Eulerian-Lagrangian method for simulation of cloud cavitation

We present a coupled Eulerian-Lagrangian method to simulate cloud cavitation in a compressible liquid. The method is designed to capture the strong, volumetric oscillations of each bubble and the bubble-scattered acoustics. The dynamics of the bubbly mixture is formulated using volume-averaged equat...

Ausführliche Beschreibung

Bibliographische Detailangaben
Veröffentlicht in:Journal of computational physics. - 1986. - 371(2018) vom: 15. Okt., Seite 994-1017
1. Verfasser: Maeda, Kazuki (VerfasserIn)
Weitere Verfasser: Colonius, Tim
Format: Online-Aufsatz
Sprache:English
Veröffentlicht: 2018
Zugriff auf das übergeordnete Werk:Journal of computational physics
Schlagworte:Journal Article Bubble dynamics Cavitation Compressible multiphase flows Eulerian-Lagrangian method Multiscale modeling Reduced-order modeling
LEADER 01000caa a22002652 4500
001 NLM29365820X
003 DE-627
005 20250224195743.0
007 cr uuu---uuuuu
008 231225s2018 xx |||||o 00| ||eng c
024 7 |a 10.1016/j.jcp.2018.05.029  |2 doi 
028 5 2 |a pubmed25n0978.xml 
035 |a (DE-627)NLM29365820X 
035 |a (NLM)30739952 
040 |a DE-627  |b ger  |c DE-627  |e rakwb 
041 |a eng 
100 1 |a Maeda, Kazuki  |e verfasserin  |4 aut 
245 1 0 |a Eulerian-Lagrangian method for simulation of cloud cavitation 
264 1 |c 2018 
336 |a Text  |b txt  |2 rdacontent 
337 |a ƒaComputermedien  |b c  |2 rdamedia 
338 |a ƒa Online-Ressource  |b cr  |2 rdacarrier 
500 |a Date Revised 30.09.2020 
500 |a published: Print-Electronic 
500 |a Citation Status PubMed-not-MEDLINE 
520 |a We present a coupled Eulerian-Lagrangian method to simulate cloud cavitation in a compressible liquid. The method is designed to capture the strong, volumetric oscillations of each bubble and the bubble-scattered acoustics. The dynamics of the bubbly mixture is formulated using volume-averaged equations of motion. The continuous phase is discretized on an Eulerian grid and integrated using a high-order, finite-volume weighted essentially non-oscillatory (WENO) scheme, while the gas phase is modeled as spherical, Lagrangian point-bubbles at the sub-grid scale, each of whose radial evolution is tracked by solving the Keller-Miksis equation. The volume of bubbles is mapped onto the Eulerian grid as the void fraction by using a regularization (smearing) kernel. In the most general case, where the bubble distribution is arbitrary, three-dimensional Cartesian grids are used for spatial discretization. In order to reduce the computational cost for problems possessing translational or rotational homogeneities, we spatially average the governing equations along the direction of symmetry and discretize the continuous phase on two-dimensional or axi-symmetric grids, respectively. We specify a regularization kernel that maps the three-dimensional distribution of bubbles onto the field of an averaged two-dimensional or axi-symmetric void fraction. A closure is developed to model the pressure fluctuations at the sub-grid scale as synthetic noise. For the examples considered here, modeling the sub-grid pressure fluctuations as white noise agrees a priori with computed distributions from three-dimensional simulations, and suffices, a posteriori, to accurately reproduce the statistics of the bubble dynamics. The numerical method and its verification are described by considering test cases of the dynamics of a single bubble and cloud cavitaiton induced by ultrasound fields 
650 4 |a Journal Article 
650 4 |a Bubble dynamics 
650 4 |a Cavitation 
650 4 |a Compressible multiphase flows 
650 4 |a Eulerian-Lagrangian method 
650 4 |a Multiscale modeling 
650 4 |a Reduced-order modeling 
700 1 |a Colonius, Tim  |e verfasserin  |4 aut 
773 0 8 |i Enthalten in  |t Journal of computational physics  |d 1986  |g 371(2018) vom: 15. Okt., Seite 994-1017  |w (DE-627)NLM098188844  |x 0021-9991  |7 nnns 
773 1 8 |g volume:371  |g year:2018  |g day:15  |g month:10  |g pages:994-1017 
856 4 0 |u http://dx.doi.org/10.1016/j.jcp.2018.05.029  |3 Volltext 
912 |a GBV_USEFLAG_A 
912 |a SYSFLAG_A 
912 |a GBV_NLM 
912 |a GBV_ILN_350 
951 |a AR 
952 |d 371  |j 2018  |b 15  |c 10  |h 994-1017