JPH0245133B2 - - Google Patents
Info
- Publication number
- JPH0245133B2 JPH0245133B2 JP59088902A JP8890284A JPH0245133B2 JP H0245133 B2 JPH0245133 B2 JP H0245133B2 JP 59088902 A JP59088902 A JP 59088902A JP 8890284 A JP8890284 A JP 8890284A JP H0245133 B2 JPH0245133 B2 JP H0245133B2
- Authority
- JP
- Japan
- Prior art keywords
- liquid
- light
- output
- container
- photoelectric conversion
- 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
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
- G01V1/16—Receiving elements for seismic signals; Arrangements or adaptations of receiving elements
- G01V1/18—Receiving elements, e.g. seismometer, geophone or torque detectors, for localised single point measurements
- G01V1/181—Geophones
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01H—MEASUREMENT OF MECHANICAL VIBRATIONS OR ULTRASONIC, SONIC OR INFRASONIC WAVES
- G01H9/00—Measuring 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)
- Engineering & Computer Science (AREA)
- Remote Sensing (AREA)
- Life Sciences & Earth Sciences (AREA)
- Acoustics & Sound (AREA)
- Environmental & Geological Engineering (AREA)
- Geology (AREA)
- General Life Sciences & Earth Sciences (AREA)
- Geophysics (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.
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1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 1 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2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。 Figure 2 shows an example of the structure of an electrodynamic seismic 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. That is, 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3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. 3 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.
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、該液体の上方には容器内を照射する光源
と、該光源が発する光のうち液体の表面からの反
射光を受光し、その光量を電気信号に変換する光
電変換素子とを備えた感知部を設け、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 emits light from the light source. A sensing section equipped with a photoelectric conversion element that receives reflected light from the surface of the liquid and converts the amount of light into an electrical signal is provided, and the inclination of the liquid surface is detected as a change in the amount of reflected light from the liquid surface. The photoelectric conversion element includes a signal processing section that outputs an output when the output electric signal of the photoelectric conversion element is larger than a predetermined value.
上述の如く構成すれば、地震による振動レベル
の検出を液体表面の反射光量の変化として捉える
ことができる。
With the configuration as described above, the detection of the vibration level due to an earthquake can be detected as a change in the amount of reflected light on the liquid surface.
本発明の基本原理は次のとおりである。 The basic principle of the present invention is as follows.
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、波の波長をλと
し、波の進路に沿つてx軸をとるとすれば第10
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
が主成分の振動をする。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。 For simplicity, when a small cylindrical container containing a liquid is vibrated in the horizontal direction with a constant vibrational acceleration, the movement of waves on the surface of the liquid is expressed as follows: the magnitude of the vibrational acceleration is A, the acceleration of gravity is g, and the amplitude of the wave. If a is the wavelength of the wave, and λ is the wavelength of the wave, and the x-axis is taken along the course of the wave, then the 10th
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. And the inclination angle θ of the liquid level
If the value is small, it is given by the following formula.
θ=A/g=2πa/λcos2πx/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/λcos2πx/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, it is sufficient to detect the inclination angle of the liquid surface. become.
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10図、上
下加振時は第11図を基本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 has peaks or troughs that are large enough to be located at the side wall. The basic mode is shown in FIG. 10, and the basic mode is shown in FIG. 11 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12図に示すとおりである。 Next, the basic optical system for detecting the angle of inclination of the liquid surface is as 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 equation if the equations are considered.
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.
