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JPS5922966B2 - Temperature control device and recording pen using it - Google Patents
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JPS5922966B2 - Temperature control device and recording pen using it - Google Patents

Temperature control device and recording pen using it

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Publication number
JPS5922966B2
JPS5922966B2 JP11824378A JP11824378A JPS5922966B2 JP S5922966 B2 JPS5922966 B2 JP S5922966B2 JP 11824378 A JP11824378 A JP 11824378A JP 11824378 A JP11824378 A JP 11824378A JP S5922966 B2 JPS5922966 B2 JP S5922966B2
Authority
JP
Japan
Prior art keywords
heating element
heat dissipation
signal
current
temperature
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
JP11824378A
Other languages
Japanese (ja)
Other versions
JPS5544653A (en
Inventor
昭雄 渡辺
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.)
NIPPON DENKI SANEI KK
Original Assignee
NIPPON DENKI SANEI KK
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 DENKI SANEI KK filed Critical NIPPON DENKI SANEI KK
Priority to JP11824378A priority Critical patent/JPS5922966B2/en
Publication of JPS5544653A publication Critical patent/JPS5544653A/en
Publication of JPS5922966B2 publication Critical patent/JPS5922966B2/en
Expired legal-status Critical Current

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  • Recording Measured Values (AREA)
  • Control Of Resistance Heating (AREA)
  • Control Of Temperature (AREA)

Description

【発明の詳細な説明】 本発明は、直接通電がなされ、ジュール熱によつて発熱
が行われる発熱体に対し、これに対する通電電流を制御
することによつてこの発熱体の動作温度を常時所定の温
度に設定するようにした温度制御装置とこれを用いた記
録ペンに係わる。
DETAILED DESCRIPTION OF THE INVENTION The present invention is directed to a heating element that is directly energized and generates heat using Joule heat, and the operating temperature of the heating element is always maintained at a predetermined level by controlling the current supplied to the heating element. The present invention relates to a temperature control device that sets the temperature at a temperature of

この種発熱体として一般に用いられている金属抵抗体、
あるいは半導体は、温度変化に対しその抵抗値が変化す
る。一般に金属抵抗体は正の温度特性を有し、半導体の
中には負の温度特性を有するものもあることが知られて
いる。一方、発熱体の使用条件、使用態様、外囲条件等
による放熱情態、即ち、熱平衡条件の相違によつて発熱
体に対する電流を一定にしたり、また電力を一定にした
りしても、発熱体の動作温度を設計通り、なιルは、所
望の温度に設定できないことになる。
A metal resistor commonly used as this type of heating element,
Alternatively, the resistance value of a semiconductor changes with temperature changes. It is known that metal resistors generally have positive temperature characteristics, and some semiconductors have negative temperature characteristics. On the other hand, even if the current to the heating element is kept constant or the electric power is constant due to differences in heat dissipation characteristics depending on the usage conditions, usage mode, surrounding conditions, etc. of the heating element, that is, the thermal equilibrium conditions, the heating element This means that the operating temperature cannot be set to the desired temperature as designed.

このような温度の変動が生じないようにする温度制御装
置としては、種々のものが提案されてい・ る。
Various types of temperature control devices have been proposed to prevent such temperature fluctuations.

