JPH0457500B2 - - Google Patents

Info

Publication number
JPH0457500B2
JPH0457500B2 JP1244283A JP1244283A JPH0457500B2 JP H0457500 B2 JPH0457500 B2 JP H0457500B2 JP 1244283 A JP1244283 A JP 1244283A JP 1244283 A JP1244283 A JP 1244283A JP H0457500 B2 JPH0457500 B2 JP H0457500B2
Authority
JP
Japan
Prior art keywords
liquid
heat
jet recording
lmin
liquid chamber
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
JP1244283A
Other languages
Japanese (ja)
Other versions
JPS59138459A (en
Inventor
Toshitami Hara
Yasuhiro Yano
Masahiro Haruta
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.)
Canon Inc
Original Assignee
Canon Inc
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 Canon Inc filed Critical Canon Inc
Priority to JP1244283A priority Critical patent/JPS59138459A/en
Publication of JPS59138459A publication Critical patent/JPS59138459A/en
Publication of JPH0457500B2 publication Critical patent/JPH0457500B2/ja
Granted legal-status Critical Current

Links

Classifications

    • BPERFORMING OPERATIONS; TRANSPORTING
    • B41PRINTING; LINING MACHINES; TYPEWRITERS; STAMPS
    • B41JTYPEWRITERS; SELECTIVE PRINTING MECHANISMS, i.e. MECHANISMS PRINTING OTHERWISE THAN FROM A FORME; CORRECTION OF TYPOGRAPHICAL ERRORS
    • B41J2/00Typewriters or selective printing mechanisms characterised by the printing or marking process for which they are designed
    • B41J2/005Typewriters or selective printing mechanisms characterised by the printing or marking process for which they are designed characterised by bringing liquid or particles selectively into contact with a printing material
    • B41J2/01Ink jet
    • B41J2/135Nozzles
    • B41J2/14Structure thereof only for on-demand ink jet heads
    • B41J2/14016Structure of bubble jet print heads
    • B41J2/14032Structure of the pressure chamber
    • B41J2/1404Geometrical characteristics
    • BPERFORMING OPERATIONS; TRANSPORTING
    • B41PRINTING; LINING MACHINES; TYPEWRITERS; STAMPS
    • B41JTYPEWRITERS; SELECTIVE PRINTING MECHANISMS, i.e. MECHANISMS PRINTING OTHERWISE THAN FROM A FORME; CORRECTION OF TYPOGRAPHICAL ERRORS
    • B41J2/00Typewriters or selective printing mechanisms characterised by the printing or marking process for which they are designed
    • B41J2/005Typewriters or selective printing mechanisms characterised by the printing or marking process for which they are designed characterised by bringing liquid or particles selectively into contact with a printing material
    • B41J2/01Ink jet
    • B41J2/135Nozzles
    • B41J2/14Structure thereof only for on-demand ink jet heads
    • B41J2002/14387Front shooter
    • BPERFORMING OPERATIONS; TRANSPORTING
    • B41PRINTING; LINING MACHINES; TYPEWRITERS; STAMPS
    • B41JTYPEWRITERS; SELECTIVE PRINTING MECHANISMS, i.e. MECHANISMS PRINTING OTHERWISE THAN FROM A FORME; CORRECTION OF TYPOGRAPHICAL ERRORS
    • B41J2/00Typewriters or selective printing mechanisms characterised by the printing or marking process for which they are designed
    • B41J2/005Typewriters or selective printing mechanisms characterised by the printing or marking process for which they are designed characterised by bringing liquid or particles selectively into contact with a printing material
    • B41J2/01Ink jet
    • B41J2/135Nozzles
    • B41J2/14Structure thereof only for on-demand ink jet heads
    • B41J2002/14467Multiple feed channels per ink chamber

Landscapes

  • Physics & Mathematics (AREA)
  • Geometry (AREA)
  • Particle Formation And Scattering Control In Inkjet Printers (AREA)

Description

【発明の詳細な説明】[Detailed description of the invention]

