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JPS6346165B2 - - Google Patents
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JPS6346165B2 - - Google Patents

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Publication number
JPS6346165B2
JPS6346165B2 JP15583382A JP15583382A JPS6346165B2 JP S6346165 B2 JPS6346165 B2 JP S6346165B2 JP 15583382 A JP15583382 A JP 15583382A JP 15583382 A JP15583382 A JP 15583382A JP S6346165 B2 JPS6346165 B2 JP S6346165B2
Authority
JP
Japan
Prior art keywords
magnetic field
spinning
magnetic
yarn
spinneret
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
Application number
JP15583382A
Other languages
Japanese (ja)
Other versions
JPS5947408A (en
Inventor
Tadashi Konishi
Takatoshi Kuratsuji
Tsutomu Kiryama
Kazumi Ookawa
Katsuo Kunugi
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.)
Teijin Ltd
Original Assignee
Teijin Ltd
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 Teijin Ltd filed Critical Teijin Ltd
Priority to JP15583382A priority Critical patent/JPS5947408A/en
Publication of JPS5947408A publication Critical patent/JPS5947408A/en
Publication of JPS6346165B2 publication Critical patent/JPS6346165B2/ja
Granted legal-status Critical Current

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  • Spinning Methods And Devices For Manufacturing Artificial Fibers (AREA)

Description

【発明の詳細な説明】 本発明は紡糸装置に関するものである。その目
的とするところは、磁界によつて紡出糸条の分子
配向に影響を与え、紡出糸条の分子配向を制御す
るための紡糸装置を提供することにある。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a spinning device. The object thereof is to provide a spinning device for controlling the molecular orientation of the spun yarn by influencing the molecular orientation of the spun yarn using a magnetic field.

従来より、人造繊維を製造するには、まず紡糸
工程で分子配向のあまり進行していない未延伸糸
を得、次いでこの未延伸糸を延伸、熱処理して配
向、結晶化させる方法がとられている。
Traditionally, in order to produce man-made fibers, the method has been to first obtain undrawn yarn with little molecular orientation in the spinning process, and then draw and heat treat the undrawn yarn to orient and crystallize it. There is.

近年になつて、紡糸速度を3000〜4000m/分と
いう比較的高速度にとり、比較的配向度の高い部
分配向糸(POY)とした後、わずかな延伸と仮
撚とを同時に行なう方法(POY−DTY加工法)
が企業化され始めている。
In recent years, a method has been developed in which the spinning speed is set to a relatively high speed of 3000 to 4000 m/min to produce partially oriented yarn (POY) with a relatively high degree of orientation, and then a slight stretching and false twisting are performed simultaneously (POY- DTY processing method)
is beginning to be commercialized.

更に最近においては、後工程における延伸処理
が不要である高配向糸を一段で得ようとして、捲
取速度が5000m/分以上の超高速紡糸が研究され
ている。
Furthermore, recently, ultrahigh-speed spinning with a winding speed of 5000 m/min or more has been studied in an attempt to obtain highly oriented yarn in one step that does not require drawing treatment in the post-process.

しかし、これらの高速紡糸及び超高速紡糸法に
おいて得られる繊維の、全体としての分子の配向
はかなりの水準にまで到達するが、非晶部の分子
の乱れは、従来の未延伸糸を延伸して得られた繊
維よりも大きくなる傾向がわかつて来た。
However, although the overall molecular orientation of the fibers obtained by these high-speed spinning and ultra-high-speed spinning methods reaches a considerable level, the molecular disorder in the amorphous portion makes it difficult to draw conventional undrawn yarn. There has been a tendency for the fibers to be larger than those obtained by

