JPS61114179A - Investigation radar device - Google Patents
Investigation radar deviceInfo
- Publication number
- JPS61114179A JPS61114179A JP59237016A JP23701684A JPS61114179A JP S61114179 A JPS61114179 A JP S61114179A JP 59237016 A JP59237016 A JP 59237016A JP 23701684 A JP23701684 A JP 23701684A JP S61114179 A JPS61114179 A JP S61114179A
- Authority
- JP
- Japan
- Prior art keywords
- target
- antenna
- transmission
- underground
- antennas
- 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
Links
Abstract
Description
【発明の詳細な説明】
〔産業上の利用分野〕
この発明は地中埋設物を探査する探査レーダ装置に関し
、特に地中埋設物の種類を判別することのできる装置に
関する。DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to an exploration radar device for exploring underground objects, and particularly to a device capable of determining the type of underground objects.
従来のこの種の装置を第2図に示す地中埋設物探査レー
ダに基づいて説明すると、図において、(1)は電波を
発生させアンテナ(2)から発信する 。A conventional device of this type will be explained based on the underground object detection radar shown in FIG. 2. In the figure, (1) generates radio waves and transmits them from an antenna (2).
発信機、(3)は反射波をアンテナ(2)ヲ介して受信
する受信機、(4)は信号処理機、(5)は探査対象と
なる地中に埋設された物標である。A transmitter, (3) a receiver that receives reflected waves via an antenna (2), (4) a signal processor, and (5) a target buried underground to be explored.
次に動作について説明すると、発信機(1)から発信さ
れる電波はアンテナ(2)ヲ介して地中に向けて放射さ
れて物標(5)に到達し、到達電波は物標(5)によっ
て発射されアンテナ(2)によって受信される。この受
信波は受信機(3)及び信号処理機(4)によって演算
処理され、物標(5)の有無及びその位置を測定する。Next, to explain the operation, the radio waves emitted from the transmitter (1) are radiated underground through the antenna (2) and reach the target (5), and the arriving radio waves reach the target (5). and received by the antenna (2). This received wave is processed by a receiver (3) and a signal processor (4) to measure the presence or absence of a target (5) and its position.
従来の地中埋設物の探査レーダ装置は以上のように構成
されていたため、地中埋設物(5)の位置及びその深さ
を探査する機能を有するのみで、埋設物(5)の種類ま
でも判別することができないという欠点があった。Since the conventional underground object detection radar device was configured as described above, it only had the function of detecting the location and depth of the underground object (5), and could not detect the type of the underground object (5). It also has the disadvantage that it cannot be distinguished.
この発明は斜上の欠点を除去するためになされたもので
、地中埋設物(5)の位置及びその深さ以外に埋設物の
種類を判定することができるようにすることを目的とし
ている。This invention was made in order to eliminate the problem of slope, and aims to make it possible to determine the type of underground object (5) other than its position and depth. .
C問題点を解決するための手段〕
この発明は送信、受信アンテナを所定距離を隔てて分離
配置し、また、送信電力と受信電力を計測することによ
って地中の媒質と物標の電気定数から、その種類を判別
することができるようにした装置を提供するものである
。Means for Solving Problem C] This invention separates the transmitting and receiving antennas at a predetermined distance and measures the transmitting power and receiving power, thereby determining the electrical constants of the underground medium and the target object. , and to provide a device that can determine the type.
以下第1図に示す実施例に基づいて従来と同−又は相当
部分には同一符号を付して説明すると、図において、(
2a)は電波を放射電力P8、反射電力PRIとして送
受信する第1アンテナ、(2b)は第1アンテナ(2a
)から距離Xを隔てて配置された反射電力P0として受
信する第2アンテナ、(3’)は送受信波を信号処理す
るとともに、第1アンテナ(2a)、第2アンテナ(2
b)から得られた反射波から地中埋設物(5)の位置、
深さを測定する他、地中埋設物(5)の種別をも演算処
理して判別することのできる信号処理演算機である。The following explanation will be given based on the embodiment shown in FIG.
2a) is the first antenna that transmits and receives radio waves as radiated power P8 and reflected power PRI; (2b) is the first antenna (2a
), the second antenna (3') receives the reflected power P0 at a distance X from the
b) The position of the underground object (5) from the reflected wave obtained from
In addition to measuring the depth, this is a signal processing computer that can also process and determine the type of underground objects (5).
次に動作について説明すると、発信機(1)からの電波
が第1アンテナ(2&)によって電力P8として放射さ
れると、地中埋設物(5)からの反射波は第1アンテナ
(2&)において電力PRIとして受信される一方、第
2アンテナ(2b)では電力pitとして受信される。Next, to explain the operation, when the radio wave from the transmitter (1) is radiated by the first antenna (2&) as power P8, the reflected wave from the underground object (5) is transmitted to the first antenna (2&). While it is received as power PRI, it is received as power PIT by the second antenna (2b).
第1アンテナ(2a)と第2アンテナ(2b)の距離が
X1地中埋設物(5)の深さがYであることから、今、
地中埋設物(5)の反射率をF1地中での電波の減衰率
をα、地中の誘電率をtl、埋設物(5)の誘電率ヲ!
、であるとすると、・・・■
又、第1.第2アンテナ(2a) 、 (2b)で受信
される電波が発信されてからの時間をそれぞれtl。Since the distance between the first antenna (2a) and the second antenna (2b) is X1 and the depth of the underground object (5) is Y, now,
The reflectance of the underground object (5) is F1, the attenuation rate of radio waves underground is α, the underground permittivity is tl, and the permittivity of the underground object (5) is wo!
