JPS6345308B2 - - Google Patents
Info
- Publication number
- JPS6345308B2 JPS6345308B2 JP56108724A JP10872481A JPS6345308B2 JP S6345308 B2 JPS6345308 B2 JP S6345308B2 JP 56108724 A JP56108724 A JP 56108724A JP 10872481 A JP10872481 A JP 10872481A JP S6345308 B2 JPS6345308 B2 JP S6345308B2
- Authority
- JP
- Japan
- Prior art keywords
- liquid
- heat
- pulse
- signal
- recording 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
Classifications
-
- B—PERFORMING OPERATIONS; TRANSPORTING
- B41—PRINTING; LINING MACHINES; TYPEWRITERS; STAMPS
- B41J—TYPEWRITERS; SELECTIVE PRINTING MECHANISMS, i.e. MECHANISMS PRINTING OTHERWISE THAN FROM A FORME; CORRECTION OF TYPOGRAPHICAL ERRORS
- B41J2/00—Typewriters or selective printing mechanisms characterised by the printing or marking process for which they are designed
- B41J2/005—Typewriters 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
- B41J2/01—Ink jet
- B41J2/015—Ink jet characterised by the jet generation process
- B41J2/04—Ink jet characterised by the jet generation process generating single droplets or particles on demand
- B41J2/045—Ink jet characterised by the jet generation process generating single droplets or particles on demand by pressure, e.g. electromechanical transducers
- B41J2/04501—Control methods or devices therefor, e.g. driver circuits, control circuits
- B41J2/04515—Control methods or devices therefor, e.g. driver circuits, control circuits preventing overheating
-
- B—PERFORMING OPERATIONS; TRANSPORTING
- B41—PRINTING; LINING MACHINES; TYPEWRITERS; STAMPS
- B41J—TYPEWRITERS; SELECTIVE PRINTING MECHANISMS, i.e. MECHANISMS PRINTING OTHERWISE THAN FROM A FORME; CORRECTION OF TYPOGRAPHICAL ERRORS
- B41J2/00—Typewriters or selective printing mechanisms characterised by the printing or marking process for which they are designed
- B41J2/005—Typewriters 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
- B41J2/01—Ink jet
- B41J2/015—Ink jet characterised by the jet generation process
- B41J2/04—Ink jet characterised by the jet generation process generating single droplets or particles on demand
- B41J2/045—Ink jet characterised by the jet generation process generating single droplets or particles on demand by pressure, e.g. electromechanical transducers
- B41J2/04501—Control methods or devices therefor, e.g. driver circuits, control circuits
- B41J2/0458—Control methods or devices therefor, e.g. driver circuits, control circuits controlling heads based on heating elements forming bubbles
-
- B—PERFORMING OPERATIONS; TRANSPORTING
- B41—PRINTING; LINING MACHINES; TYPEWRITERS; STAMPS
- B41J—TYPEWRITERS; SELECTIVE PRINTING MECHANISMS, i.e. MECHANISMS PRINTING OTHERWISE THAN FROM A FORME; CORRECTION OF TYPOGRAPHICAL ERRORS
- B41J2/00—Typewriters or selective printing mechanisms characterised by the printing or marking process for which they are designed
- B41J2/005—Typewriters 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
- B41J2/01—Ink jet
- B41J2/015—Ink jet characterised by the jet generation process
- B41J2/04—Ink jet characterised by the jet generation process generating single droplets or particles on demand
