JPH03280405A - Electromagnet and knitting machine using same - Google Patents

Electromagnet and knitting machine using same

Info

Publication number
JPH03280405A
JPH03280405A JP2082589A JP8258990A JPH03280405A JP H03280405 A JPH03280405 A JP H03280405A JP 2082589 A JP2082589 A JP 2082589A JP 8258990 A JP8258990 A JP 8258990A JP H03280405 A JPH03280405 A JP H03280405A
Authority
JP
Japan
Prior art keywords
magnetic
magnet
carriage
electromagnet
magnetic circuit
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
JP2082589A
Other languages
Japanese (ja)
Other versions
JPH0587963B2 (en
Inventor
Yasukazu Nishitani
泰和 西谷
Yoshiteru Koyama
小山 芳輝
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.)
Shima Seiki Mfg Ltd
Original Assignee
Shima Seiki Mfg 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 Shima Seiki Mfg Ltd filed Critical Shima Seiki Mfg Ltd
Priority to JP2082589A priority Critical patent/JPH03280405A/en
Publication of JPH03280405A publication Critical patent/JPH03280405A/en
Publication of JPH0587963B2 publication Critical patent/JPH0587963B2/ja
Granted legal-status Critical Current

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  • Knitting Machines (AREA)
  • Electromagnets (AREA)

Abstract

PURPOSE:To make it possible to obtain the required strength only when it is required by a method wherein a first magnetic circuit is composed of a semi-hardened magnetic member, equipped with an excitation coil, a magnet and a magnetic material to be attracted, a second magnetic circuit is composed of the above-mentioned magnet and a soft magnetical material, an excitation coil is excited by the magnet for a short period in the same direction as the magnetic field, and the attraction force of the material to be attracted is controlled through switching of forces between strong/weak. CONSTITUTION:A first magnetic circuit A is composed of semi-hardened magnetic bodies 2 and 3, equipped with excitation coils 5 and 6, and a magnet 1 in such a manner that a magnetic body 4 to be attracted will be attracted, and another second magnetic circuit B is composed of a magnet 1 and a soft magnetic soft material 7. In this magnet 1, its magnetic force can be maintained either in strong and weak states even when a current is interrupted. In this knitting machine, a device, with which the mechanism such as stitch cams 22b and 22d, a cam 25 and the like are switched according to the progressing direction of a carriage 21, is constituted by the above-mentioned electromagnet 41, the attraction force of the electromagnet is intensified only when the carriage 21 is inverted, and the attraction force is weakened when the electromagnet is travelling performing a knitting operation, thereby enabling the electromagnet to travel smoothly.

Description

【発明の詳細な説明】[Detailed description of the invention] 【 産業上の利用分野 】[ Industrial application field ]

本発明は、永久磁石と組み合わせることによって少ない
電力で吸着力を増減できる電磁石に関する。
TECHNICAL FIELD The present invention relates to an electromagnet that can increase or decrease attraction force with less electric power by combining with a permanent magnet.

【 従来の技術 】[Conventional technology]

従来にも磁石と組み合わせた構成の電磁石はあった。 これは、磁石の磁場を打ち消す方向に電磁石を励磁する
ことによって、磁力を弱く制御するように構成されてい
た。 また、従来の編機の度山等の機構の切り換え手段は、磁
石によって構成されており、キャリ・ソジの進行方向が
反転するときに、摺動バーと前記磁石との引力によって
前記磁石を引き止めようとする力か発生する。この力に
よって、前記機構を往路の状態から復路の状態に切り換
えて復路の編成に備えるように構成されている。
In the past, there were electromagnets that were configured in combination with magnets. This was configured to weakly control the magnetic force by exciting an electromagnet in a direction that canceled out the magnetic field of the magnet. In addition, the means for switching mechanisms such as the threads of conventional knitting machines is constituted by a magnet, and when the direction of movement of the carry/strip is reversed, the magnet is moved by the attractive force between the sliding bar and the magnet. A force is generated that tries to hold it back. This force is configured to switch the mechanism from the outbound trip state to the return trip state to prepare for the return trip formation.

【 発明が解決しようとする課題 】[Problem to be solved by the invention]

ところが、上述したような磁石と組み合わせた従来の電
磁石では、磁力を弱く保つには電磁石に電流を供給し続
けて励磁しておかなければならないのでエネルギーの消
費量が大きくなるという問題があった。 そして、上述したような磁石を使用した編機の切り換え
手段においては、キャリッジが反転後に編成しなから摺
動バー上を走行中においても、前記磁石と摺動バーとの
間には強い吸着力か作用するので、キャリッジ走行の負
荷となって無駄な駆動エネルギーを要するのみならず、
前記引力によってキャリッジは摺動ノく−に強く押しつ
けられながら走行するので摺接部分が摩耗しやすいとい
う問題が発生する。 この問題を解決するために、前記磁石に代えて電磁石を
使用することも考えられるか、従来の電磁石では、充分
な吸着力を得るには大きな電磁石にする必要かあるので
、スペースの限られたキャリッジに装着することは不適
当であった。たとえ装着しても励磁する時間は大きな電
力を連続して供給しなければならないので発熱量が大き
くなるという問題がある。特に電磁石を小さくすればす
る程放熱効果は悪くなるので、通常の電磁石をキャリッ
ジの切り換え手段として使用することは不適当であった
。 そこで、このような種々の問題を解決し、必要な時にの
み必要な力の磁力を得ることのできる電磁石の実現を目
的としてこの発明はなされたものである。
However, with conventional electromagnets combined with the magnets described above, in order to keep the magnetic force weak, it is necessary to continuously supply current to the electromagnet to excite it, which poses a problem in that it consumes a large amount of energy. In the switching means of the knitting machine using magnets as described above, even when the carriage is running on the sliding bar after reversing and not knitting, there is a strong attraction force between the magnet and the sliding bar. This not only creates a load for carriage travel and requires wasted driving energy, but also
Because the carriage travels while being strongly pressed against the sliding groove due to the above-mentioned attractive force, a problem arises in that the sliding contact portion is likely to wear out. In order to solve this problem, it may be possible to use electromagnets instead of the magnets mentioned above.With conventional electromagnets, it is necessary to make them large to obtain sufficient adsorption force, so It was inappropriate to attach it to the carriage. Even if the magnet is attached, a large amount of power must be continuously supplied during the excitation time, resulting in a problem of increased heat generation. In particular, the smaller the electromagnet is, the worse the heat dissipation effect becomes, so it has been inappropriate to use an ordinary electromagnet as a means for switching the carriage. Therefore, the present invention was made with the aim of solving these various problems and realizing an electromagnet that can obtain the necessary magnetic force only when necessary.

