JPH09101373A - Method for searching buried object - Google Patents

Method for searching buried object

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Publication number
JPH09101373A
JPH09101373A JP26112995A JP26112995A JPH09101373A JP H09101373 A JPH09101373 A JP H09101373A JP 26112995 A JP26112995 A JP 26112995A JP 26112995 A JP26112995 A JP 26112995A JP H09101373 A JPH09101373 A JP H09101373A
Authority
JP
Japan
Prior art keywords
magnetic field
detection
detection coil
buried
buried object
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
JP26112995A
Other languages
Japanese (ja)
Other versions
JP2865599B2 (en
Inventor
Shin Yokoi
伸 横井
Kishiharu Okumura
興志治 奥村
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.)
Yokoi Manufacturing Co Ltd
Original Assignee
Yokoi Manufacturing Co 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 Yokoi Manufacturing Co Ltd filed Critical Yokoi Manufacturing Co Ltd
Priority to JP26112995A priority Critical patent/JP2865599B2/en
Publication of JPH09101373A publication Critical patent/JPH09101373A/en
Application granted granted Critical
Publication of JP2865599B2 publication Critical patent/JP2865599B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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  • Radar Systems Or Details Thereof (AREA)

Abstract

PROBLEM TO BE SOLVED: To accurately search a buried object by eliminating such influence as direct magnetic field from an oscillator by arranging a specific number of detection coils horizontally with a space in the up-and-down direction inside a transmitter. SOLUTION: Three detection coils C1 , C2 , and C3 are horizontally arranged in a receiver R being installed on the ground with spaces L1 and L2 in the vertical direction. By positioning the receiver R directly above a buried cable K so that an axial line ϕ is in the vertical direction to the cable K, the synthetic magnetic field between magnetic fields H1 , H2 , and H3 formed by a current I flowing to the cable K and a direct magnetic field H from an oscillator cross each other, and hence detection voltages V1 , V2 , and V3 in proportional to magnetic fields H1 +H, H2 +H, and H3 are induced at coils C1 , C2 , and C3 , respectively. Two sets of differential voltages are obtained from the detection voltages V1 , V2 , and V3 and a burial depth D is calculated under conditions where magnetic field constituents are canceled from the transmitter.

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】本発明は電磁誘導を利用した
埋設物の探査技術に関するものであり、地中に埋設され
た電話ケーブル、電力ケーブル、ガス管水道管等の導体
(以下単にケーブルと云う)の探査に利用する電磁誘導
方式の埋設物探査方法の改良に関するものである。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a technique for exploring buried objects using electromagnetic induction, and conductors such as telephone cables, power cables, gas pipes and water pipes buried in the ground (hereinafter simply referred to as cables). ) Related to the improvement of the electromagnetic induction type buried object exploration method used for exploration.

【0002】[0002]

【従来の技術】電磁誘導方式の埋設物探査方法は、通常
ケーブル等の埋設導体に交流電流を流し、この交流電流
によって発生した磁界を受信機器で検出することによ
り、ケーブルの直上位置やその埋設深さを探知するもの
であって、手軽に操作ができて比較的測定精度もよく、
しかもあらゆる場所で容易に適用できると云う極めて優
れた探査方法である。
2. Description of the Related Art An electromagnetic induction type buried object search method generally involves passing an alternating current through a buried conductor such as a cable, and detecting the magnetic field generated by this alternating current with a receiving device to detect the position directly above the cable or its buried position. It detects depth, can be operated easily, and has relatively good measurement accuracy.
Moreover, it is an extremely excellent exploration method that can be easily applied to any place.

【0003】而して、前記埋設物の探査方法では、埋設
ケーブル等の埋設導体に交流電流を流す方法として、次
の三種の方法が多く利用されている。 埋設ケーブルの地上露出部へ発振器の出力側を接続
し、交流電流を直接にケーブルへ流す方法。 リング状の磁性材料に巻線を施して形成した外磁ク
ランプを埋設ケーブルにクランプし、前記外磁クランプ
の巻線を一次巻線として、二次導体である埋設ケーブル
に誘導電流を起生せしめたようにしたクランプ法。 地上に設置した発振器から交番磁界を発信し、この
交番磁界によって埋設ケーブルに誘導電流を起生せしめ
るようにした誘導法。
In the method of exploring the buried object, the following three methods are often used as a method of passing an alternating current through a buried conductor such as a buried cable. A method in which the output side of the oscillator is connected to the exposed part of the buried cable above the ground, and an alternating current is passed directly to the cable. An outer magnet clamp formed by winding a ring-shaped magnetic material is clamped on the embedded cable, and the winding of the outer magnet clamp is used as the primary winding to generate an induced current in the embedded cable that is the secondary conductor. The clamp method that was used. An induction method in which an oscillator installed on the ground emits an alternating magnetic field, and this alternating magnetic field causes an induced current in the buried cable.

【0004】ところで、前記及びの方法は埋設ケー
ブルの一部分を露出させる必要があり、手数がかかるう
えに施工場所が制約されるため、適用性に欠けると云う
難点がある。これに対して、前記の誘導法は、地表上
に発振器を設置するだけで簡単に適用することができ、
高い実用性を具備するものである。
By the way, the above-mentioned methods and methods require a part of the buried cable to be exposed, which is troublesome and restricts the construction site. On the other hand, the above-mentioned induction method can be easily applied only by installing an oscillator on the ground surface,
It has high practicality.