- B41J2/045—Ink jet characterised by the jet generation process generating single droplets or particles on demand by pressure, e.g. electromechanical transducers
- B41J2/04501—Control methods or devices therefor, e.g. driver circuits, control circuits
- B41J2/04588—Control methods or devices therefor, e.g. driver circuits, control circuits using a specific waveform
Landscapes
- Particle Formation And Scattering Control In Inkjet Printers (AREA)
Description
本発明は、飛翔的液滴を形成して記録を行う液
体噴射記録法、殊に、熱エネルギーによつて飛翔
液滴を形成する液体噴射記録法に関する。
ノンインパクト記録法は、記録時に於ける騒音
の発生が無視し得る程度に極めて小さいという点
に於いて、最近関心を集めている。その中で、高
速記録が可能であり、而も所謂普通紙に定着とい
う特別な処理を必要とせずに記録を行える所謂イ
ンクジエツト記録法(液体噴射記録法)は、極め
て有力な記録法であつて、これ迄にも様々な方式
の提案とそれを具現化する装置が考案され、改良
が加えられて商品化されたものもあれば、現在も
尚実用化への努力が続けられているものもある。
その中で、例えば特開昭54―51837号公報、ド
イツ公開(DOLS)第2843064号公報に記載され
てある液体噴射記録法は、熱エネルギーを液体に
作用させて、液滴吐出の為の原動力を得るという
点に於いて、他の液体噴射記録法とは、異なる特
徴を有している。
即ち、上記の公報に開示されてある記録法は、
熱エネルギーの作用を受けた液体が急峻な体積の
増大を伴う状態変化を起し、該状態変化に基く作
用力によつて、記録ヘツド部先端のオリフイスよ
り液滴が吐出、飛翔して被記録部材に付着し記録
が行われるという特徴である。
殊に、POLS2843064号に開示されている液体
噴射記録法は、所謂drop―on demand記録法に
極めて有効に適用されるばかりではなく、所録ヘ
ツド部をfull lineタイプで高密度マルチオリフイ
ス化として容易に具現化出来るので、高解像度、
高品質の画像を高速で得られるという特徴を有し
ている。
この様に、上記の液体噴射記録法は、優れた特
徴を有するものであるが、さらに高信頼度の記録
を可能にするためには、電気熱変換体のピーク温
度を下げ、その劣化を防ぐ必要がある。
詰り、上記の液体噴射記録法は、熱作用による
気泡の発生とその急峻な体積の増大と減衰に基く
急激な状態変化によつて、記録ヘツドのオリフイ
スより液滴を飛翔的に吐出させて記録するが、こ
の時、電気熱変換体にON―OFF動作で画素信号
に対して1つのパルス信号を与えて、熱作用部に
於いて気泡を発生・成長・減少させると電気・熱
変換体の熱作用面のピーク温度が必要以上に高く
なる。この点を第1図を参照し乍ら説明する。
ON―OFF動作で時刻t0に電気・熱変換体に電
気信号Pが入力されると、電気・熱変換体は、そ
の信号Pに応じた熱エネルギーを発生する。この
熱エネルギーは液体と電気・熱変換体とが接触す
る面としての熱作用面上に於いて、液体の気化す
る温度TBに至る時刻t1まで、液体を暖める。時刻
t1から液体は潜熱をもらい、気化し始めて液中に
気泡が形成される。気泡の体積Vは液体が熱をも
らい続ける以上膨張し続ける。この時信号Pが
OFFされる時刻t2に於いて熱作用面の温度は最高
値Tpとなり、その後減衰的に減少する。このと
き、TB以上の温度では、熱作用面上に気泡が存
在し、断熱に近い状態となつている。
従つて、熱作用面上に形成される気泡が必要以
上に熱作用面上に存在していると、熱作用面の温
度が必要以上に急速に高まり過剰なピーク温度を
与える様になる。この過剰なピーク温度は電気・
熱変換体の耐久寿命の劣化を早めるだけでなく、
インク成分の熱分解、不溶生成物の生成等が起り
やすくさせている。このことが記録画像の品質低
下、強いては、記録停止の原因となる。また、断
熱状態での熱エネルギーは液滴形成の為のエネル
ギーに効率良く、変換されにくく、消費電力の増
加を招く。
本発明は、この点に鑑み成されたものであつ
て、従来法に較べ連続的長時間記録に於いて、常
時安定して、且つ高品質の画像記録を維持するこ
とが出来る高信頼性の液体噴射記録法を提案する
事を目的とする。
本発明の液体噴射記録法は、液体を吐出して飛
翔的液滴を形成する為に設けられたオリフイス
と、該オリフイスに連通し、液体を吐出する為の
熱エネルギーが液体に作用する部分である熱作用
部とを有する液吐出部と、熱エネルギーを発生す
る手段としての電気・熱変換体とを具備する記録
ヘツドを使用する液体噴射記録法に於いて、前記
電気・熱変換体に入力する一画素信号を複数のパ
ルス信号で構成し、一画素信号の入力に対して一
液滴を形成する事を特徴とする。
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aは、本発明が適用される液体噴射記録
ヘツドの1つのオリフイス側から見た正面部分
図、第1図bは、第1図aに一点鎖線XYで示す
部分で切断した場合の切断面部分図である。
図に示される記録ヘツド1は、その表面に電
気・熱変換体2が設けられている基板3の表面
に、所定の線密度で所定の巾と深さの溝が所定数
設けられている溝付板4で覆う様に接合すること
によつて、オリフイス5と液吐出部6が形成され
た構造を有している。図に示す記録ヘツドの場
合、オリフイス5を複数有するものとして示され
てあるが、勿論本発明は、これに限定されるもの
ではなく単一オリフイスの場合の記録ヘツドへの
適用の場合も本発明の範疇に這入るものである。
液吐出部6は、その終端に液滴を吐出させる為
のオリフイス5と、電気・熱変換体2より発生さ
れる熱エネルギーが液体に作用して気泡を発生
し、その体積の膨張と収縮に依る急激な状態変化
を引起す処である熱作用部7とを有する。
熱作用部7は、電気・熱変換体2の熱発生部8
の上部に位置し、熱発生部8の液体と接触する熱
作用面9をその底面としている。
熱発生部8は、基板3上に設けられた下部層1
0、該下部層10上に設けられた発熱抵抗層1
1、該発熱抵抗層11上に設けられた上部層12
とで構成される。発熱抵抗層11には、熱を発生
させる為に該層11に通電する為の電極13,1
4がその表面に設けられてある。電極13は、各
液吐出部の熱発生部に共通の電極であり、電極1
4は、各液吐出部の熱発生部を選択して発熱させ
る為の選択電極であつて、液吐出部の流路に沿つ
て設けられてある。
上部層12は、発熱抵抗層11を、使用する液
体から化学的・物理的に保護する為に発熱抵抗層
11と液吐出部6にある液体とを隔絶すると共
に、液体を通じて電極13,14間が短絡するの
