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JPH0245137B2 - - Google Patents
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JPH0245137B2 - - Google Patents

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Publication number
JPH0245137B2
JPH0245137B2 JP59269964A JP26996484A JPH0245137B2 JP H0245137 B2 JPH0245137 B2 JP H0245137B2 JP 59269964 A JP59269964 A JP 59269964A JP 26996484 A JP26996484 A JP 26996484A JP H0245137 B2 JPH0245137 B2 JP H0245137B2
Authority
JP
Japan
Prior art keywords
light
signal
output
liquid
light source
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 - Lifetime
Application number
JP59269964A
Other languages
Japanese (ja)
Other versions
JPS61147117A (en
Inventor
Hiroshi Ko
Takashi Tokuyama
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.)
Fuji Tetsuku Kk
Original Assignee
Fuji Tetsuku Kk
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 Fuji Tetsuku Kk filed Critical Fuji Tetsuku Kk
Priority to JP59269964A priority Critical patent/JPS61147117A/en
Priority to GB08510935A priority patent/GB2160319B/en
Priority to US06/729,117 priority patent/US4662225A/en
Publication of JPS61147117A publication Critical patent/JPS61147117A/en
Publication of JPH0245137B2 publication Critical patent/JPH0245137B2/ja
Granted legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01HMEASUREMENT OF MECHANICAL VIBRATIONS OR ULTRASONIC, SONIC OR INFRASONIC WAVES
    • G01H9/00Measuring mechanical vibrations or ultrasonic, sonic or infrasonic waves by using radiation-sensitive means, e.g. optical means

Landscapes

  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Measurement Of Mechanical Vibrations Or Ultrasonic Waves (AREA)
  • Geophysics And Detection Of Objects (AREA)

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は、地震等による振動を感知する地震感
知器に関するものである。
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to an earthquake sensor that detects vibrations caused by earthquakes and the like.

〔従来の技術及び発明が解決しようとする問題点〕[Problems to be solved by conventional technology and invention]

まず、地震の周波数について説明する。 First, we will explain the frequency of earthquakes.

一般に地震波の主成分の周波数は1〜10Hzにあ
ると言われているが、そのうち特に1〜5Hzの成
分が顕著である。第2図に昭和53年6月12日17時
14分に発生した宮城県沖地震について、一例とし
て大船渡で観測された地震波のパワースペクトル
を示す。卓越振動数は2〜3Hz(2.4Hz)で、1
〜5Hzのパワーが大きい(図示していないが、フ
ーリエスペクトルもほぼ同様な形状で1〜5Hz成
分が多い)。
It is generally said that the main component of seismic waves has a frequency of 1 to 10 Hz, and among these, the 1 to 5 Hz component is particularly prominent. Figure 2 shows 17:00 on June 12, 1978.
As an example, the power spectrum of the seismic waves observed in Ofunato is shown for the Miyagi Prefecture-Oki Earthquake that occurred on the 14th minute. The predominant frequency is 2-3Hz (2.4Hz), 1
-5Hz power is large (although not shown, the Fourier spectrum has almost the same shape and has many 1-5Hz components).

又、電車、ダンプカー、建築工事及び回転機械
等種々の原因による地盤及び建物の微小振動は地
震波とは異なり外乱振動となるが、この外乱振動
は20Hz以上のものが多いが10Hz近傍のものも含ま
れるので誤動作防止の点より日本エレベータ協会
の耐震設計・施工指針の技術基準においては、感
知器の周波数特性として「普通級は1〜5Hzの範
囲でフラツト特性、精密級では0.1〜5Hzの範囲
でフラツト特性、5Hzを越える範囲では感度は下
降特性とすること」となつている。
In addition, minute vibrations in the ground and buildings caused by various causes such as trains, dump trucks, construction work, and rotating machinery are different from seismic waves and constitute disturbance vibrations, but these disturbance vibrations are often over 20Hz, but also include vibrations around 10Hz. Therefore, in order to prevent malfunction, the Japan Elevator Association's technical standards for seismic design and construction guidelines state that the frequency characteristics of the sensor are ``a flat characteristic in the range of 1 to 5 Hz for normal grade, and a flat characteristic in the range of 0.1 to 5 Hz for precision grade. The sensitivity should be flat in the range exceeding 5 Hz.''

上記のような地震の特性に対して、従来の地震
感知器としては、電気式の動電型やストレーンゲ
ージ型、圧電型、或いは機械式の重錘落下型など
が一般に用いられている。
In response to the above-mentioned characteristics of earthquakes, conventional earthquake sensors are generally of an electrodynamic type, a strain gauge type, a piezoelectric type, or a mechanical weight drop type.

