JPH06182993A - Driving method of ink jet head - Google Patents

Driving method of ink jet head

Info

Publication number
JPH06182993A
JPH06182993A JP33638692A JP33638692A JPH06182993A JP H06182993 A JPH06182993 A JP H06182993A JP 33638692 A JP33638692 A JP 33638692A JP 33638692 A JP33638692 A JP 33638692A JP H06182993 A JPH06182993 A JP H06182993A
Authority
JP
Japan
Prior art keywords
transistor
voltage
pulse voltage
variable resistor
waveform
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Granted
Application number
JP33638692A
Other languages
Japanese (ja)
Other versions
JP3156405B2 (en
Inventor
Masahiko Yoshida
昌彦 吉田
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.)
Seiko Epson Corp
Original Assignee
Seiko Epson Corp
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 Seiko Epson Corp filed Critical Seiko Epson Corp
Priority to JP33638692A priority Critical patent/JP3156405B2/en
Publication of JPH06182993A publication Critical patent/JPH06182993A/en
Application granted granted Critical
Publication of JP3156405B2 publication Critical patent/JP3156405B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

Links

Abstract

PURPOSE:To optionally set amplitude of a pulse voltage by a method wherein a rising time constant adjusting means, a rising time adjusting means and a falling time constant adjusting means for the pulse voltage applied to a piezoelectric element are provided and the rising time is optionally set. CONSTITUTION:In the case where a signal as indicated with Pc and a signal as indicated with Pd are applied to an input terminal IN1 and IN2, respectively, firstly when Pc signal becomes H level, a transistor Q6 is changed to an on- state. At that time, a transistor Q8 is changed to an on-state to charge a condenser C1 which is connected to a corrector of the transistor Q8. A corrector current of the transistor Q8 flows via a variable resistor VR1 connected to an emitter of the transistor Q8. The differential voltage between terminals of the variable resistor VR1 is equal to a base-emitter voltage of a transistor Q9. A current of charging condenser C1 via the variable resistor VR1 is rendered constant.

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【産業上の利用分野】本発明は、インクジェット記録装
置のインクジェットヘッドの駆動方法に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a method for driving an inkjet head of an inkjet recording apparatus.

【0002】[0002]

【従来の技術】圧電素子を用いたインクジェットヘッド
の構造を図5に示す。図5に示したインクジェットヘッ
ドにおいては、圧電素子3をパルス電圧を印加すること
により矢印6方向に伸縮させ、この時発生する印字液4
の圧力波により印字液4がノズル1から外部に放出され
ノズル1の出口開口部の前に配置されている記録媒体5
に記録する。このインクジェットヘッドの駆動方法の従
来技術として例えば、特開昭59−136266号公報
によれば、図6に示す回路による方法が考案されてい
る。以下に図6の回路の動作の説明を行う。
2. Description of the Related Art The structure of an inkjet head using a piezoelectric element is shown in FIG. In the inkjet head shown in FIG. 5, the piezoelectric element 3 is expanded and contracted in the direction of arrow 6 by applying a pulse voltage, and the printing liquid 4 generated at this time is printed.
The recording liquid 5 is discharged from the nozzle 1 to the outside by the pressure wave of the recording medium 5 and is arranged in front of the outlet opening of the nozzle 1.
To record. As a conventional method of driving the ink jet head, for example, according to Japanese Patent Laid-Open No. 59-136266, a method using a circuit shown in FIG. 6 has been devised. The operation of the circuit shown in FIG. 6 will be described below.

