JPH066927Y2 - Thermal head - Google Patents
Thermal headInfo
- Publication number
- JPH066927Y2 JPH066927Y2 JP2636887U JP2636887U JPH066927Y2 JP H066927 Y2 JPH066927 Y2 JP H066927Y2 JP 2636887 U JP2636887 U JP 2636887U JP 2636887 U JP2636887 U JP 2636887U JP H066927 Y2 JPH066927 Y2 JP H066927Y2
- Authority
- JP
- Japan
- Prior art keywords
- heating element
- power supply
- terminal
- supply terminal
- resistance heating
- 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 - Lifetime
Links
- 238000010438 heat treatment Methods 0.000 claims description 46
- 230000020169 heat generation Effects 0.000 description 8
- 238000010586 diagram Methods 0.000 description 3
- 230000003247 decreasing effect Effects 0.000 description 2
- 239000007787 solid Substances 0.000 description 2
- 230000000694 effects Effects 0.000 description 1
- 238000005516 engineering process Methods 0.000 description 1
- 238000004519 manufacturing process Methods 0.000 description 1
- 229920006395 saturated elastomer Polymers 0.000 description 1
Landscapes
- Electronic Switches (AREA)
Description
【考案の詳細な説明】 〔産業上の利用分野〕 本考案は、サーマルヘッドに関し、特に抵抗発熱体の駆
動回路の改良に関する。DETAILED DESCRIPTION OF THE INVENTION [Industrial application] The present invention relates to a thermal head, and more particularly to improvement of a drive circuit for a resistance heating element.
従来のサーマルヘッドが一例が日経エレクトロニクス、
NO.311,第90〜94頁(1983年2月28日発
行)に記載されている。An example of a conventional thermal head is Nikkei Electronics,
No. 311, pages 90 to 94 (published February 28, 1983).
その基本的回路構成は第2図に示す如くであり、各発熱
体1の一方の端子1aが共通接続線2aを介して共通電
極電源端子2に接続され、他方の端子1bがそれぞれ駆
動用IC3の個別出力端子3aに直結されている。25
はサーマルヘッドを駆動する各種の入出力端子及び電源
端子である。The basic circuit configuration is as shown in FIG. 2. One terminal 1a of each heating element 1 is connected to the common electrode power supply terminal 2 through the common connection line 2a, and the other terminal 1b is the driving IC 3 respectively. Is directly connected to the individual output terminal 3a. 25
Are various input / output terminals and power supply terminals for driving the thermal head.
第3図は一般的な駆動用IC3内部の回路構成を示した
もので、シフトレジスタ回路21、データラッチ回路2
2、ゲート回路23、及び駆動トランジスタ24より成
っている。FIG. 3 shows a circuit configuration inside a general driving IC 3, which includes a shift register circuit 21 and a data latch circuit 2.
2, a gate circuit 23, and a driving transistor 24.
入出力信号及び電源端子25のうち、25−1〜25−
5は、それぞれエネーブル入力、ラッチ入力、データ入
力、クロック入力、データ出力であり、一方25−6〜
25−8は電源端子である。このうち、25−8は接地
端子で、この接地端子25−8と電源端子2との間に所
定の電圧が印加される。このような構成のサーマルヘッ
ドでは、データ入力信号とエネーブル信号との組合わせ
により、発熱体に対する選択的通電がなされる。Of the input / output signals and the power supply terminal 25, 25-1 to 25-
5 is an enable input, a latch input, a data input, a clock input, and a data output, respectively.
25-8 is a power supply terminal. Of these, 25-8 is a ground terminal, and a predetermined voltage is applied between the ground terminal 25-8 and the power supply terminal 2. In the thermal head having such a configuration, the heating element is selectively energized by the combination of the data input signal and the enable signal.