第3図に、動電型地震感知器の構造の一例(垂
直方向感知器)を示す。この動電型地震感知器
は、永久磁石4により発生する磁束5の中を、お
もり2に固定されたコイル3が振動により上下に
動くと、コイル3の両端に電圧が発生し、この電
圧の大きさがコイル3の移動速度に比例すること
を利用して地震を感知するものである。なお、1
はおもり2を支持するばね系であり、6は磁路を
形成するヨークである。このばね系1の固有振動
数は、普通4Hz程度にとられているが、この方式
で周波数特性を前述のように5Hz以上で下降特性
とするのは難しく(ばね系の問題)、通常10Hz程
度以上で下降特性にしている。更に固有振動数
は、ばね系1やおもり2の精度に大きく影響を受
けるので、実際には、最終の工程で手加工により
おもりの重さ等を調整している。すなわち、この
動電型地震感知器は精度や調整の手間の点で問題
を有している。
FIG. 3 shows an example of the structure of an electrodynamic earthquake sensor (vertical sensor). In this electrodynamic earthquake sensor, when a coil 3 fixed to a weight 2 moves up and down due to vibration in a magnetic flux 5 generated by a permanent magnet 4, a voltage is generated at both ends of the coil 3. Earthquakes are sensed by utilizing the fact that the size is proportional to the moving speed of the coil 3. In addition, 1
6 is a spring system that supports the weight 2, and 6 is a yoke that forms a magnetic path. The natural frequency of this spring system 1 is normally set to about 4 Hz, but it is difficult to make the frequency characteristics fall above 5 Hz as mentioned above with this method (spring system problem), and it is usually about 10 Hz. The above results in a descending characteristic. Furthermore, since the natural frequency is greatly affected by the precision of the spring system 1 and the weight 2, the weight of the weight, etc. is actually adjusted by hand in the final process. In other words, this electrodynamic seismic sensor has problems in terms of accuracy and the amount of effort required for adjustment.

また、ストレーンゲージ型地震感知器は、スト
レーンゲージ(歪ゲージ)をX、Y方向に設置
し、これらの電気出力をベクトル合成して加速度
を求めるものであるが、歪ゲージ自身の周波数特
性は数KHzにも及ぶので、電気的フイルターで5
Hz以上を減衰させるようにしている。従つてスト
レーンゲージ型の地震感知器はこのフイルターの
特性に大きく左右され、更にベクトル合成を行う
為に掛算器等を必要とするなど、多くの誤差要因
を含んでおり信頼性の点で問題がある。なお、圧
電型地震感知器もベクトル合成方式を採用してお
り、同様の問題点を含んでいる。
In addition, in a strain gauge type earthquake sensor, strain gauges are installed in the X and Y directions, and their electrical outputs are vector-combined to obtain acceleration, but the frequency characteristics of the strain gauges themselves are Since it reaches up to KHz, an electric filter can be used to
It is designed to attenuate frequencies above Hz. Therefore, strain gauge type earthquake detectors are greatly affected by the characteristics of this filter, and also include many error factors, such as the need for multipliers to perform vector synthesis, which poses problems in terms of reliability. be. Note that piezoelectric earthquake sensors also use a vector synthesis method and have similar problems.

第4図は、重錘落下型地震感知器の構造の一例
を示すものである。これは、静止状態では重錘
(鉄等の磁性体)13が、ケース10に固定され
た永久磁石11に吸引されているが、ある一定以
上の振動が発生するとこの重錘13が落下し、重
錘13にはめ込まれているレバー12が支点15
を中心に矢印方向に回転することにより、マイク
ロスイツチ14のアクチユエータ14′を作動さ
せて地震を感知するものである。この方式は簡単
ではあるが、磁石の吸引力と重錘の重さの関係に
よつて感知レベルが左右され、その調整が大変で
あると同時に低い周波数(1Hz以下)では感知し
にくいという欠点があり、やはり精度や信頼性の
点で問題がある。
FIG. 4 shows an example of the structure of a falling weight type earthquake sensor. This is because in a stationary state, a weight 13 (magnetic material such as iron) is attracted to the permanent magnet 11 fixed to the case 10, but when vibrations above a certain level occur, the weight 13 falls. The lever 12 fitted into the weight 13 is the fulcrum 15
By rotating in the direction of the arrow around the center, the actuator 14' of the micro switch 14 is actuated to sense an earthquake. Although this method is simple, the sensing level is affected by the relationship between the attraction force of the magnet and the weight of the weight, and it is difficult to adjust, and at the same time, it has the disadvantage that it is difficult to detect at low frequencies (1 Hz or less). However, there are still problems with accuracy and reliability.

