JPH0435732Y2 - - Google Patents

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Publication number
JPH0435732Y2
JPH0435732Y2 JP1986102365U JP10236586U JPH0435732Y2 JP H0435732 Y2 JPH0435732 Y2 JP H0435732Y2 JP 1986102365 U JP1986102365 U JP 1986102365U JP 10236586 U JP10236586 U JP 10236586U JP H0435732 Y2 JPH0435732 Y2 JP H0435732Y2
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JP
Japan
Prior art keywords
heat transfer
protrusion
protrusion element
protruding
passage
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Expired
Application number
JP1986102365U
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Japanese (ja)
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JPS6312085U (en
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Priority to JP1986102365U priority Critical patent/JPH0435732Y2/ja
Publication of JPS6312085U publication Critical patent/JPS6312085U/ja
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Publication of JPH0435732Y2 publication Critical patent/JPH0435732Y2/ja
Expired legal-status Critical Current

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Description

【考案の詳細な説明】 (産業上の利用分野) 本考案は、略板状のエレメントを積層した熱交
換器に関するものである。
[Detailed Description of the Invention] (Industrial Application Field) The present invention relates to a heat exchanger in which substantially plate-shaped elements are laminated.

(従来技術及びその問題点) この種の熱交換器に関して従来から例えば実公
昭50−15641号、特開昭52−41946号が知られてい
る。この従来例では、波板状のエレメントを複数
枚積層して、エレメントの間に通路を形成してあ
る。また、平板状のエレメントに針状の突起を形
成して、通路を流れる気流の流れを乱して伝熱効
率を向上させるようにした従来例も知られてい
る。
(Prior Art and its Problems) This type of heat exchanger is known from the prior art, for example, in Japanese Utility Model Publication No. 15641/1983 and Japanese Patent Application Laid-open No. 41946/1983. In this conventional example, a plurality of corrugated elements are laminated to form passages between the elements. Furthermore, a conventional example is known in which needle-like protrusions are formed on a flat element to disrupt the flow of air flowing through a passage and improve heat transfer efficiency.

しかしながら、以上の従来例では総括伝熱係数
(U値)の向上に余地が残されており、熱交換効
率の点で充分ではなく、更に熱交換効率を向上さ
せた熱交換器が要望されている。
However, the above conventional examples leave room for improvement in the overall heat transfer coefficient (U value) and are not sufficient in terms of heat exchange efficiency, and there is a need for a heat exchanger with further improved heat exchange efficiency. There is.

(考案の目的) 本考案は、略板状のエレメントを積層した熱交
換器において、一層熱交換効率を向上させること
ができる熱交換器を提供することを目的としてい
る。
(Purpose of the invention) The object of the invention is to provide a heat exchanger in which substantially plate-shaped elements are laminated, which can further improve heat exchange efficiency.

(考案の構成) (1) 技術的手段 本考案は、長方形の山及び谷がプレス成形され
て格子状に凹凸のある波形プレート状のエレメン
ト10が通路14,16をへだてて複数枚積層さ
れた熱交換器であつて、上記の山及び谷は横向き
に長い長方形の第1の突起素子18aの4個が千
鳥状に配置されて一方へ突出し、その中央にそれ
らと90度向きの異なる縦向きに長い長方形の第2
の突起素子18bが他方へ突出する姿勢で配置さ
れたものの組合せからなり、上記の山となる第1
の突起素子18aは突出方向に急角度に傾斜した
上流側部分20とそれに続き逆方向に緩やかに傾
斜した下流側部分22とが頂上で滑らかに連続し
ており、上記第2の突起素子18bは上記第1の
突起素子18aと突出方向のみが異なる同一形状
を備え、各エレメント10の9方の通路14では
第1の流体が第1突起素子18aの上流側部分2
0から下流側部分22をへて略台形断面をなす第
2突起素子18b部分へと横方向へ流れ、他方の
通路16では第2の流体が第2突起素子18bの
上流側部分から下流側部分をへて略台形断面をな
す第1突起素子部分へと縦方向へ流れるように構
成したことを特徴とする熱交換器である。
(Structure of the invention) (1) Technical means The present invention consists of a plurality of corrugated plate-like elements 10 having rectangular peaks and valleys press-formed and having irregularities in a lattice pattern, separated by passages 14 and 16, and laminated. In the heat exchanger, the above-mentioned peaks and valleys are formed by four horizontally long rectangular first projecting elements 18a arranged in a staggered manner and protruding to one side, and in the center of which is a vertically extending element 18a that is 90 degrees different from the first protruding elements 18a. the second long rectangle
The first protrusion element 18b is arranged in such a manner that it protrudes toward the other, and the first
The protrusion element 18a has an upstream portion 20 steeply inclined in the protruding direction and a downstream portion 22 gently inclined in the opposite direction, which are smoothly continuous at the top, and the second protrusion element 18b is It has the same shape as the first protrusion element 18a, differing only in the protrusion direction, and in the nine-way passage 14 of each element 10, the first fluid flows into the upstream portion 2 of the first protrusion element 18a.
0 through the downstream portion 22 to the second projection element 18b portion having a substantially trapezoidal cross section, and in the other passage 16, the second fluid flows from the upstream portion to the downstream portion of the second projection element 18b. The heat exchanger is characterized in that the heat exchanger is configured to flow vertically through the first projection element portion having a substantially trapezoidal cross section.