例えば、発熱体に熱的に結合して温度検出素子、例えば
サーミスタを配し、これによつて発熱体に対する通電量
を制御するとか、発熱体を含んでブリツジ回路を構成し
、発熱体の抵抗の変化によつて生じた不平衡電圧による
出力によつて発熱体の電源を制御するとかの方法をとる
温度制御装置がある。しかしながら発熱体に温度検出素
子を熱的に結合して設けることは、その結合度に感度が
依存することから、結合の仕方に可成り問題があること
や、発熱体が高温のものである場合は、検出素子の耐熱
の問題が生じてくる。更に、発熱体が感熱記録器におけ
る記録ペンに用いる発熱体である場合は、このような検
出素子を発熱体、したがつて記録ペンに附加することは
、記録ペンの機械的負荷が大となつて、記録ペンの記録
紙に対する移行の応答性が低下するという欠点を招来す
る。また、ブリツジ回路構成によるものにおいては、ブ
リツジ回路を構成する各抵抗素子が、発熱体の抵抗値と
ほぼ等しい値に選ばれる必要があることから電力の損失
が大きいという欠点がある。本発明は、このような欠点
のない温度制御装置とこれを用いた記録ペンを提供する
ものである。先ず本発明を詳細に説明するに先立つて、
本発 C明の理解を容易にするために、本発明のいわば
、原理ともいう基本的思想について説明する。今、第1
図に示すように、電源Eに正の温度係数を有する発熱体
1と負性抵抗−Rとが直列に接続された回路を考える。
この回路に於て発熱体1 二の或る温度に於ける抵抗を
RTとし、電源電圧Eが一定電圧で、IOを回路電流と
すると、が成り立つ。
For example, a temperature detection element such as a thermistor may be thermally coupled to the heating element to control the amount of current to the heating element, or a bridge circuit including the heating element may be configured to resist the resistance of the heating element. There is a temperature control device that uses a method such as controlling the power source of a heating element by outputting an unbalanced voltage caused by a change in temperature. However, when providing a temperature detection element thermally coupled to a heating element, the sensitivity depends on the degree of coupling, so there are considerable problems with the method of coupling, and when the heating element is high temperature. In this case, the problem of heat resistance of the detection element arises. Furthermore, if the heating element is a heating element used in a recording pen in a thermal recorder, adding such a detection element to the heating element and therefore to the recording pen will increase the mechanical load on the recording pen. This results in a disadvantage that the responsiveness of the recording pen to the recording paper decreases. Further, in the bridge circuit configuration, each resistance element constituting the bridge circuit must be selected to have a resistance value that is approximately equal to the resistance value of the heating element, which has the disadvantage that power loss is large. The present invention provides a temperature control device free from such drawbacks and a recording pen using the same. First, before explaining the present invention in detail,
In order to facilitate understanding of invention C, the basic idea, also called the principle, of the invention will be explained. Now, the first
As shown in the figure, consider a circuit in which a power source E is connected in series with a heating element 1 having a positive temperature coefficient and a negative resistance -R.
In this circuit, if RT is the resistance of the heating element 1 2 at a certain temperature, the power supply voltage E is a constant voltage, and IO is the circuit current, then the following holds true.

そして発熱体1の放熱状態を表わす熱抵抗をβ(℃/W
)、発熱体1の消費している電力をP(VV)とすると
、\BVlbυノ となり、発熱体1の平衡する温度Tは T=β・P ・・・・・・・・・・
・・(3)となる。
Then, the thermal resistance representing the heat dissipation state of the heating element 1 is β(℃/W
), and if the power consumed by the heating element 1 is P(VV), it becomes \BVlbυノ, and the equilibrium temperature T of the heating element 1 is T=β・P...
...(3).

今、発熱体1の放熱状態の変化によりβが変化しても発
熱体1の温度Tが変化せず一定となる為の条件を考えて
みる。ここで、T,P,IO及びRTはβの関数であり
、10及びRTはT(7)関数であることから(1),
(2)及び(3)式を以下のように展開し得る。
Now, let us consider the conditions under which the temperature T of the heating element 1 does not change and remains constant even if β changes due to a change in the heat dissipation state of the heating element 1. Here, since T, P, IO and RT are functions of β, and 10 and RT are T(7) functions, (1),
Equations (2) and (3) can be expanded as follows.

先ず(3)式から−・方、第1図に於て、負性抵抗−R
がないときの1路電流をIO′とすると、1V1 このときの熱抵抗βの変化に対する発熱体1の温DT度
Tの変化を(−yとすると、AD式からAρ となる。
First, from equation (3), in Figure 1, negative resistance -R
If the one-way current when there is no current is IO', then 1V1.If the change in the temperature DT degree T of the heating element 1 with respect to the change in the thermal resistance β at this time is (-y), it becomes Aρ from the AD equation.

