JP3063027B2 - Position detection method - Google Patents

Position detection method

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Publication number
JP3063027B2
JP3063027B2 JP8318570A JP31857096A JP3063027B2 JP 3063027 B2 JP3063027 B2 JP 3063027B2 JP 8318570 A JP8318570 A JP 8318570A JP 31857096 A JP31857096 A JP 31857096A JP 3063027 B2 JP3063027 B2 JP 3063027B2
Authority
JP
Japan
Prior art keywords
magnetic field
excitation
coil
horizontal
excitation coil
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.)
Expired - Lifetime
Application number
JP8318570A
Other languages
Japanese (ja)
Other versions
JPH10148502A (en
Inventor
拓美 佐野
彰 長谷川
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.)
Takasago Ltd
Original Assignee
Takasago Ltd
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 Takasago Ltd filed Critical Takasago Ltd
Priority to JP8318570A priority Critical patent/JP3063027B2/en
Publication of JPH10148502A publication Critical patent/JPH10148502A/en
Application granted granted Critical
Publication of JP3063027B2 publication Critical patent/JP3063027B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

Links

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】この発明は、トンネルを掘削
する推進機や、非金属性配管などの管内監視装置などの
先端に発信器を設け、この発信器の発する磁界を地上か
ら検出してその位置を特定しようとする位置検出方法に
関するものであり、さらにこの原理を応用して、移動す
る車両の位置を検出したり、同時に発信器や検出器のコ
イルを利用して、道路側には車両の接近を非接触で感知
したり、道路側から車両に任意の信号を送ることができ
るものである。
BACKGROUND OF THE INVENTION The present invention relates to a transmitter provided at a tip of a propulsion device for excavating a tunnel or a monitoring device for a pipe such as a nonmetallic pipe, and detects a magnetic field generated by the transmitter from the ground. The present invention relates to a position detection method that attempts to specify a position. Further, by applying this principle, the position of a moving vehicle is detected, and at the same time, a vehicle is mounted on the road side by using a coil of a transmitter and a detector. It is possible to detect the approach of a vehicle in a non-contact manner or to send an arbitrary signal to the vehicle from the road side.

【0002】[0002]

【従来の技術】洞道や地中の配管に任意の装置を入れた
場合、この装置の位置を地上から測定する方法として、
ジャイロスコープを用いた方法などがあり、商品化も行
われている。しかし、この方法では、緩い傾斜や曲がり
に対してはジャイロが正確に作動しなかったり、ジャイ
ロの出力を積分する積分器の誤差などが重なり、正確に
位置を特定することは困難であった。この問題を解決す
るために、電磁的方法や音響を利用する方法などが試さ
れた。
2. Description of the Related Art When an arbitrary device is placed in a tunnel or underground pipe, a method of measuring the position of the device from the ground is as follows.
There is a method using a gyroscope and the like, and commercialization is being performed. However, in this method, the gyro does not operate accurately for a gentle inclination or bend, and an error of an integrator for integrating the output of the gyro overlaps, and it is difficult to specify the position accurately. In order to solve this problem, an electromagnetic method and a method using sound were tried.

【0003】[0003]

【発明が解決しようとする課題】しかしながら、音響に
よる方法は音響の伝搬が複雑で減衰も多く、位置の特定
が不可能であった。また従来の電磁的方法は、単一磁界
の磁界分布を利用したもので、この場合の磁界強度のヌ
ル点では、磁界強度が極めて微弱であり、ヌル点の位置
が正確に特定できなかったり、磁界の最大値を得る方法
は、そのピークの位置を特定するのが困難であったり、
地球磁場の影響で磁界強度を検出する目的のサーチコイ
ルを移動した場合に予期しない出力が現わるトラブル
や、商用交流電力供給用の地中線から発生する交流磁界
の影響を受けて誤動作するなどの多くの問題点があり、
実用化が困難であった。
However, in the method using sound, the propagation of sound is complicated and the attenuation is large, so that the position cannot be specified. In addition, the conventional electromagnetic method uses a magnetic field distribution of a single magnetic field.In this case, at the null point of the magnetic field strength, the magnetic field strength is extremely weak, and the position of the null point cannot be specified accurately, The method of obtaining the maximum value of the magnetic field is difficult to locate the peak,
Trouble that unexpected output appears when moving the search coil to detect the magnetic field strength under the influence of the earth's magnetic field, malfunction due to the influence of the AC magnetic field generated from the underground wire for commercial AC power supply, etc. There are many problems,
Practical application was difficult.

【0004】この発明はこれらの点に鑑みてなされたも
のであり、雑音の影響、地球磁場の影響、地中線などか
ら放射される商用交流磁場の影響等を抑えて、より正確
な検出ができる位置検出方法を提供して上記課題を解決
しようとするものである。
[0004] The present invention has been made in view of these points, and suppresses the influence of noise, the influence of the earth's magnetic field, the influence of a commercial AC magnetic field radiated from an underground wire, and the like, thereby achieving more accurate detection. An object of the present invention is to provide a position detection method capable of solving the above problems.

