JPH0157164B2 - - Google Patents
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- Publication number
- JPH0157164B2 JPH0157164B2 JP13212882A JP13212882A JPH0157164B2 JP H0157164 B2 JPH0157164 B2 JP H0157164B2 JP 13212882 A JP13212882 A JP 13212882A JP 13212882 A JP13212882 A JP 13212882A JP H0157164 B2 JPH0157164 B2 JP H0157164B2
- Authority
- JP
- Japan
- Prior art keywords
- flow tube
- yarn
- coagulation bath
- bath
- spinning
- 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
Links
- 238000009987 spinning Methods 0.000 claims description 30
- 238000000034 method Methods 0.000 claims description 27
- 230000001133 acceleration Effects 0.000 claims description 4
- 230000001112 coagulating effect Effects 0.000 claims description 4
- 239000007788 liquid Substances 0.000 claims description 3
- 230000015271 coagulation Effects 0.000 description 55
- 238000005345 coagulation Methods 0.000 description 55
- 230000000704 physical effect Effects 0.000 description 14
- 230000007547 defect Effects 0.000 description 5
- 229920000297 Rayon Polymers 0.000 description 4
- 238000004519 manufacturing process Methods 0.000 description 4
- 238000007796 conventional method Methods 0.000 description 3
- 230000000052 comparative effect Effects 0.000 description 2
- BASFCYQUMIYNBI-UHFFFAOYSA-N platinum Chemical compound [Pt] BASFCYQUMIYNBI-UHFFFAOYSA-N 0.000 description 2
- 238000011160 research Methods 0.000 description 2
- 239000007921 spray Substances 0.000 description 2
- 238000011144 upstream manufacturing Methods 0.000 description 2
- 239000003513 alkali Substances 0.000 description 1
- 238000013459 approach Methods 0.000 description 1
- 229920002678 cellulose Polymers 0.000 description 1
- 239000001913 cellulose Substances 0.000 description 1
- 230000003247 decreasing effect Effects 0.000 description 1
- 238000001514 detection method Methods 0.000 description 1
- 238000005553 drilling Methods 0.000 description 1
- 238000011156 evaluation Methods 0.000 description 1
- 230000002349 favourable effect Effects 0.000 description 1
- 239000012530 fluid Substances 0.000 description 1
- 239000011521 glass Substances 0.000 description 1
- 230000005484 gravity Effects 0.000 description 1
- 230000010355 oscillation Effects 0.000 description 1
- 229910052697 platinum Inorganic materials 0.000 description 1
- 238000012805 post-processing Methods 0.000 description 1
- 238000005086 pumping Methods 0.000 description 1
- 239000002964 rayon Substances 0.000 description 1
- 230000002123 temporal effect Effects 0.000 description 1
- 238000002166 wet spinning Methods 0.000 description 1
Landscapes
- Artificial Filaments (AREA)
- Spinning Methods And Devices For Manufacturing Artificial Fibers (AREA)
Description
本発明は湿式紡糸方法による糸条製造におい
て、改善された上向流浴紡糸方法に関するもので
ある。
ビスコースをはじめとする湿式紡糸可能な紡糸