即ちこの(自)式の意味するところは第1図に於て、負
性抵抗−Rがあるときの回路電流10を負性抵抗−Rが
ないときの回路電流10′6こなるように負性抵抗−R
があるときの電源電圧Eを減少して等しい回路電流1に
設定すれば、この設定された電流1に於て、−Rがある
ときも−Rがないときも同一発熱体で且つ同一β条件で
あるものに関するβに対する温度変化の両者の比を示す
ものRT+Rであつて、負性抵抗−Rがある回路の方が
?RT−Rの比に基づきβに対する温度変化が小さくな
ることを示している。
In other words, what this formula (self) means is that in Figure 1, the circuit current 10 when there is a negative resistance -R is changed to the circuit current 10'6 when there is no negative resistance -R. Sexual resistance-R
If we reduce the power supply voltage E and set it to the same circuit current 1, then at this set current 1, the same heating element and the same β condition when there is -R and when there is no -R. Which shows the ratio of the temperature change to β with respect to RT+R, which circuit has a negative resistance -R? It is shown that the temperature change with respect to β becomes smaller based on the RT-R ratio.

次に(自)式に於て、両者の等しい回路電流が有限値で
ある制限のもとで、RをRTに近づけるときの極限状態
を考えると、この場合第1図に於けるEは(自)式の条
件を守りながらEをOに近づけねばDRTならないが、
他のβ,一及びRTは有限値であ゛ DTdT
dT るので一/(一)′はOに近づくことが理解されdβ
dβよう。
Next, in equation (self), considering the limit state when R is brought close to RT under the restriction that the equal circuit currents of both are finite values, in this case E in Fig. 1 becomes ( DRT cannot be obtained if E approaches O while observing the conditions of formula (a).
The other β, 1 and RT are finite values. DTdT
Since dT, it is understood that 1/(1)' approaches O, and dβ
dβ Yo.

即ち負性抵抗−Rがあるときの発熱体1の熱抵抗βに対
する温度Tの変化は負性抵抗−Rがないときのそれに比
べて0に近づくことが判る。なお以上は発熱体1の抵抗
値RTをRT=RO(1+αT)で表わした時の温度係
数αが正の有ノ限値である場合にいえることである。
That is, it can be seen that the change in temperature T with respect to the thermal resistance β of the heating element 1 when there is negative resistance -R is closer to 0 than when there is no negative resistance -R. The above is true when the temperature coefficient α is a positive finite value when the resistance value RT of the heating element 1 is expressed as RT=RO(1+αT).

この温度係数αが今葭りに0であると、A5)式の幇Y
はOとなDTdT′り一―/(−)は1となり、負性抵
抗−Rの作用dβ dβがあつても発熱体1のβに対
する温度変化を小さくすることはできない。
If this temperature coefficient α is exactly 0, then the equation Y of A5)
is O and DTdT' -/(-) is 1, and even if there is an effect of the negative resistance -R dβ dβ, the temperature change of the heating element 1 with respect to β cannot be made small.

換言すればこの温度係数αの正の値は大きければ大きい
程、効果も大きくなることが05)式から判る。以上述
べてきた結論をまとめると、第1図に於て、負性抵抗−
Rの抵抗値Rを正の温度係数αを有する発熱体1の抵抗
RTに近い値に設定するときは、発熱体1の放熱状態β
のいかにかかわらず発熱体1の温度をほぼ一定の所望の
温度Tに設定できるということがいえる。
In other words, it can be seen from equation 05) that the larger the positive value of the temperature coefficient α, the greater the effect. To summarize the above conclusions, in Figure 1, negative resistance -
When setting the resistance value R of R to a value close to the resistance RT of the heating element 1 having a positive temperature coefficient α, the heat dissipation state β of the heating element 1
Regardless of the above, it can be said that the temperature of the heating element 1 can be set to a substantially constant desired temperature T.

本発明においては、このような基本的思想に基いてなさ
れたものであり、次に本発明の構成を説明する。
The present invention has been made based on such a basic idea, and the configuration of the present invention will be explained next.

