JPH01150555A - Thermal head - Google Patents
Thermal headInfo
- Publication number
- JPH01150555A JPH01150555A JP30956487A JP30956487A JPH01150555A JP H01150555 A JPH01150555 A JP H01150555A JP 30956487 A JP30956487 A JP 30956487A JP 30956487 A JP30956487 A JP 30956487A JP H01150555 A JPH01150555 A JP H01150555A
- Authority
- JP
- Japan
- Prior art keywords
- independent electrodes
- ceramic substrate
- common electrode
- heat
- independent
- 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.)
- Pending
Links
Landscapes
- Electronic Switches (AREA)
Abstract
Description
【発明の詳細な説明】
〔産業上の利用分計〕
この発明は、サーマルヘッド、特に、エツジ形厚膜ナー
マルヘッドに関するものである。DETAILED DESCRIPTION OF THE INVENTION [Industrial Application] The present invention relates to a thermal head, particularly an edge type thick film thermal head.
従来のエツジ形厚膜サーマルヘッドの加熱部分の一例を
示すと第3図のとおりである。An example of a heating portion of a conventional edge-type thick film thermal head is shown in FIG.
図において、符号(1)は各電極(21、(3)ヒに設
けられている抵抗体、(2ンはヒ記電極(2) 、 (
3)の−万であって電源(5)に接続されているコモン
電極、(3)は他方の電極であってスイッチング回路(
6)に接続の独立電極であり、コモン電極(2)及び独
立電極(りはその端部が交互に並列されてセラミック基
板(4]、ヒに設けられている。In the figure, symbol (1) indicates the resistor provided at each electrode (21, (3)), (2) indicates the resistor provided at each electrode (2), (
3) is the common electrode connected to the power supply (5), and (3) is the other electrode connected to the switching circuit (
The common electrode (2) and the independent electrode (6) are provided on the ceramic substrate (4), with their ends alternately arranged in parallel.
また、コモン電極(2)及び独立電極(りは、共にその
厚さが同じ厚さに構成されている。Further, the common electrode (2) and the independent electrode (2) are both configured to have the same thickness.
サーマルヘッドの加熱部は、このように構成されている
ので、印字に際しては、コモン電極(2)に通電すると
共に、所要のスイッチング回路(6)に通電すると、第
2B図に示すように、コモン電極(2)と独立電極(り
との間に抵抗体(1)を介して電流が流れ、この電流に
よって抵抗体(1)が図に示す発熱領域において発熱し
、この発熱によって印字する。Since the heating section of the thermal head is configured in this way, when printing, when the common electrode (2) is energized and the required switching circuit (6) is energized, the common electrode (2) is turned on as shown in Figure 2B. A current flows through the resistor (1) between the electrode (2) and the independent electrode (ri), and this current causes the resistor (1) to generate heat in the heat generating region shown in the figure, and printing is performed by this heat generation.
しかしながら、この発熱は、画電極(2) 、 (3)
及び抵抗体(1)が接しているセラミック基板(4)に
逃げる。特に、電極と発熱抵抗体の接している部分は、
電極へ熱が伝導し放熱するため他の部分より昇温か遅く
、従って、抵抗体(1)の温度分布は第2B図に示す谷
部を有する温度分布となる。However, this heat generation is caused by the image electrodes (2), (3)
and escapes to the ceramic substrate (4) which is in contact with the resistor (1). In particular, the part where the electrode and the heating resistor are in contact with each other,
Since heat is conducted to the electrode and dissipated, the temperature rises slower than other parts, so the temperature distribution of the resistor (1) becomes a temperature distribution having valleys as shown in FIG. 2B.
−万、第4図に示すように、コモン電極(2)及び独立
電極(6)を薄く構成するならば、第2C図に示すよう
に、電極による放熱作用がなくなるため、抵抗体(1)
の左右の非通電部分へも伝熱するようになり、従って、
温度分布が図の分布図に示すように、隣接ドツトである
非加熱部分に向けてなだらかに裾をひくようになる。- If the common electrode (2) and the independent electrode (6) are made thin as shown in Fig. 4, the heat dissipation effect of the electrodes will be eliminated, as shown in Fig. 2C, so that the resistor (1)
Heat also transfers to the non-current parts on the left and right sides of the
As shown in the distribution diagram in the figure, the temperature distribution gradually tapers toward the non-heated portion, which is the adjacent dot.
