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JPS6161610B2 - - Google Patents
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JPS6161610B2 - - Google Patents

Info

Publication number
JPS6161610B2
JPS6161610B2 JP56052028A JP5202881A JPS6161610B2 JP S6161610 B2 JPS6161610 B2 JP S6161610B2 JP 56052028 A JP56052028 A JP 56052028A JP 5202881 A JP5202881 A JP 5202881A JP S6161610 B2 JPS6161610 B2 JP S6161610B2
Authority
JP
Japan
Prior art keywords
seismometer
flux density
adjust
magnetic flux
magnetic
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
Application number
JP56052028A
Other languages
Japanese (ja)
Other versions
JPS57166526A (en
Inventor
Haruhisa Saito
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.)
Mitsubishi Electric Corp
Original Assignee
Mitsubishi Electric Corp
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 Mitsubishi Electric Corp filed Critical Mitsubishi Electric Corp
Priority to JP56052028A priority Critical patent/JPS57166526A/en
Publication of JPS57166526A publication Critical patent/JPS57166526A/en
Publication of JPS6161610B2 publication Critical patent/JPS6161610B2/ja
Granted legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01VGEOPHYSICS; GRAVITATIONAL MEASUREMENTS; DETECTING MASSES OR OBJECTS; TAGS
    • G01V1/00Seismology; Seismic or acoustic prospecting or detecting
    • G01V1/16Receiving elements for seismic signals; Arrangements or adaptations of receiving elements
    • G01V1/18Receiving elements, e.g. seismometer, geophone or torque detectors, for localised single point measurements
    • G01V1/181Geophones

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)
  • Measurement Of Mechanical Vibrations Or Ultrasonic Waves (AREA)

Description

【発明の詳細な説明】 この発明は、可動コイル型の地震計に関するも
のである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a moving coil type seismometer.

従来の地震計の概略構造図を第1図に示す。第
1図において、1はヨーク、3はポールピース、
4はマグネツト、5は検出コイル、6は出力引き
出し線、7はコイル巻き枠、8は付加質量体、9
はスプリング固定ホルダ、10はスプリングであ
る。
Figure 1 shows a schematic structural diagram of a conventional seismometer. In Figure 1, 1 is a yoke, 3 is a pole piece,
4 is a magnet, 5 is a detection coil, 6 is an output lead wire, 7 is a coil winding frame, 8 is an additional mass body, 9
1 is a spring fixed holder, and 10 is a spring.

次に動作について説明する。 Next, the operation will be explained.

一般に地震計においては、地盤の種々雑多な振
動より地震振動だけを検出する必要がある。その
ため地震計は、計測目的に合わせて検出可能な帯
域が調整されている。可動コイル型地震計の出力
特性は一般に次式によつて表わされる。
In general, seismometers need to detect only seismic vibrations rather than various other vibrations in the ground. Therefore, the detectable band of seismometers is adjusted according to the purpose of measurement. The output characteristics of a moving coil seismometer are generally expressed by the following equation.

h=Bg・ι/4π・m・f・R ……(3) ここに、f0:固有振動数、S:スプリングのス
テイフネス、m:振動系等価質量、U:出力値、
f:任意の周波数、h:減衰定数、R:回路全抵
抗、Bg:磁気回路磁気空隙中の磁束密度、ι:
可動コイル長さを示す。
h=Bg 2・ι 2 /4π・m・f 0・R ...(3) Here, f 0 : Natural frequency, S: Stiffness of spring, m: Equivalent mass of vibration system, U: Output value,
f: arbitrary frequency, h: attenuation constant, R: total circuit resistance, Bg: magnetic flux density in the magnetic air gap of the magnetic circuit, ι:
Indicates the moving coil length.

第(2)式よりわかるように、f=f0時に出力値U
は最大となり、第(3)式により決まる減衰定数hの
値により使用可能な帯域が決まる(第3図参
照)。すなわち、第3図に示すように、横軸に
f/f0を、縦軸に出力をとつたとき、減衰定数h
の値が大きくなる矢印A方向にしたがつて曲線
C1,C2,C3のような特性となり、それぞれ使用
帯域はB1,B2,B3となる。
As can be seen from equation (2), when f=f 0 , the output value U
is the maximum, and the usable band is determined by the value of the attenuation constant h determined by equation (3) (see FIG. 3). In other words, as shown in Figure 3, when f/f 0 is plotted on the horizontal axis and output is plotted on the vertical axis, the damping constant h
The curve increases in the direction of arrow A, where the value of
The characteristics are C 1 , C 2 , and C 3 , and the used bands are B 1 , B 2 , and B 3 , respectively.

