879 - 884 |
Pressure drop in two phase slug/bubble flows in mini scale capillaries Walsh E, Muzychka Y, Walsh P, Egan V, Punch J |
885 - 895 |
Numerical and experimental study on effect of wall geometry on wall impingement process of hollow-cone fuel spray under various ambient conditions Shim YS, Choi GM, Kim DJ |
896 - 903 |
Measurement of liquid film thickness in micro square channel Han Y, Shikazono N |
904 - 913 |
The critical role of channel cross-sectional area in microchannel flow boiling heat transfer Harirchian T, Garimella SV |
914 - 923 |
Comparison of the RANS and PDF methods for air-particle flows Kartushinsky AI, Michaelides EE, Zaichik LI |
924 - 932 |
An experimental investigation of roll waves in high pressure two-phase inclined pipe flows Johnson GW, Bertelsen AF, Nossen J |
933 - 945 |
Stochastic modeling of the multiple rebound effects for particle-rough wall collisions Konan NA, Kannengieser O, Simonin O |
946 - 951 |
Enhancement of the critical heat flux in saturated pool boiling using honeycomb porous media Mori S, Okuyama K |
952 - 962 |
Application of the scale entropy diffusion model to describe a liquid atomization process Dumouchel C, Grout S |
963 - 969 |
Interaction between two spheres placed in tandem arrangement in steady and pulsating flow Prahl L, Jadoon A, Revstedt J |
970 - 976 |
Bubble characteristics in a bubbling fluidized bed with a rotating distributor Sobrino C, Acosta-Iborra A, Santana D, de Vega M |