JPS6212609Y2 - - Google Patents
Info
- Publication number
- JPS6212609Y2 JPS6212609Y2 JP1981188686U JP18868681U JPS6212609Y2 JP S6212609 Y2 JPS6212609 Y2 JP S6212609Y2 JP 1981188686 U JP1981188686 U JP 1981188686U JP 18868681 U JP18868681 U JP 18868681U JP S6212609 Y2 JPS6212609 Y2 JP S6212609Y2
- Authority
- JP
- Japan
- Prior art keywords
- yoke
- leaf spring
- spring
- side yoke
- print head
- 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
- 230000004907 flux Effects 0.000 description 28
- BGPVFRJUHWVFKM-UHFFFAOYSA-N N1=C2C=CC=CC2=[N+]([O-])C1(CC1)CCC21N=C1C=CC=CC1=[N+]2[O-] Chemical compound N1=C2C=CC=CC2=[N+]([O-])C1(CC1)CCC21N=C1C=CC=CC1=[N+]2[O-] BGPVFRJUHWVFKM-UHFFFAOYSA-N 0.000 description 12
- 239000011159 matrix material Substances 0.000 description 5
- 230000000694 effects Effects 0.000 description 4
- 229920006395 saturated elastomer Polymers 0.000 description 4
- 238000001179 sorption measurement Methods 0.000 description 3
- 239000000696 magnetic material Substances 0.000 description 2
- 125000006850 spacer group Chemical group 0.000 description 2
- 238000007796 conventional method Methods 0.000 description 1
- 230000003247 decreasing effect Effects 0.000 description 1
- 238000010586 diagram Methods 0.000 description 1
- 239000000463 material Substances 0.000 description 1
- 238000000034 method Methods 0.000 description 1
- 229910052761 rare earth metal Inorganic materials 0.000 description 1
- 150000002910 rare earth metals Chemical class 0.000 description 1
Landscapes
- Impact Printers (AREA)
Description
【考案の詳細な説明】
近年、点の配列によつて文字を表現するドツト
マトリツクス型のプリンタが広く使われるように
なつてきた。特に機械的に針の先端をインクリボ
ンを介して印字用紙に打ち付けてドツトを印字す
るドツトインクパクト型のプリンタは、複数枚の
用紙の重ね打ちができるので事務用プリンタとし
て広く使用されるようになつた。その代表的なも
のとしては、印字用紙の横方向に沿つて移動しな
がら印字するシリアルプリンタがあるし、また最
近ではドツトマトリツクス型のラインプリンタも
出現し広く普及しようとしている。このドツトマ
トリツクス型のラインプリンタとは、一文字ある
いは数文字毎にドツトを印字する複数のハンマを
有し、そのハンマを受持ち文字幅分だけ横に揺動
させ同時に印字紙を縦方向に移動させながら、所
定の位置で上記ハンマを作動させてドツトマトリ
ツクスの形で文字を形成するものである。[Detailed description of the invention] In recent years, dot matrix printers that express characters by an array of dots have become widely used. In particular, dot ink pact printers, which print dots by mechanically striking the tip of a needle onto printing paper via an ink ribbon, have become widely used as office printers because they can print multiple sheets of paper overlappingly. Summer. Typical examples include serial printers that print while moving along the lateral direction of printing paper, and recently, dot matrix type line printers have also appeared and are becoming widespread. This dot matrix type line printer has multiple hammers that print dots every character or several characters, and the hammers are swung horizontally by the width of the character they are in charge of, and at the same time move the printing paper vertically. However, characters are formed in the form of a dot matrix by operating the hammer at a predetermined position.
本考案は、前記したドツトマトリツクス型ライ
ンプリンタの印字ヘツドに関するものである。 The present invention relates to a print head for the above-mentioned dot matrix type line printer.
さらに詳しく言えば、永久磁石を備えたヨーク
と、このヨークの一端にその一端を固定し他端を
自由端として片持ち板ばねを有し、この板ばねの
自由端近傍前面には所謂ハンマピンを備え、しか
もこの板ばねの左右側方にはわずかの空隙をあけ
て配置した側方ヨークと、を備えて構成した印字
ヘツドであり、各板ばねの前方に配置したインク
リボン、用紙、プラテンを打撃し印字する所謂ス
プリングチヤージ式ドツトラインプリンタと称す
るプリンタの印字へツドに関するものである。 More specifically, it has a yoke equipped with a permanent magnet, a cantilever leaf spring with one end fixed to one end of the yoke and the other end free, and a so-called hammer pin on the front surface near the free end of this leaf spring. The printing head is equipped with a side yoke placed on the left and right sides of this leaf spring with a slight gap between them, and an ink ribbon, paper, and platen placed in front of each leaf spring. This invention relates to a printing head of a printer called a so-called spring charge type dot line printer that prints by striking.
従来、スプリングチヤージ式ラインプリンタの
印字ヘツドは第1図に示すように板ばね1の一端
がヨークの一方であるベース2に固定板3によつ
て固定され他端が自由のいわゆる片持ち深の構造
であり、ベース2は永久磁石5を介してヨーク4
へ連なり板ばね1を経てベース2に戻る閉磁路を
構成している。そのため板ばね1の先端はヨーク
4の前面に吸着され、板ばね1は歪められた状態
となる。そこで印字をするときは、前記ヨーク4
に巻かれたコイル6に電流を流し永久磁石5の磁
束を打ち消すことにより、ヨーク4の面に吸着さ
れていた板ばね1の自由端をヨーク4の面から離
脱させ板ばね1の持つている歪エネルギで前方へ
跳ね出させる。この運動によつて板ばね1の先端
に取付けられたハンマピンクはプラテン8上にあ
るインクリボン9、用紙10を打撃し印字するも
のである。したがつてこのようなスプリングチヤ
ージ式ドツトラインプリンタでは印字状態は板ば
ねの歪エネルギによつて左右されるが、その歪エ
ネルギはまた板ばねのばね定数により定まるた
め、板ばねのばね定数を算出しかつ板ばねを吸着
できるように磁気回路の設計を行なうのである。 Conventionally, the print head of a spring charge type line printer has a so-called cantilever structure in which one end of a leaf spring 1 is fixed to a base 2, which is one of the yokes, by a fixing plate 3, and the other end is free, as shown in FIG. The base 2 is connected to the yoke 4 via the permanent magnet 5.
