JPH0452415B2 - - Google Patents
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- Publication number
- JPH0452415B2 JPH0452415B2 JP18286783A JP18286783A JPH0452415B2 JP H0452415 B2 JPH0452415 B2 JP H0452415B2 JP 18286783 A JP18286783 A JP 18286783A JP 18286783 A JP18286783 A JP 18286783A JP H0452415 B2 JPH0452415 B2 JP H0452415B2
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- Prior art keywords
- magnetic field
- field detection
- temperature
- magnetic
- detection
- Prior art date
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Description
技術分野
本発明は、ホール素子などの磁界検出素子を用
いた磁束計の較正方法に関し、特に、検出素子あ
るいは検出回路に発生する温度変化などの環境変
化に起因して生ずるオフセツト電圧や検出素子の
感度の変化に応じて、磁界検出値を自動的に較正
し得るようにしたものである。
従来技術
この種磁界検出素子、例えばホール素子を用い
た従来の磁束計においては、ホール素子駆動部に
温度補償を施し、あるいは、磁界シールドを施し
た筐体に磁界検出用プローブを挿入した状態にて
磁界検出のオフセツト値を測定するなどして、磁
界検出値の較正を行なつていた。また、磁界計測
値とその計測時における環境温度とから、温度変
化に対する磁界計測値の較正曲線を使用して、被
測定磁界の正確な磁束値を求めていたが、測定環
境の温度と磁界検出用プローブ自体の温度が異な
ることに起因する測定誤差を取除き得ないなど、
従来のこの種磁束計の較正方法には充分正確に較
正を行ない得ない欠点があつた。
さらに、ホール素子を用いた磁束計において
は、一般に、0.5ガウス/℃程度の温度変化に基
づく磁界検出オフセツト値の変動があるので、特
に、1ガウス以下の弱磁界の検出に当つては、数
℃の温度変化が磁界計測値に大きく影響する。し
たがつて、ホール素子を用いた従来の磁束計は、
弱磁界強度の計測には適さないなどの問題があ
り、さらに、磁界検出のオフセツトを自動的には
補正し得ないがために、自動制御などに磁界セン
サとして使用するについては制限がある、という
欠点もあつた。
発明の要点
本発明の目的は、上述した従来の問題を解決し
てその欠点を除去し、ホール素子などを使用する
磁界検出素子の温度変化に起因する磁界検出感度
の変動を自動的に補正して、正確な磁界計測値を
求め得るようにした、磁界検出素子を用いた磁束
計の較正方法を提供することにある。
すなわち、本発明較正方法は、互いに直交する
3方向の磁界をそれぞれ検出する3個の磁界検出
素子を組合わせ配置してなる磁束計において、前
記3個の磁界検出素子の各磁界検出出力X,Y,
Z、各磁界検出感度Rx,Ry,Rzおよび各磁界検
出オフセツトa,b,cと被検出磁界における磁
界の強さの真の値Mとの間に成立つ
(X−a/Rx)2+(Y−b/Ry)2+(Z−c/Rz)
2=M2
なる関係式に、前記磁束計を少なくとも6方向に
向けて前記3個の磁界検出素子により前記磁界の
強さの真の値Mが既知の磁界をそれぞれ検出した
ときの前記各磁界検出出力X,Y,Zの値と前記
既知の磁界の強さの真の値Mとを代入して得られ
る少なくとも6組の連立方程式から、前記各磁界
検出感度Rx,Ry,Rzおよび前記各磁界検出オフ
セツトa,b,cの値をそれぞれ算出することに
よつて前記磁束計を較正し、前記3個の磁界検出
素子により任意の方向の被検出磁界を検出して前
記各磁界検出出力X,Y,Zの値を求めたときに
当該任意の方向の被検出磁界における前記磁界の
強さの真の値Mを前記関係式から算出し得るよう
にしたことを特徴とするものである。
実施例
以下に図面を参照して実施例につき本発明を詳
細に説明する。
まず、本発明方法によつて磁束計の較正を行な
う装置の構成例を第1図に示す。図示の構成にお
いては、点線により囲んで示す磁界測定用プロー
ブ4に3個の磁界検出素子、例えば、ホール素子
5,6,7を内蔵しており、それら3個の磁界検