本発明は、吐出口より液体を吐出することで形
成された飛翔的液滴を用いて記録を行う液体噴射
記録装置、殊に熱エネルギーを利用する液体噴射
記録装置に関する。 液体噴射記録装置には、種々の方式があるが、
その中でも、例えば独国公開公報(OLS)
2944005号公報に開示された液体噴射記録装置は、
高速カラー記録が容易であつて、その出力部の主
要部である記録ヘツドは、記録用の液体を吐出し
て、飛翔的液滴を形成するための吐出口(オリフ
イス)を高密度に配列することができるために、
高解像力を得ることができると同時に、記録ヘツ
ドとして全体的にはコンパクト化が計れ、且つ量
産に向くこと、更には半導体分野において技術の
進歩と信頼性の向上が著しいIC技術やマイクロ
加工技術の長所を十二分に利用することで長尺化
及び面状化(2次元化)が容易であること等のた
めに、最近富みに熱い注目を集めている。 しかしながら、従来の記録ヘツドは、マルチオ
リフイス化タイプの場合、各オリフイスに対応し
た液流路を設け、該液流路毎に、該液流路を満た
す液体に熱エネルギーを作用させて対応するオリ
フイスより液体を吐出して、飛翔的液体を形成す
る手段としての電気熱変換体が設けられ、各液流
路には、各液流路に連通している共通液室より液
体が供給される構造となつているために、高密度
にオリフイスを配列する構造にすると前記の各液
流路は必然的に狭くなつて液流路壁抵抗が増大
し、高速記録の際には液供給(refill)が追随で
きなくなり、液滴形成が不安定になつて、高品位
の画質の画像を高速で記録することができなくな
るという問題が生じた。 この高速記録を行う場合の液供給の問題を解決
する一案として液供給がスピーデイ且つスムース
に行えるようにするために、各液流路間の液流路
壁を取り除いて、大きな空間を有する液室とし、
該液室に充分な量の液体がスピーデイ且つスムー
スに供給されるように液供給経路を設計すること
が検討されている。しかしながら、この場合に
は、隣り合う電気熱変換体間には隔離壁がないた
めに、隣り合うオリフイス間に於いて液吐出に相
互作用が生じ、各オリフイスより独立して液吐出
を行うことが難しくなる。すなわち、例えば隣り
合うオリフイスに対応する電気熱変換体をそれぞ
れ独立に駆動した場合、ONされた電気熱変換体
に対応したオリフイスより液吐出がなされると同
時に、隣りのOFF状態にある電気熱変換体に対
応するオリフイスよりも液吐出がなされるか、あ
るいは液吐出が完全になされなくともメニスカス
の移動や振動が起り、隣のオリフイスの安定的液
吐出に悪影響を与える干渉作用を引き起す。従つ
て、このような干渉作用があると、各オリフイス
から吐出される液体の吐出状態は不安定になり、
形成される液滴の飛翔スピード、飛翔方向、液滴
径等が安定せず、品質の高い画像を記録すること
ができなくなる場合が少なくない。 このことは、オリフイスを高密度で配列させて
高品位の画質を有する画像を高速で記録する場合
には、電気熱変換体より発生される熱エネルギー
量の増大に伴つて極めて深刻な問題となる。 本発明は、上記の諸点に鑑み成されたものであ
つて、高密度で高速記録が容易に行える液体噴射
記録装置を提供することを主たる目的とする。 本発明の別の目的は、高品質の画像記録に適し
た液体噴射記録装置を提供することである。 本発明の液体噴射記録装置は、熱エネルギーの
利用によつて液体を吐出し飛翔的液滴を形成する
ために設けられた複数の吐出口と、これ等の吐出
口に連通し、前記飛翔的液滴を形成するための液
体が供給される液室と、該液室に前記液体を供給
するための供給口と、前記吐出のそれぞれに対応
して設けられた、前記熱エネルギーを発生する手
段としての複数の電気熱変換体とを具備し、該電
気熱変換体のそれぞれは、発生される熱エネルギ
ーが前記液体に作用する面としての熱作用面を前
記液室の底面にし、前記吐出口のそれぞれは、該
底面に相い向かいあつて設けられてなる液体噴射
記録装置に於いて、それぞれ隣接する熱作用面間
及び吐出口間を隔離する前記液室内に設けられる
隔離壁が、該隔離壁を貫通せずに測定される前記
熱作用面間の距離の最小値をLmin、該熱作用面
とそれに対応する吐出口の中心との距離をDohと
したときに、1≦Lmin/Doh≦500なる関係式を
満たすよう設置されることを特徴とする。 上記のような構成を有する本発明の液体噴射記
録装置は、記録信号に対する応答の忠実性と確実
性に優れ、高解像度で高品質の画像を高速で記録
することができる。 以下、本発明を図面に従つて、更に具体的に説
明する。 第1図乃至第3図は、本発明に係る液体噴射記
録装置の概要を示した図であり、第1図は模式的
斜視図、第2図は第1図の一点鎖線ABで切断し
た場合の模式的切断図、第3図は内部構造を説明
するための模式的分解図である。 第1図乃至第3図に示される液体噴射記録装置
100は、基板101と、基板101上に設けら
れたn個の電気変換体102(図においては、第
一番目、第二番目及び第n番目の電気変換体が示
されている)と、液室110を形成するための、
前壁板103、後壁板105及びこれ等の壁板1
03,105にその両端で挟持されている二つの
側壁板104−1,104−2(第1図では一方
の側壁板は見えないが、第3図にその一部が見え
る)と、各電気熱変換体に対応して設けられるオ
リフイス108を構成する貫孔109が設けられ
たオリフイス板107と、側壁板104−1の後
方側面に付設された液室110に液体を供給する
ために設けれる供給管106とで主に構成され
る。 電気熱変換体102は、基板101上に基板側
から順に発熱抵抗層111、発熱抵抗層111の
一部を除いて発熱抵抗層111上に並列的に設け
られた、選択電極112、共通電極114、液室
110内の液体に直接接触する部分には少なくと
も設けられている保護層113とで構成される。 発熱抵抗層111は選択電極112と共通電極
114とを通じて通電されることによつて、これ
等の電極の間の熱発生部116で主に熱エネルギ
ーを発生する。熱作用面115は、発生した熱が
液体に作用するところであり、熱発生部116と
密接な関係がある。この熱作用面115での熱作
用により液体中にバルブが発生し、その圧力エネ
ルギーにより液体がオリフイス108から飛翔的
液滴となつて吐出され記録が実施される。 電気変換体102のそれぞれを記録信号に従つ
て駆動させて所定のオリフイス108から液滴を
吐出させるには、選択される選択電極112と共
通電極114とを通じて信号電圧を供給すること
によつて実施される。 以上説明した従前の液体噴射記録装置の構成に
加え、本発明の液体噴射記録装置に於いては、そ
れぞれ隣接する熱作用面間115及びオリフイス
108間を隔離する特定された構成を有する隔離
壁117が設けられる。 この隔離壁117は前述した各オリフイスに対
応した液流路を設ける個別液流路方式の問題点、
すなわち液供給が遅いために高周波数下の追随特
性が悪いこと、並びにで大液室個方式の問題点、
すなわち隣接オリフイス間に液吐出の干渉作用が
生じること、この両者を同時に解決するために設
けられるもので、そのためには以下に詳述する関
係式を満たすような構成の隔離壁でなければなら
ない。 すなわち、隔離壁を貫通せずに測定される熱作
用面間の距離のうちの最小値をLmin、熱作用面
とそれに対応するオリフイスの中じとの距離を
Dohとしたときに、1≦Lmin/Doh≦500なる関
係式を満たすよう設置される必要がある。 本発明の上記関係式の意味するところをより明
確にするために、本発明の一実施態様例に於ける
熱作用面と隔離壁が設けられた部分の部分拡大平
面図である第4図及びその一点鎖線XYで切断し
た切断図である第5図を用いてこれらをより具体
的に説明する。 熱作用面115は熱発生部116を液室底面に
垂直上方に投影した部分を指し、熱作用面間の距
離はL0で示されるが、隔離壁117を貫通せず
に測定される熱作用面間の距離とはL1やL2のよ
うに隔離壁117迂回して測定される距離であ
り、これら数多く測定される距離のうち最も短い
ものの値がLminとされる。一方、熱作用面とそ
れに対応する熱エネルギーの中心との距離Dohは
第5図に示されるよう一般的には各熱作用面及び
オリフイスについて一定の値をとるが、その値が
一定ではない場合には、測定される距離のうち最
とも短いものの値をDohとする。 熱作用面とオリフイスの中心との距離Dohに対
して隔離壁を貫通せずに測定される熱作用面間の
最小距離Lminが上記範囲に達しない程隔離壁1
17の長さが短い場合には、隣接オリフイス間に