本発明においては、例えば、第2図にそのプロツク図を
示すように、発熱体、即ち、本発明の1の発明において
は、感熱記録紙に対接される記録ペン2に組込まれる発
熱体1を所定の放熱条件において所望の動作温度に設定
する動作温度設定電気信号を得る動作温度設定電気信号
供給手段3と、この手段よりの動作温度設定電気信号に
よつて出力電流が制御されこの出力電流を上記発熱体1
に供給する電流供給手段4と、発熱体1の温度係数に依
存して所定の放熱条件からの放熱条件の変動に伴う発熱
体1の通電電流に基づく信号の変動を検出し放熱条件依
存電気信号を出力する故熱条件依存電気信号検出手段5
と、この検出手段5より得られる信号を所定の大きさに
規制し発熱体1に対する通電電流方向に対して正帰還の
方向に帰するように電流供給手段4に印加して発熱体側
から見た回路中に形成される負性抵抗成分の値を発熱体
の抵抗値に近接させた動作点を有せしめる正帰還手段と
を有する。
In the present invention, for example, as shown in the block diagram of FIG. an operating temperature setting electrical signal supplying means 3 for obtaining an operating temperature setting electrical signal for setting the operating temperature to a desired operating temperature under predetermined heat dissipation conditions; The above heating element 1
A current supply means 4 supplies current to the heating element 1, and detects a change in a signal based on the current flowing through the heating element 1 as the heat radiation condition changes from a predetermined heat radiation condition depending on the temperature coefficient of the heating element 1, and generates a heat radiation condition dependent electrical signal. thermal condition dependent electric signal detection means 5 that outputs
Then, the signal obtained from the detection means 5 is regulated to a predetermined magnitude and applied to the current supply means 4 so as to return the signal in the direction of positive feedback with respect to the direction of current flowing to the heating element 1, as seen from the heating element side. and positive feedback means for making the value of the negative resistance component formed in the circuit have an operating point close to the resistance value of the heating element.

この正帰還手段は電流供給手段4と規制回路6と合成回
路7とから成つている。第2図に示された例は、発熱体
1が正の温度係数を有する場合である。発熱体1が組込
まれた記録ペンは、図示しないが、感温記録紙上を記録
信号に応じて走査するようになされ、記録ペン2による
局部的加熱によつて記録紙上にペン2の走査パターンに
応じたパターンの例えば可視像を形成してその記録を行
うようになされている。動作温度設定電気信号供給手段
3は、前述したように、発熱体1を、所定の放熱条件に
おいて所望の動作温度に設定する信号電圧Eを得る例え
ば直流電源Eより構成される。
This positive feedback means consists of a current supply means 4, a regulating circuit 6, and a combining circuit 7. The example shown in FIG. 2 is a case where the heating element 1 has a positive temperature coefficient. Although not shown, the recording pen incorporating the heating element 1 is configured to scan a temperature-sensitive recording paper according to a recording signal, and local heating by the recording pen 2 causes a scanning pattern of the pen 2 to be formed on the recording paper. For example, a visible image of a corresponding pattern is formed and recorded. As described above, the operating temperature setting electrical signal supplying means 3 is constituted by, for example, a DC power supply E that obtains a signal voltage E for setting the heating element 1 to a desired operating temperature under predetermined heat dissipation conditions.

電流供給手段4は、例えば増幅度Aを有する増幅器より
構成される。
The current supply means 4 is composed of an amplifier having an amplification degree A, for example.

検出手段5は、例えば、発熱体1の抵抗値より十分低い
抵抗値を有する抵抗器RDより構成し得る。
The detection means 5 may be constituted by a resistor RD having a resistance value sufficiently lower than the resistance value of the heating element 1, for example.

