JP2813769B2 - Method and apparatus for calculating the magnitude and source area of an earthquake by observing electromagnetic fields - Google Patents
Method and apparatus for calculating the magnitude and source area of an earthquake by observing electromagnetic fieldsInfo
- Publication number
- JP2813769B2 JP2813769B2 JP26790995A JP26790995A JP2813769B2 JP 2813769 B2 JP2813769 B2 JP 2813769B2 JP 26790995 A JP26790995 A JP 26790995A JP 26790995 A JP26790995 A JP 26790995A JP 2813769 B2 JP2813769 B2 JP 2813769B2
- Authority
- JP
- Japan
- Prior art keywords
- earthquake
- magnitude
- electromagnetic field
- area
- observing
- 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
- 230000005672 electromagnetic field Effects 0.000 title claims description 43
- 238000000034 method Methods 0.000 title claims description 20
- 239000002243 precursor Substances 0.000 claims description 26
- 230000014509 gene expression Effects 0.000 claims description 3
- 238000001514 detection method Methods 0.000 claims 1
- 239000011435 rock Substances 0.000 description 7
- 238000010586 diagram Methods 0.000 description 6
- 230000005684 electric field Effects 0.000 description 6
- 238000005516 engineering process Methods 0.000 description 6
- 230000006378 damage Effects 0.000 description 4
- 230000007423 decrease Effects 0.000 description 4
- 238000001228 spectrum Methods 0.000 description 4
- 230000033001 locomotion Effects 0.000 description 3
- 238000002474 experimental method Methods 0.000 description 2
- 238000012545 processing Methods 0.000 description 2
- 230000001360 synchronised effect Effects 0.000 description 2
- 206010039203 Road traffic accident Diseases 0.000 description 1
- 229910000831 Steel Inorganic materials 0.000 description 1
- 208000013201 Stress fracture Diseases 0.000 description 1
- 230000005856 abnormality Effects 0.000 description 1
- 230000005540 biological transmission Effects 0.000 description 1
- 239000004020 conductor Substances 0.000 description 1
- 238000011161 development Methods 0.000 description 1
- 238000006073 displacement reaction Methods 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 238000004880 explosion Methods 0.000 description 1
- 230000007774 longterm Effects 0.000 description 1
- 238000012423 maintenance Methods 0.000 description 1
- 206010037844 rash Diseases 0.000 description 1
- 238000011160 research Methods 0.000 description 1
- 238000005070 sampling Methods 0.000 description 1
- 230000003068 static effect Effects 0.000 description 1
- 239000010959 steel Substances 0.000 description 1
- 238000012360 testing method Methods 0.000 description 1
- 238000003325 tomography Methods 0.000 description 1
- 238000012549 training Methods 0.000 description 1
- 230000007704 transition Effects 0.000 description 1
- 230000001960 triggered effect Effects 0.000 description 1
Landscapes
- Geophysics And Detection Of Objects (AREA)
Description
【0001】[0001]
【発明の属する技術分野】本発明は、地震前に震源域で
発生する電磁界を観測して、地震の規模と震源域を、地
震発生の少なくとも1時間前には算出する電磁界の観測
による地震の規模と震源域の算出方法及びその装置に関
する。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a method for observing an electromagnetic field generated in an epicenter area before an earthquake, and determining the magnitude and the epicenter area of the earthquake at least one hour before the occurrence of the earthquake. The present invention relates to a method and an apparatus for calculating an earthquake magnitude and an epicenter area.
【0002】[0002]
【従来の技術】現在、電磁界を観測して、定状的に、地
震前に、震源域・マグニチュウド・発生時期を予報して
いる技術には、下記の2種類がある。2. Description of the Related Art At present, there are two types of techniques for observing an electromagnetic field and routinely predicting the epicenter, magnitude, and occurrence time before an earthquake.
【0003】(1)ギリシャに於ける地電位の観測によ
る地震予報: ギリシャのアテネ大学物理部で開発され
た技術で、1996年から、0.1Hz以下の地電位の
観測による地震予報が定常的に行われている。100k
m程度離れて16以上の観測点がある。多くは陸軍の演
習場等人工雑音の少ないところにあり、降雨等による自
然雑音は人間が常時監視している。各観測点には、東西
・南北、長・短の組合せの4基線があり、局地的な雑音
は4基線上に異なった現れかたをすることから、また、
汎地球的な磁気嵐に伴う地電位は多くの観測点に同時に
現れることから、地震前兆の地電位と区別している。地
震前兆の地電位の異常から約1カ月以内に(11日後頃
に最も多く)地震が発生し、場所の誤差は約100k
m、マグニチュウドの誤差は約0.7、予報率・的中率
は共に約0.7である。(1) Earthquake Forecast by Observing Geoelectric Potential in Greece: A technology developed by the Physical Department of the University of Athens in Greece. It has been done. 100k
There are 16 or more observation points about m apart. Many are located in places where there is little artificial noise, such as in the army training grounds, and natural noise due to rainfall and the like is constantly monitored by humans. Each observation point has four baselines, east / west / north / south, and long / short, and since local noise appears differently on the four baselines,
Geopotentials associated with a global magnetic storm appear simultaneously at many observation points, and are distinguished from those at the precursor of an earthquake. An earthquake occurred within about one month (about 11 days later) from the anomaly of the earth potential of the precursor of the earthquake, and the location error was about 100 k
m, the error of the magnitude is about 0.7, and both the forecast rate and the hit rate are about 0.7.
