1、Designation: C755 10 (Reapproved 2015)1Standard Practice forSelection of Water Vapor Retarders for Thermal Insulation1This standard is issued under the fixed designation C755; the number immediately following the designation indicates the year oforiginal adoption or, in the case of revision, the yea
2、r of last revision. A number in parentheses indicates the year of last reapproval. Asuperscript epsilon () indicates an editorial change since the last revision or reapproval.1NOTEEditorially corrected Table 2 in January 2018.1. Scope1.1 This practice outlines factors to be considered, describesdesi
3、gn principles and procedures for water vapor retarderselection, and defines water vapor transmission values appro-priate for established criteria. It is intended for the guidance ofdesign engineers in preparing vapor retarder application speci-fications for control of water vapor flow through therma
4、linsulation. It covers commercial and residential building con-struction and industrial applications in the service temperaturerange from 40 to +150F (40 to +66C). Emphasis is placedon the control of moisture penetration by choice of the mostsuitable components of the system.1.2 The values stated in
5、 inch-pound units are to be regardedas standard. The values given in parentheses are mathematicalconversions to SI units that are provided for information onlyand are not considered standard.1.3 This standard does not purport to address all of thesafety concerns, if any, associated with its use. It
6、is theresponsibility of the user of this standard to establish appro-priate safety, health, and environmental practices and deter-mine the applicability of regulatory limitations prior to use.1.4 This international standard was developed in accor-dance with internationally recognized principles on s
7、tandard-ization established in the Decision on Principles for theDevelopment of International Standards, Guides and Recom-mendations issued by the World Trade Organization TechnicalBarriers to Trade (TBT) Committee.2. Referenced Documents2.1 ASTM Standards:2C168 Terminology Relating to Thermal Insul
8、ationC647 Guide to Properties and Tests of Mastics and CoatingFinishes for Thermal InsulationC921 Practice for Determining the Properties of JacketingMaterials for Thermal InsulationC1136 Specification for Flexible, Low Permeance VaporRetarders for Thermal InsulationE96/E96M Test Methods for Water V
9、apor Transmission ofMaterials3. Terminology3.1 For definitions of terms used in this practice, refer toTerminology C168.4. Significance and Use4.1 Experience has shown that uncontrolled water entry intothermal insulation is the most serious factor causing impairedperformance. Water entry into an ins
10、ulation system may bethrough diffusion of water vapor, air leakage carrying watervapor, and leakage of surface water. Application specificationsfor insulation systems that operate below ambient dew-pointtemperatures should include an adequate vapor retarder sys-tem. This may be separate and distinct
11、 from the insulationsystem or may be an integral part of it. For selection ofadequate retarder systems to control vapor diffusion, it isnecessary to establish acceptable practices and standards.4.2 Vapor Retarder FunctionWater entry into an insula-tion system may be through diffusion of water vapor,
12、 airleakage carrying water vapor, and leakage of surface water.The primary function of a vapor retarder is to control move-ment of diffusing water vapor into or through a permeableinsulation system. The vapor retarder system alone is seldomintended to prevent either entry of surface water or air lea
13、kage,but it may be considered as a second line of defense.4.3 Vapor Retarder PerformanceDesign choice of retard-ers will be affected by thickness of retarder materials, substrateto which applied, the number of joints, available length andwidth of sheet materials, useful life of the system, andinspec
14、tion procedures. Each of these factors will have an effecton the retarder system performance and each must be consid-ered and evaluated by the designer.4.3.1 Although this practice properly places major emphasison selecting the best vapor retarders, it must be recognized that1This practice is under
15、the jurisdiction of ASTM Committee C16 on ThermalInsulation and is the direct responsibility of Subcommittee C16.33 on InsulationFinishes and Moisture.Current edition approved Sept. 1, 2015. Published October 2015. Originallyapproved in 1973. Last previous edition approved in 2010 as C755 101. DOI:1
16、0.1520/C0755-10R15E01.2For referenced ASTM standards, visit the ASTM website, www.astm.org, orcontact ASTM Customer Service at serviceastm.org. For Annual Book of ASTMStandards volume information, refer to the standards Document Summary page onthe ASTM website.Copyright ASTM International, 100 Barr
17、Harbor Drive, PO Box C700, West Conshohocken, PA 19428-2959. United StatesThis international standard was developed in accordance with internationally recognized principles on standardization established in the Decision on Principles for theDevelopment of International Standards, Guides and Recommen