【 課題を解決するための手段 】[Means to solve the problem]

本発明にかかる電磁石においては、励磁コイルを備えた
半硬磁性体部材と磁石と被吸着磁性体とで第1の磁気回
路を構成するとともに、前記磁石と軟磁性体部材とで前
記第1の磁気回路とは異なる第2の磁気回路を構成し、
前記励磁コイルを前記磁石による磁場の方向と同一方向
もしくは逆方向に短時間励磁する励磁コイル駆動手段を
設けることによって、前記第1の磁気回路における前記
被吸着磁性体の吸着力を強弱切り換え制御するように構
成するという手段を講じた。 そして、本発明にかかる編機においては、磁性体からな
る摺動バーに沿って走行するキャリッジの進行方向を編
み幅の両端で反転させるときに、度山、カム等の編成機
構を切り換える切り換え手段を備えた編機において、励
磁コイルを備えた半硬磁性体部材、磁石、および前記摺
動バーとで構成された第1の磁気回路と、前記磁石と軟
磁性体部材とで構成された前記第1の磁気回路とは異な
る第2の磁気回路を備えた電磁石を、キャリッジ上の前
記摺動バーに対向する位置に配設するとともに、編み幅
の端部における反転位置にてキャリッジ反転開始信号を
出力する手段と、前記反転位置より僅かに内側の位置も
しくは前記キャリッジ反転開始信号より僅かに遅れたタ
イミングで、キャリッジ反転完了信号を出力する手段と
、前記キャリッジ反転開始信号によって前記励磁コイル
を磁石による磁場と同一方向に短時間励磁し、前記キャ
リッジ反転完了信号によって前記励磁コイルを磁石によ
る磁場と逆方向に短時間励磁する励磁コイル駆動手段と
を備え、編み幅の両端部においてキャリッジの走行方向
を反転するときに、キャリッジ反転開始信号とキャリッ
ジ反転完了信号の間のみ前記電磁石の前記第1の磁気回
路の磁束密度を高くすることによって電磁石と摺動バー
との吸着力を強くして、切り換え手段を作動させるよう
に構成するという手段を講じた。
In the electromagnet according to the present invention, the semi-hard magnetic member provided with the excitation coil, the magnet, and the attracted magnetic body constitute a first magnetic circuit, and the magnet and the soft magnetic member constitute the first magnetic circuit. configuring a second magnetic circuit different from the magnetic circuit,
By providing an excitation coil driving means that excites the excitation coil for a short time in the same direction or in the opposite direction to the direction of the magnetic field generated by the magnet, the attraction force of the attracted magnetic body in the first magnetic circuit is controlled by switching the strength or weakness. We took measures to configure it as follows. In the knitting machine according to the present invention, when the direction of movement of the carriage traveling along the sliding bar made of magnetic material is reversed at both ends of the knitting width, the switching means switches the knitting mechanism such as the stitches and cams. A knitting machine comprising: a first magnetic circuit comprising a semi-hard magnetic member having an excitation coil, a magnet, and the sliding bar; and a first magnetic circuit comprising the magnet and the soft magnetic member. An electromagnet having a second magnetic circuit different from the first magnetic circuit is disposed on the carriage at a position facing the sliding bar, and a carriage reversal start signal is sent at the reversal position at the end of the knitting width. means for outputting a carriage reversal completion signal at a position slightly inside the reversal position or at a timing slightly delayed from the carriage reversal start signal; excitation coil driving means that excites the excitation coil for a short time in the same direction as the magnetic field generated by the magnet, and excite the excitation coil for a short time in the opposite direction to the magnetic field generated by the magnet in response to the carriage reversal completion signal, When reversing, the magnetic flux density of the first magnetic circuit of the electromagnet is increased only between the carriage reversal start signal and the carriage reversal completion signal, thereby increasing the attraction force between the electromagnet and the sliding bar. Steps were taken to configure the means to operate.

【 作用 】[Effect]