原液は、紡糸口金を通して凝固浴中に吐出され、
凝固せしめられた後、浴中より引き出されて糸条
として形成され、必要に応じて後処理を施されて
製品糸となる。
従来より、生産性を上げるための紡糸速度の高
速化に関し、凝固浴を紡糸された糸条の走行方向
と同一方向に流動せしめる流浴紡糸方法が種々提
案されており、例えばビスコース法によるレーヨ
ン糸の製造方法においては、特公昭27−4931号公
報に記載の紡糸方法が良く知られている。更に例
えば、特公昭30−8866号公報、特公昭31−5963号
公報、特公昭34−6058号公報、特公昭38−3956号
公報に記載されている如き上向流浴紡糸方法が提
案されており、設備のスペース生産性が向上する
点、又特にビスコース法レーヨン糸の紡糸では、
紡糸中に発生するガスが紡糸口金表面に集積しな
いという点から、好ましい方向に改善されてい
る。
しかしながら従来提案されている上向流浴紡糸
方法にあつてはいずれも、工業的に、とりわけ高
速紡糸において、原糸の物性値を良好な水準に維
持せしめ、かつ物性値の斑を極度に減少せしめ、
かつ糸切れ、毛羽等の工程欠点を大幅に減少せし
める条件を同時に満足する方法はいまだ見出され
ていない。
例えば、特公昭31−5963号公報或いは特公昭34
−6058号公報或いは特公昭38−3956号公報では、
流管出口より流出する凝固浴を流管外径より大き
な溢流受槽に受け、或いは流管出口に向つて徐々
に連続的に流管内径を増大し、或いは流管出口付
近の流管に凝固浴流出孔を穿つことにより、流管
出口付近の凝固浴流速が急激に減少し、未だ半凝
固状態にある糸条に急激な浴抵抗を加える。又更
に、流管出口付近での該浴抵抗ベクトルは、糸条
の走行方向以外の種々の方向に複雑に分布し、か
つその向きは刻々変化するために、未だ半凝固状
態にある糸条は、複雑に動揺せしめられる。従つ
て、いまだ繊弱な単糸の半凝固表面は、急激な浴
抵抗変化により微細な損傷を生じ、或いは単糸が
複雑に動揺することにより延伸斑を生じ、紡糸工
程において糸切れ、毛羽等の工程欠点を発生し、
更に後処理工程を終えた製品糸条の物性値、とり
わけ乾伸度、湿伸度、ヤング率、収縮率等の伸縮
特性の低下及び斑を生じる。
又例えば、特公昭30−8866号公報に記載の方法
では、流管を出た凝固浴は一旦空中に噴き上げら
れた後溢流受槽に入るため、凝固浴流速の急激な
減少は回避し得るが、凝固浴が流管出口以降で垂
直に噴き上げられているために、噴き上げられた
凝固浴の頂点の高さ及び方向が時間と共に刻々変
動し、やはり半凝固状態にある糸条は、凝固糸条
が噴き上げ凝固浴頂点を通過する際の複雑な動揺
の影響を受け、延伸斑を生じ、かくて製品糸条の
物性値、とりわけ伸縮特性の斑を生じる。該方法
において、噴き上げられた凝固浴頂点の高さ及び
方向の時間的変動を抑えるためには、噴き上げる
長さを減じれば良いが、噴き上げ長の減少はとり
も直さず凝固浴流速の低下であり、即ち浴抵抗が
増大し満足な物性値を得ることが出きなくなる。
本発明者らは、従来法で克服し得なかつた上記
欠点を解決すべく鋭意研究の結果、上向きに凝固
浴を流動せしめるに際し、その流動方向が極めて
重要である事を見い出し、本発明に到達したもの
である。
即ち、本発明は垂線に対し5乃至20度の傾き角
度(Θ)をもつて流管を設け、かつ凝固液が流管
内の流速(V)によつて流管出口から円柱状にて
該流管の傾き方向に向つて空中に下記の式で表わ
される有限の長さ(H)噴き上げられていることを特
徴とする上向流浴紡糸方法である。
H=V2/(2g cosΘ)
(但し、gは重力加速度を表わす。)
本発明の方法によれば、原糸の物性値を良好な
水準に維持せしめ、かつ物性値の斑を極度に減少
せしめ、かつ糸切れ毛羽等の工程欠点を大幅に減
少せしめられ、とりわけ高速紡糸において有用で
ある。
本発明の実施態様の一例を第1図に示す。本発
明を第1図によつて詳細に説明する。
紡糸原液は紡糸原液導入管4を経て、紡糸口金
支持体5に設置されている紡糸口金6を通して、
凝固浴導入管2を導入されてきた凝固浴中に吐出
され半凝固糸条7を形成しつつ、地表に対する垂
線に対して5乃至20度の傾き角度を有して設けら
れた流管8の内部を凝固浴と共に通過し、流管出
口から第1図に示すように円柱状にて該流管8の
傾き方向に向つて、空中にH=V2/(2g cosΘ)
(但し、gは重力加速度を表わす。)で表わされる
有限の長さ(H)噴き上げられている。噴き上げ凝固
浴9中を通過する間に完全に凝固せしめられた
後、該噴き上げ凝固浴9の頂点に達して、凝固糸
条10となり必要に応じて後処理を施こされるべ
く引き取られる。
本発明において、噴き上げ凝固浴9を空中に有
限の長さ(H)噴き上げせしめた理由は下記の如くで
ある。即ち、地表に対する垂線11と流管の傾き
線12とがなす角度をθとすると、流管8の内部
を糸条の進行方向に流速Vで通過する凝固浴は、
該流管8の出口から流管内の流速と等しい流速V
で押し出される。その後初等力学で良く知られる
ように、重力加速度をgとすると、
H=V2/(2g cosθ)
なる長さHまで噴き上げられ、噴き上げ凝固浴の
頂点で流速が0となり落下を開始する。従つて、
流管8の出口を通過する時点でいまだ完全に凝固
を完了していない糸条は、凝固を完了すべく噴き
上げ凝固浴9の頂点に至るまでの間に、単位時間
内に走行した距離の1/2乗に比例する極めて緩慢
な速度の減少、即ち極めて緩慢な浴抵抗(外力)
の増加のみを経験するにとどまる。更に該噴き上
げ凝固浴の速度減少率は流管出口に近い程緩やか
なので、即ち、糸条の凝固度合が相対的に低い領
域では外力増加は小さく、糸条の凝固が充分にな
るにつれて外力増加が大きくなる。従つて糸条
は、表面の凝固が不充分な領域では該表面に加わ
る外力が小さいために、半凝固表面の損傷及び延
伸斑を生じ難く、一方大きな外力が加わる領域に
あつては、糸条の凝固が充分に進行しているため
にもはや大きな表面損傷及び延伸斑を生じないと
いう、極めて合理的な工程を経る。更に紡糸速度
を高速にする程、良好な物性値の水準を維持する
にあたつて流管内の流速を上げる必要が生じるの
で、糸条が上記工程を経ることがより有利かつ必
要となるのは明らかである。
本発明にいう凝固浴が流管出口から円柱状にて
該流管の傾き方向に向つて、空中に有限の長さ(H)
噴き上げられていること、とは上記現象を発現さ
