Daniel Madrzykowski and Robert L. Vettori
CD Version prepared by:
William D. Walton and Glenn P. Forney
April 2000
Fire Safety Engineering Division
Building and Fire Research Laboratory
National Institute of Standards and Technology
Abstract
Introduction
Fire Summary
NIST Fire Dynamics Simulator (FDS)
SMOKEVIEW
FDS Input
Model Results
Summary
References
Figures
This report describes the results of calculations using the NIST Fire Dynamics Simulator (FDS) that were performed to provide insight on the thermal conditions that occurred during the fire at 3146 Cherry Road NE, Washington D.C. on May 30, 1999. Input to the computer model was developed from 3 sources; the District of Columbia Fire and Emergency Medical Services Department Reconstruction Committee, photographs and measurements taken by NIST staff during a June 3, 1999 site visit, and from material properties taken from the FDS database.
An FDS model scenario was developed that best represented the actual building geometry, material thermal properties, and fire behavior based on information from the Reconstruction Committee and Physical Evidence. The results from this model scenario are provided with this report. Results from an additional model scenario, which included the opening of the sliding glass door on the first floor prior to opening of the sliding glass door in the basement, are also presented.
The FDS calculations that best represent the actual fire conditions indicated that the opening of the basement sliding glass doors provided outside air (oxygen) to a pre-heated, under ventilated fire compartment, which then developed into a post-flashover fire within 60 s. Some of the resulting fire gases flowed up the basement stairwell with high velocity and collected in a pre-heated, oxygen depleted first floor living room with limited ventilation.
Part of the mission of the Building and Fire Research Laboratory (BFRL) at the National Institute of Standards and Technology (NIST) is to conduct basic and applied fire research, including fire investigations, for the purposes of understanding fundamental fire behavior and to reduce losses from fire.
On May 30, 1999 a fire in a townhouse at 3146 Cherry Road NE, Washington D.C. claimed the lives of two District of Columbia firefighters and burned other firefighters. The District of Columbia Fire and Emergency Medical Services Department Reconstruction Committee requested the assistance of NIST for the purpose of examining the fire dynamics of this incident. NIST has performed computer simulations of the fire using the newly developed, NIST Fire Dynamics Simulator (FDS) and Smokeview, a visualization tool, to provide insight on the fire development and thermal conditions that may have existed in the townhouse during the fire. This document describes the input and the results of the NIST FDS calculations.
This account of the events relevant to the fire at 3146 Cherry Road NE is based on information provided to NIST by the Reconstruction Committee. Shortly after midnight, on May 30th, 1999, occupants at 3146 Cherry Road, NE awoke to a smoke alarm that had activated in the residence. The occupants went downstairs to the first floor, found hot smoky conditions, and exited the residence via the front door, leaving the front door open. At 00:17:00 hrs, the first 911 call was received. The first engine arrived on the fire scene in approximately 6 minutes. At approximately 00:24:00, firefighters began entering the first floor via the front door. Conditions on the first floor were described as “heavy smoke,” with thick black smoke coming from the doorway. Within two minutes, the front window on first floor was taken out by firefighters to provide ventilation. The window was removed from the inside, due to obstructions from security bars on the outside. Firefighters were also opening the second story windows on the front of the house. The occupants had left the second story windows on the backside of the house open.
Firefighters positioned by the sliding glass doors on the basement level, reported that the basement was fully charged with smoke and that upon arrival a few flames appeared briefly. The sliding glass door was broken out in two stages. First the right half was taken out at approximately 00:26:20. Then the left side was removed approximately 20 seconds later, due to obstructions from security bars. After the sliding glass door was broken out, firefighters entered the basement to conduct a search. They reported that there were a number of small fires on the floor of the basement, and that the fires began to increase in size after the sliding glass door was opened. The firefighters were ordered out of the basement as the fire rapidly increased in size. The firefighters reported that a tunnel or path was open in the smoke that enabled them to find their way out of the basement to the exterior, just prior to the basement becoming fully involved with fire. Within two minutes after entering the basement, flames from the basement extended up the backside of the townhouse. Seconds later there was a report that a firefighter was down. Firefighters that were working on the first floor reported that they felt an intense blast of heat prior to exiting the building. Two of the firefighters working on the first floor, one positioned near the open doorway to the basement stairs and the other located near the sofa on the back wall of the townhouse, died from injuries caused by the fire. A third firefighter, positioned between the two firefighters that died, survived the fire, but sustained substantial burn injuries.
