JPS5833167A - Current measurement - Google Patents

Current measurement

Info

Publication number
JPS5833167A
JPS5833167A JP56131825A JP13182581A JPS5833167A JP S5833167 A JPS5833167 A JP S5833167A JP 56131825 A JP56131825 A JP 56131825A JP 13182581 A JP13182581 A JP 13182581A JP S5833167 A JPS5833167 A JP S5833167A
Authority
JP
Japan
Prior art keywords
magnetic
current
circuit
magnetic field
hall element
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Granted
Application number
JP56131825A
Other languages
Japanese (ja)
Other versions
JPS6411149B2 (en
Inventor
Yasufumi Suzuki
康文 鈴木
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Hioki EE Corp
Original Assignee
Hioki Denki KK
Hioki EE Corp
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Hioki Denki KK, Hioki EE Corp filed Critical Hioki Denki KK
Priority to JP56131825A priority Critical patent/JPS5833167A/en
Publication of JPS5833167A publication Critical patent/JPS5833167A/en
Publication of JPS6411149B2 publication Critical patent/JPS6411149B2/ja
Granted legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01RMEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
    • G01R15/00Details of measuring arrangements of the types provided for in groups G01R17/00 - G01R29/00, G01R33/00 - G01R33/26 or G01R35/00
    • G01R15/14Adaptations providing voltage or current isolation, e.g. for high-voltage or high-current networks
    • G01R15/20Adaptations providing voltage or current isolation, e.g. for high-voltage or high-current networks using galvano-magnetic devices, e.g. Hall-effect devices, i.e. measuring a magnetic field via the interaction between a current and a magnetic field, e.g. magneto resistive or Hall effect devices
    • G01R15/202Adaptations providing voltage or current isolation, e.g. for high-voltage or high-current networks using galvano-magnetic devices, e.g. Hall-effect devices, i.e. measuring a magnetic field via the interaction between a current and a magnetic field, e.g. magneto resistive or Hall effect devices using Hall-effect devices

Abstract

PURPOSE:To enabe accurate detection of current free from effect of magnetic hysteresis by employing the overlapping of an A.C. bias magnetic field in a current measuring clamp instrument provided with a Hall element in a close magnetic circuit. CONSTITUTION:An A.C. bias magntic field overlaps a magnetic field corresponding to current flowing through an electric circuit 4 to be measured running through a magnetic core 2 which forms a closed magnetic circuit provided with a Hall element 1 through an A.C. attenaution oscillator 6 or the like. As a result, the final magnetized point of the core 2 is determined by a magnetic resistance, a saturated magnetized point or the like and hence takes a value linearly corresponding to the current of the electric circuit 4 not affected by magnetic hysteresis. This eliminates demagnetization required for each measurement through a winding 3, a sample hold circuit 8, an indicator 9 and the like thereby enabling accurate measurement of small current with an easy operation free from effect of the magnetic hysteresis or the like.

Description

【発明の詳細な説明】 この尭明は磁気コアと空■とによって形成される■磁路
中にホール素子を有するクランプ計器による電流測定法
に関するものである。
DETAILED DESCRIPTION OF THE INVENTION This patent relates to a current measurement method using a clamp instrument having a Hall element in a magnetic path formed by a magnetic core and an air space.

上記し九よ51タヲング計鰺におiて、微小電流をa+
*す為jllKは、蜜li1部のレフタ!ンスとスアの
とスデ9FJKよって決意書れ為農産特性を有する丸め
、過大入力信号中外部11鼻によシ零点の移動中磁9に
8賂の非直線性の影響から誤差を生じる。この九めKJ
I/園に略示するように、閉磁路申にホール素子Iを有
する前記計器の磁気コアcgo−sKsi*巻纏Fを設
け、ee巻a*に*mmmm法を流してj1#il前に
交流消磁を行なう方法が従来一般的に実施されている。
At the above-mentioned 9-51 tawing meter i, the minute current is a +
*JllK is Mitsuli 1st part's lefta! Errors occur due to the influence of non-linearity of the magnetic field 9 during the movement of the external 11 nose zero point during the rounding and excessive input signals which have agricultural characteristics. This nine KJ
As shown schematically in I/en, the magnetic core cgo-sKsi* winding F of the instrument having the Hall element I is provided in the closed magnetic circuit, and the *mmmm method is applied to the ee winding a* before j1#il. Conventionally, a method of performing AC demagnetization has been commonly practiced.

