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A time splitting projection scheme for compressible two-phase flows. Application to the interaction of bubbles with ultrasound waves

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Academic year: 2021

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Figure

Fig. 1. Comparison between Rayleigh–Plesset and Rayleigh–Plesset–Prosperetti equation
Fig. 3. Influence of the M parameter on the spatial accuracy of the Low Mach Preconditioning method with 16 computational cells on the initial bubble radius
Fig. 5. Comparison between the different numerical methods with 16 computational cells to discretize the initial radius of the bubble
Fig. 6. Temporal evolution of the bubble displacement in the x direction.
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