JPH0766059B2 - Thread detection method - Google Patents
Thread detection methodInfo
- Publication number
- JPH0766059B2 JPH0766059B2 JP60263522A JP26352285A JPH0766059B2 JP H0766059 B2 JPH0766059 B2 JP H0766059B2 JP 60263522 A JP60263522 A JP 60263522A JP 26352285 A JP26352285 A JP 26352285A JP H0766059 B2 JPH0766059 B2 JP H0766059B2
- Authority
- JP
- Japan
- Prior art keywords
- light
- yarn
- signal
- light projecting
- detection method
- 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
Links
Landscapes
- Geophysics And Detection Of Objects (AREA)
- Looms (AREA)
- Spinning Or Twisting Of Yarns (AREA)
- Optical Radar Systems And Details Thereof (AREA)
Description
【発明の詳細な説明】 〔産業上の利用分野〕 本発明は、糸の探知方法の改良、詳しくは、光学上の距
離逆2乗則(inverse−square law)を巧みに利用し
て、糸路における糸の有無を驚くほど高精度にサーチす
ることができる画期的探知方法に関するものであって、
織機・撚糸機・管巻機など各種の繊維機械に利用できる
新技術である。DETAILED DESCRIPTION OF THE INVENTION [Industrial field of application] The present invention relates to an improvement in a yarn detection method, and more specifically, to skillfully utilize an optical inverse-square law. The present invention relates to an epoch-making detection method capable of searching for the presence or absence of a thread in a road with surprisingly high accuracy,
This is a new technology that can be used for various textile machines such as weaving machines, twisting machines, and winders.
従来、織機・撚糸機・管巻機などの繊維機器における給
糸状態の異常を探知する方法としては、 (1)ドロッパー機構を利用した機械的な探知方法、 (2)圧電素子やマイクロスイッチを利用した電気的な
探知方法、 (3)投受光素子を利用した光電探知方法、 といった方法が実用化されている。Conventionally, as a method for detecting an abnormality in a yarn feeding state in a textile device such as a loom, a twisting machine, and a winder, (1) a mechanical detection method using a dropper mechanism, (2) a piezoelectric element or a microswitch is used. A method such as an electric detection method using (3) a photoelectric detection method using a light emitting / receiving element has been put into practical use.
しかしながら、上記(1)および(2)の機械的探知方
法や電気的探知方法にあっては、何れも監視対象物であ
る糸にコンタクト部材を接触させねばならぬため、必然
的に糸の強度・張力による制約を受け、細い糸や伸縮性
に富んだ糸、あるいは静止ている糸をサーチするのに不
適であるという難点があった。However, in the mechanical detection method and the electrical detection method of the above (1) and (2), the contact member must be brought into contact with the thread that is the object to be monitored, and thus the strength of the thread is inevitable. -There was a problem that it was unsuitable for searching thin yarns, highly stretchable yarns, or stationary yarns due to the constraint of tension.
他方、上記(3)の光電探知方法に関しては、投光素子
から受光素子に向けて照射されるビームを横切る物体が
あるか否かによって糸の有無をサーチする直射受光方式
のものと、投光素子から糸路に向けて投光し、其処から
帰還してくる反射光の増減変化によって糸の有無をサー
チする反射受光方式のものとがあり、何れも高速応答性
に秀れ、しかも無接触でサーチするので低張力糸や伸縮
糸にでも対応できるという利点があるのではあるが、こ
れにしても、次のような難点があった。On the other hand, regarding the photoelectric detection method of the above (3), there is a direct light receiving method that searches for the presence or absence of a yarn by whether or not there is an object that crosses the beam emitted from the light projecting element toward the light receiving element, and the light projecting method. There is a reflective light receiving system that projects light from the element to the yarn path and searches for the presence or absence of the yarn by increasing or decreasing the reflected light that returns from there, both of which have excellent high-speed response and are non-contact. Since there is an advantage that it can be applied to low-tension yarns and stretchable yarns as well, there are the following difficulties.
