JP6234690B2 - Transmitter of buried pipe detection device and induction coil for transmitter - Google Patents
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- 230000006698 induction Effects 0.000 title claims description 34
- 238000001514 detection method Methods 0.000 title claims description 28
- 230000005540 biological transmission Effects 0.000 claims description 2
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- 238000010586 diagram Methods 0.000 description 5
- 230000004907 flux Effects 0.000 description 3
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Description
本発明は、地中に埋設したガス管、水道管等の導電性を有する埋設管の位置及び深度を地上から探知する埋設管探知装置の送信器及び送信器用誘導コイルに関する。 The present invention relates to a transmitter of a buried pipe detection device for detecting the position and depth of a buried pipe having conductivity, such as a gas pipe and a water pipe buried in the ground, and an induction coil for the transmitter .
従来、地中に埋設したガス管、水道管等の導電性を有する埋設管の位置及び深度を地上から探知する装置として、電磁誘導を利用した埋設管探知装置が知られている。
埋設管探知の方式としては、送信器で発生させた交流電流を埋設管に流すことで埋設管の周囲に磁界を生成させ、この磁界を受信器で捕捉するものである(図8参照)。
送信器で発生させた交流電流を埋設管に流す方法としては、送信器を埋設管に直接接続する直接法(図9参照)やループ法(図10参照)、送信器の出力を誘導コイルに導き誘導コイルの周囲に1次磁界を形成させ、この1次磁界によって埋設管に交流電流を流して埋設管の周囲に2次磁界を生成させ、この2次磁界を受信器で捕捉する誘導法(図11参照)があるが、簡便であることから誘導法が広く使われている。
2. Description of the Related Art Conventionally, a buried pipe detection device using electromagnetic induction has been known as a device for detecting the position and depth of a conductive buried pipe such as a gas pipe or a water pipe buried in the ground from the ground.
As a buried pipe detection method, an alternating current generated by a transmitter is passed through the buried pipe to generate a magnetic field around the buried pipe, and this magnetic field is captured by the receiver (see FIG. 8).
The AC current generated by the transmitter can be passed through the buried pipe as a direct method (see FIG. 9) or a loop method (see FIG. 10) in which the transmitter is directly connected to the buried pipe, or the transmitter output is used as an induction coil. An induction method in which a primary magnetic field is formed around a guiding induction coil, an alternating current is caused to flow through the buried pipe by the primary magnetic field, a secondary magnetic field is generated around the buried pipe, and the secondary magnetic field is captured by a receiver. (See FIG. 11), but the guidance method is widely used because of its simplicity.
何れにしても、埋設管の周囲に生成した磁界を地上に配置した受信器で捕捉するのであるが、誘導法を採用した場合には、送信器による1次磁界の影響を受けないよう、送信器と受信器とをかなり離隔させて配置する必要があった。
又、探査目的とする埋設管に輻輳して他の埋設管が存在している場合には、この輻輳する埋設管にも交流電流が流れてしまい、これから発生する妨害磁界が探知精度を悪化させてしまう。
そこで、送信器を構成する誘導コイルとして、一対のコイルを垂直に並行配置し、それらコイルを逆極性に接続して、その周囲に磁界を形成させ、この磁界内に位置する埋設管に交流電流を流すようにした埋設管探知装置が提案された(特許文献1参照)。
In any case, the magnetic field generated around the buried pipe is captured by a receiver placed on the ground. However, when the induction method is adopted, transmission is performed so that the transmitter is not affected by the primary magnetic field. It was necessary to arrange the receiver and the receiver at a considerable distance.
In addition, when there is another buried pipe congested in the buried pipe for the purpose of exploration, an alternating current also flows in this buried buried pipe, and the disturbing magnetic field generated from this deteriorates the detection accuracy. End up.
Therefore, as an induction coil that constitutes a transmitter, a pair of coils are arranged vertically in parallel, these coils are connected in reverse polarity, a magnetic field is formed around them, and an alternating current is applied to a buried pipe located in this magnetic field. A buried pipe detection device has been proposed (see Patent Document 1).
この埋設管探知装置によれば、一対のコイルを垂直に並行配置することによって、1次磁界の垂直方向の磁束密度を高く、水平方向の磁束密度を低くするようにしたから、受信器を送信器により近付けることができるようになった。
又、下方向の指向性が鋭くなり、探査目的とする埋設管に輻輳する埋設管に流れる交流電流を減少させるから、探査精度を高めることができる。
According to this buried pipe detection device, the vertical magnetic flux density of the primary magnetic field is increased and the horizontal magnetic flux density is decreased by arranging a pair of coils vertically in parallel. Can now be closer to the vessel.