【0004】(2)ロシアに於けるオメガ電波の観測に
よる地震予報: ロシア科学アカデミー地球物理研究所
で開発された技術で、1991年から、オメガ電波の受
信による地震予報が行われている。9〜13kHzのオ
メガ電波は、その送受信点を除く伝搬路の近傍でマグニ
チュウド6以上の地震がある場合には、地震の約10〜
30日前に、その受信波の位相に異常が観測される。場
所の予報誤差、予報率、的中率は(1)の技術と同程度
である。(2) Earthquake Forecast by Observing Omega Radio Waves in Russia: A technology developed at the Russian Academy of Sciences Geophysical Research Institute, and since 1991, earthquake prediction has been performed by receiving omega radio waves. Omega radio waves of 9 to 13 kHz have a magnitude of 6 or more near the propagation path excluding the transmission / reception point.
30 days before, an abnormality is observed in the phase of the received wave. The forecast error, forecast rate, and hit rate of the place are similar to those of the technique of (1).
【0005】[0005]
【発明が解決しようとする課題】上述の[従来の技術]
(1)の技術は長期間の経験を必要とする欠点があり、
(2)の技術は、電波の発射を必要とし、施設の整備・
運用が困難と言う欠点がある。(1)、(2)の技術
は、共に、日時・場所の予報は何れも漠然としているた
め、これらの予報技術の有意性の有無の検定は非常に困
難である。有意性がはっきりしないこと以外にも、これ
らの予報精度が社会的要請から程遠いため、予報による
経済的損失が非常に大きい。例えば、場所の誤差を半径
100kmとし、誤差の範囲内に居住する人が、日時の
誤差の最大値の30日間避難し、この範囲・期間内では
経済活動が停滞するならば、予報したことにより生ずる
経済的損失は、予報しなかった場合の経済的被害の2倍
以上となる可能性が大きい。以上の様に、従来の予報技
術には、我が国での利用が困難なことと、精度が社会的
要請に程遠く、予報による経済的損失が大きいと言う問
題がある。[Problems to be Solved by the Invention] [Prior Art]
The technique (1) has the disadvantage of requiring long-term experience,
The technology of (2) requires the emission of radio waves,
There is a drawback that operation is difficult. In both of the techniques (1) and (2), the prediction of the date and time and place are vague, and it is very difficult to test the significance of these prediction techniques. In addition to the lack of significance, these forecasts are far from societal demands, so the economic losses from forecasts are very large. For example, if the location error is 100 km in radius, and if a person who lives within the range of the error evacuates for 30 days, which is the maximum value of the date and time error, and economic activity stagnates within this range and period, it is predicted that The resulting economic loss is likely to be more than twice the economic damage if not foreseen. As described above, the conventional forecast technology has problems that it is difficult to use in Japan, that accuracy is far from social demands, and that economic loss due to forecast is large.
【0006】本発明は、上記の問題を解決するもので、
マグニチュウド及び震度が6以上の地震は、震源域を誤
差約10kmで、1〜3時間前に確実に算出し、予報に
よる経済的損失を最小にする方法及びその装置を提供す
る。The present invention solves the above problems,
The present invention provides a method and an apparatus for calculating an earthquake area with a magnitude of 6 km or more and an earthquake area of about 10 km with an error of about 1 to 3 hours in advance and minimizing economic loss due to forecasting.
【0007】[0007]
【課題を解決するための手段】18世紀には既に、地磁
気や地電流が地震前に変化すると言われていた。196
6年3月の中国でのマグニチュウド7.2の地震が契機
となって、地震前兆電波の存在が考えられるようになっ
た。1976年からは、多数の地震前兆電波の観測例が
発表されるようになった。多くの観測例があるにもかか
わらず、電磁界の観測による地震予知がこれまで疑問視
されてきたのは、地震発生と同期した電磁界が観測され
ていなかったためである。と言うのは、前兆電磁界が発
生するのならば、地震発生時にも、同じ様なメカニズム
の電磁界が多少なりとも観測される可能性が大きく、発
生時に観測されないと云うことは、前兆電磁界が無いこ
とを示すと考えられたためである。この様な状態の中
で、1994年10月4日に観測史上最大のマグニチュ
ウド8.1の北海道東方沖地震が発生し、関東一円にあ
る発明者の7箇所の全観測点で、1〜9kHz帯で、人
工雑音・近接雷を除いて最大の電界変動が観測された。
この観測の成功が契機となって、これ以降は、地震時及
び地震前後に発生する電界の波形、スペクトル等が観測
できるようになった。これまでの観測で、マグニチュウ
ド・震度が大きいほど前兆電磁界のパルス(正確には時
間長が約5msの波束)の発生頻度・振幅が大きく、地
震の1〜3時間前に、発生頻度・振幅が共に最大となる
ことが明らかになった(図2〜図4参照)。図2は、1
994年10月4日22時23分のマグニチュウド8.
