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429
Sensors and Materials, Vol. 29, No. 4 (2017) 429–443
MYU Tokyo
S & M 1336
*Corresponding author: e-mail: hmw6789@yahoo.com.tw
**Corresponding author: e-mail: wtm@cc.kyu.edu.tw
http://dx.doi.org/10.18494/SAM.2017.1525
ISSN 0914-4935 © MYU K.K.
The Simulation of Fires in Underground Parking Floors
by Fire Dynamic Simulator
Ming-Wen Hsu,* Shin-Ku Lee,1 Lin-Lin Huang,2 Yaw-Kuang Chen, and Chun-Mu Wu3**
Department of Architecture, National Cheng-Kung University, Tainan, 701, Taiwan, R.O.C.
1Research Center for Energy Technology and Strategy, National Cheng-Kung University, Tainan, 701, Taiwan, R.O.C.
2Department of Architecture and Interior Design, Cheng Shiu University, Kaohsiung 833, Taiwan, R.O.C.
3Department of Mechanical Engineering and Automation Engineering, Kao Yuan University,
Kaohsiung 821, Taiwan, R.O.C.
(Received August 30, 2016; accepted January 12, 2017)
Keywords: undergroundparkingoor,FDS,smokeventilationsystem
Trac ow in cities is increasing rapidly as cities modernize. The problem of parking is
gettingworseandworseduetoinsucientparkinglotsinlargecities,andpeoplearepayingmore
attentiontosafetyissuesinbuildingsduetothedevelopmentofundergroundparkingoors.There
arenewproblemsforre safetybecauseabuilding’sfunctionsandmaterials,structural type,size,
and supporting facilities are very dierent between the traditional buildings and buildings with
underground parking oors. When a re occurs in an enclosed underground parking oor, it is
hard for people to evacuate due to incomplete combustion producing heavy smoke. In this work,
we use the Fire Dynamic Simulator (FDS) to study the eect of a mechanical smoke ventilation
system to retard the development of a smoke layer. The simulated results indicate that, although the
installation of a mechanical smoke ventilation system would retard the deposition of a smoke layer,
freshair alsodrawninincreases theheatreleaserateof acarre.Most importantly,amechanical
smokeventilationsystemcanextendtheescapetimeforpeopleduringtheinitialstagesofare.
1. Introduction
Withacceleratingurbanmodernizationanddevelopmentoftheautomobileindustry,thequantity
and volume of trac due to automobiles and motorcycles in cities increases continuously. The
parkingdicultiesresultingfrominsucientparking facilities has become increasingly severe in
thelargecitiesofTaiwan.Theunsustainablegrowthofparkingdemandandrelativelyinsucient
supplyofparkingfacilitieshavebroughtaseriesofproblemstourbandevelopment,suchastrac
jams resulting from vehicle parking, trac volume resulting from looking for a parking space,
environmental pollution resulting from slow running while looking for parking. This parking issue
has become a bottleneck that obstructs the further development of the national economy. Therefore,
some large cities have actively developed public underground parking buildings and aerial parking
forbusy areas withinsucient land resources. As these undergroundparking buildings are very
dierent from traditional architecture, building materials, structural style, size, and supporting
facilities,theycausemanynewproblemsforresafety.
