301 - 314 |
Detailed modeling of an isolated, ethanol droplet combustion under microgravity conditions Kazakov A, Conley J, Dryer FL |
315 - 326 |
The kinetics of vaporization of a heavy metal from a fluidized waste by an inverse method Abanades S, Flamant G, Gauthier D |
327 - 337 |
A computational study of oscillatory extinction of spherical diffusion flames Christiansen EW, Tse SD, Law CK |
339 - 353 |
Experimental study of fuel decomposition and hydrocarbon growth processes for practical fuel components: heptanes McEnally CS, Ciuparu DM, Pfefferle LD |
355 - 368 |
Effects of heat release in laminar diffusion flames lifted on round jets Boulanger J, Vervisch L, Reveillon J, Ghosal S |
369 - 379 |
Numerical study of the effects of material properties on flame stabilization in a porous burner Barra AJ, Diepvens G, Ellzey JL, Henneke MR |
381 - 387 |
Concentration profile of particles across a flame propagating through an iron particle cloud Sun JH, Dobashi R, Hirano T |
389 - 397 |
The transition from deflagration to detonation in thin channels Kagan L, Sivashinsky G |
399 - 409 |
A simple model for explosive combustion of premixed natural gas with air in a bubbling fluidized bed of inert sand Zukowski W |
411 - 420 |
Propagation speed of tribrachial (triple) flame of propane in laminar jets under normal and micro gravity conditions Lee J, Won SH, Jin SH, Chung SH, Fujita O, Ito K |
421 - 424 |
On the relative importance of different routes forming NO in hydrogen flames Konnov AA |
425 - 431 |
Effect of radiation on nitric oxide concentration under sooting oxy-fuel conditions Naik SV, Laurendeau NM, Cooke JA, Smooke MD |