を防止する発熱抵抗層11の保護的機能を有して
いる。
上部層12は、上記の様な機能を有するもので
あるが、発熱抵抗層11が、耐液性があり、且つ
液体を通じて電極13,14間が電気的に短絡す
る心配が全くない場合には、必ずしも設ける必要
はなく、発熱抵抗層11の表面に直ちに液体が接
触する構造の電気・熱変換体として設計しても良
い。
下部層10は、主に熱流量制御機能を有する。
即ち、液滴吐出の際には、発熱抵抗層11で発生
する熱が基板3側の方に伝導するよりも、熱作用
部7側の方に伝導する割合が出来る限り多くな
り、液滴吐出後、詰り発熱抵抗層11への通電が
OFFされた後には、熱作用部7及び熱発生部8
にある熱が速かに基板3側に放出されて、熱作用
部7にある液体及び発生した気泡が急冷される為
に設けられる。
本発明の液体噴射記録法は、この様な記録ヘツ
ドに於いて、第3図に示すように、電気・熱変換
体2へ一画素信号を複数のパルス信号で構成し、
この一画素信号を、即ち、一画素信号を複数に分
割したパルス波形信号として入力する。ここで、
第1パルスは、熱作用面に於いて、液体の気化す
る温度TBからそれより20%高い温度Tpに至る時
刻以内でOFFし、熱作用面の温度がTBまで冷却
される間放置する。再び、熱作用面上の温度が
TBに至つた時、第2パルスをONし、第1パルス
と同様、Tpに至ると同時にOFFする。第3パル
ス以降は第2パルスと同様にし、最終パルスの
OFFする時刻が気体が凝縮し終わる時刻t7を越え
ないような時間幅に於いて、一画素信号を複数の
パルス信号に分解して記録ヘツドを駆動する。
このことにより、電気・熱変換体2の熱作用面
9のピーク温度は低下し、TB以上の熱エネルギ
ーが同一の場合、供給する熱エネルギーを少なく
押えることができる。従つて、記録ヘツドの耐久
寿命が向上し、省電力向けの記録ヘツドの設計が
可能となる。
第4図乃至第6図には、本発明に於ける一画素
信号を構成する複数のパルス信号の好適な波形例
が示される。
第4図に示される波形例は、一画素信号をパル
ス幅、パルス間隔を等しくした信号レベルの異な
るパルス信号P1,P2,P3で構成した場合である。
図に於いて、第2パルス信号P2と第3パルス信
号P3とは同一信号レベルを有しており、第1パ
ルス信号P1の信号レベルがこれ等2つの信号の
信号レベルよりも一段と高くなつている。
第5図に示される波形例は、第2パルス信号
P2が第1パルス信号P1に較べて、パルス幅が4
倍、信号レベルが約1/3とされた一画素信号の例
である。
第6図は、一画素信号を信号レベルもパルス幅
も各々異なる3つのパルス信号P1,P2,P3で構
成した波形例である。
以下、本発明を実施例に従つて具体的に説明す
る。
実施例
シリコン基板上にSiO2層(下部層)をスパツ
タリングにより3μm厚に形成、続いて発熱抵抗
層としてHfB2を1000Å厚に、アルミニウムを電
極として3000Å厚に積層した後、選択エツチング
によつて80μm×200μmの発熱抵抗体パターンを
形成した。次にSiO2層をスパツタリングにより
0.5μm厚に保護層(上部層)として積層して基板
上に電気・熱変換体を形成した後、幅80μm×深
さ80μmの溝を刻んだガラス板を溝と発熱抵抗体
が合致するように接合した。引続いて発熱抵抗体
の先端とオリフイスの距離が300μmになるよう
オリフイス端面を研磨して記録ヘツドを作成し
た。この記録ヘツドに黒色染料とエタノールを主
成分とするインクを0.01気圧の背圧で熱作用部に
供給しながら、第1パルスとして10μs、40V、第
2パルスとして2μs、40V、第3パルスとして
2μs、40V、また、第1パルスと第2パルス、第
2パルスと第3パルスの間隔は3μsとした。連続
矩形電圧印字信号を200μsの同期で電気・熱変換
体2に24時間連続して印加したところ20μs、40V
の矩形電圧パルス信号を200μsの周期で24時間連
続印加した場合に比べ、その画質及びヘツド寿命
ともに向上した。
第1表には、上記の条件で上記と同様にして作
成したヘツド50サンプルについての画像の評価を
経時的に行つた結果が示されている。
また、第2表には、上記の50サンプル中の断線
状態を経時的に調べた結果を示す。
尚、表において、画像評価の基準は、〇…極め
て高品質、△…実用的に充分通用する品質、×…
実用的に不適な品質である。
また、ヘツド寿命評価の基準は、〇…50サンプ
ル中断線0%、△…50サンプル中断線率5%以
内、×…50サンプル中断線率10%以内である。
ここで、前記実施例中の第1パルス信号の電圧
を50Vに高めると、熱作用面上の温度上昇率が増
加し、TBに到達する時間が短縮できる。従つて、
第1パルスの幅を短かくすることが可能となり、
ヘツド噴射の応答性を一層向上させることが出来
る。
さらに、第4図に示すように各パルス幅を同じ
にとつた場合、そのパルス信号ごとの印加電圧を
変えてやれば上記と同様な効果が期待できる。
以上説明したように、電気・熱変換体に入力す
る一画素信号で液体を気化させることで飛翔的な
液滴を形成する液体噴射記録法において、その一
画素信号を気体が凝縮して液体になり終わるまで
の時刻内で分割して複数のパルス信号とし、これ
等の複数のパルス信号を一画素信号として電気・
熱変換体に入力して、飛翔的液滴を形成するとそ
の記録ヘツドの耐久寿命が著しく伸び、消費エネ
ルギーも少なくなる効果がある。
さらには、画像の品質も、長時間の連続吐出に
おいて著しく向上する。
The present invention relates to a liquid jet recording method for recording by forming flying droplets, and particularly to a liquid jet recording method for forming flying droplets using thermal energy. Non-impact recording methods have recently attracted attention because the noise generated during recording is so small that it can be ignored. Among these, the so-called inkjet recording method is an extremely powerful recording method that enables high-speed recording and does not require special processing such as fixing on so-called plain paper. Until now, various methods have been proposed and devices to realize them have been devised, and some have been improved and commercialized, while others are still being worked on to put them