(2) 作用 傾斜角度が急な突起素子の上流側部分に気流を
衝突させて気流の流れを乱し、熱伝達率の高い乱
流熱伝達域を形成し、突起素子の下流側部分で気
流を滑かに次の突起素子に導き、再び乱流熱伝達
域を形成して、熱交換効率を向上させる。
(2) Effect The airflow impinges on the upstream part of the protruding element with a steep inclination angle to disturb the airflow, forming a turbulent heat transfer region with a high heat transfer coefficient, and reducing the airflow in the downstream part of the protruding element. smoothly leads to the next protrusion element, forming a turbulent heat transfer zone again to improve heat exchange efficiency.

(実施例) 本考案を採用した熱交換器を示す第1図におい
て、10は略板状のエレメントである。エレメン
ト10の平面形状は、略正方形をなしている。こ
のエレメント10は第1A図に示すように上下縁
部と左右縁部を交互に衝合し、溶接部12を溶接
して組立てられている。したがつて、互いに隣接
するエレメント10の間に通路14,16が形成
されている。
(Example) In FIG. 1 showing a heat exchanger employing the present invention, 10 is a substantially plate-shaped element. The planar shape of the element 10 is approximately square. As shown in FIG. 1A, this element 10 is assembled by alternately abutting the upper and lower edges and the left and right edges and welding the welded portions 12 together. Passages 14, 16 are thus formed between mutually adjacent elements 10.

第2図に示すように、通路14には矢印Xに沿
つて例えば高温の空気が横方向に流れ、通路16
には矢印Y方向に例えば低温の空気が縦方向に流
通し、熱交換するようになつている。
As shown in FIG. 2, for example, high-temperature air flows laterally in the passage 14 along the arrow X, and the passage 16
For example, low-temperature air flows vertically in the direction of arrow Y to exchange heat.

次に、エレメント10のより詳細な構造を示す
第3図で、18a,18bは夫々突起素子であ
る。突起素子18aは矢印X方向に流れる気流に
対応したものであり、突起素子18bは矢印Y方
向に流れる気流に対応したもので、即ち、気流の
方向性にかかわらず同一条件になるように設定し
てある。
Next, in FIG. 3 showing a more detailed structure of the element 10, 18a and 18b are protruding elements, respectively. The protrusion element 18a corresponds to the airflow flowing in the direction of the arrow X, and the protrusion element 18b corresponds to the airflow flowing in the direction of the arrow Y. In other words, the protrusion element 18b is set to have the same conditions regardless of the directionality of the airflow. There is.

突起素子18aと突起素子18bは、互いに交
互に隣接して縦横5列に配列されている。第3図
のC矢視図である第3C図に示すように、突起素
子18aはエレメント10の上面側に向つてプレ
ス加工で略山形をなして張り出しており、第3図
のD矢視図である第3D図に示すように突起素子
18bはエレメント10の下面側に略山形をなし
て張り出している。したがつて、第3図のA−A
断面図である第3A図およびB−B断面図である
第3B図に示すように、縦横の各列では略山形の
断面と平坦な略台形の断面とが交互に隣接してい
る。
The protruding elements 18a and the protruding elements 18b are arranged adjacent to each other alternately in five rows and columns. As shown in FIG. 3C, which is a view in the direction of arrow C in FIG. As shown in FIG. 3D, the protrusion element 18b protrudes from the lower surface of the element 10 in a substantially chevron shape. Therefore, A-A in FIG.
As shown in FIG. 3A, which is a sectional view, and FIG. 3B, which is a BB sectional view, substantially chevron-shaped cross sections and flat substantially trapezoidal cross sections are alternately adjacent to each other in each row in the vertical and horizontal directions.

