JPS5999385A - Detection of matter embedded in ground - Google Patents

Detection of matter embedded in ground

Info

Publication number
JPS5999385A
JPS5999385A JP57210836A JP21083682A JPS5999385A JP S5999385 A JPS5999385 A JP S5999385A JP 57210836 A JP57210836 A JP 57210836A JP 21083682 A JP21083682 A JP 21083682A JP S5999385 A JPS5999385 A JP S5999385A
Authority
JP
Japan
Prior art keywords
ground
amplitude
embedded
wave
matters
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
JP57210836A
Other languages
Japanese (ja)
Inventor
Tetsuo Hatono
鳩野 哲男
Sumio Kobayashi
純夫 小林
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 Steel Corp
Original Assignee
Sumitomo Metal Industries Ltd
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 Sumitomo Metal Industries Ltd filed Critical Sumitomo Metal Industries Ltd
Priority to JP57210836A priority Critical patent/JPS5999385A/en
Publication of JPS5999385A publication Critical patent/JPS5999385A/en
Pending legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01VGEOPHYSICS; GRAVITATIONAL MEASUREMENTS; DETECTING MASSES OR OBJECTS; TAGS
    • G01V3/00Electric or magnetic prospecting or detecting; Measuring magnetic field characteristics of the earth, e.g. declination, deviation
    • G01V3/12Electric or magnetic prospecting or detecting; Measuring magnetic field characteristics of the earth, e.g. declination, deviation operating with electromagnetic waves

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  • Physics & Mathematics (AREA)
  • Engineering & Computer Science (AREA)
  • Remote Sensing (AREA)
  • Life Sciences & Earth Sciences (AREA)
  • Electromagnetism (AREA)
  • Environmental & Geological Engineering (AREA)
  • Geology (AREA)
  • General Life Sciences & Earth Sciences (AREA)
  • General Physics & Mathematics (AREA)
  • Geophysics (AREA)
  • Geophysics And Detection Of Objects (AREA)
  • Radar Systems Or Details Thereof (AREA)

Abstract

PURPOSE:To perform the detection of a plurality of embedded matters and the positional confirmation thereof, by a method wherein a radio wave to which frequency modulation is applied is projected into the ground and complex reflectivity is measured while high speed Fourier transformation is applied to determine the amplitude of the reflected wave from each matter embedded in the ground. CONSTITUTION:An oscillator 1 emits saw-tooth shaped FM wave showing frequency change in the band width of frequency fo-fo+B and an oscillation signal is projected toward the ground surface 7 from a transmission antenna 2 while branched to be applied to an amplitude phase measuring instrument 4. The receiving signal of a receiving antenna 3 for catching the reflected waves from the matters 8a, 8b embedded in the ground is also imparted to the amplitude phase measuring instrument 4. An operator 5 measures complex reflectivity GAMMA(f) while reading the amplitude and the phase measured by the measuring instrument 4 in a plurality of frequencies present in fo-fo+B and applies Fourier transformation to operate of the amplitude GAMMA(x) of reflected wave dependent on the distance (x) to each matter embedded in the ground. From the distance between peaks of amplitudes, the distances x1, x2 between the ground surface and the embedded matters 8a, 8b can be calculated.

Description

【発明の詳細な説明】 本発明は地中j!!設物の検知方法に崗し、更に詳述す
れば&数の埋設物が存在する場合にもこれらを分離職別
できるFMレーダ法を提案するものである。
[Detailed Description of the Invention] The present invention is based on underground j! ! This paper proposes an FM radar method that can separate and classify buried objects even when there are several buried objects.

ガス管等の各稙管体或は苓発爆弾等、地中埋設物f管設
諭”工事等のために検知する必要があることが多々ある
It is often necessary to detect underground objects such as gas pipes, explosives, etc. for construction work.

従来の検知方法としては特開昭56−140276号、
特開昭57−56769号に示された如く、地中埋設物
に電流を通じそれによって発生する電界を地上でコイル
によって検出し、その埋設位置の標定を行う方法が知ら
れているが、この方法は検知対象の存在自体が明らかで
あること、電流を通流できるものであること等の条件が
あって適用対象に限界があり、また複数の埋設物が存在
する場合にはそれらの分離識別が不可能である。
Conventional detection methods include JP-A-56-140276;
As shown in Japanese Unexamined Patent Publication No. 57-56769, there is a known method for locating the buried position by passing an electric current through an underground object and detecting the electric field generated by the electric field using a coil on the ground. However, there are limits to what can be applied due to conditions such as the existence of the object to be detected being obvious and the ability to conduct electric current, and when there are multiple buried objects, it is difficult to separate and identify them. It's impossible.