【0005】しかし、当該誘導法にも下記のような問題
点が内存する。 埋設ケーブルに誘導される誘導電流が小さいため、
大きな発振器出力を要すること。 発振器からの送信磁界の一部が、受信器によって直
接に受信され易いため、発振器と受信器間の距離が十分
に取れる場合にしか適用できないこと。
However, the following problems are inherent in the induction method. Since the induced current induced in the buried cable is small,
Requires a large oscillator output. Applicable only when the distance between the oscillator and the receiver is sufficient, because a part of the transmitted magnetic field from the oscillator is easily received directly by the receiver.

【0006】図5は、前記電磁誘導方式による従前の埋
設物探査の基本原理の一例を示すものであり、図に於い
てKは埋設ケーブル、Iは埋設ケーブルに流れる電流、
1、C2 は検出コイル、H1 、H2 は電流Iによる交
番磁界、Hは発振器から発信された直接磁界(又は外部
ノイズ磁界)、Lは検出コイル間隔、Dは埋設深さ(下
方の検出コイルC2 とケーブルKとの間隔)である。
FIG. 5 shows an example of the basic principle of a conventional buried object search by the electromagnetic induction method. In the figure, K is a buried cable, I is a current flowing through the buried cable,
C 1 and C 2 are detection coils, H 1 and H 2 are alternating magnetic fields due to the current I, H is a direct magnetic field (or external noise magnetic field) emitted from an oscillator, L is a detection coil interval, and D is a buried depth (lower). Of the detection coil C 2 and the cable K).

【0007】図5のように2本のコイルC1 、C2 を埋
設ケーブルKの直上に距離Lの間隔で配置し、コイル軸
を大地と平行とした状態でコイルC1 、C2 の検出電圧
をV 1 、V2 とすると、深さDは、D=L・V1 /(V
2 −V1 )で求める事ができる。ここで、前記V1 は誘
導電流Iによる磁界H1 と発振器からの直接磁界Hとの
合成磁界に比例し、同様にV2 は磁界H1 と直接磁界H
との合成磁界に比例する。また、前記(1)式の分母は
2 とV1 の差動電圧となり、直接磁界Hの影響は打ち
消される。これに対して、L・V1 なる分子は、直接磁
界Hの影響がそのまま存在し、したがって、前記深さD
の計算式には誤差要因が存在する事となる。その結果、
誘導法における深さの測定では、多くの場合深さDは、
深めの測定値を示すことになる。
Two coils C as shown in FIG.1, CTwoBuried
Arranged directly above the installation cable K at a distance of L, and
Coil with C parallel to the ground1, CTwoDetection voltage
To V 1, VTwoThen, the depth D is D = LV1/ (V
Two-V1) Can be requested. Where V1Is an invitation
Magnetic field H due to conductive current I1And the direct magnetic field H from the oscillator
Proportional to the composite magnetic field, and similarly VTwoIs the magnetic field H1And the direct magnetic field H
Proportional to the combined magnetic field of and. Also, the denominator of the above formula (1) is
VTwoAnd V1The differential voltage of
Be erased. On the other hand, L ・ V1Becomes a direct magnet
The influence of the field H exists as it is, and therefore the depth D
There is an error factor in the calculation formula of. as a result,
In the depth measurement in the induction method, the depth D is often
It will give a deeper measurement.

【0008】一方、上述のような誘導法を用いた場合の
直接磁界Hに起因する測定誤差を避けるため、送信磁界
(直接磁界H)と誘導磁界H1 、H2 との間に図6に示
す如く理論上90°の位相差があることに着目し、発
振器と受信器を有線あるいは無線で結合して、送信磁界
Hの位相を受信器側に送信し、これに基づいて検出磁
界を送信磁界成分Hと誘導電流Iによる磁界成分H
1 (又はH2 )に分解し、その後誘導電流Iによる磁
界成分H1 (又はH2 )を用いて深さDを算出する方法
が試みられている。
On the other hand, in order to avoid a measurement error caused by the direct magnetic field H when the above-mentioned induction method is used, FIG. 6 is shown between the transmission magnetic field (direct magnetic field H) and the induction magnetic fields H 1 and H 2 . Paying attention to the theoretical phase difference of 90 ° as shown, the oscillator and the receiver are connected by wire or wirelessly, and the phase of the transmission magnetic field H is transmitted to the receiver side, and the detection magnetic field is transmitted based on this. Magnetic field component H and magnetic field component H due to induced current I
A method has been attempted in which the depth D is decomposed into 1 (or H 2 ) and then the magnetic field component H 1 (or H 2 ) due to the induced current I is used to calculate the depth D.

【0009】しかし、この方法にも、発振器と受信器
を有線あるいは無線で結合する必要があって装置が複雑
になること、送信器と受信器の距離が変わると埋設ケ
ーブルの電気的特性によって90°の位相差から変わる
可能性があること、周囲に探査ケーブル以外の導体が
存在する場合にも位相ずれが発生すること(90°の位
相差からずれると検出磁界を送信磁界成分と誘導電流に
よる磁界成分に分解することが不可能となる)等の問題
が残されている。
However, in this method as well, it is necessary to connect the oscillator and the receiver in a wired or wireless manner, which complicates the device, and when the distance between the transmitter and the receiver changes, the electrical characteristics of the buried cable may cause a problem. There is a possibility that it will change from the phase difference of °, and a phase shift will occur even if there is a conductor other than the probe cable in the surroundings. (It becomes impossible to decompose into magnetic field components).

