JP6206976B2 - Heat exchanger - Google Patents

Heat exchanger Download PDF

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JP6206976B2
JP6206976B2 JP2014547031A JP2014547031A JP6206976B2 JP 6206976 B2 JP6206976 B2 JP 6206976B2 JP 2014547031 A JP2014547031 A JP 2014547031A JP 2014547031 A JP2014547031 A JP 2014547031A JP 6206976 B2 JP6206976 B2 JP 6206976B2
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heat exchanger
heat exchange
heat
exchange fluid
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JPWO2014077318A1 (en
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直毅 鹿園
直毅 鹿園
洋介 長谷川
洋介 長谷川
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University of Tokyo NUC
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    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F28HEAT EXCHANGE IN GENERAL
    • F28DHEAT-EXCHANGE APPARATUS, NOT PROVIDED FOR IN ANOTHER SUBCLASS, IN WHICH THE HEAT-EXCHANGE MEDIA DO NOT COME INTO DIRECT CONTACT
    • F28D1/00Heat-exchange apparatus having stationary conduit assemblies for one heat-exchange medium only, the media being in contact with different sides of the conduit wall, in which the other heat-exchange medium is a large body of fluid, e.g. domestic or motor car radiators
    • F28D1/02Heat-exchange apparatus having stationary conduit assemblies for one heat-exchange medium only, the media being in contact with different sides of the conduit wall, in which the other heat-exchange medium is a large body of fluid, e.g. domestic or motor car radiators with heat-exchange conduits immersed in the body of fluid
    • F28D1/04Heat-exchange apparatus having stationary conduit assemblies for one heat-exchange medium only, the media being in contact with different sides of the conduit wall, in which the other heat-exchange medium is a large body of fluid, e.g. domestic or motor car radiators with heat-exchange conduits immersed in the body of fluid with tubular conduits
    • F28D1/053Heat-exchange apparatus having stationary conduit assemblies for one heat-exchange medium only, the media being in contact with different sides of the conduit wall, in which the other heat-exchange medium is a large body of fluid, e.g. domestic or motor car radiators with heat-exchange conduits immersed in the body of fluid with tubular conduits the conduits being straight
    • F28D1/0535Heat-exchange apparatus having stationary conduit assemblies for one heat-exchange medium only, the media being in contact with different sides of the conduit wall, in which the other heat-exchange medium is a large body of fluid, e.g. domestic or motor car radiators with heat-exchange conduits immersed in the body of fluid with tubular conduits the conduits being straight the conduits having a non-circular cross-section
    • F28D1/05366Assemblies of conduits connected to common headers, e.g. core type radiators
    • F28D1/05391Assemblies of conduits connected to common headers, e.g. core type radiators with multiple rows of conduits or with multi-channel conduits combined with a particular flow pattern, e.g. multi-row multi-stage radiators
    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F28HEAT EXCHANGE IN GENERAL
    • F28FDETAILS OF HEAT-EXCHANGE AND HEAT-TRANSFER APPARATUS, OF GENERAL APPLICATION
    • F28F1/00Tubular elements; Assemblies of tubular elements
    • F28F1/10Tubular elements and assemblies thereof with means for increasing heat-transfer area, e.g. with fins, with projections, with recesses
    • F28F1/12Tubular elements and assemblies thereof with means for increasing heat-transfer area, e.g. with fins, with projections, with recesses the means being only outside the tubular element
    • F28F1/126Tubular elements and assemblies thereof with means for increasing heat-transfer area, e.g. with fins, with projections, with recesses the means being only outside the tubular element consisting of zig-zag shaped fins
    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F28HEAT EXCHANGE IN GENERAL
    • F28FDETAILS OF HEAT-EXCHANGE AND HEAT-TRANSFER APPARATUS, OF GENERAL APPLICATION
    • F28F2215/00Fins

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  • Engineering & Computer Science (AREA)
  • Physics & Mathematics (AREA)
  • Thermal Sciences (AREA)
  • Mechanical Engineering (AREA)
  • General Engineering & Computer Science (AREA)
  • Geometry (AREA)
  • Heat-Exchange Devices With Radiators And Conduit Assemblies (AREA)

Description

本発明は、熱交換器に関し、詳しくは、伝熱部材の表面に滑らかな曲面を用いて断面が波形で波の頂部が連続する頂部線と波底部が連続する底部線とがV字形状となるよう複数の波形凹凸が形成されており、前記複数の波形凹凸に対して第1の熱交換用流体をV字形状における上下方向に流して熱交換する熱交換器に関する。    More specifically, the present invention relates to a heat exchanger, and more specifically, a smooth curved surface is used on the surface of a heat transfer member, and a top line in which a cross section is corrugated and a wave top is continuous and a bottom line in which a wave bottom is continuous are V-shaped. The present invention relates to a heat exchanger in which a plurality of corrugations are formed so as to exchange heat by flowing a first heat exchange fluid in a vertical direction in a V shape with respect to the plurality of corrugations.

従来、この種の熱交換器としては、熱交換用チューブやフィンに、波の頂部を連ねた線や波の底部を連ねた線が空気の主要な流れに対してなす角が10度から60度の範囲となり且つ空気の主要な流れに沿った所定間隔の折り返し線で対称に折り返す波形の凹凸を形成したものが提案されている(例えば、特許文献1〜3参照)。この熱交換器では、空気の流れの剥離や局所的な増速を抑制すると共に空気の流れに有効な二次流れを生じさせて伝熱効率を向上させ、全体として熱交換効率を向上させている。    Conventionally, in this type of heat exchanger, an angle formed by a line connecting the top of the wave and a line connecting the bottom of the wave to the heat exchange tube or fin with respect to the main flow of air is 10 to 60 degrees. There has been proposed a method in which corrugated irregularities are formed that are symmetrically folded by folding lines at predetermined intervals along the main flow of air (see, for example, Patent Documents 1 to 3). In this heat exchanger, separation of air flow and local acceleration are suppressed, and an effective secondary flow is generated in the air flow to improve heat transfer efficiency, and overall heat exchange efficiency is improved. .

特開2008−180468号公報JP 2008-180468 A 特開2008−232592号公報JP 2008-232592 A 特開2012−137288号公報JP 2012-137288 A

上述の熱交換器では、熱交換用チューブやフィンに形成された波形の凹凸における波は一定の波長で一定の振幅となるように形成されており、空気などの熱交換用流体の流れに対して、伝熱促進や熱交換用流体の流動抵抗が最適となる形状であるか否かは定かではない。    In the heat exchanger described above, the waves in the corrugated irregularities formed on the heat exchanging tubes and fins are formed so as to have a constant amplitude at a constant wavelength, and with respect to the flow of heat exchanging fluid such as air. Thus, it is not certain whether the shape has the optimal flow resistance of the heat transfer promotion or heat exchange fluid.

本発明の熱交換器は、熱交換用チューブやフィンなどの熱交換部材に波形の凹凸が形成された熱交換器において、伝熱促進がより高く流動抵抗がより低くなる熱交換器を提案することを主目的とする。    The heat exchanger according to the present invention proposes a heat exchanger in which corrugated irregularities are formed in heat exchange members such as heat exchange tubes and fins, in which heat transfer promotion is higher and flow resistance is lower. The main purpose.

本発明の熱交換器は、上述の主目的を達成するために以下の手段を採った。    The heat exchanger of the present invention employs the following means in order to achieve the main object described above.

本発明の熱交換器は、
伝熱部材の表面に滑らかな曲面を用いて断面が波形で波の頂部が連続する頂部線と波底部が連続する底部線とがV字形状となるよう複数の波形凹凸が形成されており、前記複数の波形凹凸に対して第1の熱交換用流体をV字形状における上下方向に流して熱交換する熱交換器において、
前記複数の波形凹凸は、前記頂部線におけるV字の傾斜部位と前記第1の熱交換用流体の主要な流れとのなす角の平均としての第1の平均角度が、頂部と底部との中間位置となる中間部が連続する中間部線におけるV字の傾斜部位と第1の熱交換用流体の主要な流れとのなす角の平均としての第2の平均角度より小さくなるよう形成されている、
ことを特徴とする。
The heat exchanger of the present invention is
A plurality of undulations are formed so that the top surface of the heat transfer member has a smooth curved surface and has a V-shaped cross-section with a wave-like top line and a wave-bottom continuous bottom line. In a heat exchanger for exchanging heat by flowing a first heat exchange fluid in a vertical direction in a V shape with respect to the plurality of corrugated irregularities,
In the plurality of corrugations, a first average angle as an average of an angle formed between a V-shaped inclined portion of the top line and the main flow of the first heat exchange fluid is intermediate between the top and the bottom. The intermediate portion to be positioned is formed to be smaller than a second average angle as an average of an angle formed by the V-shaped inclined portion in the continuous intermediate portion line and the main flow of the first heat exchange fluid. ,
It is characterized by that.

この本発明の熱交換器では、複数の波形凹凸は、滑らかな曲面を用いて断面が波形に形成されており、更に、波の頂部が連続する頂部線と波の底部が連続する底部線とがV字形状となるように かつ、頂部線におけるV字の傾斜部位と第1の熱交換用流体の主要な流れとのなす角の平均としての第1の平均角度が、頂部と底部との中間となる中間部が連続する中間部線におけるV字の傾斜部位と第1の熱交換用流体の主要な流れとのなす角の平均としての第2の平均角度より小さくなるよう形成されている。上述した先行技術文献に記載された熱交換器と同様に、本発明の熱交換器では、滑らかな曲面を用いて波の頂部が連続する頂部線と波底部が連続する底部線とがV字形状となるように複数の波形凹凸を形成することにより、第1の熱交換用流体の流れに対して剥離や局所的な増速を抑制すると共に第1の熱交換用流体の流れに対して伝熱促進に有効な二次流れを生じさせる。そして、頂部線におけるV字の斜線部位と第1の熱交換用流体の主要な流れとのなす角の平均としての第1の平均角度が中間部線におけるV字の斜線部位と第1の熱交換用流体の主要な流れとのなす角の平均としての第2の平均角度より小さくなるようすることにより、伝熱促進がより高く流動抵抗がより小さい熱交換器とすることができる。ここで、「頂部と底部との中間となる中間部」は、頂部と底部とに対して高さ方向における中間位置(平均高さ位置)となる部分を意味している。中間部が連続する中間部線は、頂部線や底部線がV字形状となっているから、V字形状となる。波形凹凸が第1の平均角度が第2の平均角度より小さくなるように形成されているということは、頂部線のV字の屈曲部位と傾斜部位の端部(V字が連続する場合には隣接する屈曲部位)との距離が、対応する中間部線のV字の屈曲部位と斜線部位の端部(V字が連続する場合には隣接する屈曲部位)との距離より長くなるように形成されていることになる。このように形成すると、頂部線の屈曲部位における波の立ち上がり(登り)の角度が大きくなるように形成することができるから、これにより、第1の熱交換用流体の主要な流れに対して更に有効な二次流れを生じさせ、伝熱促進を向上させることができる。また、頂部線のV字の傾斜部位における波の立ち上がりの角度を小さくなるように形成することができるから、これにより、第1の熱交換用流体が頂部線を乗り越える際の抵抗を小さくすることができる。これらの結果、伝熱促進が高く流動抵抗が小さな熱交換器とすることができる。    In the heat exchanger according to the present invention, the plurality of corrugated irregularities are formed into a corrugated cross section using a smooth curved surface, and further, a top line in which the top of the wave continues and a bottom line in which the bottom of the wave continues. And the first average angle as the average of the angle formed between the V-shaped inclined portion of the top line and the main flow of the first heat exchange fluid is the top and bottom portions. An intermediate portion that is an intermediate portion is formed so as to be smaller than a second average angle as an average of an angle formed by a V-shaped inclined portion in a continuous intermediate portion line and a main flow of the first heat exchange fluid. . Similar to the heat exchanger described in the above-mentioned prior art document, in the heat exchanger of the present invention, the top line where the wave top is continuous and the bottom line where the wave bottom is continuous using a smooth curved surface are V-shaped. By forming a plurality of corrugations so as to have a shape, separation and local acceleration are suppressed with respect to the flow of the first heat exchange fluid, and at the same time, with respect to the flow of the first heat exchange fluid A secondary flow effective for heat transfer promotion is generated. The first average angle as the average of the angle formed between the V-shaped hatched portion in the top line and the main flow of the first heat exchange fluid is the V-shaped hatched portion in the intermediate line and the first heat. By making it smaller than the second average angle as an average of the angles formed with the main flow of the exchange fluid, a heat exchanger with higher heat transfer promotion and lower flow resistance can be obtained. Here, the “intermediate portion between the top portion and the bottom portion” means a portion that is an intermediate position (average height position) in the height direction with respect to the top portion and the bottom portion. The intermediate part line in which the intermediate part continues is V-shaped because the top line and the bottom line are V-shaped. The fact that the corrugated irregularities are formed so that the first average angle is smaller than the second average angle means that the V-shaped bent portion of the top line and the end of the inclined portion (when the V-shape is continuous) It is formed so that the distance between the adjacent bent portion) is longer than the distance between the corresponding bent portion of the V-shaped intermediate line and the end portion of the hatched portion (adjacent bent portion when the V-shape continues). Will be. If formed in this way, the angle of the rising (climbing) of the wave at the bent portion of the top line can be formed so as to increase, thereby further increasing the main flow of the first heat exchange fluid. An effective secondary flow can be generated and heat transfer enhancement can be improved. In addition, since the angle of the rising of the wave at the V-shaped inclined portion of the top line can be reduced, this reduces the resistance when the first heat exchange fluid crosses the top line. Can do. As a result, a heat exchanger with high heat transfer promotion and low flow resistance can be obtained.