せるための基本的な原理であり、連続して均一な
断面積を有する流管を通過した凝固浴の流速を、
該流管に連らねて設けられた該流管の断面積より
も大きい断面積を有する例えば、溢流受槽、或い
は先に進むに従つて断面積の増大するロート管、
或いは穿孔流管等を設けることによつて、流管よ
り流出した凝固浴をいわゆるオーバーフローにて
溢流させることにより、急激に減少せしめること
のない凝固浴流出方法であり、流管もしくは流管
に接続して連らなり、かつ凝固浴の流入している
部品の出口から、糸条の進行方向に向つて更に有
限の長さの噴き上げ凝固浴を有するものを指す。
意図的な噴き上げ浴の長さは、紡糸速度、所望す
る物性値の水準もしくは流管内の凝固浴の流速の
設定値によつて定められるべきものである。又、
凝固浴を流管出口から円柱状にて空中に有限の長
さ(H)噴き上げるためには凝固浴を何らかの方法で
加圧することが必要であり、例えば凝固浴をポン
プで強制送液するか、もしくはヘツド圧によつて
噴き出させることが好ましい。
しかしながら、有限の長さ(H)凝固浴の噴き上げ
を設けるだけではまだ、物性値の斑を製品糸条の
使用に際して全く支障のない水準にまで到達せし
めることは困難である。従来提案されている上向
流浴紡糸方法においても、凝固浴を上向きに流動
せしめる概念はあるが、この技術だけでは、実用
上充分に均質な製品糸条を得ることは不可能に近
い。なぜならば、噴き上げ凝固浴を地表に対して
垂直に噴き上げた場合には、噴き上げ凝固浴に作
用する重力、浴速度、糸条走行等の変動が複雑に
影響を及ぼし合い、その結果噴き上げ凝固浴の頂
点の高さ及び方向、即ち頂点位置が時間と共に
刻々変動する。該現象は身近な例では公園等の噴
水の垂直な噴き上げの場合に容易に観察されるも
のである。従つて噴き上げ方式による上向流浴紡
糸方法にあつては、噴き上げ凝固浴頂点の位置変
動を抑制し延伸斑を極度に減少せしめるために流
管が地表に対する垂線11に対して傾き角度を有
して設けられ、かつその方向に向けて凝固浴が噴
き上げられていることが必要である。本発明者ら
の詳細にわたる研究の結果では、傾き角度θが5
乃至20の範囲にあることが必要である。θが小さ
すぎる場合には前述の如く噴き上げ凝固浴9の頂
点位置が定まりにくく、糸条に加えられる張力が
大きさ、向き共に大きく変動し、製品糸条の物性
値、とりわけ乾伸度、湿伸度、ヤング率、収縮率
等の伸縮特性の斑を糸長方向に沿つて生じ易くな
り、一方該角度θが大きすぎる場合には、錘当り
の設備スペースが増大するために設備生産性が低
下し、又、必要な作業領域も大となり紡出作業が
頻雑となり、工業的規模での製造がやや難かしく
なる。更に噴き上げ凝固浴の頂点の幅が拡がりか
つ絶えず変動するようになり、更に又、噴き上げ
凝固浴中を走行する糸条に対して凝固浴の落下に
よる外力が加わり始め糸条の滑らかな走行が保障
され難くなる。
従つて、噴き上げ凝固浴の頂点の位置変動を抑
制し、延伸斑を極度に減少せしめ、更に工業的規
模での製造が容易になるためには、傾き角度を有
して流管を設け、かつその方向に向けて凝固浴を
噴き上げることが必要であり、更に好ましいの
は、傾き角度θが5乃至20度の範囲にあることで
ある。
このように、本発明は地表に対する垂線に対し
傾き角度を有して流管を設け、かつ凝固浴が流管
出口から流管内の流速にて流管の傾き方向に向か
つて、空中に意図的に噴き上げられていることを
特徴とする上向流浴紡糸方法によつて、原糸の物
性値を良好な水準に維持せしめ、かつ物性値の斑
を極度に減少せしめ、更に糸条表面の損傷や延伸
斑がないために、糸切れ、毛羽等の工程欠点を大
幅に減少せしめた製品糸条が、工業的規模で、と
りわけ高速紡糸の際に、安定し、かつ容易に製造
できる。
以下本発明を実施例をもつて説明するが、本発
明は下記の実施例に限られるものではない。
実施例 1
通常の方法にて製造したセルロース濃度8.0重
量%、アルカリ濃度5.5重量%のビスコースを、
通常の方法にて製造したH2SO4150g/、
Na2SO4280g/、ZnSO415g/の52℃の凝
固浴中に、第1図に示した紡糸方法にて200m/
分の紡糸速度にて120デニールの糸を紡糸した。
紡糸口金は0.06mmφ×26ホール(白金製)、流管
は内径5mm、長さ100mmのガラス管を用いた。凝
固紡糸は糸道、ローラーを経て遠心ポツトに捲き
取り、通常の後処理を施こして製品フイラメント
にした。
流管の傾き角度θを0乃至25度、凝固浴噴上げ
長Hを100乃至500mmの範囲で変化させた際の、糸
切れ発生回数(回/錘・日)、及びワーパー型毛
羽検知法により測定した毛羽発生数(個/106m)
を各々第1表及び第2表に示す。更に物性値を代
表するものとして、ウースター社製連続強伸度測
定装置(Type96)を用い、100mに亘つて連続し
て1m毎に糸条の乾伸度を測定した。流管の傾き
角度θ、凝固浴噴き上長Hを変化せしめた時の糸
条の乾伸度の平均値及び標準偏差値σを第3表
に示す。
The present invention relates to an improved upflow bath spinning method for producing yarn by a wet spinning method. A spinning dope that can be wet-spun, including viscose, is discharged into a coagulation bath through a spinneret,