【0010】[0010]

【発明が解決しようとする課題】本願発明は、主として
従前の誘導法を用いた電磁誘導方式の埋設物探査に於け
る上述の如き問題、即ち発振器からの直接磁界が原因
で、受信器側の検出精度が低下すること、発振器から
の直接磁界に起因する検出誤差を少なくするためには、
発振器と受信器を大きく引き離す必要があり、検出作業
が実施し難くなること、発振器からの直接磁界に起因
する検出誤差を補正する方法は、埋設物探査装置そのも
のの製造コストが上昇するうえ、検出精度を十分に且つ
安定的に高めることが困難なこと等の問題を解決せんと
するものであり、受信器側に3個の検出コイルC1 、C
2 、C3 を設けると共に、各検出コイルC1 、C2 、C
3 の検出電圧V1 、V2 、V3 から二組の差動電圧を求
め、発振器からの直接磁界成分を打ち消しした条件下で
埋設深さDを算出することにより、構造が簡単で探査装
置の製造コストの大幅な高騰を招くことなしに、極めて
高精度な埋設物探査を行えるようにした電磁誘導方式の
埋設物探査方法を提供するものである。
SUMMARY OF THE INVENTION The invention of the present application is mainly due to the above-mentioned problem in the electromagnetic induction type buried object search using the conventional induction method, that is, due to the direct magnetic field from the oscillator. To reduce the detection accuracy and the detection error due to the direct magnetic field from the oscillator,
Since it is necessary to separate the oscillator and the receiver greatly, it becomes difficult to carry out the detection work, and the method of correcting the detection error due to the direct magnetic field from the oscillator increases the manufacturing cost of the buried object exploration device itself and It is intended to solve problems such as difficulty in sufficiently and stably increasing accuracy, and three detection coils C 1 and C on the receiver side.
2 and C 3 are provided, and each detection coil C 1 , C 2 , C
The structure is simple and the exploration device is obtained by calculating two sets of differential voltages from the detection voltages V 1 , V 2 and V 3 of 3 and calculating the burial depth D under the condition in which the direct magnetic field component from the oscillator is canceled. The present invention provides an electromagnetic induction type buried object exploration method capable of performing extremely accurate exploration of an embedded object without causing a significant increase in manufacturing cost.

【0011】[0011]

【課題を解決するための手段】本願請求項1に記載の発
明は、埋設物に電流を流し、当該電流による交番磁界を
地上の受信器で検出することにより埋設物を探査する方
法に於いて、前記受信器内部に上下方向に間隔を置いて
三個の検出コイルを水平状に配置し、二組の検出コイル
の組み合せについて夫々検出コイル間の差動電圧を求
め、次に、前記二つの差動電圧を夫々増幅し、各増幅度
を調整することにより、差動電圧×増幅度の積が夫々等
しくなるようにし、その時の各増幅度と各検出コイルの
上・下方向の間隔とから埋設物の埋設深さを演算するこ
とを発明の基本構成とするものである。
The invention according to claim 1 of the present invention is a method for exploring a buried object by passing a current through the buried object and detecting an alternating magnetic field due to the current with a receiver on the ground. , Three detection coils are horizontally arranged inside the receiver at intervals in the vertical direction, and a differential voltage between the detection coils is obtained for a combination of two sets of detection coils. By amplifying each differential voltage and adjusting each amplification factor, the product of differential voltage x amplification factor is made equal, and each amplification factor at that time and the upper and lower intervals of each detection coil The calculation of the buried depth of the buried object is the basic configuration of the invention.

【0012】また、本願請求項3に記載の発明は、埋設
物に電流を流し、当該電流による交番磁界を地上の受信
器で検出することにより埋設物を探査する方法に於い
て、前記受信器内部に上下方向に間隔を置いて三個の検
出コイルを水平状に配置すると共に、中間に位置する検
出コイルを上下方向へ移動自在に支持し、前記中間に位
置する検出コイルの上下方向位置を調整して、下方に位
置する検出コイルと中間に位置する検出コイル間の差動
電圧(V3 −V2 )と、中間に位置する検出コイルと上
方に位置する検出コイル間の差動電圧(V2 −V1 )と
の差が最小となるようにし、前記両差動電圧の差が最小
の状態に於ける各検出コイル間の距離から埋設物の埋設
深さを演算することを発明の基本構成とするものであ
る。
Further, the invention according to claim 3 is a method for exploring an embedded object by causing an electric current to flow through the embedded object and detecting an alternating magnetic field due to the current with a receiver on the ground. The three detection coils are horizontally arranged at intervals in the vertical direction, and the detection coil in the middle is movably supported in the vertical direction, and the vertical position of the detection coil in the middle is determined. The differential voltage (V 3 −V 2 ) between the detection coil located below and the detection coil located in the middle, and the differential voltage between the detection coil located in the middle and the detection coil located above (V 3 −V 2 ). V 2 −V 1 ) is minimized, and the buried depth of the buried object is calculated from the distance between the detection coils when the difference between the two differential voltages is the minimum. It has a basic configuration.

