Effect of Wettability on Collapsing Cavitation Bubble near Solid Surface Studied by Multi-Relaxation-Time Lattice Boltzmann Model
Through the transformation matrix M [25], the fα and fαeq can be projected onto the moment space via m=Mf and meq=Mfeq . [...]the collision step of Equation (1) can be rewritten as: m∗=m−Λ(m−meq)+δt(I−Λ2)S where the I is the unite tensor, and the S is the forcing term in the moment space with (I−0.5...
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Published in | Applied sciences Vol. 8; no. 6; p. 940 |
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Main Authors | , , , , , |
Format | Journal Article |
Language | English |
Published |
Basel
MDPI AG
01.06.2018
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Subjects | |
Online Access | Get full text |
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Summary: | Through the transformation matrix M [25], the fα and fαeq can be projected onto the moment space via m=Mf and meq=Mfeq . [...]the collision step of Equation (1) can be rewritten as: m∗=m−Λ(m−meq)+δt(I−Λ2)S where the I is the unite tensor, and the S is the forcing term in the moment space with (I−0.5Λ)S=MF′ . Subsequently, the paper discusses the time of cavitation generation under different negative pressure conditions. [...]the paper studies these cases where the negative pressure is set as −6.02, −5.69, −5.36, −5.02, −4.69 and −4.36, respectively. [...]the effect of wettability on the density, pressure and velocity distribution of the collapsing bubble near the solid surface is discussed. The parameter G in Equation (7) was set as −1. [...]the total force F at the bottom boundary was the superposition of the intermolecular interaction force and fluid–solid interaction force. |
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ISSN: | 2076-3417 2076-3417 |
DOI: | 10.3390/app8060940 |