【0003】入力端子IN101はオープンコレクタ出
力のインバータU101に接続され、インバータU10
1の出力はR101により+5Vにプルアップされてい
る。また、インバータU101の出力はR102を通し
てエミッタ接地されているトランジスタQ101のベー
スに接続されている。トランジスタQ101のコレクタ
はR103を通して高電源電圧VHにプルアップされて
いる。さらにトランジスタQ101のコレクタには出力
段のトランジスタQ102,Q103のベースが接続さ
れている。出力段のトランジスタQ102,Q103の
各エミッタは互いに接続されて出力端子OUT101に
なっている。この出力端子OUT101とトランジスタ
Q101のベースとの間には帰還用コンデンサC101
が挿入されている。また出力端子OUT101にはこの
駆動回路の負荷である、圧電素子P101が接続されて
いる。
The input terminal IN101 is connected to an inverter U101 having an open collector output, and the inverter U10
The output of 1 is pulled up to + 5V by R101. The output of the inverter U101 is connected to the base of a transistor Q101 whose emitter is grounded through R102. The collector of the transistor Q101 is pulled up to the high power supply voltage VH through R103. Further, the bases of the output stage transistors Q102 and Q103 are connected to the collector of the transistor Q101. The emitters of the output stage transistors Q102 and Q103 are connected to each other to form the output terminal OUT101. A feedback capacitor C101 is provided between the output terminal OUT101 and the base of the transistor Q101.
Has been inserted. A piezoelectric element P101, which is the load of this drive circuit, is connected to the output terminal OUT101.

【0004】図7はこの駆動回路の入出力信号のタイミ
ングチャートである。駆動回路の入力端子IN101に
INの様な入力信号を入力した場合、入力信号INが”
H”の時トランジスタQ101はオフ状態となり駆動電
圧は+VHまで立ち上がるがトランジスタQ101とコ
ンデンサC101、抵抗R102とによりミラー積分回
路が構成されているために駆動電圧波形は直線的に立ち
上がる。入力信号INが”L”の場合も同様に駆動波形
は0Vまで直線的に立ち下がり、OUTの様な台形の駆
動電圧波形が得られる。
FIG. 7 is a timing chart of input / output signals of this drive circuit. When an input signal such as IN is input to the input terminal IN101 of the drive circuit, the input signal IN becomes "
When H ", the transistor Q101 is turned off and the drive voltage rises to + VH, but the drive voltage waveform rises linearly because the Miller integrating circuit is constituted by the transistor Q101, the capacitor C101, and the resistor R102. The input signal IN Similarly, in the case of "L", the drive waveform linearly falls to 0V, and a trapezoidal drive voltage waveform like OUT is obtained.

【0005】[0005]

【発明が解決しようとする課題】しかしながら、圧電素
子の変位量のばらつきや製造上のばらつきにより同一の
電圧波形のパルス電圧を圧電素子に印加しても吐出する
印字液の量は各インクジェットヘッド毎に異なる。その
ため、適切な量の印字液を吐出するためには各インクジ
ェットヘッド毎に圧電素子に印加するパルス電圧の電圧
振幅を適切に調整しなければならない。この時、従来技
術で説明したような駆動回路を持つインクジェットヘッ
ドの駆動方法においてはパルス電圧の電圧振幅が電源電
圧の+VHまで立ち上がるので電源電圧を各インクジェ
ットヘッド毎に変化させなければ適切な電圧振幅を得ら
れないという課題がある。また、パルス電圧の立ち下が
り時間は印字液の吐出速度に影響するので適切に調節す
る必要がある。
However, even if a pulse voltage having the same voltage waveform is applied to the piezoelectric element due to variations in the displacement amount of the piezoelectric element and variations in manufacturing, the amount of printing liquid ejected is different for each inkjet head. Different to Therefore, in order to eject an appropriate amount of printing liquid, it is necessary to appropriately adjust the voltage amplitude of the pulse voltage applied to the piezoelectric element for each inkjet head. At this time, in the method of driving the inkjet head having the driving circuit as described in the related art, the voltage amplitude of the pulse voltage rises to + VH of the power supply voltage. Therefore, if the power supply voltage is not changed for each inkjet head, an appropriate voltage amplitude is obtained. There is a problem that cannot be obtained. Further, the fall time of the pulse voltage affects the ejection speed of the printing liquid, and therefore needs to be appropriately adjusted.

