577 - 585 |
Extended Oberbeck-Boussinesq approximation study of convective instabilities in a porous layer with horizontal flow and bottom heating Nield DA, Barletta A |
586 - 593 |
Three-dimensional multi-scale plate assembly for maximum heat transfer rate density Bello-Ochende T, Meyer JP, Dirker J |
594 - 604 |
On the influence of psychrometric ambient conditions on cooling tower drift deposition Lucas M, Martinez PJ, Ruiz J, Kaiser AS, Viedma A |
605 - 614 |
Towards maximal heat transfer rate densities for small-scale high effectiveness parallel-plate heat exchangers Rogiers F, Baelmans M |
615 - 625 |
Transient double-diffusive convection in an enclosure with large density variations Sun H, Lauriat G, Sun DL, Tao WQ |
626 - 634 |
Heat transfer enhancement in a slot channel via a transversely oscillating adiabatic circular cylinder Celik B, Raisee M, Beskok A |
635 - 644 |
Binary homogeneous nucleation and growth of water-sulfuric acid nanoparticles using a TEMOM model Yu MZ, Lin JZ |
645 - 655 |
A coupled volume-of-fluid and level set (VOSET) method for computing incompressible two-phase flows Sun DL, Tao WQ |
656 - 664 |
Simulation of transient Rayleigh-Benard-Marangoni convection induced by evaporation Touazi O, Chenier E, Doumenc F, Guerrier B |
665 - 673 |
Direct numerical simulation of a differentially heated cavity of aspect ratio 4 with Rayleigh numbers up to 10(11) - Part I: Numerical methods and time-averaged flow Trias FX, Gorobets A, Soria M, Oliva A |
674 - 683 |
Direct numerical simulation of a differentially heated cavity of aspect ratio 4 with Rayleigh numbers up to 10(11) - Part II: Heat transfer and flow dynamics Trias FX, Gorobets A, Soria M, Oliva A |
684 - 693 |
Chaotic mixing efficiency in different geometries of Hele-Shaw cells Beuf A, Gence JN, Carriere P, Raynal F |
694 - 702 |
Combined effects of the filling ratio and the vapour space thickness on the performance of a flat plate heat pipe Lips S, Lefevre F, Bonjour J |
703 - 714 |
Water vapor and carbon dioxide species measurements in narrow channels Basu S, Lambe DE, Kumar R |
715 - 725 |
An experimental and theoretical investigation of the thermal treatment of wood (Fagus sylvatica L.) in the range 200-260 degrees C Turner I, Rousset P, Remond R, Perre P |
726 - 731 |
Effects of porosity, pumping power, and L/D ratio on the thermal characteristics of an N2O catalytic igniter with packed bed geometry You WJ, Moon HJ, Jang SP, Kim JK, Koo J |
732 - 743 |
Optimal design of baffles locations with interdigitated flow channels of a centimeter-scale proton exchange membrane fuel cell Jang JY, Cheng CH, Huang YX |
744 - 752 |
Generalized thermo-elastodynamics for semiconductor material subject to ultrafast laser heating. Part II: Near-field response and damage evaluation Qi XL, Suh CS |
753 - 759 |
A technique for uncertainty analysis for inverse heat conduction problems Blackwell B, Beck JV |
760 - 771 |
Mixed convective cooling of a fin in a channel Yang MH, Yeh RH, Hwang JJ |
772 - 785 |
Time-dependent model of mixed electroosmotic/pressure-driven three immiscible fluids in a rectangular microchannel Haiwang L, Wong TN, Nguyen NT |
786 - 796 |
Prediction of turbulent channel flow with superhydrophobic walls consisting of micro-ribs and cavities oriented parallel to the flow direction Jeffs K, Maynes D, Webb BW |
797 - 810 |
Cooling of a permanent magnet electric motor with a centrifugal impeller Li HM |