こうした本発明の熱交換器において、前記熱交換器はコルゲートフィン型熱交換器であり、前記伝熱部材はコルゲートフィンであり、前記波形凹凸は頂部と底部とが対称となるよう形成されている、ことを特徴とすることもできる。即ち、コルゲートフィン型熱交換器のコルゲートフィンに本発明の波形凹凸の形状を適用したものである。ここで、「波形凹凸は頂部と底部とが対称となるよう形成されている」は、フィンの一方の面における波の頂部と底部はフィンの他方の面における波の底部と頂部となることから、フィンの一方の面における波の頂部の形状とフィンの他方の面における波の頂部の形状とが同一になるように形成されていることを意味している。このように波形凹凸を形成することにより、フィンの一方の面または他方の面のいずれに流れる第1の熱交換用流体に対しても主要な流れに対する有効な二次流れを形成することができ、伝熱促進を向上させることができるのである。    In such a heat exchanger of the present invention, the heat exchanger is a corrugated fin type heat exchanger, the heat transfer member is a corrugated fin, and the corrugated irregularities are formed so that the top and bottom are symmetrical. , Can also be characterized. In other words, the corrugated fin shape of the present invention is applied to the corrugated fin of the corrugated fin heat exchanger. Here, “the corrugated irregularities are formed so that the top and bottom are symmetrical” means that the top and bottom of the wave on one side of the fin are the bottom and top of the wave on the other side of the fin. This means that the shape of the top of the wave on one side of the fin is the same as the shape of the top of the wave on the other side of the fin. By forming the corrugated irregularities in this way, it is possible to form an effective secondary flow for the main flow with respect to the first heat exchange fluid flowing on either the one surface or the other surface of the fin. The heat transfer promotion can be improved.

また、本発明の熱交換器において、前記伝熱部材は前記第1の熱交換用流体と熱交換する第2の熱交換用流体の流路を形成する扁平な複数のチューブであり、前記チューブの扁平な外表面に前記波形凹凸が形成されている、ことを特徴とするものとすることもできる。即ち、複数のチューブを有する熱交換器のチューブの外表面に本発明の波形凹凸の形状を適用したものである。ここで、「第1の熱交換用流体」と「第2の熱交換用流体」は、いずれも熱交換媒体を意味しており、例えば、「第1の熱交換用流体」として空気などを用い、「第2の熱交換用流体」としてオイルや水などを用いてもよいし、逆に、「第2の熱交換用流体」として空気などを用い、「第1の熱交換用流体」としてオイルや水などを用いてもよい。    Further, in the heat exchanger according to the present invention, the heat transfer member is a plurality of flat tubes forming a flow path of a second heat exchange fluid that exchanges heat with the first heat exchange fluid, and the tube The corrugated irregularities are formed on the flat outer surface of the film. That is, the corrugated shape of the present invention is applied to the outer surface of a tube of a heat exchanger having a plurality of tubes. Here, both the “first heat exchange fluid” and the “second heat exchange fluid” mean a heat exchange medium. For example, air or the like is used as the “first heat exchange fluid”. Oil or water may be used as the “second heat exchange fluid”, or conversely, air or the like may be used as the “second heat exchange fluid”, and the “first heat exchange fluid” Oil or water may be used.

さらに、本発明の熱交換器において、前記複数の波形凹凸は、前記第1の熱交換用流体の上流側に位置する波形凹凸の波形における振幅が前記第1の熱交換用流体の上流側に位置する波形凹凸の波形における振幅より大きくなるよう形成されている、ことを特徴とするものとすることもできる。即ち、伝熱部材において、第1の熱交換用流体の入口側に形成された波形凹凸の波形における振幅が第1の熱交換用流体の出口側に形成された波形凹凸の波形における振幅より大きくなるように波形凹凸を形成するのである。ここで「波形における振幅」は、波形凹凸の頂部の高さや底部の深さに相当する。    Furthermore, in the heat exchanger according to the present invention, the plurality of corrugated irregularities have an amplitude in the waveform of the corrugated irregularities located on the upstream side of the first heat exchange fluid on the upstream side of the first heat exchange fluid. It can also be characterized by being formed so as to be larger than the amplitude in the waveform of the waveform corrugation located. That is, in the heat transfer member, the amplitude of the waveform unevenness formed on the inlet side of the first heat exchange fluid is larger than the amplitude of the waveform unevenness formed on the outlet side of the first heat exchange fluid. Corrugated irregularities are formed so as to be. Here, the “amplitude in the waveform” corresponds to the height of the top and the depth of the bottom of the waveform unevenness.

あるいは、本発明の熱交換器において、前記複数の波形凹凸の前記頂部線および前記底部線は、V字が複数回に亘って連続して繰り返されるよう形成されている、ことを特徴とするものとすることもできる。ここで、「V字が複数回に亘って連続して繰り返される」とは、例えばV字を2回に亘って連続して繰り返すことによりW字となるように、V字を横に接触させた状態で複数個並べて得られる形状、即ちジグザグ形状を意味している。こうした複数の波形凹凸の頂部線および底部線がV字が複数回に亘って連続して繰り返されるよう形成されている態様の本発明の熱交換器において、前記複数の波形凹凸は、前記頂部線の屈曲部位が前記伝熱部材の端部近傍に位置するよう形成されている、ことを特徴とするものとすることもできる。つまり、波形凹凸の頂部線と底部線はV字が複数回に亘って連続して繰り返されるよう形成されており、更に、こうした頂部線の屈曲部位が伝熱部材の端部近傍に位置するように形成されているのである。例えば、V字が連続するように形成された波形凹凸の頂部線の端部(伝熱部材の端部)はV字の斜線部位における下方の部位となっているのである。こうすることにより、伝熱部材の表面に伝熱促進に大きく寄与する部位である頂部線の屈曲部位をより多く形成することができ、伝熱促進を向上させることができる。    Alternatively, in the heat exchanger according to the present invention, the top line and the bottom line of the plurality of corrugated irregularities are formed so that a V-shape is continuously repeated a plurality of times. It can also be. Here, “V-shape is repeated continuously over a plurality of times” means that the V-shape is brought into contact with the side so that it becomes a W-shape by repeating the V-shape continuously over two times, for example. This means a shape obtained by arranging a plurality of the components in a state where they are arranged, that is, a zigzag shape. In the heat exchanger of the present invention in which the top line and the bottom line of the plurality of corrugated irregularities are formed so that the V-shape is continuously repeated a plurality of times, the plural corrugated irregularities are formed on the top line. The bent portion is formed so as to be positioned in the vicinity of the end portion of the heat transfer member. That is, the top line and the bottom line of the corrugated irregularities are formed so that the V-shape is continuously repeated a plurality of times, and the bent portion of the top line is positioned near the end of the heat transfer member. It is formed. For example, the end portion (end portion of the heat transfer member) of the corrugated unevenness formed so that the V shape is continuous is the lower portion of the V-shaped hatched portion. By carrying out like this, the bending | flexion site | part of the top part which is a site | part which contributes largely to heat transfer promotion can be formed more on the surface of a heat transfer member, and heat transfer promotion can be improved.

また、本発明の熱交換器において、前記複数の波形凹凸は、前記頂部線の屈曲部位における頂部の高さが前記頂部線の屈曲部位とは異なる部位における頂部の高さより高くなるよう形成されている、ことを特徴とするものとすることもできる。頂部線の屈曲部位における頂部の高さが頂部線の屈曲部位とは異なる部位における頂部の高さより高くなるよう形成することにより、第1の熱交換用流体の主要な流れに対する二次流れを更に有効に生じさせて伝熱促進を向上させることができる。一方、「頂部線の屈曲部位における頂部の高さが頂部線の屈曲部位とは異なる部位における頂部の高さより高くなるように形成する」ことは、言い換えれば、「頂部線の屈曲部位とは異なる部位における頂部の高さが頂部線の屈曲部位における頂部の高さより低くなるように形成する」ことになる。これにより、頂部線の屈曲部位とは異なる部位における第1の熱交換用流体の流れに対する抵抗を小さくすることができる。これらの結果、伝熱促進が高く流動抵抗が小さな熱交換器とすることができる。    Further, in the heat exchanger of the present invention, the plurality of corrugated irregularities are formed such that the height of the top at the bent portion of the top line is higher than the height of the top at a portion different from the bent portion of the top line. It can also be characterized by that. The secondary flow with respect to the main flow of the first heat exchange fluid is further formed by forming the top height at the bent portion of the top line to be higher than the height of the top portion at a portion different from the bent portion of the top line. It can be effectively generated to improve heat transfer promotion. On the other hand, “the height of the top at the bent portion of the top line is formed to be higher than the height of the top at the portion different from the bent portion of the top line”, in other words, “is different from the bent portion of the top line. It is formed so that the height of the top portion at the portion is lower than the height of the top portion at the bent portion of the top line. Thereby, the resistance with respect to the flow of the 1st heat exchange fluid in the site | part different from the bending site | part of a top line can be made small. As a result, a heat exchanger with high heat transfer promotion and low flow resistance can be obtained.

本発明の第1実施例のコルゲートフィン型の熱交換器20の構成の概略を示す構成図である。It is a block diagram which shows the outline of a structure of the corrugated fin type heat exchanger 20 of 1st Example of this invention. 2つの扁平チューブ30の間にコルゲートフィン40が配置されている様子の外観を拡大して示す拡大外観図である。It is an expansion external view which expands and shows the external appearance of the state where the corrugated fin 40 is arrange | positioned between the two flat tubes 30. FIG. コルゲートフィン40の水平面を2つの扁平チューブ30の断面と共に示す説明図である。4 is an explanatory view showing a horizontal surface of the corrugated fin 40 together with cross sections of two flat tubes 30. FIG. 第1実施例の波形凹凸を立体的に示して説明する説明図である。It is explanatory drawing which shows and demonstrates the waveform unevenness | corrugation of 1st Example in three dimensions. 比較例と第1実施例の波形凹凸を補助線と共に立体的に示す説明図である。It is explanatory drawing which shows three-dimensionally the waveform unevenness | corrugation of a comparative example and 1st Example with an auxiliary line. 第1実施例の波形凹凸を補助線と共に模式的に示す説明図である。It is explanatory drawing which shows typically the waveform unevenness | corrugation of 1st Example with an auxiliary line. 図2のA−A断面を図中のAの矢印方向から見たA−A断面図である。It is the AA sectional view which looked at the AA cross section of FIG. 2 from the arrow direction of A in the figure. 波状の平板に一様流れの流体を導入したときに平板上に生じる流体の二次流れと温度による等高線とを示す説明図である。It is explanatory drawing which shows the secondary flow of the fluid produced on a flat plate when the fluid of a uniform flow is introduce | transduced into a wavy flat plate, and the contour line by temperature. 波形凹凸の位置と局所熱流速の等値線と局所せん断応力の等値線との関係をシミュレーションした結果を示す説明図である。It is explanatory drawing which shows the result of having simulated the relationship between the position of a waveform unevenness | corrugation, the isoline of a local heat flow rate, and the isoline of a local shear stress. 変形例の波形凹凸を立体的に示して説明する説明図である。It is explanatory drawing which shows and shows the waveform unevenness | corrugation of a modification three-dimensionally. 図10のB−B断面を図中のBの矢印方向から見たB−B断面図である。It is BB sectional drawing which looked at the BB cross section of FIG. 10 from the arrow direction of B in the figure. 図10のC−C断面を連続させて図中のCの矢印方向から見たC−C断面図である。It is CC sectional drawing which continued CC section of FIG. 10 from the arrow direction of C in the figure. 図210のD−D断面を連続させて図中のDの矢印方向から見たD−D断面図である。It is DD sectional drawing which continued the DD section of FIG. 210 from the arrow direction of D in the figure. 本発明の第2実施例としての熱交換器120の外観を示す外観図である。It is an external view which shows the external appearance of the heat exchanger 120 as 2nd Example of this invention. 第2実施例の熱交換器120に用いられる熱交換用チューブ130の扁平面を示す説明図である。It is explanatory drawing which shows the flat surface of the tube 130 for heat exchange used for the heat exchanger 120 of 2nd Example.

