JPH1144538A - Method for detecting geomagnetism - Google Patents

Method for detecting geomagnetism

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Publication number
JPH1144538A
JPH1144538A JP21568197A JP21568197A JPH1144538A JP H1144538 A JPH1144538 A JP H1144538A JP 21568197 A JP21568197 A JP 21568197A JP 21568197 A JP21568197 A JP 21568197A JP H1144538 A JPH1144538 A JP H1144538A
Authority
JP
Japan
Prior art keywords
axis
magnetic field
sensor
sensor output
reference magnetic
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.)
Pending
Application number
JP21568197A
Other languages
Japanese (ja)
Inventor
Sadaaki Abe
定明 安部
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.)
Tokin Corp
Original Assignee
Tokin 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 Tokin Corp filed Critical Tokin Corp
Priority to JP21568197A priority Critical patent/JPH1144538A/en
Publication of JPH1144538A publication Critical patent/JPH1144538A/en
Pending legal-status Critical Current

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  • Measuring Magnetic Variables (AREA)
  • Geophysics And Detection Of Objects (AREA)

Abstract

PROBLEM TO BE SOLVED: To enable highly accurate azimuth detection by constituting matrix formulae of 3 rows × 3 columns using respective outputs of three axes obtained by a reference magnetic field generator with a specific magnetic field applied to each of the three axes and by solving the formulae to compensate a detected magnetic field of geomagnetism. SOLUTION: A magnetic field to be reference is applied to a moving body 13 by a reference magnetic field generator 14, and an output of a geomagnetism sensor 11 at that time is obtained. First, a magnetic field with an X-axis = Xc, Y-axis = 0 and Z-axis = 0, which is to be a reference magnetic field, is applied to the reference magnetic field generator 14, for obtaining outputs x=xs 1, y=ys 1 and z=zs 1 (condition 1) of three axes of the sensor 11. Then a magnetic field with the X-axis = 0, Y-axis = Yc and Z-axis = 0 is applied to obtain outputs x = xs 2, y=ys 2 and z=zs 2 (condition 2) of the three axes. Similarly, a magnetic field with the X-axis = 0, Y-axis = 0 and Z-axis = Zc is applied to obtain outputs x=x3 , y =ys 3 and z=zS3 (condition 3) of the three axes. The conditions 1, 2, 3 are used to constitute matrix formulae of 3 rows × 3 columns, the formulae are solved to obtain compensation coefficients A to I, and the coefficients are used to compensate a detected magnetic field of geomagnetism.

Description

【発明の詳細な説明】DETAILED DESCRIPTION OF THE INVENTION

【0001】[0001]

【発明の属する技術分野】本発明は、地磁気の検出方
法、特に、移動体の方位を検出する方法に関し、磁気セ
ンサの検出値(出力値)を補正する方法に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a method for detecting terrestrial magnetism, and more particularly to a method for detecting the orientation of a moving object, and more particularly to a method for correcting a detection value (output value) of a magnetic sensor.

【0002】[0002]

【従来の技術】従来の地磁気の検出方法における補正方
法としては、移動体を一周もしくはそれ以上旋回させて
移動体固有の磁気量を検知する方法が知られている。
2. Description of the Related Art As a correction method in a conventional method for detecting geomagnetism, there is known a method in which a moving body is turned one or more times to detect a magnetic amount unique to the moving body.

【0003】[0003]

【発明が解決しようとする課題】従来技術は、移動体を
一周旋回させることによって得られたデータより補正を
行うため、旋回場所が一様な磁場空間で無い場合には、
誤った補正を行ってしまい、正しい方位を検出できない
という問題があった。
In the prior art, the correction is performed based on data obtained by rotating the moving body one round. Therefore, when the turning place is not a uniform magnetic field space,
There was a problem that an incorrect correction was performed and a correct orientation could not be detected.