液吐出の干渉作用が生じ、逆に隔離壁117の長
さが上記の範囲を超える程長い場合には、従来の
個別液流路方式の場合と同様、高周波数下の追随
特性が悪くなる。本発明の効果をより発揮させる
には、1≦Lmin/Doh≦100であることが好まし
く、2≦Lmin/Doh≦40であることが更に好ま
しく、最適には4≦Lmin/Doh≦20となるよう
隔離壁を設けるのがよい。 隔離壁117は、オリフイス板107と液室1
10の底面を構成する保護層113とに接して設
けられるが、前壁板103とは第3図の場合のよ
うに接していてもよいし、あるいは第4図の場合
のように接していなくともよい。 第6及び7図は本発明の液体噴射記録装置に於
ける隔離壁117の設置様式の変形例を示した模
式図であり、第6図は各隔離壁117の長さが
種々異なるものを設置した例で、この場合には
LminはL1乃至L4のうちの最小値とされる。ま
た、第7は図隔離壁117により液室を二分割
し、隣接する熱作用面が交互に一方の液室に属す
るようにした例であり、この場合には隔離壁11
7を貫通せずに測定される熱作用面間の距離は隣
接する熱作用面間の距離ではなくて一つおいた熱
作用面間の距離として測定され、L1及びL2のう
ちの小さい方の値がLminとされる。 以下、本発明を実施例に従つてより具体的に説
明する。 実施例 1 表面を熱酸化してSiO2層を3μm厚に形成したSi
基板をエツチングにより共通液室部分として
100μm取り除いた。次に発熱抵抗層としてTa層
を2000Å厚、電極としてAl層を、1μm厚積層し
た後、フオトリソ工程により形状40μm×100μm
の熱発生部(ヒーター)アレーを100μmピツチで
形成した。また、Ta層の酸化防止及びインク液
の浸透防止、液体が熱エネルギーを受けた際に発
生されるバブルによる耐機械的衝撃用の膜とし
て、SiO2層0.5μm厚、SiC層1μm厚を順次スパツ
タリングにより積層して保護層を形成した。 次にこの基板上に第1〜3図で示されるような
幅が50μmで高さが80μmの隔離壁、前壁板、後壁
板、二つの側壁板、オリフイス板及び供給管を設
置し液体噴射記録装置を作製した。隔離壁で仕切
られる液流路の幅は50μm、共通液室(ここでは
隔離壁で仕切られている液流路部分は含まない)
と熱作用面間の距離は500μmであり、Lminは約
1050μmであつた。オリフイス板は40μm厚のニク
ロム板からなり、エツチングにより35μm径のオ
リフイスがそれぞれの熱作用面の真上に位置する
よう形成されている。したがつて、熱作用面とオ
リフイスの中心との距離Dohはいづれも120μmで
あつた。 この液体噴射記録装置に対して6μsecの矩形電
圧を与えて駆動させた。この場合の液滴吐出の最
高周波数応答fmaxは7KHzであり、隣接オリフイ
ス間に液吐出の干渉作用は生じなかつた。 実施例2〜7及び比較例1 実施例1において、設置する隔離壁の長さを
種々変更したことを除いては、実施例1と同様な
液体噴射記録装置を作製した。これらの液体噴射
記録装置について実施例1と同様な条件下で該装
置を駆動させ、最高周波数応答fmaxと隣接オリ
フイス間の液吐出の干渉作用の有無について評価
した。その結果を第1表に示す。 この結果から、Lmin/Dohが1以上の場合に
は隣接オリフイス間の液吐出の干渉作用がかなり
抑制され、Lmin/Dohが2以上の場合には干渉
作用が殆ど抑制されることが判明した。また、
Lmin/Dohが500を超える場合には最高周波数応
答fmaxがかなり低下することが判明した。 実施例 8 実施例1において、設置する隔離壁の高さを
50μm、共通液室と熱作用面間の距離を320μm、
オリフイス板を30μm厚のものを使用したことを
除いては実施例1と同様な液体噴射記録装置を作
製した。すなわちこの装置ではLminは約690μm
であり、Dohは80μmであり、Lmin/Dohは、8.6
で実施例1とほぼ同様な値を取るものであつた。
この装置について実施例1と同様な条件下で該装
置を駆動させたところ、最高周波数応答fmaxは
7KHzで実施例1とほぼ同様な値を取り、もちろ
ん隣接オリフイス間に液吐出の干渉作用は生じな
かつた。 実施例9〜15及び比較例2、3 実施例1において、基板上に形状80μm×
100μmのヒーターアレーを100μmピツチで形成し
たこと、オリフイス板として20μm厚のものを使
用したこと、幅が20μmで高さが20μmの隔離壁の
長さを種々変更して設置したこと、を除いては実
施例1と同様な液体噴射記録装置を作製した。す
なわちこの装置では、Dohは40μmである。これ
らの液体噴射記録装置について実施例1と同様な
条件下で該装置を駆動させ、最高周波数応答
fmaxと隣接オリフイス間の液吐出の干渉作用の
有無について評価した。その結果を第2表に示
す。
The present invention relates to a liquid jet recording device that performs recording using flying droplets formed by discharging liquid from a discharge port, and particularly to a liquid jet recording device that uses thermal energy. There are various types of liquid jet recording devices, but
Among them, for example, the German Open Gazette (OLS)
The liquid jet recording device disclosed in Publication No. 2944005 is
High-speed color recording is easy, and the recording head, which is the main part of the output section, has ejection ports (orifices) arranged in high density for ejecting recording liquid and forming flying droplets. In order to be able to
At the same time, it is possible to obtain high resolution, and at the same time, it is possible to make the recording head more compact and suitable for mass production.Furthermore, in the semiconductor field, technological advances and reliability improvements are remarkable, such as IC technology and microprocessing technology. Recently, it has been attracting a lot of attention because it is easy to make it long and planar (two-dimensional) by making full use of its advantages. However, in the case of a conventional recording head of the multi-orifice type, a liquid flow path is provided corresponding to each orifice, and thermal energy is applied to the liquid filling the liquid flow path for each liquid flow path to create a corresponding orifice. An electrothermal converter is provided as a means for ejecting liquid to form flying liquid, and each liquid flow path is supplied with liquid from a common liquid chamber communicating with each liquid flow