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JPH047308B2 - - Google Patents

Info

Publication number
JPH047308B2
JPH047308B2 JP19389482A JP19389482A JPH047308B2 JP H047308 B2 JPH047308 B2 JP H047308B2 JP 19389482 A JP19389482 A JP 19389482A JP 19389482 A JP19389482 A JP 19389482A JP H047308 B2 JPH047308 B2 JP H047308B2
Authority
JP
Japan
Prior art keywords
voltage
wire
printer head
electrostrictive
time
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
JP19389482A
Other languages
Japanese (ja)
Other versions
JPS5983673A (en
Inventor
Takeshi Inoe
Shinichi Hori
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.)
NEC Corp
Original Assignee
Nippon Electric Co Ltd
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Nippon Electric Co Ltd filed Critical Nippon Electric Co Ltd
Priority to JP19389482A priority Critical patent/JPS5983673A/en
Publication of JPS5983673A publication Critical patent/JPS5983673A/en
Publication of JPH047308B2 publication Critical patent/JPH047308B2/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
    • B41J2/22Typewriters or selective printing mechanisms characterised by the printing or marking process for which they are designed characterised by selective application of impact or pressure on a printing material or impression-transfer material
    • B41J2/23Typewriters or selective printing mechanisms characterised by the printing or marking process for which they are designed characterised by selective application of impact or pressure on a printing material or impression-transfer material using print wires
    • B41J2/27Actuators for print wires
    • B41J2/295Actuators for print wires using piezoelectric elements

Landscapes

  • Dot-Matrix Printers And Others (AREA)
  • Impact Printers (AREA)

Description

【発明の詳細な説明】 本発明は、電歪素子を用いたインパクト形ワイ
ヤードツトプリンタヘツドの駆動方法に係わり、
ワイヤーの残留振動の抑圧を目的としたものであ
る。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a method of driving an impact type wire dot printer head using an electrostrictive element,
The purpose is to suppress residual vibration in the wire.

ワイヤーの機械的衝撃を用いて印字を行うワイ
ヤードツトプリンタは普通紙に同時複写がとれ、
画素の集合により文字を構成するためアルフアベ
ツト文字の他に漢字、図形など記録の融通性に優
れ、また低価格であるといつた長所があるため広
く普及している。従来、ワイヤードツトプリンタ
は電磁駆動方式が主流であるが、駆動電力が大き
くプリンタの高速化を行う場合に過電流による温
度上昇が大きくなるため高速化の障害になつてい
た。これに対し、電歪素子を用いたインパクト形
ワイヤードツトプリンタは原理的に上記電磁式の
欠点を一掃することができ、注目されている。
Wire dot printers, which print using the mechanical impact of wires, can make simultaneous copies on plain paper.
Since characters are composed of a collection of pixels, it has excellent flexibility in recording kanji and figures in addition to alphabetical characters, and is widely used because it has the advantage of being inexpensive. Conventionally, wire dot printers have been mainly driven by an electromagnetic drive system, but this has been an obstacle to speeding up the printer because it requires a large amount of driving power and increases temperature due to overcurrent. On the other hand, impact type wire dot printers using electrostrictive elements are attracting attention because they can theoretically eliminate the drawbacks of the electromagnetic type.

しかしながら、電磁式、電歪式いずれの方式に
せよ高速で印字するためには、飛翔したワイヤー
がインクリボン、紙を介してプラテンを衝打し復
元すると同時に次の飛翔を開始する必要があり、
ワイヤーが記録媒体に衝突し、停止するときの残
留振動を極小に抑えることが重要となる。即ち、
2回目以降の飛翔の開始に際しては、残留振動が
大きければ大きいほど前回の飛翔の複元によるプ
リンタヘツドの運動エネルギーや歪エネルギーが
重畳されるためにワイヤーの運動エネルギーが大
きくなる。このようにして2回目以降の方が印字
濃度が高くなり、均質な印字が得られなくなるわ
けである。
However, in order to print at high speed with either the electromagnetic or electrostrictive method, it is necessary for the flying wire to hit the platen through the ink ribbon and paper, and to restore its original shape and start the next flight at the same time.
It is important to minimize residual vibration when the wire collides with the recording medium and stops. That is,
When starting the second flight, the larger the residual vibration, the greater the kinetic energy of the wire because the kinetic energy and strain energy of the printer head due to the previous flight are superimposed. In this way, the print density becomes higher from the second time onwards, and it becomes impossible to obtain a homogeneous print.

以下、図面に従つて従来の電歪型プリンタヘツ
ド及びその駆動方法について説明する。
DESCRIPTION OF THE PREFERRED EMBODIMENTS A conventional electrostrictive printer head and its driving method will be described below with reference to the drawings.