出素子5,6,7は同一平面上にない3方向、例
えば互いに直交する3方向x,y,zの磁界をそ
れぞれ検出し得るように組合わせて配置してあ
る。また、それらの磁界検出素子5,6,7は3
個の駆動回路1,2,3によりそれぞれ駆動して
作動させる。例えば磁界検出素子をホール素子と
した場合には、それらの素子の各制御端子に定電
流乃至定電圧を供給する。各磁界検出出力電圧
は、3個の直流増幅回路8,9,10をそれぞれ
介して、点線により囲んで示した、例えばマイク
ロコンピユータにより構成する演算処理部11に
供給する。その演算処理部11においては、入力
端子#1,#2,#3にそれぞれ供給した各方向
x,y,zの磁界検出出力電圧をマルチプレクサ
12により順次に切換えてアナログ−デイジタル
変換器13に導き、デイジタルデータの形態にし
て演算器14に供給する。その演算器14におい
ては、リードオンリメモリ16に予め記憶させて
ある本発明較正方法のプログラムに従い、また、
ランダムアクセスメモリ17を演算過程に用い
て、後述するような演算を入力データに施し、磁
界検出出力中に含まれているオフセツト分を除去
したうえで、被測定磁界の方向、強度などを表わ
す出力データをインターフエース15を介して取
出す。なお、図示の装置を磁束計として用いる場
合には、出力データを適切に構成した表示部(図
示せず)に供給して表示するものとする。
しかして、上述の装置を磁束計として用いた場
合に測定データに含まれるオフセツトの発生要因
の一つとなる磁界検出素子の温度情報を直接に得
るためには、第2図に示すようにその構成を変更
する。すなわち、上述したと同様に駆動回路18
により駆動した磁界検出素子19の磁界検出出力
を増幅回路20を介して演算処理部21に供給す
るとともに、磁界検出素子19の入力端子間に現
われる内部抵抗値をも演算処理部21に供給し、
使用する磁界検出素子について予め測定して記憶
させておいた内部抵抗−温度特性曲線に基づいて
その磁界検出素子の温度を求め、その温度におい
て生ずる測定データのオフセツト値を算出する。
例えば、磁界検出素子19としてホール素子を用
い、駆動回路18により定電圧駆動したときに
は、その定電圧値とともにホール素子19の入力
端子間に現われる電流値を演算処理部21に供給
し、また、駆動回路19により定電流駆動したと
きには、その定電流値とともにホール素子19の
入力端子間に現われる電圧値を演算処理部21に
供給し、かかる入力電圧・電流値から求まる素子
内部抵抗値を、素子温度につか予め測定して記憶
させておいた較正値と比較して素子温度を求め
る。
つぎに、第1図示の回路装置を磁束計として用
いたときに、温度など測定環境の変化に起因して
生ずるオフセツトや検出感度の変化分を求めて検
出出力値を自動的に較正するようにした本発明の
磁束計較正方法について説明する。
いま、磁界検出素子、例えば、ホール素子5,
6,7を、それぞれの磁界検出方向が互いに直交
するように配置した場合に、磁界検出素子5,
6,7の磁界検出感度や入力出力抵抗のばらつ
き、増幅回路8,9,10の増幅度やオフセツト
の相違により、磁界検出の感度およびオフセツト
値は磁界のx,y,z各方向によつてそれぞれ異
なつている。いま、x,y,z各方向における磁
界の真の強度をそれぞれMx,My,Mzとすれば、
上述した増幅出力値X,Y,Zはそれぞれつぎの
式によつて表わされる。
X=Rx・Mx+a
Y=Ry・My+b
Z=Rz・Mz+c (1)
ここに、Rx,Ry,Rzはそれぞれx,y,z各
方向における磁界検出系の検出感度であり、ま
た、a,b,cはそれぞれそれら各系のオフセツ
ト値であつて、いずれも温度の関数となる。な
お、物理的には磁界検出感度Rx,Ry,Rzはホー
ル定数に対応し、また、増幅出力X,Y,Zはホ
ール起電力に対応する。
そこで、まず、かかる構成の磁束計により磁界
強度の真の値が既知の基準均一磁界、例えば地磁
気を検出する。その均一磁界の強度をMとする
と、x,y,z各方向は互いに直交しているので
あるから、
Mx 2+My 2+Mz 2=M2 (2)
なる関係式(2)が成立つ。ついで、(1)式をこの(2)式
に代入すると、つぎの(3)式が得られる。
(X−a/Rx)2+(Y−b/Ry)2+(Z−c/Rz)
2=M2(3)
しかして、基準均一磁界の磁界強度Mは一定で
あるから、(3)式の右辺M2は一定であり、磁界検
出方向を互いに直交させて組合わせ配置した3系
統の磁界検出素子5,6,7を種々の方向に向け
たときの各磁界検出値X,Y,Zは、第3図に示
すように、各オフセツト値a,b,cによつて与