1の北海道東方沖地震の際、茨城県波崎町で受信した1
〜9kHzの電界のパルスの頻度分布図である。横軸
は、左端に示す年月の日を示す。縦軸は、毎時の0分か
ら1分迄の、振幅が0.134mVよりも大きいパルス
の数である。図3は、1995年1月10日3時0分の
マグニチュウド6.2の茨城県沖地震の際、茨城県波崎
町で受信した1〜9kHzの電界のパルスの頻度分布図
である。その他は図2と同じである。図4は、図3の地
震の際、千葉県千倉町で受信した1〜9kHzの電界の
パルスの頻度分布図である。その他は図2と同じであ
る。この現象を利用した地震予知システム(図1参照)
の開発・整備を進めてきた結果、本発明をなすに至っ
た。In the eighteenth century, it was already said that geomagnetism and geocurrent would change before the earthquake. 196
The magnitude 7.2 earthquake in China in March 2006 triggered the possibility of the presence of earthquake precursory radio waves. Since 1976, many examples of observations of earthquake precursory radio waves have been published. Despite the many observations, the reason why earthquake prediction based on electromagnetic field observation has been questioned so far is that electromagnetic fields synchronized with the occurrence of the earthquake were not observed. The reason is that if a precursor electromagnetic field is generated, there is a high possibility that an electromagnetic field of a similar mechanism will be observed at all even during an earthquake, and that it will not be observed at the time of the occurrence. This was because it was considered to indicate that there was no world. Under such conditions, the largest earthquake in the eastern Hokkaido area, 8.1 magnitude, occurred in the history of observation on October 4, 1994. In the 9 kHz band, the largest electric field fluctuation was observed except for artificial noise and proximity lightning.
Following the success of this observation, the waveform, spectrum, etc. of the electric field generated during and before and after the earthquake can now be observed. According to the observations to date, the larger the magnitude and the seismic intensity, the higher the frequency and amplitude of the precursor electromagnetic field pulse (accurately, a wave packet with a time length of about 5 ms), and the frequency and amplitude of the occurrence 1 to 3 hours before the earthquake It became clear that both became maximum (refer FIG. 2-FIG. 4). FIG.
7. The magnitude at 22:23 on October 4, 994.
1 Received at Hasaki-cho, Ibaraki Prefecture during the 1st Hokkaido Offshore Earthquake
It is a frequency distribution figure of the pulse of the electric field of 99 kHz. The horizontal axis indicates the date of the year and month shown on the left end. The vertical axis is the number of pulses from 0 minute to 1 minute each hour with an amplitude greater than 0.134 mV. FIG. 3 is a frequency distribution diagram of 1 to 9 kHz electric field pulses received in Hasaki Town, Ibaraki Prefecture, at the time of the magnitude 6.2 earthquake off the coast of Ibaraki Prefecture at 3:00 on January 10, 1995. Others are the same as FIG. FIG. 4 is a frequency distribution diagram of 1 to 9 kHz electric field pulses received in Chikura Town, Chiba Prefecture during the earthquake of FIG. Others are the same as FIG. Earthquake prediction system using this phenomenon (see Fig. 1)
As a result of the development and maintenance of the present invention, the present invention has been achieved.
【0008】前述の従来の技術の課題を解決するため
に、本発明に係わる電磁界の観測による地震の規模と震
源域の算出方法は、地震の前に地震の発生場所たる震源
域で発生する電磁界を観測して、地震の規模と震源域を
地震の前に算出する方法において、少なくとも4箇所の
観測点で電磁界を観測し、地震前の地震前兆電磁界パル
スを同定し、その発生領域を算出して震源域とし、地震
の規模たるマグニチュウドをパルスの発生領域の広さ・
長さ、及びパルスの振幅・発生数・発生頻度から算出
し、地震の発生をパルスの発生頻度の変化から地震の発
生前に知るものとした。 また、本発明に係わる電磁界
の観測による地震の規模と震源域の算出装置は、地震の
前に地震の発生場所たる震源域で発生する電磁界を観測
して、地震の規模と震源域を地震の前に算出する装置に
おいて、少なくとも4箇所の観測点で電磁界を観測する
電磁界観測手段と、各電磁界観測手段により観測された
地震前の地震前兆電磁界パルスを同定する地震前兆電磁
界同定手段と、その発生領域を算出する震源域算出手段
と、地震の規模たるマグニチュウドをパルスの発生領域
の広さ・長さ、及びパルスの振幅・発生数・発生頻度か
ら算出するマグニチュウド算出手段と、地震の発生をパ
ルスの発生頻度の変化から発生前に知る発生検出手段と
を備えるものとした。In order to solve the above-mentioned problems of the prior art, the method of calculating the magnitude and source area of an earthquake by observing an electromagnetic field according to the present invention occurs in the source area, which is the place where the earthquake occurs, before the earthquake. In the method of observing the electromagnetic field and calculating the magnitude and source area of the earthquake before the earthquake, observe the electromagnetic field at at least four observation points, identify the pre-earthquake precursor electromagnetic field pulse, and generate it. The area is calculated as the epicenter, and the magnitude, which is the magnitude of the earthquake,
It was calculated from the length, the pulse amplitude, the number of occurrences, and the frequency of occurrence, and the occurrence of the earthquake was known from the change in the frequency of occurrence of the pulse before the occurrence of the earthquake. In addition, the apparatus for calculating the magnitude and source area of an earthquake based on the observation of an electromagnetic field according to the present invention observes the electromagnetic field generated in the source area, which is the place where the earthquake occurred, before the earthquake, and determines the magnitude and source area of the earthquake. An apparatus for calculating before an earthquake, an electromagnetic field observing means for observing an electromagnetic field at at least four observation points, and a seismic precursor electromagnetic field for identifying a pre-earthquake pre-earthquake electromagnetic field pulse observed by each electromagnetic field observing means. Field identification means, source area calculation means for calculating the generation area thereof, and magnitude calculation means for calculating the magnitude, which is the magnitude of the earthquake, from the width and length of the generation area of the pulse, and the amplitude, number of occurrences, and frequency of the pulse And an occurrence detecting means for knowing the occurrence of the earthquake before the occurrence from the change in the frequency of occurrence of the pulse.