即ち、その難点とは、前者の直射受光方式に関しては、
糸路全幅をサーチするのに多数の投・受光素子を必要と
するうえに、回路構成が複雑にならざるを得ないという
ことであり、 後者の反射受光方式に関しては、一対の投・受光素子で
糸路全幅をカバーできるものゝ、細い糸で、しかも振動
のない静止糸に対しては、投光量に応ずる糸からの反射
光量が少ないために受光量の絶対量を増幅して検出する
という構成を採らざるを得ない関係上、直流結合増幅手
段によって増幅することを余儀無くされ、その結果、温
度ドリフト等の原因で直流結合増幅手段の0点がずれ易
くなり、糸の反射光量が少ない場合には当該出力のずれ
が反射光量によるものなのか、それともドリフトによる
ものかといった区別が付きにくゝなる。このために検出
回路に特別の補正機構を付加することが必要となり、結
局、回路全体が複雑化してしまうということである。That is, the difficulty is that with respect to the former direct light receiving system,
This means that a large number of light emitting / receiving elements are required to search the entire width of the yarn path, and the circuit configuration must be complicated. Regarding the latter reflection / light receiving method, a pair of light emitting / receiving elements is used. It is possible to cover the entire width of the yarn path with a thin thread, and for a static thread that does not vibrate, the absolute amount of the received light is amplified and detected because the amount of reflected light from the yarn depending on the amount of light emitted is small. Due to the fact that the configuration must be adopted, amplification is inevitably performed by the DC coupling amplifying means, and as a result, the 0 point of the DC coupling amplifying means tends to shift due to temperature drift and the like, and the amount of light reflected by the yarn is small. In this case, it is impossible to distinguish whether the output shift is due to the amount of reflected light or due to drift. For this reason, it is necessary to add a special correction mechanism to the detection circuit, and eventually the entire circuit becomes complicated.
本発明は、高速応答性に富み、かつ、1つの投・受光素
子に対するサーチ幅の広い反射受光型の光電探知方法の
サーチ精度を向上せしめることを技術的課題とするもの
である。It is a technical object of the present invention to improve the search accuracy of a reflection-light receiving type photoelectric detection method which is rich in high-speed response and has a wide search width for one light emitting / receiving element.
即ち、本発明は、投受光関係における光量の大きさが
“光源からの距離の2乗に逆比例する”という「距離逆
2乗の法則」を利用したもので、これを2つの投光素子
L1・L2を使った場合の第1図(模式図)を参照して説明
すれば: 糸の通るべき糸路を、異なる距離に配置された同一照明
出力の投光素子L1・L2から逐次交代的に照明する一方、
前記投光素子L1・L2の照明による前記各糸からの各々の
反射光を受光素子Eにて受光し、これら反射光のレベル
差により糸路における糸の有無をサーチするようにした
ものであり、糸路に糸が存在する場合には、前記投光素
子L1と糸との距離r1が投光素子L2と糸との距離r2よりも
短いため距離逆2乗の法則により、前記投光素子L1の照
明による糸からの反射光のレベルが前記投光素子L2の照
明による糸からの反射光レベルよりも大きくなり、従っ
て2つの反射光のレベル差が一定の基準値よりも大きく
現われ、逆に糸路に糸が存在しない場合には前記レベル
差は基準値に達しないことになる。That is, the present invention utilizes the "law of inverse square of distance" in which the magnitude of the light quantity in the light-transmitting / receiving relationship is "inversely proportional to the square of the distance from the light source".
A description will be given with reference to FIG. 1 (schematic diagram) when L 1 and L 2 are used: The light emitting elements L 1 and L having the same illumination output and arranged at different distances in the yarn path through which the yarn should pass. While illuminating from 2 in turn,
A light receiving element E receives the reflected light from each of the yarns by the illumination of the light projecting elements L 1 and L 2 , and the presence or absence of the yarn in the yarn path is searched by the level difference between the reflected light. , and the if there is a yarn in the yarn path, the light projecting element L 1 and the law distance r 1 is short for the distance inverse square than the distance r 2 between the light projecting element L 2 and the thread of the thread As a result, the level of the light reflected from the yarn by the illumination of the light projecting element L 1 becomes higher than the level of the light reflected from the yarn by the illumination of the light projecting element L 2 , so that the level difference between the two reflected light is constant. It appears larger than the reference value, and conversely, when there is no yarn in the yarn path, the level difference does not reach the reference value.
