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Significance of flame-spread results

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SIGNIFICANCE OF FLAME-SPREAD RESULTS

J . H . McGuire and M.V. DrSouza

This Note describes the application of the concept of flame spread o r flammability in t h e design of a building. Tt is to be emphasized t h a t although such a concept is virtually indispensible in order to achieve a reasonable measure of fire s a f e t y , no such property as

flammability or flame spread strictly exists. Some of the limitations

imposed by this contradiction a r e discussed.

Tn developing a building design aimed a t minimizing f i r e h a z a r d ,

t w o f e a t u r e s c o n t i n u e t o be o f paramount importance. The first is t h e extent to which compartmentation [into fire resistant enclosures) is planned, with a view to containing the f i r e . The second is t h e e x t e n t to which the flammability of interior finishes (ceilings, walls and f l o o r s ) , and also contents, is restricted. The flammability of every

possible contributing surface should be limited to reduce the basic

probability of t h e development of a f i r e and, j u s t as important, to

lengthen the t i m e s c a l e o f any possible development. A longer Eire- growth period enhances t h e likelihood o f escape and of successful f i r e - f i g h t i n g and g i v e s more t i m e during which d o o r s can b e c l o s e d ( p o s s i b l y automatically) to complete compartmentation and thus c o n t a i n the f i r e .

Some architects

are

dispensing with compartmentation and regarding the provision of sprinklers as an adequate substitute. This concept i s

not discussed in t h i s Note, b u t it must be emphasized t h a t such a

substitution should not permit dismissal of flammability considerations.

The use of highly flammable linings and contents can give r i s e to s u c h

r a p i d f i r e development t h a t propagation proceeds beyond each area before

the associated sprinkle^ can operate.

MEASUREMENT OF FLAMMABILITY

Flammability b e i n g such an important d e s i g n factor, means of

assessing it are of equally critical importance. In North America the

most widely accepted metl~od is t h e tunnel t e s t . 1 2 p 3 Because this

apparatus is expensive and involves l a r g e specimens, another test officially known as 'The s t a n d a r d test method for surface flammability of materials using a radiant h e a t energy saurce0 4E162) has been

developed. The l a t t e r standard was i n t e n d e d f o r research and development purposes only, but is f i n d i n g other applications, for example, in t h e

regulation

of

the flammability of various components o f r a i l and r o a d vehicles operated by some city trznsit authorities.

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The tunnel and t h e E l 6 2 t e s t s have similar flammability rating s c a l e s

with zero representing an essentially nan-flammable m a t e r i a l with v e r y little combustible c o n t e n t to contribute to f i r e propagation. Higher

numbers represent greater f l a m a b i l i t i e s , a value of about 100 being

associated with thick heavy woods and values over 200 being regarded a s

unacceptable for applications o t h e r than f l o o r i n g .

The intended significance of such a scale is t h a t it should rank

materials (or assemblies) in

a

sequence of m e ~ i t , so t h a t if one particular

marerial is found to be acceptable (from a f l a m m a b i l i t y standpoint) then

substitution of a material with a lower ( b e t t e r ) index o r flame-spread value should also be acceptable, presenting an even lower hazard. It is usually assumed that the merit sequence is universally applicable,

regardless o f the f i r e conditions being considered. Thus T f material A has a lower flame-spread value than marerial 8 , it would be expected to give l e s s rLsk o f fire and slower development than B in any given set o f

circumstances. The r a t e o f fire propagation in a vertical s h a f t f o r b o t h

materials might be f a r faster than in the case of a l a r g e auditorium, but

f o r each of these cases, material E would be expected t o perform more

p o o r l y than material A .

It has always been known t h a t this concept is only an approximation

to the t r u t h , but

in

recent years anomalous r a t i n g s have been appearing quite f r e q u e n t l y . The following sections discuss two sets o f circumstances

i n which this can occur; a means of resolving the anomaly is given f o ~ t h e f i r s t case.

FOAMEII PLASTICS AND THERMdL INERTIA fkacl

Some years ago it w a s found t h a t many foamed plastics with tunnel

r a t i n g s of l e s s than 75

were

behaving more p o o r l y than more conventional

materials with r a t i n g s of several hundreds.

This

s i t u a t i o n created s u c h

a potential hazard t h a t the U . S . Federal Trade Commission condemned the

use of the tunnel (and certain other tests) f o r the assessment of the

f

l a m a b i l i t y o f these materials. Following consultation with thc: S o c i e t y

of the Plastics Industry, a consent order was issued recommending that

foamed plastics be cavered w i t h a substantial thickness of protecq:ive material.

A close examination of the fire behaviour of foamed p l a s t i c s in t h e tunnel has led ta a means of substantially resolving the problem of

flammability assessment6 and to a p o s s i b l e explanation of the mechanisms

responsible f o r the o r i g i n a l problem.

