ASTM C597-2002 Standard Test Method for Pulse Velocity Through Concrete《对通过混凝土的脉冲速度的标准试验方法》.pdf

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1、Designation: C 597 02Standard Test Method forPulse Velocity Through Concrete1This standard is issued under the fixed designation C 597; the number immediately following the designation indicates the year oforiginal adoption or, in the case of revision, the year of last revision. A number in parenthe

2、ses indicates the year of last reapproval. Asuperscript epsilon (e) indicates an editorial change since the last revision or reapproval.1. Scope *1.1 This test method covers the determination of the propa-gation velocity of longitudinal stress wave pulses throughconcrete. This test method does not a

3、pply to the propagation ofother types of stress waves through concrete.1.2 The values stated in SI units are to be regarded as thestandard.1.3 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

4、 establish appro-priate safety and health practices and determine the applica-bility of regulatory limitations prior to use.2. Referenced Documents2.1 ASTM Standards:C 125 Terminology Relating to Concrete and ConcreteAggregates2C 215 Test Method for Fundamental Transverse, Longitu-dinal, and Torsion

5、al Frequencies of Concrete Specimens2C 823 Practice for Examination and Sampling of HardenedConcrete in Constructions2E 1316 Terminology for Nondestructive Examinations33. Terminology3.1 DefinitionsRefer to Terminology C 125 and the sec-tion related to ultrasonic examination in Terminology E 1316for

6、 definitions of terms used in this test method.4. Summary of Test Method4.1 Pulses of longitudinal stress waves are generated by anelectro-acoustical transducer that is held in contact with onesurface of the concrete under test. After traversing through theconcrete, the pulses are received and conve

7、rted into electricalenergy by a second transducer located a distance L from thetransmitting transducer. The transit time T is measured elec-tronically. The pulse velocity V is calculated by dividing L byT.5. Significance and Use5.1 The pulse velocity, V, of longitudinal stress waves in aconcrete mas

8、s is related to its elastic properties and densityaccording to the following relationship:V 5E 1 2 !r 1 1 !1 2 2 !(1)where:E = dynamic modulus of elasticity, = dynamic Poissons ratio, andr = density.5.2 This test method is applicable to assess the uniformityand relative quality of concrete, to indic

9、ate the presence ofvoids and cracks, and to evaluate the effectiveness of crackrepairs. It is also applicable to indicate changes in the proper-ties of concrete, and in the survey of structures, to estimate theseverity of deterioration or cracking. When used to monitorchanges in condition over time,

10、 test locations are to be markedon the structure to ensure that tests are repeated at the samepositions.5.3 The degree of saturation of the concrete affects the pulsevelocity, and this factor must be considered when evaluatingtest results (Note 1). In addition, the pulse velocity in saturatedconcret

11、e is less sensitive to changes in its relative quality.NOTE 1The pulse velocity in saturated concrete may be up to 5 %higher than in dry concrete.45.4 The pulse velocity is independent of the dimensions ofthe test object provided reflected waves from boundaries do notcomplicate the determination of

12、the arrival time of the directlytransmitted pulse. The least dimension of the test object mustexceed the wavelength of the ultrasonic vibrations (Note 2).NOTE 2The wavelength of the vibrations equals the pulse velocitydivided by the frequency of vibrations. For example, for a frequency of 54kHz and

13、a pulse velocity of 3500 m/s, the wavelength is 3500/54000 =0.065 m.5.5 The accuracy of the measurement depends upon theability of the operator to determine precisely the distancebetween the transducers and of the equipment to measureprecisely the pulse transit time. The received signal strengthand

14、measured transit time are affected by the coupling of the1This test method is under the jurisdiction of ASTM Committee C09 onConcrete and Concrete Aggregates and is the direct responsibility of SubcommitteeC09.64 on Nondestructive and In-Place Testing.Current edition approved Dec. 10, 2002. Publishe

15、d February 2003. Originallyapproved in 1967. Last previous edition approved in 1997 as C 597 97.2Annual Book of ASTM Standards, Vol 04.02.3Annual Book of ASTM Standards, Vol 03.03.4Bungey, J. H., Testing of Concrete in Structures, 2nd ed., Chapman and Hall,1989, p. 52.1*A Summary of Changes section

16、appears at the end of this standard.Copyright ASTM International, 100 Barr Harbor Drive, PO Box C700, West Conshohocken, PA 19428-2959, United States.transducers to the concrete surfaces. Sufficient coupling agentand pressure must be applied to the transducers to ensure stabletransit times. The stre

