ASTM D4535-2008 Standard Test Methods for Measurement of Thermal Expansion of Rock Using Dilatometer《用膨胀计测量岩石的热膨胀的标准试验方法》.pdf
《ASTM D4535-2008 Standard Test Methods for Measurement of Thermal Expansion of Rock Using Dilatometer《用膨胀计测量岩石的热膨胀的标准试验方法》.pdf》由会员分享,可在线阅读,更多相关《ASTM D4535-2008 Standard Test Methods for Measurement of Thermal Expansion of Rock Using Dilatometer《用膨胀计测量岩石的热膨胀的标准试验方法》.pdf(6页珍藏版)》请在麦多课文档分享上搜索。
1、Designation: D 4535 08Standard Test Methods forMeasurement of Thermal Expansion of Rock UsingDilatometer1This standard is issued under the fixed designation D 4535; the number immediately following the designation indicates the year oforiginal adoption or, in the case of revision, the year of last r
2、evision. A number in parentheses indicates the year of last reapproval. Asuperscript epsilon () indicates an editorial change since the last revision or reapproval.1. Scope*1.1 These test methods cover the laboratory measurement ofthe linear (one-dimensional) thermal expansion of rocks usinga dilato
3、meter.1.2 These test methods are applicable between temperaturesof 25C to 300C. Both bench top and confined measurementtechniques are presented. Rocks of varying moisture contentcan be tested.1.3 For satisfactory results in conformance with these testmethods, the principles governing the size, const
4、ruction, anduse of the apparatus described in these methods should befollowed. If the results are to be reported as having beenobtained by this method, then all pertinent requirementsprescribed in this method shall be met.1.4 These test methods do not establish details of construc-tion and procedure
5、 to cover all test situations that might offerdifficulties to a person without technical knowledge concerningthe theory of heat flow, temperature measurement, and generaltesting practices. Standardization of these test methods doesnot reduce the need for such technical knowledge. It isrecognized als
6、o that it would be unwise, because of thestandardization of this method, to resist in any way the furtherdevelopment of improved or new methods or procedures byresearch workers.1.5 The values stated in SI units are to be regarded as thestandard. The values given in parentheses are mathematicalconver
7、sions to inch-pound units that are provided for informa-tion only and are not considered standard.1.6 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
8、 practices and determine the applica-bility of regulatory limitations prior to use.2. Referenced Documents2.1 ASTM Standards:2D 653 Terminology Relating to Soil, Rock, and ContainedFluidsE83 Practice for Verification and Classification of Exten-someter SystemsE 228 Test Method for Linear Thermal Exp
9、ansion of SolidMaterials With a Push-Rod Dilatometer3. Terminology3.1 Definitions of Terms Specific to This Standard:3.1.1 sample thermal strain, tchange in length of a unitlength of sample when the sample is subjected to heat. Themathematical expression is:t5 L22 L1!/L0(1)where:L1and L2= specimen l
10、engths corresponding to tempera-tures T1and T2, andL0= the original specimen length at some refer-ence temperature T0.Thermal strain is also equal to the specimen thermal dis-placement, dt, divided by the original sample length:t5dt/L0(2)3.1.2 mean coeffcient of linear expression, ambetweentwo tempe
11、ratures, T1and T2, is defined as follows:am5 L22 L1!/L0T22 T1!# (3)where:1These test methods are under the jurisdiction ofASTM Committee D18 on Soiland Rock and are the direct responsibility of Subcommittee D18.12 on RockMechanics.Current edition approved July 1, 2008. Published July 2008. Originall
12、y approvedin 1985. Last previous edition approved in 2004 as D 4535 85 (2004).2For referenced ASTM standards, visit the ASTM website, www.astm.org, orcontact ASTM Customer Service at serviceastm.org. For Annual Book of ASTMStandardsvolume information, refer to the standards Document Summary page ont
13、he ASTM website.1*A Summary of Changes section appears at the end of this standard.Copyright ASTM International, 100 Barr Harbor Drive, PO Box C700, West Conshohocken, PA 19428-2959, United States.L1and L2= specimen lengths at temperatures T1and T2,respectively. Therefore, amis obtained bydividing t
14、he linear thermal strain, (L1 L2)/L0, by the change in temperature units areinch/inch or centimetre/centimetre per tem-perature change in F or C, respectively. amis often expressed in parts per million perdegree.3.1.3 Upon heating ( T2 T1), an increase in the length of therock sample will give a pos
15、itive value of am. If a decrease inlength (contraction) is observed, amwill become negative.3.1.4 For definitions of other terms used in these testmethods, see Terminology D 653.4. Summary of Test Methods4.1 The application of heat to a rock causes it to expand.This expansion divided by the original
16、 length of the rockspecimens is the thermal strain from which coefficients ofexpansion can be calculated. This standard covers two methodsfor measuring rock expansion. The primary difference betweenthe two methods is in the type of dilatometer used.4.1.1 Test Method ITest Method I is the procedure u
17、sedwhen making unconfined or bench top measurements. Themethod and apparatus are similar to that described in TestMethod E 228. The rock specimen thermal displacement ismeasured using a dilatometer as shown in Fig. 1. The sampledisplacement is measured by a transducer located outside theheated area
18、of the sample; therefore, apparent strain due toapparatus expansion and contraction is minimized.4.1.2 Test Method IITest Method II employs a dilatomet-ric device which is located inside the heated zone, as shown inFig. 2. This test method is most suited for the measurement ofrock thermal strain und
19、er confined conditions.4.2 In both test methods, sample expansion is measuredcontinuously as temperature is gradually increased or allowedto stabilize at discrete temperature points.5. Significance and Use5.1 Information concerning the thermal expansion charac-teristics of rocks is important in the
20、design of any undergroundexcavation where the surrounding rock may be heated. Ther-mal strain causes thermal stresses which ultimately affectexcavation stability. Examples of applications where rockthermal strain is important include: nuclear waste repositories,underground power stations, compressed
21、 air energy storagefacilities, and geothermal energy facilities.5.2 The coefficient of thermal expansion or “alpha” or rockis known to vary as the temperature changes. These methodsprovide continuous thermal strain values as a function oftemperature, and therefore provide information on how alphacha
22、nges with temperature.5.3 Rocks are also often anisotropic, thus displaying differ-ent thermal strains depending on the orientation of strainmeasurement. These methods allow for measuring strain in onedirection only. If anisotropy is expected, samples with differentorientations should be prepared an
23、d tested.5.4 Care should be exercised in the interpretation of thermalstrain data of rocks with significant moisture content. Undercertain temperature and pressure conditions, steam may beproduced in the pore space. Steam may cause errors because ofmicrocrack production or changes in the pore pressu
24、re. Thephase change from water to steam in the pore space can resultin several phenomena which complicate data analysis, asfollows:5.4.1 Evolved steam may change the pore pressure and thusthe effective stress in the rock, resulting in anomalous strainreadings.5.4.2 Losing all the moisture may dehydr
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