JPH0566545B2 - - Google Patents
Info
- Publication number
- JPH0566545B2 JPH0566545B2 JP59172602A JP17260284A JPH0566545B2 JP H0566545 B2 JPH0566545 B2 JP H0566545B2 JP 59172602 A JP59172602 A JP 59172602A JP 17260284 A JP17260284 A JP 17260284A JP H0566545 B2 JPH0566545 B2 JP H0566545B2
- Authority
- JP
- Japan
- Prior art keywords
- defect
- propagation time
- center
- rectangular column
- ultrasonic
- 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
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Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N29/00—Investigating or analysing materials by the use of ultrasonic, sonic or infrasonic waves; Visualisation of the interior of objects by transmitting ultrasonic or sonic waves through the object
- G01N29/04—Analysing solids
- G01N29/07—Analysing solids by measuring propagation velocity or propagation time of acoustic waves
Landscapes
- Physics & Mathematics (AREA)
- Acoustics & Sound (AREA)
- Health & Medical Sciences (AREA)
- Life Sciences & Earth Sciences (AREA)
- Chemical & Material Sciences (AREA)
- Analytical Chemistry (AREA)
- Biochemistry (AREA)
- General Health & Medical Sciences (AREA)
- General Physics & Mathematics (AREA)
- Immunology (AREA)
- Pathology (AREA)
- Investigating Or Analyzing Materials By The Use Of Ultrasonic Waves (AREA)
Description
【発明の詳細な説明】
〔産業上の利用分野〕
この発明は、超音波によつて矩形柱の内部にお
ける欠陥部の形状および位置を診断する欠陥診断
方法に関するものである。DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a defect diagnosis method for diagnosing the shape and position of a defect inside a rectangular column using ultrasonic waves.
本出願人は、先に、比較的低周波の超音波を用
いて木柱中心部の欠陥を検出する方法(特願昭59
−59042)を提案した。そこで、以下この方法に
ついて簡単に説明する。
The applicant previously proposed a method for detecting defects in the center of wooden columns using relatively low-frequency ultrasound (patent application filed in 1983).
−59042) was proposed. Therefore, this method will be briefly explained below.
第7図は、中心部に腐朽部Hがある木製電柱の
一断面であり、外周を16に等分割する位置をそれ
ぞれP1,P2,……P16とする。まず、送信探触子
を位置P1に、受信探触子を位置P2に当接し伝播
時間を測定する。次に、送信接触子を前記位置と
し、受信接触子のみを位置P3として再び伝播時
間を測定する。以上の様に送信探触子は位置を固
定したまま受信探触子のみを位置P4,P5,P6お
よびP7へと変えながら伝播時間を測定する。こ
の時、両探触子間の直線距離Lと伝播時間Tとの
関係を示すと第8図のようになる。第8図中のプ
ロツトにおいて、Lの小さい方からそれぞれ受信
探触子位置はP1,P2,P3,P4,P5,P6,P7およ
びP8に対応す。これより、P5からP6に移ると伝
播時間は急に長くなることがわかる。これは、
P1とP6を結ぶ超音波の伝播経路の途中に腐朽部
Hがあるからである。したがつて、第8図に示す
ように腐朽部Hに接する点は、近似的にP5とP6
の中間点Q1とP1を結ぶ線の中点F1として表わさ
れる。 FIG. 7 shows a cross section of a wooden utility pole with a decayed part H in the center, and the positions at which the outer circumference is equally divided into 16 parts are designated as P 1 , P 2 , . . . P 16 , respectively. First, the transmission probe is brought into contact with the position P 1 and the reception probe is brought into contact with the position P 2 to measure the propagation time. Next, the propagation time is measured again with the transmitting contact at the above position and only the receiving contact at position P3 . As described above, the propagation time is measured while changing only the receiving probe to positions P 4 , P 5 , P 6 and P 7 while keeping the transmitting probe fixed in position. At this time, the relationship between the straight line distance L between both probes and the propagation time T is shown in FIG. In the plot in FIG. 8, the receiving probe positions correspond to P 1 , P 2 , P 3 , P 4 , P 5 , P 6 , P 7 and P 8 from the smallest L. From this, it can be seen that the propagation time suddenly increases when moving from P 5 to P 6 . this is,
This is because there is a decayed part H in the middle of the ultrasonic propagation path connecting P 1 and P 6 . Therefore, as shown in Fig. 8, the points in contact with the decayed part H are approximately P 5 and P 6.
It is expressed as the midpoint F 1 of the line connecting the midpoint Q 1 and P 1 .