次に、本発明を実施するための形態を実施例を用いて説明する。    Next, the form for implementing this invention is demonstrated using an Example.

図1は本発明の第1実施例のコルゲートフィン型の熱交換器20の構成の概略を示す構成図であり、図2は扁平チューブ30の間にコルゲートフィン40が配置されている様子の外観を拡大して示す拡大外観図であり、図3はコルゲートフィン40の水平面42を両側の扁平チューブ30の断面と共に示す説明図である。また、図4は第1実施例のコルゲートフィン40に形成された波形凹凸を立体的に示して説明する説明図であり、図5は第1実施例のコルゲートフィン40に形成された波形凹凸と比較例とを補助線と共に立体的に示す説明図であり、図6は第1実施例の波形凹凸を補助線と共に模式的に示す説明図であり、図7は図2のA−A断面を図中のAの矢印方向から見たA−A断面図である。    FIG. 1 is a block diagram showing an outline of the configuration of the corrugated fin heat exchanger 20 according to the first embodiment of the present invention, and FIG. 2 shows the appearance of the corrugated fin 40 disposed between the flat tubes 30. FIG. 3 is an explanatory view showing a horizontal plane 42 of the corrugated fin 40 together with cross sections of the flat tubes 30 on both sides. FIG. 4 is an explanatory view illustrating the corrugated unevenness formed on the corrugated fin 40 of the first embodiment in three dimensions, and FIG. 5 shows the corrugated unevenness formed on the corrugated fin 40 of the first embodiment. FIG. 6 is an explanatory view schematically showing the comparative example together with the auxiliary lines, FIG. 6 is an explanatory view schematically showing the corrugations of the first embodiment together with the auxiliary lines, and FIG. 7 is a cross-sectional view taken along the line AA of FIG. It is AA sectional drawing seen from the arrow direction of A in a figure.

第1実施例のコルゲートフィン型の熱交換器20は、各種の空気調和装置や冷凍装置などの冷凍サイクルに用いられる熱交換器として、或いは、内燃機関からの排ガスや燃料電池からのオフガスから熱エネルギを回収する熱回収装置などのエネルギ変換装置に用いられる熱交換器として用いられ、図1に示すように、扁平な中空管として形成されてハイドロフルオロカーボンや水,オイルなどの熱交換媒体(第2の熱交換用流体)の流路をなす複数の扁平チューブ30と、第2の熱交換用流体を全体として迂流させるための3つの隔壁28a,28b,28cと、各扁平チューブ30の間や扁平チューブ30と3つの隔壁28a,28b,28cとの間,扁平チューブ30と側壁29a,29bとの間に各々配置されて空気や排ガスなどの熱交換媒体(第1の熱交換用流体)の流路において熱交換による伝熱促進を行なう複数のコルゲートフィン40と、これらからなる熱交換部の上部に配置されて第2の熱交換用流体の流入口23と流出口24とが形成された上部ヘッダー22と、熱交換部の下部に配置された下部ヘッダー26とを備える。第1実施例のコルゲートフィン型の熱交換器20の扁平チューブ30や隔壁28a,28b,28c,側壁29a,29b,コルゲートフィン40,上部ヘッダー22,下部ヘッダー26は、第2の熱交換用流体や第1の熱交換用流体に対して耐腐食性を有すると共に熱伝導率の高い金属材料、例えば、第1の熱交換用流体として空気が用いられるときにはアルミニウムや銅,ステンレス、第1の熱交換用流体として内燃機関からの排ガスや燃料電池からの排ガスが用いられるときにはステンレスなどにより形成されている。以下の説明では、コルゲートフィン型の熱交換器20としては、空気調和装置に用いられる熱交換器であり、扁平チューブ30や隔壁28a,28b,28c,側壁29a,29b,コルゲートフィン40,上部ヘッダー22,下部ヘッダー26の各部材についてはアルミニウムにより形成され、大きさとしては、扁平チューブ30の間隔が5mm〜10mm、コルゲートフィン40の水平面42の間隔(垂直面48の高さ)が1mm〜2mm程度であり、第2の熱交換用流体としてハイドロフルオロカーボンを用い、第1の熱交換用流体として空気を用いるもの、を具体例として用いる。    The corrugated fin-type heat exchanger 20 of the first embodiment is a heat exchanger used in a refrigeration cycle such as various air conditioners and refrigeration apparatuses, or heat from exhaust gas from an internal combustion engine or off-gas from a fuel cell. It is used as a heat exchanger used in an energy conversion device such as a heat recovery device that recovers energy. As shown in FIG. 1, it is formed as a flat hollow tube and is a heat exchange medium (hydrofluorocarbon, water, oil, etc.) A plurality of flat tubes 30 forming a flow path of the second heat exchange fluid), three partition walls 28a, 28b, 28c for diverting the second heat exchange fluid as a whole, Between the flat tube 30 and the three partition walls 28a, 28b, 28c, and between the flat tube 30 and the side walls 29a, 29b, respectively, and heat such as air and exhaust gas. A plurality of corrugated fins 40 that promote heat transfer by heat exchange in the flow path of the exchange medium (first heat exchange fluid), and a second heat exchange fluid that is disposed above the heat exchange section composed of these. The upper header 22 in which the inflow port 23 and the outflow port 24 were formed, and the lower header 26 arrange | positioned at the lower part of a heat exchange part are provided. The flat tube 30 and the partition walls 28a, 28b, 28c, the side walls 29a, 29b, the corrugated fins 40, the upper header 22, and the lower header 26 of the corrugated fin heat exchanger 20 of the first embodiment are the second heat exchange fluid. And a metal material that has corrosion resistance and high thermal conductivity with respect to the first heat exchange fluid, such as aluminum, copper, stainless steel, and the first heat when air is used as the first heat exchange fluid. When exhaust gas from an internal combustion engine or exhaust gas from a fuel cell is used as a replacement fluid, it is made of stainless steel or the like. In the following description, the corrugated fin type heat exchanger 20 is a heat exchanger used in an air conditioner, and includes a flat tube 30, partition walls 28a, 28b, 28c, side walls 29a, 29b, corrugated fins 40, and an upper header. 22 and each member of the lower header 26 are made of aluminum, and the size is such that the interval between the flat tubes 30 is 5 mm to 10 mm, and the interval between the horizontal surfaces 42 of the corrugated fins 40 (the height of the vertical surface 48) is 1 mm to 2 mm. A specific example is one in which hydrofluorocarbon is used as the second heat exchange fluid and air is used as the first heat exchange fluid.

上部ヘッダー22の内側には、隔壁28a,28cと整合する位置に隔壁28a,28cが延在するように仕切壁25a,25bが形成されており、下部ヘッダー26の内側には、隔壁28bと整合する位置に隔壁28bが延在するように仕切壁27が形成されている。したがって、第2の熱交換用流体(例えばハイドロフルオロカーボン)は、図中矢印で示すように、流入口23から上部ヘッダー22の内側に流れ込み、隔壁28aより右側の3つの扁平チューブ30の内側を鉛直上方から鉛直下方に流れ、下部ヘッダー26内で仕切壁27により隔壁28a,28bの間の3つの扁平チューブ30に供給され、3つの扁平チューブ30の内側を鉛直下方から鉛直上方に流れて上部ヘッダー22の仕切壁25a,25bの間の空間に流れ込み、隔壁28b,28cの3つの扁平チューブ30の内側を鉛直上方から鉛直下方に流れて仕切壁28bの右側の空間に至り、隔壁28cより左側の3つの扁平チューブ30の内側を鉛直下方から鉛直上方に流れて上部ヘッダー22の仕切壁25bの左側の空間に入り、その後、流出口24から排出される。なお、第1の熱交換用流体(空気)は、図1では表面から裏面に向けて、図2では斜め左下から斜め右上に向けて、図3では下から上に向けて、複数の扁平チューブ30の間を抜けるように流れる。    Partition walls 25a and 25b are formed on the inner side of the upper header 22 so that the partition walls 28a and 28c extend at positions that align with the partition walls 28a and 28c, and the lower header 26 is aligned with the partition wall 28b. A partition wall 27 is formed so that the partition wall 28b extends at a position where the partition wall 28b extends. Therefore, the second heat exchange fluid (for example, hydrofluorocarbon) flows into the upper header 22 from the inlet 23 as indicated by the arrows in the figure, and vertically passes through the three flat tubes 30 on the right side of the partition wall 28a. The upper header flows vertically downward from above, is supplied to the three flat tubes 30 between the partition walls 28a and 28b by the partition wall 27 in the lower header 26, and flows vertically upward from below the three flat tubes 30. 22 flows into the space between the partition walls 25a and 25b, flows from the vertically upper side to the vertically lower side in the three flat tubes 30 of the partition walls 28b and 28c, reaches the space on the right side of the partition wall 28b, and is on the left side of the partition wall 28c. The inside of the three flat tubes 30 flows vertically downward from vertically above and enters the space on the left side of the partition wall 25b of the upper header 22, After, and is discharged from the outlet 24. Note that the first heat exchange fluid (air) is a plurality of flat tubes from the front surface to the back surface in FIG. 1, from diagonally lower left to diagonally upper right in FIG. 2, and from lower to upper in FIG. Flows through 30.

コルゲートフィン40は、水平面42と垂直面48とが交互につづら折り状(蛇腹状)に形成され、垂直面48が扁平チューブ30にろう付けなどにより接合されている。コルゲートフィン40の水平面42には、滑らかな曲面により複数の波形凹凸が形成されている。第1実施例の複数の波形凹凸は、図3に示すように、波の頂部を連ねた頂部線43や波の底部を連ねた底部線44と第1の熱交換用流体(空気)の主要な流れとのなす角が鋭角の範囲の角度となるように、頂部線43および底部線44がV字状に複数回に亘って連続して繰り返すように、頂部線43の屈曲部位43aがコルゲートフィン40の水平面42の端部近傍に位置するように、頂部線43におけるV字の斜線部位43bと第1の熱交換用流体の主要な流れとのなす角の平均としての第1の平均角度が、波形凹凸における平均高さとなる中間部が連続する中間部線45におけるV字の斜線部位45bと第1の熱交換用流体の主要な流れとのなす角の平均としての第2の平均角度より小さくなるように、水平面42の一方の面における凸部の形状と同面における凹部の形状とが表裏一体となるように、図7に示すように、第1の熱交換用流体(空気)の入口側の波の振幅が出口側の波の振幅より大きくなるように、形成されている。以下に、実施例のコルゲートフィン40に形成された波形凹凸について詳しく説明する。なお、波の頂部は、波の凸部と凹部との繰り返しにおける凸部の頂を意味しており、波の底部は、波の凸部と凹部との繰り返しにおける凹部の底を意味している。    In the corrugated fin 40, the horizontal plane 42 and the vertical plane 48 are alternately formed in a folded shape (bellows shape), and the vertical plane 48 is joined to the flat tube 30 by brazing or the like. On the horizontal plane 42 of the corrugated fin 40, a plurality of corrugated irregularities are formed by a smooth curved surface. As shown in FIG. 3, the plurality of corrugations of the first embodiment are mainly composed of a top line 43 connecting the wave tops and a bottom line 44 connecting the wave bottoms and the first heat exchange fluid (air). The bent portion 43a of the top line 43 is a corrugated so that the top line 43 and the bottom line 44 are continuously repeated in a V shape a plurality of times so that the angle formed with the straight flow is an acute angle. The first average angle as the average of the angle formed by the V-shaped oblique line portion 43b in the top line 43 and the main flow of the first heat exchange fluid so as to be positioned near the end of the horizontal surface 42 of the fin 40 Is the second average angle as the average of the angle formed between the V-shaped oblique line portion 45b in the intermediate line 45 where the intermediate part having the average height in the corrugated irregularities is continuous and the main flow of the first heat exchange fluid. Convex on one surface of the horizontal surface 42 so as to be smaller As shown in FIG. 7, the amplitude of the wave on the inlet side of the first heat exchange fluid (air) is greater than the amplitude of the wave on the outlet side so that the shape of the recess and the shape of the recess on the same surface are integrated. It is formed to be large. Hereinafter, the corrugated irregularities formed in the corrugated fin 40 of the embodiment will be described in detail. The top of the wave means the top of the convex part in the repetition of the convex part and the concave part of the wave, and the bottom of the wave means the bottom of the concave part in the repetition of the convex part and the concave part of the wave. .