430 Sensors and Materials, Vol. 29, No. 4 (2017)
The annual re accident rate in parking lots increases with their annual usage. For this
research, 5 re accidents occurring in underground parking oors have been collected from the
literature. The descriptions are as follows: On February 12, 2007, the underground parking in a
23-storyamalgamated buildinginTaichungCitysueredare atabout6p.m.,in whichoneman
died and two persons had slight smoke inhalation. The eld remen connected smoke exhaust
fans to the smoke extraction pipes to extract the dense smoke from the basement. On March 27,
2014,thebasementofabuildinginTaipeiCitysueredare,andaconagrationbrokeoutatthe
scene while the re department was rescuing people. Five remen were injured and sent to the
hospital, and the 36 year old team leader of Huashan Station lost his life while being transported
to the National Taiwan University Hospital. On June 27, 2014, the underground parking in an
amalgamatedbuildinginNewTaipeiCityraisedarealarmat9:45p.m.,andthelocalrebureau
sent out rescue personnel; according to the report, a reman went downstairs to search for the
originof the reandanypersonsin trouble andexperiencedseriouschokingwhen he inhaledtoo
muchhightemperaturedensesmoke.Althoughhewassenttothehospital,thereghterdied.At
about 7:45 a.m. on November 20, 2014, in the underground parking area of the legislator research
buildingoftheLegislativeYuan,awhiteBMWcarbegantosmokeandcaughtre,andalthough6
or7reextinguisherswereemptied,therewasnotextinguishedandthedensesmokeobstructed
escape.OnMarch22,2015,arebrokeoutintheundergroundparkinglotofa7-storyapartment
buildinginTainanCity,andonewomandied.Inrecentyears,undergroundreshavecausedmany
casualtiesamong remen.Whether byaccidentorarson,most automobileresarecausedby re
inthe engine bay. Toextinguishsuchare,theenginehoodmustbeopened, and other oils may
ignite,causingtheretospread.Whenuntrainedpeopletrytoextinguisharebythemselves,they
maymisstheopportunitytoescape,especiallyfromwithintheconnesofanundergroundparking
facility, as the parked vehicles make the re and smoke dicult to control; such dense smoke
mayresult in poor visibility within a few minutes, andif the re extinguisher fails to eectively
extinguishthere,themediumfromthereextinguisherswillacceleratetheeectofthere;when
extinguishing fails and they attempt to escape, the diused extinguishing medium may obstruct
theirescape. In addition, dense smoke mayobstruct the remen’sabilityto search for survivors
andthe origin of re.An eectivelayout of mechanical smoke vents is veryhelpful for people’s
escapeandremen’sabilitytorescue,andwhencombinedwithautomaticresprinklersorreor
smokecompartments,theymayaugmenttheeciencyofreprotectionfortheentireunderground
parking space.
The most combustible items in underground parking areas are automobiles, which consist of
complexpartscomposedofinammableoils(e.g.,gasolineandengineoil),foam,rubber,batteries,
andplastics;thus,whenareoccurs,itspreadsquicklyandproducesagreatdealofdensesmoke.
Therearenumerouscausesforvehicleres,andthecommonconditionsaredescribedasfollows:(1)
(1) Fuel system leak
The ash point of 95 unleaded gasoline is −43–−38 °C (−45–−36 °F), and the self-ignition
temperatureis280–456°C(536–853°F);theashpointofdieseloilis>52 °C(>125.6°F),andthe
self-ignition temperature is about 177 °C (351 °F).Thedatashowthataashremayoccuriffuel
vaporcontacts a spark;forexample,thehightemperature ofanexhaustpipeissucient for even
dieseloilfueltoinitiateamassreinsuchcases.
(2) Wire sparking or electrical faults
Like residential res, many underground parking res are caused by a sparking wire instead
of a gas leak. The electric wiring in vehicles is aged by long-term over-heating, even though
Sensors and Materials, Vol. 29, No. 4 (2017) 431
the material is more resistant to heat than general household wire. The storage battery is another
problem; if the charge/discharge condition is poor or a poor storage battery is used, the storage
battery may explode.
(3) Lubricating oil leak in an engine bay
A part of the leaking vehicle phenomena results from long-term aging, and part results from
faults.Whileenginesleakingoilandtransmissionuidaremostfrequentlyseen,theoilforpower
steering,brakeuid,andgasoline/dieseloilmayalsoleak.Basically,suchoilproductsusuallyleak
fromthe spaceroroilseal;however,leaksmostfrequently occurintheenginebay. Manypeople
maynot know that cooling uid leaks may cause re as well, because the cooling uid contains
a large amount of ethylene glycol, which is inammable. In addition, some of these oils are
comburent,especiallytherequisitegasoline/dieseloilforenginecombustion,whichistheoptimum
combustible,and ifitleaks,serious hazardsarise.Thesehazards includethedesignofthe system,
as the gasoline/diesel oil pipes in many vehicles go through the front and rear ends of a vehicle at
the bottom.