into practical use. be. Among them, for example, the liquid jet recording method described in Japanese Patent Application Laid-Open No. 54-51837 and German Publication of Publication (DOLS) No. 2843064 uses thermal energy to act on the liquid to generate the driving force for ejecting droplets. It has a different feature from other liquid jet recording methods in that it obtains the following information. In other words, the recording method disclosed in the above gazette is:
The liquid subjected to the action of thermal energy undergoes a state change accompanied by a sharp increase in volume, and due to the acting force based on this state change, droplets are ejected from the orifice at the tip of the recording head and fly to be recorded. It is characterized by being attached to a member and recording is performed. In particular, the liquid jet recording method disclosed in POLS2843064 is not only very effectively applicable to the so-called drop-on demand recording method, but also allows the recording head to be easily converted into a full line type high-density multi-orifice recording method. High resolution,
It has the characteristic of being able to obtain high-quality images at high speed. In this way, the liquid jet recording method described above has excellent characteristics, but in order to enable even more reliable recording, it is necessary to lower the peak temperature of the electrothermal converter and prevent its deterioration. There is a need. The above-mentioned liquid jet recording method records by ejecting liquid droplets flying from the orifice of the recording head due to the sudden change in state due to the generation of bubbles due to thermal action and their rapid volume increase and attenuation. However, at this time, if one pulse signal is applied to the pixel signal in an ON-OFF operation to the electrothermal converter, and bubbles are generated, grown, and reduced in the heat acting part, the electrothermal converter changes. The peak temperature of the heat-active surface becomes higher than necessary. This point will be explained with reference to FIG. When an electric signal P is input to the electric/thermal converter at time t 0 during ON-OFF operation, the electric/thermal converter generates thermal energy according to the signal P. This thermal energy warms the liquid on the heat acting surface, which is the surface where the liquid and the electricity/thermal converter come into contact, until time t 1 when the liquid reaches a temperature T B at which the liquid vaporizes. time
From t 1 , the liquid gains latent heat and begins to vaporize, forming bubbles in the liquid. The volume V of the bubble continues to expand as the liquid continues to receive heat. At this time, the signal P
At time t2 when the power is turned off, the temperature of the heat-active surface reaches the maximum value Tp , and then decreases in an attenuating manner. At this time, at temperatures above T B , bubbles exist on the heat-active surface, creating a state close to adiabatic. Therefore, if more bubbles formed on the heat acting surface exist on the heat acting surface than necessary, the temperature of the heat acting surface increases more rapidly than necessary, giving rise to an excessive peak temperature. This excessive peak temperature
