JPH03289587A - Apparatus and method for investigating position of boundary surface of horizontal strata of soil - Google Patents

Apparatus and method for investigating position of boundary surface of horizontal strata of soil

Info

Publication number
JPH03289587A
JPH03289587A JP2091434A JP9143490A JPH03289587A JP H03289587 A JPH03289587 A JP H03289587A JP 2091434 A JP2091434 A JP 2091434A JP 9143490 A JP9143490 A JP 9143490A JP H03289587 A JPH03289587 A JP H03289587A
Authority
JP
Japan
Prior art keywords
soil
boundary surface
horizontal
points
point
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.)
Pending
Application number
JP2091434A
Other languages
Japanese (ja)
Inventor
Sadao Kono
河野 貞男
Yasuhiro Yuya
康弘 油谷
Takashi Yoshinaga
吉永 敬
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Nippon Telegraph and Telephone Corp
Original Assignee
Nippon Telegraph and Telephone Corp
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Nippon Telegraph and Telephone Corp filed Critical Nippon Telegraph and Telephone Corp
Priority to JP2091434A priority Critical patent/JPH03289587A/en
Publication of JPH03289587A publication Critical patent/JPH03289587A/en
Pending legal-status Critical Current

Links

Abstract

PURPOSE:To easily and accurately estimate the position of the boundary surfaces of horizontal strata of soil by extracting a curve high in correlation as the reflected wave from the boundary surfaces of horizontal strata of soil and extracting the calculated change point of a section dielectric constant. CONSTITUTION:A pulse wave having wide-band frequency is generated from a pulse generator 1 to be transmitted to a transmission antenna 2. The electromagnetic wave sent out as a result is reflected from the boundary surfaces BD1, BD2 of horizontal strata of soil and the other unnecessary reflecting body NN. The reflected waves are received by a receiving antenna 3 while the receiving antenna 3 is allowed to run and the interval between the transmission antenna 2 and the receiving antenna 3 is changed by a definite distance. Next, the received reflected waves are sampled and only inflection points are extracted by an extraction circuit 4. The extracted inflection points are constituted as a plurality of point groups by an operation part 5 and the change point of a section dielectric constant is determined as the boundary surfaces of the horizontal strata of soil to be displayed on a dummy cross section display part 6.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は、電磁波を用いて土の水平地層境界面位置を推
定する探査方法および装置に関するものである。
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to an exploration method and apparatus for estimating the position of a horizontal stratum boundary surface of soil using electromagnetic waves.

〔従来の技術〕[Conventional technology]

従来から、電磁波を用いて土の水平地層境界面位置を推
定する方法が2つ提案されている。この方法の手順を次
の(i)  と(ii)に示す。
Conventionally, two methods have been proposed for estimating the position of the horizontal stratum boundary surface of soil using electromagnetic waves. The steps of this method are shown in (i) and (ii) below.

(i)送受一体アンテナによる測定法 ■試験掘りを実施し、試験掘り位置の土の水平地層境界
面位置を実測する。
(i) Measurement method using an integrated transmitting and receiving antenna ∎ Carry out test digging and actually measure the position of the horizontal stratum boundary surface of the soil at the test digging location.

■送受一体アンテナを試験掘り近傍から走行させる。■The integrated transmitting and receiving antenna will be run from near the test excavation.

■送受一体アンテナの送信部から電磁波を送出し、受信
部においてその電磁波の反射波を順次一定走行距離毎に
受信し、その伝播時間を測定する。
(2) An electromagnetic wave is sent out from the transmitter of the integrated transmitter/receiver antenna, and the receiver receives the reflected waves of the electromagnetic wave at regular intervals of travel distance, and measures the propagation time.

■試験掘り結果と試験掘り近傍の送受一体アンテナによ
る電磁波の伝播時間がら各層の誘電率を決定する。
■Determine the permittivity of each layer based on the test excavation results and the propagation time of electromagnetic waves from the integrated transmitting and receiving antenna near the test excavation.

■■で推定した誘電率を試験掘り近傍以外の探査位置に
も適用し、地層境界面の上被りに変換し、土の水平地層
境界面位置を推定する。
Apply the dielectric constant estimated in ■■ to exploration locations other than the vicinity of the test excavation, convert it to the overlay of the strata boundary surface, and estimate the horizontal stratum boundary surface position of the soil.

(ff)送受分離アンテナによる測定法■送受分離アン
テナのどちらか一方を固定し、もう一方を走行させる。
(ff) Measurement method using separate transmitting/receiving antenna ■ Fix one of the separate transmitting/receiving antennas and run the other.

■送信アンテナから電磁波を送出し、その電磁波の反射
波を受信する受信アンテナと送信アンテナとを一定距離
間隔で離し、送受アンテナ間隔を変化させながら受信し
、上記電磁波の反射波伝播時間を測定する。
■ Send electromagnetic waves from a transmitting antenna and receive the reflected waves of the electromagnetic waves.The receiving antenna and the transmitting antenna are separated by a certain distance, and the receiving antenna is received while changing the spacing between the transmitting and receiving antennas, and the reflected wave propagation time of the electromagnetic waves is measured. .

■測定した反射波波形の振幅値の大となる連続的な波形
の流れを地中の反射物体からの反射と仮定する。
■Measured reflected waves Assume that a continuous flow of waveforms with large amplitude values is reflection from a reflective object underground.