(4) Engine overheating
The automobile engine is a large metal block which does not burn. There is only one cause for
an engine to overheat: poor heat radiation. There are many causes for poor heat radiation, such as
cooling tank faults, cooling fan faults, and coolant loss; however, the cooling system is usually the
cause. Incomplete combustion is also a cause, where unburnt gas continues to burn in the exhaust
manifold, resulting in high temperatures. When the engine is overheated, and as the catalytic
converter is overheated, the peripheral comburents reach the combustion temperature and burn. In
addition, there are more peripheral components than the catalytic converter, such as the many wires,
joints, plastic containers, plastic pipes, oils, and fuel pipes around an engine, which all age with
high temperature and may melt due to excessive temperature. Some components are combustible
aftertheyaremolten,whilesomeliquidsarecomburentaftertheyleak(e.g.,engineoil).
(5) Catalytic converter overheating
Forthecurrentinternalcombustionengine-basedvehicles,theexhaustsystemisequippedwith
acatalyticconverter,whichhasthebasicfunctionofoxidizingtheHC,CO,andNOx in the exhaust
system into water and CO2, and reducing part of the NOx to nitrogen. As the catalytic converter
must convert HC, CO, and NOx simultaneously, it is also known as a three-way catalytic converter.
In a general manner, the operation of a catalytic converter requires a xed temperature range,
and it will become overheated if forced to work in a high temperature range for a long time, thus
constitutingtheheatsourceforare.Iftheconverterexistsinanoverheatedoperatingrangefora
longtime,thereisprobablyaproblemwiththecombustioneciencyoftheengine.
(6) Arson
Cases of arson, which may be arise from emotion or money, are often seen on the news. Arson
is unlike the indirect or direct factors of vehicles seen in the previous cases; its burn is the fastest,
the least preventable, and it usually results in property loss and casualties.
Are in an underground parking space behavesasfollows:“the environmental space opening
is limited and conned; lighting is insucient; the smoke is dicult to exhaust, control, or
extinguish”;“theoutsideairsupplyislimited;incompletecombustionmayproduceagreatdealof
dense smoke, especially when burning cables and wires produce toxic gas, obstructing those inside
from escaping and remen from rescuing”; “as the space is conned, heat radiation and smoke
extractionaredicult,hightemperatureislikelytocausetherescenetemperaturetoriserapidly,
thus obstructing the initial rescue and escape, which may cause heavy casualties and evolve into a
severe disaster”.(2)
432 Sensors and Materials, Vol. 29, No. 4 (2017)
Chen indicated that “underground buildings” include basements, underground streets, and
underpasses and that the structures of underground buildings are very similar to conned high-
rise buildings. Therefore, an underground building re has similar features to a high-rise re.(2)
Undergroundparkingisatypeofbasement,anditscharacteristicsareclassiedasfollows:
1. Theresceneisreachedthroughstairsoraliftduringrerescue.
2. Whenanundergroundbuildingisonre,itislledwithdensesmokeandtoxicgases,because
therearefeweropeningsontheundergroundoor,theairisinsucient,andreismorelikely
to produce a great deal of dense smoke.
3. The heat cannot dissipate; the storage of heat certainly leads to high temperatures. As the
undergroundareaofabuildingis completelyconned,theretemperatureisoftenhigherthan
1000 °C.
4. Therespreadsupwardrapidlyinanundergroundbuilding,andonce an undergroundooris
onre,theoorsunderthegroundoorareinimmediatedanger.
5. Itisdiculttoescapefromanundergroundbuilding,theundergroundoorisdark,andwiththe
obstructionofcompartments,passages,doors,orotherspace,itisverydiculttoescape,andin
the dense smoke and high heat, life is endangered in a short time.
6. It is very dicult to carry out a rescue from underground buildings when an underground
oorhasa high temperature. Becausetherescuers must carry respirators,theycannot remain
undergroundforlong.Inaddition,itisdark,diculttojudgetheextentofthecombustion,and
eectiveprotectioncannotbeadopted.
In addition to the features similar to a high-rise re, underground parking has the following
special characteristics:
1. Theundergroundbuildingrescenechangesfromtimetotime.
2. The rescue work is dangerous.
3. Itisdiculttondtheoriginofthere.
4. Itisdiculttounderstandthere’sdevelopment;
Chung and Chiu(3) described the characteristics of underground building spaces (including
underground parking spaces):
1. As the opening into the space is limited and conned, it is dicult to perceive the internal
condition of the underground building space from aboveground; it is dicult to know the
ground conditions in an underground building.
