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Shattering of unreinforced PVC roof membranes: problem

phenomenon, causes and prevention

Paroli, R. M.; Smith, T. L.; Whelan, B. J.

(2)

Shattering of unreinforced PVC roof membranes:

problem phenomenon, causes and prevention

Paroli, R.M.; Smith, T.L.; Whelan, B.J.

NRCC-40627-3

Building Better Roofs: IRC Technical Seminar, 11 Cities Across Canada,

September 1996-February 1997, pp. 93-107

(3)

SHATTERING

OF UNRFJNFORCED PVC ROOF

MEMBRANES: PROBLEM PHENOMENON,

CAUSES

AND PREVENTION

RALPH

M.

PAROLI

Nation$

Research

Council of Canada

Ottawa, Ontario, Canada

THOMAS

L*

s m

Natlanal Roofing

Contractors

Assmiation

Rosernont,

Ill.

Thi.

paper repom on the phenomenon of shattering of

unreinforcd

W C

roof membmgs. To further understand

the problem and to provide data for the assessment of

existing in-service unreinforced

PVC

roofs, samples of

unshattered (unweathered] and shamered membranes

were studied using dynamic mechanical analysis. It was

found that the glass transition temperature,

Tg.

may be use-

ful in explaining the shattering phenomenon.

Further-

more, the

*Fg

values can easily be obtained using dynamic mechanical analysis.

Recommendations to a d d shattering of existing unreE*

forced membranes (including the use of thermal analysis

to dusk shatter potential) are presented, along with mc-

ommendations regarding revisions to 'ASTM

D

4434.

Current generation reinforced

W C

roof membranes are also

discurrsect

ASTM D 4454. DMA, dynamic m&id malysis, g--

sition tempemfure, PVC, ply(vhyl chloride), roofmg mem-

branes, s h a k n g ,

Tr

t h d a d p i s , untpinforced

PI"%.

The prfonnamce of many

W C

roof membrane systems

has

been quite good. Numemm problems, however, hime been

repond with several of t h e early generatian w e i d k c e d (also referred fa as % o n - m & & ~ " ) W C meahma. The

Midwest Roofing Crmtmctcm Asmiation (MRCA) in 1979

and 1982,lb5! Griffin in 1982,s Walilace in 1983,4 and

Rosentield in 1984? reported shrinkage, embrittlement,

"impact fractures" and other unidentified types of

problem.

The rnajariry of these problem jobs utilized unreinforced membranes, although. in some instances, there were mpmts

of reinforced

PVC

m e m h e s experie-g embrittlement

and/or splitting prnkms.

As early problems b w n to appear, many people be- lieved that a thicker membrane was needed, since most of these early jabs had membranes that were a p p r o d t e l y

O.8lmm or 0.86mm (32 or 34

d)

thick A re-evaluarion

of the sheet's formulatian was also suggest4 by some.

However, Rasenfield recornmended that

W C

membranes

be "restricted" to reinfarced sheets.

Corps

of Engineers

BIUANJ.WHELAN

Sarnafil

Inc.

Canton,

Mass.

Guide Specification 07555 on W C membranes was subse-

quently developed. It prohibited the

use

af l~nreinforced

W C membranes on US. Army faIciEdeab

In these early problem reparts it

is

unclear if rhe pro& lem phenomenon referred to as "shattering" was experi- enced, Shattering is "characterized by a generalized non-

Pinear fragmentation of the membrane. Each fragment

may be a few hundred square feet in total area Typically,

when a shatter occurs, it extends throughout the entire

roof area,

from

one edge or erianeter to the other, and is

judged to be pan-repahMe.

$

Shattering typically has the pokntial to be quite devastat-

ing, since the building can suddenly become vulnerable to

water infihation throughout virtually the entire roof area.

nupais described this type of roof problem as a *failure lm1

IV.*

A level

W

&lure is "abrup~ totd, and in most

insmnces without

warning."

(See

Figures 1 to 4.)

In

e d y 1990, the National Roofing Contractors Assac-

iation (NRCA) became aware of an increased number. of

sbatter rqmrts. MRCA staff faMoWeeUp by analyzing Project

Pinpoint (a data base of problem

jobs,

as described in

Reference 9). The first incidence of shatteting was reported

to b j e c t Pmpint in 1986 A marlred increase in the num- k r of

~ p o m

in

1988 and 1909 were recorded

in

the data

base,

A sumnary of tbe Pro* Pinpoint data on shattering is presented in Appendix 1.

Althollgh

the total number of Project Pinpoint shatter

reports was small, considering the market share of

W C

membranes and the nature of the problem, NRCA decided

to contact all of the r n a ~ ~ e r s of

W C

membmes to

solicit their input on this phenomenon. Based

upon

that

input,

NRCA

surveyed its contractor membership in the

spring of 1990. A summary of the survey responses is pre-

sented in Appendix 2.

T h e

survey identified shattered

membranes

by

six manufacturers, faus of which in 1990 no longer manufactured PIC roof membranes in the U.S.

Subsequent to the sulvey, NRCA continued to compile

idomtion on reports of shattering, although there were

no additional surveys. A summary of these additional

reports is presented in Appendix 3,

As can be seen in Appendices 1 to 3. the vast majority of

the shatters reported to NRCA involved bidtasted mem- branes that were Bwerdl

years

old. Also, while many of the

(4)

membranes were 4,86rmm

(52

or

34

mils) thick, a high

percentage of the membranes were

1.22mm (48

mils) or

thicker. Membranes have shattered on bath small and

large roofs (from less than 9OmZ 110 squares] to over

9,00om2

[l,oOo

squares]).

And

whik the rnajoriy of the

shatters haw occurred on Iowslope roofs, some hawe

aha

occurred on slopes up to

k12.

The Project Pinpoint

d a b

s w c ) data and subsequent reports to NRGA are all highly corrrlated. It is also impoftant u, note that

d

the

approxi-

mately 255 shatter reports received by NRCA, a l l have

invohd unreinfomed membranes.

