JPS6259889B2 - - Google Patents
Info
- Publication number
- JPS6259889B2 JPS6259889B2 JP56208648A JP20864881A JPS6259889B2 JP S6259889 B2 JPS6259889 B2 JP S6259889B2 JP 56208648 A JP56208648 A JP 56208648A JP 20864881 A JP20864881 A JP 20864881A JP S6259889 B2 JPS6259889 B2 JP S6259889B2
- Authority
- JP
- Japan
- Prior art keywords
- flow path
- refrigerant liquid
- container
- heating element
- cooling device
- 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
Links
Classifications
-
- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F25—REFRIGERATION OR COOLING; COMBINED HEATING AND REFRIGERATION SYSTEMS; HEAT PUMP SYSTEMS; MANUFACTURE OR STORAGE OF ICE; LIQUEFACTION SOLIDIFICATION OF GASES
- F25B—REFRIGERATION MACHINES, PLANTS OR SYSTEMS; COMBINED HEATING AND REFRIGERATION SYSTEMS; HEAT PUMP SYSTEMS
- F25B23/00—Machines, plants or systems, with a single mode of operation not covered by groups F25B1/00 - F25B21/00, e.g. using selective radiation effect
- F25B23/006—Machines, plants or systems, with a single mode of operation not covered by groups F25B1/00 - F25B21/00, e.g. using selective radiation effect boiling cooling systems
-
- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F28—HEAT EXCHANGE IN GENERAL
- F28F—DETAILS OF HEAT-EXCHANGE AND HEAT-TRANSFER APPARATUS, OF GENERAL APPLICATION
- F28F13/00—Arrangements for modifying heat-transfer, e.g. increasing, decreasing
- F28F13/06—Arrangements for modifying heat-transfer, e.g. increasing, decreasing by affecting the pattern of flow of the heat-exchange media
-
- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10W—GENERIC PACKAGES, INTERCONNECTIONS, CONNECTORS OR OTHER CONSTRUCTIONAL DETAILS OF DEVICES COVERED BY CLASS H10
- H10W40/00—Arrangements for thermal protection or thermal control
- H10W40/70—Fillings or auxiliary members in containers or in encapsulations for thermal protection or control
- H10W40/73—Fillings or auxiliary members in containers or in encapsulations for thermal protection or control for cooling by change of state
Landscapes
- Engineering & Computer Science (AREA)
- Physics & Mathematics (AREA)
- Thermal Sciences (AREA)
- Mechanical Engineering (AREA)
- General Engineering & Computer Science (AREA)
- Cooling Or The Like Of Semiconductors Or Solid State Devices (AREA)
Description
【発明の詳細な説明】
この発明は、例えば電力用半導体素子などの発
熱体を沸騰熱伝達を応用して冷却する沸騰冷却装
置に関するものであり、目的とするところはその
冷却特性の改善することにある。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a boiling cooling device that cools a heating element, such as a power semiconductor element, by applying boiling heat transfer, and an object thereof is to improve the cooling characteristics thereof. It is in.
第1図は従来の沸騰冷却装置100を示す断面
図であり、1は半導体素子などの発熱体、2は冷
媒液、3は容器である。 FIG. 1 is a sectional view showing a conventional evaporative cooling device 100, in which 1 is a heating element such as a semiconductor element, 2 is a refrigerant liquid, and 3 is a container.
今、発熱体1が通電などによつて発熱すると、
発熱体1の冷媒液2に接する面(伝熱面)から気
泡4が発生する。発生した気泡すなわち蒸気は、
容器3内の気相空間5を実線の矢印に示すように
上昇し、冷却されている容器3の内壁面で凝縮液
化する。この時、凝縮潜熱として、発熱体1で発
生した熱を容器3外へ放散させる。凝縮液化した
冷媒液2Aは、容器内壁面に沿つて重力の作用で
降下し、冷媒液2中に還流する。この際、冷媒液
2は、上昇する気泡4によつてかく乱され、した
がつて、容器3の内壁面の冷媒液2に接する部分
にも、冷媒液2の対流熱伝達によつて、発熱体1
で発生した熱の一部が伝えられ、容器3の壁を介
して、容器外へ放散される。 Now, when the heating element 1 generates heat due to electricity, etc.