図示の例では手段3、即ち電源Eの両端間に合成回路7
と増幅器4と抵抗器5と発熱体1との直列回路が接続さ
れた構成となされている。正帰還手段〔4,6,7〕は
、例えば抵抗5の両端と合成回路7との間に夫々k1お
よびK2の増幅率を有する出力電圧正帰還用増幅器6a
と、発熱体1に供給されている電圧を負帰還するための
増幅器6bとより構成し得る。
In the illustrated example, the means 3, i.e. the combining circuit 7 is connected across the power supply E.
A series circuit including an amplifier 4, a resistor 5, and a heating element 1 is connected. The positive feedback means [4, 6, 7] are, for example, output voltage positive feedback amplifiers 6a having amplification factors of k1 and K2, respectively, between both ends of the resistor 5 and the combining circuit 7.
and an amplifier 6b for negative feedback of the voltage supplied to the heating element 1.

この構成において、今、増幅器4の出力電圧をEO、負
荷に流れている電流10とすると、(E+k1・EO−
K2・RT−10)A=EO・・・・・・(イ)となる
In this configuration, if the output voltage of the amplifier 4 is EO and the current flowing through the load is 10, then (E+k1・EO−
K2・RT-10) A=EO...(A).

この(有)式の関係の等価回路は第3図に示す回路にほ
かならない。即ち、K2〉k1の条件を満足するように
、k1およびK2の値を設定すれば、第2図の回路構成
のもので、発熱体1に対して、基準電圧(E/(K2−
k1))、負性抵抗({−k1/(K2−k1)}・R
D)をもつ電源が接続された関係が得られることになる
。したがつて、第1図に対応させることによつて明らか
なように、発熱体1の放熱条件が変動しても、発熱体1
の動作温度が変動することがないようにするには、rン
7・RDを発熱体の抵抗値RTに近づけ(例えばk1を
一定にした状態でK2を変以させてKl7壬、7・RD
をRTに近づけ)た後、Eを変化させてIOを説定すべ
き電流即ち、所定の放熱条件において所望の動作温度を
得る電流に近づければ、発熱体1の動作温度を一定に設
定できることになる。
The equivalent circuit of this relationship is none other than the circuit shown in FIG. That is, if the values of k1 and K2 are set so as to satisfy the condition K2>k1, then with the circuit configuration shown in FIG. 2, the reference voltage (E/(K2-
k1)), negative resistance ({-k1/(K2-k1)}・R
A relationship in which the power sources with D) are connected is obtained. Therefore, as is clear from the correspondence with FIG. 1, even if the heat radiation conditions of the heating element 1 change, the heating element
In order to prevent the operating temperature from fluctuating, it is necessary to bring rn7・RD close to the resistance value RT of the heating element (for example, by changing K2 while keeping k1 constant,
The operating temperature of the heating element 1 can be set constant by changing E to bring IO closer to the current that should be used, that is, the current that provides the desired operating temperature under predetermined heat dissipation conditions. become.

尚、上述した場合のように、増幅率Aは、A→1とする
場合に限られるものではなく有限な値をとることも何ら
支障がない。また、1式において、k1=K2=kとお
くと、となる。
Note that, as in the case described above, the amplification factor A is not limited to the case where A→1, and there is no problem in taking a finite value. Furthermore, in equation 1, if we set k1=K2=k, then

この場合は、第4図に示すプロツク図となり、この場合
、RDは電流検出抵抗として働く。(25)式において
、増幅率A、およびkは有限な値とする。ここに、とな
り、この(26)氏の等価回路は、第5図に示す回路と
なる。
In this case, the block diagram is shown in FIG. 4, and in this case, RD functions as a current detection resistor. In equation (25), the amplification factor A and k are assumed to be finite values. Here, the equivalent circuit of Mr. (26) becomes the circuit shown in FIG.

則ち、(Ak−1)〉0なる条件を満すように、増幅率
Aおよびkに選ぶと、(AE)なる一定電圧で出力抵抗
が−RO(Ak−1)の負性抵抗をもつ電源が発熱体R
Tに接続されたものと等価となる。したがつて、この回
路を第1図に対応させることによつて明らかなように、
Aは任意の値に選べるので例えばA=1にとると、kを
?′.′:[モ囗MI::;:体1の動作温度を一定に設
定できることになる。
In other words, if the amplification factors A and k are chosen to satisfy the condition (Ak-1)>0, then the output resistance will have a negative resistance of -RO(Ak-1) at a constant voltage of (AE). Power source is heating element R
It is equivalent to the one connected to T. Therefore, as is clear by making this circuit correspond to Fig. 1,
Since A can be chosen to be any value, for example, if A=1, then k? '. ':[MO囗MI::;:The operating temperature of the body 1 can be set constant.