従来装置は、上記のように構成され作用するので、電極
の厚さが厚い場合は、独立電極に接する発熱抵抗体部分
の放熱が穴縁くなり、発熱領域中に昇温不足部分を生じ
たり、あるいは、電極の厚さが薄い場合は、隣接抵抗体
へ伝熱することにより、発熱領域と非発熱領域との境界
部分が裾をひいて不鮮明になるために、印字においても
、1ドツト中に印字の不十分の部分を生じたり、あるい
は、隣接ドツトにまで影響を及ぼして印字を不鮮明にす
る等の問題点を有していた。Conventional devices are configured and operate as described above, so if the electrodes are thick, the heat dissipation of the heating resistor portion in contact with the independent electrode will be at the edge of the hole, resulting in insufficient temperature rise in the heating area. Alternatively, if the electrode is thin, heat transfers to the adjacent resistor and the boundary between the heat generating area and non-heat generating area becomes narrow and unclear. This method has problems such as insufficient printing on the dots, or even affecting adjacent dots, making the print unclear.
この発明は、L記の問題点を解決するためになされたも
ので、独立電極での熱の逃げを防止することにより、1
ドツト内の温度を均一にしかつコモン電極への放熱を充
分性なえるようにすることにより、隣接ドツトへの熱伝
達による影響を少なくしたサーマルヘッドを得ることを
目的とする。This invention was made to solve the problem described in L. By preventing heat from escaping from the independent electrode, 1.
The object of the present invention is to obtain a thermal head in which the influence of heat transfer to adjacent dots is reduced by making the temperature within the dot uniform and ensuring sufficient heat radiation to the common electrode.
この発明に係るサーマルヘッドは、独立電極をコモン電
極より薄くすると共に独立電極とセラミック基板との間
に断熱材を介装させて設けているものである。In the thermal head according to the present invention, the independent electrode is made thinner than the common electrode, and a heat insulating material is interposed between the independent electrode and the ceramic substrate.
独立電極をコモン電極より薄く構成していると共に、独
立電極とセラミック基板との間に断熱材を設けているた
めに、この部分からのセラミック基板への熱伝達が抑制
され、その結果、発熱領域の昇温か速くなり、しかも、
隣接ドツトへの伝熱は抑制されるので、境界領域におけ
る昇温領域と、非昇温領域が明瞭となる。Since the independent electrode is made thinner than the common electrode and a heat insulating material is provided between the independent electrode and the ceramic substrate, heat transfer from this part to the ceramic substrate is suppressed, and as a result, the heat generation area The temperature rises faster, and
Since heat transfer to adjacent dots is suppressed, the temperature-increased region and the non-temperature-increased region in the boundary region become clear.
以下、この発明をその一実施例を示す図に基づいて説明
する。なお、符号(1)、 (2)、 (4)〜(6)
で示すものは、従来装置において同一符号で示したもの
と同−又は同等のものである。The present invention will be explained below based on the drawings showing one embodiment thereof. In addition, codes (1), (2), (4) to (6)
Components indicated by are the same as or equivalent to those indicated by the same reference numerals in the conventional device.
第1図において、符号(11)はコモン電極(2)より
薄く、例えば、コモン電極(2)の厚さを約4μmとし
た場合に約0.4μmのように薄く構成した独立電極で
あり、スイッチング回路(6)に接続されていることは
従来と同様である。In FIG. 1, reference numeral (11) is an independent electrode that is thinner than the common electrode (2), for example, about 0.4 μm when the common electrode (2) has a thickness of about 4 μm. The connection to the switching circuit (6) is the same as in the conventional case.
また、符号(12)は独立電極(11)とセラミック基
板(4)との間に介装して設けられている断熱材であっ
て、これによって、独立電極(11)からのセラミック
基板(4)への伝熱を防止すると共に独立電極を薄くす
ることにより熱抵抗を大等<シて発熱領域内の独立電極
部に低温領域の発生を防止している。また、この断熱材
(12)の介装により、独立電極(11)の上面高さを
コモン電極(2)と同高にしているため、発熱体(1)
頂部の高さが各ドツト及びドツト内とも等しくすること
ができる。Further, reference numeral (12) is a heat insulating material interposed between the independent electrode (11) and the ceramic substrate (4). ), and by making the independent electrodes thinner, the thermal resistance is increased and the generation of a low temperature region in the independent electrode portion within the heat generating region is prevented. In addition, by interposing this heat insulating material (12), the top surface height of the independent electrode (11) is made the same as that of the common electrode (2), so that the heating element (1)
The height of the top can be made equal to each dot and within the dot.
この発明は、上記のように構成されているので、スイッ
チング回路(6)が閉じると、電流tはコモン電極(2
)から抵抗体(1)を介して独立電極(11)に流れる
。従って、抵抗体(1)は、この流れる電流によって発
熱するが、独立電極(11)とセラミック基板(4)と
の間に断熱材(12)が設けられているために、第2A
図に示すように、独立電極(11)の部分よりセラミッ
ク基板(4)への熱伝達が極めて少なく、かつ、独立電
極への伝熱も少なく、従って昇温も速くかつ発熱領域全
般にわたって均等に加熱昇温して、谷部も現われない抵
抗体温度分布を示すと共に、コモン電極(2)からセラ
ミック基板(4)への伝熱によって、抵抗体(1)から
の隣接ドツトへの伝熱を減少させて、隣接ドツトの昇温
を抑え、これらの結果、印字の均質化と昇温の迅速化及
び隣接ドツトへの影響を防止している。Since this invention is configured as described above, when the switching circuit (6) is closed, the current t is transferred to the common electrode (2).