17、ngth of the received signal is also affectedby the travel path length and by the presence and degree ofcracking or deterioration in the concrete tested.NOTE 3Proper coupling can be verified by viewing the shape andmagnitude of the received waveform. The waveform should have adecaying sinusoidal shap

18、e. The shape can be viewed by means of outputsto an oscilloscope or digitized display inherent in the device.5.6 The results obtained by the use of this test method arenot to be considered as a means of measuring strength nor asan adequate test for establishing compliance of the modulus ofelasticity

19、 of field concrete with that assumed in the design. Thelongitudinal resonance method in Test Method C 215 is rec-ommended for determining the dynamic modulus of elasticityof test specimens obtained from field concrete because Pois-sons ratio does not have to be known.NOTE 4When circumstances permit,

20、 a velocity-strength (or velocity-modulus) relationship may be established by the determination of pulsevelocity and compressive strength (or modulus of elasticity) on a numberof samples of a concrete. This relationship may serve as a basis for theestimation of strength (or modulus of elasticity) by

21、 further pulse-velocitytests on that concrete. Refer to ACI 228.1R5for guidance on theprocedures for developing and using such a relationship.5.7 The procedure is applicable in both field and laboratorytesting regardless of size or shape of the specimen within thelimitations of available pulse-gener

22、ating sources.NOTE 5Presently available test equipment limits path lengths toapproximately 50-mm minimum and 15-m maximum, depending, in part,upon the frequency and intensity of the generated signal. The upper limitof the path length depends partly on surface conditions and partly on thecharacterist

23、ics of the interior concrete under investigation. A preamplifierat the receiving transducer may be used to increase the maximum pathlength that can be tested. The maximum path length is obtained by usingtransducers of relatively low resonant frequencies (20 to 30 kHz) tominimize the attenuation of t

24、he signal in the concrete. (The resonantfrequency of the transducer assembly determines the frequency ofvibration in the concrete.) For the shorter path lengths where loss of signalis not the governing factor, it is preferable to use resonant frequencies of50 kHz or higher to achieve more accurate t

25、ransit-time measurements andhence greater sensitivity.5.8 Since the pulse velocity in steel is up to double that inconcrete, the pulse-velocity measured in the vicinity of thereinforcing steel will be higher than in plain concrete of thesame composition. Where possible, avoid measurements closeto st

26、eel parallel to the direction of pulse propagation.6. Apparatus6.1 The testing apparatus, shown schematically in Fig. 1,consists of a pulse generator, a pair of transducers (transmitterand receiver), an amplifier, a time measuring circuit, a timedisplay unit, and connecting cables.6.1.1 Pulse Genera

27、tor and Transmitting TransducerThepulse generator shall consist of circuitry for generating pulsesof voltage (Note 6). The transducer for transforming theseelectronic pulses into wave bursts of mechanical energy shallhave a resonant frequency in the range from 20 to 100 kHz(Note 7). The pulse genera

28、tor shall produce repetitive pulses ata rate of not less than 3 pulses per second. The transducer shallbe constructed of piezoelectric, magnetostrictive, or othervoltage-sensitive material (Rochelle salt, quartz, barium titan-ate, lead zirconate-titante (PZT), and so forth), housed forprotection. A

29、triggering pulse shall be produced to start thetime measuring circuit.NOTE 6The pulse voltage affects the transducer power output and themaximum penetration of the longitudinal stress waves. Voltage pulses of500 to 1000 V have been used successfully.NOTE 7Transducers with higher resonant frequencies

30、 have been usedsuccessfully in relatively small laboratory specimens.6.1.2 Receiving Transducer and AmplifierThe receivingtransducer shall be similar to the transmitting transducer. Thevoltage generated by the receiver shall be amplified as neces-sary to produce triggering pulses to the time-measuri

31、ng circuit.The amplifier shall have a flat response between one half andthree times the resonant frequency of the receiving transducer.6.1.3 Time-Measuring CircuitThe time-measuring circuitand the associated triggering pulses shall be capable ofproviding an overall time-measurement resolution of at

32、least 1s. Time measurement is initiated by a triggering voltage fromthe pulse generator, and the time measuring circuit shalloperate at the repetition frequency of the pulse generator. Thetime-measuring circuit shall provide an output when thereceived pulse is detected, and this output shall be used

33、 todetermine the transit time displayed on the time-display unit.The time-measuring circuit shall be insensitive to operatingtemperature in the range from 0 to 40C and voltage changesin the power source of 615 %.6.1.4 Display UnitTwo types of display units are avail-able. Modern units use an interva