えられる点P(a,b,c)を中心とする球面上
にあり、つねに(3)式の関係を満している。この(3)
式は6個の変数a,b,c,Rx,Ry,Rzを含ん
でいるのであるから、磁界検出素子5,6,7の
磁界検出方向を6とおり変化させたときの各磁界
検出値X,Y,Zをそれぞれ求めることにより、
6個の連立方程式が得られ、各オフセツト値a,
b,cおよび各磁界検出感度Rx,Ry,Rzを正確
に算出することができる。なお、磁界測定プロー
ブの方向、したがつて、各磁界検出素子5,6,
7の方向を6とおりに固定した状態で繰返し測定
したときの磁界検出値X,Y,Zが、温度の変化
などにより、測定の都度異なる場合には、磁界検
出素子5,6,7の方向を7とおり以上変化させ
て磁界検出値をそれぞれ求め、最小自乗法などを
用いて6個の変数a,b,c,Rx,Ry,Rzを算
出する。
つぎに、上述したように6方向につき測定した
磁界検出値の更正方法について説明する。
いま、行列Γをつぎのように定義する。
Γ=X2 1Y2 1Z2 1X1Y1Z11
X2 2Y2 2Z2 2X2Y2Z21
…
…
X2 6Y2 6Z2 6X6Y6Z61 (4)
ここに、Xk,Yk,Zk(k=1,2,…,6)は
6方向についての測定値である。
いま、6行7列からなるΓの行列式(4)につい
て、例えば、第1列(X2 1,X2 2,…,X2 6)を除い
た残余の6行6列の行列式をΓX2と表わし、第2
列(Y2 1,Y2 2,…,Y2 6)を除いた残余の行列式を
ΓY2と表わし、以下同様にして、第6列(Z1,
Z2,…,Z6)を除いた残余の行列式をΓZと表わ
すと、前述した関係式(3)の各変数a,b,c,
Rx,Ry,Rzはつぎの(5)式となる。
TECHNICAL FIELD The present invention relates to a method for calibrating a magnetometer using a magnetic field detection element such as a Hall element, and in particular to a method for calibrating a magnetometer using a magnetic field detection element such as a Hall element. The magnetic field detection value can be automatically calibrated according to changes in sensitivity. Prior Art In a conventional magnetometer using this type of magnetic field detection element, for example, a Hall element, the Hall element driving section is temperature-compensated, or the magnetic field detection probe is inserted into a magnetic field shielded casing. The magnetic field detection value was calibrated by measuring the offset value of the magnetic field detection. In addition, from the magnetic field measurement value and the environmental temperature at the time of measurement, a calibration curve of the magnetic field measurement value against temperature change was used to determine the accurate magnetic flux value of the measured magnetic field, but the temperature of the measurement environment and the magnetic field detection For example, it is impossible to eliminate measurement errors due to differences in the temperature of the probe itself.
