TW559639B - Detached turbulator configuration for cooling passages of gas turbine blades - Google Patents

Detached turbulator configuration for cooling passages of gas turbine blades Download PDF

Info

Publication number
TW559639B
TW559639B TW91110475A TW91110475A TW559639B TW 559639 B TW559639 B TW 559639B TW 91110475 A TW91110475 A TW 91110475A TW 91110475 A TW91110475 A TW 91110475A TW 559639 B TW559639 B TW 559639B
Authority
TW
Taiwan
Prior art keywords
turbulence
wall
adherent
rib
patent application
Prior art date
Application number
TW91110475A
Other languages
Chinese (zh)
Inventor
Tong-Miin Liou
Meng-Yu Chen
Original Assignee
Univ Feng Chia
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 Univ Feng Chia filed Critical Univ Feng Chia
Priority to TW91110475A priority Critical patent/TW559639B/en
Application granted granted Critical
Publication of TW559639B publication Critical patent/TW559639B/en

Links

Landscapes

  • Turbine Rotor Nozzle Sealing (AREA)

Abstract

A detached turbulator, which comprises a main body that forms a gap with a primary heat transfer surface, is arranged in a cooling passage to generate wall surface jets that accelerates the fluid and also break down thermal boundary layer and enhance turbulence to increase heat transfer gain and eliminate circulation occurring behind attached turbulator and the accompanying hot spots.

Description

559639 五、發明說明(1) ^ 【本發明的詳細說明】 本發明係有關於一種熱傳提昇的裝置,特別是針對渦 輪機葉片中的内冷卻流道表面突出物(肋條)之設計,因 此其實在是一種相當具有實用性及進步性之發明,相當值 得產業界來推廣,並公諸於社會大眾。 【本發明的背景說明】559639 V. Description of the invention (1) ^ [Detailed description of the present invention] The present invention relates to a heat transfer lifting device, especially for the design of the protrusions (ribs) on the surface of the inner cooling channel in the turbine blade, so in fact It is a very practical and progressive invention, which is worthy of being promoted by the industry and being made public. [Background of the invention]

按,在燃氣渦輪機之領域中,一般人常以提高渦輪機 進口之溫度,而可有效降低單位推力燃料消耗率並增加渦 輪機比功率以及提升循環效率。所以,先進渦輪機的設計 其進口溫度可達1 700 — 2000K,但因受限於渦輪 機葉片材料的溫度極限,因此目前發展出多種的冷卻技術 運用在渦輪機葉片冷卻上,用以降低葉片之溫度並令其達 到材料可承受之範圍,而内冷卻流道即為其中廣泛使用的 冷卻技術之一,其方法係在渦輪機葉片内加入内部流道, 並引入部分壓縮機產生的高壓冷空氣,而自渦輪機葉片根 部沿内流道進入葉片内,將葉片表面之高熱由葉片内部帶 走。In the field of gas turbines, most people often increase the temperature of the turbine inlet, which can effectively reduce the specific thrust fuel consumption rate, increase the specific power of the turbine, and improve cycle efficiency. Therefore, the design of the advanced turbine has an inlet temperature of 1 700-2000K. However, due to the temperature limit of the turbine blade material, a variety of cooling technologies have been developed for the cooling of turbine blades to reduce the temperature of the blades. Make it reach the range that the material can bear, and the internal cooling channel is one of the widely used cooling technologies. The method is to add the internal channel in the turbine blade and introduce the high-pressure cold air generated by the compressor. The root of the turbine blade enters the blade along the inner flow channel, and the high heat on the blade surface is taken away from the inside of the blade.