コルゲートフィン40の水平面42に形成された複数の波形凹凸は、図3に示すように、滑らかな曲面により、波の頂部を連ねた頂部線43や波の底部を連ねた底部線44と第1の熱交換用流体(空気)の主要な流れとのなす角が鋭角の範囲の角度となるように形成されている。ここで、頂部線43や底部線44と第1の熱交換用流体(空気)の主要な流れとのなす角は、10度ないし60度が好ましく、15度ないし45度が更に好ましく、25度ないし35度がより理想的である。このように、滑らかな曲面により波形凹凸を形成し、頂部線43や底部線44と第1の熱交換用流体(空気)の主要な流れとのなす角が10度から60度の範囲内の角度となるように波形凹凸を形成するのは、第1の熱交換用流体の流れに対して剥離や局所的な増速を抑えて、伝熱促進に有効な空気の二次流れを発生させるためである。図8に波状の平板に一様流れの流体を導入したときに平板上に生じる流体の二次流れ(矢印)と温度による等高線とを示す。図示するように、滑らかな曲面による波形凹凸により、流体の剥離や局所的な増速を抑制して強い二次流れを生じさせ、かつ、壁面付近で大きな温度勾配を生じさせていることがわかる。これにより、伝熱促進をより高くすることができると共に流動抵抗を小さくすることができる。    As shown in FIG. 3, the plurality of corrugated irregularities formed on the horizontal surface 42 of the corrugated fin 40 has a smooth curved surface and a top line 43 connecting the wave tops and a bottom line 44 connecting the wave bottoms to the first line. The angle formed with the main flow of the heat exchange fluid (air) is an acute angle. Here, the angle between the top line 43 and the bottom line 44 and the main flow of the first heat exchange fluid (air) is preferably 10 degrees to 60 degrees, more preferably 15 degrees to 45 degrees, and more preferably 25 degrees. Thirty-five degrees is more ideal. In this way, the corrugated irregularities are formed by a smooth curved surface, and the angle between the top line 43 and the bottom line 44 and the main flow of the first heat exchange fluid (air) is within a range of 10 degrees to 60 degrees. The formation of the corrugated irregularities so as to form an angle generates a secondary flow of air effective for promoting heat transfer by suppressing separation and local acceleration with respect to the flow of the first heat exchange fluid. Because. FIG. 8 shows a secondary flow (arrow) of the fluid generated on the flat plate when a uniform flow of fluid is introduced into the wavy flat plate, and contour lines due to temperature. As shown in the figure, it can be seen that the corrugated unevenness by the smooth curved surface suppresses the separation of fluid and local acceleration to generate a strong secondary flow, and also generates a large temperature gradient near the wall surface. . Thereby, heat transfer promotion can be made higher and flow resistance can be made smaller.

コルゲートフィン40の水平面42に形成された複数の波形凹凸は、頂部線43や底部線44がV字状に複数回に亘って連続して繰り返すように形成されている。V字状に複数回に亘って連続して繰り返すとは、例えばV字を2回に亘って連続して繰り返すことによりW字となるように、V字を横に接触させた状態で複数個並べて得られる形状、即ちジグザグ形状となるように形成されていることを意味している。これにより、第1の熱交換用流体による熱交換に有効な二次流れを水平面42の多くの部位に生じさせることができ、伝熱促進をより高くすることができる。    The plurality of corrugated irregularities formed on the horizontal surface 42 of the corrugated fin 40 are formed such that the top line 43 and the bottom line 44 are continuously repeated in a V shape a plurality of times. To repeat continuously in a V shape a plurality of times means, for example, that a plurality of V characters are in lateral contact with each other so that a V shape is formed by continuously repeating a V character twice. It means that it is formed so as to have a shape obtained side by side, that is, a zigzag shape. Thereby, the secondary flow effective for the heat exchange by the first heat exchange fluid can be generated in many parts of the horizontal surface 42, and the heat transfer can be further enhanced.

コルゲートフィン40の水平面42に形成された複数の波形凹凸は、頂部線43における斜線部位43bと第1の熱交換用流体の主要な流れとのなす角の平均としての第1の平均角度が、波形凹凸における平均高さとなる中間部が連続する中間部線45における斜線部位45bと第1の熱交換用流体の主要な流れとのなす角の平均としての第2の平均角度より小さくなるように形成されている。図5(a)の比較例の波形凹凸は、頂部線943と頂部線944とがV字状となるように、屈曲部位943aも斜線部位943bも第1の熱交換用流体(空気)の主要な流れとのなす角が同じで一定となるように形成されている。図4および図5(b)に示す第1実施例の波形凹凸は、図5の補助線に示すように、比較例の波形凹凸の頂部線943に対して、波型凹凸の平均高さとなる中間部が連続する中間部線945の変形がなるべく生じないように、屈曲部位943aについては図中上下に伸張するよう移動させて屈曲部位43aとし、直線の頂部線943については僅かにS字カーブを描くように変形させて頂部線43としたものである。したがって、第1実施例の波形凹凸の底部線44は比較例の底部線944と同一である。図4および図5(b)には、波形凹凸の頂部線43だけを立体的に示したが、底部線44も頂部線43と同様に形成されている。中間部線45は、頂部線43や底部線44がV字形状となっているから、V字形状となり、頂部線43の屈曲部位43aや底部線44の屈曲部位44aが比較例の位置から図中上下方向に伸張した位置とされることにより、若干ではあるが図中上下方向に伸張する。頂部線43の傾斜部位43bと第2の熱交換用流体の主要な流れとのなす角の平均としての第1の平均角度θ1は、図6に示すように、頂部線43の斜線部位43bの図中上下方向の長さL1とV字の幅Wを用いると、tanθ1=(1/2)W/L1を満たす角度として表わされ、中間部線45の傾斜部位45bと第2の熱交換用流体の主要な流れとのなす角の平均としての第2の平均角度θ2は、中間部線45の斜線部位45bの図中上下方向の長さL2とV字の幅Wを用いると、tanθ2=(1/2)W/L2を満たす角度として表わされる。中間部線45に図中上下方向への若干の伸張(図6の上下方向として長さΔL)があったとしても、中間部線45の図6中上下方向への伸張ができるだけ生じないようにするため、L1>L2+ΔLとなることから、第1の平均角度θ1は第2の平均角度θ2より小さくなる。    The plurality of corrugated irregularities formed on the horizontal surface 42 of the corrugated fin 40 has a first average angle as an average of an angle formed by the oblique line portion 43b in the top line 43 and the main flow of the first heat exchange fluid, An intermediate portion having an average height in the corrugated unevenness is made smaller than a second average angle as an average of an angle formed by a hatched portion 45b in a continuous intermediate portion line 45 and a main flow of the first heat exchange fluid. Is formed. The corrugated irregularities of the comparative example of FIG. 5A are the main heat exchange fluid (air) in both the bent portion 943a and the shaded portion 943b so that the top line 943 and the top line 944 are V-shaped. It is formed so that the angle formed by the flow is the same and constant. The corrugated irregularities of the first embodiment shown in FIG. 4 and FIG. 5B are the average height of the corrugated irregularities with respect to the top line 943 of the corrugated irregularities of the comparative example, as shown by the auxiliary line in FIG. The bent portion 943a is moved so as to extend vertically in the figure so as to avoid deformation of the intermediate portion line 945 where the intermediate portion is continuous, and is bent to a bent portion 43a, and the straight top line 943 is slightly S-curved. The top line 43 is deformed so as to draw. Accordingly, the corrugated bottom line 44 of the first embodiment is the same as the bottom line 944 of the comparative example. In FIG. 4 and FIG. 5B, only the top line 43 of the corrugated unevenness is three-dimensionally shown, but the bottom line 44 is also formed in the same manner as the top line 43. The intermediate line 45 is V-shaped because the top line 43 and the bottom line 44 are V-shaped, and the bent part 43a of the top line 43 and the bent part 44a of the bottom line 44 are illustrated from the position of the comparative example. By setting the position extended in the middle / up / down direction, the position extends slightly in the up / down direction in the figure. As shown in FIG. 6, the first average angle θ1 as an average of the angle formed between the inclined portion 43b of the top line 43 and the main flow of the second heat exchange fluid is as shown in FIG. When the vertical length L1 and the V-shaped width W are used in the figure, the angle is expressed as an angle satisfying tan θ1 = (1/2) W / L1, and the inclined portion 45b of the intermediate line 45 and the second heat exchange are expressed. The second average angle θ2 as the average of the angles formed with the main flow of the working fluid is tan θ2 using the vertical length L2 and the V-shaped width W of the hatched portion 45b of the intermediate line 45 in the drawing. = (1/2) Expressed as an angle satisfying W / L2. Even if the intermediate portion line 45 has a slight extension in the vertical direction in the drawing (length ΔL as the vertical direction in FIG. 6), the intermediate portion line 45 is prevented from extending in the vertical direction in FIG. 6 as much as possible. Therefore, since L1> L2 + ΔL, the first average angle θ1 is smaller than the second average angle θ2.