The post fire investigation determined that the fire started near an electrical fixture in the ceiling of the basement. The basement had severe fire damage throughout, indicating a well-mixed, post-flashover fire environment. The stairway from the basement to the first floor also showed signs of flame impingement on the ceiling and walls. The door at the top of the basement stairs was open during the fire and had been partially burned away. The basement stairway opened into the living room on the first floor. The living room had significant deposits of soot throughout, with limited thermal damage. Most of the paper on the gypsum board walls and ceiling remained intact and sofas in the room only showed signs of pyrolization or limited burning on the upper portions of the back cushions and top surfaces of the seat cushions. Areas in the living room away from the basement door opening had less thermal damage.
NIST has developed a computational fluid dynamics (CFD) fire model using large eddy simulation (LES) techniques [1]. This model, called the NIST Fire Dynamics Simulator (FDS), has been demonstrated to predict the thermal conditions resulting from a compartment fire [2,3]. A CFD model requires that the room or building of interest be divided into small rectangular control volumes or computational cells. The CFD model computes the density, velocity, temperature, pressure and species concentration of the gas in each cell based on the conservation laws of mass, momentum, and energy to model the movement of fire gases. FDS utilizes material properties of the furnishings, walls, floors, and ceilings to simulate fire spread. A complete description of the FDS model is given in reference 1.
In large scale fire tests reported in [2], FDS temperature predictions were found to be within 15 % of the measured temperatures and the FDS heat release rates were predicted to within 20 % of the measured values [2]. For relatively simple fire driven flows, such as buoyant plumes and flows through doorways, FDS predictions are within experimental uncertainties [3]. Therefore the results are presented as ranges to account for this uncertainty.
Smokeview is a visualization program that was developed to display the results of a FDS model simulation. Smokeview produces animations or snapshots of FDS results [4].
Estimated time that firefighters from Engine 26 & Engine 10 are burned on first floor
FDS requires as inputs the geometry of the building compartments being modeled, the computational cell size, the location of the ignition source, the ignition source, thermal properties of walls, furnishings and the size, location, and timing of vent openings to the outside which critically influence fire growth and spread. The timing of the vent openings, Table 2, used in the simulation based on an approximate timeline of the fire fighting activities in Table 1.
Incident
Time
|
Actions |
Simulation
Time
|
|
00:17:00 |
First call reporting fire |
|
|
00:18:40 |
Second call – “fire in basement” |
|
|
00:23:00 |
Engine 26 on scene – “heavy smoke showing” |
|
|
00:24:00 |
Engine 26 and Engine 10 firefighters enter front door, Engine 17 layout |
0 s |
|
00:24:50 |
Battalion Chief 1 directs Truck 4 to rear |
50 s |
|
00:26:00 |
First floor front window removed |
120 s |
|
00:26:20 |
Basement sliding glass door half out |
140 s |
|
00:26:30 |
Firefighters from Rescue Squad 1 and Truck 4 enter basement |
150 s |
|
00:26:40 |
Basement sliding glass door completely out |
160 s |
|
00:26:50 |
Engine 17 in the rear, “fire small in basement” |
170 s |
|
00:27:20 |
Firefighters from Rescue Squad 1 and Truck 4 exit basement, “basement almost fully involved” |
200 s |
| 00:28:00 | Estimated time that firefighters from Engine 26 and Engine 10 are burned on the first floor | 240 s |
|
00:28:40 |
Engine 17 in rear, “fire extending to first floor” |
280 s |
|
00:29:00 |
(End of simulation time) |
300 s |
Note: Direct comparison of simulation conditions with the actual incident
conditions begin at
approximately 100 seconds of simulation time.
