ASTM C522-2003(2009) Standard Test Method for Airflow Resistance of Acoustical Materials.pdf
《ASTM C522-2003(2009) Standard Test Method for Airflow Resistance of Acoustical Materials.pdf》由会员分享,可在线阅读,更多相关《ASTM C522-2003(2009) Standard Test Method for Airflow Resistance of Acoustical Materials.pdf(5页珍藏版)》请在麦多课文档分享上搜索。
1、Designation: C522 03 (Reapproved 2009)Standard Test Method forAirflow Resistance of Acoustical Materials1This standard is issued under the fixed designation C522; the number immediately following the designation indicates the year oforiginal adoption or, in the case of revision, the year of last rev
2、ision. A number in parentheses indicates the year of last reapproval. Asuperscript epsilon () indicates an editorial change since the last revision or reapproval.1. Scope1.1 This test method covers the measurement of airflowresistance and the related measurements of specific airflowresistance and ai
3、rflow resistivity of porous materials that can beused for the absorption and attenuation of sound. Materialscover a range from thick boards or blankets to thin mats,fabrics, papers, and screens. When the material is anisotropic,provision is made for measurements along different axes of thespecimen.1
4、.2 This test method is designed for the measurement ofvalues of specific airflow resistance ranging from 100 to10 000 mks rayls (Pas/m) with linear airflow velocities rang-ing from 0.5 to 50 mm/s and pressure differences across thespecimen ranging from 0.1 to 250 Pa. The upper limit of thisrange of
5、linear airflow velocities is a point at which the airflowthrough most porous materials is in partial or completetransition from laminar to turbulent flow.1.3 A procedure for accrediting a laboratory for the pur-poses of this test method is given in Annex A1.1.4 The values stated in SI units are to b
6、e regarded asstandard. No other units of measurement are included in thisstandard.1.5 This standard does not purport to address all of thesafety concerns, if any, associated with its use. It is theresponsibility of the user of this standard to establish appro-priate safety and health practices and d
7、etermine the applica-bility of regulatory limitations prior to use.2. Referenced Documents2.1 ASTM Standards:2E384 Test Method for Microindentation Hardness of Mate-rialsC634 Terminology Relating to Building and EnvironmentalAcousticsE691 Practice for Conducting an Interlaboratory Study toDetermine
8、the Precision of a Test Method3. Terminology3.1 Definitions: The definitions used in this test method arecontained in Terminology C634.3.2 Definitions of Terms Specific to This Standard: Thefollowing items have been modified to exclude alternatingflow.3.2.1 airflow resistance, R; mks acoustic ohm(Pa
9、s/m3)the quotient of the air pressure difference across aspecimen divided by the volume velocity of airflow through thespecimen.3.2.2 airflow resistivity, r0; mks rayl/m (Pas/m2) of ahomogeneous material, the quotient of its specific airflowresistance divided by its thickness.3.2.3 lateral airflow r
10、esistivity of an anisotropic homoge-neous material, the airflow resistivity when the direction ofairflow is parallel to the face of the material from which the testspecimen is taken.3.2.4 specific airflow resistance, r; mks rayl (Pas/m)theproduct of the airflow resistance of a specimen and its area.