このため、出願人は特願昭59−88902号にて新
しいタイプの地震感知器を提案した。それは第5
図及び第6図に示すように、円柱状の容器31に
例えば水銀や油のような液体32を入れ、この容
器31の蓋には発光ダイオード等の光源34と液
体32からの反射光を受光する受光素子35を備
えて、地震波により容器31内の液体32が揺動
すると、この液体表面の形状が変わることによつ
て変化する反射光の輝度分布を受光素子35によ
り電気信号に変換出力したものを信号処理部21
がこの出力信号20aの大きさに応じて振動レベ
ルを識別する新しいタイプの地震感知器である。
For this reason, the applicant proposed a new type of earthquake sensor in Japanese Patent Application No. 88902/1983. That's the fifth
As shown in FIG. 6 and FIG. 6, a liquid 32 such as mercury or oil is placed in a cylindrical container 31, and a light source 34 such as a light emitting diode is mounted on the lid of the container 31 to receive reflected light from the liquid 32. When the liquid 32 in the container 31 is shaken by seismic waves, the luminance distribution of reflected light that changes due to the change in the shape of the liquid surface is converted into an electrical signal by the light receiving element 35 and output. signal processing unit 21
This is a new type of earthquake sensor that identifies the vibration level according to the magnitude of this output signal 20a.

この地震感知器の動作原理は次のとおりであ
る。
The operating principle of this earthquake sensor is as follows.

即ち、簡単のため液体の入つた小円筒容器を一
定振動加速度で水平方向に振動させたときの液体
の表面の波の動きは、振動加速度の大きさをA、
重力の加速度をg、波の振幅をa、その波長をλ
とし、波の進路に沿つてx軸をとるとすれば第8
図に示すように、小円筒容器の側壁のところがち
ようど山ないし谷になる1/2波長の正弦波の振動
が主成分となる振動をする。そして、液面の傾斜
角θはその値が小さい場合には次の式で与えられ
る。
That is, for simplicity, when a small cylindrical container containing a liquid is vibrated in the horizontal direction with a constant vibration acceleration, the wave movement on the surface of the liquid is expressed as A, the magnitude of the vibration acceleration,
The acceleration of gravity is g, the amplitude of the wave is a, and its wavelength is λ
If we take the x-axis along the wave path, then the 8th
As shown in the figure, the main component of the vibration is a 1/2-wavelength sine wave that forms peaks or valleys on the side wall of the small cylindrical container. When the angle of inclination θ of the liquid level is small, it is given by the following equation.

θ=A/g=2πa/λ・cos2πx/λ…… つまり、振動加速度の大きさAは液体表面の傾
斜角に比例するから振動加速度を検出するために
は液体表面の傾斜角を検出すればよいことにな
る。
θ=A/g=2πa/λ・cos2πx/λ...In other words, the magnitude A of the vibrational acceleration is proportional to the inclination angle of the liquid surface, so in order to detect the vibrational acceleration, we need to detect the inclination angle of the liquid surface. It will be a good thing.

このような円筒容器内の波は、側壁のところで
液体が鉛直方向に動かなければならず、この波の
パターンは山ないし谷がちようど側壁の位置にく
るような大きさになり、水平加振時は第8図、上
下加振時は第9図を基本波モードとする波とな
る。
Waves in a cylindrical container like this require the liquid to move vertically at the side wall, and the wave pattern is large enough to have peaks or troughs at the side wall, resulting in horizontal excitation. The fundamental wave mode is as shown in FIG. 8 at the time, and as shown in FIG. 9 during vertical vibration.

次に、液面の傾斜角を検出する基本的な光学系
は第10図に示すとおりである。
Next, the basic optical system for detecting the angle of inclination of the liquid level is shown in FIG.

即ち、液面への入射光束をφ1、静止した液面
での反射光束をφ2、傾いた液面での反射光束を
φ3、傾斜角θだけ液面が変化したときの光電変
換素子へ入射する光束の変化量をφ4とすると、
図から明らかなように液面がθなる角度だけ傾く
と、反射光束の移動角は2θとなるので、結局光電
変換素子への入射光束の変化量φ4(液体表面から
の反射光束の変化量)はθに比例することにな
る。
That is, the incident light beam on the liquid surface is φ 1 , the reflected light beam on the stationary liquid surface is φ 2 , the reflected light beam on the tilted liquid surface is φ 3 , and the photoelectric conversion element when the liquid surface changes by the tilt angle θ If the amount of change in the luminous flux incident on is φ 4 , then
As is clear from the figure, when the liquid surface is tilted by an angle of θ, the moving angle of the reflected light flux becomes 2θ, so the amount of change in the light flux incident on the photoelectric conversion element is φ 4 (the amount of change in the light flux reflected from the liquid surface) ) is proportional to θ.