第1図は電歪素子を用いたインパクト形ワイヤ
ードツトプリンタヘツドの一例を示しており、ヘ
ツドベース102に保持された電歪素子101を
有し、第1レバー107と第2レバー108がそ
れぞれヒンジ103,104及び105,106
を介して電歪素子とヘツドベースに接続してい
る。さらに第3レバー112がヒンジ111,1
10を介して第1レバー、第2レバーと接続して
おり、該第3レバーにはアーム部分117があ
り、このアーム部にはワイヤー114が接続され
ている。またヘツドベース102にはストツパー
118が形成されている。115はインクリボ
ン、116は紙、117はプラテンである。第1
図に示したプリントヘツドの動作原理について述
べると、電歪素子101に電圧が印加されると電
歪素子101は伸び、ヒンジ104,105が圧
縮され、ヒンジ103,106が伸長される。こ
の結果、第1レバー107、第2レバー108が
それぞれ矢印で示した方向に回転する。この動き
がヒンジ110と111を介して第3レバー11
2に伝わり、さらにアーム部113を介してワイ
ヤー114に伝わる。そしてワイヤー114が矢
印の方向に直進し、リボン115、紙116、プ
ラテン117を衝打し印字が行われる。この衝打
の反発力とヒンジの復元力によりワイヤー114
は元の位置にもどり1回の往復運動が完了する。
FIG. 1 shows an example of an impact type wire dot printer head using an electrostrictive element, which has an electrostrictive element 101 held on a head base 102, and a first lever 107 and a second lever 108 are connected to hinges 103 and 108, respectively. 104 and 105, 106
It is connected to the electrostrictive element and the head base via. Further, the third lever 112 is connected to the hinge 111,1.
The third lever has an arm portion 117, and a wire 114 is connected to the arm portion. A stopper 118 is also formed on the head base 102. 115 is an ink ribbon, 116 is paper, and 117 is a platen. 1st
The principle of operation of the print head shown in the figure will be described. When a voltage is applied to electrostrictive element 101, electrostrictive element 101 is expanded, hinges 104 and 105 are compressed, and hinges 103 and 106 are expanded. As a result, the first lever 107 and the second lever 108 rotate in the directions indicated by the arrows. This movement causes the third lever 11 to move through the hinges 110 and 111.
2 and is further transmitted to the wire 114 via the arm portion 113. Then, the wire 114 moves straight in the direction of the arrow and hits the ribbon 115, paper 116, and platen 117 to perform printing. Due to the repulsive force of this impact and the restoring force of the hinge, the wire 114
returns to its original position and completes one reciprocating movement.

従来、電歪型プリンタヘツドは矩形電圧波で駆
動され、ワイヤーが記録媒体を衝打し元の位置に
戻つたところ(ここまでの時間を1周期Tとす
る。)で印加電圧を零にするが、このときプリン
タヘツド内の機械的歪エネルギーを極めて小さく
することが難かしいため一般に残留振動が顕著に
みられる。従来例として、第1図に示した形状の
プリンタヘツド(周期T=0.48msec)を用い、
矩形電圧波で駆動したときのワイヤー先端変位の
時間応答特性を第2図に示す。第2図イはワイヤ
ー先端変位の時間応答、第2図ロは電歪素子の駆
動電圧波形を示し、ワイヤーが元の位置に復元し
た時間0.48msec(1周期T)で電圧を零にしてい
る。第2図で用いたヘツドは、ワイヤー先端と、
リボン、紙、プラテンまでのギヤツプ0.40mm、電
歪素子はジルコン・チタン酸鉛系材料でつくられ
た縦効果積層セラミツク振動子(横3mm、奥行2
mm、長さ18mm)を用い、ヘツドの変位拡大率は42
倍である。即ち、従来用いられている矩形電圧波
でプリンタヘツドを駆動すると、電圧が瞬時に立
ち下がるような急激な電気的変化に対して、プリ
ンタヘツドの機械系が容易に追従することができ
ないために、ヘツド内のヒンジ、ベース、及び電
歪素子部分にかなりの歪エネルギーが蓄積され
る。そのため残留振動が顕著にみられるわけであ
る。尚、周知のごとく、プリンタヘツドの1周期
T近傍から離れたところで電圧を零にした場合、
第2図の残留振動特性に比べてさらに振幅の大き
な残留振動が生じ実用に供しない。
Conventionally, an electrostrictive printer head is driven by a rectangular voltage wave, and the applied voltage is reduced to zero when the wire hits the recording medium and returns to its original position (the time up to this point is defined as one cycle T). However, since it is difficult to minimize the mechanical strain energy within the printer head, residual vibrations are generally noticeable. As a conventional example, a printer head having the shape shown in Fig. 1 (period T = 0.48 msec) was used.
Figure 2 shows the time response characteristics of the wire tip displacement when driven by a rectangular voltage wave. Figure 2A shows the time response of the wire tip displacement, and Figure 2B shows the driving voltage waveform of the electrostrictive element.The voltage is reduced to zero at a time of 0.48msec (one cycle T) when the wire returns to its original position. . The head used in Figure 2 has a wire tip and
The gap between the ribbon, paper, and platen is 0.40 mm, and the electrostrictive element is a longitudinal effect laminated ceramic vibrator (width 3 mm, depth 2
mm, length 18 mm), and the displacement magnification rate of the head is 42
It's double. That is, when a printer head is driven with a conventionally used rectangular voltage wave, the mechanical system of the printer head cannot easily follow sudden electrical changes such as an instantaneous drop in voltage. Significant strain energy is stored in the hinge, base, and electrostrictive elements within the head. Therefore, residual vibrations are noticeable. As is well known, when the voltage is reduced to zero at a point away from the vicinity of one cycle T of the printer head,
Residual vibration with a larger amplitude than the residual vibration characteristics shown in FIG. 2 occurs, making it impractical.