This not only accelerates the deterioration of the durable life of the heat converter, but also
This makes thermal decomposition of ink components, generation of insoluble products, etc. more likely to occur. This causes a decrease in the quality of the recorded image, and even causes recording to stop. Furthermore, thermal energy in an adiabatic state is difficult to convert efficiently into energy for forming droplets, leading to an increase in power consumption. The present invention has been developed in view of this point, and is a highly reliable method that can maintain stable and high-quality image recording at all times during continuous long-term recording compared to conventional methods. The purpose is to propose a liquid jet recording method. The liquid jet recording method of the present invention includes an orifice provided for ejecting liquid to form flying droplets, and a portion communicating with the orifice where thermal energy for ejecting the liquid acts on the liquid. In a liquid jet recording method using a recording head comprising a liquid discharge section having a certain heat acting section and an electric/thermal converter as a means for generating thermal energy, an input signal to the electric/thermal converter is used. One pixel signal is composed of a plurality of pulse signals, and one droplet is formed in response to input of one pixel signal. Hereinafter, the present invention will be explained in more detail with reference to the drawings. FIG. 1a is a partial front view of a liquid jet recording head to which the present invention is applied, seen from the side of one orifice, and FIG. FIG. The recording head 1 shown in the figure has a predetermined number of grooves of a predetermined width and depth at a predetermined linear density on the surface of a substrate 3 on which an electric/thermal converter 2 is provided. It has a structure in which an orifice 5 and a liquid discharge part 6 are formed by joining so as to be covered with an attached plate 4. Although the recording head shown in the figure is shown as having a plurality of orifices 5, the present invention is of course not limited to this, and the present invention can also be applied to a recording head with a single orifice. It falls into the category of The liquid discharge part 6 has an orifice 5 at its terminal end for discharging droplets, and thermal energy generated by the electric/thermal converter 2 acts on the liquid to generate bubbles, causing the volume to expand and contract. It has a heat acting part 7 that causes a rapid state change. The heat acting part 7 is a heat generating part 8 of the electricity/thermal converter 2
The bottom surface thereof is a heat acting surface 9 which is located at the upper part of the heat generating section 8 and comes into contact with the liquid of the heat generating section 8. The heat generating section 8 is a lower layer 1 provided on the substrate 3.