【0013】[0013]

【発明の実施の形態】以下、図面に基づいて本発明の実
施の形態を説明する。図1は本発明の第1実施形態の基
本原理の説明図である。地上に設置する受信器Rには上
下方向に間隔L1 、L2 を置いて3個の検出コイル
1 、C2 、C3が同一軸線φ上に軸線φと垂直状(即
ち、大地面Eと水平状)に配設されている。今、図1に
示すように、受信器Rを埋設ケーブルKの直上に、その
軸線φがケーブルKと垂直方向になるように位置せしめ
ると、各検出コイルC1 、C2 、C 3 には、埋設ケーブ
ルKに流れる電流Iの作る磁界H1 、H2 、H3 と発振
器(図示省略)からの直接磁界Hとの合成磁界が夫々鎖
交し、その結果各検出コイルC1 、C2 、C3 には磁界
1 +H、H2 +H、H3 +Hに比例した検出電圧
1 、V2 、V3 が夫々誘起することになる。尚、上記
各検出コイルC1 、C2 、C3 は夫々電気的に同じ特性
を持つように形成されているのが望ましい。
BRIEF DESCRIPTION OF THE DRAWINGS FIG.
An embodiment will be described. FIG. 1 shows the base of the first embodiment of the present invention.
It is explanatory drawing of this principle. Above the receiver R installed on the ground
Space L downward1, LTwoPut three detector coils
C1, CTwo, CThreeAre on the same axis φ and perpendicular to the axis φ (immediately
It is arranged horizontally with the ground E). Now in Figure 1
As shown, place the receiver R directly above the buried cable K
Position the axis φ so that it is perpendicular to the cable K.
Then, each detection coil C1, CTwo, C ThreeThe buried cave
Magnetic field H created by current I flowing through1, HTwo, HThreeAnd oscillation
Magnetic field combined with direct magnetic field H from the container (not shown)
As a result, each detection coil C1, CTwo, CThreeIn the magnetic field
H1+ H, HTwo+ H, HThreeDetection voltage proportional to + H
V 1, VTwo, VThreeWill be induced respectively. The above
Each detection coil C1, CTwo, CThreeHave the same electrical characteristics
It is desirable to be formed to have.

【0014】今ここで、検出コイルC3 と検出コイルC
2 との差動電圧V3 −V2 及び検出コイルC2 と検出コ
イルC1 との差動電圧V2 −V1 を、差動回路を用いた
り、或いは検出コイルC2 の巻線方向を検出コイル
1 、C3 と逆巻きとすることによって検出すると、V
3 −V2 及びV2 −V1 の値は、発振器からの直接磁界
Hに比例する電圧成分が打ち消されたものとなり、電流
Iによる磁界H1 、H2 、H3 に比例した電圧成分のみ
となる。
Now, the detection coil C 3 and the detection coil C
2 differential voltage V 3 -V 2 and a detection coil C 2 of the differential voltage V 2 -V 1 and the detection coils C 1, or a differential circuit, or the winding direction of the detection coil C 2 When it is detected by making the detection coil C 1 and C 3 reversely wound, V
3 The value of -V 2 and V 2 -V 1 is made shall voltage component directly proportional to the magnetic field H from the oscillator is countered, only the voltage component proportional to the magnetic field H 1, H 2, H 3 due to the current I Becomes

【0015】ところで、前記各検出コイルC1 、C2
3 の設置位置に発生する電流Iによる磁界H1
2 、H3 は、前記電流Iの大きさをiとすると、下記
の(1)、(2)、(3)式で与えられる。 H1 =i/2π(D+L1 +L2 )…… (1) H2 =i/2π(D+L2 ) …… (2) H3 =i/2πD …… (3) そして、前記差動電圧V3 −V2 及びV2 −V1 の値を
夫々プログラマプルな電圧増幅器を用いて増幅し、その
増幅度をA1 、A2 を調整して下記の(4)式の関係が
成立するようにする。 A1 ・(V3 −V2 )=A2 ・(V2 −V1 )…… (4)
By the way, each of the detection coils C 1 , C 2 ,
Magnetic field H 1 due to current I generated at the installation position of C 3 ,
H 2 and H 3 are given by the following equations (1), (2) and (3), where i is the magnitude of the current I. H 1 = i / 2π (D + L 1 + L 2 ) (1) H 2 = i / 2π (D + L 2 ) (2) H 3 = i / 2πD (3) And the differential voltage V The values of 3- V 2 and V 2 -V 1 are amplified by using programmable voltage amplifiers respectively, and the amplification degree is adjusted to A 1 and A 2 so that the relation of the following equation (4) is established. To A 1 · (V 3 −V 2 ) = A 2 · (V 2 −V 1 ) ... (4)

【0016】一方、前述の通り差動電圧V3 −V2 はH
3 −H2 に、また差動電圧V2 −V 1 はH2 −H1 に夫
々比例することになるため、前記(1)〜(4)からケ
ーブルKの埋設深さDを求めると、埋設深さDは下記の
(5)式で与えられる。 D=(L1 +L2 )/(A1 /A2 )・(L1 /L2 )−1……(5) 即ち、埋設ケーブルKの埋設深さDは(4)式を成立さ
せる増幅度A1 、A2を求めることにより、(5)式を
用いて演算することができる。
On the other hand, as described above, the differential voltage VThree-VTwoIs H
Three-HTwoAnd the differential voltage VTwo-V 1Is HTwo-H1Husband
Since they are proportional to each other, the above steps (1) to (4)
When the burial depth D of the cable K is obtained, the burial depth D is
It is given by the equation (5). D = (L1+ LTwo) / (A1/ ATwo) ・ (L1/ LTwo) -1 (5) That is, the buried depth D of the buried cable K satisfies the formula (4).
Amplification A1, ATwoBy calculating
It can be calculated using.