一方、通常の溶融紡糸法によつて得た未延伸糸
に大きな張力をかけながら急速に加熱と冷却を繰
り返す、いわゆるゾーン延伸を行ない、高分子の
伸び切り鎖結晶組織からなる高弾性率、高強力繊
維を作製しようという方法がある(例えば繊維学
会誌、第38巻、第6号、第257頁(1982))。この
方法においては、加熱、冷却を繰返す点において
省エネルギー的製糸方法とは言えない。しかも、
ゾーン延伸、ゾーン熱処理された繊維の物性は、
最初の紡糸段階の未延伸糸の配向状態によつて左
右されるという限界がある。
On the other hand, undrawn yarn obtained by the usual melt spinning method is subjected to so-called zone drawing, in which the yarn is rapidly heated and cooled repeatedly while applying a large tension. There is a method for producing strong fibers (for example, Journal of the Japan Institute of Fiber Science, Vol. 38, No. 6, p. 257 (1982)). This method cannot be said to be an energy-saving silk spinning method since heating and cooling are repeated. Moreover,
The physical properties of zone-stretched and zone-heat treated fibers are as follows:
There is a limit that depends on the orientation state of the undrawn yarn at the initial spinning stage.

この様に、紡出糸条の分子配向を制御するとい
うことは、極めて重要な技術となつてきている。
In this way, controlling the molecular orientation of spun yarn has become an extremely important technology.

他方、従来から強い磁界をかけて分子の配向を
制御する技術として、次の如きものが知られてい
る。
On the other hand, the following techniques are conventionally known as techniques for controlling the orientation of molecules by applying a strong magnetic field.

まず、ある種のポリマーが適当な溶媒中で溶液
粘度が数ポアズから数十ポアズの低粘度域にある
時、磁場をかけるとポリマーが一定の方向に配向
することは公知である(例えば繊維学会誌、第35
巻、第11号、第337頁(1979))。この文献中の記
載によると、配向させる高分子の溶液は、一定の
磁界の中で静的状態にあり、長時間(例えば数分
以上)磁界の中でさらされ続けて初めて高分子の
配向が観察されているにすぎない。又、上記文献
に記載されている磁界の強さは、数キロガウスか
らせいぜい25ないし35キロガウスにすぎない。
First, it is known that when a certain type of polymer has a solution viscosity in a low viscosity range of several poise to several tens of poise in an appropriate solvent, the polymer will be oriented in a certain direction when a magnetic field is applied (for example, Magazine, No. 35
Vol. 11, p. 337 (1979)). According to the description in this document, a solution of polymers to be oriented is in a static state in a constant magnetic field, and the polymers are only oriented when exposed to the magnetic field for a long time (for example, several minutes or more). It's just being observed. Further, the strength of the magnetic field described in the above-mentioned literature is from several kilogauss to only 25 to 35 kilogauss at most.

又、液晶性のモノマーを強い磁界の中で静的に
保持し、配向させながら重合すると、配向化され
た高分子が合成できることは公知である(例えば
ジヤーナル・オブ・ポリマーサイエンス、ポリマ
ーレターズエデイシヨン(J.Polym.Sci.,Polym.
Letters Ed.)第13巻、第243頁(1975))。
It is also known that oriented polymers can be synthesized by holding liquid crystalline monomers statically in a strong magnetic field and polymerizing them while oriented (for example, Journal of Polymer Science, Polymer Letters Edition). (J.Polym.Sci., Polym.
Letters Ed.) Volume 13, Page 243 (1975)).

更に高温状態で数百ポアズ以下の中低粘度域に
おいて数分間以上の長い間15キロガウス以下の強
さの磁界をかけてネマチツク液晶を示す高分子を
配向させることが可能であることも公知である
(例えばジヤーナル・オブ・ポリマーサイエンス
(J.Polym.Sci.,Polym.Phys.Ed.)第20巻、第975
頁(1982))。
Furthermore, it is also known that it is possible to orient polymers exhibiting nematic liquid crystal by applying a magnetic field with a strength of less than 15 kilogauss for several minutes or more in a medium-low viscosity range of several hundred poise or less at high temperatures. (For example, Journal of Polymer Science (J.Polym.Sci., Polym.Phys.Ed.) Volume 20, No. 975
(1982)).

しかし、これらの文献に記載されている例は、
いずれも中低粘度状態で静的状態に保持されたも
のに数分間以上もの長い時間にわたつて磁界をか
けて、モノマーや高分子などの配向を制御してい
るものばかりである。
However, the examples described in these documents are
All of these methods control the orientation of monomers, polymers, etc. by applying a magnetic field to a medium-to-low viscosity state that is held static for a long time of several minutes or more.