■仮定した振幅値の大となる複数の連続的な波形の流れ
の中から、土の水平地層境界面と仮定した時の曲線に一
致する連続的な波形の流れを選択する。
■Select a continuous waveform flow that matches the curve assumed to be the horizontal strata boundary surface of the soil from among multiple continuous waveform flows with assumed large amplitude values.

■上記で選択された曲線の曲率から、土の水平地層境界
面位置の土被りを算出し、推定する。
■Calculate and estimate the soil cover at the horizontal stratum boundary surface position from the curvature of the curve selected above.

〔発明が解決しようとする課題〕[Problem to be solved by the invention]

しかし、(i)の送受一体アンテナによる測定法は、試
験掘り等なんらかの掘削工事が必要であり、効率的でな
いと言う点に問題があった。
However, the measurement method (i) using an integrated transmitting and receiving antenna has a problem in that it requires some kind of excavation work such as test digging, and is not efficient.

また、(ii)の送受分離アンテナによる測定法は、掘
削工事を必要としないが、振幅値の強く現れる反射波以
外の境界面の抽出が難しいこと、不要反射波の混入のた
め土の水平地層境界面と仮定した時の曲線に一致する連
続的な波形の流れを選択させることが難しいこと、また
選択可能な場合でも複数のポイント群から決定した曲線
の重みがばらつき、すべての曲線を同様に土の水平地層
境界面であると考え、曲率から土被りを比較することに
無理があること等のため精度の点で問題であった。
In addition, measurement method (ii) using separate transmitting and receiving antennas does not require excavation work, but it is difficult to extract boundary surfaces other than reflected waves that appear with strong amplitude values, and because unnecessary reflected waves are mixed in, horizontal strata of the soil It is difficult to select a continuous waveform flow that matches the curve when it is assumed to be a boundary surface, and even if it is possible to select it, the weight of the curve determined from multiple point groups varies, making it difficult to select all curves in the same way. There was a problem with accuracy because it was impossible to compare soil cover based on curvature, considering that it was a horizontal stratum boundary surface of soil.

本発明はこのような点に鑑みてなされたものであり、そ
の目的とするところは、容易に高精度で土の水平地層境
界面位置を推定し得る方法および装置を提供することに
ある。
The present invention has been made in view of these points, and an object of the present invention is to provide a method and apparatus that can easily and accurately estimate the position of a horizontal stratum boundary surface of soil.

〔課題を解決するだめの手段〕[Failure to solve the problem]

このような目的を達成するために本発明による土の水平
地層境界面位置の探査装置は、互いに分離した送信部と
受信部とを備え、送信部に、広帯域な周波数を持つパル
ス発生器と、このパルス発生器からの信号を電磁波とし
て地表面に送出する送信アンテナとを備え、受信部に、
一定間隔で送信アンテナとの距離を変化させ、送信アン
テナから送出された電磁波の反射波を捕らえる受信アン
テナと、受信アンテナで捕らえられた反射波をサンプリ
ングし、その電磁波のゼロクロス点または変曲点を抽出
する抽出回路と、この抽出回路で抽出したゼロクロス点
または変曲点を連続性を持った複数のポイント群として
構成させ、構成させた各ポイント群を土の水平地層境界
面からの反射波の場合に生ずる曲線と対比し、相関の高
いポイント群を土の水平地層境界面反射波とし、相関の
高い曲線間の区間誘電率、土被りを算出する演算部と、
演算した区間誘電率の変化点を実際の土の水平地層境界
面と決定して土被りを表示させる疑似断面表示部とを備
えるようにしたものである。
In order to achieve such an object, the present invention provides an apparatus for detecting the position of horizontal stratum boundary surfaces in soil, which includes a transmitting section and a receiving section that are separated from each other, and the transmitting section includes a pulse generator having a wide frequency band; It is equipped with a transmitting antenna that sends the signal from this pulse generator to the earth's surface as an electromagnetic wave, and the receiving section has a
The receiving antenna changes the distance from the transmitting antenna at regular intervals and captures the reflected waves of the electromagnetic waves sent out from the transmitting antenna, and the reflected waves captured by the receiving antenna are sampled to find the zero-crossing point or inflection point of the electromagnetic waves. The extraction circuit to be extracted and the zero-crossing points or inflection points extracted by this extraction circuit are configured as a plurality of continuous point groups, and each configured point group is a calculation unit that calculates the interval permittivity and soil cover between the curves with high correlation by comparing the curves that occur in the case, using a group of points with high correlation as reflected waves from the horizontal strata boundary surface of the soil;
The present invention includes a pseudo cross-section display section that determines the change point of the calculated section permittivity as the actual horizontal strata boundary surface of the soil and displays the soil cover.

また、本発明による土の水平地層境界面位置の探査方法
は、送信アンテナから広帯域な周波数を持つ電磁波を地
中に送出し、受信アンテナを一定間隔で送信アンテナか
ら遠ざけ、送信アンテナと受信アンテナの間隔を変化さ
せながら反射波を受信し、受信された反射波のゼロクロ
ス点または変曲点を抽出し、抽出したゼロクロス点また
は変曲点を連続性を持った複数のポイント群として構成
させ、構成させた各ポイント群を土の水平地層境界面か
らの反射波の場合に生ずる曲線と対比し、相関の高いポ
イント群を土の水平地層境界面からの反射波とし、相関
の高い曲線間の区間誘電率、土被りを算出し、算出した
区間誘電率の変化点を実際の土の水平地層境界面と決定
して土被りを表示させるようにしたものである。
In addition, the method for detecting the position of horizontal stratum boundary surfaces in soil according to the present invention involves transmitting electromagnetic waves with a wide band frequency into the ground from a transmitting antenna, moving the receiving antenna away from the transmitting antenna at regular intervals, and connecting the transmitting antenna and the receiving antenna. Receive reflected waves while changing the interval, extract zero-crossing points or inflection points of the received reflected waves, and configure the extracted zero-crossing points or inflection points as a group of multiple points with continuity. Each point group is compared with the curve that would occur in the case of a reflected wave from the horizontal stratum boundary surface of the soil, and the point group with a high correlation is regarded as the reflected wave from the horizontal stratum boundary surface of the soil, and the section between the curves with a high correlation is The permittivity and soil cover are calculated, and the change point of the calculated section permittivity is determined to be the horizontal stratum boundary surface of the actual soil, and the soil cover is displayed.

