JP2017020954A - Insulation resistance monitoring device in direct current non-grounded electric circuit and monitoring method - Google Patents

Insulation resistance monitoring device in direct current non-grounded electric circuit and monitoring method Download PDF

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JP2017020954A
JP2017020954A JP2015140117A JP2015140117A JP2017020954A JP 2017020954 A JP2017020954 A JP 2017020954A JP 2015140117 A JP2015140117 A JP 2015140117A JP 2015140117 A JP2015140117 A JP 2015140117A JP 2017020954 A JP2017020954 A JP 2017020954A
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純也 中村
Junya Nakamura
純也 中村
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Hikari Trading Co Ltd
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Abstract

PROBLEM TO BE SOLVED: To solve a problem that an insulation resistance monitoring of a direct current non-grounded electric circuit requires not only an insulation resistance value between an entire electric circuit and a ground, but also the insulation resistance monitoring is required even for each of positive/negative poles since the insulation resistance value of the positive/negative poles placed under the same environment is deteriorated.SOLUTION: An insulation resistance monitoring device connects in series an arbitrary one line of a positive pole side or a negative pole side of a direct current non-grounded electric circuit and a detection resistance body R, and applies rectangular wave signals of a H level and a L level to this resistance body Rfrom rectangular wave signal generation detection means. A both end voltage of the resistance body Rat each level signal is measured when the rectangular wave signal is at the H level and the L level and a line voltage V between the electric circuit are measured so as to be inputted into insulation resistance calculation means. The insulation resistance calculation means is configured to calculate the insulation resistance value between the whole electric circuit and the ground, and the insulation resistance value at the positive pole side and the negative pole side, respectively.SELECTED DRAWING: Figure 1

Description

本発明は、直流非接地式電路における絶縁抵抗監視装置と監視方法に関するものである。   The present invention relates to an insulation resistance monitoring device and a monitoring method in a DC non-grounded electric circuit.

直流非接地式電路における絶縁抵抗検出装置としては特許文献1が公知となっている。図6は、特許文献1での絶縁抵抗検出装置の等価回路を示したもので、太陽電池に接続された直流非接地式電路と大地E間に、V1,V2と電圧値の異なる直流電源をそれぞれ抵抗Rd1,Rd2を介して各別に接続する。接続された直流電源を切換スイッチSによりV1側、V2側と交互に切換えて抵抗に電圧を印加し、印加電圧差により変化した電流変化量から直流非接地式電路と大地E間の絶縁抵抗を求めている。 Patent Document 1 is known as an insulation resistance detection device in a DC ungrounded circuit. FIG. 6 shows an equivalent circuit of the insulation resistance detection device disclosed in Patent Document 1. Between direct current ungrounded circuit connected to the solar cell and ground E, direct currents having different voltage values from V 1 and V 2 are shown. The power supplies are connected separately via resistors Rd 1 and Rd 2 , respectively. The connected DC power source is alternately switched between the V 1 side and the V 2 side by the changeover switch S, and a voltage is applied to the resistor. The insulation between the DC non-grounded circuit and the ground E is determined from the amount of change in the current due to the applied voltage difference. Seeking resistance.

特開2013−33827JP2013-33827A

特許文献1で求められる絶縁抵抗値は、直流非接地式電路全体と大地E間の絶縁抵抗値であって、直流非接地式電路の正極側、または負極側の電路のそれぞれ片側毎の絶縁抵抗値を求めたことにはならない。したがって、絶縁抵抗検出装置として、例えば正・負極の何れか一方、或いは両極側の何れかの絶縁抵抗値が100kΩ以下になったら警報を出すように設定していたとき、正極側、または負極側がともに200kΩまで絶縁抵抗値が低下すると、求められた絶縁抵抗値は、正・負極の並列合成値となるため100kΩとなり、設定値より早く警報を出してしまうことになる。   The insulation resistance value obtained in Patent Document 1 is an insulation resistance value between the entire DC non-grounded circuit and the ground E, and is an insulation resistance for each one side of the positive or negative side of the DC non-grounded circuit. I didn't ask for a value. Therefore, when the insulation resistance detection device is set to issue an alarm when the insulation resistance value of either one of the positive and negative electrodes, or both of the electrode sides becomes 100 kΩ or less, the positive electrode side or the negative electrode side is When the insulation resistance value decreases to 200 kΩ in both cases, the obtained insulation resistance value becomes a combined value of the positive and negative electrodes and becomes 100 kΩ, and an alarm is issued earlier than the set value.

直流非接地式電路の正・負両極の絶縁抵抗値が略同時に劣化することは、正・負両極とも同じ環境下に置かれるため十分に起こりうる問題である。また、特許文献1では、直流印加電圧を切り換えて計測するため、計測時間に差が生じる。この時間差内で直流非接地式電路の電圧が少し変化しただけで絶縁抵抗値に大きな誤差を生じ、正確な検出ができなくなる課題がある。   The fact that the insulation resistance values of the positive and negative poles of the DC ungrounded circuit are deteriorated substantially simultaneously is a problem that can occur sufficiently because both the positive and negative poles are placed in the same environment. Moreover, in patent document 1, since it measures by switching a direct-current applied voltage, a difference arises in measurement time. Within this time difference, there is a problem that even if the voltage of the DC ungrounded circuit is slightly changed, a large error occurs in the insulation resistance value, and accurate detection cannot be performed.

本発明が目的とするところは、直流電源の切換手段を無くし、直流非接地式電路の正・負両極それぞれの計測、及び両極同時計測を可能として正確な絶縁抵抗値の計測・監視を可能とする直流非接地式電路における絶縁抵抗監視装置と監視方法を提供することにある。   The purpose of the present invention is to eliminate the DC power source switching means, and to measure both the positive and negative poles of the DC non-grounded circuit, and simultaneously measure both poles, enabling accurate measurement and monitoring of the insulation resistance value. An object of the present invention is to provide an insulation resistance monitoring device and a monitoring method for a direct current ungrounded circuit.