!た地表面上から電磁誘導の原理を利用して地中埋設物
を検知する方法も公知であるが、検知対象が導電性物で
ある必要があること、複数の埋設物の分離識別が不可能
であるという欠点がある。
! A method of detecting objects buried underground using the principle of electromagnetic induction from above the ground surface is also known, but the detection target must be a conductive object and it is impossible to separate and identify multiple buried objects. It has the disadvantage of being.

これに対して特公昭57−17273すF示された如<
 FMレーダの原理を用いる方法による場合は検知対象
物の制約は無いが、複数の同種(電波伝播定数が同じ)
埋設物が存在するときにこれらを分離識別するためには
特別の工大を必要とする。
In contrast, as shown in Tokuko Sho 57-17273
When using a method that uses the principle of FM radar, there are no restrictions on the objects to be detected, but multiple objects of the same type (with the same radio wave propagation constant)
Special engineering is required to separate and identify buried objects when they exist.

本発明はこのようなFMレーダ法において、複数の埋設
物の存否検知及び位置標定を分離して高精度で行うこと
ができる地中埋設物の検知方法全提供することを目的と
する。
It is an object of the present invention to provide an entire method for detecting underground objects in such an FM radar method, which is capable of separately detecting the presence or absence of a plurality of buried objects and locating their positions with high precision.

本発明に係る地中埋設物の検知方法は所定の帯V、幅で
の周波政変ρMを施した電波を地中へ向けて投射し、投
射波と地中からの反射波とにより、前記帯域幅内の多数
の周波数についての複素反射率を測定し、この測定値に
高速フーリエ変換を施して地中埋設物からの反射波の振
幅を定めることを特徴とする。
The method for detecting underground objects according to the present invention is to project a radio wave with a frequency change ρM in a predetermined band V and width into the ground, and to use the projected wave and the reflected wave from the underground to The method is characterized by measuring the complex reflectance for a large number of frequencies within a width, and applying fast Fourier transform to the measured values to determine the amplitude of the reflected wave from the underground object.

ます本発明の原理について説明する。First, the principle of the present invention will be explained.

地表面から深さXの位置にある物体に向けて周波数変調
(以下FM変調という)波を投射し、これから反射して
くる反射波の振幅を1′(X)とすると、周波数fでの
複素反射率r (f)は下記[l)式で表わすことがで
きる。
If a frequency modulated (hereinafter referred to as FM modulated) wave is projected toward an object at a depth The reflectance r (f) can be expressed by the following formula [l].

1− (f) oc f I’ (x) e−j 2π
fx dx  ’       −(Ijこれはフーリ
エ変換の形を示しているからフーリエ逆変換を用いて下
記(2)式を得ることができる。
1- (f) oc f I' (x) e-j 2π
fx dx' - (Ij Since this shows the form of Fourier transform, the following equation (2) can be obtained using inverse Fourier transform.

I−(x) cc J f’ (f) e+j2mf 
af         ・・・(2)この(2)式に注
目すれば、地表面からの深さに対する反射の大きさ、換
言すれば埋設物の存否、深さく位置)を検知するには、
多数の周波数につき複素反射率r(f)を測定し、それ
らに対し、て逆フーリエ変換を施せばよいことが解る。
I-(x) cc J f' (f) e+j2mf
af ... (2) If we pay attention to this equation (2), in order to detect the magnitude of reflection with respect to the depth from the ground surface, in other words, the presence or absence of buried objects, and the depth position),
It can be seen that it is sufficient to measure the complex reflectivity r(f) for a large number of frequencies and perform inverse Fourier transform on them.

なお複素反射率l”(f)は反射波の振幅及び位相を測
yvることによって求めることかできる。ただ地中埋設
物の検知は銘々害時間で行われることが望捷れるので、
演算にあたっては高速フーリエ変換を行うこととする。
The complex reflectance l''(f) can be obtained by measuring the amplitude and phase of the reflected wave. However, since it is desirable that underground objects be detected within a short period of time,
In the calculation, fast Fourier transform will be performed.

次に本発明方法を図面により具体的に説明する。Next, the method of the present invention will be specifically explained with reference to the drawings.

第1図は本発明方法の実施状恵を模式的に示している。FIG. 1 schematically shows the implementation of the method of the invention.

発振器1は第2図(イ)に示すように周期Tで周波#、
f、〜fo+Bの帯域幅の直線的な周波数便化を示す鋸
歯状のFM変調波を発振し、この発振佑彊°は送信用ア
ンテナ(空中線)2から地表7に向けて投射さね、ると
共にアンテナ2への伝送線路にて分岐して振幅・位相測
定器4へ与えられる。
The oscillator 1 generates frequencies #, with a period T, as shown in Fig. 2 (a).
It oscillates a sawtooth-shaped FM modulated wave that shows a linear frequency adjustment of the bandwidth of f, ~fo+B, and this oscillation wave is projected from the transmitting antenna (antenna) 2 toward the ground surface 7. At the same time, the signal is branched at the transmission line to the antenna 2 and given to the amplitude/phase measuring device 4 .

