JPS61280393A - Heat transfer tube - Google Patents

Heat transfer tube

Info

Publication number
JPS61280393A
JPS61280393A JP10638985A JP10638985A JPS61280393A JP S61280393 A JPS61280393 A JP S61280393A JP 10638985 A JP10638985 A JP 10638985A JP 10638985 A JP10638985 A JP 10638985A JP S61280393 A JPS61280393 A JP S61280393A
Authority
JP
Japan
Prior art keywords
tube
heat transfer
fluid
groove
port side
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.)
Pending
Application number
JP10638985A
Other languages
Japanese (ja)
Inventor
Tomoyuki Murayama
智之 村山
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Sanyo Electric Co Ltd
Original Assignee
Sanyo Electric Co Ltd
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Sanyo Electric Co Ltd filed Critical Sanyo Electric Co Ltd
Priority to JP10638985A priority Critical patent/JPS61280393A/en
Publication of JPS61280393A publication Critical patent/JPS61280393A/en
Pending legal-status Critical Current

Links

Classifications

    • 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
    • F28F1/42Tubular elements and assemblies thereof with means for increasing heat-transfer area, e.g. with fins, with projections, with recesses the means being both outside and inside the tubular element
    • 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
    • F28F1/42Tubular elements and assemblies thereof with means for increasing heat-transfer area, e.g. with fins, with projections, with recesses the means being both outside and inside the tubular element
    • F28F1/424Means comprising outside portions integral with inside portions
    • F28F1/426Means comprising outside portions integral with inside portions the outside portions and the inside portions forming parts of complementary shape, e.g. concave and convex

Landscapes

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

Abstract

PURPOSE:To improve the performance of the heat transfer tube along the whole length of the tube by a method wherein the depth of spiral grooves, provided on the inner surface of the tube, is decreased gradually from the inlet port side of the tube toward the outlet port side thereof to shorten the distance of approach run of fluid and lengthen the area of turbulent flow in the tube. CONSTITUTION:The groove 2 at a part nearest to the inlet port side of the heat transfer tube 1 is formed deeper than the groove of conventional tube, therefore, the fluid for heat exchange, which flows into the heat transfer tube 1, begins to whirl immediately along the spiral groove 2 and becomes eddy current condition near the inlet port. The distance of approach run of the fluid for heat exchange becomes shorter in this heat transfer tube 1 before. The depth of the groove 2 is formed so as to be shallower gradually toward the outlet port side of the tube and the sectional area for flowing the fluid for heat exchange is widened, therefore, the resistance of flow is reduced gradually toward the outlet port side of the tube, increase of pressure loss of the fluid may be reduced and the deterioration of flow energy may be reduced. Accordingly, better turbulent flow is generated along the whole length of the heat transfer tube 1 substantially and the heat transfer performance of the tube may become more prominent than before.

Description

【発明の詳細な説明】 (イ)産業上の利用分野 本発明は、熱交換器に用いる伝熱管に関し、特に管内面
に螺旋状の溝を有する伝熱管(以下、この種の伝熱管と
いう)の改良に関する。
Detailed Description of the Invention (a) Industrial Application Field The present invention relates to heat exchanger tubes used in heat exchangers, and particularly to heat exchanger tubes having spiral grooves on the inner surface of the tube (hereinafter referred to as this type of heat exchanger tube). Regarding improvements.

(ロ)従来の技術 この種の伝熱管の従来の技術として、螺線状の溝の深さ
が管の全長にわたって一定であるもの〔例えば、実公昭
41−24229号公報]が知られている。
(B) Conventional technology As a conventional technology for this type of heat exchanger tube, there is known one in which the depth of the spiral groove is constant over the entire length of the tube [for example, Publication of Utility Model Publication No. 41-24229]. .

(ハ)発明が解決しようとする問題点 この種の伝熱管は、管内の流れが低速であっても螺線状
の溝の機能により流体を乱流化させやすく、その伝熱性
能を高め得るので、例えば特開昭46−2490号公報
にみられるように吸収冷凍機の熱交換器用素材として以
前から使用されている。しかし、管内に流体が流入する
場合、これが管の入口から直ちに些流となるのではなく
一定の距離(以下、助走距離という)を経て乱流となる
ため、従来のこの種の伝熱管においては助走距離が長(
なってしまうという問題点を有していた。
(c) Problems to be solved by the invention This type of heat transfer tube can easily make the fluid turbulent due to the function of the spiral grooves even if the flow inside the tube is low speed, and can improve its heat transfer performance. Therefore, it has been used for a long time as a material for heat exchangers in absorption refrigerators, as shown in, for example, Japanese Patent Application Laid-Open No. 46-2490. However, when fluid flows into a tube, it does not become a small flow immediately from the entrance of the tube, but becomes a turbulent flow after a certain distance (hereinafter referred to as the run-up distance). The run-up distance is long (
This has the problem that it becomes

本発明は、この問題点に鑑み、従来のものよりも助走距
離を短かくでき、管内の乱流域を長くできるこの種の伝
熱管の提供を目的としたものである。
In view of this problem, it is an object of the present invention to provide a heat transfer tube of this type that can shorten the run-up distance and lengthen the turbulent region within the tube compared to conventional tubes.