【0004】そこで、本発明の課題は、高精度な補正を
行って、正しい方位を与える地磁気の検出方法を提供す
ることである。
[0004] Therefore, an object of the present invention is to provide a method of detecting terrestrial magnetism that gives a correct orientation by performing highly accurate correction.

【0005】[0005]

【課題を解決するための手段】本発明は、移動体に装着
される地磁気成分を互いに直交する3軸成分(x,y,
z)に分けて検出し、これら3成分に対応した地磁気信
号を出力する地磁気センサと、地磁気信号に基づき移動
体の方位信号を出力する方位演算部と、移動体に3軸
(X,Y,Z)の基準磁界を与える基準磁界発生装置
と、を用いる地磁気検出の方法であって、基準磁界発生
装置によりX軸にXc,Y軸に0,Z軸に0なる磁界を
与えて得られる、x軸のセンサ出力xs1,y軸のセンサ
出力ys1,z軸のセンサ出力zs1と、基準磁界発生装置
によりX軸に0,Y軸にYc,Z軸に0なる磁界を与え
て得られる、x軸のセンサ出力xs2,y軸のセンサ出力
ys2,z軸のセンサ出力zs2と,基準磁界発生装置によ
りX軸に0,Y軸に0,Z軸にZcなる磁界を与えて得
られる、x軸のセンサ出力xs3,y軸のセンサ出力ys
3,z軸のセンサ出力zs3と、を用いて3行3列の行列
式を構成し、前記行列式を解いて、地磁気の検出磁界を
補正する地磁気の検出方法である。
SUMMARY OF THE INVENTION According to the present invention, a geomagnetic component mounted on a moving body is converted into three axial components (x, y,
z), a geomagnetic sensor that outputs geomagnetic signals corresponding to these three components, an azimuth calculation unit that outputs an azimuth signal of the mobile object based on the geomagnetic signal, and three axes (X, Y, Z) a reference magnetic field generator for providing a reference magnetic field, which is obtained by applying a magnetic field of Xc to the X axis, 0 to the Y axis, and 0 to the Z axis by the reference magnetic field generator. The x-axis sensor output xs1, the y-axis sensor output ys1, the z-axis sensor output zs1, and the reference magnetic field generator are used to apply a magnetic field of 0 to the X-axis, Yc to the Y-axis, and 0 to the Z-axis. Axis sensor output xs2, y-axis sensor output ys2, z-axis sensor output zs2, and x-axis obtained by applying a magnetic field of 0 to the X-axis, 0 to the Y-axis, and Zc to the Z-axis by the reference magnetic field generator. Sensor output xs3, y-axis sensor output ys
This is a terrestrial magnetism detection method in which a determinant of 3 rows and 3 columns is constructed using the sensor outputs zs3 of the 3 and z axes, and the determinant is solved to correct the terrestrial magnetism detection magnetic field.

【0006】本発明の検出(補正)方法は、均一度の高
い磁界を発生し得る基準磁界発生装置を用い、一様な基
準磁界中において補正が行われるので、移動体の持つ固
有磁気量が変わらない限り、有効な補正係数が一回の補
正で、高精度に算出できる。
The detection (correction) method of the present invention uses a reference magnetic field generator capable of generating a magnetic field with a high degree of uniformity and performs correction in a uniform reference magnetic field. As long as it does not change, the effective correction coefficient can be calculated with high accuracy by one correction.

【0007】[0007]

【発明の実施の形態】以下、本発明の実施の形態を図面
に基づき説明する
Embodiments of the present invention will be described below with reference to the drawings.

【0008】図1に、本発明による補正方法の全体概念
図を示す。図1に示すように、地磁気を三軸直交成分に
分けて検出する地磁気センサ11と、地磁気センサ11
の検出信号に基づき方位を演算し出力する方位演算部1
2とを組み込んだ移動体13を、基準磁界発生装置14
内に設置する。
FIG. 1 shows an overall conceptual diagram of a correction method according to the present invention. As shown in FIG. 1, a geomagnetic sensor 11 for detecting geomagnetism by dividing it into three-axis orthogonal components,
Azimuth calculation unit 1 that calculates and outputs the azimuth based on the detection signal of
2 is mounted on a reference magnetic field generator 14.
Install inside.

