JPS588112A - Method of measuring the boiled extent of cocoons - Google Patents

Method of measuring the boiled extent of cocoons

Info

Publication number
JPS588112A
JPS588112A JP56104826A JP10482681A JPS588112A JP S588112 A JPS588112 A JP S588112A JP 56104826 A JP56104826 A JP 56104826A JP 10482681 A JP10482681 A JP 10482681A JP S588112 A JPS588112 A JP S588112A
Authority
JP
Japan
Prior art keywords
cocoon
waveform
boiling
wave
boiled
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.)
Granted
Application number
JP56104826A
Other languages
Japanese (ja)
Other versions
JPS5836085B2 (en
Inventor
Chiyuki Takabayashi
高林千幸
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.)
NORIN SUISANSYO SANSHI SHIKENJIYOU
Original Assignee
NORIN SUISANSYO SANSHI SHIKENJIYOU
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 NORIN SUISANSYO SANSHI SHIKENJIYOU filed Critical NORIN SUISANSYO SANSHI SHIKENJIYOU
Priority to JP56104826A priority Critical patent/JPS5836085B2/en
Publication of JPS588112A publication Critical patent/JPS588112A/en
Publication of JPS5836085B2 publication Critical patent/JPS5836085B2/en
Expired legal-status Critical Current

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  • Investigating Or Analyzing Materials By The Use Of Ultrasonic Waves (AREA)
  • Investigating Strength Of Materials By Application Of Mechanical Stress (AREA)

Abstract

PURPOSE:A shock wave is applied to a point on the trunk of a boiled cocoon and the damping oscillation is examined on its waveform characteristics at another point in a certain distance to give accurate information on the boiled extent of the cocoon simply. CONSTITUTION:A boiled cocoon is set in a prescribed position and a shock wave S1 is applied to a point of its trunk and the damping oscillation S2 is examined at another point in a certain distance on its characteristics such as the leading amplitude X1 of S2, logarithmic damping factor, showing the damping of S2, (it is defined by the equation where n means the n-th wave of S2 and Xn is the amplitude of the n-th wave), the frequency of S2 and the difference between its level before leading and convergent one h to evaluate the boiled extent of the cocoon.

Description

【発明の詳細な説明】 本発明は、面の煮熟状態を知るためにその粘弾性的特性
に着目して、瞬時にその特性値を求めるぺ〈計測を行う
面の煮熟度計測方法に関するものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a method for measuring the degree of boiling of a surface by focusing on its viscoelastic properties and instantly obtaining the characteristic values in order to know the degree of boiling of the surface. It is something.

一般の製糸工場の煮繭工程に於−ては、煮繭前に、与え
られた原料面の性状を把握する職出機構を有していない
ため、原料面に適した煮繭条件モチめ決めることは難し
く、成る条件を設定して煮繭を行い、然る後に繰糸を行
った結果から知られる生糸収率、生産能率、生糸品質等
によって表わされる生産情報を基として、煮繭機に於け
る温度、蒸気量、煮繭時間等を制御するという、所謂試
行、錯誤的な方法によって適正な煮繭条件を見い出して
いる。
In the cocoon-cocoon boiling process of a general silk mill, there is no system for determining the properties of the given raw material before cocoon-cocoon boiling, so the cocoon-cocoon boiling conditions suitable for the raw material are determined. However, it is difficult to set the conditions to boil cocoons, and then reel the silk.Based on the production information expressed by the raw silk yield, production efficiency, raw silk quality, etc., the cocoon boiling machine is Appropriate cocoon boiling conditions are found through a trial and error method of controlling the cocoon temperature, steam volume, cocoon boiling time, etc.

このよう罠煮繭された繭は繰糸しなければ煮熟状態が判
らないため、最適な煮繭条・件を見い出すには、かなり
の時間遅れを生じることKなる〇特に原料面の性状の異
なる不荷口面を続け、て煮繭するような場合、成る荷口
面の生産情報を把握した時には、別荷口面を煮繭しなけ
ればならな−と−うことが起こり、斯かる場合には、原
料面の性状に適した煮繭条件を見−出すことは困難であ
った。
Since the ripeness of the cocoons that have been trap-boiled in this way cannot be determined unless they are reeled, it takes a considerable amount of time to find the optimal cocoon-cocoon boiling conditions, especially when the raw materials have different properties. In the case where the non-consignment side is continued and cocooned, when the production information of the consignment side is grasped, a separate consignment side must be cocooned, and in such a case, It was difficult to find cocoon boiling conditions suitable for the properties of the raw material.

