JPS61142425A - Seismic sensor - Google Patents
Seismic sensorInfo
- Publication number
- JPS61142425A JPS61142425A JP59264901A JP26490184A JPS61142425A JP S61142425 A JPS61142425 A JP S61142425A JP 59264901 A JP59264901 A JP 59264901A JP 26490184 A JP26490184 A JP 26490184A JP S61142425 A JPS61142425 A JP S61142425A
- Authority
- JP
- Japan
- Prior art keywords
- temperature
- sensor
- liquid
- sensing
- container
- 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.)
- Granted
Links
- 239000007788 liquid Substances 0.000 claims abstract description 43
- 238000006243 chemical reaction Methods 0.000 claims description 5
- 230000035945 sensitivity Effects 0.000 abstract description 6
- 238000001514 detection method Methods 0.000 abstract description 4
- 230000007423 decrease Effects 0.000 description 5
- 230000005520 electrodynamics Effects 0.000 description 4
- 238000000034 method Methods 0.000 description 4
- 239000003921 oil Substances 0.000 description 4
- 230000001133 acceleration Effects 0.000 description 3
- 238000010586 diagram Methods 0.000 description 3
- XEEYBQQBJWHFJM-UHFFFAOYSA-N Iron Chemical compound [Fe] XEEYBQQBJWHFJM-UHFFFAOYSA-N 0.000 description 2
- 238000010276 construction Methods 0.000 description 2
- 230000000694 effects Effects 0.000 description 2
- 230000005484 gravity Effects 0.000 description 2
- 239000010720 hydraulic oil Substances 0.000 description 2
- 230000007257 malfunction Effects 0.000 description 2
- QSHDDOUJBYECFT-UHFFFAOYSA-N mercury Chemical compound [Hg] QSHDDOUJBYECFT-UHFFFAOYSA-N 0.000 description 2
- 229910052753 mercury Inorganic materials 0.000 description 2
- 238000001228 spectrum Methods 0.000 description 2
- 230000003213 activating effect Effects 0.000 description 1
- 230000015572 biosynthetic process Effects 0.000 description 1
- 238000013016 damping Methods 0.000 description 1
- 238000002474 experimental method Methods 0.000 description 1
- 239000012530 fluid Substances 0.000 description 1
- 238000010438 heat treatment Methods 0.000 description 1
- 229910052742 iron Inorganic materials 0.000 description 1
- 239000000696 magnetic material Substances 0.000 description 1
- 239000000463 material Substances 0.000 description 1
- 238000002844 melting Methods 0.000 description 1
- 230000008018 melting Effects 0.000 description 1
- 229910052709 silver Inorganic materials 0.000 description 1
- 239000004332 silver Substances 0.000 description 1
- 239000010902 straw Substances 0.000 description 1
- 238000001308 synthesis method Methods 0.000 description 1
- 238000003786 synthesis reaction Methods 0.000 description 1
- 238000009423 ventilation Methods 0.000 description 1
- 238000010792 warming Methods 0.000 description 1
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01V—GEOPHYSICS; GRAVITATIONAL MEASUREMENTS; DETECTING MASSES OR OBJECTS; TAGS
- G01V1/00—Seismology; Seismic or acoustic prospecting or detecting
- G01V1/01—Measuring or predicting earthquakes
Landscapes
- Physics & Mathematics (AREA)
- Life Sciences & Earth Sciences (AREA)
- Engineering & Computer Science (AREA)
- Acoustics & Sound (AREA)
- Environmental & Geological Engineering (AREA)
- Geology (AREA)
- Remote Sensing (AREA)
- General Life Sciences & Earth Sciences (AREA)
- General Physics & Mathematics (AREA)
- Geophysics (AREA)
- Measurement Of Mechanical Vibrations Or Ultrasonic Waves (AREA)
Abstract
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] まず、地震の周波数について説明する。[Prior art and problems to be solved by the invention] First, we will explain the frequency of earthquakes.
