3.2. Math Models
Fire simulation requires the solution of variable property, high Grashof number, turbulent, low Mach number flow including the effects of species and soot transport, radiation, and buoyancy.
Conservation laws include mass of the mixture, momentum, mass of the individual species, and energy. Length scales vary from molecular to convection dominated. For purposes of discussion, length scales are also categorized by the method of resolution.
The transport equations used to describe fire physics are based on two sets of approximations to the fundamental equations of fluid dynamics. Fast acoustic time scales are removed from the equations using low Mach number asymptotics, described in Low Mach Number Equations.
Turbulent transport at high Grashof numbers is modeled using a Reynolds averaging approach, described in RANS Temporal Filtering.
In what follows, we note that unless specifically stated otherwise all units in the equations and submodel expressions are cgs. For a more extensive treatment of units and unit conversions in Fuego, please see the “Units and Unit Conversions” section in the User’s Manual. The numerical methods we use to solve the transport equations are of the finite volume class. Therefore, we generally write the transport equations in the integral form.
- 3.2.1. Low Mach Number Equations
- 3.2.2. Laminar Flow Equations
- 3.2.3. Radiation Transport Equation
- 3.2.4. Turbulence Modeling Overview
- 3.2.5. Turbulent Flow Equations, Favre-Averaged
- 3.2.6. Turbulence Closure Models
- 3.2.6.1. Standard
RANS Model
- 3.2.6.2. Low Reynolds Number
RANS Model
- 3.2.6.3. RNG
RANS Model
- 3.2.6.4.
RANS Model
- 3.2.6.5.
RANS Model
- 3.2.6.6. Shear Stress Transport (SST)
- 3.2.6.7. Standard Smagorinsky LES Model
- 3.2.6.8. Dynamic Smagorinsky LES Model
- 3.2.6.9. Subgrid-Scale Kinetic Energy One-Equation LES Model
- 3.2.6.10. Dynamic Subgrid-Scale Kinetic Energy One-Equation LES Model
- 3.2.6.11. Buoyancy Models for the Production Rate
- 3.2.6.12. Turbulence closure model constants
- 3.2.6.1. Standard
- 3.2.7. Wall Boundary Conditions for Turbulence Models
- 3.2.7.1. Resolution of Boundary Layer; Momentum
- 3.2.7.2. Resolution of Boundary Layer; Turbulence Quantities
- 3.2.7.3. Resolution of Boundary Layer; Enthalpy
- 3.2.7.4. Wall Functions for Turbulent Flow Boundary Conditions
- 3.2.7.5. Wall Functions; Momentum
- 3.2.7.6. Wall Functions; Turbulent Kinetic Energy
- 3.2.7.7.
Wall Functions; Turbulent Kinetic Energy
- 3.2.7.8. Wall Functions; Turbulence Dissipation Transport
- 3.2.7.9. Wall Functions; Turbulent Frequency Transport
- 3.2.7.10. Wall Functions; Enthalpy Transport
- 3.2.7.11. Wall Functions; Scalar Transport
- 3.2.8. Inlet Conditions for Turbulence Quantities
- 3.2.9. Mass Injection Boundary Condition
- 3.2.10. EDC Turbulent Combustion Model
- 3.2.10.1. Model Characteristics
- 3.2.10.2. Physical Interpretation
- 3.2.10.3. Thermochemistry
- 3.2.10.4. Chemical Mechanism
- 3.2.10.5. Species Consumption/Production Limits
- 3.2.10.6. Conservation Laws
- 3.2.10.7. Effect Of Turbulence On Combustion Rates
- 3.2.10.8. Average Control Volume Properties
- 3.2.10.9. Limits Testing
- 3.2.10.10. Cell Value Information Used By Model
- 3.2.10.11. Model Outputs
- 3.2.10.12. Combustion Products Transport Equation
- 3.2.10.13. Chemical Equilibrium Models
- 3.2.11. Laminar Flamelet Turbulent Combustion Model
- 3.2.12. Turbulent Reacting Mixing Models
- 3.2.13. Soot Generation Model for Multicomponent Combustion
- 3.2.14. Absorptivity Model
- 3.2.15. Fuel Boundary Condition Submodel
- 3.2.16. Fuel Spreading Submodel
- 3.2.17. One-Dimensional Composite Fire Boundary Condition
- 3.2.18. Non-Conformal DG Boundary Condition
- 3.2.19. Porous-Fluid Coupling Algorithm
- 3.2.20. Volume of Fluid Model