本発明は、直流非接地式電路の電路と大地間に設置されて絶縁を監視する絶縁抵抗監視装置において、
前記直流非接地式電路の正極側又は負極側の任意の一線と大地間に接続された検出用抵抗体R0と、
検出用抵抗体R0と直列に接続され、一定電圧のHレベル電圧とLレベル電圧の検出用矩形波信号電圧V0を検出用抵抗体R0に印加する検出用矩形波信号発生手段と、
前記検出用抵抗体R0の両端に接続されて、両端電圧Vr0を計測する検出信号電圧計測手段と、
前記直流非接地式電路の線間電圧Vを計測する線間電圧検出手段と、
前記計測された検出用抵抗体R0の両端電圧Vr0と前記線間電圧Vを入力して絶縁抵抗値を演算する絶縁抵抗演算手段と、
前記絶縁抵抗演算手段による演算結果を計測表示する計測表示/警報手段を備え、
前記絶縁抵抗演算手段は、
前記検出用矩形波信号電圧V0がHレベル電圧のときの線間電圧Vの計測値VHと、前記検出用矩形波信号電圧V0がLレベル電圧のときの線間電圧Vの計測値VLと、前記検出用抵抗体R0の両端電圧の計測値とから前記直流非接地式電路全体と大地間の絶縁抵抗値Rgを演算し、正極側絶縁抵抗値Rgp、負極側絶縁抵抗値Rgnとしたときの直流非接地式電路全体と大地間の絶縁抵抗値Rgから正極側絶縁抵抗値Rgpと負極側絶縁抵抗値Rgnを演算するよう構成したことを特徴とする。
The present invention is an insulation resistance monitoring device that is installed between a circuit of a DC non-grounded circuit and the ground and monitors insulation.
A detection resistor R 0 connected between an arbitrary line on the positive electrode side or the negative electrode side of the DC ungrounded circuit and the ground;
Is connected in series with the detection resistor R 0, and for detecting the rectangular wave signal generating means for applying to the detecting resistor R 0 for detection square wave signal voltage V 0 which H-level voltage and L level voltage of a constant voltage,
Is connected to both ends of the detecting resistor R 0, and the detection signal voltage measuring means for measuring the voltage across Vr 0,
A line voltage detecting means for measuring a line voltage V of the DC ungrounded circuit;
Insulation resistance calculation means for calculating an insulation resistance value by inputting the measured both-ends voltage Vr 0 of the detection resistor R 0 and the line voltage V;
A measurement display / alarm means for measuring and displaying the calculation result by the insulation resistance calculation means,
The insulation resistance calculation means includes
A measured value V H of the line voltage V when the detection rectangular wave signal voltage V 0 is an H level voltage, and a measured value of the line voltage V when the detection rectangular wave signal voltage V 0 is an L level voltage. and V L, and calculates the insulation resistance value R g between the DC Nonreferenced path across the earth and a measured value of the voltage across the detecting resistor R 0, the positive electrode side insulation resistance R gp, anode-side insulating characterized by being configured for calculating a DC Nonreferenced path across the positive electrode side insulation resistance from the insulation resistance value R g between the earth R gp and the negative insulation resistance R gn when a resistance value R gn .

本発明での絶縁抵抗演算手段は、絶縁抵抗値Rg、負極側絶縁抵抗値Rgn、正極側絶縁抵抗値Rgpを次式で求めることを特徴としたものである。 The insulation resistance calculation means in the present invention is characterized in that the insulation resistance value R g , the negative electrode side insulation resistance value R gn , and the positive electrode side insulation resistance value R gp are obtained by the following equations.

g=V0×R0/{Vr0H−Vr0L×(VH/VL)}−R0
gn=VL/Vr0L/(1/Rg+1/R0)または、
gn=VH/{(Vr0H+V0)(1/Rg+1/R0)−(V0/R0
gp=(Rg×Rgn)/(Rgn−Rg
ただし、V0:検出用矩形波信号電圧の値は既知、Vr0H:検出用矩形波信号電圧のHレベル電圧、Vr0L:検出用矩形波信号電圧のLレベル電圧、R0:検出用抵抗体で値は既知、VH:検出用矩形波信号電圧V0のHレベル時の線間電圧Vの計測値、VL:検出用矩形波信号電圧V0のLレベル時の線間電圧Vの計測値、
本発明での絶縁抵抗監視方法は、直流非接地式電路の電路と大地間に設置されて絶縁を監視するとき、
前記直流非接地式電路の正極側又は負極側の任意の一線と大地間に接続された検出用抵抗体R0と直列に検出用矩形波信号発生手段を接続し、
検出用矩形波信号発生手段から前記検出用抵抗体R0に一定電圧のHレベル電圧とLレベル電圧の検出用矩形波信号電圧V0を印加し、
Hレベル時における前記直流非接地式電路の線間電圧と前記検出用抵抗体R0の両端電圧を検出信号電圧計測手段で計測し、且つ検出用矩形波信号電圧V0のLレベル時における前記検出用抵抗体R0の両端電圧と前記線間電圧を検出して絶縁抵抗演算手段に入力し、
前記絶縁抵抗演算手段により、直流非接地式電路全体と大地間の絶縁抵抗値を求め、求めた絶縁抵抗値から直流非接地式電路の正極側および負極側の絶縁抵抗値を算出し、算出した値を基に計測表示/警報手段により計測表示及び又は警報することを特徴とする。
R g = V 0 × R 0 / {Vr 0H −Vr 0L × (V H / V L )} − R 0
R gn = V L / Vr 0L / (1 / R g + 1 / R 0 ) or
R gn = V H / {(Vr 0H + V 0 ) (1 / R g + 1 / R 0 ) − (V 0 / R 0 )
R gp = (R g × R gn ) / (R gn −R g )
Where V 0 is the value of the detection rectangular wave signal voltage, Vr 0H is the H level voltage of the detection rectangular wave signal voltage, Vr 0L is the L level voltage of the detection rectangular wave signal voltage, and R 0 is the detection resistor. V H is a measured value of the line voltage V when the detection rectangular wave signal voltage V 0 is at the H level, V L is a line voltage V when the detection rectangular wave signal voltage V 0 is at the L level. Measured value of,
When the insulation resistance monitoring method in the present invention is installed between the circuit and the ground of the DC non-grounded circuit, the insulation is monitored.
A detection rectangular wave signal generating means is connected in series with a detection resistor R 0 connected between an arbitrary line on the positive electrode side or the negative electrode side of the DC ungrounded circuit and the ground,
A detection rectangular wave signal voltage V 0 is applied to the detection resistor R 0 from the detection rectangular wave signal generating means to the detection resistor R 0 as a constant voltage H level voltage and an L level voltage.
The line voltage of the DC ungrounded circuit at the H level and the voltage across the detection resistor R 0 are measured by the detection signal voltage measuring means, and the detection rectangular wave signal voltage V 0 is at the L level. The voltage across the detection resistor R 0 and the line voltage are detected and input to the insulation resistance calculation means,
The insulation resistance calculation means calculates the insulation resistance value between the entire DC non-grounded circuit and the ground, and calculates the insulation resistance values on the positive and negative sides of the DC non-grounded circuit from the obtained insulation resistance value. The measurement display / alarm means performs measurement display and / or alarm based on the value.

また、本発明はでの絶縁抵抗演算手段は、
前記検出用矩形波信号電圧V0がHレベルのときの線間電圧Vの計測値VH、前記検出用矩形波信号電圧V0がLレベルのときの線間電圧Vの計測値VL、前記直流非接地式電路全体と大地間の絶縁抵抗値をRg、正極側絶縁抵抗値Rgp、負極側絶縁抵抗値Rgnとしたとき、次の演算式で絶縁抵抗値を求めることを特徴とする。
In the present invention, the insulation resistance calculation means
The measurement value V H of the line voltage V when the detection square wave signal voltage V 0 is H level, the measured value V L of the line voltage V when the detection for the rectangular wave signal voltage V 0 which L level, When the insulation resistance value between the entire DC ungrounded circuit and the ground is R g , the positive side insulation resistance value R gp , and the negative side insulation resistance value R gn , the insulation resistance value is obtained by the following arithmetic expression. And

g=V0×R0/{Vr0H−Vr0L×(VH/VL)}−R0
gn=VL/Vr0L/(1/Rg+1/R0)または、
gn=VH/{(Vr0H+V0)(1/Rg+1/R0)−(V0/R0
gp=(Rg×Rgn)/(Rgn−Rg
ただし、R0:検出用抵抗体で値は既知、V0:検出用矩形波信号電圧の値で既知、Vr0H:検出用矩形波信号電圧のHレベル電圧、Vr0L:検出用矩形波信号電圧のLレベル電圧、VH:検出用矩形波信号電圧V0のHレベル時の線間電圧Vの計測値、VL:検出用矩形波信号電圧V0のLレベル時の線間電圧Vの計測値、
R g = V 0 × R 0 / {Vr 0H −Vr 0L × (V H / V L )} − R 0
R gn = V L / Vr 0L / (1 / R g + 1 / R 0 ) or
R gn = V H / {(Vr 0H + V 0 ) (1 / R g + 1 / R 0 ) − (V 0 / R 0 )
R gp = (R g × R gn ) / (R gn −R g )
Where R 0 is a detection resistor and the value is known, V 0 is a detection rectangular wave signal voltage value, Vr 0H is a detection rectangular wave signal voltage H level voltage, and Vr 0L is a detection rectangular wave signal. L level voltage of voltage, V H : Measurement value of line voltage V when detection rectangular wave signal voltage V 0 is at H level, V L : Line voltage V when detection rectangular wave signal voltage V 0 is at L level Measured value of,