The floor plan of the basement and first floor of the townhouse are shown in Figures 1 and 2. The two levels of the townhouse are modeled by a 10.0 m (32.8 ft) x 6.0 m (19.7 ft) x 5.1m (16.8 ft) tall rectangular volume. For the FDS simulation this volume was divided into 76,500 computational cells. Each cell had dimensions 0.2 m (7.9 in) x 0.2 m (7.9 in) x 0.1 m (3.9 in). The placement and size of the interior walls, doorways, and windows were taken from the dimensioned floor plans drawn by personnel of the DC Fire and EMS Department. FDS adjusts the dimensions to the nearest computational cell. Therefore the cell size is the resolution limit of vents, openings, furnishings, or walls within the model. The cell size was selected to give the best approximation of the actual dimensions of the townhouse geometry.
The basement was vented to the outside by a pair of sliding
glass doors 1.7 m (5.6 ft) x 2.0 m (6.6 ft) high. For the simulation, the door vent was divided into two parts.
The right half of the sliding glass door was opened at 140 s into the
simulation and the left half was opened at 160 s into the simulation.
The basement was open to the first floor by a 0.8 m (2.6 ft) x 2.0 m (6.6 ft) high doorway at the top of the stairs. As in the fire incident, this door was fully open during the simulation. The front door to the first floor was fully open during the fire and the simulation. The door was 0.9 m (3.0 ft) wide and 2.0 m (6.6 ft) high. The front window on the first floor was 1.7 m (5.6 ft) wide and 0.9 m (3.0 ft) high with a 0.9 (3.0 ft) sill height. This window was opened at 120 s into the simulation. The other opening to the outside from the first floor was a sliding glass door at the rear of the house. This sliding glass door was located directly above the basement sliding glass door. This door remained closed and intact during the entire simulation.
The stairway opening from the first floor to the second floor was 0.9 m (3.0 ft) wide and 3.4 m (11.2 ft) deep. This vent remained open during the entire simulation due to the windows in the front and rear of the second floor being open. The exact position of the open rear windows on the second floor is not known; therefore, the stairway opening was used to represent the assumed area of the open second floor windows. The details of the second floor were not modeled in the simulation.
At the time of the fire, there was no wind, therefore for the simulation it was assumed that openings to the exterior were at ambient pressure.
|
|
Time of Event |
|||
Vent |
Initial Conditions |
120 s |
140 s |
160 s |
|
Front Door |
Open |
Open |
Open |
Open |
|
Front Window |
Closed |
Open |
Open |
Open |
|
First half of basement sliding glass door |
Closed |
Closed |
Open |
Open |
|
Second half of basement sliding glass door |
Closed |
Closed |
Closed |
Open |
|
Stairway door between basement & first floor |
Open |
Open |
Open |
Open |
|
Stairway opening between first and second floor |
Open |
Open |
Open |
Open |
The ceiling of the basement was composed of wood fiber ceiling tiles attached to wood furring strips, which were attached to the bottom of open wood trusses. Given the multiple surfaces in the ceiling floor system, several different approximations were used for the ignition temperature (320 °C to 390 °C) and the heat release rate per unit area (200 kW/m2 to 400 kW/m2). The assumptions used for the basement ceiling materials are shown in Table 3.
The walls of the townhouse were painted gypsum board,
assumed 12 mm (0.5 in) thick. The
sub-flooring was plywood and was covered with carpeting in the living room area
of the house. The ceiling on the
first floor was also painted gypsum board.
Several large furniture items were included in the scenario; a bookcase,
bar, desk and sofa in the basement as well as a door and sofa on the first floor.
The model inputs utilized for each material type are given below in Table
3 and the size of the furnishings are given in Table 4.
|
Material |
Thickness (m) |
Ignition Temperature (° C) |
Heat Release Rate (kW/m2) |
Thermal Conductivity |
Thermal Diffusivity (m2/s) |
|
Basement Ceiling |
0.025 |
330 |
300 |
0.14 |
8.3E-8 |
|
Gypsum Board |
0.013 |
400 |
100 |
0.48 |
4.1E-7 |
|
Pine |
0.013 |
390 |
200 |
0.14 |
8.3E-8 |
|
Upholstered Cushion |
0.10 |
370 |
700 |
0.20 |
1.2E-6 |
|
Item |
Material |
Size |
|
Bookcase |
Pine |
2 m wide, 0.3 m deep, 2.4 m high |
|
Bar |
Pine |
2 m wide, 1 m deep, 1.2 m high |
|
Desk |
Pine |
1.5 m wide, 0.75 m deep, 0.75 m high |
|
Sofa |
Upholstered cushion |
2 m wide, 0.75 m deep, 0.9 m high |
|
First floor door to basement |
Pine |
0.85 m wide, 0.05 m thick, 2.05 m high |
For the FDS simulation, a small fire with a specified heat release rate
was
used to start the fire growth. In
this case a 30 kW source, 0.2 m (8 in) square, located 0.1 m (4 in)
below the basement ceiling served as the FDS fire source. Starting the simulation with a flaming ignition enabled fire development
to be modeled within a reasonable computational time. The actual fire may have taken several hours to develop to
the flaming stage. As the simulated
fire
spreads from the ignition source, first along the ceiling and then to other
items in the basement, it develops quickly, but depletes its supply of oxygen
for combustion. This rapidly
decreases the heat release rate or energy that is being produced by the fire.
