Title: COMPUTER FIRE MODELING
1COMPUTER FIRE MODELING
- Principals, Applications, and Validation
2Overview
4
- Principals of modeling
- Zone Models
- Assumptions
- Governing Equations
- Zone Model Example (CFAST)
- CFD Models
- Assumptions
- Governing Equations
- CFD Model Example (FDS)
- Need for verification and validation
3Principals of Modeling2
8
- Probabilistic
- Based on statistics and risk assessments
- Network Model (Decision Tree)
- Statistical Modeling (Risk Assessment)
- Simulation Models
- Deterministic
- Utilize known inputs to compute a specific
result (Computer Fire Model) - Same output achieved with same input
4Deterministic Models for Life Safety2
2
- Detector/Sprinkler Activations
- DETACT
- People Movement in Evacuations
- Course
- Node/Arc
- EVACNET
- ERM
- EXITT
- Fine
- Grid
- SIMULEX
- EXODUS
5Deterministic Models for Life Safety Continued2
3
- Building Thermal Element Response
- SAFIR
- VULCAN
- Hydraulic Calculations
- SprinkCAD
- HASS
- (Hydraulic Analyzer of Sprinkler Systems)
- Transport of Smoke and Heat in Enclosures
- CFAST
- (Consolidated Fire And Smoke Transport Model)
- NIST FDS (Fire Dynamics Simulator)
6Enclosure Fire Models
2
- Zone Model
- CFAST (Consolidated Fire And Smoke Transport
Model) - CFD (Computational Fluid Dynamics)
- NIST FDS (Fire Dynamics Simulator)
7Enclosure Fire Models Continued
6
- Scientific Tool
- All dimensions are metric
- Output is only as good as input
- Dont try this at home!
- Unlike most computer programs theuser must be
informed in the underlying operation of the
program - Utilized in the research industry and educational
realm - Still requires the scientific process
8Zone Model
4
- Single Enclosure
- Known fire size
- Will not generate smoke/heat transport times.
-
9Zone Model Continued
1
- Conservation equations are applied to each zone.
10Zone Model Continued
5
- Assumptions
- Each zone contains only ideal gas with a constant
molecular weight and specific heat. Cp and Cv. - Mass transport/exchange occurring at free
boundariesis due to difference in pressure or
shear mixing effects. - Combustion is modeled as a source of mass and
energy. - Fire plume is assumed to be instantly at the
ceiling, and time to transport mass horizontally
and vertically is ignored.
11Zone Model Continued
6
- Assumptions
- Room contents are ignored with regards to their
mass or heat sink capacity. - Horizontal cross section is constant with respect
to area. - Pressure is considered uniform, the stack effect
is neglected. - Mass flow into the plume is turbulent and
linearly proportionate to velocity. - Fluid frictional effects are ignored at the
boundaries.
12Conservation Equations
3
13Conservation Equations
1
14Conservation Equations
14
15Vent Flow
1
16Zone Model Example
4
- CFAST(Consolidated Fire And Smoke Transport
Model) - Two Zone Model
- Most Current Version 6.0
- Utilizes a Windows Based Input Screen
- Developed and maintained by the Building Fire and
Research Lab at the National Institute of
Standards and Technology
17Zone Model Example
3
- CFAST cont.
- (Consolidated Fire And Smoke Transport Model)
- Solves the conservation equations discusses for
each zone - Outputs values both visually and numerically
18Zone Model Example Continued
3
- Enclosure
- Room 15m x 15m x 3m
- Vents
- Double Door 1.5m x 1.4m
- Fire
- T2 Fire Growth reaching 1 MW _at_ 300s
19Zone Model Example Continued
20Zone Model Example Continued
21Zone Model Example Continued
22Zone Model Example Continued
23Zone Model Example Continued
- Output Excel (Flow) cont.
24Zone Model ExampleContinued
25Zone Model Example Continued
- Output Excel (Species) cont.
26CFD Model5
3
- Area of interest divided into grids
- Each grid is its own control volume as in Zone
Model - Capable of more advanced analysis
- Combustion
- Phase Change
- Multi Phase Flow
- Chemical Reactions
27CFD Model Continued
3
- NIST FDS
- (Fire Dynamics Simulator)
- Computational fluid dynamics model for
fire-driven fluid flow.4 - Solves a modified version of the Navier-Stokes
equations appropriate for low-speed,
thermally-driven flow with an emphasis on smoke
and heat transport from fires.4
28CFD Model Continued
5
- Governing Equations
- Conservation of Mass
- Conservation of Momentum
- Transport of Sensible Enthalpy
- Equation of State for a Perfect Gas
29CFD Model Continued
5
- Conservation of Mass (Zone)
Conservation of Mass (CFD)
u Velocity Vector (u,v,w)
30CFD Model Continued
4
- Conservation of Species (Zone)
Mixture Fraction Combustion Model (CFD)
- A Single-Step, Instantaneous Reaction
31CFD Model Continued
3
- Mixture Fraction - combination of the mass
fractions of the fuel and the carbon-carrying
combustion products -
Function of space and time
32CFD Model Continued
4
- Stoichiometric mixture fraction
- Assume combustion occurs instantaneously
- Fuel and oxygen cannot coexist
33CFD Model Continued
4
- A Single-Step Reaction with location extinction
- Single-step adaptation eliminates assumption that
oxygen and fuel cannot co-exist
- No Burn O2 and Fuel mix but do not combust.