これに対し、本発明の目的はワイヤーが元の位
置に復元しようとするときに、プリンタヘツドの
残留振動を極小にすることが可能な電歪型プリン
タヘツドの駆動方法を提供するものである。
In view of this, an object of the present invention is to provide a method for driving an electrostrictive printer head that can minimize the residual vibration of the printer head when the wire attempts to return to its original position.

すなわち、本発明は電圧印加により生じる電歪
素子の歪みがヒンジを介してレバー部に伝わり、
該レバー部の変位がアーム部を介してワイヤーに
伝わり、該ワイヤーが記録媒体を衝打することに
より印字を行なう電歪型プリンタヘツドの駆動方
法において電圧が印加されてからワイヤーが記録
媒体を衝打して元の位置にもどるまでの時間をT
とし、印加開始時の電圧をV0とし、時間をt、
微小時間間隔をΔTとしたとき、印加電圧Vを 0<tT−ΔTのとき V=V0 T−ΔT<t<T+ΔTのとき V=−(V0/2ΔT)(t−T)+1/2V0 とすることを特徴とする電歪型プリンタヘツドの
駆動方法である。
That is, in the present invention, the strain of the electrostrictive element caused by voltage application is transmitted to the lever part via the hinge,
In an electrostrictive printer head driving method in which the displacement of the lever section is transmitted to the wire via the arm section, and the wire strikes the recording medium to perform printing, the wire strikes the recording medium after voltage is applied. The time it takes to return to the original position after hitting the ball is T.
The voltage at the start of application is V 0 , the time is t,
When the minute time interval is ΔT, the applied voltage V is: When 0<tT-ΔT, V=V 0 When T-ΔT<t<T+ΔT, V=-(V 0 /2ΔT)(t-T)+1/2V This is a method of driving an electrostrictive printer head characterized by setting the head to zero .

本発明に関する、電歪素子を用いたプリンタヘ
ツドの駆動電圧波形を第3図に示す。第3図に示
した駆動電圧波形は、立ち上がり部分は従来の矩
形波と同じであるが、立ち下がり部分においてプ
リンタヘツドの周期Tに対してΔTだけ短い時間
から時間経過に比例して電圧が低下し、点P(T,
1/2V0)を通り、時間T+ΔTで電圧が零になる
ものである。このように駆動電圧が緩やかに立ち
下がる場合にはプリンタヘツドの機械系が容易に
追従し、前記理由により残留振動が極小に抑圧さ
れるわけである。
FIG. 3 shows a driving voltage waveform of a printer head using an electrostrictive element according to the present invention. In the drive voltage waveform shown in Figure 3, the rising part is the same as the conventional rectangular wave, but in the falling part, the voltage decreases in proportion to the passage of time from a time ΔT shorter than the period T of the printer head. Then, point P(T,
1/2V 0 ), and the voltage becomes zero at time T+ΔT. When the drive voltage falls slowly in this way, the mechanical system of the printer head easily follows, and for the reason mentioned above, residual vibrations are suppressed to a minimum.