【0009】図2は、本発明に用いる地磁気センサの構
造を示し、21はx軸検出用磁気センサ、22はy軸検
出用磁気センサ、23はz軸検出用磁気センサを示し、
互いに直交するよう配置される。個々のセンサ21,2
2,23は、地磁気を三軸直交成分に分けて検出する。
FIG. 2 shows the structure of a geomagnetic sensor used in the present invention. Reference numeral 21 denotes a magnetic sensor for detecting an x-axis, 22 denotes a magnetic sensor for detecting a y-axis, and 23 denotes a magnetic sensor for detecting a z-axis.
They are arranged to be orthogonal to each other. Individual sensors 21, 22
2, 23 detect the geomagnetism by dividing it into triaxial orthogonal components.

【0010】図3は、基準磁界発生装置を示し、基準磁
界発生装置は、X軸基準磁界発生用ヘルムホルツコイル
41、Y軸基準磁界発生用ヘルムホルツコイル42、Z
軸基準磁界発生用ヘルムホルツコイル43と、定電流電
源44で構成される。この時、X軸基準磁界発生用ヘル
ムホルツコイル41とx軸検出用磁気センサ21、Y軸
基準磁界発生用ヘルムホルツコイル42とy軸検出用磁
気センサ22、Z軸基準磁界発生用ヘルムホルツコイル
43とz軸検出用磁気センサ23とは、軸を一致させて
いる。
FIG. 3 shows a reference magnetic field generator. The reference magnetic field generator includes a Helmholtz coil 41 for generating an X-axis reference magnetic field, a Helmholtz coil 42 for generating a Y-axis reference magnetic field,
It comprises a Helmholtz coil 43 for generating an axial reference magnetic field and a constant current power supply 44. At this time, the Helmholtz coil 41 for generating the X-axis reference magnetic field and the magnetic sensor 21 for detecting the x-axis, the Helmholtz coil 42 for generating the Y-axis reference magnetic field and the magnetic sensor 22 for detecting the y-axis, the Helmholtz coil 43 for generating the Z-axis reference magnetic field and z The axis is aligned with the axis detecting magnetic sensor 23.

【0011】この状態において、基準磁界発生装置14
(ヘルムホルツコイル41,42,43)によって、基
準となる磁界を移動体13に印加し、その時の地磁気セ
ンサ11の出力を得る。
In this state, the reference magnetic field generator 14
The reference magnetic field is applied to the moving body 13 by the (Helmholtz coils 41, 42, 43), and the output of the geomagnetic sensor 11 at that time is obtained.

【0012】基準磁界発生装置14に基準磁界となる条
件1(X軸=Xc,Y軸=0,Z軸=0)の磁界を与
え、地磁気センサ11の三軸の出力x=xs1,y=ys
1,z=zs1が得られる(条件1)。
A magnetic field under condition 1 (X-axis = Xc, Y-axis = 0, Z-axis = 0), which is a reference magnetic field, is applied to the reference magnetic field generator 14, and three-axis outputs x = xs1, y = ys
1, z = zs1 is obtained (condition 1).

【0013】次に、基準磁界発生装置14に基準磁界と
なる条件2(X軸=0,Y軸=Yc,Z軸=0)の磁界
を与え、地磁気センサ11の三軸の出力x=xs2,y=
ys2,z=zs2が得られる(条件2)。
Next, a magnetic field under condition 2 (X axis = 0, Y axis = Yc, Z axis = 0) is applied to the reference magnetic field generator 14 as a reference magnetic field, and the triaxial output x = xs2 of the geomagnetic sensor 11 is given. , Y =
ys2, z = zs2 is obtained (condition 2).

