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JP2012198158A - Current sensor - Google Patents

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JP2012198158A
JP2012198158A JP2011063531A JP2011063531A JP2012198158A JP 2012198158 A JP2012198158 A JP 2012198158A JP 2011063531 A JP2011063531 A JP 2011063531A JP 2011063531 A JP2011063531 A JP 2011063531A JP 2012198158 A JP2012198158 A JP 2012198158A
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iron core
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JP5713744B2 (en
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Hiroshi Nishizawa
博志 西沢
Yoshimasa Watanabe
佳正 渡邊
Hajime Nakajima
一 仲嶋
Yuichi Yamaji
祐一 山地
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Mitsubishi Electric Corp
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Abstract

PROBLEM TO BE SOLVED: To provide a current sensor capable of securing measurement accuracy by suppressing magnetic saturation in current measurement and capable of reducing size and cost.SOLUTION: A current sensor 1 includes an iron core part 102 formed like a circular shape to collect magnetic flux generated by a primary current flowing into a current line 101 to be measured which is arranged through the center part of the circular shape and winding 103 wound around the iron core part 102 in a toroidal direction to detect a magnetic flux change in the iron core part 102 and is configured to measure the primary current from an output of the winding 103. The iron core part 102 includes a core division area Km in which a plurality of grooves 107 are arranged along the toroidal direction and a core connection area Ks connected in the toroidal direction. In the core division area Km of the iron core part 102, a ratio of a cross section of the iron core part 102 to a cross section of the groove 107 in a section of a diameter direction is fixed over a toroidal circumference.

Description

本発明は、導体に流れる電流を測定する電流センサに関する。   The present invention relates to a current sensor that measures a current flowing through a conductor.

従来の電流センサでは、被測定対象電流が大きくなると鉄心が磁気飽和してしまい、電流値を正確に測定することができなくなる。そのため、大電流を測定するためには、鉄心が磁気飽和しないように、鉄心の体積や磁束が通過する断面積を大きくする必要があるが、電流センサが大型化し重量も増加してしまう。   In the conventional current sensor, when the current to be measured increases, the iron core is magnetically saturated, and the current value cannot be measured accurately. Therefore, in order to measure a large current, it is necessary to increase the volume of the iron core and the cross-sectional area through which the magnetic flux passes so that the iron core is not magnetically saturated. However, the current sensor is increased in size and weight.

こうした大電流計測用の電流センサを小型軽量化するために、鉄心が磁気飽和しないように、鉄心を分割して、鉄心を貫通する磁束を減らして磁気飽和を抑制する方法が考えられる。例えば、鉄心部を鉄系の粉末と非磁性系の粉末を混成して硬化させたものを用いることが提案されている(例えば、特許文献1)。また、鉄の部分と非磁性の部分を均一に配置する形状にすることにより、計測精度を確保することが提案されている(例えば、特許文献2)。   In order to reduce the size and weight of such a current sensor for measuring a large current, a method is conceivable in which the iron core is divided and the magnetic flux penetrating the iron core is reduced to prevent magnetic saturation so that the iron core does not become magnetically saturated. For example, it has been proposed to use an iron core portion in which iron-based powder and non-magnetic powder are mixed and hardened (for example, Patent Document 1). In addition, it has been proposed to ensure measurement accuracy by forming a shape in which an iron portion and a nonmagnetic portion are uniformly arranged (for example, Patent Document 2).

特開2006−24844号公報(図2)Japanese Patent Laying-Open No. 2006-24844 (FIG. 2) 特許第4499707号公報(図1)Japanese Patent No. 4499707 (FIG. 1)