The conventional method of calibrating this type of magnetometer has the disadvantage that it cannot be calibrated with sufficient accuracy. Furthermore, in a magnetometer using a Hall element, the magnetic field detection offset value generally fluctuates based on temperature changes of about 0.5 Gauss/°C, so in particular when detecting weak magnetic fields of 1 Gauss or less, Temperature changes in degrees Celsius greatly affect magnetic field measurements. Therefore, the conventional magnetometer using a Hall element is
It has problems such as being unsuitable for measuring weak magnetic field strength, and furthermore, it cannot automatically correct the offset of magnetic field detection, which limits its use as a magnetic field sensor for automatic control. There were also drawbacks. Summary of the Invention It is an object of the present invention to solve the above-mentioned conventional problems and eliminate their drawbacks, and to automatically correct fluctuations in magnetic field detection sensitivity caused by temperature changes of magnetic field detection elements using Hall elements etc. Therefore, it is an object of the present invention to provide a method for calibrating a magnetometer using a magnetic field detection element, which makes it possible to obtain accurate magnetic field measurement values. That is, in the calibration method of the present invention, in a magnetometer in which three magnetic field detecting elements each detecting magnetic fields in three directions orthogonal to each other are arranged in combination, each magnetic field detection output X, Y,
Z, each magnetic field detection sensitivity R x , R y , R z and each magnetic field detection offset a, b, c, and the true value M of the magnetic field strength in the detected magnetic field (X-a/R x ) 2 + (Y-b/R y ) 2 + (Z-c/R z )
2 = M 2 , each of the magnetic fields when the magnetic flux meter is directed in at least six directions and the three magnetic field detection elements detect each magnetic field for which the true value M of the strength of the magnetic field is known. From at least six sets of simultaneous equations obtained by substituting the values of the detection outputs X, Y, and Z and the true value M of the known magnetic field strength, each of the magnetic field detection sensitivities R x , R y , R z The magnetometer is calibrated by calculating the values of each of the magnetic field detection offsets a, b, and c, and the magnetic field to be detected in any direction is detected by the three magnetic field detection elements, and each of the magnetic fields is When the values of the detection outputs X, Y, and Z are obtained, the true value M of the strength of the magnetic field in the detected magnetic field in any direction can be calculated from the relational expression. It is. EXAMPLES The present invention will be explained in detail below using examples with reference to the drawings. First, FIG. 1 shows an example of the configuration of an apparatus for calibrating a magnetometer according to the method of the present invention. In the illustrated configuration, a magnetic field measuring probe 4 shown surrounded by a dotted line includes three magnetic field detecting elements, for example, Hall elements 5, 6, and 7, and these three magnetic field detecting elements 5, 6, 7 are arranged in combination so as to be able to detect magnetic fields in three directions that are not on the same plane, for example, three mutually orthogonal directions x, y, and z. Moreover, those magnetic field detection elements 5, 6, 7 are 3
They are driven and operated by respective drive circuits 1, 2, and 3. For example, when the magnetic field detection element is a Hall element, a constant current or a constant voltage is supplied to each control terminal of these elements. Each magnetic field detection output voltage is supplied via three DC amplifier circuits 8, 9, and 10 to an arithmetic processing unit 11, which is indicated by a dotted line and constituted by, for example, a microcomputer. In the arithmetic processing unit 11, the magnetic field detection output voltages in each direction x, y, and z supplied to input terminals #1, #2, and #3 are sequentially switched by a multiplexer 12 and guided to an analog-digital converter 13. , and supplies it to the arithmetic unit 14 in the form of digital data. In the arithmetic unit 14, according to the program of the calibration method of the present invention stored in advance in the read-only memory 16, and
The random access memory 17 is used in the calculation process to perform calculations as will be described later on the input data, remove the offset included in the magnetic field detection output, and then generate an output that represents the direction, strength, etc. of the magnetic field to be measured. Data is retrieved via interface 15. Note that when the illustrated device is used as a magnetometer, output data is supplied to and displayed on an appropriately configured display section (not shown). However, in order to directly obtain temperature information of the magnetic field detection element, which is one of the causes of offset included in measurement data when the above-mentioned device is used as a magnetometer, the configuration shown in Figure 2 is required. change. That is, as described above, the drive circuit 18
The magnetic field detection output of the magnetic field detection element 19 driven by is supplied to the arithmetic processing unit 21 via the amplifier circuit 20, and the internal resistance value appearing between the input terminals of the magnetic field detection element 19 is also supplied to the arithmetic processing unit 21,
The temperature of the magnetic field detecting element to be used is determined based on an internal resistance-temperature characteristic curve that has been previously measured and stored, and the offset value of the measurement data generated at that temperature is calculated.
