JPS6214791B2 - - Google Patents
Info
- Publication number
- JPS6214791B2 JPS6214791B2 JP55076235A JP7623580A JPS6214791B2 JP S6214791 B2 JPS6214791 B2 JP S6214791B2 JP 55076235 A JP55076235 A JP 55076235A JP 7623580 A JP7623580 A JP 7623580A JP S6214791 B2 JPS6214791 B2 JP S6214791B2
- Authority
- JP
- Japan
- Prior art keywords
- waves
- wave
- borehole
- magnetic fluid
- water
- 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
Links
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01V—GEOPHYSICS; GRAVITATIONAL MEASUREMENTS; DETECTING MASSES OR OBJECTS; TAGS
- G01V1/00—Seismology; Seismic or acoustic prospecting or detecting
- G01V1/02—Generating seismic energy
- G01V1/143—Generating seismic energy using mechanical driving means, e.g. motor driven shaft
- G01V1/155—Generating seismic energy using mechanical driving means, e.g. motor driven shaft using reciprocating masses
Landscapes
- Engineering & Computer Science (AREA)
- Remote Sensing (AREA)
- Physics & Mathematics (AREA)
- Life Sciences & Earth Sciences (AREA)
- Acoustics & Sound (AREA)
- Environmental & Geological Engineering (AREA)
- Geology (AREA)
- General Life Sciences & Earth Sciences (AREA)
- General Physics & Mathematics (AREA)
- Geophysics (AREA)
- Geophysics And Detection Of Objects (AREA)
Description
【発明の詳細な説明】
本発明は、孔内水を有する孔井内で使用される
S波検層用の振源に関し、更に詳しくは、ゴムシ
ートで封止した磁性流体にコイルの電磁力を作用
させることにより、メカニカルな機構を用いるこ
となく、孔内水を介して孔壁面に振源力を作用さ
せるようにした振源に関するものである。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an oscillation source for S-wave logging used in a well containing borehole water, and more specifically, the present invention relates to an oscillation source for S-wave logging used in a well containing borehole water. This invention relates to an oscillation source that causes an oscillation force to act on a hole wall surface through water in the hole without using a mechanical mechanism.
PS検層は、孔井中で地下の弾性波速度、すな
わちP波(縦波)速度とS波(横波)速度を直接
測定し、その値から地下の弾性的性質を調査する
方法である。 PS logging is a method of directly measuring underground elastic wave velocities, that is, P wave (longitudinal wave) velocity and S wave (transverse wave) velocity, in a wellbore and investigating the elastic properties of the underground from these values.
近年、地震工学や資源工学等の方面から、地下
深部における高精度の弾性波のデータが要求され
ている。しかし、地下深部の弾性波を測定する装
置としては、P波検層器だけが実用機として普及
しているにすぎない。それは、P波が弾性波のう
ち最も速い速度で伝搬するから、その確認が比較
的平易なのに対して、S波は、それより速く伝播
する波(主としてP波に起因するチユーブウエー
ブ)によつて、その波形がみだされやすく、確認
が困難なためである。 In recent years, highly accurate elastic wave data deep underground has been required from fields such as earthquake engineering and resource engineering. However, as a device for measuring elastic waves deep underground, only the P-wave logging device is in widespread use. This is because P waves propagate at the fastest speed among elastic waves, so it is relatively easy to confirm, whereas S waves are caused by waves that propagate faster (mainly tube waves caused by P waves). This is because the waveform is easily visible and difficult to confirm.