一般に地震波の主成分の周波数は1〜lOH2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、−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2〜3 Hz(2,4Hz)で、1〜5 Hzのパ
ワーが大き 。It is generally said that the frequency of the main component of seismic waves is in the range of 1 to 1OH2, of which the component of 1 to 5 Hz is particularly prominent. Figure 2 shows the power spectrum of the seismic waves observed in Ofunato as an example for the Miyagi Prefecture-oki Earthquake that occurred at 17:14 on June 12, 1973.The dominant frequency was 2 to 3 Hz (2, 4Hz), and the power between 1 and 5 Hz is large.
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)。(Although not shown, the Fourier spectrum has almost the same shape and has many 1 to 5 Hz 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「普通縁
は1〜5Hzの範囲でフラット特性、精密級では0.1
〜5Hzの範囲でフラット特性、5Hzを越える範囲で
は感度は下降特性とすること」となっている。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. In order to prevent malfunctions, the Japan Elevator Association's technical standards for seismic design and construction guidelines state that the frequency characteristics of the sensor are ``flat in the range of 1 to 5 Hz for normal edges, and 0.1 for precision grade.
The sensitivity should be flat in the range of ~5 Hz, and the sensitivity should decrease 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−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 detectors are generally of an electrodynamic type, a strain gauge type, a piezoelectric type, or a mechanical weight drop type.
゛ 第3図は、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
フィル3が振動により上下に動くと、フィル30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。゛ Figure 3 shows an example of the structure of an electrodynamic earthquake sensor (vertical sensor). When the filter 3 moves up and down due to vibration, a voltage is generated at both ends of the filter 30, and the magnitude of this voltage is proportional to the moving speed of the coil 3, which is used to detect an earthquake.
なお、1はおもり2を支持するばね系であり、6は藁路
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(ばね系の間!l)、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、と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。Note that 1 is a spring system that supports the weight 2, and 6 is a yoke that forms a straw 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 with this method fall at 5 Hz or higher as described above (between spring systems!l), and usually It has a falling characteristic at about 10Hz or higher. 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, the electrodynamic seismic sensor has problems in terms of accuracy and adjustment effort.
また、ストレーンゲージ型地震感知器it、ストレーン
ゲージ(歪ゲージ)をX、Y方向番こ設置し、これらの
電気出力をペクトJし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、電気的フィルターで5Hz以上を減衰させるように
して警する。In addition, a strain gauge type earthquake sensor IT, a strain gauge (strain gauge) is installed in the X and Y directions, and these electrical outputs are combined to determine the acceleration, but the frequency of the strain gauge itself is Since the characteristics extend to several kHz, an electric filter should be used to attenuate frequencies above 5 Hz.
従ってストレーンゲージ型の地震感知器+1このフィル
ターの特性に大きく左右され、更にベクトル合成を行な
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、圧電製地震感
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。Therefore, the strain gauge type earthquake sensor + 1 is greatly influenced by the characteristics of this filter, and it also includes many error factors such as the need for a multiplier to perform vector synthesis, which poses a problem in terms of reliability. . 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+1重錘(鉄等の磁性体
)13が、ケース10番こ固定きれた永久磁石11に吸
引されて塾するが、ある−室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(するし
/<−12が支点15を中心に矢印方向に回転すること
により、マイクロスイッチ14のアクチュエータ14′
を作動させて地震を感知するものである。FIG. 4 shows an example of the structure of a falling weight type earthquake sensor. This is because in a stationary state, a +1 weight (magnetic material such as iron) 13 is attracted to the permanent magnet 11 fixed to the case 10, but when a vibration of a certain degree or more occurs, this weight 13 falls, is fitted into the weight 13, and rotates in the direction of the arrow around the fulcrum 15, causing the actuator 14' of the microswitch 14 to move.
It is used to sense earthquakes by activating the
この方式は簡単ではあるが、磁石の吸引力と重錘の重さ
の関係によって感知レベルが左右きれ、その調整が大変
であると同時に低い周波数(IHz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。Although this method is simple, it has the disadvantage that the sensing level varies depending on the relationship between the attraction force of the magnet and the weight of the weight, making it difficult to adjust, and at the same time, it is difficult to detect at low frequencies (below IHz). There are still problems with accuracy and reliability.