【0006】[0006]

【課題を解決するための手段】上記の課題を解決するた
めに本発明においては圧電素子に印加するパルス電圧の
立ち上がり時定数調整手段と立ち上がり時間調整手段と
立ち下がり時定数調整手段とを具備し、立ち上がり時間
を任意に設定することによりパルス電圧の電圧振幅を任
意に設定することを特徴とする。
In order to solve the above problems, the present invention comprises a rise time constant adjusting means, a rise time adjusting means, and a fall time constant adjusting means of a pulse voltage applied to a piezoelectric element. The voltage amplitude of the pulse voltage is arbitrarily set by setting the rising time arbitrarily.

【0007】[0007]

【作用】圧電素子に印加するパルス電圧の電圧振幅を電
源電圧によらず、パルス電圧の立ち上がり時定数と立ち
上がり時間により任意に設定できるので適切な量の印字
液を吐出できる。
The voltage amplitude of the pulse voltage applied to the piezoelectric element can be arbitrarily set by the rise time constant and rise time of the pulse voltage regardless of the power supply voltage, so that an appropriate amount of printing liquid can be ejected.

【0008】[0008]

【実施例】以下に本発明を図示した実施例に基いて詳し
く説明する。図1は本発明の請求項1に対する一実施例
におけるインクジェットヘッドのパルス電圧発生部の回
路図であり、図2は本実施例に用いる入出力信号のタイ
ミングチャートを示したものである。
The present invention will be described in detail below with reference to the illustrated embodiments. FIG. 1 is a circuit diagram of a pulse voltage generator of an ink jet head in an embodiment according to claim 1 of the present invention, and FIG. 2 is a timing chart of input / output signals used in this embodiment.

【0009】IN1、IN2は入力信号の入力端子、Q
6はレベルシフト用のトランジスタ、トランジスタQ
8,Q9,可変抵抗VR1は充電波形用の定電流回路、
トランジスタQ4,Q5,可変抵抗VR2は放電波形用
の定電流回路、C1は駆動波形形成用のコンデンサ、O
UT1は駆動波形の出力端子であり、P1は負荷である
圧電素子である。
IN1 and IN2 are input terminals for input signals, and Q
6 is a transistor for level shift, transistor Q
8, Q9, variable resistor VR1 is a constant current circuit for charging waveform,
Transistors Q4, Q5, variable resistor VR2 are constant current circuits for discharge waveform, C1 is a capacitor for drive waveform formation, O
UT1 is an output terminal of a drive waveform, and P1 is a piezoelectric element that is a load.