そこで本発明者らは、人造繊維の紡糸工程で磁
界を働かせることにつき検討を重ねた結果、紡糸
口金から吐出された溶液粘度又は溶融粘度の高い
ポリマー流体に、数秒以内という短時間の間、強
い磁界をかけて、紡出糸条の分子配向を制御しう
る装置を開発することに成功し、本発明に到達し
た。
As a result of repeated studies on applying a magnetic field during the spinning process of artificial fibers, the present inventors discovered that a strong magnetic field can be applied to a polymer fluid with high solution viscosity or melt viscosity discharged from a spinneret for a short period of time, within a few seconds. The present invention was achieved by successfully developing a device that can control the molecular orientation of spun yarn by applying a magnetic field.

即ち、本発明は、一部が互いに対峙するように
屈曲してなる磁性体において、該対峙部分の一方
を紡糸口金とすると共に、該対峙部分の他方に糸
条通過孔を形成せしめ、両対峙部分間で紡出糸条
に対してほぼ平行方向の磁界をかけるようにした
ことを特徴とする紡糸装置である。
That is, in the present invention, in a magnetic body whose parts are bent so as to face each other, one of the facing parts is used as a spinneret, and a thread passing hole is formed in the other of the facing parts, so that both facing parts are bent. This spinning device is characterized in that a magnetic field is applied in a direction substantially parallel to the spun yarn between sections.

以下、本発明を図面により説明する。 Hereinafter, the present invention will be explained with reference to the drawings.

第1図は本発明装置の一例を示すものであり、
1は紡糸パツク、は両端部が互いに対峙するよ
うに屈曲してなる磁性体で、上方端部が紡糸口金
3を構成し、下方端部に紡出糸条Yの通る糸条通
過孔4が形成されている。5,5′は引取ゴデツ
トローラ、6は巻取装置である。紡糸口金3に
は、通常の口金と同じ様に、ポリマーの導入孔7
とオリフイス8とを有しており、ここから吐出さ
れた糸条Yは、引取ゴデツトローラ5,5′によ
り一定の紡糸速度で引取られ、巻取装置6に巻取
られる。
FIG. 1 shows an example of the device of the present invention,
1 is a spinning pack; 2 is a magnetic body bent such that both ends thereof face each other; the upper end constitutes a spinneret 3; the lower end has a yarn passing hole 4 through which the spun yarn Y passes; is formed. 5 and 5' are take-up godet rollers, and 6 is a winding device. The spinneret 3 has a polymer introduction hole 7 like a normal spinneret.
The yarn Y discharged from this is taken up at a constant spinning speed by take-up godet rollers 5, 5', and wound up by a winding device 6.

紡糸パツク1は、通常のパツクと同様フイルタ
ー9,9′や材10等から構成されているが、
材質はいずれも非磁性体(例えば黄銅、アルミニ
ウム、SUS−304−Lなど)である。
The spinning pack 1 is composed of filters 9, 9', material 10, etc., like a normal pack.
All materials are non-magnetic (eg, brass, aluminum, SUS-304-L, etc.).

磁界は紡糸口金3を構成している磁性体2の上
方端部と、糸条通過孔4が形成されている磁性体
2の下方端部の間で発生するが、これは、磁性体
2の中間部11に巻いたコイル12に電源13か
ら電流を流すことによつて行なわれる。
The magnetic field is generated between the upper end of the magnetic body 2 constituting the spinneret 3 and the lower end of the magnetic body 2 where the thread passing hole 4 is formed. This is done by passing current from a power source 13 through a coil 12 wound around the intermediate portion 11.

第2図に、本発明装置における磁界発生部分の
種々の実施態様を示す。
FIG. 2 shows various embodiments of the magnetic field generating portion in the device of the present invention.

