ASTM E662-2014 red 4329 Standard Test Method for Specific Optical Density of Smoke Generated by Solid Materials《固体材料产生的烟雾比光密度的标准试验方法》.pdf
《ASTM E662-2014 red 4329 Standard Test Method for Specific Optical Density of Smoke Generated by Solid Materials《固体材料产生的烟雾比光密度的标准试验方法》.pdf》由会员分享,可在线阅读,更多相关《ASTM E662-2014 red 4329 Standard Test Method for Specific Optical Density of Smoke Generated by Solid Materials《固体材料产生的烟雾比光密度的标准试验方法》.pdf(30页珍藏版)》请在麦多课文档分享上搜索。
1、Designation: E662 13dE662 14 An American National StandardStandard Test Method forSpecific Optical Density of Smoke Generated by SolidMaterials1This standard is issued under the fixed designation E662; the number immediately following the designation indicates the year oforiginal adoption or, in the
2、 case of revision, the year 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.This standard has been approved for use by agencies of the U.S. Department of Defense.1. Scope Scop
3、e*1.1 This fire-test-response standard covers determination of the specific optical density of smoke generated by solid materialsand assemblies mounted in the vertical position in thicknesses up to and including 1 in. (25.4 mm).1.2 Measurement is made of the attenuation of a light beam by smoke (sus
4、pended solid or liquid particles) accumulating withina closed chamber due to nonflaming pyrolytic decomposition and flaming combustion.1.3 Results are expressed in terms of specific optical density which is derived from a geometrical factor and the measuredoptical density, a measurement characterist
5、ic of the concentration of smoke.1.4 This test method is intended for use in research and development and not as a basis for ratings for regulatory purposes.1.5 The values stated in inch-pound units are to be regarded as standard. The values given in parentheses are mathematicalconversions to SI uni
6、ts that are provided for information only and are not considered standard.1.6 This standard measures and describes the response of materials, products, or assemblies to heat and flame under controlledconditions, but does not by itself incorporate all factors required for fire hazard or fire risk ass
7、essment of the materials, productsor assemblies under actual fire conditions.1.7 This standard does not purport to address all of the safety concerns, if any, associated with its use. It is the responsibilityof the user of this standard to establish appropriate safety and health practices and determ
8、ine the applicability of regulatorylimitations prior to use.2. Referenced Documents2.1 ASTM Standards:2D2843 Test Method for Density of Smoke from the Burning or Decomposition of PlasticsE176 Terminology of Fire Standards3. Terminology3.1 DefinitionsFor definitions of terms found in this test method
9、 refer to Terminology E176.4. Summary of Test Method4.1 This test method employs an electrically heated radiant-energy source mounted within an insulated ceramic tube andpositioned so as to produce an irradiance level of 2.2 Btu/sft2 (2.5 W/cm2) averaged over the central 1.5-in. (38.1-mm) diameterar
10、ea of a vertically mounted specimen facing the radiant heater. The nominal 3 by 3-in. (76.2 by 76.2-mm) specimen is mountedwithin a holder which exposes an area measuring 2916 by 2916 in. (65.1 by 65.1 mm).The holder is able to accommodate specimensup to 1 in. (25.4 mm) thick. This exposure provides
11、 the nonflaming condition of the test.4.2 For the flaming condition, a six-tube burner is used to apply a row of equidistant flamelets across the lower edge of theexposed specimen area and into the specimen holder trough. This application of flame in addition to the specified irradiance levelfrom th
12、e heating element constitutes the flaming combustion exposure.1 This test method is under the jurisdiction ofASTM Committee E05 on Fire Standards and is the direct responsibility of Subcommittee E05.21 on Smoke and CombustionProducts.Current edition approved Aug. 1, 2013Aug. 1, 2014. Published Septe
13、mber 2013September 2014. Originally approved in 1979. Last previous edition approved in 2013 asE662 13c.E662 13d. DOI: 10.1520/E0662-13D.10.1520/E0662-14.2 For referencedASTM standards, visit theASTM website, www.astm.org, or contactASTM Customer Service at serviceastm.org. For Annual Book of ASTM S
14、tandardsvolume information, refer to the standards Document Summary page on the ASTM website.This document is not an ASTM standard and is intended only to provide the user of an ASTM standard an indication of what changes have been made to the previous version. Becauseit may not be technically possi
15、ble to adequately depict all changes accurately, ASTM recommends that users consult prior editions as appropriate. In all cases only the current versionof the standard as published by ASTM is to be considered the official document.*A Summary of Changes section appears at the end of this standardCopy
16、right ASTM International, 100 Barr Harbor Drive, PO Box C700, West Conshohocken, PA 19428-2959. United States14.3 The test specimens are exposed to the flaming and nonflaming conditions within a closed chamber. A photometric systemwith a vertical light path is used to measure the varying light trans
17、mission as smoke accumulates. The light transmittancemeasurements are used to calculate specific optical density of the smoke generated during the time period to reach the maximumvalue.35. Significance and Use5.1 This test method provides a means for determining the specific optical density of the s
18、moke generated by specimens ofmaterials and assemblies under the specified exposure conditions. Values determined by this test are specific to the specimen orassembly in the form and thickness tested and are not to be considered inherent fundamental properties of the material tested. Thus,it is like
19、ly that closely repeatable or reproducible experimental results are not to be expected from tests of a given material whenspecimen thickness, density, or other variables are involved.5.2 The photometric scale used to measure smoke by this test method is similar to the optical density scale for human
20、 vision.However, physiological aspects associated with vision are not measured by this test method. Correlation with measurements byother test methods has not been established.45.3 At the present time no basis is provided for predicting the density of smoke generated by the materials upon exposure t
21、oheat and flame under other fire conditions.5.4 The test method is of a complex nature and the data obtained are sensitive to variations which in other test methods mightbe considered to be insignificant (see Section 6). A precision statement based on the results of a roundrobin test by a prior draf
22、tversion of this test method is given in 14.15.5 In this procedure, the specimens are subjected to one or more specific sets of laboratory test conditions. If different testconditions are substituted or the end-use conditions are changed, it is not always possible by or from this test method to pred
23、ictchanges in the fire-test-response characteristics measured. Therefore, the results are valid only for the fire test exposure conditionsdescribed in this procedure.6. Limitations6.1 If during the test of one or more of the three replicate samples there occurs such unusual behavior as (1) the speci
24、men fallingout of the holder, (2) melted material overflowing the sample holder trough, (3) self-ignition in the pyrolysis mode, (4)extinguishment of the flame tiplets (even for a short period of time), or (5) a specimen being displaced from the zone of controlledirradiance, then an additional three
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