JPS6352310B2 - - Google Patents
Info
- Publication number
- JPS6352310B2 JPS6352310B2 JP18148481A JP18148481A JPS6352310B2 JP S6352310 B2 JPS6352310 B2 JP S6352310B2 JP 18148481 A JP18148481 A JP 18148481A JP 18148481 A JP18148481 A JP 18148481A JP S6352310 B2 JPS6352310 B2 JP S6352310B2
- Authority
- JP
- Japan
- Prior art keywords
- tube
- groove
- lead angle
- heat exchanger
- heat transfer
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Expired
Links
- 239000003507 refrigerant Substances 0.000 claims description 26
- 239000012530 fluid Substances 0.000 claims description 8
- 239000011295 pitch Substances 0.000 description 14
- 238000009833 condensation Methods 0.000 description 13
- 230000005494 condensation Effects 0.000 description 13
- 238000001704 evaporation Methods 0.000 description 12
- 230000008020 evaporation Effects 0.000 description 11
- 230000000694 effects Effects 0.000 description 6
- 238000010586 diagram Methods 0.000 description 4
- 238000009835 boiling Methods 0.000 description 3
- 230000007423 decrease Effects 0.000 description 3
- 238000004519 manufacturing process Methods 0.000 description 3
- 229910003460 diamond Inorganic materials 0.000 description 2
- 239000010432 diamond Substances 0.000 description 2
- 239000010409 thin film Substances 0.000 description 2
- 229910000838 Al alloy Inorganic materials 0.000 description 1
- RYGMFSIKBFXOCR-UHFFFAOYSA-N Copper Chemical compound [Cu] RYGMFSIKBFXOCR-UHFFFAOYSA-N 0.000 description 1
- 229910000881 Cu alloy Inorganic materials 0.000 description 1
- 229910000831 Steel Inorganic materials 0.000 description 1
- 229910052782 aluminium Inorganic materials 0.000 description 1
- XAGFODPZIPBFFR-UHFFFAOYSA-N aluminium Chemical compound [Al] XAGFODPZIPBFFR-UHFFFAOYSA-N 0.000 description 1
- 229910052802 copper Inorganic materials 0.000 description 1
- 239000010949 copper Substances 0.000 description 1
- 238000002474 experimental method Methods 0.000 description 1
- 239000007788 liquid Substances 0.000 description 1
- 239000000463 material Substances 0.000 description 1
- 229910052751 metal Inorganic materials 0.000 description 1
- 239000002184 metal Substances 0.000 description 1
- 150000002739 metals Chemical class 0.000 description 1
- 230000001737 promoting effect Effects 0.000 description 1
- 239000011347 resin Substances 0.000 description 1
- 229920005989 resin Polymers 0.000 description 1
- 239000010959 steel Substances 0.000 description 1
- 238000003756 stirring Methods 0.000 description 1
Classifications
-
- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F28—HEAT EXCHANGE IN GENERAL
- F28F—DETAILS OF HEAT-EXCHANGE AND HEAT-TRANSFER APPARATUS, OF GENERAL APPLICATION
- F28F1/00—Tubular elements; Assemblies of tubular elements