path. Therefore, if the orifices are arranged in a high-density structure, each liquid flow path will inevitably become narrower and the wall resistance of the liquid flow path will increase.During high-speed recording, the liquid supply (refill) A problem arose in that the droplet formation became unstable, making it impossible to record high-quality images at high speed. One way to solve this problem of liquid supply when performing high-speed recording is to remove the liquid flow path walls between each liquid flow path so that the liquid supply can be performed quickly and smoothly. As a room,
Studies are underway to design a liquid supply path so that a sufficient amount of liquid can be quickly and smoothly supplied to the liquid chamber. However, in this case, since there is no separation wall between adjacent electrothermal converters, interaction occurs in liquid discharge between adjacent orifices, and liquid cannot be discharged independently from each orifice. It becomes difficult. In other words, for example, if electrothermal transducers corresponding to adjacent orifices are driven independently, liquid will be discharged from the orifice corresponding to the electrothermal transducer that is turned on, and at the same time, the electrothermal transducer that is in the OFF state will discharge liquid. Even if the liquid is ejected more than the corresponding orifice, or even if the liquid is not completely ejected, the meniscus moves or vibrates, causing an interference effect that adversely affects the stable liquid ejection of the adjacent orifice. Therefore, if there is such an interference effect, the discharge state of the liquid discharged from each orifice will become unstable.
In many cases, the flying speed, flying direction, droplet diameter, etc. of the formed droplets are not stable, making it impossible to record a high quality image. This becomes an extremely serious problem as the amount of thermal energy generated by the electrothermal converter increases when high-quality images are recorded at high speed by arranging orifices at high density. . The present invention has been made in view of the above points, and a main object of the present invention is to provide a liquid jet recording device that can easily perform high-density and high-speed recording. Another object of the present invention is to provide a liquid jet recording device suitable for recording high quality images. The liquid jet recording device of the present invention has a plurality of ejection ports provided for ejecting liquid to form flying droplets by using thermal energy, and a plurality of ejection ports communicating with these ejection ports to form flying droplets. A liquid chamber to which a liquid for forming droplets is supplied, a supply port for supplying the liquid to the liquid chamber, and means for generating the thermal energy, which are provided corresponding to each of the discharges. a plurality of electrothermal converters, each of which has a heat acting surface on which generated thermal energy acts on the liquid, the bottom surface of the liquid chamber, and a bottom surface of the liquid chamber; In each of the liquid jet recording devices provided opposite to each other on the bottom surface, a separation wall provided in the liquid chamber that isolates the adjacent heat acting surfaces and the ejection ports, respectively, When Lmin is the minimum distance between the heat acting surfaces measured without penetrating the wall, and Doh is the distance between the heat acting surfaces and the center of the corresponding discharge port, 1≦Lmin/Doh≦ It is characterized by being installed to satisfy a relational expression of 500. The liquid jet recording apparatus of the present invention having the above configuration has excellent fidelity and reliability of response to recording signals, and can record high-resolution, high-quality images at high speed. Hereinafter, the present invention will be explained in more detail with reference to the drawings. 