したがつて感知部は、容器内の液体が地震波に
よつて揺動し、液体表面の形状が変わることによ
つて変化する液体表面からの反射光の輝度分布を
電気信号に変換して出力し、信号処理部はこの出
力信号の大きさにより振動レベルを識別する。こ
れにより、簡単な構成で信頼性が高く、しかも水
平振動波(以下S波という)と垂直上下振動波
(以下P波という)のいずれでも感知しうる高精
度の地震感知器を提供するものである。 Therefore, the sensing unit converts the luminance distribution of reflected light from the liquid surface, which changes as the liquid in the container is shaken by seismic waves and the shape of the liquid surface changes, into an electrical signal and outputs it. , the signal processing section identifies the vibration level based on the magnitude of this output signal. This provides a highly reliable earthquake sensor with a simple configuration and high accuracy that can detect both horizontal vibration waves (hereinafter referred to as S waves) and vertical vertical vibration waves (hereinafter referred to as P waves). be.
第4図は、本発明の一実施例の構成を示すブロ
ツク図で、図中、20は液体の入つた密閉構造の
容器内の液体からの反射光を受光し、受光量に応
じた信号20aを出力する感知部、21は信号2
0aが所定値を越えると出力を発する信号処理部
である。この例では、信号処理部21は2段階の
設定値を設けており、前置増幅器(交流増幅器)
22の出力が第1の設定値より大きい場合は第1
のコンパレータ23及び出力回路24により信号
24aが出力され、更に第2の設定値より大きい
場合は第2のコンパレータ25及び出力回路26
により信号26aが出力される。なお、前置増幅
器22の後にノイズ除去の為のフイルターを設け
てもよく、設定値は上記のように2段階に限ら
ず、任意の複数段階の設定値を設けることもでき
る。
FIG. 4 is a block diagram showing the configuration of an embodiment of the present invention. In the figure, 20 receives reflected light from a liquid in a sealed container containing liquid, and a signal 20a corresponding to the amount of light received. The sensing section 21 outputs the signal 2.
This is a signal processing section that generates an output when 0a exceeds a predetermined value. In this example, the signal processing unit 21 has two stages of setting values, and the preamplifier (AC amplifier)
If the output of 22 is larger than the first set value, the first
The comparator 23 and output circuit 24 output the signal 24a, and if the signal 24a is larger than the second set value, the second comparator 25 and output circuit 26 output the signal 24a.
A signal 26a is output. Note that a filter for noise removal may be provided after the preamplifier 22, and the set value is not limited to two stages as described above, but may be set to any number of stages.
第5図は、感知部20の一実施例の構造を示す
断面図で、31は外部からの光を遮断する密閉構
造の容器、32は容器31内に入れられた光を反
射する油や水銀等の液体、33は電源、34は容
器31内を照射する例えば発光ダイオード等の光
源、35は光を受光する光電変換素子である。第
5図において、容器31が静止状態に置かれてい
る場合は液体32も静止状態にあり、従つて液体
32からの反射光線の分布は一定で、光電変換素
子35の出力20aも一定であるが、地震等の振
動により液体32が揺動すると液体表面の形状が
変わり、特に液体32からの光の反射や散乱の形
態が変化して容器31内の輝度分布も変化し、そ
れに対応して光電変換素子35の出力20aも変
動する。 FIG. 5 is a cross-sectional view showing the structure of one embodiment of the sensing unit 20, in which 31 is a container with a closed structure that blocks light from the outside, and 32 is oil or mercury contained in the container 31 that reflects light. 33 is a power source, 34 is a light source such as a light emitting diode that illuminates the inside of the container 31, and 35 is a photoelectric conversion element that receives light. In FIG. 5, when the container 31 is placed in a stationary state, the liquid 32 is also in a stationary state, so the distribution of reflected light from the liquid 32 is constant, and the output 20a of the photoelectric conversion element 35 is also constant. However, when the liquid 32 shakes due to vibrations such as earthquakes, the shape of the liquid surface changes, and in particular, the form of reflection and scattering of light from the liquid 32 changes, causing the brightness distribution inside the container 31 to change as well. The output 20a of the photoelectric conversion element 35 also fluctuates.
