Newsletter 2023.10 Index
| Theme : "AJK FED 2023" 
 | 
Unsteady Characteristic of Tip Leakage Vortex Cavitation in the Occurrence of Cavitation Instability in Inducer
|  Koki TAMURA Tohoku University,  Yuto NAKURA Tohoku University,  Satoshi KAWASAKI Japan Aerospace Exploration Agency,  Yuka IGA Tohoku University | 
Abstract
Cavitation is a phase change phenomenon from liquid to gas that occurs in the low-pressure region of high-speed fluid machinery. In liquid rocket inducer, the tip leakage vortex cavitation (T.L.V.C.) is the primary occurrence, and unsteady oscillation of T.L.V.C. causes pump unstable, called cavitation instability. This instability frequently encountered during the development of the turbopump. Therefore, it is crucial to elucidate the unsteady characteristics of T.L.V.C. as a cause of cavitation instability. The present study focuses on T.L.V.C. arising in the inducer, with particular emphasis on cavity length. Additionally, the fundamental characteristics of T.L.V.C. arising in NACA0009 hydrofoil with tip clearance is also examined to consider the characteristics of T.L.V.C. in the inducer.
 The  tested inducer and hydrofoil are depicted in Fig. 1 and 2. Cavitation was  visualized to determine the cavity length and frequency of cavity oscillation  in both experiments, and the Strouhal number based on cavity length ( ) was calculated.
) was calculated.
In the inducer experiment, it was found that the  characteristic of  of T.L.V.C.  in the occurrence of cavitation surge (C.S.) differ from that of T.L.V.C. in  super-synchronous rotating cavitation (super-S R.C.). The result of
 of T.L.V.C.  in the occurrence of cavitation surge (C.S.) differ from that of T.L.V.C. in  super-synchronous rotating cavitation (super-S R.C.). The result of  in super-S  R.C. at the beginning to the middle is consistence with that of T.L.V.C.  arising in the hydrofoil. However, the characteristic of
 in super-S  R.C. at the beginning to the middle is consistence with that of T.L.V.C.  arising in the hydrofoil. However, the characteristic of  of T.LV.C. at  the end of super-S R.C. showed a different trend than before. Assuming that the  characteristic of
 of T.LV.C. at  the end of super-S R.C. showed a different trend than before. Assuming that the  characteristic of  of T.L.V.C.  arising in the hydrofoil represents the natural oscillation characteristic of  T.L.V.C., the T.L.V.C. at the beginning to the middle of super-S R.C. oscillate  naturally. Subsequently super-S R.C. ended when the T.L.V.C. become less prone  to oscillation and starts transitioning to different mode of oscillation. In  contrast, the T.L.V.C. in the occurrence of C.S., which has different  characteristic of
 of T.L.V.C.  arising in the hydrofoil represents the natural oscillation characteristic of  T.L.V.C., the T.L.V.C. at the beginning to the middle of super-S R.C. oscillate  naturally. Subsequently super-S R.C. ended when the T.L.V.C. become less prone  to oscillation and starts transitioning to different mode of oscillation. In  contrast, the T.L.V.C. in the occurrence of C.S., which has different  characteristic of  from  T.L.V.C. arising in hydrofoil, oscillates unnaturally.
 from  T.L.V.C. arising in hydrofoil, oscillates unnaturally.
Key words
Rotating Cavitation, Cavitation Surge, Tip Leakage Vortex Cavitation, Inducer, NACA0009
Figures

        Fig. 1       Tested inducer (THK inducer).

        Fig. 2        Tested hydrofoil (NACA0009).