11、This is equivalent to the air pressure difference across thespecimen divided by the linear velocity of airflow measuredoutside the specimen.3.2.5 transverse airflow resistivity of an anisotropic ho-mogeneous material, the airflow resistivity when the directionof airflow is perpendicular to the face
12、of the material fromwhich the test specimen is taken.3.3 Application of Terms:3.3.1 The term airflow resistance can be applied to speci-mens of any kind.3.3.2 The term specific airflow resistance has meaning onlywhen applied to a specimen of uniform thickness that ishomogeneous in directions paralle
13、l to its surface but notnecessarily homogeneous in the direction of airflow perpen-dicular to its surface.3.3.3 The term airflow resistivity has meaning only whenapplied to a specimen that is homogeneous in directionsparallel to a and perpendicular to its surface but not necessarilyisotropic.3.4 Sym
14、bols:3.4.1 P = air pressure difference across test specimen, Pa.1This test method is under the jurisdiction ofASTM Committee E33 on Buildingand Environmental Acoustics and is the direct responsibility of SubcommitteeE33.01 on Sound Absorption.Current edition approved Oct. 1, 2009. Published February
15、 2010. Originallyapproved in 1963. Last previous edition approved in 2003 as C522 03. DOI:10.1520/C0522-03R09.2For 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 st
16、andards Document Summary page onthe ASTM website.1Copyright ASTM International, 100 Barr Harbor Drive, PO Box C700, West Conshohocken, PA 19428-2959, United States.3.4.2 U = volume velocity of airflow through the specimen,m3/s.3.4.3 u = U/S = linear velocity of airflow outside thespecimen, m/s.3.4.4
17、 S = area of specimen, m.23.4.5 T = thickness of specimen, m.4. Summary of Test Method4.1 This test method describes how to measure a steady flowof air through a test specimen, how to measure the air pressuredifference across the specimen, and how to measure thevolume velocity of airflow through the
18、 specimen. From themeasurements may be calculated the airflow resistance, R, thespecific airflow resistance, r, and the airflow resistivity, r0.5. Significance and Use5.1 The specific airflow resistance of an acoustical materialis one of the properties that determine its sound-absorptive andsound-tr
19、ansmitting properties. Measurement of specific airflowresistance is useful during product development, for qualitycontrol during manufacture, and for specification purposes.5.2 Valid measurements are made only in the region oflaminar airflow where, aside from random measurement errors,the airflow re
20、sistance (R = P/U) is constant. When the airflowis turbulent, the apparent airflow resistance increases with anincrease of volume velocity and the term “airflow resistance”does not apply.5.3 The specific airflow resistance measured by this testmethod may differ from the specific resistance measured
21、by theimpedance tube method in Test Method E384 for two reasons.In the presence of sound, the particle velocity inside a porousmaterial is alternating while in this test method, the velocity isconstant and in one direction only. Also, the particle velocityinside a porous material is not the same as
22、the linear velocitymeasured outside the specimen.6. Apparatus6.1 The apparatus, assembled as shown schematically inFig. 1, consists of the following components:6.1.1 Air Supply, a suction generator or positive air supplyarranged to draw or force air at a uniform rate through the testspecimen.NOTE 1I
23、t may be necessary to use a large surge tank or other meansto reduce pressure fluctuations.6.1.2 Flowmeter, to measure the volume velocity of airflowthrough the specimen. It is preferable to have two or moreflowmeters with overlapping ranges to enable different airflowvelocities to be measured to th
24、e same precision.6.1.3 Differential Pressure Measuring Device, for measur-ing the static pressure difference between the faces of thespecimen with respect to atmosphere.NOTE 2Aslant manometer or pressure transducer system with a rangefrom 0 to 250 Pa is usually satisfactory, but a second instrument
- 1.请仔细阅读文档,确保文档完整性,对于不预览、不比对内容而直接下载带来的问题本站不予受理。
- 2.下载的文档,不会出现我们的网址水印。
- 3、该文档所得收入(下载+内容+预览)归上传者、原创作者;如果您是本文档原作者,请点此认领!既往收益都归您。
下载文档到电脑,查找使用更方便
10000 积分 0人已下载
下载 | 加入VIP,交流精品资源 |
- 配套讲稿:
如PPT文件的首页显示word图标,表示该PPT已包含配套word讲稿。双击word图标可打开word文档。
- 特殊限制:
部分文档作品中含有的国旗、国徽等图片,仅作为作品整体效果示例展示,禁止商用。设计者仅对作品中独创性部分享有著作权。
- 关 键 词:
- ASTMC52220032009STANDARDTESTMETHODFORAIRFLOWRESISTANCEOFACOUSTICALMATERIALSPDF

链接地址:http://www.mydoc123.com/p-466922.html