ところで、地震計において、目的とする帯域に
地震計の使用可能帯域を合わせるために、固有振
動数f0の調整と減衰定数hの調整を行う必要があ
る。ここに使用帯域幅だけを調整しようとした場
合、第(2)式よりわかるように減衰定数hを調整す
ればよい。hの調整は第(3)式よりBg,ι,m,
f0,Rのいずれからの定数を調整すればよいが、
f0は帯域中心値が動いてしまうので動かせない。
mはf0を固定してしまうと、Sの値も同時に調整
しなければならない。ι,Rは互いに関連をもつ
ているため、一方の値のみの調整はできない。ま
た、可動コイルは巻きほどく方向の調整のみが可
能であり、hの減少方向の調整のみが可能であ
る。このような理由によりhの調整には、Bgの
調整によることが最も簡便な方法であることがわ
かる。しかし従来の地震計においては、Bgの値
の調整は地震計を一度分解し、着磁・減磁を行つ
て目的のBgの値を得るか、または分解しないま
まで着磁・減磁測定を繰り返し、目的の帯域幅に
合わせるという方法が必要であつた。また、着
磁・減磁のための高価な装置も必要としていた。
By the way, in a seismometer, in order to match the usable band of the seismometer to the target band, it is necessary to adjust the natural frequency f 0 and the damping constant h. If one attempts to adjust only the used bandwidth, the attenuation constant h may be adjusted as shown in equation (2). The adjustment of h is based on equation (3) using Bg, ι, m,
You can adjust the constant from either f 0 or R, but
f 0 cannot be moved because the band center value will move.
If m is fixed at f 0 , the value of S must be adjusted at the same time. Since ι and R are related to each other, it is not possible to adjust only one value. Further, the movable coil can only be adjusted in the unwinding direction, and only in the decreasing direction of h. For these reasons, it can be seen that the easiest way to adjust h is to adjust Bg. However, in conventional seismometers, to adjust the Bg value, either disassemble the seismometer and perform magnetization/demagnetization to obtain the desired Bg value, or measure magnetization/demagnetization without disassembling it. A method of repeatedly adjusting to the desired bandwidth was required. It also required expensive equipment for magnetization and demagnetization.

この発明は上述の点にかんがみなされたもの
で、地震計組立後でも外部より簡便にBgの調整
を可能にすることにより、高価な装置や繁雑な調
整なしにhの調整を可能とすることを目的として
いる。以下この発明の一実施例について説明す
る。
This invention was made in consideration of the above points, and aims to make it possible to adjust Bg easily from the outside even after assembling the seismometer, thereby making it possible to adjust h without expensive equipment or complicated adjustments. The purpose is An embodiment of this invention will be described below.

第2図はこの発明の一実施例を示すものであ
る。この図において、2は外周にねじが切られ、
中心部にねじ回し用溝が付いた磁束密度調整用プ
レートである。1aは前記ヨーク1の下部マグネ
ツト貼付面の一部にあけられたねじ孔である。こ
のねじ孔1aに磁束密度調整用プレート2を磁気
回路組立後ねじ込む。
FIG. 2 shows an embodiment of the present invention. In this figure, 2 is threaded on the outer periphery;
This is a magnetic flux density adjustment plate with a screwdriver groove in the center. Reference numeral 1a denotes a screw hole drilled in a part of the lower magnet attachment surface of the yoke 1. After assembling the magnetic circuit, the magnetic flux density adjusting plate 2 is screwed into this screw hole 1a.