After being coagulated, it is pulled out from the bath and formed into a thread, which is then subjected to post-treatment as required to become a product thread. Conventionally, various fluid bath spinning methods have been proposed in which the coagulation bath is made to flow in the same direction as the running direction of the spun yarn in order to increase the spinning speed to increase productivity. As a method for manufacturing yarn, the spinning method described in Japanese Patent Publication No. 27-4931 is well known. Further, for example, upward flow bath spinning methods have been proposed as described in Japanese Patent Publication No. 30-8866, Japanese Patent Publication No. 5963-1983, Japanese Patent Publication No. 6058-1982, and Japanese Patent Publication No. 38-3956. This improves the space productivity of the equipment, and especially when spinning rayon yarn using the viscose method,
This is a favorable improvement in that the gas generated during spinning does not accumulate on the spinneret surface. However, all of the upstream bath spinning methods that have been proposed so far maintain the physical properties of the raw yarn at a good level and extremely reduce unevenness in the physical properties, especially in high-speed spinning. Seshime,
A method that simultaneously satisfies the conditions of significantly reducing process defects such as thread breakage and fluffing has not yet been found. For example, Special Publication No. 31-5963 or Special Publication No. 34
In Publication No.-6058 or Special Publication No. 38-3956,
The coagulation bath flowing out from the flow tube outlet is received in an overflow receiving tank larger than the flow tube outer diameter, or the flow tube inner diameter is gradually and continuously increased toward the flow tube outlet, or the coagulation bath is coagulated in the flow tube near the flow tube outlet. By drilling the bath outlet hole, the flow rate of the coagulating bath near the outlet of the flow tube is rapidly reduced, and a sudden bath resistance is applied to the yarn, which is still in a semi-coagulated state. Furthermore, the bath resistance vector near the outlet of the flow tube is distributed in a complicated manner in various directions other than the running direction of the yarn, and its direction changes from time to time. , is complicated and unsettling. Therefore, the semi-solidified surface of the still weak single yarn may cause minute damage due to rapid changes in bath resistance, or the complicated movement of the single yarn may cause stretching unevenness, resulting in yarn breakage, fuzz, etc. during the spinning process. process defects occur,
Furthermore, the physical properties of the product yarn after the post-treatment process, particularly the elastic properties such as dry elongation, wet elongation, Young's modulus, and shrinkage rate, deteriorate and unevenness occurs. For example, in the method described in Japanese Patent Publication No. 30-8866, the coagulation bath exiting the flow tube is once blown up into the air and then enters the overflow receiving tank, so a sudden decrease in the flow rate of the coagulation bath can be