0, heating resistance layer 1 provided on the lower layer 10
1. Upper layer 12 provided on the heating resistance layer 11
It consists of The heating resistance layer 11 includes electrodes 13, 1 for supplying electricity to the layer 11 to generate heat.
4 is provided on its surface. The electrode 13 is an electrode common to the heat generating part of each liquid discharge part, and
Reference numeral 4 denotes a selection electrode for selectively generating heat in the heat generating section of each liquid discharge section, and is provided along the flow path of the liquid discharge section. The upper layer 12 isolates the heating resistance layer 11 from the liquid in the liquid discharge part 6 in order to chemically and physically protect the heating resistance layer 11 from the liquid used, and also connects the electrodes 13 and 14 through the liquid. The heating resistor layer 11 has a protective function of preventing short circuits. The upper layer 12 has the above-mentioned functions, but if the heating resistance layer 11 is liquid resistant and there is no fear of electrical short circuit between the electrodes 13 and 14 through liquid, However, it is not necessary to provide the heat generating resistor layer 11, and the heat generating resistor layer 11 may be designed as an electric/thermal converter having a structure in which the liquid comes into immediate contact with the surface of the heat generating resistor layer 11. The lower layer 10 mainly has a heat flow control function.
That is, when ejecting a droplet, the proportion of heat generated in the heat generating resistor layer 11 being conducted toward the heat acting section 7 side is as large as possible than being conducted toward the substrate 3 side, and the droplet is ejected. After that, electricity is not applied to the clogged heat generating resistor layer 11.
After being turned off, the heat acting part 7 and the heat generating part 8
This is provided so that the heat present in the heat acting portion 7 is quickly released to the substrate 3 side, and the liquid present in the heat acting portion 7 and the generated air bubbles are rapidly cooled. In the liquid jet recording method of the present invention, in such a recording head, as shown in FIG.
This one pixel signal is input as a pulse waveform signal obtained by dividing the one pixel signal into a plurality of parts. here,
The first pulse is turned off within the time from the temperature T B at which the liquid vaporizes to T p , which is 20% higher than the temperature at which the liquid vaporizes, on the heat effect surface, and is left until the temperature of the heat effect surface cools to T B. do. Again, the temperature on the heat-active surface is
When T B is reached, the second pulse is turned on, and like the first pulse, it is turned off at the same time as T p is reached. The third and subsequent pulses are the same as the second pulse, and the final pulse
One pixel signal is decomposed into a plurality of pulse signals and the recording head is driven in a time width such that the OFF time does not exceed the time t7 when the gas finishes condensing. As a result, the peak temperature of the heat acting surface 9 of the electric/thermal converter 2 is lowered, and when the thermal energy above T B is the same, the thermal energy to be supplied can be kept low. Therefore, the durability of the recording head is improved, and the recording head can be designed to save power. 4 to 6 show preferred waveform examples of a plurality of pulse signals constituting one pixel signal in the present invention. The waveform example shown in FIG. 4 is a case where one pixel signal is composed of pulse signals P 1 , P 2 , and P 3 of different signal levels with equal pulse width and pulse interval.
In the figure, the second pulse signal P 2 and the third pulse signal P 3 have the same signal level, and the signal level of the first pulse signal P 1 is one step higher than the signal level of these two signals. It's getting expensive. The waveform example shown in FIG. 5 is the second pulse signal
P 2 has a pulse width of 4 compared to the first pulse signal P 1 .
This is an example of a single pixel signal in which the signal level is approximately 1/3. FIG. 6 is a waveform example in which one pixel signal is composed of three pulse signals P 1 , P 2 , and P 3 having different signal levels and pulse widths. The present invention will be specifically described below with reference to Examples. Example: Two SiO layers (lower layer) were formed on a silicon substrate to a thickness of 3 μm by sputtering, then HfB 2 was layered to a thickness of 1000 Å as a heat generating resistor layer, and aluminum was laminated to a thickness of 3000 Å as an electrode, followed by selective etching. A heating resistor pattern of 80 μm x 200 μm was formed. Next, two layers of SiO are added by sputtering.