【0014】次に、基準磁界発生装置14に基準磁界と
なる条件3(X軸=0,Y軸=0,Z軸=Zc)の磁界
を与え、地磁気センサ11の三軸の出力x=xs3,y=
ys3,z=zs3が得られる(条件3)。
Next, a magnetic field of condition 3 (X axis = 0, Y axis = 0, Z axis = Zc) is applied to the reference magnetic field generator 14 as a reference magnetic field, and the triaxial output x = xs3 of the geomagnetic sensor 11 is given. , Y =
ys3, z = zs3 is obtained (condition 3).

【0015】条件1より次式の数1が得られる。なお、
式中、Aは、x軸検出用磁気センサのX軸に対する補正
係数、Bは、x軸検出用磁気センサのY軸に対する補正
係数、Cは、x軸検出用磁気センサのZ軸に対する補正
係数、Dは、y軸検出用磁気センサのX軸に対する補正
係数、Eは、y軸検出用磁気センサのY軸に対する補正
係数、Fは、y軸検出用磁気センサのZ軸に対する補正
係数、Gは、z軸検出用磁気センサのX軸に対する補正
係数、Hは、z軸検出用磁気センサのY軸に対する補正
係数、Iは、z軸検出用磁気センサのZ軸に対する補正
係数である。
From the condition 1, the following equation 1 is obtained. In addition,
In the formula, A is a correction coefficient of the x-axis detection magnetic sensor with respect to the X-axis, B is a correction coefficient of the x-axis detection magnetic sensor with respect to the Y-axis, and C is a correction coefficient of the x-axis detection magnetic sensor with respect to the Z-axis. , D is a correction coefficient of the y-axis detection magnetic sensor with respect to the X-axis, E is a correction coefficient of the y-axis detection magnetic sensor with respect to the Y-axis, F is a correction coefficient of the y-axis detection magnetic sensor with respect to the Z-axis, G Is a correction coefficient of the z-axis detection magnetic sensor with respect to the X-axis, H is a correction coefficient of the z-axis detection magnetic sensor with respect to the Y-axis, and I is a correction coefficient of the z-axis detection magnetic sensor with respect to the Z-axis.

【0016】[0016]

【数1】 (Equation 1)

【0017】同様に、条件2より次式の数2が得られ
る。
Similarly, the following equation (2) is obtained from condition 2.

【0018】[0018]

【数2】 (Equation 2)

【0019】同じく、条件3より次式の数3が得られ
る。
Similarly, the following equation (3) is obtained from the condition (3).

【0020】[0020]

【数3】 (Equation 3)

【0021】数1、数2、数3より、下式の数4が得ら
れる。
From Expressions 1, 2, and 3, Expression 4 of the following expression is obtained.

【0022】[0022]

【数4】 (Equation 4)

【0023】そこで、求める補正係数は下式の数5とな
る。
The correction coefficient to be obtained is given by the following equation (5).

【0024】[0024]

【数5】 (Equation 5)

【0025】[0025]

【実施例】図3に示すように、呼び径2mmのマグネッ
トワイヤを内径2,705mm()(X軸用)、2,90
5mm(Y軸用)、2,505mm(Z軸用)に84タ
ーン巻回したコイルを2個ずつ用意し、2,705mm
(X軸)、2,905mm(Y軸)、2,505mm(Z
軸)の間隔で3軸(X軸,Y軸,Z軸)に配置して、X
軸基準磁界発生用ヘルムホルツコイル41、Y軸基準磁
界発生用ヘルムホルツコイル42、Z軸基準磁界発生用
ヘルムホルツコイル43とした。
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS As shown in FIG.
Prepare two coils of 84 turns each wound 5 mm (for Y axis) and 2,505 mm (for Z axis), and 2,705 mm
(X axis), 2,905 mm (Y axis), 2,505 mm (Z
3 axes (X axis, Y axis, Z axis) at intervals of
A Helmholtz coil 41 for generating an axial reference magnetic field, a Helmholtz coil 42 for generating a Y-axis reference magnetic field, and a Helmholtz coil 43 for generating a Z-axis reference magnetic field.