avoided. Since the coagulation bath is blown up vertically after the outlet of the flow tube, the height and direction of the top of the blown up coagulation bath fluctuate with time, and the yarn, which is still in a semi-solidified state, is not a coagulated yarn. When the yarn passes through the top of the blown coagulation bath, it is affected by complicated oscillations, which causes stretching unevenness, and thus causes unevenness in the physical properties of the product yarn, especially in its elastic properties. In this method, in order to suppress temporal fluctuations in the height and direction of the top of the coagulating bath that is blown up, it is sufficient to reduce the length of the blown up coagulation bath. In other words, the bath resistance increases and it becomes impossible to obtain satisfactory physical property values. As a result of intensive research to solve the above-mentioned drawbacks that could not be overcome with conventional methods, the present inventors discovered that the direction of flow is extremely important when causing a coagulation bath to flow upward, and thus arrived at the present invention. This is what I did. That is, in the present invention, the flow tube is provided with an inclination angle (Θ) of 5 to 20 degrees with respect to the perpendicular line, and the coagulating liquid flows from the flow tube outlet in a cylindrical shape according to the flow velocity (V) in the flow tube. This is an upflow bath spinning method characterized by a finite length (H) expressed by the following formula being sprayed into the air in the direction of inclination of the tube. H=V 2 /(2g cosΘ) (However, g represents gravitational acceleration.) According to the method of the present invention, the physical properties of the yarn can be maintained at a good level, and unevenness in the physical properties can be extremely reduced. It can significantly reduce process defects such as yarn breakage and fluff, and is particularly useful in high-speed spinning. An example of an embodiment of the present invention is shown in FIG. The present invention will be explained in detail with reference to FIG. The spinning dope passes through a spinning dope introduction pipe 4 and a spinneret 6 installed on a spinneret support 5.
The flow tube 8, which is installed at an angle of inclination of 5 to 20 degrees with respect to the perpendicular to the ground surface, is discharged into the coagulation bath introduced through the coagulation bath introduction tube 2 and forms a semi-coagulated thread 7. H=V 2 /(2g cosΘ) in the air, passing through the interior together with the coagulation bath, from the outlet of the flow tube in a cylindrical shape toward the direction of inclination of the flow tube 8, as shown in FIG.