【0005】[0005]

【課題を解決するための手段】そこでこの発明は、複数
の励磁コイルを設け、それぞれの励磁コイルを時分割に
励磁し、この励磁コイルの駆動信号と同期を取った増幅
器でそれぞれの励磁コイルの発生する磁界を検出し、そ
れぞれの出力の割合から励磁コイルの位置を測定しよう
とするものである。この方法では磁界のヌル点ではな
く、相互の磁界強度の強い点で磁界強度の割合を利用す
るので測定点の磁界強度が高く、雑音の影響を少なくで
きるだけでなく、それぞれの信号を差動増幅器に加える
方法によって地球磁場の影響や地中線等から放射される
商用交流磁場の影響を極力抑えることができるものであ
る。以下この発明を具体的に説明する。
SUMMARY OF THE INVENTION Accordingly, the present invention provides a plurality of exciting coils, excites each exciting coil in a time-division manner, and uses an amplifier synchronized with a drive signal of the exciting coil to control each exciting coil. The purpose is to detect the generated magnetic field and measure the position of the exciting coil from the ratio of each output. In this method, the ratio of the magnetic field strength is used not at the null point of the magnetic field but at the point where the mutual magnetic field strength is strong, so that the magnetic field strength at the measurement point is high, so that not only can the effect of noise be reduced, but also each signal is amplified by a differential amplifier. In this method, the influence of the earth's magnetic field and the influence of the commercial AC magnetic field radiated from the underground wire can be minimized. Hereinafter, the present invention will be described specifically.

【0006】請求項1項の発明は、被測定点に、交互に
水平又は垂直方向の磁界を発生させる複数の励磁コイル
を設け、これらの励磁コイルを励磁回路によって交互に
励磁して交互に水平又は垂直成分の交流磁界を発生さ
せ、測定点では、水平又は垂直方向の磁界を検出する複
数の検出コイルを有する磁界検出器を設け、この検出器
の位置を移動させて上記それぞれの励磁タイミングに対
する任意の点における交流磁場と方向成分を検出してこ
れを電圧信号に変換し、この電圧信号を上記励磁回路の
励磁タイミングと同期を取ったスイッチで選択して、水
平励磁コイル及び垂直励磁コイルのいずれか一方の励磁
コイルから発生した磁界成分による電圧信号と水平励磁
コイル及び垂直励磁コイルのいずれか他方の励磁コイル
から発生した磁界成分による電圧信号の二つの信号に分
離し、これらの二つの信号を差動増幅器にかけ、この差
動増幅器の出力が零になる位置から励磁コイルの位置を
求める、位置検出方法とした。
According to a first aspect of the present invention, a plurality of exciting coils for generating a magnetic field in a horizontal or vertical direction are provided alternately at a point to be measured, and these exciting coils are alternately excited by an exciting circuit to be alternately horizontal. Alternatively, an alternating magnetic field of a vertical component is generated, and at the measurement point, a magnetic field detector having a plurality of detection coils for detecting a magnetic field in the horizontal or vertical direction is provided, and the position of the detector is moved to correspond to the respective excitation timings. An AC magnetic field and a directional component at an arbitrary point are detected and converted into a voltage signal, and this voltage signal is selected by a switch synchronized with the excitation timing of the excitation circuit, and the horizontal excitation coil and the vertical excitation coil are selected. The voltage signal due to the magnetic field component generated from one of the exciting coils and the magnetic field component generated from the other exciting coil, the horizontal exciting coil or the vertical exciting coil, Separated into two signals of voltage signals by, multiplying these two signals to the differential amplifier, the output of the differential amplifier determine the position of the excitation coil from the position where the zero and the position detection method.

【0007】また請求項2項の発明は、被測定点から任
意の距離に置かれ、交互に水平又は垂直方向の磁界を発
生させる複数の励磁コイルを設け、これらの励磁コイル
を励磁回路によって交互に励磁して交互に水平又は垂直
の交流磁界を発生させ、測定点では、水平又は垂直方向
の磁界を検出する複数の検出コイルを有する磁界検出器
を設け、この検出器の位置を移動させて上記それぞれの
励磁タイミングに対する任意の点における交流磁場と方
向成分を検出してこれを電圧信号に変換し、この電圧信
号を上記励磁回路の励磁タイミングと同期を取ったスイ
ッチで選択して、水平励磁コイル及び垂直励磁コイルの
いずれか一方の励磁コイルから発生した磁界成分による
電圧信号と水平励磁コイル及び垂直励磁コイルのいずれ
か他方の励磁コイルから発生した各磁界成分による電圧
信号の二つの信号に分離し、これらの二つの信号を差動
増幅器にかけ、この作動増幅器の出力が零になる位置か
ら励磁コイルの位置を求める、位置検出方法とした。
According to a second aspect of the present invention, a plurality of excitation coils are provided at an arbitrary distance from a point to be measured and alternately generate a magnetic field in a horizontal or vertical direction, and these excitation coils are alternately switched by an excitation circuit. A magnetic field detector having a plurality of detection coils for detecting a magnetic field in the horizontal or vertical direction is provided at the measurement point by exciting the magnetic field alternately to generate a horizontal or vertical AC magnetic field, and moving the position of the detector. The AC magnetic field and the directional component at any point with respect to the respective excitation timings are detected and converted into a voltage signal, and this voltage signal is selected by a switch synchronized with the excitation timing of the excitation circuit, and the horizontal excitation is performed. A voltage signal due to a magnetic field component generated from one of the excitation coil of the coil and the vertical excitation coil and the excitation coil of the other one of the horizontal excitation coil and the vertical excitation coil A position detection method for obtaining a position of an exciting coil from a position where the output of the operational amplifier becomes zero, separating the two signals into two signals of a voltage signal by each magnetic field component generated from the differential amplifier. did.