なお、上記説明においては異なる距離に投光素子L1・L2
を設置した場合について挙げているけれども、投光素子
L1・L2を一点からの距離が等しい同一円周上に配置する
場合にあっては投光素子L1・L2の照明出力を違えること
によっても、また3つ以上の投光素子L1・L2・L3…Lnを
用いることによって反射光のレベル差が生じない「等距
離ライン上の盲点」(blindspot)をなくすることも可
能である。In the above description, the light projecting elements L 1 and L 2 are placed at different distances.
Although it mentions about the case where the
When L 1 and L 2 are arranged on the same circumference with the same distance from one point, it is also possible to use three or more light emitting elements L by changing the illumination output of the light emitting elements L 1 and L 2. It is also possible to eliminate the "blindspot" on the equidistant line where the level difference of the reflected light does not occur by using 1 · L 2 · L 3 ... L n .
以下、本発明を添附図面に示す実施例に基いて更に詳し
く説明する。Hereinafter, the present invention will be described in more detail with reference to the embodiments shown in the accompanying drawings.
第1図は本発明方法の模式図、第2図は本発明方法を実
施する実施例システムの概要図、第3図はタイミングチ
ャート図であって、A例に列挙される信号ラインは”糸
有り信号”、B例に列挙される信号ラインは”糸無し信
号”を示す。なお、第3図(a)は光電出力増幅器3に
おける出力波形、同図(b)は微分器4における出力波
形、同図(c)は微分値信号増幅器5における出力波
形、同図(d)は比較器6における出力波形、同図
(e)はリトリガー8における出力波形を表わす。FIG. 1 is a schematic diagram of the method of the present invention, FIG. 2 is a schematic diagram of an embodiment system for carrying out the method of the present invention, FIG. 3 is a timing chart diagram, and the signal lines listed in Example A are “threads”. The signal line enumerated in the “present signal” and the example B indicates the “no thread signal”. 3 (a) is an output waveform in the photoelectric output amplifier 3, FIG. 3 (b) is an output waveform in the differentiator 4, FIG. 3 (c) is an output waveform in the differential signal amplifier 5, and FIG. Shows the output waveform in the comparator 6, and FIG. 8E shows the output waveform in the retrigger 8.
第2図において、符号1は緯糸ガイドリングを示してお
り、同一の照明出力を有する投光素子L1・L2、および受
光素子Eが当該ガイドリング1の周りに内方に向けて配
設されている。なお、ガイドリング1の内部空間に符号
Yで指示される物体は緯糸である。また、本実施例にお
ける糸路は、投光素子L1の形成する照射スペースと投光
素子L2の形成する照射スペースとがオーバーラップする
範囲(φ・χ・ψ・ω)内にして、L1・L2の等距離ライ
ンP−Pを含まない(α・β・φ・χ・ω)で囲われる
領域、または(α・β・ψ)で囲われる領域に設定して
ある(第1図参照)。In FIG. 2, reference numeral 1 denotes a weft guide ring, and the light projecting elements L 1 and L 2 and the light receiving element E having the same illumination output are arranged inward around the guide ring 1. Has been done. The object designated by the symbol Y in the inner space of the guide ring 1 is a weft. Further, the yarn path in this embodiment is set within a range (φ · χ · ψ · ω) in which the irradiation space formed by the light projecting element L 1 and the irradiation space formed by the light projecting element L 2 overlap, It is set to the area surrounded by (α, β, φ, χ, ω) or the area surrounded by (α, β, ψ) that does not include the equidistant line PP of L 1 and L 2 . (See Figure 1).
符号2で指示するものは切換回路であって、電源Pから
供給される直流電気を電圧調節器VR1・VR2を介して投光
素子L1またはL2に瞬時交代的に供給する。Reference numeral 2 indicates a switching circuit, which supplies DC electricity supplied from the power source P to the light projecting element L 1 or L 2 via the voltage regulators VR 1 and VR 2 instantaneously and alternately.