- F28F1/10—Tubular elements and assemblies thereof with means for increasing heat-transfer area, e.g. with fins, with projections, with recesses
- F28F1/40—Tubular elements and assemblies thereof with means for increasing heat-transfer area, e.g. with fins, with projections, with recesses the means being only inside the tubular element
Landscapes
- Physics & Mathematics (AREA)
- Engineering & Computer Science (AREA)
- Geometry (AREA)
- Thermal Sciences (AREA)
- Mechanical Engineering (AREA)
- General Engineering & Computer Science (AREA)
- Rigid Pipes And Flexible Pipes (AREA)
- Heat-Exchange Devices With Radiators And Conduit Assemblies (AREA)
Description
本発明は管内でフレオン等の冷媒を蒸発又は凝
縮させて、管外を流れる流体との間で熱交換を行
なわせる伝熱管に関するもので、特に圧力損失を
増大させることなく、蒸発作用を増大させ、かつ
凝縮作用を増進させて、伝熱特性を向上せしめた
ものである。
一般に空気調和機、冷凍機等の熱交換器には管
内でフレオン等の冷媒を蒸発又は凝縮させて、管
外を流れる流体との間で熱交換させる伝熱管が用
いられている。このような伝熱管として従来は平
滑管が用いられていたが、最近では、管内面に一
方向の多数の螺旋状溝を形成した伝熱管や、管内
面に交差する多数の螺旋状溝を形成した伝熱管が
用いられている。これ等の内面溝付伝熱管は、管
内伝熱性能を上昇させると共に圧力損失の増大を
押える工夫が行なわれており、内面平滑な伝熱管
と比較し、優れた伝熱性能を示す。しかるに、最
近では省エネルギーの見地から更に伝熱性能の優
れた伝熱管が要求されている。
本発明はこれに鑑み、従来の内面溝付伝熱管の
伝熱特性を更に向上させるため、管内を流れるフ
レオン等の冷媒の蒸発及び凝縮現象における流れ
の挙動、伝熱性能及び圧力損失と、管内面に形成
した突起の形状との関連について、種々の実験、
検討を行なつた結果、管内面に一方向の多数の螺
旋状溝又は交差する多数の螺旋状溝を設けた伝熱
管と比較し、同等の圧力損失で、はるかに優れた
伝熱性能を有する伝熱管を開発したもので、管内
で冷媒を蒸発又は凝縮させて管外を流れる流体と
の間で熱交換を行なわせる伝熱管において、管内
面に管軸に対して互に逆方向のリード角α1,α2を
有する多数の螺旋状の溝と、該溝間にそれぞれ同
一形状の突起を形成し、リード角α1の溝の螺旋方
向にうねりを設け、リード角α2の溝を螺旋方向に
直進させ、突起のリード角α1の溝側斜面を凹面と
し、リード角α2の溝側斜面を凸面として、突起の
形状を底辺が歪んだ菱形で、頂部が鞍型又は丸味
を有する菱形となし、螺旋状のリード角α1,α2を
5〜45゜、リード角α1の溝のピツチP1及びリード
角α2の溝のピツチP2を0.2〜1.0mm、突起の高さh
を0.05〜0.75mmとしたことを特徴とするものであ
る。
即ち、本発明は、第1図に示すように伝熱管1
の内面に、第2図に示すように管軸Aに対して互
に逆方向のリード角α1,α2を有する螺旋状の溝
2,3と、該溝2,3間にそれぞれ同一形状の突
起4を形成し、図に示すようにリード角α1の溝2
を螺旋方向にうねりを設け、リード角α2の溝3を
螺旋方向に直進させ、突起4のリード角α1の溝2
に相対する面5を第3図に示すように凹面状の斜
面とし、突起4のリード角α2の溝3に相対する面
6を第4図に示すように凸面状の斜面として、該
突起4の形状が底辺が歪んだ菱形で、頂部が鞍型
又は丸味を有する菱形(図は鞍型を示す)とした
もので、管軸Aに対し互いに逆向きのリード角
α1,α2をそれぞれ5〜45゜とし、リード角α1の溝
2のピツチP1及びリード角α2の溝3のピツチP2
をそれぞれ0.2〜1.0mmとし、また突起5の高さh
を0.05〜0.75mmとしたものである。
伝熱管の材質としては、鉄鋼、非鉄金属、樹脂
等、種々のものが用いられるが、特に熱伝導性の
優れた銅、銅合金、アルミニウム、アルミニウム
合金等が適している。
本発明伝熱管は以上の構成からなり、空気調和
機、冷凍機等の熱交換器の伝熱管として、管内で
フレオン等の冷媒を蒸発又は凝縮させ、管外を流
れる流体との間で熱交換させると、次のように伝
熱性能を向上する。
(1) 管内に形成した多数の突起により、管内表面
積が拡大し、これが有効伝熱面積として作用
し、伝熱性能を向上する。
(2) 管内で冷媒が凝縮する時に多数の突起の鞍型
又は丸味を有する菱形の頂部及び曲率をもつ斜
面部に薄膜部が形成し、凝縮作用を促進させ
る。また管内で冷媒が蒸発する時に、冷媒は主
として螺旋状に直進する溝を流れ、該溝から螺
旋方向にうねりを設けた溝に流れ込み、うねり
を有する溝空間が核沸騰の核として作用し、蒸
発作用を増大させる。
(3) 管軸に対して互いに逆方向のリード角α1,α2
を有する螺旋状の溝が冷媒の流れを撹拌するた
め乱流効果が著しく、これにより管内伝熱性能
が向上する。
(4) リード角α1,α2と適切な溝のピツチP1,P2
により、溝部分での毛細管現象が著しく、冷媒
やその湿り蒸気が管内表面を全体的に覆つて吸
着し、伝熱面として有効に作用する。しかし
て、本発明伝熱管において、リード角α1,α2、
溝のピツチP1,P2突起の高さhを前記の如く
限定したのは次の理由によるものである。
リード角α1,α2は、第8図に示すリード角α1,
α2と伝熱性能及び圧力損失の実験結果から明らか
なように、リード角α1,α2が5〜45゜の範囲内で
優れた特性を示すも、リード角α1,α2が5゜未満で
は明らかに性能が低下し、45゜を越えると圧力損
失が増大するためである。また本発明伝熱管の製
造に際し、リード角α1,α2が大きくなればなるほ
ど加工性が低下するためである。また突起の高さ
