2022
DOI: 10.1016/j.camwa.2022.01.001
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A projection scheme for phase change problems with convection

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Cited by 11 publications
(5 citation statements)
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“…To solve the stokes problem (6), we formulate the coupled projection scheme based on a rotational pressure correction with a BDF2 time integration method as those studied in Reference 22. Thus, we solve the Stokes problem (6) for updating the velocity field and pressure at every step using the coupled projection scheme in order to complete the implementation of semi‐Lagrangian finite element approach for solving incompressible Navier–Stoke equations (1).…”
Section: Methodsmentioning
confidence: 99%
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“…To solve the stokes problem (6), we formulate the coupled projection scheme based on a rotational pressure correction with a BDF2 time integration method as those studied in Reference 22. Thus, we solve the Stokes problem (6) for updating the velocity field and pressure at every step using the coupled projection scheme in order to complete the implementation of semi‐Lagrangian finite element approach for solving incompressible Navier–Stoke equations (1).…”
Section: Methodsmentioning
confidence: 99%
“…Comparing to the standard projection methods, the presence of previous gradient step in the velocity prediction problem improves the order of the scheme. Moreover, the rotational pressure correction projection enhanced the method to avoids artificial boundary conditions on the pressure and improves its rate of convergence 22 . Hence, assuming that truebold-italicU^n$$ {\hat{\boldsymbol{U}}}^n $$, truebold-italicU^nprefix−1$$ {\hat{\boldsymbol{U}}}^{n-1} $$, trueC^n$$ {\hat{C}}^n $$, trueC^nprefix−1$$ {\hat{C}}^{n-1} $$ and pn$$ {p}^n $$ are known, the Stokes equations (6) are solved using the following steps: Solve for Cn+1boldVh$$ {C}^{n+1}\in {\mathbf{V}}_h $$ 32normalΔtCn+1prefix−·()DCn+1=prefix−42normalΔttrueC^n+12normalΔttrueC^nprefix−1+Sn.$$ \frac{3}{2\Delta t}{C}^{n+1}-\nabla \cdotp \left(D\nabla {C}^{n+1}\right)=-\frac{4}{2\Delta t}{\hat{C}}^n+\frac{1}{2\Delta t}{\hat{C}}^{n-1}+{S}^n.…”
Section: Methodsmentioning
confidence: 99%
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“…A common approach is to use a single domain method [1,2] for the momentum equation. Projection schemes [3] or Newton based algorithms [1,4] have been shown to give accurate results. Enthalpy models have been proven to be suitable for phase change, even with different thermophysical properties between the two phases, especially when combined with adaptive mesh refinement [5,6].…”
Section: Introductionmentioning
confidence: 99%