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ACOUSTIC–MEAN FLOW INTERACTION AND VORTEX SHEDDING IN SOLID ROCKET MOTORS

✍ Scribed by A. KOURTA


Publisher
John Wiley and Sons
Year
1996
Tongue
English
Weight
898 KB
Volume
22
Category
Article
ISSN
0271-2091

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✦ Synopsis


The present work is devoted to the numerical simulation of two important phenomena in the field of solid propellant rocket motors: the first is acoustic boundary layers that develop above the burning propellant; the other is a periodic vortex-shedding phenomenon which is the result of a strong coupling between the instability of mean flow shear layers and acoustic motions in the chamber. To predict the acoustic boundary layer, computations were performed for the lower half of a rectangular chamber with bottom-side injection. The outflow pressure is sinusoidally perturbed at a given frequency. For the highest CFL numbers the implicit scheme is not able to compute the unsteadiness in the acoustic boundary layer. With very low CFL numbers or with the explicit scheme the main features of the acoustic field are captured. To simulate the vortex-shedding mechanism in a segmented solid rocket motor, the explicit version is used. This computation shows a mechanism for 'self-excited' vortex shedding close to the second axial mode frequency. The use of the flux-splitting technique reduces substantially the amplitude of the oscillations. A few iterations are done with flux splitting, then the computation is performed without this technique. In this case both the frequency and the intensity are well predicted. A geometry more representative of the solid rocket motor is also computed. In this case the vortex-shedding process is more complex and pairing is observed.


📜 SIMILAR VOLUMES


Shear layer instability and acoustic int
✍ A. Kourta 📂 Article 📅 1997 🏛 John Wiley and Sons 🌐 English ⚖ 232 KB

Segmentation of solid propellant rocket motors has been demonstrated to be a source of unpredicted and undesirable pressure and thrust oscillations. Surface discontinuities are the primary cause of these vortex-sheddingdriven oscillations, which result from a strong coupling between the shear layer