(However, g represents gravitational acceleration.) It is ejected over a finite length (H). After being completely coagulated while passing through the blown-up coagulation bath 9, it reaches the top of the blown-up coagulation bath 9 and becomes a coagulated thread 10, which is taken off to be subjected to post-treatment as required. In the present invention, the reason why the blown-up coagulation bath 9 is blown up into the air over a finite length (H) is as follows. That is, if the angle between the perpendicular 11 to the earth's surface and the inclination line 12 of the flow tube is θ, then the coagulation bath passing through the flow tube 8 in the direction in which the yarn travels at a flow rate of V is
A flow velocity V equal to the flow velocity within the flow tube from the outlet of the flow tube 8
is pushed out. After that, as is well known in elementary mechanics, when the gravitational acceleration is g, the liquid is blown up to a length H of H=V 2 /(2g cosθ), and at the top of the blown-up coagulation bath, the flow velocity becomes 0 and it begins to fall. Therefore,
The yarn, which has not yet completely coagulated at the time of passing through the outlet of the flow tube 8, is blown up to reach the top of the coagulation bath 9 to complete coagulation. A very slow decrease in velocity proportional to /2, i.e. a very slow bath resistance (external force)
will only experience an increase in Furthermore, the speed reduction rate of the blown-up coagulation bath is gradual as it approaches the outlet of the flow tube. That is, in the region where the degree of coagulation of the yarn is relatively low, the increase in external force is small, and as the coagulation of the yarn becomes sufficient, the increase in external force increases. growing. Therefore, in areas where the surface of the yarn is insufficiently coagulated, the external force applied to the surface is small, so damage to the semi-solidified surface and uneven stretching are less likely to occur.On the other hand, in areas where a large external force is applied, the yarn It goes through an extremely rational process in which large surface damage and stretching spots no longer occur because the coagulation has progressed sufficiently. Furthermore, as the spinning speed increases, it becomes necessary to increase the flow rate in the flow tube in order to maintain a good level of physical properties, so it is more advantageous and necessary for the yarn to undergo the above steps. it is obvious. The coagulation bath referred to in the present invention is cylindrical from the flow tube outlet toward the inclination direction of the flow tube, and has a finite length (H) in the air.
Being blown up is the basic principle for producing the above phenomenon.
For example, an overflow receiving tank having a cross-sectional area larger than the cross-sectional area of the flow pipe provided in series with the flow pipe, or a funnel pipe whose cross-sectional area increases as it advances;
Alternatively, by providing a perforated flow tube or the like, the coagulation bath flowing out from the flow tube is caused to overflow in a so-called overflow, thereby preventing the coagulation bath from decreasing rapidly. Refers to a device that is connected in a series and has a blown-up coagulation bath of a finite length in the direction of thread movement from the outlet of the component into which the coagulation bath is flowing.
The intended length of the blow-up bath should be determined by the spinning speed, the desired level of physical properties, or the setpoint of the flow rate of the coagulation bath in the flow tube. or,
In order to spray the coagulation bath up a finite length (H) into the air in a cylindrical shape from the outlet of the flow tube, it is necessary to pressurize the coagulation bath in some way, for example, by forcibly pumping the coagulation bath, Alternatively, it is preferable to blow it out by head pressure. However, it is still difficult to bring the unevenness of physical properties to a level that does not pose any problem when using the product yarn just by providing a jet of coagulation bath of finite length (H). Although the upstream bath spinning method proposed in the past has the concept of causing the coagulation bath to flow upward, it is nearly impossible to obtain a product yarn with sufficient homogeneity for practical use using this technique alone. This is because when the blown-up coagulation bath is blown up perpendicular to the ground surface, variations in gravity acting on the blown-up coagulation bath, bath speed, yarn running, etc. affect each other in a complex manner, resulting in The height and direction of the vertex, that is, the vertex position, changes moment by moment with time. A familiar example of this phenomenon is that it is easily observed in the case of vertical fountains in parks and the like. Therefore, in the upflow bath spinning method using the blow-up method, the flow tube has an inclination angle with respect to the perpendicular line 11 to the ground surface in order to suppress the positional fluctuation of the top of the blow-up coagulation bath and to extremely reduce stretching unevenness. It is necessary that the coagulation bath is spouted in that direction. According to the results of detailed research by the present inventors, the inclination angle θ is 5