第6図は、水平方向の振動が生じた場合に、液
体32が容器31内で揺動する様子を示した図
で、比較的低い周波数の場合はaに示すように、
液体32は矢印方向に大きく移動し、比較的高い
周波数の場合はbに示すように、液体32の表面
が小刻みに揺れ(液体の移動はない)液体の表面
の傾斜角は時々刻々変動する。 FIG. 6 is a diagram showing how the liquid 32 oscillates within the container 31 when horizontal vibration occurs. In the case of a relatively low frequency, as shown in a,
The liquid 32 moves largely in the direction of the arrow, and when the frequency is relatively high, as shown in b, the surface of the liquid 32 shakes little by little (there is no movement of the liquid), and the inclination angle of the surface of the liquid changes from moment to moment.
このように、振動の周波数の違いによつて液体
の揺動の様子が異なり、その結果前述の原理に基
づき光電変換素子35の出力の変動も振動周波数
によつて異なる。 In this way, the manner in which the liquid oscillates differs depending on the vibration frequency, and as a result, based on the above-mentioned principle, the fluctuation in the output of the photoelectric conversion element 35 also differs depending on the vibration frequency.
第7図は、光電変換素子35の出力20a(但
し前置増幅器22を介した後の出力)についての
実験結果を示したもので、aは振動数が低い場合
を、bは振動数が高い場合をそれぞれ示してい
る。 FIG. 7 shows the experimental results for the output 20a of the photoelectric conversion element 35 (output after passing through the preamplifier 22), where a indicates the case where the frequency is low and b indicates the case where the frequency is high. Each case is shown.
第8図は、液体としてエンジン油を用いた場合
について、第7図に示した出力電圧の、振動周波
数に対する出力特性の実験結果を示す図である。
ここで、パラメータ(a1、a2、a3、a4)は振動
加速度であり、一例としてa1=30gal、a2=
80gal、a3=120gal、a4=150galとすると、5Hz
のときの出力電圧はそれぞれb1=0.45V、b2=
1.2V、b3=1.85V、b4=2.3Vとなり加速度の大き
さと出力電圧の比はほぼ比例する。 FIG. 8 is a diagram showing the experimental results of the output characteristics of the output voltage shown in FIG. 7 with respect to the vibration frequency when engine oil is used as the liquid.
Here, the parameters (a1, a2, a3, a4) are vibration accelerations, and as an example, a1=30gal, a2=
80gal, a3=120gal, a4=150gal, 5Hz
The output voltages when are b1=0.45V and b2=
1.2V, b3 = 1.85V, b4 = 2.3V, and the ratio of the magnitude of acceleration and output voltage is almost proportional.
このように、加速度と出力電圧の関係はリニア
であり、また第8図から明らかなように、1〜5
Hzはほぼフラツト特性、5Hz以上では下降特性で
地震波の周波数特性と合致しており、地震感知器
に理想的な特性となつている(水銀の場合は3〜
4Hzで特に鋭い出力特性を示す)。 In this way, the relationship between acceleration and output voltage is linear, and as is clear from FIG.
Hz is almost a flat characteristic, and above 5Hz it is a falling characteristic, matching the frequency characteristic of seismic waves, making it an ideal characteristic for earthquake detectors (in the case of mercury, it is 3~3Hz).
It shows particularly sharp output characteristics at 4Hz).
なお、以上はS波の場合について述べたが、P
波の場合には液体の揺動の様子は第9図に示すよ
うになり、液体からの反射光の輝度分布の変化、
すなわち感知部の出力電圧の変化を捉えることに
よりP波の感知もS波と同様に行うことができ
る。 In addition, although the above has been described for the case of S waves, P
In the case of waves, the liquid oscillates as shown in Figure 9, and changes in the brightness distribution of the reflected light from the liquid,
That is, by capturing changes in the output voltage of the sensing section, P waves can be sensed in the same way as S waves.