上述したように、中間部線45は若干ではあるが図中上下方向に伸張しているが、説明の容易のために、図6には図中上下方向には伸張しないものとして表わした。図6中、太実線が頂部線43であり、細実線が伸張前の比較例の頂部線943であり、太破線が底部線44であり、細破線が伸張前の比較例の底部線944であり、太一点鎖線が中間部線45である。第1の熱交換用流体(空気)の流れに沿って見たときに、頂部線43や底部線44の逆V字の屈曲部位において、頂部線43の屈曲部位43aと中間部線45の屈曲部位45aとの距離をL11、中間部線45の屈曲部位45aと底部線44の屈曲部位44aとの距離をL12、底部線44の屈曲部位44aと中間部線45の屈曲部位45との距離をL13、中間部線45の屈曲部位45aと頂部線43の屈曲部位43aとの距離をL14、頂部線43や底部線44のV字の屈曲部位において、頂部線43の屈曲部位43aと中間部線45の屈曲部位45aとの距離をL21、中間部線45の屈曲部位45aと底部線44の屈曲部位44aとの距離をL22、底部線44の屈曲部位44aと中間部線45の屈曲部位45との距離をL23、中間部線45の屈曲部位45aと頂部線43の屈曲部位43aとの距離をL24とすると、以下の式(1)が成立する。このため、波形凹凸は、図中上から下に向けて第2の熱交換用流体(空気)を流したときには、逆V字の屈曲部位では、底部線44の屈曲部位44aから中間部線45の屈曲部位45aまでは比較的緩やかな登りの傾斜となり、中間部線45の屈曲部位45aから頂部線43の屈曲部位43aまでは比較的急な登りの傾斜となり、頂部線43の屈曲部位43aから中間部線45の屈曲部位45aまでは比較的緩やかな下りの傾斜となり、中間部線45の屈曲部位45aから底部線44の屈曲部位44aまでは比較的急な下りの傾斜となる。また、V字の屈曲部位では、底部線44の屈曲部位44aから中間部線45の屈曲部位45aまでは比較的急な登りの傾斜となり、中間部線45の屈曲部位45aから頂部線43の屈曲部位43aまでは比較的緩やかな傾斜となり、頂部線43の屈曲部位43aから中間部線45の屈曲部位45aまでは比較的急な下りの傾斜となり、中間部線45の屈曲部位45aから底部線44の屈曲部位44aまでは比較的緩やかな下りの傾斜となる。    As described above, the intermediate portion line 45 slightly extends in the vertical direction in the figure, but for ease of explanation, it is shown in FIG. 6 as not extending in the vertical direction in the figure. In FIG. 6, the thick solid line is the top line 43, the thin solid line is the top line 943 of the comparative example before expansion, the thick broken line is the bottom line 44, and the thin broken line is the bottom line 944 of the comparative example before expansion. Yes, the thick dotted line is the intermediate part line 45. When viewed along the flow of the first heat exchange fluid (air), the bent portion 43a of the top wire 43 and the bent portion 45 of the middle wire 45 are bent at the inverted V-shaped bent portion of the top wire 43 and the bottom wire 44. L11 is the distance to the part 45a, L12 is the distance between the bent part 45a of the intermediate line 45 and the bent part 44a of the bottom line 44, and the distance between the bent part 44a of the bottom line 44 and the bent part 45 of the intermediate line 45 is L13, the distance between the bent part 45a of the intermediate line 45 and the bent part 43a of the top line 43 is L14, and the bent part 43a of the top line 43 and the intermediate part line in the V-shaped bent part of the top line 43 and the bottom line 44 45, the distance between the bent part 45a of the intermediate line 45 is L21, the distance between the bent part 45a of the intermediate part line 45 and the bent part 44a of the bottom part 44 is L22, and the bent part 44a of the bottom part line 44 and the bent part 45 of the intermediate part line 45 are Distance L23, medium When the distance between the bent portion 43a of the bent portion 45a and the top line 43 parts lines 45 and L24, the following equation (1) is satisfied. For this reason, when the second heat exchanging fluid (air) is flowed from the top to the bottom in the figure, the corrugated irregularities are bent from the bent portion 44a of the bottom line 44 to the intermediate portion line 45 in the inverted V-shaped bent portion. From the bent portion 43a of the top line 43 to the bent portion 45a of the top line 43, and from the bent portion 43a of the top line 43 to the bent portion 43a of the top line 43. The intermediate line 45 has a relatively gentle downward slope to the bent part 45a, and the intermediate part 45 has a relatively steep downward slope from the bent part 45a of the intermediate line 45 to the bent part 44a of the bottom line 44. Further, in the bent portion of the V shape, a relatively steep upward slope is obtained from the bent portion 44a of the bottom line 44 to the bent portion 45a of the intermediate line 45, and the bent portion 45a of the intermediate line 45 is bent from the bent portion 45a. The portion 43a has a relatively gentle slope, and the bent portion 43a of the top line 43 to the bent portion 45a of the intermediate portion line 45 has a relatively steep downward slope, and the bent portion 45a of the intermediate portion 45 has a bottom line 44. A relatively gentle downward slope is obtained up to the bent portion 44a.

L11=L13=L22=L24>L12=L14=L21=L23 (1)    L11 = L13 = L22 = L24> L12 = L14 = L21 = L23 (1)

このように複数の波形凹凸を頂部線43の斜線部位43bと第1の熱交換用流体の主要な流れとのなす角の平均(第1の平均角度)が中間部線45の斜線部位45bと第1の熱交換用流体の主要な流れとのなす角の平均(第2の平均角度)より小さくなるように形成するのは、次の理由による。図9は、比較例の波形凹凸の位置と局所熱流速の等値線と局所せん断応力の等値線との関係をシミュレーションした結果を示す説明図である。図示するように、局所熱流速は、第1の熱交換用流体の流れの方向から見て、底部線44から頂部線43に至る部位で大きく、頂部線43から底部線44に至る部位で小さくなっている。また、底部線44の屈曲部位44aから頂部線43の屈曲部位43aに至る部位は、底部線44の傾斜部位44bから頂部線43の傾斜部位43bに至る部位より大きくなっており、この部位でも第1の熱交換用流体の流入側の方が流出側より大きくなっている。局所せん断応力は、頂部線43で大きくなっており、屈曲部位43aの方が傾斜部位43bより大きくなっている。また、第1の熱交換用流体の流出側の方が流入側より大きくなっている。局所熱流速が大きな部位は、伝熱促進が高く熱交換に大きく寄与する部位を示し、局所せん断応力が大きな部位は、第1の熱交換用流体の流れに対する抵抗が大きな部位を示す。したがって、局所熱流速が大きな部位の形状を強調すると共に局所せん断応力が大きな部位の形状を緩和することにより、伝熱促進が高く流動抵抗が小さい熱交換器とすることができる。逆V字の屈曲部位における中間部線45の屈曲部位45aから頂部線43の屈曲部位43aまでの部位は局所熱流速が大きな部位であるから、この部位を比較的急な登りの傾斜とすることにより、伝熱促進を高くすることができる。一方、頂部線43の傾斜部位43bと第2の熱交換用流体とのなす角の平均(第1の平均角度)は比較例の頂部線943と同様となる中間部線45の傾斜部位45bと第1の熱交換用流体とのなす角の平均(第2の平均角度)が小さくなっていると共にV字の屈曲部位における中間部線45の屈曲部位45aから頂部線43の屈曲部位43aまでの部位が比較的緩やかな登りの傾斜となっているから、第1の熱交換用流体は頂部線43を乗り越えやすくなる。このため、第1の熱交換用流体の流れに対する流動抵抗が小さくなる。    In this way, the average (first average angle) of the angle formed by the plurality of corrugated irregularities between the hatched portion 43 b of the top line 43 and the main flow of the first heat exchange fluid is the hatched portion 45 b of the intermediate line 45. The reason why the first heat exchange fluid is formed to be smaller than the average angle (second average angle) with the main flow of the first heat exchange fluid is as follows. FIG. 9 is an explanatory diagram showing the result of simulating the relationship between the position of the corrugated surface of the comparative example, the contour line of the local heat flow velocity, and the contour line of the local shear stress. As shown in the figure, the local heat flow rate is large in the region from the bottom line 44 to the top line 43 and small in the region from the top line 43 to the bottom line 44 when viewed from the direction of the flow of the first heat exchange fluid. It has become. Further, the part from the bent part 44a of the bottom line 44 to the bent part 43a of the top line 43 is larger than the part from the inclined part 44b of the bottom line 44 to the inclined part 43b of the top line 43. The inflow side of 1 heat exchange fluid is larger than the outflow side. The local shear stress is larger at the top line 43, and the bent portion 43a is larger than the inclined portion 43b. In addition, the outflow side of the first heat exchange fluid is larger than the inflow side. A region where the local heat flow rate is large indicates a region where heat transfer is highly promoted and greatly contributes to heat exchange, and a region where the local shear stress is large indicates a region where resistance to the flow of the first heat exchange fluid is large. Therefore, by emphasizing the shape of the region where the local heat flow rate is large and relaxing the shape of the region where the local shear stress is large, a heat exchanger with high heat transfer promotion and low flow resistance can be obtained. Since the portion from the bent portion 45a of the intermediate line 45 to the bent portion 43a of the top line 43 in the inverted V-shaped bent portion is a portion having a large local heat flow rate, this portion should be a relatively steep climb slope. Therefore, the heat transfer promotion can be increased. On the other hand, the average angle (first average angle) formed between the inclined portion 43b of the top line 43 and the second heat exchange fluid is the same as that of the top line 943 of the comparative example. The average angle (second average angle) formed with the first heat exchange fluid is small, and from the bent portion 45a of the intermediate line 45 to the bent portion 43a of the top line 43 in the V-shaped bent portion. Since the portion has a relatively gentle slope, the first heat exchange fluid can easily get over the top line 43. For this reason, the flow resistance with respect to the flow of the first heat exchange fluid is reduced.

コルゲートフィン40の水平面42に形成された複数の波形凹凸は、水平面42の一方の面における凸部(頂部線43における屈曲部位43aおよび傾斜部位43b)の形状と同面における凹部(底部線44における屈曲部位44aおよび傾斜部位44b)の形状とが表裏一体となるように形成されている。即ち、水平面42の一方の面における頂部線43の屈曲部位43aと傾斜部位43bの形状と同面における底部線44の屈曲部位44aと傾斜部位44bの形状とが表裏一体、即ち表裏入れ替えれば一致するように形成されている。これにより、コルゲートフィン40の水平面42の一方の面側に流れる第1の熱交換用流体との熱交換と水平面42の他方の面側に流れる第1の熱交換用流体との熱交換とを同様に行なうことができ、伝熱促進がより高く流動抵抗のより小さな熱交換器とすることができる。    The plurality of corrugated irregularities formed on the horizontal plane 42 of the corrugated fin 40 are concave portions (on the bottom line 44) on the same plane as the projections on one surface of the horizontal plane 42 (the bent portion 43 a and the inclined portion 43 b on the top line 43). The bent portion 44a and the inclined portion 44b) are formed so as to be integrated with each other. That is, the shape of the bent portion 43a and the inclined portion 43b of the top line 43 on one surface of the horizontal plane 42 and the shape of the bent portion 44a and the inclined portion 44b of the bottom line 44 on the same surface are the same when the front and back sides are integrated, that is, the front and back are interchanged. It is formed as follows. Thus, heat exchange with the first heat exchange fluid flowing on one surface side of the horizontal surface 42 of the corrugated fin 40 and heat exchange with the first heat exchange fluid flowing on the other surface side of the horizontal surface 42 are performed. This can be done in the same manner, and a heat exchanger with higher heat transfer and lower flow resistance can be obtained.

コルゲートフィン40の水平面42に形成された複数の波形凹凸は、頂部線43の屈曲部位43aがコルゲートフィン40の水平面42の端部近傍に位置するように形成されている。即ち、頂部線43の屈曲部位43aがより多く形成されるように複数の波形凹凸が形成されているのである。これにより、局所熱流速が高い部位である頂部線43の屈曲部位43aを水平面42により多く形成することができ、伝熱促進がより高い熱交換器とすることができる。    The plurality of corrugated irregularities formed on the horizontal plane 42 of the corrugated fin 40 are formed such that the bent portion 43 a of the top line 43 is positioned near the end of the horizontal plane 42 of the corrugated fin 40. That is, a plurality of corrugations are formed so that more bent portions 43a of the top line 43 are formed. Thereby, the bending part 43a of the top line 43 which is a site | part with a high local heat flow rate can be formed more in the horizontal surface 42, and it can be set as a heat exchanger with higher heat transfer promotion.

コルゲートフィン40の水平面42に形成された複数の波形凹凸は、第1の熱交換用流体(例えば空気)の入口側の波の振幅が出口側の波の振幅より大きくなるように形成されている。図7に示すように、頂部線43の屈曲部位43aの高さは、第1の熱交換用流体(例えば空気)の入口に最も近い屈曲部位43aの高さHinから出口に最も近い屈曲部位43aの高さHoutとなるように徐々に低くなっている。同様に、底部線44の屈曲部位44aの深さは、第1の熱交換用流体(例えば空気)の入口に最も近い屈曲部位44aの深さHinから出口に最も近い屈曲部位44aの深さHoutとなるように徐々に浅くなっている。図9の局所せん断応力では、第1の熱交換用流体の流出側の方が流入側より大きくなっているから、局所せん断応力の大きな第1の熱交換用流体の出口側の頂部線43の高さを入口側の高さに比して低くすることにより、第1の熱交換用流体の流れに対する流動抵抗を小さくすることができる。    The plurality of corrugated irregularities formed on the horizontal surface 42 of the corrugated fin 40 are formed such that the amplitude of the wave on the inlet side of the first heat exchange fluid (for example, air) is larger than the amplitude of the wave on the outlet side. . As shown in FIG. 7, the height of the bent portion 43a of the top wire 43 is such that the bent portion 43a closest to the outlet from the height Hin of the bent portion 43a closest to the inlet of the first heat exchange fluid (for example, air). The height is gradually lowered so as to become the height Hout. Similarly, the depth of the bent portion 44a of the bottom line 44 is determined by the depth Hout of the bent portion 44a closest to the outlet from the depth Hin of the bent portion 44a closest to the inlet of the first heat exchange fluid (for example, air). It becomes gradually shallower. In the local shear stress of FIG. 9, since the outflow side of the first heat exchange fluid is larger than the inflow side, the top line 43 on the outlet side of the first heat exchange fluid having a large local shear stress is used. By making the height lower than the height on the inlet side, the flow resistance against the flow of the first heat exchange fluid can be reduced.

