ASTM E2884-2013e1 Standard Guide for Eddy Current Testing of Electrically Conducting Materials Using Conformable Sensor Arrays《使用适合的传感器阵列对导电材料进行涡流检测的标准指南》.pdf

《ASTM E2884-2013e1 Standard Guide for Eddy Current Testing of Electrically Conducting Materials Using Conformable Sensor Arrays《使用适合的传感器阵列对导电材料进行涡流检测的标准指南》.pdf》由会员分享，可在线阅读，更多相关《ASTM E2884-2013e1 Standard Guide for Eddy Current Testing of Electrically Conducting Materials Using Conformable Sensor Arrays《使用适合的传感器阵列对导电材料进行涡流检测的标准指南》.pdf（7页珍藏版）》请在麦多课文档分享上搜索。

1、Designation: E2884 131Standard Guide forEddy Current Testing of Electrically Conducting MaterialsUsing Conformable Sensor Arrays1This standard is issued under the fixed designation E2884; the number immediately following the designation indicates the year oforiginal adoption or, in the case of revis

2、ion, 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.1NOTESection 2 was corrected editorially in June 2104.1. Scope1.1 This guide covers the use of conformable eddy c

3、urrentsensor arrays for nondestructive examination of electricallyconducting materials for discontinuities and material quality.The discontinuities include surface breaking and subsurfacecracks and pitting as well as near-surface and hidden-surfacematerial loss. The material quality includes coating

4、 thickness,electrical conductivity, magnetic permeability, surface rough-ness and other properties that vary with the electrical conduc-tivity or magnetic permeability.1.2 This guide is intended for use on nonmagnetic andmagnetic metals as well as composite materials with anelectrically conducting c

5、omponent, such as reinforced carbon-carbon composite or polymer matrix composites with carbonfibers.1.3 This guide applies to planar as well as non-planarmaterials with and without insulating coating layers.1.4 UnitsThe values stated in SI units are to be regardedas standard. The values given in par

6、entheses are mathematicalconversions to inch-pound units that are provided for informa-tion only and are not considered standard.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

7、 appro-priate safety and health practices and determine the applica-bility of regulatory limitations prior to use.2. Referenced Documents2.1 ASTM Standards:2E543 Specification for Agencies Performing NondestructiveTestingE1316 Terminology for Nondestructive ExaminationsE2338 Practice for Characteriz

8、ation of Coatings Using Con-formable Eddy-Current Sensors without Coating Refer-ence Standards2.2 ASNT Documents:3SNT-TC-1A Recommended Practice for Personnel Qualifi-cation and Certification in Nondestructive TestingANSI/ASNT-CP-189 Standard for Qualification and Certifi-cation of NDT Personnel2.3

9、AIA Standard:NAS 410 Certification and Qualification of NondestructiveTesting Personnel42.4 Department of Defense Handbook:MIL-HDBK1823A Nondestructive Evaluation System Re-liability Assessment3. Terminology3.1 DefinitionsFor definitions of terms relating to thisguide refer to Terminology E1316.3.2

10、Definitions of Terms Specific to This Standard:3.2.1 B-Scana method of data presentation utilizing ahorizontal base line that indicates distance along the surface ofa material and a vertical deflection that represents a measure-ment response for the material being examined.3.2.2 C-Scana method of da

11、ta presentation which pro-vides measurement responses for the material being examinedin two-dimensions over the surface of the material.3.2.3 conformablerefers to an ability of sensors or sensorarrays to conform to non-planar surfaces without significanteffects on the measurement results, or with ef

12、fects that arelimited to a quantifiable bound.1This guide is under the jurisdiction of ASTM Committee E07 on Nondestruc-tive Testing and is the direct responsibility of Subcommittee E07.07 on Electro-magnetic Method.Current edition approved June 1, 2013. Published June 2013. Originallyapproved in 20

13、13. Last previous edition approved in 2013 as E288413. DOI:10.1520/E2884-13E01.2For 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 standards Document Summary page o

14、nthe ASTM website.3Available fromAmerican Society for Nondestructive Testing (ASNT), P.O. Box28518, 1711 Arlingate Ln., Columbus, OH 43228-0518, http:/www.asnt.org.4Available from Aerospace Industries Association of America, Inc. (AIA), 1000Wilson Blvd., Suite 1700,Arlington, VA22209-3928, http:/www