以上のとおり、本発明によれば、次のような効果が得られるものである。
(1)直流非接地式電路の電路と大地間の絶縁監視のための検出用信号として、
直流非接地式電路の正極側又は負極側の一線と大地間に、検出用抵抗体R0を介して矩形波信号を印加することで、特許文献1のような直流電源の切り換え手段を必要とすることがなく、装置構成が簡易となる。
(2)直流非接地式電路の正極側、負極側の何れか一方側の絶縁抵抗値、および両極同時に絶縁劣化するときの絶縁抵抗値を正確に検出できる。
(3)計測時における直流非接地式電路の電圧が変化しても、正確な絶縁抵抗値の計測が可能となる。
As described above, according to the present invention, the following effects can be obtained.
(1) As a detection signal for insulation monitoring between the circuit of the DC non-grounded circuit and the ground,
By applying a rectangular wave signal via the detection resistor R 0 between the positive electrode side or negative electrode side of the DC ungrounded circuit and the ground, a switching means for the DC power supply as in Patent Document 1 is required. Therefore, the apparatus configuration is simplified.
(2) It is possible to accurately detect the insulation resistance value on either the positive electrode side or the negative electrode side of the DC non-grounded circuit, and the insulation resistance value when both electrodes are simultaneously deteriorated.
(3) Even if the voltage of the DC non-grounded circuit during measurement changes, it is possible to accurately measure the insulation resistance value.

本発明の実施形態を示す構成図。The block diagram which shows embodiment of this invention. 説明のための等価回路で、(a)は等価回路、(b)は検出用矩形波信号電圧。It is an equivalent circuit for explanation, (a) is an equivalent circuit, (b) is a rectangular wave signal voltage for detection. 等価回路で、(a)はHレベル(T1)時の等価回路、(b)はLレベル(T2)時の等価回路。An equivalent circuit, (a) is an equivalent circuit at the H level (T 1 ), and (b) is an equivalent circuit at the L level (T 2 ). 電路電圧源が無しでHレベル(T1)と仮定したときの等価回路。Equivalent circuit when assuming the H level (T 1 ) without the circuit voltage source. 線間電圧の変動有無時の説明図で、(a)は変動無し、(b)変動有り。It is explanatory drawing at the time of the presence or absence of the fluctuation | variation of a line voltage, (a) is no fluctuation, (b) There is a fluctuation. 従来の絶縁抵抗監視装置の構成図。The block diagram of the conventional insulation resistance monitoring apparatus.

図1は本発明の実施形態を示す直流非接地式電路における絶縁抵抗監視装置10の構成図を示したものである。11は検出用矩形波信号発生手段で、検出用抵抗体R0を介して直流非接地式電路の正極側Pと大地E間に接続される。12は検出信号電圧計測手段で、検出用抵抗体R0の両端に接続されて両端電圧Vr0を計測する。13は線間電圧検出手段で、直流非接地式電路の正極側Pと負極側N間の線間電圧Vを検出する。14は絶縁抵抗演算手段で、計測された両端電圧Vr0と線間電圧を入力して絶縁抵抗値を演算し、その出力を計測表示/警報手段15に入力して計測値の表示と異常時での警報を行う。 FIG. 1 shows a configuration diagram of an insulation resistance monitoring device 10 in a DC non-grounded electric circuit showing an embodiment of the present invention. Reference numeral 11 denotes a detection rectangular wave signal generating means, which is connected between the positive electrode side P of the DC non-grounded electric circuit and the ground E through the detection resistor R 0 . 12 is a detection signal voltage measuring means, connected to both ends of the detecting resistor R 0 measures the voltage across Vr 0 to. Reference numeral 13 denotes a line voltage detecting means for detecting a line voltage V between the positive electrode side P and the negative electrode side N of the direct current ungrounded circuit. 14 is an insulation resistance calculation means, which calculates the insulation resistance value by inputting the measured both-end voltage Vr 0 and the line voltage, and inputs the output to the measurement display / alarm means 15 to display the measured value and when there is an abnormality. Alarm at.

なお、1は線間電圧Vを有する電路電圧源、2は直流非接地式電路の正極側P、3は直流非接地式電路の負極側N、Rgpは正極側絶縁抵抗、Rgnは負極側絶縁抵抗、V0は検出用矩形波信号電圧である。 1 is a circuit voltage source having a line voltage V, 2 is a positive side P of a DC non-grounded circuit, 3 is a negative side N of the DC non-grounded circuit, R gp is a positive side insulation resistance, and R gn is a negative side The side insulation resistance, V 0, is a detection rectangular wave signal voltage.

図2は説明のための等価回路を示したもので、図2(a)で示すように検出用矩形波信号発生手段11は検出用抵抗体R0に対して生成された検出用矩形波信号電圧V0を印加する。検出信号電圧計測手段12は、図2(b)の(ア)で示すように矩形波信号のHレベル(T1)が印加されたときの線間電圧VHと、その時の検出用抵抗体R0の両端電圧Vr0Hを計測する。次に、矩形波信号のLレベル(T2)が印加されたときの線間電圧VLと、その時の検出用抵抗体R0の両端電圧Vr0Lを計測し、各計測値を絶縁抵抗演算手段14に出力する。 FIG. 2 shows an equivalent circuit for explanation. As shown in FIG. 2A, the detection rectangular wave signal generating means 11 is a detection rectangular wave signal generated for the detection resistor R 0 . A voltage V 0 is applied. The detection signal voltage measuring means 12 includes a line voltage V H when the H level (T 1 ) of the rectangular wave signal is applied and a detection resistor at that time, as shown in FIG. The voltage Vr 0H across R 0 is measured. Next, the line voltage V L when the L level (T 2 ) of the rectangular wave signal is applied and the voltage Vr 0L across the detection resistor R 0 at that time are measured, and each measured value is calculated as an insulation resistance. Output to means 14.

図3(a)は矩形波信号がHレベル(T1)のときの等価回路、図3(b)は矩形波信号がLレベル(T2)のときの等価回路を示す。ただし、矩形波信号レベル(T1)、(T2)の計測時に線間電圧Vに変動がないときは、V=VH=VLとする。図3(a)の矩形波信号がHレベル(T1)で抵抗体Rgn、Rgp、R0に流れる電流をそれぞれInH,IpH,I0Hとし、図3(b)の矩形波信号がLレベル(T2)のときのそれぞれの電流をInL,IpL,I0Lとする。 3A shows an equivalent circuit when the rectangular wave signal is at the H level (T 1 ), and FIG. 3B shows an equivalent circuit when the rectangular wave signal is at the L level (T 2 ). However, if there is no fluctuation in the line voltage V when measuring the rectangular wave signal levels (T 1 ) and (T 2 ), V = V H = V L. When the rectangular wave signal in FIG. 3A is at the H level (T 1 ), the currents flowing through the resistors R gn , R gp , and R 0 are I nH , I pH , and I 0H , respectively , and the rectangular wave in FIG. signal to the respective current when the L-level (T 2) I nL, I pL, and I 0L.