そこで煮繭工程にお−て、過速〈面の煮熟状態、を知る
ために、技術者は長年の経験と勘により煮上がった面の
色相、指答で圧縮した時の硬さ、弾力などで感覚的に判
定していたが、更に面の煮唱状St的確に計測する手法
の開発が望まれていた。
Therefore, in the cocoon boiling process, in order to know the overspeed (boiled state of the cocoon), technicians use their years of experience and intuition to determine the hue of the cocoon, the hardness and elasticity when compressed according to instructions. However, it has been desired to develop a method to more accurately measure the boiling shape of the surface.

本発明は的確且つ迅速に、しかも取扱いの容易な面の煮
熟度情報を得る方法1に提供することをその目的とする
もので、煮熟面を定位置にセットシ、その胴部の一点に
衝撃力を与え、その応答波として生ずる繭層の減衰振動
波を衝撃力を与えた点より一定間隔離れたところで検出
し、該減衰振動波の波形の立上りの大きさxl、対数減
衰率δ、応答開演1 t 1誼波形の立ち上がりレベル
と収束レベルの差り等の骸波形の幹性値によって面の煮
熟状St計測評価することを特徴とする。
The purpose of the present invention is to provide a first method for obtaining boiling level information of a surface accurately and quickly, and which is easy to handle. Applying an impact force, detecting the damped vibration wave of the cocoon layer generated as a response wave at a certain distance from the point where the impact force was applied, and determining the rise size xl of the waveform of the damped vibration wave, the logarithmic damping rate δ, Response start 1 t 1 It is characterized by measuring and evaluating the boiling state of the surface based on the stemness value of the skeleton waveform, such as the difference between the rise level and the convergence level of the waveform.

以下本発明の実施例を図面につ禽説明する。Embodiments of the present invention will be explained below with reference to the drawings.

第1図は衝撃応答特性による面の煮熟度計測方法を実施
するための装置のプ四ツク図を示す。
FIG. 1 shows a schematic diagram of an apparatus for carrying out a method for measuring the degree of boiling of a surface based on impact response characteristics.

第1図示の装置は、煮熟繭へ衝撃波を与えるための振動
子を駆動する部分と煮熟繭からの応答波管検出し、記録
・表示する部分7−に分かれる。
The apparatus shown in the first figure is divided into a part for driving a vibrator for applying a shock wave to the cooked cocoon, and a part for detecting, recording and displaying the response wave tube from the cooked cocoon.