In the mmmer of

1990,

the S i f e Ply

R&g

Institute

(SPRI) and NRCA began work an a jaint document

regard-

ing shattering. The document, which was completed 'm

September of that year, described the shattering phmame-

non, discussed membrane identification and early warning

signs, and presented information on maintenance and

cold weather precautions? SPRI

aIso

formed a

task

force to

address this subjecr-l0

In

1991, NRCA a d the Institute for Research

in

Con-

struction,

of

the National Research Council

af Canada,

began a cooperarive research

pmgmm

on

PVC

shattering.

The purpose of th.e research, is to further understand the

shattering phenomenon, develop a technique that

cran

be

used

to

assess the shatter

pkntlal

of existing uateinfomd

membranes, and develop additiond criteria for

incorpora-

tion into ASTM

D

4494 (the standard for PVC roofing

sheets]l.ll

This

paper is a

progress

report on the work ac- complished to date-

The

cause ur muses of shattering

are

not precisely under-

stood. However, it is believed that shattering is related to a change in the physical properties of

the

m e r n b e which,

when combined with cold temperatures, results la the

dm~opmenf

af

Sarge tensile str- in the membrane.

Membrane tensile stresses can *be induced

by

membrane

shinkagt due

m

plasticizer mipatian or formation

d

new

lchemiml bonds. Stresses rran also

be

induced

by

1wtern-

perature, as reported by Dupuis in 1983.12 In addidon to

inducing stress, low tempemmres

may

cause the mem-

brane to become rigid (brittle).

If

an

unreinforcd membrane accum- enough ten-

sile srras, it

may rupture. The mpme may be

spontaneous or it nay occur by someone walking on the roof or by some

object falling on the roof.

Upon

rupture, the membrane

m d y lack d c i e n t -s to

prevwt

propagation

of

the split.

As

the split propagates, it branches into multiple

h e s ofrupture, as can be seen in

F

v

I

to

3.

Information gathered to date indicates that onEy a rela- k l y smnIl number of umehfiorced membranes

have

&at-

tered. However, sbce most

crf

the

mannlkctmzw of

these

products are no longer

in

business, it

is

diffic~lrt to deter-

mine the

nureber

of rod3 installed wirb

this

product

Also,

d a m

are not mailable on

the

number of shatters reported

(or attempted to be rep&) to these manufbcturers. The

number of pomtial s h a d

jobs

has

aLsD

been

reduced

to some extent by buildkg owners replacing

d.

The following sections d d b e

how

m d

why the ph@-

4 properties of a membrane may change. Tlwuugh the

utilization

af

thermal analysis, the membrane's

glass

transi-

tion temperature (the paint at which the membrane

becomes brittle) carv be determined. T h e glass transition t e m p e m

appears

to play an i-rtant role in b t k r h g .

The

application of t l m m ~ o a n ~ c a l techniques

in

the char-

audzdon of

mfmg

membranes % amently being studied

by

the CII3/ELEM joint cornmittm

on

roofing.13 Apprax-

bate@ a dozen papers have been wrimn r e g a r d l

&ennal

analysis and roofing membrane characterization.lCP6

Thema1 analysis

is

a technique that can provide same

insight

as to why some roofing M sf%l more than

others. D p u d c mechanical analysis

( D M

or DWA)

can

k med routinely to d e e m h e d a u s properties of a

d-

i g memtmme, e-g., the

g k

transition 2empemwe.

DMPL

instruments M y employ hmed vibration condi~i~rw to

d&rm a sample and sltudy i t s ~regro~lse. ~ c Since &rhe

instruments have the caphility af not only varying the

applied bquenq but a h alsothe

tenqxmnrre, DhaA Mls

under

the

broad

terminology of r h d a d y k Polymmk m u h g

mmbranes

are evaluated using d o u s test

methods

ahewel-

oped

for the assessment of d d t y -

M m m l

properties of polpmic materials h;we two facets; one Is related to the xmcrwspic behavior and the &her, to the r n o I e a k kebv-

i

m

which

indudes chemical ~]lm#~011 and pbj&aI s f r ~ c -

ture. For engineering applications the description of

mechardcal behavior under the design conditions is g e n d all

that

is reqoired. A C C O ~ , the idmmation o b h e d

fram these tests does not "plain why a material

Izas

Wed

and

how

it

can

b~

ixnprwed,

unless the Wurc is related to s i n m u d stfeqph. If& failure

is

related ta molecuk

ty, additional informalion is necessary

to

comprehend the

pmb1em fdq-

In

the work reported here, the

glass

transition tempera-

ture of unreinforced

W C

&g membranes which

had

shattered, was obtained

by

dynamic mecha3lical the&

analtysisr

T h r e

dm

were then c a m p d with tlie appm

priate

(ie..

same

manufacturer, product and thickness)

W C

sample stwed in

the

NRCA archives (sconaol sam-

ples"). A brief description rrh

Tg

and Dh4A.are given

h e .

A more derailed description can

be

found

in

Reference 13. The glass transition temperature (Tg) is a property of a

power and

is defined

as

the tempelat- at which the polper lases fhdbiIity and

becoraes

t r r f t t ~ e . ~ ~ - ~ ~ This is a

reversible process and the polymer will regain flexibility

above

the

Tg.

The

glass

tramifion t e r n m e is affected

by iree volme, a t t m c k forces between moledes, r o e

don about molecular h d s , st if he^^

of

mole^ chain -

and length of moledar chain. Plasricizers c a n help

in

reducing the

Tg

by

intdering with the chain motions

and

thereby sokening the polymer. Xt is

alsol

important m note that the

glass

transition temperature is always below the

melting temperaaxre of

the

polpmer. Generally, the tensile

strength

of polymeric mamiah belaw the

glass transi.tion

tmperam is

superior to the strength a-

Tg.

H o w ,

this is not necessarily a positive attribute.

The glass

transitioa temperature of a

polymer

can

change with aging of the mataid

(ems,

weathering).

T h e

emmition temperature map be i n a d due to fbef-

d

degradation of

PVC

or loss of plasticizer. The t h d

(5)

Iy darkening) of t h e membrane, and deterioration of

chemical and physicaI properties. The heat degradation of

PVC is attributed to the dehydrocklorinatian of the p l y - mer (evolution of HCl gas). In some W C membranes this can occur at temperatures as low as 100°C (21 2°F) .18*2*

Photochemical degradation (i.e., ultraviolet radiation) shows similar characteristics as those described in thermal

degradation. T h e main difference is that the changes

might not be visually observed (e.g., n o color change

might be noted

1.

