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JP6609984B2 - Insulation resistance measuring method and apparatus - Google Patents
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JP6609984B2 - Insulation resistance measuring method and apparatus - Google Patents

Insulation resistance measuring method and apparatus Download PDF

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JP6609984B2
JP6609984B2 JP2015096300A JP2015096300A JP6609984B2 JP 6609984 B2 JP6609984 B2 JP 6609984B2 JP 2015096300 A JP2015096300 A JP 2015096300A JP 2015096300 A JP2015096300 A JP 2015096300A JP 6609984 B2 JP6609984 B2 JP 6609984B2
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insulation resistance
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JP2016211978A (en
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泰弘 高林
謙二 馬場
徹 引地
陽介 樋口
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Fuji Electric Co Ltd
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Description

この発明は、システムの運転状態、つまり活線状態で給電回路の絶縁抵抗を測定する方法および装置に関する。例えば、直流電源を用いた電気推進船舶などにおいては、運転中の安全確認の見地から、給電回路はいつでも活線状態で、しかも連続的に絶縁抵抗を監視できることが要求されるが、この発明はこのような用途に使用して好適なものである。   The present invention relates to a method and an apparatus for measuring an insulation resistance of a power feeding circuit in an operating state of a system, that is, in a live line state. For example, in an electric propulsion ship using a DC power source, from the viewpoint of safety confirmation during operation, the power supply circuit is required to be always in a live state and continuously monitor the insulation resistance. It is suitable for use in such applications.

非接地給電路の絶縁抵抗の測定装置として、特許文献1に示す装置が知られている。この従来の絶縁抵抗測定装置を図6に示す。   As an apparatus for measuring the insulation resistance of an ungrounded power supply path, an apparatus disclosed in Patent Document 1 is known. This conventional insulation resistance measuring apparatus is shown in FIG.

図6に示す従来の絶縁抵抗測定装置は、検出抵抗101〜105によってT型検出回路を構成し、抵抗102,104および105の各々から信号106(電圧V1),108(電圧V2)および107(電圧V3)をそれぞれ得る。これら信号106〜108は絶縁変換器109,110,111の一次側に入力され、それぞれ絶縁変換されて二次信号112〜114となる。   The conventional insulation resistance measuring apparatus shown in FIG. 6 constitutes a T-type detection circuit by the detection resistors 101 to 105, and signals 106 (voltage V1), 108 (voltage V2) and 107 ( Each voltage V3) is obtained. These signals 106 to 108 are input to the primary sides of the isolation converters 109, 110, and 111, respectively, and are converted to secondary signals 112 to 114, respectively.

二次信号112〜114は、ローパスフィルタ115、116、118により高調波成分が除去されて信号119〜121となり、そのうち信号119と120が正極側割算器125に、また信号120と121が負極側割算器126に入力され、割算が実行される。また、極性判別器122は信号120の極性を判別し、信号120が(+)方向のとき、すなわち電圧VR3が(+)方向のときは信号123をオンとする出力を発生し、(−)方向のときは信号124をオンとする出力を発生する。   Harmonic components are removed from the secondary signals 112 to 114 by the low-pass filters 115, 116, and 118 to become signals 119 to 121, of which the signals 119 and 120 are the positive divider 125, and the signals 120 and 121 are the negative electrodes. Input to the side divider 126 and division is performed. The polarity discriminator 122 discriminates the polarity of the signal 120 and generates an output that turns on the signal 123 when the signal 120 is in the (+) direction, that is, when the voltage VR3 is in the (+) direction. When the direction is the direction, an output that turns on the signal 124 is generated.

極性判別器122(PC)が(+)方向の信号123を出力したときは、正極側の演算器125,131や表示装置135,警報装置136を動作させ、負極側をロックする。同様に、極性判別器122が(−)方向の信号124を出力したときは、負極側の演算器126,132や表示装置135,警報装置136を動作させ、正極側をロックする。   When the polarity discriminator 122 (PC) outputs the signal 123 in the (+) direction, the positive side calculators 125 and 131, the display device 135, and the alarm device 136 are operated to lock the negative side. Similarly, when the polarity discriminator 122 outputs a signal 124 in the (−) direction, the negative side calculators 126 and 132, the display device 135, and the alarm device 136 are operated to lock the positive side.

以下、極性判別器122(PC)が(+)方向の信号123を出力し、正極電路の絶縁抵抗を測定する場合について説明する。 Hereinafter, the polarity discriminator 122 (PC) is (+) outputs a direction signal 123, it will be described for measuring the insulation resistance of the positive electrode sheet path.

図7の絶縁抵抗の測定動作説明図を参照して正極電路の絶縁抵抗を測定する場合について説明する。 Referring to measure operation explanatory diagram of the insulation resistance of FIG. 7 will be described for measuring the insulation resistance of the positive electrode sheet path.

ここで、正極側の抵抗101の抵抗値R11対抵抗102の抵抗値R12、または、負極側の抵抗103の抵抗値R21対抵抗104の抵抗値R22の抵抗値の比をそれぞれ1:1/100〜1:1/25程度とするが、これは測定しようとする回路の電圧値、または測定しようとする絶縁抵抗値の範囲などによって最適な値を選定する。   Here, the ratio of the resistance value R11 of the positive-side resistor 101 to the resistance value R12 of the resistor 102 or the resistance value R21 of the negative-side resistor 103 to the resistance value R22 of the resistor 104 is 1: 1/100, respectively. Although it is about ˜1: 1/25, an optimum value is selected depending on the voltage value of the circuit to be measured or the range of the insulation resistance value to be measured.

例えば、直流電圧500V回路の絶縁抵抗を測定する場合、検出抵抗101、103の抵抗値R11、R21を1MΩ、検出抵抗102、104の抵抗値R12,R22を10KΩに選定したとき、絶縁抵抗が無限大の場合にはRPx=∞であるとすると、図7に示す絶縁抵抗RPxに流れる電流IPXは流れない。その結果、検出抵抗102,104の両端電圧V1,V2はV1=V2で、検出抵抗101、102,103,104に流れる電流ISは、
IS≒V÷(R11+R12+R21+R22)
であり、M電位はVP=VN=250Vで、抵抗101と102の抵抗比は1:1/100であるから、抵抗102,104には、250V/100≒2.5Vの電圧が発生することになる。
For example, when measuring the insulation resistance of a DC voltage 500V circuit, when the resistance values R11 and R21 of the detection resistors 101 and 103 are set to 1 MΩ and the resistance values R12 and R22 of the detection resistors 102 and 104 are set to 10 KΩ, the insulation resistance is infinite. If RPx = ∞ in the large case, the current IPX flowing through the insulation resistance RPx shown in FIG. 7 does not flow. As a result, the voltages V1, V2 across the detection resistors 102, 104 are V1 = V2, and the current IS flowing through the detection resistors 101, 102, 103, 104 is
IS≈V / (R11 + R12 + R21 + R22)
Since the M potential is VP = VN = 250V and the resistance ratio of the resistors 101 and 102 is 1: 1/100, a voltage of 250V / 100≈2.5V is generated in the resistors 102 and 104. become.

いま、給電回路の正極電路Pの絶縁抵抗RPxが低下したとすると、接地回路には接地電流IPX=V÷(RPx+R3+R21+R22)が流れ、検出抵抗105の両端には
V3=IPX×R3
の電圧が発生する。このとき、検出抵抗102の両端電圧V1は電流ISで決定され、検出抵抗105の両端電圧V3は電流IPXで決定される。すなわち、抵抗101,絶縁抵抗RPxの抵抗値がそれぞれ抵抗102,105の抵抗値よりも充分に大きい場合、R12=R3とすれば、V1とV3の電圧値の割合は検出抵抗101の抵抗値R11と絶縁抵抗のRPxの抵抗値RPxの割合の逆数と考えられるから、V1とV3の電圧比n(=V1/V3)を求め、この比nに検出抵抗101の抵抗値R11を乗じると、すなわちn×R11=RPxから絶縁抵抗値RPxを求めることができる。
Now, the insulation resistance RPx of positive feed path P of the feed circuit and decreases, ground current IPX = V ÷ (RPx + R3 + R21 + R22) flows in the grounding circuit, at both ends of the detection resistor 105 V3 = IPX × R3
Is generated. At this time, the voltage V1 across the detection resistor 102 is determined by the current IS, and the voltage V3 across the detection resistor 105 is determined by the current IPX. That is, when the resistance values of the resistor 101 and the insulation resistor RPx are sufficiently larger than the resistance values of the resistors 102 and 105, respectively, if R12 = R3, the ratio of the voltage values of V1 and V3 is the resistance value R11 of the detection resistor 101. Therefore, the voltage ratio n (= V1 / V3) of V1 and V3 is obtained, and the ratio n is multiplied by the resistance value R11 of the detection resistor 101, that is, The insulation resistance value RPx can be obtained from n × R11 = RPx.

以上のことは、図6の回路では、以下のように実行される。   The above is performed as follows in the circuit of FIG.

すなわち、検出抵抗102の両端電圧V1の信号106が、絶縁変換器109→信号112→ローパスフィルタ115を介して信号119となり、割算器125の一方に入力される。また、電流IPXによって発生する検出抵抗105の両端電圧V3の信号107が絶縁変換器110→信号113→ローパスフィルタ116を介して信号120となり、割算器25の他方に入力されるとともに、極性判別器122へ入力される。   That is, the signal 106 of the voltage V1 across the detection resistor 102 becomes the signal 119 via the insulation converter 109 → the signal 112 → the low pass filter 115 and is input to one of the dividers 125. Further, the signal 107 of the voltage V3 across the detection resistor 105 generated by the current IPX becomes the signal 120 through the isolation converter 110 → the signal 113 → the low pass filter 116, and is input to the other of the divider 25, and the polarity is discriminated. Input to the instrument 122.