It forms a closed magnetic path that connects to the base 2 via the leaf spring 1. Therefore, the tip of the leaf spring 1 is attracted to the front surface of the yoke 4, and the leaf spring 1 is in a distorted state. When printing there, the yoke 4
By applying a current to the coil 6 wound around the coil 6 and canceling the magnetic flux of the permanent magnet 5, the free end of the leaf spring 1, which was attracted to the surface of the yoke 4, is released from the surface of the yoke 4, and the free end of the leaf spring 1, which is held by the leaf spring 1, is released from the surface of the yoke 4. Jump forward with distortion energy. Due to this movement, the hammer pink attached to the tip of the leaf spring 1 hits the ink ribbon 9 and paper 10 on the platen 8 to print. Therefore, in such a spring charge type dot line printer, the printing condition depends on the strain energy of the leaf spring, but the strain energy is also determined by the spring constant of the leaf spring, so the spring constant of the leaf spring is The magnetic circuit is designed so that it can be calculated and the leaf spring can be attracted.
ドツトプリンタでは一般に高速性が要求されて
いる。すなわち、高速性を実現するには板ばねの
ヨークへの吸引、吸着、離脱、プラテンへの打撃
の各サイクルを速めることであり、これには板ば
ねの固有振動数を高くすることが要求される。こ
の場合、板ばねの固有振動数は板ばねのばね定数
の平方根に比例する。したがつて高速性にするに
はばね定数を大きくすれば良いのであるが、その
ためには板ばねを吸着するのに必要な磁束を大き
くすることが必要であり、磁束を生じる磁石部分
すなわち永久磁石と磁路を形成するヨークを大型
にせざるを得なくなるし、これに伴つて永久磁石
から板ばねを解放するためのコイルに流す電流も
また大きくする必要を生じ、大きな電源を要す
る、等々の不都合を生じることとなつていた。こ
うした不都合を解消するためには、磁石、ヨーク
で構成される磁気回路を極力小さくし、その小さ
な磁石に対しても板ばねの吸着力を低減させない
ような磁気回路の設計を行なうことが課題とな
り、従来から各種の方式のラインプリンタ印字ヘ
ツドが提案されてきたわけであるが、充分な解決
策は得られていなかつた。 Dot printers generally require high speed. In other words, in order to achieve high speed, it is necessary to speed up each cycle of the leaf spring's attraction to the yoke, adsorption, detachment, and impact on the platen, and this requires increasing the natural frequency of the leaf spring. Ru. In this case, the natural frequency of the leaf spring is proportional to the square root of the spring constant of the leaf spring. Therefore, in order to achieve high speed, it is sufficient to increase the spring constant, but in order to do so, it is necessary to increase the magnetic flux required to attract the leaf spring, and the magnetic part that generates the magnetic flux, that is, the permanent magnet The yoke that forms the magnetic path has to be made larger, and along with this, the current flowing through the coil to release the leaf spring from the permanent magnet also needs to be increased, which requires a large power source, etc., and other inconveniences. It was supposed to occur. In order to eliminate these inconveniences, the challenge is to make the magnetic circuit made up of the magnet and yoke as small as possible, and to design a magnetic circuit that does not reduce the adhesion force of the leaf spring to the small magnet. Various types of line printer print heads have been proposed in the past, but no satisfactory solutions have been found.
従来の方式の一つとして前記した第1図につい
て説明する。これは永久磁石5上にコイル6を巻
いたヨーク4があり、ヨーク4の先端に板ばね1
の一端が位置している。また板ばね1の他端は永
久磁石5をのせるベース2と称するヨークに固定
されており、永久磁石5から出た磁束の流れが1
つのループになつている。この種の印字ヘツドは
1ポール型と呼ばれている。この方式は部品数も
少なくコストを安くできるが、反面、ヨーク4に
対し板ばね1の板厚を厚くできないため、永久磁
石5からヨーク4に流れる磁束は板ばね1で十分
な磁路を得られず板ばね1が磁気的に飽和する。
したがつて板ばね1に流れるだけの磁束で板ばね
1を吸着することになるためその吸引力は小さ
く、そのため吸着される板ばね1のばね定数を大
きくできず、結果として高速化ができない欠点が
あつた。 As one of the conventional methods, FIG. 1 mentioned above will be explained. This has a yoke 4 with a coil 6 wound around a permanent magnet 5, and a leaf spring 1 at the tip of the yoke 4.
One end of is located. The other end of the leaf spring 1 is fixed to a yoke called a base 2 on which a permanent magnet 5 is placed, so that the flow of magnetic flux from the permanent magnet 5 is
It has two loops. This type of print head is called a one-pole type. This method has fewer parts and can reduce costs, but on the other hand, it is not possible to make the leaf spring 1 thicker than the yoke 4, so the magnetic flux flowing from the permanent magnet 5 to the yoke 4 can have a sufficient magnetic path in the leaf spring 1. Therefore, the leaf spring 1 becomes magnetically saturated.
Therefore, the magnetic flux that flows through the leaf spring 1 attracts the leaf spring 1, so the attractive force is small. Therefore, the spring constant of the attracted leaf spring 1 cannot be increased, and as a result, the speed cannot be increased. It was hot.