It is necessary to be in the range of 20 to 20. If θ is too small, the apex position of the jet coagulation bath 9 will be difficult to determine as described above, and the tension applied to the yarn will vary greatly in magnitude and direction, resulting in poor physical properties of the product yarn, especially dry elongation and wet Unevenness in elastic properties such as elongation, Young's modulus, and shrinkage rate tends to occur along the yarn length direction.On the other hand, if the angle θ is too large, equipment space per weight increases, resulting in equipment productivity. Moreover, the necessary working area becomes large, the spinning operation becomes frequent, and production on an industrial scale becomes somewhat difficult. Furthermore, the width of the apex of the blown-up coagulation bath expands and constantly fluctuates, and furthermore, external force due to the falling coagulation bath begins to be applied to the yarn running in the blown-up coagulation bath, ensuring smooth running of the yarn. It becomes difficult to be treated. Therefore, in order to suppress the fluctuation in the position of the apex of the blown-up coagulation bath, to extremely reduce stretching unevenness, and to facilitate production on an industrial scale, it is necessary to provide a flow tube with an inclined angle and It is necessary to spray the coagulation bath in that direction, and more preferably the inclination angle θ is in the range of 5 to 20 degrees. As described above, the present invention provides a flow tube having an inclination angle with respect to the perpendicular to the ground surface, and the coagulation bath is directed from the outlet of the flow tube in the direction of the inclination of the flow tube at the flow velocity within the flow tube, so that the coagulation bath is intentionally suspended in the air. The upflow bath spinning method, which is characterized by the fact that the yarn is blown up, maintains the physical properties of the raw yarn at a good level, extremely reduces unevenness in the physical properties, and also prevents damage to the yarn surface. Since there is no unevenness or drawing unevenness, the product yarn can be produced stably and easily on an industrial scale, especially during high-speed spinning, with greatly reduced process defects such as yarn breakage and fuzz. The present invention will be explained below with reference to examples, but the present invention is not limited to the following examples. Example 1 Viscose with a cellulose concentration of 8.0% by weight and an alkali concentration of 5.5% by weight, produced by a conventional method,
150g of H 2 SO 4 produced in the usual way,
In a coagulation bath of 280 g of Na 2 SO 4 and 15 g of ZnSO 4 at 52°C, a spinning method of 200 m/
A 120 denier yarn was spun at a spinning speed of 120 min.
The spinneret was 0.06 mmφ x 26 holes (made of platinum), and the flow tube was a glass tube with an inner diameter of 5 mm and a length of 100 mm. The coagulated and spun yarn passed through a thread path and rollers, was wound up into a centrifugal pot, and was subjected to standard post-processing to form a product filament. Based on the number of thread breakages (times/weight/day) and the warper-type fluff detection method when the inclination angle θ of the flow tube was varied from 0 to 25 degrees and the coagulation bath jet length H was varied from 100 to 500 mm. Measured number of fluff (pieces/10 6 m)
are shown in Tables 1 and 2, respectively. Furthermore, as a representative physical property value, the dry elongation of the yarn was continuously measured every 1 m over 100 m using a continuous strength and elongation measuring device (Type 96) manufactured by Wooster. Table 3 shows the average value and standard deviation value σ of the dry elongation of the yarn when the inclination angle θ of the flow tube and the top length H of the coagulation bath were varied.
【表】【table】
【表】【table】
【表】【table】
【表】
比較例 1
第1図で示した流管8の出口に連続して内径50
mmの円筒形の溢流受槽を設け、流管出口より20mm
の高さにて凝固浴を溢流させた他は、実施例1と
全く同様にして、流管の傾き角度θを0及び12度
にした際の、実施例1でのH=100、300、500mm
に相当する5mmφ流管部分の流内流速にて紡糸及
び評価を行なつた。該流速は比較し易い様に以下
の表では相当H長として表示する。糸切れ発生回
数(回/錘・日)及び毛羽発生数(個/106m)
を各々第4表及び第5表に乾伸度の平均値及び標
準偏差値を第6表に示す。[Table] Comparative Example 1 Continuously connected to the outlet of the flow tube 8 shown in Fig. 1, the inner diameter
A cylindrical overflow receiving tank of mm is provided, 20 mm from the flow pipe outlet.
