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The Effects of Temperature on Insulation Performance: Considerations for Optimizing Wall and Roof Designs

May 15, 2016

3 1 s t RC I I n t e r n a t i o n a l C o n v e n t i o n a n d T r a d e S h ow • Ma rc h 1 0 – 1 5 , 2 0 1 6 S c h u m a c h e r e t a l . • 1 6 5
The Effects of Temperature on
Insulation Performance: Considerations
for Optimizing Wall and Roof Designs
Chris Schumacher and John Straube, PEng
Building Science Consulting, Inc.
167 Lexington Court, Unit 6, Waterloo, Ontario N2J 4R9
Phone: 519-342-4731 • Fax: 519-885-9449 • E-mail: chris@buildingsciencelabs.com
Lorne Ricketts, EIT, and Graham Finch, PEng
RDH Building Engineering, Ltd.
224 W. 8th Avenue, Vancouver, British Columbia V5Y 1N5
Phone: 604-873-1181 • Fax: 604-873-0933 • E-mail: lricketts@rdh.com
Abstract
Recent research into the real-world performance of insulation materials in roofs and
walls has shown that the industry’s reliance on R-value at a standard temperature does
not always tell the whole story. This paper will present measurements from several fieldmonitoring
studies across North America that demonstrate how insulated roofs and walls
exhibit thermal performance that is different than assumed by designers. Specifically,
results show that insulation properties vary with temperature (i.e., performance changes at
high or low temperatures). This is important because of peak energy demand, annual heating
and cooling costs, occupant comfort, and durability considerations.
Speakers
Chris Schumacher — Building Science Consulting, Inc.
Christopher Schumacher is a principal with Building Science Consulting, Inc.
(BSCI), a consulting firm specializing in design facilitation, building enclosure commissioning,
forensic investigation, and training and communications. Its research division,
Building Science Laboratories (BSL), provides a range of research and development services.
Schumacher’s presentations on temperature-dependent R-values include the Westford
Building Science Symposium in 2011 and the Rockwool Research Symposium in 2014. He
has also written on this topic for buildingscience.com.
Lorne Ricketts, EIT — RDH Building Engineering, Ltd.
Lorne Ricketts is a buildings science engineer with RDH Building Engineering, Ltd.
in Vancouver, BC. He is actively involved in forensic investigations, building monitoring, and
new construction projects, as well as laboratory and field-testing. Lorne’s practical experience,
combined with his theoretical training and proficiency with state-of-the-art thermal
and hygrothermal (heat, air, and moisture) software modeling tools, have enabled him to
evaluate a wide variety of enclosure systems.
Non-presenting Coauthors
John Straube, PEng — Building Science Consulting, Inc.
Graham Finch, PEng — RDH Building Engineering, Ltd.
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ABSTRACT
Recent field and laboratory research
into the real-world performance of insulation
materials in roofs and walls has shown
that the industry’s reliance on R-value at a
standard temperature does not always provide
the whole picture. Insulation properties
vary significantly with cold to hot temperatures,
meaning that heat loss or gain into
a building is not always as predicted using
standard calculation techniques. This is
a consideration for all insulation types, in
particular those used in roofing or continuous
exterior insulation applications where
they are exposed to more extreme cold or
hot temperatures.
This paper will present measurements
from field-monitoring studies, which identify
and demonstrate how insulated roofs
and walls exhibit thermal performance that
is different than assumed by designers.
This is important because of peak energy
demand and annual heating and cooling
costs, as well as comfort and durability
considerations.
Laboratory testing results are also presented
to demonstrate and explain these
phenomena. New testing methods have
been developed to quantify this temperature
dependency. Temperature-dependent
R-value curves will be presented for all common
building insulation materials.
Finally, computer simulations were
prepared using the updated insulation
properties. These were calibrated with the
field data and extended to demonstrate
the impact that these insulation properties
have on the actual energy use, temperature
profiles, moisture risk, and thermal comfort
implications in buildings. The computer
simulations allow us to explore possible
solutions for the building industry, including
optimizing the design of roof and wall
assemblies in different climate zones.