また、符号3で指示するものは、反射光を光電変換する
受光素子Eの光電出力信号を増幅する光電出力増幅器、
4は微分器、5は微分値信号増幅器、6は比較器、7は
シキイ値設定器、8はリトリガーである。Indicated by reference numeral 3 is a photoelectric output amplifier that amplifies the photoelectric output signal of the light receiving element E that photoelectrically converts the reflected light,
Reference numeral 4 is a differentiator, 5 is a differential signal amplifier, 6 is a comparator, 7 is a value setting device, and 8 is a retrigger.
ところで、前記投光素子L1・L2により逐次交代的に照射
される照明光は糸路に存する糸Yに反射して受光素子E
に入射されるが、この場合におけるL1およびL2に対応す
る受光素子Eの受光量は光学上の距離逆2乗則(B=1/
r2:たゞし、Bは照度、rは光源との距離)に支配され
る。いま、仮に第1図において、L2と糸Yとの距離r
2が、L1と糸Yとの距離r1の2倍の値であるとするなら
ば、糸Yを照明するL2による明るさはL1による照明の1/
4となり、受光素子Eが受ける反射光量にも、それに応
じた大きなレベル差が生ずる。したがって、受光素子E
による光電出力信号は、上記投光素子L1・L2と糸Yとの
距離に支配されてレベル変化する振幅波形として現われ
ることになるのであり(第3図のA列(a)に示す)、
糸路に糸Yが存在しない場合には振幅する波形の光電出
力は発生されない(第3図のB列(a)に示す)。By the way, the illumination light sequentially and alternately emitted by the light projecting elements L 1 and L 2 is reflected by the yarn Y existing in the yarn path and is received by the light receiving element E.
The incident light quantity of the light receiving element E corresponding to L 1 and L 2 in this case is the optical distance inverse square law (B = 1 /
r 2 : However, B is controlled by the illuminance and r is the distance from the light source. Now, suppose that in FIG. 1, the distance r between L 2 and the thread Y is
If 2 is twice the distance r 1 between L 1 and the yarn Y, the brightness of L 2 illuminating the yarn Y is 1 / l of the illumination of L 1.
4, the amount of reflected light received by the light receiving element E also has a large level difference. Therefore, the light receiving element E
The photoelectric output signal by means of appears as an amplitude waveform whose level changes depending on the distance between the light projecting elements L 1 and L 2 and the yarn Y (shown in column A (a) of FIG. 3). ,
When the yarn Y does not exist in the yarn path, the photoelectric output having an oscillating waveform is not generated (shown in the column B (a) of FIG. 3).
次いで、この光電出力信号は光電出力増幅器3で増幅さ
れて微分器4に入力され、其処で微分されて振幅波形の
レベル差を量的な微分値信号として出力する。なお、本
実施例においては、便宜上微分波形が「正」の場合につ
いてのみ説明しておく(第3図のA列(b)参照)。Next, this photoelectric output signal is amplified by the photoelectric output amplifier 3 and input to the differentiator 4, where it is differentiated and the level difference of the amplitude waveform is output as a quantitative differential value signal. In this embodiment, for convenience, only the case where the differential waveform is "positive" will be described (see column A (b) of FIG. 3).
この微分値信号は、さらに微分値信号増幅器5に入力さ
れて必要なレベルに増幅され、比較器6へ送致される
(第3図のA列(c)参照)。他方、シキイ値設定器7
からは、予じめ設定されたシキイ値に応ずるレベルのシ
キイ値信号が比較器6に送致されており(第3図のA・
B列において点線sで示す)、当該比較器6において前
記微分値信号とシキイ値信号とが比較される。そして、
微分値信号の値がシキイ値信号の値よりも大きいときに
“糸有り信号”を出力してリトリガー8へ入力するので
あり(第3図のA列(d)参照)、逆に微分値信号の値
がシキイ値信号の値よりも小さいときに“糸無し異常信
号"abを出力してリトリガー8へ入力することになる
(第3図のB列(d)参照)。しかして、この”糸無し
信号"abが一定時間以上継続してリトリガー8に入力さ
れたときに、このリトリガー8は停止信号stを出力して
当該織機を停止せしめることになるのである(第3図の
B列(e)参照)。なお、上記実施例においては、切換
回路2による切換時間はリトリガー8の停止信号発生待
機時間よりも短く設定しておくものとする。この場合、
切換回路2による切換時間は短くすればするほどサーチ
時間密度が高くなるのであるが、1mm/s〜10mm/s程度の
時間幅で問題はない。This differential value signal is further input to the differential value signal amplifier 5, amplified to a required level, and sent to the comparator 6 (see column A (c) of FIG. 3). On the other hand, shiki value setter 7
From FIG. 3, a shiki value signal having a level corresponding to the preliminarily set shiki value is sent to the comparator 6 (A in FIG. 3).