【0017】前記図1に於いては、プログラブルな電圧
増幅器を利用し、その増幅度A1 、A2 を調整すること
により前記(4)式を成立させるようにしたが、図2に
示すように、中央に位置する検出コイルC2 を水平姿勢
で保持しつつ軸線φに沿って上下方向へ移動可能な構成
とし、検出コイルC2 を移動させ乍ら、差動電圧V3
2 と差動電圧V2 −V1 とが等しく(又は両者の差が
最小となる)なる位置を求めるようにしてもよい。今、
図2に於いて、V3 −V2 =V2 −V1 ……(6)式が
成立したときの検出コイルC1 、C2 及びC2 、C3
の位置をL1 ′、L2 ′とすると、深さDは(1)〜
(3)及び(6)式から、下記の(7)式により与えら
れる。 D=(L1 +L2 )/(L1 ′/L2 ′)−1…… (7)
In FIG. 1, a programmable voltage amplifier is used, and the amplification degree A 1 , A 2 is adjusted to satisfy the equation (4). As described above, the detection coil C 2 located at the center is configured to be movable in the vertical direction along the axis φ while being held in the horizontal posture. When the detection coil C 2 is moved, the differential voltage V 3
A position where V 2 and the differential voltage V 2 −V 1 are equal (or the difference between them is minimized) may be obtained. now,
In FIG. 2, the positions of the detection coils C 1 , C 2 and C 2 , C 3 when V 3 −V 2 = V 2 −V 1 (6) are established are L 1 ′, L Assuming 2 ', the depth D is (1) ~
From the expressions (3) and (6), it is given by the following expression (7). D = (L 1 + L 2 ) / (L 1 ′ / L 2 ′) −1 (7)

【0018】即ち、前記(5)及び(7)式は発振器か
らの直接磁界Hの成分を打ち消した条件で埋設ケーブル
Kの深さDを算出出来る事を示し、測定精度が向上する
ことにより、これまで発振器と受信器R間の距離が十分
に取れる時のみ適用可能であった誘導法による探査が、
発振器の近くでも可能となる。また、センサーであるコ
イル部でノイズ磁界成分をキャンセル出来る事により、
後段に続く電子回路の簡略化が行なえる。
That is, the above equations (5) and (7) show that the depth D of the buried cable K can be calculated under the condition that the component of the magnetic field H directly from the oscillator is canceled, and the measurement accuracy is improved. The exploration by the guidance method, which was previously applicable only when the distance between the oscillator and the receiver R was sufficiently large,
It is possible near the oscillator. Also, because the noise magnetic field component can be canceled by the coil part that is the sensor,
The electronic circuit that follows can be simplified.

【0019】尚、前記図1及び図2に示した本発明の実
施態様は、発振器からの発信磁界によって埋設ケーブル
Kに誘導電流を発生させるようにした所謂誘導法による
埋設物探査法のみならず、埋設ケーブルKへ直接に電流
を供給するようにした場合に於いても、外部ノイズ磁界
の影響が排除されるため、優れた効用を奏するものであ
る。
The embodiment of the present invention shown in FIGS. 1 and 2 is not limited to the so-called inductive method for exploring the buried object in which the induced current is generated in the buried cable K by the magnetic field emitted from the oscillator. Even in the case where the electric current is directly supplied to the buried cable K, the effect of the external noise magnetic field is eliminated, so that the excellent effect is achieved.

【0020】(実施例1)図3は、前記図1で示した本
願発明の実施に使用する埋設物探査装置の受信器Rのブ
ロック構成図である。図3に於いて、C1 、C2 、C3
は検出コイル、4a、4b、4cは増幅器、5a、5b
は差動増幅器、6a、6bはフィルタ、7a、7bはA
C/DC変換器、8はDA変換器、9は比較器、10は
クロック発振器、11は論理ゲート、12はカウンタ、
13は演算カウンタ、14は表示部である。
(Embodiment 1) FIG. 3 is a block diagram of a receiver R of the buried object exploration apparatus used for implementing the present invention shown in FIG. In FIG. 3, C 1 , C 2 , C 3
Is a detection coil, 4a, 4b and 4c are amplifiers, 5a and 5b
Is a differential amplifier, 6a and 6b are filters, and 7a and 7b are A
C / DC converter, 8 DA converter, 9 comparator, 10 clock oscillator, 11 logic gate, 12 counter,
Reference numeral 13 is a calculation counter, and 14 is a display unit.