INTRODUCTION
In North America, the thermal performance
of building materials is most
commonly reported in terms of R-value,
and most insulation materials have label
R-values stamped on them (or at least
displayed in large print on the packaging).
R-value is a measure of the thermal resistance
of a material—it tells how effectively a
layer of material limits heat flow (for a given
thickness).
Many credit Everett Shuman with proposing
R-value as an easy-to-compare,
repeatable measure of insulation performance.
Shuman was the director of Penn
State’s Institute for Building Research
through the 1960s. He may not have been
the first to introduce the concept of thermal
resistance, but he actively promoted the
concept on the basis of its simplicity (Moe,
2014). Prior to the adoption of R-value, thermal
performance was expressed in terms
of conductance or the ability of materials
to conduct heat. Materials provide better
performance when they have lower thermal
conductance, but industry decision makers
felt that consumers would be confused by
the concept that “smaller is better.” When
thermal performance is expressed in terms
of R-value or thermal resistance, higher
numbers represent better performance.
The R-value went on to become the de
facto metric across North America, familiar
to both consumers and professionals.
It has helped many designers and
consumers make more energy-efficient
choices, but its importance in influencing
purchase decisions has also led to some
unscrupulous marketing claims. In the
aftermath of the 1970s energy crisis1 in the
United States, fraudulent R-value claims
became so widespread the United States
Congress passed a consumer-protection law
in response, the “R-Value Rule” (16 Code of
Federal Regulations [CFR] Part 460, “Trade
Regulation Rule Concerning the Labeling
and Advertising of Home Insulation”).
Measurement of Label R-Values
Under this rule, claims about residential
insulation must be based on specific
ASTM procedures. The most commonly
used are ASTM C177, Standard Test Method
for Steady-State Heat Flux Measurements
and Thermal Transmission Properties by
Means of the Guarded-Hot-Plate Apparatus,
and ASTM C518, Standard Test Method
for Steady-State Thermal Transmission
Properties by Means of the Heat Flow Meter
Apparatus. Tests can be quickly completed
using commercially available machines and
small, easy-to-handle samples—typically
between 12 x 12 in. (305 x 305 mm) and
24 x 24 in. (609 x 609 mm). Samples are
placed in direct contact with a pair of airimpermeable
hot and cold plates in the
machine. The rule requires R-value tests
to be conducted at a mean temperature of
24°C (75°F) and a temperature differential of
27.8°C (50°F). For reasons of technical ease,
this means insulation is usually tested with
the cold side at approximately 10°C (50°F),
and the warm side at around 38°C (100°F).2
In other words, the label R-value typically
only provides a metric of a material’s thermal
performance under one standard test
condition.
Industry Use of Label R-Values
Label R-values are used by designers,
contractors, code officials, etc. to:
1. V erify code compliance
2. Assess energy performance
3. Assess durability/moisture performance3
Some codes simply require that insulation
materials meet a specific label R-value;
however, codes are moving towards requiring
assemblies with specific effective R-values
that account for thermal bridging through
penetrating slabs, roof, and wall framing;
primary, secondary, and cladding-related
structural elements; and, in some cases,
even through fasteners. Label R-values are
used in all code-compliance applications,
but this does not accurately reflect in-service
performance.
Label R-values might provide a good
starting point for assessing energy performance
and durability/moisture performance;
however, as this paper illustrates,
The Effects of Temperature on
Insulation Performance: Considerations
for Optimizing Wall and Roof Designs
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they may not result in accurate predictions
of performance. Thermal bridging is only
one factor that influences in-service performance
of building assemblies. Aging,
thermal mass, moisture impacts, and
temperature dependence are but some of
the other factors that explain why label
R-values do not adequately reflect in-service
performance of building assemblies and
materials. Where appropriate, aging or longterm
thermal resistance (LTTR) can be
accounted for using methods described
in ASTM C1303 and CAN/ULC S770-09.
Codes and practices are established to
prevent insulation materials from accumulating
moisture at levels that have a
significant impact on thermal
performance. Researchers at
Oak Ridge National Lab evaluated
the benefit of thermal
mass across a range of different
climates and demonstrated
opportunity for energy
savings (Kosny et al., 2001).