(Indicated by a dotted line s in column B), the differential value signal and the squeeze value signal are compared in the comparator 6. And
When the value of the differential value signal is larger than the value of the shiki value signal, the "thread present signal" is output and input to the retrigger 8 (see column A (d) of Fig. 3), and conversely the differential value signal. When the value of is smaller than the value of the shiki value signal, the "thread absence abnormality signal" ab is output and input to the retrigger 8 (see column B (d) of FIG. 3). When the "no-thread signal" ab is continuously input to the retrigger 8 for a certain period of time or longer, the retrigger 8 outputs a stop signal st to stop the loom (third part). (See column B (e) of the figure). In the above embodiment, the switching time of the switching circuit 2 is set shorter than the stop signal generation standby time of the retrigger 8. in this case,
The shorter the switching time by the switching circuit 2, the higher the search time density, but there is no problem with the time width of about 1 mm / s to 10 mm / s.
第4図は、本発明方法を実施する他の探知システム例で
ある。この実施例システムは3個の投光素子のうち、1
個の投光量を調節して糸路を照明する場合を示したもの
であり、投光素子L2・L3の投光出力を同一とし、投光素
子L1は投光出力が調節されて前記L2・L3よりも低く設定
してある。FIG. 4 is an example of another detection system for carrying out the method of the present invention. In this embodiment, one of the three light projecting elements is used.
This shows the case of illuminating the yarn path by adjusting the light emitting amount of each piece, and the light emitting outputs of the light emitting elements L 2 and L 3 are the same, and the light emitting output of the light emitting element L 1 is adjusted. It is set lower than the above L 2 and L 3 .
いま、第4図の実施例システムにおいて、投光素子L1と
L2との等距離ラインP1−P1、投光素子L1とL3との等距離
ラインP2−P2、投光素子L2とL3との等距離ラインP3−P3
が互いにクロスする交叉点上に糸Yが来たとすると、本
実施例システムでは投光素子L1の投光出力が他の投光素
子L2・L3より低くしてあるので受光素子Eが受光する光
量レベル変動は、光電出力増幅器3においては第5図の
A列(a)に示す通りとなる。なお、このシステム例に
おける信号処理は、第2図の場合と同様に、光電出力増
幅器3、微分器4、微分値信号増幅器5を経由して出力
される微分値信号を比較器6においてシキイ値信号と比
較するというシステムにより為すものとし、比較器6に
よる”糸無し信号"abの出力が一定時間以上継続したと
きリトリガー8は停止信号stを出力することになるので
ある。この場合、前記投光素子L1・L2・L3の切換時間幅
(L1L2L3と切換えてゆく1サイクル)を、リトリガ
ー8の停止信号発生待機時間の幅よりも短く設定すべき
ことは云うまでもない。Now, in the embodiment system of FIG. 4, the light projecting element L 1
Equidistance P 1 -P 1 and L 2, equidistant lines P 3 -P 3 with equidistance P 2 -P 2, the light emitting element L 2 and L 3 between the light projecting element L 1 and L 3
Assuming that the yarn Y comes to the crossing point where the two cross each other, the light emitting output of the light emitting element L 1 is lower than that of the other light emitting elements L 2 and L 3 in the system of this embodiment. In the photoelectric output amplifier 3, the fluctuation of the received light amount level is as shown in the column A (a) of FIG. In the signal processing in this system example, as in the case of FIG. 2, the differential value signal output via the photoelectric output amplifier 3, the differentiator 4, and the differential value signal amplifier 5 is processed by the comparator 6 as a skew value. The retrigger 8 outputs a stop signal st when the output of the "thread-free signal" ab by the comparator 6 continues for a certain period of time or more. In this case, the switching time width of the light projecting elements L 1 , L 2 , L 3 (one cycle of switching to L 1 L 2 L 3 ) is set shorter than the width of the stop signal generation standby time of the retrigger 8. Needless to say.
