| Adaptive mesh finite-volume calculation of 2D lid-cavity corner vortices JPP Magalhães, DMS Albuquerque, JMC Pereira, JCF Pereira Journal of computational physics 243, 365-381, 2013 | 39 | 2013 |
| Continuity constrained least-squares interpolation for SFO suppression in immersed boundary methods DMC Martins, DMS Albuquerque, JCF Pereira Journal of Computational Physics 336, 608-626, 2017 | 26 | 2017 |
| Simulation and control of continuous glass melting by microwave heating in a single-mode cavity with energy efficiency optimization RMC Mimoso, DMS Albuquerque, JMC Pereira, JCF Pereira International Journal of Thermal Sciences 111, 175-187, 2017 | 25 | 2017 |
| Residual Least-Squares Error Estimate for Unstructured h-Adaptive Meshes DMS Albuquerque, JMC Pereira, JCF Pereira Numerical Heat Transfer, Part B: Fundamentals 67 (3), 187-210, 2015 | 19 | 2015 |
| Calculation of Spotting Particles Maximum Distance in Idealised Forest Fire Scenarios DMSA José C. F. Pereira, José M. C. Pereira, André L. A. Leite Journal of Combustion 513576, 17 pages, 2015 | 17* | 2015 |
| Numerical simulation and optimization of the ceramic pigments production process using microwave heating PAV Ramos, DMS Albuquerque, JCF Pereira Chemical Engineering and Processing-Process Intensification 169, 108567, 2021 | 12 | 2021 |
| A very high-order finite volume method based on weighted least squares for elliptic operators on polyhedral unstructured grids AGR Vasconcelos, DMS Albuquerque, JCF Pereira Computers & Fluids 181, 383-402, 2019 | 10 | 2019 |
| On the use of polyhedral unstructured grids with a moving immersed boundary method DMC Martins, DMS Albuquerque, JCF Pereira Computers & Fluids 174, 78-88, 2018 | 7 | 2018 |
| Numerical Computation of Incompressible Flows on Adaptive and Unstructured Grids DMS Albuquerque PhD Thesis, Instituto Superior Técnico, Universidade de Lisboa, Portugal, 2013 | 7 | 2013 |
| Calculation of a deformable membrane airfoil in hovering flight DMS Albuquerque, JMC Pereira, JCF Pereira Computer Modeling in Engineering and Sciences 72 (4), 337, 2011 | 5 | 2011 |
| A novel approach for temporal simulations with very high-order finite volume schemes on polyhedral unstructured grids PMP Costa, DMS Albuquerque Journal of Computational Physics 453, 110960, 2022 | 4 | 2022 |
| A novel eighth-order diffusive scheme for unstructured polyhedral grids using the weighted least-squares method DMS Albuquerque, AGR Vasconcelos, JCF Pereira Spectral and High Order Methods for Partial Differential Equations ICOSAHOM …, 2020 | 2 | 2020 |
| Modelling and energy efficiency analysis of the microwave continuous processing of limestone SN Gonçalves, DMS Albuquerque, JCF Pereira Journal of Cleaner Production, 142912, 2024 | 1 | 2024 |
| Numerical modeling of ceramics sintering and melting by microwave heating DMS Albuquerque, JMC Pereira, JCF Pereira 11th World Congress on Computational Mechanics, 5th European Conference on …, 2014 | 1 | 2014 |
| A NEW RESIDUAL LEAST SQUARES ERROR ESTIMATOR FOR FINITE VOLUME METHODS–APPLICATIONS TO LAMINAR FLOWS DMS Albuquerque, JMC Pereira, JCF Pereira Int. Conf. on Adaptive Modeling and Simulation, ADMOS, Lisbon, 2013 | 1 | 2013 |
| A Face-Based Eight-Order Scheme for Convection-Diffusion Problems with Polyhedral Unstructured Grids DMS Albuquerque, FJM Diogo Spectral and High Order Methods for Partial Differential Equations ICOSAHOM …, 2022 | | 2022 |
| Research Article Calculation of Spotting Particles Maximum Distance in Idealised Forest Fire Scenarios JCF Pereira, JMC Pereira, ALA Leite, DMS Albuquerque | | 2015 |
| Application of an automatic h-adaptive refinement algorithm in a second order immersed boundary code D Albuquerque, JCF Pereira CIMNE, 2015 | | 2015 |
| AN IMMERSED BOUNDARY METHOD WITH DIVERGENCE-FREE INTERPOLATION FOR UNSTRUCTURED POLYHEDRAL GRIDS DMS ALBUQUERQUE, DMC Martins, JCF Pereira | | |
| Comparison between the results obtained with structured and unstructured grids for the cases of a laminar and a turbulent axisymmetric jet flow ALA Leite, DMS Albuquerque, JCF Pereira MEFTE 2014 3 (4), 27, 0 | | |