【0008】また請求項3項の発明は、被測定点から任
意の距離に置かれ、交互に水平又は垂直方向の磁界を発
生させる複数の励磁コイルを設け、これらの励磁コイル
を励磁回路によって交互に励磁して交互に水平又は垂直
の交流磁界を発生させ、測定点では、それぞれの上記励
磁コイルを遮断した直後に励磁コイルの近傍の導体から
発生する渦電流による磁界を励磁コイルと同期を取った
同期増幅器で選択的に検出して、上記導体を検出すると
ともに、任意の点における交流磁場と方向成分を励磁コ
イルの近傍に設けた水平又は垂直方向の磁界を検出する
複数の検出コイルを有する磁界検出器で検出し、この信
号を上記励磁回路と同期を取った同期増幅器で増幅し、
それぞれの励磁コイルによる任意の点の磁界強度を求
め、水平励磁コイル及び垂直励磁コイルのいずれか一方
の励磁コイルから発生した磁界成分による電圧信号と水
平励磁コイル及び垂直励磁コイルのいずれか他方の励磁
コイルから発生した各磁界成分による電圧信号の二つの
信号に分離し、これらの二つの信号を差動増幅器にか
け、この差動増幅器の出力が零になる位置から励磁コイ
ルの位置を求める、位置検出方法とした。
According to a third aspect of the present invention, a plurality of exciting coils are provided at an arbitrary distance from a point to be measured and alternately generate a magnetic field in a horizontal or vertical direction, and these exciting coils are alternately switched by an exciting circuit. At the measurement points, the magnetic field due to the eddy current generated from the conductor near the excitation coil is synchronized with the excitation coil immediately after the excitation coil is shut off. And a plurality of detection coils for detecting the conductors selectively and detecting the magnetic field in a horizontal or vertical direction provided near the excitation coil with an AC magnetic field and a directional component at an arbitrary point. This signal is detected by a magnetic field detector, and this signal is amplified by a synchronous amplifier synchronized with the excitation circuit.
The magnetic field intensity at an arbitrary point by each excitation coil is obtained, and the voltage signal by the magnetic field component generated from one of the horizontal excitation coil and the vertical excitation coil and the excitation of the other one of the horizontal excitation coil and the vertical excitation coil are obtained. Separation into two signals of the voltage signal by each magnetic field component generated from the coil, these two signals are applied to the differential amplifier, and the position of the exciting coil is obtained from the position where the output of the differential amplifier becomes zero. Method.

【0009】また請求項4項の発明は、上記請求項1
項、2項、3項のうちのいずれか一つの位置検出方法に
おいて、励磁コイルの励磁周波数と異なる周波数を励磁
コイルに重畳し、位置検出や導体検出を行いながら励磁
コイルから検出コイルに任意信号を送る、位置検出方法
とした。
Further, the invention of claim 4 provides the above-mentioned claim 1.
In the position detecting method of any one of the paragraphs 2, 2 and 3, a frequency different from the excitation frequency of the excitation coil is superimposed on the excitation coil, and an arbitrary signal is transmitted from the excitation coil to the detection coil while performing position detection and conductor detection. And the position detection method.

【0010】[0010]

【実施の形態例】以下この発明の実施の形態例を説明す
る前に、最も説明の容易な円形ループコイルを励磁コイ
ルと検出コイルに使用した実例を説明する。まず図1に
示すごとく、半径aの円形コイルに電流Iを流した場
合、コイルの半径aに比べて充分に離れた距離rのP点
に生じる磁界を求めると。
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS Before describing an embodiment of the present invention, an example in which a circular loop coil, which is the easiest to describe, is used for an excitation coil and a detection coil will be described. First, as shown in FIG. 1, when a current I is passed through a circular coil having a radius a, a magnetic field generated at a point P at a distance r sufficiently far from the radius a of the coil is obtained.

【0011】[0011]

【数1】 (Equation 1)

【0012】[0012]

【数2】 (Equation 2)

【0013】[0013]

【数3】 (Equation 3)

【0014】[0014]

【数4】 (Equation 4)

【0015】[0015]

【数5】 (Equation 5)

【0016】[0016]

【数6】 (Equation 6)

【0017】[0017]

【数7】 (Equation 7)

【0018】[0018]

【数8】 (Equation 8)

【0019】[0019]

【数9】 (Equation 9)

【0020】磁界の水平成分と垂直成分をそれぞれ検出
するには、磁界を発生する送信コイルと同じように、そ
れぞれの磁界の成分に対してコイルのループが作る面を
水平又は垂直にした受信コイルによって検出できる。こ
の場合の結果を図示すると図4となる。図4で楕円によ
って示すコイルの図は、送信コイルと受信コイルの相対
方向を示す。
In order to detect the horizontal component and the vertical component of the magnetic field, respectively, like the transmission coil that generates the magnetic field, the receiving coil in which the plane formed by the coil loop for each magnetic field component is made horizontal or vertical. Can be detected by FIG. 4 shows the result in this case. The diagram of the coil indicated by an ellipse in FIG. 4 shows the relative directions of the transmitting coil and the receiving coil.

【0021】図4から、送信コイルが作る磁界の水平成
分と垂直成分をそれぞれ独立に検出し、それぞれの磁界
の相対強度の絶対値が一致する点を求めると、送信コイ
ルと受信コイルとの距離dを求めることができる。この
時図4に示す磁界強度の絶対値は、水平距離xに対して
対称に現われるので、それぞれの磁界強度の絶対値が一
致する点はx軸に対して対称に発生する。そこでこの条
件の適合する二点を求め、この二点間の距離を求め、こ
の距離の1/2が送信コイルと受信コイルの水平距離と
なる。
From FIG. 4, the horizontal component and the vertical component of the magnetic field generated by the transmitting coil are detected independently, and the point where the absolute values of the relative intensities of the respective magnetic fields match is determined. d can be determined. At this time, since the absolute value of the magnetic field strength shown in FIG. 4 appears symmetrically with respect to the horizontal distance x, the point where the absolute value of each magnetic field strength coincides occurs symmetrically with respect to the x-axis. Therefore, two points that satisfy this condition are determined, and the distance between the two points is determined. One half of this distance is the horizontal distance between the transmitting coil and the receiving coil.