In addition, the directivity in the downward direction becomes sharp and the alternating current flowing in the buried pipe congested with the buried pipe targeted for exploration is reduced, so that the exploration accuracy can be improved.
しかし、特許文献1に開示された埋設管探知装置によれば、一対のコイルを垂直に並行配置し、それらコイルを逆極性に接続した誘導コイルでは、各々のコイルが発生する磁界が互いに打ち消しあうことから、1次磁界が弱まり、探査目的とする埋設管に流れる電流も減ってしまう。
このような状態では、受信器が検出するのに充分な強さの2次磁界を発生させることができず、外部雑音などの影響により受信器の探知精度を低下させた。受信器が検出するのに充分な強さの2次磁界を発生させるためには、送信器の出力を上げる外はなく、送信器の大型化等の弊害を生じる。
However, according to the buried pipe detection device disclosed in
In such a state, a secondary magnetic field having a sufficient strength for detection by the receiver cannot be generated, and the detection accuracy of the receiver is lowered due to the influence of external noise and the like. In order to generate a secondary magnetic field having a sufficient strength for detection by the receiver, there is no doubt that the output of the transmitter is increased, and problems such as an increase in the size of the transmitter occur.
本発明は、かかる従来の問題点を解決するために為されたものであって、その目的とするところは、埋設管の近傍に輻輳する他の埋設管が存在しても、これら埋設管には極力電流を流さず、かつ、探査目的とする埋設管に生成する2次磁界の強度を低減させず、受信器の探知精度を低下させることのない埋設管探知装置の送信器を提供することにある。 The present invention has been made in order to solve such conventional problems, and the object of the present invention is to provide these buried pipes even if other buried pipes are present near the buried pipe. To provide a transmitter of a buried pipe detection device that does not cause a current to flow as much as possible, does not reduce the strength of a secondary magnetic field generated in a buried pipe to be searched, and does not reduce the detection accuracy of a receiver. It is in.
上記目的を達成するために、本発明の埋設管探知装置の送信器は、2本のコイルを水平方向に所定距離をおいて配置し、各コイルの軸線がコイルの上方で交差するように、各コイルの軸線を垂直方向から内側に傾斜角度θが5〜20°となるように傾斜させると共に、各コイルの出力を逆極性になるように接続した送信器用誘導コイルを構成したことを特徴とする。 In order to achieve the above object, the transmitter of the buried pipe detection device of the present invention arranges two coils at a predetermined distance in the horizontal direction, and the axis of each coil intersects above the coils. The transmitter coil is configured such that the axis of each coil is tilted inward from the vertical direction so that the tilt angle θ is 5 to 20 °, and the output of each coil is connected to have a reverse polarity. To do.
ここで、送信器用誘導コイルの2本のコイルの距離2lは40〜60cmであるのが好ましい。 Here, the distance 2l between the two coils of the transmitter induction coil is preferably 40 to 60 cm .
本発明の埋設管探知装置の送信器によれば、探査目的とする埋設管の近傍に輻輳する他の埋設管が存在した場合にも、これら埋設管には電流を極力流さず、かつ、探査目的とする埋設管に生成する2次磁界の強度を低減させないから、受信器の探知精度を低下させることはない。 According to the transmitter of the buried pipe detection device of the present invention, even when there is another buried pipe that is congested in the vicinity of the buried pipe targeted for the exploration, current is not passed through these buried pipes as much as possible. Since the strength of the secondary magnetic field generated in the target buried pipe is not reduced, the detection accuracy of the receiver is not lowered.
以下、本発明の埋設管探知装置の送信器の好適な実施形態について、図面を参照して説明する。
図1は、本発明の埋設管探知装置の誘導コイルの構成図、図2は、図1に示す誘導コイルと埋設管との位置関係を示す説明図、図3は、本発明の埋設管探知装置の送信器の構成図である。
DESCRIPTION OF EXEMPLARY EMBODIMENTS Hereinafter, a preferred embodiment of a transmitter of a buried pipe detection device of the invention will be described with reference to the drawings.
FIG. 1 is a configuration diagram of an induction coil of the buried pipe detection device of the present invention, FIG. 2 is an explanatory diagram showing a positional relationship between the induction coil and the buried pipe shown in FIG. 1, and FIG. 3 is a buried pipe detection of the present invention. It is a block diagram of the transmitter of an apparatus.