このため、出願人は特願昭59−98902号にて新し
いタイプの地震感知器を提案した。For this reason, the applicant proposed a new type of earthquake sensor in Japanese Patent Application No. 59-98902.
それは第5図及び第6図に示すように、円柱状の容器3
1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とこの容!I
31内の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って変化する容器31内の輝度
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の大ききに応
じて震動レベルを識別する新しいタイプの地震感知器で
ある。As shown in Figs. 5 and 6, it is a cylindrical container 3.
A liquid 32 such as mercury or oil is placed in a container 31, and a light source 34 such as a light emitting diode is attached to the lid of the container 31. I
When the liquid 32 in the container 31 is shaken by seismic waves, the light receiving element 35 electrically detects the luminance distribution inside the container 31, which changes as the shape of the liquid surface changes. This is a new type of earthquake sensor in which a signal processing unit 21 identifies the vibration level according to the magnitude of the output signal 20a.
即ち、この地震感知器は感知部2oの受光素子35かも
出力きれた容器31内の輝度分布に応じた信号20aを
前置増幅器22(交流増幅器)により増幅し、フンパレ
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、容器31内の液体32の重要、な特性
である粘度が周囲温度の影響を受けて変化するため、温
度による粘度変化に伴い同一振動レベルで1あっても感
知器の感度が変化し、これが誤検出の原因となる今など
正確な検出ができにくい欠点がその後の実験結果で明ら
かとなった。That is, in this earthquake sensor, a signal 20a corresponding to the luminance distribution inside the container 31, which has been outputted by the light receiving element 35 of the sensing part 2o, is amplified by the preamplifier 22 (AC amplifier), and then sent to the amplifiers 23, 25, etc. by: This device detects earthquakes at multiple levels, but since the viscosity, which is an important property of the liquid 32 in the container 31, changes due to the influence of ambient temperature, it is possible to detect earthquakes at multiple levels at the same vibration level. Subsequent experimental results revealed that even if the sensor is present, the sensitivity of the sensor changes, causing false positives and making accurate detection difficult.
本発明は上記の点に鑑みなきれたもので、たとえ周囲温
度が変わうても感知・器の感度が変わることのない地震
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 an object of the present invention is to provide an earthquake sensor in which the sensitivity of the sensor/device does not change even if the ambient temperature changes.
第1図は本発明による感知器の一例を示す断面図で、図
中40は円柱状の容器、41は例えば水銀のように比重
が大きく低粘度でかつ表面反射率の高い液体、42は液
体4iと比べ比重が小さく温度による粘度変化の少ない
高粘度でかつ表面反射率の低い、例えば航空機の作動油
のような液体で二重層液体43を構成している(二重層
液体を用いる理由は常温での周波数特性を理想的な特性
にするためである)、44は電源、45は例えば発光ダ
イオード等の光源、46は光を受光する光電変換素子、
47は二重層液体43を温めるためのヒータ、48は例
えばサーミスタ等の温度センサ、49は温度に比例した
温度センサ4Bの出力信号を増幅する増幅器、50は増
幅器49の出力電圧が所定値以下、即ち二重層液体43
が所定の温度(例えば0℃)以下になると出力信号を発
し、所定の温度(例えば10°C)を超えると出力信号
の発生を止めるヒステリスをもったフンパレータ、51
はコンパレータ50が出力信号を発すると接点51mを
閉路させ、出力信号がなくなると開路きせる操作部、5
2は接点51aを通じてヒー゛り47に電流を供給する
電源である。信号処理部については第5図と全く同一で
ある。FIG. 1 is a sectional view showing an example of a sensor according to the present invention, in which 40 is a cylindrical container, 41 is a liquid such as mercury, which has a high specific gravity, low viscosity, and high surface reflectance, and 42 is a liquid. The double layer liquid 43 is made of a liquid such as aircraft hydraulic oil, which has a high viscosity with a small specific gravity and little change in viscosity due to temperature compared to 4i, and has a low surface reflectance. 44 is a power source, 45 is a light source such as a light emitting diode, 46 is a photoelectric conversion element that receives light,
47 is a heater for warming the double layer liquid 43; 48 is a temperature sensor such as a thermistor; 49 is an amplifier that amplifies the output signal of the temperature sensor 4B which is proportional to the temperature; That is, double layer liquid 43
a humpator with hysteresis that emits an output signal when the temperature drops below a predetermined temperature (for example, 0°C) and stops generating the output signal when the temperature exceeds a predetermined temperature (for example, 10°C), 51
5 is an operation unit that closes the contact 51m when the comparator 50 issues an output signal, and opens the contact 51m when the output signal disappears;
Reference numeral 2 denotes a power source that supplies current to the heating element 47 through the contact 51a. The signal processing section is exactly the same as in FIG. 5.
