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The effect of increased insulation on exposed bituminous roofing membranes
Turenne, R. G.
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THI
THE EFFECT OF INCREASED INSULATION
ON EXPOSED BITUMINOUS ROOFING W R A N E S
Division of Building Research National Research Council of Canada
O t t a w a
January 1977
THE
EFFECT
OF INCREASED INSULATIONON EXPOSED BIWINOUS ROOFING MEMBRANES
R.G. Turenne
Concern is expressed from time to t h e that increasing the amount
of insulation or specifying insufations having a loner k factor t o
improve the thermal resistance of conventional roofing systems might
adversely affect the performance of t h e membrane. Lower membrane
temperatures caused by increased thermal resistance could induce
higher stresses in the membrane, thus increasing the incidence of splitting failures. It is also feared that additional insulation could result in larger differential stresses
in
roofing membranespartially covered
with
snow, due to greater temperature differencesbetween
snow
covered and bare membrane areas.To evaluate these various factors, a specific roof construction
was studied. Roof insulation thichesses ranged from 0 to 4 in.
and
twooutside
temperatures and wind conditions were assumed;OaP with a IS mph wind and -45'F w i t h no wind. These conditions corresponded closely to the mean daily January temperature and the extreme minkmum temperature for Winnipeg, Manitoba during the past
32 years.
The membrane temperatures were calculated assuming two conditions:
a bare roof and one covered w i t h 12 in. of snow, The snow was assumed
to have a t h e m resistance of 10 units per foot. For simplicity,
t h e underside of the roof deck was assumed to be unfinished and the interior temperature to be
70°F.
me design of t h e roof selected for this study was as follows: 4-ply built-up membrane
insulation (assumed 4 units of resistance per inch) 2 -ply vapour barrier
4- in. concrete deck (standard aggregate)
.
Assuming winter conditions of O'F, 15-mph wind and
no
snow,the thermal resistance of t h i s construction w a s calculated as
Construction (heat flow up)
Top surface Membrane
Insulation of thickness "tmt
2 -ply vapcrur barrier
4-in. concrete deck
Bottom surface. [still air]
no insulation is used
If 1 in. of insulation is used
If
2 in. of insulation are used I f 4 in. of insulation are usedResistance
R
Adding 12
in.
of snow on the roof changes the t h e m 1 resistance as follows:Construct ion
(heat flow up)
Top surface snow
Membrane
Insulation of thickness "ttl
2-ply vapow barrier
4-in. concrete deck
[standard aggxegate) -
Bottom surface [still air]
If no insulation is used
If 1 in. of insulation is used
I f 2 in. of insulation a r e used
If 4 in. of insulation are used
Resistance
The same technique was used to calculate thermal resistance of- the roof system at - 4 5 ' ~ . With a no-wind condition, however, the
resistance of the top surface increases by 0.44 to 0.61. This amount
(0.44), therefore, was added t o all previously determined values,
The temperature
of
the upper surface of the membrane cannotexceed 32'~ as long as it is covered w i t h snow. In the ensuing
calculations, therefore, the membrane surface temperature was
maintained at 3 2 O ~ whenever the resistance above the membrane was high enough to produce a temperature greater than 32'~ at the membrane
surface. The heat flow from the inside to the membrane surface and from the membrane surface to the outside air was then calculated, the difference between these values being the heat available for melting
(see Table I ) .
Discussion of Results
in
Table I(a) The mean membrane temperature changes very little when the thickness of insulation is increased f r o m
X
to 4 in. For anoutside temperature of
o°F,
the difference is 2 112OF; for -45OFthe difference is 10°~.
(b] The temperature difference across a membrane is due to its
thermal resistance. It decreases as the thermal insulation increases. Table I (Column 73 shows that at -45°F and no snow,
the temperature difference across a membrane placed over an uninsulated roof is 2 0 . 3 O ~ . I t is 6.4OF when placed over 1 in. of insulation and 2 . 2 a ~ with 4 in. of insulation.
( c ) Adding insulation to a roof i n i t i a l l y increases the spatial
temperature variation of the membrane on a roof partially covered with snow. However, as more insulation is used, this temperature
difference decreases. For example, at -4S°F the difference in
temperature between arr area of membrane clear of snow and one
having a. 1-ft snow cover is 62.S°F when there is 1 in. of insulation
under
the membrane; if the thickness of insulationis increased to 4 i n , , the difference in temperature between the
two areas is reduced to 3g°F. In column 4, Table I additional
values are listed for other thicknesses of insulation. These values are p l o t t e d against the insulation thiclmess in Fig, 1. The graph shows that insulation first increases the spatial temperature variation, but as the amount of insulation is
increased the temperature variation decreases.