如上述之作動結構,茲再將其詳述之,請參閱第一圖 及第二圖所示,其係燃氣渦輪機葉片縱向剖面與橫截面示 意圖,其中渦輪機葉片2 0 0内具有蛇形冷卻流道2 1 0 ,此蛇形冷卻流道2 1 0是由多個徑向外流管道2 5 0 ( 流體朝向葉片頂部2 0 1流動)與徑向内流管道2 5 1 ( 流體遠離葉片頂部2 0 1流動)所組成,而徑向外流管道 250與徑向内流管道25 1則是由迎風壁30、背風壁The above-mentioned operating structure will be described in detail. Please refer to the first and second figures, which are schematic diagrams of the longitudinal section and cross-section of a gas turbine blade, in which the turbine blade 2000 has serpentine cooling Flow channel 2 1 0, this serpentine cooling flow channel 2 1 0 is composed of multiple radial outflow pipes 2 5 0 (the fluid flows toward the blade top 2 0 1) and radial inflow pipes 2 5 1 (the fluid is away from the blade top 2 0 1 flow), while the radial outflow pipe 250 and the radial inflow pipe 25 1 are composed of the windward wall 30 and the leeward wall

第4頁 559639 五、發明說明(2) 3 1以及二個隔板3 2與3 3所形成之内流道; 該冷流體2 0 4從渦輪機葉片根部2 0 2進入蛇形冷 卻流道2 1 0 ,流過徑向外流管道2 5 0與徑向内流管道 2 5 1 ,最後可經由葉片頂部2 0 1上的洞2 0 3排出; 承上所述,然一般人為增加其内冷卻流道的熱傳效率 ,常見的做法係於内冷卻流道表面安置有不同形狀與配置 之肋條或稱紊流增益器,其主要的目的係藉由流體與壁面 有更激烈的交互作用而增加熱傳。 然觀之習知之肋條結構,請參閱第三圖所示,係習知 之貼壁式正交肋條於徑向外流之内流道冷卻方式之側視圖 與A — A之剖面視圖,在内流道主要熱傳壁面:迎風壁内 面3 0A與背風壁内面3 1 A加上了貼壁式正交肋條4 0 ,利用肋條周圍的流場加速1 1 ,來破壞熱邊界層的成長 ,並增加紊流動能,以增進熱傳效率,亦或如第四圖所示 ,係習知之貼壁式正交肋條於徑向内流之内流道冷卻方式 的側視圖與B — B剖面視圖,其係於迎風壁内面3 Ο A與 背風壁内面3 1 A加上了貼壁式正交肋條,來促進熱傳效 率,然上述之兩者結構,於使用上卻未能臻至完善,茲將 其缺陷敘述如下: 1、 首先因第三圖或第四圖之肋條40後緣會有低速 迴流區1 2產生,如此而造成局部低熱傳區域,會有熱點 存在,而影到整體結構之功效; 2、 又,當渦輪機在運轉時(旋轉方向100),該 葉片内流道2 5 0與2 5 1内的流體會受葉片轉動的影響Page 4 559639 V. Description of the invention (2) 3 1 and the inner flow channel formed by the two partition plates 3 2 and 3 3; the cold fluid 2 0 4 enters the serpentine cooling flow channel 2 from the turbine blade root 2 0 2 1 0, flowing through the radial outflow pipe 2 50 and the radial inflow pipe 2 5 1, and finally can be discharged through the hole 2 0 3 on the blade top 2 0 1; as mentioned above, but generally the artificial cooling is increased. The heat transfer efficiency of the flow channel is a common practice. Ribs or turbulence gainers with different shapes and configurations are arranged on the surface of the internal cooling flow channel. The main purpose is to increase the flow through the more intense interaction between the fluid and the wall. Heat transfer. However, for the conventional rib structure, please refer to the third figure, which is a side view of the cooling method of the inner channel with a conventional orthogonal rib in a radial outflow and a cross-sectional view of A—A. Main heat transfer wall surface: The inner surface of the windward wall 3A and the inner surface of the leeward wall 3 1A are added with close-fitting orthogonal ribs 40. The flow field around the ribs is accelerated by 1 1 to destroy the growth of the thermal boundary layer and increase the turbulence. Flow energy to improve heat transfer efficiency, or as shown in the fourth figure, it is a side view and a B-B cross-sectional view of the cooling method of a conventional internally-adhered orthogonal rib in a radial inflow. The inner surface of the windward wall 3 Ο A and the inner surface of the leeward wall 3 1 A are added with orthogonal ribs to promote heat transfer efficiency. However, the above two structures have not been perfected in use. The defects are described as follows: 1. First, a low-speed recirculation zone 12 will be generated at the trailing edge of the rib 40 in the third or fourth picture, which will cause local low heat transfer areas, and there will be hot spots, which affect the effectiveness of the overall structure; 2. Also, when the turbine is running (rotation direction 100), the blade The flow passage 250 and the fluid will affect the inner blade 251 is rotated by the