今、光電変換素子としてホトダイオードのよう
なものを使用すると、その出力は入射光束(光
量)に比例するから、円筒容器が加速されると、
そのときの出力uは式を考慮すれば次のような
式で表わされる。
Now, when we use something like a photodiode as a photoelectric conversion element, its output is proportional to the incident luminous flux (light amount), so when the cylindrical container is accelerated,
The output u at that time can be expressed by the following formula, considering the formula.

u=K1・θ=K2・A …… 但し、K1、K2は定数 つまり、光電変換素子の出力は振動加速度に比
例する。
u= K1・θ= K2・A... However, K1 and K2 are constants. In other words, the output of the photoelectric conversion element is proportional to the vibration acceleration.

即ち、この地震感知器は感知部20の受光素子
35から出力された振動加速度に比例した信号2
0aを交流増幅器22により増幅し、コンパレー
タ23,25等により複数のレベルの地震を感知
するものであるが、この感知特性に影響を及ぼす
要素としては、容器の形状、液体の種類や量、発
受光素子自体の特性など種々雑多なものが考えら
れ、とりわけ電源電圧変動、周囲温度変化や経年
変化等に起因する発光素子の発光量の変動や受光
素子の受光量の変動は感知部20の出力電圧20
aの出力レベルを大きく変動させることになり、
地震感知器の感度や精度に大きな影響を与える恐
れがある。
That is, this earthquake sensor receives a signal 2 proportional to the vibration acceleration output from the light receiving element 35 of the sensing section 20.
0a is amplified by an AC amplifier 22, and multiple levels of earthquakes are detected by comparators 23, 25, etc., but factors that affect this sensing characteristic include the shape of the container, the type and amount of liquid, and the emitted Various miscellaneous factors such as the characteristics of the light-receiving element itself can be considered, and in particular, fluctuations in the amount of light emitted by the light-emitting element and fluctuations in the amount of light received by the light-receiving element due to fluctuations in power supply voltage, changes in ambient temperature, changes over time, etc. voltage 20
This will cause the output level of a to fluctuate greatly,
There is a risk that the sensitivity and accuracy of earthquake detectors will be significantly affected.

本発明は上記の点に鑑みなされたもので、たと
え環境の変化や経年変化が起つても、それらの影
響を受ける恐れがなく永年の使用に十分耐えうる
感度補正付地震感知器を提供することを目的とす
る。
The present invention has been made in view of the above points, and it is an object of the present invention to provide an earthquake sensor with sensitivity correction that can withstand long-term use without the risk of being affected by changes in the environment or changes over time. With the goal.

〔問題点を解決するための手段〕[Means for solving problems]

本発明は、外部からの光を遮断する密閉構造の
容器を備え、該容器には光を反射する液体が入つ
ており、液体の上方には容器内を照射する光源
と、光源が発する光のうち液体表面からの反射光
を受光し、その光量を電気信号に変換する光電変
換素子とを設け、液体の液面の傾きを液体表面か
らの反射光量の変化として捉え、光電変換素子の
出力電気信号が所定値よりも大きいとき出力を発
する信号処理部を備えた地震感知器において、常
に一定の電圧指令を出力する基準電圧器と、光電
変換素子の出力電気信号から直流成分を取り出す
フイルタとを設け、基準電圧器の電圧指令とフイ
ルタの直流成分とを比較しその差信号を増幅出力
する比較増幅器を備え、比較増幅器の出力信号に
応じて光源に流れる電圧を制御する電流制御部を
備えるものである。
The present invention includes a container with a sealed structure that blocks light from the outside, the container contains a liquid that reflects light, and above the liquid there is a light source that illuminates the inside of the container, and a light source that reflects the light emitted by the light source. A photoelectric conversion element that receives reflected light from the liquid surface and converts the amount of light into an electrical signal is installed. An earthquake sensor equipped with a signal processing unit that outputs an output when a signal is larger than a predetermined value includes a reference voltage generator that always outputs a constant voltage command, and a filter that extracts a DC component from the output electrical signal of a photoelectric conversion element. A comparison amplifier that compares the voltage command of the reference voltage generator with the DC component of the filter and amplifies and outputs the difference signal, and a current control section that controls the voltage flowing to the light source according to the output signal of the comparison amplifier. It is.

