JPS6161027A - Measuring instrument for tension of wire body - Google Patents
Measuring instrument for tension of wire bodyInfo
- Publication number
- JPS6161027A JPS6161027A JP18399384A JP18399384A JPS6161027A JP S6161027 A JPS6161027 A JP S6161027A JP 18399384 A JP18399384 A JP 18399384A JP 18399384 A JP18399384 A JP 18399384A JP S6161027 A JPS6161027 A JP S6161027A
- Authority
- JP
- Japan
- Prior art keywords
- tension
- speed
- sensor
- ultrasonic wave
- wire body
- 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
- 238000001514 detection method Methods 0.000 claims abstract description 13
- 210000001577 neostriatum Anatomy 0.000 claims description 18
- 230000000644 propagated effect Effects 0.000 claims description 3
- 230000005540 biological transmission Effects 0.000 abstract description 2
- 238000005259 measurement Methods 0.000 description 8
- 230000036772 blood pressure Effects 0.000 description 2
- 238000000034 method Methods 0.000 description 2
- 239000011347 resin Substances 0.000 description 2
- 229920005989 resin Polymers 0.000 description 2
- 239000004925 Acrylic resin Substances 0.000 description 1
- 229920000178 Acrylic resin Polymers 0.000 description 1
- 239000004743 Polypropylene Substances 0.000 description 1
- 239000003795 chemical substances by application Substances 0.000 description 1
- 238000007796 conventional method Methods 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 238000005516 engineering process Methods 0.000 description 1
- 239000003822 epoxy resin Substances 0.000 description 1
- 238000002474 experimental method Methods 0.000 description 1
- 239000004519 grease Substances 0.000 description 1
- 239000000463 material Substances 0.000 description 1
- 229920000647 polyepoxide Polymers 0.000 description 1
- -1 polypropylene Polymers 0.000 description 1
- 229920001155 polypropylene Polymers 0.000 description 1
- 230000001902 propagating effect Effects 0.000 description 1
- 230000008054 signal transmission Effects 0.000 description 1
- 238000009987 spinning Methods 0.000 description 1
- 238000004804 winding Methods 0.000 description 1
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01L—MEASURING FORCE, STRESS, TORQUE, WORK, MECHANICAL POWER, MECHANICAL EFFICIENCY, OR FLUID PRESSURE
- G01L5/00—Apparatus for, or methods of, measuring force, work, mechanical power, or torque, specially adapted for specific purposes
- G01L5/04—Apparatus for, or methods of, measuring force, work, mechanical power, or torque, specially adapted for specific purposes for measuring tension in flexible members, e.g. ropes, cables, wires, threads, belts or bands
- G01L5/042—Apparatus for, or methods of, measuring force, work, mechanical power, or torque, specially adapted for specific purposes for measuring tension in flexible members, e.g. ropes, cables, wires, threads, belts or bands by measuring vibrational characteristics of the flexible member
Landscapes
- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Force Measurement Appropriate To Specific Purposes (AREA)
Abstract
Description
【発明の詳細な説明】
〔産業上の利用分野〕
この発明は、テニスやバドミントン等のラケットに張ら
れたガツト張力の測定、あるいは紡績、電線、コード工
場での引き抜き、巻き取り時の張力測定、さらには機械
、構造物、建築物等におけるローブやワイヤ等の張力測
定等を超音波信号を利用して行なう線条体の張力測定装
置に関するものである。[Detailed Description of the Invention] [Industrial Application Field] This invention is applicable to the measurement of string tension on rackets for tennis, badminton, etc., or the measurement of tension during pulling and winding in spinning, electric wire, and cord factories. Furthermore, the present invention relates to a tension measuring device for striatal bodies that uses ultrasonic signals to measure the tension of lobes, wires, etc. in machines, structures, buildings, etc.