次に、線間電圧Vが無いと仮定し、検出用矩形波信号電圧V0がHレベル(T1)としたときの等価回路は図4となり、その時の抵抗体Rgn、Rgp、R0に流れる電流をそれぞれInf,Ipf,I0fとすると、線間電圧VH有りで検出用矩形波信号電圧V0がHレベル(T1)としたときの電流InH,IpH,I0Hは、重ね合わせの理により式(1)〜(3)となる。
nH=InL+Inf … (1)
pH=IpL+Ipf … (2)
0H=I0L+I0f … (3)
0HとI0Lは、検出用抵抗体R0の両端電圧Vr0H,Vr0Lを計測することで式(4)、(5)より求めることができる。
0H=Vr0H/R0 … (4)
0L=Vr0L/R0 … (5)
検出用抵抗体R0を流れる電流I0fは、式(3)、(4)、(5)より
0f=I0H−I0L=Vr0H/R0−Vr0L/R0=(Vr0H−Vr0L)/R0…(6)
となる。
0fは、線間電圧Vが無く検出用矩形波信号電圧V0がHレベル(T1)であると仮定したときに検出用抵抗体R0に流れる電流とみなすことができるから、
0−R0×I0f−Rg×I0f=0 … (7)
となり、
正極側絶縁抵抗Rgpと負極側絶縁抵抗Rgnの並列合成抵抗Rg=Rgp×Rgn/(Rgp+Rgn)は、式(6)、(7)から式(8)により求められる。
g=V0/I0f−R0=V0×R0/(Vr0H−Vr0L)−R0 … (8)
次に、検出用矩形波信号電圧V0がHレベル(T1)のとき線間電圧がVHで、検出用矩形波信号電圧V0がLレベル(T2)のとき線間電圧がVLに変動したとすると、その際には誤差が発生することになるが、その時の等価回路を図5で示し、以下の演算で説明する。
Next, assuming that there is no line voltage V, the equivalent circuit when the detection rectangular wave signal voltage V 0 is at the H level (T 1 ) is shown in FIG. 4, and the resistors R gn , R gp , R at that time Assuming that the currents flowing in 0 are I nf , I pf , and I 0f , respectively , currents I nH , I pH , when the detection rectangular wave signal voltage V 0 is at the H level (T 1 ) with the line voltage V H. I 0H is expressed by equations (1) to (3) based on the principle of superposition.
I nH = I nL + I nf (1)
I pH = I pL + I pf (2)
I 0H = I 0L + I 0f (3)
I 0H and I 0L can be obtained from equations (4) and (5) by measuring the voltages Vr 0H and Vr 0L across the detection resistor R 0 .
I 0H = Vr 0H / R 0 (4)
I 0L = Vr 0L / R 0 (5)
The current I 0f flowing through the detection resistor R 0 is calculated from the equations (3), (4), and (5) as follows: I 0f = I 0H −I 0L = Vr 0H / R 0 −Vr 0L / R 0 = (Vr 0H −Vr 0L ) / R 0 (6)
It becomes.
I 0f can be regarded as a current flowing through the detection resistor R 0 when it is assumed that there is no line voltage V and the detection rectangular wave signal voltage V 0 is at the H level (T 1 ).
V 0 −R 0 × I 0f −R g × I 0f = 0 (7)
And
The parallel combined resistance R g = R gp × R gn / (R gp + R gn ) of the positive electrode side insulation resistance R gp and the negative electrode side insulation resistance R gn is obtained from the equations (6), (7) to (8). .
R g = V 0 / I 0f −R 0 = V 0 × R 0 / (Vr 0H −Vr 0L ) −R 0 (8)
Next, when the detection rectangular wave signal voltage V 0 is H level (T 1 ), the line voltage is V H , and when the detection rectangular wave signal voltage V 0 is L level (T 2 ), the line voltage is V If it changes to L , an error will occur at that time. The equivalent circuit at that time is shown in FIG. 5 and will be explained by the following calculation.

検出用矩形波信号電圧V0がLレベル(T2)の計測時に線間電圧Vの変動が無いとき(V=VH=VL)のInLは、
nL=VL/{Rgn+(Rgp×R0)/(Rgp+R0)} … (9)
となり、検出用抵抗体R0に流れる電流I0Lは、分流の法則により
0L=InL×Rgp/(Rgp+R0) … (10)
となる。
I nL when the detection square wave signal voltage V 0 there is no variation in the line voltage V when measuring the L level (T 2) (V = V H = V L) is
I nL = V L / {R gn + (R gp × R 0) / (R gp + R 0)} ... (9)
Thus, the current I 0L flowing through the detection resistor R 0 is expressed as I 0L = I nL × R gp / (R gp + R 0 ) (10)
It becomes.

計測時の線間電圧Vに変動があり、そのときの線間電圧をVLXとしたときの電流InLXは、
nLX=VLX/{Rgn+(Rgp×R0)/(Rgp+R0)} … (11)
となり、検出用抵抗体R0に流れる電流I0LXは、分流の法則により
0LX=InLX×Rgp/(Rgp+R0) … (12)
となり、式(9)〜(12)より
0L/I0LX=InL/InLX=VL/VLX
0L=I0LX×(VL/VLX
線間電圧Vに変動が無いときのVLは、VL=VHであるから両辺にR0を掛けて、
0×I0L=R0×I0LX×(VH/VLX
Vr0L=Vr0LX×(VH/VLX
となり、線間電圧Vが変動する前のVr0Lの値は、線間電圧Vが変動したときに検出したVr0LXの値に(VH/VLX)を掛けることで求めることが出来る。このVLXおよびVr0LXは線間電圧変動時に計測したVL、Vr0Lであるから、式(8)を
g=V0×R0/{Vr0H−Vr0L×(VH/VL)}−R0 … (13)
とすることで、線間電圧変動時の誤差を無くすことができる。
The line voltage V at the time of measurement varies, and the current InLX when the line voltage at that time is V LX is
I nLX = V LX / {R gn + (R gp × R 0) / (R gp + R 0)} ... (11)
Thus, the current I 0LX flowing through the detection resistor R 0 is I 0LX = InLX × R gp / (R gp + R 0 ) (12) according to the law of shunting.
Next, I the equation (9) ~ (12) 0L / I 0LX = I nL / I nLX = V L / V LX
I 0L = I 0LX × (V L / V LX )
V L when there is no fluctuation in the line voltage V is V L = V H , so both sides are multiplied by R 0 ,
R 0 × I 0L = R 0 × I 0LX × (V H / V LX )
Vr 0L = Vr 0LX × (V H / V LX )
Thus, the value of Vr 0L before the line voltage V fluctuates can be obtained by multiplying the value of Vr 0LX detected when the line voltage V fluctuates by (V H / V LX ). Since V LX and Vr 0LX are V L and Vr 0L measured at the time of line voltage fluctuation, Equation (8) can be changed to R g = V 0 × R 0 / {Vr 0H −Vr 0L × (V H / V L )}-R 0 (13)
By doing so, the error at the time of line voltage fluctuation can be eliminated.