hを0.05〜0.75mm、溝ピツチP1,P2を0.2〜1.0mm
としたのは突起の高さが0.05mm未満でも溝ピツチ
P1,P2が0.2mm未満でも、伝熱管として管内面が
平滑管に近くなり、上記に述べた性能が得られ
ず、突起の高さhが0.75mmを越え、溝ピツチP1,
P2が1mmを越えると、伝熱性能は向上するも、
管内を流れる流体の圧力損失が増大するため、伝
熱性能の増大のみを目的とする本発明伝熱管とし
ての効果が得られないためである。このことは、
第9図及び第10図に示す実験結果からも明らか
である。
また突起の頂部形状を鞍型又は丸味を有する菱
形とし、リード角α1,α2の溝の一方を螺旋方向に
うねりを設け、他方を螺旋方向に直進させたの
は、冷媒の凝縮において突起より凝縮液の流れ落
ちをスムースにし、液に薄膜部を形成させて凝縮
作用を促進させ、冷媒の蒸発において、直進する
溝を湿り蒸気の流れの主流とし、うねりを有する
溝の空間部に分流させ、該空間部を核沸騰を発生
させる沸騰核として作用させるためであり、更に
リード角α1,α2をα1≒α2、溝ピツチP1,P2をP1
≒P2とすると冷媒の流れの均一化が起り、上記
作用がより有効に作用する。
また突起の頂部を鞍型又は丸味を有する菱形と
し、リード角α1,α2をα1≒α2、溝ピツチP1,P2
をP1≒P2することにより、本発明伝熱管の製造
において、加工力が管に均一に加わり、品質の良
いものが得られる。更に空気調和機等のプレート
フイン型熱交換器の伝熱管として用いた場合、プ
レートフインを固定する拡管作業において、突起
先端の潰れが少なく、しかも均一な加工のために
組立て誤差の少ない歪のない熱交換器が製作でき
るため、大量生産、自動組立てラインへの適用が
容易となる。
以下、本発明を実施例について詳細に説明す
る。
第1表に示す寸法の第2図に示す形状の本発明
伝熱管と、従来の平滑管及び内面に螺旋状凹溝を
設けた内面溝付管を作成し、これらについて、伝
熱性能及び圧力損失を測定した。その結果を第5
図乃至第10図に示す。
The present invention relates to a heat exchanger tube that evaporates or condenses a refrigerant such as freon inside the tube to exchange heat with a fluid flowing outside the tube.In particular, the present invention relates to a heat exchanger tube that evaporates or condenses a refrigerant such as Freon inside the tube and exchanges heat with a fluid flowing outside the tube. , and the condensation effect is enhanced to improve heat transfer characteristics. Generally, heat exchangers such as air conditioners and refrigerators use heat transfer tubes that evaporate or condense a refrigerant such as Freon inside the tubes and exchange heat with a fluid flowing outside the tubes. Conventionally, smooth tubes were used as such heat exchanger tubes, but recently, heat exchanger tubes with many spiral grooves in one direction formed on the inner surface of the tube, and many spiral grooves formed intersecting on the inner surface of the tube have recently been introduced. heat exchanger tubes are used. These heat exchanger tubes with internal grooves are designed to improve the heat transfer performance within the tube and suppress the increase in pressure loss, and exhibit superior heat transfer performance compared to heat exchanger tubes with smooth inner surfaces. However, recently, from the viewpoint of energy saving, heat transfer tubes with even better heat transfer performance are required. In view of this, the present invention aims to further improve the heat transfer characteristics of conventional internally grooved heat transfer tubes, and to improve the flow behavior, heat transfer performance, and pressure loss during the evaporation and condensation phenomena of refrigerants such as Freon flowing inside the tubes. Various experiments were conducted to investigate the relationship between the shape of the protrusions formed on the surface.