【0010】以下にこの回路の動作について説明する。
入力端子IN1にPc、入力端子IN2にPdの様な信
号を入力した場合、まずPc信号が”H”になった時ト
ランジスタQ6はオン状態になる。この時トランジスタ
Q8がオン状態になり、トランジスタQ8のコレクタに
接続されているコンデンサC1が充電される。トランジ
スタQ8のコレクタ電流はトランジスタQ8のエミッタ
に接続されている可変抵抗VR1を介して流れており、
可変抵抗VR1の両端の電位差はトランジスタQ9のベ
ース−エミッタ間の電位になる。トランジスタQ9がオ
ン状態の時ベース−エミッタ間の電位はほぼ一定である
ので、可変抵抗VR1を介してコンデンサC1を充電す
る電流は定電流となる。定電流でコンデンサC1に充電
するのでコンデンサC1の両端の電位差の波形は図2の
Po1に示すように、0[V]から直線的に立ち上が
る。その波形Po1の傾きである立ち上がり時定数τc
[V/sec]は、可変抵抗VR1の抵抗値r1[Ω]と
コンデンサC1の容量値c1[F]とトランジスタQ9
のベース−エミッタ間電圧VBE9[V]から、 τc=VBE9÷(r1×c1) <式1> で求められ、可変抵抗VR1の抵抗値r1あるいはコン
デンサC1の容量値c1を変更することで調節する。こ
のままPc信号が”H”の状態が続くとコンデンサC1
の両端の電位差は電源電圧VMまで立ち上がるが、Pc
信号が”H”になってからtc[sec]後にPc信号
が”L”になった時、トランジスタQ6がオフ状態にな
り、トランジスタQ8がオフ状態になるので、コンデン
サC1の両端の電位差V1[V]は、 V1=τc×tc まで立ち上がり、コンデンサC1に蓄積された電荷によ
りその電位差が保持される。さらにth[sec]後に、
Pd信号が”H”になった時、トランジスタQ4はオン
状態になり、コンデンサC1に蓄積された電荷を可変抵
抗VR2を介して放電する。可変抵抗VR2の両端の電
位差はトランジスタQ5のベース−エミッタ間の電位に
なるので、立ち上がりの場合と同様に定電流でコンデン
サC1から放電し、コンデンサC1の両端の電位差の波
形は直線的に立ち下がる。その波形の傾きである立ち下
がり時定数τd[V/sec]は、可変抵抗VR2の抵抗
値r2[Ω]とコンデンサC1の容量値c1[F]とト
ランジスタQ5のベース−エミッタ間電圧VBE5[V]
から、 τd=VBE5÷(r2×c1) <式2> で求められ、可変抵抗VR2の抵抗値r2あるいはコン
デンサC1の容量値c1を変更することで調節する。P
d信号が”H”になってからPc信号が”L”になるま
での時間を立ち下がり時間td[sec]、 td=V1÷τd より十分長くすることでコンデンサC1の両端の電位差
は0[V]まで直線的に立ち下がる。このようにして任
意の電圧振幅、立ち上がり時間、定電圧を保持した時
間、立ち下がり時間を持ったパルス電圧をコンデンサC
1の両端に発生している。
The operation of this circuit will be described below.
When a signal such as Pc is input to the input terminal IN1 and a signal such as Pd is input to the input terminal IN2, the transistor Q6 is turned on when the Pc signal becomes "H". At this time, the transistor Q8 is turned on, and the capacitor C1 connected to the collector of the transistor Q8 is charged. The collector current of the transistor Q8 flows through the variable resistor VR1 connected to the emitter of the transistor Q8,
The potential difference across the variable resistor VR1 becomes the potential between the base and emitter of the transistor Q9. Since the potential between the base and the emitter is substantially constant when the transistor Q9 is in the ON state, the current for charging the capacitor C1 via the variable resistor VR1 becomes a constant current. Since the capacitor C1 is charged with a constant current, the waveform of the potential difference across the capacitor C1 rises linearly from 0 [V], as indicated by Po1 in FIG. Rising time constant τc, which is the slope of the waveform Po1
[V / sec] is the resistance value r1 [Ω] of the variable resistor VR1, the capacitance value c1 [F] of the capacitor C1 and the transistor Q9.
From the base-emitter voltage VBE9 [V] of τc = VBE9 ÷ (r1 × c1) <Equation 1>, and is adjusted by changing the resistance value r1 of the variable resistor VR1 or the capacitance value c1 of the capacitor C1. . If the Pc signal remains "H" as it is, the capacitor C1
The potential difference between both ends of the voltage rises to the power supply voltage VM, but Pc
When the Pc signal becomes "L" after tc [sec] after the signal becomes "H", the transistor Q6 is turned off and the transistor Q8 is turned off, so that the potential difference V1 [both ends of the capacitor C1 is V] rises to V1 = τc × tc, and the potential difference is held by the charges accumulated in the capacitor C1. After th [sec],
When the Pd signal becomes "H", the transistor Q4 is turned on, and the electric charge accumulated in the capacitor C1 is discharged through the variable resistor VR2. Since the potential difference across the variable resistor VR2 becomes the potential between the base and emitter of the transistor Q5, the capacitor C1 is discharged with a constant current as in the case of rising, and the waveform of the potential difference across the capacitor C1 falls linearly. . The falling time constant τd [V / sec], which is the slope of the waveform, is the resistance value r2 [Ω] of the variable resistor VR2, the capacitance value c1 [F] of the capacitor C1 and the base-emitter voltage VBE5 [V of the transistor Q5. ]
Τd = VBE5 ÷ (r2 × c1) <Equation 2>, and adjustment is performed by changing the resistance value r2 of the variable resistor VR2 or the capacitance value c1 of the capacitor C1. P
The potential difference between both ends of the capacitor C1 is set to 0 [by setting the time from the d signal being “H” to the Pc signal being “L” sufficiently longer than the fall time td [sec], td = V1 ÷ τd. V] and falls linearly. In this way, a pulse voltage having an arbitrary voltage amplitude, rise time, constant voltage holding time, and fall time is applied to the capacitor C.
It occurs at both ends of 1.

