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Optical neural engine for solving scientific partial differential equations. [PDF]
Tang Y +7 more
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Complex transition pathways in boiling and cavitation. [PDF]
Gallo M +3 more
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Evaluating the accuracy of one-dimensional glottal flow model in predicting voice production: comparison to experiments and three-dimensional flow simulations. [PDF]
Yoshinaga T, Zhang Z.
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Stability of Partially Congested Travelling Wave Solutions for the Dissipative Aw-Rascle System. [PDF]
Deléage É, Mehmood MA.
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An importance sampling vortex particle method for turbulence visualization simulation in maritime simulators. [PDF]
Zhu T, Ren H, Tao R, Wei D, Xie P.
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Quantitative analysis of ferrohydrodynamics of blood containing magnetic nanocarriers for advanced drug delivery design via hybrid machine learning. [PDF]
Alsaab HO, Althobaiti YS.
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Applied Mathematics Letters, 2023
The relaxed Navier-Stokes equations of the form \[ \begin{split} \partial_t\rho + \operatorname{div}(\rho u) & = 0,\\ \partial_t(\rho u) + \operatorname{div}(\rho u\otimes u) + \nabla p(\varrho) & = \operatorname{div}S_1 +\nabla S_2,\\ \tau_1(\partial_t S_1 + u\cdot \nabla S_1) + S_1 &= \mu\left(\nabla u + (\nabla u)^\top - \frac 23 \operatorname{div ...
Ju, Qiangchang, Wang, Zhao
openaire +1 more source
The relaxed Navier-Stokes equations of the form \[ \begin{split} \partial_t\rho + \operatorname{div}(\rho u) & = 0,\\ \partial_t(\rho u) + \operatorname{div}(\rho u\otimes u) + \nabla p(\varrho) & = \operatorname{div}S_1 +\nabla S_2,\\ \tau_1(\partial_t S_1 + u\cdot \nabla S_1) + S_1 &= \mu\left(\nabla u + (\nabla u)^\top - \frac 23 \operatorname{div ...
Ju, Qiangchang, Wang, Zhao
openaire +1 more source