As a result of our studies, we found that compared to heat transfer tubes with multiple spiral grooves in one direction or multiple intersecting spiral grooves on the inner surface of the tube, this product has much better heat transfer performance with the same pressure loss. This is a developed heat transfer tube that evaporates or condenses the refrigerant inside the tube and exchanges heat with the fluid flowing outside the tube. A large number of spiral grooves having α 1 and α 2 and protrusions of the same shape are formed between the grooves, undulations are provided in the spiral direction of the groove with a lead angle α 1 , and the groove with a lead angle α 2 is formed into a spiral shape. The groove side slope of the protrusion with a lead angle α 1 is a concave surface, the groove side slope with a lead angle α 2 is a convex surface, and the shape of the protrusion is a diamond shape with a distorted base and a saddle-shaped or rounded top. The lead angles α 1 and α 2 of the diamond-shaped and spiral shapes are 5 to 45 degrees, the pitch P 1 of the groove with lead angle α 1 and the pitch P 2 of the groove with lead angle α 2 are 0.2 to 1.0 mm, and the height of the protrusion is Sah
It is characterized by having a diameter of 0.05 to 0.75 mm. That is, the present invention provides a heat exchanger tube 1 as shown in FIG.
As shown in FIG. 2, spiral grooves 2 and 3 having lead angles α 1 and α 2 in opposite directions with respect to the tube axis A are formed on the inner surface of the tube, and grooves 2 and 3 having the same shape are formed between the grooves 2 and 3, respectively. A groove 2 with a lead angle α 1 is formed as shown in the figure.
is undulated in the helical direction, the groove 3 with the lead angle α 2 is made to run straight in the helical direction, and the groove 2 with the lead angle α 1 of the protrusion 4 is formed.
The surface 5 facing the protrusion 4 is a concave slope as shown in FIG. 4 is a diamond shape with a distorted base and a saddle-shaped or rounded top (the figure shows a saddle shape), and the lead angles α 1 and α 2 are opposite to each other with respect to the tube axis A. Pitch P 1 of groove 2 with lead angle α 1 and pitch P 2 of groove 3 with lead angle α 2 , respectively .
are respectively 0.2 to 1.0 mm, and the height h of the protrusion 5 is
is set to 0.05 to 0.75 mm. Various materials can be used for the heat exchanger tubes, such as steel, nonferrous metals, and resins, but copper, copper alloys, aluminum, aluminum alloys, and the like, which have excellent thermal conductivity, are particularly suitable. The heat exchanger tube of the present invention has the above-mentioned configuration and is used as a heat exchanger tube for a heat exchanger such as an air conditioner or a refrigerator, by evaporating or condensing a refrigerant such as Freon within the tube, and exchanging heat with a fluid flowing outside the tube. By doing so, the heat transfer performance will be improved as follows. (1) The numerous protrusions formed inside the tube expand the inner surface area of the tube, which acts as an effective heat transfer area and improves heat transfer performance. (2) When the refrigerant condenses in the pipe, a thin film is formed on the saddle-shaped or rounded diamond-shaped tops of the many protrusions and the curved slopes, promoting the condensation action. Furthermore, when the refrigerant evaporates in the pipe, the refrigerant mainly flows in a straight spiral groove, and from the groove flows into a groove with undulations in the spiral direction, and the undulation groove space acts as a nucleus for nucleate boiling, causing evaporation. Increases effect. (3) Lead angles α 1 and α 2 in opposite directions with respect to the tube axis
The spiral grooves stir the flow of refrigerant, resulting in a significant turbulence effect, which improves the heat transfer performance within the tube. (4) Lead angle α 1 , α 2 and appropriate groove pitch P 1 , P 2
As a result, the capillary phenomenon in the groove portion is significant, and the refrigerant and its wet vapor completely cover and adsorb the inner surface of the tube, effectively acting as a heat transfer surface. Therefore, in the heat exchanger tube of the present invention, the lead angles α 1 , α 2 ,
The pitches of the grooves P 1 and P 2 and the height h of the protrusions are limited as described above for the following reasons. The lead angles α 1 and α 2 are the lead angles α 1 and α 2 shown in FIG.