,...■ Also, the first. The time from when the radio waves received by the second antennas (2a) and (2b) are transmitted is tl, respectively.
’I、自由空間での電波の速度1cとすると、という関
係式が成立する。'I, the speed of radio waves in free space 1c, the following relational expression holds true.
したがって上記各式から を得ることができる。Therefore, from each of the above equations, can be obtained.
したがって0式から地中埋設物(5)の深さを、0式に
よって得られる地中の誘電率(tl)から地質を算出で
き、0式での地中埋設物(5)の示す誘電率(ε、)か
らその種類を判別することができる。Therefore, the depth of the underground object (5) can be calculated from the 0 formula, and the geology can be calculated from the underground dielectric constant (tl) obtained by the 0 formula, and the dielectric constant of the underground object (5) in the 0 formula The type can be determined from (ε,).
これらのことから、第1.第2アンテナ(4a) 。From these points, 1. Second antenna (4a).
(4b)間の距離、送信電力P、と受信電力pHl l
PRl、及びそれぞれの到達時間f1. tlの計測
値を信号処理演算機(3′)によって計算することによ
って地中埋設物(5)の位置を知り、種別を判別するこ
とができる。(4b) Distance between, transmission power P, and reception power pHl
PRl, and their respective arrival times f1. By calculating the measured value of tl by the signal processing computer (3'), the position of the underground object (5) can be known and the type can be determined.
なお、上記実施例では第1.第2アンテナを(2a)
、 (2b)としてアンテナを2台用いた場合について
示したが、地中の誘電率(ε1)が予めわかっていれば
アンテナが1台であっても埋設物の誘電率(ε、)ヲ求
めることにより地中埋設物(5)の種類を判別すること
ができる。Note that in the above embodiment, the first. 2nd antenna (2a)
, (2b) shows the case where two antennas are used, but if the underground permittivity (ε1) is known in advance, the permittivity (ε, ) of the buried object can be found even if there is only one antenna. This allows the type of underground object (5) to be determined.
以上この発明によれば地中に埋設された物標の位置を探
査する他物様の種類を判別することができる探査レーダ
装置を得ることができる。As described above, according to the present invention, it is possible to obtain an exploration radar device capable of determining the type of object to be explored for the position of a target buried underground.
第1図は、本発明に係ぬ地中埋設物探査レーダを示す図
、第2図は、従来の地中埋設物探査レーダを示す第1図
相当図である。
(1)は発信機、(2)は送受信アンテナ、(2a)は
第1アンテナ、(2b)は第2アンテナ、(3)は受信
機、(3勺は演算機、(4)は信号処理機、(5)は物
標である。FIG. 1 is a diagram showing an underground object detection radar according to the present invention, and FIG. 2 is a diagram corresponding to FIG. 1 showing a conventional underground object detection radar. (1) is the transmitter, (2) is the transmitting and receiving antenna, (2a) is the first antenna, (2b) is the second antenna, (3) is the receiver, (3) is the computing device, (4) is the signal processing machine, (5) is a target.
Claims (1)
する探査レーダ装置において、上記物標に電波を放射し
、その反射波を受信する第1アンテナと、この第1アン
テナから所定距離隔てて配置され、上記物標からの反射
波を受信する第2アンテナとを備え、上記第1アンテナ
および第2アンテナから得られる各所要送受信時間、送
受信電力およびこれら両アンテナ間距離をデータ信号と
して演算処理して上記物標の誘電率を算出し、この物標
の種類を判別する演算処理部とを設けたことを特徴とす
る探査レーダ装置。In an exploration radar device that searches for a target by emitting radio waves to a target and receiving the reflected waves, there is provided a first antenna that emits radio waves to the target and receives the reflected waves; and a second antenna arranged at a predetermined distance apart and receiving reflected waves from the target object, and data on each required transmission/reception time, transmission/reception power, and distance between these two antennas obtained from the first antenna and the second antenna. An exploration radar device comprising: a calculation processing unit that calculates the dielectric constant of the target object by performing calculation processing as a signal and determines the type of the target object.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP59237016A JPS61114179A (en) | 1984-11-09 | 1984-11-09 | Investigation radar device |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP59237016A JPS61114179A (en) | 1984-11-09 | 1984-11-09 | Investigation radar device |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS61114179A true JPS61114179A (en) | 1986-05-31 |
Family
ID=17009136
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP59237016A Pending JPS61114179A (en) | 1984-11-09 | 1984-11-09 | Investigation radar device |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS61114179A (en) |
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS63142284A (en) * | 1986-12-04 | 1988-06-14 | Komatsu Ltd | Buried article finder |
JPH0552949A (en) * | 1991-08-28 | 1993-03-02 | Toda Constr Co Ltd | Underground detecting radar system |
JPH06214043A (en) * | 1993-01-13 | 1994-08-05 | Kyushu Denki Kensetsu Koji Kk | Method for detecting underground buried circuit position |
-
1984
- 1984-11-09 JP JP59237016A patent/JPS61114179A/en active Pending
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS63142284A (en) * | 1986-12-04 | 1988-06-14 | Komatsu Ltd | Buried article finder |
JPH0552949A (en) * | 1991-08-28 | 1993-03-02 | Toda Constr Co Ltd | Underground detecting radar system |
JPH06214043A (en) * | 1993-01-13 | 1994-08-05 | Kyushu Denki Kensetsu Koji Kk | Method for detecting underground buried circuit position |
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