Moreover, the precesses causing thermal

degradation are understood better than those causing

photochemical degradation.

Description of

DMA

~ h r e e - t e r m s can be derived from the stresstrain rehtion- ship as measured by D M

The

first term is the st- mod-

ulus ( E ) and is a measure of recoverable strain en@& in a deformed body (I.e., it is related to stiffness). The second term is the Iass modulus

(El

and is associated with the loss

of energy as heat due to the deformation of the material. The third term is the ratio of E'"/E' which yields the loss

tangent or damping factor (tan&). A more detailed descrip

tion of DMA can be obtained in References 17 and 33-37.

A typical D m plot containing E',

E"

and rang, as a func-

tion of temperature, is s h m in Figure 5. ff more than one peak is observed in a given

F'

or m 6 curve. then the peak closest to the melting paint or degradation point is usually

labelled as the a-peak. The Fpeak is the peak immediately

k l o w the a-peak T h e Tg due ro the main hackbone of rhe

polymer can normally be obtained from the most intense

peak observed in either the E" or ran6 curves Often, this

intense peak mrresponds to the u-mnsition. This can

bk

ver-

ified by a DMA experiment at various Erequendes I t should be noted

that

the

Tg

obtained by

E"

and

tan6

will be differ- ent. AKlM recommends using the peak in the

E"

cum.

The glass siti ion temperature, dewmined by DMA, is

dependent on the heating rate and frequency. Therefore,,

T values obmined by this dynamic technique are generally

d h e r e n t from that obtained by staric techniques (with

respect to frequency) such as differential scanning caIorimeq (DSC). Moreover, the t e m p e r a m of a poly-

mer can also be increased by subjecting the materia1 to

high frequency and high amplitude oscillations. Thus,

when studying dynamic mechanical propedes, low fre-

quencies and low strain amplitudes should be used. Low

strain amplitude is associated with the linear region of a

su-ess-su%in curve, but if a large stress or strain amplitude is

applied to a vkcoelastic material, high internal heat due to molecuEar vibration is generated. Thi results in a nonlin- ear viscoelastic response that is quite complex to analyze. Also, in nonlinear viscwlastic regions, the material is per-

manently modified. For example, microscopic crack forma-

tion or failure due to fatigue can result.

Clamping will affect modulus results and therefore absolute modulus ~ l u e s are obtained with great d i ~ c u l t y

using DMA. If care is taken, results within a given l a b r a t e r y will be reproducible, heme comparison amongst various

materials is feasible. Although DMA is weak with respect to the accuracy of absolute modulus, the transition tempera- tures can mhtinely be determined with great accuracy; The method used to obtain

T

(i.e., E" or tan6 peak tempera- ture) affects the MLue an& therefore, the parameter must

be specified. As long as t h e s a m e parameter is used throughout a study. the trend observed will b e the same regardless of the parameter used.

All PVC membrane samples obtained from shattered roofs

were unreinforced. Wherever possible, a sample was taken

from an area that was unexposed (the buttom portion of an "unbonded flap" at a seam (see Figure S)), az, well as from the exposed shattered area. Moreover, samples kom

the NRCA archives (i.e., unexposed and unweathered)

were included in this study. A typical composition for a genetic unreidorced PVC membrane is shown in Table 1.

B y n d c

M ~ c a i A 4 a l ~ IDMA)

The glass transition temperature of the membranes was

obtained using a Rheometrics RSA I1 [softwar version

3.0.1) dynamic mechanical analyzer equippea with a

mechanical cooIing device. The following experimental

profile was 4 far this study

Geometry: Sample width: Sample thickness: Sample length: Sweep type: Frequency: Temperature range: Heating rate:

Time per measurement: Strain:

Delay before test:

Correlation delay: Auto tension: Auto strxin: Dual cantilever 3.75-6.0mm 0.7-1.3mm 36.67mm I3rne/cure 1 Hz (6.28 rad./sec.) -70°C

+3O0C

2.0°C/min. 1.0 min. 1" 1@3 to gX lOrS 1.0 sec. 1

.o

sec.

No

No

The glass transition temperature was obtained from the average of at least two and- nr, more than four specimens

h r n the same sample. The values are reported as the maxi- mum in the loss modulus ( E ) vs. temperature curve. It is

a h possible to use the maximum of the. tan6 peak vs. tern- peratwe c u m , however, it was found that the

E"

c u m

gave

a better correlation with traditional mechanical data (e.g..

tensile and elongation). The glass transition tempera-

tures of the Mlious samples are summarized in Tables 2-5.

When examined under 8% magnification. wder-induced

checking on the exposed side of the samples from mmhani- rally attached membranes could be easily seen. It appeared that the checking depth was minor. On sample 90/91-20 (10

years old, from California), pronounced surface checking was visible with the naked eye. Surface checking was

also

visi- ble on 90/91-23 (7.5 years old, from Michigan). (Set Figure

7.)

Under 8x magd?cation, the width of the check lines on

this sample was greater

than

that observed on samples kum

other mechanically attached jobs. AII of the mechanically

atmched samples included in this study were of the same

mnuEaeturer, except for 90/93-23. Samples from ballasted

membranes were examined under 8x magnification, but checking was net observed.

(6)

On some of the samples from ballasted and mechanical-

ly attached sanples, scratches could be seen in the top side of the membrane. These appeared to be mused during or

after membrane application. Some of them may have been

caused during membrane removal, however, others ap- peared to be old scratches. The role (if any), in terms of

stress concmtration, &hat scratches play in Ehe shattering

phenomenon is unknown.

On some of the samp1es ti-om 90/91-2 (10 years otd,

hI-

lasted, Virginia), an "orange peel" surface was visible on

the top side of the sheet, This only occurred on samples

that were fairly clean. Other samples from this job had a

good

deal

of dirt on the membrane. These samples exhibit-

ed a smooth surface after the dirt was removed. (See

Figure 8.)