As is clear from the experimental results of α 2 , heat transfer performance, and pressure drop, excellent characteristics are exhibited when the lead angles α 1 and α 2 are in the range of 5 to 45°, but when the lead angles α 1 and α 2 are 5°, This is because if the angle is less than 45°, the performance will clearly deteriorate, and if it exceeds 45°, the pressure loss will increase. This is also because when manufacturing the heat exchanger tube of the present invention, the larger the lead angles α 1 and α 2 are, the lower the workability is. Also, the height h of the protrusion is 0.05 to 0.75 mm, and the groove pitch P 1 and P 2 are 0.2 to 1.0 mm.
The reason for this is that even if the protrusion height is less than 0.05 mm, the groove pitch will not occur.
Even if P 1 and P 2 are less than 0.2 mm, the inner surface of the heat exchanger tube will be close to that of a smooth tube, and the performance described above will not be obtained, and the height h of the protrusion will exceed 0.75 mm, and the groove pitch P 1 ,
When P 2 exceeds 1 mm, heat transfer performance improves, but
This is because the pressure loss of the fluid flowing inside the tube increases, so that the effect of the heat transfer tube of the present invention, which only aims to increase heat transfer performance, cannot be obtained. This means that
This is also clear from the experimental results shown in FIGS. 9 and 10. In addition, the shape of the top of the protrusion is saddle-shaped or rounded rhombus, one of the grooves with lead angles α 1 and α 2 is undulated in the spiral direction, and the other is made to run straight in the helical direction. This allows the condensate to flow down more smoothly, forming a thin film in the liquid to promote condensation, and in the evaporation of the refrigerant, the straight grooves are used as the main flow of wet steam, and the flow is diverted to the undulating spaces in the grooves. This is to make the space act as a boiling nucleus that generates nucleate boiling, and further, the lead angles α 1 and α 2 are set to α 1 ≒ α 2 , and the groove pitches P 1 and P 2 are set to P 1
When ≒P 2 , the flow of the refrigerant becomes uniform, and the above-mentioned effect works more effectively. In addition, the top of the protrusion is saddle-shaped or rounded diamond-shaped, the lead angles α 1 and α 2 are α 1 ≒ α 2 , and the groove pitches P 1 and P 2
By setting P 1 ≒ P 2 , in the production of the heat exchanger tube of the present invention, processing force is uniformly applied to the tube, and a product of good quality can be obtained. Furthermore, when used as a heat transfer tube in a plate fin type heat exchanger such as an air conditioner, the tip of the protrusion is less likely to be crushed during the tube expansion work to fix the plate fin, and because of the uniform processing, there are fewer assembly errors and no distortion. Since the heat exchanger can be manufactured, it is easy to apply it to mass production and automatic assembly lines. Hereinafter, the present invention will be described in detail with reference to examples. A heat transfer tube of the present invention having the dimensions shown in Table 1 and the shape shown in FIG. Losses were measured. The result is the fifth
This is shown in Figures 1 to 10.