しかしながら、上記構成のサーマルヘッドでは、電源端
子2から各発熱体への通電路の長さ即ち配線長がそれぞ
れ異なるから、電源端子2に与える電圧が一定であって
も、各発熱体の両端にかかる電圧値は共通接続線2aに
よる電圧降下のため異なり、従って発熱体に流れる電流
値がそれぞれ異なり、このため、発熱量もそれぞれ異な
る。すなわち、電源端子から最も遠い発熱体ほど発熱量
が小さくなる。従って、感熱記録紙等への印字に濃度ム
ラが生じ、印字品質が悪くなる。この濃度ムラは全発熱
体が発熱するいわゆるベタ黒印字のとき最も顕著とな
る。However, in the thermal head having the above-mentioned configuration, the lengths of the current paths from the power supply terminals 2 to the respective heating elements, that is, the wiring lengths, are different, so that even if the voltage applied to the power supply terminals 2 is constant, both ends of each heating element are Such voltage values are different due to the voltage drop due to the common connection line 2a, and therefore the current values flowing through the heating elements are different, and therefore the heat generation amounts are also different. That is, the heat generation amount becomes smaller as the heating element is farthest from the power supply terminal. Therefore, density unevenness occurs in printing on a thermal recording paper or the like, and print quality deteriorates. This density unevenness is most noticeable in so-called solid black printing in which all heating elements generate heat.
この考案は以上述べたサーマルヘッドの共通電極電源端
子から遠い発熱体ほど発熱体の両端にかかる電圧が小さ
くなり、結果的に濃度ムラが生ずるという欠点を除去
し、濃度ムラの少ない、印字品質の良好なサーマルヘッ
ドを提供することを目的とする。This invention eliminates the above-mentioned disadvantage that the voltage applied to both ends of the heating element becomes smaller as the heating element is farther from the common electrode power supply terminal of the thermal head, resulting in uneven density. It is intended to provide a good thermal head.
本考案のサーマルヘッドは、複数個の抵抗発熱体と、上
記複数個の抵抗発熱体の一方の端子に共通接続線を介し
て接続された第1の電源端子と、上記複数個の抵抗発熱
体にそれぞれ対応して設けらた、各々対応する抵抗発熱
体の他方の端子と、第2の電源端子との間に介在する駆
動トランジスタとを備え、上記駆動トランジスタの各々
は、対応する抵抗発熱体の上記一方の端子から上記第1
の電源端子までの配線距離が長いもの程飽和電圧がより
小さいものであることを特徴とするものである。The thermal head of the present invention comprises a plurality of resistance heating elements, a first power supply terminal connected to one terminal of the plurality of resistance heating elements through a common connection line, and a plurality of the resistance heating elements. And a driving transistor interposed between the other terminal of the corresponding resistance heating element and the second power supply terminal, which are provided corresponding to each of the above-mentioned driving transistors, and each of the driving transistors corresponds to the corresponding resistance heating element. From the one terminal of the
The longer the wiring distance to the power supply terminal, the smaller the saturation voltage is.
各発熱体は、駆動トランジスタ、共通接続線を介して、
定電圧源に接続された形となっている。従って、トラン
ジスタがオンしたときの発熱体を流れる電流Iは I=(Vop−Von)/(Rdot+Rc……(1) で与えられる。ここで、Vopは電源電圧、Vonはトラン
ジスタの飽和電圧、Rdotは発熱体の抵抗、Rcは共通
接続線の配線抵抗である。Each heating element, through the drive transistor, common connection line,
It is connected to a constant voltage source. Therefore, the current I flowing through the heating element when the transistor is turned on is given by I = (V op −V on ) / (R dot + R c ...... (1) where V op is the power supply voltage and V on Is the saturation voltage of the transistor, R dot is the resistance of the heating element, and R c is the wiring resistance of the common connection line.
発熱体の発熱量はI2Rdotに比例するから該発熱量を
一定にするにはIを一定にする必要がある。即ち、(1)
式を変形して、 Von=Vop−IRdot−IRc……(2) (2)式でVop,I,Rdotを一定とすると、Vonは−Rc
に比例する。即ち、Rcの増大に伴ってVonを減少させ
ることが、Iを一定にし、従って、発熱量を一定にする
条件であることが分かる。Rcは発熱体から共通電極端
子までの配線長に比例するから該配線長の長いもの程、
対応する駆動トランジスタの飽和電圧をより小さいもの
とすることにより、各発熱体の発熱量を一定にすること
ができる。Since the heat generation amount of the heating element is proportional to I 2 R dot , it is necessary to keep I constant in order to keep the heat generation amount constant. That is, (1)
V on = −R c If V on = V op −IR dot −IR c (2) (2) is fixed and V op , I, and R dot are constant, V on is −R c.
Proportional to. That is, it can be seen that decreasing V on with an increase in R c is a condition for making I constant and thus making the heat generation amount constant. Since R c is proportional to the wiring length from the heating element to the common electrode terminal, the longer the wiring length,
By making the saturation voltage of the corresponding drive transistor smaller, the heat generation amount of each heating element can be made constant.