【0009】[0009]
【発明の実施の形態】次に、本発明に係わる電磁界の観
測による地震の規模と震源域の算出方法の実施形態を説
明する。先ず、第一段階において、少なくとも4箇所の
観測点で電磁界を観測することにより、例えば、観測点
間の距離が10〜1000km程度の場合に、受信時刻
の差がそれぞれ0.1〜10ms以下でパルスが観測さ
れた場合、少なくとも3個の独立の受信時刻差から、パ
ルスの発生源を同定する。第二段階において、上記のパ
ルスの波形・スペクトルと既知の地震前兆電磁界のそれ
らと比較して異質なパルスは排除する。また、パルスの
発生源と、市売されている雷発生領域のデータを比較し
て、雷によるパルスの発生領域を排除する。第三段階に
おいて、排除されなっかったパルスの発生領域を地震前
兆電磁界の発生領域と同定し、震源域とする。第四段階
において、同定した領域の広さ・長さ、及びパルスの振
幅・発生数からマグニチュウドを算出する。第五段階と
して、震源域から出ているパルスの発生頻度の変化か
ら、地震の発生を地震前に知る。DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS Next, an embodiment of a method of calculating an earthquake magnitude and an epicenter according to the present invention by observing an electromagnetic field will be described. First, in the first stage, by observing the electromagnetic field at at least four observation points, for example, when the distance between the observation points is about 10 to 1000 km, the difference between the reception times is 0.1 to 10 ms or less, respectively. If a pulse is observed in the above, the source of the pulse is identified from at least three independent reception time differences. In the second stage, extraneous pulses are eliminated as compared with those of the above-mentioned pulse waveform and spectrum and those of the known pre-seismic electromagnetic field. In addition, the pulse generation source is compared with the data of the lightning generation region on the market to exclude the pulse generation region due to lightning. In the third stage, the region where the pulse that has not been eliminated is identified as the region where the pre-earthquake electromagnetic field is generated is defined as the epicenter region. In the fourth step, the magnitude is calculated from the width and length of the identified area, and the amplitude and number of generated pulses. The fifth step is to know the occurrence of the earthquake before the earthquake based on the change in the frequency of the pulse emitted from the epicenter.
【0010】次に、図1に基づいて、本発明に係わる電
磁界の観測による地震の規模と震源域の算出装置の実施
形態を説明する。なお、本実施形態においては、マグニ
チュウドと震度が共に一定値(例えば6)以上の地震の
場合に、マグニチュウドを誤差1以下、場所を誤差10
km程度で、1〜3時間前に算出するものとして説明す
る。Next, an embodiment of an apparatus for calculating the magnitude and source area of an earthquake by observing an electromagnetic field according to the present invention will be described with reference to FIG. In the present embodiment, when the magnitude and the seismic intensity are both equal to or larger than a predetermined value (for example, 6), the magnitude is set to an error of 1 or less, and the location is set to an error of 10 or less.
The description will be made on the assumption that the distance is calculated about 1 km to about 1 km before.
【0011】互いに約100km離れた少なくとも4箇
所の観測点で、図1の、第1センサー1a及び第1観測
装置2aよりなる第1観測局、第2センサー1b及び第
2観測装置2bよりなる第2観測局、第3センサー1c
及び第3観測装置2cよりなる第3観測局、並びに第4
センサー1d及び第4観測装置2dよりなる第4観測局
に於て電磁界を観測する。これら第1観測局〜第4観測
局が、少なくとも4箇所の観測点で電磁界を観測する電
磁界観測手段として機能する。この観測技術としては、
既存の技術、例えば、「地震前兆の電界変動の観測法」
(特許第1813589号)に関する技術、即ち電磁界
の検出のためのセンサーとして深井戸のケーシング鋼
管、または海底に敷設したダイポールアンテナ及びルー
プアンテナを用いる。観測された任意の一定値以上の振
幅(:A0)(下記の仕様例参照)のパルスを、図1の
主局に伝送し、第1データ記録装置3a〜第4データ記
録装置3dに記録し、各観測点毎の任意の一定値以上の
振幅(:A1>A0)のパルス数及びその頻度分布を出
力する。異なる観測点で、受信時刻差が一定値(例えば
1ms)以下で、振幅が任意の一定値(:A2>A0)
以上で受信されたパルスがあるときは、第1相関器4a
〜第3相関器4cにより相関強度(振幅)と遅延時間を
算出し、誤差 10μs以下で受信時刻差を求める。電
磁波の伝搬速度として、3×105 〜 105 km/s
を仮定して、データ処理装置5により、2点で観測され
た場合は、発生源の可能性のある位置の軌跡(双曲線)
を、3点で観測された場合は虚点(イマジナリポイン
ト)を含めて、発生源の可能性のある位置を、4点以上
で観測された場合は発生源の可能性のある位置を、市売
されている雷情報と一緒に地図上に、表示装置6を用い
て表示する。At least four observation points approximately 100 km apart from each other, a first observation station composed of the first sensor 1a and the first observation device 2a and a first observation station composed of the second sensor 1b and the second observation device 2b shown in FIG. 2 observation stations, 3rd sensor 1c
And a third observation station composed of the third observation device 2c and a fourth observation station
An electromagnetic field is observed at a fourth observation station including the sensor 1d and the fourth observation device 2d. These first to fourth observation stations function as electromagnetic field observation means for observing the electromagnetic field at at least four observation points. As this observation technology,
Existing technology, for example, "Earthquake precursor electric field fluctuation observation method"
A technique related to (Japanese Patent No. 1813589), that is, a deep well casing steel pipe or a dipole antenna and a loop antenna laid on the sea floor are used as sensors for detecting an electromagnetic field. A pulse having an amplitude (: A0) (refer to the following specification example) of an observed value equal to or larger than a given constant value is transmitted to the master station in FIG. 1 and recorded in the first to fourth data recording devices 3a to 3d. , The number of pulses having an amplitude (: A1> A0) equal to or greater than an arbitrary constant value for each observation point and the frequency distribution thereof are output. At different observation points, the reception time difference is equal to or less than a fixed value (for example, 1 ms) and the amplitude is an arbitrary fixed value (: A2> A0).