そこで吸引力を大きくする手段として、第2図
に示すように、側方ヨーク11と呼ばれる磁路補
足手段を用いた印字ヘツドが考案された。この印
字ヘツドは、前記した1ポール型において、板ば
ね1の左右にわずかの空隙をあけて磁性体ででき
たヨーク、すなわち側方ヨーク11を配置し、さ
らに側方ヨーク11の根元は板ばね1の固定端を
ベース2の間ではさみ固定板3で共に固定されて
おり、永久磁石5、ヨーク4、板ばね1の先端
部、側方ヨーク11、ベース2、を一巡する閉磁
路を構成している。すなわち、永久磁石5から発
した磁束は磁石上面のヨーク4を通り、ヨーク4
先端から板ばね1先端部に到達する。板ばね1の
先端部に入つた磁束は、第3図に示した板ばね先
端部周辺の拡大図に例示するように、板ばね1自
身に流れる磁束12とは別に、板ばね1の両側面
より側方ヨーク11に流れ込むバイパス磁束13
が生じ、それぞれベース2を経て永久磁石5に到
達するループとなる。このような磁束の流れを等
価回路で説明すると、板ばねが飽和した状態を定
常状態とする前記第1図の如き1ポール型では第
4図となり、第2図の如き側方ヨーク型では第5
図となる。第4図に等価回路を示した1ポール型
においては、板ばね1とヨーク4との間の空隙部
すなわち板ばね1の吸引部のパーミアンスPgに
流れる磁束φは磁石5から発した磁束φpが磁路
途中の漏れのパーミアンスRtによつて減少しな
がら板ばね1の先端部に達するが、実際に板ばね
の吸引吸着に寄与する磁束は板ばね1が飽和する
磁束φsと同じという制限がある。しかし第5図
に示した側方ヨーク型では、板ばね1と側方ヨー
ク11の間のパーミアンスPlが並列になるた
め、吸引吸着に寄与する部位のパーミアンスPg
に流れる磁束φはφ=(1+2Pl/Ps)φsとな
る。したがつて実質的に板ばね1の吸引吸着に寄
与する磁路が拡大されたことになり、ヨーク4か
ら板ばね1に流れる磁束が大きくなるため吸引力
も大きくなり、そのため板ばね1のばね定数も大
きくできるので、高速化が可能となるわけであ
る。 Therefore, as a means to increase the attractive force, a printing head using a magnetic path complementing means called a side yoke 11 was devised, as shown in FIG. This printing head is of the one-pole type described above, but a yoke made of a magnetic material, that is, a side yoke 11 is arranged with a slight gap left and right on the left and right sides of the leaf spring 1, and the base of the side yoke 11 is a leaf spring. 1 is sandwiched between the bases 2 and fixed together by a fixing plate 3, forming a closed magnetic path that goes around the permanent magnet 5, the yoke 4, the tip of the leaf spring 1, the side yoke 11, and the base 2. are doing. In other words, the magnetic flux emitted from the permanent magnet 5 passes through the yoke 4 on the upper surface of the magnet, and passes through the yoke 4.
The tip reaches the tip of leaf spring 1 from the tip. As illustrated in the enlarged view around the tip of the leaf spring 1 shown in FIG. Bypass magnetic flux 13 flowing more into the side yoke 11
occurs, forming a loop that reaches the permanent magnet 5 via the base 2. To explain the flow of magnetic flux using an equivalent circuit, the one-pole type shown in Fig. 1 whose steady state is the state in which the leaf spring is saturated is shown in Fig. 4, and the side yoke type shown in Fig. 2 is shown in Fig. 4. 5
It becomes a figure. In the one-pole type, the equivalent circuit of which is shown in FIG . p reaches the tip of leaf spring 1 while decreasing due to permeance R t of leakage in the middle of the magnetic path, but the magnetic flux that actually contributes to the attraction and attraction of the leaf spring is the same as the magnetic flux φ s that saturates leaf spring 1. There is a restriction. However, in the side yoke type shown in FIG. 5, the permeance P l between the leaf spring 1 and the side yoke 11 is parallel, so the permeance P g of the part that contributes to suction and adsorption
The magnetic flux φ flowing in is φ=(1+2P l /P s )φ s . Therefore, the magnetic path that contributes to the attraction and attraction of the leaf spring 1 has been expanded, and the magnetic flux flowing from the yoke 4 to the leaf spring 1 has increased, so the attractive force has also increased, and the spring constant of the leaf spring 1 has therefore increased. Since it can also be made larger, it is possible to increase the speed.
しかしながら、第2図、第3図のように側方ヨ
ーク11を単に設けただけの従来の側方ヨーク型
印字ヘツドでは、板ばね1がヨーク4への吸引、
吸着、離脱を繰り返すように動きのあるのに対
し、側方ヨーク11はその一端がベース2に単に
固定されているだけであり、最適磁路を形成する
ための配慮は特になされてはいなかつた。 However, in the conventional side yoke type print head in which the side yoke 11 is simply provided as shown in FIGS. 2 and 3, the leaf spring 1 attracts the yoke 4,
In contrast, the side yoke 11 has one end simply fixed to the base 2, and no special consideration has been taken to form an optimal magnetic path. .