特許文献1のような電流センサは、磁性材と非磁性材の混合磁心を使用しているが、鉄の箇所と非磁性体の箇所が不定なので、磁束密度が局所的に増大するなどして均一にならない。その結果、場所により巻線を鎖交する磁束の本数が変わってしまうため、一部は磁気飽和し他の箇所は磁気飽和しないという現象が起こる。そのため、被測定対象電流線に対する直線性の精度が低下する。また、鉄心の飽和特性が一周にわたって均一で、かつ、巻線が一周すべてにわたって一様に巻かれていれば、外乱磁界が生じた場合でもその影響をキャンセルすることができるが、鉄心の飽和特性が場所により異なればキャンセルできず、計測精度が低下するという問題がある。   The current sensor as in Patent Document 1 uses a mixed magnetic core of magnetic material and non-magnetic material, but the location of iron and the location of non-magnetic material are indefinite, so the magnetic flux density locally increases. Not uniform. As a result, the number of magnetic fluxes interlinking the windings varies depending on the location, so that a phenomenon occurs in which some portions are magnetically saturated and other portions are not magnetically saturated. Therefore, the accuracy of linearity with respect to the current line to be measured is lowered. In addition, if the saturation characteristics of the iron core are uniform over the entire circumference and the winding is wound uniformly over the entire circumference, the influence can be canceled even if a disturbance magnetic field occurs. However, there is a problem that if it differs depending on the location, it cannot be canceled and the measurement accuracy is lowered.

また、特許文献2のような電流センサは、鉄心を均一に配置できるため、計測精度は確保できるものの、鉄心と非磁性体の位置を精度良く配置しようとすると、製造コストが高くなる傾向がある。   In addition, the current sensor as in Patent Document 2 can uniformly arrange the iron core, so that the measurement accuracy can be ensured. However, if the position of the iron core and the non-magnetic material is arranged with high accuracy, the manufacturing cost tends to increase. .

本発明の目的は、電流測定時における磁気飽和の抑制によって測定精度を確保でき、小型化、低コスト化が図られる電流センサを提供することである。   An object of the present invention is to provide a current sensor that can ensure measurement accuracy by suppressing magnetic saturation during current measurement, and can be reduced in size and cost.

上記目的を達成するために、本発明は、円環状に形成され、その中心部を貫通して配置された一次導体を流れる一次電流にて発生した磁束を集磁する鉄心部と、
鉄心部に対しポロイダル方向に巻回され、鉄心部内の磁束変化を検出するための巻線とを備え、
巻線の出力から一次電流を測定するための電流センサであって、
鉄心部は、溝がトロイダル方向に沿って複数配置されたコア分割領域と、トロイダル方向に連結したコア連結領域とを含み、
鉄心部のコア分割領域において、径方向断面における鉄心部の断面積と溝の断面積との比がトロイダル全周に渡って一定であることを特徴とする。
In order to achieve the above object, the present invention is formed in an annular shape, and an iron core portion that collects magnetic flux generated by a primary current flowing through a primary conductor disposed through a central portion thereof,
It is wound in the poloidal direction with respect to the iron core, and includes a winding for detecting a magnetic flux change in the iron core,
A current sensor for measuring the primary current from the output of the winding,
The iron core part includes a core division region in which a plurality of grooves are arranged along the toroidal direction, and a core connection region connected in the toroidal direction,
In the core divided region of the iron core, the ratio of the cross-sectional area of the iron core to the cross-sectional area of the groove in the radial cross section is constant over the entire toroidal circumference.

本発明によれば、電流測定時においてコア連結領域で磁気飽和が生ずると、主にコア分割領域が鉄心として機能するようになる。そのため鉄心内の磁束密度が低減し、磁気飽和を生じさせる一次電流を大きくでき、かつ、巻線断面内の磁束密度が均一化され、測定精度を確保できる。また、鉄心部は、単一部材として形成した場合、製作が容易になり、高精度な電流センサを低コストで実現できる。   According to the present invention, when magnetic saturation occurs in the core connection region during current measurement, the core division region mainly functions as an iron core. Therefore, the magnetic flux density in the iron core is reduced, the primary current that causes magnetic saturation can be increased, and the magnetic flux density in the winding cross section is made uniform, so that measurement accuracy can be ensured. Further, when the iron core portion is formed as a single member, it can be easily manufactured, and a highly accurate current sensor can be realized at low cost.