〔作用〕[Effect]

上述の如く構成すれば、直流成分が常に一定の
電圧値になるように光源の明るさが制御される。
With the above configuration, the brightness of the light source is controlled so that the DC component always has a constant voltage value.

〔実施例〕〔Example〕

第1図は本発明の一実施例の構成を示すブロツ
ク図で、第5図及び第6図と同一符号のものは同
一のものを示すが、40は感知部20の出力信号
20aの直流成分を取り出すフイルタ、41は直
流増幅器、42は常に一定の電圧指令42aを出
力する基準電圧器、43は基準電圧器42の電圧
指令42aと直流増幅器41の出力信号41aと
を比較し、その差信号を増幅出力する比較増幅
器、44は比較増幅器43の出力信号43aに応
じて発光素子34に流れる電流を制御する、例え
ばトランジスタ等で構成される電流制御部、45
は例えばそれぞれ違う4つの基準レベルの電圧4
5a1,45a2,45a3,45a4(例えば
昇降機の技術基準の設定値を参考にして、45a
1は10gal、45a2は80gal、45a3は
120gal、45a4は150galに対応する電圧値)を
出力している基準電圧器、46,47,48,4
9は帯域通過フイルタを含む交流増幅器22′の
出力信号22′aつまり感知部20の出力信号2
0aの交流信号と基準電圧器45の各レベル電圧
45a1,45a2,45a3,45a4とを比
較し信号22′aの方が大きい場合はHighレベ
ル、信号22′aの方が小さい場合はLowレベル
の信号を出力するコンパレータ、50はコンパレ
ータ46がパルス信号を出力すればそれを計数し
計数した値が所定値に達すればHighレベルの出
力信号50aを発するカウンタ、51はコンパレ
ータ46が一旦Highレベルの出力信号を出力し
て後所定時間経過してもコンパレータ47が
Highレベルの出力信号を出力しなければあるい
はコンパレータ46がHighレベル、コンパレー
タ47がLowレベル信号を出力する状態が所定
時間続ければHighレベル信号を出力する自動リ
セツト信号発生装置、52は4つのRSフリツプ
フロツプからなる記憶装置で、端子S1,S2,
S3,S4にHighレベルの信号が入力されれば
端子R1,R2,R3,R4にHighレベルのリ
セツト信号が入力されないかぎり端子01,0
2,03,04にHighレベルの信号を出力しつ
づける。
FIG. 1 is a block diagram showing the configuration of an embodiment of the present invention, in which the same reference numerals as in FIGS. 41 is a DC amplifier, 42 is a reference voltage generator that always outputs a constant voltage command 42a, and 43 is a filter that compares the voltage command 42a of the reference voltage generator 42 and the output signal 41a of the DC amplifier 41, and generates a difference signal. A comparison amplifier 44 amplifies and outputs the output signal 43a, and a current control section 45 composed of, for example, a transistor, which controls the current flowing through the light emitting element 34 in accordance with the output signal 43a of the comparison amplifier 43.
For example, there are four different reference level voltages 4.
5a1, 45a2, 45a3, 45a4 (for example, 45a with reference to the setting values of technical standards for elevators)
1 is 10gal, 45a2 is 80gal, 45a3 is
120gal, 45a4 is a reference voltage generator that outputs the voltage value corresponding to 150gal), 46, 47, 48, 4
9 is the output signal 22'a of the AC amplifier 22' including a bandpass filter, that is, the output signal 2 of the sensing section 20.
Compare the AC signal 0a with each level voltage 45a1, 45a2, 45a3, 45a4 of the reference voltage generator 45, and if the signal 22'a is larger, it is a high level, and if the signal 22'a is smaller, it is a low level. A comparator that outputs a signal; 50 is a counter that counts when the comparator 46 outputs a pulse signal; and when the counted value reaches a predetermined value, outputs a high-level output signal 50a; 51 is a counter that outputs a high-level output once the comparator 46 outputs a high-level signal; Even if a predetermined period of time elapses after outputting the signal, the comparator 47
52 is an automatic reset signal generator that outputs a high level signal if it does not output a high level output signal or if the state in which the comparator 46 outputs a high level signal and the comparator 47 outputs a low level signal continues for a predetermined period of time; 52 is a four RS flip-flop; A storage device consisting of terminals S1, S2,
If a high level signal is input to S3 and S4, terminals 01 and 0 will be reset unless a high level reset signal is input to terminals R1, R2, R3, and R4.
It continues to output high level signals on 2, 03, and 04.