Bubbles 4 are generated from the surface of the heating element 1 that is in contact with the refrigerant liquid 2 (heat transfer surface). The bubbles or steam generated are
The gas rises through the gas phase space 5 in the container 3 as shown by the solid arrow, and is condensed and liquefied on the inner wall surface of the container 3, which is being cooled. At this time, the heat generated by the heating element 1 is radiated to the outside of the container 3 as latent heat of condensation. The condensed and liquefied refrigerant liquid 2A descends under the action of gravity along the inner wall surface of the container and flows back into the refrigerant liquid 2. At this time, the refrigerant liquid 2 is disturbed by the rising bubbles 4, and therefore, the portion of the inner wall surface of the container 3 that is in contact with the refrigerant liquid 2 also has a heating element due to convective heat transfer of the refrigerant liquid 2. 1
A part of the heat generated is transferred and radiated out of the container 3 through the wall of the container 3.
しかしながら、従来の沸騰冷却装置100で
は、上昇する気泡4による冷媒液2のかく乱が、
不確定であつたため、対流熱伝達率が極めて小さ
い。 However, in the conventional evaporative cooling device 100, the disturbance of the refrigerant liquid 2 by the rising bubbles 4
Since it was uncertain, the convective heat transfer coefficient was extremely small.
実際に、第1図に示すような構成の場合には、
気泡4によるかく乱は、気泡4が発生している発
熱体1の表面近くの冷媒液2中の付近に限られて
おり、その気泡のかく乱によつては容器3の下部
にまでは、気泡4のかく乱による対流が及んでい
ない事が認められる。したがつて、対流熱伝達に
よる熱の放散効果は極めて小さかつた。 In fact, in the case of the configuration shown in Figure 1,
The disturbance caused by the bubbles 4 is limited to the area in the refrigerant liquid 2 near the surface of the heating element 1 where the bubbles 4 are generated, and depending on the disturbance of the bubbles, the bubbles 4 may reach the lower part of the container 3. It is recognized that the convection caused by the disturbance has not reached the area. Therefore, the heat dissipation effect by convective heat transfer was extremely small.
この発明は、上昇する気泡4によつて誘発され
た冷媒液2の流れを積極的に利用することによ
り、冷却特性を改善した沸騰冷却装置を提供する
ことを目的とするものである。 An object of the present invention is to provide a boiling cooling device with improved cooling characteristics by actively utilizing the flow of the refrigerant liquid 2 induced by the rising bubbles 4.
第2図は先行技術(特願昭56−053466=特開昭
57−167663)である沸騰冷却装置を示す断面図で
ある。図において、1〜5は上記従来装置と全く
同様のものを示す。6は発熱体1の内部に形成さ
れた冷媒液2の流路で、この例では発熱体6より
下方に延長されている。7は冷媒液2の下向きの
流れが容器3の内壁面に沿つて流れるような流路
を形成する整流板である。発熱体1が発熱する
と、流路すなわちダクト6内に発生した気泡4の
上昇によつて、気泡4と冷媒液2間に粘性に基づ
く摩擦力が働き、流路6内の冷媒液2をかき上げ
るいわゆる気泡ポンプ作用が働く。また、発熱体
1からの発生熱が小さくて流路6内に気泡が発生
しない場合には、流路6内の冷媒液2が加熱され
て、密度が小さくなり浮力が生じる。したがつ
て、いずれにしても、発熱体1が発熱すると、流
路6内では、上昇流が生じる。この冷媒液2を上
昇させる駆動力は流路6内の気体(気泡4を示
す)と液体との平均密度と、流路6外の冷媒液2
の平均密度との差が大きい程、また流路6の鉛直
方向の高さが大きい程大きくなることが知られて
いる。 Figure 2 shows the prior art (Japanese Patent Application No. 56-053466 =
57-167663) is a sectional view showing a boiling cooling device. In the figure, numerals 1 to 5 indicate devices completely similar to the conventional device described above. Reference numeral 6 denotes a flow path for the refrigerant liquid 2 formed inside the heating element 1, which extends downward from the heating element 6 in this example. Reference numeral 7 denotes a rectifier plate that forms a flow path through which the refrigerant liquid 2 flows downward along the inner wall surface of the container 3. When the heating element 1 generates heat, the bubbles 4 generated in the flow path, that is, the duct 6 rise, and a frictional force based on viscosity acts between the bubbles 4 and the refrigerant liquid 2, which scrapes the refrigerant liquid 2 in the flow path 6. The so-called bubble pump effect works to raise the temperature. Furthermore, when the heat generated from the heating element 1 is small and no bubbles are generated within the flow path 6, the refrigerant liquid 2 within the flow path 6 is heated, its density is reduced, and buoyancy is generated. Therefore, in any case, when the heating element 1 generates heat, an upward flow occurs in the flow path 6. The driving force for raising the refrigerant liquid 2 is determined by the average density of the gas (indicated by bubbles 4) and liquid in the flow path 6 and the refrigerant liquid 2 outside the flow path 6.