本発明の実施の形態1による電流センサを示す斜視図である。It is a perspective view which shows the current sensor by Embodiment 1 of this invention. 図1に示した電流センサの平面図である。It is a top view of the current sensor shown in FIG. 図1に示した鉄心部の平面図である。It is a top view of the iron core part shown in FIG. 図3中のA部の拡大図である。It is an enlarged view of the A section in FIG. 鉄心部内の磁束の様子を模式的に表した説明図である。It is explanatory drawing which represented the mode of the magnetic flux in an iron core part typically. 鉄心部内の磁束の様子を模式的に表した説明図である。It is explanatory drawing which represented the mode of the magnetic flux in an iron core part typically. 電流センサについて被測定電流に対する出力特性の一例を示すグラフである。It is a graph which shows an example of the output characteristic with respect to to-be-measured current about a current sensor. 鉄心部形状の他の例を示す平面図である。It is a top view which shows the other example of an iron core part shape. 鉄心部形状のさらに他の例を示す平面図である。It is a top view which shows the other example of an iron core part shape. 本発明の実施の形態2による電流センサの鉄心部を示す部分平面図である。It is a fragmentary top view which shows the iron core part of the current sensor by Embodiment 2 of this invention. 本発明の実施の形態3による電流センサを示す斜視図である。It is a perspective view which shows the current sensor by Embodiment 3 of this invention. バイアス磁界印加機構の他の例を示す斜視図である。It is a perspective view which shows the other example of a bias magnetic field application mechanism.

実施の形態1.
図1は、本発明の実施の形態1による電流センサ1を示す斜視図である。電流センサ1は、鉄心部102と、巻線103などを備える。鉄心部102は、円環状に形成された磁性材料で構成され、その径方向断面は、例えば、矩形状または隅丸矩形状である。鉄心部102の中心部を貫通するように、被測定電流線101が一次導体として配置される。被測定電流線101に一次電流が流れると、その周囲に磁束104を発生し、鉄心部102は、発生した磁束104を集磁する。
Embodiment 1 FIG.
FIG. 1 is a perspective view showing a current sensor 1 according to Embodiment 1 of the present invention. The current sensor 1 includes an iron core portion 102, a winding 103, and the like. The iron core portion 102 is made of a magnetic material formed in an annular shape, and its radial cross section has, for example, a rectangular shape or a rounded corner rectangular shape. The current wire to be measured 101 is arranged as a primary conductor so as to penetrate the central portion of the iron core portion 102. When the primary current flows through the measured current line 101, a magnetic flux 104 is generated around the current line 101, and the iron core 102 collects the generated magnetic flux 104.

巻線103は、円環状の鉄心部102に対しポロイダル方向に巻回され、二次巻線として鉄心部102内の磁束変化を検出する機能を有する。巻線103の両端には、例えば、負担抵抗105が接続されており、被測定電流線101に流れる交流電流により磁束104が時間変化すると、それに伴い巻線103に誘導電流が生ずる。そこで、外部測定器を用いて負担抵抗105の両端電圧を計測することにより、被測定電流線101に流れる一次電流の振幅、周波数および位相を測定することができる。こうした電流センサ1は、例えば、変流器(CT)として動作可能である。   The winding 103 is wound in the poloidal direction around the annular iron core portion 102 and has a function of detecting a magnetic flux change in the iron core portion 102 as a secondary winding. For example, a burden resistor 105 is connected to both ends of the winding 103. When the magnetic flux 104 changes with time due to an alternating current flowing through the current wire 101 to be measured, an induced current is generated in the winding 103 accordingly. Therefore, by measuring the voltage across the load resistor 105 using an external measuring instrument, the amplitude, frequency and phase of the primary current flowing through the current line 101 to be measured can be measured. Such a current sensor 1 can operate as a current transformer (CT), for example.

図2は、図1に示した電流センサ1の平面図である。図3は、図1に示した鉄心部102の平面図である。図4は、図3中のA部の拡大図である。被測定電流線101は、紙面垂直方向に延びており、円環状の鉄心部102の中心を貫通している。巻線103は、円環状の鉄心部102に対しポロイダル方向に巻回されている。   FIG. 2 is a plan view of the current sensor 1 shown in FIG. FIG. 3 is a plan view of the iron core portion 102 shown in FIG. FIG. 4 is an enlarged view of a portion A in FIG. The measured current line 101 extends in the direction perpendicular to the paper surface and passes through the center of the annular iron core 102. The winding 103 is wound around the annular core 102 in the poloidal direction.