ここで地震感知器の容器が静止状態に置かれて
いる場合は、容器の内の液体も静止状態にあり、
従つて容器内の輝度分布は一定で受光素子35の
出力信号20aも第7図aに示すとおり一定の直
流電圧のみであるが、地震等の振動により容器内
の液体が揺動すると、液体の表面の形状が変わり
光の反射や散乱の形態が変化して容器内の輝度分
布も変化し、それに対応して前述の原理に基づき
受光素子35の出力信号20aも第7図b及びc
に示すように変化する。(第7図bは振動数が低
い場合、第7図cは振動数が高い場合を示す)そ
して振動の加速度と出力信号20aの変流成分の
電圧とは略比例関係にある。
Here, if the container of the earthquake sensor is placed in a stationary state, the liquid inside the container is also in a stationary state,
Therefore, the brightness distribution inside the container is constant and the output signal 20a of the light receiving element 35 is only a constant DC voltage as shown in FIG. The shape of the surface changes, the form of reflection and scattering of light changes, and the brightness distribution inside the container also changes. Correspondingly, based on the above-mentioned principle, the output signal 20a of the light receiving element 35 also changes as shown in FIGS. 7b and c.
Changes as shown in . (FIG. 7b shows the case where the vibration frequency is low, and FIG. 7c shows the case where the vibration frequency is high.) There is a substantially proportional relationship between the acceleration of the vibration and the voltage of the variable current component of the output signal 20a.

ところで、感知部20の出力信号20aの直流
成分Vaは第6図に示すように電源33を直接発
光素子34につなぐ方法ではとりわけ電源電圧変
動、周囲温度変化や経年変化等に起因する発光素
子の発光量の変動や受光素子の受光量の変動によ
り変化し、この直流成分Vaの大きさに応じて同
一加速度による振動であつても交流成分の出力幅
に違いが生じ、このままでは誤検出につながる恐
れがあるが、本発明では受光素子の直流成分41
a(但しフイルタ40と直流増幅器41を介した
後の出力)が基準電圧器42の指令する一定の電
圧指令42aに常に一致するように電流制御部4
4により発光素子34に流れる電流を制御するた
め、同一加速度で振動されるかぎり交流増幅器2
2′の出力信号22′aは常に同一信号となり、そ
の後の信号処理で誤検出がなされる恐れはない。
By the way, as shown in FIG. 6, the direct current component Va of the output signal 20a of the sensing unit 20 is affected by the effects of the light emitting element due to fluctuations in the power supply voltage, changes in ambient temperature, changes over time, etc. It changes due to fluctuations in the amount of light emitted and the amount of light received by the light receiving element, and depending on the magnitude of this DC component Va, the output width of the AC component will differ even if the vibration is caused by the same acceleration, leading to false detection if left as is. However, in the present invention, the DC component 41 of the light receiving element
The current controller 4 controls the current controller 4 so that a (output after passing through the filter 40 and the DC amplifier 41) always matches the constant voltage command 42a commanded by the reference voltage generator 42.
4 to control the current flowing to the light emitting element 34, as long as the AC amplifier 2 is vibrated with the same acceleration.
The output signal 22'a of 2' is always the same signal, and there is no possibility of erroneous detection in subsequent signal processing.