【0022】次にこの発明の方法を実現するための具体
的装置を図5に示す。図中Aは受信機を示し、1は受信
機Aの受信コイルであり、このコイルの配置によって異
なるが水平又は垂直成分の磁界を検出する。2は抵抗器
であり、入力インピーダンスと負帰還量を調整する。3
は初段増幅器であり、受信コイル1で受信した電圧を増
幅する。4は同期スイッチであり、他の同期増幅器と同
期を取って交互に切り替わる。5は差動増幅器であり、
水平又は垂直成分の磁界に対応する信号をそれぞれの差
動入力に加えてこの差分を増幅する。6は積分器であ
り、差動増幅器5の出力を平均化して平滑化する。7は
当該受信機Aの出力端子10の出力の一部を負帰還する
ための負帰還量を調整する帰還補償減衰器である。8は
利得−1の反転増幅器であり、上記同期スイッチ4の負
帰還用スイッチに加えて出力信号の一部が負帰還となる
ように抵抗器9を通して初段増幅器3に加えられる。こ
の帰還補償減衰器7、反転増幅器8及び抵抗器9による
負帰還作用は、受信信号が弱い場合や、雑音の多い場合
に効果的に作用するが、受信信号が強い場合は必要とし
ない。
FIG. 5 shows a specific apparatus for realizing the method of the present invention. In the figure, A denotes a receiver, and 1 denotes a receiving coil of the receiver A, which detects a magnetic field of a horizontal or vertical component depending on the arrangement of the coil. Reference numeral 2 denotes a resistor for adjusting the input impedance and the amount of negative feedback. 3
Is a first-stage amplifier, which amplifies the voltage received by the receiving coil 1. Reference numeral 4 denotes a synchronous switch, which is alternately switched in synchronization with another synchronous amplifier. 5 is a differential amplifier,
A signal corresponding to the magnetic field of the horizontal or vertical component is applied to each differential input to amplify this difference. Reference numeral 6 denotes an integrator, which averages and smoothes the output of the differential amplifier 5. Reference numeral 7 denotes a feedback compensation attenuator that adjusts a negative feedback amount for negatively feeding back a part of the output of the output terminal 10 of the receiver A. Reference numeral 8 denotes an inverting amplifier having a gain of -1, which is added to the first-stage amplifier 3 through a resistor 9 so that a part of the output signal becomes negative feedback in addition to the negative feedback switch of the synchronous switch 4. The negative feedback effect of the feedback compensation attenuator 7, the inverting amplifier 8, and the resistor 9 works effectively when the received signal is weak or has a lot of noise, but is not required when the received signal is strong.

【0023】Bは駆動回路を示し、11は水晶発振器
で、この水晶発振器11で発生されたパルス信号を分周
器12を介してタイミング発生器13に送り、このタイ
ミング発生器13から上記受信機Aの同期スイッチ4及
び後述の送信機Cの水平垂直切り替え器14に切り替え
信号を送り、また当該水平垂直切り替え器14に励磁信
号を送る。また上記受信機Aの初段増幅器3にマスク信
号を送る。Cは送信機であり、上記励磁信号をこの送信
機Cの水平垂直切り替え器14で入力し、上記切り替え
信号により垂直駆動回路15又は水平駆動回路16を動
かす。これらの垂直駆動回路15及び水平駆動回路16
の出力に相互に垂直位置となった垂直磁界コイル17及
び水平磁界コイル18をそれぞれ励磁する。
B denotes a drive circuit, and 11 denotes a crystal oscillator, which sends a pulse signal generated by the crystal oscillator 11 to a timing generator 13 via a frequency divider 12, and outputs the pulse signal from the timing generator 13 to the receiver. A switching signal is sent to the synchronous switch 4 of A and a horizontal / vertical switch 14 of the transmitter C described later, and an excitation signal is sent to the horizontal / vertical switch 14. Further, a mask signal is sent to the first-stage amplifier 3 of the receiver A. C is a transmitter, and the excitation signal is input to the horizontal / vertical switch 14 of the transmitter C, and the vertical drive circuit 15 or the horizontal drive circuit 16 is operated by the switch signal. These vertical drive circuit 15 and horizontal drive circuit 16
, The vertical magnetic field coil 17 and the horizontal magnetic field coil 18 which are positioned vertically with respect to each other are excited.

【0024】図6は図5の回路の動作を説明するもの
で、T1の期間に水平磁界コイル18を励磁し、この磁
界による受信コイルの電圧を受信コイル1で受信し、こ
の電圧を初段増幅器3及び同期スイッチ4で増幅して差
動増幅器5の一方の端子に加える。T1の終わりでは、
水平磁界コイル18の電流を遮断する。T2はマスクす
る期間である。時間T3では上記垂直磁界コイル17を
励磁する。この時、増幅された受信電圧も同期スイッチ
4により差動増幅器5の他方の端子に加えられる。T3
の終期には垂直磁界コイルの電流も遮断する。T4は過
渡電圧のマスク期間である。同様にしてT5、T6、T
7、T8と繰り返し、受信コイルで受信した水平磁界コ
イル18による成分と垂直磁界コイル17による成分の
受信電圧の差分を増幅し、両者の値が一致する点で図5
の受信機Aの出力端子10の出力が零となる様に動作さ
せる。
FIG. 6 explains the operation of the circuit shown in FIG. 5. In the period T1, the horizontal magnetic field coil 18 is excited, the voltage of the receiving coil due to this magnetic field is received by the receiving coil 1, and this voltage is supplied to the first-stage amplifier. 3 and the signal is amplified by the synchronous switch 4 and applied to one terminal of the differential amplifier 5. At the end of T1,
The current of the horizontal magnetic field coil 18 is cut off. T2 is a period for masking. At time T3, the vertical magnetic field coil 17 is excited. At this time, the amplified reception voltage is also applied to the other terminal of the differential amplifier 5 by the synchronous switch 4. T3
At the end of the period, the current of the vertical magnetic field coil is also cut off. T4 is a transient voltage mask period. Similarly, T5, T6, T
7 and T8 are repeated, and the difference between the received voltage of the component of the horizontal magnetic field coil 18 and the received voltage of the component of the vertical magnetic field coil 17 received by the receiving coil is amplified.
Is operated so that the output of the output terminal 10 of the receiver A becomes zero.