鉄心部102は、溝107がトロイダル方向に沿って複数配置されたコア分割領域Kmと、トロイダル方向に連結したコア連結領域Ksとを含む。コア分割領域Kmにおいて、溝107は、鉄心部102の径方向と斜めに交差するように、鉄心部102の外側から内側へ向かって切れ目状に形成され、隣接する鉄部106の間のエアギャップとして機能する。一方、コア連結領域Ksでは、溝107が存在せず、鉄部106同士が一体的に連結されている。   The iron core portion 102 includes a core division region Km in which a plurality of grooves 107 are arranged along the toroidal direction, and a core connection region Ks connected in the toroidal direction. In the core division region Km, the groove 107 is formed in a cut shape from the outer side to the inner side of the iron core part 102 so as to obliquely intersect the radial direction of the iron core part 102, and an air gap between adjacent iron parts 106. Function as. On the other hand, in the core connection region Ks, the groove 107 does not exist, and the iron portions 106 are integrally connected.

ここで、図4に示すように、ある溝107に着目して、径方向断面においてコア分割領域Kmの内側エッジから溝107の内側エッジまでの距離をc1、溝107のギャップ長をg、溝107の外側エッジからコア分割領域Kmの外側エッジまでまでの距離をc2とする。また、別の溝107に着目して、径方向断面においてコア分割領域Kmの内側エッジから溝107の内側エッジまでの距離をc1’、溝107のギャップ長をg’、溝107の外側エッジからコア分割領域Kmの外側エッジまでまでの距離をc2’とする。このとき、g:(c1+c2)=g’:(c1’+c2’)が成立する。   Here, as shown in FIG. 4, focusing on a certain groove 107, the distance from the inner edge of the core division region Km to the inner edge of the groove 107 in the radial cross section is c1, the gap length of the groove 107 is g, and the groove Let c2 be the distance from the outer edge 107 to the outer edge of the core division area Km. Further, paying attention to another groove 107, the distance from the inner edge of the core split region Km to the inner edge of the groove 107 in the radial section is c1 ′, the gap length of the groove 107 is g ′, and from the outer edge of the groove 107. Let c2 ′ be the distance to the outer edge of the core division area Km. At this time, g: (c1 + c2) = g ′ :( c1 ′ + c2 ′) is established.

換言すると、鉄心部102のコア分割領域Kmにおいて、径方向断面における鉄心部102の断面積と溝107の断面積との比が、トロイダル全周に渡って一定である。こうした部品形状は、例えば、板状の鉄材をプレス加工などにより一度に形成することができるので、高い寸法精度を低い製造コストで実現することができる。   In other words, in the core division region Km of the iron core portion 102, the ratio of the cross-sectional area of the iron core portion 102 to the cross-sectional area of the groove 107 in the radial cross section is constant over the entire toroidal circumference. Such a component shape can be formed, for example, by pressing a plate-shaped iron material at a time by pressing or the like, so that high dimensional accuracy can be realized at a low manufacturing cost.

次に、電流センサ1の動作について説明する。被測定電流線101に電流が流れると、鉄心部102の内部では磁束がトロイダル方向に通過する。   Next, the operation of the current sensor 1 will be described. When a current flows through the current wire 101 to be measured, the magnetic flux passes in the toroidal direction inside the iron core portion 102.

図5および図6は、鉄心部102内の磁束の様子を模式的に表した説明図である。ここで、矢印の密度が磁束密度に対応する。被測定電流線101を流れる電流が少ないときは、図5に示すように、磁束は内側の一体化されたコア連結領域Ksを主に流れる。このとき磁束が低いため、磁気飽和は起こっていない。従って、通常の変流器の動作と同様に、鉄心部102を貫く磁束変化がそのまま巻線103の誘導電流として出力される。   5 and 6 are explanatory diagrams schematically showing the state of magnetic flux in the iron core portion 102. FIG. Here, the density of the arrows corresponds to the magnetic flux density. When the current flowing through the measured current line 101 is small, as shown in FIG. 5, the magnetic flux mainly flows through the inner core connection region Ks. At this time, magnetic saturation does not occur because the magnetic flux is low. Therefore, similarly to the operation of a normal current transformer, a change in magnetic flux passing through the iron core 102 is output as an induction current of the winding 103 as it is.

