流是否為三相配線TRS中R相配線的0.7倍、0.8倍、0.9倍、1.0倍、1.1倍、1.2倍、1.3倍中的任一者;於圖8的(b)的橫軸顯示,T相配線的貫通電流是否為三相配線TRS中R相配線的0.7倍、0.8倍、0.9倍、1.0倍、1.1倍、1.2倍、1.3倍中的任一者。接著,不平衡係數δ顯示在彼此的交點。 In addition, the vertical axis of (b) of FIG. 8 shows whether the penetration current of the S-phase wiring is 0.7 times, 0.8 times, 0.9 times, 1.0 times, 1.1 times, 1.2 times, 1.3 times of the R-phase wiring in the three-phase wiring TRS Any one of the times; the horizontal axis in (b) of FIG. 8 shows whether the through current of the T-phase wiring is 0.7 times, 0.8 times, 0.9 times, 1.0 times, 1.1 times of the R-phase wiring in the three-phase wiring TRS , 1.2 times, 1.3 times. Next, the unbalance coefficient δ is shown at the intersection of each other.
藉此,舉例來說,在S相配線的貫通電流為R相配線的0.8倍,且T相配線的貫通電流為R相配線的0.9倍時,不平衡係數δ為0.9。結果,β’=β*δ(不平衡係數)=0.9*β。 Thus, for example, when the penetration current of the S-phase wiring is 0.8 times that of the R-phase wiring and the penetration current of the T-phase wiring is 0.9 times that of the R-phase wiring, the unbalance coefficient δ is 0.9. As a result, β'=β*δ (unbalance coefficient)=0.9*β.
因此,藉由將此等α’、β’代入(式3),並代入R相配線的貫通電流,能夠對於經測量之零相電流進行修正,並求得真正的零相電流。 Therefore, by substituting these α', β'(Equation 3) and the penetration current of the R-phase wiring, the measured zero-phase current can be corrected and the true zero-phase current can be obtained.
之後,在從真正的零相電流求得電阻分量洩漏電流(Ior)的同時,另外再藉由將在電壓取得部14c所求得之相配線間電壓除以前述電阻分量洩漏電流(Ior),而能夠求得三相配線TRS的絕緣電阻值。此時,即使流過各三相配線TRS及各匯流排11.11.11的貫通電流互為不同,各相配線間電壓亦幾乎不會變化。因此,針對各相配線間電壓,使用一個相配線間電壓的測量即可。
After that, the resistance component leakage current (Ior) is obtained from the true zero-phase current, and the voltage between the phase wirings obtained by the
又,圖8的(a)、(b)所示之表格,係著眼於作為不平衡狀態之電流值的大小在各三相配線TRS係相異的,並表示不平衡係數γ‧δ者。然而,因為作為不平衡狀態之相位各自變化,亦有必要針對相位進行修正。因此,較佳 係準備用於求得關於相位的相位用不平衡係數之表格,並算出殘留電流修正值。 In addition, the tables shown in (a) and (b) of FIG. 8 focus on those in which the magnitude of the current value as an unbalanced state differs in each of the three-phase wiring TRS systems and represents the unbalanced coefficient γ‧δ. However, it is necessary to correct the phase because the phases as the unbalanced state change individually. Therefore, it is better It prepares a table for obtaining the phase imbalance coefficient about the phase and calculates the residual current correction value.