【表】
測定は冷媒としてフレオンR−22を用いた二重
管式熱交換器に各伝熱管を組み込み、蒸発特性の
測定は蒸発圧力を3.5〜4.2Kgf/cm2Gとし、凝縮
特性の測定は凝縮圧力を17.0〜18.2Kgf/cm2Gと
して行なつた。また伝熱管の長さはすべて5mと
した。
第5図は横軸に冷媒流量を縦軸に管内蒸発伝熱
性能を表わしたもので、本発明伝熱管No.1〜No.4
は何れも従来の平滑管No.8と比較し、約3倍、従
来の内面溝付管No.5〜No.7と比較しても約1.3〜
1.5倍の管内蒸発性能を有していることが判る。
また第6図は横軸に冷媒流量を、縦軸に管内凝縮
伝熱性能を表わしたもので、本発明伝熱管No.1〜
No.4は、従来の平滑管No.8と比較し、約2.8倍、
従来の内面溝付管No.5〜No.7と比較しても約1.2
〜1.5倍の管内凝縮伝熱性能を有することが判る。
第7図は横軸に冷媒流量を、縦軸に圧力損失を
表わしたもので、本発明伝熱管No.1〜No.4は従来
の内面平滑管No.8と比較し、同一冷媒流量におい
て、圧力損失が幾分大きくなつているが、従来の
内面溝付管No.5〜7と比較し、ほとんど同等であ
る。また第8図は第1表中の本発明伝熱管No.1に
ついて、管軸に対して逆方向のリード角α1,α2を
0゜〜60゜の範囲で変化させ、冷媒流量を50Kg/h
に固定して管内伝熱性能と圧力損失を測定した結
果を示したもので、横軸にリード角α1,α2を縦軸
に管内熱伝達率と圧力損失(図中Aは蒸発性能、
Bは凝縮性能、△Pは圧力損失を示す)を表わし
た。図から判るようにリード角α1,α2が5゜以上で
は余り伝熱性能に差がなく、5゜末満では伝熱性能
が低下する。一方リード角α1,α2が45゜を越える
と圧力損失が急激に増大する。
第9図は同様にして第1表中本発明伝熱管No.4
について、突起高さhのみを0.02〜0.8mmの間で
変動させて管内伝熱特性と圧力損失を測定した結
果を示し、第10図は同じく第1表中本発明伝熱
管No.1について溝ピツチP1,P2を0.1〜1.2mmの範
囲で変化させて管内伝熱性能と圧力損失を測定し
た結果を示したもので、冷媒流量を50Kg/hに固
定して行なつた。図から判るように突起高さhが
0.05mm未満でも、溝ピツチP1,P2が0.2mm未満で
も蒸発性能A及び凝縮性能Bが著しく低下し、突
起高さhが0.75mmを越えても、溝ピツチP1,P2が
1.0mmを越えても圧力損失△Pが急激に増大して
いる。
このように本発明伝熱管は、管内でフレオン等
の冷媒を蒸発又は凝縮させ、管外を流れる流体と
の間で熱交換させるタイプの熱交換器の伝熱管と
して、圧力損失を増大させることなく蒸発及び凝
縮伝熱性能を著しく向上し得るもので、熱交換器
の小型化、軽量化又はコストダウンを可能にし、
更にはヒートパイプに使用し、伝熱性能を改善し
得る等顕著な効果を奏するものである。[Table] Each heat exchanger tube was installed in a double tube heat exchanger using Freon R-22 as the refrigerant, and the evaporation characteristics were measured at an evaporation pressure of 3.5 to 4.2 Kgf/cm 2 G, and the condensation characteristics were measured. The condensation pressure was set at 17.0 to 18.2 Kgf/cm 2 G. Moreover, the length of all heat exchanger tubes was 5 m. Figure 5 shows the refrigerant flow rate on the horizontal axis and the evaporative heat transfer performance in the tubes on the vertical axis.
Both are approximately 3 times larger than conventional smooth tube No. 8, and approximately 1.3 to 1.3 times larger than conventional internally grooved tubes No. 5 to No. 7.
It can be seen that the evaporation performance inside the tube is 1.5 times higher.
In addition, Fig. 6 shows the refrigerant flow rate on the horizontal axis and the condensation heat transfer performance in the tube on the vertical axis.
No. 4 is approximately 2.8 times larger than the conventional smooth tube No. 8.
Approximately 1.2 compared to conventional internally grooved tubes No. 5 to No. 7
It can be seen that the pipe condensation heat transfer performance is ~1.5 times higher. Fig. 7 shows the refrigerant flow rate on the horizontal axis and the pressure loss on the vertical axis. Heat exchanger tubes No. 1 to No. 4 of the present invention are compared with conventional smooth inner surface tube No. 8 at the same refrigerant flow rate. Although the pressure loss is somewhat larger, it is almost the same as the conventional internally grooved tubes No. 5 to 7. FIG. 8 also shows the lead angles α 1 and α 2 in the opposite direction to the tube axis for heat exchanger tube No. 1 of the present invention in Table 1.
Change the refrigerant flow rate in the range of 0° to 60° at 50 kg/h.