次に本発明の一実施例として第2図と同様に第
1図に示したプリンタヘツドを用いて残留振動抑
圧の検証を行つた。それを第4図に示す。第4図
イの実線の特性は本発明に従つた駆動電圧波を用
いたワイヤー先端変位特性である。また点線の特
性は、従来の第2図ロに示した矩形駆動電圧波を
用いたときのワイヤー先端変位特性を示す。第4
図ロは本発明に従つた駆動電圧波形の一例を示
し、235Vの一定電圧から0.42msecで立ち下がり
周期0.48msecで117.5Vとなり0.54msecで電圧が
零となる。第4図から明らかな如く本発明に従う
と、従来の矩形駆動電圧波形を用いた場合に比
べ、プリンタヘツドの残留振動が3分の1以下に
抑圧されていることがわかる。なお、駆動電圧の
立ち下がりはプリンタヘツドの周期Tを考慮した
上で行うべきであり、むやみになだらかに下げれ
ば良いというものではない。例えば、第3図の点
Qを通るような電圧波形で駆動した場合にはプリ
ンタヘツドの残留振動抑圧の効果は全くなかつ
た。
Next, as an embodiment of the present invention, residual vibration suppression was verified using the printer head shown in FIG. 1 in the same manner as in FIG. 2. This is shown in Figure 4. The characteristic shown by the solid line in FIG. 4A is the wire tip displacement characteristic using a driving voltage wave according to the present invention. Further, the dotted line indicates the wire tip displacement characteristic when the conventional rectangular drive voltage wave shown in FIG. 2B is used. Fourth
Figure 9 shows an example of the drive voltage waveform according to the present invention, where the voltage falls from a constant voltage of 235V in 0.42msec to 117.5V with a fall period of 0.48msec, and the voltage becomes zero in 0.54msec. As is clear from FIG. 4, according to the present invention, the residual vibration of the printer head is suppressed to one-third or less compared to when a conventional rectangular drive voltage waveform is used. Incidentally, the fall of the drive voltage should be done in consideration of the period T of the printer head, and it is not sufficient to reduce it unnecessarily and gently. For example, when the printer was driven with a voltage waveform passing through point Q in FIG. 3, there was no effect of suppressing residual vibrations in the printer head.

尚、本プリンタヘツドの駆動回路を第5図に示
す。すなわち、この駆動回路は、電源122の電
圧を電歪素子127の端子123,124両端に
印加するように接続された開閉回路120と、電
歪素子127の端子123,124両端を短絡す
るように接続された開閉回路121とにより構成
され印字制御信号Va及びそれをインバータ回路
126により反転した信号により制御する回路で
ある。ここで、前述の駆動電圧の立ち下がり時間
を制御するには、電歪素子端子123,124と
開閉回路121との間に直列に抵抗125を接続
して電歪素子127の制動容量と抵抗125の抵
抗値によつて定まる時定数をもたすことによつて
実現可能である。
Incidentally, the drive circuit of this printer head is shown in FIG. That is, this drive circuit has an opening/closing circuit 120 connected to apply the voltage of a power source 122 to both terminals 123 and 124 of the electrostrictive element 127, and a short-circuit between both terminals 123 and 124 of the electrostrictive element 127. This circuit is constituted by a connected opening/closing circuit 121 and is controlled by a printing control signal Va and a signal inverted by an inverter circuit 126. Here, in order to control the fall time of the driving voltage described above, a resistor 125 is connected in series between the electrostrictive element terminals 123 and 124 and the switching circuit 121, and the braking capacity of the electrostrictive element 127 and the resistor 125 are connected in series. This can be realized by providing a time constant determined by the resistance value of .

以上詳述したように本発明に従うとワイヤー先
端変位の残留振動を極小に抑えることができ、駆
動電圧第1波が入力された直後さらに第2波をつ
づけて入力することができるわけであるから、ワ
イヤードツトプリンタの高速化、高印字品質化に
有効である。
As detailed above, according to the present invention, the residual vibration of the wire tip displacement can be suppressed to a minimum, and the second wave can be continuously input immediately after the first wave of the drive voltage is input. This method is effective for increasing the speed and print quality of wire dot printers.