For example, when a Hall element is used as the magnetic field detection element 19 and driven at a constant voltage by the drive circuit 18, the constant voltage value and the current value appearing between the input terminals of the Hall element 19 are supplied to the arithmetic processing unit 21, and the driving When constant current is driven by the circuit 19, the constant current value and the voltage value appearing between the input terminals of the Hall element 19 are supplied to the arithmetic processing section 21, and the element internal resistance value determined from the input voltage and current value is calculated based on the element temperature. The element temperature is determined by comparing it with a calibration value that has been measured and stored in advance. Next, when the circuit device shown in Figure 1 is used as a magnetometer, the detection output value is automatically calibrated by determining offsets and changes in detection sensitivity caused by changes in the measurement environment such as temperature. The magnetometer calibration method of the present invention will be explained. Now, a magnetic field detection element, for example, a Hall element 5,
6 and 7 are arranged so that their respective magnetic field detection directions are orthogonal to each other, the magnetic field detection elements 5,
Due to variations in the magnetic field detection sensitivity and input/output resistance of 6 and 7, and differences in the amplification degree and offset of the amplifier circuits 8, 9, and 10, the magnetic field detection sensitivity and offset value vary depending on the x, y, and z directions of the magnetic field. Each one is different. Now, if the true strength of the magnetic field in each of the x, y, and z directions is M x , M y , and M z , then
The amplified output values X, Y, and Z mentioned above are each expressed by the following equations. X=R x・M x +a Y=R y・M y +b Z=R z・M z +c (1) Here, R x , R y , and R z are magnetic field detection in each direction of x, y, and z, respectively. It is the detection sensitivity of the system, and a, b, and c are the offset values of each of these systems, all of which are functions of temperature. Note that, physically, the magnetic field detection sensitivities R x , R y , and R z correspond to Hall constants, and the amplified outputs X, Y, and Z correspond to Hall electromotive force. Therefore, first, a reference uniform magnetic field whose true value of magnetic field strength is known, such as earth's magnetism, is detected using a magnetometer having such a configuration. If the strength of the uniform magnetic field is M, the x, y, and z directions are perpendicular to each other, so the relational expression (2) holds: M x 2 + M y 2 + M z 2 = M 2 (2) Two. Then, by substituting equation (1) into equation (2), the following equation (3) is obtained. (X-a/R x ) 2 + (Y-b/R y ) 2 + (Z-c/R z )
2 = M 2 (3) Therefore, since the magnetic field strength M of the reference uniform magnetic field is constant, the right-hand side M 2 of equation (3) is constant, and the three systems are arranged in combination with the magnetic field detection directions orthogonal to each other. The magnetic field detection values X, Y, and Z when the magnetic field detection elements 5, 6, and 7 are oriented in various directions are given by the offset values a, b, and c, as shown in It is on a spherical surface centered on point P (a, b, c), and always satisfies the relationship of equation (3). This (3)
Since the formula includes six variables a, b, c, R x , R y , R z , each magnetic field when the magnetic field detection directions of the magnetic field detection elements 5, 6, and 7 are changed in six ways. By obtaining the detected values X, Y, and Z, respectively,
Six simultaneous equations are obtained, and each offset value a,
b, c and each magnetic field detection sensitivity R x , R y , R z can be calculated accurately. Note that the direction of the magnetic field measurement probe, and therefore each magnetic field detection element 5, 6,
If the magnetic field detection values X, Y, Z when repeatedly measured with the directions of the magnetic field detection elements 5, 6, and 7 fixed in six different ways differ each time due to changes in temperature, etc., the directions of the magnetic field detection elements 5, 6, and 7 are changed in seven or more ways to obtain the respective detected magnetic field values, and six variables a, b, c, R x , R y , and R z are calculated using the least squares method or the like. Next, a method of correcting the detected magnetic field values measured in six directions as described above will be explained. Now, define the matrix Γ as follows. Γ=X 2 1 Y 2 1 Z 2 1 X 1 Y 1 Z 1 1 X 2 2 Y 2 2 Z 2 2 X 2 Y 2 Z 2 1 … … X 2 6 Y 2 6 Z 2 6 6 1 (4) Here, X k , Y k , Z k (k=1, 2,..., 6) are measured values in six directions. Now, regarding the determinant (4) of Γ consisting of 6 rows and 7 columns, for example, the determinant of the remaining 6 rows and 6 columns after removing the first column (X 2 1 , X 2 2 , ..., X 2 6 ) is Expressed as ΓX 2 , the second
The remaining determinant after removing the columns (Y 2 1 , Y 2 2 , ..., Y 2 6 ) is expressed as ΓY 2 , and in the same manner, the 6th column (Z 1 ,
When the residual determinant after removing Z 2 ,..., Z 6 ) is expressed as ΓZ, each variable a, b, c,
R x , R y , and R z are expressed by the following equation (5).