送信用アンテナ2の近傍には地中埋設物8a 、8bか
らの反射波を捉える受信用アンテナ3が設けられており
、この受信信号も振幅・位相測定器4へ与えられる。振
1¥!! ”位相測定器4は入力された送。
A receiving antenna 3 is provided near the transmitting antenna 2 to capture reflected waves from underground objects 8a and 8b, and this received signal is also given to the amplitude/phase measuring device 4. Furi 1 yen! ! ``The phase measuring device 4 receives the input signal.

受@信号から反射波の振幅及び位相を測定する。Measure the amplitude and phase of the reflected wave from the received signal.

演算器5けjilt定器4によって測定された振幅及び
位相をいずれもf。−f、+ B内にある多数の周波数
f+ 、 f2・・・ら−3.fn〔第2図(イ)参照
〕において読取り、各周波数における値を用いてフーリ
エ変換しアンテナ2から地中埋設物までの距離Xに 依
存する反射波の振幅’r (X)を演算するものである
The amplitude and phase measured by the 5-digit calculator 4 are both f. A large number of frequencies f+, f2... et al-3. fn [see Figure 2 (a)] and performs Fourier transform using the values at each frequency to calculate the amplitude 'r (X) of the reflected wave, which depends on the distance X from antenna 2 to the underground object. It is.

第2図(ロ)けl!11定器4にて測定された各周波数
fl+f2・・・fll−1nfnにおける相対振幅r
 (f)の変化を示したものであり、第2図を−)は同
じく相対位相θ(f)の変化を示しである。
Figure 2 (b) Kel! 11 Relative amplitude r at each frequency fl+f2...fll-1nfn measured by the regulator 4
(f) shows the change in relative phase θ(f), and -) in FIG.

いま送信波’(rAte”j2πft 9信波をAr 
e+j2m(t−τ(X))として表すこととする。但
し式効は深さXにある地中埋設物による時間遅れを示し
、τ(x) = 2x/Cで表わされる(C:地中での
電波伝播速度)。
Now the transmitted wave'(rAte"j2πft 9 signal wave is Ar
Let it be expressed as e+j2m(t-τ(X)). However, the formula effect indicates the time delay due to underground objects at depth X, and is expressed as τ(x) = 2x/C (C: radio wave propagation speed underground).

そうすると周波&fにおける複素反射率r (f)は下
記(3)式にて表わされる。 − L” (0(:CA t/A、 、 e−j 2πfx
−F(x) e−j2πfx −f’(x)e−jθ           ・・・(
3)従って地、中の8!設物が複数個である場合はm式
にて示したように r(f) ccfr (x) e−j 2πfxdxと
なり、これにフーリエ変換を伽、丁場合H+3+式より
r(X) QCJ I” (f) e+ j2mf d
(= 1” (f) e+2〕θ(f) df−= +
4+となる。
Then, the complex reflectance r (f) at the frequency &f is expressed by the following equation (3). −L” (0(:CA t/A, , e-j 2πfx
-F(x) e-j2πfx -f'(x)e-jθ ...(
3) Therefore, 8 in the earth! If there are multiple facilities, as shown in the formula m, it becomes r(f) ccfr (x) e−j 2πfxdx, and then Fourier transform is applied to this, and in the case of H+3+, r(X) QCJ I (f) e+ j2mf d
(= 1” (f) e+2]θ(f) df-= +
It becomes 4+.

つ捷り演′IJ−器5は多数の周波数f(f、、f2・
・・rfi、−1+fn)Kついての相対振IQF(f
)、相対位相θ(f) f用いて(4)式のl係に基き
フーリエ変換を行い部内(1,xからの反射波の振幅F
(x)を得るのである。
The switcher 5 has a large number of frequencies f(f, , f2・
Relative vibration IQF (f
), relative phase θ(f)F is used to perform Fourier transformation based on the l factor of equation (4), and the amplitude F of the reflected wave from the internal part (1,
(x) is obtained.

第3図は演算器5の演算出力を例示したものであって、
例えばペンレコーダ等の記録計6にて記録される。
FIG. 3 shows an example of the calculation output of the calculation unit 5,
For example, it is recorded by a recorder 6 such as a pen recorder.

第3図V(おいては3つのピーク値を認め得るが、X値
が最も小さいへの部分は地表面での反射、B。
In Figure 3 V (3 peak values can be recognized, but the part with the smallest X value is the reflection on the ground surface, B).