このときは、信号120が正(+)方向であるから、極性判別器122が(+)方向を判別してオンとなる信号123を出力し、割算器125および掛算器131を演算状態とし、表示装置135および警報装置136を正極側に切替える。また、オフとなる信号124により、割算器126および掛算器132を非演算状態とし、負極側の表示装置135および警報装置136の動作をロックする。   At this time, since the signal 120 is in the positive (+) direction, the polarity discriminator 122 discriminates the (+) direction and outputs a signal 123 that is turned on, and the divider 125 and the multiplier 131 are set in the calculation state. The display device 135 and the alarm device 136 are switched to the positive electrode side. Further, the signal 124 that is turned off causes the divider 126 and the multiplier 132 to be in a non-computation state, and locks the operations of the display device 135 and the alarm device 136 on the negative electrode side.

上記切替えによって、割算器125では信号119と信号120との比nであるV1/V3を示す信号127を出力し、掛算器131の一方に入力する。定数設定器129は、設定値Kを検出抵抗R11およびR21と同値とする信号130を出力し、掛算器131の他方に入力する。従って、掛算器131は割算器125からの出力信号127と、定数設定器129からの定数Kを示す信号130とを掛け合わせ、信号133を出力する。   By the above switching, the divider 125 outputs a signal 127 indicating V1 / V3, which is the ratio n of the signal 119 and the signal 120, and inputs the signal 127 to one of the multipliers 131. The constant setter 129 outputs a signal 130 for setting the set value K to the same value as the detection resistors R11 and R21, and inputs the signal 130 to the other of the multiplier 131. Therefore, the multiplier 131 multiplies the output signal 127 from the divider 125 and the signal 130 indicating the constant K from the constant setter 129 and outputs a signal 133.

信号133は、
RPx=n×K=(V1/V3)×R11 (1)
で求められ、求めるべき絶縁抵抗値RPxを示す。
Signal 133 is
RPx = n × K = (V1 / V3) × R11 (1)
And the insulation resistance value RPx to be obtained.

この式で、nはV1/V3、Kは抵抗101の抵抗値と等しい値の定数である。   In this equation, n is V1 / V3, and K is a constant having a value equal to the resistance value of the resistor 101.

これは表示装置135に与えられて表示される一方、警報装置136では予め設定した絶縁抵抗値よりも低下したら警報を発するとともに、出力信号137を時系列に記録することにより絶縁抵抗値の時系列の変化を記録するなど、安全管理のための処理をする。なお、図6のように、測定用電源138および電源スイッチ139を設けておき、これらを使用することで無通電状態、つまり活線状態でない状態での給電電路,機器または装置の絶縁抵抗の測定が可能となる。   While this is given and displayed on the display device 135, the alarm device 136 issues an alarm when the insulation resistance value falls below a preset insulation resistance value, and records the output signal 137 in time series to time-series the insulation resistance value. Process changes for safety management, such as recording changes. As shown in FIG. 6, a measurement power source 138 and a power switch 139 are provided, and by using these, measurement of the insulation resistance of a power supply circuit, device, or apparatus in a non-energized state, that is, in a state not in a live line state. Is possible.

次に、負極電路の絶縁抵抗を測定する場合について説明する。 Next, the case where the insulation resistance is measured of the negative electrode sheet path.

この場合、測定しようとする絶縁抵抗はRNxであり、これに電流INXが流れることにより、抵抗102を抵抗104に置き換えることで上記と同様の関係から、求めるべき絶縁抵抗値RNxは、
RNx=n×K=(V2/V3)×R21 (2)
として求めることができる。この式において、nはV2/V3であり、Kは抵抗103の抵抗値R21と等しい値の定数である。
In this case, the insulation resistance to be measured is RNx, and when the current INX flows therethrough, the insulation resistance value RNx to be obtained from the relationship similar to the above by replacing the resistor 102 with the resistor 104 is
RNx = n × K = (V2 / V3) × R21 (2)
Can be obtained as In this equation, n is V2 / V3, and K is a constant having a value equal to the resistance value R21 of the resistor 103.

図6の回路における、信号106,112,119,127および133を信号108,114,121,128および134に、演算回路125,131を演算回路126,132に、また信号123をOFF,信号124をONにそれぞれ置き換えることにより、正極電路の絶縁抵抗RPxを測定する場合と全く同様にして負極電路の絶縁抵抗RNxを測定することができる。 In the circuit of FIG. 6, the signals 106, 112, 119, 127, and 133 are converted to the signals 108, 114, 121, 128, and 134, the arithmetic circuits 125 and 131 are switched to the arithmetic circuits 126 and 132, the signal 123 is turned OFF, and the signal 124 is switched off. the by replacing each to oN, it is possible to measure the insulation resistance RNx of the negative electrode sheet path in the same manner as the case of measuring the insulation resistance RPx of the positive electrode sheet path.

絶縁抵抗の抵抗値RPx=1MΩであるとし、R11=RPx=1MΩ、R12=R3=10KΩとすると、図7からV1=V3は、およそ1.65Vとなり、両電圧の比nは、V1/V3=1.65/1.65=1となるので、正極電路の絶縁抵抗RPxとして、前記(1)式から、1MΩを求めることができる。 Assuming that the resistance value RPx = 1 MΩ of the insulation resistance, R11 = RPx = 1 MΩ, and R12 = R3 = 10 KΩ, from FIG. 7, V1 = V3 is approximately 1.65 V, and the ratio n between the two voltages is V1 / V3. since = the 1.65 / 1.65 = 1, as the insulation resistance RPx of the positive electrode sheet path, from the equation (1), can be obtained 1 M.OMEGA.

同様に、電圧比n=V1/V3=10では、絶縁抵抗RPxとして、(1)式からRPx=(K=1MΩ)×(n=10)=10MΩが求まる。同様に、電圧比n=V1/V3=100では、RPx=(K=1MΩ)×(n=100)=100MΩ、電圧比n=0.1では、RPx=(K=1MΩ)×(n=0.1)=0.1MΩを求めることができる。   Similarly, at the voltage ratio n = V1 / V3 = 10, RPx = (K = 1 MΩ) × (n = 10) = 10 MΩ is obtained from the equation (1) as the insulation resistance RPx. Similarly, when the voltage ratio n = V1 / V3 = 100, RPx = (K = 1 MΩ) × (n = 100) = 100 MΩ, and when the voltage ratio n = 0.1, RPx = (K = 1 MΩ) × (n = 0.1) = 0.1 MΩ can be obtained.

なお、給電回路の電源100の電圧が変動した場合、これに比例して電流IS,IPXおよびINXが変動してV1,V2およびV3も変動するが、電圧比n=V1/V3およびn=V2/V3は変わらない。従って、この従来装置によれば、測定しようとする給電回路の電圧が変動しても測定値はその影響を受けないで、安定して絶縁抵抗の測定ができる利点が得られる。   When the voltage of the power supply 100 of the power feeding circuit varies, the currents IS, IPX and INX vary in proportion to this, and V1, V2 and V3 also vary, but the voltage ratios n = V1 / V3 and n = V2 / V3 does not change. Therefore, according to this conventional apparatus, even if the voltage of the power supply circuit to be measured fluctuates, the measurement value is not affected by this, and the advantage that the insulation resistance can be measured stably is obtained.

特開2007−198330号公報JP 2007-198330 A

しかしながら、上記特許文献1に記載の従来装置には、正極電路と負極電路の絶縁抵抗の差が大きいときは、測定誤差は小さいが、両極の絶縁抵抗の差が小さい場合は、測定誤差が大きくなり、また、両極電路の絶縁抵抗が同じ値になれば測定不能となる問題がある。 However, the conventional apparatus described in Patent Document 1, when the time difference between the insulation resistance of the positive electrode sheet path and the negative supply path is large, the measurement error is small, the difference between the insulation resistance of the poles is small, the measurement error becomes large, there is a problem that the insulation resistance of the bipolar supply path becomes unmeasurable if the same value.

図8に従来装置における両極電路の絶縁抵抗の抵抗比の変化による検出特性を示す。 Shows the detection characteristics due to a change in the insulation resistance of the resistance ratio of the bipolar supply path in the conventional apparatus in FIG.

この図8の検出特性図の横軸は、P極電路の絶縁抵抗RPxとN極電路の絶縁抵抗RNxの比RNx/RPxまたはRPx/RNxを示し、縦軸は、T型検出回路による絶縁抵抗測定値と実絶縁抵抗値の比(RPxの測定抵抗値/RPxの実抵抗値)、(RNxの測定抵抗値/RNxの実抵抗値)を示す。 The horizontal axis of the detection characteristic diagram of FIG. 8 shows the ratio RNx / RPx or RPx / RNx insulation resistance RNx insulation resistance RPx and N-pole feeding path of the P-pole feed path and the vertical axis, due to T-type detecting circuit The ratio between the measured insulation resistance value and the actual insulation resistance value (measured resistance value of RPx / actual resistance value of RPx) and (measured resistance value of RNx / actual resistance value of RNx) are shown.

正極側絶縁抵抗RPx=1で、負極側絶縁抵抗RNx=1で両極絶縁抵抗が同値であると、接地電流IPXとINXが等しくなるから、検出抵抗R3を流れる接地電流IPXとINXが互いに打ち消し合って、検出電圧V3は0となり、これによって求まる絶縁抵抗値が無限大となって、絶縁抵抗RPxおよびRNxの測定が不能となる。   If the positive-side insulation resistance RPx = 1, the negative-side insulation resistance RNx = 1, and the bipolar insulation resistances have the same value, the ground currents IPX and INX are equal, so the ground currents IPX and INX flowing through the detection resistor R3 cancel each other. Thus, the detection voltage V3 becomes 0, and the insulation resistance value obtained thereby becomes infinite, and the insulation resistances RPx and RNx cannot be measured.