即ち、地震には垂直上下振動波(以下P波とい
う)と水平振動波(以下S波という)の2種類の
振動波が混じつているが、P波は地震の初期段階
に発生する振動加速度の値が比較的小さく10gal
〜数10gal程度のもので、この地震によるP波が
発生すれば、交流増幅器22′の出力電圧22′a
が周期的に基準電圧値45a1よりも大きくなつ
てコンパレータ46が連続的なパルス信号を発生
するため、カウンタ50が所定のパルス数計数後
Highレベルの出力信号を発し(雑振動によるP
波であれば単発的なパルス信号に終るため計数装
置50はHighレベルの出力信号を発しない)、記
憶装置52は地震が発生したことを記憶するとと
もにエレベータの制御装置(図示しない)等に最
寄階停止指令52a1を出力する。又、S波は初
期微振動P波発生後、略7秒〜30秒(震源地と観
測地との距離によつて変化するが、過去の地震デ
ータにより現実にエレベータ等に被害の生じる地
震での時間)経過してから発生する振動加速度の
値が大きい数+gal程度以上のもので、この本震
S波が発生し例えば80galになれば、交流増幅器
22′の出力電圧22′aが基準電圧値45a2よ
りも一瞬大きくなつた時点で、コンパレータ47
がHighレベルの信号を出力し、記憶装置52は
本震がきたことを記憶するとともにエレベータ制
御装置等にエレベータが走行中であれば非常停止
指令52a2等を出力する。さらに地震が強くな
り120galあるいは150galに達すれば、交流増幅器
22′の出力電圧22′aが基準電圧値45a3あ
るいは45a4よりも一瞬大きくなつた時点で、
コンパレータ48,49がHighレベルの信号を
出力し、記憶装置52は強度の地震がきたことを
記憶するとともにエレベータ制御装置等に運転禁
止指令52a3,52a4を出力し、専門技術者
による点検を行つた後手動によるリセツト信号5
2bを入力して解除しないかぎり運転禁止は継続
される。一方、記憶装置52の出力信号52a
1、及び52a2はコンパレータ46の出力信号
がHighレベル、コンパレータ47の出力信号が
Lowレベルの状態が所定時間(少なくとも30秒)
続けば自動リセツト信号発生装置51により自動
的にリセツトされるため、専門技術者の点検を待
つまでもなくエレベータの運転が再開可能とな
る。
In other words, two types of vibration waves are mixed in an earthquake: vertical vibration waves (hereinafter referred to as P waves) and horizontal vibration waves (hereinafter referred to as S waves), and P waves are caused by vibration acceleration that occurs in the early stages of an earthquake. The value is relatively small 10gal
~ several tens of gal, and if a P wave occurs due to this earthquake, the output voltage 22'a of the AC amplifier 22'
becomes larger than the reference voltage value 45a1 periodically and the comparator 46 generates a continuous pulse signal, so the counter 50 counts the predetermined number of pulses and then
Emit a high level output signal (P due to noise vibration)
(If the wave is a wave, it will end up as a single pulse signal, so the counting device 50 will not emit a high level output signal).The storage device 52 stores the occurrence of an earthquake and also sends it to an elevator control device (not shown), etc. A stop command 52a1 is output. In addition, the S wave occurs approximately 7 to 30 seconds after the initial tremor P wave occurs (depending on the distance between the epicenter and the observation site, but past earthquake data indicates that it is actually an earthquake that causes damage to elevators, etc.) If the value of the vibration acceleration that occurs after the elapse of time) is greater than a large number + gal, and this main shock S wave occurs and reaches, for example, 80 gal, the output voltage 22'a of the AC amplifier 22' will become the reference voltage value. 45a2, the comparator 47
outputs a high level signal, and the storage device 52 memorizes that the main shock has occurred, and outputs an emergency stop command 52a2 etc. to the elevator control device etc. if the elevator is running. If the earthquake becomes even stronger and reaches 120 gal or 150 gal, the moment the output voltage 22'a of the AC amplifier 22' momentarily becomes larger than the reference voltage value 45a3 or 45a4,
The comparators 48 and 49 output high-level signals, and the storage device 52 stores the fact that a strong earthquake has occurred, and outputs operation prohibition commands 52a3 and 52a4 to the elevator control device, etc., and an inspection is performed by a specialized engineer. Post-manual reset signal 5
The driving prohibition will continue unless it is canceled by inputting 2b. On the other hand, the output signal 52a of the storage device 52
1 and 52a2, the output signal of the comparator 46 is at High level, and the output signal of the comparator 47 is at High level.
Low level state for a specified period of time (at least 30 seconds)
If this continues, the automatic reset signal generator 51 will automatically reset the elevator, so that the elevator can resume operation without waiting for an inspection by a specialist engineer.

〔発明の効果〕〔Effect of the invention〕

以上述べたように本発明によれば、周囲環境の
変化、経年変化など、地震感知器を使用する上に
おいて避けることのできない変動要因があつても
十分その変動を吸収できる補正回路を備えている
ため、信頼性の極めて高い地震感知器を得ること
ができる。
As described above, according to the present invention, even if there are fluctuation factors that cannot be avoided when using an earthquake sensor, such as changes in the surrounding environment and aging, the correction circuit is provided that can sufficiently absorb the fluctuations. Therefore, an extremely reliable earthquake sensor can be obtained.