After cleaning off the dirt, one of the samples from

90/91-15 (10 years old, baHasted, Colorado) &so exhibited

an orange peel surface, but it was not as pronounced as on

the samples

from

90/91-2. All of the samples from 90/91-

13 were quite dirty. The sample that had the omge pee1

also had a discolored mottled pattern. The discolored

areas were light purple. Similar discolorations were ob-

served on some of the samples from other jobs.

SeYed samples, or portions of samples were noticeably embrittled. Far those samples with an e n d e d flap, typi-

cally the unexposed flap was supple, whereas the exposed

portion of the membrane was often relatively stiff.

~ ~

AND

DXSCUSSION T S

Table 2 contains

T

data for the control sample obtained

from the NRCA aFEim. AS am

be

am, the

gas

transition

temperature for samples C-IA through G9A ranges

h m

-23°C to

-50°C.

"Fhe shaaewd samples l i d in Table 3 are those that shattered in 1988/89 and 19189/90. In nearly ail

the the

Tg

shifted to much higher krnperatures. It is

interesting that for shattered samples not exposed to h e

environment (e+g., 88/89-2.1A b t m m and

88/842.3A

b t -

torn)

the

ATg was negligible (sm

F

w

9). Hence, it would

appear that only faaom refared to outside exposure to the emrironmenr are affecting the samples. %me of these factors

include contact with mud, mirnrganisms, oxygen, temper-

ature, md dtrwiele t radiation (depending upon degree of

ballast It is dm

possible

that

dirt in

the bgmast

and/or fungus atmck might be extmxbg some of the p M -

cizer

present

in

the membrane. Apart

fPom

samples 88/89- P . 4 A and 89/W1, the

Tg

was between 8'C and 17% higher than when it was originally installed.

If

the cause of the

change

in

T

is

due to plasridzer migrarion or formation of new chemid bmdr, then

h

h +ble that the -inforced

material

is

shrinking and/or rhat the md5cient of

~~

expansion is changing, thus generates an induced Isad.

Mmowr, the technique used irl the rnanuktw-hg process

may

also

be a factor in dimensional stability. Some rnanufac- huing prc~esses are more likely than others to buildin

szrrss.

The

glass

transition temperatures of the samples from

rook that shattered in 1990/91 are tabuSad in

Table

4. As

was seen for t!!e previous series, ATg varied quite extensive-

k.

The

Tg

of some sarnples &itled to a

higher

temperam

$ as much as S60C when eompared to the control. Once

again, samples mken from an unhanded flap yielded a

Tg

iimilar to that of the control. The only exceptions are

those belonging to the 90J91-10 series. In this case, the

b u m

unbonded flap

sample

was -41°C while the control

(G9A) was -23'C. It is possible that the control sample

is

not for Ehis series of sample5.

This

could haw occumd if

the formulations had been modified between the produc-

tion of control and the actual roof membrane. I f it is assumed chat the conwoi

should

have been in the vicinity of

41QC,

then the ATg for this series ranges from 205C to

43°C. Morewer, it is interesting to observe how, for a given roof sample, the Tg varies as sample is tested as one gets

further away from the shatter Iine. For example, sample

90/91-1D.lA

,

area #P and area #2 have a T of approxi- mately -21°C. while area 113 (oeu the shatter fne) has a

Tg

of only -7?2.

The data far the 91/92 wries follows the same mend as

the other series (see Table 5). In some mses, the

Tg

was

shifted to 19°C higher for the shattered sample than for

the corresponding control. The only exception was for

sample 91/92-lk In this case, the control sample is e 9 A and as previously mentioned might be the

m n g

control.

Generally, it would appear that the glass transition tem- perature as well as the ATg may be

useful

in explaining why

a roof shattered. The T howwer, cannot explain dl the

causes of shattering, an&ther facton m a y

be

invohrrd. For

example, samples 88/89-2.4A and &9/9@1 both have

Tg

less than -30%

and

a AT of only

+B

and +3 (see Table 5). In these cases, it is pwsiEle that on th day the rmk shat-

tered the temperature was below -30°C. To verify this

hypothesis, meteorological data

is

required.

The

findings of this earnpadscbn will be publiihed in the near future.

All of the abcwe dimmion applies to unreinforced PVC

membranes.

This

type

of roofing membrane has almost

exdusively been replaced

by

reinforced PVC membranes

which exhibit superior & m e d o m l stability. Therefore, it is imparrant m verifp. if the glass transition temperature can

still be applied in predicting the behavior of these rein-

forced membranes. P m l i and Dutt have recently p u b lished &dr findings on the application of

DMA

in ranking

the thermal stability of reinforced

W C

membranes.= En t b i

study

PVC samples were heat

aged

in an wen and then

characterized by D M . The resulb are summarized in

Table 6. As c2m be seen, the

Tg

for samples

Vl

and V3 changed significantly as

the

s a m p k were aged. The glass

transition tempemlure far sample

V%

only changed when

the sample was subjected to aging at 13C1°G for at least seven

days;..

It was conduded &om this study that sample

V1

was the least heat-resistant

W C

membrane. It is important

to note that this was also observed

in

the field, i-e., roof2

with membrane

VI

had more problems than with V2 or

V3. Thwefore, even though

W C

membranes are now rein- fmced, the

Tg

of

these

membranes should still be verified

and mcmimd to predict reladve stability. It appears that

formulatian of the

W C

membrane

if

critical LO the

long-

term performance.

CONCLUSIONS

Glass transition temperature may be useful in explaining

the shattering of unreinforced roofing membranes.

Tg

can

dso be used to predict the behavim of reinforced ro&g

(7)

Dynamic mechanical analysis is a Mtuable taol

in

character- king reinforced and unreinforced PVC roofing membranes.

More research is required to ccorreiaw the mechanical

properties of the shattered samples with the glass transition temperature. Also, correlation with meterrrological data is

required. Research also shouId include samples from older

roofs that have not shattered.

RECOMMWDATIONS

To

reduce the possibility of shattering existing unreinforced PVC membranes:

m Avoid rooftop t r f i c when the ambient temperature is below approximately +B°C (+50aF). or consult the mem-

brane manufacturer for a recommendation regarding

minimum temperature.7 (Note: A relatitle(y high lemp"nture

is recumtnended due tu bided kmpemte dab ot time ofsktlcr-

ing. A h , the membram limpmalure may be s.ubstantio@ b e h

tlre nmh& teqkmttrre).