After laminating a protective layer (upper layer) to a thickness of 0.5 μm to form an electrical/thermal converter on the substrate, a glass plate with grooves of 80 μm wide x 80 μm deep was placed so that the grooves and the heating resistor matched. It was joined to. Subsequently, the end face of the orifice was polished so that the distance between the tip of the heating resistor and the orifice was 300 μm, thereby creating a recording head. While supplying ink containing black dye and ethanol as main components to the recording head with a back pressure of 0.01 atm to the heating section, the first pulse was 10 μs at 40 V, the second pulse was 2 μs at 40 V, and the third pulse was
2μs, 40V, and the interval between the first pulse and the second pulse, and between the second pulse and the third pulse, was 3μs. When a continuous rectangular voltage printing signal was applied continuously for 24 hours to the electric/thermal converter 2 with 200 μs synchronization, the output was 40 V for 20 μs.
Compared to the case where a rectangular voltage pulse signal with a period of 200 μs was continuously applied for 24 hours, both the image quality and head life improved. Table 1 shows the results of image evaluation over time for 50 head samples prepared in the same manner as above under the above conditions. Furthermore, Table 2 shows the results of examining the state of disconnection over time in the 50 samples mentioned above. In addition, in the table, the criteria for image evaluation are: 〇...extremely high quality, △...quality that is sufficient for practical use, ×...
The quality is inappropriate for practical use. Further, the criteria for head life evaluation are: ○...50 sample break line rate 0%, △...50 sample break line rate within 5%, ×...50 sample break line rate within 10%. Here, if the voltage of the first pulse signal in the above embodiment is increased to 50V, the temperature increase rate on the heat acting surface increases and the time to reach T B can be shortened. Therefore,
It becomes possible to shorten the width of the first pulse,
The responsiveness of head jetting can be further improved. Furthermore, when each pulse width is set to be the same as shown in FIG. 4, the same effect as described above can be expected by changing the applied voltage for each pulse signal. As explained above, in the liquid jet recording method in which flying droplets are formed by vaporizing liquid with a single pixel signal input to an electric/thermal converter, the gas condenses and turns into a liquid. It is divided into multiple pulse signals within the time until the end of the signal, and these multiple pulse signals are used as one pixel signal to generate electrical signals.
Forming flying droplets by inputting them to a heat converter has the effect of significantly increasing the durability of the recording head and reducing energy consumption. Furthermore, the quality of the image is also significantly improved during continuous ejection over a long period of time.
【表】【table】
第1図は、記録ヘツドに1パルス信号で構成さ
れた一画素信号を入力する時の電気・熱変換体の
熱作用面の表面温度T、及び形成される気泡の体
積Vの時間的変化を示すタイミング図、第2図a
は、本発明の適用される液体噴射記録ヘツドの好
適な実施態様の1つのオリフイス側からの正面部
分図、第2図bは、第2図aの一点鎖線XYで示
す部分で切断した場合の切断面部分図、第3図
は、本発明を説明する為のものであつて記録ヘツ
ドに一画素信号としてマルチパルス信号を入力し
た時の電気・熱変換体2の熱作用面9の表面温度
T、及び気泡体積Vの時間的変化を示すタイミン
グ図、第4図乃至第6図は、夫々本発明に於ける
一画素信号の構成例を示す図である。
1…液体噴射記録ヘツド、2…電気・熱変換
体、3…基板、4…溝付板、5…オリフイス、6
…液吐出部、7…熱作用部、8…熱発生部、9…
熱作用面、10…下部層、11…発熱抵抗層、1
2…上部層、13…共通電極、14…選択電極。
Figure 1 shows the temporal changes in the surface temperature T of the heat-active surface of the electrothermal converter and the volume V of the bubbles formed when a one-pixel signal composed of one pulse signal is input to the recording head. Timing diagram shown in Figure 2a
2 is a partial front view from the orifice side of a preferred embodiment of the liquid jet recording head to which the present invention is applied, and FIG. A partial cross-sectional view, FIG. 3, is for explaining the present invention, and shows the surface temperature of the heat acting surface 9 of the electric/thermal converter 2 when a multi-pulse signal is input as a one-pixel signal to the recording head. Timing diagrams showing temporal changes in T and bubble volume V, and FIGS. 4 to 6 are diagrams showing configuration examples of one pixel signal in the present invention, respectively. DESCRIPTION OF SYMBOLS 1...Liquid jet recording head, 2...Electrical/thermal converter, 3...Substrate, 4...Grooved plate, 5...Orifice, 6
...Liquid discharge part, 7...Heat action part, 8...Heat generation part, 9...