本発明にかかる電磁石の作用を第1図、第2図。 及び第7図を参照しつつ説明する。 本発明の電磁石においては、励磁コイル5,6を備えた
半硬磁性体2,3と磁石1で第1の磁気回路Aを構成し
て被吸着磁性体4を吸着するように構成するとともに、
前記磁気回路と異なる第2の磁気回路Bを磁石lと軟磁
性体部材7とで形成した。 即ち、前記磁石lにおいては、前記半硬磁性体部材2,
3で形成された第1の磁気回路Aと、磁石lと軟磁性体
部材7で形成された第2の磁気回路Bとが並列に形成さ
れている。 上記電磁石lにおいて、前記励磁コイル5,6を励磁し
ていない状態では、磁石lの磁力線は主に透磁率のより
高い軟磁性体部材7の第2の磁気回路Bの方を通り、透
磁率のより小さい前記第1の磁気回路Aには僅かな漏れ
磁束のみが通り、前記被吸着磁性体4を吸着す、る力(
Fl)は弱い。 この漏れ磁束では半硬磁性体2,3は飽和しない。 ところが、前記励磁コイル5に通電して前記磁石lによ
る磁界Zと同方向Xに励磁して磁場Hsを与えると、こ
の第1の磁気回路Aを構成する半硬磁性体部材2,3は
飽和磁化Msを得るとともに透磁率が高くなって磁束密
度が上がり、被吸着磁性体4を強く吸着するようになる
。 このとき、前記励磁コイル5への電流を遮断しても半硬
磁性体部材2,3にはその残留磁化特性によって残留磁
化Mrが残存し、第1の磁気回路への磁束密度は高い状
態で保たれ、強い吸着力(F2)が保持されるのである
。 ここで、前記励磁コイル6に通電して磁石lによる磁力
線の向きZと逆方向Yに励磁し、この第1の磁気回路A
を構成する半硬磁性体部材2,3にその抗磁場(−He
)以上の逆磁場を与えると、この半硬磁性体部材2,3
の残留磁化が零以下となり、この状態は通電を止めても
保たれる。よって、第2の磁気回路Bの方が透磁率が高
くなって磁束密度が高くなり、前記第1の磁気回路Aの
磁束密度は低くなり、前記被吸着磁性体4を吸着する力
(Fl)は弱くなる。即ち、本発明における半硬磁性体
部材とは残留磁化の得られる磁性体である。 このように、磁力を強弱に切り換える瞬間だけそれぞれ
逆方向に励磁するよう通電するだけで、電流を切っても
磁力を強弱いずれかの状態に保つことができるのである
。 そして、本発明にかかる編機によれば、キャリッジの進
行方向によって度山、カム等の機構を切り換える手段を
上記構成の電磁石によって構成したので、キャリッジの
進行方向が反転するとき瞬間に、この電磁石の励磁コイ
ルに通電して内蔵する磁石による磁束と同じ方向に励磁
すると、電流の供給を止めても第1の磁気回路A′の磁
束密度が高くなった状態が保たれる。よって、被吸着磁
性体としての摺動バーを強く吸着し、キャリッジの進行
方向と逆の方向の抵抗力か前記切り換え手段に作用し、
前記機構を切り換える。 そして、前記カム等の機構の切り換えが完了すると、今
度はこの電磁石の励磁コイルに前記と逆方向に励磁する
ように通電すると、前記第1の磁気回路A′の磁束密度
は低下し、電流の供給を止めても前記第1の磁気回路A
′の磁束密度は低い状態に保たれる。よって、被吸着磁
性体としての摺動バーに対する吸着力は弱くなるので、
キャリッジの進行を妨けようとする抵抗力は弱まりキャ
リッジはスムーズに走行する。
FIGS. 1 and 2 show the action of the electromagnet according to the present invention. This will be explained with reference to FIG. In the electromagnet of the present invention, the semi-hard magnetic bodies 2 and 3 provided with excitation coils 5 and 6 and the magnet 1 constitute a first magnetic circuit A to attract the magnetic body 4 to be attracted, and
A second magnetic circuit B, different from the magnetic circuit described above, was formed by a magnet l and a soft magnetic member 7. That is, in the magnet l, the semi-hard magnetic member 2,
A first magnetic circuit A made up of magnets 3 and a second magnetic circuit B made of magnets 1 and soft magnetic material members 7 are formed in parallel. In the electromagnet 1, when the excitation coils 5 and 6 are not excited, the lines of magnetic force of the magnet 1 mainly pass through the second magnetic circuit B of the soft magnetic member 7, which has a higher magnetic permeability. Only a small amount of leakage magnetic flux passes through the first magnetic circuit A, which is smaller than , and the force (
Fl) is weak. The semi-hard magnetic bodies 2 and 3 are not saturated with this leakage magnetic flux. However, when the excitation coil 5 is energized and excited in the same direction X as the magnetic field Z by the magnet l to provide a magnetic field Hs, the semi-hard magnetic members 2 and 3 forming the first magnetic circuit A become saturated. As the magnetization Ms is obtained, the magnetic permeability increases, the magnetic flux density increases, and the magnetic body 4 to be attracted is strongly attracted. At this time, even if the current to the excitation coil 5 is cut off, residual magnetization Mr remains in the semi-hard magnetic members 2 and 3 due to their residual magnetization characteristics, and the magnetic flux density to the first magnetic circuit remains high. The strong adsorption force (F2) is maintained. Here, the excitation coil 6 is energized to be excited in the direction Y opposite to the direction Z of the magnetic lines of force caused by the magnet l, and the first magnetic circuit A
The coercive magnetic field (-He
) When a reverse magnetic field of more than
The residual magnetization of the magnet becomes less than zero, and this state is maintained even when the current is turned off. Therefore, the second magnetic circuit B has a higher magnetic permeability and a higher magnetic flux density, and the first magnetic circuit A has a lower magnetic flux density, which increases the force (Fl) for attracting the magnetic body 4 to be attracted. becomes weaker. That is, the semi-hard magnetic material member in the present invention is a magnetic material that can obtain residual magnetization. In this way, the magnetic force can be maintained in either the strong or weak state even if the current is turned off by simply applying current to excite in the opposite direction only at the moment when the magnetic force is switched to strong or weak. According to the knitting machine according to the present invention, the means for switching mechanisms such as the stitches and cams depending on the direction of movement of the carriage is constituted by the electromagnet having the above structure. When the excitation coil is energized to excite it in the same direction as the magnetic flux generated by the built-in magnet, the magnetic flux density of the first magnetic circuit A' remains high even if the current supply is stopped. Therefore, the sliding bar as the magnetic body to be attracted is strongly attracted, and a resistance force in a direction opposite to the traveling direction of the carriage acts on the switching means,
Switch the mechanism. When the switching of the mechanism such as the cam is completed, when the excitation coil of this electromagnet is energized in the opposite direction, the magnetic flux density of the first magnetic circuit A' decreases, and the current Even if the supply is stopped, the first magnetic circuit A
The magnetic flux density at ′ is kept low. Therefore, the attraction force against the sliding bar as a magnetic body to be attracted becomes weaker.
The resistance force that tries to prevent the carriage from moving is weakened, and the carriage runs smoothly.