2. Undergroundbuildingshavecomplexstructures,andtherescenechangesquickly,presenting
a very unstable state.
3. It is dicult to nd the re’s origin and control its behavior in an underground building,
remen’srescue islikely to belimited by the distance between the gateway andthe origin of
there,andthepath andspaceleadingtotherecannotcontaintoomany rescuepersonnelor
equipment,orreinforcementwillberestricted.
4. As underground building spaces are without windows or are conned spaces without open
oors,theoutsideairsupplyisrestricted.Thus,duetotheinsucientairforare,combustion
will remain in the smoldering state, rendering the problem of dense smoke more severe,
especiallyinareofsmoke-producingmaterials,suchascablesandelectricalequipment.
5. If the underground space is connected to other facilities, wherever a re breaks out, it may
spread to the other side.
6. The water jetted by an automatic re-extinguishing system or a remen’s hose is likely to
accumulate, thus obstructing rescue and escape, and resulting in heavy water damage and loss.
Sensors and Materials, Vol. 29, No. 4 (2017) 433
Zhang et al.(4) simulated re spread and fume ow in a simulated underground parking lot,
and the re spread rate and ow of smoke were observed under dierent ventilation conditions
by setting the same automobile re heat release rate. The plume in the parking space was very
disorderlyat15min,andtherebehaviorwasexpanded,makingrescueandescapedicult.Merci
and Shipp(5)discussedtheeectofsmokeandtemperatureonan undergroundparkinglot,smoke
extraction by mechanical ventilation, and the dynamics of smoke and heat. The condition of spray
sprinklers was input into the probable result, and the probabilities were studied. Deckers et al.(6)
testedfumecontrolinalarge-scalemotorparkusingcomputationaluiddynamics(CFD)software
tosimulatetheeectofmechanicalsmokeextractiononthefumeandfoundthat,ifthesmokewas
stuckintherecirculationzone,evenifthesmokeextractionratewasincreased,itwasimpossibleto
eliminate the smoke layer.
In this study, we use the Fire Dynamic Simulator (FDS) to observe the generation time and
rangeof dense smokein an undergroundparking re anddiscuss a mechanicalsmoke extraction
system to study how to postpone the smoke layer generation time and prevent a disaster from
developing further.
2. Methodology
2.1 Basic theory and governing equation of FDS
This study uses FDS 6.0 to build the experimental model and discusses smoke movement, the
reheatreleaserate,andsmokeheight inanundergroundparkingoorre.Thecharacteristicsof
FDS 6.0 are described as follows:(7,8)
FDS is a eld-based re simulation software developed by the Building and Fire Research
Laboratory, National Institute of Standards and Technology (NIST). It is a CFD model, which
takestheuidmotioninareasthe mainmodelobject.Theresultsofcalculationsareprocessed
by post-processing software (Smokeview), with which the plume, gas temperature distribution,
and ow eld distribution in the re scene are displayed in animation, the re scenario can be
establishedrapidly,andtheresceneinformationcanbeknownintime.Theprocessstructureand
leformatofFDSandSmokeviewareshowninFig.1.
FDS is a special computational uid dynamics software using 3D numerical calculation to
simulate the air ow driven by re buoyancy. The core of the software is the Navier–Stokes
equationset.Theequationsaredescribed,asfollows:
1. Massconservationequation
∂ρ
∂t
+∇ρu=
0
· (1)
ρ:uiddensity(kg/m3)
u:uidairvelocity(m/s)
2. Momentumconservationequation
ρ
∂u
∂t
+(u·)u+∇p=ρg+f+∇τ
∇
[
[
· (2)
434 Sensors and Materials, Vol. 29, No. 4 (2017)
p: pressure (Pa)
f: external force term, including friction (N), resulting from water droplets sprayed from the
sprinkler head
g: gravity + air velocity (m/s2)
τ: viscous stress tensor
3. Energyconservationequation
∂
∂t(ρh)+∇·ρhu =
Dp
Dt −∇·q+∇·k∇T
r+
l
∇·hlρDl∇Yl (3)
h: entropy (J/kg)
k: thermal conductivity (W/m·K)
T: temperature (K)
Dl:diusioncoecient(m2/s)
Yl: mass fraction of species l
4. Speciesconservationequation
∂
∂t
ρYl+∇·ρYlu = ∇·(ρD)l∇Yl+˙m′′′
l
(
(
(4)
ml′′′:massproductionrateperunitvolumeofspeciesl
5. Idealgasequation
p = ρRT (5)
Fig.1. OrganizationalstructureandsimulationcomputingprocessofFDSandSmokeview.