如此一來,在本實施形態的絕緣測量裝置10B中,設置3個CT23a.23b.23c,以分別檢測流過各匯流排11.11.11的貫通電流。藉此,根據測量三相配線TRS中各相的貫通電流,能夠不斷地監測貫通電流的不平衡狀態。因此,能夠進行配合電流不平衡的修正。
In this way, three CT23a are provided in the
又,在本實施形態的絕緣測量裝置10B中,控制部24係具備:作為第二測量零相電流取得部的測量零相電流取得部24a,其係從由ZCT12所檢測之零相電流,來測量該零相電流的大小及相位,以求得測量零相電流;作為第二修正部的修正部24b,其係使用對應於任意貫通電流的殘留電流修正值,並演算出因應在CT 23a.23b.23c所檢測之流過各匯流排11.11.11的各貫通電流之電流對應修正值,並對於測量零相電流使用該電流對應修正值,來修正測量零相電流並求得作為修正後的零相電流之真正的零相電流;作為第二電壓取得部的電壓取得部24c,其係測量匯流排11.11.11的相配線間電壓之大小及相位,並取得匯流排電壓;作為第二演算部的演算部24d,其係藉由真正的零相電流與匯流排電壓,演算出電阻分量洩漏電流(Ior)。
In addition, in the
結果,在不平衡狀態的貫通電流流過各匯流排11.11.11時,能夠具體地提供一種絕緣測量裝置10B,其係能夠確實地去除檢測時的誤差因子,並精確度良好地求得真正的電阻分量洩漏電流(Ior)。
As a result, when the through current in the unbalanced state flows through each bus bar 11.11.11, an
如上所述,本揭示一態樣的絕緣測量裝置,係測量從電源連接到三相電動機之三相配線的電阻分量洩漏電流,其係包含:各導電部件,其係分別接通前述三相配線;零相比流器,其係具有貫通孔,以絕緣的方式固定支 撐各前述導電部件並使各前述導電部件貫通前述貫通孔,且檢測將流過各前述導電部件的各貫通電流所合成之零相電流;貫通電流比流器,其係檢測流過至少一個前述導電部件的貫通電流;及控制部,其係使用在前述貫通電流比流器所檢測之至少一個前述貫通電流,來修正經檢測之前述零相電流,並測量前述電阻分量洩漏電流。 As described above, the insulation measurement device according to the present disclosure measures the leakage current of the resistance component of the three-phase wiring connected to the three-phase motor from the power supply. It includes: each conductive member, which is connected to the three-phase wiring ; Zero-phase current transformer, which has a through-hole, fixed support in an insulated manner Supporting each of the conductive members, allowing each of the conductive members to pass through the through-holes, and detecting a zero-phase current synthesized by each through current flowing through each of the conductive members; a through-current comparator that detects the flow of at least one of the foregoing A through-current of the conductive member; and a control unit that corrects the detected zero-phase current using at least one of the through-currents detected by the through-current rectifier, and measures the resistance component leakage current.
本揭示一態樣的絕緣測量方法,係測量從電源連接到三相電動機之三相配線的電阻分量洩漏電流,其係包含:設置步驟,其係設置分別接通前述三相配線的各導電部件;零相電流檢測步驟,其係在零相比流器,以絕緣的方式固定支撐各前述導電部件並使各前述導電部件貫通前述貫通孔,且檢測將流過各前述導電部件的各貫通電流所合成之零相電流;貫通電流檢測步驟,其係在貫通電流比流器,檢測流過至少一個前述導電部件的貫通電流;及測量步驟,其係使用在前述貫通電流比流器所檢測之至少一個前述貫通電流,來修正經檢測之前述零相電流,並測量前述電阻分量洩漏電流。 The disclosed insulation measurement method measures the leakage current of the resistance component of the three-phase wiring connected from the power supply to the three-phase motor. It includes: a setting step, which is to set each conductive component that is connected to the three-phase wiring A zero-phase current detection step, which is a zero-phase current transformer, which supports and insulates each of the conductive members in an insulated manner so that each of the conductive members penetrates the through-hole, and detects each through-current that will flow through each of the conductive members The synthesized zero-phase current; the penetrating current detection step, which detects the penetrating current flowing through at least one of the aforementioned conductive parts in the penetrating current comparator; and the measurement step, which uses the detection in the penetrating current comparator At least one of the through currents to correct the detected zero-phase current and measure the resistance component leakage current.
一直以來,一般而言,若使用零相比流器檢測三相配線的零相電流,作為誤差之殘留電流會成為問題,故使用者測量接地線的零相電流,並將測量後的零相電流分離為電容分量洩漏電流(Ioc)和電阻分量洩漏電流(Ior),來測量電阻分量洩漏電流(Ior)。然而,因為只有洩漏電流(Io)在接地線中流動,且大的電流不流動,故作為誤差的殘留電流的影響也不會成為問題。另一方面,系統接地線上的零相電流的測量,係指測量包含連接於此系統的電動機及其他負載之多個負載的洩漏電流,故無法監視一個電動機的負載的絕緣劣化狀態。 All along, in general, if the zero-phase current is used to detect the zero-phase current of the three-phase wiring, the residual current as an error will be a problem. Therefore, the user measures the zero-phase current of the ground wire and compares the measured zero-phase current. The current is separated into a capacitance component leakage current (Ioc) and a resistance component leakage current (Ior) to measure the resistance component leakage current (Ior). However, since only the leakage current (Io) flows in the ground line and a large current does not flow, the influence of the residual current as an error will not be a problem. On the other hand, the measurement of the zero-phase current on the system ground wire refers to the measurement of the leakage current of multiple loads including the motor and other loads connected to the system, so it is impossible to monitor the insulation degradation state of the load of one motor.