第6図は本発明方法を実施する他の緯糸探知システム例
である。この実施例システムでは、距離逆2乗の法則を
利用して糸の有無をサーチできない領域、つまり投光素
子L1からの距離と、投光素子L2からの距離とが等しい等
距離ラインP−Pの延長線上にサブ投光素子L3を設置
し、このサブ投光素子L3にて当該ラインP−Pに沿って
受光素子Eへ向け補助的に照明しておき、前記サブ投光
素子L3による受光素子Eの受光量が一定の基準値より急
激に減少した状態を等距離ラインP−P上に“糸有り”
と補完的に検出するのであり、恰も、本発明方法に従来
周知の直射受光探知方法を組み合わせたような態様とな
る。なお、このシステム例における信号処理は、第2図
の場合と同様光電出力増幅器3、微分器4、微分値信号
増幅器5を経由して出力される微分値信号を比較器6で
シキイ値信号と比較するというシステムにて行うものと
し、比較器6による“糸無し信号"abの出力が一定時間
以上継続したときリトリガー8は停止信号stを出力す
る。FIG. 6 is an example of another weft detection system for carrying out the method of the present invention. In this example system, by using the distance inverse-square law can not search the existence of yarn region, i.e. the distance from the light projecting element L 1, the distance are equal equidistant line P from the light emitting element L 2 It established a sub-light projecting element L 3 on the extension of -P, leave supplementary illuminated toward the light receiving elements E along with the sub-light projecting element L 3 to the line P-P, the sub-light projecting When the amount of light received by the light-receiving element E by the element L 3 is drastically reduced from a certain reference value, "thread is present" on the equidistant line PP.
In addition, the method of the present invention is combined with a conventionally known direct light reception detection method. In the signal processing in this system example, the differential value signal output via the photoelectric output amplifier 3, the differentiator 4, and the differential value signal amplifier 5 is converted into a false value signal by the comparator 6 as in the case of FIG. It is assumed that the comparison is performed by a system, and the retrigger 8 outputs a stop signal st when the output of the “thread-free signal” ab by the comparator 6 continues for a certain time or longer.
以上実施例をもって説明したとおり、本発明方法におい
ては、少なくとも2つ以上の投光素子から糸路を逐次交
代的に照明するという手段を採用したことにより、各投
光素子の照明によって糸から反射される反射光との間に
明確なレベル差が生じ、このため、糸路における糸の有
無によって受光素子が発生する光電出力信号の波形に明
確な変化が現われる。As described above with reference to the embodiments, in the method of the present invention, the means for illuminating the yarn path alternately from at least two light projecting elements is employed. A clear level difference is generated between the reflected light and the reflected light, which causes a clear change in the waveform of the photoelectric output signal generated by the light receiving element depending on the presence or absence of the yarn in the yarn path.
したがって、本発明方法によれば、この受光素子による
光電出力信号を監視するだけで糸路における糸の有無を
高精度にサーチできるのである。Therefore, according to the method of the present invention, the presence / absence of the yarn in the yarn path can be searched with high accuracy only by monitoring the photoelectric output signal from the light receiving element.
このように本発明方法は、従来反射受光タイプの糸探知
方法の利点をそのまゝ継承しながらも、糸サーチ感度に
ついては飛躍的に向上するのに加え、これを実施する場
合におけるコストは従来の光電探知方法と殆ど変わらな
い等、その実用上のメリットは頗る大と云える。As described above, the method of the present invention, while inheriting the advantages of the conventional reflection / reception type yarn detection method, dramatically improves the yarn search sensitivity, and the cost for implementing the method is conventionally reduced. It can be said that the practical merit is almost the same as that of the photoelectric detection method described in 1.