It is known that the larger the difference from the average density, or the larger the height of the flow path 6 in the vertical direction, the larger the difference.
したがつて、第2図に示すように整流板7およ
び流路6を沸騰冷却装置100内に構成しておく
と、冷媒液2は実線の矢印に示すように循環する
ことになる。すなわち、発熱体1内の流路6で発
生した駆動力によつて、冷媒液2は、流路6の下
部より、流路6内に流入し、流路6の上部から流
出する。流出した冷媒液2は、容器3の内壁面と
整流板7間に形成された流路8を下向きに流れ
て、流路6の下部へ流入する。したがつて、発熱
体1内で誘発された冷媒液2は整然と流路8を流
れ、流路8内の冷媒液2と容器3の内壁面間の対
流熱伝達特性を上昇させることになる。 Therefore, if the baffle plate 7 and flow path 6 are configured in the boiling cooling device 100 as shown in FIG. 2, the refrigerant liquid 2 will circulate as shown by the solid arrows. That is, due to the driving force generated in the flow path 6 in the heating element 1, the refrigerant liquid 2 flows into the flow path 6 from the lower part of the flow path 6 and flows out from the upper part of the flow path 6. The outflowing refrigerant liquid 2 flows downward through a channel 8 formed between the inner wall surface of the container 3 and the baffle plate 7, and flows into the lower part of the channel 6. Therefore, the refrigerant liquid 2 induced in the heating element 1 flows through the flow path 8 in an orderly manner, increasing the convective heat transfer characteristics between the refrigerant liquid 2 in the flow path 8 and the inner wall surface of the container 3.
ところが、先行技術においては、第2図に示さ
れるように整流板7と容器3との間の流路の断面
積Sこの例では幅がほぼ均一であるため、第3図
の斜線部で示す容器3の底部9の冷媒液2が淀ん
でしまい、そのため、この部分9における放熱が
疎外されるという欠点があつた。実験によれば、
この部分の面積は全放熱面積の20%以上占めるこ
とが確認された。このような傾向は、第4図に示
すように、発熱体1の底部9が大きくなる程、換
言すれば発熱体1の下端と容器3の下端との距離
Hが大きくなる程、顕著となる。 However, in the prior art, as shown in FIG. 2, the cross-sectional area S of the flow path between the current plate 7 and the container 3 is almost uniform in this example, so The refrigerant liquid 2 at the bottom 9 of the container 3 stagnates, resulting in a drawback that heat dissipation in this portion 9 is hindered. According to experiments,
It was confirmed that this area accounts for more than 20% of the total heat dissipation area. As shown in FIG. 4, this tendency becomes more pronounced as the bottom portion 9 of the heating element 1 becomes larger, in other words, as the distance H between the lower end of the heating element 1 and the lower end of the container 3 becomes larger. .
この発明は上述した先行技術の欠点を改善する
ためになされたものである。 This invention has been made to improve the drawbacks of the prior art described above.