次に、矩形波信号がLレベル(T2)の計測時の値から、Rgp、Rgnをそれぞれ求める。図3(b)の場合、直流非接地式電路の正極側Pと大地E間の電圧Vpeは、ミルマンの定理を用いると
pe=(VL/Rgn+0/Rgp+0/R0)/(1/Rgn+1/Rgp+1/R0
=(VL/Rgn)/(1/Rg+1/R0) … (14)
で現すことができ、検出用抵抗体R0は既知で、線間電圧VLは線間電圧検出手段13で計測され、また、Vpe=Vr0Lで検出用抵抗体R0の両端電圧が検出信号電圧計測手段12で計測される。
Next, R gp and R gn are respectively obtained from values at the time when the rectangular wave signal is measured at the L level (T 2 ). In the case of FIG. 3B, the voltage V pe between the positive electrode side P of the DC ungrounded circuit and the ground E is V pe = (V L / R gn + 0 / R gp + 0 / R 0 , using Milman's theorem. ) / (1 / R gn + 1 / R gp + 1 / R 0 )
= (V L / R gn ) / (1 / R g + 1 / R 0 ) (14)
Can be expressed by, detecting resistor R 0 is known, the line voltage V L is measured in the line voltage detecting unit 13, also the voltage across the V pe = detecting resistor at Vr 0L R 0 is It is measured by the detection signal voltage measuring means 12.

絶縁抵抗演算手段14では、直流非接地式電路全体と大地間の絶縁抵抗値Rgを式(13)で求められることから、負極側絶縁抵抗値Rgnを式(14)より式(15)で求める。
gn=VL/Vr0L/(1/Rg+1/R0) … (15)
よって、正極側絶縁抵抗値/Rgpは、
gp=(Rg×Rgn)/(Rgn−Rg) … (16)
で求めることができる。
In the insulation resistance computing means 14, a DC Nonreferenced path across the insulation resistance value R g between the earth because it is determined by the formula (13), wherein the negative electrode side insulation resistance R gn (14) from equation (15) Ask for.
R gn = V L / Vr 0L / (1 / R g + 1 / R 0 ) (15)
Therefore, the positive-side insulation resistance value / R gp is
R gp = (R g × R gn ) / (R gn −R g ) (16)
Can be obtained.

なお、上記では検出用矩形波信号電圧V0がLレベル(T2)の計測時の値から求める方法についての説明であるが、Hレベル(T1)の計測時の値からも求めることができ、負極側絶縁抵抗値Rgnの演算式は式(17)となる。正極側絶縁抵抗値Rgpは同様に式(16)で求められる。
gn=VH/{(Vr0H+V0)(1/Rg+1/R0)−(V0/R0) … (17)
また、図1の構成では、検出用矩形波信号発生手段11を直流非接地式電路の正極側Pと大地E間に接続した場合を示しているが、検出用矩形波信号発生手段11は負極側Nと大地E間に接続してもよい。その場合、図2(a)で示す電路の線間電圧Vの極性を反転させたと同じであり、式(15)、(16)、(17)の符号Rgn,Rgnを換えることで、同様にして求めることができる。
In the above description, the method for obtaining the detection rectangular wave signal voltage V 0 from the value at the time of measurement of the L level (T 2 ) has been described, but it can also be obtained from the value at the time of measurement of the H level (T 1 ). In addition, the arithmetic expression of the negative electrode side insulation resistance value R gn is given by Expression (17). Similarly, the positive electrode side insulation resistance value R gp is obtained by the equation (16).
R gn = V H / {(Vr 0H + V 0 ) (1 / R g + 1 / R 0 ) − (V 0 / R 0 ) (17)
1 shows a case where the detection rectangular wave signal generating means 11 is connected between the positive electrode side P of the DC non-grounded electric circuit and the ground E, the detection rectangular wave signal generating means 11 is a negative electrode. You may connect between side N and ground E. In that case, it is the same as the polarity of the line voltage V of the electric circuit shown in FIG. 2A is reversed, and by changing the signs R gn and R gn of the equations (15), (16) and (17), It can be obtained in the same way.

また、図2(b)では、検出用矩形波信号発生手段11による矩形波信号のHレベルをプラス電圧、Lレベルを零ボルトとしているが、Hレベルを零ボルト、Lレベルをマイナス電圧としてもよい。また、検出用矩形波信号発生回路および演算は複雑となるが、矩形波信号のHレベル、Lレベルのそれぞれに一定の電圧値を持たせても絶縁抵抗値を求めることができる。   In FIG. 2B, the H level of the rectangular wave signal generated by the detection rectangular wave signal generating means 11 is a positive voltage and the L level is zero volts, but the H level is zero volts and the L level is a negative voltage. Good. In addition, although the detection rectangular wave signal generation circuit and the calculation are complicated, the insulation resistance value can be obtained even if the rectangular wave signal has a constant voltage value at each of the H level and the L level.

10… 絶縁抵抗監視装置
11… 検出用矩形波信号発生手段
12… 検出信号電圧計測手段
13… 線間電圧検出手段
14… 絶縁抵抗演算手段
15… 計測表示/警報手段
0… 検出用抵抗体
DESCRIPTION OF SYMBOLS 10 ... Insulation resistance monitoring apparatus 11 ... Detection rectangular wave signal generation means 12 ... Detection signal voltage measurement means 13 ... Line voltage detection means 14 ... Insulation resistance calculation means 15 ... Measurement display / alarm means R0 ... Detection resistor

本発明は、直流非接地式電路の電路と大地間に設置されて絶縁を監視する絶縁抵抗監視装置において、
前記直流非接地式電路の正極側又は負極側の任意の一線と大地間に接続された検出用抵抗体R0と、
検出用抵抗体R0と直列に接続され、一定電圧のHレベル電圧とLレベル電圧の検出用矩形波信号電圧V0を検出用抵抗体R0に印加して検出用抵抗体R0に両端電圧Vr0を発生させる検出用矩形波信号発生手段と、
前記検出用抵抗体R0の両端に接続されて、両端電圧Vr0を計測する検出信号電圧計測手段と、
前記直流非接地式電路の線間電圧Vを計測する線間電圧検出手段と、
前記計測された検出用抵抗体R0の両端電圧Vr0と前記線間電圧Vを入力して絶縁抵抗値を演算する絶縁抵抗演算手段と、
前記絶縁抵抗演算手段による演算結果を計測表示する計測表示手段を備え、
前記絶縁抵抗演算手段は、
前記検出用矩形波信号電圧V0がHレベル電圧のときの線間電圧Vの計測値VHと、前記検出用矩形波信号電圧V0がLレベル電圧のときの線間電圧Vの計測値VLと、前記検出用抵抗体R0の両端電圧の計測値とから前記直流非接地式電路全体と大地間の絶縁抵抗値Rgを演算し、正極側絶縁抵抗値Rgp、負極側絶縁抵抗値Rgnとしたときの直流非接地式電路全体と大地間の絶縁抵抗値Rgから正極側絶縁抵抗値Rgpと負極側絶縁抵抗値Rgnを演算するよう構成したことを特徴とする。
The present invention is an insulation resistance monitoring device that is installed between a circuit of a DC non-grounded circuit and the ground and monitors insulation.
A detection resistor R0 connected between an arbitrary line on the positive electrode side or the negative electrode side of the DC ungrounded circuit and the ground;
Connected in series with the detection resistor R0, a rectangular voltage signal voltage V0 having a constant voltage of H level and L level voltage is applied to the detection resistor R0 to generate a voltage Vr0 across the detection resistor R0. and the rectangular wave signal generating means for detecting the cause,
Detection signal voltage measuring means connected to both ends of the detection resistor R0 and measuring the voltage Vr0 at both ends;
A line voltage detecting means for measuring a line voltage V of the DC ungrounded circuit;
Insulation resistance calculation means for calculating an insulation resistance value by inputting the measured both-ends voltage Vr0 of the detection resistor R0 and the line voltage V;
Comprising measurement display means for measuring and displaying the calculation result by the insulation resistance calculation means,
The insulation resistance calculation means includes
The measured value V H of the line voltage V when the detection rectangular wave signal voltage V0 is the H level voltage, and the measured value V L of the line voltage V when the detection rectangular wave signal voltage V0 is the L level voltage. Then, the insulation resistance value Rg between the whole DC non-grounded circuit and the ground is calculated from the measured value of the voltage across the detection resistor R0 to obtain the positive side insulation resistance value Rgp and the negative side insulation resistance value Rgn. The positive-side insulation resistance value Rgp and the negative-side insulation resistance value Rgn are calculated from the insulation resistance value Rg between the entire DC ungrounded electric circuit and the ground.