18、dations issued by the World Trade Organization Technical Barriers to Trade (TBT) Committee.1faulty installation techniques can impair vapor retarder perfor-mance. The effectiveness of installation or application tech-niques in obtaining design water vapor transmission (WVT)performance must be consid
19、ered in the selection of retardermaterials.4.3.2 As an example of the evaluation required, it may beimpractical to specify a lower “as installed” value, becausedifficulties of field application often will preclude “as installed”attainment of the inherent WVT values of the vapor retardermaterials use
20、d. The designer could approach this requirementby selecting a membrane retarder material that has a lowerpermeance manufactured in 5-ft (1.5-m) width or a sheetmaterial 20 ft (6.1 m) wide having a higher permeance. Thesealternatives may be approximately equivalent on an installedbasis since the wide
21、r material has fewer seams and joints.4.3.3 For another example, when selecting mastic or coatingretarder materials, the choice of a product having a permeancevalue somewhat higher than the lowest obtainable might bejustified on the basis of its easier application techniques, thusensuring “as instal
22、led” system attainment of the specifiedpermeance. The permeance of the substrate and its effects onthe application of the retarder material must also be consideredin this case.5. Factors to Be Considered in Choosing Water VaporRetarders5.1 Water Vapor Pressure Difference is the difference in thepres
23、sure exerted on each side of an insulation system orinsulated structure that is due to the temperature and moisturecontent of the air on each side of the insulated system orstructure. This pressure difference determines the direction andmagnitude of the driving force for the diffusion of the waterva
24、por through the insulated system or structure. In general, fora given permeable structure, the greater the water vaporpressure difference, the greater the rate of diffusion. Watervapor pressure differences for specific conditions can becalculated by numerical methods or from psychrometric tablesshow
25、ing thermodynamic properties of water at saturation.5.1.1 Fig. 1 shows the variation of dew-point temperaturewith water vapor pressure.5.1.2 Fig. 2 illustrates the magnitude of water vapor pres-sure differences for four ambient air conditions and cold-sideoperating temperatures between +40 and 40F (
26、+4.4and 40C).5.1.3 At a stated temperature the water vapor pressure isproportional to relative humidity but at a stated relativehumidity the vapor pressure is not proportional to temperature.5.1.4 Outdoor design conditions vary greatly dependingupon geographic location and season and can have a subs
27、tantialimpact on system design requirements. It is therefore necessaryto calculate the actual conditions rather than rely on estimates.As an example, consider the cold-storage application shown inTable 1. The water vapor pressure difference for the facilitylocated in Biloxi, MS is 0.96 in. Hg (3.25
28、kPa) as compared toa 0.001 in. Hg (3 Pa) pressure difference if the facility wasFIG. 1 Dew Point (Dp) Relation to Water Vapor PressureC755 10 (2015)12located in International Falls, MN. In the United States thedesign dew point temperature seldom exceeds 75F (24C)(1).35.1.5 The expected vapor pressur
29、e difference is a veryimportant factor that must be based on realistic design data (notestimated) to determine vapor retarder requirements.5.2 Service ConditionsThe direction and magnitude ofwater vapor flow are established by the range of ambientatmospheric and design service conditions. These cond
30、itionsnormally will cause vapor flow to be variable in magnitude,and either unidirectional or reversible.5.2.1 Unidirectional flow exists where the water vaporpressure is constantly higher on one side of the system. Withbuildings operated for cold storage or frozen food storage, thesummer outdoor ai
31、r conditions will usually determine vaporretarder requirements, with retarder placement on the outdoor(warmer) side of the insulation. In heating only buildings forhuman occupancy, the winter outdoor air conditions wouldrequire retarder placement on the indoor (warmer) side of theinsulation. In cool
32、ing only buildings for human occupancy(that is, tropic and subtropic locations), the summer outside airconditions would require retarder placement on the outdoor(warmer) side.5.2.2 Reversible flow can occur where the vapor pressuremay be higher on either side of the system, changing usuallybecause o
33、f seasonal variations. The inside temperature andvapor pressure of a refrigerated structure may be below theoutside temperature and vapor pressure at times, and above theoutside temperature and vapor pressure at other times. Coolerrooms with operating temperatures in the range from 35 to45F (2 to 7C