即ち、前者はパルス信号発生器ムよりパルス信号を出力
し、増幅器Bにて該パルス信号を増幅し、振動子OKよ
り電気的なパルス信号を機械力に変換して第2図f4)
K示すような波形の衝撃力を繭層コに与える機構にして
振動子Cに入力するパルス波の大きさは記録計nにて記
録できる機能を有する。一方に於いて後者は、繭層へ与
叉る衝撃力の入力点から一定間隔、例えば10閤離れた
ところで繭層を伝播する応答波を検出し、その波形を記
憶及び表示する機能を有するものである。つまり検出器
mKて応答波を検出した後、増幅器IKて増幅し、波形
記憶装置Gに波形をいったん記憶させる。これは応答波
である減衰振動波が瞬時にして起こ抄、その11オシロ
グラフ等へ波形を描かせても解析困難なため波形記憶装
置Gに波形を記憶させ、然る後に緩速度で再生して解析
し易いようにするためである。本実施例に於いて使用し
た波形記憶装置Gは、アナログ信号を任意のタイ々ング
でサンプリングし、ム/D変換11.にて8ビツトのデ
ィジタル信号に変換し、8ビツトX 1024ワードの
メモリーに記憶するものである。この実施結果によれば
検出された波形が8ビツトのディジタル信号に゛変換さ
れても、その原形1殆んど変えることなく再生できる仁
とが確認された。こうして応答波を波形記憶装置Gに記
憶さ(、然る後にオシpスコープR管面上に応答波管表
示させるとともに記録計xK該波形様Sを記録させる。
That is, in the former case, a pulse signal is output from a pulse signal generator, the pulse signal is amplified by an amplifier B, and the electrical pulse signal is converted into mechanical force by a vibrator OK (Fig. 2 f4).
It has a mechanism that applies an impact force having a waveform as shown in K to the cocoon layer, and has a function of recording the magnitude of the pulse wave input to the vibrator C with a recorder n. On the other hand, the latter has the function of detecting a response wave propagating through the cocoon layer at a fixed interval, for example, 10 meters away from the input point of the impact force acting on the cocoon layer, and storing and displaying the waveform. It is. That is, after the response wave is detected by the detector mK, it is amplified by the amplifier IK, and the waveform is temporarily stored in the waveform storage device G. This is because a damped oscillatory wave, which is a response wave, is generated instantaneously, and it is difficult to analyze even if the waveform is drawn on an oscilloscope, etc., so the waveform is stored in the waveform storage device G and then played back at a slow speed. This is to make it easier to analyze. The waveform storage device G used in this embodiment samples the analog signal at arbitrary timing and performs the M/D conversion 11. The signal is converted into an 8-bit digital signal and stored in a memory of 8 bits x 1024 words. According to the results of this experiment, it has been confirmed that even if the detected waveform is converted into an 8-bit digital signal, it can be reproduced without changing its original form. In this way, the response wave is stored in the waveform storage device G (and then the response waveform is displayed on the oscilloscope R screen and the waveform S is recorded on the recorder xK.

次に、第2図(ロ)に示す応答波形の解析方法に就いて
説明すれば、煮熟面に衝撃力を与えた時の応答mmをオ
シシスコープHまたは記録計Iにより観察すると、第2
図(ロ)に示すような減衰振動曲線を描く0面の煮熟状
1lIt若煮から老煮へ移行させることにより減衰振動
曲線の形態が成る一定の傾向に従って変化することが知
られたので、第2開−)に示す減衰振動波形を端的に表
現するため、次に示す特性値によって評価する方法を案
出した。即ち、■波形の立上がり振幅の大きさXl、■
波形の減衰状態を表わす対数滅ジー 衰率δ!ニー1ogs、九だしnは減衰振動曲線1k 
       !II の%nサイクル目を示し、ZSはnサイクル目の振幅の
大きさを示す。■波形の周波数f、■波形の立ち上がり
レベルと収束レベルとの差りである。
Next, to explain the method for analyzing the response waveform shown in Fig. 2 (b), when the response mm when an impact force is applied to the boiling surface is observed using an oscilloscope H or a recorder I, the second
It is known that the form of the damped oscillation curve changes according to a certain tendency by transitioning from simmered to aged simmered on the 0 side, which draws a damped oscillation curve as shown in Figure (b). In order to clearly express the damped vibration waveform shown in 2nd opening-), we devised a method of evaluation using the following characteristic values. That is, ■ The magnitude of the rising amplitude of the waveform Xl, ■
Logarithmic decay rate δ that represents the attenuation state of the waveform! Knee 1ogs, nine dashes n is damped vibration curve 1k
! %nth cycle of II is shown, and ZS shows the magnitude of the amplitude of the nth cycle. (2) Frequency f of the waveform; (2) Difference between the rising level and convergence level of the waveform.