1 to 3 are diagrams showing an outline of the liquid jet recording device according to the present invention, in which FIG. 1 is a schematic perspective view, and FIG. 2 is a diagram taken along the dashed-dotted line AB in FIG. 1. FIG. 3 is a schematic exploded view for explaining the internal structure. The liquid jet recording apparatus 100 shown in FIGS. 1 to 3 includes a substrate 101, and n electrical transducers 102 (in the figure, a first, a second, and an n-th electrical converter) provided on the substrate 101. (the second electrical transducer is shown) and a liquid chamber 110 for forming the liquid chamber 110.
Front wall board 103, rear wall board 105, and these wall boards 1
The two side wall plates 104-1 and 104-2 (one of the side wall plates is not visible in Fig. 1, but a part of it is visible in Fig. 3) held at both ends by the 03 and 105, and each electric An orifice plate 107 provided with a through hole 109 constituting an orifice 108 provided corresponding to the heat converter and a liquid chamber 110 attached to the rear side of the side wall plate 104-1 are provided for supplying liquid. It is mainly composed of a supply pipe 106. The electrothermal converter 102 includes a heating resistance layer 111, a selection electrode 112, and a common electrode 114, which are provided in parallel on the heating resistance layer 111 except for a part of the heating resistance layer 111, in order from the substrate side on the substrate 101. , and a protective layer 113 provided at least in a portion that directly contacts the liquid in the liquid chamber 110. When the heat generating resistive layer 111 is energized through the selection electrode 112 and the common electrode 114, it mainly generates thermal energy in the heat generating portion 116 between these electrodes. The heat acting surface 115 is a place where the generated heat acts on the liquid, and is closely related to the heat generating part 116. A valve is generated in the liquid due to the heat action on the heat action surface 115, and the pressure energy causes the liquid to be ejected from the orifice 108 as a flying droplet, thereby performing recording. Driving each of the electrical transducers 102 in accordance with a recording signal to eject a droplet from a predetermined orifice 108 is performed by supplying a signal voltage through a selected selection electrode 112 and a common electrode 114. be done. In addition to the configuration of the conventional liquid jet recording device described above, in the liquid jet recording device of the present invention, a separation wall 117 having a specified configuration that isolates the adjacent heat acting surfaces 115 and the orifice 108, respectively. is provided. This separation wall 117 has the problems of the individual liquid flow path method in which liquid flow paths are provided corresponding to each orifice as described above.
In other words, the tracking characteristics at high frequencies are poor due to the slow liquid supply, and the problems with the large liquid chamber individual system.
That is, the separation wall is provided to simultaneously solve both of the problems of liquid discharge interference occurring between adjacent orifices, and for this purpose, the separation wall must be configured to satisfy the relational expression described in detail below. That is, Lmin is the minimum distance between the heat-active surfaces measured without penetrating the separating wall, and the distance between the heat-active surface and the center of the corresponding orifice is Lmin.