次に、被測定電流線101の電流値が大きくなると、図6(a)に示すように、鉄心部102を貫く磁束の大部分は、内側の一体化されたコア連結領域Ksをさらに貫くようになり、このコア連結領域Ksだけが磁気飽和するようになる。磁気飽和した箇所は、透磁率が低下し、完全に飽和すると透磁率はほぼ空気と同等になる。その結果、透磁率の高い領域、すなわち実効的な鉄心領域は、図6(b)に示すように、コア連結領域Ksを除いた、コア分割領域Kmだけになる。この状態は、すなわち高い寸法精度で位置決めされた分割鉄心と同等である。この状態になれば、被測定電流が大きくなったとしても、実効的な鉄心領域は、分割された鉄心と同様に機能するため、エアギャップによる磁気飽和の抑制が可能になり、大電流でも精度良く測定することができる。   Next, when the current value of the current wire 101 to be measured increases, as shown in FIG. 6A, most of the magnetic flux passing through the iron core portion 102 further passes through the inner integrated core connection region Ks. Thus, only the core connection region Ks becomes magnetically saturated. The magnetically saturated portion has a reduced magnetic permeability, and when fully saturated, the magnetic permeability is almost equal to that of air. As a result, the region having high magnetic permeability, that is, the effective core region is only the core division region Km excluding the core connection region Ks, as shown in FIG. This state is equivalent to a split iron core positioned with high dimensional accuracy. In this state, even if the current to be measured becomes large, the effective core region functions in the same way as the divided core, so magnetic saturation due to the air gap can be suppressed, and accuracy can be achieved even with a large current. It can be measured well.

図7は、電流センサ1について被測定電流に対する出力特性の一例を示すグラフである。被測定電流がゼロからスタートして、コア連結領域Ksが磁気飽和する電流値I1までの小さな電流範囲では、非線形特性を示している。一方、電流値がI1を超えると、コア分割領域Kmが分割鉄心として機能するため、広い電流範囲に渡って線形性が確保されていることが判る。従って、電流センサ1の測定範囲を、電流値I1からコア分割領域Km自体が磁気飽和を示す電流値I2までの範囲に設定することにより、十分実用に耐えられる高い測定精度を確保できる。また、鉄心部102の鉄部105は、プレス加工などにより低コストで良好な寸法精度が得られるので、出力の線形性は高く、また、外乱磁界に対する耐性も高い。   FIG. 7 is a graph showing an example of output characteristics with respect to the current to be measured for the current sensor 1. In the small current range from the current to be measured starting from zero to the current value I1 at which the core connection region Ks is magnetically saturated, nonlinear characteristics are shown. On the other hand, when the current value exceeds I1, the core divided region Km functions as a divided iron core, and thus it can be seen that linearity is ensured over a wide current range. Therefore, by setting the measurement range of the current sensor 1 to the range from the current value I1 to the current value I2 in which the core division region Km itself indicates magnetic saturation, it is possible to ensure a high measurement accuracy that can sufficiently withstand practical use. In addition, since the iron portion 105 of the iron core portion 102 can be obtained with good dimensional accuracy at low cost by pressing or the like, the output linearity is high and the resistance against the disturbance magnetic field is also high.

コア連結領域Ksは、磁気飽和を容易にするために、磁束が通過するエリアの幅や断面積は可能な限り小さい方が望ましい。図4に示すように、径方向断面においてコア連結領域Ksの幅をa、コア分割領域Kmの幅をbとして、幅aは幅bの10%以下(0<a/b≦0.1)であることが好ましい。また、磁束が通過する断面積に換算すると、径方向断面においてコア連結領域Ksの断面積Saは、コア分割領域Kmの断面積Sbの10%以下(0<Sa/Sb≦0.1)であることが好ましい。これにより、被測定電流が小さくても磁気飽和し易くなり、図7のグラフにおいて電流値I1をより小さくできるため、電流の計測範囲を拡大することができる。   In order to facilitate magnetic saturation, the core connection region Ks desirably has the smallest possible width and cross-sectional area of the area through which the magnetic flux passes. As shown in FIG. 4, in the radial cross section, the width of the core connection region Ks is a, the width of the core division region Km is b, and the width a is 10% or less of the width b (0 <a / b ≦ 0.1). It is preferable that In terms of the cross-sectional area through which the magnetic flux passes, the cross-sectional area Sa of the core coupling region Ks in the radial cross-section is 10% or less (0 <Sa / Sb ≦ 0.1) of the cross-sectional area Sb of the core divided region Km. Preferably there is. Thereby, even if the current to be measured is small, the magnetic saturation is likely to occur, and the current value I1 can be further reduced in the graph of FIG. 7, so that the current measurement range can be expanded.

