JPH0430585A - thermoelectric device - Google Patents
thermoelectric deviceInfo
- Publication number
- JPH0430585A JPH0430585A JP2137832A JP13783290A JPH0430585A JP H0430585 A JPH0430585 A JP H0430585A JP 2137832 A JP2137832 A JP 2137832A JP 13783290 A JP13783290 A JP 13783290A JP H0430585 A JPH0430585 A JP H0430585A
- Authority
- JP
- Japan
- Prior art keywords
- conductor
- type semiconductor
- heat
- thermoelectric device
- semiconductor
- 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.)
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- Cooling Or The Like Of Semiconductors Or Solid State Devices (AREA)
Abstract
(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。(57) [Summary] This bulletin contains application data before electronic filing, so abstract data is not recorded.
Description
【発明の詳細な説明】
産業上の利用分野
本発明はベルチェ効果を利用し 電気的に冷房もしくは
暖房を行う空調装置 もしくはゼーベック効果により温
度差を用いて発電を行う発電装置に有用な熱電装置に関
する。DETAILED DESCRIPTION OF THE INVENTION Field of Industrial Application The present invention relates to a thermoelectric device useful for air conditioners that electrically cool or heat air using the Beltier effect, or power generation devices that generate electricity using temperature differences due to the Seebeck effect. .
従来の技術
従来 熱を電気に変換し もしくは電気を熱に変換する
熱電装置!よ 第3図に示す従来例の様に熱電素子1の
両側にコルゲートフィン2を有じ両側のコルゲートフィ
ンの温度差により発電を行しく もしくは電流を通ずる
ことにより冷却を行うものであ4 以下の説明について
はベルチェ効果による冷却について行なう。Conventional technologyConventional Thermoelectric device that converts heat into electricity or converts electricity into heat! As in the conventional example shown in Fig. 3, a thermoelectric element 1 has corrugated fins 2 on both sides, and electricity is generated by the temperature difference between the corrugated fins on both sides, or cooling is performed by passing an electric current. The explanation will be about cooling due to the Beltier effect.
熱電素子1の拡大断面を第4図に示す。絶縁性フィルム
基板3の片面にN型半導体4、導電体5、P型半導体6
、導電体5が順に成膜されてい42つのコルゲートフィ
ン2は 導電体5を1つおき&ミ か2 接する導電体
5がおのおの異なるように設置されてい4 N型半導体
4、導電体5、P型半導体6(上 各々の端部が電気的
の接触する構造になっており、熱電装置に流れ込んだ電
流は半導体4、6と導電体5の界面でペルチェ効果によ
り発熱もしくは吸熱すム このとき、N型半導体4とP
型半導体6は交互に並んでいることか板溝電体5は交互
に発熱部または吸熱部となり、前述のごとく導電体5の
1つおきに接するコルゲートフィン2は 一方が発熱フ
ィン他方が吸熱フィンとなる。したがって、フィルム基
板3上部の空気から熱を吸収(もしくは空気への熱の発
散)、フィルム基板3の下部の空気への熱の発散(もし
くは空気からの熱の吸収)となも
発明が解決しようとする課題
しかしなが収 このような従来の熱電装置でcヨ第5図
に示すごとくコルゲートフィンの熱伝達率が空気入口側
と出口側で大きく異なることかペフィン温度のバラツキ
が大きく有効な熱処理が行えず、熱電装置全体が大きく
なるという課題があつ九
本発明番え 上記問題点にもとづき、フィンの有効利
用を図り熱電装置の軽量([、コンパクト化を実現する
熱電装置を提供するものである。An enlarged cross section of the thermoelectric element 1 is shown in FIG. An N-type semiconductor 4, a conductor 5, and a P-type semiconductor 6 are disposed on one side of an insulating film substrate 3.