に)問題点を解決するための手段 本発明は、上記の問題点を解決する手段として、従来の
ものよりも管の入口側における螺線状の溝を深くし、そ
の深さを出口側へ向って次第に小さくするようにこの種
の伝熱管を構成したものである。
B) Means for Solving the Problems The present invention, as a means for solving the above problems, makes the spiral groove deeper on the inlet side of the pipe than the conventional one, and increases the depth toward the outlet side. This type of heat exchanger tube is configured to gradually become smaller.

(ホ)作用 本発明の伝熱管においては、管の入口側の溝が深く形成
されていて管内に流入した流体の旋回が入口近傍で促進
される機能(作用)をもたせであるので、従来のものよ
りも助走距離を短かくできる。かつまた、溝が管の出[
]側へ向って次第に浅くなるように形成されていて流れ
の抵抗が小さくなる機能をもたせであるので、流体の圧
力損失の増大も軽減でき、管のほぼ全長にわたって良好
な乱流域を生じさせることが可能である。したがって、
本発明によれば、この種の伝熱管の性能を従来のものよ
りも高め得る。
(E) Function In the heat transfer tube of the present invention, the groove on the inlet side of the tube is formed deeply and has the function (effect) of promoting swirling of the fluid flowing into the tube near the inlet. The run-up distance can be shorter than that of a conventional model. Also, the groove is the protrusion of the tube [
] Since it is formed so that it becomes gradually shallower toward the side and has the function of reducing flow resistance, it can also reduce the increase in fluid pressure loss and create a good turbulent area over almost the entire length of the pipe. is possible. therefore,
According to the present invention, the performance of this type of heat exchanger tube can be improved compared to conventional ones.

(へ)実施例 図面は本発明による伝熱管の一実施例の断面を示した概
略構成説明図である。図において、(1)は吸収冷凍機
の発生器や吸収器などの熱交換器用の素材として用いら
れている伝熱管で、この伝熱管の内面にはらせん状の溝
(2) 、 (2)・・・が形成されている。そして、
溝(2)は、その深さI■が管の入口側〔図の右側〕か
ら出口側へ向って次第に小さくなるように、形成されて
いる〔例えば、管の内径8゜5龍、管の長さ1.8mの
もので、Hは0.68 mtxから0龍]。なお、Hは
伝熱管(11へ流入する熱交換用流体の流速、管径、長
さなどによって適宜選定される。なおまた、131 、
 +31は熱交換器用の管板である。
(F) Embodiment The drawing is a schematic structural diagram showing a cross section of an embodiment of a heat exchanger tube according to the present invention. In the figure, (1) is a heat exchanger tube used as a material for heat exchangers such as generators and absorbers in absorption refrigerators, and the inner surface of this heat exchanger tube has spiral grooves (2), (2). ... is formed. and,
The groove (2) is formed so that its depth I becomes gradually smaller from the inlet side (right side in the figure) to the outlet side of the tube (for example, if the inner diameter of the tube is 8.5 mm, 1.8m long, H is 0.68mtx to 0ryu]. Note that H is appropriately selected depending on the flow rate, pipe diameter, length, etc. of the heat exchange fluid flowing into the heat transfer tube (11).
+31 is a tube sheet for a heat exchanger.

次に、このように構成された伝熱管(以下、本伝熱管と
いう)内における熱交換用流体の動作例を説明する。
Next, an example of the operation of the heat exchange fluid in the heat exchanger tube configured as described above (hereinafter referred to as the main heat exchanger tube) will be described.