9 It is recommended the building owner have the roof inspected serniannudiy by a roofing professional knowl- edgeable of PVC membranes. In particular, the inspector

should look for potential early warning signs of shatter-

ing, such as woad nailers, b e flashings or metal flash-

ings that have pulled away from their initial position (see

Figure 10). Also, look for plumbing vents or other pene- trations that have been displaced (see Figure 1 1 ) , A

membrane under high stress may appear to be visibly taut. Another potential early warning sign is an embrit-

tled membrane (i.e., the membrane has lost flexibility).

@ During tbe inspecdon, if items are found that could either

puncture the membrane (e.g., probrusions at flashings) or

fall onto the roof (e.g.. tree limbs), corrective action is rec-

ommended, as these items may initiate shattering.

Although these potential early warning signs do not

necessarily indicate the roof will shatter, it is recom-

mended that they not be ignored if found.

*

If potentid early warning signs are observed, membrane

replacement or repair work is recommended.

As

a repair to relieve membrane stress, new membrane

material may be added around the building perimeter

and at penetrations (if needed) as Carlson described in

1991.99 However, the repair may or

may

not

tLe success-

ful in greatly extending the rouf s service He. The shat- tered roof in Figure 1 reportedly had relief strips added at the perimeter a year or two before the job shattered.

Prior to executing repairs or maintenance ta relieve

stress or for other reasons, it is recommended the manu-

facturer of the membrane be contacted for recommen-

dations. If the manufacturer is no longer in business,

refer to Carlson's articles.=

In evaluating repair versus replacement, there are sev- eral issues to consider. Chief among these are the con- tents or occupancy of the building. If a shatter and subse-

quent water infiltration would be extremeIy detrimental

(either in the cost of damaged g o o h or to business inter-

ruption), then replacement may be prudent, since the

consequences of implementing a repair {which may Eail)

would be severe. Morewer, in considering repair versus replacement, lab analysis af samples from the roof in

question may provide useful data (see 'Laboratory evalu- ation of shatter potentiat" below).

It is recommended the slip sheet underlapent also be

evaluated when considering repair versus replacement.

For a time, unsaturated asbestos felt was sometimes used

as the slip sheet. If such a sheet was utilized, the dfficul- ties of dealing with a shattered job could be greatly corn- pounded by the asbestosxontainifig slip sheet. Because

the felt tvas not saturated with asphalt, it could be friable.

Accordingly, if the roof is exhibiting potential early warn-

ing signs of shattering and if ir has an unsaturated

asbestos felt slip sheet, roef replacement under con-

trolled conditions may be a prudent de~ision by the

building owner.

If an mreinforced membrane is to be recovered, special

precautions are r e c ~ m m d e d . ~ ~ If the membrane is to be left in place, it is reammended h a t it be cut at the prime- ter and around penetrations. And irl the field of the roof,

cut into pieces approximately 9m x 3m (10 ft x 10 ft).

It is recornmended that work be performed in tempem

tures greater than approximately +8"C (+50°F), to avoid

shattering during the teraohg work and thus avoid poten-

tial interior water damage. If work is conducted below i-8

"C

(+50 OF), special cold weather precautions are recornmen&

ed. These include warming the membrane prior to cutting

and having a contingency plan in place to deal with a shatter if it ownrs. Also, night tie-ins may

be

problematic, since the

existing membrane may shrink after the tie-in is made.

Labamtory embation of shatter potential

It appears that some insights into a membrane's shatter

potential may be achieved by performing thermal analysis

on several samples taken h m the roof. As part of the

Tg

analysis, it would be important ta find and analyze at least

one unbonded flap, since it appears to represent the mem-

brane in an aged, but unexposed condition.

In addition to

Tg

work, it m a y be helpful to also perform

temperature-induced load teats on samples &om the roof,

as described by Dupuis.l2

Jf an existing unreinforced membrane is exhibiting

potential early warning signs of shattering, laboratory 4-

=tian may be useful. While there b time and expense

involved in testing,

if

the roof is Iarge enough, h i s evalua- tion may indeed be worthwhile. If the analysis indicates that the

Tg

has changed significantly, then it should be realized that the original properties of the membrane have changed. This information could then be utilized in con-

junction with field and other laboratory investigations to

determine what remedial or replacement

work

would be

appropriate.

As currently drafted, the next edition of ASTM D 4434 will

only include reinforced membranes. However, the stan-

dard should also include criteria and test methods regard-

ing the relative sdility of the glass tr;anition temperature.

As can be seen in Table 6, the T stability of three different

reinforred products varied rig&cantly.

In addition, PllFTM D 4454 needs to be strengthened to

differentiate between those reinfmed PVC sheers that offer

(8)

Figure 12 is of a reinforced PVC membrane that has cracked

completely through the sheet (however, the reinforcement

is still intact). WhiIe repairable, this condition does allow

water infiltration. And if this type of problem occurs exten-

sively, repair is problematic.

The accelerated weathering test procedure introduced

bv Lys in 1985 should be considered.41

PVG

MfWBRANES TODAY

Essentially all PVC roaf membranes supplied to the U.S. market are now reinforced. At this time, it appears unlikely chat these products will experience shattering. In addition

to the utiliza~ion of reinforcement, PVC membranes are

typically much thicker than the early generation products. The increased thickness typically results in a greater reser-

voir of plasticizer, which should result in a longer mem- brane service life.58 However, simply having a thicker rein-

forced sheet does not necessarily ensure good long-term

performance, as other factors {such as amount and quality

of plasticizer, formulation and manufacturing process) influence performance.

Reinforced W C roof membrane systems can be expect-

ed ta perform quite welt when quality products are in-

stalled by professiona1 roofing contractors in welldesigned

systems. Many reinforced

PVC

roof membranes have suc-

cessfully performed for 30 years in Europe and nearly 20

pars in the U.S. and Canada. If the next edition of A!XM

D 4434 is similar to the present draft, this should be a

greatly improved standard for reinforced

PVC

roaf sheets,

which will allow specifying these types of products with

greater confidence in their p e r f a m c e .