また、容器内の液体としては光を反射する性質
の水銀や適当な粘度を有する油が適しているが、
地震波のみをとらえる精度においては油の方が、
高層ビル等の高所で0.1Hzの周波数をも感知する
必要があるような場合には水銀の方が、それぞれ
若干優れている。 Also, as the liquid in the container, mercury that reflects light or oil that has an appropriate viscosity is suitable.
Oil is better in terms of accuracy in capturing only seismic waves.
Mercury is slightly better in cases where it is necessary to detect frequencies as low as 0.1 Hz in high places such as high-rise buildings.
本発明によれば、前述のように感知部自身極め
て地震波の周波数に合致するものであつて、誤動
作をほとんどなくすことができ、また取付調整の
手間もほとんどかからず(厳しい水平出しは不
要)、その構成では大変シンプル(低価格)であ
る。更に、加速度の大きさに対して感知部の出力
電圧はリニアとなるので、設定値を任意に何段に
も分けて設定でき、また、P波、S波のいずれの
地震波をも感知する事ができるという、従来にな
い秀れた特徴を数多く有するものである。
According to the present invention, as mentioned above, the sensing part itself matches the frequency of seismic waves, and malfunctions can be almost eliminated, and installation adjustment requires almost no effort (no need for strict leveling). , its configuration is very simple (low cost). Furthermore, since the output voltage of the sensing section is linear with respect to the magnitude of acceleration, the set value can be set in any number of stages, and it is possible to detect both P-wave and S-wave seismic waves. It has many excellent features that have not been seen before.
第1図は地震波のパワースペクトルの一例を示
す図、第2図は動電型地震感知器の構造の一例を
示す図、第3図は重錘落下型地震感知器の構造の
一例を示す図、第4図は本発明の一実施例の構成
を示すブロツク図、第5図は感知部の一実施例の
構造を示す断面図、第6図はS波に対する容器内
の液体の揺動の様子を示す図、第7図は感知部の
出力についての実験結果を示す図、第8図は第7
図の出力電圧について振動周波数に対する出力特
性の実験結果を示す図、第9図はP波に対する容
器内の液体の揺動の様子を示す、第10図乃至第
12図は本発明の基本原理を説明するための説明
図である。
20……感知部、21……信号処理部、22…
…前置増幅器、23,25……コンパレータ、2
4,26……出力回路、31……容器、32……
液体、34……光源、35……光電変換素子。
Figure 1 shows an example of the power spectrum of seismic waves, Figure 2 shows an example of the structure of an electrodynamic earthquake sensor, and Figure 3 shows an example of the structure of a falling weight earthquake sensor. , FIG. 4 is a block diagram showing the structure of an embodiment of the present invention, FIG. 5 is a sectional view showing the structure of an embodiment of the sensing section, and FIG. Figure 7 is a diagram showing the experimental results regarding the output of the sensing section, and Figure 8 is a diagram showing the
Figure 9 shows the experimental results of the output characteristics of the output voltage versus vibration frequency; Figure 9 shows how the liquid in the container oscillates in response to P waves; Figures 10 to 12 illustrate the basic principle of the present invention. It is an explanatory diagram for explanation. 20... Sensing section, 21... Signal processing section, 22...
...Preamplifier, 23, 25...Comparator, 2
4, 26... Output circuit, 31... Container, 32...
Liquid, 34...Light source, 35...Photoelectric conversion element.
