ASTM D4535-1985(2004) Standard Test Methods for Measurement of Thermal Expansion of Rock Using a Dilatometer《用膨胀计测量岩石的热膨胀的试验方法》.pdf
《ASTM D4535-1985(2004) Standard Test Methods for Measurement of Thermal Expansion of Rock Using a Dilatometer《用膨胀计测量岩石的热膨胀的试验方法》.pdf》由会员分享,可在线阅读,更多相关《ASTM D4535-1985(2004) Standard Test Methods for Measurement of Thermal Expansion of Rock Using a Dilatometer《用膨胀计测量岩石的热膨胀的试验方法》.pdf(6页珍藏版)》请在麦多课文档分享上搜索。
1、Designation: D 4535 85 (Reapproved 2004)Standard Test Methods forMeasurement of Thermal Expansion of Rock Using aDilatometer1This 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
2、, the year of last revision. A number in parentheses indicates the year of last reapproval. Asuperscript epsilon (e) indicates an editorial change since the last revision or reapproval.1. Scope1.1 These test methods cover the laboratory measurement ofthe linear (one-dimensional) thermal expansion of
3、 rocks usinga dilatometer.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 gover
4、ning the size, construction, 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 constru
5、c-tion and procedure 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.
6、 It isrecognized also 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 This standard does not purport to address all of thesafety concerns, if any, associated with its us
7、e. It is theresponsibility of the user of this standard to establish appro-priate safety and health practices and determine the applica-bility of regulatory limitations prior to use.2. Referenced Documents2.1 ASTM Standards:2E83 Practice for Verification and Classification of Exten-sometersE 228 Tes
8、t Method for Linear Thermal Expansion of SolidMaterials with Vitreous a Silica Dilatometer3. Terminology3.1 Definitions of Terms Specific to This Standard:3.1.1 sample thermal strain, et change in length of a unitlength of sample when the sample is subjected to heat. Themathematical expression is:et
9、5 L22 L1!/L0(1)where:L1and L2= specimen lengths 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:et5dt/L0(2)3.1.2 mean coeffcien
10、t of linear expression, ambetweentwo temperatures, T1and T2, is defined as follows:am5 L22 L1!/L0T22 T1!# (3)where:L1and L2= specimen lengths at temperatures T1and T2,respectively. Therefore, amis obtained bydividing the linear thermal strain, (L1 L2)/L0, by the change in temperature units areinch/i
11、nch 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 positive value of am. If a decrease inlength (contraction) is observed, amwill become
12、 negative.4. Summary of Test Methods4.1 The application of heat to a rock causes it to expand.This expansion divided by the original length of the rockspecimens is the thermal strain from which coefficients ofexpansion can be calculated. This standard covers two methods1These test methods are under
13、the jurisdiction ofASTM Committee D18 on Soiland Rock and are the direct responsibility of Subcommittee D18.12 on RockMechanics.Current edition approved Nov. 1, 2004. Published December 2004. Originallyapproved in 1985. Last previous edition approved in 2000 as D 453585(2000)2For referenced ASTM sta
14、ndards, 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 onthe ASTM website.1Copyright ASTM International, 100 Barr Harbor Drive, PO Box C700, West Conshohocken,
15、PA 19428-2959, United States.for 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 usedwhen making unconfined or bench top measurements. Themethod and apparatus are similar to that described in
16、 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 of the sample; therefore, apparent strain due toapparatus expansion and contraction is minimized.4.1.2 Test M
17、ethod 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 under confined conditions.4.2 In both test methods, sample expansion is measuredcontinuously as temperature is g
18、radually 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 design of any undergroundexcavation where the surrounding rock may be heated. Ther-mal strain causes thermal
19、stresses which ultimately affectexcavation stability. Examples of applications where rockthermal strain is important include: nuclear waste repositories,underground power stations, compressed air energy storagefacilities, and geothermal energy facilities.5.2 The coefficient of thermal expansion or “
20、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 alphachanges with temperature.5.3 Rocks are also often anisotropic, thus displaying differ-ent thermal strains depend
21、ing on the orientation of strainmeasurement. These methods allow for measuring strain in onedirection only. If anisotropy is expected, samples with differentorientations should be prepared and tested.5.4 Care should be exercised in the interpretation of thermalstrain data of rocks with significant m
22、oisture 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 pressure. Thephase change from water to steam in the pore space can resultin several phenomena which complicate dat
23、a 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 dehydrate clays in thepore space and thus change expansion characteristics, espe-cially in layered rocks.5.5 The re
24、searcher using this standard must use best judg-ment as to how to make the thermal expansion measurement sothat it accurately represents the conditions in the field.5.6 Method II is amenable to confined thermal strain deter-minations. Confined tests may be most appropriate when:5.6.1 Pore pressure m
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