The figure shows the results of measuring the heat transfer performance and pressure loss in the tube by fixing the lead angles α 1 and α 2 on the horizontal axis, and the heat transfer coefficient and pressure loss in the tube on the vertical axis (A in the figure shows the evaporation performance,
B represents condensation performance and ΔP represents pressure loss). As can be seen from the figure, when the lead angles α 1 and α 2 are 5° or more, there is not much difference in heat transfer performance, and when the lead angles are less than 5°, the heat transfer performance decreases. On the other hand, when the lead angles α 1 and α 2 exceed 45°, the pressure loss increases rapidly. Similarly, FIG. 9 shows heat exchanger tube No. 4 of the present invention in Table 1.
Figure 10 shows the results of measuring the heat transfer characteristics and pressure loss in the tube by varying only the protrusion height h between 0.02 and 0.8 mm. This figure shows the results of measuring the in-pipe heat transfer performance and pressure loss while varying the pitches P 1 and P 2 in the range of 0.1 to 1.2 mm, with the refrigerant flow rate fixed at 50 kg/h. As can be seen from the figure, the protrusion height h is
Even if the groove pitches P 1 and P 2 are less than 0.05 mm, the evaporation performance A and condensation performance B will decrease significantly, and even if the protrusion height h exceeds 0.75 mm, the groove pitches P 1 and P 2 will decrease significantly.
Pressure loss △P increases rapidly even when it exceeds 1.0 mm. In this way, the heat exchanger tube of the present invention can be used as a heat exchanger tube in a type of heat exchanger that evaporates or condenses a refrigerant such as Freon inside the tube and exchanges heat with a fluid flowing outside the tube, without increasing pressure loss. It can significantly improve evaporation and condensation heat transfer performance, making it possible to reduce the size, weight, and cost of heat exchangers.
Furthermore, it can be used in heat pipes and has remarkable effects such as improving heat transfer performance.
第1図は本発明伝熱管の一例を一部切欠いて示
す側面図、第2図は第1図の内面を拡大して示す
斜視図、第3図は第2図のY−Y線における断面
図、第4図は第2図のX−X線における断面図、
第5図乃至第7図は本発明伝熱管と従来伝熱管の
伝熱特性を示すもので、第5図は冷媒流量と管内
蒸発性能との関係図、第6図は冷媒流量と管内凝
縮性能との関係図、第7図は冷媒流量と圧力損失
との関係図、第8図は本発明伝熱管におけるリー
ド角と管内熱伝達率及び圧力損失との関係図、第
9図は同突起高さと管内熱伝達率及び圧力損失と
の関係図、第10図は同溝ピツチと管内熱伝達率
及び圧力損失との関係図である。
1……伝熱管、2,3……管軸に対して互いに
逆方向のリード角α1,α2を有する螺旋溝、4……
突起、A……蒸発特性、B……凝縮特性、△P…
…圧力損失。
Fig. 1 is a partially cutaway side view of an example of the heat transfer tube of the present invention, Fig. 2 is an enlarged perspective view of the inner surface of Fig. 1, and Fig. 3 is a cross section taken along line Y-Y in Fig. 2. Figure 4 is a cross-sectional view taken along line X-X in Figure 2,
Figures 5 to 7 show the heat transfer characteristics of the heat exchanger tube of the present invention and the conventional heat exchanger tube. Figure 5 is a relationship between the refrigerant flow rate and the evaporation performance in the tube, and Figure 6 is the relationship between the refrigerant flow rate and the condensation performance in the tube. Figure 7 is a diagram of the relationship between refrigerant flow rate and pressure loss, Figure 8 is a diagram of the relationship between lead angle, internal heat transfer coefficient and pressure loss in the heat exchanger tube of the present invention, and Figure 9 is a diagram of the relationship between the refrigerant flow rate and pressure loss. Fig. 10 is a diagram showing the relationship between the groove pitch, the heat transfer coefficient in the pipe, and pressure loss. 1... Heat exchanger tube, 2, 3... Spiral groove having lead angles α 1 and α 2 in mutually opposite directions with respect to the tube axis, 4...
Protrusion, A...evaporation property, B...condensation property, △P...
...Pressure loss.
