JPH0572348A - Differential sensitivity distribution electric image tomographic method - Google Patents
Differential sensitivity distribution electric image tomographic methodInfo
- Publication number
- JPH0572348A JPH0572348A JP4203590A JP4203590A JPH0572348A JP H0572348 A JPH0572348 A JP H0572348A JP 4203590 A JP4203590 A JP 4203590A JP 4203590 A JP4203590 A JP 4203590A JP H0572348 A JPH0572348 A JP H0572348A
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- electrode
- electrodes
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- ground surface
- wires
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- 238000000034 method Methods 0.000 title claims description 10
- 230000035945 sensitivity Effects 0.000 title abstract description 12
- 238000009826 distribution Methods 0.000 title abstract description 9
- 238000003325 tomography Methods 0.000 claims description 6
- 238000003384 imaging method Methods 0.000 claims description 2
- 239000000463 material Substances 0.000 abstract description 2
- 238000005553 drilling Methods 0.000 abstract 2
- 230000015572 biosynthetic process Effects 0.000 abstract 1
- 238000006243 chemical reaction Methods 0.000 abstract 1
- 238000007689 inspection Methods 0.000 description 5
- 230000000694 effects Effects 0.000 description 3
- 230000002159 abnormal effect Effects 0.000 description 2
- 239000004020 conductor Substances 0.000 description 2
- 230000002547 anomalous effect Effects 0.000 description 1
- 239000002131 composite material Substances 0.000 description 1
- 239000003673 groundwater Substances 0.000 description 1
- 238000005065 mining Methods 0.000 description 1
- 239000011435 rock Substances 0.000 description 1
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- Geophysics And Detection Of Objects (AREA)
Abstract
Description
【発明の詳細な説明】 (産業上の利用分野) この発明は、とくに、見掛比抵抗が算出で きないとして回避・省いている差動的な電極 配列を、地表とボーリング孔(あるいは坑井 )やトンネルなども用いて、立体的にも積極 的に配列した複合立体電極配置によって取得 される電気探査データから、鉱山、地下水、 土木建設基礎地盤・岩盤、地質構造などをは じめ、ひろく媒質・材料の探査(検査)に、 新しく差動感度分布によって断面画像を得る 電気トモグラフィ法に関するものである。DETAILED DESCRIPTION OF THE INVENTION (Industrial field of application) The present invention is particularly applicable to a differential electrode array which is avoided or omitted because the apparent resistivity cannot be calculated, and is provided on the ground surface and the boring hole (or well). Wells, tunnels, etc. are also used to identify mining, groundwater, civil engineering foundation grounds / rocks, geological structures, etc. based on electrical exploration data acquired by composite three-dimensional electrode arrangement that is also actively arranged in three dimensions. The present invention relates to an electric tomography method for obtaining cross-sectional images by a new differential sensitivity distribution for exploration (inspection) of mediums and materials.
(従来の技術) 従来の比抵抗トモグラフィでは、単に、 地表あるいはボーリング孔(あるいは坑井) などに配列する電極配置観測パターンによる 見掛比抵抗データのみから逆解析している。 (Prior Art) In conventional resistivity tomography, reverse analysis is performed only from apparent resistivity data based on an electrode arrangement observation pattern arranged on the surface of the earth or a borehole (or well).
したがって、均質媒質の場合に電位(あるい は電位差)が零となり見掛比抵抗の算出がで きない種々の電極配列の場合には、データを 回避・省いており、その断面画像の形成法は なかった。地下など媒質の電気探査では、ボ ーリング孔(あるいは坑井)、トンネルなど と地表といった、立体的に配列する場合を含 めた色々な複数の電極配置による観測パター ンが必須となるが、見掛比抵抗の算出が精度 良く得られない場合を回避・省いていること が多い。Therefore, in the case of various electrode arrangements where the potential (or potential difference) is zero in the case of a homogeneous medium and the apparent resistivity cannot be calculated, data is avoided or omitted, and the method of forming the cross-sectional image is used. There was no. In electrical exploration of media such as underground, observation patterns with various electrode arrangements including three-dimensional arrangements such as boring holes (or wells), tunnels, and the ground surface are essential. In many cases, it is avoided or omitted when the calculation of the multiplication resistivity cannot be obtained accurately.