また、図8から、明らかなように、絶縁抵抗RPxとRNxの比が2であれば、測定抵抗値と実抵抗値の比は2となり、測定誤差は2倍と大きくなる。しかし、絶縁抵抗RPxとRNxの比が20と大きくなると、測定抵抗値と実抵抗値の比は1.05となり、測定誤差は、1.05倍と小さくなる。   As is clear from FIG. 8, if the ratio between the insulation resistances RPx and RNx is 2, the ratio between the measured resistance value and the actual resistance value is 2, and the measurement error is doubled. However, when the ratio of the insulation resistances RPx and RNx is increased to 20, the ratio of the measured resistance value to the actual resistance value is 1.05, and the measurement error is reduced to 1.05 times.

したがって、この発明の課題は、前記のような従来装置における問題点を解決するため、絶縁抵抗を煩雑な測定操作をすることなく連続的に、しかも電源電圧の変動の影響を受けずに、絶縁抵抗を安定して測定でき、かつ、両極の絶縁抵抗の差が小さくても、高精度の測定ができる絶縁抵抗の測定方法および測定装置を提供することにある。   Therefore, an object of the present invention is to solve the problems in the conventional apparatus as described above, and to insulate the insulation resistance continuously without complicated measurement operation and without being affected by fluctuations in the power supply voltage. An object of the present invention is to provide an insulation resistance measurement method and measurement apparatus that can measure resistance stably and can perform high-accuracy measurement even when the difference in insulation resistance between both electrodes is small.

このような課題を解決するため、請求項1の発明は、非接地の直流給電回路の正極給電路負極給電路との間に、等しい値の高抵抗の第1抵抗器および第2抵抗器と、低抵抗の第3抵抗器とを直列接続して構成した2組の抵抗回路を直列接続し、これら2組の抵抗回路が互いに接続された中性点を低抵抗の第4抵抗器を介して接地してなるT型検出回路を備え、このT型検出回路の各組の抵抗回路に前記第1抵抗器および第2抵抗器の抵抗値分を加減する抵抗可変手段をそれぞれ設け、これらの抵抗可変手段により前記各組の抵抗回路の抵抗値を加減しながら、前記2組の抵抗回路の第3抵抗器の両端に発生する各電圧と、前記第4抵抗器の両端に発生する電圧を検出し、一方の組の抵抗回路の第3抵抗器の電圧と第4抵抗器との電圧比、または、他方の組の抵抗回路の第3抵抗器の電圧と第4抵抗器との電圧比を演算し、これらの電圧比のいずれかに前記第1抵抗器または第2抵抗器と同じ値の定数K値を乗算して前記両極の絶縁抵抗値を得ることを特徴とする。 In order to solve such a problem, the invention according to claim 1 is the first resistor and the second resistor having the same high resistance between the positive electrode feeding path and the negative electrode feeding path of the ungrounded DC feeding circuit. Are connected in series to a low resistance third resistor, and a neutral point where these two resistance circuits are connected to each other is connected to a low resistance fourth resistor. T-type detection circuits that are grounded through each of them, and variable resistance means for adjusting the resistance values of the first resistor and the second resistor are provided in each pair of resistance circuits of the T-type detection circuit, respectively. The voltage generated at both ends of the third resistor of the two sets of resistor circuits and the voltage generated at both ends of the fourth resistor while adjusting the resistance value of each set of resistor circuits by the variable resistance means And the voltage ratio between the third resistor and the fourth resistor of one of the resistor circuits, Calculates the voltage ratio between the third resistor and the fourth resistor of the other set of resistor circuits, and either of these voltage ratios has the same value as the first resistor or the second resistor. A constant K value is multiplied to obtain the insulation resistance value of the two electrodes.

この請求項1の発明おいては、前記抵抗可変手段より前記各組の抵抗回路の抵抗値の一方を増大するときは、他方の組の抵抗回路の抵抗値が低減されるように相補的に交互に調整して両極の絶縁抵抗を測定するのがよい(請求項2の発明)。   In the first aspect of the invention, when one of the resistance values of each of the resistance circuits is increased by the resistance variable means, the resistance values of the other resistance circuit are complementarily complemented. It is preferable to measure the insulation resistance of both poles by alternately adjusting (invention of claim 2).

請求項3の発明は、非接地の直流給電回路の正極給電路負極給電路との間に、等しい値の高抵抗の第1抵抗器および第2抵抗器と、低抵抗の第3抵抗器とを直列接続して構成した2組の抵抗回路を直列接続し、これら2組の抵抗回路が互いに接続された中性点を低い抵抗の第4抵抗器を介して接地したT型検出回路と、
このT型検出回路の各組の抵抗回路の前記第1抵抗器と第2抵抗器の抵抗値分をそれぞれ加減する抵抗可変手段と、
前記各抵抗可変手段を選択的に動作指令を与えて測定位置を選択する手段と、
前記各組の抵抗回路の第3抵抗器の各両端と前記第4抵抗器の両端に発生する電圧をそれぞれ検出する電圧検出手段と、
正極給電路側の抵抗回路の第3抵抗器の電圧と前記第4抵抗器との電圧比を演算する第1演算手段と、負極給電路側の抵抗回路の第3抵抗器の電圧と前記第4抵抗器の電圧比を演算する第2演算手段と、
前記第1演算手段からの電圧比に前記正極電路側の抵抗回路の第1抵抗器または第2抵抗器の抵抗値と同じ値の定数K値を乗算する第3演算手段と、前記第2演算手段からの電圧比に前記負極給電路の抵抗回路の第1抵抗器または第2抵抗器の抵抗値と同じ値の定数K値を乗算する第4演算手段と、
前記第3または第4演算手段のそれぞれの出力を絶縁抵抗値として表示する表示手段とを有することを特徴とする。
According to a third aspect of the present invention, a high-resistance first resistor and a second resistor having an equal value and a low-resistance third resistor are provided between a positive electrode feeding path and a negative electrode feeding path of a non-grounded DC feeding circuit. A T-type detection circuit in which two resistance circuits configured in series are connected in series, and a neutral point where the two resistance circuits are connected to each other is grounded via a fourth resistor having a low resistance; ,
Variable resistance means for adjusting the resistance value of the first resistor and the second resistor of each pair of resistance circuits of the T-type detection circuit;
Means for selectively giving each of the resistance variable means an operation command and selecting a measurement position;
Voltage detection means for detecting voltages generated at both ends of each of the third resistors and at both ends of the fourth resistor of each set of resistor circuits;
Wherein the first calculating means for calculating a voltage ratio of the voltage of the third resistor of the resistor of the positive feed line side and the fourth resistor, and the voltage of the third resistor of the resistor of the negative electrode feed line side first Second computing means for computing the voltage ratio of the four resistors;
A third arithmetic means for multiplying the first resistor or a constant K value equal to the resistance of the second resistor of the positive supply path side of the resistor circuit to a voltage ratio from the first calculating means, the second a fourth computing means for multiplying the first resistor or a constant K value equal to the resistance of the second resistor of the resistor of the negative electrode feed line side voltage ratio from the calculating means,
And display means for displaying each output of the third or fourth arithmetic means as an insulation resistance value.

請求項3の発明においては、前記各組の抵抗回路の可変手段より一方の組の抵抗回路の抵抗値を増大するときは他方の組の抵抗回路の抵抗値が低減されるように相補的に交互に調整する機能を備えるようにするのがよい(請求項4の発明)。   According to a third aspect of the present invention, when the resistance value of one set of resistance circuits is increased by the variable means of each set of resistance circuits, the resistance value of the other set of resistance circuits is complementarily reduced. It is preferable to provide a function of adjusting alternately (invention of claim 4).

前記第4抵抗器に発生する電圧の極性を判別する極性判別手段を設け、正極性のときは正極側の演算および表示を可能として負極側の演算および表示をロックし、負極性のときは負極側の演算および表示を可能として正極側の演算および表示をロックすることができる(請求項5の発明)。   Polarity discrimination means for discriminating the polarity of the voltage generated in the fourth resistor is provided. When the polarity is positive, the calculation and display on the positive side can be performed and the calculation and display on the negative side are locked. When the polarity is negative, the polarity is negative. The calculation and display on the positive side can be performed and the calculation and display on the positive electrode side can be locked (invention of claim 5).

さらに、前記絶縁抵抗値が予め設定された設定値より低下したことを判別して警報を発する警報手段を設けるようにしてもよい(請求項6の発明)。   Further, an alarm means for issuing an alarm upon determining that the insulation resistance value has fallen below a preset value may be provided (invention of claim 6).

この発明によれば、絶縁抵抗を測定するためのT型検出回路の2組の抵抗回路に設けた抵抗可変手段により、各組の抵抗回路の抵抗値を一方は増大し、他方は減少するように相補的に調整することにより、両極電路の絶縁抵抗の抵抗値に見かけ上大きな差をつけて測定することが可能となるので、測定誤差が小さくなり、測定精度を高めることができる。 According to the present invention, by the resistance variable means provided in the two resistance circuits of the T-type detection circuit for measuring the insulation resistance, one of the resistance values of each resistance circuit is increased and the other is decreased. a by adjusting complementary, since it is possible to measure with a great difference apparent to the resistance value of the insulation resistance of the bipolar supply path, the measurement error is reduced, it is possible to improve the measurement accuracy.