まず、紡出糸条Yの走行方向と、磁性体の一
対の磁極(紡糸口金3と糸条通過孔4形成部)の
間で発生する磁界のベクトル方向(図中点線で示
す)との相互関係は、第2図aの如く中間部11
に巻いたコイル12に直流電源13から電流を流
し紡出糸条Yの走行方向と同一方向の磁束線を生
ぜしめる場合もあり、bの如く直流電源13′か
らaの場合とは逆方向の電流を流して、紡出糸条
Yの走行方向と反対方向の磁束線を生ぜしめる場
合もある。又cの如く交流電源13″により、磁
束線の方向を経時的に変化させる場合もある。更
にdの如く、紡出糸条Yの走行方向と磁束線の方
向が45度未満の任意の角度θをなす如く傾いてい
る場合もある。これらはいずれも「紡出糸条に対
して、ほぼ平行方向の磁界をかける」という範疇
に含まれるものである。
First, the running direction of the spun yarn Y and the vector direction of the magnetic field (indicated by the dotted line in the figure) generated between the pair of magnetic poles of the magnetic body 2 (spinneret 3 and yarn passage hole 4 forming part) are The mutual relationship is as shown in FIG.
In some cases, a current is passed from the DC power source 13 to the coil 12 wound around the coil 12 to generate a magnetic flux line in the same direction as the running direction of the spun yarn Y, and as shown in b, a current is applied from the DC power source 13' in the opposite direction to that in case a. In some cases, a current is applied to generate lines of magnetic flux in the direction opposite to the traveling direction of the spun yarn Y. Also, as shown in c, the direction of the magnetic flux lines may be changed over time using an AC power source 13''.Furthermore, as shown in d, the running direction of the spun yarn Y and the direction of the magnetic flux lines may be at any angle less than 45 degrees. In some cases, it is tilted to form an angle θ. All of these fall under the category of ``applying a magnetic field in a substantially parallel direction to the spun yarn.''

一方、磁性体2の中間部11に巻かれるコイル
は、eの如く複数のコイル12,12′,12″に
分割し、それぞれに別個の電源13a,13b,
13cを設けることができる。又、fの如く、分
割された複数のコイル12,12′,12″にそれ
ぞれ電流の方向が異なる直流電源13,13′及
び交流電源13″を接続し各コイル12,12′,
12″に流れる電流の方向を部分的に変えること
も可能である。
On the other hand, the coil wound around the intermediate portion 11 of the magnetic body 2 is divided into a plurality of coils 12, 12', 12'' as shown in e, and each has a separate power source 13a, 13b,
13c can be provided. Further, as shown in f, a DC power source 13, 13' and an AC power source 13'' having different current directions are connected to a plurality of divided coils 12, 12', 12'', respectively.
It is also possible to partially change the direction of the current flowing through 12''.

次に磁場発生装置によつて発生する磁界の強さ
について具体的に説明する。第3図は磁性体芯型
マグネツトによつて発生した磁界の強さと時間と
の関係を示した図である。磁場発生装置の糸条通
路における磁界の強さは、第3図aの如く尚に一
定であつてもよく、bの如く時間と共に変化して
もよい。更にcの如くステツプ状或いは傾向をつ
けて変化してもよい。又、第2図a,b,cの如
く、磁界のベクトル方向を一定方向とする直流磁
界であつてもよく、逆に磁界のベクトル方向が変
化する交番磁界であつてもよい。これらは紡出糸
条の分子配向をどのように制御したいかという目
的に従つて、任意に選択、使用される。
Next, the strength of the magnetic field generated by the magnetic field generator will be specifically explained. FIG. 3 is a diagram showing the relationship between the strength of the magnetic field generated by the magnetic core type magnet and time. The strength of the magnetic field in the thread path of the magnetic field generator may be constant as shown in FIG. 3a, or may vary with time as shown in FIG. 3b. Furthermore, it may change stepwise or with a tendency as shown in c. Further, as shown in FIGS. 2a, b, and c, it may be a direct current magnetic field in which the vector direction of the magnetic field is constant, or alternatively, it may be an alternating magnetic field in which the vector direction of the magnetic field changes. These are arbitrarily selected and used depending on the purpose of controlling the molecular orientation of the spun yarn.