第1図において、容器40が静止状態に置かれている場
合は、二重層液体43も静止状態にあり、従って容器4
0内の輝度分布は一定で光電変換素子46の出力203
も一定の直流電圧のみであるが、地震等の振動により二
重層液体43が揺動すると二重層を構成する各々の液体
41゜42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40内の輝度分布も変化し、それに対
応して光電変換素子46の出力20a(但し前置増幅器
22を介した後の出力、以下感知器20の出力電圧とい
う)は第7図((a)は振動数が低い場合、(b)は振
動数が高い場合を示す)に示すように変化する。
−・地震の振動周波数が変われば液体43#揺動
の様子も垂直上下振動波(以下P波という)の゛場合と
水平振動波(以下S波という)の場合で異なるため、容
器40内の輝度分布も微妙に変化してその影響が出力電
圧に現われる。In FIG. 1, when the container 40 is placed at rest, the double layer liquid 43 is also at rest and therefore the container 40 is placed at rest.
The brightness distribution within 0 is constant and the output 203 of the photoelectric conversion element 46
is only a constant DC voltage, but when the double layer liquid 43 is shaken due to vibrations such as earthquakes, the shape of the surface of each liquid 41 and 42 that makes up the double layer changes, and the form of light reflection and scattering changes. As a result, the luminance distribution inside the container 40 changes, and correspondingly, the output 20a of the photoelectric conversion element 46 (output after passing through the preamplifier 22, hereinafter referred to as the output voltage of the sensor 20) changes as shown in FIG. (a) shows the case where the vibration frequency is low, and (b) shows the case where the vibration frequency is high).
- If the vibration frequency of the earthquake changes, the behavior of the liquid 43# will also differ depending on whether it is a vertical vertical vibration wave (hereinafter referred to as P wave) or a horizontal vibration wave (hereinafter referred to as S wave). The brightness distribution also changes slightly, and its influence appears on the output voltage.
ところで、一定の加速度でこの新タイプの感知器を加振
した場合の感知部20の振動周波数に対する出力特性は
第8図のようになる。第8図(a)は水平振動(以下水
平動という)、第8図(b)垂直上下振動(以下上下動
という)の場合を示し、パラメータTI、T2.TIは
液体42の種類によって相違するが、例えば航空機の作
動油の場合T1は40℃程度、T2は0℃。Incidentally, when this new type of sensor is vibrated with a constant acceleration, the output characteristics of the sensing section 20 with respect to the vibration frequency are as shown in FIG. FIG. 8(a) shows the case of horizontal vibration (hereinafter referred to as horizontal motion), FIG. 8(b) shows the case of vertical vertical vibration (hereinafter referred to as vertical motion), and the parameters TI, T2. TI differs depending on the type of liquid 42, but for example, in the case of aircraft hydraulic fluid, T1 is about 40°C and T2 is 0°C.