Claims (1)
え、該容器には光を反射する液体が入つており、
前記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の表面から
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備えた感知部を設け、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
理部を備えたことを特徴とする地震感知器。 2 前記液体は表面反射率の高い液体であること
を特徴とする特許請求の範囲第1項記載の地震感
知器。 3 前記液体は水銀であることを特徴とする特許
請求の範囲第2項記載の地震感知器。 4 前記信号処理部は複数の所定値と比較するコ
ンパレータを備えたことを特徴とする特許請求の
範囲第1項記載の地震感知器。 5 前記信号処理部は前記光電変換素子の出力電
気信号を入力として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る交流
増幅器を備えたことを特徴とする特許請求の範囲
第1項記載の地震感知器。[Claims] 1. A container having a sealed structure that blocks light from the outside, the container containing a liquid that reflects light,
A sensing device is provided above the liquid, and includes a light source that illuminates the inside of the container, and a photoelectric conversion element that receives reflected light from the surface of the liquid among the light emitted by the light source and converts the amount of light into an electrical signal. and a signal processing unit that detects the inclination of the liquid level as a change in the amount of reflected light from the liquid surface and outputs an output when the output electric signal of the photoelectric conversion element is larger than a predetermined value. Features an earthquake sensor. 2. The earthquake sensor according to claim 1, wherein the liquid is a liquid with high surface reflectance. 3. The earthquake sensor according to claim 2, wherein the liquid is mercury. 4. The earthquake sensor according to claim 1, wherein the signal processing section includes a comparator for comparing with a plurality of predetermined values. 5. Claims characterized in that the signal processing unit includes an AC amplifier that receives the output electric signal of the photoelectric conversion element as input and detects the inclination of the liquid level as a change in the amount of light reflected from the liquid surface. Earthquake sensor according to paragraph 1.
Priority Applications (3)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP59088902A JPS60231120A (en) | 1984-05-01 | 1984-05-01 | Earthquake sensor |
| 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 |
|---|---|---|---|
| JP59088902A JPS60231120A (en) | 1984-05-01 | 1984-05-01 | Earthquake sensor |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS60231120A JPS60231120A (en) | 1985-11-16 |
| JPH0245133B2 true JPH0245133B2 (en) | 1990-10-08 |
Family
ID=13955880
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP59088902A Granted JPS60231120A (en) | 1984-05-01 | 1984-05-01 | Earthquake sensor |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS60231120A (en) |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS61147117A (en) * | 1984-12-20 | 1986-07-04 | Fujitec Co Ltd | Earthquake sensor with sensitivity correction |
Family Cites Families (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US4214485A (en) * | 1978-06-07 | 1980-07-29 | Paul J. Berger | Electro-mechanical transducer |
-
1984
- 1984-05-01 JP JP59088902A patent/JPS60231120A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS60231120A (en) | 1985-11-16 |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| US6350983B1 (en) | Micro-electro-opto-mechanical inertial sensor | |
| US4800267A (en) | Optical fiber microbend horizontal accelerometer | |
| KR20050086918A (en) | Methods and systems for decelarating proof mass movements within mems structures | |
| US20090320592A1 (en) | Multistage proof-mass movement deceleration within mems structures | |
| US10802040B2 (en) | Acceleration sensor | |
| US9823265B2 (en) | Geophysical acceleration sensor and method | |
| JPH0245133B2 (en) | ||
| US5461918A (en) | Vibrating beam accelerometer | |
| US4662225A (en) | Seismic detector | |
| JPH0245135B2 (en) | ||
| KR100395749B1 (en) | Sensing device of earthquake wave | |
| JPH0326431Y2 (en) | ||
| JPS61164125A (en) | Earthquake sensor | |
| JPH0245134B2 (en) | ||
| JPH0245137B2 (en) | ||
| JPH0245136B2 (en) | ||
| JPH0338532B2 (en) | ||
| JPH0421083Y2 (en) | ||
| JPH0725641Y2 (en) | Elevator device with seismic detector | |
| US7045371B2 (en) | Foreign material removing method for capacitance type dynamic quantity sensor | |
| Davies et al. | Micromechanical structures and microelectronics for acceleration sensing | |
| JP2007033428A (en) | Earthquake evaluation method and earthquake evaluation device | |
| JPS61165626A (en) | Elevator equipment complete with seismograph | |
| RU2017160C1 (en) | Piezoelectric accelerometer | |
| JPH053940U (en) | Weight measuring instrument |
Legal Events
| Date | Code | Title | Description |
|---|---|---|---|
| LAPS | Cancellation because of no payment of annual fees |