本実施形態では、図2〜図4に示したように、鉄心部102の内側にコア連結領域Ksを配置し、鉄心部102の外側にコア分割領域Kmを配置した場合を例示している。代替として、図8に示すように、鉄心部102の内側にコア分割領域Kmを配置し、鉄心部102の外側にコア連結領域Ksを配置しても構わない。また、図9に示すように、鉄心部102の内側および外側にコア連結領域Ksをそれぞれ配置し、2つのコア連結領域Ksの間にコア分割領域Kmを配置しても構わない。また、図示していないが、鉄心部102の内側および外側にコア分割領域Kmをそれぞれ配置し、2つのコア分割領域Kmの間にコア連結領域Ksを配置しても構わない。   In the present embodiment, as illustrated in FIGS. 2 to 4, the case where the core connection region Ks is disposed inside the iron core portion 102 and the core division region Km is disposed outside the iron core portion 102 is illustrated. Alternatively, as shown in FIG. 8, the core division region Km may be disposed inside the iron core portion 102, and the core connection region Ks may be disposed outside the iron core portion 102. Moreover, as shown in FIG. 9, the core connection region Ks may be disposed inside and outside the iron core portion 102, and the core division region Km may be disposed between the two core connection regions Ks. Moreover, although not shown in figure, the core division | segmentation area | region Km may be arrange | positioned at the inner side and the outer side of the iron core part 102, respectively, and the core connection area | region Ks may be arrange | positioned between the two core division areas Km.

本実施形態によれば、電流測定時においてコア連結領域Ksで磁気飽和が生ずると、コア分割領域Kmが分割鉄心として機能するようになる。そのため鉄心内の磁束密度が低減し、磁気飽和を生じさせる一次電流を大きくでき、かつ、巻線断面内の磁束密度が均一化され、測定精度を確保できる。また、鉄心部102は、単一部材として形成した場合、製作が容易になり、製造工程が簡略化され、高精度な電流センサを低コストで実現できる。   According to the present embodiment, when magnetic saturation occurs in the core connection region Ks during current measurement, the core divided region Km functions as a divided iron core. Therefore, the magnetic flux density in the iron core is reduced, the primary current that causes magnetic saturation can be increased, and the magnetic flux density in the winding cross section is made uniform, so that measurement accuracy can be ensured. Further, when the iron core portion 102 is formed as a single member, the manufacturing becomes easy, the manufacturing process is simplified, and a highly accurate current sensor can be realized at low cost.

実施の形態2.
図10は、本発明の実施の形態2による電流センサ1の鉄心部102を示す部分平面図である。本実施形態は、実施の形態1と同様な構成を有するが、コア連結領域Ksにおいて、磁路を長くし磁気抵抗を増大させている点が相違する。
Embodiment 2. FIG.
FIG. 10 is a partial plan view showing the iron core portion 102 of the current sensor 1 according to the second embodiment of the present invention. The present embodiment has the same configuration as that of the first embodiment, but is different in that the magnetic path is lengthened and the magnetic resistance is increased in the core connection region Ks.