上記と同様に、P3を送信探触子2aとして、
受信探触子をP4,P5……と位置を変えながら伝
播時間を測定する。すると、第8図と同様に変曲
点を見い出すことができるので、腐朽部Hに接す
る近似点F2をもとめられる。以下同様に、P5,
P7,P9,P11,P13,P15を起点とし測定を行なう
と、F1,F2……,F8が得られるので、これらを
直線で結ぶと第9図の結果が得られる。 Similarly to the above, with P 3 as the transmitting probe 2a,
The propagation time is measured while changing the position of the receiving probe as P 4 , P 5 , etc. Then, the point of inflection can be found as in FIG. 8, and the approximate point F2 that is in contact with the decayed part H can be found. Similarly, P 5 ,
If we measure from P 7 , P 9 , P 11 , P 13 , P 15 as starting points, we will obtain F 1 , F 2 . It will be done.
以上述べた方法は、丸材に対しては、第7図と
第8図を比較すれば明らかなように有効な診断方
法ではあるが、しかしこの方法はあくまでも円形
木柱に対する腐朽診断方法であるため、矩形の柱
の内部欠陥診断には用いることができず、その矩
形の柱に対する診断方法の開発が望まれていた。
The method described above is an effective diagnostic method for round wood, as is clear from comparing Figures 7 and 8, but this method is only a method for diagnosing rot for circular wooden columns. , it cannot be used for diagnosing internal defects in rectangular pillars, and it has been desired to develop a diagnostic method for rectangular pillars.
この発明の矩形柱の欠陥診断方法は、矩形柱の
一断面における2対の対辺間の超音波伝播時間を
数ケ所測定して、各対の対辺間において伝播時間
が最長となる測定線の交点から欠陥中心をもとめ
る第1の過程と、前記の一断面における一辺の中
点付近に超音波送信子または受信子の一方を固定
し、隣接変において前記探触子に近い位置から超
音波送信子または受信子の他方を順次遠ざけて、
伝播時間の急増点から内部欠陥への外接線を見い
出す第2の過程と、前記欠陥中心から前記各々の
外接線に垂線をおろすことによつてもとまるいく
つかの接点をなめらかな曲線で結んで欠陥形状を
表わす第3の過程によつて欠陥検出を行なうこと
を特徴とする。
The method for diagnosing defects in a rectangular column according to the present invention involves measuring the ultrasonic propagation time between two pairs of opposite sides at several locations in one cross section of a rectangular column, and measuring the intersection of the measurement lines where the propagation time is the longest between each pair of opposite sides. A first process of finding the center of the defect from the center of the defect, fixing either the ultrasonic transmitter or the receiver near the midpoint of one side in the one cross section, and moving the ultrasonic transmitter or receiver from a position close to the probe in the adjacent section. Or move the other receiver further away one by one,
A second process of finding the external tangent from the point of rapid increase in propagation time to the internal defect, and connecting several tangent points that are stopped by drawing perpendicular lines from the defect center to each of the external tangents with a smooth curve. The present invention is characterized in that defect detection is performed by a third process that represents the defect shape.
以下、この発明の実施例を第1図乃至第6図に
基づいて説明する。
Embodiments of the present invention will be described below with reference to FIGS. 1 to 6.
第2図は内部腐朽の矩形柱の例を表わす一断面
であり、以下の説明のためのその外周部に等間隔
に配した位置記号を記す。 FIG. 2 is a cross-section showing an example of a rectangular column with internal decay, and position symbols arranged at equal intervals on its outer circumference are shown for the purpose of the following explanation.
まず、位置M1およびM1′に超音波送信子を当
接し超音波伝播時間を測定する。次にはM2〜
M2′間での伝播時間測定し、順次M3〜M3′,M4
〜M4′,…M7〜M7′のように測定する。また、
N1〜N1′,N2〜N2′,…N7〜N7′においても同
様に測定する。これらの位置と伝播時間の関係を
示すと第3図a,bのようになる。これから、
M4〜M4′上およびN4〜N4′上に腐朽の最大があ
り、両線の交点が腐朽の中心Qであることがわか
る。すなわち、超音波は、腐朽部は伝播できずに
遠まわりをするが、まさにM4〜M4′およびN4〜
N4′において最も遠まわりになるからである。な
お第5図のように腐朽部がない柱の場合には、第
6図に示すように、年輪が中心近くを通る場合ほ
ど伝播時間が短くなり、第3図a,bと逆の特性
を示す。したがつて、第3図のa,bの特性によ
つて内部腐朽の存在を知ることができる。 First, ultrasonic transmitters are brought into contact with positions M 1 and M 1 ', and the ultrasonic propagation time is measured. Next is M 2 ~
Measure the propagation time between M 2 ′ and sequentially from M 3 to M 3 ′, M 4
〜M 4 ′, ...M 7 〜M 7 ′ are measured. Also,
Measurements are made in the same manner for N 1 to N 1 ′, N 2 to N 2 ′, ...N 7 to N 7 ′. The relationship between these positions and propagation time is shown in Figures 3a and 3b. from now,
It can be seen that the maximum decay occurs above M 4 to M 4 ′ and above N 4 to N 4 ′, and the intersection of both lines is the center Q of decay. In other words, the ultrasonic waves cannot propagate through the decayed area and take a long detour, but they do not propagate through the decayed areas, but they do travel around M 4 ~ M 4 ' and N 4 ~
This is because the circuit becomes the most distant at N 4 ′. In addition, in the case of a column with no decayed parts as shown in Figure 5, the propagation time becomes shorter as the growth rings pass closer to the center, as shown in Figure 6, and the characteristics opposite to those in Figures 3a and b are obtained. show. Therefore, the presence of internal decay can be known from the characteristics a and b in FIG.