第5頁 559639 五、發明說明(3) 而承受一旋轉力,此旋轉力即是所知之科氏力,而科氏力 會造成内流道内流體產生循環流動,如第三圖所示,此循 環流動的方向與流體在内流道内徑向流動的方向有關,該 第三圖係描繪出了 一對在徑向外流管道2 5 0由於科氏力 作用而形成之相反循環流動1 5與1 6 ,使流體從迎風壁 3 0朝背風壁3 1移動。相對地,第四圖則描繪出在徑向 内流管道2 5 1由於科氏力作用而形成之相反循環流動1 7與1 8,使流體從背風壁3 1朝迎風壁3 0移動; 而由於科氏力的影響,將使得内流道内的流體1 0朝 向背風壁3 1 ,而形成有二次流1 5與1 6 ,此二次流1 5與1 6係直接衝擊背風壁内面3 1 A,如此而增加背風 壁3 1的熱傳增益,而如第四圖則因主流2 0流向不同, 造成科氏力朝向迎風壁3 0 ,所形成的二次流1 7與1 8 直接衝擊迎風壁内面3 0A,增加迎風壁3 0的熱傳效益 如上述可知,二次流1 5、1 6雖可增加單面熱傳效 益,但對於另一面則會造成熱傳效果變差之情形,其如第 三、四圖所示,當管流為徑向外流時,背風壁熱傳增益, 迎風壁熱傳即變差,而又當管流為徑向内流時,背風壁熱 傳會變差,迎風壁之熱傳則呈增益狀; 由此可知,習知之紊流增益器,其不僅易於肋條4 0 後緣會有低速迴流區1 2產生,而造成局部低熱傳區域之 熱點產生,其亦會因葉片轉動時,而伴隨著科氏力之產生 ’造成結構上之缺陷’而此主要亦係因先前的技術在設計Page 5 559639 V. Description of the invention (3) When subjected to a rotating force, this rotating force is known as the Coriolis force, and the Coriolis force will cause the fluid in the inner channel to circulate, as shown in the third figure, The direction of this circulating flow is related to the direction of the radial flow of the fluid in the internal flow channel. The third diagram depicts a pair of opposite circulating flows formed in the radially outward flowing pipeline 2 5 0 due to the Coriolis force. 16 to move the fluid from the windward wall 30 to the leeward wall 31. In contrast, the fourth diagram depicts the reverse circulating flow 17 and 18 formed by the Coriolis force in the radial inflow pipe 2 5 1, so that the fluid moves from the leeward wall 31 to the windward wall 30; Due to the influence of the Coriolis force, the fluid 10 in the inner flow channel is directed toward the leeward wall 3 1, and secondary flows 15 and 16 are formed. The secondary flows 15 and 16 directly impact the inner surface 3 of the leeward wall. 1 A, thus increasing the heat transfer gain of the leeward wall 31, and as shown in the fourth figure, the Coriolis force is directed toward the windward wall 30 due to the different flow direction of the mainstream 20, and the secondary flow 1 7 and 1 8 formed directly Shock the inner surface of the windward wall 30A, increase the heat transfer benefit of the windward wall 30. As can be seen from the above, although the secondary flow 15 and 16 can increase the heat transfer benefit on one side, it will cause the heat transfer effect to deteriorate on the other side. As shown in the third and fourth figures, when the tube flow is radially outward, the leeward wall heat transfer gain is deteriorated, and the windward wall heat transfer becomes worse, and when the tube flow is radially inward, the leeward wall heat is increased. The heat transfer will be worse, and the heat transfer of the windward wall will show a gain. From this, it can be known that the conventional turbulence gain device is not only easy to rib 40 The low-speed recirculation zone 12 is generated, resulting in hot spots in the local low heat transfer area. It will also be caused by the Coriolis force when the blades rotate, which is mainly due to the previous technology. design