〔作用〕[Effect]

本発明は、送信アンテナと受信アンテナとの間隔を変化
させて探査する方法において、測定した波形のうちゼロ
クロス点または変曲点のみを抽出し、抽出したゼロクロ
ス点または変曲点を連続性を持った複数のポイント群と
して構成させ、構成させた各ポイント群を土の水平地層
境界面からの反射波の場合に生ずる曲線に比して相関の
高いポイント群を土の水平地層境界面からの反射波とし
て分離し、相関の高い曲線間の区間誘電率、土被りを算
出し、算出した区間誘電率の変化点を実際の土の水平地
層境界面と決定して土被りを表示させる。これにより、
土の水平地層境界面の振幅値が小さくても、また不要反
射波の混入があり、土の水平地層境界面からの反射波の
場合に生ずる曲線の当てはめが難しくても、当てはめた
曲線の相関係数を比較することにより、曲線の重みを判
断することができ、容易に高精度で土の水平地層境界面
位置を推定することができる。
The present invention extracts only zero-crossing points or inflection points from a measured waveform in a method of searching by changing the distance between a transmitting antenna and a receiving antenna, and makes the extracted zero-crossing points or inflection points continuous. Each point group is configured as a plurality of point groups, and a group of points with a higher correlation is compared to a curve generated in the case of reflected waves from the horizontal stratum boundary surface of the soil. Separate the curves as waves, calculate the interval permittivity and soil cover between the highly correlated curves, determine the change point of the calculated interval permittivity as the actual horizontal stratum boundary surface of the soil, and display the earth cover. This results in
Even if the amplitude value of the horizontal stratum boundary surface of the soil is small, or even if unnecessary reflected waves are mixed in and it is difficult to fit the curve that occurs in the case of reflected waves from the horizontal stratum boundary surface of the soil, the phase of the fitted curve is By comparing the relationship coefficients, the weight of the curve can be determined, and the position of the horizontal stratum boundary surface of the soil can be easily estimated with high accuracy.

〔実施例〕〔Example〕

次に、本発明の実施例について説明する。なお実施例は
一つの例示であって、本発明の範囲を逸脱しない範囲で
、種々の変更あるいは改良を行ない得ることはいうまで
もない。
Next, examples of the present invention will be described. Note that the embodiments are merely illustrative, and it goes without saying that various changes and improvements can be made without departing from the scope of the present invention.

第1図は、本発明による土の水平地層境界面位置の探査
装置の一実施例を示すブロック系統図である。同図にお
いて、(a)は発信部、(b)は受信部を示す。
FIG. 1 is a block system diagram showing an embodiment of an apparatus for detecting the horizontal stratum boundary position of soil according to the present invention. In the figure, (a) shows a transmitting section, and (b) shows a receiving section.

第1図(a)の発信部において、1は広帯域な周波数を
持つパルス発生器、2はパルス発生器1のパルスを電磁
波として地中に向けて発信する送信アンテナである。
In the transmitting section shown in FIG. 1(a), 1 is a pulse generator having a wide frequency band, and 2 is a transmitting antenna that transmits the pulses of the pulse generator 1 as electromagnetic waves into the ground.

第1図(b)の受信部において、3は土の水平地層境界
面および他の反射物体から反射される電磁波を受信する
ための受信アンテナ、4は受信アンテナ3で受信した電
磁波をサンプリングし、サンプリングした電磁波のゼロ
クロス点または変曲点を抽出する抽出回路、5は演算部
である。演算部5は、抽出回路4から抽出したゼロクロ
ス点または変曲点を連続性を持った複数のポイント群と
して構成させ、構成させた各ポイント群を土の水平地層
境界面からの反射波の場合に生ずる曲線と対比し、相関
の高いポイント群を土の水平地層境界面からの反射波と
し、相関の高い曲線間の区間誘電率、土被りを算出する
。また、6は演算部5で演算した区間誘電率の変化点を
実際の土の水平地層境界面位置と決定して土被りを表示
させる疑似断面表示部である。
In the receiving section of FIG. 1(b), 3 is a receiving antenna for receiving electromagnetic waves reflected from the horizontal stratum boundary surface of soil and other reflective objects, 4 is a receiving antenna for sampling the electromagnetic waves received by the receiving antenna 3, An extraction circuit extracts a zero-crossing point or an inflection point of a sampled electromagnetic wave, and 5 is an arithmetic unit. The calculation unit 5 configures the zero-crossing points or inflection points extracted from the extraction circuit 4 as a plurality of continuous point groups, and calculates the case where each of the configured point groups is a reflected wave from a horizontal stratum boundary surface of soil. The point group with high correlation is regarded as the reflected wave from the horizontal stratum boundary surface of the soil, and the interval permittivity and soil cover between the curves with high correlation are calculated. Reference numeral 6 denotes a pseudo cross-section display section that determines the point of change in the section permittivity calculated by the calculation section 5 as the position of the actual horizontal strata boundary surface of the soil and displays the soil cover.