【0026】定電流電源44を用いて、ヘルムホルツコ
イル41に3,224.7ミリアンペアの電流を流したと
ころ、磁界均一度1nT、磁界強度60,000nTの
X軸基準磁界が得られた。
When a current of 3,224.7 milliamps was passed through the Helmholtz coil 41 using the constant current power supply 44, an X-axis reference magnetic field having a magnetic field uniformity of 1 nT and a magnetic field strength of 60,000 nT was obtained.

【0027】上記のようにして得られたX軸の基準磁界
Xc60,000nT中に移動体13を置き、地磁気セ
ンサの出力を測定して得られた出力値は、xs1が60,4
00nT、Ys1が−270nT、zs1が1,030nTで
あった。
The output value obtained by placing the moving body 13 in the X-axis reference magnetic field Xc of 60,000 nT obtained as described above and measuring the output of the geomagnetic sensor is xs1 of 60,4.
00nT, Ys1 was -270nT, and zs1 was 1,030nT.

【0028】同様にして、Y軸については、ヘルムホル
ツコイル41に3,463.5ミリアンペアの電流を流し
て得たYc60,000nTに対して、xs2は180n
T、ys2は60,360nT、zs2は1,270nTであっ
た。
Similarly, with respect to the Y axis, xs2 is 180 ns with respect to Yc 60,000 nT obtained by flowing a current of 3,463.5 milliamperes through the Helmholtz coil 41.
T and ys2 were 60,360 nT and zs2 was 1,270 nT.

【0029】同様にして、Z軸については、ヘルムホル
ツコイル43に2,986.8ミリアンペアの電流を流し
て得たZc60,000nTに対して、xs3は1,500
nT、ys3は−700nT、zs3は58,610nTであ
った。
Similarly, on the Z axis, xs3 is 1,500 for Zc 60,000 nT obtained by flowing a current of 2,986.8 milliamperes through the Helmholtz coil 43.
nT and ys3 were -700 nT, and zs3 was 58,610 nT.

【0030】上記のようにして得られた値を数4に代入
して補正係数を得た。x軸検出用磁気センサのX軸に対
する補正係数(A)は、0.99380、x軸検出用磁
気センサのY軸に対する補正係数(B)は、−0.00
243、x軸検出用磁気センサのZ軸に対する補正係数
(C)は、−0.02546であり、y軸検出用磁気セ
ンサのX軸に対する補正係数(D)は、0.0042
4、y軸検出用磁気センサのY軸に対する補正係数
(E)は、0.99378、y軸検出用磁気センサのZ
軸に対する補正係数(F)は、0.01176であり、
z軸検出用磁気センサのX軸に対する補正係数(G)
は、−0.01756、z軸検出用磁気センサのY軸に
対する補正係数(H)は、−0.02149、z軸検出
用磁気センサのZ軸に対する補正係数(I)は、1.0
2391であった。
A correction coefficient was obtained by substituting the value obtained as described above into Equation 4. The correction coefficient (A) of the x-axis detection magnetic sensor for the X axis is 0.999380, and the correction coefficient (B) of the x-axis detection magnetic sensor for the Y axis is -0.000.
243, the correction coefficient (C) of the x-axis detecting magnetic sensor with respect to the Z-axis is -0.022546, and the correction coefficient (D) of the y-axis detecting magnetic sensor with respect to the X-axis is 0.0042.
4. The correction coefficient (E) of the y-axis detecting magnetic sensor with respect to the Y-axis is 0.999378, and the Z-axis of the y-axis detecting magnetic sensor is
The correction factor (F) for the axis is 0.01176,
Correction coefficient (G) for the X-axis of the magnetic sensor for z-axis detection
Is -0.01756, the correction coefficient (H) of the z-axis detecting magnetic sensor with respect to the Y axis is -0.02149, and the correction coefficient (I) of the z-axis detecting magnetic sensor with respect to the Z axis is 1.0.
2391.