When there is a pulse received as described above, the first correlator 4a
To calculate the correlation strength (amplitude) and delay time by the third correlator 4c, and obtain the reception time difference with an error of 10 μs or less. 3 × 10 5 to 10 5 km / s as the propagation speed of the electromagnetic wave
If the data processing device 5 observes at two points, the trajectory (hyperbola) of the position where the source may be generated
If three or more observations are made, the location of the potential source, including the imaginary point (imaginary point), is taken. The information is displayed on the map together with the sold lightning information using the display device 6.
【0012】上記の各観測点でのデータの取り込みの仕
様の一例を下記に示す。An example of a specification for taking in data at each of the above observation points is shown below.
【0013】仕様概要(仕様例)Specification overview (example of specification)
【0014】周波数:1〜9kHz. 振幅:10μv〜100mV. サンプリング周波数:50kHz. 時刻精度:1μs.Frequency: 1 to 9 kHz. Amplitude: 10 μv to 100 mV. Sampling frequency: 50 kHz. Time accuracy: 1 μs.
【0015】地震前兆電磁界パルス(前兆パルス)の同
定は、パルスの振幅・周期。波形・スペクトル及び発生
領域の広さ・形・動きが、既知の前兆パルスのそれらと
同質のパルスを選び出すことにより行う。即ち、以下の
(1)〜(4)の条件に沿って判断する。The identification of an earthquake precursor electromagnetic field pulse (precursor pulse) is based on the pulse amplitude and period. The size, shape, and movement of the waveform, spectrum, and generation area are determined by selecting pulses of the same quality as those of the known precursor pulses. That is, the determination is made according to the following conditions (1) to (4).
【0016】(1)一定範囲の振幅(例えば、上記の仕
様例)以外のパルスは前兆パルスとはしない。 (2)一定周期を持つパルスは人工雑音と見なし、前兆
パルスとはしない。 (3)波形・スペクトルが、既知の前兆パルスのそれら
と異なるパルスは前兆パルスとはしない。 (4)前述の表示結果を用いて、パルスの発生領域を、
雷情報と比較し、発生領域が空電のそれと同じ広さ・形
・動きをする領域のパルスは、前兆パルスとはしない。(1) Pulses other than a certain range of amplitudes (for example, the above specification example) are not regarded as precursor pulses. (2) A pulse having a fixed period is regarded as artificial noise, and is not a precursor pulse. (3) A pulse whose waveform / spectrum is different from those of the known precursor pulse is not regarded as a precursor pulse. (4) Using the above display result, the pulse generation area
Compared with the lightning information, the pulse in the area where the generation area has the same size, shape, and movement as that of static is not a precursor pulse.
【0017】パルスの発生領域の同定は、既存の技術、
例えば市売されている雷位置標定システム、地震の震源
決定システム、または「地震前兆の長波・地電流の発生
領域のトモグラフイ法」(特許第1813607号)に
関する異なる観測点の観測電磁界間の相互相関により発
生領域のトモグラフを作成することにより行う。The identification of the region where the pulse is generated can be performed by using an existing technique,
For example, the mutual relationship between observed electromagnetic fields at different observation points concerning a lightning location system, a hypocenter determination system of an earthquake, or a tomography method of a long wave / ground current generation region of an earthquake precursor (Patent No. 1813607). This is performed by creating a tomograph of the generation area by correlation.
【0018】これまでの地震前兆電磁界の観測及び岩石
の破壊実験の結果によれば、震源域は上述の前兆パルス
の発生領域と一致する。このことは理論的には次の様に
説明できる。地震前の震源域では、地殻の比抵抗の急減
が観測されており、岩石の破壊実験でも、崩壊前の比抵
抗の急減が観測されている。比抵抗の急減は崩壊前の微
小亀裂の発生と同期しており、亀裂面が良導体となるこ
とによる。地震前の震源域の抵抗が急減すれば、そこを
流れている地電流が急変し、電磁界変動の発生源とな
る。地震の際には、震源域の岩石は破壊されるから、地
震時及びその前後には震源域では電磁界変動、即ち電磁
界パルスが発生する。According to the results of the observation of the electromagnetic field before the earthquake and the results of the rock destruction experiment, the epicenter area coincides with the above-mentioned generation region of the precursor pulse. This can be explained theoretically as follows. In the epicenter area before the earthquake, a sharp decrease in the resistivity of the crust was observed, and even in a rock destruction experiment, a sharp decrease in the resistivity before the collapse was observed. The rapid decrease in specific resistance is synchronized with the generation of microcracks before collapse, and the crack surface becomes a good conductor. If the resistance of the epicenter before the earthquake sharply decreases, the ground current flowing there will change suddenly, and it will be a source of electromagnetic field fluctuations. During an earthquake, rocks in the epicenter are destroyed, so that an electromagnetic field fluctuation, that is, an electromagnetic pulse, occurs in the epicenter before and after the earthquake.