然し乍らこのように’J&置され良計#kにおいても、
爽際の測定時には入°力信号中外藻磁昇の大きさ及び極
性によ珈、繭記磁鬼圃賂の履Nl5I性に基づく測定誤
差を生じる。
However, even in 'J & good plan #k like this,
When measuring the fresh air, a measurement error occurs due to the magnitude and polarity of the input signal's magnetic flux, which is based on the magnitude and polarity of the magnetic field.

叉JIIJIiK略示するようK、層中aIJを用いて
その負層RKよ)II気履絡の磁束が當に零となるよう
に廖處されている亀のゼw7ツツタスmKよ為タヲンプ
計MEシいて一岡皺にφ鋤で麦流綱IIlが行なわれて
いるが、−五綱mis大#1な外藻磁鼻中急激謙遥大入
力信号が印加畜れ為と増巾#l1lD応答が遍従不■と
な)、ゼw7ツツタス法の動作から逸脱し、i+ucs
賂の帯磁によ)脂作戚が大畷く変化して了りので側室誤
差を生じる。叉上記しえ場合、人的IIk作によって消
磁を行なっているから、処置を忘れ九tk1m定を行な
って了う等の事態を乗111KIF止する仁とが困難で
、特に最時詞にIる記l&測定の際には磁化1受けに後
の測定値は信頼がsI−#′jないものKなって了り。
叉JIIJIiK As shown in the diagram, using the aIJ in the layer and its negative layer RK) II, the tortoise ze w7 which has been removed so that the magnetic flux of the circuit becomes zero, the tap meter ME. Then, Kazuoka wrinkles are being performed with a φ plow, but - a large input signal is suddenly applied in the outer seaweed magnetic nose of the five class mis large #1, and the response is increased. deviates from the operation of the ze w7 tutus method, i+ucs
Due to the magnetization of bribes, the relatives of Fusaku changed drastically, resulting in the error of concubines. In the above case, since the demagnetization is done manually, it is difficult to prevent the situation such as forgetting the procedure and completing the 9tk1m determination, especially when it comes to the last sentence. At the time of measurement, the measured values after magnetization 1 were unreliable.

この発WAは閉磁路中にホール素子を有するタヲンデ計
器を用i丸電流測定において、被#l定電流によって発
生する磁界に一様に減衰する交流磁界を重畳することに
よ如、磁気囲路が有する履MI!#性に影響されること
なく直線性の優れ九電流検崗を特徴とする請Nil津農
産磁化機構に墓づi九電流測定法に関するものである1
次にこの発明の夷1例をまずjlJ図、1s#図を参履
し乍ら説明する。
This WA is generated by superimposing a uniformly attenuated alternating current magnetic field on the magnetic field generated by a constant current when measuring a circular current using a Tawonde meter that has a Hall element in the closed magnetic circuit. I have MI! This is related to the nine-current measurement method, which is based on the agricultural and industrial magnetization mechanism, which is characterized by excellent linearity and nine-current detection without being affected by
Next, one example of the present invention will be explained with reference to the jlJ diagram and the 1s# diagram.