従来の線条体、例えばテニスラケットに張ったガツトの
張力の測定に関しては、■張設した1本1本のがツ1−
張力、■縦横に張設したガツトの網目の大きさも含めた
ネットとしての張力すなわち血圧、が測定対象となって
いる。しかし、■についてはガラ1〜をラケッ1〜に張
設する時点での張力は測定できるが、ボール打撃及び時
間経過によってガラ1〜張力の緩和が生じたとしても、
このような状態に至った後で1本1本のガツト張力を測
る手段はなかった。■の血圧の測定は、第7図に示すよ
うな測定器100で測ることができ、この測定器100
は一定の荷重をラケットフレーム20に張設されたガラ
h 211、h11+、ガツト21に生ずるたりみ畿(
=よりカット210面圧を測っていた。Regarding the conventional measurement of tension in striatal bodies, for example, strings stretched on tennis rackets,
The object of measurement is the net tension, which includes the mesh size of the guts stretched vertically and horizontally, that is, blood pressure. However, regarding (2), although the tension at the time when the racket 1~ is stretched on the racket 1~ can be measured, even if the tension on the racket 1~ is relaxed due to the ball hit and the passage of time,
There was no way to measure the tension of each string after reaching such a state. Measurement of blood pressure in (2) can be performed using a measuring device 100 as shown in FIG.
applies a constant load to the racks h211, h11+, and guts 21 stretched on the racket frame 20 (
= The cut 210 surface pressure was measured.
(解決しようとする問題点)
従来は、1本1本の線条fk(ガツト21)の張力を測
定することはできず、複数本張設したネット状線条体群
の所定面にお1する面圧を測定できるのみであり、しか
も面圧測定後は線条体の張力に変化を生じさせてしまう
ような測定手段であった。(Problem to be solved) Conventionally, it was not possible to measure the tension of each filament fk (gut 21), and it was not possible to measure the tension of each filament fk (gut 21). This measuring method can only measure the surface pressure that occurs, and furthermore, after measuring the surface pressure, it causes a change in the tension in the striatum.
そこで、この発明は、1本1本の線条体の張力測定を可
能ならしめ、測定によってその後の張力に変化を生じさ
せないような張力測定@置を提供することを目的どして
開光された。Therefore, the present invention was developed with the aim of providing a tension measurement system that makes it possible to measure the tension of each striatum and does not cause subsequent changes in tension due to the measurement. .
一ヒ述の問題点を解決し、1本1本の線条体の張力を簡
単に測定するI、め、この発明は、所定の距離間(:張
設された線条体に刻し一定間隔をおいて取付けられる超
音波信号の入射用しごンリー及び当該セン勺−から線条
体に伝播した超音波信号を検出する検出用センサーと、
入射用センリーーに接続された超音波信号発振器と、検
出用セン1ナーに接続された超音波信号受信器と、超音
波信号の速度を測定する速度測定器とから測定装置を構
成した。This invention solves the above-mentioned problems and easily measures the tension in each striatum. an ultrasonic signal incidence sensor mounted at intervals, and a detection sensor for detecting the ultrasonic signal propagated from the sensor to the striatum;
The measuring device was composed of an ultrasonic signal oscillator connected to the incident sensor, an ultrasonic signal receiver connected to the detection sensor, and a speed measuring device for measuring the speed of the ultrasonic signal.
lス下にこの発明の好適な実施例を図面を参照しつつ説
明する。Below, preferred embodiments of the present invention will be described with reference to the drawings.
図面上符号1は、ガツト・電線・コード・ワイヤ等の線
条体であり、この線条体1は、所定の距離間に張設しで
ある。線条体1に対し一定間隔(をおいて2つのセンサ
ー2.3を取付ける。一方のセン1J−2は、超音波信
号発生器4に接続され、線条体1へ信号を入射するため
の入射用センサー2であり、他方のセンナ−3は、超音
波信号受信器5に接続され線条体1を伝播してくる信号
を検出するための検出用センサー3である。Reference numeral 1 in the drawings indicates a striated body such as a string, an electric wire, a cord, or a wire, and this striated body 1 is stretched over a predetermined distance. Two sensors 2 . The other sensor 3 is a detection sensor 3 that is connected to an ultrasonic signal receiver 5 and detects a signal propagating through the striatum 1 .