(実施例) 本発明の実施例を第1図に基づいて説明す る。1は、地表である。2は、ボーリング孔 (あるいは坑井)で、3は、ボーリング孔の 上端で、4は、孔(坑)内に置く正の電流電 極である。5は、地表に置く正の電位電極で ある。6は、孔内に置く負の電流電極である。(Example) An example of the present invention will be described with reference to FIG. 1 is the ground surface. 2 is a borehole (or well), 3 is the upper end of the borehole, and 4 is a positive current electrode placed in the borehole. 5 is a positive potential electrode placed on the surface of the earth. 6 is a negative current electrode placed in the hole.
7は、地表に置く負の電位電極である。(第 2図では、ボーリング孔1内に正の電流電極 4を置き、正負の電位電極5、7をボーリン グ孔2内に置く。負の電流電極6は、ボーリ ング孔1から遠くの地表に置く。第3図で は、地表に正負の電流電極4、6を置き、正 負の電位電極5、7をトンネル内に置く。) 8は電源、9は電流計である。10は電位差 計である。11、12、13および14は、 電線である。15、16、17および18は、 この差動方式の立体電極配列観測パターンの 電極配置の組み合わせを示す線である。19 は、孔内電極の最下端である。(第2図では、 16、17は孔の上端の電極で、18、19 は孔の最下端の電極である。第3図では、 16、17は地表の左端および右端の電極で、 18、19はトンネル内の左端および右端の 電極である。) つぎに、本特許出願の電気探査画像を形成す る基礎定数となる差動方式の立体電極配列の 感度分布の作成を、第1図、第2図および第 3図に対応して説明する。 第4図は、孔内 の深度30mと40mに正と負の電流電極を 置き、地表の30mと50mに正と負の電位 電極を置いた場合で、第5図は、孔1内の深 度31.5mに正の電流電極、孔1から遠く の地表に負の電流電極を置き、孔2内の深度 7mと17mに正と負の電位電極を置いた場 合である。第6図は、地表の40mと60m に正と負の電流電極を置き、地下深度32. 5mのトンネル内の20mと30mに正と負 の電位電極を置いた場合である。3次元異常 導体による差動感度分布で、図中の数値は、 負が順感度、正が逆感度となり、大きい値は 良感度を示す。このような、差動感度分布を 電極配置観測パターンを複数種類あるいは、 複合して用いることによって、電気探査(検 査)断面画像の形成を行う。Reference numeral 7 is a negative potential electrode placed on the ground surface. (In FIG. 2, the positive current electrode 4 is placed in the boring hole 1 and the positive and negative potential electrodes 5, 7 are placed in the boring hole 2. The negative current electrode 6 is located on the ground surface far from the boring hole 1. In Fig. 3, positive and negative current electrodes 4 and 6 are placed on the ground surface, and positive and negative potential electrodes 5 and 7 are placed in the tunnel.) 8 is a power source and 9 is an ammeter. 10 is a potentiometer. 11, 12, 13 and 14 are electric wires. Reference numerals 15, 16, 17, and 18 are lines showing combinations of electrode arrangements of this differential type three-dimensional electrode array observation pattern. 19 is the lowermost end of the in-hole electrode. (In FIG. 2, 16 and 17 are electrodes at the upper end of the hole, and 18 and 19 are electrodes at the lower end of the hole. In FIG. 3, 16 and 17 are electrodes at the left and right ends of the ground surface, 18, 19 are electrodes at the left end and the right end in the tunnel.) Next, the sensitivity distribution of the differential type three-dimensional electrode array, which is the basic constant forming the electric exploration image of the present patent application, is created as shown in FIG. The description will be given with reference to FIGS. 2 and 3. Fig. 4 shows the case where positive and negative current electrodes are placed at the depths of 30 m and 40 m in the hole, and positive and negative potential electrodes are placed at the surface of 30 m and 50 m. Fig. 5 shows the depth inside the hole 1. This is the case where a positive current electrode is placed at a distance of 31.5 m, a negative current electrode is placed on the ground surface far from hole 1, and positive and negative potential electrodes are placed at depths 7 m and 17 m in hole 2. In Fig. 6, positive and negative current electrodes are placed at 40 m and 60 m on the surface of the earth, and the depth of 32. This is the case where positive and negative potential electrodes are placed at 20 m and 30 m in a 5 m tunnel. The differential sensitivity distribution due to a three-dimensional anomalous conductor. In the figures, negative values indicate forward sensitivity, positive values indicate reverse sensitivity, and large values indicate good sensitivity. Such differential sensitivity distribution is used to form an electrical exploration (inspection) cross-sectional image by using a plurality of electrode arrangement observation patterns or a combination thereof.
