TY - JOUR
T1 - Sub-Hinze scale bubble production in turbulent bubble break-up
AU - Rivière, Aliénor
AU - Mostert, Wouter
AU - Perrard, Stéphane
AU - Deike, Luc
N1 - Funding Information:
This work was supported by the NSF CAREER award 1844932 to L.D., and the American Chemical Society Petroleum Research Fund Grant 59697-DNI9 to L.D., A.R. was supported by an International Fund grant from Princeton University to L.D., S.P. and A.R. were supported by the Labex ENS-ICFP. Computations were performed on the Princeton supercomputer Tiger2, as well as on Stampede, through XSEDE allocations to L.D. and W.M., XSEDE is an NSF funded program 1548562. We would like to acknowledge high-performance computing support from Cheyenne (doi:10.5065/D6RX99HX) provided by NCAR's Computational and Information Systems Laboratory, sponsored by the National Science Foundation.
Funding Information:
This work was supported by the NSF CAREER award 1844932 to L.D., and the American Chemical Society Petroleum Research Fund Grant 59697-DNI9 to L.D., A.R. was supported by an International Fund grant from Princeton University to L.D., S.P. and A.R. were supported by the Labex ENS-ICFP. Computations were performed on the Princeton supercomputer Tiger2, as well as on Stampede, through XSEDE allocations to L.D. and W.M., XSEDE is an NSF funded program 1548562. We would like to acknowledge high-performance computing support from Cheyenne (doi:10.5065/D6RX99HX) provided by NCAR's Computational and Information Systems Laboratory, sponsored by the National Science Foundation.
Publisher Copyright:
© The Author(s), 2021. Published by Cambridge University Press.
PY - 2021
Y1 - 2021
N2 - We study bubble break-up in homogeneous and isotropic turbulence by direct numerical simulations of the two-phase incompressible Navier-Stokes equations. We create the turbulence by forcing in physical space and introduce the bubble once a statistically stationary state is reached. We perform a large ensemble of simulations to investigate the effect of the Weber number (the ratio of turbulent and surface tension forces) on bubble break-up dynamics and statistics, including the child bubble size distribution, and discuss the numerical requirements to obtain results independent of grid size. We characterize the critical Weber number below which no break-up occurs and the associated Hinze scale. At Weber number close to stable conditions (initial bubble sizes), we observe binary and tertiary break-ups, leading to bubbles mostly between and, a signature of a production process local in scale. For large Weber numbers (3d_h$]]>), we observe the creation of a wide range of bubble radii, with numerous child bubbles between and, an order of magnitude smaller than the parent bubble. The separation of scales between the parent and child bubble is a signature of a production process non-local in scale. The formation mechanism of these sub-Hinze scale bubbles relates to rapid large deformation and successive break-ups: the first break-up in a sequence leaves highly deformed bubbles which will break again, without recovering a spherical shape and creating an array of much smaller bubbles. We discuss the application of this scenario to the production of sub-Hinze bubbles under breaking waves.
AB - We study bubble break-up in homogeneous and isotropic turbulence by direct numerical simulations of the two-phase incompressible Navier-Stokes equations. We create the turbulence by forcing in physical space and introduce the bubble once a statistically stationary state is reached. We perform a large ensemble of simulations to investigate the effect of the Weber number (the ratio of turbulent and surface tension forces) on bubble break-up dynamics and statistics, including the child bubble size distribution, and discuss the numerical requirements to obtain results independent of grid size. We characterize the critical Weber number below which no break-up occurs and the associated Hinze scale. At Weber number close to stable conditions (initial bubble sizes), we observe binary and tertiary break-ups, leading to bubbles mostly between and, a signature of a production process local in scale. For large Weber numbers (3d_h$]]>), we observe the creation of a wide range of bubble radii, with numerous child bubbles between and, an order of magnitude smaller than the parent bubble. The separation of scales between the parent and child bubble is a signature of a production process non-local in scale. The formation mechanism of these sub-Hinze scale bubbles relates to rapid large deformation and successive break-ups: the first break-up in a sequence leaves highly deformed bubbles which will break again, without recovering a spherical shape and creating an array of much smaller bubbles. We discuss the application of this scenario to the production of sub-Hinze bubbles under breaking waves.
KW - bubble dynamics
KW - multiphase flow
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U2 - 10.1017/jfm.2021.243
DO - 10.1017/jfm.2021.243
M3 - Article
AN - SCOPUS:85104069869
SN - 0022-1120
VL - 917
JO - Journal of Fluid Mechanics
JF - Journal of Fluid Mechanics
M1 - A40
ER -