Theoretical and numerical combustion

By Thierry Poinsot, D. Veynante. 2001

3,290 citations recorded by the source corpus.

View Paper: https://www.semanticscholar.org/paper/f7216b952af5bb89b11039ea5a5ebc0edf2f45ca

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Citations in the corpus

Compressible large eddy simulation of turbulent combustion in complex geometry on unstructured meshes (2004, background): “Large-eddy simulation (LES) is becoming a standard tool to study the dynamics of turbulent flames [1,2].”
Actual impedance of nonreflecting Boundary conditions: Implications for computation of resonators (2004, unknown): “Their expression is obtained through characteristic analysis 2 , 27 : where the wave amplitudes L 1 ,... , L 5 are deﬁned by Equations (1–5) provide a simple method to choose the incoming wave amplitudes to be imposed at a boundary.”
Statistical modeling of thermal radiation transfer in buoyant turbulent diffusion flames (2004, background): “lation between the reaction rate and the temperature fluctuation [37]) is neglected, which may result in underestimated prediction of T ′2.”
LES of an ignition sequence in a gas turbine engine (2008, methodology): “The reaction rate ω̇k is modeled by an Arrhenius law [20] with coefficients fitted from a detailed chemistry [53] to the present one-step irreversible chemistry: JP10+14 O2 → 10 CO2 +8 H2O, using criteria based on laminar flame speed and thickness.”
Conditional Moment Closure for Large Eddy Simulations (2005, background): “Even though simple conditional averaging leads to non-smooth conditional scalar dissipation, the time averages are smooth and the model is able to capture the influence of the pilot flame on the profile (see Figure 2) [10] or a presumed”
Effects of radiation and compression on propagating spherical flames of methane/air mixtures near the lean flammability limit (2010, unknown): “[46].”
Flame Dynamics and Combustion Noise: Progress and Challenges (2009, methodology): “In TFLES, the flame is artificially thickened by a factor F to resolve its inner structure on the numerical mesh (in general, combustion is a subgrid scale phenomenon as flames are thinner than typical filter sizes (Poinsot and Veynante (2005))), keeping constant the laminar flame speed.”
Filtered Density Function for Subgrid Scale Modeling of Turbulent Combustion (2006, background): “It is believed widely that the optimal means of capturing the detailed, unsteady physics of turbulent combustion is via large eddy simulation (LES) [1-6].”
Large eddy simulation of spark ignition in a turbulent methane jet (2009, methodology): “The compressible LES equations solved by the code can be written [45]: ∂w ∂t + ∇ · F = Sc (2)”