これに対し、P波の輻射を抑制し、S波を効果
的に輻射させうるような方法として、振源体内の
運動機構を動作させることによつて孔軸と直交す
る一方向の振源力を孔内水を介して正負の間接加
圧として孔壁面に加え、それによつてその振源力
と直交する方向に卓越した指向性をもつS波を輻
射させる方法も提案されている(特開昭54−
107401号公報参照)。 On the other hand, as a method to suppress the radiation of P waves and effectively radiate S waves, the source force in one direction perpendicular to the hole axis is generated by operating the motion mechanism inside the source body. A method has also been proposed in which S-waves with excellent directivity are radiated in the direction orthogonal to the source force by applying positive and negative indirect pressure to the hole wall through the water in the hole (Unexamined Japanese Patent Publication No. Showa 54-
(See Publication No. 107401).
しかし、このような方法も含めて、従来の方法
では、加振作用をする剛体を一方向に移動自在に
保持するなど何らかのメカニカルな機構が必要で
あつたため、装置がどうしても大型化、複雑化し
てしまうばかりでなく、S波の受振にとつて妨害
波となるチユーブ・ウエーブやP波をもある程度
は輻射してしまうといつた欠点を有していた。 However, conventional methods, including this method, require some kind of mechanical mechanism, such as holding a rigid body that acts on vibration so that it can move freely in one direction, which inevitably increases the size and complexity of the device. It has the disadvantage that it not only radiates a certain amount of tube waves and P waves, which are interference waves for receiving S waves.
本発明の目的は、このような従来技術の欠点を
解消し、メカニカルな機構がなく、それ故装置を
小型化、簡略化することができ、しかもS波の受
振の妨げとなるチユーブ・ウエーブやP波の輻射
をほぼ完壁に防止することができるようなS波検
層用振源を提供することにある。 The purpose of the present invention is to eliminate the drawbacks of the prior art, to make the device smaller and simpler because it does not require a mechanical mechanism, and to avoid tube waves and other problems that hinder the reception of S waves. An object of the present invention is to provide an S-wave logging source that can almost completely prevent P-wave radiation.
かかる目的を達成するため、本発明は、ゴムシ
ートで封止されている磁性流体にコイルからの電
磁力を作用させて駆動することにより、前記ゴム
シートに接している孔内水を直接動かして孔壁に
力を加えるよう構成されている。 In order to achieve this object, the present invention directly moves the water in the hole in contact with the rubber sheet by applying electromagnetic force from a coil to the magnetic fluid sealed with the rubber sheet to drive it. It is configured to apply a force to the hole wall.
以下、図面に基づき本発明について詳述する。
第1図は、本発明に係る振源の一例を模式的に示
したものであり、まずそれにより基本構成と動作
原理について説明する。振源は、孔内水を有する
孔井内において使用される。プローブ1は、その
内部にゴムシート2で仕切られた領域を有し、そ
の領域内に磁性流体3が封止され、また、その領
域の外側の両端部近傍にそれぞれコイル輪4a,
4bが配置されている構造をなしている。前記ゴ
ムシート2は孔内水5に接している。なお、ここ
で“磁性流体”とは、比較的強い磁性をもち、か
つ流体の挙動を示すもので、例えば粒径が100Å
程度のマグネタイトあるいはその他のフエライト
の微粒子の表面に界面活性剤の単分子層を化学吸
着させ、水や有機溶媒中に分散させたものであ
る。 Hereinafter, the present invention will be explained in detail based on the drawings.
FIG. 1 schematically shows an example of an oscillation source according to the present invention, and the basic configuration and operating principle will first be explained using it. The source is used in a borehole with borehole water. The probe 1 has a region inside thereof partitioned by a rubber sheet 2, and a magnetic fluid 3 is sealed within the region, and coil rings 4a, 4a and 4a are arranged near both ends outside the region.
4b is arranged. The rubber sheet 2 is in contact with the borehole water 5. Note that "magnetic fluid" here refers to something that has relatively strong magnetism and exhibits the behavior of a fluid, for example, a particle size of 100 Å.
A monomolecular layer of a surfactant is chemically adsorbed onto the surface of fine particles of magnetite or other ferrite, and then dispersed in water or an organic solvent.