Heat action surface, 10... Lower layer, 11... Heat generating resistance layer, 1
2... Upper layer, 13... Common electrode, 14... Selection electrode.
Claims (1)
けられたオリフイスと、該オリフイスに連通し、
液体を吐出する為の熱エネルギーが液体に作用す
る部分である熱作用部とを有する液吐出部と、熱
エネルギーを発生する手段としての電気・熱変換
体とを具備する記録ヘツドを使用する液体噴射記
録法に於いて、前記電気・熱変換体に入力する一
画素信号を複数のパルス信号で構成し、一画素信
号の入力に対して一液滴を形成する事を特徴とす
る液体噴射記録法。1 An orifice provided for discharging liquid to form flying droplets, communicating with the orifice,
A liquid that uses a recording head that includes a liquid ejecting part that has a heat acting part that is a part where thermal energy acts on the liquid to eject the liquid, and an electric/thermal converter as a means for generating thermal energy. In the jet recording method, one pixel signal input to the electric/thermal converter is composed of a plurality of pulse signals, and one droplet is formed for each input pixel signal. Law.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP10872481A JPS5811169A (en) | 1981-07-10 | 1981-07-10 | Liquid-injection recording method |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP10872481A JPS5811169A (en) | 1981-07-10 | 1981-07-10 | Liquid-injection recording method |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5811169A JPS5811169A (en) | 1983-01-21 |
| JPS6345308B2 true JPS6345308B2 (en) | 1988-09-08 |
Family
ID=14491939
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP10872481A Granted JPS5811169A (en) | 1981-07-10 | 1981-07-10 | Liquid-injection recording method |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS5811169A (en) |
Families Citing this family (11)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH0643128B2 (en) * | 1983-02-05 | 1994-06-08 | キヤノン株式会社 | Inkjet head |
| JPS59146861A (en) * | 1983-02-14 | 1984-08-22 | Canon Inc | Liquid jet recording head |
| US4503444A (en) * | 1983-04-29 | 1985-03-05 | Hewlett-Packard Company | Method and apparatus for generating a gray scale with a high speed thermal ink jet printer |
| JPS60120067A (en) * | 1983-12-01 | 1985-06-27 | Canon Inc | liquid jet recording head |
| JPH062416B2 (en) * | 1984-01-30 | 1994-01-12 | キヤノン株式会社 | Liquid jet recording head manufacturing method |
| JPS6287354A (en) * | 1985-10-15 | 1987-04-21 | Sanyo Electric Co Ltd | Temperature controller in ink jet printer |
| JP2793622B2 (en) * | 1988-12-27 | 1998-09-03 | 株式会社リコー | Liquid jet recording device |
| EP0609997B1 (en) * | 1993-02-05 | 1998-03-18 | Hewlett-Packard Company | A system for reducing drive energy in a high speed thermal ink jet printer |
| JP2612232B2 (en) * | 1994-02-14 | 1997-05-21 | コニカ株式会社 | Pulse voltage generation circuit for on-demand ink jet recording device |
| US6109732A (en) * | 1997-01-14 | 2000-08-29 | Eastman Kodak Company | Imaging apparatus and method adapted to control ink droplet volume and void formation |
| EP0867284A3 (en) * | 1997-03-26 | 1999-08-25 | Eastman Kodak Company | Imaging apparatus and method adapted to control ink droplet volume and void formation |
Family Cites Families (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5463295A (en) * | 1977-10-28 | 1979-05-22 | Canon Inc | Thermal head |
| JPH0237301B2 (en) * | 1979-06-01 | 1990-08-23 | Canon Kk | EKITAIFUNSHAKIROKUHO |
| JPS5617276A (en) * | 1979-07-20 | 1981-02-19 | Mitsubishi Electric Corp | Heat-sensitive recording system |
-
1981
- 1981-07-10 JP JP10872481A patent/JPS5811169A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5811169A (en) | 1983-01-21 |
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