【0031】上記のようにして得られた、補正係数を用
いた時の検出誤差は、標準磁界測定器(精度SSS)を
用いて照合したところ、10nT以下、方位角度にして
0.1度以下であり、検出精度は、従来比、1桁向上し
た(従来の検出精度は、約1度)。
The detection error obtained by using the correction coefficient obtained as described above was collated using a standard magnetic field measuring instrument (accuracy SSS) and found to be 10 nT or less and azimuth angle of 0.1 degree or less. The detection accuracy is improved by one digit compared to the conventional one (the conventional detection accuracy is about 1 degree).

【0032】本実施の形態では、3軸の場合で説明した
が、2軸の場合にも適用できることは原理的に明らかで
ある。
Although the present embodiment has been described for the case of three axes, it is in principle apparently applicable to the case of two axes.

【0033】[0033]

【発明の効果】以上、述べた如く、本発明によれば、移
動体内に装着された地磁気検出センサにおいて、移動体
の固有磁界を補正することが可能となり、より高精度に
方位検出が行えることが可能となった。すなわち、本発
明よれば、高精度な補正を行って、正しい方位を与える
地磁気の検出方法が得られる。
As described above, according to the present invention, it is possible to correct the intrinsic magnetic field of a moving body in a geomagnetic detection sensor mounted in the moving body, and to perform azimuth detection with higher accuracy. Became possible. That is, according to the present invention, it is possible to obtain a method of detecting geomagnetism that performs accurate correction and gives a correct azimuth.

【図面の簡単な説明】[Brief description of the drawings]

【図1】本発明による検出方法の全体ブロック図。FIG. 1 is an overall block diagram of a detection method according to the present invention.

【図2】本発明に用いる磁気センサの構造図。FIG. 2 is a structural view of a magnetic sensor used in the present invention.

【図3】基準磁界発生装置を示す説明図。FIG. 3 is an explanatory view showing a reference magnetic field generator.

【符号の説明】[Explanation of symbols]

11 地磁気検出センサ 12 方位演算部 13 移動体 14 基準磁界発生装置 21 (x軸検出用)磁気センサ 22 (y軸検出用)磁気センサ 23 (z軸検出用)磁気センサ 41 (X軸基準磁界発生用)ヘルムホルツコイル 42 (Y軸基準磁界発生用)ヘルムホルツコイル 43 (Z軸基準磁界発生用)ヘルムホルツコイル 44 定電流電源 Reference Signs List 11 geomagnetic detection sensor 12 azimuth calculation unit 13 moving body 14 reference magnetic field generator 21 (for x-axis detection) magnetic sensor 22 (for y-axis detection) magnetic sensor 23 (for z-axis detection) magnetic sensor 41 (x-axis reference magnetic field generation Helmholtz coil 42 (for generating Y-axis reference magnetic field) Helmholtz coil 43 (for generating Z-axis reference magnetic field) Helmholtz coil 44 Constant current power supply