今、コイル輪4aに通電すると、そのまわりに
磁場が生じ、磁性流体3は、磁気回路的にはソレ
ノイドのプランジヤーに相当するからX方向に動
くことになる。このときの磁性流体の力学的な運
動は流体そのものである。従つて、孔内水5はな
んらの体積変化もうけずにX方向に動く。換言す
れば、孔内水5を直接X方向に動かしたのと同じ
とみなせる。この孔内水5の運動により、X方向
の孔壁6に力が加えられ、孔軸方向にS波だけを
輻射することができるのである。なお、コイル輪
4aへの通電をやめれば、ゴムシート2の弾性に
より、磁性流体3は戻の状態に復帰する。又、コ
イル輪4bに電流を流せば、磁性流体3は逆方向
に(−X方向に)駆動され、平易にS波の反転記
録が得られるので、その確認も確実に行える。 Now, when the coil ring 4a is energized, a magnetic field is generated around it, and the magnetic fluid 3 moves in the X direction because it corresponds to the plunger of a solenoid in terms of a magnetic circuit. The mechanical motion of the magnetic fluid at this time is the fluid itself. Therefore, the borehole water 5 moves in the X direction without any volume change. In other words, it can be regarded as the same as moving the borehole water 5 directly in the X direction. This movement of the water 5 in the hole applies force to the hole wall 6 in the X direction, making it possible to radiate only the S wave in the direction of the hole axis. Note that when the coil ring 4a is no longer energized, the elasticity of the rubber sheet 2 causes the magnetic fluid 3 to return to its original state. Furthermore, when a current is passed through the coil ring 4b, the magnetic fluid 3 is driven in the opposite direction (in the -X direction), and the inversion record of the S wave can be easily obtained, so that confirmation can be made with certainty.
本発明に係る振源の一実施例を第2図、第3図
に示す。プローブ1には、その中心軸に直角の方
向に円筒状の外ケース10が取付けられ、その内
部に振源本体が収容される。振源本体は、第2図
に明瞭に示されているように、対称の構造をなし
ており、中央に位置して二つの磁気回路を分離す
る厚肉の非磁性筒状ブロツク11と、それにOリ
ング12を介して圧着する中央部で外方に膨出す
るゴムシート2と、そのゴムシート2を押える筒
状鍔付の押え部材13および内側磁性ヨーク14
と、該内側磁性ヨーク14の段部に嵌合するボビ
ン15に巻装されたコイル輪4a,4bと、それ
らを締付ける止めネジを兼ねた外側磁性ヨーク1
6とからなる。なお、符号17,18はそれぞれ
Oリングシールである。ゴムシート2と中央の非
磁性筒状ブロツク11とで囲まれた領域に磁性流
体3が満たされる。コイル輪4a,4bを取り囲
むヨーク、すなわち内側及び外側の磁性ヨーク1
4,16は開磁路構造であり、その磁路が開いて
いる近傍に、ゴムシート2の膨出端が位置するよ
うになつている。つまり、ゴムシート2で封止さ
れた磁性流体3は、コイル輪4a,4b及び内
側・外側磁性ヨーク14,16によつて構成され
るソレノイドにおけるプランジヤーと同じ様なも
のとみなすことができる。従つて、コイル輪4a
に通電すれば磁性流体全体をX方向へ、逆にコイ
ル輪4bに通電すれば磁性流体全体を−X方向へ
動かすことができる。通電をやめれば、ゴムシー
ト2の弾性によつて磁性流体3はもとの位置にも
どる。 An embodiment of the vibration source according to the present invention is shown in FIGS. 2 and 3. A cylindrical outer case 10 is attached to the probe 1 in a direction perpendicular to its central axis, and the vibration source main body is housed inside the outer case 10 . The main body of the vibration source has a symmetrical structure, as clearly shown in FIG. A rubber sheet 2 that bulges outward at the center and is pressed through an O-ring 12, a pressing member 13 with a cylindrical flange that presses down the rubber sheet 2, and an inner magnetic yoke 14.