次に、第1図の装置を用いた土の水平地層境界面位置測
定方法を、第2図の実際の土層で行なった結果を示す第
3図〜第9図を用いて説明する。
Next, a method for measuring the horizontal stratum boundary surface position of soil using the apparatus shown in FIG. 1 will be explained with reference to FIGS. 3 to 9, which show the results obtained using the actual soil layer shown in FIG. 2.

なお、第2図において、SUFは地表面、LAI。In Figure 2, SUF is the ground surface and LAI.

LA2は例えば山砂、関東ロームの地層、BDIBD2
は水平地層境界面、NNは不要反射物である。
LA2 is for example mountain sand, Kanto loam stratum, BDIBD2
is a horizontal strata boundary surface, and NN is an unnecessary reflective object.

i)第2図のパルス発生器1から広帯域な周波数を持つ
パルス波を発生させ、同図の送信アンテナ2から送信す
る。
i) A pulse wave having a wide band frequency is generated from the pulse generator 1 shown in FIG. 2, and transmitted from the transmitting antenna 2 shown in the same figure.

ii )その結果、送出された電磁波は第2図の土の水
平地層境界面BDI、BD2および他の不要反射物NN
により反射する。
ii) As a result, the emitted electromagnetic waves are transmitted to the horizontal strata boundary surfaces BDI, BD2 and other unnecessary reflectors NN of the soil shown in Figure 2.
reflected by.

iii )その反射波を、第2図の受信アンテナ3を走
行させ、同図の送信アンテナ2との送受アンテナ間隔を
一定距離ずつ変化させながら、同図の受信アンテナ3で
受信する。
iii) The reflected wave is received by the receiving antenna 3 shown in FIG. 2 while the receiving antenna 3 shown in FIG.

iv)次に、第2図の抽出回路4で、受信した反射波を
電磁波伝播時間と送受アンテナ間隔の座標軸に第3図の
ようにサンプリングし、変曲点のみを第4図のように抽
出する。
iv) Next, in the extraction circuit 4 shown in Fig. 2, the received reflected waves are sampled on the coordinate axes of the electromagnetic wave propagation time and the transmitting/receiving antenna interval as shown in Fig. 3, and only the inflection points are extracted as shown in Fig. 4. do.

第3図の■〜■は、縦軸に電磁波の反射伝播時間、横軸
に電磁波の振幅強度をとり、送受アンテナ間隔をOmか
ら一定間隔毎に広げた時のそれぞれの反射波形を表示さ
せたものである。
■ to ■ in Figure 3 show the reflection propagation time of electromagnetic waves on the vertical axis and the amplitude intensity of electromagnetic waves on the horizontal axis, and display the respective reflected waveforms when the transmitting/receiving antenna interval is widened at regular intervals from Om. It is something.

第4図の○印は第3図における振幅強度がプラス方向か
らマイナス方向あるいはマイナス方向からプラス方向へ
推移する変曲点を表示させたものである。
The circles in FIG. 4 indicate inflection points where the amplitude intensity in FIG. 3 changes from a positive direction to a negative direction or from a negative direction to a positive direction.

■)第2図の演算部5で、iv)で抽出した変曲点を連
続性を持った複数のポイント群として構成させ、構成さ
せた各ポイント群を土の水平地層境界面からの反射波の
場合に生ずる曲線と対比し、相関の高いポイント群を土
の水平地層境界面波とし、相関の高い曲線間の区間誘電
率、土被りを算出する。
■) The calculation unit 5 in Fig. 2 configures the inflection points extracted in iv) as a plurality of continuous point groups, and each configured point group is used as a reflection wave from the horizontal stratum boundary surface of the soil. In comparison with the curves that occur in the case of , the point group with high correlation is treated as the horizontal strata interface wave of the soil, and the interval permittivity and soil cover between the curves with high correlation are calculated.

以下に、第2図の演算部5において行なう処理例の一つ
を示す。
An example of processing performed in the calculation unit 5 in FIG. 2 will be shown below.

(a)第2図の抽出回路4で、第4図のように抽出され
た変曲点を電磁波伝播時間と送受アンテナ間隔の座標軸
にそれぞれ二乗して第5図のように表示させる。第5図
の○印は第4図における変曲点の電磁波伝播時間、送受
アンテナ間隔のそれぞれの二乗を第4図と同様の座標軸
に表示させたものである。
(a) In the extraction circuit 4 of FIG. 2, the inflection points extracted as shown in FIG. 4 are squared on the coordinate axes of the electromagnetic wave propagation time and the transmitting/receiving antenna interval, respectively, and displayed as shown in FIG. The circle mark in FIG. 5 indicates the electromagnetic wave propagation time at the inflection point in FIG. 4 and the square of the transmitting/receiving antenna interval, respectively, on the same coordinate axes as in FIG. 4.

(′b)第5図で表示させた変曲点のポイント群の中か
ら、第6図のように連続性を持っていると思われるポイ
ント群を■、■、〜、@と複数個推定し、直線上に近似
させるべく、始点と終点a、  b、〜、nをそれぞれ
のポイント群に与え、近似直線A、B、〜、Nを決定さ
せる。
('b) From among the point group of inflection points displayed in Fig. 5, multiple point groups that seem to have continuity as shown in Fig. 6 are estimated as ■, ■, ~, @. Then, in order to approximate on a straight line, a starting point and an ending point a, b, . . . , n are given to each point group, and approximate straight lines A, B, .