因此,在本揭示一態樣的絕緣測量裝置中,設置各導電部件,其係分別接通三相配線。接著,以絕緣的方式固定支撐各導電部件並使各導電部件貫通零相比流器的貫通孔,且使用零相比流器檢測將流過各導電部件的各貫通電流所合成之零相電流。結果,在本揭示的一態樣中,因為直接檢測朝向三相電動機的電源線之零相電流,故能夠測量僅顯示三相電動機的絕緣劣化狀態之電阻分量洩漏電流(Ior)。 Therefore, in the insulation measurement device according to the aspect of the present disclosure, each conductive member is provided, which is connected to the three-phase wiring, respectively. Next, each conductive member is fixedly supported in an insulated manner so that each conductive member passes through the through hole of the zero-phase current transformer, and the zero-phase current synthesized by each through current flowing through each conductive member is detected using the zero-phase current transformer . As a result, in one aspect of the present disclosure, since the zero-phase current toward the power supply line of the three-phase motor is directly detected, it is possible to measure the resistance component leakage current (Ior) that only shows the insulation deterioration state of the three-phase motor.
又,導電部件具有導電性,各導電部件係以絕緣的方式固定支撐於零相比流器的貫通孔並貫通貫通孔。因此,因為三相電動機的電源線的位置固定在零相比流器的貫通孔內,故殘留電流的相位及大小不會改變。結果,可以消除誤差因子,且前述誤差因子係指根據零相比流器的貫通孔中的各三相配線的貫通位置而改變殘留電流的大小和相位。因此,可以修正殘留電流,並且可以測量nA等級的微小電阻分量洩漏電流。 In addition, the conductive member has conductivity, and each conductive member is fixedly supported by and penetrates the through hole of the zero-phase current transformer in an insulated manner. Therefore, since the position of the power supply line of the three-phase motor is fixed in the through hole of the zero-phase current transformer, the phase and magnitude of the residual current will not change. As a result, the error factor can be eliminated, and the aforementioned error factor refers to changing the magnitude and phase of the residual current according to the penetration position of each three-phase wiring in the through hole of the zero-phase current transformer. Therefore, the residual current can be corrected, and the leakage current of the minute resistance component of nA level can be measured.
又,在本揭示一態樣的絕緣測量裝置中,還具備控制部,其係使用在貫通電流比流器所檢測之至少一個貫通電流,來修正經檢測之零相電流,並測量電阻分量洩漏電流。 In addition, the insulation measurement device according to the aspect of the present disclosure further includes a control unit that uses at least one penetration current detected by the penetration current rectifier to correct the detected zero-phase current and measure the resistance component leakage Current.
藉此,因為使用在貫通電流比流器所檢測之至少一個貫通電流,來修正測量零相電流,故能夠排除基於三相電動機之電動機容量的誤差因子。又,因為在控制部測量電阻分量洩漏電流,故能夠在修正測量零相電流後,求得真正的電阻分量洩漏電流(Ior)。 With this, since at least one penetration current detected by the penetration current rectifier is used to correct the measured zero-phase current, an error factor based on the motor capacity of the three-phase motor can be eliminated. In addition, since the resistance component leakage current is measured by the control unit, the true resistance component leakage current (Ior) can be obtained after the zero-phase current is corrected and measured.
因此,能夠提供一種絕緣測量裝置及絕緣測量方法,其係能夠確實地去除檢測時的誤差因子,並精確度良好地求得真正的電阻分量洩漏電 流。更甚者,因為能夠及早發現三相電動機的絕緣劣化,故能夠有計畫地保全。 Therefore, it is possible to provide an insulation measurement device and an insulation measurement method which can surely remove the error factor at the time of detection and accurately obtain the true resistance component leakage current flow. What's more, because the insulation deterioration of the three-phase motor can be detected early, it can be preserved in a planned way.
在本揭示一態樣的絕緣測量裝置中,前述導電部件較佳係具有剛性。 In the insulation measuring device of the aspect of the present disclosure, the conductive member preferably has rigidity.