第2図のような磁束密度調整用プレート2を有
した磁気回路を備える地震計においては、可動コ
イルの挿入される磁気空隙の他に、マグネツト4
の下部のヨーク1の底面に連続的に可変できる磁
気抵抗を備えていることになる。この連続的に可
変できる磁気抵抗、すなわち磁束密度調整用プレ
ート2をねじ回しにより回転することにより、マ
グネツト4と磁束密度調整用プレート2との空隙
が連続的に変化し、Bgが連続的に可変できる。
また、第2図のような構成にすれば、Bgの調整
は、地震計組立完成後でも容易に可能となる。
In a seismograph equipped with a magnetic circuit having a magnetic flux density adjustment plate 2 as shown in Fig. 2, in addition to the magnetic gap into which the moving coil is inserted, the magnet 4
A continuously variable magnetic resistance is provided on the bottom surface of the yoke 1 at the bottom of the yoke. This continuously variable magnetic resistance, that is, by rotating the magnetic flux density adjustment plate 2 with a screwdriver, the gap between the magnet 4 and the magnetic flux density adjustment plate 2 changes continuously, and Bg can be continuously changed. can.
Furthermore, if the configuration is as shown in Figure 2, Bg adjustment can be easily made even after the seismometer is assembled.

以上説明したように、この発明は可動コイル型
地震計においてBgを外部より容易に調整可能と
しているので、組立完成後においても分解するこ
となしに、容易にhの調整が可能であり、使用目
的に応じて簡便に効率の良い調整が可能である利
点を有する。
As explained above, this invention allows Bg to be easily adjusted from the outside in a moving coil seismometer, so even after assembly is completed, h can be easily adjusted without disassembling it, and it is possible to adjust h without disassembling it even after assembly is completed. It has the advantage that it can be easily and efficiently adjusted depending on the situation.

【図面の簡単な説明】[Brief explanation of the drawing]

第1図は従来の可動コイル型地震計を示す断面
図、第2図はこの発明の一実施例を示す断面図、
第3図は地震計の出力と周波数との関係を示す特
性図である。 図中、1はヨーク、1aはねじ孔、2は磁束密
度調整用プレート、3はポールピース、4はマグ
ネツト、5は検出コイル、6は出力引き出し線、
7はコイル巻き枠、8は付加質量体、9はスプリ
ング固定ホルダ、10はスプリングである。な
お、図中の同一符号は同一または相当部分を示
す。
FIG. 1 is a sectional view showing a conventional moving coil seismometer, and FIG. 2 is a sectional view showing an embodiment of the present invention.
FIG. 3 is a characteristic diagram showing the relationship between the output of the seismograph and the frequency. In the figure, 1 is a yoke, 1a is a screw hole, 2 is a magnetic flux density adjustment plate, 3 is a pole piece, 4 is a magnet, 5 is a detection coil, 6 is an output lead wire,
7 is a coil winding frame, 8 is an additional mass body, 9 is a spring fixing holder, and 10 is a spring. Note that the same reference numerals in the figures indicate the same or corresponding parts.

Claims (1)

【特許請求の範囲】[Claims] 1 可動コイル型地震計において、磁気回路を構
成するヨーク中にねじ孔を形成しこのねじ孔に磁
気空隙の磁束密度を外部より調整する磁束密度調
整用プレートを螺合したことを特徴とする地震
計。
1. An earthquake characterized in that, in a moving coil seismometer, a screw hole is formed in the yoke constituting the magnetic circuit, and a magnetic flux density adjustment plate for adjusting the magnetic flux density of the magnetic gap from the outside is screwed into the screw hole. Total.
JP56052028A 1981-04-07 1981-04-07 Seismometer Granted JPS57166526A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP56052028A JPS57166526A (en) 1981-04-07 1981-04-07 Seismometer

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP56052028A JPS57166526A (en) 1981-04-07 1981-04-07 Seismometer

Publications (2)

Publication Number Publication Date
JPS57166526A JPS57166526A (en) 1982-10-14
JPS6161610B2 true JPS6161610B2 (en) 1986-12-26

Family

ID=12903352

Family Applications (1)

Application Number Title Priority Date Filing Date
JP56052028A Granted JPS57166526A (en) 1981-04-07 1981-04-07 Seismometer

Country Status (1)

Country Link
JP (1) JPS57166526A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6344209U (en) * 1986-09-10 1988-03-24

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
FR2788163B1 (en) * 1998-12-30 2001-03-16 Sextant Avionique ELECTROMAGNETIC ACTUATOR EQUIPPED WITH MEANS FOR ADJUSTING THE POSITION OF ITS MOBILE POLAR ELEMENT

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6344209U (en) * 1986-09-10 1988-03-24

Also Published As

Publication number Publication date
JPS57166526A (en) 1982-10-14

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