第1図において両センサー2.3は、直接線条体1へ取
付けずに接触端子6.7を介して線条体1に取付けであ
る。この接触端子6(7も同様)は、第2図(a )、
(b)、(C)に示すように、線条体1に単に接触する
もの(第2図(a))、線条体1を挾むもの(第2図(
b))、線条体1を通す乙の(#12図(C))等積々
のタイプのものが考えられる。また、接@端子6(7)
と線条体1との間にグリース8、リップリング剤9を使
用し、線条体1との密着を図り、超音波信号の伝達を容
易にすることもできる(第3図参照)。グリース8やカ
ンー/’IIン〃剤9 it、第3図に示す形状の接触
端子6(7)のみならず、第2図(a )、(b )に
示す形状の接触端子6(7)にも用いられる。接触端子
6(7)とし・では、アクリル樹脂、ボリスヂレン樹脂
、ポリアクリレ−1〜tH1,ポリプロピレン樹脂、エ
ポキシ樹脂等の一定の固さを有し機械的加工が可能なも
のであれば良い。なお、両センυ−2,3の振動子自体
を第2図(a )、(b)、(C)の如き形状に加工し
て直接線条体1に取付けることも勿論可能である。In FIG. 1, both sensors 2.3 are not attached directly to the strip 1, but via contact terminals 6.7. This contact terminal 6 (same as 7) is shown in Fig. 2(a).
As shown in (b) and (C), those that simply touch the striatum 1 (Fig. 2(a)) and those that sandwich the striatum 1 (Fig. 2(a))
b)), which passes through the striatum 1 (Fig. #12 (C)), etc., can be considered. Also, contact @terminal 6 (7)
It is also possible to use grease 8 and lip ring agent 9 between the wire and the striated body 1 to achieve close contact with the striated body 1 and facilitate the transmission of ultrasonic signals (see FIG. 3). Not only the contact terminal 6 (7) having the shape shown in Fig. 3, but also the contact terminal 6 (7) having the shape shown in Fig. 2 (a) and (b) Also used for The contact terminal 6 (7) may be made of any material that has a certain hardness and can be mechanically processed, such as acrylic resin, borisdyrene resin, polyacrylate-1 to tH1, polypropylene resin, or epoxy resin. Of course, it is also possible to process the vibrators of both sensors υ-2 and 3 into shapes as shown in FIGS. 2(a), (b), and (C) and attach them directly to the filament body 1.
超音波信号発信、受信器4.5には速宜測定器10を取
付け、当該測定器10により入射用ヒンサー2から超音
波信号を線条体1へ入射し検出センサーから検出し、こ
の2つの信号の時間!!tを測定する。両ヒンサー2.
3の間隔(と時間差【とから音速Cを次の如<III稗
する。Ultrasonic signal transmission, a quick measuring device 10 is attached to the receiver 4.5, and the measuring device 10 makes the ultrasonic signal enter the striatum 1 from the incident hinter 2 and detect it from the detection sensor, and the ultrasonic signal is detected by the detection sensor. Signal time! ! Measure t. Both Hinsa 2.
From the interval (and time difference [) of 3, the speed of sound C is calculated as follows.
を
次にテニスラケットのガツト張力を第4図、第5図示す
ような接触端子6.7を用い、間隔(を一方(J!+)
r46m++i、他方(、e2)r261mとして張力
を変えたときの音速を測定した。その結果は第6図に示
す通りであった。第6図中0印のグラフが第4図に示す
ものの実験結果であり、Δ印のグラフが第5ii!lに
示すものの実験結果である。Next, measure the tension of the tennis racket using a contact terminal 6.7 as shown in Figures 4 and 5, and set the distance (on one side (J!+)
The sound speed was measured when the tension was changed with r46m++i and the other (e2) r261m. The results were as shown in FIG. The graph marked 0 in Fig. 6 is the experimental result of the one shown in Fig. 4, and the graph marked Δ is the result of the experiment shown in Fig. 4. These are the experimental results shown in 1.
この結果から明らかなように、ガツト張h(li%i条
体1の張力)が増加すると音速も増加することが判明し
た。As is clear from this result, it was found that as the tension h (tension of the li%i strip 1) increases, the speed of sound also increases.