34、l timer and a direct-readingdigital display of the transit time. Older units use a cathode raytube (CRT) on which the pulses transmitted and received aredisplayed as deflections of the traces in relation to an estab-lished time scale.5“In-Place Methods to Estimate Concrete Strength,” ACI 228.1R, Ame

35、ricanConcrete Institute, Farmington Hills, MI.NOTE 1It is advantageous to incorporate the pulse generator, timemeasuring circuit, receiver amplifier, and time display into one unit.FIG. 1 Schematic of Pulse Velocity ApparatusC5970226.1.5 Reference BarA bar of metal or other durablematerial for which

36、 the transit time of longitudinal waves isknown. The transit time shall be marked permanently on thereference bar.6.1.6 Connecting CablesWhere pulse-velocity measure-ments on large structures require the use of long interconnect-ing cables, use low-capacitance, shielded, coaxial cables.6.1.7 Couplin

37、g AgentA viscous material (such as oil,petroleum jelly, water soluble jelly, moldable rubber, or grease)to ensure efficient transfer of energy between the concrete andthe transducers. The function of the coupling agent is toeliminate air between the contact surfaces of the transducersand the concret

38、e. Water is an acceptable coupling agent whenponded on the surface, or for underwater testing.7. Procedure7.1 Functional Check of Equipment and Zero-timeAdjustmentVerify that the equipment is operating properlyand perform a zero-time adjustment. Apply coupling agent tothe ends of the reference bar,

39、and press the transducers firmlyagainst the ends of the bar until a stable transit time isdisplayed. Adjust the zero reference until the displayed transittime agrees with the value marked on the bar. For someinstruments, the zero adjustment is made by applying couplingagent and pressing the faces of

40、 the transducers together. Theseinstruments use a microprocessor to record this delay time,which is automatically subtracted from subsequent transit timemeasurements. For such instruments, measure the transit timethrough the reference bar to verify that the proper zero-timecorrection has been made.

41、Check the zero adjustment on anhourly basis during continuous operation of the instrument, andevery time a transducer or connecting cable is changed. If thedisplayed time cannot be adjusted to agree with transit time ofthe reference bar, do not use the instrument, and return the barand instrument to

42、 the manufacturer for repair.7.2 Determination of Transit Time:7.2.1 For testing existing construction, select test locationsin accordance with Practice C 823, or follow the requirementsof the party requesting the testing, whichever is applicable.7.2.2 For best results, locate the transducers direct

43、ly oppo-site each other. Because the beam width of the vibrationalpulses emitted by the transducers is large, it is permissible tomeasure transit times across corners of a structure but withsome loss of sensitivity and accuracy. Measurements along thesame surface shall not be used unless only one fa

44、ce of thestructure is accessible since such measurements may be indica-tive only of surface layers, and calculated pulse velocities willnot agree with those obtained by through transmission (Note8).NOTE 8One of the sources of uncertainty in surface tests is thelengths of the actual travel paths of t

45、he pulses. Hence, individual readingsare of little value. Surface tests, however, have been used to estimate thedepth of a lower quality surface layer by making multiple measurementsof transit time with varying distances between the transducers. From theplot of travel time versus spacing, it may be

46、possible to estimate the depthof the lower quality concrete.67.2.3 Apply an appropriate coupling agent (such as water,oil, petroleum jelly, grease, moldable rubber, or other viscousmaterials) to the transducer faces or the test surface, or both.Press the faces of the transducers firmly against the s

47、urfaces ofthe concrete until a stable transit time is displayed, andmeasure the transit time (Note 9). Determine the straight-linedistance between centers of transducer faces.NOTE 9The quality of the coupling is critically important to theaccuracy and maximum range of the method. Inadequate coupling

48、 willresult in unstable and inaccurate time measurements, and will significantlyshorten the effective range of the instrument. Repeat measurements shouldbe made at the same location to minimize erroneous readings due to poorcoupling.8. Calculation8.1 Calculate the pulse velocity as follows:V 5 L/T (

49、2)where:V = pulse velocity, m/s,L = distance between centers of transducer faces, m, andT = transit time, s.9. Report9.1 Report at least the following information:9.1.1 Location of test or identification of specimen.9.1.2 Location of transducers.9.1.3 Distance between centers of transducer faces, reportedto a precision of at least 0.5 % of the distance.9.1.4 Transit time, reported to a precision of at least 0.5 %of the transit time.9.1.5 Pulse velocity reported to the nearest 10 m/s.10. Precision and Bias10.1 Precision:10.1.1 Repeatability of results have