第6図の・は連続性を持っていると思われるポイント群
の一つ■であり、始点a=O・と終点a→・とを与え、
近似直線Aを決定させたところである。さらに、次に連
続性を持っていると思われるOのポイント群■を推定し
、始点a=+・と終点a=O・とを与え、近似直線Bを
決定させる。このように順次連続性を持っていると思わ
れるポイント群■、■、〜■から近似直線A、B、〜、
Nを決定させていく、なお、◎はポイント群■に対応す
る。
In Figure 6, . is one of the point groups that are considered to have continuity, and given the starting point a=O・ and the ending point a→・,
The approximate straight line A has just been determined. Furthermore, the next point group (2) of O, which is thought to have continuity, is estimated, a starting point a=+. and an ending point a=O. are given, and an approximate straight line B is determined. Approximate straight lines A, B, ~, from the point group ■, ■, ~■, which seem to have sequential continuity in this way.
N is determined, and ◎ corresponds to point group ■.

(C) (b)で決定した近似直線A、B、〜、Nに第
7図のように電磁波伝播時間軸において一致あるいは最
短のポイント群■′、■′、〜、■′を決定させ、さら
に決定したそれぞれのポイント群■′、■′、〜、■′
に対して、すべての反射波を土の水平地層境界面からの
反射波と仮定した直iA’、B’、〜、N′を最小二乗
法により当てはめ表示させる。
(C) Let the approximate straight lines A, B, ~, N determined in (b) determine the matching or shortest point group ■', ■', ~, ■' on the electromagnetic wave propagation time axis as shown in Figure 7, Furthermore, each determined point group ■′, ■′, ~, ■′
, the lines iA', B', .

第7図の・は第6図の近似直liAに電磁波伝播時間軸
において一致あるいは最短のポイント群■′であり、こ
のポイント群■′から最小二乗法により土の水平地層境
界面からの反射波と仮定した直線A′を決定させる。さ
らに、次の(のポイント群■′からも最小二乗法により
土の水平地層境界面からの反射波と仮定した直線B′を
決定させる。このように順次ポイント群■′、■′、〜
、■′から直線A’、B’、〜、N′を決定していく。
7 in Fig. 7 is the point group ■' that coincides with or is the shortest point group on the electromagnetic wave propagation time axis with the approximate straight line liA in Fig. 6, and from this point group ■', the reflected wave from the horizontal stratum boundary surface of the soil is calculated by the least squares method. A straight line A' is determined based on the assumption that Furthermore, the straight line B', which is assumed to be a reflected wave from the horizontal strata boundary surface of the soil, is determined by the least squares method from the following point group ■'.In this way, the point group ■', ■', ~
, ■', straight lines A', B', . . . , N' are determined.

なお、◎はポイント@′に対応する。Note that ◎ corresponds to point @'.

(d)直線A’、B’、〜、N′とポイント群■′■′
、〜、○′とのそれぞれの相関関係を算出し、相関の高
いもののみの直線の勾配と縦軸切片から直線間の区間誘
電率、土被りを第8図のように算出する。
(d) Straight lines A', B', ~, N' and point group ■'■'
, ~, and ○', and calculate the interval permittivity and earth cover between the straight lines from the slope and vertical axis intercept of only those lines with high correlation, as shown in FIG.

第8図の実線で結ぶ○はポイント群■′■′、〜、■′
の相関係数、太線で結ぶ○は相関係数の高いもののみの
区間誘電率、実線で結ふ・は同相関係数の高いもののみ
の土被りである。
○ connected by solid lines in Figure 8 is a point group ■′■′, ~, ■′
Correlation coefficients of , ○ connected by thick lines indicate interval permittivity of only those with high correlation coefficients, and ○ connected by solid lines indicate overburden of only those with high correlation coefficients.

vi)v)で算出した区間誘電率の変化点を土の水平地
層境界面と決定し、第2図の疑似断面表示部6において
第9図のように表示させる。
vi) The point of change in the section permittivity calculated in v) is determined to be the horizontal strata boundary surface of the soil, and is displayed as shown in FIG. 9 on the pseudo section display section 6 of FIG. 2.

以上の動作説明は変曲点のみについて述べたが、ゼロク
ロス点についても同様な装置、同様な動作で変曲点の場
合と同様の効果を奏することができる。
Although the above description of the operation has been made only for the inflection point, the same effects as those for the inflection point can be achieved with the same device and the same operation for the zero cross point.

第10図は上述の測定方法の手順を示すフローチャート
である。同図において、まず送信アンテナ2(第1図参
照)から電磁波を発信しくステップ11)、受信アンテ
ナ3で反射波を受信しくステップ12)、受信した反射
波をサンプリングする(ステップ13)。次に、ゼロク
ロス点または変曲点を抽出しくステップ14)、ゼロク
ロス点、変曲点の複数の連続したポイント群を抽出しく
ステップ15)、複数の連続したポイント群に対する水
平地層境界面と仮定した曲線の当てはめを行ないくステ
ップ16)、各相関係数を算出しくステップ17)、相
関係数の一定値以上の仮定曲線を抽出しくステップ18
)、抽出した仮定曲線間の区間誘電率、土被りを算出し
くステップ19)、区間誘電率の変化点を水平地層境界
面と決定しくステップ20)、水平地層境界面の疑似断
面を表示する(ステップ21)。
FIG. 10 is a flowchart showing the procedure of the above-mentioned measuring method. In the figure, first, an electromagnetic wave is transmitted from the transmitting antenna 2 (see FIG. 1) (step 11), a reflected wave is received by the receiving antenna 3 (step 12), and the received reflected wave is sampled (step 13). Next, step 14) to extract zero-crossing points or inflection points, and step 15) to extract multiple consecutive point groups of zero-crossing points and inflection points. Step 16) to fit the curves, step 17) to calculate each correlation coefficient, and step 18 to extract hypothetical curves whose correlation coefficients are above a certain value.
), Calculate the interval permittivity and soil cover between the extracted hypothetical curves (Step 19), Determine the change point of the interval permittivity as the horizontal strata boundary (Step 20), Display the pseudo cross section of the horizontal strata boundary ( Step 21).