このように面の煮熟状St表わす特性値として前記■〜
■で評価したが、面の煮熟状態変化による諸特性値の変
化傾向を簡潔に要約すれば、繭が着意から老煮に移行す
ることにより波形の立ち上がりの大きさX、は大吉〈な
り・、波形がはやく減衰する状態となって、煮熟面に永
久歪が生ずるようKなる。即ち対数減衰率′−は大きく
なり、波形の立ち上がりレベルと収束レベルとの差、所
謂煮熟面の永久歪を寥すh#大きくなる。一方、波形の
周波数fは低くなる傾向を示す・ このような傾向は、一般にモデル的にあられされる粘弾
性体に於ける傾向と同等であるか歪か゛検討するため、
粘弾性体モデルの挙動を示す微分方程式を組み立て電子
計算機によりシミュレ−シ■ンを行ったところ、粘弾性
体の応答波形と実際に煮熟繭KRvhて計測した結果と
はその傾向が一致し、本計測方−法の信憑性が裏付けら
れた。
In this way, as the characteristic value representing the cooked state St of the surface, the above-mentioned ■ ~
As evaluated in section 2, to briefly summarize the tendency of changes in various characteristic values due to changes in the state of boiling of the surface, as the cocoon transitions from simmering to stale, the magnitude of the rise in the waveform, X, becomes Daikichi. , the waveform rapidly attenuates, and the temperature reaches K such that permanent distortion occurs on the boiling surface. That is, the logarithmic attenuation rate '- increases, and the difference between the rising level and the convergence level of the waveform, h#, which causes permanent distortion of the boiling surface, increases. On the other hand, the frequency f of the waveform shows a tendency to become lower. In order to examine whether such a tendency is equivalent to the tendency in viscoelastic bodies that is generally modeled,
When a differential equation representing the behavior of the viscoelastic body model was assembled and a simulation was performed using an electronic computer, the tendency of the response waveform of the viscoelastic body and the results actually measured using boiled cocoons KRvh was found to be consistent. The credibility of this measurement method was confirmed.

而して本計測装置によ秒得られる煮熟面の応答波形の特
性値は、成る一定の傾向を−って変化しているため、煮
熟状態を判定する場合前記■〜■に示す4特性値の1つ
に着目してその変化を把えても良いし、適煮状態の応答
波形パターンと計測結果を比較検討することによっても
煮熟状態を判定出来る。
Since the characteristic values of the response waveform of the boiling surface obtained by this measuring device change according to a certain tendency, when determining the boiling state, it is necessary to The cooked state can be determined by focusing on one of the characteristic values and understanding its change, or by comparing and examining the response waveform pattern of the properly cooked state and the measurement results.

かくして煮繭直後に於いて従来指頭での圧縮線等によっ
て判定してきた面の煮熟状態t−瞬発的に生ずる応答波
形の特性値として把えることが可能で、また波形記憶装
置を、波形を記憶し尚且つ即座に諸特性値を演算出来る
!イクロコンピュータ等と置換することにより過速〈応
答波形の解析が出来る。尚、本計測装置は煮繭前に原料
繭特性を把握するために、繭層の硬さ、緊緩状態等の繭
層構造を知ることに一適用し得るものである。
In this way, immediately after cocooning, it is possible to grasp the boiling state t of the surface, which has conventionally been determined by the compression line with the fingertip, as a characteristic value of the response waveform that occurs instantaneously, and also to store the waveform in the waveform storage device. You can memorize and calculate various characteristic values instantly! By replacing it with a microcomputer, etc., it is possible to analyze the overspeed response waveform. This measuring device can be applied to the cocoon layer structure, such as the hardness of the cocoon layer and its state of relaxation, in order to understand the characteristics of raw cocoons before boiling them.

このように゛本発明の方法によれば、煮繭後に面の煮熟
状at−特性値として的確に掌握出来るため、電子計算
機による最適煮繭システムを構築するにあたり、有効な
る情報を提供する手法となり得る効果を有する。
As described above, according to the method of the present invention, since it is possible to accurately grasp the boiling state of the surface after cocoon boiling as the characteristic value, it is a method of providing effective information when constructing an optimal cocoon cocoon boiling system using an electronic computer. It has the potential to be effective.