【 実施例 】【 Example 】

以下に本発明にかかる電磁石の実施例を図面に基づいて
詳説する。 第1図は本発明の電磁石の実施例の側面断面図、第2図
は前記電磁石の強弱を切り換えるタイミングチヤード図
である。 図面において、 1は硬磁性体を着磁しS極IAとN極IBを形成した磁
石、2はその端部2Aが前記磁石lのN極IBに接合さ
れた半硬質磁性体部材、3はその端部3Aが前記磁石1
のS極IAに接合された半硬質磁性体部材、4は被吸着
磁性体、5,6はそれぞれ前記半硬質磁性体部材2,3
に巻かれた励磁コイルである。8,9は前記励磁コイル
5,6を直流電源10に短時間接続するスイッチであり
、スイッチ8がオンされると励磁コイル5に下向きの磁
場Xを生成し、スイッチ9がオンされると励磁コイル6
に下向きの磁場Yを生成すよう構成されている。7はそ
の両端が前記半硬質磁性体部材2.3の端部2A、3A
に接合された軟磁性体部材である。 この場合、前記磁石1としては3.5ミリX 11.9
ミ+) X 7 ミ・)の磁石を二個合わせたものを用
い、半硬磁性体部材2,3としては厚さ44すの炭素鋼
(S450)を用い、励磁コイル5,6としては、径0
.18”す9巻数550回、長さ11ミリ、抵抗値15
Ωのコイルを用い、軟磁性体部材7として厚さ3ミリの
電磁軟鉄(SUYP)を用いた。 上述した磁石1.半硬質磁性体部材2.被吸着磁性体4
.半硬質磁性体部材3で第1の磁気回路Aを構成し、磁
石l、半硬質磁性体部材2の端部2A、軟磁性体部材7
.半硬質磁性体部材3の端部3Aで第2の磁気回路Bを
構成している。 上記構成の電磁石11において、初期状態においては、
前記磁石1の生成する磁束はより軟質の磁性体で構成さ
れた第2の磁気回路Bの方へ主に流れ、第1の磁気回路
Aを構成する半硬質磁性体部材2,3の磁束密度は前記
磁石1からの漏れ磁束のみであるので低い。よって、被
吸着磁性体4を吸着する力は弱い(Fl)。 そこで、前記スイッチ8をオンすると前記励磁コイル5
には前記下向きの磁場Xが生成され、第1の磁気回路A
には時計回りの強い磁界か発生する。よって、被吸着磁
性体4は強い力で吸着される。 次に、前記スイッチ8をオフすると前記励磁コイル5は
励磁電流はなくなるが、前記半硬質磁性体部材2,3に
はそのヒステリシス特性によって残留磁化が残存するの
で、第1の磁気回路Aには時計回りの強い磁束が引き続
き存在する。よって、被吸着磁性体4は引き続き強い力
(F2)で吸着される。即ちこの状態では、前記励磁コ
イル5゜6には何ら電力が供給されていないにもかかわ
らず、強い吸着力(F2)が持続するのである。このと
きの、摺動力は実測値で1.0kgfか得られた。 なおこの摺動力とは、吸着した状態の被吸着部材と電磁
石とを摺動させるのに必要な力のことである。 次に、前記スイッチ9をオンすると前記励磁コイル6に
は前記下向きの磁場Yが生成され、第1の磁気回路Aに
は半時針目りの半硬磁性体の抗磁場を上回る強い磁場が
生成し、この磁場によってこの半硬磁性体部材2,3の
残留磁化は零以下になり、第1の磁気回路Aには、僅か
に前記磁石1による漏れ磁束のみが存在し、被吸着磁性
体4を吸着する力は弱(なる(Fl)。 次に、前記スイッチ9をオフすると前記励磁コイル6は
励磁されず、前記磁石による漏れ磁束のみでは、第1の
磁気回路Aの半硬磁性体部材2゜3に高い残留磁化を与
えることはできず、第1の磁気回路Aには僅かな漏れ磁
束しか存在しない状態が保たれる。よって、被吸着磁性
体4を吸着する力は引き続き弱い状態が保たれる(Fl
)。このときの、摺動力は実測値で0.3 kg fが
得られた。 よって、電磁石の吸着力を強弱切り換えて、0゜7kg
fの摺動力の変化を得ることかできたのである。上記励
磁コイル5.6に通電している時間は数m5ec、程度
で充分である。 なお、この電磁石11の材料構成としては、第1図に示
したものに限定されるものでは無い。例えば、前記磁石
1として3.5ミリX11.9”す×729の磁石を一
個たけにすると、摺動力をOkg fと0゜4kgfと
に切り換えることができ、前記軟磁性体部材7として炭
素鋼(845C)を使用すると摺動力を0.4 kg 
fと1.1kgfとに切り換えることかでき、前記軟磁
性体部材7として炭素鋼(S450)を使用し、前記半
硬磁性体部材2,3として電磁軟鉄(SUYP)を使用
すると摺動力を0.45kgfと0.7 kg fとに
切り換えることができた。 そこで、前記軟磁性体部材7も前記半硬磁性体部材2,
3も電磁軟鉄(SUYP)を使用してみると摺動力は殆
ど変化しなかった。 このように0.5 kg f以上の摺動力の変化を得る
には、半硬磁性体部材2,3としては電磁軟鉄では不都
合であり345C程度以上の硬質の炭素鋼が適当である
といえる。 なお、巻線の向きを変えた二個の励磁コイルに代えて、
−個の励磁コイルへ供給する電流の極性を変えるように
しても良く、また巻き方等も上記実施例に限定されるこ
とはなく、例えばバイファイラもしくはユニファイラと
しても良いことは当然である。 次に、本発明にかかる編機の実施例を図面に基づいて詳
説する。 第3図は本発明にかかる編機のキャリッジの一部を切除
した状態の平面図構造図、第4図は同キャリッジの磁気
吸着部材の一部拡大断面図、第5図は同編機の制御回路
のブロック構成図、第6図は同編機の吸着力切り換えの
タイミングチャート図である。 第3図乃至第6図において、 キャリッジ21の地板23に上げ山24が固定され、昇
降動可能に支持された度山22a、22bがそのカム面
24a、24bに対面して設けられている。度山22a
、22bはスプリング31a。 31bによって溝の沿って斜め下方に移動するよう付勢
されている。ガイド板13a、13bの上面に設けられ
たローラ12a、12bは、地板23のガイド部材26
 a、  26 bによってキャリッジ21の移行方向
と平行に摺動できるように支持されたカム板25に接し
ている。 カム板25は、中央部に凹陥部32を形成し、凹陥部3
2の傾斜面32a、32b付近で前記ローラ12a、1
2bを受けている。また、カム板25の両端付近には段
部27a、27bが形成され、カム板25が左右に移行
したときに、段部27a、27bがガイド部材26a、
26bと当接し、それ以上のカム板25の移動を阻止す
る。カム板25には磁気吸着部材28を設け、この磁気
吸着部材28の両端に設けた凹部にはフェルトを嵌合固
定し、中間部には吸着力を強弱切り換え可能な電磁石4
1を設けた。 この磁気吸着部材28は第4図に示したように、磁石4
2、軟磁性体部材43、半硬磁性体部材44a、44b
、および励磁コイル45a、45bから構成された電磁
石41を備えている。そして、磁石42.半硬磁性体部
材44a、摺動バー29゜そして半硬磁性体部材44b
によって第1の磁気回路A′を構成し、磁石42と軟磁
性体部材43によって第2の磁気回路B′を構成してい
る。 この電磁石41の吸着力を強くした場合には、この磁気
吸着部材28はキャリッジ21の移行方向に延びる摺動
バー29を強く吸着し、この電磁石41の吸着力を弱く
した場合には、吸着力は弱くなるように構成した。 制御部51は、キャリッジ21の位置を示すパルス信号
γを、前記摺動バー29に沿って設けられた磁気的もし
くは光学的なストライプ等のパターンを走査するエンコ
ーダー56から常時得ているので、一つのコースを編成
し終わってキャリッジ21が編み幅の端部にきたとき、
処理回路55において、前記パルス信号゛γのカウント
値と、編み幅の左端設定器53と編み幅の右端設定器5
4とにおいて設定された値とを比較して一致したときキ
ャリッジ反転開始信号αを出力し、このキャリッジ反転
開始信号αの所定時間後(もしくは所定数のパルス信号
γをカウントした後)にキャリッジ反転完了信号βを出
力する。 電磁石駆動回路52は、このキャリッジ反転開始信号α
の入力によって前記電磁石41の励磁コイル45aに磁
石42の磁場の向きと同一方向の磁場を発生する励磁電
流を数m5ec、程度の短時間供給する。すると、第1
の磁気回路A′の磁束密度が高(なり、摺動バー29を
強く吸着する。なお、前記キャリッジ反転開始信号αが
キャリッジ駆動装置57に入力されるとキャリッジ21
の走行方向は反転する。 そして、前記キャリッジ反転完了信号βの入力によって
、電磁石駆動回路52は前記電磁石41の励磁コイル4
5bに、磁石41aの磁場と逆方向の磁場を発生する励
磁電流を数m5ec、程度の短時間供給する。 すると、電磁石41の半硬磁性体部材44a。 44bの残留磁化は消滅し、第2の磁気回路B′の磁束
密度は高くなるが第1の磁気回路A′の磁束密度は低く
なり、摺動バー29を吸着する力は弱くなる。 上記構成の編機において、 いま、キャリッジ21が、そのカム板25の凹陥部32
をキャリッジ進行方向の後側に位置させて段部27bを
ガイド部材26bに当接させた状態で、第3図の矢印の
方向に編成しつつ移動しているとする。このとき、先行
度山22aのローラ12aはスプリング31aの弾性力
に抗してカム板25の傾斜面32aを上がっているので
、度山22aは上昇位置にある。 一方、後行側の度山22b側のローラ12bはスプリン
グ31bの弾性力によってカム板25の傾斜面32bを
下がって凹陥部32に位置するので、度山22bは所定
の下降位置にある。 次に、キャリッジ21が所定の編み幅の編成を終了し反
転するとき、制御部51はキャリッジ反転開始信号αを
出力する。電磁石駆動回路52は、このキャリッジ反転
開始信号αによって電磁石41の吸着力を強くし、磁気
吸着部材28は摺動バー29に強く吸着する。このまま
キャリッジ21が反転して左行開始すると、磁気吸着部
材28は摺動バー29に吸着しているためカム板25は
左への移動を開始できず静止状態を保とうとしてキャリ
ッジ21の地板23に対して相対的に右側にスライドす
る。このとき、度山22a側のローラ12aはスプリン
グ31aの弾性力によってカム板25の傾斜面32aを
下がって凹陥部32に位置し、度山22b側のローラ1
2bはスプリング31bの弾性力に抗してカム板25の
傾斜面32bを上がる。 そして、カム板25の段部27aがガイド部材26aに
当接することにより、カム板25は静止状態を保てなく
なり、キャリッジ21の左行に伴って左行を開始する。 続いて、キャリッジ反転完了信号βが電磁石駆動回路5
2に入力されると、電磁石41の吸着力は弱くなり、キ
ャリッジ21はスムーズに編成しつつ左行するようにな
る。 このように一つのコースを編成しつつ左行してるいると
きには、上述したように電磁石の吸着力を弱くしてキャ
リッジ走行の負荷とならないようにしているのである。 また、編み幅の左端に来てキャリッジ21が左行から右
行に反転するときにも、再び制御部51はキャリッジ反
転開始信号αを出力し、前記電磁石41の吸着力を強く
し、カム板25を地板23に対して相対的に左ヘスライ
トさせて度山22a。 22bの位置を切り換え、制御部51からキャリッジ反
転完了信号βが出力されると、前記電磁石41の吸着力
を弱くして走行をスムーズにする。 なお、当然ながら編機の構造は上記構造に限定されるも
のではなく、磁性体による摺動バーに沿ってキャリッジ
が走行し、編み幅の両端で度山等の機構を切り換える構
造の編機であれば良い。また前記電磁石41の構造も第
4図に示した構造に限定されるものでは無く、゛またキ
ャリッジ反転開始信号αは前記エンコーダーから得すに
リミットスイッチ等の位置検出手段から得るようにして
も良い。 このように、本発明にかかる編機によれば、キャリッジ
21を反転させるときにのみ電磁石の吸着力を強くして
カム板25をスライドさせて度山22a、22bの位置
を切り換え、キャリッジが編成しながら走行している間
は電磁石41の吸着力を弱くしてスムーズに走行できる
のである。 よって、通電時間は短時間で良いので省エネルギー効果
があるとともに、発熱も少なく電磁石を小さくできると
いう効果も得られ、限られたスペースしか無いキャリッ
ジに装着することか可能となったのである。よって、コ
ンパクトで消費エネルギーの少ない編機を提供できるの
である。
Embodiments of the electromagnet according to the present invention will be explained in detail below based on the drawings. FIG. 1 is a side sectional view of an embodiment of the electromagnet of the present invention, and FIG. 2 is a timing chart for switching the strength of the electromagnet. In the drawings, 1 is a magnet in which a hard magnetic material is magnetized to form a south pole IA and a north pole IB, 2 is a semi-hard magnetic member whose end 2A is joined to the north pole IB of the magnet 1, and 3 is a semi-hard magnetic member. The end portion 3A is the magnet 1
4 is a magnetic member to be attracted, and 5 and 6 are the semi-hard magnetic members 2 and 3, respectively, which are joined to the S pole IA.
It is an excitation coil wound around. 8 and 9 are switches that connect the excitation coils 5 and 6 to the DC power supply 10 for a short time; when the switch 8 is turned on, a downward magnetic field X is generated in the excitation coil 5, and when the switch 9 is turned on, the excitation is coil 6
It is configured to generate a downward magnetic field Y. 7 has both ends 2A and 3A of the semi-hard magnetic member 2.3.
It is a soft magnetic material member joined to. In this case, the magnet 1 is 3.5 mm x 11.9
The semi-hard magnetic members 2 and 3 are made of carbon steel (S450) with a thickness of 44mm, and the excitation coils 5 and 6 are made of Diameter 0