次に、探触子の一方を例えば最大の伝播時間を
示したM4におき、また他方をN7′において伝播
時間を測定する。続いて、一方側のM4はそのま
まにして、他方側をN6′にして測定し、以降
N5′,N4′……N1′と順次M4から遠ざけてゆく
と、それらの伝播時間は第4図のようになり、途
中に伝播時間が急変するところが表われる。これ
は、探触子間を結ぶ直線が腐朽部にかかつたため
であり、これが内部腐朽の外接線である。したが
つて、先にもとめた腐朽の中心Qからこの接線に
垂線をおろせば、腐朽部との接点J1をもとめるこ
とができる。次に、一方の探触子をN4′に固定
し、他方をM7′から順次遠ざける測定を行なえ
ば、前記の場合と同様にして腐朽部との接点J2が
もとめられる。以降、同様の方法で各辺について
の測定を行なうことによつて内部腐朽の外周の点
J3,J4がもとめられる。そして、これらの4点
J1,J2,J3,J4を結ぶなめらかな曲線によつて、
第1図に表わすように腐朽形状の概略の形状がも
とまる。 Next, one of the probes is placed, for example, at M 4 , which indicates the maximum propagation time, and the other probe is placed at N 7 ' to measure the propagation time. Next, leave M 4 on one side as is, set N 6 ′ on the other side, and measure.
When N 5 ', N 4 '...N 1 ' are successively moved away from M 4 , their propagation times become as shown in Fig. 4, and a sudden change in propagation time appears in the middle. This is because the straight line connecting the probes crosses the decayed area, and this is the outer tangent of the internal decay. Therefore, if we draw a perpendicular line from the center Q of the decay found earlier to this tangent, we can find the point of contact J1 with the decayed part. Next, by fixing one probe at N 4 ' and moving the other probe away from M 7 ' sequentially, the contact point J 2 with the decayed part can be found in the same way as in the previous case. Thereafter, by measuring each side using the same method, the points on the outer periphery of internal decay can be determined.
J 3 and J 4 are required. And these four points
By the smooth curve connecting J 1 , J 2 , J 3 , and J 4 ,
As shown in Figure 1, the approximate shape of the decayed shape is determined.
以上説明したように、この発明の矩形柱の欠陥
診断方法は、超音波の伝播時間から内部欠陥の中
心をもとめる第1の過程と、内部欠陥への外接線
を見い出す第2の過程と、欠陥の中心から各外接
線に垂線をおろしてもとまる接点をなめらかな曲
線で結ぶ第3の過程によつて、矩形柱内部の腐朽
などによる欠陥を簡便に検知することができ、ま
た白蟻などによる腐朽の診断等にも利用すことが
できる。
As explained above, the method for diagnosing defects in rectangular pillars according to the present invention includes a first process of finding the center of an internal defect from the propagation time of ultrasonic waves, a second process of finding the circumscribed line to the internal defect, and a second process of finding the circumscribed line to the internal defect. By the third process of drawing a perpendicular line from the center to each external tangent line and connecting the stopping points with a smooth curve, it is possible to easily detect defects such as decay inside the rectangular column, and also to detect decay caused by termites, etc. It can also be used for diagnosis, etc.