例えば通路14の拡大断面図である第4図のよ
うに、突起素子18aの上流側部分20は比較的
急角度で傾斜しており、この上流側部分20に矢
印Xに沿つて流れてくる気流を衝突させて乱流を
形成し、乱流熱伝達域Tの範囲で熱伝達率の高い
乱流熱伝達域を形成している。
For example, as shown in FIG. 4, which is an enlarged cross-sectional view of the passageway 14, the upstream portion 20 of the protrusion element 18a is inclined at a relatively steep angle, and air flows into this upstream portion 20 along the arrow X. collide to form a turbulent flow, and a turbulent heat transfer region with a high heat transfer coefficient is formed within the turbulent heat transfer region T.

上流側部分20の下流側には緩やかに傾斜した
下流側部分22が形成されており、この下流側部
分22において乱流熱伝達域Tで形成された乱流
状態をそのまま滑かな傾斜面に沿わしながら気流
を案内するようになつている。したがつて、前述
のように略台形断面をなしている突起素子18b
を隔てて次の突起素子18aに気流が衝突する場
合には上流側部分20で再び熱伝達率の良い乱流
熱伝達域Tが形成されるように配慮されている。
A gently sloped downstream portion 22 is formed on the downstream side of the upstream portion 20, and in this downstream portion 22, the turbulent flow state formed in the turbulent heat transfer region T is maintained along a smooth slope. It is designed to guide the airflow while doing so. Therefore, as mentioned above, the protruding element 18b has a substantially trapezoidal cross section.
When the airflow collides with the next protrusion element 18a across the gap, consideration is given so that a turbulent heat transfer region T with a high heat transfer rate is again formed in the upstream portion 20.

なお、通路16でも同様に気流が突起素子18
bに沿つて案内されて突起素子18b毎に乱流熱
伝達域Tを形成している。
Note that in the passage 16 as well, the airflow is caused by the protruding element 18.
b to form a turbulent heat transfer region T for each protrusion element 18b.

以上のように通路14では矢印X方向の気流か
らエレメント10に熱伝達され、通路16ではエ
レメント10から気流に熱伝達されるようになつ
ている。
As described above, in the passage 14, heat is transferred from the airflow in the direction of arrow X to the element 10, and in the passage 16, heat is transferred from the element 10 to the airflow.

次に作用を説明する。まず第4図に示すよう
に、例えば通路14では、突起素子18aの上流
側部分20に矢印X方向の気流が衝突して、乱流
熱伝達域Tの範囲で高熱伝達率の乱流熱伝達が行
なわれる。下流側部分22では乱流の気流をその
まま下流に向つて案内し、隣接する突起素子18
aの間に配置されている突起素子18bを経て次
の突起素子18aに衝突し、再び上流側部分20
で気流が乱流になり、乱流熱伝達域Tで乱流熱伝
達が行なわれる。
Next, the effect will be explained. First, as shown in FIG. 4, for example, in the passage 14, an airflow in the direction of arrow X collides with the upstream portion 20 of the protrusion element 18a, and turbulent heat transfer with a high heat transfer coefficient occurs in the turbulent heat transfer region T. will be carried out. In the downstream part 22, the turbulent airflow is guided downstream as it is, and the adjacent protrusion element 18
It collides with the next protruding element 18a through the protruding element 18b disposed between a and the upstream portion 20 again.
The airflow becomes turbulent, and turbulent heat transfer occurs in the turbulent heat transfer region T.

したがつて、通路14を流れる気流からエレメ
ント10へは、突起素子18aの上流側部分20
近傍で乱流熱伝達域Tが形成され、高熱伝達率の
乱流熱伝達で伝熱される。
Therefore, from the airflow flowing through the passage 14 to the element 10, the upstream portion 20 of the protruding element 18a
A turbulent heat transfer region T is formed nearby, and heat is transferred by turbulent heat transfer with a high heat transfer coefficient.

一般に、熱伝達の性能を示す総括熱伝達係数、
すなわちU値は U=1/1/h1+δ/λ+1/h2 …(1) h1,h2:境膜伝熱係数 λ:エレメント材料の熱伝導率 δ:板厚 で表される。境膜伝熱係数h1,h2の影響が大き
いことが(1)式により分るが、この境膜伝熱係数
h1,h2を本エレメントの表面形状により増大さ
せることができる。このため伝熱係数h1,h2が
大きくなれば、U値も当然に大きくなり、単位面
積当りの熱伝達量が多い。
In general, the overall heat transfer coefficient, which indicates the performance of heat transfer,
That is, the U value is expressed as U=1/1/h1+δ/λ+1/h2...(1) h1, h2: film heat transfer coefficient λ: thermal conductivity of element material δ: plate thickness. Equation (1) shows that the influence of the film heat transfer coefficients h1 and h2 is large;
h1 and h2 can be increased depending on the surface shape of this element. Therefore, as the heat transfer coefficients h1 and h2 increase, the U value naturally increases, and the amount of heat transfer per unit area increases.