, coil rings 4a and 4b wound around a bobbin 15 that fits into the stepped portion of the inner magnetic yoke 14, and an outer magnetic yoke 1 that also serves as a set screw to tighten them.
It consists of 6. Note that numerals 17 and 18 are O-ring seals, respectively. A region surrounded by the rubber sheet 2 and the central non-magnetic cylindrical block 11 is filled with magnetic fluid 3. Yokes surrounding the coil rings 4a and 4b, that is, inner and outer magnetic yokes 1
4 and 16 have an open magnetic path structure, and the bulging end of the rubber sheet 2 is located near the open magnetic path. In other words, the magnetic fluid 3 sealed with the rubber sheet 2 can be considered to be similar to a plunger in a solenoid constituted by the coil rings 4a and 4b and the inner and outer magnetic yokes 14 and 16. Therefore, the coil ring 4a
If the coil ring 4b is energized, the entire magnetic fluid can be moved in the X direction, and conversely, if the coil ring 4b is energized, the entire magnetic fluid can be moved in the -X direction. When the electricity is turned off, the elasticity of the rubber sheet 2 causes the magnetic fluid 3 to return to its original position.
このような振源は、受振器等とともに一連のゾ
ンデとして孔井水に挿入される。実際にP波、S
波検層に応用した例を第4図に示す。下からゾン
デの挿入を容易にするための重り40、それぞれ
P波用の上下動受振素子とS波用の水平動受振素
子が組込まれている2個の漂遊型受振器41,4
2と、S波の受振を妨害する孔中音波を遮断する
ためのフイルタチユーブ43、プリアンプ部4
4、ゾンデ本体を伝播する妨害波を防ぐためのダ
ンパ45、本発明に係るS波用振源およびそれと
は別個のP波用振源を内蔵した振源46、該振源
46を駆動する振源ドライバ47がこの順序で連
続しており、シーブ49を介してウインチ50で
孔井10内の所定位置まで上げ下ろしされる。ま
た、地表には制御記録装置52やバツテリ53が
設置される。 Such sources, along with geophones and the like, are inserted into the well water as a series of sondes. In fact, P waves, S waves
Figure 4 shows an example of application to wave logging. A weight 40 for facilitating the insertion of the sonde from below, and two stray geophones 41 and 4 each incorporating a vertical motion receiving element for P waves and a horizontal motion receiving element for S waves.
2, a filter tube 43 for blocking in-hole sound waves that interfere with the reception of S waves, and a preamplifier section 4
4. A damper 45 for preventing interference waves propagating through the sonde body, an oscillation source 46 incorporating the S-wave oscillation source according to the present invention and a separate P-wave oscillation source, and a vibration source 46 for driving the oscillation source 46. The source drivers 47 are successive in this order and are raised and lowered to a predetermined position in the borehole 10 by a winch 50 via a sheave 49. Further, a control recording device 52 and a battery 53 are installed on the ground surface.
測定系のブロツク図を第5図に示す。ゾンデア
センブリ54と制御記録装置52間の信号および
エネルギーの伝送はロギングケーブル55によつ
て行われる。測定モード選択回路60で起振方向
NもしくはR、および入力切換61,62をコン
トロールする。直流高電圧源64からは振源ドラ
イバ47へ電力が供給される。シヨツトパルス発
生器65によつて振源ドライバ47へシヨツトパ
ルスが印加され、磁性流体3を予め定められたN
もしくはR方向に駆動する。それによつて孔内水
は体積変化なしに動かされ、孔軸方向にS波だけ
を輻射できる。参考までに、S波の輻射パターン
を第4図に示しておく。輻射したS波は、漂遊型
受振器41,42で検知され、プリアンプ44で
増幅されてから地表の6チヤンネル波形記憶装置
66に送られて、そこで一時的に記憶されてか
ら、8チヤンネル電磁オシログラフ67で記録紙
にタイムマークと共に記録が取られる。S波の確
認は、起振方向を変えること(NとR)によつて
波形が反転することから確実に行える。これらの
データからS波の速度分布等の解析を行うのは、
従来同様の手法による。 A block diagram of the measurement system is shown in Figure 5. The transmission of signals and energy between the sonde assembly 54 and the control recording device 52 takes place by means of a logging cable 55. A measurement mode selection circuit 60 controls the vibration direction N or R and input switches 61 and 62. Power is supplied from the DC high voltage source 64 to the vibration source driver 47 . A shot pulse is applied to the vibration source driver 47 by the shot pulse generator 65, and the magnetic fluid 3 is heated to a predetermined N.