Sensors and Materials, Vol. 29, No. 4 (2017) 435
TheFDS classiesthetemperature,density,andpressureintospatiallyaveragedquantitiesand
perturbationsaccordingtotheBoussinesqapproximationequation,whichisexpressedasfollows:
T=T0(t)1 + ˜
T
( )
(6)
ρ=ρ0(t) (1 + ˜ρ)
(7)
p(r,t)=p0(t)−0(t)gz +˜
p(r,t)ρ
(8)
The spatially averaged quantity can be expressed by Eqs. (1), (2), and (5), and the adiabatic
process is as follows:
p0
∂Ω
u·dS+
V
γ
dp
0
dt
=
γ−1
γΩ
qdV +
∂Ω
k∇T·dS (9)
p0 = ρ0RT0 (10)
ρ0
ρ
∞
=p0
p
∞
1
γ (11)
The perturbation of velocity, temperature, and pressure can be expressed as:
∂˜
T
∂t
+u·∇˜
T= 1 + ˜
T∇·u+
dp
0
dt
(12)
∂u
∂t
−u×ω+∇H=
1
ρ
(ρ−ρ∞)g+f+∇·τ
[
[
(13)
∇
2H=−
∂∇·u
∂t
−∇
F
()
(14)
where H is the total pressure,
H
=
˜p
ρ0
+
|u|2
2
(15)
F
=−u×ω−
1
ρ
(ρ−ρ∞)g+f+∇·τ
[
]
(16)
Tosumup,FDSusestheenergyequation,Eq.(13),themomentumequation,Eq.(14),thetotal
pressureequation, Eq. (15), and the spatial average temperature, density,and pressure equations,
Eqs. (9)–(11), to compute the velocity, temperature, density, and pressure of the computational
domain.In terms of the numerical method of the governing equation, FDS uses the second-order
central dierence method for the derivative term of space coordinates and uses the dominant
second-order Runge–Kutta method to discretize the derivative term of time. The total pressure
dierentialequationinthePoissonequationformiscomputeddirectlyusingfastFouriertransform.
436 Sensors and Materials, Vol. 29, No. 4 (2017)
2.2 Undergroundparkingremodelsetting
The subject selected for simulation in this study is a one-story underground parking lot, which
is36mwide,36m long, and 3 m high. Atwo-way entrance–exit islocatedonboththeleft and
right, and the lane is at the bottom left corner. There are 21 cars parked in the parking lot. Each
caris 4.6mlong,1.9m wide,and1.4mhigh. Theinammable materialsaresetasgasoline and
afoamingsubstance,andthere arethreereoriginsinthisstudy.Therstreoriginisset asthe
rstcaron the upper left; the second re originissetastherstcarontheleftofthe lower row;
thethird re origin is set as therst car on the right of the lower row(labeled in red in Fig. 2).
There are six smoke height monitoring points shown in Fig. 3. The smoke height is estimated from
a continuous vertical prole of temperature. The method(9,10) is described as follows: Consider a
continuous function T(z)deningtemperatureTasafunctionofheightabovetheoorz, where z =
0istheoorandz = Histheceiling.DeneTu as the upper layer temperature, Tl as the lower layer
temperature, and zintastheinterfaceheight.Computethequantities:
Tu + zintTl =
H
0
T (z) dz = I
l
H−zint (17)
H−zint
1
Tu
+zint
1
Tl
=
H
0
1
T(z)
dz =I
2
(18)
Solve for zint:
Fig.2. (Coloronline)Thereignitionlocationsdenedinthisstudy.
Fig. 3. (Color online) Location of smoke height monitoring systems.