この糸条通過孔4の形成部と紡糸口金3との間
の距離は任意であるが、あまり離れすぎると磁界
の強さを保つために大電流を流さなければならな
い。好ましくは30cm以下、更に好ましくは15cm以
下である。
The distance between the forming part of the yarn passing hole 4 and the spinneret 3 is arbitrary, but if the distance is too large, a large current must be passed to maintain the strength of the magnetic field. The length is preferably 30 cm or less, more preferably 15 cm or less.

以上の説明では、磁性体2として同じ材質の一
体成型物を用いた例を示したが紡糸口金3の部
分、糸条通過孔4の形成部分、あるいは中間部1
1を別々の材質の磁性体で構成することもでき
る。磁性体としては、通常ニツケル、コバルト、
鉄類などが用いられ、特に紡糸口金3の部分は鉄
類が好ましい。
In the above explanation, an example is shown in which an integrally molded product made of the same material is used as the magnetic body 2.
1 can also be made of different magnetic materials. Magnetic materials are usually nickel, cobalt,
Iron or the like is used, and iron is particularly preferable for the spinneret 3 portion.

本発明における磁場発生装置では、紡出糸条に
かける磁界の最高強さは10キロガウス以上である
ことが望ましく、好ましくは15キロガウス以上で
ある。しかし、磁界強さの最適値は紡糸するポリ
マーの種類や紡糸条件によつて異なる。
In the magnetic field generator of the present invention, the maximum strength of the magnetic field applied to the spun yarn is desirably 10 kilogauss or more, preferably 15 kilogauss or more. However, the optimum value of the magnetic field strength varies depending on the type of polymer to be spun and the spinning conditions.

以上の説明では磁性体として、その一部にコイ
ルを巻いた磁性体芯型マグネツトの例について述
べたが、本発明はこれに限定されるものではな
く、目的に応じて任意のマグネツトを用いること
ができる。
In the above explanation, an example of a magnetic material core type magnet with a coil wound around a part of the magnetic material was described as an example, but the present invention is not limited to this, and any magnet can be used depending on the purpose. I can do it.

本発明の紡糸装置は、紡糸口金から吐出された
糸条を、重力の作用する方向、即ち上から下へ向
つて走行させて巻取る通常の紡糸装置であつても
よく、又その逆に、下に設けた紡糸口金から紡出
糸条を上方へ引取る様にした紡糸装置であつても
よい。更に紡糸口金からの紡出糸条を水平方向に
走行させて引取る様にした紡糸装置であつてもさ
しつかえない。
The spinning device of the present invention may be a normal spinning device that winds the yarn discharged from the spinneret by running it in the direction of gravity, that is, from top to bottom, or vice versa. It may be a spinning device that takes the spun yarn upward from a spinneret provided below. Furthermore, a spinning device may be used in which the spun yarn from the spinneret is moved horizontally and taken up.

本発明の紡糸装置は、コンジユゲート紡糸、混
合紡糸等にも適用することが出来る。又、異形断
面糸、中空断面糸等の紡糸にも適用することが出
来る。
The spinning apparatus of the present invention can also be applied to conjugate spinning, mixed spinning, etc. It can also be applied to spinning yarns with irregular cross sections, hollow cross sections, etc.

本発明の紡糸装置においては、該磁場発生装置
と共に、他のエネルギー付加装置や繊維加工装置
を組み合せて使用することも可能である。例え
ば、他のエネルギー付加手段として、電界発生装
置や糸条走行方向と垂直方向の他の磁場発生装置
を用い、本発明装置の磁場発生装置と共に併用し
て、紡出糸条の分子配向の制御をより確実、有効
ならしめることができる。
In the spinning device of the present invention, it is also possible to use the magnetic field generating device in combination with other energy adding devices or fiber processing devices. For example, as another energy adding means, an electric field generator or another magnetic field generator in a direction perpendicular to the yarn running direction may be used together with the magnetic field generator of the apparatus of the present invention to control the molecular orientation of the spun yarn. can be made more reliable and effective.