すなわち第6図に1個の印字ヘツドのみを取り
出してその断面を示し、更に第7図にその吸引吸
着部周辺を拡大して示したように、板ばね1がヨ
ーク4に吸着された状態では吸引力が最大になる
ように板ばね1とヨーク4の先端面14とが密着
するようにすることが望ましい。板ばね1がヨー
ク4に吸引され吸着された状態では板ばね1がた
わみ曲線を描いて曲がるため、磁力や歪エネルギ
ーを受けていない自由状態の板ばねの裏面とヨー
ク4の先端面とが平行では密着できない。したが
つて板ばね1を固定しているベース固定端部を板
ばねたわみ角分だけ傾きを持たせるか、ベース2
に対しヨーク4を傾ける必要がある。しかしなが
ら、側方ヨーク11もまた板ばね1と共にベース
2に固定されており、かつ板ばね1に作用する吸
引力によつてたわむことがないような寸法形状に
ならざるを得ないため、板ばね1の吸引吸着時に
は板ばね1の側面は側方ヨーク11の側面からは
み出して対面する領域が減つたり完全に離れたり
して、板ばね1の側面と側方ヨーク11の側面と
の実効間隔は増大する。特に吸着領域である板ば
ね1の先端部においてこのはみ出し量が大きくな
る。一例として、板ばねの厚さが0.7mmで吸引さ
れて移動する量が0.4mmならば単純に考えたとし
ても0.3mm程度はみ出すことになる。このため、
板ばね1の吸着時には、ヨーク4から板ばね1に
入つた磁束は板ばね1から空気中を迂回するよう
にして側方ヨーク11に流れ込むため、磁束に対
して板ばね1と側方ヨーク11との間の抵抗が大
きくなる。すなわち第5図に示した等価回路中の
式φ=(1+2Pl/Ps)φsでパーミアンスPlが小
さくなり、板ばねの吸引吸着部に流れる磁束は小
さくなり、吸引吸着力も小さくなる。このような
わけで、従来の側方ヨークでは側方ヨークの効果
が十分には発揮されていなかつた。 That is, as shown in Fig. 6, which shows the cross section of only one print head, and in Fig. 7, which shows an enlarged view of the suction and adsorption portion, it is desirable that when leaf spring 1 is attached to yoke 4, leaf spring 1 and tip surface 14 of yoke 4 are in close contact with each other so that the suction force is maximized. When leaf spring 1 is attached to yoke 4, leaf spring 1 bends along a deflection curve, so that the back surface of the leaf spring in a free state not receiving magnetic force or distortion energy and the tip surface of yoke 4 cannot be in close contact with each other if they are parallel. Therefore, it is necessary to incline the fixed end of the base that fixes leaf spring 1 by the deflection angle of the leaf spring, or to tilt base 2 in such a way that the leaf spring 1 is in contact with the tip surface of yoke 4.
It is necessary to incline the yoke 4 with respect to the leaf spring 1. However, since the side yoke 11 is also fixed to the base 2 together with the leaf spring 1, and must have a size and shape that will not bend due to the suction force acting on the leaf spring 1, when the leaf spring 1 is attracted and attached, the side of the leaf spring 1 protrudes from the side of the side yoke 11, reducing the area that faces it or separating them completely, and the effective distance between the side of the leaf spring 1 and the side of the side yoke 11 increases. This protrusion amount is particularly large at the tip of the leaf spring 1, which is the attraction area. As an example, if the thickness of the leaf spring is 0.7 mm and the amount of movement due to attraction is 0.4 mm, then even if we consider it simply, it will protrude by about 0.3 mm. For this reason,
When the leaf spring 1 is attracted, the magnetic flux that entered the leaf spring 1 from the yoke 4 flows into the side yoke 11, bypassing the leaf spring 1 through the air, so that the resistance to the magnetic flux between the leaf spring 1 and the side yoke 11 becomes large. That is, the permeance Pl becomes small in the equation φ=(1+ 2Pl / Ps ) φs in the equivalent circuit shown in Figure 5, so that the magnetic flux flowing in the attracting and adsorbing portion of the leaf spring becomes small, and the attracting and adsorbing force also becomes small. For this reason, the effect of the side yoke was not fully exerted in the conventional side yoke.
本考案は従来の側方ヨークの以上の如き欠点を
除去し、側方ヨークの本来の機能を十分はたして
磁石の持つ吸引吸着エネルギを効率よく利用し得
る磁気回路を形成し、結果として高速性のスプリ
ングチヤージ式ドツトラインプリンタを提供する
ものである。 The present invention eliminates the above-mentioned drawbacks of the conventional side yokes, forms a magnetic circuit that fully fulfills the original function of the side yokes, and efficiently utilizes the attraction energy of the magnets, resulting in high-speed performance. This invention provides a spring charge type dot line printer.
本考案によれば、ヨークへ吸着した状態の板ば
ねの吸引側の面と、前記側方ヨークの板ばね吸引
方向の面とが実効的に一致するように、一端がベ
ースに固定された側方ヨークの他端、従来自由端
であつた方の端部を前記板ばね吸引吸着方向にた
わませかつ固定してある、ことを特徴とするドツ
ト式ラインプリンタ印字ヘツドが得られる。 According to the present invention, one end of the leaf spring is fixed to the base so that the suction side surface of the leaf spring adsorbed to the yoke and the surface of the side yoke in the leaf spring suction direction effectively match. There is obtained a print head for a dot type line printer characterized in that the other end of the yoke, which was conventionally a free end, is bent in the suction direction of the leaf spring and fixed.
以下本考案について実施例を示す図面を参照し
て説明する。第8図は本考案の一実施例を一部切
欠いて示した模式的立体図であり、第9図は第8
図の断面図である。永久磁石5の上面にはライン
状に並べられたヨーク4がある。また各ヨーク4
には永久磁石5から流れる磁束を打ち消すための
コイル6がある。その各ヨーク4の先端にはドツ
トを印字するためのハンマピン7を有する板ばね
1があり、さらに板ばね1の左右の側面には板ば
ね1と同時にベース2に固定板3で固定された側
方ヨーク15があり、その側方ヨーク15を複数
個同時にたわませて固定するようにこの実施例で
は特にヨーク頭部の自由端を一体化し板ばね1の
跳ね出す部分は窓状となつている。またハンマピ
ン7の前方にはインクリボン9を介して印字する
用紙10がプラテン8上に配置してある。実施例
では、側方ヨーク15の一体化した従来の自由端
をたわませた状態で固定する手段として、L型に
曲げた非磁性体でできた支柱板16を設けて例え
ば印字ヘツド後部のベース2に固定し、この支柱
板16の端部に前記側方ヨーク15の頭部を固定
してある。このとき、側方ヨーク15の内側の面
17すなわち板ばね1の吸引方向の面を、板ばね
1がヨーク4に吸着したときの吸着面と実効的に
一致するように側方ヨーク15の頭部を支柱板1
6方向にたわませて固定する。この調整は、支柱
板16の切削する機械精度で所定の長さに調整し
ても勿論良いが、固定部にはさむスペーサ18で
調整する方が容易でコストも安い。 The present invention will be described below with reference to drawings showing embodiments. FIG. 8 is a schematic three-dimensional view showing an embodiment of the present invention with a portion cut away, and FIG.
