Research of Supersonic Free-Vortex Aerodynamic Window : 1st Report, Design Procedure of Free Vortex Nozzle and Operating Condition
In the development of continuous high-power gas laser systems, the supersonic free-vortex aerodynamic window is one of the key technologies for extracting a laser beam from the laser cavity. The present paper describes the design procedure of the two-dimensional supersonic free-vortex nozzle, and de...
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Published in | Transactions of the Japan Society of Mechanical Engineers Series B Vol. 62; no. 599; pp. 2687 - 2694 |
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Main Authors | , , , |
Format | Journal Article |
Language | Japanese |
Published |
The Japan Society of Mechanical Engineers
25.07.1996
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Subjects | |
Online Access | Get full text |
ISSN | 0387-5016 1884-8346 |
DOI | 10.1299/kikaib.62.2687 |
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Abstract | In the development of continuous high-power gas laser systems, the supersonic free-vortex aerodynamic window is one of the key technologies for extracting a laser beam from the laser cavity. The present paper describes the design procedure of the two-dimensional supersonic free-vortex nozzle, and demonstrates the operating conditions of the window, taking into account the phase transition of the working fluid in the nozzle expansion process and the operating conditions of the supersonic diffuser. Generally, the high-power laser will be operated in the atmospheric environment without auxiliary equipment, i. e., a heater installed in the nozzle supply and/or a vacuum pump connected with the ventage of the supersonic diffuser. Therefore, the temperature of the working fluid at the nozzle supply is nearly 300 K, and the back pressure of the supersonic diffuser is inevitably atmospheric pressure. Hence, when using nitrogen gas as the working fluid in such an environment, the pressure ratio of the laser cavity to the atmosphere, which can be achieved with no phase transition, is about 20. In order to attain the higher pressure ratio of about 50, helium gas is required as the working fluid. |
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AbstractList | In the development of continuous high-power gas laser systems, the supersonic free-vortex aerodynamic window is one of the key technologies for extracting a laser beam from the laser cavity. The present paper describes the design procedure of the two-dimensional supersonic free-vortex nozzle, and demonstrates the operating conditions of the window, taking into account the phase transition of the working fluid in the nozzle expansion process and the operating conditions of the supersonic diffuser. Generally, the high-power laser will be operated in the atmospheric environment without auxiliary equipment, i. e., a heater installed in the nozzle supply and/or a vacuum pump connected with the ventage of the supersonic diffuser. Therefore, the temperature of the working fluid at the nozzle supply is nearly 300 K, and the back pressure of the supersonic diffuser is inevitably atmospheric pressure. Hence, when using nitrogen gas as the working fluid in such an environment, the pressure ratio of the laser cavity to the atmosphere, which can be achieved with no phase transition, is about 20. In order to attain the higher pressure ratio of about 50, helium gas is required as the working fluid. |
Author | NANBA, Kazumi WADA, Tomohisa SONODA, Keisuke OHIRA, Katsuhide |
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References | (3) Masuda, W. and Yuasa, M., J. P., Colloque C9, supplement au n_??_ll, Tome 41 (1980), C9-423-429. (9) 生井武文•松尾一泰,機械工学基礎講座圧縮性流体の力学,(1978), 88-90,理工学社. (6) 松尾一泰•ほか3名,機論,50-459,B (1983), 2557-2582. (2) Guile, R. N. and Hilding, W. E., AIAA Paper, 75 122 (1975). (5) Gilerson, A. A.,ほか4名,Sov. Phys. Tech. Phys., 35-12 (1990), 1379-1382. (8) ENCYCLOPEDIE DES GAZ, (1976), ELSEVIER/L′AIRLIQUIDE. (4) Emanuel, G., Gasdynamics: Theory and Applications, AIAA E. S., (1986), 329-345. (1) Parmentier, E. M. and Greenberg, R. A., AIAA J., 11-7 (1973), 943-949. (7) Shapiro, A. H., The Dynamics and Thermodynamics of COMPRESSIBLE FLUID FLOW, I (1953), 512-516, THE RONALD PRESS COMPANY. |
References_xml | – reference: (6) 松尾一泰•ほか3名,機論,50-459,B (1983), 2557-2582. – reference: (1) Parmentier, E. M. and Greenberg, R. A., AIAA J., 11-7 (1973), 943-949. – reference: (4) Emanuel, G., Gasdynamics: Theory and Applications, AIAA E. S., (1986), 329-345. – reference: (7) Shapiro, A. H., The Dynamics and Thermodynamics of COMPRESSIBLE FLUID FLOW, I (1953), 512-516, THE RONALD PRESS COMPANY. – reference: (5) Gilerson, A. A.,ほか4名,Sov. Phys. Tech. Phys., 35-12 (1990), 1379-1382. – reference: (9) 生井武文•松尾一泰,機械工学基礎講座圧縮性流体の力学,(1978), 88-90,理工学社. – reference: (3) Masuda, W. and Yuasa, M., J. P., Colloque C9, supplement au n_??_ll, Tome 41 (1980), C9-423-429. – reference: (8) ENCYCLOPEDIE DES GAZ, (1976), ELSEVIER/L′AIRLIQUIDE. – reference: (2) Guile, R. N. and Hilding, W. E., AIAA Paper, 75 122 (1975). |
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Snippet | In the development of continuous high-power gas laser systems, the supersonic free-vortex aerodynamic window is one of the key technologies for extracting a... |
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Title | Research of Supersonic Free-Vortex Aerodynamic Window : 1st Report, Design Procedure of Free Vortex Nozzle and Operating Condition |
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