This produced a pre-heated oxygen depleted condition similar to that described by
firefighters upon their
arrival at the Cherry Road fire.
A time history of the fire’s heat release rate, as predicted by FDS, is shown in Figure 3. Annotations on the figure highlight the venting activities and the resulting impact on the development of the fire. As shown in the graph, venting the basement results in a heat release rate increase of more than 10,000 kW or 10 MW within approximately one minute.
Figure 4 shows a perspective view of the three-dimensional
townhouse simulation. The basement
level and first floor levels are shown with furnishings.
Figure 5 provides a side view of the townhouse.
The grid depicting the computational cell size is also shown.
The simulation results in Figures 6 through 15 have had all of the walls and other
obstructions removed to provide a clear view.
The horizontal clear area is the floor between the basement and the first
floor level. The results are shown
as a “slice” or a “plane” with a color bar that represents the
corresponding numerical quantities. The
results presented are taken at 200 s of the simulation.
At that time, the heat release rate and the thermal conditions have
reached a quasi-steady state condition. These
figures provide a snapshot of the calculated fire environment conditions that
the firefighters may have been exposed to at approximately 00:27:20.
Figures 6 and 7 show the plane of temperatures and
velocities that align with the center of the first sliding glass panel that was
taken out on the basement level. This
plane is located 3.4 m (11.2 ft) into the townhouse from the front of Figures 6
and 7. The upper portions of the
figures represent the kitchen area on the left and the living room area on the
right. In Figure
6, temperatures in
excess of 820 °C
(1500 °F)
are shown throughout the basement, with the exception of the cool air entering
the basement through the open sliding glass doorway at the right of the figure.
Similar hot gas temperature conditions exist in the living room area.
The maximum temperatures in the kitchen are in the 500 °C
to 660 °C
(932 °F
to 1220 °F)
range. The velocity vector plot in
Figure 7 provides gas flow direction as well as the approximate velocities.
The dominant flows in this plane are the fresh air entering the open
basement doorway at approximately 4 m/s (10 mph) and the hot gas flow exiting
the upper portion of the doorway at approximately 7 m/s (16 mph).
Figures 8 and 9 show the plane of temperatures and
velocities aligned with the center of the front door and the hallway, 1.4 m (4.6
ft) into the townhouse from the front of the figure. The upper portions of the figures represent the hallway and
living room areas and the lower portions represent the open area in the basement on the left
and an area in the storage room (cooler temperatures) on the right.
Predicted temperatures in the open area of the basement are in excess of
820 °C
(1500 °F),
from the ceiling to the floor level in some areas.
On the first floor, hot gases can be seen along the ceiling, cooling as
the gases move from the back of the townhouse to the front.
Outside air at approximately 20 °C
(68 °F)
can be seen entering the front door from the left. The gas moving into the townhouse, along the floor, from the
front door increases from 180 °C
to 260 °C
(350 °F
to 500 °F)
by the time it reaches the back of the townhouse (right side of figure).
The flow direction of the gases can be seen in Figure
9.
On the first floor, outside air is entering the lower portion of the open
front doorway in the range of 4 m/s to 5.6 m/s (10 mph to 12.5 mph).
Hot gases are exiting the upper portion of the same doorway with maximum
velocities in the range of 5.6 m/s to 6.4 m/s (12.5 mph to 14 mph). Toward the rear of the townhouse on the first floor, hot gas
flows from the basement doorway in excess of 8 m/s (18 mph).