第6頁 559639 559639 五、發明說明(5) ·、 本發明係有關於一種渦輪機葉片内冷卻流道之非貼壁 式紊流增益器裝置,請參閱第五圖與第六圖係本發明非貼 壁式紊流增益器及其配置方式於徑向外流與徑向内流之内 流道冷卻方式的側視圖與剖面視圖。 如第五圖與第六圖所示,肋條4 1與主要熱傳壁面: 迎風壁3 0與背風壁3 1存在有一間隙C,流體流經此間 隙C時,產生壁面喷流1 3以及對流體有加速作用,可增 加紊流動能,提昇熱傳增益,並且可消除貼壁式肋條所產 生的熱點。 而根據實際實驗結果發現(如第1表所示,請參閱附 件一),非貼壁式紊流增益器4 1於徑向外流2 5 0之迎 風壁3 0與徑向内流之背風壁3 1 ,較習知之貼壁式正交 肋條4 0擁有較佳之熱傳係數,最高約可增加2 1 %,但 是,非貼壁式紊流增益器4 1於徑向外流2 5 0之背風壁 3 1與徑向内流之迎風壁3 0 ,則較習知之貼壁式正交肋 條4 0擁有較差之熱傳係數,這是由於非貼壁式紊流增益 器4 1所產生之壁面喷流1 3削弱了流體因科氏力作用對 壁面的衝擊。 另外,如第2表所示,非貼壁式紊流增益器4 1其熱 傳均勻性較習知之貼壁式正交肋條4 0為佳。 基於上述,爰是,本發明人發明出一種非貼壁式/貼 壁式紊流增益器及其配置方式。第七圖與第八圖係本發明 非貼壁式/貼壁式紊流增益器及其配置方式於徑向外流與 徑向内流之内流道冷卻方式的側視圖與剖面視圖。如第七Page 6 559639 559639 V. Description of the invention (5) · The present invention relates to a non-adherent turbulence gain device for a cooling channel in a turbine blade. Please refer to the fifth and sixth figures of the present invention. Side view and cross-sectional view of a wall-mounted turbulence gainer and its configuration in the inner channel cooling mode of radial outward and radial inflow. As shown in the fifth and sixth figures, the rib 41 and the main heat transfer wall surface: There is a gap C between the windward wall 30 and the leeward wall 31, and when the fluid flows through this gap C, a wall jet 13 and a The fluid has an acceleration effect, which can increase the turbulent flow energy, increase the heat transfer gain, and eliminate hot spots generated by the adherent ribs. According to the actual experimental results (as shown in Table 1, please refer to Annex 1), the non-adherent turbulence gainer 41 is located on the windward wall 30 of the radial outflow 2 50 and the leeward wall of the radial inflow. 3 1, which has a better heat transfer coefficient than the conventional wall-mounted orthogonal ribs 40, which can increase by about 21%, but the non-wall-mounted turbulence gainer 41 is leeward from the radial outflow 2 5 0 The wall 31 and the windward wall 30 of the radial inward flow have a lower heat transfer coefficient than the conventional wall-mounted orthogonal ribs 40, which is due to the wall surface generated by the non-wall-mounted turbulence gain device 41. The jets 1 3 weaken the impact of the fluid on the wall due to the Coriolis force. In addition, as shown in Table 2, the heat transfer uniformity of the non-adherent turbulence gainer 41 is better than that of the conventional orthogonal ribs 40. Based on the above, it is true that the inventor has invented a non-adherent / adherent turbulence gain device and a configuration manner thereof. The seventh and eighth figures are side and cross-sectional views of a non-adherent / adherent turbulent flow gain device and a cooling method of an inner flow channel in a radial outflow and a radial inflow according to the present invention. As seventh