この発明の実施例を示す回路構成図。The circuit block diagram which shows the Example of this invention. この発明における絶縁抵抗の測定動作の説明図。Explanatory drawing of the measurement operation | movement of the insulation resistance in this invention. この発明における測定位置選択スイッチの選択位置と抵抗短絡用スイッチの開閉状態の関係を示す図。The figure which shows the relationship between the selection position of the measurement position selection switch in this invention, and the open / close state of the switch for resistance short circuits. この発明による正極電路の絶縁抵抗の測定動作の説明図。Illustration of measurement operation of the insulation resistance of the positive electrode sheet path according to the present invention. この発明による負極電路の絶縁抵抗の測定動作の説明図。Illustration of measurement operation of the insulation resistance of the negative electrode sheet path according to the present invention. 従来の絶縁抵抗測定装置を示す回路構成図。The circuit block diagram which shows the conventional insulation resistance measuring apparatus. 従来の絶縁抵抗測定装置の測定動作の説明図。Explanatory drawing of the measurement operation | movement of the conventional insulation resistance measuring apparatus. 従来の絶縁抵抗測定装置の測定特性を示す図。The figure which shows the measurement characteristic of the conventional insulation resistance measuring apparatus.

この発明の実施の形態を図に示す実施例について説明する。   Embodiments of the present invention will be described with reference to the embodiments shown in the drawings.

図1はこの発明の実施例を示す構成図である。   FIG. 1 is a block diagram showing an embodiment of the present invention.

図1において、1は直流電源であり、Pは直流電源1の正極から引き出された正極給電路、Nは、負極給電路、RPは検出抵抗3(R1A)〜5(R1C)を直列接続した第1抵抗回路(正極抵抗回路と呼ぶこともある)、RNは検出抵抗7(R2A)〜9(R2C)を直列接続した第2抵抗回路(負極抵抗回路と呼ぶこともある)である。この2組の抵抗回路RP,RNは、抵抗5と9が向き合うように対称的に配列して、直流電源1に接続された正極給電路Pと負極給電路Nとの間に直列に接続される。さらに2組の抵抗回路RP,RNが互いに接続された中性点Mに検出抵抗11(R3)の一端を接続し、その他端を接地することによりT型検出回路が構成される。   In FIG. 1, 1 is a DC power source, P is a positive electrode feeding path drawn from the positive electrode of the DC power source 1, N is a negative electrode feeding path, and RP is a series connection of detection resistors 3 (R1A) to 5 (R1C). A first resistance circuit (sometimes referred to as a positive resistance circuit) and RN are a second resistance circuit (also referred to as a negative resistance circuit) in which detection resistors 7 (R2A) to 9 (R2C) are connected in series. The two sets of resistance circuits RP and RN are arranged symmetrically so that the resistors 5 and 9 face each other, and are connected in series between the positive electrode feeding path P and the negative electrode feeding path N connected to the DC power source 1. The Furthermore, a T-type detection circuit is configured by connecting one end of the detection resistor 11 (R3) to a neutral point M where two sets of resistance circuits RP and RN are connected to each other and grounding the other end.

抵抗回路RP,RNには、それぞれ直列接続された2個の抵抗を短絡する第1スイッチPS1およびNS1と1個の抵抗を短絡する第2スイッチPS2およびNS2が並列に設けられている。第1スイッチPS1およびNS1が、それぞれ各抵抗回路の抵抗3、4および7、8に並列に接続され、第2スイッチPS2およびNS2がそれぞれ抵抗4および8に並列に接続される。このような第1スイッチPS1,NS1および第2スイッチPS2,NS2は開閉によって抵抗回路RPおよびRNの抵抗値を加減する抵抗可変手段となる
測定位置選択スイッチ (ただ単に選択スイッチと呼ぶこともある)2は、回転操作によって絶縁抵抗測定する電路の選択を行うもので、その選択位置によって第1スイッチPS1およびNS1と第2スイッチPS2およびNS2の開閉を制御する。
The resistance circuits RP and RN are provided in parallel with first switches PS1 and NS1 that short-circuit two resistors connected in series and second switches PS2 and NS2 that short-circuit one resistor, respectively. First switches PS1 and NS1 are connected in parallel to resistors 3, 4 and 7, 8 of each resistance circuit, respectively, and second switches PS2 and NS2 are connected in parallel to resistors 4 and 8, respectively. Such first switches PS1, NS1 and second switches PS2, NS2 serve as resistance variable means for adjusting the resistance values of the resistance circuits RP and RN by opening and closing .
A measurement position selection switch (sometimes simply referred to as a selection switch) 2 is used to select an electric circuit for measuring insulation resistance by rotating operation. Depending on the selection position, the first switch PS1 and NS1 and the second switch PS2 and NS2 are selected. Controls the opening and closing of.

正、負極両極の電路P、Nの絶縁抵抗を同時に測定する場合は、選択スイッチ2が「常」で示される通常測定位置に置かれる。正極電路Pの絶縁抵抗を測定する場合は、選択スイッチ2を「P」で示される正極測定位置に置き、そして負極電路Nの絶縁抵抗を測定する場合は、選択スイッチ2を「N」で示される負極測定位置に置く。 Positive feed path P of the negative electrode poles, when measuring the insulation resistance of the N at the same time, placed in the normal measuring position selection switch 2 is indicated by "normally". When measuring the insulation resistance of the positive electrode sheet path P is placed in the positive electrode measurement position shown select switch 2 in the "P", and when measuring the insulation resistance of the negative electrode sheet path N is a selection switch 2 "N" Is placed at the negative electrode measurement position indicated by.

選択スイッチ2の選択位置と、スイッチPS1、NS1、PS2、NS2の開閉状態の関係を図3に示す。この図3の横方向に選択位置「P」、「常」、「N」を採って、縦方向にスイッチPS1、PS2,NS1、NS2を示し、マトリックスの交点上の×印は、スイッチがオン(閉)していることを示し、無印は、スイッチがオフ(開)していることを示す。   FIG. 3 shows the relationship between the selection position of the selection switch 2 and the open / closed states of the switches PS1, NS1, PS2, and NS2. The selected positions “P”, “always”, and “N” in the horizontal direction in FIG. 3 indicate the switches PS1, PS2, NS1, and NS2 in the vertical direction. It indicates that it is (closed), and no mark indicates that the switch is off (open).

図3に示すように、選択スイッチ2で「常」で示される通常測定位置が選択されたときは、第2スイッチPS2とNS2がオンとなる。これにより両極抵抗回路RPおよびRNの抵抗4および8が短絡される。   As shown in FIG. 3, when the normal measurement position indicated by “always” is selected by the selection switch 2, the second switches PS2 and NS2 are turned on. As a result, the resistors 4 and 8 of the bipolar resistor circuits RP and RN are short-circuited.

選択スイッチ2で正極給電路Pの絶縁抵抗を測定する位置「P」が選択されときは、負極側抵抗回路RNの第1スイッチNS1がオン(閉)となり、負極側抵抗回路RNの2つの抵抗7、8が短絡される。そして、選択スイッチ2で負極給電路Nの絶縁抵抗を測定する位置「N」が選択されたときは、正極側抵抗回路RPの第1スイッチPS1がオン(閉)となり、正極側抵抗回路RPの2つの抵抗3,4が短絡される。   When the position “P” for measuring the insulation resistance of the positive electrode feeding path P is selected by the selection switch 2, the first switch NS1 of the negative resistance circuit RN is turned on (closed), and the two resistances of the negative resistance circuit RN are selected. 7 and 8 are short-circuited. When the position “N” for measuring the insulation resistance of the negative electrode feeding path N is selected by the selection switch 2, the first switch PS1 of the positive resistance circuit RP is turned on (closed), and the positive resistance circuit RP The two resistors 3 and 4 are short-circuited.

検出抵抗5(R1C),9(R2C)および11(R31)の各々の両端に絶縁型の電圧検出器6、10および12が接続され、それぞれ1次側とは絶縁された電圧検出信号V1、V2およびV3を得る。   Insulated voltage detectors 6, 10 and 12 are connected to both ends of each of the detection resistors 5 (R1C), 9 (R2C) and 11 (R31), and voltage detection signals V1, which are insulated from the primary side, respectively. V2 and V3 are obtained.

なお、検出抵抗11は、測定レンジ選択器13によって開閉される接点を介して3個の抵抗が並列接続され、検出抵抗11の抵抗値R3が変更可能に構成されているので、選択された測定レンジ1,2,3に応じてその端子電圧V3を変更することができる。 The detection resistor 11 is configured such that three resistors are connected in parallel via a contact that is opened and closed by the measurement range selector 13, and the resistance value R3 of the detection resistor 11 can be changed. The terminal voltage V3 can be changed according to the ranges 1, 2, and 3.

これらの電圧検出信号V1〜V3は、ローパスフィルタ14〜16により高調波成分が除去されて、そのうち信号V1とV3が正極側割算器17に、また信号V2とV3が負極側割算器18に入力され、割算が実行される。   These voltage detection signals V1 to V3 have their harmonic components removed by the low-pass filters 14 to 16, among which the signals V1 and V3 are supplied to the positive divider 17 and the signals V2 and V3 are supplied to the negative divider 18. And division is performed.

割算器17および18からそれぞれ出力される電圧比(n)V1/V3およびV2/V3を示す出力信号SP1およびSN1は、それぞれ掛算器19および20に加えられ、定数設定器21に設定された検出抵抗3または7の抵抗値R1AまたはR2Aに等しい抵抗値を示す定数SKと乗算される。掛算器19、20の出力信号SP2、SN2は、監視記録装置22で処理されて表示装置23および警報装置24に加わる。   Output signals SP1 and SN1 indicating the voltage ratios (n) V1 / V3 and V2 / V3 respectively output from the dividers 17 and 18 are applied to the multipliers 19 and 20, respectively, and set in the constant setter 21. It is multiplied by a constant SK indicating a resistance value equal to the resistance value R1A or R2A of the detection resistor 3 or 7. Output signals SP <b> 2 and SN <b> 2 of the multipliers 19 and 20 are processed by the monitoring recording device 22 and applied to the display device 23 and the alarm device 24.