以上説明した第1実施例の熱交換器20によれば、コルゲートフィン40の水平面42に形成された複数の波形凹凸を、滑らかな曲面により、頂部線43や底部線44と第1の熱交換用流体の主要な流れとのなす角が鋭角の範囲の角度となるように、頂部線43や底部線44がV字状に複数回に亘って連続して繰り返すように、頂部線43における斜線部位43bと第1の熱交換用流体の主要な流れとのなす角の平均としての第1の平均角度が、波形凹凸における平均高さとなる中間部が連続する中間部線45における斜線部位45bと第1の熱交換用流体の主要な流れとのなす角の平均としての第2の平均角度より小さくなるように形成することにより、第1の熱交換用流体の流れに対して剥離や局所的な増速を抑えて伝熱促進に有効な空気の二次流れを発生させることができ、局所熱流速の大きな部位を強調して伝熱促進を図り、局所せん断応力の大きな部位のせん断応力を小さくして第1の熱交換用流体の流れに対する流動抵抗を小さくすることができる。これらの結果、伝熱促進がより高く流動抵抗のより小さな熱交換器とすることができる。    According to the heat exchanger 20 of the first embodiment described above, the plurality of corrugated irregularities formed on the horizontal surface 42 of the corrugated fin 40 are exchanged with the top line 43 and the bottom line 44 by the first heat exchange with a smooth curved surface. The oblique line in the top line 43 so that the top line 43 and the bottom line 44 are continuously repeated in a V shape a plurality of times so that the angle formed with the main flow of the working fluid is an acute angle. The first average angle as the average of the angle formed between the portion 43b and the main flow of the first heat exchange fluid is the hatched portion 45b in the intermediate portion line 45 where the intermediate portion having the average height in the corrugated irregularities is continuous. By forming the first heat exchange fluid so as to be smaller than the second average angle as an average of the angles formed with the main flow of the first heat exchange fluid, separation or locality is caused with respect to the flow of the first heat exchange fluid. Effective for preventing heat increase and promoting heat transfer Secondary flow can be generated, heat transfer is promoted by emphasizing the region where the local heat flow rate is large, and the shear stress at the region where the local shear stress is large is reduced to reduce the flow of the first heat exchange fluid. Flow resistance can be reduced. As a result, a heat exchanger with higher heat transfer promotion and lower flow resistance can be obtained.

しかも、第1実施例の熱交換器20によれば、コルゲートフィン40の水平面42に形成された複数の波形凹凸を、水平面42の一方の面における凸部の形状と同面における凹部の形状とが表裏一体となるように形成することにより、コルゲートフィン40の水平面42の一方の面側に流れる第1の熱交換用流体との熱交換と水平面42の他方の面側に流れる第1の熱交換用流体との熱交換とを同様に行なうことができる。この結果、伝熱促進がより高く流動抵抗のより小さな熱交換器とすることができる。    In addition, according to the heat exchanger 20 of the first embodiment, the plurality of corrugated irregularities formed on the horizontal plane 42 of the corrugated fin 40 are formed with a convex shape on one surface of the horizontal plane 42 and a concave shape on the same surface. Is formed so as to be integrated with the front and back, heat exchange with the first heat exchange fluid flowing on one surface side of the horizontal surface 42 of the corrugated fin 40 and first heat flowing on the other surface side of the horizontal surface 42 Heat exchange with the replacement fluid can be performed in the same manner. As a result, a heat exchanger with higher heat transfer acceleration and lower flow resistance can be obtained.

また、第1実施例の熱交換器20によれば、コルゲートフィン40の水平面42に形成された複数の波形凹凸を、頂部線43の屈曲部位43aがコルゲートフィン40の水平面42の端部近傍に位置するように形成することにより、局所熱流速が高い部位である頂部線43の屈曲部位43aを水平面42により多く形成することができ、伝熱促進がより高い熱交換器とすることができる。    Further, according to the heat exchanger 20 of the first embodiment, the plurality of corrugated irregularities formed on the horizontal surface 42 of the corrugated fin 40 are arranged so that the bent portion 43 a of the top line 43 is near the end of the horizontal surface 42 of the corrugated fin 40. By forming so that it may be located, the bending part 43a of the top line 43 which is a site | part with a high local heat flow rate can be formed more in the horizontal surface 42, and it can be set as a heat exchanger with higher heat transfer promotion.

さらに、第1実施例の熱交換器20によれば、コルゲートフィン40の水平面42に形成された複数の波形凹凸を、第1の熱交換用流体(例えば空気)の入口側の波の振幅が出口側の波の振幅より大きくなるように形成することにより、第1の熱交換用流体の流れに対する流動抵抗を小さくすることができる。    Furthermore, according to the heat exchanger 20 of the first embodiment, the wave amplitude on the inlet side of the first heat exchange fluid (for example, air) is changed between the plurality of waveform irregularities formed on the horizontal surface 42 of the corrugated fin 40. By forming it so as to be larger than the amplitude of the wave on the outlet side, the flow resistance to the flow of the first heat exchange fluid can be reduced.

第1実施例の熱交換器20では、コルゲートフィン40の水平面42に形成された複数の波形凹凸を、水平面42の一方の面における凸部の形状と同面における凹部の形状とが表裏一体となるように形成するものとしたが、水平面42の一方の面における凸部の形状と同面における凹部の形状とが異なるものとなるように形成するものとしてもよい。例えば、複数の波形凹凸を、頂部線43については屈曲部位43aの高さが斜線部位43bの高さより高くなるように形成するが、底部線44については屈曲部位44aの深さが斜線部位44bの深さと同じになるよう形成するものとしたり、逆に、底部線44については屈曲部位44aの深さが斜線部位44bの深さより深くなるように形成するが、頂部線43については屈曲部位43aの高さが斜線部位43bの高さと同じになるよう形成するものとしたりしてもよい。    In the heat exchanger 20 of the first embodiment, the plurality of corrugated irregularities formed on the horizontal surface 42 of the corrugated fin 40 are formed so that the shape of the convex portion on one surface of the horizontal surface 42 and the shape of the concave portion on the same surface are integrated. However, the shape of the convex portion on one surface of the horizontal surface 42 may be different from the shape of the concave portion on the same surface. For example, the plurality of corrugations are formed so that the height of the bent portion 43a is higher than the height of the shaded portion 43b with respect to the top line 43, but the depth of the bent portion 44a is the height of the shaded portion 44b with respect to the bottom line 44. The bottom line 44 is formed so that the bent part 44a is deeper than the hatched part 44b, whereas the top line 43 is formed with the bent part 43a. The height may be the same as the height of the hatched portion 43b.

第1実施例の熱交換器20では、コルゲートフィン40の水平面42に形成された複数の波形凹凸を、頂部線43の屈曲部位43aがコルゲートフィン40の水平面42の端部近傍に位置するように形成するものとしたが、頂部線43の屈曲部位43aがコルゲートフィン40の水平面42の端部近傍に位置しないように形成するものとしても構わない。    In the heat exchanger 20 of the first embodiment, a plurality of corrugated irregularities formed on the horizontal surface 42 of the corrugated fin 40 are arranged such that the bent portion 43a of the top line 43 is positioned near the end of the horizontal surface 42 of the corrugated fin 40. Although formed, the bent portion 43 a of the top line 43 may be formed so as not to be positioned in the vicinity of the end of the horizontal surface 42 of the corrugated fin 40.

第1実施例の熱交換器20では、コルゲートフィン40の水平面42に形成された複数の波形凹凸を、第1の熱交換用流体の入口側の波の振幅が出口側の波の振幅より大きくなるように形成するものとしたが、第1の熱交換用流体の入口側の波の振幅も出口側の波の振幅も同じになるように形成するものとしてもよい。    In the heat exchanger 20 of the first embodiment, the plurality of corrugated irregularities formed on the horizontal surface 42 of the corrugated fins 40 are such that the amplitude of the wave on the inlet side of the first heat exchange fluid is larger than the amplitude of the wave on the outlet side. However, it may be formed such that the amplitude of the wave on the inlet side and the amplitude of the wave on the outlet side of the first heat exchange fluid are the same.

第1実施例の熱交換器20では、コルゲートフィン40の水平面42に形成された複数の波形凹凸を、頂部線43や底部線44がV字状に複数回に亘って連続して繰り返すように形成するものとしたが、頂部線43や底部線44がV字状に2回だけ連続してW字状になるように形成するものとしてもよいし、頂部線43や底部線44が単一のV字の形状になるよう形成するものとしてもよい。    In the heat exchanger 20 of the first embodiment, the plurality of corrugated irregularities formed on the horizontal surface 42 of the corrugated fin 40 are repeated so that the top line 43 and the bottom line 44 are continuously V-shaped multiple times. The top line 43 and the bottom line 44 may be formed so as to be continuously W-shaped twice in a V shape, or the top line 43 and the bottom line 44 are single. It may be formed so as to have a V shape.

第1実施例の熱交換器20では、コルゲートフィン40の水平面42に形成された複数の波形凹凸を、頂部線43における斜線部位43bと底部線44における斜線部位44bがS字カーブとなるように形成するものとしたが、頂部線43における斜線部位43bと底部線44における斜線部位44bがS字カーブを描く必要はなく、第1の熱交換用流体の流れに対して凸となる形状や凹となる形状としてもよいし、直線となる形状としてもよい。    In the heat exchanger 20 of the first embodiment, a plurality of corrugated irregularities formed on the horizontal surface 42 of the corrugated fin 40 are formed so that the oblique line portion 43b in the top line 43 and the oblique line portion 44b in the bottom line 44 have an S-shaped curve. However, it is not necessary for the hatched portion 43b in the top line 43 and the hatched portion 44b in the bottom line 44 to form an S-curve, and the shape or recess that is convex with respect to the flow of the first heat exchange fluid. The shape may be a straight line or a straight line.