Figures 10 and 11 show the plane of temperatures and
velocities that align with the center of the basement stairway, 0.4 m (1.3 ft)
into the townhouse from the front of the figure. The temperature plot shows hot gases in excess of 820 °C
(1500 °F)
filling the stairwell, flowing out into the living room, across the living room
ceiling and down the back wall. The
clear-notched area on the right side is the outline of the sofa.
Between the doorway to the basement and the sofa, the temperatures
approximately 0.5 m (1.6 ft) above the floor, to floor level are in the range of
180 °C
to 260 °C
(350 °F
to 500 °F).
The areas near the floor where the temperatures were the highest, were
near the doorway to the stairs and near the sofa on the back wall. These locations correspond to the areas where the two
firefighter fatalities were believed to have occurred.
Figure 11 shows the effect of the stairway on channeling
the hot gases up to the first floor. The
speed at which the fire gases flow up the stairway and across the ceiling of the
first floor exceed 8 m/s (18 mph). At
these velocities, the travel time for the gases from the front of the basement
(left side of figure) to the back of the first floor (right side of figure) is
less than 2 s. Between the doorway
to the basement and the sofa, the velocities from approximately 0.5 m (1.6 ft)
above the floor to floor level are in the range of 0 m/s to 1.6 m/s (0 mph to
3.5 mph). The right side of the
basement shown is the storage area under the stairs.
Figures 12 and 13 show oxygen concentrations.
Even though the previous temperature plots have indicted temperatures
that are consistent with flaming conditions, that cannot be assumed.
In addition to fuel and heat, oxygen is needed for flaming combustion to
be present. These figures provide
some insight on the amount of oxygen that was available in different parts of
the townhouse. The upper, hot gas
layers in the basement and on the first floor in the living room area contained
less than 6 % oxygen. These are
areas where the fire may not have had enough oxygen to produce visible flames.
Figure 12 shows the slice aligned with the center of the
right side of the basement sliding glass door.
Again the outside air can be seen entering the basement through the open
doorway from the lower right side of the plot.
A thin layer of 16 % to 19 % oxygen can be seen close to the floor on the
first floor. This airflow is coming
from the front door.
Figure 13 gives a view of the oxygen conditions along the
centerline of the basement stairway. The
hot gases that are flowing up from the basement are oxygen depleted, ranging
from 14 % to 16 % oxygen at the base of the stairs and decreasing to 6 % to 11 %
oxygen at the top of the stairs. The
high velocity hot gas layer that flows across the living room ceiling and down
the back wall of the townhouse (right side of figure) contains less than 6 %
oxygen. Given the oxygen depleted
conditions, little if any flaming combustion would be taking place in the living
room area at this time. The right
portion of the basement represents the storage area under the steps.
Figures 14 and 15 show the velocity flow patterns near the
ceiling of the first floor and at approximately 1.6 m (5.2 ft) above the floor,
respectively. The velocities in
front of the doorway to the basement are in the range of 8 m/s (18 mph).
Figure 15 shows the circulation of gases from the doorway to the
basement, across the back wall of the townhouse and then out the front window.
Velocities flowing through the house in this U– shaped pattern range
from 0.80 m/s to 4.8 m/s (2 mph to 11 mph) at this level.
These velocities coupled with the high gas temperatures will increase the
rate of convective heat transfer to people or objects in that area.
At the request of the Reconstruction Committee, a second fire simulation
was conducted. All of the input to
the second simulation was the same as the first, with one exception; the sliding
glass door in the living room on the first floor of the house was opened at 120 s into the simulation.
In the basement, the results
of the second simulation were similar to the first. On the first floor the
hot gases were not as confined as in simulation 1 resulting in cooler
temperatures near the floor.
Figure 16 shows the plane of temperatures that align with
the center of the basement stairway, 0.4 m (1.3 ft) into the townhouse from the
front of the figure. The
temperature plot shows hot gases in excess of 820 °C
(1500 °F)
filling the stairwell, flowing out into the living room, across the living room
ceiling and down the back wall. The
clear-notched area on the right side is the outline of a sofa.
This hot gas ceiling jet is similar to the hot gas conditions shown in
Figure 10. The significant
difference is in the region close to the floor.