.. 18" 9 turns 550 times, length 11mm, resistance value 15
A coil of Ω was used, and a 3 mm thick electromagnetic soft iron (SUYP) was used as the soft magnetic member 7. Magnet 1 mentioned above. Semi-hard magnetic member 2. Adsorbed magnetic material 4
.. The first magnetic circuit A is composed of the semi-hard magnetic member 3, and includes the magnet l, the end portion 2A of the semi-hard magnetic member 2, and the soft magnetic member 7.
.. The end portion 3A of the semi-hard magnetic member 3 constitutes a second magnetic circuit B. In the electromagnet 11 having the above configuration, in the initial state,
The magnetic flux generated by the magnet 1 mainly flows toward the second magnetic circuit B made of a softer magnetic material, and the magnetic flux density of the semi-hard magnetic members 2 and 3 constituting the first magnetic circuit A increases. is only the leakage flux from the magnet 1, so it is low. Therefore, the force for attracting the magnetic body 4 to be attracted is weak (Fl). Therefore, when the switch 8 is turned on, the excitation coil 5
The downward magnetic field X is generated in the first magnetic circuit A.
A strong clockwise magnetic field is generated. Therefore, the magnetic body 4 to be attracted is attracted with a strong force. Next, when the switch 8 is turned off, the excitation current in the excitation coil 5 disappears, but residual magnetization remains in the semi-hard magnetic members 2 and 3 due to their hysteresis characteristics. A strong clockwise magnetic flux continues to exist. Therefore, the magnetic body 4 to be attracted continues to be attracted with a strong force (F2). That is, in this state, the strong attraction force (F2) continues even though no power is supplied to the excitation coil 5.6. At this time, the measured sliding force was 1.0 kgf. Note that this sliding force is the force required to cause the electromagnet to slide between the attracted member and the electromagnet. Next, when the switch 9 is turned on, the downward magnetic field Y is generated in the excitation coil 6, and a strong magnetic field that exceeds the coercive magnetic field of the semi-hard magnetic material at the half-hour hand is generated in the first magnetic circuit A. However, due to this magnetic field, the residual magnetization of the semi-hard magnetic members 2 and 3 becomes zero or less, and in the first magnetic circuit A, only a slight leakage magnetic flux due to the magnet 1 exists, and the magnetic body to be attracted 4 The force to attract the magnet is weak (Fl).Next, when the switch 9 is turned off, the excitation coil 6 is not excited, and the semi-hard magnetic member of the first magnetic circuit A is 2.3 cannot be given a high residual magnetization, and the first magnetic circuit A remains in a state where only a small amount of leakage magnetic flux exists.Therefore, the force that attracts the magnetic body 4 to be attracted continues to be weak. is maintained (Fl
). At this time, the measured sliding force was 0.3 kgf. Therefore, by switching the attraction force of the electromagnet to strong and weak, the
It was possible to obtain a change in the sliding force of f. It is sufficient that the excitation coil 5.6 is energized for several m5 ec. Note that the material composition of this electromagnet 11 is not limited to that shown in FIG. For example, if the magnet 1 is a single magnet measuring 3.5 mm x 11.9" (845C) reduces the sliding force by 0.4 kg.
If carbon steel (S450) is used as the soft magnetic member 7 and electromagnetic soft iron (SUYP) is used as the semi-hard magnetic members 2 and 3, the sliding force can be changed to 0. I was able to switch between .45kgf and 0.7kgf. Therefore, the soft magnetic member 7 also has the semi-hard magnetic member 2,
3 also used electromagnetic soft iron (SUYP), and the sliding force hardly changed. In order to obtain a change in sliding force of 0.5 kg f or more in this way, it is inconvenient to use electromagnetic soft iron as the semi-hard magnetic members 2 and 3, and it can be said that hard carbon steel of about 345C or more is suitable. In addition, instead of two excitation coils with different winding directions,
- The polarity of the current supplied to the excitation coils may be changed, and the winding method is not limited to the above embodiment, and it goes without saying that, for example, a bifilar or unifier coil may be used. Next, embodiments of the knitting machine according to the present invention will be explained in detail based on the drawings. Fig. 3 is a plan view structural diagram with a part of the carriage of the knitting machine according to the present invention cut away, Fig. 4 is a partially enlarged sectional view of the magnetic attraction member of the carriage, and Fig. 5 is a diagram of the knitting machine. FIG. 6 is a block diagram of the control circuit and a timing chart for changing the suction force of the knitting machine. 3 to 6, a raised crest 24 is fixed to the base plate 23 of the carriage 21, and raised ridges 22a, 22b supported so as to be movable up and down are provided facing the cam surfaces 24a, 24b. Toyama 22a
, 22b is a spring 31a. 31b, it is urged to move diagonally downward along the groove. The rollers 12a and 12b provided on the upper surface of the guide plates 13a and 13b are connected to the guide member 26 of the main plate 23.
a and 26 b are in contact with a cam plate 25 supported so as to be slidable in parallel to the direction of movement of the carriage 21 . The cam plate 25 has a concave portion 32 formed in the center thereof, and the concave portion 3
The rollers 12a, 1 near the inclined surfaces 32a, 32b of 2
I am receiving 2b. Further, step portions 27a and 27b are formed near both ends of the cam plate 25, and when the cam plate 25 moves from side to side, the step portions 27a and 27b move toward the guide member 26a,
26b and prevents further movement of the cam plate 25. A magnetic attraction member 28 is provided on the cam plate 25, felt is fitted and fixed in the recesses provided at both ends of the magnetic attraction member 28, and an electromagnet 4 whose attraction force can be switched between strong and weak is provided in the middle part.
1 was established. As shown in FIG. 4, this magnetic adsorption member 28
2. Soft magnetic member 43, semi-hard magnetic member 44a, 44b
, and an electromagnet 41 composed of excitation coils 45a and 45b. And magnet 42. Semi-hard magnetic member 44a, sliding bar 29°, and semi-hard magnetic member 44b