, conductors 5 are deposited in order, and the 42 corrugated fins 2 are arranged so that the conductors 5 in contact are different from each other. type semiconductor 6 (upper) Each end is in electrical contact with each other, and the current flowing into the thermoelectric device generates heat or absorbs heat at the interface between the semiconductors 4, 6 and the conductor 5 due to the Peltier effect.At this time, N-type semiconductor 4 and P
The type semiconductors 6 are arranged alternately, and the plate groove electric bodies 5 alternately act as heat generating parts or heat absorbing parts, and as mentioned above, the corrugated fins 2 that touch every other conductor 5 have a heat generating fin on one side and a heat absorbing fin on the other side. becomes. Therefore, the invention can solve the problems of absorbing heat from the air above the film substrate 3 (or dissipating heat to the air) and dissipating heat to the air below the film substrate 3 (or absorbing heat from the air). However, the problem with conventional thermoelectric devices is that the heat transfer coefficient of the corrugated fins differs greatly between the air inlet and outlet sides, as shown in Figure 5, and the variation in the fin temperature is large, making it difficult to carry out effective heat treatment. Based on the above-mentioned problems, the present invention provides a thermoelectric device that makes effective use of the fins and makes the thermoelectric device lighter and more compact. be.
課題を解決するための手段
そこで本発明による熱電装置は 絶縁性上フイルム基板
の面方向1’= N型半導恢 導電体1、P型半導恢
導電体2の顆間 各半導体・導電体の端部が電気的に
接触するように設置し かつ前記導電体lと熱的に接触
する熱交換手段を前記基板の片側に 前記導電体2と熱
的に接触する熱交換手段を前記基板の反対側に設置する
熱電装置において、前記熱交換手段の局所熱伝達率の大
きい部分と接触する導電体1または2に隣接するN型半
導体およびP型半導体の膜厚を部分的に厚くす黴または
前記熱交換手段の局所熱伝達率の大きい部分と接触す
る導電体lまたは2に隣接するN型半導体およびP型半
導体の長さを部分的に短くすることにより、上記のよう
な問題点を解決するための手段となしたものであ4
作用
上記のような構成もしくは手段によって、得られる作用
は次の通りであ4
以下、冷却特性を例にとて説明すも 半導体の冷却能力
Q c 11 半導体の物性であるセーベツク係数S
、比抵抗ρ、熱伝導率λを用いて、で表される。ここで
、記号i!T; 冷却側温度、■: 電LL; 半導
体良木A; 半導体断面積(膜厚X幅)、△T; 半導
体の両端の温度差である。Means for Solving the Problems Therefore, the thermoelectric device according to the present invention has the following features: Planar direction 1' of insulating upper film substrate = N-type semiconductor conductor 1, P-type semiconductor conductor 2 Between the condyles of each semiconductor/conductor A heat exchange means is installed on one side of the substrate so that the ends thereof are in electrical contact with the conductor 1, and the heat exchange means is placed in thermal contact with the conductor 2 on one side of the substrate. In the thermoelectric device installed on the opposite side, mold or mildew that partially thickens the film thickness of the N-type semiconductor and P-type semiconductor adjacent to the conductor 1 or 2 that contacts the portion of the heat exchange means with a large local heat transfer coefficient. The above problems are solved by partially shortening the lengths of the N-type semiconductor and the P-type semiconductor adjacent to the conductor 1 or 2 that are in contact with the portion of the heat exchange means having a large local heat transfer coefficient. 4 Effects The effects obtained by the above configuration or means are as follows. 4 Below, we will explain the cooling characteristics using an example. Cooling capacity of semiconductor Q c 11 Savek coefficient S, which is a physical property of semiconductors
, specific resistance ρ, and thermal conductivity λ. Here, the symbol i! T: Cooling side temperature, ■: Electrical LL; Semiconductor wood A: Semiconductor cross-sectional area (film thickness x width), ΔT: Temperature difference between both ends of the semiconductor.
式から解るように 冷却能力は電流に関する2次関数と
なる。したがって、最高冷却能力を示す電流値(I q
)が存在する。式(1)を、電流に関して微分すること
によりIqが得られ さらに式(1)にIQを代入する
ことにより、最大冷却能力Qmaxζよ
1 82・T2 A
・・・(2)
で与えられも
したがって、半導体断面積(A)または長さ(L)を変
えることによりQmaxを変えることが可能となa こ
の作用を利用して、半導体の形状を空気の流れ方向で変
えることにより、部分的にQmaxを大きくすることが
できも つまり、コルゲートフィンの熱伝達率が大きい
空気入口部において、半導体の(A/L)を大きくし
処理熱量を増やすことにより、奥行きを小さくすること
が可能となa
本発明C友 上記課題にもとづき、軽量・コンパクト
な熱電装置を提供するものであも
実施例
以下本発明による実施例を図面により説明する。As can be seen from the equation, cooling capacity is a quadratic function of current. Therefore, the current value (I q
) exists. By differentiating equation (1) with respect to the current, Iq can be obtained.Furthermore, by substituting IQ into equation (1), the maximum cooling capacity Qmaxζ 1 82・T2 A
...(2) Therefore, it is possible to change Qmax by changing the cross-sectional area (A) or length (L) of the semiconductor.Using this effect, the shape of the semiconductor can be changed to By changing the flow direction, Qmax can be partially increased.In other words, the (A/L) of the semiconductor can be increased at the air inlet section where the heat transfer coefficient of the corrugated fin is high.