【式】
この(5)式に基づいて各変数を算出する演算のプ
ログラムを演算処理部11内のリードオンメモリ
16に記憶させておき、較正用ボタンスイツチを
押下して演算処理部11にそのプログラムに従つ
た演算を実行させる。すなわち、各磁界検出素子
5,6,7を組合わせた磁界測定用プローブ4を
前述した6方向に順次に向けて得た測定データを
演算処理部11内のアナログ・デイジタル変換器
13によりデイジタル化したうえでランダムアク
セスメモリ17に順次に蓄えておき、演算処理に
必要な測定点数に達したときに読出して、リード
オンリメモリ16から読出したフログラムに従
い、演算器14にて自動的に較正用演算処理を行
ない、得られた各変数a,b,c,Rx,Ry,Rz
の値を再びランダムアクセスメモリ17に記憶さ
せておく。
通常の磁界測定時には、(5)式の演算処理を施し
た磁界測定真値をインターフエース15を介して
取出すようにする。
しかして、前述したようにして求めた各変数、
すなわち、各系のオフセツト値a,b,cおよび
検出感度Rx,Ry,Rzと測定環境温度との関係を
求めるには、磁界測定と同時に環境温度も測定す
る。この温度の測定は、
(1) ホール素子等の磁界検出素子の温度を直接に
測定し、あるいは、
(2) 第2図について説明したように、ホール素子
の入力端子間に印加する電圧と入力端子間に流
れる電流との値、もしくは、入力端子間に流す
電流と入力端子間に現われる電圧との値を検出
し、それらの電流電圧より求めた内部抵抗値の
温度による変化を予め較正しておくことによつ
て行なうことができる。
つぎに、上述した(2)項の方法、すなわち、磁界
検出素子温度の間接側定について詳細に説明す
る。
まず、磁界検出素子、例えば、ホール素子の入
力等価回路を第4図に示す。磁界検出のオフセツ
トは、ホール素子の入力端子間電流電圧から求ま
る内部抵抗値の温度による変化によつて発生す
る。また、磁界検出感度の変化はホール素子の素
子定数が変化することによつても生ずる。すなわ
ち、ホール素子の駆動端子、すなわち、素子駆動
電圧もしくは電流を供給する入力端子には、定電
圧もしくは定電流を供給して素子を駆動するが、
その入力抵抗が変化すると、入力端子間に流れる
電流もしくは入力端子間に現われる電圧が変化す
るので、入力電圧・電流値を測定することによつ
て素子の状態を知ることができる。かかる素子状
態の検出はホール素子自体を温度センサとして用
いるのに等しく、温度のみを計測する通常の温度
センサより正確に素子の状態を検出することがで
きる。
また、オフセツト電圧値および検出感度の温度
特性曲線を求めるには、所望の温度範囲内におい
て例えば5℃刻みにて温度を上昇させ、それらの
各温度におけるオフセツト電圧値および検出感度
を前述したようにして求め、プロツトして中間温
度点を線形補間するのが好適である。
上述のようにしてホール素子の温度など素子の
状態をホール素子自体から検出することにより、
ホール素子のオフセツト値対温度特性および検出
感度対温度特性を自動的に求めることが可能とな
る。
効 果
以上の説明から明らかなように、本発明によれ
ば、磁界検出素子、例えば、ホール素子の温度に
よつて変化するオフセツト値や検出感度を計算に
よつて自動的に較正して微弱な強度の磁界につい
ても、その磁界の強度の真の値を容易かつ正確に
求めることができる、という格別の効果が得られ
る。[Formula] A calculation program for calculating each variable based on this formula (5) is stored in the read-on memory 16 in the calculation processing unit 11, and the calibration button switch is pressed to send the calculation program to the calculation processing unit 11. Execute calculations according to the program. That is, the measurement data obtained by sequentially pointing the magnetic field measurement probe 4, which is a combination of magnetic field detection elements 5, 6, and 7 in the six directions mentioned above, is digitized by the analog-to-digital converter 13 in the arithmetic processing section 11. Then, it is sequentially stored in the random access memory 17, read out when the number of measurement points required for calculation processing is reached, and the calculation unit 14 automatically performs the calibration calculation according to the program read out from the read-only memory 16. The obtained variables a, b, c, R x , R y , R z
The value of is stored in the random access memory 17 again. During normal magnetic field measurement, the true value of the magnetic field measurement, which has been subjected to the arithmetic processing of equation (5), is taken out via the interface 15. Therefore, each variable obtained as described above,
That is, in order to determine the relationship between the offset values a, b, c and detection sensitivities R x , R y , R z of each system and the measured environmental temperature, the environmental temperature is also measured at the same time as the magnetic field measurement. This temperature can be measured by (1) directly measuring the temperature of a magnetic field detection element such as a Hall element, or (2) as explained in Figure 2, by applying a voltage between the input terminals of the Hall element and input voltage. Detect the value of the current flowing between the terminals or the value of the current flowing between the input terminals and the voltage appearing between the input terminals, and calibrate in advance the change in internal resistance value determined from these currents and voltages