本発明の埋設管探知装置の送信器1は、図3に示すように、誘導コイル2、電圧増幅器3、発信器4から構成される。
As shown in FIG. 3, the
誘導コイル2は、図3に示すように、2本のコイル2A,2Bを水平方向に所定距離2lおいて配置し、各コイル2A,2Bの軸線Ao,Boを垂直方向Vから内側に所定角度θだけ傾斜させてある。
そして、各コイル2A,2Bの出力を逆極性になるよう接続して、電圧増幅器3から交流電流を流すようになっている。
As shown in FIG. 3, the
And the output of each
誘導コイル2は、埋設管Pの上方に位置させて、埋設管Pが位置する領域内に磁界を生成するから、誘導コイル2と埋設管Pとの位置関係は、図2に示すようになる。
ここで、xは、2本のコイル2A,2Bの中心から埋設管Pまでの水平距離、yは、2本のコイル2A,2Bの中心から埋設管Pまでの垂直距離を示している。
Since the
Here, x represents the horizontal distance from the center of the two
ここで、誘導コイル2、すなわち、2本のコイル2A,2Bに交流電流を流した時の埋設管Pに生成する誘起起電力eは、下記の式で示すことができる。
Here, the induced electromotive force e generated in the buried pipe P when an alternating current is passed through the
先ず、誘導コイル2を埋設管の直上(x=0m)に位置させた場合に比べて、誘導起電力eが1/21/2(電力で1/2)となる水平距離x′を半値幅と定義し、誘導特性を評価する尺度とした。
そして、2l=10〜100cm、θ=0〜90°、y=0.5,1.0,2.0mと変更して、半値幅x′の変化を確認した。
First, compared to the case where the
Then, 2l = 10 to 100 cm, θ = 0 to 90 °, y = 0.5, 1.0, and 2.0 m were changed, and the change of the half-value width x ′ was confirmed.
半値幅x′の確認結果を図4乃至図6に示す。尚、単一コイルから構成した誘導コイル11の場合には、各々、y=0.642,1.286,2.574に相当する。
ここで、半値幅x′としては深度yの1.2倍以下であれば実用上問題ないから、深度0.5〜2.0mの埋設管に対して、コイル間距離2l=40〜60cm、コイル傾斜角θ=5〜20°が適当であることが理解される。
The confirmation results of the half-value width x ′ are shown in FIGS. In the case of the induction coil 11 constituted by a single coil, it corresponds to y = 0.642, 1.286, 2.574, respectively.
Here, since the half-value width x ′ is 1.2 times or less than the depth y, there is no practical problem. Therefore, for an embedded pipe having a depth of 0.5 to 2.0 m, the inter-coil distance 2l = 40 to 60 cm, It is understood that a coil tilt angle θ = 5-20 ° is suitable.
次に、x=0m、y=1mに設定して、2l=10〜100cm、θ=0〜90°と変更して、誘導コイル2誘導効率を確認した。
Next, x = 0 m, y = 1 m were set and 2l = 10 to 100 cm and θ = 0 to 90 ° were changed to confirm the
誘導効率の確認結果を図7に示す。尚、このグラフは、単一コイルから構成した誘導コイル11の誘導起電力の値を1として、正規化したものである。
ここで、誘導効率としては0.3〜0.5であれば実用上問題ないから、深度1.0mの埋設管に対して、コイル間距離2l=40〜60cm、コイル傾斜角θ=5〜20°が適当であることが理解される。
The result of confirming the induction efficiency is shown in FIG. This graph is normalized by setting the value of the induced electromotive force of the induction coil 11 composed of a single coil to 1.
Here, since there is no practical problem if the induction efficiency is 0.3 to 0.5, the distance between the coils 2l = 40 to 60 cm and the coil inclination angle θ = 5 to 5 with respect to the buried pipe having a depth of 1.0 m. It will be appreciated that 20 ° is suitable.
本発明の埋設管探知装置の送信器は、2本のコイルの軸線を垂直方向から内側に所定角度傾斜させ、各コイルの出力を逆極性になるよう接続して、誘導コイルの一対のコイルの配列方向の磁束密度を低くしたから、探査目的とする埋設管の近傍に輻輳する他の埋設管が存在したとしても、これら埋設管には電流が殆ど流れず、かつ、探査目的とする埋設管に生成する2次磁界の強度は低減せず、受信器の探知精度を低下させることはない。 The transmitter of the buried pipe detection device of the present invention inclines the axis of the two coils inward by a predetermined angle from the vertical direction, and connects the outputs of the coils so as to have opposite polarities. Since the magnetic flux density in the arrangement direction has been lowered, even if there are other buried pipes converging in the vicinity of the buried pipe intended for exploration, there is almost no current flowing through these buried pipes, and the buried pipe intended for exploration. Therefore, the intensity of the secondary magnetic field generated in the receiver is not reduced, and the detection accuracy of the receiver is not lowered.
1 送信器
2 誘導コイル
2A,2B コイル
P 埋設管
1
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