【0011】トランジスタQ1、Q2、Q3、Q7は電
流バッファを構成しており、出力端子OUT1にコンデ
ンサC1の両端に発生させた電圧波形と同様の波形を出
力し、OUT1に接続される負荷の圧電素子を駆動する
ために必要な電流を供給している。このとき、出力端子
OUT1に出力される電圧波形の電圧振幅V2[V]は
コンデンサC1の両端の電圧波形の電圧振幅V1よりト
ランジスタQ1、Q2、Q3、Q7のベース−エミッタ
間の電圧分だけ少なくなり、V2はV1とトランジスタ
Q1、Q2、Q3、Q7のベース−エミッタ間の電圧V
BE1、VBE2、VBE3、VBE7より、 V2=V1−(|VBE1|+|VBE3|+|VBE2|+
|VBE7|) で求められる。なお、本実施例では電流バッファをトラ
ンジスタQ1とQ3、トランジスタQ2とQ7をダーリ
ントン接続により2段の増幅で構成しているが、負荷の
圧電素子を駆動するために必要な電流によっては1段あ
るいは3段以上のトランジスタで構成することも可能で
あり、その場合も同様の効果が得られることは明かであ
る。この場合出力端子OUT1に出力される電圧波形の
電圧振幅はコンデンサC1の両端の電位差V1より電流
バッファを構成するトランジスタのベース−エミッタ間
の電圧分だけ少なくなる。
The transistors Q1, Q2, Q3 and Q7 form a current buffer, which outputs a waveform similar to the voltage waveform generated across the capacitor C1 to the output terminal OUT1 and connects the piezoelectric element of the load connected to OUT1. It supplies the necessary current to drive the device. At this time, the voltage amplitude V2 [V] of the voltage waveform output to the output terminal OUT1 is smaller than the voltage amplitude V1 of the voltage waveform across the capacitor C1 by the voltage between the base and emitter of the transistors Q1, Q2, Q3, and Q7. And V2 is V1 and the voltage V between the base and emitter of the transistors Q1, Q2, Q3 and Q7.
From BE1, VBE2, VBE3 and VBE7, V2 = V1- (| VBE1 | + | VBE3 | + | VBE2 | +
| VBE7 |). In this embodiment, the current buffer is composed of transistors Q1 and Q3 and transistors Q2 and Q7 in two stages of amplification by Darlington connection. However, depending on the current required to drive the piezoelectric element of the load, one stage or It is also possible to configure the transistors with three or more stages, and it is clear that the same effect can be obtained in that case as well. In this case, the voltage amplitude of the voltage waveform output to the output terminal OUT1 becomes smaller than the potential difference V1 across the capacitor C1 by the voltage between the base and emitter of the transistor forming the current buffer.