【0025】図4のHvx又はHhyによる磁界は励磁
コイルの真上で零になり、極性が反転する。従って実際
の回路では、励磁コイルの励磁方向を逆転させ、受信信
号の極性が同一方向になるように切り替えるか、受信機
Cの同期スイッチ4の出力に極性切り替えスイッチを設
け、互いに水平磁界と垂直磁界による、受信電圧の絶対
値を比較できるようにするが、図面ではこれを省略し
た。
The magnetic field due to Hvx or Hhy in FIG. 4 becomes zero immediately above the exciting coil, and the polarity is reversed. Therefore, in an actual circuit, the direction of excitation of the exciting coil is reversed and the polarity of the received signal is switched so as to be in the same direction, or a polarity switch is provided at the output of the synchronization switch 4 of the receiver C, and the horizontal magnetic field and the vertical Although it is possible to compare the absolute value of the reception voltage due to the magnetic field, it is omitted in the drawings.

【0026】図7は地中19に埋設又は掘削された推進
管20のなかに、水平磁界コイル21と垂直磁界コイル
22を設置し、駆動回路23によって交互にこれらのコ
イル21又は22を励磁し、地上に設置された受信機2
5に受信コイル24を取付け、洞道の深さyと位置を計
測する場合の略図を示す。ここで、受信機25の同期増
幅器と励磁回路は、有線又は無線による励磁信号の受信
回路とPLL回路によって同期をとる。
FIG. 7 shows that a horizontal magnetic field coil 21 and a vertical magnetic field coil 22 are installed in a propulsion pipe 20 buried or excavated in the underground 19, and these coils 21 or 22 are alternately excited by a drive circuit 23. , Receiver 2 installed on the ground
5 shows a schematic diagram when the receiving coil 24 is attached and the depth y and the position of the sinus are measured. Here, the synchronization amplifier and the excitation circuit of the receiver 25 are synchronized by a wired or wireless excitation signal reception circuit and a PLL circuit.

【0027】この状態で地上にある受信コイル24を這
わせて探索し、水平磁界コイル21の水平成分と垂直磁
界コイル22の垂直成分とが等しくなるヌル点は、水平
コイルの励磁極性を切り替えると水平コイルの面と一致
する面に対して対称になった場合は、上記(18)式の
条件となり、この面に対して対称に求まる。この二点間
の最小距離を1/2にし、この距離を0.281で割る
と、地表面にある受信コイル24から洞道内の磁界コイ
ル21又は22までの距離を求めることが可能となり、
この位置を確定できる。
In this state, the search is performed by creeping the receiving coil 24 on the ground, and the null point where the horizontal component of the horizontal magnetic field coil 21 is equal to the vertical component of the vertical magnetic field coil 22 is obtained by switching the excitation polarity of the horizontal coil. If the plane is symmetric with respect to the plane coinciding with the plane of the horizontal coil, the condition of the above equation (18) is satisfied, and the condition is obtained symmetrically with respect to this plane. If the minimum distance between these two points is halved and this distance is divided by 0.281, the distance from the receiving coil 24 on the ground surface to the magnetic field coil 21 or 22 in the sinus can be obtained.
This position can be determined.

【0028】なお、励磁コイルの形状や受信コイルの形
状は任意であり、その配置中心部を共通にせず、任意の
位置に配置することもできる。また上記実施の形態例で
は、被測定点に励磁コイルを設けたが、予め被測定点と
励磁コイルの位置関係が分かっていれば、被測定点から
任意の距離に励磁コイルを設けてもよく、上記結果にそ
の位置関係を加えれば、被測定点が求められる。
The shape of the exciting coil and the shape of the receiving coil are arbitrary, and they may be arranged at arbitrary positions without using a common arrangement center. In the above embodiment, the excitation coil is provided at the point to be measured. However, if the positional relationship between the point to be measured and the excitation coil is known in advance, the excitation coil may be provided at an arbitrary distance from the point to be measured. By adding the positional relationship to the above result, the point to be measured can be obtained.

【0029】また励磁コイルに金属などの導体が接近す
ると、励磁コイルの励磁電流を完全に遮断した後も、こ
の導体に流れる渦電流によって、微小な磁界が発生す
る。この渦電流の減衰時間よりも早く励磁コイルの電流
を遮断し、励磁コイルの電流が完全に遮断するまでの図
6に示すマスク時間T2又はT3を取り、その直後に励
磁コイルに加える励磁電流の立ち上がりタイミングを遅
らせ、それぞれの励磁コイルに励磁を全くしない期間を
設けると、この期間に励磁コイルには近接導体の渦電流
による電圧が発生し、励磁コイルに導体が接近したこと
を検出できる。この場合、検出距離を伸ばすにはこの励
磁コイルに発生した電圧だけをスイッチによって選択的
に受信し、この電圧を差動増幅器に加えて増幅すればよ
い。
When a conductor such as a metal approaches the exciting coil, a minute magnetic field is generated by the eddy current flowing through the conductor even after the exciting current of the exciting coil is completely cut off. The current of the exciting coil is cut off earlier than the decay time of the eddy current, and a mask time T2 or T3 shown in FIG. 6 is taken until the current of the exciting coil is completely cut off. If the start-up timing is delayed and a period during which no excitation is performed on each excitation coil is provided, a voltage is generated in the excitation coil by an eddy current of a nearby conductor, and it is possible to detect that the conductor approaches the excitation coil. In this case, in order to extend the detection distance, only the voltage generated in the excitation coil is selectively received by the switch, and this voltage is applied to the differential amplifier and amplified.