The authors of this paper wish to thank those contractors, building owners and designers who sent in samples o r reparts

of shattered jobs. Our thanks are also extended to

Ms,

Ana DeIgado for her assistance in obtaining the DMA data.

Dupuis. R.M. and Morris, P.L., Single Ply Systems Session,

MRCQ Convention Program, 1979.

Roofing Systems Survey. MRCA, November 1982.

Griffin. C.W., Manual of Built-up Roof Sysrems, Second Edition, pp. 265,1982.

Wallace, RJ., 'Field Experiences with Single-ply Roofing Systems", Proceedings of the 7th Conference on Roofing Technology, pp. 12, April 1983.

Rosenfield, M.J., Construction of Experimental Polyvinyl Chloride (PVC) Roofing. pp. 17-1 8. April 1984.

Rosenfield. MJ,, Experimental Polyvinyl Chloride [PVC) Roofing: Field Test Results, pp. 17, February 1987.

Shattering of Aged Unreinforced PVC Roof Membranes,

NRCA/SPRI Joint Document, September 1990.

El Dupuis. R.M.. 'Different roof systems have different failure modes," P r ~ J ~ m a l Ro$ng, pp. 30, June 1990.

Cullen. W.C.. Project Pinpoint analysis: Trends and problems in low-dope roofing 1983-1988.1988,

' 0 ~ u s c h . J., 'SPRI task force scrutinizes PVC shattering issue,"

Aojmdmrrl Wng, pp, 32, August 1990.

I1'Standard Specification for PoIy(Viny1 Chloride) Sheet

Roofing" ASTM D 4434-87. Volume 04.04. Annual Book of

A!XM Sumdards, 1992.

12~upuis, R.M., "Single-Ply Test Report Part I," RooJng Spec, pp. 32, November 1983.

13u~erformance Teuing or Roofing Membrane Materials", Recorn mendations of the Conseil International du Batiment pour la ltccfierche ]'Etude et la Documentation (CIB) W.83 and R6union Internalionale des Paborntoires d'Essai et de Recherche sur les

Materiaux ct les Consuuctions (RILEM) 75SL.R Joint Committee on Elastomeric, Thermoplastic and Modified Bitumen Roofing, RILEM. Paris, France, November 1988.

14cash, C.G.. Thermal Evaluation of One-Ply Sheet Roofmg,"

Single Ply Roofing Technology, ASTM STP 790, pp. 55-64,

1982.

1 5 ~ c k e n s t o w , D. and Flueler, P., Thermal Analysts for Charat-

terizatian." Proceedings, 9th Conference on Roofing Technol-

ogy. National Roofing Contractors Association. Rosemont, Ill., pp. 5443, April 1987.

16Gaddy, G.D., Rossiter, W.J. Jr. and Eby, R.K. T h c Application

of Thermal w s i s to the Characieriz;rtion of EPDM Roofing

Membrane Materials." Roofing Research and Standards Dewl-

opment. MTM STP 1088, pp. 37-52, 1990.

I f ~ u t t , 0.. Paroll, R.M., Mailvagmarn. N.P. and Turenne. RC..

W;lassTransitions in Polymeric Roofing Membranes." Praceed- ings, 1991 International Symposium o n Roofing Technology,

pp. 495501, (1991).

Iliparoli, R.M. and Dutt, O., 'Dynamic Mechanical Anaiysis Studies of Reinforced Polyvinyl Chloride [PVC) Roofing Membranes," Polymeric Materials Science and Engineering. 65,

pp. 362-363, 1991.

1 ~ ~ a r o l i , RM., Dutt. O., Delgado, A.H. and Mech. M., T h e Char- acterization of EPDM Roofing Membranes by Themogravi- metry and Dynamic Mechanical Analysis." Thennochimica

Acta, 182, pp. 503-317,1991.

20~addy, G.D., Rossiter, W.J. Jr. and R K Eby, T h e Application of Thermal Analysis to the Characterization of EPDM Roofing

Membrane Materials After Exposure in Semce," Proceedings, 1991 International Symposium o n Roofing Technology. pp.

562-507,1991.

2 1 ~ a d d ~ . C.D., Rassiter, WJ. Jr. and Eby. R.K. T h e Use of TMA

to Characterize EPDM Roofing Membrane Materials," ASTM STP 1136.16&175,1991.

2 Z ~ a r o ~ i . R.M., Duti, 0.. Delgado, A.H. and7Stenman, H.K.

"Ranking PolyvinyI Chloride

[We)

Roofing Membranes Using

Thermal Analysis," Journal of Materials in Civil Engineering,

5(1), pp. 8595,1993.

25~elgado, A.H., Faroli, RM. and Dutt, O., Thermal Analysis in

the Roofing Area: Applications and Correla~ion with Mechm- . ical Properties." CIB World Building Congress. Montreal.

Canada, May 18-22, 1992.

Z4paroli, RM., Dutt, 0. and Delgado, GH., T h e Characteriza-

tion of Roofing Membranes using Thermal Analysis and

Mechanical Testing." CIB World Building Congress. hionwed,

Canada. May 1822, 1992.

2 5 ~ e n n , J.J. and Paroli, RM., Tvaluaring the EfFecrs of Aging on

the Thermal Properties of EPDM Roofing Materials," (In p H ,

Zlst North American Thermal Analysis Society (NATM)

Conference Atlanta, Ga., Sept. 13-18. 1992).

26~aroli, EM. and Penn. J.J.. "Measufing the ~ l a d m n s i t i o n Temperature of EPDM Roofing Materials: Comparison of

DMA, TMA and DSC Techniques," (Submitted to ASTM Symposium on Assignment of the Glass Transition." Atlanu.

Ga., March 44,1993).

ZT~eldrnan, I)., Polymeric Building Materials, Elsevier Scientific

(9)

z%illmeyer. F.W., Textbook of Polymer =ence. 3rd U, john Wley and S n s , New York, 1984-

29youngt

RJ.,

Inuoduction to Polymers, Chapman and )Itall, New York, 198 1.

3D~ikales, N.M., Mechanical Properties of Polymers, John Wiley and S a n ~ New York, 1921.