By increasing the amount of processing heat, it is possible to reduce the depth.A Friend of the present invention Based on the above-mentioned problems, a lightweight and compact thermoelectric device is provided. explain.
〈実施例1〉
第1図に本発明の一実施例の熱電装置の要部を示すもの
であ4 絶縁フィルム基板11にJ& N型半導体1
2、導電体13、P型半導体14、導電体13が順に成
膜されてい4N型半導体12、導電体13、P型半導体
14ζよ 各々の端部が重なり合う構造になっており、
接触部の電気抵抗および熱抵抗が大きくならない構造と
なっていも導電体13の材料としては 電気抵抗の小さ
い銅またはアルミが用いられも 本実施例でζよ 半導
体12、14の空気入口側に位置する部分の膜厚を大き
くしていも
冷却装置として使用する場合に(よ 絶縁性フィルム基
板11と平行に半導体12、14および導電体13に電
流を流す。これにより、半導体12.14と導電体13
の界面でペルチェ効果により発熱もしくは吸熱を生じも
このとき、N型半導体12とP型半導体14は交互に
並んでいることか収 導電体13は交互に発熱部または
吸熱部となり、従来例に示したごとく導電体13の1つ
おきに接する片側のコルゲートフィン(図には示さず)
Cヨ 吸熱(または発熱)とな4 −X 反対側に
設置されたコルゲートフィン&瓜 発熱(または吸熱)
となる。したがって、絶縁性フィルム基板11の上部の
空気から熱を吸収(もしくは空気への熱の発散)、下部
の空気への熱の発散(もしくは流体からの熱の吸収)と
な4 この隊 半導体12、14の空気入口側の膜厚を
大きくしていることか収 電流は膜厚の大きい部分に多
く流れ 冷却熱量も増加すム 前述のように空気入口側
の熱伝達率は大きいことか収 処理できる熱量も大きく
、冷却熱量が増加しても十分処理することが可能である
。したがって、熱電装置の奥行きを小さくすることが可
能となり、全体として軽量・コンパクトな熱電装置とな
も
発電装置として使用する場合には 双方のコルゲートフ
ィンに接する空気に温度差をつけも これにより、導電
体13は交互に高温と低温となり、ゼーベック効果によ
り起電力を生ずることができる。<Example 1> Fig. 1 shows the main parts of a thermoelectric device according to an example of the present invention.
2. The conductor 13, the P-type semiconductor 14, and the conductor 13 are formed in this order, and the ends of the 4N-type semiconductor 12, the conductor 13, and the P-type semiconductor 14ζ overlap each other,
Even if the structure is such that the electrical resistance and thermal resistance of the contact parts do not increase, copper or aluminum with low electrical resistance may be used as the material of the conductor 13. Even if the thickness of the film is increased in the area where the film is formed, when used as a cooling device, a current is passed through the semiconductors 12, 14 and the conductor 13 in parallel with the insulating film substrate 11. 13
At this time, the N-type semiconductor 12 and the P-type semiconductor 14 are arranged alternately. Corrugated fins on one side that touch every other conductor 13 (not shown)
C yo Endothermic (or heat-generating) 4 -X Corrugated fin & melon installed on the opposite side Heat-generating (or heat-absorbing)
becomes. Therefore, heat is absorbed from the air above the insulating film substrate 11 (or heat is dissipated to the air), and heat is dissipated to the air below (or heat is absorbed from the fluid). The reason for this is that the thickness of the film on the air inlet side of No. 14 is increased, and the current flows to the thicker part, and the amount of cooling heat increases.As mentioned above, the heat transfer coefficient on the air inlet side is large. The amount of heat is also large, and even if the amount of cooling heat increases, it is possible to perform sufficient processing. Therefore, it is possible to reduce the depth of the thermoelectric device, making it lightweight and compact as a whole.When used as a power generation device, it is possible to create a temperature difference between the air in contact with both corrugated fins. The body 13 becomes hot and cold alternately, and an electromotive force can be generated due to the Seebeck effect.