【0012】以上に説明した動作を行うパルス電圧発生
部を持つインクジェットヘッドにおいて、あらかじめ適
切にパルス電圧の立ち上がり時間tcは設定しておき、
各インクジェットヘッドの適正なパルス電圧の電圧振幅
V2が得られるように立ち上がり時定数τcを、 τc=(V2+|VBE1|+|VBE3|+|VBE2|+
|VBE7|)÷tc を目安に設定することで、電源電圧をインクジェットヘ
ッド毎に変更すること無く適正なパルス電圧の電圧振幅
に設定できる。
In the ink jet head having the pulse voltage generator for performing the above-described operation, the rising time tc of the pulse voltage is appropriately set in advance,
The rising time constant τc is set so that an appropriate voltage amplitude V2 of the pulse voltage of each inkjet head is obtained, and τc = (V2 + | VBE1 | + | VBE3 | + | VBE2 | +
By setting | VBE7 |) ÷ tc as a standard, it is possible to set an appropriate voltage amplitude of the pulse voltage without changing the power supply voltage for each inkjet head.

【0013】τc及びτdは<式1>及び<式2>によ
り得られるが、VBE9及びVBE5は素子の固有の値であ
り、c1はτcとτdについて共通であるので、τcと
τdを独立して調整するためにr1とr2によりτcと
τdの調整を行う。図1において、可変抵抗VR1及び
VR2により、τc及びτdを決めるパラメータである
抵抗値r1及びr2を任意に設定できる。
Τc and τd are obtained by <Equation 1> and <Equation 2>. VBE9 and VBE5 are unique values of the device, and c1 is common to τc and τd, so τc and τd are independent. In order to adjust by adjusting r1 and r2, τc and τd are adjusted. In FIG. 1, variable resistors VR1 and VR2 can arbitrarily set resistance values r1 and r2, which are parameters for determining τc and τd.

【0014】前記の第1の実施例には圧電素子に印加す
るパルス電圧の立ち上がり時間、立ち下がり時間、電圧
振幅を任意に設定できる反面、個々の回路基板を使用す
るヘッド毎に立ち上がり時定数τcと立ち下がり時定数
τdの調節をしなければならない。そこで、本発明の第
2の実施例として、図3を示す。図3は図1の可変抵抗
VR1を可変抵抗VR1と着脱可能な固定抵抗R1とを
直列に接続して構成し、同様に図1の可変抵抗VR2を
可変抵抗VR2と着脱可能な固定抵抗R2とを直列に接
続して構成したものである。この構成において、固定抵
抗R1と可変抵抗VR1の抵抗値の和と固定抵抗R2と
可変抵抗VR2の抵抗値の和をあらかじめ必要とする複
数のパルス電圧の電圧振幅について求めておき、調整分
の抵抗値を差し引いた値の抵抗値を固定抵抗R1とR2
に割り当てる。これらの固定抵抗R1とR2に使用する
インクジェットヘッドの適正なパルス電圧の電圧振幅に
対応した抵抗値のものを選んで回路基板に装着すること
でパルス電圧の電圧振幅を設定できる。この場合回路基
板毎に各素子の値にばらつきがありパルス電圧の電圧振
幅とパルス電圧の立ち下がり時間の精度が低下するの
で、各回路基板についてあらかじめ抵抗R1とR2に基
準となる抵抗値の抵抗を装着して、可変抵抗VR1とV
R2により、適正なパルス電圧の電圧振幅と立ち下がり
時間が得られるように調節することで回路基板毎の各素
子の定数のばらつきによるパルス電圧の電圧振幅とパル
ス電圧の立ち下がり時間の精度の低下を抑えている。
In the first embodiment, the rise time, fall time, and voltage amplitude of the pulse voltage applied to the piezoelectric element can be set arbitrarily, but the rise time constant τc for each head using each circuit board. And the fall time constant τd must be adjusted. Therefore, FIG. 3 is shown as a second embodiment of the present invention. In FIG. 3, the variable resistor VR1 of FIG. 1 is configured by connecting the variable resistor VR1 and a removable fixed resistor R1 in series, and similarly, the variable resistor VR2 of FIG. 1 is connected to the variable resistor VR2 and a removable fixed resistor R2. Are connected in series. In this configuration, the sum of the resistance values of the fixed resistor R1 and the variable resistor VR1 and the sum of the resistance values of the fixed resistor R2 and the variable resistor VR2 are obtained in advance for the voltage amplitudes of a plurality of pulse voltages required, and the resistances for the adjustments are adjusted. The resistance value minus the value is the fixed resistance R1 and R2.
Assign to. The voltage amplitude of the pulse voltage can be set by selecting the fixed resistors R1 and R2 having resistance values corresponding to the appropriate voltage amplitude of the pulse voltage of the inkjet head used and mounting them on the circuit board. In this case, the value of each element varies from circuit board to circuit board, and the accuracy of the voltage amplitude of the pulse voltage and the fall time of the pulse voltage decreases. Therefore, the resistance of the reference resistance value is previously set to the resistors R1 and R2 for each circuit board. Attach the variable resistors VR1 and V
By adjusting R2 so that the proper voltage amplitude and fall time of the pulse voltage can be obtained, the precision of the voltage amplitude of the pulse voltage and the fall time of the pulse voltage decreases due to the variation in the constants of each element on each circuit board. Is suppressed.