- Burn O2 and Fuel react but not necessarily
completely
34CFD Model Continued
5
- In order to utilize this model mixture
fraction must be broken into two terms
35CFD Model Continued
2
- Instead of having transport equations for Z we
now have two separate transport equations for Z1
and Z2.
- Fuel and oxygen can co-exist however only react
if the conditions permit.
36CFD Model Continued
5
- Reaction is the conversion of fuel to products or
the conversion from Z1 to Z2.
- The HRR (Heat Release Rate) is determined through
the equation
37CFD Model Continued
5
- Can also be further complicated where fuel stream
may by diluted with an inert gas. (Ex. Nitrogen)
- Restate Z1 to Z2 keeping in mind the soot yield
and CO yield remain fixed
38CFD Model Continued
4
- Being that the a species mass fraction is a
linear combination of that species mixture
fraction variables the following are true.
39CFD Model Continued
5
40CFD Model Continued
8
- Where the stoichiometric coefficients are defined
as
41CFD Model Continued
3
- Import assumptions
- Z1 and Z2 do not imply a the rate of combustion
- Combustion is only assumed to occur in a single
step
42CFD Model Example
4
- Enclosure
- Room 15m x 15m x 3m
- Grid
- 0.5m x 0.5m x 0.5 m
- Vents
- Double Door 1.5m x 1.4m
- Fire
- T2 Fire Growth reaching 1 MW _at_ 300s
43CFD Model Example Continued
HEAD CHID'Presentation', TITLE'Sample Room for
Engineering Expo Presentation' / A 15m x 15m x 3
meter room with a vent 7 meter MESH
IJK32,30,30 XB-1.0,15.0,0.0,15.0,0.0,3.0 /
TIME T_END600. / SURF ID 'FIRE' HRRPUA
1054. COLOR 'RED' TAU_Q 300 /T2 fire
growth reaching 1054 at 300 seconds. SURF ID
'WALL' COLOR 'GRAY' / HOLE XB-0.5, 0.5,
6.0, 7.5, 0.0, 1.4 / VENT MB'XMIN',
SURF_ID'OPEN' / VENT XB7.0,8.0,7.0,8.0,0.0,0.0
, SURF_ID'FIRE' / OBST XB0.0, 0.0, 0.0, 15.0,
0.0, 3.0, SURF_ID'WALL' / TAIL /
44CFD Model Example Continued
45CFD Model Example Continued
46CRD Model Example Continued
10
- Output More User Input required for desired
output - Surface Temperatures
- Vent Flows
- Thermocouples
- Heat Flux Gages
- Temperature Gages
- Sprinklers
- Smoke Detectors
- Species Concentration
- And Many Others
47Verification/Validation
5
- What is validation? 6
- Answering the following questions
- Does it accurately represent physical and
chemical phenomena of interest? - Was the Model appropriate for use in with the
given scenario?
Check the physics!!
48Verification/Validation
6
- What is Verification?6
- Answering the following questions
- What is the mathematical uncertainty associated
with the model - What is the mathematical uncertainty associated
with the experiments? - Is the difference between known experimental
values and the models results explained by
mathematical uncertainty?
Check the math!!
49Verification/Validation
5
- Validation of Model7
- Validation is the responsibility of the user not
the creator of the model. - Can be done through the following
- Comparing the results to known experimental
results - Conducting scaled or full scale experiments to
evaluate the results
50Verification/Validation
7
- Verification of Model6
- Verification is the responsibility of the user
not the creator of the model. - Can be done through the following
- Checking the models calculations
- By hand or through the use of other models
- Comparing calculations to exact solutions
- Considering the sensitivity of parameters
51References
- DiNenno, Philip J. et.al., eds. SFPE Handbook of
Fire Protection Engineering, Third Edition.
Quincy National Fire Protection Association,
2006. - Karlsson, BjÖrn and James G. Quintiere. Enclosure
Fire Dynamics. Boca Raton CRC Press LLC, 1999. - Quintiere, James G. Fundamentals of Fire
Phenomena. West Sussex Wiley, 2006. - United States. National Institute of Standards
and Technology. Fire Dynamics Simulator (Version
5) Users Guide. Washington GPO, 2007. - United States. National Institute of Standards
and Technology. Fire Dynamics Simulator (Version
5) Technical Reference Guide Volume 1
Mathematical Model. Washington GPO, 2007. - United States. National Institute of Standards
and Technology. Fire Dynamics Simulator (Version
5) Technical Reference Guide Volume 2
Verification. Washington GPO, 2007. - United States. National Institute of Standards
and Technology. Fire Dynamics Simulator (Version
5) Technical Reference Guide Volume 2
Validation. Washington GPO, 2007.
521
QUESTIONS ?
- Robin Zevotek
- Fire Protection Engineer
- CS Companies
- rzevotek_at_cscos.com