JIJIIK示すようKlfi磁路中磁路−ル素子(υ
と燦遺増巾器偽)jPよび磁気コア(2)の−蕗に設け
た巻線(2)によって構成されるゼロ7フツタス法によ
る電流検出は従来と岡皺であるが、この発明では被測定
電路(4)の電流によって発生す為磁界に、一様Kmf
iする交流磁界を短周期を4って閲けつ的1つfi続釣
に重畳させる−のである。jlち制御四路(1)によ)
交流減衰発振41IB−およびサンプル・*−〜ド禰賂
(8)を1aE重畳imriarx、’sp重畳期関r
sに応じてそれぞれ交互に駆動制御する。例えば制御側
路け)011号によって歇wmsipら数S程度の如き
周期をもって非重畳期岡TSではタッンデ計器の出力電
圧をサンプル・傘−〜ド―絡(2)Kてサング!ングし
、次いで重畳期間TIではナンデ〜・傘−ルド圓賂に)
を−−ルド状襲として直着の非重畳期Hrs鯵の値を保
持し且つ同時に交流減衰発振鰺■を動4wさせて帰還増
巾器(勾、巻線(2)を介して交流減衰磁界を磁気コア
儲)K供給す為、jlち前記したよう&煉屑鋼をもって
前記重畳、非重畳を交互に繰返し、ナンデ〜・*−A/
)″開路(2)によって得られる織方電圧を表示M(1
)によって表示し測定可能とするものでh暴。
As shown in JIJIIK, the magnetic path element (υ
The current detection by the zero-7 foot-tasting method, which is constructed by the winding (2) provided on the base of the magnetic core (2), is conventional and OKASI, but in this invention, the current detection is The magnetic field generated by the current in the measurement circuit (4) has a uniform Kmf
The alternating current magnetic field that generates i is superimposed on one target over four short periods. (according to the control method (1))
AC damped oscillation 41IB- and sample *- ~ donegi (8) 1aE superimposed imriarx,'sp superimposed period relation r
Drive control is performed alternately according to s. For example, in the non-superimposed period Oka TS, the output voltage of the tande meter is sampled by the control side (control side) No. 011 with a period of about several S. and then in the superimposed period TI to Nande ~ Umbrella ~ Ludo Ensai)
- Hold the directly applied non-superimposed period Hrs value as a waveform, and at the same time operate the AC damped oscillation 4W to create an AC damped magnetic field via the feedback amplifier (gradient) and winding (2). In order to supply the magnetic core (K), repeat the superposition and non-superposition alternately with the brick scrap steel as described above, and then
)''Display the weaving voltage obtained by opening (2)M(1
) that can be displayed and measured.

lI!、夕1141番錫の動作法要を示す−ので、it
cは交流滅責電流波彫、ipは被j1重電路0)の電流
法要、盃はそれらKよってlI気開回路発生す為磁束波
廖、町はサンプル・*−kr園路の^力電圧波形でシー
バスフィルl#cよってフィルIデングす番ことによ)
被測定電流Kl:lIK比例する出方電圧法要りを得る
ことができる。なお予め被#定電流法要の時間的変化に
比して充分に蓋かい周期でw/i記重畳、非重畳を繰返
すことによ)*測定電流法要をm喪に−示す為ことがで
きみことは伺らかに場廖書れるべ會でhる。
lI! , it shows the action memorial service of No. 1141 in the evening, so it
c is the alternating current wave carving, ip is the electric current of the subject j1 heavy electric circuit 0), the cup is the magnetic flux wave liang because the open circuit is generated by them K, the town is the sample *-kr the power voltage of the garden path The waveform shows the seabass fill l#c, so the fill I dengue is the best.)
An output voltage method that is proportional to the current to be measured Kl:lIK can be obtained. By repeating the superimposition and non-superimposition of w/i at a sufficient interval compared to the temporal change of the constant current to be measured in advance) The matter will be revealed at the meeting where I will be able to write about it.