FIG. On the upper surface of the permanent magnet 5, there are yokes 4 arranged in a line. Also each yoke 4
There is a coil 6 for canceling the magnetic flux flowing from the permanent magnet 5. At the tip of each yoke 4 there is a leaf spring 1 having a hammer pin 7 for printing dots, and on the left and right sides of the leaf spring 1 there are also sides fixed to the base 2 with a fixing plate 3 at the same time as the leaf spring 1. In this embodiment, the free end of the yoke head is particularly integrated, and the protruding portion of the leaf spring 1 is shaped like a window so that a plurality of side yokes 15 can be bent and fixed at the same time. There is. Further, in front of the hammer pin 7, a sheet 10 on which printing is to be performed via an ink ribbon 9 is arranged on a platen 8. In this embodiment, as a means for fixing the integrated free end of the side yoke 15 in a bent state, an L-shaped support plate 16 made of a non-magnetic material is provided, for example, at the rear of the print head. It is fixed to the base 2, and the head of the side yoke 15 is fixed to the end of this support plate 16. At this time, the head of the side yoke 15 is adjusted so that the inner surface 17 of the side yoke 15, that is, the surface in the suction direction of the leaf spring 1, is effectively aligned with the suction surface when the leaf spring 1 is attracted to the yoke 4. Part of the support plate 1
Flex it in 6 directions and fix it. Of course, this adjustment may be performed by adjusting the length to a predetermined length using the machine precision of cutting the support plate 16, but it is easier and less costly to adjust using the spacer 18 sandwiched between the fixed parts.
このように構成した印字ヘツドは、板ばね1が
ヨーク4に吸着したとき、ヨーク4から流れた磁
束は板ばね1自身内でベース2に向つて流れる他
に、板ばね1の両側面より最小短距離の空隙を経
て左右にある側方ヨーク15に流れるため、板ば
ね1の側面と左右側方ヨーク15間のパーミアン
トPlは大きくなり、式φ=(1+2Pl/Ps)φsで
示されるように吸引部に流れる磁束φは大きくな
る。そのため板ばね1を吸引する吸引力FはF∝
φ2で表わされるように吸引力は増大し、板ばね
のばね定数を大きくできるし、歪エネルギや固有
振動数を大きくでき、高速化が可能となる。 In the print head configured in this way, when the leaf spring 1 is attracted to the yoke 4, the magnetic flux flowing from the yoke 4 not only flows within the leaf spring 1 itself toward the base 2, but also flows from both sides of the leaf spring 1 to a minimum. Since the flow passes through a short gap and flows to the left and right side yokes 15, the permeant P l between the side surface of the leaf spring 1 and the left and right side yokes 15 increases, and is expressed by the formula φ = (1 + 2P l /P s ) φ s As shown, the magnetic flux φ flowing into the attraction section increases. Therefore, the suction force F that attracts the leaf spring 1 is F∝
As expressed by φ2 , the attractive force increases, the spring constant of the leaf spring can be increased, the strain energy and the natural frequency can be increased, and high speeds can be achieved.
これは見方を変えると次のようにもなる。すな
わち、板ばね1の吸引吸着部では、ヨーク4から
流れた磁束φは板ばね1から側方ヨーク11に流
れる磁束をφlとするとφ>2φlとなる。一方、
材料の飽和磁束密度をBs、磁路の面積をSとす
ると、φ=BsSの関係が成立するので、もしヨ
ーク4の幅と板ばね1の幅とを同じ値のbとし、
ヨーク4の吸引部の高さをhとし、板ばねの厚さ
をtとすると、
φ=Bsbh、φl=Bsthとなり
前に示したφ>2φlなる関係を考慮すれば、
t<b/2
となり、板ばねの厚さはヨーク4および板ばね1
の幅bの半分以下で良いことになる。これは、板
ばね1の重さも軽くなり固有振動数は大きくなり
さらに高速化できる効果に結びつく。 If you look at it differently, it becomes something like this: That is, in the attraction portion of the plate spring 1, the magnetic flux φ flowing from the yoke 4 satisfies φ>2φ l , where φ l is the magnetic flux flowing from the plate spring 1 to the side yoke 11. on the other hand,
If the saturation magnetic flux density of the material is B s and the area of the magnetic path is S, the relationship φ=B s S holds, so if the width of the yoke 4 and the width of the leaf spring 1 are the same value b,
If the height of the suction part of the yoke 4 is h and the thickness of the leaf spring is t, then φ=B s bh, φ l =B s th, and considering the relationship φ>2φ l shown earlier, t<b/2, and the thickness of the leaf spring is yoke 4 and leaf spring 1.
It is sufficient that the width b is less than half of the width b. This leads to the effect that the weight of the leaf spring 1 is reduced, the natural frequency is increased, and the speed can be further increased.