(a) (b) (c)
(a) (b)
Sensors and Materials, Vol. 29, No. 4 (2017) 437
zint =
l
I1I2−H
2
I1+I2T
2
l−2TlH
T (19)
Let Tl be the temperature in the lowest mesh cell and, using Simpson’s Rule, perform the
numerical integration of I1 and I2. Tuisdenedastheaverageupperlayertemperaturevia
H − zint T
u
=
H
zint
T(z)d
z
(
) (20)
In addition, this paper discusses the eect on the smoke height and re heat release rate of
mounting one and two mechanical smoke vents. The smoke vent is 0.5 m long and 0.5 m wide, and
its location is shown in Fig. 4. The computing grids used in this study are the maximum grid at 0.36
m and the minimum grid at 0.2 m; thus, the total number of computing grid points is 150000 (100 ×
100 × 15).
3. Results and discussion
Case1:Undergroundparkingreinactualstate(withoutmechanicalsmokeventilation)
To obtain a basis for comparison, the condition of an underground parking lot without a smoke
extractor is simulated rst. The simulated result in Fig. 5 shows that, when the rst car on the
upperleftoftheparkinglotisthere’sorigin,thesmokelayerattheS1monitoringpointdescends
Fig. 4. (Color online) Location of smoke vents. (a) Case 2 and (b) Case 3.
(a) (b)
Fig. 5. (Color online) Analysis of smoke height without smoke vent (Case 1-1).
(a) (b)
438 Sensors and Materials, Vol. 29, No. 4 (2017)
to a height of about 2.3 m at 20 s, and visibility is sucient for escape, as most of the smoke
layeraccumulatesnearthe re’sorigin, andtherehas not yet spread. At 50 s, the smokelayer
beginstodepositnearExit2,andthesmokeheightisabout1.5m.At80sofre,theheightofthe
neutral plane of the smoke layer at the S1 monitoring point is about 2 m, the smoke layer at the S2
monitoringpointdescendstotheheightof about1.6m, therebeginstospread,andvisibilityfor
escapeis severely inuenced. At 100 s, the smoke layer does not descend continuously,and the
smokeheight is1.6–2m. However,asthe rehasspread,the areaofthesmokelayer expandsto
the lane, thus severely obstructing escape.
Figure6 shows thesmokedepositwithoutasmoke vent when therstcaronthelower left of
theparkinglotison re.Thesmoke layer begins to deposit attheS2monitoringpoint under the
eectofthesmoke plume; however,as the smoke layercontinuesto diuse horizontally,itstops
depositing downward, and the smoke height is maintained above 2 m. The smoke deposits at the
S4 monitoring point at 40 s, rapidly descends to 0.7 m, and most of the dense smoke is discharged
through Exit 2; thus the smoke height at S4 returns to 1.7 m. However, the dense smoke begins to
aecthumansightifpeoplelookfortheexit.ThesmokelayerdiusestoS1at60s,andthenal
smoke height is lower than 1.5 m. Dense smoke diuses to the monitoring points (S3, S5, and
S6) near Exit 1 and the lane; however, because the lane is wide enough, the smoke height does not
inuencevisibility.
Figure7 showsthesmokedepositwhenthe rst caronthelowerright of theparkinglotison
re.AsmokejetpassestheS2monitoringpointbefore20s,this resultisidenticaltotheprevious
Fig. 6. (Color online) Analysis of smoke height without smoke vent (Case 1-2).
Fig. 7. (Color online) Analysis of smoke height without smoke vent (Case 1-3).
(a) (b)
(a) (b)
Sensors and Materials, Vol. 29, No. 4 (2017) 439
Fig. 8. (Color online) Fire HRR simulation results.
(a) (b)
(c) (d)
(e)
case.AstheS4monitoringpointisclosetothereorigin,thesmokelayerbeginstodepositat20
s. The smoke begins to deposit at S1 at 40 s, and because there is no mechanical smoke extraction,
thenalsmokelayerislowerthan1.59m.Asthere’soriginisontherightsideoftheparkinglot,
mostofthedensesmokeaccumulatesontherightandspreadstotheabovegroundoorsviaExit2.
Thestairsmaycauseastackingeectduetothedensesmoke,leadingtoheaviercasualties.There
islittledense smoke deposit at the left measuring point; thus the smoke height does not inuence
sight.
While the re’s origins are dierent in the re simulation, as there is no enough fresh air
imported,the car on re isnotburntcompletely,andthemaximumheatrelease rate of Case 1-1–
Case 1-3 shown in Fig. 8(a) is 1 MW.