以上のように本発明においては 空気入口側の半導体の
膜厚を大きくすることにより、軽量・コンパクトな熱電
装置が提供されも
〈実施例2〉
第2図は第2の発明の一実施例であり、熱電素子の断面
を示すものであも
絶縁フィルム基板15に(友 N型半導体16、導電体
17、P型半導体18、導電体17が順に成膜されてい
も 本実施例は 半導体16、18の長さを空気の流れ
方向で変化させており、入口部で小さく、出口部で大き
くしていも 電流を流すと、半導体の長さが短い部分に
多く流れ 冷却熱量も増加すも 前述のように空気入口
側の熱伝達率は大きいことか収 処理できる熱量も大き
く、冷却熱量が増加しても十分処理することが可能であ
も したがって、熱電装置の奥行きを小さくすることが
可能となり、全体として軽量・コンパクトな熱電装置と
なも
その他の構成および使用法は 第1の発明と同様である
ので説明を省略すも
発明の効果
本発明による熱電装置は 熱交換手段の局所熱伝達率の
大きい部分と接触する第1または第2の導電体に隣接す
るN型半導体およびP型半導体の膜厚を部分的に厚くす
ゑ または 前記熱交換手段の局所熱伝達率の大きい部
分と接触する第1または第2の導電体に隣接するN型半
導体およびP型半導体の長さを部分的に短くすることに
より、軽量・コンパクトな熱電装置の実現が可能となる
。As described above, in the present invention, by increasing the thickness of the semiconductor on the air inlet side, a lightweight and compact thermoelectric device can be provided. This example shows a cross section of a thermoelectric element, even if an N-type semiconductor 16, a conductor 17, a P-type semiconductor 18, and a conductor 17 are formed in this order on an insulating film substrate 15. Even if the length of 18 is changed in the direction of air flow, making it smaller at the inlet and larger at the outlet, when current is applied, more current flows to the shorter part of the semiconductor, and the amount of cooling heat increases. Because the heat transfer coefficient on the air inlet side is high, the amount of heat that can be collected and processed is also large, and even if the amount of cooling heat increases, it can be sufficiently processed. Therefore, it is possible to reduce the depth of the thermoelectric device. The overall construction and usage of the thermoelectric device, which is lightweight and compact, is the same as that of the first invention, so the explanation will be omitted. Effects of the Invention The thermoelectric device according to the present invention has the following advantages: Partially thickening the film thickness of the N-type semiconductor and the P-type semiconductor adjacent to the first or second conductor that is in contact with a large portion; or Alternatively, by partially shortening the lengths of the N-type semiconductor and the P-type semiconductor adjacent to the second conductor, it is possible to realize a lightweight and compact thermoelectric device.
第1図は本発明の一実施例の熱電素子の拡大斜視医 第
2図は本発明の第2の実施例の熱電素子の拡大斜視医
第3図は従来例の熱電装置の断面阻 第4図は従来例の
熱電素子の断面医 第5図は空気側の熱伝達特性図であ
も
4、6.12.14.16.18・・半導& 3.1
1.15・・絶縁性フィルム基板、5.13.17・・
導電体・・コルゲートフィン。
代理人の氏名 弁理士 粟野重孝 はか1名第
図
第
図FIG. 1 shows an enlarged perspective view of a thermoelectric element according to an embodiment of the present invention. FIG. 2 shows an enlarged perspective view of a thermoelectric element according to a second embodiment of the present invention.
Fig. 3 shows a cross section of a conventional thermoelectric device; Fig. 4 shows a cross section of a conventional thermoelectric element; Fig. 5 shows a heat transfer characteristic diagram on the air side.・Semiconductor & 3.1
1.15... Insulating film substrate, 5.13.17...