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】 移動体に装着される地磁気成分を互いに
直交する3軸成分(x,y,z)に分けて検出し、これ
ら3成分に対応した地磁気信号を出力する地磁気センサ
と、地磁気信号に基づき移動体の方位信号を出力する方
位演算部と、移動体に3軸(X,Y,Z)の基準磁界を
与える基準磁界発生装置とを用いる地磁気検出の方法で
あって、前記基準磁界発生装置によりX軸にXc,Y軸
に0,Z軸に0なる磁界を与えて得られるx軸のセンサ
出力xs1,y軸のセンサ出力ys1,z軸のセンサ出力z
s1と、前記基準磁界発生装置によりX軸に0,Y軸にY
c,Z軸に0なる磁界を与えて得られる、x軸のセンサ
出力xs2,y軸のセンサ出力ys2,z軸のセンサ出力z
s2と、前記基準磁界発生装置によりX軸に0,Y軸に
0,Z軸にZcなる磁界を与えて得られる、x軸のセン
サ出力xs3、y軸のセンサ出力ys3、z軸のセンサ出力
zs3とを用いて得られる3行3列の行列式の解を用いて
地磁気の検出磁界を補正することを特徴とする地磁気の
検出方法。
1. A geomagnetic sensor for detecting a geomagnetic component attached to a moving body into three orthogonal components (x, y, z) orthogonal to each other and outputting a geomagnetic signal corresponding to the three components, and a geomagnetic signal. A geomagnetic detection method using an azimuth calculation unit that outputs an azimuth signal of a moving object based on a reference magnetic field, and a reference magnetic field generator that applies a three-axis (X, Y, Z) reference magnetic field to the moving object, An x-axis sensor output xs1, a y-axis sensor output ys1, and a z-axis sensor output z obtained by applying a magnetic field of Xc to the X-axis, 0 to the Y-axis, and 0 to the Z-axis by the generator.
s1 and 0 on the X axis and Y on the Y axis by the reference magnetic field generator.
The x-axis sensor output xs2, the y-axis sensor output ys2, and the z-axis sensor output z obtained by applying a magnetic field of 0 to the c and Z axes.
s2, the x-axis sensor output xs3, the y-axis sensor output ys3, and the z-axis sensor output obtained by applying a magnetic field of 0 to the X axis, 0 to the Y axis, and Zc to the Z axis by the reference magnetic field generator. A method for detecting terrestrial magnetism, comprising correcting a terrestrial magnetism detection magnetic field by using a solution of a determinant of three rows and three columns obtained by using zs3.
JP21568197A 1997-07-25 1997-07-25 Method for detecting geomagnetism Pending JPH1144538A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP21568197A JPH1144538A (en) 1997-07-25 1997-07-25 Method for detecting geomagnetism

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP21568197A JPH1144538A (en) 1997-07-25 1997-07-25 Method for detecting geomagnetism

Publications (1)

Publication Number Publication Date
JPH1144538A true JPH1144538A (en) 1999-02-16

Family

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Family Applications (1)

Application Number Title Priority Date Filing Date
JP21568197A Pending JPH1144538A (en) 1997-07-25 1997-07-25 Method for detecting geomagnetism

Country Status (1)

Country Link
JP (1) JPH1144538A (en)

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP1178284A3 (en) * 2000-08-01 2003-05-28 Seiko Instruments Inc. Method and system for adjusting an electronic azimuth meter
KR100757839B1 (en) 2006-04-04 2007-09-11 삼성전자주식회사 Control system, having control system moving robot apparatus and control method thereof
WO2014057506A1 (en) * 2012-10-08 2014-04-17 Microtest S.R.L. Test equipment for checking sensors sensitive to magnetic fields
JP2022008432A (en) * 2016-09-26 2022-01-13 マジック リープ, インコーポレイテッド Calibration of magnetic and optical sensors in virtual reality or augmented reality display system

Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP1178284A3 (en) * 2000-08-01 2003-05-28 Seiko Instruments Inc. Method and system for adjusting an electronic azimuth meter
US6662459B2 (en) 2000-08-01 2003-12-16 Seiko Instruments Inc. Electronic azimuth meter and timepiece
KR100757839B1 (en) 2006-04-04 2007-09-11 삼성전자주식회사 Control system, having control system moving robot apparatus and control method thereof
WO2014057506A1 (en) * 2012-10-08 2014-04-17 Microtest S.R.L. Test equipment for checking sensors sensitive to magnetic fields
JP2022008432A (en) * 2016-09-26 2022-01-13 マジック リープ, インコーポレイテッド Calibration of magnetic and optical sensors in virtual reality or augmented reality display system

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