Between the doorway to the basement and the sofa, the temperatures from
approximately 0.6 m (2 ft) above the floor, to floor level are in the range of
20 °C
to 100 °C
(68 °F
to 212 °F).
This is at least an 80 °C
(176 °F)
temperature reduction in this area with the open sliding glass doorway on the
first floor.
Figure 17 shows the velocity field at the ceiling of the
first floor. Comparing this to
Figure 14 shows that the velocity range is similar, approximately 8.5 m/s
(19 mph) vs. 8 m/s (18 mph).
The flow pattern at the ceiling is wider for the second simulation
because part of the flow stream is going out of the open sliding glass doorway.
The NIST FDS computer simulation predicted fire conditions
and events that correlate well with information from the Reconstruction
Committee and the damage, or lack of damage, to portions of
the townhouse. The model simulated
a fire that started in a combustible ceiling assembly in the basement of the
townhouse. The fire grew and spread
across the ceiling and into other fuels in the basement until it exhausted the
available oxygen supply in the basement. While
the fire’s heat release rate was being constrained by the lack of oxygen,
firefighters made entry on the first floor of the building.
Venting of the windows on the front of the townhouse on the first and
second floors had no noticeable impact on the fire development.
However, the venting of the sliding glass doors in the
basement increased the heat release rate of the fire very rapidly.
The FDS calculation indicates that the opening of the basement sliding
glass doors provided outside air (oxygen) to a pre-heated, under-ventilated fire
compartment, which then developed into a post-flashover fire within 60 s.
The fire filling the basement forced high temperature gases
(approximately 820 °C
(1500 °F))
up the basement stairwell at velocities in excess of 8 m/s (18 mph).
The high velocity gas stream flowed into a pre-heated, oxygen depleted
first floor living room. The FDS predictions show the hot gas flow moving across the
living room ceiling and banking down the back wall of the townhouse.
Between the doorway to the basement and the sofa on the back wall of the
townhouse, the temperatures from approximately 0.5 m (1.6 ft) above the floor,
to floor level are in the range of 180 °C
to 260 °C
(350 °F
to 500 °F).
These thermal conditions developed within seconds of the rapid fire
growth in the basement.
Even though the upper layer hot gas temperatures have
predicted temperatures that are consistent with flaming conditions, that cannot
be assumed. In addition to fuel and
heat, oxygen is needed for flaming combustion to be present.
The upper, hot gas layers in the basement and on the first floor in the
living room area contained less than 6 % oxygen when the basement fire was fully
developed and extending up the stairs. These
are areas, particularly the living room, where the fire may not have had enough
oxygen to produce visible flames.
A second NIST FDS simulation was performed.
The only difference was the opening of the sliding glass door on the
first floor at 120 s of the simulation or 20 s prior to opening the basement
sliding glass door. The most
significant difference in the predictions is in the region close to the living
room floor. Between the doorway to
the basement and the sofa, the temperatures from approximately 0.6 m (2 ft)
above the floor, to floor level are in the range of 20 °C
to 100 °C
(68 °F
to 212 °F).
This is at least an 80 °C
(176 °F)
temperature reduction in this area with the open sliding glass doorway on the
first floor as compared to the first simulation with the door closed.
1. McGrattan, Kevin B., Baum, Howard R., Rehm, Ronald G., Hamins, Anthony, Forney, Glenn P., Fire Dynamics Simulator – Technical Reference Guide, National Institute of Standards and Technology, Gaithersburg, MD., NISTIR 6467, January 2000.
2. McGrattan, Kevin B., Hamins, Anthony, and Stroup, David, Sprinkler, Smoke & Heat Vent, Draft Curtain Interaction – Large Scale Experiments and Model Development, National Institute of Standards and Technology, Gaithersburg, MD., NISTIR 6196-1, September 1998.
3. McGrattan, Kevin B., Baum, Howard R., Rehm, Ronald G., Large Eddy Simulations of Smoke Movement, Fire Safety Journal, vol 30 (1998), p 161-178.
4. McGrattan, Kevin B., Forney, Glenn P., Fire Dynamics Simulator – User’s Manual, National Institute of Standards and Technology, Gaithersburg, MD., NISTIR 6469, January 2000.