なお、第1図に示す速度測定器10には表示装置と;ノ
でオシログラフ11を設けである。速+t*定11f1
0に所定のgI算をして張力の値を即座に表示するよう
なマイコン利用の表示器を取付けることも勿論可能であ
る。The speed measuring device 10 shown in FIG. 1 is equipped with a display device and an oscillograph 11. speed + t * constant 11f1
Of course, it is also possible to install a display using a microcomputer that calculates a predetermined gI value to 0 and immediately displays the tension value.
以上説明したように、この発明によれば、所定の距離間
に張設されたtm条体に対し・て一定間隔をおいて取付
けられる超音波信号の入射用センサー及び当該セン号−
から線条体に伝播した超音波信号を検出する検出用セン
υ−と、入射用センサーに接続された超音波信号発振器
と、検出用セン9−に接続された超音波信号光1ト器と
、超音波信号の速度を測定する速度測定器とから成り、
1本1本の線条体の張力の測定が可能となるのみならず
、測定に当っては単に両センサーを線条体に当てがうだ
けでありきわめてMl!でぶ)る。また、従来のように
張設した線条体に荷重をかけたり1ノないので、線条体
に恩影誓を及(よqtTともない。As explained above, according to the present invention, there is provided an incident sensor for ultrasonic signals that is attached at regular intervals to the tm strip stretched over a predetermined distance, and
a detection sensor υ- for detecting the ultrasonic signal propagated from the to the striatum; an ultrasonic signal oscillator connected to the incident sensor; and an ultrasonic signal light unit connected to the detection sensor 9-. , a speed measuring device that measures the speed of the ultrasonic signal;
Not only is it possible to measure the tension in each striatum, but the measurement requires simply applying both sensors to the striatum, making it extremely easy to use! Fat). In addition, since there is no need to apply a load to the stretched striatum as in the conventional method, there is no impact on the striatum.
第1図はこの発明の好適な実施例を示−11全体図、第
2図(a )ないしくC)は接触端子の8例を示す斜視
図、第3図は線条体と接触端子との断面図、第4図及び
第5図は異なる接触端子を用い各端子間の間隔を変えた
例を示′?i斜?52図、第6図は第4図及び第5図の
例による張力と音速との関係を示すグラフ、第7図1オ
従来例を示す一部断面図である。
1・・・・・・線条体、
2・・・・・・入射用センサー、
3・・・・・・検出用セン9−。
4・・・・・・超音波信号発振器、
5・・・・・・超音波信号受信器、
6.7・・・・・・接触端子、
10・・・・・・速度測定器。Fig. 1 shows a preferred embodiment of the present invention - 11 overall view, Fig. 2 (a) to C) is a perspective view showing eight examples of contact terminals, and Fig. 3 shows the relationship between the wire body and the contact terminal. The cross-sectional views of FIGS. 4 and 5 show examples in which different contact terminals are used and the spacing between each terminal is changed. i oblique? 52 and 6 are graphs showing the relationship between tension and sound velocity according to the examples shown in FIGS. 4 and 5, and FIG. 7 is a partial sectional view showing the conventional example. 1...Striatum, 2...Incidence sensor, 3...Detection sensor 9-. 4... Ultrasonic signal oscillator, 5... Ultrasonic signal receiver, 6.7... Contact terminal, 10... Speed measuring device.