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

第1図は本発明の一実施例の構成を示すブロツ
ク図、第2図は地震波のパワースペクトルの一例
を示す図、第3図は動電型地震感知器の構造の一
例を示す図、第4図は重錘落下型地震感知器の構
造の一例を示す図、第5図は新タイプの地震感知
器の一構成を示すブロツク図、第6図は新タイプ
の地震感知器の感知部の一例を示す構造断面図、
第7図は感知部の出力信号20aの波形を示す
図、第8図乃至第10図は新タイプの地震感知器
の基本原理を示す説明図である。 20……感知部、21……信号処理部、22,
22′……交流増幅器、23,25,46,47,
48,49……コンパレータ、24,26……出
力回路、31……容器、32……液体、34……
光源、35……受光素子、40……フイルタ、4
2……基準電圧器、43……比較増幅器、44…
…電流制御部。
FIG. 1 is a block diagram showing the configuration of an embodiment of the present invention, FIG. 2 is a diagram showing an example of the power spectrum of seismic waves, FIG. 3 is a diagram showing an example of the structure of an electrodynamic earthquake sensor, and FIG. Figure 4 shows an example of the structure of a falling weight earthquake sensor, Figure 5 is a block diagram showing the configuration of a new type of earthquake sensor, and Figure 6 shows the sensing section of a new type of earthquake sensor. A structural sectional view showing an example,
FIG. 7 is a diagram showing the waveform of the output signal 20a of the sensing section, and FIGS. 8 to 10 are explanatory diagrams showing the basic principle of the new type of earthquake sensor. 20... Sensing unit, 21... Signal processing unit, 22,
22'... AC amplifier, 23, 25, 46, 47,
48, 49... Comparator, 24, 26... Output circuit, 31... Container, 32... Liquid, 34...
Light source, 35... Light receiving element, 40... Filter, 4
2... Reference voltage generator, 43... Comparison amplifier, 44...
...Current control section.

Claims (1)

【特許請求の範囲】 1 外部からの光を遮断する密閉構造の容器を備
え、該容器には光を反射する液体が入つており、
該液体の上方には前記容器内を照射する光源と、
該光源が発する光のうち前記液体表面からの反射
光を受光し、その光量を電気信号に変換する光電
変換素子とを設け、前記液体の液面の傾きを前記
液体表面からの反射光量の変化として捉え、前記
光電変換素子の出力電気信号が所定値よりも大き
いとき出力を発する信号処理部を備えた地震感知
器において、 常に一定の電圧指令を出力する基準電圧器と、
前記光電変換素子の出力電気信号から直流成分を
取り出すフイルタとを設け、前記基準電圧器の電
圧指令と前記フイルタの直流成分とを比較しその
差信号を増幅出力する比較増幅器を備え、該比較
増幅器の出力信号に応じて前記光源に流れる電流
を制御する電流制御部を備えてなる感度補正付地
震感知器。
[Claims] 1. A container having a sealed structure that blocks light from the outside, the container containing a liquid that reflects light,
A light source that illuminates the inside of the container above the liquid;
A photoelectric conversion element is provided that receives reflected light from the liquid surface out of the light emitted by the light source and converts the amount of light into an electrical signal, and changes in the amount of reflected light from the liquid surface are determined based on the inclination of the liquid surface. In an earthquake sensor equipped with a signal processing unit that outputs an output when the output electrical signal of the photoelectric conversion element is larger than a predetermined value, a reference voltage generator that always outputs a constant voltage command;
a filter for extracting a DC component from the output electrical signal of the photoelectric conversion element, and a comparison amplifier for comparing the voltage command of the reference voltage generator with the DC component of the filter and amplifying and outputting a difference signal, the comparison amplifier An earthquake sensor with sensitivity correction, comprising a current control section that controls a current flowing through the light source according to an output signal of the light source.
JP59269964A 1984-05-01 1984-12-20 Earthquake sensor with sensitivity correction Granted JPS61147117A (en)

Priority Applications (3)

Application Number Priority Date Filing Date Title
JP59269964A JPS61147117A (en) 1984-12-20 1984-12-20 Earthquake sensor with sensitivity correction
GB08510935A GB2160319B (en) 1984-05-01 1985-04-30 Detecting of seismic waves by sensing the movement of a liquid surface
US06/729,117 US4662225A (en) 1984-05-01 1985-04-30 Seismic detector

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP59269964A JPS61147117A (en) 1984-12-20 1984-12-20 Earthquake sensor with sensitivity correction

Publications (2)

Publication Number Publication Date
JPS61147117A JPS61147117A (en) 1986-07-04
JPH0245137B2 true JPH0245137B2 (en) 1990-10-08

Family

ID=17479672

Family Applications (1)

Application Number Title Priority Date Filing Date
JP59269964A Granted JPS61147117A (en) 1984-05-01 1984-12-20 Earthquake sensor with sensitivity correction

Country Status (1)

Country Link
JP (1) JPS61147117A (en)

Family Cites Families (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5237789A (en) * 1975-09-20 1977-03-23 Agency Of Ind Science & Technol Process for production of photovoltaic elements
JPS5435116U (en) * 1977-08-11 1979-03-07
US4214485A (en) * 1978-06-07 1980-07-29 Paul J. Berger Electro-mechanical transducer
JPS60231120A (en) * 1984-05-01 1985-11-16 Fujitec Co Ltd Earthquake sensor

Also Published As

Publication number Publication date
JPS61147117A (en) 1986-07-04

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