Or drive in the R direction. As a result, the water in the hole is moved without changing its volume, and only S waves can be radiated in the direction of the hole axis. For reference, the radiation pattern of S waves is shown in Figure 4. The radiated S waves are detected by stray geophones 41 and 42, amplified by a preamplifier 44, and sent to a 6-channel waveform storage device 66 on the ground, where they are temporarily stored and then sent to an 8-channel electromagnetic oscilloscope. A graph 67 is recorded on the recording paper along with time marks. The S wave can be reliably confirmed because the waveform is reversed by changing the direction of vibration (N and R). Analyzing the S wave velocity distribution etc. from these data is as follows.
Using the same method as before.
本発明は、上記のように、コイル輪からの電磁
力を磁性流体に作用させてそれを駆動し、ゴムシ
ートを介して孔内水を直接動かし孔壁に力を及ぼ
すように構成されているから、従来の振源のよう
なメカニカルな機構がないので装置を小型化、簡
略化することができるし、可動部は磁性流体だか
ら孔内水を直接動かしたのと同じとみなせるので
S波の受振の妨げとなるチユーブ・ウエーブやP
波の輻射をほぼ完壁に抑制することができる。す
なわち、孔内水中の振源がP波、チユーブウエー
ブを輻射しないためには、加振作用によつて体積
変化の全くないことが必須要件である。ところが
前掲特開昭54−107401号公報に記載のような、可
動体であるコイルがボデーの中に吊され、その周
囲をゴムチユーブでつつみ、コイルとボデーの間
には空間が形成されている場合、加振前の状態で
コイルの両端面はそれぞれゴムチユーブに接触し
ていても、つぎにコイルを例えば右側に駆動した
とき、右側のゴムチユーブ部分が積極的に押され
て生じた変位と、左側のゴムチユーブ部分が消極
的に引かれて生じた変位とは前者が大であるた
め、左側のコイル端面と該端面に対向する左側の
ゴムチユーブ部分とにはわずかの隙間を生じ、そ
の分、体積変化を招く結果となつた。これに対し
て、本発明の振源では、可動体を磁性流体とした
ことによつて、上記空間相当のものをなくし、全
体を移動させることにより、体積変化のない振源
とすることができるなど、数々のすぐれた効果を
奏しうるものである。 As described above, the present invention is configured so that the electromagnetic force from the coil ring acts on the magnetic fluid to drive it, and the water in the hole is directly moved through the rubber sheet to exert a force on the hole wall. Since there is no mechanical mechanism like a conventional vibration source, the device can be made smaller and simpler, and since the movable part is a magnetic fluid, it can be regarded as the same as directly moving the water in the hole, so the S wave Tube waves and P that impede reception
Wave radiation can be suppressed almost completely. That is, in order for the vibration source in the borehole water not to radiate P waves and tube waves, it is essential that there is no volume change at all due to the vibration action. However, as described in the above-mentioned Japanese Patent Application Laid-Open No. 54-107401, when a movable coil is suspended in a body and surrounded by a rubber tube, a space is formed between the coil and the body. Even though both end faces of the coil are in contact with the rubber tube before excitation, when the coil is then driven, for example, to the right, the rubber tube on the right is actively pushed and the displacement occurs, and the rubber tube on the left is displaced. Since the displacement caused by passively pulling the rubber tube part is large, a slight gap is created between the left side coil end face and the left rubber tube part facing the end face, and the volume change is reduced by that amount. The result was a nuisance. In contrast, in the vibration source of the present invention, by using a magnetic fluid as the movable body, the space equivalent to the above is eliminated, and by moving the entire body, it is possible to create an vibration source with no volume change. It can produce many excellent effects.
