1617 - 1629 |
Implications of a flame surface density approach to large eddy simulation of premixed turbulent combustion Hawkes ER, Cant RS |
1630 - 1639 |
Particle transport in a counter-flow Carrier GF, Fendell FE, Fink SF, Folley CN |
1640 - 1654 |
Contribution of curvature to flame-stretch effects on premixed flames Choi CW, Puri IK |
1655 - 1661 |
Mass spectrometric study of combustion of GAP- and ADN-based propellants Kuibida LV, Korobeinichev OP, Shmakov AG, Volkov EN, Paletsky AA |
1662 - 1668 |
The mass transfer coefficient for the combustion of pulverized carbon particles Fortsch D, Schnell U, Hein KRG, Essenhigh RH |
1669 - 1679 |
Soot pyrometry using modulated absorption/emission Jenkins TP, Hanson RK |
1680 - 1698 |
A comprehensive analysis of laser-induced ignition of RDX monopropellant Liau YC, Kim ES, Yang V |
1699 - 1713 |
Effects of reformer gas addition on the laminar flame speeds and flammability limits of n-butane and iso-butane flames Sung CJ, Huang Y, Eng JA |
1714 - 1724 |
Vaporization of arsenic, selenium and antimony during coal combustion Zeng TF, Sarofim AF, Senior CL |
1725 - 1735 |
Combined cavity ringdown absorption and laser-induced fluorescence imaging measurements of CN(B-X) and CH(B-X) in low-pressure CH4-O-2-N-2 and CH4-NO-O-2-N-2 flames Luque J, Jeffries JB, Smith GP, Crosley DR |
1736 - 1745 |
Photodissociation of glycidyl azide polymer with a Nd : YAG laser at 1.064 mu m Kumar A, Lee YP, Chen DM |
1746 - 1746 |
Coupling thermal deactivation with oxidation for predicting the combustion of a solid fuel (vol 125, pg 1341, 2001) Zolin A, Jensen A, Dam-Johansen K |