本考案一実施例のサーマルヘッドの全体的回路構成は第
2図および第3図に示したものと同じである。異なるの
は、駆動トランジスタの各々が対応する発熱体から共通
電極2までの配線長に応じて異なる飽和電圧値を持つこ
とである。即ち、配線長が長い程飽和電圧が低く定めら
れている。The overall circuit configuration of the thermal head of one embodiment of the present invention is the same as that shown in FIGS. 2 and 3. The difference is that each of the drive transistors has a different saturation voltage value depending on the wiring length from the corresponding heating element to the common electrode 2. That is, the longer the wiring length, the lower the saturation voltage.
第1図は各発熱体の発熱量と駆動トランジスタの飽和電
圧の関係を説明するための部分的な回路図で、発熱体1
個と駆動トランジスタ1個のみを示したものである。同
図で1は発熱体、24は駆動用IC内の出力トランジス
タ、即ち駆動トランジスタ、2,25−8は発熱体に通
電するための電源端子で、2がプラス側である。15は
駆動トランジスタ24のベース電流入力端子である。ト
ランジスタ24をONにするときは、トランジスタ24
を飽和させるベース電流が端子15を通して入力され
る。16は共通接続線の配線抵抗で発熱体1の一方の端
子から端子2までの電気抵抗を模式的に表わしたもの
で、端子2から発熱体1までの通電路の長さに依存す
る。FIG. 1 is a partial circuit diagram for explaining the relationship between the heat generation amount of each heating element and the saturation voltage of the driving transistor.
Only one and one drive transistor are shown. In the figure, 1 is a heating element, 24 is an output transistor in the driving IC, that is, a driving transistor, 2, 25-8 are power supply terminals for energizing the heating element, and 2 is a positive side. Reference numeral 15 is a base current input terminal of the drive transistor 24. When turning on the transistor 24,
A base current that saturates is input through the terminal 15. Reference numeral 16 is a wiring resistance of the common connection line, which schematically represents the electric resistance from one terminal of the heating element 1 to the terminal 2, and depends on the length of the current path from the terminal 2 to the heating element 1.
発熱体1の発熱量は、発熱体の消費電力に比例する。こ
の消費電力は、発熱体を流れる電流Iの2乗と、発熱体
の抵抗Rdotとの積で与えられる。従って、この消費電
力を一定にするには電流Iを一定にする必要がある。電
流Iは次式で与えられる。The heat generation amount of the heating element 1 is proportional to the power consumption of the heating element. This power consumption is given by the product of the square of the current I flowing through the heating element and the resistance R dot of the heating element. Therefore, it is necessary to keep the current I constant in order to keep the power consumption constant. The current I is given by the following equation.
I=(Vop−Von)/(Rdot+Rc)……(3) ここでVopは電源電圧、Vonは駆動トランジスタ24の
飽和電圧、Rcは共通接続線の配線抵抗である。Vop,
Rdotは一定であるので、Iを一定にするための条件
は、(3)式を変形し、 Von=Vop−IRdot−IRc……(4) この式から、Rcの増加に伴って、Vonを減少させれば
よいことが分かる。即ち、端子2から遠い位置にある発
熱体ほど駆動トランジスタの飽和電圧Vonが小さいもの
を対応させればよいことが分かる。I = (V op −V on ) / (R dot + R c ) ... (3) where V op is the power supply voltage, V on is the saturation voltage of the drive transistor 24, and R c is the wiring resistance of the common connection line. . V op ,
Since R dot is constant, the condition for making I constant is to modify equation (3) to obtain V on = V op −IR dot −IR c (4) From this equation, increase of R c It can be seen that V on should be decreased in accordance with the above. That is, it is understood that the heating element located farther from the terminal 2 should correspond to one having a smaller saturation voltage V on of the drive transistor.
飽和電圧Vonは流れる電流値すなわち共通抵抗Rcにも
依存するが、通常充分飽和している時のVonの電流異存
性はかなり小さくまた実用的なサーマルヘッドでの使用
範囲程度ではほぼ一定と考えてよい。The saturation voltage V on also depends on the flowing current value, that is, the common resistance R c , but the current dissimilarity of V on when the saturation voltage is sufficiently saturated is usually small, and is almost constant in the practical use range of the thermal head. You can think of it.