When Doh is set, it must be installed so that the relational expression 1≦Lmin/Doh≦500 is satisfied. In order to clarify the meaning of the above relational expression of the present invention, FIGS. These will be explained in more detail using FIG. 5, which is a cutaway view taken along the dashed line XY. The heat action surface 115 refers to the part of the heat generating section 116 projected vertically upward onto the bottom surface of the liquid chamber, and the distance between the heat action surfaces is indicated by L 0 , but the heat action surface 115 is the part where the heat action is measured without penetrating the separation wall 117. The distance between surfaces is a distance measured by bypassing the separation wall 117, such as L1 and L2 , and the shortest value among these many measured distances is taken as Lmin. On the other hand, the distance Doh between the heat acting surface and the center of the corresponding thermal energy generally takes a constant value for each heat acting surface and orifice, as shown in Figure 5, but if this value is not constant. In this case, Doh is the shortest value among the measured distances. Separation wall 1 is such that the minimum distance Lmin between the heat action surfaces measured without penetrating the separation wall does not reach the above range for the distance Doh between the heat action surface and the center of the orifice.
If the length of the separating wall 117 is short, interference effect of liquid discharge occurs between adjacent orifices, and conversely, if the length of the separating wall 117 is so long that it exceeds the above range, the conventional individual liquid flow path method As in the case, the tracking characteristics at high frequencies deteriorate. In order to make the effects of the present invention more effective, it is preferable that 1≦Lmin/Doh≦100, more preferably 2≦Lmin/Doh≦40, and optimally 4≦Lmin/Doh≦20. It is a good idea to install an isolation wall. The isolation wall 117 separates the orifice plate 107 and the liquid chamber 1.
Although it is provided in contact with the protective layer 113 constituting the bottom surface of 10, it may be in contact with the front wall plate 103 as in the case of FIG. 3, or it may not be in contact with the front wall plate 103 as in the case of FIG. Tomoyoshi. 6 and 7 are schematic diagrams showing a modification of the installation style of the separation walls 117 in the liquid jet recording device of the present invention, and FIG. 6 shows the installation of the separation walls 117 having various lengths. In this case,
Lmin is the minimum value among L1 to L4 . In addition, the seventh example is an example in which the liquid chamber is divided into two by a separating wall 117, and adjacent heat-acting surfaces alternately belong to one liquid chamber. In this case, the separating wall 117
The distance between heat-active surfaces measured without penetrating 7 is not measured as the distance between adjacent heat-active surfaces, but as the distance between adjacent heat-active surfaces, and is the smaller of L 1 and L 2 . This value is taken as Lmin. Hereinafter, the present invention will be explained in more detail according to Examples. Example 1 Si whose surface was thermally oxidized to form two SiO layers with a thickness of 3 μm
By etching the substrate as a common liquid chamber part
100 μm was removed. Next, a Ta layer with a thickness of 2000 Å as a heating resistance layer and an Al layer with a thickness of 1 μm as an electrode were laminated, and then a photolithography process was performed to form a shape of 40 μm x 100 μm.
