Bulletin of the American Physical Society
77th Annual Meeting of the Division of Fluid Dynamics
Sunday–Tuesday, November 24–26, 2024; Salt Lake City, Utah
Session R22: Particle-Laden Flows: Theory and Modeling I
1:50 PM–3:47 PM,
Monday, November 25, 2024
Room: 250 F
Chair: Jesse Capecelatro, University of Michigan
Abstract: R22.00004 : Phase interaction force model for nonuniform particle laden flows*
2:29 PM–2:42 PM
Presenter:
Duan Zhong Zhang
(Los Alamos National Laboratory (LANL))
Authors:
Duan Zhong Zhang
(Los Alamos National Laboratory (LANL))
Min Wang
(Los Alamos National Laboratory)
S Balachandar
(University of Florida)
To address this issue, we note that the gradient operator ∇ on an average quantity is of order 1/L. Accurate to the first order of the length scale ratio between the inter-particle distance d and L, the corrections to phase interaction force density can be expressed as this operator acting on quantities proportional to the length scale d. The dimension of the quantities is the dimension of stress. It turns out there are two such stresses. They are the particle–fluid–particle stress and the diffusion stress. The phase interaction force density is then decomposed into three terms, a force density in a homogeneous flow, and two terms related to the stresses. These terms can be calculated and studied in statistically homogeneous flows.
*This work is sponsored by ASC program of U.S. DOE.
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