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JPS6326855B2 - - Google Patents
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JPS6326855B2 - - Google Patents

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Publication number
JPS6326855B2
JPS6326855B2 JP54090760A JP9076079A JPS6326855B2 JP S6326855 B2 JPS6326855 B2 JP S6326855B2 JP 54090760 A JP54090760 A JP 54090760A JP 9076079 A JP9076079 A JP 9076079A JP S6326855 B2 JPS6326855 B2 JP S6326855B2
Authority
JP
Japan
Prior art keywords
ice
semiconductor element
radiator
contact
junction
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
JP54090760A
Other languages
Japanese (ja)
Other versions
JPS5614172A (en
Inventor
Takeshi Aoki
Shigeru Yoneda
Takashi Ando
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.)
Sanyo Electric Co Ltd
Original Assignee
Sanyo 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 Sanyo Electric Co Ltd filed Critical Sanyo Electric Co Ltd
Priority to JP9076079A priority Critical patent/JPS5614172A/en
Publication of JPS5614172A publication Critical patent/JPS5614172A/en
Publication of JPS6326855B2 publication Critical patent/JPS6326855B2/ja
Granted legal-status Critical Current

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  • Measurement Of Length, Angles, Or The Like Using Electric Or Magnetic Means (AREA)
  • Investigating Or Analyzing Materials Using Thermal Means (AREA)
  • Investigating Or Analyzing Materials By The Use Of Electric Means (AREA)
  • Geophysics And Detection Of Objects (AREA)

Description

【発明の詳細な説明】 本発明は、物体に接触することに依つて熱容量
が変化し、その変化を検出することに依つて物体
の有無を検出する物体検出素子に関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an object detection element whose heat capacity changes upon contact with an object, and which detects the presence or absence of an object by detecting the change.

一般に物体の有無を検出する必要がある場合、
例えば製氷機等に於いて貯氷室の氷を一定量に保
つ場合、氷があるベルにあるか否かを光電素子あ
るいは機械的手段に依つて検出するが、光電素子
を用いた場合には霜等が付着して誤動作を行なう
ことがあり、また機械的手段はサーモスタツトあ
るいはリードスイツチ等の機械的接点を用いたも
のであり、低温度で氷と直接接触する部分の機械
的強度に特別の注意をしなければならないし、ま
た接点が湿気や霜に依り凍りつくことがある。
Generally when you need to detect the presence or absence of an object,
For example, when maintaining a constant amount of ice in the ice storage compartment of an ice maker, etc., the presence of ice in the bell is detected using a photoelectric element or mechanical means. Otherwise, mechanical means such as thermostats or reed switches are used, and the mechanical strength of the parts that come into direct contact with ice at low temperatures must be specially improved. Care must be taken, and the contacts may freeze due to moisture or frost.

本発明は上述した点に鑑みて為されたものであ
り、従来の検出素子とは全く異なる新規な物体検
出装置を提供するものである。以下図面を参照し
て本発明を詳細に説明する。
The present invention has been made in view of the above points, and provides a novel object detection device that is completely different from conventional detection elements. The present invention will be described in detail below with reference to the drawings.

第1図は本発明の実施例を示す断面図であり、
1は放熱器、2は半導体素子、3はリード線、4
は封止部である。
FIG. 1 is a sectional view showing an embodiment of the present invention,
1 is a heat sink, 2 is a semiconductor element, 3 is a lead wire, 4
is the sealing part.