コア連結領域Ksは、複数の溝107が交差指状に配置され、折り返し線(いわゆるミアンダライン)108の形状を有する。こうした構造により、磁束がコア連結領域Ksを通過する際、実施の形態1と比べて、磁束が通過する断面積が小さくなり、しかも磁束が通過する距離が増加するため、コア連結領域Ksでの磁気飽和レベルが低くなる。その結果、被測定電流が小さくても飽和し易くなり、図7のグラフにおいて電流値I1をより小さくできるため、電流の計測範囲を拡大でき、ワイドレンジな電流センサを実現できる。   In the core connection region Ks, a plurality of grooves 107 are arranged in a cross finger shape and have a shape of a fold line (so-called meander line) 108. With such a structure, when the magnetic flux passes through the core coupling region Ks, the cross-sectional area through which the magnetic flux passes is smaller than in the first embodiment, and the distance through which the magnetic flux passes increases. Magnetic saturation level is lowered. As a result, even if the current to be measured is small, it is easy to saturate, and the current value I1 can be made smaller in the graph of FIG. 7, so that the current measurement range can be expanded and a wide range current sensor can be realized.

実施の形態3.
図11は、本発明の実施の形態3による電流センサ1を示す斜視図である。本実施形態は、実施の形態1と同様な構成を有するが、鉄心部102に対してトロイダル方向のバイアス磁界を印加するためのバイアス磁界印加機構が設けられている点で相違する。
Embodiment 3 FIG.
FIG. 11 is a perspective view showing a current sensor 1 according to Embodiment 3 of the present invention. The present embodiment has the same configuration as that of the first embodiment, but is different in that a bias magnetic field application mechanism for applying a toroidal bias magnetic field to the iron core portion 102 is provided.

図11において、バイアス磁界印加機構として、被測定電流線101とは別個の電流線109を被測定電流線101と平行に配置している。電流線109の両端は電流源(不図示)に接続されており、電流線109に所定の直流電流が流れることによって、鉄心部102のトロイダル方向に直流バイアス磁界が発生する。これにより鉄心部102の内部では、被測定電流線101による磁界に対して電流線109によるバイアス磁界が重畳することになる。その結果、鉄心部102のコア連結領域Ksが磁気飽和に達する磁界が小さくなる。換言すると、コア連結領域Ksは、被測定電流線101の電流値が小さくても容易に磁気飽和することになる。その結果、被測定電流が小さくても飽和し易くなり、図7のグラフにおいて電流値I1をより小さくできるため、電流の計測範囲を拡大でき、ワイドレンジな電流センサを実現できる。   In FIG. 11, as a bias magnetic field application mechanism, a current line 109 separate from the current line 101 to be measured is arranged in parallel with the current line 101 to be measured. Both ends of the current line 109 are connected to a current source (not shown). When a predetermined DC current flows through the current line 109, a DC bias magnetic field is generated in the toroidal direction of the iron core portion 102. As a result, the bias magnetic field generated by the current line 109 is superimposed on the magnetic field generated by the current line 101 to be measured inside the iron core portion 102. As a result, the magnetic field at which the core coupling region Ks of the iron core portion 102 reaches magnetic saturation is reduced. In other words, the core connection region Ks is easily magnetically saturated even if the current value of the measured current line 101 is small. As a result, even if the current to be measured is small, it is easy to saturate, and the current value I1 can be made smaller in the graph of FIG. 7, so that the current measurement range can be expanded and a wide range current sensor can be realized.

図12は、バイアス磁界印加機構の他の例を示す斜視図である。バイアス磁界印加機構として、巻線103とは別個の巻線110を、円環状の鉄心部102に対しポロイダル方向に巻回している。巻線110の両端は電流源111に接続されており、巻線110に所定の直流電流が流れることによって、図11と同様に、鉄心部102のトロイダル方向に直流バイアス磁界が発生する。その結果、鉄心部102のコア連結領域Ksが磁気飽和に達する磁界が小さくなり、図7のグラフにおいて電流値I1をより小さくできるため、電流の計測範囲を拡大でき、ワイドレンジな電流センサを実現できる。   FIG. 12 is a perspective view showing another example of the bias magnetic field applying mechanism. As a bias magnetic field applying mechanism, a winding 110 separate from the winding 103 is wound around the annular core 102 in the poloidal direction. Both ends of the winding 110 are connected to a current source 111, and when a predetermined DC current flows through the winding 110, a DC bias magnetic field is generated in the toroidal direction of the iron core portion 102, as in FIG. As a result, the magnetic field at which the core connection region Ks of the iron core portion 102 reaches magnetic saturation is reduced, and the current value I1 can be further reduced in the graph of FIG. 7, so that the current measurement range can be expanded and a wide-range current sensor is realized. it can.