また通路16においても同様である。 The same applies to the passage 16.

(考案の効果) 以上説明したように本考案によれば、エレメン
ト10に突起素子18a,18bを形成し、突起
素子18a,18bを急傾斜の上流側部分20と
緩やかな下流側部分22で形成したので、例えば
通路14では、突起素子18aの上流側部分20
に矢印X方向の気流が衝突して、乱流熱伝達域T
の範囲で高熱伝達率の乱流熱伝達で熱を伝えるこ
とができ、しかも、下流側部分22では乱流の気
流をそのまま下流に向つて案内し、隣接する突起
素子18aの間に配置されている突起素子18b
を経て次の突起素子18aに衝突させることがで
き、再び上流側部分20で気流を乱流にして、乱
流熱伝達域Tで乱流熱伝達を行なうことができ
る。
(Effect of the invention) As explained above, according to the invention, the protruding elements 18a, 18b are formed on the element 10, and the protruding elements 18a, 18b are formed by the steep upstream part 20 and the gentle downstream part 22. Therefore, for example, in the passage 14, the upstream portion 20 of the protruding element 18a
The airflow in the direction of arrow X collides with the turbulent heat transfer area T.
Heat can be transferred by turbulent heat transfer with a high heat transfer coefficient in the range of protrusion element 18b
The air can be made to collide with the next protruding element 18a through the above process, and the airflow can be made turbulent again in the upstream portion 20, thereby allowing turbulent heat transfer to occur in the turbulent heat transfer region T.

したがつて、前記(1)式の総括伝熱係数U値を大
きくして、エレメント10の単位面積当りの熱伝
達量を従来より増やして熱伝達効率を大幅に向上
することができる。
Therefore, by increasing the overall heat transfer coefficient U value in equation (1), the amount of heat transfer per unit area of the element 10 can be increased compared to the conventional one, and the heat transfer efficiency can be greatly improved.

更に本考案においては下流側部分22が上流側
部分22の背後に滑らかに連続しかつ傾斜が緩や
かである為、乱流熱伝達域Tの乱流が下流側部分
22に滞留する恐れがなく(死水域ができず)、
適度に乱れた状態で通路14を流れ、しかも下流
側部分22に突起素子18bの背面でできる低い
台形断面の部分が滑らかに連続するので、エレメ
ント10と乱れた流体との接触の機会が増し、流
路損失を増すことなく熱伝達効率を高めることが
できる。本考案のように長方形の山と谷を組合せ
た長方形波形プレートと楕円形波形プレートの十
字向流の場合に付き伝熱性能を比較し、同時に流
れの可視化実験を行つたところ、伝熱係数は楕円
形波形プレートに比べて本考案品の方が略6パー
セント増加しており、又各山の部分で乱れが発生
しているにもかかわらず谷の部分に死水域が全く
認められなかつた。
Furthermore, in the present invention, since the downstream part 22 smoothly continues behind the upstream part 22 and has a gentle slope, there is no risk that the turbulent flow in the turbulent heat transfer region T will stay in the downstream part 22 ( (dead zone is not formed),
The fluid flows through the passage 14 in a moderately turbulent state, and the low trapezoidal cross-section formed by the back surface of the protrusion element 18b continues smoothly in the downstream portion 22, increasing the chances of contact between the element 10 and the turbulent fluid. Heat transfer efficiency can be increased without increasing flow path loss. When we compared the heat transfer performance of a rectangular corrugated plate with a combination of rectangular peaks and troughs as in the present invention and an elliptical corrugated plate in the case of cross-counterflow, and at the same time conducted a flow visualization experiment, we found that the heat transfer coefficient was Compared to the elliptical corrugated plate, the product of the present invention had an increase of about 6%, and even though turbulence occurred at each mountain part, no dead area was observed in the valley part.