T3は一10℃のようにTs >Tt >Tsの条件を
満足する液体43の温度、vlは液体温度Ts、水平振
動周波数l11zのときの感知部20の出力電圧、v2
は液体温度T2、水平振動周波数112〜5Hzまでの
ときの感知部20の出力電圧、■3は液体温度T3、水
平振動周波数IHzのときの感知部20の出力電圧、V
4はは液体温度T1、上下振動周波数IHzのときの感
知部20の出力電圧、v5は液体温度T2、上下振動周
波数IHz〜5Hzまでのときの感知部20の出力電圧
、v6は液体温度T3、上下振動周波数IHzのときの
感知部20の出力電圧である。T3 is the temperature of the liquid 43 that satisfies the condition of Ts > Tt > Ts such as -10°C, vl is the output voltage of the sensing unit 20 when the liquid temperature Ts is the horizontal vibration frequency l11z, and v2
is the output voltage of the sensing unit 20 when the liquid temperature is T2 and the horizontal vibration frequency is from 112 to 5 Hz, 3 is the output voltage of the sensing unit 20 when the liquid temperature is T3 and the horizontal vibration frequency is IHz, V
4 is the output voltage of the sensing unit 20 when the liquid temperature T1 is the vertical vibration frequency IHz, v5 is the output voltage of the sensing unit 20 when the liquid temperature T2 is the vertical vibration frequency IHz to 5Hz, v6 is the liquid temperature T3, This is the output voltage of the sensing section 20 when the vertical vibration frequency is IHz.
第8図から明らかなように、液体温度がT2の場合くは
周波数特性が111z〜511zの間でフラットな特性
の感知器として理想的な特性とな“るが、液体温度がT
1以上及びT3以下の場合は周波数特性がIHz〜5H
zの間でフラ′ットではな゛く、液体温度T!に゛比べ
低い液体温度T3の場合にはInx側が上がり、一方液
体温度12に□・比べ高い液体温度T1の場合にはIn
x側が下がる傾向になり、又5Hz近辺では前述と逆の
傾向が現出する。つまり、液体温度がT1以上及びT3
以下の場合にはたとえ一定加速度で感知器20を加振し
ても周波数が変われば感知器20の出力電圧が変わり誤
検出の恐れがでてくる。゛因゛み番こ80galで感知
器′を水平方向番こ加振した場合の実際に得られる感知
器の出力特性は第9図ニ示すトオリ、出力電FEVt
−1,2V(Tt−0℃)、v1Φ1.14V(Tl
−40℃)+ Vs゛*1.26V(Ts *−10
℃)であり、□「昇降機の技術基準、には普通縁感知器
の精度が±(設定値の10%+7)gal 、精密
級感知器の精度が±(設定値の5%+5 )’galと
定められており、又エレベータの機械室の室温は4G”
C以下に保持できるように換気装置を設けねばならない
と決められているので、温度が12以上であれば精密級
の感知器としての条件を満たすことができることが実験
により明らかとなった。As is clear from Fig. 8, when the liquid temperature is T2, the frequency characteristics are ideal as a flat sensor between 111z and 511z, but when the liquid temperature is T2, the frequency characteristics are ideal as a flat sensor.
If it is 1 or more and T3 or less, the frequency characteristic is IHz to 5H.
The liquid temperature is not flat between z and T! When the liquid temperature T3 is lower than □, the Inx side rises, while when the liquid temperature T1 is higher than the liquid temperature 12, the Inx side rises.
There is a tendency for the x side to decrease, and a tendency opposite to that described above appears near 5 Hz. In other words, the liquid temperature is T1 or higher and T3
In the following cases, even if the sensor 20 is vibrated at a constant acceleration, if the frequency changes, the output voltage of the sensor 20 will change and there is a risk of false detection. The output characteristics of the sensor that are actually obtained when the sensor is vibrated in the horizontal direction with an electric current of 80 gal are as shown in Figure 9, and the output voltage FEVt
-1,2V (Tt-0℃), v1Φ1.14V (Tl
-40℃)+Vs゛*1.26V(Ts*-10
℃), and □ "The technical standard for elevators is that the accuracy of a normal edge sensor is ± (10% of the setting value + 7) gal, and the accuracy of a precision grade sensor is ± (5% of the setting value + 5) 'gal. The room temperature in the elevator machine room is 4G.