また、極性判別器25は信号V3の極性を判別し、信号V3が(+)方向のときは信号VPをオンにする出力を発生し、(−)方向のときは信号VNをオンにする出力を発生する。   The polarity discriminator 25 discriminates the polarity of the signal V3 and generates an output that turns on the signal VP when the signal V3 is in the (+) direction, and an output that turns on the signal VN when the signal V3 is in the (−) direction. Is generated.

極性判別器25が(+)方向の信号VPを出力したときは、正極側の演算器17,19や表示装置23,警報装置24を動作させ、負極側をロックする。同様に、極性判別器25が(−)方向の信号VNを出力したときは、負極側の演算器18,20や表示装置23,警報装置24を動作させ、正極側をロックする。   When the polarity discriminator 25 outputs the signal VP in the (+) direction, the calculators 17 and 19 on the positive electrode side, the display device 23 and the alarm device 24 are operated to lock the negative electrode side. Similarly, when the polarity discriminator 25 outputs the signal VN in the (−) direction, the negative side calculators 18 and 20, the display device 23, and the alarm device 24 are operated to lock the positive side.

図2は絶縁抵抗を測定する場合の説明図である。この図を参照して、絶縁抵抗の測定方法を説明する。   FIG. 2 is an explanatory diagram for measuring the insulation resistance. With reference to this figure, the measuring method of insulation resistance is demonstrated.

ここで、正極側抵抗回路RPの抵抗3(R1A)、4(R1B)、と負極側抵抗回路RNの抵抗7(R2A),8(R2B)は等しい抵抗値に選ばれている。抵抗5(R1C)と9(R2C)も等しい抵抗値に選ばれている。そして、抵抗3,4,7,8の抵抗値は、低抵抗値を有する抵抗5、9に対して25〜100倍程度の高抵抗値とするが、これらの抵抗値は測定しようとする回路電圧値、または測定しようとする絶縁抵抗値の範囲などによって最適な値を選定する。   Here, the resistors 3 (R1A) and 4 (R1B) of the positive-side resistor circuit RP and the resistors 7 (R2A) and 8 (R2B) of the negative-side resistor circuit RN are selected to have the same resistance value. Resistors 5 (R1C) and 9 (R2C) are also selected to have the same resistance value. The resistance values of the resistors 3, 4, 7, and 8 are about 25 to 100 times as high as the resistors 5 and 9 having low resistance values. Select the optimum value according to the voltage value or the range of the insulation resistance value to be measured.

例えば、直流電圧500Vの給電回路の絶縁抵抗を測定する場合、抵抗3、4、7、8の抵抗値(R1A,R1B,R2A,R2B)を33kΩ、抵抗5、9の抵抗値(R1C,R2C)を330Ωに選定し、抵抗11は、測定レンジを変更するために1から10kΩの範囲で抵抗値を可変できる抵抗とする。   For example, when measuring the insulation resistance of a feeding circuit with a DC voltage of 500 V, the resistance values (R1A, R1B, R2A, R2B) of the resistors 3, 4, 7, 8 are 33 kΩ and the resistance values of the resistors 5, 9 (R1C, R2C). ) Is selected to be 330Ω, and the resistor 11 is a resistor whose resistance value can be varied in the range of 1 to 10 kΩ in order to change the measurement range.

選択スイッチ2を「常」で示される通常位置におき、正、負両極の電路P,Nの測定位置を選択したときは、各抵抗回路の第2スイッチPS2およびNS2がオンし、高抵抗値の抵抗4と8が短絡される。絶縁抵抗が無限大の場合にはRPx=RNx=∞であるから、図2に示す絶縁抵抗RPxおよびRNxを流れる電流IPXおよびINXは流れない。その結果、検出抵抗5、9の両端電圧V1,V2はV1=V2で、両抵抗回路RPおよびRNを通して流れる電流ISは、
IS=V÷(R1A+R1C+R2A+R2C)≒V÷(R1A+R2A)
となる。
Place the selection switch 2 to the normal position indicated by "normal", the positive feed path P of the negative polarities, when selecting the measurement position of N second switches PS2 and NS2 of each resistor circuit is turned on, the high-resistance Value resistors 4 and 8 are short-circuited. Since RPx = RNx = ∞ when the insulation resistance is infinite, the currents IPX and INX flowing through the insulation resistances RPx and RNx shown in FIG. 2 do not flow. As a result, the voltages V1, V2 across the detection resistors 5, 9 are V1 = V2, and the current IS flowing through both resistance circuits RP and RN is
IS = V ÷ (R1A + R1C + R2A + R2C) ≈V ÷ (R1A + R2A)
It becomes.

中性点Mの電位はVP=VN=250Vで、抵抗3、5(R1C)と抵抗3、9(R2C)の抵抗比は1:1/100であるから、抵抗5と抵抗9には、250V/100≒2.5Vの電圧が発生する。   The potential of the neutral point M is VP = VN = 250V, and the resistance ratio between the resistors 3, 5 (R1C) and the resistors 3, 9 (R2C) is 1: 1/100. A voltage of 250V / 100≈2.5V is generated.

いま、電源回路の正極電路P側の絶縁抵抗RPxが低下したとすると、接地回路には、
IPX=V÷(RPx+R31+R2A+R2C)
となる接地電流IPXが流れ、検出抵抗11の両端には、
V3=IPX×R31
の電圧が発生する。このとき、検出抵抗5の両端電圧V1は電流ISで決定され、検出抵抗11の両端電圧V3は接地電流IPXで決定される。すなわち、ここでは、抵抗3の抵抗値R1Aと接地抵抗の抵抗値RPxがそれぞれ抵抗5の抵抗値R1C,抵抗11の抵抗値R31よりも充分に大きいので、検出電圧V1とV3の比は抵抗3の抵抗値R1Aと接地抵抗の抵抗値RPxの比の逆数となるから、電圧V1とV3の電圧比nを求め、この比nに検出抵抗3の抵抗値R1Aを乗じることにより、すなわち
RPx=n×R1A=(V1/V3)×R1A
から絶縁抵抗値を求めることができる。
Now, the insulation resistance RPx of the positive electrode sheet path P of the power supply circuit is to have decreased, the ground circuit,
IPX = V ÷ (RPx + R31 + R2A + R2C)
A ground current IPX flows, and both ends of the detection resistor 11
V3 = IPX × R31
Is generated. At this time, the voltage V1 across the detection resistor 5 is determined by the current IS, and the voltage V3 across the detection resistor 11 is determined by the ground current IPX. That is, here, since the resistance value R1A of the resistor 3 and the resistance value RPx of the ground resistance are sufficiently larger than the resistance value R1C of the resistor 5 and the resistance value R31 of the resistor 11, respectively, the ratio of the detection voltages V1 and V3 is the resistance 3 Therefore, the voltage ratio n of the voltages V1 and V3 is obtained, and the ratio n is multiplied by the resistance value R1A of the detection resistor 3, that is, RPx = n * R1A = (V1 / V3) * R1A
From this, the insulation resistance value can be obtained.

以上のことは、図1の回路では、以下のように実行される。   The above is performed as follows in the circuit of FIG.

すなわち、検出抵抗5の両端電圧V1が、絶縁検出器6→ローパスフィルタ14を介して割算器17の一方に入力される。また、電流IPXによって発生する検出抵抗11の両端電圧V3が絶縁検出器12→ローパスフィルタ16を介して割算器17の他方に入力されるとともに、極性判別器25へ入力される。   That is, the voltage V1 across the detection resistor 5 is input to one of the dividers 17 via the insulation detector 6 → the low pass filter 14. Further, the voltage V3 across the detection resistor 11 generated by the current IPX is input to the other of the divider 17 via the insulation detector 12 → low pass filter 16 and to the polarity discriminator 25.

このとき、電圧V3が正極(+)方向であるから、極性判別器25が(+)方向を判別して信号VPをオンにして出力し、割算器17および掛算器19を演算状態とし、表示装置23および警報装置24を正極側に切替える。また、信号VNはオフとなることにより、割算器18および掛算器20が非演算状態とされ、表示装置23および警報装置24の負極側の動作がロックされる。   At this time, since the voltage V3 is in the positive (+) direction, the polarity discriminator 25 discriminates the (+) direction, turns on and outputs the signal VP, puts the divider 17 and the multiplier 19 in the calculation state, The display device 23 and the alarm device 24 are switched to the positive electrode side. Further, when the signal VN is turned off, the divider 18 and the multiplier 20 are put into a non-calculation state, and the operations on the negative side of the display device 23 and the alarm device 24 are locked.

上記切替えによって、割算器17では信号V1と信号V3との比nであるV1/V3を示す信号SP1を出力し、掛算器19の一方に入力する。定数設定器21は、設定値Kを検出抵抗3および7の抵抗値R1AおよびR2Aと同値とする信号SKを出力し、掛算器19の他方に入力する。従って、掛算器19は割算器17からの出力信号SP1と、定数設定器21からの定数Kを示す信号SKとを掛け合わせて、信号SP2を出力する。   By the switching, the divider 17 outputs a signal SP1 indicating V1 / V3, which is a ratio n between the signal V1 and the signal V3, and inputs the signal SP1 to one of the multipliers 19. The constant setter 21 outputs a signal SK that makes the set value K the same as the resistance values R1A and R2A of the detection resistors 3 and 7, and inputs the signal SK to the other side of the multiplier 19. Accordingly, the multiplier 19 multiplies the output signal SP1 from the divider 17 and the signal SK indicating the constant K from the constant setter 21 and outputs a signal SP2.