また、上記実施例では構造的に強固にするため
もあつて側方ヨーク15の頭部の従来は自由端で
あつた部位を一体化して固定しているが、これは
ドツトラインプリンタで文字を描く際に印字ヘツ
ドを受持ち文字幅分だけ用紙に対し横に揺動する
ことにより生ずる振動に対して安定した磁気回路
を得る。すなわち、側方ヨーク15を頭部で固定
する場合は、板ばね1の吸引状態において板ばね
1および側方ヨーク15の側面を実効的に最短距
離で対面でき、またその精度も多くても±0.05mm
以内で固定し得るし、振動に対しても安定した磁
気回路が容易に構成できる。側方ヨークの頭部を
一体化する必要は必らずしもないが、その固定は
極めて有効である。固定しないと振動にともなつ
て板ばね1と側方ヨーク15間の微少間隙が変化
し、磁気回路におけるパーミアンスも変化するた
め不安定な磁気回路となるからで、この不安定が
あると印字力のバラツキを生じ、印字品質の低下
となる。固定に替えて側方ヨーク15の厚さを厚
くすることも考えられるが、こうすると、板ばね
1の自由端近傍に設けたハンマピン7の先端とプ
ラテン8との間に入る印字用紙10及びインクリ
ボン9を接近させて配置することが困難になる。
これらのことも考え併せると、側方ヨーク15の
厚さを厚くする考えには自ずと制限があり、従来
では側方ヨークも一端自由の片持ち粱構成とする
のが常識であり、心ならずも振動の影響を受けや
すい構造となつていたわけである。本考案はこの
点からも従来の欠点を解消し、設計の範囲も広が
り、かつコストも低くできる利点を有する。 In addition, in the above embodiment, in order to strengthen the structure, the part of the head of the side yoke 15, which was conventionally a free end, is integrated and fixed, but this is because the characters are printed using a dot line printer. To obtain a magnetic circuit that is stable against vibrations caused by holding a print head and swinging it laterally with respect to the paper by the width of a character when drawing. That is, when the side yoke 15 is fixed by the head, the side surfaces of the leaf spring 1 and the side yoke 15 can effectively face each other at the shortest distance when the leaf spring 1 is in the suction state, and the accuracy is ± at most. 0.05mm
It can be fixed within a certain range, and a magnetic circuit that is stable against vibration can be easily constructed. Although it is not necessary to integrate the heads of the side yokes, their fixation is extremely effective. If not fixed, the minute gap between the leaf spring 1 and the side yoke 15 will change with vibration, and the permeance in the magnetic circuit will also change, resulting in an unstable magnetic circuit. If this instability occurs, the printing force will decrease. This causes variations in the printing quality, resulting in a decrease in print quality. It may be possible to increase the thickness of the side yoke 15 instead of fixing it, but if this is done, the printing paper 10 and ink that will fit between the tip of the hammer pin 7 provided near the free end of the leaf spring 1 and the platen 8 can be considered. It becomes difficult to arrange the ribbons 9 closely together.
Taking these things into consideration, there is naturally a limit to the idea of increasing the thickness of the side yoke 15, and conventionally, it is common sense that the side yoke has a cantilever structure with one end free, which may inadvertently reduce the vibration. This meant that the structure was susceptible to influence. From this point of view as well, the present invention has the advantage of eliminating the conventional drawbacks, widening the range of design, and lowering costs.
ここで本考案の側方ヨーク構成による場合と従
来の側方ヨーク構成による場合との差を具体的な
一例で示せば次のようである。今たとえば希土類
系の永久磁石を用いてその形状を5mm×10mm×2
mmにし、ヨーク先端の吸着面積を6mm2とし、板ば
ねを長さ15mm、厚さ0.7mm、幅2mmとした場合
の、板ばねの吸引吸着特性(吸引力と板ばね・ヨ
ーク間隙との関係)の一例を示すと第10図のよ
うになる。第10図において、従来の側方ヨーク
の付いた印字ヘツドの特性19と、本考案の特性
20とを比較すれば判るように、本考案の構成は
板ばねとヨークとの間隙が小さくなればなるほど
その吸引吸着力が大きくなる。すなわち、今後の
技術動向が小型化、高速化、印字印画の高品質
化、等々であるとするならば、本考案の有用性は
極めて大きなものとなることが判る。 Here, a specific example of the difference between the side yoke structure of the present invention and the conventional side yoke structure is as follows. For example, if we use a rare earth permanent magnet, we can change its shape to 5mm x 10mm x 2.
mm, the suction area at the tip of the yoke is 6 mm2 , and the leaf spring is 15 mm long, 0.7 mm thick, and 2 mm wide. ) is shown in FIG. 10. As can be seen by comparing the characteristic 19 of the conventional print head with side yokes and the characteristic 20 of the present invention in FIG. 10, the structure of the present invention has a smaller gap between the leaf spring and the yoke. As you can see, the suction force increases. In other words, if future technological trends include miniaturization, speeding up, and higher quality printing, it can be seen that the present invention will be extremely useful.
以上第8図に例示した実施例を中心として本考
案を説明してきたが、以下本考案の他の実施例に
ついて補足説明する。第11図はその一例につい
て一部切欠いて模式的に示した斜視図であり、第
12図はその模式的断面図である。 Although the present invention has been described above with a focus on the embodiment illustrated in FIG. 8, supplementary explanations will be given below regarding other embodiments of the present invention. FIG. 11 is a perspective view schematically showing one example with a portion cut away, and FIG. 12 is a schematic cross-sectional view thereof.
この実施例は、前記実施例の構成においてベー
ス2、ヨーク4、板ばね1、側方ヨーク15を反
転した形式である。この形式では、側方ヨーク1
5の旧自由端部を引張り固定するために、支柱板
21に溝を付け、その溝に側方ヨーク15の自由
端部を差し込み結合し、さらに支柱板21を印字
ヘツドベース22に固定している。また、印字ヘ
ツドベース22には、ヨーク4、磁石5、ベース
2を囲うようにして取付けたハウジング23を取
付けている。このように構成すると、ラインプリ
ンタのように、印字ハンマを複数個並列に並べて
構成するのも容易であり、また側方ヨーク15を
板ばね1の吸引方向にたわませて固定するのも容
易であり、さらに側方ヨーク15の脱着も容易
で、板ばね1、コイル6などの部品交換も容易に
なる。 In this embodiment, the base 2, yoke 4, leaf spring 1, and side yoke 15 are reversed in the structure of the previous embodiment. In this type, the side yoke 1
In order to tension and fix the old free ends of the yoke 15, a groove is formed in the support plate 21, and the free end of the side yoke 15 is inserted into the groove and connected, and the support plate 21 is further fixed to the print head base 22. . Further, a housing 23 is attached to the print head base 22 so as to surround the yoke 4, the magnet 5, and the base 2. With this configuration, it is easy to arrange a plurality of printing hammers in parallel like in a line printer, and it is also easy to bend and fix the side yoke 15 in the suction direction of the leaf spring 1. Furthermore, the side yoke 15 can be easily attached and detached, and parts such as the leaf spring 1 and the coil 6 can be easily replaced.