440 Sensors and Materials, Vol. 29, No. 4 (2017)
Case 2: With one smoke vent
In this simulation, a mechanical smoke vent is mounted at the center of the underground parking
lot. Figures 9–11 show the simulated results of the upper left, lower left, and lower right cars
beingonre. When the re occursintheupperleftcar,the smoke layer deposition rate attheS1
monitoringpointintherst80sisalmostthesameascase1,meaningthesmokelayerdescendsto2m.
At 100 s, the smoke layer at the S1 monitoring point descends to 1.55 m, which is lower than the
smokelayer without smoke extraction,meaning that smoke extractioncan accelerate theair ow
in the underground space, the heat release rate is increased, and the dense smoke layer descends
fasterthaninthecasewithoutsmokeextraction.Figure8(b)indicatesthatthereheatreleaserate
Fig. 9. (Color online) Analysis of smoke height with one mechanical smoke vent (Case 2-1).
Fig. 10. (Color online) Analysis of smoke height with one mechanical smoke vent (Case 2-2).
Fig. 11. (Color online) Analysis of smoke height with one mechanical smoke vent (Case 2-3).
(a) (b)
(a) (b)
(a) (b)
Sensors and Materials, Vol. 29, No. 4 (2017) 441
ofCase2-1isclosetoCase1at theinitialstageofthere,butthereheatreleaserateatthelate
stage of Case 2-1 exceeds 1.0 MW, which is higher than the value of Case 1, meaning fresh outside
air is imported by the smoke exhaust system, which supports combustion. In addition, the smoke
layer begins to deposit at the S2 monitoring point after 80 s. The smoke layer is quite obvious
and dense at the S4 monitoring point near Exit 2, and the smoke layer descends to 1.43 m. When
asmoke vent ismounted in thecenter,the dense smoke ow is more disorderly than inthe case
without smoke extraction, and the smoke layer descent is not retarded in some areas. At S5, the
airow resultingfromthesmoke ventattractsthedensesmoke todiusetotheleft. Thestarting
time of deposit at S5 is almost the same as S1, which is much earlier than the case without smoke
extraction.
Whenthe re breaks out in the rst car on the lower left of the parking lot, theblack smoke
generatedbythere isattractedbythemechanicalsmokevent,andthesmokediuses fasterthan
the case without smoke extraction (Case 1). Furthermore, the fresh air imported by mechanical
smokeextraction acceleratesthere,and thegenerationofdense smokeisgreaterthanin Case1;
therefore, the dense smoke cannot be completely discharged from the smoke vent, and the dense
smoke accumulates at Exits 1 and 2. Figure 9 is the smoke height analysis. The smoke layer at Exit
2 (S4 monitoring point) is lower than 1.5 m, and the smoke height changes greatly, meaning the
poorsmoke extraction eectresultsinaturbulentstream. Ontheotherhand,asthe dense smoke
isattractedbythemechanicalsmokevent,itisdeectedtowardstherightside(Exit2).Therefore,
the starting time of the smoke layer deposit at Exit 1 (S5 monitoring point) in this case is later than
thecasewheretherebreaksoutattheupperleftcar.Whentherebreaksoutintherstcaron
the lower right of the parking lot, the dense smoke soon reaches Exit 2 (S4 monitoring point); thus
itdeposits after 20 s,and the smokeheight is 1.5–2.0 m.The smoke beginsto deposit at Exit1
(S5 monitoring point) after 70 s; however, the smoke volume is increased as the heat release rate is
increased by mechanical smoke extraction, and the smoke layer at S2 descends to 1.43 m, which is
lower than the smoke layer in the case without smoke extraction.
Inthe caseofonesmokevent, there’soriginhasasignicanteect onthere’sheatrelease
rate.Whenthere’soriginisontheupperleft,lowerleft,orlowerright,themaximumheatrelease
rate[Figs.8(b)–8(d)]is2.1,2.5,and1.0MW,respectively.Whenthe rebreaksoutonthelower
left,asthemechanicalsmokeventisclosetothere’sorigin,thefreshoutsideairdrawninbythe
mechanicalsmokeextractionincreasesthere’sheatreleaserate.However,when the re breaks
out on the lower right, the fresh outside air cannot be imported into the re scene, and the heat
release rate is close to the case without smoke extraction; thus there is smoldering or extinguishing
after 70 s.