この方法を用いると、どのような掘削工事も伴わずに土
の水平地層境界面が推定でき、連続的な波形のゼロクロ
ス点または変曲点のみを抽出することにより、振幅値が
小さい土の水平地層境界面でも捕らえることができ、ま
た不要反射波の混入のため土の水平地層境界面からの反
射波の場合に生ずる曲線に一致するものの選択が難解で
も、構成させた複数のポイント群を土の水平地層境界面
からの反射波の場合に生ずる曲線と対比し、相関係数を
比較することによりポイント群の重みが比較でき、相関
の高い曲線を土の水平地層境界面からの反射波として抽
出し、相関の高い曲線間の区間誘電率、土被りを算出し
、算出した区間誘電率の変化点を抽出することにより容
易に精度よく土の水平地層境界面位置を推定することが
できる。
Using this method, the horizontal stratum boundary surface of soil can be estimated without any excavation work, and by extracting only the zero-crossing points or inflection points of continuous waveforms, horizontal strata of soil with small amplitude values can be estimated. It can also be captured at a stratum boundary surface, and even if it is difficult to select a curve that matches the curve that would occur in the case of a reflected wave from a horizontal stratum boundary surface due to the inclusion of unnecessary reflected waves, it is possible to capture the The weight of the point group can be compared by comparing the correlation coefficient with the curve that occurs when the wave is reflected from the horizontal stratum boundary surface of the soil. By extracting, calculating the interval permittivity and soil cover between curves with high correlation, and extracting the points of change in the calculated interval permittivity, it is possible to easily and accurately estimate the position of the horizontal stratum boundary surface of the soil.

〔発明の効果〕〔Effect of the invention〕

以上説明したように本発明は、送信アンテナから広帯域
な周波数を持つ電磁波を地中に送出し、受信アンテナを
一定間隔で送信アンテナから遠ざけ、送信アンテナと受
信アンテナの間隔を変化させながら反射波を受信し、受
信された反射波のゼロクロス点または変曲点を抽出し、
抽出したゼロクロス点または変曲点を連続性を持った複
数のポイント群として構成させ、構成させた各ポイント
群を土の水平地層境界面からの反射波の場合に生ずる曲
線と対比し、相関の高いポイント群を土の水平地層境界
面からの反射波とし、相関の高い曲線間の区間誘電率、
土被りを算出し、算出した区間誘電率の変化点を実際の
土の水平地層境界面と決定して土被りを表示させること
により、どのような掘削工事も伴わずに土の水平地層境
界面位置が推定でき、連続的な波形のゼロクロス点また
は変曲点のみを抽出することにより、振幅値が小さい土
の水平地層境界面波でも捕らえることができる効果があ
る。
As explained above, the present invention sends electromagnetic waves with a wide band frequency from the transmitting antenna underground, moves the receiving antenna away from the transmitting antenna at regular intervals, and collects reflected waves while changing the distance between the transmitting antenna and the receiving antenna. Receive and extract the zero crossing point or inflection point of the received reflected wave,
The extracted zero-crossing points or inflection points are configured as a plurality of continuous point groups, and each configured point group is compared with a curve that occurs in the case of a reflected wave from the horizontal strata boundary surface of soil, and the correlation is calculated. The high point group is the reflected wave from the horizontal stratum boundary surface of the soil, and the interval permittivity between the curves with high correlation,
By calculating the soil cover and determining the change point of the calculated interval permittivity as the actual horizontal stratum boundary surface of the soil and displaying the soil cover, the horizontal stratum boundary surface of the soil can be determined without any excavation work. By estimating the position and extracting only the zero-crossing points or inflection points of a continuous waveform, it is possible to capture even horizontal strata boundary waves of soil with small amplitude values.

また不要反射波の混入のため土の水平地層境界面からの
反射波の場合に生ずる曲線に一致するものの選択が難解
でも、−律に、構成させた複数のポイント群を土の水平
地層境界面からの反射波の場合に生ずる曲線と対比し、
相関係数を比較することによりポイント群の重みが比較
でき、相関の高い曲線を土の水平地層境界面からの反射
波として抽出し、相関の高い曲線間の区間誘電率、土被
りを算出し、算出した区間誘電率の変化点を抽出するこ
とにより容易に精度よく土の水平地層境界面位置を推定
することができる。
In addition, even if it is difficult to select a curve that matches the curve that occurs in the case of reflected waves from the horizontal stratum boundary surface of soil due to the inclusion of unnecessary reflected waves, it is possible to In contrast to the curve that occurs in the case of reflected waves from
By comparing the correlation coefficients, the weights of point groups can be compared, and curves with high correlation are extracted as reflected waves from the horizontal stratum boundary surface of the soil, and the interval permittivity and soil cover between the curves with high correlation are calculated. By extracting the points of change in the calculated interval permittivity, it is possible to easily and accurately estimate the position of the horizontal strata boundary surface of the soil.