本発明の絶縁抵抗演算手段は、
前記絶縁抵抗値Rgを式(3−1)で演算し、求まっ絶縁抵抗値Rgを用いて前記検出用矩形波信号電圧V0がLレベル計測時は式(3−2)で、検出用矩形波信号電圧V0がHレベル計測時には式(3−3)でそれぞれ負極側絶縁抵抗値Rgnを演算し、
正極側絶縁抵抗値Rgpは前記検出用矩形波信号電圧V0がLレベル計測時に式(3−4)で演算すると共に、
前記計測表示手段に、演算結果の負極側絶縁抵抗値Rgn、正極側絶縁抵抗値Rgpを各別に、若しくは両極同時に計測表示することを特徴とする。
Rg=V0×R0/{Vr0 H −Vr0 L ×(V H /V L )}−R0(3−1)
Rgn=V L /Vr0 L /(1/Rg+1/R0)(3−2)
Rgn=V H /{(Vr0 H +V0)(1/Rg+1/R0)−(V0/R0)}(3−3)
Rgp=(Rg×Rgn)/(Rgn−Rg)(3−4)
ただし、V0:検出用抵抗体R0に両端電圧Vr0を発生させる検出用矩形波信号電圧で値は既知、Vr0 H :検出用矩形波信号電圧のHレベル電圧、Vr0 L :検出用矩形波信号電圧のLレベル電圧、R0:検出用抵抗体で値は既知、V H :検出用矩形波信号電圧V0のHレベル時の線間電圧Vの計測値、V L :検出用矩形波信号電圧V0のLレベル時の線間電圧Vの計測値、
Insulation resistance calculation means of the present invention,
The insulation resistance value Rg is calculated by the equation (3-1), and when the detected rectangular wave signal voltage V0 is measured at the L level using the obtained insulation resistance value Rg, the detection rectangle is obtained by the equation (3-2). When the wave signal voltage V0 is measured at the H level, the negative side insulation resistance value Rgn is calculated by the equation (3-3).
The positive-side insulation resistance value Rgp is calculated by the equation (3-4) when the detection rectangular wave signal voltage V0 is measured at the L level, and
The measurement display means is configured to measure and display the negative electrode side insulation resistance value Rgn and the positive electrode side insulation resistance value Rgp separately or both at the same time .
Rg = V0 × R0 / {Vr0 H -Vr0 L × (V H / V L)} - R0 ... (3-1)
Rgn = V L / Vr0 L / (1 / Rg + 1 / R0) (3-2)
Rgn = V H / {(Vr0 H + V0) (1 / Rg + 1 / R0) - (V0 / R0)} ... (3-3)
Rgp = (Rg × Rgn) / (Rgn−Rg) (3-4)
Where V0 is a detection rectangular wave signal voltage for generating a voltage Vr0 across the detection resistor R0, and the value is known, Vr0 H is a high- level voltage of the detection rectangular wave signal voltage , and Vr0 L is a detection rectangular wave signal voltage. L level voltage, R0: detection resistor, value is known, V H : measurement value of line voltage V when detection rectangular wave signal voltage V0 is at H level, V L : detection rectangular wave signal voltage V0 Measured value of line voltage V at L level,

本発明での絶縁抵抗監視方法は、直流非接地式電路の電路と対地間に設置されて絶縁を監視するとき、
前記直流非接地式電路の正極側又は負極側の任意の一線と大地間に接続された検出用抵抗体R0と直列に検出用矩形波信号発生手段を接続し、
検出用矩形波信号発生手段から前記検出用抵抗体R0に一定電圧のHレベル電圧とLレベル電圧の検出用矩形波信号電圧V0を印加して検出用抵抗体R0に両端電圧Vr0を発生させ、
Hレベル時における前記直流非接地式電路の線間電圧と前記検出用抵抗体R0の両端電圧を検出信号電圧計測手段で計測し、且つ検出用矩形波信号電圧V0のLレベル時における前記検出用抵抗体R0の両端電圧と前記線間電圧を検出して絶縁抵抗演算手段に入力し、
前記絶縁抵抗演算手段により、直流非接地式電路全体と大地間の絶縁抵抗値を求め、求めた絶縁抵抗値から直流非接地式電路の正極側および負極側の絶縁抵抗値を算出し、算出した値を基に計測表示手段により計測表示及び警報することを特徴とする。
When the insulation resistance monitoring method in the present invention is installed between the electric circuit of the DC ungrounded electric circuit and the ground and monitors the insulation,
A detection rectangular wave signal generating means is connected in series with a detection resistor R0 connected between an arbitrary line on the positive electrode side or the negative electrode side of the DC ungrounded circuit and the ground,
A detection rectangular wave signal voltage V0 is applied to the detection resistor R0 from the detection rectangular wave signal generating means to generate a voltage Vr0 across the detection resistor R0 .
The line voltage of the DC ungrounded circuit at the H level and the voltage across the detection resistor R0 are measured by the detection signal voltage measuring means, and the detection rectangular wave signal voltage V0 is at the L level. The voltage across the resistor R0 and the line voltage are detected and input to the insulation resistance calculation means,
The insulation resistance calculation means calculates the insulation resistance value between the entire DC non-grounded circuit and the ground, and calculates the insulation resistance values on the positive and negative sides of the DC non-grounded circuit from the obtained insulation resistance value. Based on the value, the measurement display means performs measurement display and alarm.

また、本発明での絶縁抵抗演算手段は、
前記検出用矩形波信号発生手段からの検出用矩形波信号電圧V0がHレベルのときの線間電圧Vの計測値VH、前記検出用矩形波信号電圧V0がLレベルのときの線間電圧Vの計測値VL、前記直流非接地式電路全体と大地間の絶縁抵抗値をRg、正極側絶縁抵抗値Rgp、負極側絶縁抵抗値Rgnとしたとき、
絶縁抵抗値Rgを式(4−1)で演算し、求まった絶縁抵抗値Rgを用いて前記検出用矩形波信号電圧V0がLレベル計測時には式(4−2)で、検出用矩形波信号電圧V0がHレベル計測時には式(4−3)でそれぞれ負極側絶縁抵抗値Rgnを演算し、正極側絶縁抵抗値Rgpは、前記検出用矩形波信号電圧V0がLレベル計測時に式(4−4)で演算すると共に
前記計測表示手段に、算出された負極側絶縁抵抗値Rgn、正極側絶縁抵抗値Rgpを各別に、若しくは両極同時に計測表示することを特徴とする。
Also, the insulation resistance calculation means in the present invention is:
The measured value V H of the line voltage V when the detection rectangular wave signal voltage V0 from the detection rectangular wave signal generating means is at the H level, and the line voltage when the detection rectangular wave signal voltage V0 is at the L level. When the measured value V L of V, the insulation resistance value between the entire DC ungrounded circuit and the ground is Rg, the positive side insulation resistance value Rgp, and the negative side insulation resistance value Rgn,
The insulation resistance value Rg is calculated by the equation (4-1), and when the detected rectangular wave signal voltage V0 is measured at the L level using the obtained insulation resistance value Rg, the detection rectangular wave signal is obtained by the equation (4-2). When the voltage V0 is measured at the H level, the negative electrode side insulation resistance value Rgn is calculated by the equation (4-3). The positive electrode side insulation resistance value Rgp is calculated by the equation (4-4) when the detection rectangular wave signal voltage V0 is measured at the L level. While calculating in 4) ,
The measurement display means displays and displays the calculated negative electrode side insulation resistance value Rgn and positive electrode side insulation resistance value Rgp separately or simultaneously .