【0019】前述のパルスの振幅(相関強度)・総数・
発生頻度がマグニチュウド・震度と共に大きくなる経験
則を基に、マグニチュウドを推定するとともに、下記の
経験式を用いてマグニチュウドを算出する。 M=Log(S)+3.9、 M=2×Log(L)+3.6、 ここに、M:マグニチュウド、 S:前兆パルスの発生領域の広さ(km2 )、 L:前兆パルスの発生領域の長さ(km)。The above-mentioned pulse amplitude (correlation strength), total number,
Based on the empirical rule that the occurrence frequency increases with the magnitude and seismic intensity, the magnitude is estimated, and the magnitude is calculated using the following empirical formula. M = Log (S) +3.9, M = 2 × Log (L) +3.6, where M: magnitude, S: width (km 2 ) of the precursor pulse generation area, L: generation of precursor pulse The length of the area (km).
【0020】上式は理論的には次のように説明できる。
地震のエネルギーをE、すべり量をDとすると、EはS
・Dにほぼ比例する。一方、SはLの2乗にほぼ比例
し、DはLにほぼ比例する。これらの関係を下記のMと
Eの関係式(定義)に代入すると、常数項を除いて、前
述のMとS、及びMとLの関係式が得られる。 1.5×M=Log(E)+k、 ここに、k:常数The above equation can be theoretically explained as follows.
If the energy of the earthquake is E and the slip is D, E is S
-It is almost proportional to D. On the other hand, S is approximately proportional to the square of L, and D is approximately proportional to L. By substituting these relations into the following relational expression (definition) of M and E, the above-mentioned relational expressions of M and S and M and L are obtained except for the constant term. 1.5 × M = Log (E) + k, where k: constant
【0021】地震発生前の震源域とマグニチュウドの算
出は下記の様に行う。即ち、「今、上記の場所(前兆パ
ルスの発生領域)で地震が起きれば、そのマグニチュウ
ドは上記の値となる。」とする。観測では、1時間で
は、前述のパルス頻度は30倍以上(Mが1増えれば、
地震のエネルギーは約31.6倍となる)は変わってい
ないため(図2〜図4参照)、前述の方法で、例えば、
Mが5になった時から始めれば、Mが6以上の地震は、
誤差1以下で、1時間以上前には算出できることにな
る。即ち、Mの計算値が5になったとき、前兆パルスの
発生領域で、1時間後以降に、Mが5〜6の地震が起き
ると算出し、以後、Mの計算値が変わり、大きくなれ
ば、その都度、それに応じてMを大きくしていく。The calculation of the source area and magnitude before the occurrence of the earthquake is performed as follows. In other words, "if an earthquake occurs at the above-mentioned location (a region where a precursor pulse is generated), the magnitude will be the above value". According to observations, in one hour, the above pulse frequency is 30 times or more (if M increases by 1,
Since the energy of the earthquake is about 31.6 times) (see FIGS. 2 to 4), the method described above, for example,
If we start from when M becomes 5, an earthquake with M over 6 will
With an error of 1 or less, it can be calculated one hour or more ago. That is, when the calculated value of M becomes 5, it is calculated that an earthquake with M of 5 to 6 occurs after 1 hour in the region where the precursor pulse is generated, and thereafter, the calculated value of M changes and becomes larger. In each case, M is increased accordingly.
【0022】この方法は理論的には次の様に説明でき
る。岩石破壊の際、横軸に変移量、縦軸に電気伝導度ま
たは微小亀裂の発生頻度を取ると、図2〜4と同じ様な
形のグラフが得られる。このことは、地震前兆のパルス
が岩石の微小破壊に対応するとした前述の説明を支持し
ている。分布がほぼ正規分布であり、変移は時間にほぼ
比例し、ある時点から微小亀裂が増加し、微小亀裂の頻
度がほぼ最大となる時点(通常は最大値を少し過ぎた時
点)で岩石は崩壊する。即ち、微小亀裂の増加から、崩
壊前にそれを知ることが出来る。地震は岩石の崩壊を伴
うから、上記の理由により、地震前に、地震前兆パルス
の増加から地震の発生を知ることが出来ることになる。This method can be explained theoretically as follows. In the case of rock destruction, if the horizontal axis indicates displacement and the vertical axis indicates electric conductivity or the frequency of occurrence of microcracks, graphs similar to those in FIGS. This supports the earlier explanation that seismic precursor pulses correspond to rock microfracture. The distribution is almost normal, the transition is almost proportional to time, the microcracks increase from a certain point, and the rock collapses when the frequency of the microcracks becomes almost maximum (usually a little after the maximum value) I do. That is, it can be known before the collapse from the increase in the microcracks. Since an earthquake involves the collapse of rock, the occurrence of an earthquake can be known from the increase in the number of precursor signs before the earthquake for the above reason.
