| 1 |
Optimal Distributed Control of Two-Dimensional Nonlocal Cahn-Hilliard-Navier-Stokes Systems with Degenerate Mobility and Singular Potential
Frigeri S, Grasselli M, Sprekels J
Applied Mathematics and Optimization, 81(3), 899, 2020 |
| 2 |
A new insight into pore body filling mechanism during waterflooding in a glass micro-model
Dehshibi RR, Sadatshojaie A, Mohebbi A, Riazi M
Chemical Engineering Research & Design, 151, 100, 2019 |
| 3 |
Numerical prediction of the Flame Describing Function and thermoacoustic limit cycle for a pressurised gas turbine combustor
Xia Y, Laera D, Jones WP, Morgans AS
Combustion Science and Technology, 191(5-6), 979, 2019 |
| 4 |
Capillary viscous flow and melting dynamics: Coupled simulations for additive manufacturing applications
Blank M, Nair P, Poschel T
International Journal of Heat and Mass Transfer, 131, 1232, 2019 |
| 5 |
A decoupling penalty finite element method for the stationary incompressible MagnetoHydroDynamics equation
Deng JE, Si ZY
International Journal of Heat and Mass Transfer, 128, 601, 2019 |
| 6 |
An efficient segregated algorithm for two-dimensional incompressible fluid flow and heat transfer problems with unstructured grids
Li J, Zhang Q, Zhai ZQ
International Journal of Heat and Mass Transfer, 133, 1052, 2019 |
| 7 |
Assessing compressibility effects on the performance of large horizontal-axis wind turbines
Yan C, Archer CL
Applied Energy, 212, 33, 2018 |
| 8 |
FROM HIGH-FIDELITY NUMERICAL SIMULATIONS OF A LIQUID-FILM ATOMIZATION TO A REGIME CLASSIFICATION
Bilger C, Cant RS
Atomization and Sprays, 28(1), 65, 2018 |
| 9 |
Predictive model for the scale-out of small channel two-phase flow contactors
Ortega EG, Tsaoulidis D, Angeli P
Chemical Engineering Journal, 351, 589, 2018 |
| 10 |
Dynamic capillary phenomena using Incompressible SPH
Nair P, Poschel T
Chemical Engineering Science, 176, 192, 2018 |