第6図は、本発明装置の具体的回路例を示すものであり
、発熱体1が正の温度係数を有する場合で第2図と対応
する部分には同一符号を付して重複説明を省略する。今
、2つの正温度係数の発熱体AおよびBに、第6図の回
路構成による本発明の温度制御装置を付設して、発熱体
1の周囲条件を夫々0℃の氷水中と、27℃の空気中と
して各周囲条件における発熱体抵抗値を測定し、これら
をグラフに表わしてみると、第7図中実線14Aおよび
14Bとなつた。
FIG. 6 shows a specific circuit example of the device of the present invention, and when the heating element 1 has a positive temperature coefficient, parts corresponding to those in FIG. do. Now, the temperature control device of the present invention having the circuit configuration shown in FIG. 6 is attached to two heating elements A and B having a positive temperature coefficient, and the ambient conditions of the heating element 1 are set to ice water at 0°C and 27°C. When the heating element resistance values were measured in air under various ambient conditions and plotted on a graph, solid lines 14A and 14B in FIG. 7 were obtained.

次に同様の2つの発熱体AおよびBを定電甲加熱とした
場合の同様の測定を行つて、これらをグラフに表わして
みると第7図中破線15Aおよび15Bとなつて外囲条
件で大きく変動している。尚、試料としての発熱体A,
Bの温度係数は約+0,05%/℃であり、発熱体の抵
抗値の測?は、これの供給電圧と供給電流から換算して
求めた。この結果からも明らかなように本発明によれば
、発熱体が外囲条件、即ち放熱条件の影響を受けて変動
することが効果的に回避されている。
Next, similar measurements were made when two similar heating elements A and B were subjected to constant electric heating, and when these were expressed in a graph, the broken lines 15A and 15B in Figure 7 were obtained under the surrounding conditions. It's changing a lot. In addition, heating element A as a sample,
The temperature coefficient of B is approximately +0.05%/°C, which is a measure of the resistance value of the heating element. was calculated from the supply voltage and current. As is clear from this result, according to the present invention, it is effectively possible to prevent the heating element from changing due to the influence of the surrounding conditions, that is, the heat dissipation conditions.

尚、本発明による温度制御装置の具体的回路例は上述し
た例に限らず種々の構成を採り得るものである。
Note that the specific circuit example of the temperature control device according to the present invention is not limited to the above-mentioned example, and various configurations may be adopted.

例えば、第8図に示すようにパルス変換器8を設けて発
熱体1をパルス電流で動作するようにすることもできる
。尚、第8図においては、信号規制回路6として積分回
路6aおよび6bを用いた場合である。上述したように
、本発明による温度制御装置によれば、発熱体の外囲条
件による放熱条件に変動が生じても確実に所定の動作温
度に保持でき、しかも、従来のように感熱素子等の温度
検出素子を設けるものではないので冒頭に述べたような
熱的結合の問題がない。
For example, as shown in FIG. 8, a pulse converter 8 may be provided to operate the heating element 1 with a pulsed current. Incidentally, FIG. 8 shows a case where integrating circuits 6a and 6b are used as the signal regulation circuit 6. As described above, the temperature control device according to the present invention can reliably maintain a predetermined operating temperature even if there are variations in heat dissipation conditions due to the surrounding conditions of the heating element, and moreover, the temperature control device according to the present invention can reliably maintain a predetermined operating temperature. Since no temperature detection element is provided, there is no problem of thermal coupling as mentioned at the beginning.

またブリツジ回路を構成する場合における電力の損失の
問題も生じないという利点がある。また、本発明による
温度制御装置を用いた本発明による記録ペンによれば、
この記録ペン自体に温度検出素子を付設することがない
ので、これによる機械的負荷の増大を招来することがな
くその走査の応答速度を早めることができる。
Another advantage is that there is no problem of power loss when configuring a bridge circuit. Further, according to the recording pen according to the present invention using the temperature control device according to the present invention,
Since no temperature detection element is attached to the recording pen itself, the scanning response speed can be increased without causing an increase in mechanical load.