Claims (1)
おいて取付けられる超音波信号の入射用センサー及び当
該センサーから線条体に伝播した超音波信号を検出する
検出用センサーと、 前記入射用センサーに接続された超音波信号発振器と、 前記検出用センサーに接続された超音波信号受信器と、 超音波信号の速度を測定する速度測定器とから成る線条
体の張力測定器。 2、前記速度測定器は、入射用センサーから線条体へ信
号を入射後検出用センサーがこの信号を検出するまでの
時間と両センサー間の距離とから音速を求めるように構
成されていることを特徴とする特許請求の範囲第1項に
記載の線条体の張力測定装置。[Claims] 1. A sensor for the incidence of ultrasonic signals that is attached at regular intervals to the striatum stretched over a predetermined distance, and an ultrasonic signal propagated from the sensor to the striatum. It consists of a detection sensor for detecting, an ultrasonic signal oscillator connected to the incident sensor, an ultrasonic signal receiver connected to the detection sensor, and a speed measuring device for measuring the speed of the ultrasonic signal. Striatal tension measuring device. 2. The speed measuring device is configured to determine the speed of sound from the time it takes for the detection sensor to detect this signal after the signal is input from the incident sensor to the striatum and the distance between both sensors. A striatal body tension measuring device according to claim 1, characterized in that:
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP18399384A JPS6161027A (en) | 1984-09-03 | 1984-09-03 | Measuring instrument for tension of wire body |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP18399384A JPS6161027A (en) | 1984-09-03 | 1984-09-03 | Measuring instrument for tension of wire body |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPS6161027A true JPS6161027A (en) | 1986-03-28 |
Family
ID=16145438
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP18399384A Pending JPS6161027A (en) | 1984-09-03 | 1984-09-03 | Measuring instrument for tension of wire body |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS6161027A (en) |
Cited By (8)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| FR2747472A1 (en) * | 1996-04-12 | 1997-10-17 | Cousin Trestec | Fatigue control system particularly for textile cables |
| US9048521B2 (en) | 2011-03-24 | 2015-06-02 | Etegent Technologies, Ltd. | Broadband waveguide |
| US9182306B2 (en) | 2011-06-22 | 2015-11-10 | Etegent Technologies, Ltd. | Environmental sensor with tensioned wire exhibiting varying transmission characteristics in response to environmental conditions |
| JP2017219369A (en) * | 2016-06-06 | 2017-12-14 | 西松建設株式会社 | Vibration device, vibration measurement system, vibration measurement method, and measurement method of tensile force |
| US10352778B2 (en) | 2013-11-01 | 2019-07-16 | Etegent Technologies, Ltd. | Composite active waveguide temperature sensor for harsh environments |
| US10854941B2 (en) | 2013-11-01 | 2020-12-01 | Etegent Technologies, Ltd. | Broadband waveguide |
| US10852277B2 (en) | 2014-04-09 | 2020-12-01 | Etegent Technologies, Ltd. | Active waveguide excitation and compensation |
| US11473981B2 (en) | 2017-04-10 | 2022-10-18 | Etegent Technologies Ltd. | Damage detection for mechanical waveguide sensor |
-
1984
- 1984-09-03 JP JP18399384A patent/JPS6161027A/en active Pending
Cited By (10)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| FR2747472A1 (en) * | 1996-04-12 | 1997-10-17 | Cousin Trestec | Fatigue control system particularly for textile cables |
| US9048521B2 (en) | 2011-03-24 | 2015-06-02 | Etegent Technologies, Ltd. | Broadband waveguide |
| US9182306B2 (en) | 2011-06-22 | 2015-11-10 | Etegent Technologies, Ltd. | Environmental sensor with tensioned wire exhibiting varying transmission characteristics in response to environmental conditions |
| US10352778B2 (en) | 2013-11-01 | 2019-07-16 | Etegent Technologies, Ltd. | Composite active waveguide temperature sensor for harsh environments |
| US10854941B2 (en) | 2013-11-01 | 2020-12-01 | Etegent Technologies, Ltd. | Broadband waveguide |
| US10852277B2 (en) | 2014-04-09 | 2020-12-01 | Etegent Technologies, Ltd. | Active waveguide excitation and compensation |
| US11982648B2 (en) | 2014-04-09 | 2024-05-14 | Etegent Technologies, Ltd. | Active waveguide excitation and compensation |
| JP2017219369A (en) * | 2016-06-06 | 2017-12-14 | 西松建設株式会社 | Vibration device, vibration measurement system, vibration measurement method, and measurement method of tensile force |
| US11473981B2 (en) | 2017-04-10 | 2022-10-18 | Etegent Technologies Ltd. | Damage detection for mechanical waveguide sensor |
| US11686627B2 (en) | 2017-04-10 | 2023-06-27 | Etegent Technologies Ltd. | Distributed active mechanical waveguide sensor driven at multiple frequencies and including frequency-dependent reflectors |
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