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

第1図は本考案を採用した熱交換器を示す正面
図、第1A図は第1図のA部拡大図、第2図は第
1図の要部拡大斜視図、第3図はエレメントの側
面図、第3A図は第3図のA−A断面図、第3B
図は第3図のB−B断面図、第3C図は第3図の
C矢視図、第3D図は第3図のD矢視図、第4図
は通路の要部拡大断面図である。 10……エレメント、12……溶接部、14,
16……通路、18a,18b……突起素子、2
0……上流側部分、22……下流側部分。
Fig. 1 is a front view showing a heat exchanger adopting the present invention, Fig. 1A is an enlarged view of part A in Fig. 1, Fig. 2 is an enlarged perspective view of the main part of Fig. 1, and Fig. 3 is an enlarged view of the element. Side view, Figure 3A is a sectional view taken along line A-A in Figure 3, Figure 3B
The figure is a sectional view taken along line B-B in Fig. 3, Fig. 3C is a view taken in the direction of arrow C in Fig. 3, Fig. 3D is a view taken in the direction of arrow D in Fig. 3, and Fig. 4 is an enlarged sectional view of the main part of the passage. be. 10...Element, 12...Welding part, 14,
16... Passage, 18a, 18b... Projection element, 2
0... Upstream part, 22... Downstream part.

Claims (1)

【実用新案登録請求の範囲】[Scope of utility model registration request] 長方形の山及び谷がプレス形成されて格子状に
凹凸のある波形プレート状のエレメント10が通
路14,16をへだてて複数枚積層された熱交換
器であつて、上記の山及び谷は横向きに長い長方
形の第1の突起素子18aの4個が千鳥状に配置
されて一方へ突出し、その中央にそれらと90度向
きの異なる縦向きに長い長方形の第2の突起素子
18bが他方へ突出する姿勢で配置されたものの
組合せからなり、上記の山となる第1の突起素子
18aは突出方向に急角度に傾斜した上流側部分
20とそれに続き逆方向に緩やかに傾斜した下流
側部分22とが頂上で滑らかに連続しており、上
記第2の突起素子18bは上記第1の突起素子1
8aと突出方向のみが異なる同一形状を備え、各
エレメント10の一方の通路14では第1の流体
が第1突起素子18aの上流側部分20から下流
側部分をへて略台形断面をなす第2突起素子18
b部分へと横方向へ流れ、他方の通路16では第
2の流体が第2突起素子18bの上流側部分から
下流側部分をへて略台形断面をなす第1突起素子
部分へと縦方向へ流れるように構成したことを特
徴とする熱交換器。
The heat exchanger is a heat exchanger in which a plurality of corrugated plate-shaped elements 10 having rectangular peaks and valleys formed by pressing and having irregularities in a lattice pattern are laminated with passages 14 and 16 separated, and the above-mentioned peaks and valleys are arranged horizontally. Four long rectangular first protruding elements 18a are arranged in a staggered manner and protrude to one side, and at the center thereof, a vertically long rectangular second protruding element 18b, which is oriented at 90 degrees and is different from them, protrudes to the other side. The first protrusion element 18a, which forms a mountain, has an upstream portion 20 that is steeply inclined in the protruding direction, and a downstream portion 22 that is gently inclined in the opposite direction. The second protrusion element 18b is smoothly continuous at the top, and the second protrusion element 18b is connected to the first protrusion element 1.
In one passage 14 of each element 10, the first fluid passes from the upstream portion 20 of the first protrusion element 18a to the downstream portion of the first protrusion element 18a, and the second protrusion element 18a has a substantially trapezoidal cross section. Projection element 18
b, and in the other passage 16 the second fluid flows longitudinally from the upstream portion of the second projection element 18b through the downstream portion to the first projection element portion having a substantially trapezoidal cross section. A heat exchanger characterized by having a flowing structure.
JP1986102365U 1986-07-03 1986-07-03 Expired JPH0435732Y2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP1986102365U JPH0435732Y2 (en) 1986-07-03 1986-07-03

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP1986102365U JPH0435732Y2 (en) 1986-07-03 1986-07-03

Publications (2)

Publication Number Publication Date
JPS6312085U JPS6312085U (en) 1988-01-26
JPH0435732Y2 true JPH0435732Y2 (en) 1992-08-24

Family

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Family Applications (1)

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JP1986102365U Expired JPH0435732Y2 (en) 1986-07-03 1986-07-03

Country Status (1)

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JP (1) JPH0435732Y2 (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP5206032B2 (en) * 2008-03-06 2013-06-12 パナソニック株式会社 Heat exchanger

Family Cites Families (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS496559U (en) * 1972-04-19 1974-01-21
JPS5237659U (en) * 1975-09-10 1977-03-17

Also Published As

Publication number Publication date
JPS6312085U (en) 1988-01-26

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