藉此,在零相比流器的貫通孔的內部固定支撐各導電部件的情況下,能夠使用簡單的支撐部件並使導電部件不容易移動。 Thereby, when each conductive member is fixedly supported inside the through hole of the zero-phase current regulator, a simple support member can be used and the conductive member cannot be easily moved.
又,在本實施形態的絕緣測量裝置中,前述控制部係可具備:第一測量零相電流取得部,其係從由前述零相比流器所檢測之零相電流,來測量該零相電流的大小及相位,以求得測量零相電流;第一修正部,其係使用對應於任意貫通電流的殘留電流修正值,演算出因應在貫通電流比流器檢測之貫通電流的電流對應修正值,並對於前述測量零相電流使用該電流對應修正值,來修正測量零相電流並求得修正後的零相電流;第一電壓取得部,其係測量前述導電部件中的至少一個的相配線間電壓之大小及相位,並取得導電部件電壓;第一演算部,其係藉由前述修正後的零相電流與前述導電部件電壓,並演算出電阻分量洩漏電流。 In addition, in the insulation measurement device of this embodiment, the control unit may include a first measurement zero-phase current acquisition unit that measures the zero-phase from the zero-phase current detected by the zero-phase current comparator The magnitude and phase of the current to obtain the measured zero-phase current; the first correction unit uses the residual current correction value corresponding to any penetrating current to calculate the corresponding correction of the penetrating current corresponding to the penetrating current detected by the penetrating current ratio. Value, and use the current corresponding correction value for the aforementioned measured zero-phase current to correct the measured zero-phase current and obtain the corrected zero-phase current; a first voltage acquisition unit that measures the phase of at least one of the aforementioned conductive members The magnitude and phase of the voltage between the wirings and the voltage of the conductive component are obtained; the first calculation unit calculates the resistance component leakage current by using the corrected zero-phase current and the conductive component voltage.
藉此,第一測量零相電流取得部係從由零相比流器所檢測之零相電流,來測量該零相電流的大小及相位,並求得測量零相電流。 With this, the first measured zero-phase current acquisition unit measures the magnitude and phase of the zero-phase current from the zero-phase current detected by the zero-phase current comparator, and obtains the measured zero-phase current.
又,第一修正部係使用對應於任意貫通電流的殘留電流修正值,演算出因應在貫通電流比流器所檢測之貫通電流的電流對應修正值,並對於測量零相電流使用該電流對應修正值,修正測量零相電流,且求得修正後的零相電流。此修正後的零相電流係顯示接近真正的零相電流。 In addition, the first correction unit uses the residual current correction value corresponding to any penetrating current, calculates the current corresponding correction value corresponding to the penetrating current detected by the penetrating current ratio, and uses the current corresponding correction for measuring the zero-phase current Value, correct the measured zero-phase current, and find the corrected zero-phase current. This corrected zero-phase current shows close to true zero-phase current.
接著,第一電壓取得部係測量導電部件的至少一個的相配線間電壓之大小及相位,並取得導電部件電壓。第一演算部係藉由修正後的零相電流與導電部件電壓,演算出電阻分量洩漏電流。 Next, the first voltage acquiring unit measures the magnitude and phase of the voltage between the phase wires of at least one of the conductive members, and acquires the conductive member voltage. The first calculation unit calculates the resistance component leakage current by the corrected zero-phase current and the voltage of the conductive member.
結果,具體來說,能夠提供一種絕緣測量裝置,其係能夠確實地去除檢測時的誤差因子,並精確度良好地求得真正的電阻分量洩漏電流。 As a result, specifically, it is possible to provide an insulation measurement device that can surely remove the error factor at the time of detection and accurately obtain the true resistance component leakage current with good accuracy.
又,在本揭示一態樣的絕緣測量裝置中,前述第一修正部係從第一殘留電流與第二殘留電流,來預先求得對應任意貫通電流之殘留電流修正值,其中,第一殘留電流係包含誤差,其係因應第一貫通電流流過前述導電部件時之在前述貫通電流比流器所檢測的該第一貫通電流的大小;第二殘留電流係包含誤差,其係因應第二貫通電流流過前述導電部件時之在前述貫通電流比流器所檢測的該第二貫通電流的大小。 Furthermore, in the insulation measurement device according to the aspect of the present disclosure, the first correction unit obtains a residual current correction value corresponding to any through current in advance from the first residual current and the second residual current. The current includes an error, which corresponds to the magnitude of the first through current detected by the through current than the current penetrator when the first through current flows through the conductive member; the second residual current includes an error, which corresponds to the second When the penetrating current flows through the conductive member, the magnitude of the second penetrating current detected by the penetrating current is greater than that of the current penetrator.