Since it is stipulated that a ventilation system must be provided to maintain the temperature below C, experiments have revealed that if the temperature is 12 or higher, it can meet the requirements for a precision sensor.
このように温度によって特性が変化する理由は、温度が
下がると油の粘度が高くなり容器4゜内の液体が粘性抵
抗の大きな油のみの液体の特性(第10図(a)に図示
つに近くなり、又温度が上がると油の粘度が低くなり粘
性抵抗が小感くなってダンピング作用が少なくなり、第
10図(b)に図示する特性(容器40内の液体が水、
銀のみの特性)が優勢になるからである。The reason why the characteristics change with temperature is that as the temperature decreases, the viscosity of the oil increases, and the liquid within the 4° container has the characteristics of an oil-only liquid with a large viscous resistance (as shown in Figure 10 (a)). As the temperature increases, the viscosity of the oil decreases, the viscous resistance becomes less sensitive, and the damping effect decreases, resulting in the characteristics shown in FIG.
This is because the characteristics of silver alone become dominant.
したがって本発明では、例えば温度センサ48の感知温
度がT2になればフンパレータ50が出力信号を発し、
操作部51により接点51aを閉路してヒータ47に電
流を供給して液体43ヲ温め、フンパレータ50のヒス
テリシスの働きにより感知温度がT2を超えてT1まで
のある温度に達するとフンパレータ50は出力信号の発
生を止めて操作部51により接点518を開路する。そ
の後また温度センサ48の感知温度がT2以下になれば
再び接点51aを介してヒータ47に電流が供給されて
液体43の温度を上げ、この動作を繰り返すことにより
液体43の温度をT2近辺に保ち、常にIHz〜5Hz
の間で略フラットな周波数特性を維持して特に寒冷
地域での地震感知器の利用に支障が生じないようにする
ものである。Therefore, in the present invention, for example, when the temperature sensed by the temperature sensor 48 reaches T2, the humpator 50 emits an output signal,
The operation unit 51 closes the contact 51a and supplies current to the heater 47 to warm the liquid 43. When the sensed temperature exceeds T2 and reaches a certain temperature up to T1 due to the hysteresis of the fan plater 50, the fan plater 50 outputs an output signal. The operation section 51 opens the contact 518 after stopping the occurrence of the . After that, when the temperature sensed by the temperature sensor 48 falls below T2 again, current is again supplied to the heater 47 via the contact 51a to raise the temperature of the liquid 43, and by repeating this operation, the temperature of the liquid 43 is maintained near T2. , always IHz ~ 5Hz
This is to maintain a substantially flat frequency characteristic between the two regions, so that there is no problem in using the earthquake sensor, especially in cold regions.
以上の説明では、液体42番こ航空機の作動油を使用し
た一例を述べたもので、別の液体の場合番こけ温度をパ
ラメータとした周波数特性も変わってくるが、本発明の
技術思想は液体の種類が変わっても容易に応用のきくこ
とは明白である。The above explanation describes an example in which liquid No. 42 aircraft hydraulic oil is used.If other liquids are used, the frequency characteristics using the melting temperature as a parameter will be different, but the technical idea of the present invention is It is clear that the method can be easily applied even if the type of material changes.
以上述べたように本発明によれば、液体の温度を所定範
囲内に収める温度制御部を設けたため、地震波の周波数
特性と合致した理想的な特性を周囲温度4二関係なく常
に確保でき、誤動作の恐れをなくせるとともに、新タイ
プの地震感知器特有の1台の感知器で複数段の感知レベ
ルを設けることができる特徴をさらに生かすことができ
る特有の効果を発揮する。As described above, according to the present invention, since a temperature control unit is provided that keeps the temperature of the liquid within a predetermined range, ideal characteristics that match the frequency characteristics of seismic waves can always be maintained regardless of the ambient temperature, and malfunctions can occur. The new type of earthquake sensor has the unique effect of eliminating the fear of this, and making full use of the unique feature of the new type of earthquake sensor, which is the ability to provide multiple levels of sensing with a single sensor.
