493 - 504 |
Conductive mass transport from a semi-infinite lattice of particles Pozrikidis C |
505 - 520 |
An experimental study of heat transfer from a cylinder in low-amplitude zero-mean oscillatory flows Gopinath A, Harder DR |
521 - 538 |
Effects of phonon pore scattering and pore randomness on effective conductivity of porous silicon Chung JD, Kaviany M |
539 - 553 |
Effective thermal conductivity of frost during the crystal growth period Sahin AZ |
555 - 575 |
The effect of nozzle aspect ratio on stagnation region heat transfer characteristics of elliptic impinging jet Lee J, Lee SJ |
577 - 587 |
Lattice Boltzmann scheme for cooling of packed cut flowers van der Sman RGM, Ernst MH, Berkenbosch AC |
589 - 610 |
Linear stability of mixed convection flows in horizontal rectangular channels of finite transversal extension heated from below Nicolas X, Luijkx JM, Platten JK |
611 - 621 |
Free convection near a stagnation point in a porous medium resulting from an oscillatory wall temperature Merkin JH, Pop I |
623 - 628 |
Conduction through a grooved surface and Sierpinsky fractals Kacimov AR, Obnosov YV |
629 - 637 |
Trapping of impurity molecules in condensation from mixtures of gases Levdansky VV, Smolik J, Moravec P |
639 - 642 |
Surface temperature of a flat plate of finite thickness under conjugate laminar forced convection heat transfer condition Chida K |
643 - 652 |
Experimental results of the time to the onset of ice formation at metal surface and a correlation based on a sub-layer reactor model Chen XD, Chen P, Free KW |