第1図は本発明に係る振源の動作原理を示す説
明図、第2図は本発明に係る振源の一実施例を示
す断面図、第3図はその一部破断斜視図、第4図
は使用状態の一例を示す説明図、第5図は測定系
の一例を示す説明図である。
1…プローブ、2…ゴムシート、3…磁性流
体、4a,4b…コイル輪、5…孔内水、6…孔
壁。
FIG. 1 is an explanatory diagram showing the operating principle of the vibration source according to the present invention, FIG. 2 is a sectional view showing an embodiment of the vibration source according to the present invention, FIG. 3 is a partially cutaway perspective view thereof, and FIG. The figure is an explanatory diagram showing an example of a usage state, and FIG. 5 is an explanatory diagram showing an example of a measurement system. DESCRIPTION OF SYMBOLS 1... Probe, 2... Rubber sheet, 3... Magnetic fluid, 4a, 4b... Coil ring, 5... Hole water, 6... Hole wall.
Claims (1)
けた可動体を運動させることによつてそれに接し
ている孔内水を介して孔軸に直交する一方向の孔
壁面に振源力を作用させるS波用振源において、
前記可動体は、ゴムシート及びそれによつて封止
されている磁性流体であり、その外側端部近傍に
設けた電磁コイル部に通電することによつて、前
記磁性流体に電磁力を作用させ、駆動するように
したS波検層用振源。1 It is inserted into a borehole that has borehole water, and by moving a movable body installed inside, a vibration source force is applied to the borehole wall surface in one direction perpendicular to the borehole axis through the borehole water that is in contact with it. In the S-wave vibration source to be applied,
The movable body is a rubber sheet and a magnetic fluid sealed by the rubber sheet, and an electromagnetic force is applied to the magnetic fluid by energizing an electromagnetic coil section provided near an outer end of the movable body, A driven vibration source for S-wave logging.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP7623580A JPS573065A (en) | 1980-06-06 | 1980-06-06 | Exciting source for s wave detecting layer |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP7623580A JPS573065A (en) | 1980-06-06 | 1980-06-06 | Exciting source for s wave detecting layer |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS573065A JPS573065A (en) | 1982-01-08 |
| JPS6214791B2 true JPS6214791B2 (en) | 1987-04-03 |
Family
ID=13599498
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP7623580A Granted JPS573065A (en) | 1980-06-06 | 1980-06-06 | Exciting source for s wave detecting layer |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS573065A (en) |
Families Citing this family (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US4932003A (en) * | 1982-05-19 | 1990-06-05 | Exxon Production Research Company | Acoustic quadrupole shear wave logging device |
| MA19839A1 (en) * | 1982-07-06 | 1984-04-01 | Exxon Production Research Co | ACOUSTIC LOGGING APPARATUS AND METHOD AND METHOD FOR REDUCING NOISE FROM COMPRESSION AND STONELEY WAVES. |
| JP4984242B2 (en) * | 2007-01-30 | 2012-07-25 | 独立行政法人産業技術総合研究所 | Stationary earthquake source using electromagnetic coil |
Family Cites Families (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS54107401A (en) * | 1978-02-09 | 1979-08-23 | Nagarou Kozaki | Vibrating method for s wave detecting layer |
-
1980
- 1980-06-06 JP JP7623580A patent/JPS573065A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS573065A (en) | 1982-01-08 |
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