due to temperature. This can be done by leaving it in place. Next, the method of the above-mentioned item (2), that is, the indirect determination of the magnetic field detection element temperature will be explained in detail. First, FIG. 4 shows an input equivalent circuit of a magnetic field detection element, such as a Hall element. An offset in magnetic field detection is caused by a change in internal resistance value determined from the current voltage between the input terminals of the Hall element due to temperature. Further, changes in magnetic field detection sensitivity also occur due to changes in the element constant of the Hall element. That is, a constant voltage or constant current is supplied to the drive terminal of the Hall element, that is, the input terminal that supplies the element drive voltage or current, to drive the element.
When the input resistance changes, the current flowing between the input terminals or the voltage appearing between the input terminals changes, so the state of the element can be known by measuring the input voltage and current values. Detecting the state of the element in this manner is equivalent to using the Hall element itself as a temperature sensor, and the state of the element can be detected more accurately than a normal temperature sensor that measures only temperature. In addition, to obtain the temperature characteristic curve of offset voltage value and detection sensitivity, increase the temperature in steps of, for example, 5°C within the desired temperature range, and calculate the offset voltage value and detection sensitivity at each temperature as described above. It is preferable to calculate the temperature, plot the temperature, and linearly interpolate the intermediate temperature points. By detecting the state of the Hall element, such as its temperature, from the Hall element itself as described above,
It becomes possible to automatically determine the offset value versus temperature characteristic and the detection sensitivity versus temperature characteristic of the Hall element. Effects As is clear from the above explanation, according to the present invention, the offset value and detection sensitivity, which change depending on the temperature of a magnetic field detection element, such as a Hall element, are automatically calibrated by calculation to detect weak signals. Even in the case of a strong magnetic field, a special effect can be obtained in that the true value of the strength of the magnetic field can be easily and accurately determined.
第1図は本発明較正方法に用いる磁界検出装置
の構成例を示すブロツク線図、第2図は同じくそ
の磁界検出装置の他の構成例を示すブロツク線
図、第3図は本発明方法による較正の原理を示す
線図、第4図はホール素子の等価回路を示す回路
図である。
1,2,3,18……駆動回路、4……磁界測
定プローブ、5,6,7,19……磁界検出素子
(ホール素子)、8,9,10,20……増幅回
路、11,21……演算処理部、12……マルチ
プレクサ、13……アナログ−デイジタル変換
器、14…演算器、15……インターフエース、
16……リードオンリメモリ、17……ランダム
アクセスメモリ。
FIG. 1 is a block diagram showing an example of the configuration of a magnetic field detection device used in the calibration method of the present invention, FIG. 2 is a block diagram showing another example of the configuration of the magnetic field detection device, and FIG. A diagram showing the principle of calibration, and FIG. 4 is a circuit diagram showing an equivalent circuit of a Hall element. 1, 2, 3, 18... Drive circuit, 4... Magnetic field measurement probe, 5, 6, 7, 19... Magnetic field detection element (Hall element), 8, 9, 10, 20... Amplification circuit, 11, 21... Arithmetic processing unit, 12... Multiplexer, 13... Analog-digital converter, 14... Arithmetic unit, 15... Interface,
16...Read-only memory, 17...Random access memory.