【0030】図5に示す回路では、差動増幅器による差
動効果によって、増幅器の入力に加わる同相電圧に対し
ては強い抑制効果がある。従って励磁コイルに励磁信号
と大きく異なる周波数の同相電圧が加わっても位置測定
の効果は変わらない。それ故励磁コイルに異なる周波数
の信号を重畳し、この重畳した信号に変調をかけ、受信
コイルでフィルタによって分離し、さらにこの信号を復
調する方法によって、励磁コイルから受信コイルに変調
信号を送信し、受信コイル側でこれを復調でき、位置測
定と通信を同時に行うことが可能となる。
The circuit shown in FIG. 5 has a strong suppressing effect on the common mode voltage applied to the input of the amplifier due to the differential effect of the differential amplifier. Therefore, even if an in-phase voltage having a frequency significantly different from that of the excitation signal is applied to the excitation coil, the effect of position measurement does not change. Therefore, a signal of a different frequency is superimposed on the exciting coil, the modulated signal is modulated, separated by a filter by a receiving coil, and further, a modulation signal is transmitted from the exciting coil to the receiving coil by a method of demodulating this signal. This can be demodulated on the receiving coil side, and position measurement and communication can be performed simultaneously.

【0031】[0031]

【発明の効果】請求項1項及び2項の発明は、複数の磁
界の成分差に対する差動効果によって、極めて高い検出
感度と、地磁気等の外乱や雑音に対する高い耐性を得る
ことが可能となり、1ターンのループ又は帰線をアース
とした単線による励磁コイルでも、移動自在な磁気検出
器でこの磁界を容易に検出することが可能である。従っ
て地下等の不可視な部分にある励磁コイルの位置を地上
から容易かつ正確に求めることが可能となり、地下埋設
管を目標に向かって正確に推進したり、無人の推進機の
位置を地上からトレースできる。さらに励磁コイルを道
路に沿って長い矩形又は楕円にして地下に埋設し、この
磁界を自動車などの移動体に設けた検出器で検出し、こ
の出力で自動車の方向を制御すると、自動車をこのコイ
ルに沿って走行するように制御が可能となる。この様に
この発明は不可視部分にある励磁コイルの位置を特定す
る以外に、その構成を利用して、車両の誘導や検出の目
的にも利用可能である。
According to the first and second aspects of the present invention, it is possible to obtain an extremely high detection sensitivity and a high resistance to disturbances such as terrestrial magnetism and noise by a differential effect with respect to a plurality of component differences of a magnetic field. This magnetic field can be easily detected by a movable magnetic detector even with a single-turn loop or a single-wire excitation coil with the return line grounded. Therefore, it is possible to easily and accurately determine the position of the excitation coil in the invisible part such as underground from the ground, accurately propell the underground pipe toward the target, and trace the position of the unmanned propulsion machine from the ground. it can. Furthermore, the exciting coil is laid underground in the shape of a long rectangle or ellipse along the road, and this magnetic field is detected by a detector provided on a moving body such as an automobile, and the output is used to control the direction of the automobile. Can be controlled so as to travel along. As described above, the present invention can be used not only for specifying the position of the exciting coil in the invisible portion but also for the purpose of guiding and detecting the vehicle by using the configuration.

【0032】また請求項3項の発明は、上記請求項1項
及び2項の発明の効果に加え、励磁コイルの近くに導体
が接近したことを検出でき、これを車両検出器として利
用することが可能となる。
According to a third aspect of the present invention, in addition to the effects of the first and second aspects of the present invention, it is possible to detect that a conductor has approached the vicinity of an exciting coil, and to use this as a vehicle detector. Becomes possible.

【0033】また請求項4項の発明は、上記請求項1項
及び2項の発明の効果に加え、励磁コイルの励磁周波数
と異なる周波数を励磁コイルに重畳することにより位置
測定に際して測定点と被測定点とで通信を行うことがで
き、より正確に位置検出ができる。また励磁コイルを安
全な車間距離の間隔になるように道路に埋設し、それぞ
れの励磁コイルの一つ前方の励磁コイルが車両を検出し
ているか否かを、励磁信号と異なる周波数を重畳して伝
送し、この信号を車両に非接触で伝達すると、衝突防止
装置としても機能する。
According to a fourth aspect of the present invention, in addition to the effects of the first and second aspects of the present invention, a frequency different from the exciting frequency of the exciting coil is superimposed on the exciting coil so that the measuring point and the measuring point can be measured at the time of position measurement. Communication can be performed with the measurement point, and position detection can be performed more accurately. In addition, the excitation coil is buried in the road so as to have a safe inter-vehicle distance, and whether or not the excitation coil in front of each excitation coil detects the vehicle is superimposed with a frequency different from the excitation signal. When transmitted and transmitted in a non-contact manner to the vehicle, it also functions as a collision prevention device.

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

【図1】この発明の実施の形態例の第1原理説明図であ
る。
FIG. 1 is a diagram illustrating a first principle of an embodiment of the present invention.

【図2】この発明の実施の形態例の第2原理説明図であ
る。
FIG. 2 is an explanatory diagram of a second principle of the embodiment of the present invention.

【図3】この発明の実施の形態例の第3原理説明図であ
る。
FIG. 3 is an explanatory diagram of a third principle of the embodiment of the present invention.