This paper focuses on the
role of temperature dependence—
that is, the change
in an insulating material’s
apparent thermal resistance
(or conductivity) with change
in temperature (i.e., the mean
temperature, which is defined
as the average of the temperatures
on hot and cold
sides of the layer of insulation
material).
The potential issues are demonstrated
through comparisons between predicted
performance and field-measured performance
of roof and wall assemblies.
Predicted Vs. Measured Field
Performance of Low-Slope Roofs
A recent study of conventional
roof assemblies in
the Lower Mainland of British
Columbia, a Zone 4 climate,
assessed the in-service thermal
performance of different
assemblies installed on the
same building (Rickets et al.,
2014). For comparison, two
different insulation arrangements—
polyisocyanurate
(PIC) only, and stone wool
(SW) only—and three different
roof membrane colors
(white, gray, and black) were
investigated, for a total of six
different roof assemblies as
shown in Figure 1. The two
insulation combinations were
designed to have similar label
R-values (R-21.0 and R-21.9
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Figure 1 – PIC-only roof assembly (left) and stone wool only roof assembly (right).
Figure 2 – Photo of test roof area showing three different roof membrane colors: black, white,
and gray.
Figure 3 – Chart comparing theoretical calculated heat flux and measured heat flux through
the average of the PIC and SW roof assemblies in the study for the year 2014.
for the PIC and SW arrangements respectively)
to allow for direct comparison of their
in-service performance. An image of the test
roof area is provided in Figure 2 (Finch et
al., 2014).
To date, this field study has been running
for approximately three
years, with hourly monitoring
of performance parameters,
including heat flux, temperatures,
and relative humidity
(RH) levels within the assemblies.
Figure 3 and Figure 4
show the theoretical heat flux
through the roof assemblies
calculated using ambient air
temperature, interior temperature,
and the label R-values
as compared to the measured
heat flux.
Figure 3 and Figure 4
clearly indicate that theoretically
calculated heat flux
through the roof assemblies
is substantially different from
that measured in-service. This
difference is a clear example
of how label R-values
do not account for all
aspects of heat flow
through an assembly—
even at locations
where there are
no thermal bridges or
other discontinuities
in the insulation (i.e.,
clear wall locations).
Incorrect accounting
of assembly thermal
performance in design
calculations has realworld
implications for
building energy consumption,
thermal
comfort, and moisture
risk. Energy modelling
has shown that the
heating and cooling
energy consumption
for a commercial retail
building can be underpredicted
by up to 15%
when not accounting
for temperaturedependent
thermal
conductivities and
roof color (Finch et al.,
2014).
Predicted Vs. Measured Field Performance
of Exterior-Insulated Wall Assemblies
Another recent study assessed the thermal
and moisture performance of exteriorinsulated
wall assemblies on the northand
south-facing orientations of a test hut
in Waterloo, Ontario, a Zone 5/6 climate
(Straube, 2015). On each orientation, four
base wall assemblies (each 4 x 8 ft.) were
constructed using ½-in. gypsum wallboard
(GWB) on a 2 x 6 wood frame with fiberglass
batt insulation (label R-value of R-22),
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Figure 5 – Datum test wall assembly.
Figure 4 – Chart comparing theoretical calculated heat flux and measured heat flux through
the average of the black, gray, and white roof assemblies in the study for the year 2014.
7/16-in. OSB sheathing, a spun-bonded polyolefin
water-resistive barrier (WRB), a ¾-in.
drained and ventilated air space, and clad
with fiber cement clapboard siding. North
and south datum walls were designated
and completed without any exterior insulation.
A 6-mil polyethylene vapor retarder
was installed in accordance with Canadian
Building Code requirements, on the inside
of the stud frame, as shown in Figure
5. The remaining six walls (three north
and three south) were completed without
interior vapor retarders, but with exterior
insulation installed between the WRB and
the air space. Three types of exterior insulation
were investigated (three in stone wool,
2.5 in. extruded polystyrene [XPS], and two
in PIC). In each case, the thickness of the
exterior insulation was specified to achieve
a label R-value of R-12. Figure 6 shows
the exterior-insulated and datum test wall
assemblies prior to installation of the fiber
cement clapboard siding.