Rg=V0×R0/{Vr0H−Vr0L×(VH/VL)}−R0 … (4−1)
Rgn=VL/Vr0L/(1/Rg+1/R0) … (4−2)
Rgn=VH/{(Vr0H+V0)(1/Rg+1/R0)−(V0/R0)…(4−3)
Rgp=(Rg×Rgn)/(Rgn−Rg) … (4−4)
ただし、R0:検出用抵抗体で値は既知、V0:検出用抵抗体R0に両端電圧Vr0を発生させる検出用矩形波信号電圧で値は既知、Vr0H:検出用矩形波信号電圧のHレベル電圧、Vr0L:検出用矩形波信号電圧のLレベル電圧、VH:検出用矩形波信号電圧V0のHレベル時の線間電圧Vの計測値、VL:検出用矩形波信号電圧V0のLレベル時の線間電圧Vの計測値、
Rg = V0 × R0 / {Vr0 H -Vr0 L × (V H / V L)} - R0 ... (4-1)
Rgn = V L / Vr0 L / (1 / Rg + 1 / R0) (4-2)
Rgn = V H / {(Vr0 H + V0) (1 / Rg + 1 / R0) - (V0 / R0)} ... (4-3)
Rgp = (Rg × Rgn) / (Rgn−Rg) (4-4)
Where R0: detection resistor has a known value, V0: detection rectangular wave signal voltage that causes the detection resistor R0 to generate a voltage Vr0 at both ends, and a known value , Vr0H: detection rectangular wave signal voltage H level voltage , Vr0L: L level voltage of the detection rectangular wave signal voltage, VH: Measured value of the line voltage V when the detection rectangular wave signal voltage V0 is H level, VL: When the detection rectangular wave signal voltage V0 is L level Measured value of line voltage V,

図1は本発明の実施形態を示す直流非接地式電路における絶縁抵抗監視装置10の構成図を示したものである。11は検出用矩形波信号発生手段で、検出用抵抗体R0を介して直流非接地式電路の正極側Pと大地E間に接続される。12は検出信号電圧計測手段で、検出用抵抗体R0の両端に接続されて両端電圧Vr0を計測する。13は線間電圧検出手段で、直流非接地式電路の正極側Pと負極側N間の線間電圧Vを検出する。14は絶縁抵抗演算手段で、計測された両端電圧Vr0と線間電圧を入力して絶縁抵抗値を演算し、その出力を計測表示手段15に入力して計測値の表示と異常時での警報を行う。 FIG. 1 shows a configuration diagram of an insulation resistance monitoring device 10 in a DC non-grounded electric circuit showing an embodiment of the present invention. Reference numeral 11 denotes a detection rectangular wave signal generating means, which is connected between the positive electrode side P of the DC non-grounded electric circuit and the ground E through a detection resistor R0. A detection signal voltage measuring means 12 is connected to both ends of the detection resistor R0 and measures a both-end voltage Vr0. Reference numeral 13 denotes a line voltage detecting means for detecting a line voltage V between the positive electrode side P and the negative electrode side N of the direct current ungrounded circuit. 14 is an insulation resistance calculation means, which calculates the insulation resistance value by inputting the measured both-end voltage Vr0 and the line voltage, and inputs the output to the measurement display means 15 to display the measured value and alarm in case of abnormality. I do.

10… 絶縁抵抗監視装置
11… 検出用矩形波信号発生手段
12… 検出信号電圧計測手段
13… 線間電圧検出手段
14… 絶縁抵抗演算手段
15… 計測表示手段
R0… 検出用抵抗体
DESCRIPTION OF SYMBOLS 10 ... Insulation resistance monitoring apparatus 11 ... Detection rectangular wave signal generation means 12 ... Detection signal voltage measurement means 13 ... Line voltage detection means 14 ... Insulation resistance calculation means 15 ... Measurement display means R0 ... Detection resistor

Claims (4)