(発明の効果) 一般には、見掛比抵抗が精度良く計算でき ないとして回避・省いている立体的あるいは 地表に配列する観測電極配置が少なくない。(Effects of the Invention) Generally, there are not a few observation electrode arrangements that are three-dimensionally or arranged on the ground surface, which are avoided or omitted because the apparent resistivity cannot be calculated accurately.
本発明は、新しく見つけた差動感度分布の作 成法に基づく差動電気探査(検査)画像(ト モグラフィ)法に関するものである。見掛比 抵抗データ方式よりも、より多くのデータの 利用が可能となり、媒質断面画像の信頼性の 向上に役立つ。The present invention relates to a differential electrical exploration (inspection) imaging (tomography) method based on a newly found method of creating a differential sensitivity distribution. It is possible to use more data than the apparent resistivity data method, which helps improve the reliability of medium cross-section images.
第7図、第8図と第9図は、発明の効果 を示した一例で、比抵抗100Ω・mの均質 な3次元媒質内に比抵抗0Ω・mの単一の塊 状構造(球)が存在する場合の、第1図、第 2図および第3図の、それぞれの方式による 電気探査(検査)断面画像である。構造によ る異常を画像の等数値線で示している。数値 は、異常体の出現確率(%)で、形成された 断面画像の信頼性も識別できる。 FIGS. 7, 8 and 9 are examples showing the effect of the invention. In a homogeneous three-dimensional medium having a specific resistance of 100 Ω · m, a single lump structure (sphere) having a specific resistance of 0 Ω · m is shown. 4A, 2B, and 3 are electrical cross-sectional images of electric exploration (inspection) according to the respective methods in the case where is present. Anomalies due to the structure are shown by iso-value lines in the image. The numerical value is the probability of occurrence of an abnormal body (%), which can also identify the reliability of the formed cross-sectional image.
第1図から第3図までは、本発明の実施例 を示す断面図である。第1図を例に説明する。 1は地表、 2はボーリング孔(あるいは坑 井)、3はボーリング孔の上端、4 は電流 電極(正極)、5は電位電極(正極)、6 電流電極(負極)、7は電位電極(負極)、 8は 電源、9は電流計、10は電位差計、 11、12、13と14は電線、15、16、 17および18は、この差動方式の立体電極 配列観測パターンの電極配置の組み合わせを 示す線である。19はボーリング孔(坑井) 内最下端の電極である。 第4図から第6図までは、差動電気探査画 像(トモグラフィ)を得る基礎定数となる差 動感度分布の例である。縦軸は、深度 単位 (m)、横軸は、水平距離 単位(m)であ る。水平距離40mにあるボーリング孔( あるいは坑井) 1本を利用する場合(第4 図)、水平距離20mと60mにある2本の ボーリング孔を利用する場合(第5図)、お よび地下深度32.5mのトンネルと地表を 利用する場合(第6図)である。 第7図から第9図までは、本発明の効果 を示す断面画像で、第1から第3図の方式 に対応する例である。比抵抗100Ω・mの 均質な3次元媒質内に比抵抗0Ω・mの単一 の球状(半径5m)異常導体が存在する場合 である。 縦軸は、深度 単位(m)、横軸 は、水平距離 単位(m)である。探査(検 査)対象物である構造の中心は、+ 印で示 している。 1 to 3 are sectional views showing an embodiment of the present invention. An example will be described with reference to FIG. 1 is the surface of the earth, 2 is a borehole (or well), 3 is the upper end of the borehole, 4 is a current electrode (positive electrode), 5 is a potential electrode (positive electrode), 6 is a current electrode (negative electrode), 7 is a potential electrode (negative electrode) ), 8 is a power supply, 9 is an ammeter, 10 is a potentiometer, 11, 12, 13 and 14 are electric wires, 15, 16, 17 and 18 are combinations of electrode arrangements of this differential type three-dimensional electrode array observation pattern Is a line indicating. Reference numeral 19 is an electrode at the bottom end of the borehole (well). 