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

第1図は電歪素子を用いたインパクト形ワイヤ
ードツトプリンタヘツドの構成図。第2図イは第
1図に示したプリンタヘツドを従来用いられてい
る矩形電圧波で駆動したときのワイヤー先端変位
の時間応答特性図、第2図ロは電歪素子の駆動電
圧波形図。第3図は本発明の駆動方法に従つた駆
動電圧波形図、第4図は本発明に従つた駆動電圧
波と従来の矩形駆動電圧波によるプリンタヘツド
ワイヤー先端変位の差異を示す図で、第4図イは
本発明に従つた駆動電圧波を用いたワイヤー先端
変位特性図。第4図ロは本発明に従つた駆動電圧
波形の一実施例を示す図。第5図は本発明のプリ
ンタヘツドの駆動回路を示す図。 図において、101,127は電歪素子、10
2はヘツドベース、103,104,105,1
06,110,111はヒンジ、107,10
8,112はそれぞれ第1レバー、第2レバー、
第3レバー、113は第3レバーアーム部分、1
14はワイヤー、115はインクリボン、116
は紙、117はプラテン、118はストツパー、
120,121は開閉回路、122は電源、12
3,124は電歪素子の端子、125は抵抗、1
26はインバータ回路。
FIG. 1 is a configuration diagram of an impact type wire dot printer head using an electrostrictive element. FIG. 2A is a time response characteristic diagram of the displacement of the wire tip when the printer head shown in FIG. 1 is driven with a conventionally used rectangular voltage wave, and FIG. 2B is a diagram of the drive voltage waveform of the electrostrictive element. FIG. 3 is a drive voltage waveform diagram according to the drive method of the present invention, and FIG. 4 is a diagram showing the difference in printer head wire tip displacement between the drive voltage wave according to the present invention and the conventional rectangular drive voltage wave. Figure 4A is a wire tip displacement characteristic diagram using a driving voltage wave according to the present invention. FIG. 4B is a diagram showing an example of a driving voltage waveform according to the present invention. FIG. 5 is a diagram showing a printer head drive circuit according to the present invention. In the figure, 101 and 127 are electrostrictive elements, 10
2 is head base, 103, 104, 105, 1
06, 110, 111 are hinges, 107, 10
8, 112 are the first lever, the second lever,
3rd lever, 113 is the 3rd lever arm part, 1
14 is a wire, 115 is an ink ribbon, 116
is paper, 117 is platen, 118 is stopper,
120, 121 are switching circuits, 122 is a power supply, 12
3, 124 is the terminal of the electrostrictive element, 125 is the resistor, 1
26 is an inverter circuit.

Claims (1)

【特許請求の範囲】 1 電圧印加により生じる電歪素子の歪みがヒン
ジを介してレバー部に伝わり、該レバー部の変位
がアーム部を介してワイヤーに伝わり、該ワイヤ
ーが記録媒体を衝打することにより印字を行なう
電歪型プリンタヘツドの駆動方法において、電圧
が印加されてからワイヤーが記録媒体を衝打して
元の位置にもどるまでの時間をTとし、印加開始
時の電圧をV0とし、時間をt、微小時間間隔を
ΔTとしたとき、印加電圧Vを 0<tT−ΔTのとき V=V0 T−ΔT<t<T+ΔTのとき V=−(V0/2ΔT)(t−T)+1/2V0 とすることを特徴とする電歪型プリンタヘツドの
駆動方法。
[Claims] 1. Distortion of the electrostrictive element caused by voltage application is transmitted to the lever section via the hinge, displacement of the lever section is transmitted to the wire via the arm section, and the wire hits the recording medium. In a method of driving an electrostrictive printer head that performs printing, T is the time from when voltage is applied until the wire hits the recording medium and returns to its original position, and the voltage at the start of application is V 0 When the time is t and the minute time interval is ΔT, the applied voltage V is: When 0<tT−ΔT, V=V 0 When T−ΔT<t<T+ΔT, V=−(V 0 /2ΔT)(t -T) +1/2V 0. A method for driving an electrostrictive printer head.
JP19389482A 1982-11-04 1982-11-04 Method for driving electrostriction type printer head Granted JPS5983673A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP19389482A JPS5983673A (en) 1982-11-04 1982-11-04 Method for driving electrostriction type printer head

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP19389482A JPS5983673A (en) 1982-11-04 1982-11-04 Method for driving electrostriction type printer head

Publications (2)

Publication Number Publication Date
JPS5983673A JPS5983673A (en) 1984-05-15
JPH047308B2 true JPH047308B2 (en) 1992-02-10

Family

ID=16315507

Family Applications (1)

Application Number Title Priority Date Filing Date
JP19389482A Granted JPS5983673A (en) 1982-11-04 1982-11-04 Method for driving electrostriction type printer head

Country Status (1)

Country Link
JP (1) JPS5983673A (en)

Families Citing this family (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0423009Y2 (en) * 1985-01-28 1992-05-27
JPS6360763A (en) * 1986-09-02 1988-03-16 Nec Corp Piezoelectric printing head drive circuit
JPH01190464A (en) * 1988-01-26 1989-07-31 Juki Corp Printer head drive device using piezoelectric elements

Also Published As

Publication number Publication date
JPS5983673A (en) 1984-05-15

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