34、) at 90 % relative humidity and located innorthern latitudes will experience an outward vapor flow inwinter and an inward flow in summer. This reversing vaporflow requires special design consideration.5.3 Properties of Insulating Materials with Respect toMoistureInsulating materials permeable to wat
35、er vapor willallow moisture to diffuse through at a rate defined by itspermeance and exposure. The rate of movement is inverselyproportional to the vapor flow resistance in the vapor path.Insulation having low permeance and vapor-tight joints mayact as a vapor retarder.5.3.1 If condensation of water
36、 occurs within the insulationits thermal properties can be significantly affected where3The boldface numbers in parentheses refer to the list of references at the end ofthis practice.FIG. 2 Magnitude of Water Vapor Pressure Difference for Selected Conditions (Derived from Fig. 1)TABLE 1 Cold Storage
37、 ExampleLocationSeasonBiloxi, MSSummerInternationalFalls, MNWinterOutside Design ConditionsTemperature , F (C) 93 (34) -35 (-37)Relative Humidity, % 63 67Dew Point Temperature, F (C) 78.4 (26) -42 (-41)Water Vapor Pressurein. Hg (kPa).9795 (3.32) .003 (0.01)Inside Design ConditionsTemperature, F (C)
38、 -10 -10Relative Humidity, % 90 90Water Vapor Pressure in.Hg (kPa).02 .02System Design ConditionsWater Vapor PressureDifference in. Hg (kPa)0.9795 0.001 (0.067)Direction of Diffusion From outside From insideC755 10 (2015)13wetted. Liquid water resulting from condensation has a thermalconductivity so
39、me fifteen times greater than that of a typicallow-temperature insulation. Ice conductivity is nearly fourtimes that of water. Condensation reduces the thermal effec-tiveness of the insulation in the zone where it occurs, but if thezone is thin and perpendicular to the heat flow path, thereduction i
40、s not extreme. Water or ice in insulation joints thatare parallel to the heat flow path provide higher conductancepaths with consequent increased heat flow. Generally, hygro-scopic moisture in insulation can be disregarded.5.3.2 Thermal insulation materials range in permeabilityfrom essentially 0 pe
41、rm-in. (0 g/Pa-s-m) to greater than 100perm-in. (1.45 10-7g/Pa-s-m) Because insulation is suppliedin pieces of various size and thickness, vapor diffusion throughjoints must be considered in the permeance of the materials asapplied. The effect of temperature changes on dimensions andother physical c
42、haracteristics of all materials of the assemblymust be considered as it relates to vapor flow into the joints andinto the insulation.5.4 Properties of Boundary or Finish Materials at the ColdSide of InsulationWhen a vapor pressure gradient exists thelower vapor pressure value usually will be on the
43、lowertemperature side of the system, but not always. (There are fewexceptions, but these must be considered as special cases.) Thefinish on the cold side of the insulation-enclosing refrigeratedspaces should have high permeance relative to that of the warmside construction, so that water vapor penet
44、rating the systemcan flow through the insulation system without condensing.This moisture should be free to move to the refrigeratingsurfaces where it is removed as condensate. When the cold sidepermeance is zero, as with insulated cold piping, water vaporthat enters the insulation system usually wil
45、l condense withinthe assembly and remain as an accumulation of water, frost, orice.5.5 Effect of Air LeakageWater vapor can be transportedreadily as a component of air movement into and out of anair-permeable insulation system. This fact must be taken intoaccount in the design and construction of an
46、y system in whichmoisture control is a requirement. The quantity of water vaporthat can be transported by air leakage through cracks orair-permeable construction can easily be several times greaterthan that which occurs by vapor diffusion alone.5.5.1 Air movement occurs as a result of air pressuredi
47、fferences. In insulated structures these may be due to windaction, buoyancy forces due to temperature difference betweeninterconnected spaces, volume changes due to fluctuations intemperature and barometric pressure, and the operation ofmechanical air supply or exhaust systems. Air leakage occursthr
48、ough openings or through air-permeable construction acrosswhich the air pressure differences occur. Water vapor in airflowing from a warm humidified region to a colder zone in aninsulation system will condense in the same way as watervapor moving only by diffusion.5.5.2 If there is no opportunity fo
49、r dilution with air at lowervapor pressure along the flow path, there will be no vaporpressure gradient. Condensation may occur when the air streampasses through a region in the insulation system where thetemperature is equal to or lower than the dew point of the warmregion of origin. The airflow may be from a warm region onone side of the system through to a cold region on the otherside, or it may consist of recirculation between interconnectedair spaces at different temperatures forming only a part of thesystem. Sufficient airflow rate could virtu