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

第1図は本発明による土の水平地層境界面位置の探索装
置の一実施例を示すブロック系統図、第2図は本発明に
よる探索方法の一実施例を説明し、実際に探査した土層
を示すための説明図、第3図は観測信号のサンプリング
波を示すグラフ、第4図はサンプリング波からの変曲点
抽出状況を示すグラフ、第5図は変曲点を電磁波伝播時
間と送受アンテナ間隔の座標軸にそれぞれ二乗したもの
を表示させたグラフ、第6図は始点と終点とを指定する
ことにより変曲点の連続性を持った複数のポイント群に
近似した直線を与えた状況を示すグラフ、第7図は第6
図で与えた直線に一致あるいは縦軸において最短のポイ
ント群を選択し、すべて地中の水平地層境界面と仮定し
た直線を最上二乗法により当てはめた状況を示すグラフ
、第8図は第7図で当てはめた直線群の相関係数を計算
し、相関係数の高い物の区間誘電率、土被りを算出した
結果を示すグラフ、第9図は第8図で算出した区間誘電
率の変化点を土の水平地層境界面位置とし、アンテナ走
行区間における疑似断面表示をさせた表示図、第10図
は本発明による土の水平地層境界面位置の探索方法の一
実施例を説明するためのフローチャートである。 1・・・パルス発生器、2・・・送信アンテナ、3・・
・受信アンテナ、4・・・抽出回路、5・・・演算部、
6・・・疑似断面表示部、SUF・・・地表面、LAl
、LA2・・・地層、BDl、BD2・・・水平地層境
界面、NN・・・不要反射物。
Fig. 1 is a block system diagram showing an embodiment of an apparatus for searching for the horizontal stratum boundary position of soil according to the present invention, and Fig. 2 shows an embodiment of the search method according to the present invention, and shows the soil layers actually explored. Fig. 3 is a graph showing the sampling wave of the observation signal, Fig. 4 is a graph showing the extraction of inflection points from the sampling wave, and Fig. 5 is a graph showing the inflection point with electromagnetic wave propagation time and transmission/reception. Figure 6 is a graph displaying the antenna spacing squared on the coordinate axes, and shows a situation where a straight line approximated to a group of points with continuity of inflection points is given by specifying the starting point and ending point. The graph shown in Fig. 7 is the 6th
A graph showing the situation in which a group of points that match the straight line given in the figure or are the shortest on the vertical axis are selected, and the straight line is fitted using the best squares method, assuming that all the points are horizontal strata boundary surfaces underground. Figure 8 is the same as Figure 7. A graph showing the results of calculating the correlation coefficient of the straight line group fitted by , and calculating the interval permittivity and soil cover of objects with high correlation coefficients. Figure 9 shows the change points of the interval permittivity calculated in Figure 8. 10 is a flowchart for explaining an embodiment of the method for searching for the horizontal stratum boundary position of soil according to the present invention. It is. 1...Pulse generator, 2...Transmission antenna, 3...
- Receiving antenna, 4... Extraction circuit, 5... Arithmetic unit,
6...Pseudo cross section display section, SUF...Ground surface, LAl
, LA2...Geological stratum, BDl, BD2...Horizontal stratum boundary surface, NN...Unnecessary reflective object.

Claims (2)

【特許請求の範囲】[Claims] (1)互いに分離した送信部と受信部とを備え、前記送
信部は、広帯域な周波数を持つパルス発生器と、このパ
ルス発生器からの信号を電磁波として地表面に送出する
送信アンテナとを備え、前記受信部は、一定間隔で前記
送信アンテナとの距離を変化させ、前記送信アンテナか
ら送出された電磁波の反射波を捕らえる受信アンテナと
、前記受信アンテナで捕らえられた反射波をサンプリン
グし、その電磁波のゼロクロス点または変曲点を抽出す
る抽出回路と、この抽出回路で抽出したゼロクロス点ま
たは変曲点を連続性を持った複数のポイント群として構
成させ、構成させた各ポイント群を土の水平地層境界面
からの反射波の場合に生ずる曲線と対比し、相関の高い
ポイント群を土の水平地層境界面反射波とし、相関の高
い曲線間の区間誘電率、土被りを算出する演算部と、演
算した区間誘電率の変化点を実際の土の水平地層境界面
と決定して土被りを表示させる疑似断面表示部とを備え
た土の水平地層境界面位置の探査装置。
(1) A transmitting section and a receiving section are provided which are separated from each other, and the transmitting section is provided with a pulse generator having a wide frequency band and a transmitting antenna that transmits a signal from the pulse generator to the ground surface as an electromagnetic wave. , the receiving section changes the distance from the transmitting antenna at regular intervals, and includes a receiving antenna that captures reflected waves of electromagnetic waves sent out from the transmitting antenna, and samples the reflected waves captured by the receiving antenna, and An extraction circuit extracts zero-crossing points or inflection points of electromagnetic waves, and the zero-crossing points or inflection points extracted by this extraction circuit are configured as a plurality of continuous point groups, and each configured point group is A calculation unit that compares the curves that occur in the case of reflected waves from horizontal stratum boundary surfaces, uses points with high correlation as reflected waves from horizontal stratum boundary surfaces of soil, and calculates the interval permittivity and earth cover between curves with high correlation. and a pseudo cross section display section that determines the point of change of the calculated interval permittivity as the actual horizontal stratum boundary surface of the soil and displays the soil cover.
(2)送信アンテナから広帯域な周波数を持つ電磁波を
地中に送出し、受信アンテナを一定間隔で前記送信アン
テナから遠ざけ、前記送信アンテナと受信アンテナの間
隔を変化させながら反射波を受信し、受信された反射波
のゼロクロス点または変曲点を抽出し、抽出したゼロク
ロス点または変曲点を連続性を持った複数のポイント群
として構成させ、構成させた各ポイント群を土の水平地
層境界面からの反射波の場合に生ずる曲線と対比し、相
関の高いポイント群を土の水平地層境界面からの反射波
とし、相関の高い曲線間の区間誘電率、土被りを算出し
、算出した区間誘電率の変化点を実際の土の水平地層境
界面と決定して土被りを表示させることを特徴とする土
の水平地層境界面位置の探査方法。
(2) Send electromagnetic waves with a wide band frequency underground from the transmitting antenna, move the receiving antenna away from the transmitting antenna at regular intervals, and receive the reflected waves while changing the distance between the transmitting antenna and the receiving antenna. The zero-crossing points or inflection points of the reflected waves are extracted, the extracted zero-crossing points or inflection points are configured as a plurality of points with continuity, and each configured point group is connected to the horizontal strata boundary surface of the soil. Contrast this with the curve that occurs when the reflected wave from A method for detecting the position of a horizontal stratum boundary surface of soil, characterized by determining a point of change in permittivity as the actual horizontal stratum boundary surface of soil and displaying the soil cover.
JP2091434A 1990-04-06 1990-04-06 Apparatus and method for investigating position of boundary surface of horizontal strata of soil Pending JPH03289587A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP2091434A JPH03289587A (en) 1990-04-06 1990-04-06 Apparatus and method for investigating position of boundary surface of horizontal strata of soil