第5図、第6図はこの発明のそれぞれ一実施例
を示す断面図である。整流板7と容器3との間に
形成される流路8の断面積Sが容器3の下部に行
く程徐々に小さくなり、距離Hが小さくなつてい
る。このようにすると容器3の下部程流路8を流
れる冷媒液2の流速が早くなり、熱伝達率が上昇
する。また、容器3の底部における冷媒液の淀み
が小さくなる。このことは、例えば、沸騰冷却装
置100が電車などの床下に取り付けられる場合
には容器3の底部が特に放熱と寄与しているた
め、極めて有効である。すなわち、第7図に示す
ように、車両10の床下には、種々の電気機器1
1が艤装されており、車両10が動いたときに生
じる床下の走行風は、沸騰冷却装置100の底部
程大きく、上部では他の電気機器11に邪魔され
ることによつて小さくなつている。したがつて、
沸騰冷却装置100の底部程、熱伝達率を大きく
してやり、熱放散を大きくする方が、発熱体1の
温度上昇を押える上で有利となる。12は線路、
13は車輪である。 FIGS. 5 and 6 are sectional views showing one embodiment of the present invention, respectively. The cross-sectional area S of the flow path 8 formed between the rectifying plate 7 and the container 3 gradually becomes smaller toward the lower part of the container 3, and the distance H becomes smaller. In this way, the flow rate of the refrigerant liquid 2 flowing through the flow path 8 becomes faster toward the lower part of the container 3, and the heat transfer coefficient increases. Furthermore, stagnation of the refrigerant liquid at the bottom of the container 3 is reduced. This is extremely effective, for example, when the boiling cooling device 100 is installed under the floor of a train or the like, since the bottom of the container 3 particularly contributes to heat radiation. That is, as shown in FIG. 7, various electrical devices 1 are installed under the floor of the vehicle 10.
1 is equipped, and the running wind under the floor generated when the vehicle 10 moves is larger at the bottom of the boiling cooling device 100, and smaller at the top because it is obstructed by other electrical equipment 11. Therefore,
It is advantageous to increase the heat transfer coefficient toward the bottom of the boiling cooling device 100 and increase heat dissipation in order to suppress the temperature rise of the heating element 1. 12 is the railway line,
13 is a wheel.
第8図はこの発明の他の実施例である。整流板
7の容器3の底部に近い端部が滑らかに曲げられ
ている。このようにすると、流路8を流れる冷媒
液2の流れが円滑になり、圧力損失が小さくなる
という特徴を有する。 FIG. 8 shows another embodiment of the invention. The end of the current plate 7 near the bottom of the container 3 is smoothly bent. By doing so, the flow of the refrigerant liquid 2 through the flow path 8 becomes smooth, and the pressure loss is reduced.
第9図、第10図はこの発明の他の実施例を示
す断面図で、それぞれ容器3が6角筒、4角筒で
ある。第10図では第2の流路8の終端部が第2
流路8の下部に当り、この部分の断面積が上部の
断面積より小さくしてある。 9 and 10 are sectional views showing other embodiments of the present invention, in which the container 3 is a hexagonal cylinder and a square cylinder, respectively. In FIG. 10, the terminal end of the second flow path 8 is the second
It corresponds to the lower part of the flow path 8, and the cross-sectional area of this part is smaller than the cross-sectional area of the upper part.
以上説明したように、この発明は、第2流路8
の上部断面積より下部断面積を小さくしたので、
容器の下部で流路8を流れる冷媒液の流速が早く
なり、容器の底部における冷媒液の淀みが小さく
なり、そのため、容器の底部での放熱効果を極め
て高めることができる。 As explained above, the present invention provides the second flow path 8
Since the lower cross-sectional area is smaller than the upper cross-sectional area of
The flow rate of the refrigerant liquid flowing through the channel 8 at the bottom of the container becomes faster, and the stagnation of the refrigerant liquid at the bottom of the container becomes smaller, so that the heat dissipation effect at the bottom of the container can be extremely enhanced.
又第2の流路8を第1の流路6の下部に接続す
ると、冷媒液の所望する循環路が形成され、所望
する循環路外の巻込み流が減少するので、一層放
熱効果が促進される。 Furthermore, when the second flow path 8 is connected to the lower part of the first flow path 6, a desired circulation path for the refrigerant liquid is formed, and the entrainment flow outside the desired circulation path is reduced, so that the heat dissipation effect is further promoted. be done.