A heat generating part (heater) array was formed with a pitch of 100 μm. In addition, as a film to prevent oxidation of the Ta layer, to prevent penetration of ink liquid, and to resist mechanical shock caused by bubbles generated when the liquid receives thermal energy, we sequentially added two 0.5 μm thick SiO layers and 1 μm thick SiC layer. A protective layer was formed by laminating by sputtering. Next, on this substrate, as shown in Figures 1 to 3, an isolation wall with a width of 50 μm and a height of 80 μm, a front wall plate, a rear wall plate, two side wall plates, an orifice plate, and a supply pipe are installed. An injection recording device was created. The width of the liquid flow path partitioned by the separation wall is 50μm, and the common liquid chamber (here, the liquid flow path section partitioned by the separation wall is not included).
The distance between and the heat acting surface is 500μm, and Lmin is approximately
It was 1050μm. The orifice plate is made of a nichrome plate with a thickness of 40 μm, and an orifice with a diameter of 35 μm is formed by etching so as to be located directly above each heat-active surface. Therefore, the distance Doh between the heat acting surface and the center of the orifice was 120 μm in each case. This liquid jet recording device was driven by applying a rectangular voltage of 6 μsec. In this case, the highest frequency response fmax of droplet ejection was 7KHz, and no interference effect of liquid ejection occurred between adjacent orifices. Examples 2 to 7 and Comparative Example 1 A liquid jet recording device similar to that of Example 1 was manufactured except that the length of the separating wall to be installed was variously changed. These liquid jet recording devices were driven under the same conditions as in Example 1, and the highest frequency response fmax and the presence or absence of interference in liquid ejection between adjacent orifices were evaluated. The results are shown in Table 1. From this result, it was found that when Lmin/Doh is 1 or more, the interference effect of liquid discharge between adjacent orifices is considerably suppressed, and when Lmin/Doh is 2 or more, the interference effect is almost suppressed. Also,
It was found that when Lmin/Doh exceeds 500, the maximum frequency response fmax decreases considerably. Example 8 In Example 1, the height of the isolation wall to be installed was
50μm, distance between common liquid chamber and heat acting surface 320μm,
A liquid jet recording device similar to that of Example 1 was manufactured except that an orifice plate having a thickness of 30 μm was used. In other words, with this device, Lmin is approximately 690μm
, Doh is 80 μm, and Lmin/Doh is 8.6
The value was almost the same as in Example 1.
When this device was driven under the same conditions as in Example 1, the highest frequency response fmax was
At 7 KHz, the value was almost the same as in Example 1, and of course no interference effect of liquid discharge occurred between adjacent orifices. Examples 9 to 15 and Comparative Examples 2 and 3 In Example 1, a shape of 80 μm×
Except for forming a 100μm heater array with a 100μm pitch, using a 20μm thick orifice plate, and installing various lengths of isolation walls with a width of 20μm and a height of 20μm. A liquid jet recording device similar to that of Example 1 was manufactured. That is, in this device, Doh is 40 μm. These liquid jet recording devices were driven under the same conditions as in Example 1, and the highest frequency response was obtained.
The presence or absence of interference between fmax and liquid discharge between adjacent orifices was evaluated. The results are shown in Table 2.