The unsatisfactory r a t i n g s only arise f o r those foamed plastics t h a t g i v e flame fronts that i n i t i a l l y advance r a p i d l y , b u t h a l t b e f o r e r e a c h i n g t h e end of the tunnel. It has been found t h a t the hazard o f such a

material

can

be satisfactorily assessed by a~plying a rate index (now incorporated i n t h e ULC Standard] to the f l a m e - f ~ o n t behaviour during the

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times t h e main index s p e c i f i e d in t h e s t a n d a r d . For

more

conventional materials, however, discrepancies are usually minimal.

The suggested explanation for the anomalous behavieur of foamed

p l a s t i c s in the t u n n e l is t h a t it is associated wEth t h e environmental

thermal i n e r t i a of t h e tunnel and the extraordfnarily low thermal

i n e r t i a and d e n s i t y of foamed p l a s t i c s . Thermal inertia ( t h e product

kpc where k = thermal conductivity and pc = volumetric heat capacity) is the thermal factor controlling the rate of heat f l o w in and onto a

specimen (and t h e su~rounding walls) to produce a particular temperature

distribution w i t h i n the specimen, A foamed plastlc with a low p r o d u c t

kpc can be warned with q u i t e small h e a t flows, whereas similar

tempexature distributions

in,

say, a dense wood would r e q u i r e much g r e a t e r flows.

The implicit assumption that a flammability merit or r a n k i n g

sequence

is

independent

of

the environmental thermal inertia in a given

s e t of circumstances has hitherto been reasonably valid, presumably

because t h e prevailing range o f thermal i n e r t i a [and d e n s i t i e s ) of

combustible materials was l i m i t e d . With t h e advent o f foamed p l a s t i c s , however, t h i s is no longer so and t h e behaviour of some of them i n t h e

tunnel illustrates t h i s feature-

Initially, during a tunnel exposure, a foamed p l a s t i c can behave

as

if it were highly flammable. After some involvement, however, when

the environmental thermal i n e r t i a o f t h e tunnel becomes significant, it can then behave as a relatively non-flammable material. I f t h e most a d v e ~ s e environment is to be c a t e r e d for, the flammability should be

assessed b y t h e suggested

rare

index. Such an approach is conservativc and avoids unexpected hazard, at The expense of penalising the foamed p l a s t i c in the rarer circumstance when it should be regarded as q u i t e

a non-flammable material. In fact some foams have proved to be of remarkably low flammability regardless of prevailing test or f i r e conditions.

The u s e of t h e rate index can thus be regarded as a reasonably satisfactory solution to the problem associated w i t h t h e assessrnenr o f

t h e flammability of foamed plastics. NON-HOMOGENEOUS SPECIMENS

The second set of circumstances giving r i s e to anomalous merit sequences involves non-homogeneous specimens tested by a method using a

time scale n o t representative

of

t h e f i r e scenario under consideration. A f e w isolated examples o f the e f f e c t , primarily associated w i t h steel-

backed specimens, have been known for many years. The advent of foil-

covered foamed plastics however has l e d to serious anomalies and it i s

now appreciated t h a t t h e mechanism responsible is similar t o t h a t

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The time s c a l e of a test, or o f the development of a f i r e , will govern the depth to which t h e specimen is thermally involved, Figure 1

illustrates a test (OT fire) situation

in

which two specimens, i d e n x i c a l t o a c e r t a i n depth b u t radically d i f f e r e n t thereafter, will give t h e

same performance. Figure 2 on the other hand illustrates depths o f involvement for which t h e same t w o specimens will behave markedly

d i f f e r e n t l y from each o t h e r , specTmen 2 behaving better than specimen 1 .

Figure 3 illustrates a metal-foil-covered foamed p l a s t i c and

the

depths of (thermal) involvement created by two d i f f e r e n t test methods A

and B. During the rapid test A , t h e influence of t h e metal foil (as a

heat capacity] will be substantial in view af the small depth of

combustible generating heat. The slower test B, on the other hand, will

involve m c h more combustible and hence the heat sink constituted by the metal f o i l will have much less i n f l u e n c e . Assuming that b o t h t e s t s rate most materials

in

the same sequence of merit, test A will rate t h e

specimen h i g h e r in t h e sequence ( i . e . , b e t t e r ) than will test B.