前記放熱器1は熱良導性の金属、例えばアルミ
ニウムから成るパイプで一端が閉じている。放熱
器1の内部には半導体素子2が放熱器1と熱的に
結合して固着され、半導体素子2のリード線3は
放熱器1の他端の開口した部分から外部に導出さ
れ、更に放熱器1の開口した部分及びリード線3
は封止部4に依つてハーメチツクシールされる。
ハーメチツクシールする際に内部に水分が残こる
のを防ぐために窒素等を封入しても良い。また半
導体素子2はPNP型あるいはNPN型のトランジ
スタを用い、コレクタ電流を流した時にPNジヤ
ンクシヨンに発生する熱が放熱器1に伝わるもの
である。この様に形成された物体検出素子は例え
ば製氷機の貯氷室の任意位置に設置され、氷が一
定レベルに達すると第1図の破線で示される様に
氷5が放熱器1の一部に接触する。
The heat sink 1 is a pipe made of a metal with good thermal conductivity, such as aluminum, and is closed at one end. A semiconductor element 2 is thermally coupled and fixed to the heat sink 1 inside the heat sink 1, and the lead wire 3 of the semiconductor element 2 is led out from the open part at the other end of the heat sink 1, and further heat radiation is carried out. Open part of container 1 and lead wire 3
is hermetically sealed by the sealing portion 4.
Nitrogen or the like may be filled in to prevent moisture from remaining inside during hermetic sealing. Further, the semiconductor element 2 uses a PNP type or NPN type transistor, and heat generated in the PN junction is transmitted to the heat sink 1 when a collector current is passed. The object detection element formed in this way is installed at an arbitrary position in the ice storage compartment of an ice maker, for example, and when the ice reaches a certain level, the ice 5 becomes a part of the radiator 1 as shown by the broken line in FIG. Contact.

次に物体の有無の検出原理を説明する。第2図
は第1図に示された物体検出素子の熱的な等価回
路であり、6は半導体素子2のジヤンクシヨンを
示す熱源であり、R1はジヤンクシヨンと半導体
素子2全体の熱抵抗、C1は半導体素子2全体の
熱容量、R2は半導体素子2と放熱器1との間の
熱抵抗、Cnは放熱器1及び放熱器1と接触する
空気及び物体検出素子を支持するものの熱容量成
分、Rnは放熱器1及び放熱器1と接触する空気
及び物体検出素子を支持するものの熱抵抗成分を
示すものであり、物体検出素子の等価回路は熱源
6と熱抵抗R1,R2,Rnが直列接続され、熱容量
C1,Cnが並列に接続された回路となり、熱抵抗
R1,R2,Rnと熱容量C1,Cnに依つてそれぞれ熱
的な時定数が形成される。第1図の破線で示され
る如く氷5が物体検出素子の放熱器1に接触する
と、その接触する部分は氷5を溶すために熱が吸
収され、その部分の温度は0℃に固定される。こ
れを等価回路で示すと熱抵抗R1,R2,Rnと熱容
量C1,Cnで形成される時定数の回路の途中に熱
ツエナー7を挿入した回路となり、熱ツエナー7
により熱的にシヨートされ、それより先に熱が伝
わらなくなる。従つて放熱器1に氷5が接触して
いるときと、いないときでは物体検出素子全体と
しての熱的な時定数が異なり、半導体素子2のジ
ヤンクシヨンの温度上昇率及び飽和状態になるま
での時間及び温度が異なる。
Next, the principle of detecting the presence or absence of an object will be explained. FIG. 2 is a thermal equivalent circuit of the object detection element shown in FIG. 1, where 6 is a heat source indicating the juncture of the semiconductor element 2, R 1 is the thermal resistance of the juncture and the entire semiconductor element 2, and C 1 is the heat capacity of the entire semiconductor element 2, R2 is the thermal resistance between the semiconductor element 2 and the radiator 1, Cn is the heat capacity component of the radiator 1, the air in contact with the radiator 1, and the material that supports the object detection element, Rn indicates the thermal resistance component of the radiator 1, the air in contact with the radiator 1, and the material that supports the object detection element, and the equivalent circuit of the object detection element is the heat source 6 and the thermal resistance R 1 , R 2 , Rn. connected in series, heat capacity
C 1 and Cn are connected in parallel, resulting in a thermal resistance
A thermal time constant is formed depending on R 1 , R 2 , Rn and heat capacity C 1 , Cn. When the ice 5 comes into contact with the radiator 1 of the object detection element as shown by the broken line in FIG. 1, the contact area absorbs heat to melt the ice 5, and the temperature of that area is fixed at 0°C. Ru. If this is shown as an equivalent circuit, it becomes a circuit in which the thermal zener 7 is inserted in the middle of the time constant circuit formed by the thermal resistances R 1 , R 2 , Rn and the thermal capacities C 1 , Cn.
It is thermally shot, and the heat is no longer transmitted beyond that point. Therefore, the thermal time constant of the object detection element as a whole is different when the ice 5 is in contact with the heat sink 1 and when it is not, and the temperature increase rate of the juncture of the semiconductor element 2 and the time until it reaches the saturation state are different. and different temperatures.