本伝熱管+11の入口側に最も近い部分の溝(2)は従
来のもののそれよりも深く〔例えば、本伝熱管のHが0
.68mgであるのに対し、従来のもののそれは0.0
2ないし0.2 u程度である。〕形成されているので
、本伝熱管(1)内へ流入した熱交換用流体はらせん状
の溝(2)に沿って直ちに旋回し始め本伝熱管(11の
入口部近傍で渦流状態になる。すなわち、本伝熱管(1
)においては従来のものよりも熱交換用流体の助走距離
が短かくなる。かつまた、溝(2)は出口側へ向って次
第に浅くなるように形成されていて熱交換用流体の流通
断面が広くなるので、流れの抵抗が出口側へ向って次第
に小さくなり、熱交換用流体の圧力損失の増大も軽減さ
れ、流れの勢いの衰えも小さい。したがって、本伝熱管
(1)にあっては、そのほぼ全長にわたって管内に良好
な乱流を生じ、従来のものよりもその伝熱性能に秀れる
。特に、本伝熱管は、熱交換用流体の流速に制限のある
吸収冷凍機その他の熱交換器用素材として、好適である
The groove (2) at the part closest to the inlet side of the present heat exchanger tube +11 is deeper than that of the conventional one [for example, the H of the present heat exchanger tube is 0
.. 68mg, whereas the conventional one is 0.0
It is about 2 to 0.2 u. ], the heat exchange fluid that flows into the main heat exchanger tube (1) immediately begins to swirl along the spiral groove (2) and becomes a vortex near the inlet of the main heat exchanger tube (11). .That is, this heat exchanger tube (1
), the run-up distance of the heat exchange fluid is shorter than that of the conventional method. In addition, the groove (2) is formed to become gradually shallower toward the outlet side, and the flow cross section of the heat exchange fluid becomes wider, so the flow resistance gradually decreases toward the outlet side, and the heat exchange fluid becomes shallower. The increase in fluid pressure loss is also reduced, and the decline in flow momentum is also small. Therefore, in the present heat transfer tube (1), good turbulence is generated within the tube over almost its entire length, and its heat transfer performance is superior to that of the conventional tube. In particular, the present heat exchanger tube is suitable as a material for absorption refrigerators and other heat exchangers in which the flow rate of heat exchange fluid is limited.

なお、管内を流れる熱交換用流体としては、水その他の
液体や空気その他の気体あるいは蒸気のように相変化す
る流体など、種々゛のものが使用できる。
Note that various types of heat exchange fluid can be used as the heat exchange fluid flowing inside the pipe, such as water or other liquids, air or other gases, or fluids that change phase such as steam.

(ト)発明の効果 以上のとおり、本発明によれば、管内に流入した熱交換
用流体の渦流化を入口部で促進し、管のほぼ全長にわた
って良好な乱流域を生じさせ得るので、この種の伝熱管
の性能を従来のものよりも向上させる効果をもたらす。
(G) Effects of the Invention As described above, according to the present invention, the turbulence of the heat exchange fluid that has flowed into the pipe is promoted at the inlet part, and a good turbulent area can be created over almost the entire length of the pipe. This has the effect of improving the performance of heat exchanger tubes compared to conventional ones.

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

図面は本発明によるこの種の伝熱管の一実施例の断面を
示した概略構成説明図である。 (1)・・・伝熱管、 +21 、 (2)・・・溝、
 13+ 、 (3)・・・管板。
The drawing is a schematic structural explanatory diagram showing a cross section of an embodiment of this type of heat exchanger tube according to the present invention. (1)...heat exchanger tube, +21, (2)...groove,
13+, (3)...Tube plate.

Claims (1)

【特許請求の範囲】[Claims] (1)管内面に螺旋状の溝を有する伝熱管において、そ
の溝の深さが管の入口側から出口側へ向って次第に小さ
くなるように溝が形成されていることを特徴とした伝熱
管。
(1) A heat exchanger tube having a spiral groove on the inner surface of the tube, characterized in that the groove is formed so that the depth of the groove gradually decreases from the inlet side to the outlet side of the tube. .
JP10638985A 1985-05-17 1985-05-17 Heat transfer tube Pending JPS61280393A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP10638985A JPS61280393A (en) 1985-05-17 1985-05-17 Heat transfer tube

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP10638985A JPS61280393A (en) 1985-05-17 1985-05-17 Heat transfer tube

Publications (1)

Publication Number Publication Date
JPS61280393A true JPS61280393A (en) 1986-12-10

Family

ID=14432339

Family Applications (1)

Application Number Title Priority Date Filing Date
JP10638985A Pending JPS61280393A (en) 1985-05-17 1985-05-17 Heat transfer tube

Country Status (1)

Country Link
JP (1) JPS61280393A (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS63172894A (en) * 1987-01-12 1988-07-16 Matsushita Refrig Co Heat exchanger
CN102538539A (en) * 2012-02-14 2012-07-04 张扩潮 Heat exchange tube
KR20180135143A (en) * 2017-06-09 2018-12-20 한국원자력연구원 A heat exchanger for a reactor including a turbulent flow forming member

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS63172894A (en) * 1987-01-12 1988-07-16 Matsushita Refrig Co Heat exchanger
CN102538539A (en) * 2012-02-14 2012-07-04 张扩潮 Heat exchange tube
KR20180135143A (en) * 2017-06-09 2018-12-20 한국원자력연구원 A heat exchanger for a reactor including a turbulent flow forming member

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