【0021】図3に基づいて、作動の概要を説明する
と、検出コイルC1 、C2 、C3 の出力信号は増幅器4
a、4b、4cによって電圧増幅され、差動増幅器5
a、5bでそれぞれコイルC2 とC1 、コイルC3 とC
2 の差動電圧を得る。差動増幅器5a、5bの出力は、
フィルター6a、6bを通して信号成分の分離を行った
あと、AC/DCコンバータ7a、7bによって交流か
ら直流に変換される。DA変換器8、比較器9、クロッ
ク発振器10、論理ゲート11、カウンタ12はプログ
ラマブルな増幅器を構成する。D/A変換器8の出力と
AC/DC変換器7bの出力は比較器9によって比較さ
れ、D/A変換器8とAC/DC変換器7bの出力値が
異なる時、論理ゲート11を開いてクロック発振器10
の出力をカウンタ12に入力する。カウンタ12の出力
はD/A変換器8の出力を制御し、AC/DC変換器7
bの出力と一致した時、論理ゲートを閉じてカウンタ1
2の動作を停止させる。この時、カウンタ12の出力は
(5)式の(A1 /A2 )の値を与える事となり、演算
回路13で深度が計算され、表示部14によって表示さ
れる。
An outline of the operation will be described with reference to FIG. 3. The output signals of the detection coils C 1 , C 2 and C 3 are output from the amplifier 4.
The voltage is amplified by a, 4b, and 4c, and the differential amplifier 5
a and 5b are coils C 2 and C 1 , and coils C 3 and C, respectively.
Get the differential voltage of 2 . The outputs of the differential amplifiers 5a and 5b are
After the signal components are separated through the filters 6a and 6b, the AC / DC converters 7a and 7b convert the AC to DC. The DA converter 8, the comparator 9, the clock oscillator 10, the logic gate 11, and the counter 12 form a programmable amplifier. The output of the D / A converter 8 and the output of the AC / DC converter 7b are compared by the comparator 9, and when the output values of the D / A converter 8 and the AC / DC converter 7b are different, the logic gate 11 is opened. Clock generator 10
Is input to the counter 12. The output of the counter 12 controls the output of the D / A converter 8, and the output of the AC / DC converter 7
When the output of b matches, the logic gate is closed and the counter 1
The operation of 2 is stopped. At this time, the output of the counter 12 gives the value of (A 1 / A 2 ) in the equation (5), the arithmetic circuit 13 calculates the depth, and the display unit 14 displays the depth.

【0022】(実施例2)図4は、前記図2で示した本
願発明の実施に使用する埋設物探査装置の受信器のブロ
ック構成図である。図4に於いて、4a、4b、4cは
増幅器、5a、5b、5cは差動増幅器、6a、6bは
フィルタ、7a、7bはAC/DCコンバータ、14は
表示部、15は深度目盛板である。
(Embodiment 2) FIG. 4 is a block diagram of a receiver of the buried object exploration apparatus used for implementing the present invention shown in FIG. In FIG. 4, 4a, 4b and 4c are amplifiers, 5a, 5b and 5c are differential amplifiers, 6a and 6b are filters, 7a and 7b are AC / DC converters, 14 is a display unit, and 15 is a depth scale plate. is there.

【0023】而して、検出コイルC1 、C2 、C3 の出
力信号は増幅器4a、4b、4cによって電圧増幅さ
れ、差動増幅器5a、5bで夫々コイルC2 とC1 間及
びコイルC3 とC2 間の差動電圧を得る。前記差動増幅
器5a、5bの出力は、フィルタ6a、6bを通して信
号成分の分離を行なったあと、AC/DCコンバータ7
a、7bにより交流から直流に変換される。また、AC
/DC変換器7a、7bの出力は差動増幅器5cによっ
て差動増幅され、差動電圧は表示部14によって表示さ
れる。操作者は、表示部14を見ながら中央のコイルC
2 を上下方向に動かし、表示部14に表示される指示値
が最小になる所でコイルC2 を固定する。深度目盛板1
5上には深度を表示する目盛が印してあり、コイルC2
の固定位置から深度目盛板15で直接深度Dを読み取
る。
Thus, the output signals of the detection coils C 1 , C 2 , C 3 are voltage-amplified by the amplifiers 4a, 4b, 4c, and are differential amplifiers 5a, 5b between the coils C 2 and C 1 and the coil C, respectively. Obtain the differential voltage between 3 and C 2 . The outputs of the differential amplifiers 5a and 5b are separated into signal components through filters 6a and 6b, and then the AC / DC converter 7
AC is converted to DC by a and 7b. AC
The outputs of the / DC converters 7a and 7b are differentially amplified by the differential amplifier 5c, and the differential voltage is displayed by the display unit 14. The operator looks at the display unit 14 and looks at the central coil C.
2 is moved up and down, and the coil C 2 is fixed at the place where the indicated value displayed on the display unit 14 becomes the minimum. Depth scale 1
A scale indicating depth is marked on the coil 5, and the coil C 2
The depth D is directly read from the fixed position of the depth scale plate 15.