第1図は本発明方法の模式図、第2図はジェットルーム
における緯糸貯留装置と噴射ノズルとの間に介装される
緯糸ガイドリングに本発明方法を適用した場合の緯糸探
知システムの概要図、第3図は投光素子を2個使用した
実施例システムにおけるタイミングチャート図、第4図
は投光素子を3個使用した実施例システムの模式図、第
5図は第4図の実施例システムにおけるタイミングチャ
ート図、第6図は更に他の緯糸探知システム例を示した
概要図である。 L1・L2・L3〜Ln……投光素子、E……受光素子、VR1・V
R2・VR3〜VRn……電圧調節器。FIG. 1 is a schematic diagram of the method of the present invention, and FIG. 2 is a schematic view of a weft detection system when the method of the present invention is applied to a weft guide ring interposed between a weft storage device and a jet nozzle in a jet loom. FIG. 3 is a timing chart diagram of an embodiment system using two light emitting elements, FIG. 4 is a schematic view of an embodiment system using three light emitting elements, and FIG. 5 is an embodiment of FIG. FIG. 6 is a timing chart in the system, and FIG. 6 is a schematic diagram showing still another example of the weft detection system. L 1 / L 2 / L 3 to L n …… Emitting element, E …… Receiving element, VR 1・ V
R 2 · VR 3 ~VR n ...... voltage regulator.
───────────────────────────────────────────────────── フロントページの続き (51)Int.Cl.6 識別記号 庁内整理番号 FI 技術表示箇所 G01V 8/20 ─────────────────────────────────────────────────── ─── Continuation of the front page (51) Int.Cl. 6 Identification code Internal reference number FI technical display location G01V 8/20
Claims (3)
の投光素子(L1・L2…Ln)から逐次交代的に照明する一
方、 前記投光素子(L1・L2…Ln)の照明による前記糸からの
各々の反射光を受光素子(E)にて受光し、これらの反
射光のレベル差により糸の有無をサーチするようにした
ことを特徴とする糸の探知方法。1. A yarn path through which a yarn passes is illuminated alternately from at least two or more light projecting elements (L 1 , L 2 ... L n ) while the light projecting elements (L 1 , L 2 ) are sequentially illuminated. Ln ) each reflected light from the yarn by the illumination is received by the light receiving element (E), and the presence or absence of the yarn is searched by the level difference between these reflected lights. Detection method.
1つを、電圧調節器(VR1・VR2・VR3…VRn)の何れかの
調節によって光量調節するようにした請求項1記載の、
糸の探知方法。2. The light quantity of at least one of the light projecting elements (L 1 , L 2 ... L n ) is adjusted by adjusting any of the voltage regulators (VR 1 , VR 2 , VR 3 ... VR n ). According to claim 1,
Thread detection method.
1つを、設置距離を異にすることによって光量加減した
請求項1記載の、糸の探知方法。3. The yarn detecting method according to claim 1, wherein at least one of the light projecting elements (L 1 · L 2 ... L n ) is adjusted in amount of light by making the installation distance different.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP60263522A JPH0766059B2 (en) | 1985-11-22 | 1985-11-22 | Thread detection method |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP60263522A JPH0766059B2 (en) | 1985-11-22 | 1985-11-22 | Thread detection method |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS62123385A JPS62123385A (en) | 1987-06-04 |
| JPH0766059B2 true JPH0766059B2 (en) | 1995-07-19 |
Family
ID=17390706
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP60263522A Expired - Lifetime JPH0766059B2 (en) | 1985-11-22 | 1985-11-22 | Thread detection method |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0766059B2 (en) |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH02271280A (en) * | 1989-04-13 | 1990-11-06 | Stanley Electric Co Ltd | Optical object detection device |
Family Cites Families (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5821132B2 (en) * | 1977-06-29 | 1983-04-27 | 株式会社神崎高級工機製作所 | Traveling speed control device for agricultural tractors, etc. |
| JPS5969979U (en) * | 1982-11-01 | 1984-05-12 | 石原 順太郎 | Photoelectric warp break detection device for looms |
-
1985
- 1985-11-22 JP JP60263522A patent/JPH0766059B2/en not_active Expired - Lifetime
Also Published As
| Publication number | Publication date |
|---|---|
| JPS62123385A (en) | 1987-06-04 |
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