第1図乃至第6図はこの発明を説明するための
図であつて、第1図はこの発明によりもとめた矩
形柱の欠陥形状を表わす図、第2図は診断対象と
した矩形柱の欠陥形状を表わす図、第3図a,b
はそれぞれ第2図の内部欠陥を有する矩形柱の2
対の対辺間の超音波伝播時間とその測定位置の関
係を表わす図、第4図はこの発明の第2過程にお
いてもとめられた伝播時間の急増点を表わす図、
第5図は内部欠陥を有しない矩形柱の断面形状を
表わす図、第6図は第5図の内部欠陥を有しない
矩形柱の2対の対辺間の超音波伝播時間とその測
定位置の関係を表わす図、第7図乃至第9図は本
出願人が先に提案した円形の柱に対する診断方法
を説明するための図であつて、第7図は診断対象
とした円柱の柱の欠陥形状を表わす図、第8図は
探触子間の距離と超音波伝播時間の関係を表わす
図、第9図は本診断方法によつてもとめた円形の
柱の欠陥形状を表わす図である。
M1〜M7,M1′〜M7′,N1〜N7,N1′〜N7′…
…測定点、H……欠陥。
1 to 6 are diagrams for explaining the present invention, in which FIG. 1 is a diagram showing the defect shape of a rectangular column obtained by the present invention, and FIG. 2 is a diagram showing the defect shape of a rectangular column that is the object of diagnosis. Diagrams representing the shape, Figure 3 a, b
are the two rectangular pillars with internal defects shown in Fig. 2, respectively.
A diagram showing the relationship between the ultrasonic propagation time between a pair of opposite sides and its measurement position, FIG.
Fig. 5 is a diagram showing the cross-sectional shape of a rectangular column without internal defects, and Fig. 6 is the relationship between the ultrasonic propagation time and its measurement position between two pairs of opposite sides of the rectangular column without internal defects in Fig. 5. Figures 7 to 9 are diagrams for explaining the diagnosis method for circular pillars previously proposed by the applicant, and Figure 7 shows the defect shape of the circular pillar that was the subject of diagnosis. 8 is a diagram showing the relationship between the distance between the probes and the ultrasonic propagation time, and FIG. 9 is a diagram showing the defect shape of a circular pillar determined by the present diagnostic method. M 1 to M 7 , M 1 ′ to M 7 ′, N 1 to N 7 , N 1 ′ to N 7 ′…
...Measurement point, H...Defect.
Claims (1)
おいて、矩形柱の一断面における2対の対辺間の
超音波伝播時間を数ケ所測定して、各対の対辺間
において伝播時間が最長となる測定線の交点から
欠陥中心をもとめる第1の過程と、前記の一断面
における一辺の中点付近に超音波送信子または受
信子の一方を固定し、隣接辺において前記探触子
に近い位置から超音波送信子または受信子の他方
を順次遠ざけて、伝播時間の急増点から内部欠陥
への外接線を見い出す第2の過程と、前記欠陥中
心から前記各々の外接線に垂線をおろすことによ
つてもとまるいくつかの接点をなめらかな曲線で
結んで欠陥形状を表わす第3の過程によつて欠陥
検出を行なうことを特徴とする矩形柱の欠陥診断
方法。1 In a method of diagnosing internal defects in a rectangular column using ultrasound, the ultrasonic propagation time between two pairs of opposite sides in one cross section of a rectangular column is measured at several points, and the propagation time is the longest between each pair of opposite sides. The first step is to find the center of the defect from the intersection of the measurement lines, and fix one of the ultrasonic transmitter or the receiver near the midpoint of one side in the one cross section, and measure the center of the defect from a position close to the probe on the adjacent side. A second process of sequentially moving the other of the ultrasonic transmitter or the receiver away and finding the external tangent to the internal defect from the point where the propagation time increases; and by drawing a perpendicular line from the center of the defect to each external tangent. A method for diagnosing a defect in a rectangular column, characterized in that defect detection is performed by a third process in which a number of contact points that stop at each other are connected with a smooth curve to represent the defect shape.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP59172602A JPS6150064A (en) | 1984-08-20 | 1984-08-20 | Diagnosis of defect in square pilar |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP59172602A JPS6150064A (en) | 1984-08-20 | 1984-08-20 | Diagnosis of defect in square pilar |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS6150064A JPS6150064A (en) | 1986-03-12 |
| JPH0566545B2 true JPH0566545B2 (en) | 1993-09-22 |
Family
ID=15944898
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP59172602A Granted JPS6150064A (en) | 1984-08-20 | 1984-08-20 | Diagnosis of defect in square pilar |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS6150064A (en) |
Families Citing this family (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| FR2646239B1 (en) * | 1989-04-24 | 1991-08-16 | Dassault Avions | ACOUSTIC METHOD AND DEVICE FOR LOCATING DEFECTS IN THE MATERIAL CONSTITUTING A PART AND ACOUSTIC TRANSMITTER FOR USE IN THIS DEVICE |
| JP3724135B2 (en) * | 1996-10-31 | 2005-12-07 | 日立電線株式会社 | Manufacturing method of irregular cross section |
-
1984
- 1984-08-20 JP JP59172602A patent/JPS6150064A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS6150064A (en) | 1986-03-12 |
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