【図4】この発明の実施の形態例の送信コイルにより発
生させた磁界の垂直成分及び水平成分を受信コイルで検
出した際の中心軸からの移動距離xに対する磁界強度を
表わすグラフ図である。
FIG. 4 is a graph showing a magnetic field intensity with respect to a moving distance x from a central axis when a vertical direction component and a horizontal direction component of a magnetic field generated by a transmission coil according to an embodiment of the present invention are detected by a reception coil;

【図5】この発明の実施の形態例に使用した装置の概略
構成図である。
FIG. 5 is a schematic configuration diagram of an apparatus used in an embodiment of the present invention.

【図6】この発明の実施の形態例の装置の各動作を説明
する出力波形図である。
FIG. 6 is an output waveform chart for explaining each operation of the device according to the embodiment of the present invention.

【図7】この発明の実施の形態例における地中に埋設ま
た掘削された推進管の先端の位置を地上から検出する例
を示す概要説明図である。
FIG. 7 is a schematic explanatory diagram showing an example in which the position of the tip of a propulsion pipe buried or excavated in the ground according to the embodiment of the present invention is detected from the ground.

【符号の説明】[Explanation of symbols]

A 受信機 B 駆動回路 C 送信機 1 受信コイル 2 抵抗 3 初段増幅器 4 同期スイッチ 5 差動増幅器 6 積分器 7 帰還補正減
衰器 8 反転増幅器(利得−1) 9 抵抗器 10 出力端子 11 水晶発振
器 12 分周器 13 タイミン
グ発生器 14 水平垂直切換え器 15 垂直軸駆
動回路 16 水平軸駆動回路 17 垂直磁界
コイル 18 水平磁界コイル 19 地中 20 推進管 21 垂直磁界
コイル 22 水平磁界コイル 23 駆動回路 24 受信コイル 25 受信機
Reference Signs List A Receiver B Drive circuit C Transmitter 1 Receiving coil 2 Resistor 3 First stage amplifier 4 Synchronous switch 5 Differential amplifier 6 Integrator 7 Feedback correction attenuator 8 Inverting amplifier (gain-1) 9 Resistor 10 Output terminal 11 Crystal oscillator 12 Frequency divider 13 Timing generator 14 Horizontal / vertical switch 15 Vertical axis drive circuit 16 Horizontal axis drive circuit 17 Vertical magnetic field coil 18 Horizontal magnetic field coil 19 Underground 20 Propulsion pipe 21 Vertical magnetic field coil 22 Horizontal magnetic field coil 23 Drive circuit 24 Receiving coil 25 Receiver

フロントページの続き (56)参考文献 特開 平10−82275(JP,A) 特開 平8−146145(JP,A) (58)調査した分野(Int.Cl.7,DB名) G01B 7/00 - 7/34 Continuation of the front page (56) References JP-A-10-82275 (JP, A) JP-A-8-146145 (JP, A) (58) Fields investigated (Int. Cl. 7 , DB name) G01B 7 / 00-7/34

Claims (4)