信号SP2は、求めるべき絶縁抵抗値RPx、すなわち、
RPx=n×K=(V1/V3)×R1A (3)
を示しており、これは、監視記録制御装置22を介して表示装置23に与えられて表示される一方、警報装置24では、この絶縁抵抗測定値が予め設定した絶縁抵抗値よりも低下したら警報を発するとともに、監視記録制御装置22は、出力信号SP2で時系列に変化する絶縁抵抗値を記録するなど、安全管理のための処理をする。
The signal SP2 is an insulation resistance value RPx to be obtained, that is,
RPx = n × K = (V1 / V3) × R1A (3)
This is given to and displayed on the display device 23 via the monitoring and recording control device 22, while the alarm device 24 warns when this measured insulation resistance value falls below a preset insulation resistance value. The monitoring and recording control device 22 performs a process for safety management such as recording an insulation resistance value that changes in time series with the output signal SP2.

なお、図1のように、測定用電源38および電源スイッチ39を設けておき、これらを使用することにより、給電回路の直流電源1を遮断した無通電状態、つまり活線状態でない状態での電路,機器または装置の絶縁抵抗の測定が可能となる。   As shown in FIG. 1, a power supply for measurement 38 and a power switch 39 are provided, and by using these, the electric circuit in a non-energized state in which the DC power source 1 of the power feeding circuit is cut off, that is, in a state where it is not in a live line state , It is possible to measure the insulation resistance of equipment or equipment.

負極側の絶縁抵抗RNxが低下した場合、負極側絶縁抵抗RNxを通して電流INXが流れることにより、抵抗3を抵抗7に置き換えることで上記と同様の関係から、求めるべき絶縁抵抗値RNxは、
RNx=n×K=(V2/V3)×R2A (4)
として求めることができる。
When the negative-side insulation resistance RNx decreases, the current INX flows through the negative-side insulation resistance RNx, so that the insulation resistance value RNx to be obtained from the relationship similar to the above by replacing the resistor 3 with the resistor 7 is
RNx = n × K = (V2 / V3) × R2A (4)
Can be obtained as

図1の回路も、信号V1、SP1、SP2を信号V2、SN1、SN2に、演算回路17、19を演算回路18,20に、また信号VPをオフ,信号VNをオンにそれぞれ置き換えることにより、正極側絶縁抵抗を測定する場合と全く同様にして負極側絶縁抵抗を測定することができる。   The circuit of FIG. 1 also replaces the signals V1, SP1, and SP2 with the signals V2, SN1, and SN2, the arithmetic circuits 17 and 19 with the arithmetic circuits 18 and 20, the signal VP off, and the signal VN on. The negative electrode side insulation resistance can be measured in exactly the same manner as when measuring the positive electrode side insulation resistance.

図2の回路では、電源回路の電圧が変動した場合、これに比例して電流IS,IPXが変動してV1,V3も変動するが、電圧比n=V1/V3は変わらない。従って、この発明によれば、測定しようとする給電回路の電圧が変動しても測定値はその影響を受けないので、安定した絶縁抵抗の測定が可能となる利点が得られる。   In the circuit of FIG. 2, when the voltage of the power supply circuit fluctuates, the currents IS and IPX fluctuate proportionally and V1 and V3 also fluctuate, but the voltage ratio n = V1 / V3 does not change. Therefore, according to the present invention, even if the voltage of the power supply circuit to be measured fluctuates, the measurement value is not affected by this, so that there is an advantage that stable insulation resistance can be measured.

次に、各抵抗3〜5および7〜9の抵抗値R1A〜R2Cの選定について説明する。   Next, selection of the resistance values R1A to R2C of the resistors 3 to 5 and 7 to 9 will be described.

以上では、電圧500Vの回路を抵抗3、4、7、8の抵抗値を33kΩ、抵抗5、9の抵抗値を330Ωとして測定する場合について説明した。このとき、絶縁抵抗RPx,RNxが無限大のときは、中性点Mの電位は250V、検出電圧V1=V2≒2.5Vである。   In the above description, a case where a circuit having a voltage of 500 V is measured by setting the resistance values of the resistors 3, 4, 7, and 8 to 33 kΩ and the resistance values of the resistors 5 and 9 to 330Ω. At this time, when the insulation resistances RPx and RNx are infinite, the potential of the neutral point M is 250V, and the detection voltage V1 = V2≈2.5V.

ここで、電圧500Vの電圧が600V(+20%)〜400V(−20%)の範囲で変動した場合、絶縁抵抗RPx,RNxが無限大では、検出電圧V1=V2≒3V〜2Vの範囲で変動する。しかし、検出電圧比nは変わらないので、測定値への影響はない。また、電圧1000Vの回路の絶縁抵抗を測定するときは、中性点Mの電位は500V、検出電圧VR12=VR22=500/100≒5Vとなるが、この場合も検出電圧比nは変わらないので、測定値への影響はない。   Here, when the voltage of 500V fluctuates in the range of 600V (+ 20%) to 400V (−20%), if the insulation resistances RPx and RNx are infinite, the detection voltage V1 = V2≈ fluctuates in the range of 3V to 2V. To do. However, since the detection voltage ratio n does not change, there is no influence on the measured value. When measuring the insulation resistance of a circuit with a voltage of 1000 V, the potential at the neutral point M is 500 V, and the detection voltage VR12 = VR22 = 500 / 100≈5 V. However, in this case as well, the detection voltage ratio n does not change. There is no effect on the measured value.

さらに、各抵抗値をR1A,R1B、R2A、R2Bを1MΩとし、抵抗R1C,R2Cを10KΩの抵抗比1:1/100を、抵抗比1:1/50、すなわち抵抗R1C,R2Cを20KΩにすれば、V1,V2は2.5Vから5V、また抵抗比を1:1/25、抵抗RC,R2C=40KΩにすれば、V1,V2は2.5Vから10Vのように検出電圧は変わるが、電圧比は不変なので、測定への影響はない。   Further, each resistance value is set to 1 MΩ for R1A, R1B, R2A, and R2B, the resistance ratio 1: 1/100 for the resistors R1C, R2C is set to 1: 1/100, that is, the resistance R1C, R2C is set to 20 KΩ. For example, if V1 and V2 are 2.5V to 5V, the resistance ratio is 1: 1/25, and the resistance RC and R2C = 40KΩ, the detection voltages of V1 and V2 are changed from 2.5V to 10V. Since the voltage ratio is unchanged, there is no effect on the measurement.

以上では、抵抗値R1A,R1B,R2A、R2Bを固定し、抵抗値R1C,R2Cを変更したが、抵抗値R1C,R2Cの抵抗値を固定し、抵抗値R1A,R1B、R2A、R2Bを変更しても良いのは言うまでもない。すなわち、抵抗3,4,7,8および抵抗5,9の抵抗値R1A,R1B、R2A、R2BおよびR1C,R2Cは、測定回路の電圧と最適な検出電圧を得るため最適値に選択することができる。   In the above, the resistance values R1A, R1B, R2A and R2B are fixed and the resistance values R1C and R2C are changed. However, the resistance values R1C and R2C are fixed, and the resistance values R1A, R1B, R2A and R2B are changed. It goes without saying. That is, the resistance values R1A, R1B, R2A, R2B and R1C, R2C of the resistors 3, 4, 7, 8 and 5 and 9 can be selected to be optimum values in order to obtain the voltage of the measurement circuit and the optimum detection voltage. it can.

なお、この発明は非接地回路を対象とするもので、一線接地回路では測定すべき絶縁抵抗が短絡されることから適用できず、また、測定位置選択スイッチ2を「常」の位置の通常測定位置における設定抵抗測定方法は、特許文献1に示された従来の測定方法と同じとなるので、正極側絶縁抵抗および負極側絶縁抵抗の両方が同程度に低下する場合は、接地回路(検出抵抗11)に電流が流れないことにより、測定できないものである。   Note that the present invention is intended for a non-grounded circuit, and cannot be applied to a one-wire grounded circuit because the insulation resistance to be measured is short-circuited, and the measurement position selection switch 2 is normally measured at the “normal” position. Since the set resistance measurement method at the position is the same as the conventional measurement method disclosed in Patent Document 1, if both the positive-side insulation resistance and the negative-side insulation resistance decrease to the same extent, a ground circuit (detection resistor) 11) It cannot be measured because no current flows.

この発明では、給電電路の正極側絶縁抵抗および負極側絶縁抵抗の両方が同程度に低下した場合でも絶縁抵抗を正確に測定するために、測定位置選択スイッチ2を「P」位置または「N」位置に切換えて測定を行うようする。   In the present invention, the measurement position selection switch 2 is set to the “P” position or “N” in order to accurately measure the insulation resistance even when both the positive side insulation resistance and the negative side insulation resistance of the power supply circuit are reduced to the same extent. Switch to position and perform measurement.

次にその方法について説明する。   Next, the method will be described.