以上二つの実施例を基に本考案を説明してき
た。そこでは側方ヨークの旧自由端を複数個同時
に固定するため側方ヨーク15の複数を一体に
し、板ばね1の出る部分を窓状にした例を挙げて
きたが、第2図に示したくし状の側方ヨーク11
の如き形状の場合でも本考案の基本的構成を満た
すことは一応可能であり、それなりの効果は発揮
できる。 The present invention has been explained based on the above two embodiments. In this article, we have given an example in which a plurality of side yokes 15 are integrated in order to simultaneously fix a plurality of former free ends of the side yokes, and the part where the leaf spring 1 comes out is made into a window shape. side yoke 11
Even in the case of a shape like this, it is possible to satisfy the basic structure of the present invention, and a certain effect can be achieved.
さらに本考案は、前記各実施例において使用し
た側方ヨークと板ばねを重ねて固定していた固定
板については、格段の必要があるわけではない。
特にこうした固定板を用いずとも固定する手段は
多くあり、それらはそれなりに有効だからであ
る。たとえば第13図にハンマ部分の断面図を示
したように、板ばね1の固定端を重ねた側方ヨー
ク15で固定し、側方ヨーク15が固定板を兼ね
ても勿論よいのである。このような場合でも側方
ヨーク15の自由端を引張り固定する手段21に
何の支障もなく、前記本考案の効果は確実に発揮
されている。すなわち、板ばね1の吸引吸着部付
近で板ばね1の側面と側方ヨーク15の側面とが
最短距離で対面して安定な余裕のある磁路を構成
するように、板ばね1、ヨーク4、側方ヨーク1
5、等々を直接接続固定をすればよいのである。 Furthermore, in the present invention, there is no particular need for the fixing plate used in each of the embodiments described above to fix the side yokes and leaf springs in an overlapping manner.
In particular, there are many means for fixing without using such a fixing plate, and these are effective in their own way. For example, as shown in the sectional view of the hammer portion in FIG. 13, the fixed ends of the leaf springs 1 may be fixed by overlapping side yokes 15, and the side yokes 15 may also serve as the fixing plate. Even in such a case, there is no problem with the means 21 for tensioning and fixing the free ends of the side yokes 15, and the effects of the present invention are reliably exhibited. That is, the leaf spring 1 and the yoke 4 are arranged so that the side surface of the leaf spring 1 and the side surface of the side yoke 15 face each other at the shortest distance near the suction part of the leaf spring 1 to form a stable magnetic path with sufficient margin. , lateral yoke 1
5, etc. can be directly connected and fixed.
以上本考案によると、高速でかつ安定な印字の
できる効率のよいスプリングチヤージ式ドツトラ
インプリンタの印字ヘツドが得られる。 As described above, according to the present invention, a printing head for an efficient spring charge type dot line printer capable of high-speed and stable printing can be obtained.
第1図は従来のスプリングチヤージ式ラインプ
リンタ印字ヘツド及びその使用形態を示す模式的
斜視図、第2図は従来の側方ヨークを取付けた印
字ヘツドを示す模式的斜視図、第3図は第2図の
板ばねの吸引吸着部周辺を拡大し磁束の流れを示
した部分斜視図、第4図は従来の印字ヘツドの等
価回路、第5図は側方ヨークを取付けたヘツドの
等価回路、第6図は従来の側方ヨークを取付けた
印字ヘツドの模式的断面図、第7図は第6図の板
ばねの吸引吸着周辺を拡大した模式的断面図、第
8図は本考案の一実施例である印字ヘツドを用い
たラインプリンタの構成概念を示す部分切欠き斜
視図、第9図は第8図の断面図、第10図は第2
図示した従来の側方ヨークを取付けた印字ヘツド
と第6図に示した本考案の印字ヘツドとについて
板ばね・ヨーク間距離と吸引力との関係の一例を
対比して示した図、第11図は本考案の他の実施
例を模式的に示した部分切欠き斜視図、第12図
は第11図の断面図、第13図は側方ヨークが固
定板を兼ねた場合の本考案の他の実施例を示す模
式的部分断面図である。
図中各記号はそれぞれ次のものを示す。1……
板ばね、2……ベース、3……固定板、4……ヨ
ーク、5……永久磁石、6……コイル、7……ハ
ンマピン、8……プラテン、9……インクリボ
ン、10……用紙、11……従来の側方ヨーク、
12……板ばねに流れる磁束、13……側方ヨー
クに流れる磁束、14……ヨークの先端面、15
……本考案の側方ヨーク、16……支柱板、17
……側方ヨークの内側の面、18……スペーサ、
19……従来の側方ヨークを使つた印字ヘツドの
板ばね・ヨーク間の距離と吸引力との関係の一
例、20……本考案の側方ヨークを使つた印字ヘ
ツドの板ばね・ヨーク間の距離と吸引力との関係
の一例、21……本考案の他の実施例の支柱板、
22……印字ヘツドベース、23……ハウジン
グ。φp……磁石より生じる磁束、φ……板ば
ね・ヨークの吸引部に流れる磁束、φs……板ば
ね自身に流れ、板ばねが飽和するときの磁束、P
t……磁石から板ばね吸引部までの漏れのパーミ
アンス、Pg……板ばね・ヨーク間の吸引部のパ
ーミアンス、Ps……板ばねの飽和するときのパ
ーミアンス、Pl……板ばねと側方ヨーク間のパ
ーミアンス。
Fig. 1 is a schematic perspective view showing a conventional spring charge type line printer print head and its usage pattern, Fig. 2 is a schematic perspective view showing a print head with a conventional side yoke attached, and Fig. 3 is a schematic perspective view showing a print head with a conventional side yoke attached. Figure 2 is a partial perspective view showing the flow of magnetic flux by enlarging the area around the attraction part of the leaf spring, Figure 4 is an equivalent circuit of a conventional print head, and Figure 5 is an equivalent circuit of a head with a side yoke attached. , Fig. 6 is a schematic sectional view of a printing head with a conventional side yoke attached, Fig. 7 is an enlarged schematic sectional view of the vicinity of the suction suction of the leaf spring in Fig. 6, and Fig. 8 is a schematic sectional view of the printing head with a conventional side yoke attached. A partially cutaway perspective view showing the structural concept of a line printer using a print head according to an embodiment, FIG. 9 is a sectional view of FIG. 8, and FIG.