Conductor: Corrugated fin. Name of agent: Patent attorney Shigetaka Awano
Claims (2)
第1の導電体、P型半導体、第2の導電体2の順に、各
半導体と導電体の端部が電気的に接触するように設置し
、かつ前記導電体1と熱的に接触する熱交換手段を第1
の基板の片側に、第2の導電体と熱的に接触する熱交換
手段を前記基板の反対側に設置する熱電装置において、
前記熱交換手段の局所熱伝達率の大きい部分と接触する
第1または第2の導電体に隣接するN型半導体およびP
型半導体の膜厚を部分的に厚くした熱電装置。(1) N-type semiconductor,
A first conductor, a P-type semiconductor, and a second conductor 2 are installed in this order so that the ends of each semiconductor and the conductor are in electrical contact with each other, and the heat generated by thermal contact with the conductor 1 is The means of exchange is the first
A thermoelectric device in which a heat exchange means in thermal contact with a second conductor is installed on one side of the substrate on the opposite side of the substrate,
an N-type semiconductor and a P semiconductor adjacent to the first or second conductor in contact with a portion of the heat exchange means having a large local heat transfer coefficient;
A thermoelectric device in which the film thickness of the type semiconductor is partially thickened.
第1の導電体、P型半導体、第2の導電体の順に、各半
導体・導電体の端部が電気的に接触するように設置し、
かつ前記第1の導電体と熱的に接触する熱交換手段を前
記基板の片側に、前記第2の導電体と熱的に接触する熱
交換手段を前記基板の反対側に設置する熱電装置におい
て、前記熱交換手段の局所熱伝達率の大きい部分と接触
する第1または第2の導電体に隣接するN型半導体およ
びP型半導体の長さを部分的に短くした熱電装置。(2) N-type semiconductor,
A first conductor, a P-type semiconductor, and a second conductor are installed in this order so that the ends of each semiconductor/conductor are in electrical contact with each other,
and a thermoelectric device in which a heat exchange means in thermal contact with the first conductor is installed on one side of the substrate, and a heat exchange means in thermal contact with the second conductor is installed on the opposite side of the substrate. . A thermoelectric device in which the lengths of the N-type semiconductor and the P-type semiconductor adjacent to the first or second conductor that are in contact with a portion of the heat exchange means having a large local heat transfer coefficient are partially shortened.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2137832A JPH0430585A (en) | 1990-05-28 | 1990-05-28 | thermoelectric device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2137832A JPH0430585A (en) | 1990-05-28 | 1990-05-28 | thermoelectric device |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH0430585A true JPH0430585A (en) | 1992-02-03 |
Family
ID=15207882
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP2137832A Pending JPH0430585A (en) | 1990-05-28 | 1990-05-28 | thermoelectric device |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0430585A (en) |
Cited By (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| WO2009022698A1 (en) * | 2007-08-13 | 2009-02-19 | National Institute Of Advanced Industrial Science And Technology | Process for producing fine thermoelectric element, the fine thermoelectric element, and product employing the fine thermoelectric element |
| JP2016184599A (en) * | 2015-03-25 | 2016-10-20 | 三菱マテリアル株式会社 | Nitride thermoelectric conversion material, method for producing the same, and thermoelectric conversion element |
| JP2016184600A (en) * | 2015-03-25 | 2016-10-20 | 三菱マテリアル株式会社 | Nitride thermoelectric conversion material, manufacturing method therefor and thermoelectric conversion element |
-
1990
- 1990-05-28 JP JP2137832A patent/JPH0430585A/en active Pending
Cited By (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| WO2009022698A1 (en) * | 2007-08-13 | 2009-02-19 | National Institute Of Advanced Industrial Science And Technology | Process for producing fine thermoelectric element, the fine thermoelectric element, and product employing the fine thermoelectric element |
| JP2009049050A (en) * | 2007-08-13 | 2009-03-05 | National Institute Of Advanced Industrial & Technology | Manufacturing method of fine thermoelectric element, fine thermoelectric element and product using the fine thermoelectric element |
| JP2016184599A (en) * | 2015-03-25 | 2016-10-20 | 三菱マテリアル株式会社 | Nitride thermoelectric conversion material, method for producing the same, and thermoelectric conversion element |
| JP2016184600A (en) * | 2015-03-25 | 2016-10-20 | 三菱マテリアル株式会社 | Nitride thermoelectric conversion material, manufacturing method therefor and thermoelectric conversion element |
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