The test wall assemblies were monitored
for more than two years. Temperature, wood
moisture content, and RH were measured
at key points. The monitoring facilitated an
assessment of the moisture sensitivity of
the different systems under normal operating
conditions, as well as their resilience
when subjected to simulated rain leaks (via
injection of water at the sheathing layer) or
imposed air leakage (via a controlled flow
rate from the interior).
In cold climates, continuous exterior
insulation may be applied over structural
sheathing (e.g., OSB) to increase sheathing
temperatures, reducing the potential
for air leakage condensation and moisture
accumulation in the sheathing. Figure 7
plots the temperature measured at the
indoor side of the OSB sheathing (i.e., the
condensing plane) of the four north-facing
test walls over the first 10 days of 2014. As
expected, the sheathing temperatures track
the outdoor temperature, and the datum
wall (without exterior insulation) exhibits
the lowest temperatures. The other three
test walls exhibit higher sheathing
temperatures, owing to the
exterior insulation.
Four snapshots (indicated by
the dashed rectangular regions)
were identified for further analysis.
Table 1 summarizes the
calculated sheathing surface
temperatures (based on label
R-value) and compares these to
the measured temperatures. It
is reasonable to expect small
differences between the calculated
and measured sheathing
temperatures for the datum wall
because there is little insulation
outside of the OSB, so changes
in insulation or sheathing
R-value have little impact on the
predicted surface temperature.
However, the other three wall
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Figure 6 – Exterior-insulated (three on left) and datum (one at middle) test wall assemblies before siding.
Figure 7 – Temperature measured at inside of OSB sheathing over first 10 days of 2014.
assemblies have roughly one-third of the
total insulation on the exterior of the OSB
sheathing; and for these assemblies, there
is more significant difference between the
calculated (based on label R-values) and
measured temperatures.
Better R-Value Measurement and
Documentation
The predicted durability and energy performance
of insulations might be improved
by moving from a single-label R-value
(determined at mean temperature 24°C,
or 75°F) to a table of R-values determined
over a range of mean temperatures. The
National Roofing Contractors Association
(NRCA) recommends the use of two R-values
for PIC roof insulation: R-5/in. for heating
conditions and R-5.6/in. for cooling
conditions (Graham 2015). However, even
further breakdown (i.e., R-values at more
mean temperatures) may be justified. ASTM
C1058, Standard Practice for Selecting
Temperatures for Evaluating and Reporting
Thermal Properties of Thermal Insulation,
suggests six mean temperatures for measuring
and documenting the thermal performance
of insulation materials intended
for building enclosure applications. The
suggested mean temperatures and associated
hot- and cold-side temperatures are
summarized in Table 2.4 In all cases, the
temperature difference is 50°F, or approximately
28°C. Table 3 presents measured
R-value/in. for the roof and wall insulation
materials employed in the two field studies.
Here, PIR refers to polyisocyanurate wall
insulation with reflective (foil) facers.
The standard temperature measurements
confirm that all of the tested insulation
materials exhibit some temperature
dependency. Where the R-value exhibits
a near-linear temperature dependency, it
should be possible to use the data in Table 3
to predict the material R-value over the full
range of temperatures that buildings typically
experience. However, in those cases
where the temperature dependence does not
exhibit a near straight-line relationship, it is
necessary to conduct further material testing
and analysis.
The authors have developed a measurement
and analysis method5 to produce
temperature-dependent R-value curves that
can be employed to predict the thermal performance
of any insulation material, under
any temperature conditions.6 The method
uses regression to determine a convergent
R-value curve from numerous measurements
made while the temperature difference
decreases towards zero.
Figure 8 presents the temperaturedependent
R-value curves for the three
wall exterior insulation materials and two
roof insulation materials used in the field
studies.
