2021
DOI: 10.1016/j.icheatmasstransfer.2020.105002
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Numerical simulation of HIFU with dual transducers: The implementation of dual-phase lag bioheat and non-linear Westervelt equations

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Cited by 18 publications
(6 citation statements)
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“…The simulation is performed in two consecutive phases of acoustic pressure and flow field determination. To capture the local fluctuations of the pressure field, the grid sizing for the acoustic simulation should be lowered to about λ /10 (where λ is the wavelength) [43] . A nearly uniform triangular grid is implemented in the entire domain except for PML layers where mapped triangular cell layers are utilized.…”
Section: Methodsmentioning
confidence: 99%
“…The simulation is performed in two consecutive phases of acoustic pressure and flow field determination. To capture the local fluctuations of the pressure field, the grid sizing for the acoustic simulation should be lowered to about λ /10 (where λ is the wavelength) [43] . A nearly uniform triangular grid is implemented in the entire domain except for PML layers where mapped triangular cell layers are utilized.…”
Section: Methodsmentioning
confidence: 99%
“…Implementation of the transformation, Eq. (14) can be rewritten as: The oscillations frequency is denoted by [34] .…”
Section: Methodsmentioning
confidence: 99%
“…Finally, since the computational domain was finite, the perfectly matched layer boundary condition was adopted at the bottom of the petri dish (end surface) to control the acoustic reflections from the end of the domain using artificial absorption (39).…”
Section: Methodsmentioning
confidence: 99%