Claims (1)
する3個の磁界検出素子を組合わせ配置してなる
磁束計において、前記3個の磁界検出素子の各磁
界検出出力X,Y,Z、各磁界検出感度Rx,Ry,
Rzおよび各磁界検出オフセツトa,b,cと被
検出磁界における磁界の強さの真の値Mとの間に
成立つ (X−a/Rx)2+(Y−b/Ry)2+(Z−c/Rz)
2=M2 なる関係式に、前記磁束計を少なくとも6方向に
向けて前記3個の磁界検出素子により前記磁界の
強さの真の値Mが既知の磁界をそれぞれ検出した
ときの前記各磁界検出出力X,Y,Zの値と前記
既知の磁界の強さの真の値Mとを代入して得られ
る少なくとも6組の連立方程式から、前記各磁界
検出感度Rx,Ry,Rzおよび前記各磁界検出オ
フセツトa,b,cの値をそれぞれ算出すること
によつて前記磁束計を較正し、前記3個の磁界検
出素子により任意の方向の被検出磁界を検出して
前記各磁界検出出力X,Y,Zの値を求めたとき
に当該任意の方向の被検出磁界における前記磁界
の強さの真の値Mを前記関係式から算出し得るよ
うにしたことを特徴とする磁界検出素子を用いた
磁束計の較正方法。[Scope of Claims] 1. In a magnetometer configured by combining and arranging three magnetic field detection elements that respectively detect magnetic fields in three directions perpendicular to each other, each magnetic field detection output X, Y of the three magnetic field detection elements , Z, each magnetic field detection sensitivity R x , R y ,
(X-a/R x ) 2 + (Y-b/R y ) is established between R z and each magnetic field detection offset a, b, c and the true value M of the magnetic field strength in the detected magnetic field. 2 + (Z-c/ Rz )
2 = M 2 , each of the magnetic fields when the magnetic flux meter is directed in at least six directions and the three magnetic field detection elements detect each magnetic field for which the true value M of the strength of the magnetic field is known. From at least six sets of simultaneous equations obtained by substituting the values of the detection outputs X, Y, Z and the true value M of the known magnetic field strength, each of the magnetic field detection sensitivities R x , Ry, R z and The magnetic flux meter is calibrated by calculating the values of the magnetic field detection offsets a, b, and c, and the magnetic field to be detected in any direction is detected by the three magnetic field detection elements to detect each magnetic field. Magnetic field detection characterized in that when the values of the outputs X, Y, and Z are determined, the true value M of the strength of the magnetic field in the detected magnetic field in any direction can be calculated from the relational expression. Calibration method of magnetometer using element.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP18286783A JPS6073474A (en) | 1983-09-30 | 1983-09-30 | Calibrating method of fluxmeter using magnetic field detecting element |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP18286783A JPS6073474A (en) | 1983-09-30 | 1983-09-30 | Calibrating method of fluxmeter using magnetic field detecting element |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS6073474A JPS6073474A (en) | 1985-04-25 |
| JPH0452415B2 true JPH0452415B2 (en) | 1992-08-21 |
Family
ID=16125823
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP18286783A Granted JPS6073474A (en) | 1983-09-30 | 1983-09-30 | Calibrating method of fluxmeter using magnetic field detecting element |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS6073474A (en) |
Families Citing this family (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS6448685U (en) * | 1987-09-21 | 1989-03-27 | ||
| JPH01219683A (en) * | 1988-02-29 | 1989-09-01 | Shimadzu Corp | Squid magnetometer |
-
1983
- 1983-09-30 JP JP18286783A patent/JPS6073474A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS6073474A (en) | 1985-04-25 |
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