更に、例えば磁場発生装置の次に、インターレ
ース加工ノズルとか捲縮加工装置などの繊維加工
手段を種々組み合せて繊維を形成することも可能
である。
Furthermore, it is also possible to form fibers by combining various fiber processing means such as an interlacing nozzle or a crimping device next to the magnetic field generating device.

以上説明した如く、本発明の紡糸装置は、紡糸
口金と、それに相対峙する磁極との間で、紡出糸
条に対してほぼ平行方向の磁界をかける磁場発生
装置を設けたものであるから、容易に紡出糸条の
分子配向を制御することが出来る。
As explained above, the spinning device of the present invention is equipped with a magnetic field generating device that applies a magnetic field in a direction substantially parallel to the spun yarn between the spinneret and the magnetic poles facing it. , the molecular orientation of the spun yarn can be easily controlled.

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

第1図は本発明装置の一例を模式的に示す概略
図、第2図は本発明装置に用いられる磁場発生装
置の種々の実施態様を示す図、第3図は本発明装
置に用いられる磁場発生装置における磁界の強さ
と時間との関係を示すグラフである。 …磁性体、3…紡糸口金、4…糸条通過孔、
12,12′,12″…コイル。
Fig. 1 is a schematic diagram schematically showing an example of the device of the present invention, Fig. 2 is a diagram showing various embodiments of the magnetic field generator used in the device of the present invention, and Fig. 3 is a diagram showing the magnetic field used in the device of the present invention. It is a graph showing the relationship between magnetic field strength and time in a generator. 2 ... Magnetic material, 3... Spinneret, 4... Yarn passage hole,
12, 12', 12''...Coil.

Claims (1)

【特許請求の範囲】 1 一部が互いに対峙するように屈曲してなる磁
性体において、該対峙部分の一方を紡糸口金とす
ると共に、該対峙部分の他方に糸条通過孔を形成
せしめ、両対峙部分間で紡出糸条に対してほぼ平
行方向の磁界をかけるようにしたことを特徴とす
る紡糸装置。 2 磁性体芯型マグネツトが直流磁界を発生させ
るものである特許請求の範囲第1項記載の紡糸装
置。 3 磁性体芯型マグネツトが交番磁界を発生させ
るものである特許請求の範囲第1項記載の紡糸装
置。 4 磁性体芯型マグネツトが、10キロガウス以上
の最大磁界強さを有するものである特許請求の範
囲第1項記載の紡糸装置。
[Scope of Claims] 1. In a magnetic material whose parts are bent so as to face each other, one of the facing parts is used as a spinneret, and the other of the facing parts is formed with a thread passage hole, and both of the facing parts are bent to face each other. A spinning device characterized in that a magnetic field is applied in a substantially parallel direction to a spun yarn between opposing parts. 2. The spinning apparatus according to claim 1, wherein the magnetic core type magnet generates a DC magnetic field. 3. The spinning apparatus according to claim 1, wherein the magnetic core type magnet generates an alternating magnetic field. 4. The spinning apparatus according to claim 1, wherein the magnetic core type magnet has a maximum magnetic field strength of 10 kilogauss or more.
JP15583382A 1982-09-09 1982-09-09 Spinning device Granted JPS5947408A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP15583382A JPS5947408A (en) 1982-09-09 1982-09-09 Spinning device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP15583382A JPS5947408A (en) 1982-09-09 1982-09-09 Spinning device

Publications (2)

Publication Number Publication Date
JPS5947408A JPS5947408A (en) 1984-03-17
JPS6346165B2 true JPS6346165B2 (en) 1988-09-13

Family

ID=15614491

Family Applications (1)

Application Number Title Priority Date Filing Date
JP15583382A Granted JPS5947408A (en) 1982-09-09 1982-09-09 Spinning device

Country Status (1)

Country Link
JP (1) JPS5947408A (en)

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
DE102008003847A1 (en) * 2008-01-10 2009-07-16 Robert Bosch Gmbh Process for the production of fibers, fibers and their use
CN103015082B (en) * 2012-12-25 2014-08-13 西安建筑科技大学 Spinning head and method for preparing braided tube/polymer composite membrane by using spinning head

Also Published As

Publication number Publication date
JPS5947408A (en) 1984-03-17

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