しかも温度制御装置の付設によつて、外囲条件の変動に
よつても一定の温度での記録ができ、むらのない記録が
可能となる。また、動作の開始において、従来の温度制
御装置を付設しない記録ペンのように、この記録ペンが
記録可能な温度に加熱するまでの立ち上り時間が長くな
ることがなく、温度制御装置の動作によつてその立ち上
り時間が短縮化され、直ちに明瞭な記録を開始できると
いう利点がある。
Moreover, by adding a temperature control device, recording can be performed at a constant temperature even when the surrounding conditions change, and even recording can be performed. In addition, at the start of operation, unlike conventional recording pens that do not have a temperature control device, there is no longer a long startup time until the recording pen heats up to a recordable temperature, and the temperature control device operates. This has the advantage that the rise time is shortened and clear recording can be started immediately.

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

第1図は本発明の基本的思想の説明に供する等価回路、
第2図、第4図は夫々本発明の例のプロツク図、第3図
、第5図は夫々その等価回路図、第6図は本発明の具体
的回路例を示す回路図、第7図は本発明の例と従来例と
の外囲条件の変化による抵抗値変化を示す測定図、第8
図は本発明の他の例のプロツク図である。 1は発熱体、2は記録ペン、3は動作温度設定電気信号
供給手段、4は発熱体への電流供給手段、5は放熱条件
依存電気信号検出手段、6は信号規制回路、7は合成回
路である。
FIG. 1 shows an equivalent circuit for explaining the basic idea of the present invention.
FIGS. 2 and 4 are block diagrams of examples of the present invention, FIGS. 3 and 5 are equivalent circuit diagrams thereof, FIG. 6 is a circuit diagram showing a specific circuit example of the present invention, and FIG. 7 is a block diagram of an example of the present invention. 8 is a measurement diagram showing the change in resistance value due to changes in the surrounding conditions between the example of the present invention and the conventional example.
The figure is a block diagram of another example of the present invention. 1 is a heating element, 2 is a recording pen, 3 is an operating temperature setting electric signal supply means, 4 is a current supply means to the heating element, 5 is a heat dissipation condition dependent electric signal detection means, 6 is a signal regulation circuit, and 7 is a synthesis circuit. It is.

Claims (1)