15、.aia-aerospace.org.(Replacement standard for MIL-STD-410.)Copyright ASTM International, 100 Barr Harbor Drive, PO Box C700, West Conshohocken, PA 19428-2959. United States13.2.4 depth of sensitivitydepth to which the sensor re-sponse to features or properties of interest exceeds a noisethreshold.3.2

16、.4.1 DiscussionThe depth of sensitivity is generallysmaller than the depth of penetration since it incorporates acomparison between the signal obtained from a feature as wellas measurement noise, whereas the depth of penetration refersto the decrease in field intensity with distance away from a test

17、coil.3.2.5 discontinuity-containing reference standarda regionof the material under examination or a material having elec-tromagnetic properties similar to the material under examina-tion for which a discontinuity having known characteristics ispresent.3.2.6 discontinuity-free reference standarda re

18、gion of thematerial under examination or a material having electromag-netic properties similar to the material under examination forwhich no discontinuities are present.3.2.7 drive windinga conductor pattern or coil that pro-duces a magnetic field that couples to the material beingexamined.3.2.7.1 D

19、iscussionThe drive winding can have variousgeometries, including: 1) a simple linear conductor that isplaced adjacent to a one-dimensional array of sensing ele-ments; 2) one or multiple conducting loops driven to create acomplex field pattern; and 3) multiple conducting loops with aseparate loop for

20、 each sensing element.3.2.8 insulating shimsconformable and substantially non-conducting or insulating foils that are used to measure effectsof small lift-off excursions on sensor response.3.2.9 lift offnormal distance from the plane of the con-formable sensor winding conductors to the surface of th

21、econducting material under examination.3.2.10 model for sensor responsea relation between theresponse of the sensor (for example, impedance magnitude andphase or real and imaginary parts) and properties of interest(for example, electrical conductivity, magnetic permeability,lift-off, and material th

22、ickness) for at least one sensing elementand at least one drive winding.3.2.10.1 DiscussionThese model responses may be ob-tained from database tables and may be analysis-based orempirical.3.2.11 sensing elementa means for measuring the mag-netic field intensity or rate of change of magnetic fieldin

23、tensity, such as an inductive coil or a solid-state device.3.2.11.1 DiscussionThe sensing elements can be arrangedin one or two-dimensional arrays. They can provide either anabsolute signal related to the magnetic field in the vicinity ofthe sense element or a differential signal.3.2.12 spatial half

24、-wavelengthspacing between the con-ductors of a linear drive winding with current flow in oppositedirections.3.2.12.1 DiscussionThis spacing affects the depth of sen-sitivity. The spatial wavelength equals two times this spacing.For a circular drive winding, the effective spatial half-wavelength is

25、equal to the drive winding diameter.3.2.13 system performance verificationthe use of a mea-surement of one or more response values, typically physicalproperty values, for a reference part to confirm that theresponse values are within specified tolerances to validate thesystem standardization and ver

26、ify proper instrument operation.4. Summary of Guide4.1 The examination is performed by scanning a conform-able eddy current sensor array over the surface of the materialof interest, with the sensor array energized with alternatingcurrent of one or more frequencies. The electrical responsefrom each s

27、ensing element of the eddy current sensor array ismodified by the proximity and local condition of the materialbeing examined. The extent of this modification is determinedby the distance between the eddy current sensor array and thematerial being examined, as well as the dimensions andelectrical pr

28、operties (electrical conductivity and magnetic per-meability) of the material. The presence of metallurgical ormechanical discontinuities in the material alters the measuredimpedance of the eddy current sense elements. While scanningover the material, the position at each measurement locationshould

29、be recorded along with the response of each sensingelement in the sensor array. The measured responses andlocation information can then be used, typically in the form ofa displayed image (C-scan (3.2.2) or in the form of a plot(B-scan (3.2.1), to determine the presence and characteristicsof material

30、 property variations or discontinuities.4.2 The eddy current sensor arrays used for the examinationare flexible and, with a suitable backing layer, can conform toboth flat and curved surfaces, including fillets, cylindricalsurfaces, etc. The sensor array can have a variety of configu-rations. These

31、include: 1) a linear drive conductor that isenergized by the instrument alternating current and a lineararray of absolute sense elements positioned parallel to the driveconductor; 2) a complex drive conductor that produces adesired field pattern at each sensing element; and 3) individualdrive conduc

32、tors associated with each sensing element. Asso-ciated with each sense element are one or more measurementresponses that reflect the local material condition at eachlocation over the surface. The sensor arrays may be used withmodels for the sensor response and appropriate algorithms toconvert measur