【0024】[0024]

【発明の効果】本願請求項1乃至請求項3の発明に於い
ては、二組のコイルの組み合せについて夫々検出コイル
間の電圧を求め、両差動電圧を基礎にして埋設物の埋設
深さを演算するようにしている。即ち、発振器からの直
接磁界Hや外部ノズル磁界による影響が全て相殺された
検出値を用いて、埋設深さDの演算を行うようにしてい
るため、演算精度が著しく向上すると共に、発振器と受
信器R間の距離が短い場合に於いても、埋設物の探査を
高精度で実施することができる。また、請求項2の発明
に於いては、両差動電圧を増幅する増幅器の増幅度を調
整するだけで容易に埋設深さDを求めることができ、取
扱性に優れた自動埋設物探査が可能となる。更に、請求
項3の発明に於いては、中間に位置する検出コイルの上
・下位置調整だけで埋設深さDを直読することができる
うえ、受信器の電子回路等の大幅な簡素化が可能とな
る。本発明は上述の通り、優れた実用的効用を奏するも
のである。
According to the inventions of claims 1 to 3, the voltage between the detection coils is obtained for each of the combinations of the two coils, and the buried depth of the buried object is based on both differential voltages. Is calculated. That is, since the buried depth D is calculated by using the detection value in which the effects of the direct magnetic field H from the oscillator and the external magnetic field of the nozzle are all canceled, the calculation accuracy is significantly improved and the oscillator and the receiver Even if the distance between the vessels R is short, the buried object can be searched with high accuracy. Further, in the invention of claim 2, the buried depth D can be easily obtained only by adjusting the amplification degree of the amplifier that amplifies both differential voltages, and the automatic buried object search excellent in handleability can be realized. It will be possible. Further, in the invention of claim 3, the buried depth D can be directly read only by adjusting the upper and lower positions of the detection coil positioned in the middle, and the electronic circuit of the receiver can be greatly simplified. It will be possible. As described above, the present invention has excellent practical utility.

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

【図1】請求項1の発明に於ける埋設物探査の基本原理
の説明図である。
FIG. 1 is an explanatory diagram of a basic principle of buried object exploration according to the invention of claim 1.

【図2】請求項3の発明に於ける埋設物探査の基本原理
の説明図である。
FIG. 2 is an explanatory view of the basic principle of exploration of a buried object in the invention of claim 3;

【図3】請求項1の発明の実施に使用する受信器のブロ
ック構成図である。
FIG. 3 is a block diagram of a receiver used to implement the invention of claim 1.

【図4】請求項3の発明の実施に使用する受信器のブロ
ック構成図である。
FIG. 4 is a block diagram of a receiver used to implement the invention of claim 3;

【図5】従前の電磁誘導方式の埋設物探査装置を用いた
埋設物探査の基本原理の説明図である。
FIG. 5 is an explanatory diagram of a basic principle of a buried object search using a conventional electromagnetic induction type buried object search apparatus.

【図6】誘導法による場合の送信磁界と誘導磁界と検出
磁界の関係を示す説明図である。
FIG. 6 is an explanatory diagram showing a relationship between a transmission magnetic field, an induction magnetic field, and a detection magnetic field when the induction method is used.

【符号の説明】[Explanation of symbols]

K は 埋設ケーブル I は 電流(交流) R は 受信器 C1 、C2 、C3 は検出コイル H1 、H2 、H3 は電流Iによる磁界 H は 発振器からの直接磁界 V1 、V2 、V3 は各検出コイルの検出電圧 L1 、L2 は 各検出コイルC1 、C2 、C3 間の距
離 D は 検出コイルC2 とケーブル間の距離
(埋設深さ) φ は 受信器の垂直軸線 E は 大地面 4a、4b、4cは増幅器 5a、5b は差動増幅器 6a、6b はフィルタ 7a、7b はAC/DC変換器 8 は DA変換器 9 は 比較器 10 は クロック発振器 11 は 論理ゲート 12 は カウンタ 13 は 演算回路 14 は 表示部 15 は 深度目盛板。
K is the buried cable I is the current (alternating current) R is the receiver C 1 , C 2 , C 3 is the detection coil H 1 , H 2 , H 3 is the magnetic field due to the current I H is the direct magnetic field from the oscillator V 1 , V 2 , V 3 is the detection voltage of each detection coil L 1 , L 2 is the distance between each detection coil C 1 , C 2 , C 3 D is the distance between the detection coil C 2 and the cable (buried depth) φ is the receiver Vertical axis E is the ground plane 4a, 4b, 4c is an amplifier 5a, 5b is a differential amplifier 6a, 6b is a filter 7a, 7b is an AC / DC converter 8 is a DA converter 9 is a comparator 10 is a clock oscillator 11 is A logic gate 12, a counter 13, an arithmetic circuit 14, a display unit 15, and a depth scale plate.

Claims (3)