第8頁 559639 五、發明說明(6) 圖與第八圖所示,肋條4 1與徑向外流2 5 0之迎風壁内 面3 Ο A以及徑向内流之背風壁内面3 1 B存在有一間隙 C,流體流經此間隙C時,產生壁面喷流1 3以及對流體 有加速作用,可增加棄流動能,提昇熱傳係數,並且可消 除點壁式肋條所產生的熱點;肋條4 0與徑向外流2 5 0 之背風壁内面3 1 A以及徑向内流之迎風壁内面3 Ο B緊 密接合,維持科氏力的作用,保持較佳之熱傳係數。 第九圖與第十圖是本發明之非貼壁式/貼壁式紊流增 益器及其配置方式之設計參數示意圖,Η代表非貼壁式或 貼壁式肋條的高度,W代表非貼壁式或貼壁式肋條的寬度 ,乙代表非貼壁式或貼壁式肋條的長度,C代表非貼壁式 肋條與主熱傳壁面的間隙,其中W/H的值為介於0 · 2 一 5内的任一值,C/Η的值為介於0 · 2 — 1内的任一 值。Ρ代表肋條節距,即相鄰熱傳增益器之間隔距離,本 發明之非貼壁式/貼壁式紊流增益器4 1與4 0可以依内 流道長度任意選定肋條節距Ρ ,以各種數量組合,安置在 内流道壁面,以達到内流道冷卻之目的。 第1表是本發明與習知之貼壁式正交肋條於内流道冷 卻設計之熱傳增益性能比較,結果顯示非貼壁式紊流增益 器4 1於徑向外流2 5 0之迎風壁3 0與徑向内流2 5 1 之背風壁3 1 ,較習知之貼壁式正交肋條4 0擁有較佳之 熱傳係數,最高約可增加2 1 %,但是,非貼壁式紊流增 益器4 1徑向外流2 5 0之背風壁3 1與徑向内流2 5 1 之迎風壁3 0 ,則較習知之貼壁式正交肋條4 0擁有較差Page 8 559639 V. Description of the invention (6) As shown in the figure and the eighth figure, the rib 4 1 and the inner surface of the windward wall 3 0 A with radial outflow 2 5 0 and the inner surface of the leeward wall 3 1 B with radial inflow exist. Gap C, when the fluid flows through this gap C, the wall jet 13 and the acceleration of the fluid can increase the abandoned flow energy, improve the heat transfer coefficient, and eliminate the hot spots generated by point wall ribs; ribs 4 0 It is tightly connected to the inner surface 3 1 A of the leeward wall with radial outflow 2 50 and the inner surface 3 0 B of the windward wall with radial inflow to maintain the Coriolis force and maintain a better heat transfer coefficient. The ninth figure and the tenth figure are schematic diagrams of design parameters of the non-adherent / adherent turbulence gain device and its configuration of the present invention. The width of the wall or wall-mounted rib, B represents the length of the non-wall-mounted or wall-mounted rib, and C represents the gap between the non-wall-mounted rib and the main heat transfer wall surface, where the value of W / H is between 0 · Any value between 2 and 5 and the value of C / Η is any value between 0 · 2 — 1. P represents the rib pitch, that is, the distance between adjacent heat transfer gain devices. The non-adherent / adherent turbulence gain devices 41 and 40 of the present invention can arbitrarily select the rib pitch P according to the length of the inner flow channel. The wall surface of the inner flow channel is arranged in various quantities to achieve the purpose of cooling the inner flow channel. The first table is a comparison of the heat transfer gain performance of the present invention and the conventional adherent orthogonal ribs in the cooling design of the inner flow channel. The results show that the non-adherent turbulence gainer 41 is in the windward wall of the radial outflow 2 50. The leeward wall 3 1 of 3 0 and radial inflow 2 5 1 has a better heat transfer coefficient than the conventional close-mounted orthogonal ribs 40, which can increase up to about 21%. However, non-adherent turbulence Gainer 4 1 leeward wall 3 1 with radial outflow 2 5 0 and windward wall 3 0 with radial inward flow 2 5 1 have worse performance than the conventional close-mounted orthogonal rib 4 0

第9頁 559639 五、發5月說明(Ό 之熱傳增益。而本發明之非貼壁式/貼壁式紊流增益器於 徑向外流2 5 0之迎風壁3 0與徑向内流2 5 1之背風壁 3 1 ,較習知之貼壁式正交肋條4 0擁有較佳之熱傳增益 ,最高約可增加4 2 %,而於徑向外流2 5 0之背風壁3 1與徑向内流2 5 1之迎風壁3 0 ,仍可維持貼壁式正交 肋條4 0之熱傳增益。Page 9 559639 V. May explanation (The heat transfer gain of Ό. And the non-adherent / adherent turbulence gain device of the present invention flows outward in the radial wall 2 50 and the radial inflow 2 50 The leeward wall 3 1 of 2 5 1 has a better heat transfer gain than the conventional close-mounted orthogonal ribs 40, which can increase up to about 4 2%, while the leeward wall 3 1 and the radial outflow 2 5 0 The windward wall 3 0 flowing inward 2 5 1 can still maintain the heat transfer gain of the close orthogonal ribs 40.

