| 1111 - 1121 |
Thermodynamic optimization alternatives: Minimization of physical size subject to fixed power
Bejan A |
| 1123 - 1131 |
Artificial neural networks for thermopiezoelectric systems
Sunar M |
| 1133 - 1142 |
Entropy analysis of a flow past a heat-generated bluff body
Shuja SZ, Yilbas BS, Budair MO, Hussaini IS |
| 1143 - 1152 |
Experimental studies on mushroom and pollen drying
Midilli A, Olgun H, Ayhan T |
| 1153 - 1163 |
Exergy analysis of waste emissions
Rosen MA, Dincer I |
| 1165 - 1175 |
Effect of the equivalence ratio on the concentration of CH4/NO2/O-2 combustion products
Al-Farayedhi AA, Antar MA, Khan A |
| 1177 - 1185 |
Demonstration of coal gas run molten carbonate fuel cell concept
Mathur A, Bali S, Balakrishnan M, Perumal R, Batra VS |
| 1187 - 1198 |
The cost of uncertainty in capacity expansion problems
Wang JH, Sparrow FT |
| 1199 - 1200 |
Comments on ＇Effects of transverse magnetic field, Prandtl number and Reynolds number on non-Darcy mixed convective flow of an incompressible viscous fluid past a porous vertical flat plate in a saturated porous medium＇ by H. S. Takhar and O. A. Beg
Nield DA |
| 1201 - 1202 |
Comments on ＇Effects of transverse magnetic field, Prandtl number and Reynolds number on non-Darcy mixed convective flows of an incompressible viscous fluid past a porous vertical flat plate in a saturated porous medium＇ by H. S. Takhar and O. A. Beg - Reply
Takhar HS, Beg OA |