31 Hoq, PJ,. Principles of" Polymer Chemistry, Cornell University

h m , 1967.

%tosen, S,L, Fund-cnd Principles of Pofymeric Materials. Barnes and Nable. Inc., 1971.

SS~urayama,

T.,

Dynamic Me~hanical Analysis of Polymeric Material. Elsevier Scientific Publishing Campmy, New York,

1978.

34~endl;tnd~, W.W., Chemical Analysis 19: Thermal Analysis, 3rd

Edition, John W17cy 2nd Sons, 1%.

S f i ~ a r n ~ b e l l . B. and White, J.R.. Polymer Characterization: Physid Techniques, Cbapman a d Hall, New York, 1989. S6~rompton. T,R., Analysis of Pdyrners: An In~oduction,

Pergarnon Press. 1989.

s7~kmvmek, D.J. amd Schaff, CK. Rogreas in Organic Coatings,

16. pp. 1%-169,198$.

~ ~ ~ m t u s k a . C., "Roaf Covering Made of PVC Sheetings; The

ElTecr of Ptastic~ers on Lifetime and Semite Perfbfmanm,' Proceedings of the Second International Sympsium on Romf-

ing Technolw, pp. 173.1W5.

*~arlstln, J., "PVC maintenance and repair for raof system

longevity," and -%pair techniques far deficient details in W C mf membmes," RujhiimsI mng, pp, 58 and 64, January and Febmay 1991, respettively.

a M t C N ~ Cornention P q p n , at the 1991 N R M Cwwmbn. H.P., -Aging Criteria for PVC Roofing Membranes," h

eeedhgs af the Second laternational 5yqwsim an hofmg Technology, pp. 270,1985.

+P-=l

S

-

of Project PiPpait Amlys&, Prepared in

1990

1. The data base contained 22 shattered jobs. During

fol-

low-up

telephone conversations to verifj and obtain

additional data, four additional shattered jobs were reparted

The

following summary includes all 26&k 2. Seventyseven percent

of

the jobs

were

unreinforcled.

Far the remaining jobs, it was unknown whether the

sheets were reinforred. Based upon subsequent

reports

(Appendices

2 and 31, it is

probable that

hese

unknown sheets were dso unreinfarced.

3. Swenty percent of the shatters occurred, in 1988-1 990.

Four percent of the shatters occurred prior to 1985.

The

earliest shatter occurred in 1983.

4.

T h e

median roof age at

time

of failure was

73

years. The mof age at time of failure ranged fkam three to I1 years.

The

age was unknown on 15

percent

of the

jabs.

5. Membrane Attachenc masted:

...

.

.

...

mechamidly attached:

-...

8%

...

fully adhered:

...

....

4% unknown:

...,...

...

4% 6. Nominal memlmme thickness (at time of cnan-turr):

...

0.81mm or 0.Wmrn (32 or 34 mils):

97%

...

1.22mm

(48 mils): ,..42% 1.52mm (60 mils):

...--...

....,.

4% other/unknown:

...

27%

7. The shauers 0c:mrred in 24 smtes, including a few of the Southern states.

1. Eighty-four contractors reported 186 shatter

jobs.

2. A11 1% jobs utilized unreinford membranes*

3. Seventy-ueven percent of the shatters occurred in 1988- 1990. Three percent of the shatters occurred prior to 1985. The earliest shatter mcurred

in

1978.

4. The medim roof ;age at time of failure was 8 3 years. The roof age at t i n e ofbilure ranged from three to 13

years.

The

age was unknown on six percent of the jobs.

5. Membrane Artachrnenr:

bakted:

...

.

.,

...

..9 1 %

mechanically attached:

...

b...bb.6%

fully adhered:

...

3%

6. Nominal membrane thickness (at time

of

manuEac~e] :

O.&lmm or 0.86mm (32 or

34

mils):

...

47%

...

1.22mm (48 mils): 39%

1.52mm (60 mils):

...-...

*.-.--9%

other/unknown:

...

--.-

...

,..

...

,..

11% 7. %meone

was

on roof at time of shatter:

yes:

...

&

no:

...

67 %

unknown:

...

11% 8. Significant temgerature drop prior to shatter:

yes:

...*....*...

...**.*

...

-...

no:

.-

...

..

...

....--*-.

...

-.ZB%

...

unknown:

-19 %

9, Ambient temperature at time afshamr:

10,

The

~hntters acamed in 30 states, including several of

the *uthern states.

11. The mmuhcmrer was idenaed for

72

percent of h e

jabs, These jobs u N i e d sir manuEactusers. At the time

of the survey, faur

of

the six m a n u f a c r ~ m reportedly

no longer mzlnufactured W C roof

membranes

in the

us.

Note:

TJse

s u t v ~ p d u b w e rrot &&d ly NdltG4.

1. Tweny-two shattered jobs were reported during the

(10)

during 1991/1992.

All

29 jobs utilized unreinforced

membranes

2. The median age at time of failure was 10.5 years.

The

rmf age at time of f~Iure ranged from six m 14 years.

The age was unknown on 28 percent of the jobs.

3, Membrane Attachrnenc

ballasted:

...

,.

...

59%

mtcharricdy attached:

...

.

21

3

not reported:

...,...

4. Nominal membrane thickness (at

time

o f m u f m ) :

0 . 8 l m or 0.86rnm (32 or 34 mils) : .b..-.21

5%

1 .Emm (40 mils) :

...,...

-..-.---54%

...

...

1.52mrn (60 mils): ., 10% other/unknm:

...

34%

5. The shatten occurred in 14 states, hcIuding the Saa

Franusca Bay area of California.

6. Foliowing the 1990 survey, I 1 shattered jabs were

reported, which occurred in 1988,1989 or 1990. These

had nat been reported in the survey or in Projeer

Finpoint. Seven of these jobs were baUastd. Faur were

mechanically attached.

7. Three shatters were reported during the winter of

1992/1993

(thrwgh

FeImmjj 1995).

AU

rhree jobs were

m&~cally attached. Two wem 1.52mm (60 mils) and

one was 1.22rnm

(48

mils) nomid thickness at time of

rnanficture. O n e jab was 9 yean old and one was 10 years old, The age dthe otherjob was unlusm.