このJIwの方法による動作原塩は曽記しぇ通)交流磁
界とIIIfJIIJILとを重畳して印加し九と1に
得られ為磁化機構であ)、減資す為*流磁界の豪中最大
値がJl気関賂を飽和す石だけの充分傘大龜亀値で島れ
ば%ll気關賂開路して+V%る寿直纏性中残臂磁電K
11ll&<信号磁界の大自書によって決*書れ為と−
ラxsxpsa−農産磁化搗構によ1もので畠る。し−
kがってこのi&嘴の方決によるタフンデ計一番1単に
交流#1mlを行なっ丸後信号磁昇を印−す為g!来方
式のものと異なって直線性が優れ、III謙電流測定が
可能である。いま上記重畳期間のJIIi*について磁
気囲路のヒステyyスに一デを示す篇J図を参照し乍ら
詳瀘すると、従来方式のように一1交流#JllLえ懺
信号磁犀1.を印加すれば、JIll負Hjllの暮層
a1化―纏によって決定され11LKII化書れる。し
九がって初期磁化−纏の一直線性の影響を受けるし、儒
81111えは外S*算の大自書および値性方崗により
ては部層特性を有し、最悪の場合Kitg’慮tえは1
″慮に磁化されJhことがあって夏lN1kIE漉淵意
が不可能とをる。
The operating principle of this JIw method is as described in Zeng's records)) The alternating current magnetic field and IIIfJIIJIL are applied superimposed and 9 and 1 are obtained, so it is a magnetization mechanism). If there are enough stones to saturate the Jl air pressure, then the air flow will open and +V% will be completed.
11ll &< It was decided * written by the autograph of the signal magnetic field -
Laxsxpsa - Agricultural magnetization structure is used to grow one product. Shi-
Then, the total number of tafunde by this i & beak method is simply 1 ml of alternating current and the signal magnetic rise is printed after the round g! Unlike the conventional method, this method has excellent linearity and enables III-mode current measurement. Now, regarding JIIi* during the above-mentioned superimposition period, referring to Figure J showing the hysteresis of the magnetic enclosure in detail, as in the conventional system, the 11 AC #JllL signal magnetic signal 1. If you apply JIll negative Hjll, it is determined by the low layer a1 conversion to 11LKII conversion and is written. As a result, it is affected by the linearity of initial magnetization and magnetization, and Confucianism 81111 has partial layer characteristics depending on the Great Book of Gai S*kan and the value-related method, and in the worst case, Kitg' Consideration is 1
``There are times when I am magnetized by thought, and it is impossible to write a book in the summer.