換言之,申請人係能夠確定貫通電流的大小與殘留電流的大小係呈線性變化的特性。因此,預先準備將對應於任意貫通電流之殘留電流修正值作為修正式。 In other words, the applicant system can determine that the magnitude of the through current and the magnitude of the residual current vary linearly. Therefore, a residual current correction value corresponding to an arbitrary through current is prepared as a correction formula in advance.
具體而言,因為對應於任意貫通電流之殘留電流修正值的修正式係能夠以貫通電流的一次式來表示,藉由第一貫通電流流動時的第一殘留電流與第二貫通電流流動時的第二殘留電流,能夠求得修正式的斜率及截距。結果,能夠求得對應於任意貫通電流的殘留電流修正值。 Specifically, because the correction formula corresponding to the correction value of the residual current of any penetration current can be expressed as a linear expression of the penetration current, the first residual current when the first penetration current flows and the second residual current when it flows For the second residual current, the slope and intercept of the correction formula can be obtained. As a result, the residual current correction value corresponding to any through current can be obtained.
因此,因為能夠使用修正式,來決定由貫通電流的大小而變化之殘留電流的修正值,能夠省去使用者修正的時間,且能夠提供具有便利性的絕緣測量裝置。 Therefore, since the correction formula can be used to determine the correction value of the residual current that changes according to the magnitude of the through current, the time for the user to correct can be saved, and a convenient insulation measurement device can be provided.
在本揭示一態樣的絕緣測量裝置中,能夠設置3個前述貫通電流比流器,且其係分別檢測流動於各前述導電部件的貫通電流。 In the insulation measurement device according to the aspect of the present disclosure, three of the through-current current transformers can be provided, and each of them detects the through-current flowing through each of the conductive members.
換言之,具有因為電源環境惡化,而產生電流不平衡,且貫通電流在各相產生變化之情形。也就是說,具有三相配線的貫通電流各自為不同之情形。結果,根據在各相之貫通電流的電流不平衡,而使殘留電流的修正值產生變化。 In other words, there is a case where current imbalance occurs due to the deterioration of the power supply environment, and the through current changes in each phase. In other words, the through currents with three-phase wiring are different. As a result, the correction value of the residual current changes according to the imbalance of the current passing through each phase.
然而,在本揭示一態樣的絕緣測量裝置中,因為設置3個貫通電流比流器,以分別檢測流過各導電部件之貫通電流,故藉由測量各相的貫通電流,能夠不斷地監測不平衡狀態的貫通電流。因此,能夠進行配合電流不平衡的修正。 However, in the insulation measurement device of the aspect of the present disclosure, since three penetrating current comparators are provided to separately detect the penetrating current flowing through each conductive member, it is possible to continuously monitor by measuring the penetrating current of each phase Unbalanced through current. Therefore, it is possible to correct the imbalance of the matching current.
又,在本揭示一態樣的絕緣測量裝置中,前述控制部係能夠具備:第二測量零相電流取得部,其係從由前述零相比流器所檢測之零相電流,來測量該零相電流的大小及相位,以求得測量零相電流;第二修正部,其係在預先求得對應任意貫通電流之殘留電流修正值的同時,演算出因應在前述貫通電流比流器所檢測之流過各前述導電部件的各前述貫通電流之電流對應修正值,並對於前述測量零相電流使用該電流對應修正值,來修正前述測量零相電流並求得修正後的零相電流;第二電壓取得部,其係測量前述導電部件的相配線間電壓之大小及相位,並取得導電部件電壓;第二演算部,其係藉由前述修正後的零相電流與導電部件電壓,演算前述電阻分量洩漏電流。 In addition, in the insulation measurement device according to the aspect of the present disclosure, the control unit can include: a second measurement zero-phase current acquisition unit that measures the zero-phase current detected by the zero-phase current transformer The magnitude and phase of the zero-phase current to obtain the measured zero-phase current; the second correction unit is to obtain the correction value of the residual current corresponding to any penetrating current in advance, and to calculate the response to the above penetrating current ratio. The detected current corresponding to each of the through currents flowing through the conductive members corresponds to the correction value, and the current corresponding correction value is used for the measured zero-phase current to correct the measured zero-phase current and obtain the corrected zero-phase current; The second voltage acquisition part, which measures the magnitude and phase of the voltage between the phase wires of the conductive member, and obtains the voltage of the conductive member; the second calculation part, which calculates from the corrected zero-phase current and the conductive member voltage The aforementioned resistance component leakage current.