第3図は半導体素子2のジヤンクシヨンの温度
と時間の関係を示す。aで示される曲線は氷5が
放熱器1に接触していない場合、bで示される曲
線は氷5が放熱器1に接触している場合を示す。
半導体素子2に電流を流し始めてからT0の間は
半導体素子2全体の熱抵抗R1及び熱容量C1とで
決定される時定数に依つてジヤンクシヨンの温度
がa,b共に同じ様に上昇するが、それ以後は、
氷5が放熱器1に接触していない場合には全ての
熱抵抗R1,R2,Rnと熱容量C1,Cnに依つて決定
される時定数に依つて、aに示される如く上昇す
る。一方氷5が放熱器1に接触していると熱ツエ
ナー7に依つて全体としての時定数が大幅に小さ
くなるために、ジヤンクシヨンの温度が飽和状態
に達する時間が短かくなり、またその温度も低く
なるためbで示される曲線となる。従つてT0
びT1に於けるジヤンクシヨンの温度を測定し、
その差があるレベル以上であればaで示される曲
線即ち氷5が無いと判断でき、あるレベル以下で
あればbで示される曲線即ち氷5が有ると判断で
きるのであるが、ジヤンクシヨンの温度を直接測
定することは不可能であるので半導体素子2から
出力される電気信号を用いる。
FIG. 3 shows the relationship between temperature and time for the juncture of the semiconductor element 2. The curve shown by a shows the case where the ice 5 is not in contact with the radiator 1, and the curve shown by b shows the case where the ice 5 is in contact with the radiator 1.
During T 0 after the current starts flowing through the semiconductor element 2, the junction temperatures a and b rise in the same way depending on the time constant determined by the thermal resistance R 1 and heat capacity C 1 of the entire semiconductor element 2. But after that,
When the ice 5 is not in contact with the heat sink 1, all the thermal resistances R 1 , R 2 , Rn and the time constant determined by the heat capacities C 1 , Cn rise as shown in a. . On the other hand, when the ice 5 is in contact with the radiator 1, the overall time constant becomes significantly smaller due to the thermal zener 7, so the time for the juncture temperature to reach the saturated state is shortened, and the temperature also increases. Since it becomes lower, it becomes a curve indicated by b. Therefore, measure the temperature of the junction at T 0 and T 1 ,
If the difference is above a certain level, it can be determined that the curve shown by a, that is, there is no ice 5, and if it is below a certain level, it can be determined that the curve shown by b, that is, ice 5 is present. Since direct measurement is impossible, the electrical signal output from the semiconductor element 2 is used.