第1図は本発明による感知部の一例を示す断面図、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ック図、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図は感知部の出力についての実験結果を示す図
、第8図及び第9図は本発明に、よる地m感知器の振動
周波数に対する出−力特性の実験結果を示す図、第10
図は本発明の地震感知器の特性を説明する説明図である
。
2σ00.感知部
21、、、信号処理部
22、、、前置、増幅器
23 、25 、、 、 、フンパレータ24.2B、
、、出力回路
31.40.、、容 器
32.41,42,43.、、液 体
34.45.、、光 源
35.46.、、光電変換素子
47、、、ヒータ
48、、、温度センサ
特許出願人 フジチック株式会社
恥 J 図
62V21
株動?!(J(x)
第 3 回
兜 4 [¥l
も 5[21
I
To 6 図
児 7 図
(IIL) (b)¥iJ
8 図
(c) Cb)田FIG. 1 is a sectional view showing an example of a sensing section according to the present invention, and FIG.
Figure 3 shows an example of the structure of an electrodynamic seismic sensor; Figure 4 shows an example of the structure of a drop-weight seismic sensor; Figure 5 is a block diagram showing the configuration of a new type of earthquake sensor, Figure 6 is a cross-sectional view of the structure of an example of the sensing section of the new type of earthquake sensor, and Figure 7 is an experimental result of the output of the sensing section. FIGS. 8 and 9 are diagrams showing experimental results of the output characteristics of the ground m sensor with respect to vibration frequency according to the present invention, and FIGS.
The figure is an explanatory diagram illustrating the characteristics of the earthquake sensor of the present invention. 2σ00. Sensing unit 21, , Signal processing unit 22, Preamplifiers 23, 25, , Humperator 24.2B,
,,output circuit 31.40. ,, Container 32.41,42,43. ,,liquid 34.45. ,, light source 35.46. ,,Photoelectric conversion element 47,,,Heater 48,,,Temperature sensor patent applicant Fujichik Co., Ltd. J Figure 62V21 Stock movement? ! (J(x) 3rd helmet 4 [¥l も 5 [21 I To 6 fig. 7 fig. (IIL) (b) ¥iJ
8 Figure (c) Cb) field
Claims (1)
素子を備えた感知部と、該感知部の出力が所定値より大
きいとき出力を発する信号処理部とからなる感知器にお
いて、前記液体の温度制御部を備えたことを特徴とする
地震感知器。[Scope of Claims] A container containing a liquid, a light source that illuminates the inside of the container, a sensing section that includes a photoelectric conversion element that receives light in the container and converts it into an electrical signal, and an output of the sensing section that has a predetermined value. What is claimed is: 1. An earthquake sensor comprising a signal processing section that emits an output when the temperature is greater than a value, and further comprising a temperature control section for the liquid.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP59264901A JPS61142425A (en) | 1984-12-14 | 1984-12-14 | Seismic sensor |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP59264901A JPS61142425A (en) | 1984-12-14 | 1984-12-14 | Seismic sensor |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS61142425A true JPS61142425A (en) | 1986-06-30 |
| JPH0245136B2 JPH0245136B2 (en) | 1990-10-08 |
Family
ID=17409790
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP59264901A Granted JPS61142425A (en) | 1984-12-14 | 1984-12-14 | Seismic sensor |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS61142425A (en) |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH0743134U (en) * | 1993-12-20 | 1995-08-18 | こだま軽器工業株式会社 | Vacuum packaging machine |
Citations (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS54160261A (en) * | 1978-06-07 | 1979-12-18 | Berger Paul J | Method of converting mechanical motion of article into electric signal and electric to mechanical converter for executing same |
-
1984
- 1984-12-14 JP JP59264901A patent/JPS61142425A/en active Granted
Patent Citations (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS54160261A (en) * | 1978-06-07 | 1979-12-18 | Berger Paul J | Method of converting mechanical motion of article into electric signal and electric to mechanical converter for executing same |
Also Published As
| Publication number | Publication date |
|---|---|
| JPH0245136B2 (en) | 1990-10-08 |
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