4 to 6 are examples of differential sensitivity distributions that are basic constants for obtaining differential electrical exploration images (tomography). The vertical axis represents the depth unit (m), and the horizontal axis represents the horizontal distance unit (m). When using one boring hole (or well) at a horizontal distance of 40 m (Fig. 4), when using two boring holes at a horizontal distance of 20 m and 60 m (Fig. 5), and underground depth. This is when using a 32.5 m tunnel and ground surface (Fig. 6). FIGS. 7 to 9 are sectional images showing the effect of the present invention, which are examples corresponding to the systems of FIGS. 1 to 3. This is the case where a single spherical (radius 5 m) abnormal conductor with a specific resistance of 0 Ω · m exists in a homogeneous three-dimensional medium with a specific resistance of 100 Ω · m. The vertical axis represents the depth unit (m), and the horizontal axis represents the horizontal distance unit (m). The center of the structure, which is the object of exploration (inspection), is indicated by a + sign.
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【手続補正書】[Procedure amendment]
【提出日】平4.10.12 (1)願書 別紙の通り。 (2)明細書の発明の名称を「差動感度分布電気画像トモ
グラフィ法」と補正する。 (3)明細書第1頁10行目の「3.発明の詳細な明細」
を「3.発明の詳細な説明」と補正する。[Submission date] Hei 4.10.12 (1) Application form As attached. (2) The title of the invention in the description is corrected to “differential sensitivity distribution electric image tomography method”. (3) “3. Detailed description of the invention” on page 1, line 10 of the specification.
Is corrected as “3. Detailed description of the invention”.
Claims (1)
と して回避・省いていた差動方式電極配列を立 体的にも積極的に用いて、その電気探査デー タから地下構造断面を電気的に画像化する トモグラフィ法1. Particularly, the differential type electrode array, which is generally avoided or omitted because an apparent resistivity cannot be obtained, is positively and actively used from the standpoint of the electrical survey data and the underground structure cross section. Tomography method for electrically imaging images
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP4203590A JPH0572348A (en) | 1990-02-22 | 1990-02-22 | Differential sensitivity distribution electric image tomographic method |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP4203590A JPH0572348A (en) | 1990-02-22 | 1990-02-22 | Differential sensitivity distribution electric image tomographic method |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH0572348A true JPH0572348A (en) | 1993-03-26 |
Family
ID=12624903
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP4203590A Pending JPH0572348A (en) | 1990-02-22 | 1990-02-22 | Differential sensitivity distribution electric image tomographic method |
Country Status (1)
| Country | Link |
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| JP (1) | JPH0572348A (en) |
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2010230689A (en) * | 2010-07-12 | 2010-10-14 | Fujita Corp | Natural mountain exploration method |
| RU2642967C2 (en) * | 2015-11-27 | 2018-01-29 | Владимир Петрович Колесников | Method of geoelectrical prospecting |
-
1990
- 1990-02-22 JP JP4203590A patent/JPH0572348A/en active Pending
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2010230689A (en) * | 2010-07-12 | 2010-10-14 | Fujita Corp | Natural mountain exploration method |
| RU2642967C2 (en) * | 2015-11-27 | 2018-01-29 | Владимир Петрович Колесников | Method of geoelectrical prospecting |
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