The effect of t h e metal facing, as j u s t described, is the opposite

of the metal backing, described e a r l i e r . All o t h e r aspects of t h e i r behaviaur also d i f f e r . For example t h e metal facing produces t h e

greatest e f f e c t with a s h o r t time-scale test, and a n e g l i g i b l e effect

with a long time-scale t e s t . Metal backing, on the o t h e r hand, has l i t t l e influence fn s h a ~ t time-scale tests but some e f f e c t w i t h slower

t e s t s . Usually t h e magnitude o f t h e effects is also less marked. The discussion on non-homogeneous materials has beem confined to

composites involving combustibles and metals, the density and thermal d i f f u s i v i t y of t h e l a t t e r being so markedly d i f f e r e n t from t h o s e of combustibles t h a t t h e e f f e c t described is maximum. Ifiere the component

materials are

more

similar, t h e effect may still occur, but will be of smaller magnitude. This i s illustrated by f i ~ e and test experience with

thin plywoad veneers. The f i r e behavlour of 118-in. ( 3 - 2 mm) plywood

veneer backed by glass-fibre insulation h a s not been inconsistent w i t h

tunnel r e s u l t s for t h e same t e s t assembly, In constructing mobile homes,

however, designers have used flame-spread results, intended for an

i n s u l a t e d assembly, that have been derived from specimens o f the 1 / 8 - i n .

plywood backed by asbestos cement. These have proved anomalous and f i r e

performance h a s been much poorer than i n d i c a t e d by the spurious test r e s u l t . When t h e e f f e c t o f I-in. glass-fibre backing w a s investigated,

a test result of 197 was obtained, whereas t e s t s

on

the same plywood

d i r e c t l y backed by t h e asbeszos cement of the tunnel l i d gave an average of 118.

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From the foregoing discussion t h e following conclusions can be dram.

(1) It s h o u l d be assumed t h a t t h e function o f a flame-spread (or flammability) test is to list materials in a sequence

o f

m e This assumption is seasonably valid for conventional

homogeneous materials and most composites o t h e r t h a n t h o s e t h a t

aTe metal -foil faced,

( 2 ) The test assembly must correspond to t h e assembly for which information i s required, to the depth o f themal involvement in

t h e t e s t . T h i s will usually not exceed an i n c h . An example o f a n

invalid t e s t i s t h e tunnel t e s t i n g o f plywood veneer backed by t h e

asbestos cement of t h e tunnel lid, when the assembly under discussion involves a lightweight insulation behind the veneer.

( 3 ) \fiere the material involved has a very low thermal i n e r t i a [product kpc) as with a foamed plastic, the assumption of a universally applicable merit sequence may n o t b e a satisfactory approximation to t h e truth. I n a conventional kpc environment t h e material may n o t propagate f i r e as far as some standard reference

material, whereas in a low LPC environment it may propagate it faster and f u r t h e r . A merit sequence applicable to adverse conditions f o r t h e lightweight material may be derived from a

tunnel test by using a ate index.

( 4 ) Where the assembly involves laminates of sharply d i f f e r e n t thermal

p r o p e r t i e s , a test method may rate the assembly satisfactorfly o n l y f o r fire scenarios involving similar time-scales. The effect will probably be substantial o n l y where metals are involved and then

o n l y when t h e metal is a facing or is very n e a r to the surface o f t h e assembly.

REFERENCES

1 "Standard Method of T e s t f o r Surface Burning Characteristics of

Building Materials,'VUnerrwriters' Laboratories of Canada,

ULC-S102-1977.

2 '3Standard Method of Test f o r Surface Burning Characteristics of Flooring, Floor Covering and Miscellaneous Materials," Underwritcrsr Laboratories of Canada, ULC-5102.2-1978.

3 "Standard Test Method for Surface Burning Characteristics of Building Materials,"AAST/ASTM E84-76a-

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4 "Standard T e s t Method f o r Surface Flammability of Materials Using a

Radiant Heat Energy Source,'qASTM E162-76.

5 "Cellular P l a s t i c s Products," U.S- Federal R e g i s t e r , Vol. 40,

No.

1 4 2 ,

July 23, 1975, p . FR 30842.

6 D%oauza,

M.V.

and J.H. McGuire. "ASTM E-84 and the Flammability of Foamed Thermosetting P l a s t i c s , ' q i r e Technology, Vo9, 13, No. 2, May 1977, pp. 85-94.

7 McGuire, J . H . "Flammability Merit Sequence and Specimen H o m ~ g e n e i t y , ~ ~

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S P E C I M E N 1 S P E C I M E N 2 E X P O S E D S U R F A C

@&Q

D E P T H TO W H I C H S P E C I M E M I N V O L V E D D U R I N G T E S T A S P E C I M E W 1 S P E C I M E N 2 FIGURE 2 p E p f # I N ' I O L V E M E N ~ : TEST M E T A L F O I L ~ ( E X P D S E D S U R r A C E ) DEPTH 0 I N V O L V E T E S T A DEPTH OF ~ w v o L V E M E N T : TEST 8 FIGURE 3 D E P T H INVOLVEMENT. F O I L - F A C E D F O A M E D P L A I T I C

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