−1このlI−の7mによれば1ljs閣におけJh虫
のよ51液瀞の碓犀が印m電れ為ため重畳層属TIの碓
化遥禍ではJIg7閣のにステIFスルー−1”Kh−
で、メジャールーfネらマイt−p−デを鋳て最終II
kKhJILK頃れん電れる。この時最終磁化点にはJ
Il気厘賂の有するにステ91スの抗碓カIcト麹徊i
t化慮ムの閾、即ち Ire < Hz 十1m e < IwmII:信号
磁界、Jar:交諌滅責磯鼻に&る時点で決定され、曹
肥従来方式と^を伽磯鬼禰賂の部層IIII性に友會畜
れ慶い直纏懺の優れえ114:がff!われで夏纏亀電
流#I電がで−る。資良藺遠しえ制御囲路(7)%をン
デμ・傘−I〜ド圃賂(2)は例えば積分履ノ1変換−
を利用して岡釣に濃ゎすこと−できる。*S***Sは
入力を一定時調積分し、ついで1準電圧をms分し、1
1分電圧が−電電MEK遍する逃の時間を表示すること
によ)アを買グ入カをダepp*表示に変換するもので
あ為から、入力II分時を本11w4によるタヲンデ計
鰺のサンプに時、jlち一重畳期閾に、逆積分時をホー
ルY時、即ち重畳JII属時#l:対応書せて動作させ
1ことKよ)電流の#II重*示を行をわ讐ることがで
自為、岡皺にして地被1[#)変換−を層いえ場合にも
応用でIIIhc七線lIらかであ為、叉この見―は上
記の細くイ買7ツツタス綾Ellるζトラく、例えばJ
IIIK示すように磁気鵬路會會め九罎還に−rを書し
謙−従来オ式のタフンデ計MK4適周することがで自る
-1 According to the 7m of this lI-, in the Jh insect in the 1ljs kaku, the Usui of the 51 liquid is electrified, so in the superimposed layer genus TI's Usuka Youkai, the JIg7 kaku's Niste IF through-1 “Kh-
So, I cast the major loop fnera my t-p-de and made the final II.
Around kKhJILK, you can hear the Renden. At this time, the final magnetization point is J
The resistance of the 91st step to the resistance of Il's bribe is I
It is determined at the time when the threshold of t conversion, i.e., Ire < Hz 11m e < Iwm II: signal magnetic field, Jar: intersection is determined, and the conventional method of Caofei and the part of the 114: is ff! We are the summer-wearing turtle current #I electrician. For example, convert the integral control fence (7)% into the integral μ・umbrella−I〜de field (2)−
You can use it to concentrate on Oka fishing. *S***S performs constant time-scale integration of the input, then divides 1 quasi-voltage into ms, and calculates 1
By displaying the escape time when the 1-minute voltage changes over -Denden MEK, it converts the input power into the Epp* display, so the input II minute time can be calculated according to Book 11w4. At the sample time of jl, which is the single-fold period threshold, write the inverse integration time at the Hall Y time, that is, when the superposition JII belongs to #l: and operate it. However, it is natural that it is natural, and the ground cover 1 [#) conversion is applied to the case where it is layered. For example, J
As shown in IIIK, it is possible to write -r in the 9th round of the magnetic road meeting and make the proper rotation of the conventional O-type tahunde meter MK4.

飄上詳謔したよ5にこのla*にシいてはタフング計響
は本質的Km鬼圃賂の部層神性の影響を責けない九め、
I!来綱難であつえ直流の徽少電流測*において夏確表
電流検出を■能とする著効を貴し、五つ重畳、非重畳の
周期を充分に鰹か<**すれば交流電流法要をもJL夷
に検崗真示することがで龜る。更KF−の弛−の方法は
人的操Iwに刺ることが1に−丸め、測定器取扱いに起
因す1瞑道中、長時間に亘る記録測定の場合の誤差も防
止できるものである。
Regarding this la*, which I have explained in detail in detail, the Tafunkyo is essentially not responsible for the influence of the sub-level divinity of the Km demons.
I! It is very effective to make summer accurate current detection ■ possible in direct current measurement*, and if five superimposed and non-superimposed periods are sufficiently repeated, then alternating current can be detected. It will be difficult to show the true nature of the memorial service to JL Yi. Furthermore, KF's relaxation method is able to reduce human manipulation and prevent errors in recording measurements over a long period of time during one meditation session due to handling of measuring instruments.

【図面の簡単な説明】[Brief explanation of the drawing]