【0023】[0023]
【発明の効果】以上述べたように、本発明に基づき、災
害を伴う大地震の定量的直前予報が可能となるため、地
震動に伴う反応炉の暴走・爆発・火災・交通事故・圧死
等の地震災害の軽減が可能となる。また、噴火は地震を
伴い、津波は地震に伴うため、本発明に基づき、噴火・
津波の直前予報も可能となる。As described above, according to the present invention, it is possible to make a quantitative forecast immediately before a large earthquake accompanying a disaster, and it is possible to prevent runaway, explosion, fire, traffic accident, pressure death, etc. of the reactor due to earthquake motion. Earthquake disaster can be reduced. In addition, eruptions are accompanied by earthquakes, and tsunamis are caused by earthquakes.
Forecast just before the tsunami is also possible.
【図1】 地震前兆電磁界及びその発生領域を同定する
システムの概念を示すブロック図FIG. 1 is a block diagram showing the concept of a system for identifying a pre-earthquake electromagnetic field and its generation region.
【図2】 パルス頻度分布の第1例を示すパルス頻度分
布図FIG. 2 is a pulse frequency distribution diagram showing a first example of a pulse frequency distribution.
【図3】 パルス頻度分布の第2例を示すパルス頻度分
布図FIG. 3 is a pulse frequency distribution diagram showing a second example of the pulse frequency distribution.
【図4】 パルス頻度分布の第3例を示すパルス頻度分
布図FIG. 4 is a pulse frequency distribution diagram showing a third example of the pulse frequency distribution.
1:観測点にある観測局のセンサー(電極、アンテナま
たは磁気センサー)。 2:観測装置。 3:データ記録装置。 4:相関器。 5:データ処理装置。 6:表示装置。1: Sensor (electrode, antenna or magnetic sensor) of the observation station at the observation point. 2: Observation device. 3: Data recording device. 4: Correlator. 5: Data processing device. 6: Display device.
Claims (2)
発生する電磁界を観測して、地震の規模と震源地を地震
の前に算出する方法において、少なくとも4箇所の観測
点で電磁界を観測し、地震前の地震前兆電磁界パルスを
同定し、その発生領域を算出して震源域とし、地震の規
模たるマグニチュウドMをパルスの発生領域の広さSも
しくは長さLから「M=log(S)+3.9」もしく
は「M=2×log(L)+3.6」の関係式に基づき
算出し、算出したマグニチュウドMもしくはM+1の規
模の地震の発生可能性を1時間以上前に知ることを特徴
とする電磁界の観測による地震の規模と震源域の算出方
法。1. A method of observing an electromagnetic field generated in an epicenter area where an earthquake occurs before an earthquake, and calculating the magnitude and the epicenter of the earthquake before the earthquake. Observing the field, identifying the pre-earthquake precursor electromagnetic field pulse, calculating the area where the pulse occurred, and setting it as the epicenter area, the magnitude M, which is the magnitude of the earthquake, is also the size S of the pulse generation area
"M = log (S) +3.9" is properly from the length L Moshiku
Is calculated based on the relational expression of “M = 2 × log (L) +3.6”, and the calculated magnitude M or M + 1 is calculated.
A method of calculating the magnitude and source area of an earthquake by observing an electromagnetic field, wherein the possibility of occurrence of a model earthquake is known at least one hour before.
発生する電磁界を観測して、地震の規模と震源地を地震
の前に算出する装置において、少なくとも4箇所の観測
点で電磁界を観測する電磁界観測手段と、各電磁界観測
手段により観測された地震前の地震前兆電磁界パルスを
同定する地震前兆電磁界同定手段と、その発生領域を算
出する震源域算出手段と、地震の規模たるマグニチュウ
ドMをパルスの発生領域の広さSもしくは長さLから
「M=log(S)+3.9」もしくは「M=2×lo
g(L)+3.6」の関係式に基づき算出するマグニチ
ュウド算出手段と、算出したマグニチュウドMもしくは
M+1の規模の地震の発生可能性を1時間以上前に知る
発生検出手段とを備えることを特徴とする電磁界の観測
による地震の規模と震源域の算出装置。2. An apparatus for observing an electromagnetic field generated in an epicenter area where an earthquake occurs before an earthquake, and calculating the magnitude and the epicenter of the earthquake before the earthquake. Electromagnetic field observing means for observing the field, seismic precursor electromagnetic field identifying means for identifying a pre-earthquake precursor electromagnetic field pulse observed by each electromagnetic field observing means, and an epicenter area calculating means for calculating an occurrence area thereof; The magnitude M, which is the magnitude of the earthquake, is determined from the width S or length L of the pulse generation area.