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP2091434A JPH03289587A (en) 1990-04-06 1990-04-06 Apparatus and method for investigating position of boundary surface of horizontal strata of soil

Publications (1)

Publication Number Publication Date
JPH03289587A true JPH03289587A (en) 1991-12-19

Family

ID=14026261

Family Applications (1)

Application Number Title Priority Date Filing Date
JP2091434A Pending JPH03289587A (en) 1990-04-06 1990-04-06 Apparatus and method for investigating position of boundary surface of horizontal strata of soil

Country Status (1)

Country Link
JP (1) JPH03289587A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2002023226A1 (en) * 2000-09-18 2002-03-21 Cos Co., Ltd. Method of measuring in-medium dielectric constant in electromagnetic prober, and electromagnetic prober
EP1291669A1 (en) * 2001-09-05 2003-03-12 Österreichische Bundesbahnen Device and method for identifying inhomogeneities in at least one snow layer

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2002023226A1 (en) * 2000-09-18 2002-03-21 Cos Co., Ltd. Method of measuring in-medium dielectric constant in electromagnetic prober, and electromagnetic prober
AU2002238196B2 (en) * 2000-09-18 2005-09-01 Cos Co., Ltd. Method of measuring in-medium dielectric constant in electromagnetic prober, and electromagnetic prober
EP1291669A1 (en) * 2001-09-05 2003-03-12 Österreichische Bundesbahnen Device and method for identifying inhomogeneities in at least one snow layer

Similar Documents

Publication Publication Date Title
US7034740B2 (en) Method and apparatus for identifying buried objects using ground penetrating radar
McCarthy et al. Ground-penetrating radar measurements of debris thickness on Lirung Glacier, Nepal
US5673050A (en) Three-dimensional underground imaging radar system
US6866098B1 (en) Method for controlling a producing zone of a well in a geological formation
CN104020495B (en) Automatic underground pipeline parameter recognizing method on basis of ground penetrating radar
CN106022339B (en) A kind of extracting method of Reclaimed Land shallow embedding underground pipe depth
Arcone et al. Ground-penetrating radar profiles of the McMurdo Shear Zone, Antarctica, acquired with an unmanned rover: Interpretation of crevasses, fractures, and folds within firn and marine ice
US7791981B2 (en) Velocity analysis for VSP data
CN104267440A (en) Common middle point (CMP) detection method used for ground penetrating radar (GPR)
JP2003302465A (en) Underground radar exploration method, device and program of frequency variable system
CN114814961A (en) Ground penetrating radar data accurate positioning method for high-precision terrain correction
CN107656270A (en) The measurement apparatus and measuring method of a kind of contactless buried pipe track forces cun
JPH03289587A (en) Apparatus and method for investigating position of boundary surface of horizontal strata of soil
JP2528148B2 (en) Method and device for detecting underground buried objects
Sun et al. Research on detection and visualization of underground pipelines
Sun et al. Application of ground penetrating radar with GPS in underwater topographic survey
CN111691876A (en) Method and device for imaging adjacent well by using acoustic logging and storage medium
RU2054690C1 (en) One-point method of determination of position of electromagnetic radiation source
Luo et al. Hyperbolic feature detection and radius calculation of underground pipeline
CN111880223B (en) Attribute analysis method for well-side sound wave remote detection imaging fracture-cave carving
JP2994570B2 (en) Underground exploration radar
RU2664253C1 (en) Method for remote search of underground service lines and determination of their transverse dimension and depth of ground position
Henson Jr et al. Georadar investigation of karst in a limestone quarry near Anna, Illinois
JPH057671B2 (en)
Bakhtiari et al. Minor fault detection by integration of seismic attributes in an oil reservoir