The magnet 42 and the soft magnetic member 43 constitute a second magnetic circuit B'. When the attraction force of this electromagnet 41 is made strong, this magnetic attraction member 28 strongly attracts the sliding bar 29 extending in the moving direction of the carriage 21, and when the attraction force of this electromagnet 41 is made weak, the attraction force is was configured to be weak. The control unit 51 constantly obtains the pulse signal γ indicating the position of the carriage 21 from the encoder 56 that scans a pattern such as a magnetic or optical stripe provided along the sliding bar 29. When the carriage 21 reaches the end of the knitting width after knitting one course,
In the processing circuit 55, the count value of the pulse signal ゛γ, the left end setting device 53 of the knitting width, and the right end setting device 5 of the knitting width are processed.
4, and when they match, a carriage reversal start signal α is output, and the carriage reversal is performed after a predetermined time of this carriage reversal start signal α (or after counting a predetermined number of pulse signals γ). Outputs a completion signal β. The electromagnet drive circuit 52 receives this carriage reversal start signal α
In response to the input, an excitation current that generates a magnetic field in the same direction as the magnetic field of the magnet 42 is supplied to the excitation coil 45a of the electromagnet 41 for a short time of several m5ec. Then, the first
The magnetic flux density of the magnetic circuit A' becomes high (and strongly attracts the sliding bar 29. When the carriage reversal start signal α is input to the carriage drive device 57, the carriage 21
The direction of travel is reversed. Then, upon input of the carriage reversal completion signal β, the electromagnet drive circuit 52 causes the excitation coil 4 of the electromagnet 41 to
5b, an excitation current that generates a magnetic field in the opposite direction to the magnetic field of the magnet 41a is supplied for a short time of about several m5ec. Then, the semi-hard magnetic member 44a of the electromagnet 41. The residual magnetization of 44b disappears, and the magnetic flux density of the second magnetic circuit B' becomes high, but the magnetic flux density of the first magnetic circuit A' becomes low, and the force that attracts the sliding bar 29 becomes weak. In the knitting machine having the above configuration, the carriage 21 is now moving to the concave portion 32 of the cam plate 25.
It is assumed that the carriage is moved while being knitted in the direction of the arrow in FIG. 3, with the step part 27b being in contact with the guide member 26b with the carriage being positioned on the rear side in the direction of carriage movement. At this time, the roller 12a of the leading arm 22a is moving up the inclined surface 32a of the cam plate 25 against the elastic force of the spring 31a, so the arm 22a is in the raised position. On the other hand, the roller 12b on the trailing side of the dowel 22b moves down the inclined surface 32b of the cam plate 25 to be located in the recessed portion 32 due to the elastic force of the spring 31b, so the dowel 22b is at a predetermined lowered position. Next, when the carriage 21 finishes knitting a predetermined width and reverses, the control section 51 outputs a carriage reversal start signal α. The electromagnet drive circuit 52 strengthens the attraction force of the electromagnet 41 based on the carriage reversal start signal α, and the magnetic attraction member 28 strongly attracts the sliding bar 29. If the carriage 21 continues to reverse and starts moving leftward, the magnetic attraction member 28 is attracted to the sliding bar 29, so the cam plate 25 cannot start moving to the left and tries to remain stationary, causing the main plate 21 of the carriage 21 to Slide to the right relative to. At this time, the roller 12a on the side of the thread 22a moves down the slope 32a of the cam plate 25 due to the elastic force of the spring 31a and is located in the recessed part 32, and the roller 1 on the side of the thread 22b
2b moves up the inclined surface 32b of the cam plate 25 against the elastic force of the spring 31b. Then, as the stepped portion 27a of the cam plate 25 comes into contact with the guide member 26a, the cam plate 25 can no longer remain stationary and starts moving leftward as the carriage 21 moves leftward. Subsequently, the carriage reversal completion signal β is sent to the electromagnet drive circuit 5.
2, the attraction force of the electromagnet 41 becomes weaker, and the carriage 21 moves to the left while knitting smoothly. When the carriage is moving to the left while forming one course in this manner, the attraction force of the electromagnet is weakened as described above to prevent it from becoming a load on the carriage travel. Further, when the carriage 21 is reversed from the left row to the right row at the left end of the knitting width, the control section 51 again outputs the carriage reversal start signal α, strengthens the attraction force of the electromagnet 41, and 25 to the left heslite relative to the main plate 23 to form a dowel 22a. When the position of the carriage 22b is switched and the carriage reversal completion signal β is output from the control section 51, the attraction force of the electromagnet 41 is weakened to make the traveling smooth. Of course, the structure of the knitting machine is not limited to the above structure, but is a knitting machine with a structure in which a carriage runs along a sliding bar made of magnetic material, and mechanisms such as stitches are switched at both ends of the knitting width. It's good to have. Furthermore, the structure of the electromagnet 41 is not limited to the structure shown in FIG. 4, and the carriage reversal start signal α may be obtained not only from the encoder but also from position detection means such as a limit switch. . As described above, according to the knitting machine according to the present invention, only when reversing the carriage 21, the attraction force of the electromagnet is strengthened and the cam plate 25 is slid to switch the positions of the threads 22a and 22b, so that the carriage knits. While the vehicle is running, the attraction force of the electromagnet 41 is weakened so that the vehicle can run smoothly. Therefore, the energization time is short, which has an energy saving effect, and it also generates less heat and allows the electromagnet to be made smaller, making it possible to install it in a carriage with limited space. Therefore, it is possible to provide a knitting machine that is compact and consumes less energy.