なお、図11と図12では、電流線の追加設置によるバイアス磁界の重畳について説明したが、代替として、電磁石や永久磁石の追加設置によってトロイダル方向のバイアス磁界を重畳するように構成してもよい。   11 and 12, the bias magnetic field superposition by the additional installation of the current line has been described. Alternatively, the toroidal bias magnetic field may be superposed by the additional installation of an electromagnet or a permanent magnet. .

また、バイアス磁界の印加方向は、図11や図12のように、鉄心部102のトロイダル方向が望ましいが、これに限ることはなく、コア連結領域Ksが磁気飽和すれば足りるため、バイアス磁界方向について特に制限は無い。   The bias magnetic field application direction is preferably the toroidal direction of the iron core portion 102 as shown in FIGS. 11 and 12, but is not limited to this, and it is sufficient if the core connection region Ks is magnetically saturated. There is no particular restriction on.

1 電流センサ、 101 被測定電流線、 102 鉄心部、 103 巻線、
104 磁束、 105 負担抵抗、 106 鉄部、 107 溝、
108 折り返し線、 109 バイアス磁界印加用電流線、
110 バイアス磁界印加用巻線、 111 電流源、 Km コア分割領域、
Ks コア連結領域。
1 current sensor, 101 current wire to be measured, 102 iron core, 103 windings,
104 magnetic flux, 105 burden resistance, 106 iron part, 107 groove,
108 fold line, 109 current line for applying bias magnetic field,
110 Bias magnetic field application winding, 111 Current source, Km core split region,
Ks Core connection region.

Claims (5)

円環状に形成され、その中心部を貫通して配置された一次導体を流れる一次電流にて発生した磁束を集磁する鉄心部と、
鉄心部に対しポロイダル方向に巻回され、鉄心部内の磁束変化を検出するための巻線とを備え、
巻線の出力から一次電流を測定するための電流センサであって、
鉄心部は、溝がトロイダル方向に沿って複数配置されたコア分割領域と、トロイダル方向に連結したコア連結領域とを含み、
鉄心部のコア分割領域において、径方向断面における鉄心部の断面積と溝の断面積との比がトロイダル全周に渡って一定であることを特徴とする電流センサ。
An iron core that collects magnetic flux generated by a primary current that flows through a primary conductor that is formed in an annular shape and passes through a central portion thereof;
It is wound in the poloidal direction with respect to the iron core, and includes a winding for detecting a magnetic flux change in the iron core,
A current sensor for measuring the primary current from the output of the winding,
The iron core part includes a core division region in which a plurality of grooves are arranged along the toroidal direction, and a core connection region connected in the toroidal direction,
A current sensor characterized in that a ratio of a cross-sectional area of a core part and a cross-sectional area of a groove in a radial cross section is constant over the entire toroidal circumference in a core division region of the iron core part.
コア連結領域は、鉄心部の内側および外側のいずれか一方または両方に配置されることを特徴とする請求項1記載の電流センサ。   The current sensor according to claim 1, wherein the core connection region is disposed on one or both of an inner side and an outer side of the iron core. 径方向断面において、コア連結領域の断面積は、コア分割領域の断面積の10%以下であることを特徴とする請求項1または2記載の電流センサ。   3. The current sensor according to claim 1, wherein a cross-sectional area of the core connection region is 10% or less of a cross-sectional area of the core division region in the radial cross section. コア連結領域は、複数の溝が交差指状に配置された折り返し線の形状を有することを特徴とする請求項1〜3のいずれかに記載の電流センサ。   The current sensor according to any one of claims 1 to 3, wherein the core connection region has a shape of a folding line in which a plurality of grooves are arranged in a cross finger shape. 鉄心部に対してトロイダル方向のバイアス磁界を印加するためのバイアス磁界印加機構をさらに備えたことを特徴とする請求項1記載の電流センサ。   The current sensor according to claim 1, further comprising a bias magnetic field applying mechanism for applying a toroidal bias magnetic field to the iron core.
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