(57)【特許請求の範囲】(57) [Claims] 【請求項1】 被測定点に、交互に水平又は垂直方向の
磁界を発生させる複数の励磁コイルを設け、これらの励
磁コイルを励磁回路によって交互に励磁して交互に水平
又は垂直成分の交流磁界を発生させ、測定点では、水平
又は垂直方向の磁界を検出する複数の検出コイルを有す
る磁界検出器を設け、この検出器の位置を移動させて上
記それぞれの励磁タイミングに対する任意の点における
交流磁場と方向成分を検出してこれを電圧信号に変換
し、この電圧信号を上記励磁回路の励磁タイミングと同
期を取ったスイッチで選択して、水平励磁コイル及び垂
直励磁コイルのいずれか一方の励磁コイルから発生した
磁界成分による電圧信号と水平励磁コイル及び垂直励磁
コイルのいずれか他方の励磁コイルから発生した磁界成
分による電圧信号の二つの信号に分離し、これらの二つ
の信号を差動増幅器にかけ、この差動増幅器の出力が零
になる位置から励磁コイルの位置を求めることを特徴と
する、位置検出方法。
1. A plurality of exciting coils for alternately generating a horizontal or vertical magnetic field are provided at a point to be measured, and these exciting coils are alternately excited by an exciting circuit to alternately generate an alternating magnetic field of a horizontal or vertical component. At the measurement point, a magnetic field detector having a plurality of detection coils for detecting a magnetic field in the horizontal or vertical direction is provided, and the position of the detector is moved to change the AC magnetic field at an arbitrary point with respect to the respective excitation timings. And the direction component is detected and converted into a voltage signal, and this voltage signal is selected by a switch synchronized with the excitation timing of the excitation circuit, and either one of the horizontal excitation coil and the vertical excitation coil is selected. And the voltage signal due to the magnetic field component generated from either the horizontal excitation coil or the vertical excitation coil. A position detecting method comprising: separating the two signals into two signals; applying the two signals to a differential amplifier; and determining a position of the exciting coil from a position where the output of the differential amplifier becomes zero.
【請求項2】 被測定点から任意の距離に置かれ、交互
に水平又は垂直方向の磁界を発生させる複数の励磁コイ
ルを設け、これらの励磁コイルを励磁回路によって交互
に励磁して交互に水平又は垂直の交流磁界を発生させ、
測定点では、水平又は垂直方向の磁界を検出する複数の
検出コイルを有する磁界検出器を設け、この検出器の位
置を移動させて上記それぞれの励磁タイミングに対する
任意の点における交流磁場と方向成分を検出してこれを
電圧信号に変換し、この電圧信号を上記励磁回路の励磁
タイミングと同期を取ったスイッチで選択して、水平励
磁コイル及び垂直励磁コイルのいずれか一方の励磁コイ
ルから発生した磁界成分による電圧信号と水平励磁コイ
ル及び垂直励磁コイルのいずれか他方の励磁コイルから
発生した各磁界成分による電圧信号の二つの信号に分離
し、これらの二つの信号を差動増幅器にかけ、この作動
増幅器の出力が零になる位置から励磁コイルの位置を求
めることを特徴とする、位置検出方法。
2. A plurality of exciting coils which are placed at an arbitrary distance from a point to be measured and which alternately generate a magnetic field in a horizontal or vertical direction are provided, and these exciting coils are alternately excited by an exciting circuit to be alternately horizontal. Or generate a vertical alternating magnetic field,
At the measurement point, a magnetic field detector having a plurality of detection coils for detecting a magnetic field in the horizontal or vertical direction is provided, and the position of this detector is moved to change the AC magnetic field and the directional component at any point with respect to the respective excitation timings. This is detected and converted into a voltage signal, and this voltage signal is selected by a switch synchronized with the excitation timing of the excitation circuit, and the magnetic field generated from one of the horizontal excitation coil and the vertical excitation coil Component signal and a voltage signal due to each magnetic field component generated from one of the other excitation coils, the horizontal excitation coil and the vertical excitation coil, and these two signals are applied to a differential amplifier. A position of the exciting coil from a position at which the output of the excitation coil becomes zero.
【請求項3】 被測定点から任意の距離に置かれ、交互
に水平又は垂直方向の磁界を発生させる複数の励磁コイ
ルを設け、これらの励磁コイルを励磁回路によって交互
に励磁して交互に水平又は垂直の交流磁界を発生させ、
測定点では、それぞれの上記励磁コイルを遮断した直後
に励磁コイルの近傍の導体から発生する渦電流による磁
界を励磁コイルと同期を取った同期増幅器で選択的に検
出して、上記導体を検出するとともに、任意の点におけ
る交流磁場と方向成分を励磁コイルの近傍に設けた水平
又は垂直方向の磁界を検出する複数の検出コイルを有す
る磁界検出器で検出し、この信号を上記励磁回路と同期
を取った同期増幅器で増幅し、それぞれの励磁コイルに
よる任意の点の磁界強度を求め、水平励磁コイル及び垂
直励磁コイルのいずれか一方の励磁コイルから発生した
磁界成分による電圧信号と水平励磁コイル及び垂直励磁
コイルのいずれか他方の励磁コイルから発生した各磁界
成分による電圧信号の二つの信号に分離し、これらの二
つの信号を差動増幅器にかけ、この差動増幅器の出力が
零になる位置から励磁コイルの位置を求めることを特徴
とする、位置検出方法。
3. A plurality of excitation coils which are placed at an arbitrary distance from a point to be measured and generate alternately horizontal or vertical magnetic fields are provided, and these excitation coils are alternately excited by an excitation circuit to be alternately horizontal. Or generate a vertical alternating magnetic field,
At the measurement point, the conductor is detected by selectively detecting a magnetic field due to an eddy current generated from a conductor near the excitation coil by a synchronous amplifier synchronized with the excitation coil immediately after the respective excitation coils are cut off. In addition, an AC magnetic field and a directional component at an arbitrary point are detected by a magnetic field detector having a plurality of detection coils for detecting a magnetic field in a horizontal or vertical direction provided near the excitation coil, and this signal is synchronized with the excitation circuit. Amplified by the synchronous amplifier that was taken, the magnetic field strength at any point by each excitation coil was obtained, and the voltage signal due to the magnetic field component generated from either the horizontal excitation coil or the vertical excitation coil and the horizontal excitation coil and the vertical It separates into two signals of voltage signal by each magnetic field component generated from one of the exciting coils, and differentially increases these two signals. Subjected to vessel, the output of the differential amplifier and obtains the position of the excitation coil from the position becomes zero, the position detection method.
【請求項4】 励磁コイルの励磁周波数と異なる周波数
を励磁コイルに重畳し、位置検出や導体検出を行いなが
ら励磁コイルから検出コイルに任意信号を送ることを特
徴とする、上記請求項1項、2項、3項のうちのいずれ
か一つに記載の位置検出方法。
4. The apparatus according to claim 1, wherein a frequency different from the excitation frequency of the excitation coil is superimposed on the excitation coil, and an arbitrary signal is transmitted from the excitation coil to the detection coil while performing position detection and conductor detection. Item 3. The position detection method according to any one of Items 3 and 3.
JP8318570A 1996-11-15 1996-11-15 Position detection method Expired - Lifetime JP3063027B2 (en)

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US6172499B1 (en) * 1999-10-29 2001-01-09 Ascension Technology Corporation Eddy current error-reduced AC magnetic position measurement system
JP4615762B2 (en) * 2001-05-23 2011-01-19 株式会社日立国際電気 Moving object detection system
EP1843177A1 (en) * 2006-04-06 2007-10-10 Leica Geosystems AG Calibration method and calibration apparatus for a hand-held locating device
JP5004646B2 (en) * 2007-04-26 2012-08-22 旭化成エレクトロニクス株式会社 Position / orientation detection system, detection method thereof, and position / orientation detection apparatus
DE102009022992A1 (en) 2009-03-02 2010-10-07 Micro-Epsilon Messtechnik Gmbh & Co. Kg position sensor
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CN115012915B (en) * 2022-06-02 2023-01-24 中国石油天然气集团有限公司 Magnetic field positioning method, system, device, equipment and medium based on straight wire

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN104515462A (en) * 2014-12-23 2015-04-15 柳州柳工叉车有限公司 Displacement detection device and method

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