H=100, 300 in Example 1 when the inclination angle θ of the flow tube was set to 0 and 12 degrees, except that the coagulation bath was overflowed at the height of . ,500mm
Spinning and evaluation were performed at a flow rate within the flow tube section of 5 mmφ corresponding to . The flow rate is expressed as the equivalent H length in the table below for easy comparison. Number of thread breakages (times/weight/day) and number of fuzz occurrences (pieces/10 6 m)
are shown in Tables 4 and 5, respectively, and Table 6 shows the average and standard deviation values of dry elongation.
【表】【table】
【表】【table】
【表】
以上の実施例1及び比較例1より、本発明にな
る上向流浴紡糸方法が従来法に比して、極めて工
程欠点が少なく、また実用上充分に均質な、かつ
格段に優れた製品糸条を供するものであることは
明白である。[Table] From the above Example 1 and Comparative Example 1, it is clear that the upflow bath spinning method of the present invention has extremely few process defects, is sufficiently homogeneous for practical use, and is significantly superior to the conventional method. It is clear that the product is intended to provide a product yarn with a high quality.
第1図は本発明の実施の一例を示す縦断面図で
ある。
1は凝固浴導入の方向、2は凝固浴導入管、3
は紡糸原液導入の方向、4は紡糸原液導入管、5
は紡糸口金支持体、6は紡糸口金、7は半凝固糸
条、8は流管、9は噴き上げ凝固浴、10は凝固
糸条、11は地表に対する垂線、12は流管の傾
き線を示す。
FIG. 1 is a longitudinal sectional view showing an example of the implementation of the present invention. 1 is the direction of coagulation bath introduction, 2 is the coagulation bath introduction pipe, 3
is the spinning dope introduction direction, 4 is the spinning dope introduction tube, and 5 is the spinning dope introduction tube.
is a spinneret support, 6 is a spinneret, 7 is a semi-coagulated thread, 8 is a flow tube, 9 is a blow-up coagulation bath, 10 is a coagulated thread, 11 is a line perpendicular to the ground surface, and 12 is an inclination line of the flow tube. .
Claims (1)
つて流管を設け、かつ凝固液が流管内の流速
(V)によつて流管出口から円柱状にて該流管の
傾き方向に向つて空中に下記の式で表わされる有
限の長さ(H)噴き上げられていることを特徴とする
上向流浴紡糸方法。 H=V2/(2g cosΘ) (但し、gは重力加速度を表わす。)[Claims] 1. A flow tube is provided with an inclination angle (Θ) of 5 to 20 degrees with respect to the perpendicular line, and the coagulating liquid is cylindrical from the flow tube outlet due to the flow velocity (V) in the flow tube. An upflow bath spinning method characterized in that a finite length (H) expressed by the following formula is spouted into the air in the direction of inclination of the flow tube. H=V 2 /(2g cosΘ) (However, g represents gravitational acceleration.)
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP13212882A JPS5926509A (en) | 1982-07-30 | 1982-07-30 | Spinning in upward counter flow bath |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP13212882A JPS5926509A (en) | 1982-07-30 | 1982-07-30 | Spinning in upward counter flow bath |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5926509A JPS5926509A (en) | 1984-02-10 |
| JPH0157164B2 true JPH0157164B2 (en) | 1989-12-04 |
Family
ID=15074044
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP13212882A Granted JPS5926509A (en) | 1982-07-30 | 1982-07-30 | Spinning in upward counter flow bath |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS5926509A (en) |
Families Citing this family (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2603971B2 (en) * | 1987-11-09 | 1997-04-23 | 旭化成工業株式会社 | Flow tube wet spinning method |
| EP2392700B1 (en) * | 2010-04-28 | 2012-06-20 | Teijin Aramid B.V. | Process for spinning graphene ribbon fibers |
-
1982
- 1982-07-30 JP JP13212882A patent/JPS5926509A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5926509A (en) | 1984-02-10 |
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