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Datum 3-In. SW 2.5-In. XPS 2-In. PIC
Snapshot (day) 10 9 5 3 3 3 3
Interior T (°F) 68 68 68 68 68 68 68
Exterior T (°F) 35.6 11.3 25.7 -9.4 -9.4 -9.4 -9.4
Delta T (°F) 32.4 56.7 42.3 77.4 77.4 77.4 77.4
R-value In (ft2·°F·hr/Btu) 23.2 23.2 23.2 23.2 23.2 23.2 23.2
R-value Out (ft2·°F·hr/Btu) 2.1 2.1 2.1 2.1 14.1 14.6 15.1
R-value Total (ft2·°F·hr/Btu) 25.3 25.3 25.3 25.3 37.3 37.8 38.3
Ratio (-) 0.08 0.08 0.08 0.08 0.38 0.39 0.39
Calculated OSB T (°F) 38.3 16.1 29.3 -2.9 19.9 20.6 21.2
Measured OSB T (°F) 37.8 16.0 29.3 -2.6 23.4 21.6 16.7
Difference (°F) -0.6 -0.1 0.0 0.3 3.4 1.0 -4.5
Table 1 – Comparison between predicted vs. measured sheathing temperature (using label R-values).
Mean Temperature “Hot Side” “Cold Side”
(°F) (°C) (°F) (°C) (°F) (°C)
25 -4 50 10 0 -18
40 4 65 18 15 -10
50 10 75 24 25 -4
75 24 100 38 50 10
100 38 125 52 75 24
110 43 135 57 85 29
Table 2 – ASTM C1058 suggested mean temperatures for testing building envelope
insulations.
Mean Temperature Roof Insulation Exterior Insulation for Walls
(°F) SW PIC SW XPS PIR
25 4.2 4.6 4.7 5.5 4.9
40 4.1 5.1 4.5 5.3 5.2
75 3.8 5.3 4.2 4.9 5.4
110 3.7 4.9 3.9 4.6 4.9
Table 3 – Measured R-value/in. at standard mean temperatures.
Comparison of “Improved” Predictions
Vs. Measurements for Roof
Using the same roof assemblies as previously
discussed, it is possible to calculate
an improved theoretical estimate of the
heat flow through the roof assembly. This
improved calculation accounts for actual inservice
roof temperatures that are primarily
impacted by roof membrane color, but
are also influenced by the insulation type
and arrangement. The calculation is also
improved by accounting for temperaturedependent
thermal conductivity for both the
PIC and the SW insulations. The nonlinear
conductivity of the PIC was measured
using the converging delta
T method described above. The
result of this improved theoretical
calculation is compared to
the measured results and the
original theoretical calculation
in Figure 9 and Figure 10 for
the PIC roofs and the gray roofs,
respectively.
Figure 9 and Figure 10 clearly
indicate that when actual inservice
roof temperatures and
temperature-dependent conductivity
effects are accounted for,
theoretical calculations more
closely match measured results.
That said, room for improvement
exists, and this may be due, in
part, to movement of moisture
within the roof assemblies and
differences in insulation thermal
mass.
Comparison of “Improved” Predicted
Vs. Measured Performance of Wall
Assemblies
The temperature-dependent R-value
curves were used to improve the surface
temperature predictions made for the OSB
sheathings in the wall field study.
Table 4 presents a comparison of the
improved predictions and the measured
surface temperatures for the Day 3 snapshot.
Use of the temperature-dependent
R-values results in much better agreement
between predicted and measured surface
temperatures.
CONCLUSIONS AND
RECOMMENDATIONS
In North America, building insulation
materials are typically tested and labeled
in accordance with the “R-Value Rule”
(16 CFR Part 460, “Trade Regulation Rule
Concerning the Labeling and Advertising of
Home Insulation”). Thermal performance,
specifically R-value, is assessed under a
single set of conditions: at a mean temperature
of 74°F (24°C) and under a temperature
difference of approximately 50°F (28°C).
Laboratory measurements made at other
standard mean temperatures (suggested by
ASTM C1058) indicate that, for most insulation
materials, R-value is temperaturedependent.
Many insulation materials
exhibit nearly linear temperature dependency,
while others exhibit unique temperature-
dependent R-value curves. The latter
can be characterized and quantified using
special measurement techniques.
Field-monitoring studies on roof and
exterior insulated wall assemblies suggest
that more complex thermal and durability
considerations may not be adequately
represented using conventional-label R values.
The use of temperature-dependent
R-values has been demonstrated to improve
predictions of the energy performance and
moisture durability of building enclosure
assemblies.