【 効果 】【 effect 】

以上述べたように、本発明にかかる電磁石によれば、吸
着力を強弱に切り換える瞬間だけそれぞれ逆方向に励磁
するよう通電するだけで、電流を切っても吸着力を強弱
いずれかの状態に保つことができるので、極めてエネル
ギー消費量の少ない強弱切り換え可能な電磁石を提供で
きるという効果が得られるのである。この電磁石は発熱
量も少ないので、かかる効果の得られる電磁石を小さく
できるという効果も得られる。 そして、本発明にかかる編機によれば、キャリッジを反
転するときにのみ電磁石の吸着力を強くして度山等の機
構を切り換え、キャリッジが編成しながら走行している
ときは電磁石の吸着力を弱くしてスムーズに走行できる
ようにしたので、短時間の通電で吸着力を強弱切り換え
ることができ、消費エネルギーを節減できるという効果
が得られる。 エネルギー消費量が少ないために、発熱量も少ないので
電磁石を小さくでき、編機のキャリッジという限られた
スペースにも設置できコンパクトで消費エネルギーの少
ない編機を提供できるのである。
As described above, according to the electromagnet according to the present invention, the attraction force is maintained in either the strong or weak state even when the current is turned off by simply energizing it in the opposite direction only at the moment when the attraction force is switched to strong or weak. Therefore, it is possible to provide an electromagnet that consumes very little energy and whose strength can be switched. Since this electromagnet has a small amount of heat generation, it is also possible to obtain the effect that the electromagnet capable of achieving this effect can be made smaller. According to the knitting machine of the present invention, the attraction force of the electromagnet is strengthened only when reversing the carriage to switch mechanisms such as dowels, and when the carriage is traveling while knitting, the attraction force of the electromagnet is This makes it possible to run smoothly by weakening the adsorption force, so the adsorption force can be switched from strong to weak in a short period of time, resulting in the effect of reducing energy consumption. Since it consumes less energy and generates less heat, the electromagnet can be made smaller, and it can be installed in the limited space of the carriage of the knitting machine, making it possible to provide a compact knitting machine that consumes less energy.

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

第1図は本発明にかかる電磁石の実施例の側面断面図、
第2図は前記電磁石の強弱を切り換えるタイミングチャ
ート図、第3図は本発明にかかる編機のキャリッジの一
部を切除した状態の平面図構造図、第4図は前記キャリ
ッジの磁気吸着部材の一部拡大断面図、第5図は同編機
に用いる制御回路のブロック構成図、第6図は同編機の
吸着力切り換えのタイミングチャート図、第7図は半硬
磁性体部材の磁気ヒステリシス曲線を示す図である。 A・・・第1の磁気回路、B・・・第2の磁気回路、■
・・・磁石、      2・・・半硬磁性体部材、3
・・・半硬磁性体部材、4・・・被吸着磁性体、7・・
・軟磁性体部材、  lO・・・電磁石駆動回路、11
・・・電磁石、 A′・・・第1の磁気回路、B′・・・第2の磁気回路
、α・・・キャリッジ反転開始信号、 β・・・キャリッジ反転完了信号、 21・・・キャリッジ、25・・・カム板(切り換え手
段)、29・・・摺動バー 28・・・磁気吸着部材、
41・・・電磁石、42・・・磁石、43・・・軟磁性
体部材、44a・・・半硬磁性体部材、44b・・・半
硬磁性体部材、45a・・・励磁コイル、45b・・・
励磁コイル、51・・・制御回路(キャリッジ反転開始
信号、キャリッジ反転完了信号を出力する手段)、 5
2・・・電磁石駆動回路。
FIG. 1 is a side sectional view of an embodiment of an electromagnet according to the present invention;
FIG. 2 is a timing chart for switching the strength of the electromagnet, FIG. 3 is a plan view structural diagram of the carriage of the knitting machine according to the present invention with a part cut away, and FIG. 4 is a diagram of the magnetic attraction member of the carriage. A partially enlarged sectional view, Figure 5 is a block diagram of the control circuit used in the knitting machine, Figure 6 is a timing chart for switching the attraction force of the knitting machine, and Figure 7 is the magnetic hysteresis of the semi-hard magnetic member. It is a figure showing a curve. A: first magnetic circuit, B: second magnetic circuit, ■
...Magnet, 2...Semi-hard magnetic member, 3
... Semi-hard magnetic material member, 4... Magnetic material to be attracted, 7...
・Soft magnetic material member, lO... electromagnet drive circuit, 11
...Electromagnet, A'...First magnetic circuit, B'...Second magnetic circuit, α...Carriage reversal start signal, β...Carriage reversal completion signal, 21...Carriage , 25... cam plate (switching means), 29... sliding bar, 28... magnetic attraction member,
41... Electromagnet, 42... Magnet, 43... Soft magnetic member, 44a... Semi-hard magnetic member, 44b... Semi-hard magnetic member, 45a... Excitation coil, 45b.・・・
Excitation coil, 51...control circuit (means for outputting a carriage reversal start signal and a carriage reversal completion signal), 5
2...Electromagnet drive circuit.