“M = log (S) +3.9” or “M = 2 × lo
g (L) +3.6 ”, and a magnitude calculation unit that calculates the magnitude M or the calculated magnitude M
An apparatus for calculating a magnitude and a source area of an earthquake by observing an electromagnetic field, comprising: an occurrence detection means for knowing the possibility of occurrence of an M + 1-scale earthquake at least one hour before.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP26790995A JP2813769B2 (en) | 1995-09-21 | 1995-09-21 | Method and apparatus for calculating the magnitude and source area of an earthquake by observing electromagnetic fields |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP26790995A JP2813769B2 (en) | 1995-09-21 | 1995-09-21 | Method and apparatus for calculating the magnitude and source area of an earthquake by observing electromagnetic fields |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH0990051A JPH0990051A (en) | 1997-04-04 |
| JP2813769B2 true JP2813769B2 (en) | 1998-10-22 |
Family
ID=17451311
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP26790995A Expired - Lifetime JP2813769B2 (en) | 1995-09-21 | 1995-09-21 | Method and apparatus for calculating the magnitude and source area of an earthquake by observing electromagnetic fields |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JP2813769B2 (en) |
Families Citing this family (6)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2002082176A (en) * | 2000-09-07 | 2002-03-22 | Kato Hiroshi | System providing data for inferring event whose occurrence needs to be predicted |
| JP2004233053A (en) * | 2000-12-12 | 2004-08-19 | Hiroyuki Inubushi | Apparatus and method for solving problem occurring immediately before or after earthquake |
| JP2006145234A (en) * | 2004-11-16 | 2006-06-08 | Toshiba Corp | Emergency earthquake flash report terminal and its usage |
| JP2008076321A (en) * | 2006-09-25 | 2008-04-03 | Kozo Takahashi | Earthquake prediction method and earthquake prediction apparatus |
| JP5470632B2 (en) * | 2008-10-01 | 2014-04-16 | 公立大学法人首都大学東京 | Method and apparatus for issuing an emergency earthquake warning |
| CN114222934B (en) * | 2019-08-20 | 2025-08-12 | 日本电气株式会社 | Earthquake observation apparatus, earthquake observation method, and recording medium |
Family Cites Families (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH05267909A (en) * | 1992-03-19 | 1993-10-15 | Taiyo Yuden Co Ltd | Antenna shared device |
-
1995
- 1995-09-21 JP JP26790995A patent/JP2813769B2/en not_active Expired - Lifetime
Also Published As
| Publication number | Publication date |
|---|---|
| JPH0990051A (en) | 1997-04-04 |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| Hayakawa et al. | Current status of seismo-electromagnetics for short-term earthquake prediction | |
| US6462549B1 (en) | Method and system for electroseismic monitoring of microseismicity | |
| Wu | Progress on development of an earthquake early warning system using low-cost sensors | |
| US7277797B1 (en) | Prediction system and method | |
| US8200434B2 (en) | Tsunami detection method and system | |
| JPH0194286A (en) | Method for foretelling earthquake by tomography or generation region of long wave earth current being premonitory symptoms of earthquake | |
| Hayakawa | Earthquake precursor studies in Japan | |
| Grapenthin et al. | The utility of GNSS for earthquake early warning in regions with sparse seismic networks | |
| Hayakawa | Seismo electromagnetics and earthquake prediction: History and new directions | |
| Iio et al. | Which is heterogeneous, stress or strength? An estimation from high-density seismic observations | |
| JP2813769B2 (en) | Method and apparatus for calculating the magnitude and source area of an earthquake by observing electromagnetic fields | |
| Doi et al. | Landslide characteristics revealed by high‐frequency seismic waves from the 2017 landslide in central Japan | |
| CN104142522B (en) | A kind of detection method of city buried faults | |
| Liu et al. | An integrated study of anomalies observed before four major earthquakes: 2004 Sumatra M9. 3, 2006 Pingtung M7. 0, 2007 Chuetsu Oki M6. 8, and 2008 Wenchuan M8. 0 | |
| Peng et al. | The Namche barwa temporary seismic network (NBTSN) and its application in monitoring the 18 november 2017 M 6.9 mainling, Tibet, China, earthquake | |
| Ashenden et al. | Some challenges of monitoring a potentially active volcanic field in a large urban area: Auckland volcanic field, New Zealand | |
| Zhang et al. | Test of the Predictability of the PI Method for Recent Large Earthquakes in and near Tibetan Plateau | |
| Pulinets et al. | Multiparameter approach and LAIC validation | |
| Gladychev et al. | Study of electromagnetic emissions associated with seismic activity in Kamchatka region | |
| Novoselov et al. | Seismoacoustic study of thunder and lightning using the AlpArray | |
| Cho et al. | Ionospheric Irregularities Signature Correlation on ROT Variation for Earthquake Detection and Epicenter Estimation: Case Study of Tohoku (2011) & Turkey-Syria (2023) Earthquakes | |
| Pilipenko et al. | Seismoelectromagnetic and seismoionospheric phenomena: From the pioneering works of GA Sobolev to present | |
| Eshkuvatov et al. | Pre-seismic ionospheric disturbances following the 2025 Mw 7.7 Mandalay, Burma (Myanmar) Earthquake from GNSS observations | |
| Adebayo et al. | First report on coseismic ionospheric disturbances following the deep-focus earthquake (Mw 6.6) in Tarauacá, Acre, Brazil: Ground uplift and TEC analysis | |
| Ramdhan et al. | Earthquake location determination using data from DOMERAPI and BMKG seismic networks: a preliminary result of DOMERAPI project |
Legal Events
| Date | Code | Title | Description |
|---|---|---|---|
| S533 | Written request for registration of change of name |
Free format text: JAPANESE INTERMEDIATE CODE: R313533 |
|
| R350 | Written notification of registration of transfer |
Free format text: JAPANESE INTERMEDIATE CODE: R350 |
|
| S533 | Written request for registration of change of name |
Free format text: JAPANESE INTERMEDIATE CODE: R313533 |
|
| R350 | Written notification of registration of transfer |
Free format text: JAPANESE INTERMEDIATE CODE: R350 |
|
| EXPY | Cancellation because of completion of term |