-4

l h s d p h n of Job!!i Frmn which Sampk Wem Ob-

Note:

Age at time of shatter is approximate. Thickness is the probable nominal thickness at b e

of

manufactwe,

88/89-1: Balilasted, 8 years old, 1.22mm (48 mils). over

foil-fked pIyisoqmurate, Iowa.

88/89-2: B a h t e d , 11 years old, 1.22mrn (48 mils), over a

kraft

paper slip sheet

over

polyurethane, hdiana.

89/90-1: Mechanically attached, 9.5 years old, 1.52mrn

(&I mils), wer a smooth surface built-wp mem- .

brane, Pennsylvania.

90/81-2: B d b t e d , 10 years old.

1.22mm

(48 mils), aver

kraft paper slip sheet. over rigid fiberglass/

polyurethane cornposi~ lnm-d*

Virginia

90/91-S: Ballasted, age unknown, unknown thieltness,

substrate

not idenmed,

IUinois.

90/91-5: Ballasted, 6 years old, O.86mm (34 mils), aver

irraft paper slip sheet aver pslyqrene, Virginia.

90/91-7: Ballasted, 8 yeam old, 0.86mm (34 mils), over

kraft

paper slip sheet over polystyrene, V i i a . W/9Z-10: Ballasted, 7.5 years old, 0 . 8 6 ~ ~ ~ (34 mils), over

polyater slip sheet over perlite, Illinois,

90/91-13: Mlasted, 10 years old, 1.22mm (48 mils), rwer

kraft slip sheet over polystyrene. Colorado,

Temperame at a t e of &a- was reported to

be

-28°C {-19=F). Someone was on the roof ar time og shatter.

90/91-14; Mechanically attached, 8 years old, 1.52mrn

(60

mils)#, over h a f t paper over expanded poiy-

styrene, Illinois.

Tempemre

at time of shatter

was reparted to be around -7°C (+2QuF).

93/91-16: Mechanically attached, 14 years

old.

1.52rnm

(60 mils), wer slip sheet over expanded

poly-

styrene, Pennsylvania, Temperature at rime of

shatter reparted to be around -15°C (45°F).

W/91-2& Mechanically attached, 10 years old, 1.52mm

(60

mils), w e r kraft paper over expanded poly- styrene, California.

90/91-23: Mechanically attached. 7-5 years, unknown

nominal thickness at time of manufacture, over

insularion (type not reported), Michigan. Roof

slope was approxbateEy 4: 12.

91/92-1: Ballasted, 19 years old, 0.86mm (34 mils), over

fabric scrim slip sheet over lightweight insulat- ing concrete. Illinois.

91/92-2: Ballasted, 13 years old, 1.22rnm (48 mils), over

kraft paper over expanded

palystyrene,

Colorado. Temperature at time of shatter was

reported

to be m u d -7°C (.t*W).

9 1 Ballasted, 11 years old, 112mm (48 mils), sub

rtrate not identifled, Indiana.

91/92-5: BaIlasteu, 11 years old, 1.92rnm (43 mils), sub

strate nat identified, Maine.

91/92-7: Ballasted, 7 3 years old, 1,22rnm (48 mils), over expanded polystyrene (a separator sheet was not

r e p o d ) , Iowa. 'Fernperamre at time of shatter was reported t5 be

wound

-1Z0C (+ll°F), or a

(11)

*

W 9= Year of shatter, winter of 1988/88

-2

=

chmnological order of sh* reports to NRCA (in this case, this was the second job reported in 1988/89).

*

.I

=

chronological order of samp8es from job number 2.

.C = thissample was taken f m a larger specimen.

*

88189-2.lA (top) = specimen taken from a sample with an "unbnded flap." Tap* iM~cates that the specimen is frarn the exposed m m b m e .

e 88189-2.1A @oftom) = specirrren taken from a sample with an " u n h d e d flap." 'Bottwn" ind'kates that the specimen is from

the unexpwd fxrttorn Aap

area

2. Jobs 881891 and W89-2 were baliasted. C-6A

C-7A G 8 A

C-9A

Table 3 GlBfS tram~rion v f u r c s of shaSlcrtd u m e i n f d PVC m m h a n a (88/89 a d 89/W s d ] .

Note: Sample from shattered jobs that corrdate to control samples C-44 C-5A, G 6 A and C-8A were not obtained. 1 mil = 0.0254 m m

Table 2 Glasr horn-tian tpmperahrres of unmnfwcd PVC d a m s j h n h"RCA archim (*conml ~a+ 3.

-22 -45 -33 -9 -30 -43 -36 -23 48 34 45 34 47-51 32 44 33 1985 1979 1979 1974-75 Ballasted B d l ~ s t e d Ballasted Ballasted C E E B

(12)
(13)

Tg Sample

Tg

Control A yg Probable

Nominal

I

ATg = Tg (Shattered sample)-Tg (cnntrof). 1 mil = 0.0254mm Note: All of these jobs were ballasted,

See Appendix 4 for further detail.

Area #I, #2. #3: Specimens from the same sample.

Note: 1. ATg = Tg (heat aged sample)

-%

(control). 2. Control = Unheated material

3. Sample thickness was between I rnm and 1 .l mm

(14)

Rjpm 3 GmmI vicar oJs SJLaltsnd d d p

t w d d

u a m . w pw: mIrpp*mr.

(15)

+

6 IrmoJan knbotrdadfip. ." Thc smm occun when? idca&d q P t k a m n u . ~ i n k ~ i s I q i R C : o n t b u n ~ ~ o a k i t A a d m d c d u n d m a m t h t h e ~ f M d i & b p d ~ @ . 100 IB'

6

3

3

CI 0 V I@ I@ 1017 -f - a 0 40.0 -20.0 0.0 20.0 40.0 511.0 -80.0 TEMP J 1 0 ~ ~ c. 10" u

-

o?

e

:>

I@ w 3 ,P

-

- i

, a F

d

3 )

td

rrF

19

-

-

-

7

E

' *

-

==

...mmm @ e m * * .

t

J

8 : . * m a

-

a

*

5

-

a

==.

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