) flows to the independent electrode (11) via the resistor (1). Therefore, the resistor (1) generates heat due to this flowing current, but since the heat insulating material (12) is provided between the independent electrode (11) and the ceramic substrate (4), the second A
As shown in the figure, the heat transfer from the independent electrode (11) to the ceramic substrate (4) is extremely small, and the heat transfer to the independent electrode is also small, so the temperature rises quickly and evenly over the entire heat generating area. As the temperature increases, the temperature distribution of the resistor shows no valleys, and the heat transfer from the resistor (1) to the adjacent dots is enhanced by the heat transfer from the common electrode (2) to the ceramic substrate (4). This reduces the temperature increase of adjacent dots, resulting in uniform printing, rapid temperature rise, and prevention of influence on adjacent dots.
以ヒのように、この発明によれば、独立電極をコモン電
極に比べて薄くすると共に独立電極とセラミック基板と
の間に断熱材を設けているので、抵抗体の昇温も速くか
つ独立電極からのセラミック基板への熱の伝達もきわめ
て少なくなって昇温も速くなり、かつ、1ドツト間の昇
温も均等になると共に隣接ドツトへの温度の影響も防止
し得るサーマルヘッドが得られる効果を有している。As described below, according to this invention, the independent electrode is made thinner than the common electrode, and a heat insulating material is provided between the independent electrode and the ceramic substrate, so that the temperature of the resistor increases quickly and the independent electrode This has the effect of providing a thermal head in which the transfer of heat from the dot to the ceramic substrate is extremely reduced, the temperature rises quickly, the temperature rise between dots is even, and the influence of temperature on adjacent dots can be prevented. have.
第1図はこの発明の一実施例の斜視図、第2A図は第1
図の発熱領域における抵抗体の温度分布図、第2B図及
び第2C図は従来装置を示す第6図及び第4図のそれぞ
れの発熱領域における抵抗体の温度分布図、第3図及び
第4図は従来のサーマルヘッドの加熱部の2例の斜視図
である。
(1)・・抵抗体、(2)・・コモン電極、(4)・・
セラミック基板、(11)・・独立電極、(12)・・
断熱材。
なお、各図中、同一符号は同−又は相当部分を示す。
1 、祢抗体
2 ゛ フt″−電櫓
4t!フミーlり基板
11: 独在電榴
12 前塾枕
昂2A図
昂2B図
篤2C図FIG. 1 is a perspective view of one embodiment of the invention, and FIG. 2A is a perspective view of an embodiment of the invention.
Figures 2B and 2C are temperature distribution diagrams of the resistor in the heat generation area of the figure, Figures 2B and 2C are temperature distribution diagrams of the resistor in the heat generation area of Figures 6 and 4, respectively, showing the conventional device. The figures are perspective views of two examples of heating parts of conventional thermal heads. (1)...Resistor, (2)...Common electrode, (4)...
Ceramic substrate, (11)...Independent electrode, (12)...
Insulation. In each figure, the same reference numerals indicate the same or corresponding parts. 1, Nei Antibody 2 ゛ Fut''-Electron tower 4t! Fumyi board 11: Dokusei electric shell 12 Maejuku Makura 2A figure 2B figure Atsushi 2C figure
Claims (1)
設されているエッジ形厚膜のサーマルヘツドにおいて、
独立電極がコモン電極より薄く構成されていると共に独
立電極とセラミック基板との間に断熱材が設けられてい
ることを特徴とするサーマルヘツド。In an edge-type thick film thermal head in which common electrodes and independent electrodes are arranged alternately on a ceramic substrate,
A thermal head characterized in that the independent electrodes are thinner than the common electrodes, and a heat insulating material is provided between the independent electrodes and the ceramic substrate.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP30956487A JPH01150555A (en) | 1987-12-09 | 1987-12-09 | Thermal head |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP30956487A JPH01150555A (en) | 1987-12-09 | 1987-12-09 | Thermal head |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH01150555A true JPH01150555A (en) | 1989-06-13 |
Family
ID=17994539
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP30956487A Pending JPH01150555A (en) | 1987-12-09 | 1987-12-09 | Thermal head |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH01150555A (en) |
-
1987
- 1987-12-09 JP JP30956487A patent/JPH01150555A/en active Pending
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