第1実施例の熱交換器20では、コルゲートフィン40の水平面42に形成された複数の波形凹凸を、滑らかな曲面により、波の頂部を連ねた頂部線43や波の底部を連ねた底部線44と第1の熱交換用流体の主要な流れとのなす角γが鋭角の範囲の角度となるように、頂部線43や底部線44がV字状に複数回に亘って連続して繰り返すように、頂部線43におけるV字の斜線部位43bと第1の熱交換用流体の主要な流れとのなす角の平均としての第1の平均角度が、波形凹凸における平均高さとなる中間部が連続する中間部線45におけるV字の斜線部位45bと第1の熱交換用流体の主要な流れとのなす角の平均としての第2の平均角度より小さくなるように形成するものとしたが、更に、頂部線における屈曲部位の高さが頂部線におけるV字の斜線部位の高さより高くなるように形成するものとしてもよい。図10に変形例の波形凹凸を立体的に示す。図10の変形例の波形凹凸は、図4の第1実施例の波形凹凸と比較して、頂部線53の屈曲部位53aについては第1実施例の頂部線43の屈曲部位43aを若干隆起した形状として、頂部線53の斜線部位53bについては第1実施例の頂部線43の斜線部位43bを若干つぶした形状として得ることができる。図11は、図10の波形凹凸の頂部線53に沿ったA−A断面であり、頂部線53の波形凹凸の平均高さとなる中心位置からの高さも示している。図示するように、V字状の頂部線53の屈曲部位53aは、中心位置からの高さHuaが斜線部位53bの中心位置からの高さHubより高くなるように形成されている。このように、頂部線53の屈曲部位53aについては第1実施例の頂部線43の屈曲部位43aを若干隆起した形状とし、頂部線53の斜線部位53bについては第1実施例の頂部線43の斜線部位43bを若干つぶした形状とするのは、図9を用いて説明したように、局所熱流速が大きな部位の形状を強調すると共に局所せん断応力が大きな部位の形状を緩和するためである。即ち、局所熱流速が大きな部位である頂部線53の屈曲頂部53aの高さを高くすることにより伝熱促進を高くし、局所せん断応力が大きな頂部線53の傾斜部位53bの高さを低くすることにより流動抵抗を小さくすることができる。なお、図10には、頂部線53の形状を説明するために底部線54の形状については示さないものとしたが、変形例の波形凹凸は、頂部線53の形状と底部線54の形状とが表裏一体のものとなっている。したがって、頂部線53における屈曲部位53aの高さが頂部線53におけるV字の斜線部位53bの高さより高くなるように形成されているのと同様に、底部線54における屈曲部位54aの深さが頂部線53におけるV字の斜線部位53bの深さより深くなるように形成されている。図12は、図10のC−C断面に相当する変形例の波形凹凸の断面図であり、図13、図10のD−D断面に相当する変形例の波形凹凸の断面図である。図12および図13に示すように、変形例の波形凹凸は、頂部線53の屈曲部位53aの高さHuaが頂部線53の傾斜部位53bの高さHubより高くなるように、底部線54の屈曲部位54aの深さHdaが底部線54の傾斜部位53bの深さHdbより深くなるように、頂部線53の屈曲部位53aの高さHuaと底部線54の屈曲部位54aの深さHdaとが一致するように、頂部線53の傾斜部位53bの高さHubと底部線54の傾斜部位53bの深さHdbとが一致するように、形成されている。これにより、コルゲートフィン40の水平面42の一方の面側に流れる第1の熱交換用流体との熱交換と水平面42の他方の面側に流れる第1の熱交換用流体との熱交換とを同様に行なうことができ、伝熱促進がより高く流動抵抗のより小さな熱交換器とすることができる。    In the heat exchanger 20 of the first embodiment, a plurality of corrugated irregularities formed on the horizontal surface 42 of the corrugated fin 40 are formed by a smooth curved surface, and a top line 43 connecting the wave tops and a bottom line connecting the wave bottoms. The top line 43 and the bottom line 44 are continuously repeated in a V shape a plurality of times so that the angle γ formed between the main flow of the first heat exchange fluid and the angle 44 is an acute angle. As described above, the first average angle as the average of the angle formed between the V-shaped oblique line portion 43b in the top line 43 and the main flow of the first heat exchange fluid is an intermediate portion where the average height in the corrugated unevenness is Although the intermediate portion 45 is formed so as to be smaller than the second average angle as an average of the angle formed by the V-shaped oblique portion 45b in the continuous intermediate line 45 and the main flow of the first heat exchange fluid, Furthermore, the height of the bent part in the top line is the top line. Or as forming it takes to be higher than the height of the hatched portion of the V-shape. FIG. 10 three-dimensionally shows the waveform irregularities of the modification. Compared with the corrugated unevenness of the first embodiment of FIG. 4, the corrugated unevenness of the modification of FIG. 10 slightly raised the bent portion 43a of the top line 43 of the first embodiment with respect to the bent portion 53a of the top line 53. As the shape, the hatched portion 53b of the top line 53 can be obtained as a slightly collapsed shape of the hatched portion 43b of the top line 43 of the first embodiment. FIG. 11 is an AA cross section along the top line 53 of the corrugated unevenness of FIG. 10, and also shows the height from the center position that is the average height of the corrugated unevenness of the top line 53. As illustrated, the bent portion 53a of the V-shaped top line 53 is formed such that the height Hua from the center position is higher than the height Hub from the center position of the hatched portion 53b. As described above, the bent portion 53a of the top line 53 has a slightly raised shape in the bent portion 43a of the top line 43 of the first embodiment, and the oblique portion 53b of the top line 53 has a shape of the top line 43 of the first embodiment. The reason why the hatched portion 43b is slightly crushed is to emphasize the shape of the portion where the local heat flow rate is large and relax the shape of the portion where the local shear stress is large, as described with reference to FIG. That is, by increasing the height of the bent top portion 53a of the top line 53 where the local heat flow rate is large, the heat transfer acceleration is increased, and the height of the inclined portion 53b of the top line 53 having a large local shear stress is decreased. As a result, the flow resistance can be reduced. In FIG. 10, the shape of the bottom line 54 is not shown in order to explain the shape of the top line 53, but the waveform irregularities of the modified example are the shape of the top line 53 and the shape of the bottom line 54. Is an integrated front and back. Accordingly, the depth of the bent portion 54a in the bottom line 54 is the same as that in which the height of the bent portion 53a in the top line 53 is higher than the height of the V-shaped hatched portion 53b in the top line 53. The top line 53 is formed so as to be deeper than the depth of the V-shaped oblique line part 53b. 12 is a cross-sectional view of the corrugated irregularities of the modified example corresponding to the CC cross section of FIG. 10, and is a sectional view of the corrugated irregularities of the modified example corresponding to the DD cross section of FIGS. As shown in FIG. 12 and FIG. 13, the corrugated unevenness of the modified example is such that the height Hua of the bent portion 53 a of the top line 53 is higher than the height Hub of the inclined portion 53 b of the top line 53. The height Hua of the bent portion 53a of the top line 53 and the depth Hda of the bent portion 54a of the bottom line 54 are set so that the depth Hda of the bent portion 54a is deeper than the depth Hdb of the inclined portion 53b of the bottom line 54. The height Hub of the inclined portion 53b of the top line 53 and the depth Hdb of the inclined portion 53b of the bottom line 54 are formed so as to match. Thus, heat exchange with the first heat exchange fluid flowing on one surface side of the horizontal surface 42 of the corrugated fin 40 and heat exchange with the first heat exchange fluid flowing on the other surface side of the horizontal surface 42 are performed. This can be done in the same manner, and a heat exchanger with higher heat transfer and lower flow resistance can be obtained.

こうした変形例の波形凹凸でも、頂部線53の屈曲部位53aがコルゲートフィン40の水平面42の端部近傍に位置するように形成するものとしてもよいし、第1の熱交換用流体の入口側の波の振幅が出口側の波の振幅より大きくなるように形成するものとしてもよいし、頂部線53や底部線54がV字状に2回だけ連続してW字状になるように形成するものとしてもよいし、頂部線53や底部線54が単一のV字の形状になるよう形成するものとしてもよいし、水平面42の一方の面における凸部の形状と同面における凹部の形状とが異なるものとなるように形成するものとしてもよい。    Even in the corrugated unevenness of such a modified example, the bent portion 53a of the top line 53 may be formed in the vicinity of the end of the horizontal surface 42 of the corrugated fin 40, or on the inlet side of the first heat exchange fluid. It is good also as what forms so that the amplitude of a wave may become larger than the amplitude of the wave of an exit side, and forms so that the top line 53 and the bottom line 54 may become W shape continuously in a V shape only twice. The top line 53 and the bottom line 54 may be formed into a single V-shape, or the shape of the concave portion on the same surface as the shape of the convex portion on one surface of the horizontal surface 42. It is good also as what forms so that it may become different.

図14は本発明の第2実施例としての熱交換器120の外観を示す外観図であり、図15は第2実施例の熱交換器120に用いられる熱交換用チューブ130の扁平面を示す説明図である。第2実施例の熱交換器120は、図示するように、偏平な中空管として形成され並列に配置された複数の熱交換用チューブ130と、この複数の熱交換用チューブ130の端部を覆うように取り付けられて複数の熱交換用チューブ30に熱交換流体を流出入する一対のヘッダー140,150とにより構成されている。    FIG. 14 is an external view showing the external appearance of the heat exchanger 120 as the second embodiment of the present invention, and FIG. 15 shows the flat surface of the heat exchange tube 130 used in the heat exchanger 120 of the second embodiment. It is explanatory drawing. As shown in the drawing, the heat exchanger 120 of the second embodiment includes a plurality of heat exchange tubes 130 that are formed as flat hollow tubes and arranged in parallel, and ends of the plurality of heat exchange tubes 130. A pair of headers 140 and 150 are attached so as to cover and flow heat exchange fluid into and out of the plurality of heat exchange tubes 30.

熱交換用チューブ130は、熱伝導性を有する材料、例えば、ステンレス材料により厚みが0.1mmに形成された板材をプレス加工及び折り曲げ加工等を用いて、厚み0.5mmの偏平な管状に形成されている。熱交換用チューブ130の偏平面(正面および裏面)の外壁面側には、滑らかな曲面により複数の波形凹凸が形成されている。第2実施例の複数の波形凹凸は、第1実施例のコルゲートフィン40の水平面42に形成された複数の波形凹凸と同様に、波の頂部を連ねた頂部線143や波の底部を連ねた底部線144と第1の熱交換用流体(例えば、空気)の主要な流れとのなす角γが鋭角の範囲の角度(第2実施例では約30度)となるように、頂部線143および底部線144がV字状に複数回に亘って連続して繰り返すように、頂部線143におけるV字の斜線部位143bと第1の熱交換用流体の主要な流れとのなす角の平均としての第1の平均角度が、波形凹凸における平均高さとなる中間部が連続する中間部線145におけるV字の斜線部位145bと第1の熱交換用流体の主要な流れとのなす角の平均としての第2の平均角度より小さくなるように、頂部線143の屈曲部位143aが扁平面の端部近傍に位置するように、第1の熱交換用流体(空気)の入口側の波の振幅が出口側の波の振幅より大きくなるように、形成されている。    The heat exchanging tube 130 is formed into a flat tube having a thickness of 0.5 mm by using a plate having a thickness of 0.1 mm made of a material having thermal conductivity, such as a stainless material, by pressing or bending. Has been. On the outer wall surface side of the flat surfaces (front and back surfaces) of the heat exchange tube 130, a plurality of corrugated irregularities are formed by a smooth curved surface. The plurality of corrugated irregularities of the second embodiment are connected to the top line 143 that connects the tops of the waves and the bottom of the waves, similarly to the plurality of corrugated irregularities formed on the horizontal surface 42 of the corrugated fin 40 of the first embodiment. The top wire 143 and the top wire 143 so that the angle γ between the bottom wire 144 and the main flow of the first heat exchange fluid (eg, air) is an acute angle (about 30 degrees in the second embodiment). As the average of the angle formed by the V-shaped hatched portion 143b in the top line 143 and the main flow of the first heat exchange fluid so that the bottom line 144 repeats continuously in a V-shape a plurality of times. The first average angle is an average of the angles formed by the V-shaped oblique line portion 145b in the intermediate line 145 and the main flow of the first heat exchange fluid in the intermediate part line 145 where the intermediate part is the average height of the corrugated irregularities. The top to be smaller than the second average angle It is formed so that the amplitude of the wave on the inlet side of the first heat exchange fluid (air) is larger than the amplitude of the wave on the outlet side so that the bent portion 143a of 143 is positioned in the vicinity of the end of the flat surface. ing.

第2実施例の複数の波形凹凸が、滑らかな曲面により、頂部線143や底部線144と第1の熱交換用流体(空気)の主要な流れとのなす角γが鋭角の範囲の角度となるように、頂部線143や底部線144がV字状に複数回に亘って連続して繰り返すように、頂部線143の斜線部位143bと第1の熱交換用流体の主要な流れとのなす角の平均(第1の平均角度)が中間部線145の斜線部位145bと第1の熱交換用流体の主要な流れとのなす角の平均(第2の平均角度)より小さくなるように形成されている理由や、第2実施例の複数の波形凹凸が頂部線143の屈曲部位143aが扁平面の端部近傍に位置するように形成されている理由、第2実施例の複数の波形凹凸が第1の熱交換用流体(空気)の入口側の波の振幅が出口側の波の振幅より大きくなるように形成されている理由は、第1実施例の波形凹凸と同様である。    The plurality of corrugations of the second embodiment are smooth curved surfaces, and the angle γ between the top line 143 and the bottom line 144 and the main flow of the first heat exchange fluid (air) is an acute angle range. As shown, the oblique line 143b of the top line 143 and the main flow of the first heat exchange fluid are formed so that the top line 143 and the bottom line 144 are continuously repeated in a V shape over a plurality of times. The average angle (first average angle) is formed to be smaller than the average angle (second average angle) formed by the hatched portion 145b of the intermediate portion line 145 and the main flow of the first heat exchange fluid. The reason is that the plurality of corrugations of the second embodiment are formed such that the bent portion 143a of the top line 143 is located near the end of the flat surface, the plurality of corrugations of the second embodiment Is the amplitude of the wave on the inlet side of the first heat exchange fluid (air) Reason is formed as larger than the amplitude is the same as the waveform irregularity of the first embodiment.

