TY - JOUR
T1 - Coherent Particle Structures in High-Prandtl-Number Liquid Bridges
AU - Barmak, Ilya
AU - Romanò, Francesco
AU - Kannan, Parvathy Kunchi
AU - Kuhlmann, Hendrik C.
N1 - Publisher Copyright:
© 2021, The Author(s).
PY - 2021/2
Y1 - 2021/2
N2 - Clustering of small rigid spherical particles into particle accumulation structures (PAS) is studied numerically for a high-Prandtl-number (Pr = 68) thermocapillary liquid bridge. The one-way-coupling approach is used for calculation of the particle motion, modeling PAS as an attractor for a single particle. The attractor is created by dissipative forces acting on the particle near the boundary due to the finite size of the particle. These forces can dramatically deflect the particle trajectory from a fluid pathline and transfer it to certain tubular flow structures, called Kolmogorov–Arnold–Moser (KAM) tori, in which the particle is focused and from which it might not escape anymore. The transfer of particles can take place if a KAM torus, which is a property of the flow without particles, enters the narrow boundary layer on the flow boundaries in which the particle experiences extra forces. Since the PAS obtained in this system depends mainly on the finite particle size, it can be classified as a finite-size coherent structure (FSCS).
AB - Clustering of small rigid spherical particles into particle accumulation structures (PAS) is studied numerically for a high-Prandtl-number (Pr = 68) thermocapillary liquid bridge. The one-way-coupling approach is used for calculation of the particle motion, modeling PAS as an attractor for a single particle. The attractor is created by dissipative forces acting on the particle near the boundary due to the finite size of the particle. These forces can dramatically deflect the particle trajectory from a fluid pathline and transfer it to certain tubular flow structures, called Kolmogorov–Arnold–Moser (KAM) tori, in which the particle is focused and from which it might not escape anymore. The transfer of particles can take place if a KAM torus, which is a property of the flow without particles, enters the narrow boundary layer on the flow boundaries in which the particle experiences extra forces. Since the PAS obtained in this system depends mainly on the finite particle size, it can be classified as a finite-size coherent structure (FSCS).
KW - Finite-size coherent structure
KW - High Prandtl number
KW - Particle accumulation
KW - Thermocapillary liquid bridge
UR - http://www.scopus.com/inward/record.url?scp=85101040796&partnerID=8YFLogxK
U2 - 10.1007/s12217-020-09845-5
DO - 10.1007/s12217-020-09845-5
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AN - SCOPUS:85101040796
SN - 0938-0108
VL - 33
JO - Microgravity Science and Technology
JF - Microgravity Science and Technology
IS - 1
M1 - 19
ER -