[d) Adding insulation reduces or eliminates snow melting, especially
at lower temperatures, by decreasing the heat loss through the
roof. As ice on roofs may be a contributing factor to premature membrane failure, a measure minimizing snow melting could be desirable.
[e) The mean temperature of
the
membrane may be lower due to theincreased thermal resistance; however, as the mean temperature
drops, so does the temperature difference across the membrane. The effect of increased insulation
on
t h e daily variation ofthe membrane temperature due t o solar radiation has nut yet been considered. Steady state calculatims were made to determine the
possible range of temperatures that the membrane might experience
under severe exposure. A case
involving
t h e following winter cwnditionswas assumed:
Inside air t q e r a t u r e Solar radiation
Outside ai.r temperature -10°F day, - 3 0 ° ~ night
Sky temperature -30'F day, -SOOF night
Crmvective
coefficient hc 0.8 Btu/f~r ft2 O FRoof emissivity and absorption 1.0
The c a l m l a t i o n s gave the fo1,lowing results:
Ruof Temperature day, F'
Roof Temperature night, OF
The heat capacity of the roof would likely result
in
a smaller variation between day and night, particularly for the uninsulatedroof. The calculated temperatures do, however, give a reasonable
coutparism for insulated roofs. They show very l i t t l e difference between a roof having a minimal thermal resistance and one having
16 units.
Ix
may be concluded, therefore, t h a t increasing theinsulation on raofs does not appreciably increase the severity of
therrnal cycling of the membrane due t o solar radiation.
' h e added thickness of insulation, however, means that the membrane and the stmctu.lra1 deck are spaced further a p a r t ,
The
physicalproperties of the insulation and the adhesives take on added
significance therefore, since thermal stresses shauld be transferred from the membrane t o t h e deck in well designed and well built roofs, These stresses must he considered by the designer and roofing con- tractor in selecting the insulation, the adhesive, t h e felts, and
t h e installation technique. Proper adhesion of all components
between the- membrane and the deck s h w l d be ensured. The insulation should have adequate shear and tensile strength. A l l layers should be firmly bonded together when more than one layer is used.
If
these recommendations are followed,- splitting failures andincidences of thermal shrinkage of membranes installed on roofs having
increased thermal resistance should be no more numerous than at
present.
Acknow ledgernmts
The author wishes to acknowledge the contribution of information
by Mr. K.R. Solvasan on the effect of s o l a r radiation and night time
cooling on the membrane. The suggestions and comments made by Mr.
T H I C K N E S S O F I N S U L A T I O N , I N - F I G U R E 1 CURVES S H O W I N G R E L A T l O N S H I F B E T W E E N T H I C K N E S S O F I N S U L A T I O N
A N D
S P A T I A L T E M P E R A T U R E D l F f E RENCE O F . M E M B R A N E S P A R T I A L L Y COVERED W I T H S N O WTABLE
I Insulation Thfckness
"trTin.
0 1 2 4 Heat LossFrom
I n t e r i o r ~tulhr-ftZ 30,2 7.0 4 .O 2 . 2 30.2 7.0 4.0 2.2 Heat for Melting Btu/hr- ft 27 3 . 8 0.8 None 23 None None NoneMean Membrane Difference
h e
t o Snow O F Temp. NoSnow
1 4 . 5 4.0 2.5 1 . 5 2.5 -30.0 -36.0 - 4 0 . 0 O F 1 ftSnow
37.0 33.0 32.5 26.0 37.0 32.5 17.0 -1.0 SurfaceTemp.
a~Conditions for a o O E Outside Temperatu're
Temp. Difference Across Membrane
F
NO
Snow1
ft SnowNo Snow
20.5 29.0
SO.
0 24.51
ftSnow
32 32 32 25.8 8 . 3 2.1 1.2 0 . 7Conditions for a - 4 5 ' ~ Outside Temperature
16.5 4.2 2.5 1 . 5 34.5 62.5 53. Q 41.0 10.0 2.3 1.3 0.7 10.0 2 , 5 2 . 0 1.4