以上説明した第2実施例の熱交換器120によれば、熱交換用チューブ130の扁平面の外壁面側に形成された複数の波形凹凸を、滑らかな曲面により、波の頂部を連ねた頂部線143や波の底部を連ねた底部線144と第1の熱交換用流体(空気)の主要な流れとのなす角γが鋭角の範囲の角度となるように、頂部線143や底部線144がV字状に複数回に亘って連続して繰り返すように、頂部線143の斜線部位143bと第1の熱交換用流体の主要な流れとのなす角の平均(第1の平均角度)が中間部線145の斜線部位145bと第1の熱交換用流体の主要な流れとのなす角の平均(第2の平均角度)より小さくなるように形成することにより、剥離や局所的な増速を抑えて伝熱促進に有効な空気の二次流れを有効に発生させることができ、局所熱流速の大きな部位を強調して伝熱促進を図り、局所せん断応力の大きな部位のせん断応力を小さくして第1の熱交換用流体の流れに対する流動抵抗を小さくすることができる。これらの結果、伝熱促進がより高く流動抵抗のより小さな熱交換器とすることができる。    According to the heat exchanger 120 of the second embodiment described above, a plurality of corrugated irregularities formed on the flat outer wall surface side of the heat exchanging tube 130 are connected to the top of the wave by a smooth curved surface. The top line 143 and the bottom line 144 are such that the angle γ between the line 143 and the bottom line 144 connecting the bottoms of the waves and the main flow of the first heat exchange fluid (air) is an acute angle. Of the angle formed by the oblique portion 143b of the top line 143 and the main flow of the first heat exchanging fluid so as to continuously repeat a plurality of times in a V shape (first average angle). By forming the intermediate portion 145 so as to be smaller than the average angle (second average angle) between the oblique line portion 145b of the intermediate line 145 and the main flow of the first heat exchange fluid, peeling or local acceleration is achieved. It is possible to effectively generate a secondary flow of air that is effective for heat transfer and It is possible to enhance the heat transfer by emphasizing the part where the local heat flow rate is large, and to reduce the shear resistance at the part where the local shear stress is large to reduce the flow resistance against the flow of the first heat exchange fluid. . As a result, a heat exchanger with higher heat transfer promotion and lower flow resistance can be obtained.

しかも、第2実施例の熱交換器120によれば、熱交換用チューブ130の扁平面の外壁面側に形成された複数の波形凹凸を、頂部線143の屈曲部位143aが扁平面の端部近傍に位置するように形成することにより、局所熱流速が高い部位である頂部線143の屈曲部位143aを扁平面により多く形成することができ、伝熱促進がより高い熱交換器とすることができる。    Moreover, according to the heat exchanger 120 of the second embodiment, the plurality of corrugated irregularities formed on the outer wall surface side of the flat surface of the heat exchanging tube 130 are the end portions where the bent portions 143a of the top line 143 are flat surfaces. By forming so that it may be located in the vicinity, the bending part 143a of the top line 143 which is a site | part with a high local heat flow rate can be formed more by a flat surface, and it is set as a heat exchanger with higher heat-transfer promotion. it can.

また、第2実施例の熱交換器120によれば、熱交換用チューブ130の扁平面の外壁面側に形成された複数の波形凹凸を、第1の熱交換用流体(例えば空気)の入口側の波の振幅が出口側の波の振幅より大きくなるように形成することにより、第1の熱交換用流体の流れに対する流動抵抗を小さくすることができる。    Further, according to the heat exchanger 120 of the second embodiment, the plurality of corrugated irregularities formed on the outer wall surface side of the flat surface of the heat exchanging tube 130 are replaced with the inlet of the first heat exchanging fluid (for example, air). By forming the side wave so that the amplitude of the wave on the side is larger than the amplitude of the wave on the outlet side, the flow resistance to the flow of the first heat exchange fluid can be reduced.

第2実施例の熱交換器120では、熱交換用チューブ130の扁平面の外壁面側に形成された複数の波形凹凸を、頂部線143の屈曲部位143aが扁平面の端部近傍に位置するように形成するものとしたが、頂部線143の屈曲部位143aが扁平面の端部近傍に位置しないように形成するものとしても構わない。    In the heat exchanger 120 of the second embodiment, a plurality of corrugated irregularities formed on the outer flat wall surface side of the heat exchanging tube 130 are arranged such that the bent portion 143a of the top line 143 is located near the end of the flat surface. However, the bent portion 143a of the top line 143 may be formed so as not to be positioned near the end portion of the flat surface.

第2実施例の熱交換器120では、熱交換用チューブ130の扁平面の外壁面側に形成された複数の波形凹凸を、第1の熱交換用流体の入口側の波の振幅が出口側の波の振幅より大きくなるように形成するものとしたが、第1の熱交換用流体の入口側の波の振幅も出口側の波の振幅も同じになるように形成するものとしてもよい。    In the heat exchanger 120 of the second embodiment, a plurality of corrugations formed on the flat outer wall surface side of the heat exchanging tube 130 has a wave amplitude on the inlet side of the first heat exchanging fluid. However, it may be formed such that the amplitude of the wave on the inlet side and the amplitude of the wave on the outlet side of the first heat exchange fluid are the same.

第2実施例の熱交換器120では、熱交換用チューブ130の扁平面の外壁面側に形成された複数の波形凹凸を、頂部線143や底部線144がV字状に複数回に亘って連続して繰り返すように形成するものとしたが、頂部線143や底部線144がV字状に2回だけ連続してW字状になるように形成するものとしてもよいし、頂部線143や底部線144が単一のV字の形状になるよう形成するものとしてもよい。    In the heat exchanger 120 of the second embodiment, a plurality of corrugated irregularities formed on the outer wall surface side of the flat surface of the heat exchange tube 130 are formed a plurality of times so that the top line 143 and the bottom line 144 are V-shaped. The top line 143 and the bottom line 144 may be formed so as to be continuously W-shaped twice in a V shape, or the top line 143 and the bottom line 144 may be formed continuously. The bottom line 144 may be formed in a single V shape.

第1実施例の熱交換器20では、熱交換用チューブ130の扁平面の外壁面側に形成された複数の波形凹凸を、滑らかな曲面により、波の頂部を連ねた頂部線143や波の底部を連ねた底部線144と第1の熱交換用流体の主要な流れとのなす角γが鋭角の範囲の角度となるように、頂部線143および底部線144がV字状に複数回に亘って連続して繰り返すように、頂部線143の斜線部位143bと第1の熱交換用流体の主要な流れとのなす角の平均(第1の平均角度)が中間部線145の斜線部位145bと第1の熱交換用流体の主要な流れとのなす角の平均(第2の平均角度)より小さくなるように形成するものとしたが、更に、頂部線における屈曲部位の高さが頂部線におけるV字の斜線部位の高さより高くなるように形成するものとしてもよい。即ち、熱交換用チューブ130の扁平面の外壁面側に形成された複数の波形凹凸を、図10に例示した変形例の波形凹凸の形状としてもよい。    In the heat exchanger 20 of the first embodiment, a plurality of corrugated irregularities formed on the flat outer wall surface side of the heat exchanging tube 130 are formed by a smooth curved surface with a top line 143 connecting the wave tops and The top wire 143 and the bottom wire 144 are V-shaped multiple times so that the angle γ formed by the bottom wire 144 connecting the bottom and the main flow of the first heat exchange fluid is an acute angle. The average angle (first average angle) formed between the hatched portion 143b of the top line 143 and the main flow of the first heat exchange fluid is the hatched portion 145b of the intermediate line 145 so as to be continuously repeated. And the main flow of the first heat exchange fluid is formed so as to be smaller than the average angle (second average angle), but the height of the bent portion in the top line is further the top line. It is formed so as to be higher than the height of the shaded portion of the V shape in It may be used as the. That is, a plurality of corrugated irregularities formed on the outer wall surface side of the flat surface of the heat exchanging tube 130 may be the corrugated irregularities of the modification illustrated in FIG.

以上、本発明を実施するための形態について第1実施例および第2実施例を用いて説明したが、本発明はこうした実施例に何等限定されるものではなく、本発明の要旨を逸脱しない範囲内において、種々なる形態で実施し得ることは勿論である。    As mentioned above, although the form for implementing this invention was demonstrated using 1st Example and 2nd Example, this invention is not limited to these Examples at all, and the range which does not deviate from the summary of this invention Of course, it can be implemented in various forms.

本発明は、熱交換器の製造産業などに利用可能である。

The present invention can be used in the heat exchanger manufacturing industry and the like.

Claims (7)

伝熱部材の表面に滑らかな曲面を用いて断面が波形で波の頂部が連続する頂部線と波の底部が連続する底部線とがV字形状となるよう複数の波形凹凸が形成されており、前記複数の波形凹凸に対して第1の熱交換用流体をV字形状における上下方向に流して熱交換する熱交換器において、
前記複数の波形凹凸は、前記頂部線におけるV字の傾斜部位と前記第1の熱交換用流体の主要な流れとのなす角の平均としての第1の平均角度が、頂部と底部との中間となる中間部が連続する中間部線におけるV字の傾斜部位と前記第1の熱交換用流体の主要な流れとのなす角の平均としての第2の平均角度より小さくなるよう形成されている、
ことを特徴とする熱交換器。
Using a smooth curved surface on the surface of the heat transfer member, a plurality of corrugations are formed so that the top line where the cross section is corrugated and the top of the wave is continuous and the bottom line where the bottom of the wave is continuous are V-shaped. In the heat exchanger for exchanging heat by flowing the first heat exchanging fluid in the vertical direction in the V shape with respect to the plurality of corrugated irregularities,
In the plurality of corrugations, a first average angle as an average of an angle formed between a V-shaped inclined portion of the top line and the main flow of the first heat exchange fluid is intermediate between the top and the bottom. The intermediate portion is formed so as to be smaller than a second average angle as an average of an angle formed by the V-shaped inclined portion in the continuous intermediate portion line and the main flow of the first heat exchange fluid. ,
A heat exchanger characterized by that.
請求項1記載の熱交換器であって、
前記熱交換器は、コルゲートフィン型熱交換器であり、
前記伝熱部材は、コルゲートフィンであり、
前記波形凹凸は、頂部と底部とが対称となるよう形成されている、
ことを特徴とする熱交換器。
The heat exchanger according to claim 1,
The heat exchanger is a corrugated fin heat exchanger,
The heat transfer member is a corrugated fin,
The corrugated irregularities are formed such that the top and bottom are symmetrical.
A heat exchanger characterized by that.
請求項1または2記載の熱交換器であって、
前記伝熱部材は、前記第1の熱交換用流体と熱交換する第2の熱交換用流体の流路を形成する扁平な複数のチューブであり、
前記チューブの扁平な外表面に前記波形凹凸が形成されている、
ことを特徴とする熱交換器。
The heat exchanger according to claim 1 or 2,
The heat transfer member is a plurality of flat tubes that form flow paths for a second heat exchange fluid that exchanges heat with the first heat exchange fluid;
The corrugated irregularities are formed on the flat outer surface of the tube,
A heat exchanger characterized by that.
請求項1ないし3のうちのいずれか1つの請求項に記載の熱交換器であって、
前記複数の波形凹凸は、前記第1の熱交換用流体の上流側に位置する波形凹凸の波形における振幅が前記第1の熱交換用流体の上流側に位置する波形凹凸の波形における振幅より大きくなるよう形成されている、
ことを特徴とする熱交換器。
The heat exchanger according to any one of claims 1 to 3,
In the plurality of corrugations, the amplitude of the corrugations on the upstream side of the first heat exchange fluid is larger than the amplitude of the corrugations on the upstream side of the first heat exchange fluid. Formed to be,
A heat exchanger characterized by that.
請求項1ないし4のうちのいずれか1つの請求項に記載の熱交換器であって、
前記複数の波形凹凸の前記頂部線および前記底部線は、V字が複数回に亘って連続して繰り返されるよう形成されている、
ことを特徴とする熱交換器。
A heat exchanger according to any one of claims 1 to 4, wherein
The top line and the bottom line of the plurality of corrugated irregularities are formed such that a V-shape is repeated continuously over a plurality of times.
A heat exchanger characterized by that.
請求項5記載の熱交換器であって、
前記複数の波形凹凸は、前記頂部線の屈曲部位が前記伝熱部材の端部近傍に位置するよう形成されている、
ことを特徴とする熱交換器。
The heat exchanger according to claim 5,
The plurality of corrugations are formed such that the bent portion of the top line is located near the end of the heat transfer member,
A heat exchanger characterized by that.
請求項1ないし6のうちのいずれか1つの請求項に記載の熱交換器であって、
前記複数の波形凹凸は、前記頂部線の屈曲部位における頂部の高さが前記頂部線の屈曲部位とは異なる部位における頂部の高さより高くなるよう形成されている、
ことを特徴とする熱交換器。

The heat exchanger according to any one of claims 1 to 6,
The plurality of corrugated irregularities are formed such that the height of the top at the bent portion of the top line is higher than the height of the top at a portion different from the bent portion of the top line.
A heat exchanger characterized by that.

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