Case 3: With two smoke vents (symmetrically allocated)
Thiscasediscussestheeect on the smoke layer accumulation and heat release rate of having
two mounted mechanical smoke vents in the underground parking re. The mechanical smoke
vents are located at the S1 and S2 monitoring points, and the total exhaust smoke level of the two
smokeventsisthesameasthepreviouscase.Figures12–14showthesimulationresultsofsmoke
layeraccumulationwhentherebreaksoutintheupperleft,lowerleft,orlowerrightcars.When
therebreaksoutintherstcarontheupperleft,partofthedensesmokeisexhaustedfromsmoke
vent 1, thus reducing the descent speed of the smoke layer. The smoke height at the S1 monitoring
pointisstabilizedat2.1minthesimulation,andthesmokelayerattheS2monitoringpointbegins
to deposit 70 s before that, as the mechanical smoke extraction accelerates dense smoke ow.
442 Sensors and Materials, Vol. 29, No. 4 (2017)
However, the smoke height is maintained at 1.7 m, which is a little higher than the smoke height
inCase1.ThesmokelayersatS4andS5(Exit2andExit1)aremaintainedabove1.8–1.9m;this
result shows that the smoke layer in the case with two smoke vents is higher than the case without
a smoke vent, which is very helpful for escape. However, according to the simulation results of
Cases 1–3, the location and number of smoke vents can inuence the volume of imported fresh
outsideair;thusthereheatreleaserateischanged.Mechanicalsmokeextractioncanincreasethe
heatreleaserate,andthere heat release rate is 2.0 MWin thecasewithtwomechanical smoke
vents[Fig.8(e)].
Fig. 12. (Color online) Analysis of smoke height with two mechanical smoke vents (Case 3-1).
Fig. 13. (Color online) Analysis of smoke height with two mechanical smoke vents (Case 3-2).
Fig. 14. (Color online) Analysis of smoke height with two mechanical smoke vents (average) (Case 3-3).
(a) (b)
(a) (b)
(a) (b)
Sensors and Materials, Vol. 29, No. 4 (2017) 443
Whenarebreaks out in therstcar on the lowerleftof the parking lot, thedensesmoke at
there’soriginisconnedtothere’sorigin;the smokelayeratS2descends rapidlytoabout1.5
m. However, because the smoke vents continuously discharge the smoke, the smoke layer at S2 is
maintainedat1.5m.ThoughS1isfarfromthe re’soriginandthere isasmokeventnearby,the
smokedoesnotdeposit until 72 s, andtheheight is stabilized at about1.8m.Thesmoke height
atS4ismaintainedat1.7–1.8m. Asthereoriginisclosetothelane,thestartingtimeofsmoke
deposit at S5 is earlier than in Case 3-1, and there is little smoke deposit at S6.
Whentherebreaksoutintherstcaronthelowerrightoftheparkinglot,asthereoriginis
fairlyfarawayfromthetwosmokevents,thedensesmokediusesuniformly,andthedensesmoke
begins to deposit at S2 and S4 at almost the same time. As the smoke is attracted by smoke vent 1,
the starting time of smoke deposit at S1 (47 s) is earlier than that at S5 (70 s).
4. Conclusions
Oncearebreaksoutinanundergroundparkinglot,whichisaoorwithoutanopening,the
building structure is damaged. It is necessary to enhance the re safety of underground parking
lotssothatpeoplecanbesafelyevacuatedandreextinguishingworkcanbesmoothlyperformed.
Inthispaper,weuseFDSsoftwarefortheanalysisofsimulatedres inundergroundparkinglots.
According to the results of this study,the eective layout of smoke vents can create the critical
time required for escape and initial rescue. The smoke vent location is signicantly correlated
withsmoke deposit.Ifthesmokevent islocatednearthere, the importedoutsideairmakesthe
reandsmokespreadquickly.Foranundergroundparking lot smaller than 1000 m2, the present
re code does not require mounted smoke exhaust fans. However, the simulations show that an
ecient layout of smoke vents (compared with one smoke vent for 500 m2 specied for smoke
compartments) can eectively prolong escape time. The ndings of this study can provide a
reference for underground parking lots to install the smoke detection sensors for detecting smoke at
earlyregrowingstagesinthefuture.
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