Claims (2)

【特許請求の範囲】[Claims] (1)励磁コイルを備えた半硬磁性体部材と磁石と被吸
着磁性体とで第1の磁気回路を構成するとともに、 前記磁石と軟磁性体部材とで前記第1の磁気回路とは異
なる第2の磁気回路を構成し、 前記励磁コイルを前記磁石による磁場の方向と同一方向
もしくは逆方向に短時間励磁する励磁コイル駆動手段を
設けることによって、 前記第1の磁気回路における前記被吸着磁性体の吸着力
を強弱切り換え制御するように構成したことを特徴とす
る電磁石。
(1) A first magnetic circuit is configured by a semi-hard magnetic member having an excitation coil, a magnet, and an attracted magnetic body, and the magnet and the soft magnetic member are different from the first magnetic circuit. By configuring a second magnetic circuit and providing an excitation coil driving means that excites the excitation coil for a short time in the same direction or in the opposite direction to the direction of the magnetic field generated by the magnet, the attracted magnetism in the first magnetic circuit can be reduced. An electromagnet characterized by being configured to control the adsorption force of the body by switching between strength and weakness.
(2)磁性体からなる摺動バーに沿って走行するキャリ
ッジの進行方向を編み幅の両端で反転させるときに、度
山、カム等の編成機構を切り換える切り換え手段を備え
た編機において、 励磁コイルを備えた半硬磁性体部材、磁石、および前記
摺動バーとで構成された第1の磁気回路と、前記磁石と
軟磁性体部材とで構成された前記第1の磁気回路とは異
なる第2の磁気回路とを備えた電磁石を、キャリッジ上
の前記摺動バーに対向する位置に配設するともに、 編み幅の端部における反転位置にてキャリッジ反転開始
信号を出力する手段と、 前記反転位置より僅かに内側の位置もしくは前記キャリ
ッジ反転開始信号より僅かに遅れたタイミングでキャリ
ッジ反転完了信号を出力する手段と、 前記キャリッジ反転開始信号によって前記励磁コイルを
磁石による磁場と同一方向に短時間励磁し、前記キャリ
ッジ反転完了信号によって前記励磁コイルを磁石による
磁場と逆方向に短時間励磁する励磁コイル駆動手段とを
備え、 編み幅の両端部においてキャリッジの走行方向を反転す
るときに、キャリッジ反転開始信号とキャリッジ反転完
了信号の間のみ、前記電磁石の前記第1の磁気回路の磁
束密度を高くすることによって電磁石と摺動バーとの吸
着力を強くして、切り換え手段を作動させるように構成
したことを特徴とする編機。
(2) In a knitting machine equipped with a switching means for switching knitting mechanisms such as stitches and cams when reversing the traveling direction of a carriage running along a sliding bar made of a magnetic material at both ends of the knitting width, excitation is applied. A first magnetic circuit composed of a semi-hard magnetic member with a coil, a magnet, and the sliding bar is different from the first magnetic circuit composed of the magnet and a soft magnetic member. means for disposing an electromagnet having a second magnetic circuit at a position facing the sliding bar on the carriage, and outputting a carriage reversal start signal at a reversal position at the end of the knitting width; means for outputting a carriage reversal completion signal at a position slightly inside the reversal position or at a timing slightly delayed from the carriage reversal start signal, and the excitation coil is moved in the same direction as the magnetic field by the magnet for a short time by the carriage reversal start signal. excitation coil drive means for exciting the excitation coil in a direction opposite to the magnetic field of the magnet for a short time in response to the carriage reversal completion signal, and when reversing the running direction of the carriage at both ends of the knitting width, Only between the start signal and the carriage reversal completion signal, the magnetic flux density of the first magnetic circuit of the electromagnet is increased to strengthen the attraction force between the electromagnet and the sliding bar, thereby operating the switching means. This knitting machine is characterized by:
JP2082589A 1990-03-28 1990-03-28 Electromagnet and knitting machine using same Granted JPH03280405A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP2082589A JPH03280405A (en) 1990-03-28 1990-03-28 Electromagnet and knitting machine using same

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP2082589A JPH03280405A (en) 1990-03-28 1990-03-28 Electromagnet and knitting machine using same

Publications (2)

Publication Number Publication Date
JPH03280405A true JPH03280405A (en) 1991-12-11
JPH0587963B2 JPH0587963B2 (en) 1993-12-20

Family

ID=13778672

Family Applications (1)

Application Number Title Priority Date Filing Date
JP2082589A Granted JPH03280405A (en) 1990-03-28 1990-03-28 Electromagnet and knitting machine using same

Country Status (1)

Country Link
JP (1) JPH03280405A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US7216513B2 (en) 2003-10-10 2007-05-15 Shima Seiki Manufacturing Limited Apparatus for applying sliding resistance for weft knitting machine
CN114775155A (en) * 2022-04-22 2022-07-22 宁波慈星股份有限公司 Leg pressing seat complete mechanism of computerized flat knitting machine

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US7216513B2 (en) 2003-10-10 2007-05-15 Shima Seiki Manufacturing Limited Apparatus for applying sliding resistance for weft knitting machine
CN114775155A (en) * 2022-04-22 2022-07-22 宁波慈星股份有限公司 Leg pressing seat complete mechanism of computerized flat knitting machine
CN114775155B (en) * 2022-04-22 2023-09-12 宁波慈星股份有限公司 Leg pressing seat complete set mechanism of computerized flat knitting machine

Also Published As

Publication number Publication date
JPH0587963B2 (en) 1993-12-20

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