第1図は従来の沸騰冷却装置を示す断面図、第
2図は先行技術である沸騰冷却装置を示す断面
図、第3図〜第6図はそれぞれこの発明の沸騰冷
却装置の一実施例を示す断面図である。第7図は
この発明の応用例を示す概略正面図、第8図〜第
10図は、それぞれこの発明の一実施例を示す断
面図である。
図において、1は発熱体、2は冷媒液、3は容
器、4は気ほう、6は第1の流路、7は整流板、
8は第2の流路、10は車両である。尚、各図中
同一符号は同一または相当部分を示すものとす
る。
FIG. 1 is a sectional view showing a conventional evaporative cooling device, FIG. 2 is a sectional view showing a prior art evaporative cooling device, and FIGS. 3 to 6 each show an embodiment of the evaporative cooling device of the present invention. FIG. FIG. 7 is a schematic front view showing an application example of the present invention, and FIGS. 8 to 10 are sectional views showing one embodiment of the invention. In the figure, 1 is a heating element, 2 is a refrigerant liquid, 3 is a container, 4 is an air chamber, 6 is a first flow path, 7 is a rectifying plate,
8 is a second flow path, and 10 is a vehicle. Note that the same reference numerals in each figure indicate the same or corresponding parts.
Claims (1)
冷媒液と発熱体を収容した容器、上記発熱体の熱
によつて生じる上記冷媒液の気泡が上向きに流れ
るように上記発熱体中に形成した第1の流路、上
記気泡の上向きの流れで生じる駆動力によつて上
記冷媒液が上記容器の内壁面に接して下向きに流
れ、かつ下降した上記冷媒液が第1の流路に導か
れるように形成した第2の流路を有するものにお
いて、上記第2の流路はその上部断面積よりその
下部断面積が小さいことを特徴とする沸騰冷却装
置。 2 特許請求の範囲第1項記載のものにおいて、
第2の流路は容器の内壁面と整流板で形成し、上
記整流板の下端部が滑らかに湾曲している沸騰冷
却装置。 3 特許請求の範囲第1項又は第2項記載のもの
において、第2の流路は第1の流路の下部と接続
している沸騰冷却装置。[Scope of Claims] 1. A refrigerant liquid, a heating element immersed in the refrigerant liquid, a container containing the refrigerant liquid and the heating element, and a structure in which air bubbles in the refrigerant liquid generated by the heat of the heating element flow upward. The refrigerant liquid flows downward in contact with the inner wall surface of the container due to the driving force generated by the upward flow of the air bubbles in the first flow path formed in the heating element, and the refrigerant liquid that has descended flows into the first flow path. 1. A boiling cooling device having a second flow path formed to be guided to the first flow path, wherein the second flow path has a lower cross-sectional area smaller than an upper cross-sectional area. 2. In what is stated in claim 1,
The second flow path is formed by the inner wall surface of the container and a rectifying plate, and the lower end of the rectifying plate is smoothly curved. 3. The boiling cooling device according to claim 1 or 2, wherein the second flow path is connected to the lower part of the first flow path.
Priority Applications (8)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP56208648A JPS58108759A (en) | 1981-12-22 | 1981-12-22 | Boiling and cooling device |
| KR8201479A KR860000253B1 (en) | 1981-04-07 | 1982-04-03 | Boiling cooling apparatus |
| MX192188A MX157055A (en) | 1981-04-07 | 1982-04-06 | IMPROVEMENTS IN COOLING DEVICE FOR AUTOTRANSPORT |
| US06/366,124 US4572286A (en) | 1981-04-07 | 1982-04-07 | Boiling cooling apparatus |
| DE19823213112 DE3213112A1 (en) | 1981-04-07 | 1982-04-07 | BOILER REFRIGERATOR |
| ES511289A ES511289A0 (en) | 1981-04-07 | 1982-04-07 | REFRIGERATION DEVICE BY BOILING. |
| AU82439/82A AU551611B2 (en) | 1981-04-07 | 1982-04-07 | Ebullition cooling apparatus |
| US06/805,538 US4653579A (en) | 1981-04-07 | 1985-12-06 | Boiling cooling apparatus |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP56208648A JPS58108759A (en) | 1981-12-22 | 1981-12-22 | Boiling and cooling device |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS58108759A JPS58108759A (en) | 1983-06-28 |
| JPS6259889B2 true JPS6259889B2 (en) | 1987-12-14 |
Family
ID=16559722
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP56208648A Granted JPS58108759A (en) | 1981-04-07 | 1981-12-22 | Boiling and cooling device |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS58108759A (en) |
-
1981
- 1981-12-22 JP JP56208648A patent/JPS58108759A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS58108759A (en) | 1983-06-28 |
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