第2表是本發明與習知之貼壁式正交肋條於内流道冷 卻設計之熱傳不均勻性比較,結果顯示非貼壁式紊流增益 器4 1擁有最佳之熱傳均勻性,非貼壁式/貼壁式紊流增 益器次之,而貼壁式正交肋條4 0最差。 附件一說明: 第1表:係為本發明與習知技術(貼壁式正交肋條)之熱傳 係數比較實驗結果。 第2表:係為本發明與習知技術(貼壁式正交肋條)之熱傳 不均勻性比較實驗結果。The second table is a comparison of the heat transfer inhomogeneity between the present invention and the conventional orthogonal ribs in the inner channel cooling design. The results show that the non-adherent turbulence gainer 41 has the best thermal uniformity. Non-adherent / adherent turbulence gainers are next, and adhering orthogonal ribs 40 are the worst. Explanation of Annex 1: Table 1: The experimental results of comparison of the heat transfer coefficients of the present invention and the conventional technology (adhered orthogonal ribs). Table 2: The experimental results of the heat transfer inhomogeneity comparison between the present invention and the conventional technique (adherent orthogonal ribs).

第ίο頁 559639 圖式簡單說明 / 本發明的較佳實施例可以配合所附的圖式而作一更加 詳細的說明,俾使審查委員對於本發明可以獲致更進一步 之瞭解,其中: A ·主要元件符號說明: 10 徑向外流之冷卻流體主流 11 肋條周圍流體 12 低速迴流區 13 壁面喷流 15 二次流 16 二次流 17 二次流 18 二次流 20 徑向内流之冷卻流體主流 21 肋條周圍流體 23 壁面喷流 30 迎風壁 3 0 A徑向外流之迎風壁内面 3 0 B徑向内流之迎風壁内面 31 背風壁 3 1 A徑向外流之背風壁内面 3 1 B徑向内流之背風壁内面 32 左隔板 33 右隔板 40 貼壁式正交肋條Page ί 559639 Brief description of the drawings / The preferred embodiment of the present invention can be described in more detail in conjunction with the attached drawings, so that the reviewers can obtain a further understanding of the present invention, of which: A · Main Description of component symbols: 10 The main stream of cooling fluid flowing radially 11 The fluid around the ribs 12 Low-speed return zone 13 Wall spray 15 The second stream 16 The second stream 17 The second stream 18 The second stream 20 The main stream of cooling fluid radially inward 21 Fluid around the ribs 23 Wall jet 30 Windward wall 3 0 A Inward wall of radial outflow 3 0 B Inward wall of radial inflow 31 Leeward wall 3 1 A Outward wall of radial outflow 3 1 B Inward radial Inside surface of the leeward wall of the stream 32 Left partition 33 Right partition 40 Adhesive orthogonal ribs