Claims (1)
れる流体との間で熱交換を行なわせる伝熱管にお
いて、管内面に管軸に対して互いに逆方向のリー
ド角α1,α2を有する多数の螺旋状の溝と、該溝間
にそれぞれ同一形状の突起を形成し、リード角α1
の溝の螺旋方向にうねりを設け、リード角α2の溝
を螺旋方向に直進させ、突起のリード角α1の溝側
斜面を凹面とし、リード角α2の溝側斜面を凸面と
して、突起の形状を底辺が歪んだ菱形で、頂部が
鞍型又は丸味を有する菱形となし、螺旋状の溝の
リード角α1,α2を5〜45゜、リード角α1の溝のピ
ツチP1及びリード角α2の溝のピツチP2を0.2〜1.0
mm、突起の高さhを0.05〜0.75mmとしたことを特
徴とする伝熱管。 2 管軸に対して互いに逆方向のリード角α1,α2
をα1≒α2とする特許請求の範囲第1項記載の伝熱
管。 3 リード角α1の溝のピツチP1とリード角α2の
溝のピツチP2をP1≒P2とする特許請求の範囲第
1項又は第2項記載の伝熱管。 4 管の外径を6〜20mm、最小肉厚を0.2〜1.2mm
とする特許請求の範囲第1項、第2項又は第3項
記載の伝熱管。[Claims] 1. In a heat transfer tube that evaporates or condenses a refrigerant inside the tube and exchanges heat with a fluid flowing outside the tube, a lead angle α in mutually opposite directions with respect to the tube axis is formed on the inner surface of the tube. A large number of spiral grooves having lead angles α 1 and α 2 and protrusions of the same shape are formed between the grooves, and the lead angle α 1
The groove has undulations in the helical direction, the groove with a lead angle α 2 runs straight in the helical direction, the slope on the groove side of the protrusion with a lead angle α 1 is made concave, the slope on the groove side with a lead angle α 2 is made a convex surface, and the protrusion The shape is a rhombus with a distorted base and a saddle or rounded top, the lead angles α 1 and α 2 of the spiral groove are 5 to 45°, and the pitch of the groove with the lead angle α 1 is P 1 And the pitch P 2 of the groove with lead angle α 2 is 0.2 to 1.0.
mm, and the height h of the protrusions is 0.05 to 0.75 mm. 2 Lead angles α 1 and α 2 in opposite directions with respect to the tube axis
The heat exchanger tube according to claim 1, wherein α 1 ≒ α 2 . 3. The heat exchanger tube according to claim 1 or 2, wherein the pitch P 1 of the groove with a lead angle α 1 and the pitch P 2 of the groove with a lead angle α 2 satisfy P 1 ≈P 2 . 4. The outer diameter of the pipe should be 6 to 20 mm, and the minimum wall thickness should be 0.2 to 1.2 mm.
A heat exchanger tube according to claim 1, 2, or 3.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP18148481A JPS5883189A (en) | 1981-11-12 | 1981-11-12 | Heat-transmitting pipe |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP18148481A JPS5883189A (en) | 1981-11-12 | 1981-11-12 | Heat-transmitting pipe |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5883189A JPS5883189A (en) | 1983-05-18 |
| JPS6352310B2 true JPS6352310B2 (en) | 1988-10-18 |
Family
ID=16101560
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP18148481A Granted JPS5883189A (en) | 1981-11-12 | 1981-11-12 | Heat-transmitting pipe |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS5883189A (en) |
Families Citing this family (7)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US5203404A (en) * | 1992-03-02 | 1993-04-20 | Carrier Corporation | Heat exchanger tube |
| US6067712A (en) * | 1993-12-15 | 2000-05-30 | Olin Corporation | Heat exchange tube with embossed enhancement |
| US6176301B1 (en) * | 1998-12-04 | 2001-01-23 | Outokumpu Copper Franklin, Inc. | Heat transfer tube with crack-like cavities to enhance performance thereof |
| JP5566001B2 (en) * | 2007-03-30 | 2014-08-06 | 株式会社コベルコ マテリアル銅管 | Internally grooved heat transfer tube for gas coolers using carbon dioxide refrigerant |
| DE102009060395A1 (en) | 2009-12-22 | 2011-06-30 | Wieland-Werke AG, 89079 | Heat exchanger tube and method for producing a heat exchanger tube |
| JP5578415B2 (en) * | 2010-04-21 | 2014-08-27 | 株式会社リコー | Cooling device and image forming apparatus |
| JP7151253B2 (en) * | 2018-08-01 | 2022-10-12 | 株式会社デンソー | Heat transfer tubes and heat exchangers |
-
1981
- 1981-11-12 JP JP18148481A patent/JPS5883189A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5883189A (en) | 1983-05-18 |
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