直流非接地式電路の電路と大地間に設置されて絶縁を監視する絶縁抵抗監視装置において、
前記直流非接地式電路の正極側又は負極側の任意の一線と大地間に接続された検出用抵抗体R0と、
検出用抵抗体R0と直列に接続され、一定電圧のHレベル電圧とLレベル電圧の検出用矩形波信号電圧V0を検出用抵抗体R0に印加する検出用矩形波信号発生手段と、
前記検出用抵抗体R0の両端に接続されて、両端電圧Vr0を計測する検出信号電圧計測手段と、
前記直流非接地式電路の線間電圧Vを計測する線間電圧検出手段と、
前記計測された検出用抵抗体R0の両端電圧Vr0と前記線間電圧Vを入力して絶縁抵抗値を演算する絶縁抵抗演算手段と、
前記絶縁抵抗演算手段による演算結果を計測表示する計測表示/警報手段を備え、
前記絶縁抵抗演算手段は、
前記検出用矩形波信号電圧V0がHレベル電圧のときの線間電圧Vの計測値VHと、前記検出用矩形波信号電圧V0がLレベル電圧のときの線間電圧Vの計測値VLと、前記検出用抵抗体R0の両端電圧の計測値とから前記直流非接地式電路全体と大地間の絶縁抵抗値Rgを演算し、正極側絶縁抵抗値Rgp、負極側絶縁抵抗値Rgnとしたときの直流非接地式電路全体と大地間の絶縁抵抗値Rgから正極側絶縁抵抗値Rgpと負極側絶縁抵抗値Rgnを演算するよう構成したことを特徴とした直流非接地式電路における絶縁抵抗監視装置。
In the insulation resistance monitoring device that is installed between the circuit of the DC ungrounded circuit and the ground and monitors insulation,
A detection resistor R 0 connected between an arbitrary line on the positive electrode side or the negative electrode side of the DC ungrounded circuit and the ground;
Is connected in series with the detection resistor R 0, and for detecting the rectangular wave signal generating means for applying to the detecting resistor R 0 for detection square wave signal voltage V 0 which H-level voltage and L level voltage of a constant voltage,
Is connected to both ends of the detecting resistor R 0, and the detection signal voltage measuring means for measuring the voltage across Vr 0,
A line voltage detecting means for measuring a line voltage V of the DC ungrounded circuit;
Insulation resistance calculation means for calculating an insulation resistance value by inputting the measured both-ends voltage Vr 0 of the detection resistor R 0 and the line voltage V;
A measurement display / alarm means for measuring and displaying the calculation result by the insulation resistance calculation means,
The insulation resistance calculation means includes
A measured value V H of the line voltage V when the detection rectangular wave signal voltage V 0 is an H level voltage, and a measured value of the line voltage V when the detection rectangular wave signal voltage V 0 is an L level voltage. and V L, and calculates the insulation resistance value R g between the DC Nonreferenced path across the earth and a measured value of the voltage across the detecting resistor R 0, the positive electrode side insulation resistance R gp, anode-side insulating and characterized by being configured so as to calculate the DC Nonreferenced path across the positive electrode side insulation resistance from the insulation resistance value R g between the earth R gp and the negative insulation resistance R gn when a resistance value R gn Insulation resistance monitoring device for DC ungrounded circuit.
前記絶縁抵抗演算手段は、絶縁抵抗値Rg、負極側絶縁抵抗値Rgn、正極側絶縁抵抗値Rgpを次式で求めることを特徴とした請求項1記載の直流非接地式電路における絶縁抵抗監視装置。
g=V0×R0/{Vr0H−Vr0L×(VH/VL)}−R0
gn=VL/Vr0L/(1/Rg+1/R0)または、
gn=VH/{(Vr0H+V0)(1/Rg+1/R0)−(V0/R0
gp=(Rg×Rgn)/(Rgn−Rg
ただし、V0:検出用矩形波信号電圧の値は既知、Vr0H:検出用矩形波信号電圧のHレベル電圧、Vr0L:検出用矩形波信号電圧のLレベル電圧、R0:検出用抵抗体で値は既知、VH:検出用矩形波信号電圧V0のHレベル時の線間電圧Vの計測値、VL:検出用矩形波信号電圧V0のLレベル時の線間電圧Vの計測値、
2. The insulation in a DC ungrounded circuit according to claim 1, wherein the insulation resistance calculation means obtains an insulation resistance value R g , a negative electrode side insulation resistance value R gn , and a positive electrode side insulation resistance value R gp by the following equations. Resistance monitoring device.
R g = V 0 × R 0 / {Vr 0H −Vr 0L × (V H / V L )} − R 0
R gn = V L / Vr 0L / (1 / R g + 1 / R 0 ) or
R gn = V H / {(Vr 0H + V 0 ) (1 / R g + 1 / R 0 ) − (V 0 / R 0 )
R gp = (R g × R gn ) / (R gn −R g )
Where V 0 is the value of the detection rectangular wave signal voltage, Vr 0H is the H level voltage of the detection rectangular wave signal voltage, Vr 0L is the L level voltage of the detection rectangular wave signal voltage, and R 0 is the detection resistor. V H is a measured value of the line voltage V when the detection rectangular wave signal voltage V 0 is at the H level, V L is a line voltage V when the detection rectangular wave signal voltage V 0 is at the L level. Measured value of,
直流非接地式電路の電路と大地間に設置されて絶縁を監視する絶縁抵抗監視方法において、
前記直流非接地式電路の正極側又は負極側の任意の一線と大地間に接続された検出用抵抗体R0と直列に検出用矩形波信号発生手段を接続し、
検出用矩形波信号発生手段から前記検出用抵抗体R0に一定電圧のHレベル電圧とLレベル電圧の検出用矩形波信号電圧V0を印加し、
Hレベル時における前記直流非接地式電路の線間電圧と前記検出用抵抗体R0の両端電圧を検出信号電圧計測手段で計測し、且つ検出用矩形波信号電圧V0のLレベル時における前記検出用抵抗体R0の両端電圧と前記線間電圧を検出して絶縁抵抗演算手段に入力し、
前記絶縁抵抗演算手段により、直流非接地式電路全体と大地間の絶縁抵抗値を求め、求めた絶縁抵抗値から直流非接地式電路の正極側および負極側の絶縁抵抗値を算出し、算出した値を基に計測表示/警報手段により計測表示及び又は警報することを特徴とした直流非接地式電路における絶縁抵抗監視方法。
In the insulation resistance monitoring method that is installed between the circuit of the DC ungrounded circuit and the ground and monitors insulation,
A detection rectangular wave signal generating means is connected in series with a detection resistor R 0 connected between an arbitrary line on the positive electrode side or the negative electrode side of the DC ungrounded circuit and the ground,
A detection rectangular wave signal voltage V 0 is applied to the detection resistor R 0 from the detection rectangular wave signal generating means to the detection resistor R 0 as a constant voltage H level voltage and an L level voltage.
The line voltage of the DC ungrounded circuit at the H level and the voltage across the detection resistor R 0 are measured by the detection signal voltage measuring means, and the detection rectangular wave signal voltage V 0 is at the L level. The voltage across the detection resistor R 0 and the line voltage are detected and input to the insulation resistance calculation means,
The insulation resistance calculation means calculates the insulation resistance value between the entire DC non-grounded circuit and the ground, and calculates the insulation resistance values on the positive and negative sides of the DC non-grounded circuit from the obtained insulation resistance value. A method for monitoring insulation resistance in a DC non-grounded electric circuit, wherein measurement display / alarm means is used for measurement display / alarm based on the value.
前記絶縁抵抗演算手段は、
前記検出用矩形波信号電圧V0がHレベルのときの線間電圧Vの計測値VH、前記検出用矩形波信号電圧V0がLレベルのときの線間電圧Vの計測値VL、前記直流非接地式電路全体と大地間の絶縁抵抗値をRg、正極側絶縁抵抗値Rgp、負極側絶縁抵抗値Rgnとしたとき、次の演算式で絶縁抵抗値を求めることを特徴とした請求項3記載の直流非接地式電路における絶縁抵抗監視方法。
g=V0×R0/{Vr0H−Vr0L×(VH/VL)}−R0
gn=VL/Vr0L/(1/Rg+1/R0)または、
gn=VH/{(Vr0H+V0)(1/Rg+1/R0)−(V0/R0
gp=(Rg×Rgn)/(Rgn−Rg
ただし、R0:検出用抵抗体で値は既知、V0:検出用矩形波信号電圧の値で既知、Vr0H:検出用矩形波信号電圧のHレベル電圧、Vr0L:検出用矩形波信号電圧のLレベル電圧、VH:検出用矩形波信号電圧V0のHレベル時の線間電圧Vの計測値、VL:検出用矩形波信号電圧V0のLレベル時の線間電圧Vの計測値、
The insulation resistance calculation means includes
The measurement value V H of the line voltage V when the detection square wave signal voltage V 0 is H level, the measured value V L of the line voltage V when the detection for the rectangular wave signal voltage V 0 which L level, When the insulation resistance value between the entire DC ungrounded circuit and the ground is R g , the positive side insulation resistance value R gp , and the negative side insulation resistance value R gn , the insulation resistance value is obtained by the following arithmetic expression. The insulation resistance monitoring method in the DC ungrounded circuit according to claim 3.
R g = V 0 × R 0 / {Vr 0H −Vr 0L × (V H / V L )} − R 0
R gn = V L / Vr 0L / (1 / R g + 1 / R 0 ) or
R gn = V H / {(Vr 0H + V 0 ) (1 / R g + 1 / R 0 ) − (V 0 / R 0 )
R gp = (R g × R gn ) / (R gn −R g )
Where R 0 is a detection resistor and the value is known, V 0 is a detection rectangular wave signal voltage value, Vr 0H is a detection rectangular wave signal voltage H level voltage, and Vr 0L is a detection rectangular wave signal. L level voltage of voltage, V H : Measurement value of line voltage V when detection rectangular wave signal voltage V 0 is at H level, V L : Line voltage V when detection rectangular wave signal voltage V 0 is at L level Measured value of,
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