11 is a diagram showing an example of the relationship between the distance between the leaf spring and the yoke and the suction force for the conventional print head shown in the figure and the print head of the present invention shown in FIG. 6; FIG. The figure is a partially cutaway perspective view schematically showing another embodiment of the present invention, FIG. 12 is a sectional view of FIG. 11, and FIG. FIG. 7 is a schematic partial cross-sectional view showing another embodiment. Each symbol in the figure indicates the following. 1...
Leaf spring, 2... Base, 3... Fixed plate, 4... Yoke, 5... Permanent magnet, 6... Coil, 7... Hammer pin, 8... Platen, 9... Ink ribbon, 10... Paper , 11... conventional side yoke,
12... Magnetic flux flowing in the leaf spring, 13... Magnetic flux flowing in the side yoke, 14... Tip surface of the yoke, 15
... Side yoke of the present invention, 16 ... Support plate, 17
...Inner surface of the side yoke, 18...Spacer,
19...An example of the relationship between the distance between the leaf spring and the yoke of the print head using the conventional side yoke and the suction force, 20...The relationship between the leaf spring and the yoke of the print head using the side yoke of the present invention An example of the relationship between the distance and the suction force, 21... Support plate of another embodiment of the present invention,
22...print head base, 23...housing. φ p ...Magnetic flux generated by the magnet, φ...Magnetic flux flowing to the attraction part of the leaf spring/yoke, φ s ...Magnetic flux flowing to the leaf spring itself and when the leaf spring is saturated, P
t ...Leakage permeance from the magnet to the leaf spring suction part, Pg ...Permeance of the suction part between the leaf spring and yoke, Ps ...Permeance when the leaf spring is saturated, Pl ...Leakage between the leaf spring and the yoke Permeance between lateral yokes.
Claims (1)
を用いて片持ち板ばねの自由端近傍をヨーク面に
吸引することにより前記板ばねに生ずる歪みエネ
ルギを印字エネルギ源としたハンマ機構に、前記
板ばねの両側に配列した側方ヨークを設け、前記
永久磁石とヨーク、板ばね、側方ヨークとで閉磁
路を形成した印字ハンマを複数個並列に配置した
スプリングチヤージ式ドツトラインプリンタ印字
ヘツドにおいて、前記側方ヨークはその一端を前
記ヨークの一端に固定し、しかも前記板ばねの自
由端がヨークへ吸着している状態で前記板ばねの
吸着面と前記側方ヨークの板ばね吸引方向の面と
が実効的に一致するように前記側方ヨーク頭部の
自由端を前記板ばねの吸引方向にたわませかつ固
定してある、ここを特徴とするドツト式ラインプ
リンタ印字ヘツド。 The plate is attached to a hammer mechanism that uses strain energy generated in the plate spring as a printing energy source by attracting the vicinity of the free end of the cantilever plate spring to the yoke surface using a suction mechanism configured with a permanent magnet and a yoke. In a spring charge type dot line printer print head, in which side yokes are arranged on both sides of a spring, and a plurality of print hammers are arranged in parallel, each of which has a closed magnetic path formed by the permanent magnet, the yoke, the leaf spring, and the side yoke. , one end of the side yoke is fixed to one end of the yoke, and in a state where the free end of the leaf spring is attracted to the yoke, the attraction surface of the leaf spring and the leaf spring suction direction of the side yoke are A dot-type line printer print head characterized in that the free end of the side yoke head is bent in the suction direction of the leaf spring and fixed so that the side yoke head is effectively aligned with the surface of the print head.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP18868681U JPS5894531U (en) | 1981-12-18 | 1981-12-18 | Dot type line printer print head |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP18868681U JPS5894531U (en) | 1981-12-18 | 1981-12-18 | Dot type line printer print head |
Publications (2)
Publication Number | Publication Date |
---|---|
JPS5894531U JPS5894531U (en) | 1983-06-27 |
JPS6212609Y2 true JPS6212609Y2 (en) | 1987-04-01 |
Family
ID=30102984
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP18868681U Granted JPS5894531U (en) | 1981-12-18 | 1981-12-18 | Dot type line printer print head |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS5894531U (en) |
Citations (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS5551568A (en) * | 1978-10-09 | 1980-04-15 | Fujitsu Ltd | Printing head |
JPS5649279A (en) * | 1979-09-28 | 1981-05-02 | Fujitsu Ltd | Releasing type printer head |
-
1981
- 1981-12-18 JP JP18868681U patent/JPS5894531U/en active Granted
Patent Citations (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS5551568A (en) * | 1978-10-09 | 1980-04-15 | Fujitsu Ltd | Printing head |
JPS5649279A (en) * | 1979-09-28 | 1981-05-02 | Fujitsu Ltd | Releasing type printer head |
Also Published As
Publication number | Publication date |
---|---|
JPS5894531U (en) | 1983-06-27 |
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