【0015】以下に請求項1の第3の実施例について説
明する。前記第2の実施例において固定抵抗R1及びR
2を図4に示すような集合抵抗RM1で構成しても同様
の効果を得ることが可能であり、1つの集合抵抗RM1
を差し換えることで、パルス電圧の電圧振幅とそれに適
したパルス電圧の立ち下がり時間が同時に設定できる。
The third embodiment of claim 1 will be described below. In the second embodiment, the fixed resistors R1 and R
It is possible to obtain the same effect even if 2 is configured by the collective resistance RM1 as shown in FIG.
By replacing the, the voltage amplitude of the pulse voltage and the falling time of the pulse voltage suitable for it can be set at the same time.

【0016】[0016]

【発明の効果】以上に説明したように本発明におけるイ
ンクジェットヘッドの駆動方法は、電源電圧を変更する
こと無くインクジェットヘッド毎の適正なパルス電圧の
電圧振幅が容易に設定できるので印字液の吐出量が安定
し、印字品質の向上の効果が大きい。また、このインク
ジェットヘッドを駆動するための電源の電源電圧は、パ
ルス電圧の電圧振幅より高ければ良いので、プリンタを
構成する例えばキャリッジ駆動や紙送りなどの他の駆動
系の電源電圧がインクジェットヘッドを駆動するパルス
電圧の電圧振幅より高ければこれらの電源と電源の共用
が出来るのでプリンタの構成を簡略化できる効果もあ
る。
As described above, in the method of driving an ink jet head according to the present invention, a proper voltage amplitude of the pulse voltage for each ink jet head can be easily set without changing the power supply voltage. Is stable, and the effect of improving print quality is great. Further, since the power supply voltage of the power supply for driving the inkjet head may be higher than the voltage amplitude of the pulse voltage, the power supply voltage of another drive system such as a carriage drive or a paper feed which configures the printer does not drive the inkjet head. If the voltage amplitude is higher than that of the pulse voltage to be driven, these power sources can be shared and the printer can be simplified in structure.

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

【図1】本発明の第1の実施例の回路図。FIG. 1 is a circuit diagram of a first embodiment of the present invention.

【図2】本発明の実施例の入出力信号のタイミングチャ
ート。
FIG. 2 is a timing chart of input / output signals according to the embodiment of the present invention.

【図3】本発明の第2の実施例の回路図。FIG. 3 is a circuit diagram of a second embodiment of the present invention.

【図4】本発明の第3の実施例の説明図。FIG. 4 is an explanatory diagram of a third embodiment of the present invention.