【特許請求の範囲】[Claims] 【請求項1】 埋設物に電流を流し、当該電流による交
番磁界を地上の受信器で検出することにより埋設物を探
査する方法に於いて、前記受信器内部に上下方向に間隔
を置いて三個の検出コイルを水平状に配置し、二組の検
出コイルの組み合せについて夫々検出コイル間の差動電
圧を求め、次に、前記二つの差動電圧を夫々増幅し、各
増幅度を調整することにより、差動電圧×増幅度の積が
夫々等しくなるようにし、その時の各増幅度と各検出コ
イルの上・下方向間隔とから埋設物の埋設深さを演算す
ることを特徴とする埋設物の探査方法。
1. A method for exploring a buried object by passing an electric current through the buried object and detecting an alternating magnetic field due to the current with a receiver on the ground, wherein three spaces are vertically provided inside the receiver. The detection coils are arranged horizontally, the differential voltage between the detection coils is obtained for each combination of the two detection coils, and then the two differential voltages are amplified respectively to adjust each amplification degree. By doing so, the product of differential voltage × amplification is made equal, and the buried depth of the buried object is calculated from each amplification at that time and the spacing between the detection coils in the up / down direction. How to search for things.
【請求項2】 二組の差動電圧を、下方に位置する検出
コイルと中間に位置する検出コイル間の差動電圧(V3
−V2 )及び中間に位置する検出コイルと上方に位置す
る検出コイル間の差動電圧(V2 −V1 )とし、前記両
差動電圧の増幅器の増幅度A1 及び増幅度A2 を調整す
ることにより、A1 (V3 −V2 )=A2 (V2
1 )の関係を成立させるようにした請求項1に記載の
埋設物の探査方法。
2. A differential voltage (V 3 between a detection coil located below and a detection coil located in the middle)
-V 2 ) and the differential voltage (V 2 -V 1 ) between the detection coil positioned in the middle and the detection coil positioned above, and the amplification degree A 1 and the amplification degree A 2 of the amplifiers of the both differential voltages are By adjusting, A 1 (V 3 −V 2 ) = A 2 (V 2
The buried object exploration method according to claim 1, wherein the relationship of V 1 ) is established.
【請求項3】 埋設物に電流を流し、当該電流による交
番磁界を地上の受信器で検出することにより埋設物を探
査する方法に於いて、前記受信器内部に上下方向に間隔
を置いて三個の検出コイルを水平状に配置すると共に、
中間に位置する検出コイルを上下方向へ移動自在に支持
し、前記中間に位置する検出コイルの上下方向位置を調
整して、下方に位置する検出コイルと中間に位置する検
出コイル間の差動電圧(V3 −V2 )と、中間に位置す
る検出コイルと上方に位置する検出コイル間の差動電圧
(V2 −V1 )との差が最小となるようにし、前記両差
動電圧の差が最小の状態に於ける各検出コイル間の距離
から埋設物の埋設深さを演算することを特徴とする埋設
物の探査方法。
3. A method for exploring a buried object by causing an electric current to flow through the buried object and detecting an alternating magnetic field due to the current with a receiver on the ground. While arranging the individual detection coils horizontally,
A differential voltage between the detection coil located below and the detection coil located in the middle is supported by movably supporting the detection coil located in the middle in the vertical direction and adjusting the vertical position of the detection coil located in the middle. The difference between (V 3 −V 2 ) and the differential voltage (V 2 −V 1 ) between the detection coil located in the middle and the detection coil located above is minimized, and A method for exploring a buried object, which comprises calculating a buried depth of a buried object from a distance between respective detection coils in a state where the difference is minimum.
JP26112995A 1995-10-09 1995-10-09 Exploration methods for buried objects Expired - Lifetime JP2865599B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP26112995A JP2865599B2 (en) 1995-10-09 1995-10-09 Exploration methods for buried objects

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP26112995A JP2865599B2 (en) 1995-10-09 1995-10-09 Exploration methods for buried objects

Publications (2)

Publication Number Publication Date
JPH09101373A true JPH09101373A (en) 1997-04-15
JP2865599B2 JP2865599B2 (en) 1999-03-08

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ID=17357505

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Publication number Priority date Publication date Assignee Title
GB2458121A (en) * 2008-03-03 2009-09-09 Radiodetection Ltd A detector for calculating a depth of a buried conductor
WO2013036686A1 (en) * 2011-09-06 2013-03-14 Ray Merewether Systems and methods for locating buried or hidden objects using sheet current flow models
US8566043B2 (en) 2008-03-03 2013-10-22 Radiodetection Limited Detector for calculating the distortion of an electromagnetic field produced by a buried current carrying conductor
JP2014215066A (en) * 2013-04-23 2014-11-17 高千穂産業株式会社 Method for measuring position of long-size article
CN104154856A (en) * 2013-05-13 2014-11-19 雷迪有限公司 Electronic marker locator systems and methods
JP2015111109A (en) * 2013-11-01 2015-06-18 株式会社沖縄中央エンジニアリング Detection method of magnetic matter and magnetic sensor
US9131693B2 (en) 2010-09-01 2015-09-15 E I Du Pont De Nemours And Company Fungicidal pyrazoles

Cited By (9)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
GB2458121A (en) * 2008-03-03 2009-09-09 Radiodetection Ltd A detector for calculating a depth of a buried conductor
GB2458121B (en) * 2008-03-03 2012-01-25 Radiodetection Ltd A detector for calculating a depth of a buried conductor
US8183851B2 (en) 2008-03-03 2012-05-22 Radiodetection Detector for calculating a depth of a buried conductor
US8566043B2 (en) 2008-03-03 2013-10-22 Radiodetection Limited Detector for calculating the distortion of an electromagnetic field produced by a buried current carrying conductor
US9131693B2 (en) 2010-09-01 2015-09-15 E I Du Pont De Nemours And Company Fungicidal pyrazoles
WO2013036686A1 (en) * 2011-09-06 2013-03-14 Ray Merewether Systems and methods for locating buried or hidden objects using sheet current flow models
JP2014215066A (en) * 2013-04-23 2014-11-17 高千穂産業株式会社 Method for measuring position of long-size article
CN104154856A (en) * 2013-05-13 2014-11-19 雷迪有限公司 Electronic marker locator systems and methods
JP2015111109A (en) * 2013-11-01 2015-06-18 株式会社沖縄中央エンジニアリング Detection method of magnetic matter and magnetic sensor

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