第11頁 559639 Λ 月 曰 修正 案號 91110475 圖式簡單說明 50 空氣入口 51 網狀加熱器 52 氬離子雷射 53 馬達 54 鼓風機 55 排氣 56 電腦 Β ·圖示編號說明: 第 一 圖 係 燃 氣 渦 輪 機 葉 片 縱 向 剖 面 示 意 圖 , 第 二 圖 係 燃 氣 渦 輪 機 葉 片 橫 截 面 示 意 圖 • 9 第 二 圖 係 貼 壁 式 正 交 肋 條 於 徑 向 外 流 管 道 之 冷 卻 方 式 第 四 圖 係 貼 壁 式 正 交 肋 條 於 徑 向 内 流 管 道 之 冷 卻 方 式 , 第 五 圖 係 本 發 明 非 貼 壁 式 正 交 肋 條 於 徑 向 外 流 管 道 之 冷 卻 方 式 第 六 圖 係 本 發 明 非 貼 壁 式 正 交 肋 條 於 徑 向 内 流 管 道 之 冷 卻 方 式 第 七 圖 係 本 發 明 非 貼 壁 式 / 貼 壁 式 正 交 肋 條 於 徑 向 外 流 管 道 之冷卻 方 式 ’ 第 八 圖: :係 本 發 明 非 貼 壁 式 / 貼 壁 式 正 交 肋 條 於 徑 向 内 流 管 道 之冷卻 方 式 , 第 九 圖 :係 本 發 明 非 貼 壁 式 / 貼 壁 式 正 交 肋 條 於 徑 向 外 流 管 道 設計參 數 示 意 圖 , 第 十 TS1 圖 :係 本 發 明 非 貼 壁 式 / 貼 壁 式 正 交 肋 條 於 徑 向 内 流 管道設計參數示意圖;以及 第十一圖:係本實驗之設備裝置示意圖。Page 11 559639 Λ Month Amendment No. 91110475 Brief description of the diagram 50 Air inlet 51 Mesh heater 52 Argon ion laser 53 Motor 54 Blower 55 Exhaust 56 Computer B Schematic diagram of the longitudinal section of a turbine blade. The second diagram is a schematic diagram of the cross section of a gas turbine blade. • The second diagram is the cooling method of the close-out orthogonal ribs in the radial outflow pipe. The fourth diagram is the close-up orthogonal ribs in the radial direction. The cooling method of internal flow pipes, the fifth figure is the cooling method of the non-adherent orthogonal ribs of the present invention in the radial outflow pipe. The seventh diagram is the cooling method of the non-adherent / adherent orthogonal ribs in the radial outflow pipe according to the present invention. The eighth diagram: The non-adhesive according to the present invention Cooling method of wall / adherent orthogonal ribs in radial inflow pipes, Figure 9: Schematic diagram of design parameters of non-adherent / adherent orthogonal ribs in radial outflow pipes of the present invention, Tenth TS1 diagram : It is a schematic diagram of the design parameters of the non-adherent / adherent orthogonal ribs in the radial inflow pipeline of the present invention; and the eleventh diagram: a schematic diagram of the equipment of the experiment.

第13頁Page 13

Claims (1)

559639 六、申請專利祀圍 ·' 1 、一種非貼壁式紊流增益器,主體為一任意形狀截 面之肋條,其中於肋條與壁面間存有一間隙者。 2 、如申請專利範圍第1項所述之非貼壁式紊流增益 器,其中該肋條係為矩形。 3 、如申請專利範圍第2項之紊流增益器,其中矩形 截面肋條的寬高比可為大於0 · 2且小於5之任意選定值 〇 4 、如申請專利範圍第1項之紊流增益器,其中間隙 與肋條高度的比可為大於0·2且小於1之任意選定值。 5 、如申請專利範圍第1項之紊流增益器,主體為一 三角形截面之肋條。 6 、如申請專利範圍第5項之紊流增益器,其中肋條 截面可為任意三角形。 7 、如申請專利範圍第5項之紊流增益器,其中間隙 與肋條高度的比可為大於0 · 2且小於1之任意選定值。 8 、如申請專利範圍第1項之紊流增益器,主體為一 圓形截面肋條。 9 、如申請專利範圍第8項之紊流增益器,其中間隙 與圓形截面肋條直徑的比可為大於0 · 2且小於1之任意 選定值。 1 0、一種内流道冷卻方式,採用申請專利範圍第1項 之紊流增益器,該紊流增益器可以任意之數量與位置組合 ,安置於内流道之壁面。 1 1 、一種非貼壁式/貼壁式紊流增益器配置,採用如559639 VI. Application for patent enclosing sacrifice · '1. A non-adherent turbulence gain device, the main body of which is a rib with any cross section, with a gap between the rib and the wall. 2. The non-adherent turbulence gain device as described in item 1 of the scope of patent application, wherein the ribs are rectangular. 3. The turbulence gain device as described in the second item of the patent application, wherein the width-to-height ratio of the rectangular cross-section ribs can be any selected value greater than 0 · 2 and less than 5. The turbulence gain as described in the first item of the patent application Device, wherein the ratio of the gap to the rib height can be any selected value greater than 0 · 2 and less than 1. 5. If the turbulence gain device in the first item of the patent application scope, the main body is a rib with a triangular cross section. 6. The turbulence gain device according to item 5 of the patent application, wherein the rib cross section can be any triangle. 7. The turbulence gain device according to item 5 of the patent application, wherein the ratio of the gap to the rib height can be any selected value greater than 0 · 2 and less than 1. 8. As for the turbulence gain device in the first scope of the patent application, the main body is a circular cross-section rib. 9. The turbulence booster according to item 8 of the scope of the patent application, wherein the ratio of the gap to the diameter of the circular cross-section rib may be any selected value greater than 0 · 2 and less than 1. 10. An internal flow channel cooling method adopts the turbulence gain device of the first patent application scope. The turbulence gain device can be combined in any number and position and placed on the wall surface of the internal flow channel. 1 1. A non-adherent / adherent turbulence gain configuration, using 第14頁 559639 六、申請專利範圍 申請專利範圍第1項之非貼壁式紊流增益器安置在與科氏 力方向相反的内流道壁面,貼壁式紊流增益器安置在與科 氏力方向相同的内流道壁面,以提高熱傳效率。Page 14 559639 VI. Application for patent scope The non-adherent turbulence booster of item 1 of the patent scope is placed on the wall surface of the inner flow channel opposite to the Coriolis force direction. The inner flow channel wall surface with the same force direction to improve the heat transfer efficiency. 第15頁Page 15
TW91110475A 2002-05-20 2002-05-20 Detached turbulator configuration for cooling passages of gas turbine blades TW559639B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
TW91110475A TW559639B (en) 2002-05-20 2002-05-20 Detached turbulator configuration for cooling passages of gas turbine blades