【図5】インクジェットヘッドの構造を示す断面図。FIG. 5 is a sectional view showing the structure of an inkjet head.

【図6】従来技術の実施例の回路図。FIG. 6 is a circuit diagram of a prior art embodiment.

【図7】従来技術の実施例の入出力信号のタイミングチ
ャート。
FIG. 7 is a timing chart of input / output signals according to the example of the related art.

【符号の説明】[Explanation of symbols]

IN1 入力信号の入力端子 IN2 入力信号の入力端子 Q6 レベルシフト用のトランジスタ Q8 充電波形の定電流用のトランジスタ Q9 充電波形の定電流用のトランジスタ VR1 充電波形の定電流用の可変抵抗 R1 充電波形の定電流用の固定抵抗 Q4 放電波形の定電流用のトランジスタ Q5 放電波形の定電流用のトランジスタ R2 放電波形の定電流用の固定抵抗 C1 駆動波形形成用のコンデンサ OUT1 駆動波形の出力端子 P1 負荷の圧電素子 IN1 Input signal input terminal IN2 Input signal input terminal Q6 Level shift transistor Q8 Charge waveform constant current transistor Q9 Charge waveform constant current transistor VR1 Charge waveform constant current variable resistor R1 Charge waveform Fixed resistance for constant current Q4 Transistor for constant current of discharge waveform Q5 Transistor for constant current of discharge waveform R2 Fixed resistor for constant current of discharge waveform C1 Capacitor for driving waveform formation OUT1 Driving waveform output terminal P1 Load Piezoelectric element

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】 ノズルと前記ノズルに印字液を供給する
流路と、前記流路の壁面に配置されたパルス電圧により
伸縮する圧電素子からなるインクジェットヘッドの駆動
方法において、 前記圧電素子に印加する前記パルス電圧の立ち上がり時
定数調整手段と立ち上がり時間調整手段と立ち下がり時
定数調整手段とを具備し、立ち上がり時定数を任意に設
定することによりパルス電圧の電圧振幅を任意に設定す
ることを特徴とするインクジェットヘッドの駆動方法。
1. A method for driving an ink jet head comprising a nozzle, a flow path for supplying a printing liquid to the nozzle, and a piezoelectric element arranged on the wall surface of the flow path to expand and contract, and which is applied to the piezoelectric element. A pulse voltage rise time constant adjusting means, a rise time adjusting means, and a fall time constant adjusting means, wherein the rise time constant is arbitrarily set to arbitrarily set the voltage amplitude of the pulse voltage. Method for driving an inkjet head.
JP33638692A 1992-12-16 1992-12-16 Driving method of inkjet head Expired - Lifetime JP3156405B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP33638692A JP3156405B2 (en) 1992-12-16 1992-12-16 Driving method of inkjet head

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP33638692A JP3156405B2 (en) 1992-12-16 1992-12-16 Driving method of inkjet head

Publications (2)

Publication Number Publication Date
JPH06182993A true JPH06182993A (en) 1994-07-05
JP3156405B2 JP3156405B2 (en) 2001-04-16

Family

ID=18298601

Family Applications (1)

Application Number Title Priority Date Filing Date
JP33638692A Expired - Lifetime JP3156405B2 (en) 1992-12-16 1992-12-16 Driving method of inkjet head

Country Status (1)

Country Link
JP (1) JP3156405B2 (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0899102A2 (en) 1997-08-18 1999-03-03 Nec Corporation Inkjet head control system and method

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0899102A2 (en) 1997-08-18 1999-03-03 Nec Corporation Inkjet head control system and method
EP0899102A3 (en) * 1997-08-18 1999-12-08 Nec Corporation Inkjet head control system and method
US6286922B1 (en) 1997-08-18 2001-09-11 Nec Corporation Inkjet head control system and method

Also Published As

Publication number Publication date
JP3156405B2 (en) 2001-04-16

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