【特許請求の範囲】 1 発熱体自体に直接通電する電流を制御して上記発熱
体を所望の動作温度に制御するようにした温度制御装置
において、上記発熱体を所定の放熱条件において所望の
動作温度に設定する動作温度設定電気信号を得る動作温
度設定電気信号供給手段と、該手段よりの動作温度設定
電気信号によつて出力電流が制御され該出力電流を上記
発熱体に供給する電流供給手段と、上記発熱体の温度係
数に依存して上記所定の放熱条件からの放熱条件の変動
に伴う上記発熱体の通電電流に基づく信号の変動を検出
し放熱条件依存電気信号を出力する放熱条件依存電気信
号検出手段と、該検出手段より得られる信号を所定の大
きさに規制し上記発熱体の通電電流方向に対して正帰還
の方向に帰するように上記電流供給手段に印加して上記
発熱体側から見た回路中に形成される負性抵抗成分の値
を上記発熱体の抵抗値に近接させた動作点を有せしめる
正帰還手段とを具備することを特徴とする温度制御装置
。 2 感熱記録紙に対し相対的に移動するようになされた
記録ペンに発熱体が組み込まれて成り、上記発熱体を所
定の放熱条件において所望の動作温度に設定する動作温
度設定電気信号を得る動作温度設定電気信号供給手段と
、該手段よりの動作温度設定電気信号によつて出力電流
が制御され該出力電流を上記発熱体に供給する電流供給
手段と、上記発熱体の温度係数に依存して上記所定の放
熱条件からの放熱条件の変動に伴う上記発熱体の通電電
流に基ずく信号の変動を検出し放熱条件依存電気信号を
出力する放熱条件依存電気信号検出手段と、該検出手段
より得られる信号を所定の大きさに規制し上記発熱体の
通電電流方向に対して正帰還の方向に帰するように上記
電流供給手段に印加して上記発熱体側から見た回路中に
形成される負性抵抗成分の値を上記発熱体の抵抗値に近
接させた動作点を有せしめる正帰還手段とを具備する温
度制御装置が連結された記録ペン。
[Scope of Claims] 1. A temperature control device that controls the current flowing directly through the heating element itself to control the heating element to a desired operating temperature, which controls the heating element to operate at a desired temperature under predetermined heat dissipation conditions. an operating temperature setting electrical signal supplying means for obtaining an operating temperature setting electrical signal to set the temperature; and a current supplying means whose output current is controlled by the operating temperature setting electrical signal from the means and supplies the output current to the heating element. and a heat dissipation condition dependent device that detects fluctuations in a signal based on the energizing current of the heat generating body depending on the temperature coefficient of the heat dissipation condition from the predetermined heat dissipation condition and outputs a heat dissipation condition dependent electrical signal. electric signal detecting means; and regulating the signal obtained from the detecting means to a predetermined magnitude and applying it to the current supply means so as to return the signal in the direction of positive feedback with respect to the direction of current flowing through the heating element, thereby generating the heat. 1. A temperature control device comprising: positive feedback means for making the value of a negative resistance component formed in the circuit viewed from the body side close to the resistance value of the heating element. 2. A heating element is incorporated in a recording pen that is movable relative to thermal recording paper, and an operation of obtaining an operating temperature setting electrical signal for setting the heating element to a desired operating temperature under predetermined heat dissipation conditions. temperature setting electric signal supply means; current supply means whose output current is controlled by the operating temperature setting electric signal from the means and supplies the output current to the heating element; heat dissipation condition dependent electric signal detection means for detecting a change in a signal based on the current flowing through the heating element as the heat dissipation condition changes from the predetermined heat dissipation condition and outputting a heat dissipation condition dependent electric signal; A negative signal formed in the circuit as seen from the heating element side is applied to the current supply means so as to regulate the signal to a predetermined magnitude and return the signal in the direction of positive feedback with respect to the direction of current flowing through the heating element. A recording pen connected to a temperature control device including positive feedback means for having an operating point where the value of the resistance component approaches the resistance value of the heating element.
JP11824378A 1978-09-26 1978-09-26 Temperature control device and recording pen using it Expired JPS5922966B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP11824378A JPS5922966B2 (en) 1978-09-26 1978-09-26 Temperature control device and recording pen using it

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP11824378A JPS5922966B2 (en) 1978-09-26 1978-09-26 Temperature control device and recording pen using it

Publications (2)

Publication Number Publication Date
JPS5544653A JPS5544653A (en) 1980-03-29
JPS5922966B2 true JPS5922966B2 (en) 1984-05-30

Family

ID=14731772

Family Applications (1)

Application Number Title Priority Date Filing Date
JP11824378A Expired JPS5922966B2 (en) 1978-09-26 1978-09-26 Temperature control device and recording pen using it

Country Status (1)

Country Link
JP (1) JPS5922966B2 (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5999163U (en) * 1982-12-23 1984-07-04 スズキ株式会社 EGR device for supercharged internal combustion engine

Families Citing this family (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS586709U (en) * 1981-07-01 1983-01-17 石垣機工株式会社 filter press
IT1212548B (en) * 1982-08-18 1989-11-30 Santoro Giovanni E Francolini LIGHTWEIGHT WELDER, ESPECIALLY SUITABLE FOR SILVER TIN WELDING AND SIMILAR
AU711690B2 (en) * 1995-03-24 1999-10-21 Peter Marcus Harley Filter press apparatus

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5999163U (en) * 1982-12-23 1984-07-04 スズキ株式会社 EGR device for supercharged internal combustion engine

Also Published As

Publication number Publication date
JPS5544653A (en) 1980-03-29

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