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Figure 8 – Temperature-dependent R-value curves for roof and wall insulations
studied.
Figure 9 – Chart comparing calculated heat flux using the improved method with that
calculated using the original method and the measured heat flux through the average of the
PIC roof assemblies in the study for the year 2014.
REFERENCES
G. Finch, M. Dell, B. Hanam,
and L. Ricketts. (2014)
“Conventional Roofing
Assemblies: Measuring the
Thermal Benefits of Light
to Dark Roof Membranes
and Alternate Insulation
Strategies.” Proceedings of
the 28th RCI International
Convention and Trade Show.
M. Graham. “Testing R-Values:
Polyisocyanurate’s R-Values
Are Found to Be Less
Than Their LTTR Values.”
Professional Roofing, March
2015.
J. Kosny, T. Petrie, D. Gawin, P.
Childs, A. Desjarlais, and J.
Christian. “Thermal Mass-
Energy Savings Potential
in Residential Buildings.”
Retrieved Oct. 28, 2015.
K. Moe. (2014). Insulating Modernism:
Isolated and Non-Isolated Thermodynamics
in Architecture. Birkhäuser.
L. Ricketts, G. Finch, M. Dell. (2014)
Study of Conventional Roof Performance.
Vancouver, BC: RDH
Building Engineering Ltd.
J. Straube. (2015), “Field Hygrothermal
Performance of Highly Insulated
Wood-Framed Wall Systems.”
Research report for NRCan, Building
Engineering Group, University of
Waterloo, Waterloo, ON, Canada.
Footnotes
1. For more information about the
1970s energy crisis, its causes, and
effects, the reader is directed to
en.wikipedia.org/wiki/1970s_energy_
crisis.
2. The actual language of the rule permits
test temperature differentials
of 27.8ºC ± 5.6ºC (50ºF ± 10ºF) for
cold-side temperatures of 7.2º to
12.7ºC (45º to 55ºF) and hot-side
temperatures of 35º to 40ºC (95º to
105ºF).
3. Designers use the label R-values of
insulation installed between framing
members (i.e., in the stud spaces)
and as continuous insulation on
the outside of framing (e.g., exterior
insulation) to estimate condensing
plane temperatures and evaluate
the potential for moisture accumulation
(due to air leakage and vapor
diffusion) and problems in building
enclosure assemblies.
4. Some materials exhibit very linear
temperature dependence and can
be characterized using only two or
three set points. Other materials
exhibit much more dramatic temperature
dependence (as illustrated
in this paper) and may require testing
at more than the six set points
identified in ASTM C1058.
5. This measurement and analysis method
is the subject of a draft paper proposed
for ASTM C16’s Symposium on
Advances in Hygrothermal Performance
of Building Envelopes: Materials,
Systems and Simulations, October
2016.
6. The method specifically addresses
the insulation material. It does not
address the assembly with all thermal
bridges due to framing, fasteners,
etc. However, the method does
produce data that can be used to
evaluate the performance of insulation
layers in hybrid-insulated
assemblies (e.g., walls with some
insulation between the framing
members and more installed as continuous
exterior insulation).
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Figure 10 – Chart comparing calculated heat flux using the improved method with that
calculated using the original method and the measured heat flux through the average of
the gray roof assemblies in the study for the year 2014.
3 In. 2 In.
SW 2.5 In. XPS PIC
Snapshot (day) 3 3 3
Interior T (°F) 68 68 68
Exterior T (°F) -9.4 -9.4 -9.4
Delta T (°F) 77.4 77.4 77.4
R-value In (ft2·°F·hr/Btu) 23.2 23.2 23.2
R-value Out (ft2·°F·hr/Btu) 17.0 15.5 11.3
R-value Total (ft2·°F·hr/Btu) 40.2 38.7 34.5
Ratio (-) 0.42 0.40 0.33
Calculated OSB T (°F) 23.4 21.7 16.0
Measured OSB T (°F) 23.4 21.6 16.7
Difference (°F) 0.0 -0.1 0.7
Table 4 – Comparison between predicted vs. measured sheathing temperature
(using R-value curves).