正極電路P側の絶縁抵抗RPxを測定する場合は、測定位置選択スイッチ2を「P」位置に切換える。これにより、図3に示すように、負極側抵抗回路RNの第1スイッチNS1だけがオンし、その他のスイッチはオフとなる。これにより、負極側抵抗回路RNでは2つの高抵抗値を有する抵抗7,8が短絡され、低抵抗値を有する抵抗9だけが回路に残る。一方、正極側抵抗回路RPには、直列接続された3個の抵抗3〜5が残っている。 When measuring the insulation resistance RPx of the positive electrode sheet path P side switches the measurement position selection switch 2 to the "P" position. Thereby, as shown in FIG. 3, only the first switch NS1 of the negative-side resistor circuit RN is turned on, and the other switches are turned off. As a result, in the negative resistance circuit RN, the two resistors 7 and 8 having a high resistance value are short-circuited, and only the resistor 9 having a low resistance value remains in the circuit. On the other hand, three resistors 3 to 5 connected in series remain in the positive-side resistor circuit RP.

この状態の等価的な回路構成を図4に示す。   An equivalent circuit configuration in this state is shown in FIG.

このとき、電路P,N間に接続された抵抗回路の抵抗は、2個の高抵抗3、4と2個の低抵抗5、9となり、この抵抗回路に流れる電流ISは、前記した測定位置選択スイッチ2を「常」で示す通常測定位置に切換えた状態と同じになる。回路電圧、回路定数を前記と同じにすれば、検出抵抗5と9に発生する電圧V1,V2はおよそ2.5Vで、前記の場合と同じなる。 At this time, the sheet path P, the resistance of the connected resistor circuit between N, the two high-resistance 3,4 and two next lower resistance 5,9, current IS flowing through the resistor circuit, the measurement described above This is the same as when the position selection switch 2 is switched to the normal measurement position indicated by “normal”. If the circuit voltage and the circuit constant are the same as described above, the voltages V1 and V2 generated in the detection resistors 5 and 9 are approximately 2.5 V, which is the same as the above case.

しかし、正極側絶縁抵抗RPxに流れる接地電流IPXは、2個の低抵抗値の抵抗11、9を通して流れ、負極側絶縁抵抗RNxに流れる接地電流INXは2個の高抵抗値の抵抗3,4と2個の低抵抗値の抵抗5、11を通して流れるため、絶縁抵抗RPxとRNxが等しくても、接地電流はIPX>INXとなり、両電流の電流差にしたがって検出抵抗11に(+)方向の電圧V3が発生する。これによって、図1の極性判別器25が正出力VPをオンにする出力を発生する。   However, the ground current IPX flowing through the positive-side insulation resistance RPx flows through the two low-resistance resistors 11 and 9, and the ground current INX flowing through the negative-side insulation resistance RNx is the two high-resistance resistors 3 and 4. Since the current flows through the two low resistance resistors 5 and 11, even if the insulation resistances RPx and RNx are equal, the ground current becomes IPX> INX, and the detection resistor 11 in the (+) direction according to the current difference between the two currents. A voltage V3 is generated. As a result, the polarity discriminator 25 of FIG. 1 generates an output that turns on the positive output VP.

これにより、割算器17で、検出抵抗5の電圧V1と検出抵抗11の電圧V3の比nを求め、この比nに、定数設定器21に設定された抵抗3または4の抵抗値R1AまたはR1Bと等しい定数Kを乗算することにより、正極電路Pの絶縁抵抗RPxを求めることができる。 Thereby, the divider 17 obtains the ratio n between the voltage V1 of the detection resistor 5 and the voltage V3 of the detection resistor 11, and the resistance value R1A of the resistor 3 or 4 set in the constant setter 21 or by multiplying the R1B equal constant K, it is possible to determine the insulation resistance RPx of the positive electrode sheet path P.

図4の状態は、正負両極の絶縁抵抗RPxとRNxが等しくても、RNxには2個の高抵抗値の抵抗3、4の合計の抵抗値が加算され、RPxには1個の低抵抗値の抵抗9の抵抗値が加算されることとになる。このため、相対的に、絶縁抵抗RPxがRNxより高抵抗値の抵抗2個分の抵抗値だけ減少したのと同じになり、両絶縁抵抗の見かけ上の比RNx/RPxが大きくなる。   In the state of FIG. 4, even if the insulation resistances RPx and RNx of both positive and negative electrodes are equal, the total resistance value of the two high resistance resistors 3 and 4 is added to RNx, and one low resistance is added to RPx. The resistance value of the value resistor 9 is added. For this reason, it is the same as the insulation resistance RPx is reduced by the resistance value of two resistances higher than RNx, and the apparent ratio RNx / RPx of both insulation resistances is increased.

このように見かけ上、両絶縁抵抗に差が生じ、両者の比が大きくなると、図8に示す測定特性から理解できるように測定誤差が低下するので、絶縁抵抗の測定精度を高めることができる。   In this way, when there is a difference between the two insulation resistances and the ratio between the two increases, the measurement error decreases as can be understood from the measurement characteristics shown in FIG. 8, so that the measurement accuracy of the insulation resistance can be increased.

次に、測定位置選択スイッチ2を「N」位置に切換えることにより、負極電路Nの絶縁抵抗RNxを測定することができる。 Next, the measurement position selection switch 2 by switching to the "N" position, it is possible to measure the insulation resistance RNx the negative supply path N.

この場合は、測定位置選択スイッチ2が「N」位置に切換えられているので、図3に示すように、正極側抵抗回路RPの第1スイッチPS1だけがオンとなり、そのスイッチはオフとなる。   In this case, since the measurement position selection switch 2 is switched to the “N” position, only the first switch PS1 of the positive resistance circuit RP is turned on and the switch is turned off as shown in FIG.

この状態の等価的な回路構成を図5に示す。   An equivalent circuit configuration in this state is shown in FIG.

この図5から明らかなように、抵抗回路に流れる電流ISは、2個の低抵抗値の抵抗5、9および2個の高抵抗値の抵抗7、8を通して流れる。そして、負極側絶縁抵抗RNxに流れる電流INXは、2個の低抵抗値の抵抗11と5を通して流れるが、正極側絶縁抵抗RPxに流れる電流IPXは、2個の低抵抗値の抵抗11、9と2個の高抵抗値の抵抗8,7を通して流れる。   As is apparent from FIG. 5, the current IS flowing through the resistance circuit flows through the two low resistance resistors 5 and 9 and the two high resistance resistors 7 and 8. The current INX that flows through the negative-side insulation resistance RNx flows through the two low-resistance resistors 11 and 5, while the current IPX that flows through the positive-side insulation resistance RPx includes the two low-resistance resistors 11, 9 And two high resistance resistors 8 and 7.

したがって、相対的に絶縁抵抗RNxがRPxより抵抗値が小さくなり、接地電流はINX>IPXとなって検出抵抗11には(−)方向の電圧V3が発生する。これによって、図1の極性判別器25が負出力VNをオンとする出力を発生する。   Accordingly, the resistance value of the insulation resistance RNx is relatively smaller than that of RPx, the ground current is INX> IPX, and the voltage V3 in the (−) direction is generated in the detection resistor 11. As a result, the polarity discriminator 25 of FIG. 1 generates an output that turns on the negative output VN.

これにより、割算器18で、検出抵抗5の電圧V1と検出抵抗11の電圧V3の比nを求め、掛算器20で、この比nに、定数設定器21に設定された抵抗7または8の抵抗値R2AまたはR2Bと等しい定数Kを乗算することにより、負極電路Nの絶縁抵抗RNxを求めることができる。 Thereby, the divider 18 determines the ratio n of the voltage V1 of the detection resistor 5 and the voltage V3 of the detection resistor 11, and the multiplier 20 sets the ratio 7 to the resistance 7 or 8 set in the constant setting unit 21. by multiplying the resistance value R2A or R2B equal constant K, it is possible to determine the insulation resistance RNx the negative supply path N.

この場合も、正絶縁抵抗RPxと負絶縁抵抗RNxとの比RPx/RNxを見かけ上大きくすることができるので、絶縁抵抗を高精度で測定することができる。   Also in this case, since the ratio RPx / RNx of the positive insulation resistance RPx and the negative insulation resistance RNx can be apparently increased, the insulation resistance can be measured with high accuracy.

前記においては、測定位置選択スイッチ2を人手により切換えることを前提に説明したが、抵抗回路RPおよびRNの抵抗短絡用の第1スイッチPS1、NS1および第2スイッチPS2、NS2を自動で切換えるようにしてもよい。   In the above description, it is assumed that the measurement position selection switch 2 is manually switched. However, the first switches PS1 and NS1 and the second switches PS2 and NS2 for short-circuiting the resistance circuits RP and RN are automatically switched. May be.

この場合に、第1スイッチPS1とNS1を所定の時間間隔で周期的に交互に開閉を制御する手段を設けることにより、正および負極電路の絶縁抵抗RPxおよびRNxを交互に連続して高精度で測定することができ、常時監視することが可能となる。 In this case, by providing means for controlling the opening and closing of the first switch PS1 and NS1 regularly alternately at predetermined time intervals, accurate continuous positive and insulation resistance RPx and RNx the negative supply path alternately Can be measured and can be constantly monitored.

この発明においては、図1に示すように検出抵抗11に並列に切り替え可能に複数の抵抗R32,R33を接続して、検出抵抗11の抵抗値を可変できる構成とすることにより、測定倍率を調整することができる。   In the present invention, as shown in FIG. 1, a plurality of resistors R32 and R33 are connected to the detection resistor 11 so that they can be switched in parallel, and the resistance value of the detection resistor 11 can be varied to adjust the measurement magnification. can do.