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
TW91110475A TW559639B (en) 2002-05-20 2002-05-20 Detached turbulator configuration for cooling passages of gas turbine blades

Publications (1)

Publication Number Publication Date
TW559639B true TW559639B (en) 2003-11-01

Family

ID=32322866

Family Applications (1)

Application Number Title Priority Date Filing Date
TW91110475A TW559639B (en) 2002-05-20 2002-05-20 Detached turbulator configuration for cooling passages of gas turbine blades

Country Status (1)

Country Link
TW (1) TW559639B (en)

Similar Documents

Publication Publication Date Title
US8128366B2 (en) Counter-vortex film cooling hole design
Ekkad et al. A review of hole geometry and coolant density effect on film cooling
JP5826516B2 (en) System and method for facilitating mixing of turbine wakes using fluidly generated vortices
CN106437863B (en) Turbine engine component
US7637720B1 (en) Turbulator for a turbine airfoil cooling passage
CN100485166C (en) Grooving gaseous film cooling hole
RU2299991C2 (en) Turbine blade
US9017027B2 (en) Component having cooling channel with hourglass cross section
CN101245974A (en) Finned heat exchanger
JP2007198727A (en) Wall elements for gas turbine engine combustors
US8876475B1 (en) Turbine blade with radial cooling passage having continuous discrete turbulence air mixers
JP2011089519A (en) Structure and method for improving film cooling using shallow trench with holes oriented along length of trench
JP5635816B2 (en) Cooling hole outlet for turbine bucket tip shroud
RU2285804C1 (en) Member of gas-turbine engine and method of its manufacture
WO2007077968A1 (en) Heat transfer device
CN112459852B (en) Be applied to two water conservancy diversion rib water conservancy diversion structures of turbine blade trailing edge half-splitting seam
JP2007327494A (en) Turbine engine component and cooling micro circuit
JP2008546984A (en) Heat transfer venturi
CN108757047A (en) Turbine blade of gas turbine with cooling structure inside the droplet-shaped rib of column
CN109931114A (en) A kind of novel impinging cooling turbulence structure
CN112343666B (en) Be applied to half corrugated rib water conservancy diversion structure of splitting seam of turbine blade trailing edge
US8281564B2 (en) Heat transfer tubes having dimples arranged between adjacent fins
US9644903B1 (en) Shaped recess flow control
AU2019339973B2 (en) Stator assembly, motor having same and wind power generator set
TW559639B (en) Detached turbulator configuration for cooling passages of gas turbine blades

Legal Events

Date Code Title Description
GD4A Issue of patent certificate for granted invention patent