第4図は半導体素子2にNPN型トランジスタ
Trを用いた場合の回路図であり、トランジスタ
Trのコレクタには負荷抵抗R0が電源電圧Vccと
の間に接続され、またベース−コレクタ間及びベ
ース−エミツタ間には分割抵抗RB1及びRB2
各々接続されている。今電源電圧Vccを印加する
と、分割抵抗RB1及びRB2に依つて決定されるコ
レクタ電流Icが負荷抵抗R0を介して流れ、コレ
クタ電圧即ち出力電圧outにはVcc―IcR0の電圧
が生じる。コレクタ電流Icが温度依存性を有する
ことは周知の如くであり、従つてコレクタ電流Ic
に依つて発生するジヤンクシヨンの熱に依り、温
度が上昇するとコレクタ電流Icは増し、コレクタ
電圧即ち出力電圧outは低くなる。第5図に出力
電圧outと時間の関係を示す。時間T0まではジヤ
ンクシヨンの温度は氷5が放熱器1に接触してい
るか否かにかかわらず同様に上昇するので、出力
電圧outも同様に小さくなる。その後は、氷5が
放熱器1に接触してない場合は第3図aで示され
る如くジヤンクシヨン温度が上昇するため出力電
圧outは第5図cで示される如く減少して行く。
一方氷5が放熱器1に接触している場合には第3
図bに示される如くジヤンクシヨン温度が短かい
間に一定となるため、出力電圧outは第5図dで
示される如く、短時間に一定電圧となるのであ
る。従つて時間T0及びT1に於ける出力電圧を測
定し、その差が一定レベル以上であれば氷5が無
いと判断でき一定レベル以下であれば氷5が有る
と判断できるのである。
Figure 4 shows an NPN transistor in semiconductor element 2.
This is a circuit diagram when using a transistor.
A load resistor R 0 is connected to the collector of the Tr between it and the power supply voltage Vcc, and dividing resistors R B1 and R B2 are connected between the base and the collector and between the base and the emitter, respectively. When the power supply voltage Vcc is applied now, the collector current Ic determined by the dividing resistors R B1 and R B2 flows through the load resistor R 0 , and a voltage of Vcc - IcR 0 is generated at the collector voltage, that is, the output voltage out. . It is well known that the collector current Ic has temperature dependence, and therefore the collector current Ic
When the temperature rises due to the heat generated by the juncture, the collector current Ic increases, and the collector voltage, that is, the output voltage out, decreases. FIG. 5 shows the relationship between output voltage out and time. Until time T 0 , the temperature of the junction rises in the same way regardless of whether the ice 5 is in contact with the heat sink 1 or not, so the output voltage out also becomes small. Thereafter, if the ice 5 is not in contact with the radiator 1, the juncture temperature increases as shown in FIG. 3a, so the output voltage out decreases as shown in FIG. 5c.
On the other hand, if the ice 5 is in contact with the radiator 1, the third
Since the junction temperature becomes constant for a short period of time as shown in FIG. 5B, the output voltage out becomes a constant voltage for a short period of time as shown in FIG. 5D. Therefore, the output voltages at times T 0 and T 1 are measured, and if the difference between them is above a certain level, it can be determined that there is no ice 5, and if the difference is below a certain level, it can be determined that there is ice 5.

尚出力電圧の測定及び氷の有無の判断をマイク
ロコンピユータで行えばより一層確実な判断がで
きる。
If the measurement of the output voltage and the determination of the presence or absence of ice are performed using a microcomputer, a more reliable determination can be made.

本実施例に於いて物体検出素子を氷の検出を例
に説明したが、放熱器に接触する物体が大きな熱
容量を有し、熱ツエナー効果を与えるものであれ
ば氷に限らず何でも検出可能となる。
In this embodiment, the object detection element was explained using the detection of ice as an example, but it is possible to detect anything other than ice as long as the object that comes into contact with the radiator has a large heat capacity and gives a thermal Zener effect. Become.

上述の如く本発明に依れば、熱良導性の放熱器
に半導体素子を熱的に結合して固着し、その検出
素子全体としての熱的な時定数が、物体が接触し
た場合に減少することを利用し、物体の有無を検
出するものであり、物体検出素子に可動部分が無
いため構造が簡単となり、機械的強度が増すもの
で、更に電気的信号に依り検出するため誤動作が
無く確実な検出が行なえるものである。特に、本
発明では、放熱器として一端が閉じられ他端に開
口部を有するパイプ状のものを用い、内部に半導
体素子を固着し、半導体素子のリード線を導出し
た状態で開口部を封止するようにしたので、小型
で耐久性の優れた検出素子を実現でき、氷と直接
接触する製氷機等に於ける氷の検出に好適とな
る。
As described above, according to the present invention, a semiconductor element is thermally bonded and fixed to a heat sink with good thermal conductivity, and the thermal time constant of the detection element as a whole decreases when an object comes into contact with it. The object detection element has no moving parts, which simplifies the structure and increases mechanical strength.Furthermore, since it relies on electrical signals for detection, there is no possibility of malfunction. This allows reliable detection. In particular, in the present invention, a pipe-shaped heatsink with one end closed and an opening at the other end is used, a semiconductor element is fixed inside, and the opening is sealed with the lead wire of the semiconductor element led out. As a result, it is possible to realize a small-sized and highly durable detection element, which is suitable for detecting ice in ice making machines and the like that come into direct contact with ice.