1 直流電源
2 測定位置選択スイッチ
3、4、7、8 高抵抗値の検出抵抗
5、9,11 低抵抗値の検出抵抗
6,10、12 絶縁電圧検出器
13 測定レンジ選択器
14、15、16 フィルタ
17、18 割算器
19、20 掛算器
21 定数設定器
22 監視記録制御装置
23 表示装置
24 警報装置
25 極性判別器
38 測定用電源
39 電源スイッチ
PS1、NS1 抵抗短絡用第1スイッチ
PS2、NS2 抵抗短絡用第2スイッチ
DESCRIPTION OF SYMBOLS 1 DC power supply 2 Measurement position selection switch 3, 4, 7, 8 High resistance detection resistors 5, 9, 11 Low resistance detection resistors 6, 10, 12 Insulation voltage detector 13 Measurement range selectors 14, 15, 16 Filters 17 and 18 Dividers 19 and 20 Multiplier 21 Constant setter 22 Monitoring and recording control device 23 Display device 24 Alarm device 25 Polarity discriminator 38 Power supply for measurement 39 Power switch PS1, NS1 First switch PS2 for resistance short circuit, NS2 Second switch for resistance short circuit

Claims (6)

非接地の直流給電回路の正極給電路負極給電路との間に、等しい値の高抵抗の第1抵抗器および第2抵抗器と、低抵抗の第3抵抗器とを直列接続して構成した2組の抵抗回路を直列接続し、これら2組の抵抗回路が互いに接続された中性点を低抵抗の範囲で抵抗値を変更可能な第4抵抗器を介して接地してなるT型検出回路を備え、このT型検出回路の各組の抵抗回路に前記第1抵抗器および第2抵抗器の抵抗値分を加減する抵抗可変手段をそれぞれ設け、
これらの抵抗可変手段により、正極給電路および負極給電路の絶縁抵抗を同時に測定する場合は、前記2組の抵抗回路の第1抵抗器または第2抵抗器を短絡させ、正極給電路または負極給電路の絶縁抵抗を測定する場合は、いずれか一方の組の抵抗回路の第1抵抗器および第2抵抗器を短絡させながら、
前記2組の抵抗回路の第3抵抗器の両端に発生する各電圧と、前記第4抵抗器の両端に発生する電圧を検出し、
一方の組の抵抗回路の第3抵抗器の電圧と第4抵抗器との電圧比、または、他方の組の抵抗回路の第3抵抗器の電圧と第4抵抗器との電圧比を演算し、
これらの電圧比のいずれかに前記第1抵抗器または第2抵抗器と同じ値の定数K値を乗算して前記両極の絶縁抵抗値を得ることを特徴とする絶縁抵抗測定方法。
A structure in which a high-resistance first resistor and a second resistor having the same value and a low-resistance third resistor are connected in series between a positive electrode supply path and a negative electrode supply path of a non-grounded DC power supply circuit. T-type formed by connecting two resistance circuits in series and grounding a neutral point where these two resistance circuits are connected to each other via a fourth resistor whose resistance value can be changed within a low resistance range A detection circuit, and variable resistance means for adjusting the resistance value of the first resistor and the second resistor in each set of resistance circuits of the T-type detection circuit,
When simultaneously measuring the insulation resistance of the positive electrode feeding path and the negative electrode feeding path using these resistance variable means, the first resistor or the second resistor of the two sets of resistance circuits are short-circuited, and the positive electrode feeding path or the negative electrode feeding is performed. When measuring the insulation resistance of the road , while short-circuiting the first resistor and the second resistor of either one of the resistor circuits,
Detecting each voltage generated at both ends of the third resistor of the two sets of resistor circuits, and voltage generated at both ends of the fourth resistor;
The voltage ratio between the third resistor and the fourth resistor in one set of resistor circuits, or the voltage ratio between the third resistor and the fourth resistor in the other set of resistor circuits is calculated. ,
A method of measuring an insulation resistance, wherein one of these voltage ratios is multiplied by a constant K value having the same value as that of the first resistor or the second resistor to obtain an insulation resistance value of the two electrodes.
前記抵抗可変手段より前記各組の抵抗回路の一方の組の抵抗回路の抵抗値を増大するときは、他方の組の抵抗回路の抵抗値が低減されるように相補的に交互に調整して両極の絶縁抵抗を測定することを特徴とする請求項1記載の絶縁抵抗測定方法。   When the resistance value of one set of resistance circuits of each set of resistance circuits is increased by the variable resistance means, the resistance values of the other set of resistance circuits are adjusted alternately and complementarily so as to be reduced. 2. The insulation resistance measuring method according to claim 1, wherein the insulation resistance of both electrodes is measured. 非接地の直流給電回路の正極給電路負極給電路との間に、等しい値の高抵抗の第1抵抗器および第2抵抗器と、低抵抗の第3抵抗器とを直列接続して構成した2組の抵抗回路を直列接続し、これら2組の抵抗回路が互いに接続された中性点を低抵抗の範囲で抵抗値を変更可能な第4抵抗器を介して接地したT型検出回路と、
このT型検出回路の各組の抵抗回路の前記第1抵抗器と第2抵抗器の抵抗値分をそれぞれ加減する抵抗可変手段と、
正極給電路および負極給電路の絶縁抵抗を同時に測定する場合は、前記2組の抵抗回路の第1抵抗器または第2抵抗器が短絡され、正極給電路または負極給電路の絶縁抵抗を測定する場合は、いずれか一方の組の抵抗回路の第1抵抗器および第2抵抗器が短絡されるように、前記各抵抗可変手段に選択的に動作指令を与えて絶縁抵抗を測定する電路を選択する手段と、
前記各組の抵抗回路の第3抵抗器の各両端と前記第4抵抗器の両端に発生する電圧をそれぞれ検出する電圧検出手段と、
正極給電路側の抵抗回路の第3抵抗器の電圧と前記第4抵抗器との電圧比を演算する第1演算手段と、負極給電路側の抵抗回路の第3抵抗器の電圧と前記第4抵抗器の電圧比を演算する第2演算手段と、
前記第1演算手段からの電圧比に前記正極電路側の抵抗回路の第1抵抗器または第2抵抗器の抵抗値と同じ値の定数K値を乗算する第3演算手段と、前記第2演算手段からの電圧比に前記負極電路側の抵抗回路の第1抵抗器または第2抵抗器の抵抗値と同じ値の定数K値を乗算する第4演算手段と、
前記第3または第4演算手段のそれぞれの出力を絶縁抵抗値として表示する表示手段とを有することを特徴とする絶縁抵抗測定装置。
A structure in which a high-resistance first resistor and a second resistor having the same value and a low-resistance third resistor are connected in series between a positive electrode supply path and a negative electrode supply path of a non-grounded DC power supply circuit. T-type detection circuit in which two sets of resistance circuits are connected in series and a neutral point where these two sets of resistance circuits are connected to each other is grounded via a fourth resistor whose resistance value can be changed within a low resistance range When,
Variable resistance means for adjusting the resistance value of the first resistor and the second resistor of each pair of resistance circuits of the T-type detection circuit;
When simultaneously measuring the insulation resistance of the positive electrode feeding path and the negative electrode feeding path , the first resistor or the second resistor of the two sets of resistance circuits is short-circuited, and the insulation resistance of the positive electrode feeding path or the negative electrode feeding path is measured. In this case, an electric path for measuring the insulation resistance by selectively giving an operation command to each of the resistance variable means is selected so that the first resistor and the second resistor of any one of the resistor circuits are short-circuited. Means to
Voltage detection means for detecting voltages generated at both ends of each of the third resistors and at both ends of the fourth resistor of each set of resistor circuits;
Wherein the first calculating means for calculating a voltage ratio of the voltage of the third resistor of the resistor of the positive feed line side and the fourth resistor, and the voltage of the third resistor of the resistor of the negative electrode feed line side first Second computing means for computing the voltage ratio of the four resistors;
A third arithmetic means for multiplying the first resistor or a constant K value equal to the resistance of the second resistor of the positive supply path side of the resistor circuit to a voltage ratio from the first calculating means, the second a fourth computing means for multiplying the first resistor or a constant K value equal to the resistance of the second resistor of the resistor of the negative electrode sheet path side voltage ratio from the calculating means,
Insulation resistance measuring apparatus comprising display means for displaying respective outputs of the third or fourth arithmetic means as insulation resistance values.
前記各組の抵抗回路の抵抗可変手段が、前記各組の抵抗回路の抵抗値を前記抵抗可変手段より一方の組の抵抗回路の抵抗値を増大するときは他方の組の抵抗回路の抵抗値が低減されるように相補的にて交互に調整する機能を備えることを特徴とする請求項3に記載の絶縁抵抗測定装置。   When the resistance variable means of each set of resistance circuits increases the resistance value of one set of resistance circuits from the resistance variable means by increasing the resistance value of each set of resistance circuits, the resistance value of the other set of resistance circuits The insulation resistance measuring apparatus according to claim 3, further comprising a function of alternately adjusting in a complementary manner so as to be reduced. 前記第4抵抗器に発生する電圧の極性を判別する極性判別手段を設け、正極性のときは正極側の演算および表示を可能として負極側の演算および表示をロックし、負極性のときは負極側の演算および表示を可能として正極側の演算および表示をロックすることを特徴とする請求項3または4に記載の絶縁抵抗の測定装置。   Polarity discrimination means for discriminating the polarity of the voltage generated in the fourth resistor is provided. When the polarity is positive, the calculation and display on the positive side can be performed and the calculation and display on the negative side are locked. When the polarity is negative, the polarity is negative. 5. The insulation resistance measuring device according to claim 3, wherein the calculation and display on the positive side are enabled and the calculation and display on the positive electrode side are locked. 前記絶縁抵抗値が予め設定された設定値より低下したことを判別して警報を発する警報手段を設けることを特徴とする請求項3から5の何れか1項に記載の絶縁抵抗の測定装置。   6. The insulation resistance measuring device according to claim 3, further comprising alarm means for issuing an alarm upon determining that the insulation resistance value has fallen below a preset value.
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