第1図、第2図はクランプ計器における従来の摘磁方法
を示す説明図、第3図はこの発明の方法によるJll[
開路ll!施飼麿、菖ダ閤はこの俺−にシけム崗力滅I
EII  I11縄は磁気開路のにステ響vX4−デa
11.114關はこの慟買・方決によ為瀾定閾賂麹夷1
例閾で番る。 (支)・・・中−〜素子、(2)・・・磁気コア、(2
)。 ―・・・巻線、に)・・・被馬電電路、(転)・・・*
*増申働、(2)、d・・・3!!流滅責l&振器、(
7)。 (カ・・・制御囲路、■、Id・・・をン1声・*−ル
ドH路、 #)、 @f−−−表示器、iac −@ 
@交流減責電流法要、 is・・・被測寓電流法要、盃
・・・発生磁束液廖、%、屹・・・サンプ〜・ホールド
1回路幽力波廖 第1■   井20 パ
FIGS. 1 and 2 are explanatory diagrams showing the conventional magnetization method in a clamp instrument, and FIG.
Open circuit! Shigemaro, Ayuda Kyou is the one who will destroy the power of Shikem to me.
EII I11 rope is magnetically open circuit Stekyo vX4-a
11.114 As for this matter, the threshold for bribery is based on this decision.
Number by example threshold. (Support)... Middle ~ element, (2)... Magnetic core, (2
). ――・・・Winding, ni) ・・・Electric circuit, (transfer) *
* Increased work, (2), d...3! ! Flowing Responsibility & Shaker, (
7). (K... Control circuit, ■, Id... 1 voice, * - LED H path, #), @f --- Display, iac -@
@ AC reduced liability current memorial service, is... measurable current memorial service, cup... generated magnetic flux liquid, %, 屹... sump ~ hold 1 circuit force wave order 1 ■ I20 Pa

Claims (1)

【特許請求の範囲】[Claims] 1、開磁路中にホール素子を有するクランプ計器による
電流側定において、被測定電路から発生する信号磁犀に
*滝減責電流による交流111jFを蓋肩廟をもって闘
けつ的に磁路に重畳畜ぜ、非重畳11MIK麹生する上
記被測定篭絡電流に比例し友中ール素子出力電圧を測定
することを特徴とする電流測定法。
1. In current measurement using a clamp instrument with a Hall element in the open magnetic path, the signal magnetic field generated from the electrical circuit to be measured is overlaid with AC 111JF caused by a waterfall reduction current onto the magnetic path. Damn it, a current measuring method characterized by measuring the output voltage of a loop element in proportion to the above-mentioned non-superimposed 11 MIK current to be measured.
JP56131825A 1981-08-21 1981-08-21 Current measurement Granted JPS5833167A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP56131825A JPS5833167A (en) 1981-08-21 1981-08-21 Current measurement

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP56131825A JPS5833167A (en) 1981-08-21 1981-08-21 Current measurement

Publications (2)

Publication Number Publication Date
JPS5833167A true JPS5833167A (en) 1983-02-26
JPS6411149B2 JPS6411149B2 (en) 1989-02-23

Family

ID=15066976

Family Applications (1)

Application Number Title Priority Date Filing Date
JP56131825A Granted JPS5833167A (en) 1981-08-21 1981-08-21 Current measurement

Country Status (1)

Country Link
JP (1) JPS5833167A (en)

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
FR2643460A1 (en) * 1989-02-18 1990-08-24 Diehl Gmbh & Co NON-CONTACT MEASUREMENT OF A DIRECT CURRENT
FR2645650A1 (en) * 1989-04-06 1990-10-12 Merlin Gerin SYSTEM FOR CONTROLLING THE ISOLATION OF A DIRECT CURRENT NETWORK
JPH05254816A (en) * 1991-11-21 1993-10-05 Pechiney Rech Group Interet Economique Regie Par Ordonnance Du 23 Septembre 1967 Preparation of metal carbide having large specific surface from activated carbon foam
DE10204425B4 (en) * 2002-02-04 2010-12-09 Vacuumschmelze Gmbh & Co. Kg Current sensor according to the compensation principle

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
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FR2645650A1 (en) * 1989-04-06 1990-10-12 Merlin Gerin SYSTEM FOR CONTROLLING THE ISOLATION OF A DIRECT CURRENT NETWORK
JPH05254816A (en) * 1991-11-21 1993-10-05 Pechiney Rech Group Interet Economique Regie Par Ordonnance Du 23 Septembre 1967 Preparation of metal carbide having large specific surface from activated carbon foam
DE10204425B4 (en) * 2002-02-04 2010-12-09 Vacuumschmelze Gmbh & Co. Kg Current sensor according to the compensation principle

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