駆動トランジスタのVonの大小は設計的にもある程度意
図して設計可能であり、製造工程におけるVonのバラツ
キをランク分けして使うことも簡単にできる。即ち、駆
動用IC毎にVonの平均値が異なる場合、Vonの平均値
が大きいもの程共通電極電源端子2により近い発熱体に
接続することとしてもよい。The size of V on of the drive transistor can be designed intentionally to some extent in terms of design, and the variation in V on in the manufacturing process can be easily ranked and used. That is, when the average value of V on is different for each driving IC, the larger the average value of V on , the closer to the common electrode power supply terminal 2 the heating element may be connected to.
以上説明したように、本考案によれば、共通電極電源端
子からの配線長が長い発熱体に対応する駆動トランジス
タとして飽和電圧の小さいものを用いることとしている
ので、各発熱体の発熱量が略同一となり、印字ムラのな
いサーマルヘッドが実現できる。この特徴はいわゆるベ
タ黒印字の時より効果的であり、そのような印字を行な
う場合にも高品質を維持できる。また階調印字のように
各発熱体の発熱量を微妙に制御する場合に特にいちじる
しい効果がある。As described above, according to the present invention, since a driving transistor having a small saturation voltage is used as a driving transistor corresponding to a heating element having a long wiring from the common electrode power supply terminal, the heating value of each heating element is substantially the same. As a result, a thermal head with uniform printing can be realized. This feature is more effective than the so-called solid black printing, and high quality can be maintained even when such printing is performed. Further, it is particularly effective when the amount of heat generated by each heating element is delicately controlled as in gradation printing.
第1図は本考案一実施例における1個の発熱体とそれに
つながった駆動トランジスタ、配線抵抗を示す配線図、 第2図はサーマルヘッドの全体的回路構成を示す図、 第3図は駆動用IC内の概要を示す図である。 1……抵抗発熱体、2……共通電極電源端子、16……
共通接続線の配線抵抗、24……駆動トランジスタ、2
5−8……接地端子。FIG. 1 is a wiring diagram showing one heating element and a driving transistor connected thereto and wiring resistance in one embodiment of the present invention, FIG. 2 is a diagram showing an overall circuit configuration of a thermal head, and FIG. 3 is a driving circuit. It is a figure which shows the outline in IC. 1 ... Resistance heating element, 2 ... Common electrode power supply terminal, 16 ...
Wiring resistance of common connection line, 24 ... Driving transistor, 2
5-8 ... Ground terminal.
Claims (1)
して接続された第1の電源端子と、 上記複数個の抵抗発熱体にそれぞれ対応して設けられ、
各々対応する抵抗発熱体の他方の端子と第2の電源端子
との間に介在する駆動トランジスタとを備え、 上記第1の電源端子と第2の電源端子間には一定の電圧
を印加し、 第1の電源端子から抵抗発熱体までの配線距離が長いも
の程対応する駆動トランジスタの飽和電圧をより小さい
もので構成し上記抵抗発熱体の発熱量を一定にしたこと
を特徴とするサーマルヘッド。1. A plurality of resistance heating elements, a first power supply terminal connected to one terminal of the plurality of resistance heating elements via a common connection line, and each of the plurality of resistance heating elements. Correspondingly provided,
A driving transistor interposed between the other terminal of the corresponding resistance heating element and the second power supply terminal, and a constant voltage is applied between the first power supply terminal and the second power supply terminal; A thermal head characterized in that the longer the wiring distance from the first power supply terminal to the resistance heating element, the smaller the saturation voltage of the corresponding drive transistor, and the more constant the heating value of the resistance heating element.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2636887U JPH066927Y2 (en) | 1987-02-26 | 1987-02-26 | Thermal head |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2636887U JPH066927Y2 (en) | 1987-02-26 | 1987-02-26 | Thermal head |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS63134745U JPS63134745U (en) | 1988-09-05 |
| JPH066927Y2 true JPH066927Y2 (en) | 1994-02-23 |
Family
ID=30827390
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP2636887U Expired - Lifetime JPH066927Y2 (en) | 1987-02-26 | 1987-02-26 | Thermal head |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH066927Y2 (en) |
-
1987
- 1987-02-26 JP JP2636887U patent/JPH066927Y2/en not_active Expired - Lifetime
Also Published As
| Publication number | Publication date |
|---|---|
| JPS63134745U (en) | 1988-09-05 |
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