C(7) 6分ばAに近いBの方が地表に近い埋設物8
aでの反射、Cの方が地表に遠い埋設物8bでの反射に
基因するものである。従ってA、B、CのビークIIυ
距離よj)a表〜We物8 a 、 8 b Ill 
k t’& XI I X2を個々に求めることができ
る。以上のように不発tJ、、1方法による場合は棉電
、性物以外の物についてもイf、鶴1位tirf ? 
!’irガ]でき、し7かも複数存在してもそ11らを
犬々に分W〔検9七できることとなり、神々の’i”i
’体が錯綜埋設ζ力でいる部分においてもそれらの存在
1位1t1′分り−1(Hlに区別することがi]J能
に々る。
C (7) After 6 minutes, B is closer to A, and buried object 8 is closer to the ground surface.
Reflection at point a, and point C are due to reflection at buried object 8b, which is farther from the ground surface. Therefore, the beak IIυ of A, B, and C
Distance j) a table ~ We thing 8 a, 8 b Ill
k t'& XI I X2 can be determined individually. As mentioned above, if you use the 1st method, it's a cotton den, and if it's something other than sex, it's also tirf.
! 'irga], and even if there were more than one, it would be possible to divide them into dogs, and the gods''i'i
Even in the part where the ' body is a complex embedded ζ force, their existence is 1 t 1 ' min -1 (i] J ability to be distinguished into Hl.

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

第1図は本発明のヂ施状!島を示す模式図、第2し1(
イ)〜C′1は本発明方法の説明のための信号波形図、
第:3区IC測定h′□東を示すチャートである。 l・・・グCIL*器 2,3・・・アンテナ 4・・
・振幅・位相測定器 5・・演算器 6・・・記録器特
f1゛ 出 願 人  住友企糾工業株式会社代P1!
人 弁理士  河  野  登 大株  1 図 グ、  2 図 苑  3  図
Figure 1 shows the implementation of the present invention! Schematic diagram showing the island, No. 2 and 1 (
b) ~C'1 are signal waveform diagrams for explaining the method of the present invention,
No. 3: This is a chart showing the 3rd section IC measurement h'□East. l...G CIL* device 2, 3...Antenna 4...
・Amplitude/phase measuring instrument 5...Calculator 6...Recorder special f1 Applicant: Sumitomo Planning Industries Co., Ltd. P1!
Person Patent Attorney Noboru Kono Daikabu 1. Figure 2. 2. Zuen 3.

Claims (1)

【特許請求の範囲】[Claims] 1、所定の帯域幅での周波数変調を施した電波を地中へ
向けて投射し、投射波と地中からの反射波とにより、前
記帯域幅内の多数の周波数についての複素反射率全測定
し、この測定値に高速フーリエ変換を施して地中埋設物
からの反射波の振幅を定めることを特徴とする地中埋設
物検知方法。
1. Project a frequency-modulated radio wave into the ground with a predetermined bandwidth, and measure all complex reflectances for a large number of frequencies within the bandwidth using the projected wave and the reflected wave from the ground. An underground object detection method characterized in that the measured value is subjected to fast Fourier transform to determine the amplitude of a reflected wave from the underground object.
JP57210836A 1982-11-30 1982-11-30 Detection of matter embedded in ground Pending JPS5999385A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP57210836A JPS5999385A (en) 1982-11-30 1982-11-30 Detection of matter embedded in ground

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP57210836A JPS5999385A (en) 1982-11-30 1982-11-30 Detection of matter embedded in ground

Publications (1)

Publication Number Publication Date
JPS5999385A true JPS5999385A (en) 1984-06-08

Family

ID=16595912

Family Applications (1)

Application Number Title Priority Date Filing Date
JP57210836A Pending JPS5999385A (en) 1982-11-30 1982-11-30 Detection of matter embedded in ground

Country Status (1)

Country Link
JP (1) JPS5999385A (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4706031A (en) * 1984-03-30 1987-11-10 Hitachi, Ltd. Method and system for detecting an object with a radio wave
US4937580A (en) * 1988-05-19 1990-06-26 Trustees Of Dartmouth College Geophysical radar apparatus and method
JPH02212793A (en) * 1989-02-10 1990-08-23 Honda Motor Co Ltd Fm-cw radar

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4706031A (en) * 1984-03-30 1987-11-10 Hitachi, Ltd. Method and system for detecting an object with a radio wave
US4937580A (en) * 1988-05-19 1990-06-26 Trustees Of Dartmouth College Geophysical radar apparatus and method
JPH02212793A (en) * 1989-02-10 1990-08-23 Honda Motor Co Ltd Fm-cw radar

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