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

第1図は本発明の実施例を示す断面図、第2図
は第1図に示した実施例の熱的等価回路、第3図
はジヤンクシヨン温度特性図、第4図は第1図に
示した実施例に用いられる回路図、第5図は出力
電圧特性図である。 1……放熱器、2……半導体素子、3……リー
ド線、4……封止部、5……氷、6……熱源、7
……熱ツエナーである。
FIG. 1 is a sectional view showing an embodiment of the present invention, FIG. 2 is a thermal equivalent circuit of the embodiment shown in FIG. 1, FIG. 3 is a junction temperature characteristic diagram, and FIG. 4 is a diagram shown in FIG. The circuit diagram used in the embodiment shown in FIG. 5 is an output voltage characteristic diagram. DESCRIPTION OF SYMBOLS 1... Heat sink, 2... Semiconductor element, 3... Lead wire, 4... Sealing part, 5... Ice, 6... Heat source, 7
...It's a hot zener.

Claims (1)

【特許請求の範囲】[Claims] 1 PN接合部を有する半導体素子と、一端が閉
じられ他端に開口部を有するパイプ状であつて、
前記半導体素子が熱的結合するよう内部に固着さ
れ、前記半導体素子のリード線を前記開口部より
外部へ導出した状態で該開口部が封止され、前記
リード線を通して前記半導体素子に電流を流すこ
とにより前記PN接合部に生ずる熱を放熱させる
ための放熱器とを備え、前記半導体素子に電流を
流したときの前記PN接合部の温度上昇が前記放
熱器に物体が接触しているか否かで異なることに
依つて物体の有無を検出することを特徴とする物
体検出素子。
1 A semiconductor element having a PN junction, and a pipe-shaped device having one end closed and an opening at the other end,
The semiconductor element is fixed inside so as to be thermally coupled, the opening is sealed with the lead wire of the semiconductor element led out from the opening, and a current is passed through the lead wire to the semiconductor element. and a radiator for dissipating heat generated in the PN junction, and whether or not a temperature rise in the PN junction when a current is passed through the semiconductor element is caused by whether an object is in contact with the radiator. 1. An object detection element that detects the presence or absence of an object based on a difference in .
JP9076079A 1979-07-16 1979-07-16 Body detecting element Granted JPS5614172A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP9076079A JPS5614172A (en) 1979-07-16 1979-07-16 Body detecting element

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP9076079A JPS5614172A (en) 1979-07-16 1979-07-16 Body detecting element

Publications (2)

Publication Number Publication Date
JPS5614172A JPS5614172A (en) 1981-02-10
JPS6326855B2 true JPS6326855B2 (en) 1988-05-31

Family

ID=14007555

Family Applications (1)

Application Number Title Priority Date Filing Date
JP9076079A Granted JPS5614172A (en) 1979-07-16 1979-07-16 Body detecting element

Country Status (1)

Country Link
JP (1) JPS5614172A (en)

Family Cites Families (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS50941A (en) * 1973-05-08 1975-01-08
JPS5093694A (en) * 1973-12-21 1975-07-25
JPS5612568A (en) * 1979-07-11 1981-02-06 Sanyo Electric Co Ltd Body detecting device

Also Published As

Publication number Publication date
JPS5614172A (en) 1981-02-10

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