【表】【table】

【表】【table】

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

第1図乃至第3図は、本発明に係る液体噴射記
録装置の概要を示した図であり、第1図は模式的
斜視図、第2図は第1図の一点鎖線ABで切断し
た場合の模式的切断図、第3図は内部構造を説明
するための模式的分解図である。第4図は本発明
の一実施態様例に於ける部分拡大平面図であり、
第5図は第4図の一点鎖線XYで切断した切断図
である。第6及び7図は本発明の液体噴射記録装
置に置ける隔離壁117の設置状態の変形例を示
した模式図である。 100:液体噴射記録装置、101:基板、1
02:電気変換体、103:前壁板、104:側
壁板、105:後壁板、106:供給管、10
7:オリフイス板、108:オリフイス、10
9:貫通、110:液室、111:発熱抵抗層、
112:選択電極、113:保護層、114:共
通電極、115:熱作用面、116:熱発生部、
117:隔離壁、Lmin:隔離壁を貫通せずに測
定される熱作用面間の距離のうちの最小値、
Doh:熱作用面とそれに対応するオリフイスの中
心との距離。
1 to 3 are diagrams showing an outline of a liquid jet recording device according to the present invention, in which FIG. 1 is a schematic perspective view, and FIG. 2 is a diagram taken along the dashed-dotted line AB in FIG. 1. FIG. 3 is a schematic exploded view for explaining the internal structure. FIG. 4 is a partially enlarged plan view of an embodiment of the present invention;
FIG. 5 is a cutaway view taken along the dashed line XY in FIG. 6 and 7 are schematic diagrams showing a modification of the installation state of the separation wall 117 in the liquid jet recording apparatus of the present invention. 100: Liquid jet recording device, 101: Substrate, 1
02: Electric converter, 103: Front wall plate, 104: Side wall plate, 105: Rear wall plate, 106: Supply pipe, 10
7: Orifice plate, 108: Orifice, 10
9: Penetration, 110: Liquid chamber, 111: Heat generating resistance layer,
112: Selective electrode, 113: Protective layer, 114: Common electrode, 115: Heat action surface, 116: Heat generating part,
117: Isolation wall, Lmin: Minimum distance between heat-active surfaces measured without penetrating the isolation wall,
Doh: Distance between the heat acting surface and the corresponding center of the orifice.

Claims (1)

【特許請求の範囲】 1 熱エネルギーの利用によつて液体を吐出し飛
翔的液滴を形成するために設けられた複数の吐出
口と、これ等の吐出口に連通し、前記飛翔的液滴
を形成するための液体が供給される液室と、該液
室に前記液体を供給するための供給口と、前記吐
出口のそれぞれに対応して設けられた、前記熱エ
ネルギーを発生する手段としての複数の電気熱変
換体とを具備し、該電気熱変換体のそれぞれは、
発生される熱エネルギーが前記液体に作用する面
としての熱作用面を前記液室の底面に有し、前記
吐出口のそれぞれは、該底面に相い向かいあつて
設けられてなる液体噴射記録装置に於いて、それ
ぞれ隣接する熱作用面間及び吐出口間を隔離する
前記液室内に設けられる隔離壁が、該隔離壁を貫
通せずに測定される前記熱作用面間の距離の最小
値をLmin、該熱作用面とそれに対応する吐出口
の中心との距離をDohとしたときに、 1≦Lmin/Doh≦500 なる関係式を満たすよう設置されることを特徴と
する液体噴射記録装置。
[Scope of Claims] 1. A plurality of ejection ports provided for ejecting liquid to form flying droplets by using thermal energy, and a plurality of ejection ports communicating with these ejection ports to form the flying droplets. The means for generating the thermal energy is provided corresponding to a liquid chamber to which a liquid is supplied to form a liquid, a supply port for supplying the liquid to the liquid chamber, and a discharge port. a plurality of electrothermal converters, each of the electrothermal converters comprising:
A liquid jet recording device having a heat acting surface on the bottom surface of the liquid chamber as a surface on which generated thermal energy acts on the liquid, and each of the ejection ports being provided opposite to the bottom surface. In this case, a separation wall provided in the liquid chamber that isolates adjacent heat-action surfaces and discharge ports, respectively, has a minimum value of the distance between the heat-action surfaces measured without penetrating the separation wall. A liquid jet recording device characterized in that it is installed so as to satisfy the relational expression 1≦Lmin/Doh≦500, where Lmin is the distance between the heat acting surface and the center of the corresponding ejection port.
JP1244283A 1983-01-28 1983-01-28 liquid jet recording device Granted JPS59138459A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP1244283A JPS59138459A (en) 1983-01-28 1983-01-28 liquid jet recording device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP1244283A JPS59138459A (en) 1983-01-28 1983-01-28 liquid jet recording device

Publications (2)

Publication Number Publication Date
JPS59138459A JPS59138459A (en) 1984-08-08
JPH0457500B2 true JPH0457500B2 (en) 1992-09-11

Family

ID=11805422

Family Applications (1)

Application Number Title Priority Date Filing Date
JP1244283A Granted JPS59138459A (en) 1983-01-28 1983-01-28 liquid jet recording device

Country Status (1)

Country Link
JP (1) JPS59138459A (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2810187B2 (en) * 1990-02-13 1998-10-15 キヤノン株式会社 Liquid jet recording head and liquid jet recording apparatus including the head

Also Published As

Publication number Publication date
JPS59138459A (en) 1984-08-08

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