33、ed responses for each sensing element intophysical properties, such as lift-off, electrical conductivity,magnetic permeability, coating thickness, and/or substratethickness. Baseline values for these measurement responses orphysical properties are used to ensure proper operation duringthe examinatio

34、n while local variations in one or more of theseproperties can be used to detect and characterize the disconti-nuity. For example, although, an impedance magnitude or othersensing element response can be used without a model todetermine the presence of a flaw, a measurement of the lift-offat each se

35、nsing element location ensures that the sensor isconforming properly to the surface. Also, a position measure-ment capability, such as a rolling position encoder, can be usedto measure location in the scan direction and ensure thatsufficient data resolution is achieved. Visual or audio signalingdevi

36、ces may be used to indicate the position of the disconti-nuity.E2884 13125. Significance and Use5.1 Eddy current methods are used for nondestructivelylocating and characterizing discontinuities in magnetic ornonmagnetic electrically conducting materials. Conformableeddy current sensor arrays permit

37、examination of planar andnon-planar materials but usually require suitable fixtures tohold the sensor array near the surface of the material ofinterest, such as a layer of foam behind the sensor array alongwith a rigid support structure.5.2 In operation, the sensor arrays are standardized withmeasur

38、ements in air and/or a reference part. Responses mea-sured from the sensor array may be converted into physicalproperty values, such as lift-off, electrical conductivity, and/ormagnetic permeability. Proper instrument operation is verifiedby ensuring that these measurement responses or propertyvalue

39、s are within a prescribed range. Performance verificationon reference standards with known discontinuities is performedperiodically.5.3 The sensor array dimensions, including the size andnumber of sense elements, and the operating frequency areselected based on the type of examination being performe

40、d.The depth of penetration of eddy currents into the materialunder examination depends upon the frequency of the signal,the electrical conductivity and magnetic permeability of thematerial, and some dimensions of the sensor array. The depthof penetration is equal to the conventional skin depth at hi

41、ghfrequencies but is also related to the sensor array dimensions atlow frequencies, such as the size of the drive winding and thegap distance between the drive winding and sense elementarray. For surface-breaking discontinuities on the surfaceadjacent to the sensor array, high frequencies should be

42、usedwhere the penetration depth is less than the thickness of thematerial under examination. For subsurface discontinuities orwall thickness measurements, lower frequencies and largersensor dimensions should be used so that the depth ofpenetration is comparable to the material thickness.5.4 Insulati

43、ng layers or coatings may be present between thesensor array and the surface of the electrically conductingmaterial under examination. The sensitivity of a measurementto a discontinuity generally decreases as the coating thicknessand/or lift-off increases. For eddy current sensor arrays havinga line

44、ar drive conductor and a linear array of sense elements,the spacing between the drive conductor and the array of senseelements should be smaller than or comparable to the thicknessof the insulating coating. For other array formats the depth ofsensitivity should be verified empirically.5.5 Models for

45、 the sensor response may be used to convertresponses measured from the sensor array into physical prop-erty values, such as lift-off, electrical conductivity, magneticpermeability, coating thickness, and/or substrate thickness. Fordetermining two property values, one operational frequencycan be used

46、. For nonmagnetic materials and examination forcrack-like discontinuities, the lift-off and electrical conductiv-ity should be determined. For magnetic materials, when theelectrical conductivity can be measured or assumed constant,then the lift-off and magnetic permeability should be deter-mined. Th

47、e thickness can only be determined if a sufficientlylow excitation frequency is used where the depth of sensitivityis greater than the material thickness of interest. For determin-ing more than two property values, measurements at operatingconditions having at least two depths of penetration should

48、beused; these different depths of penetration can be achieved byusing multiple operational frequencies or multiple spatialwavelengths.5.6 Processing of the measurement response or propertyvalue data may be performed to highlight the presence ofdiscontinuities, to reduce background noise, and to char

49、acterizedetected discontinuities. As an example, a correlation filter canbe applied in which a reference signature response for adiscontinuity is compared to the measured responses for eachsensor array element to highlight discontinuity-like defects.Care must be taken to properly account for the effect ofinterferences such as edges and coatings on such signatures.6. Basis of Application6.1 The following items are subject to contractual agree-ment between the parties using or referencing this standard.6.2 Personnel QualificationIf specified in the contrac