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

第1図は、本発明の方法を実施するための装置のプルツ
ク図を示す。 第2図(イ)は煮熟繭へ付与する衝撃波・の波形、第2
開−)は該衝撃波によって生ずる減衰振動波形管示す。 ム・・・パルス信号発生器   B、XP・・・増 幅
 器0・・・振動子  D、工・・・記録計重・・・検
 出 器   G・・・波形、記憶装置H・・・オシリ
スコープ  J・・・煮 熟 繭手続補正書C自発2 昭和 g〜8月10  日 特許庁長官殿 1、事件の表示 昭和56年特許願第104・26号 2、発明の名称 衝撃応答特性による面の煮熟度計測方法3、補正をする
者 事件との関係   特許出願人 Wi場長間和夫 4、代 理 人 収 補正の対象 明細書の”「発明の名称工発明の詳細な説明」の各欄 7111正°の内容 11)  明細書の「発明の名称」を「衝撃応答特性に
よる面の煮熟度計測方法」と補正する。 (2)  明細書第2頁第20行「指笛」を「指頭」と
補正する。 (3)同書第4頁第9行「繭層−を伝播する」を「該」
と補正する。 (5)  同書第6頁第2行rX11Jを「X惰」と補
正する@ (6)  同書第6頁第18行「歪」を「否」と補正す
る。
FIG. 1 shows a pull diagram of an apparatus for carrying out the method of the invention. Figure 2 (a) shows the waveform of the shock wave applied to the boiled cocoon.
Open-) shows a damped vibration corrugated tube caused by the shock wave. M...Pulse signal generator B, Oscilloscope J...Mature Cocoon Procedural Amendment C Spontaneous Issue 2 Showa g~August 10th, Mr. Commissioner of the Japan Patent Office 1, Indication of the case, Patent Application No. 104/26 of 1982, 2, Name of the invention: Based on impact response characteristics Method for measuring the degree of ripeness of a surface 3, relationship with the case of the person making the amendment Patent applicant Wi Ba Nagama Kazuo 4, agent Personal income ``Detailed explanation of the invention in the name of the invention'' in the specification to be amended Contents of each column 7111 correct degree 11) The "title of the invention" in the specification is corrected to "method for measuring the degree of boiling of a surface using impact response characteristics." (2) "Finger whistle" on page 2, line 20 of the specification is amended to read "finger tip." (3) "Propagate through the cocoon layer" in line 9 of page 4 of the same book as "applicable"
and correct it. (5) Correct rX11J, page 6, line 2 of the same book, to “X inertia” @ (6) Correct “distortion”, line 18, page 6 of the same book, to “no”.

Claims (1)

【特許請求の範囲】[Claims] 煮m1t一定位置にセットし、その胴部の一点に衝撃力
を与え、その応答波として生ずる繭層の減衰振動波を衝
撃力管与えた点よ抄−走間隔離れたところで検出し、該
減衰振動波の波形の立上りの大きさxl、対数減衰率a
、応応答波波数、該波形の立ち上がりレベルと収束レベ
ルの差り等の腋波形の特性値によって面の煮熟状態を計
測評価することを特徴とする面の煮熟度計測方法。
An impact force is applied to one point on the body of the boiling m1t, and the damped vibration wave of the cocoon layer generated as a response wave is detected at a distance from the point where the impact force was applied. The magnitude of the rising edge of the waveform of the vibration wave xl, the logarithmic damping rate a
A method for measuring the degree of boiling of a surface, characterized in that the state of boiling of the surface is measured and evaluated based on characteristic values of an axillary waveform, such as the wave number of a response wave and the difference between the rising level and the convergence level of the waveform.
JP56104826A 1981-07-04 1981-07-04 Method for measuring cocoon ripeness using shock response characteristics Expired JPS5836085B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP56104826A JPS5836085B2 (en) 1981-07-04 1981-07-04 Method for measuring cocoon ripeness using shock response characteristics

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP56104826A JPS5836085B2 (en) 1981-07-04 1981-07-04 Method for measuring cocoon ripeness using shock response characteristics

Publications (2)

Publication Number Publication Date
JPS588112A true JPS588112A (en) 1983-01-18
JPS5836085B2 JPS5836085B2 (en) 1983-08-06

Family

ID=14391189

Family Applications (1)

Application Number Title Priority Date Filing Date
JP56104826A Expired JPS5836085B2 (en) 1981-07-04 1981-07-04 Method for measuring cocoon ripeness using shock response characteristics

Country Status (1)

Country Link
JP (1) JPS5836085B2 (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0636378B2 (en) * 1984-08-24 1994-05-11 バ−ンデイ・コ−ポレ−シヨン Conductive contact

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0636378B2 (en) * 1984-08-24 1994-05-11 バ−ンデイ・コ−ポレ−シヨン Conductive contact

Also Published As

Publication number Publication date
JPS5836085B2 (en) 1983-08-06

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