Transactions of the Visualization Society of Japan
Online ISSN : 1346-5260
ISSN-L : 1346-5252
Volume 27, Issue 12
Displaying 1-2 of 2 articles from this issue
  • Masahiro NAKASHIMA, Kentaro KURA, Takahide TABATA, Akira RINOSHIKA
    2007 Volume 27 Issue 12 Pages 105-112
    Published: 2007
    Released on J-STAGE: December 28, 2007
    JOURNAL FREE ACCESS
    The flow structures of the circular jet issuing from a pipe with the fluttering fins were experimentally investigated by the flow visualization of the LIF method and the PIV analysis. Especially, the effects of the fin length on the flow structures were studied. As a result, it is evident that the large-scale structures were broken into smaller-scale ones and the jet diffusion was enhanced in using the short fluttering fins, such as L/d=1.5. However, the long fluttering fins, such as L/d=2.5, caused the strong fluctuation of jet. Therefore, it may say that there exists a suitable fin length L/d=1.5, producing the strongest jet diffusion.
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  • Masashi KASHITANI, Yutaka YAMAGUCHI, Takeshi SUDA, Hideki KITANO
    2007 Volume 27 Issue 12 Pages 113-120
    Published: 2007
    Released on J-STAGE: December 28, 2007
    JOURNAL FREE ACCESS
    In the present study, we adopt a rod lighting system to the focusing schlieren system to obtain the higher and more uniform bright lighting at the test section. And flow visualization around a double wedge airfoil was performed in the transonic shock tube flow by using the focusing schlieren system. The span, chord length and maximum thickness of the model are 60mm, 75mm and 7.5mm, respectively. The hot gas Mach numbers (test Mach numbers) are from 0.80 to 0.86, and the Reynolds numbers are from 4.0x10^5 to 4.6x10^5. The test results show that an increment of light intensity was obtained by the experiments of the rod extended light source, and relatively constant light intensity was achieved at the test plane surface, and that, on the shock tube airfoil testing at the angle of attack 0 deg., if the Mach number is increased, the shock wave on the airfoil model moves to further downstream. This latter result is nearly the same as aerodynamic characteristics of NACA0012 airfoil model.
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