2777 - 2779 |
Professor Peter Gray, MA, PhD, ScD, FRSC, FRS (1926-2012) In Memoriam Griffiths J, Hayhurst A |
2780 - 2788 |
Application of a novel charge preparation approach to testing the autoignition characteristics of JP-8 and camelina hydroprocessed renewable jet fuel in a rapid compression machine Allen C, Toulson E, Edwards T, Lee T |
2789 - 2798 |
Numerical investigation of soot formation mechanisms in partially-premixed ethylene-air co-flow flames Chernov V, Zhang QG, Thomson MJ, Dworkin SB |
2799 - 2805 |
Modeling of ammonia combustion at low pressure Duynslaegher C, Contino F, Vandooren J, Jeanmart H |
2806 - 2816 |
Effects of CO addition on the propagation characteristics of laminar CH4 triple flame Wu CY, Li YH, Chang TW |
2817 - 2828 |
Radiation effects on flame stabilization on flat flame burners Schoegl I |
2829 - 2840 |
Numerical simulation of transcritical strained laminar flames Giovangigli V, Matuszewski L |
2841 - 2843 |
Experimental and computational infrared imaging of bluff body stabilized laminar diffusion flames Rankin BA, Blunck DL, Katta VR, Stouffer SD, Gore JP |
2844 - 2855 |
Kernel density weighted principal component analysis of combustion processes Coussement A, Gicquel O, Parente A |
2856 - 2871 |
Numerical simulations and physical analysis of an overexpanded reactive gas flow in a planar nozzle Sainte-Rose B, Bertier N, Deck S, Dupoirieux F |
2872 - 2882 |
Characterization of flame-shedding behavior behind a bluff-body using proper orthogonal decomposition Kostka S, Lynch AC, Huelskamp BC, Kiel BV, Gord JR, Roy S |
2883 - 2895 |
Influence of heat release and turbulence on scalar dissipation rate in autoigniting n-heptane/air mixtures Mukhopadhyay S, Abraham J |
2896 - 2911 |
The structure of turbulent stratified and premixed methane/air flames I: Non-swirling flows Sweeney MS, Hochgreb S, Dunn MJ, Barlow RS |
2912 - 2929 |
The structure of turbulent stratified and premixed methane/air flames II: Swirling flows Sweeney MS, Hochgreb S, Dunn MJ, Barlow RS |
2930 - 2943 |
One-dimensional-turbulence simulation of flame extinction and reignition in planar ethylene jet flames Lignell DO, Rappleye DS |
2944 - 2953 |
The critical tube diameter and critical energy for direct initiation of detonation in C2H2/N2O/Ar mixtures Zhang B, Ng HD, Lee JHS |
2954 - 2966 |
Visualization study of ignition modes behind bifurcated-reflected shock waves Yamashita H, Kasahara J, Sugiyama Y, Matsuo A |
2967 - 2973 |
Effect of an axial electric field on detonation waves Kamenskihs V, Lee JHS |
2974 - 2984 |
Prediction of the mass loss rate of polymer materials: Impact of residue formation Kempel F, Schartel B, Linteris GT, Stoliarov SI, Lyon RE, Walters RN, Hofmann A |
2985 - 2998 |
Measurement of in-cylinder soot particles and their distribution in an optical HSDI diesel engine using time resolved laser induced incandescence (TR-LII) Menkiel B, Donkerbroek A, Uitz R, Cracknell R, Ganippa L |
2999 - 3002 |
Prediction of the critical condition for flame acceleration over wood surface with different sample orientations Zhang Y, Ji J, Wang QS, Huang XJ, Wang QH, Sun JH |