藉此,第二測量零相電流取得部係從由零相比流器所檢測之零相電流,來測量該零相電流的大小及相位,並求得測量零相電流。 With this, the second measured zero-phase current acquisition unit measures the magnitude and phase of the zero-phase current from the zero-phase current detected by the zero-phase current transformer, and obtains the measured zero-phase current.
又,第二修正部係在預先求得對應任意貫通電流之殘留電流修正值的同時,演算出因應在前述貫通電流比流器所檢測之各貫通電流的電流對應修正值,並對於測量零相電流使用該電流對應修正值,來修正測量零相電流並求得修正後的零相電流。此修正後的零相電流係顯示接近真正的零相電流。 In addition, the second correction unit calculates the correction value of the current corresponding to each of the through currents detected by the through current ratio while calculating the residual current correction value corresponding to any through current in advance, and measures the zero phase The current uses the corresponding correction value of the current to correct the measured zero-phase current and obtain the corrected zero-phase current. This corrected zero-phase current shows close to true zero-phase current.
接著,第二電壓取得部係測量導電部件的相配線間電壓之大小及相位,並取得導電部件電壓。第二演算部係藉由修正後的零相電流與導電部件電壓,演算出電阻分量洩漏電流。 Next, the second voltage acquiring unit measures the magnitude and phase of the voltage between the phase wires of the conductive member, and acquires the voltage of the conductive member. The second calculation unit calculates the leakage current of the resistance component by the corrected zero-phase current and the voltage of the conductive member.
結果,具體來說,在不平衡狀態的貫通電流流過各導電部件的情況下,能夠提供一種絕緣測量裝置,其係能夠確實地去除檢測時的誤差因子,並精確度良好地求得真正的電阻分量洩漏電流。 As a result, specifically, in the case where an unbalanced through current flows through each conductive member, it is possible to provide an insulation measurement device that can surely remove the error factor at the time of detection and accurately obtain the true Resistance component leakage current.
在本揭示一態樣之絕緣測量裝置中,前述控制部係能夠設置於由遮蔽電及磁的遮蔽材料而成之殼體的內部。 In the insulation measuring device according to the aspect of the present disclosure, the aforementioned control unit can be provided inside a housing made of a shielding material that shields electricity and magnetism.
藉此,藉由使用由遮蔽材料而成之殼體覆蓋控制部,能夠從微小的雜訊隔離控制部。藉此,能夠減少感應雜訊的誤差,能夠進行nA等級之微小電流測量。 In this way, by covering the control portion with a housing made of a shielding material, the control portion can be isolated from minute noise. In this way, errors in induced noise can be reduced, and minute current measurements of nA level can be performed.
又,本揭示並不限定於上述各實施形態,可在請求項所示之範圍內做各種的變更,且將不同的實施形態中所揭示之技術手段適宜地組合而得之實施形態亦包含在本揭示的技術範圍內。又,能夠藉由組合各實施形態各自揭示的技術手段,而形成新的技術特徵。 In addition, the present disclosure is not limited to the above-mentioned embodiments, various changes can be made within the scope shown in the claims, and embodiments obtained by appropriately combining the technical means disclosed in different embodiments are also included in Within the technical scope of this disclosure. In addition, new technical features can be formed by combining the technical means disclosed in each embodiment.
1:電源 1: power supply
2:三相電動機 2: three-phase motor
10A:絕緣測量裝置 10A: Insulation measuring device
11:匯流排(導電部件) 11: busbar (conductive parts)
12:零相比流器(ZCT) 12: ZCT (ZCT)
12a,13a:貫通孔 12a, 13a: through hole
13:貫通電流比流器(CT) 13: through current ratio (CT)
14:控制部 14: Control Department
14a:測量零相電流取得部(第一測量零相電流取得部) 14a: Measurement zero-phase current acquisition section (first measurement zero-phase current acquisition section)
14b:修正部(第一修正部) 14b: Correction section (first correction section)
14c:電壓取得部(第一電壓取得部) 14c: Voltage acquisition unit (first voltage acquisition unit)
14d:演算部(第一演算部) 14d: Calculation Department (First Calculation Department)
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