ISO-2360-2003.pdf

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1、 Reference number ISO 2360:2003(E) ISO 2003 INTERNATIONAL STANDARD ISO 2360 Third edition 2003-11-15 Non-conductive coatings on non-magnetic electrically conductive basis materials Measurement of coating thickness Amplitude-sensitive eddy current method Revtements non conducteurs sur matriaux de bas

2、e non magntiques conducteurs de llectricit Mesurage de lpaisseur de revtement Mthode par courants de Foucault sensible aux variations damplitude ISO 2360:2003(E) PDF disclaimer This PDF file may contain embedded typefaces. In accordance with Adobes licensing policy, this file may be printed or viewe

3、d but shall not be edited unless the typefaces which are embedded are licensed to and installed on the computer performing the editing. In downloading this file, parties accept therein the responsibility of not infringing Adobes licensing policy. The ISO Central Secretariat accepts no liability in t

4、his area. Adobe is a trademark of Adobe Systems Incorporated. Details of the software products used to create this PDF file can be found in the General Info relative to the file; the PDF-creation parameters were optimized for printing. Every care has been taken to ensure that the file is suitable fo

5、r use by ISO member bodies. In the unlikely event that a problem relating to it is found, please inform the Central Secretariat at the address given below. ISO 2003 All rights reserved. Unless otherwise specified, no part of this publication may be reproduced or utilized in any form or by any means,

6、 electronic or mechanical, including photocopying and microfilm, without permission in writing from either ISO at the address below or ISOs member body in the country of the requester. ISO copyright office Case postale 56 CH-1211 Geneva 20 Tel. + 41 22 749 01 11 Fax + 41 22 749 09 47 E-mail copyrigh

7、tiso.org Web www.iso.org Published in Switzerland ii ISO 2003 All rights reserved ISO 2360:2003(E) ISO 2003 All rights reserved iii Contents Page Forewordiv 1 Scope1 2 Principle.1 3 Apparatus.1 4 Sampling1 5 Factors affecting measurement uncertainty2 5.1 Coating thickness .2 5.2 Electrical propertie

8、s of the basis materials2 5.3 Basis metal thickness.2 5.4 Edge effects.2 5.5 Surface curvature2 5.6 Surface roughness3 5.7 Lift-off effect 3 5.8 Probe pressure3 5.9 Probe tilt.3 5.10 Temperature effects3 5.11 Intermediate coatings.3 6 Procedure.4 6.1 Calibration of instruments .4 6.2 Determination5

9、7 Expression of results5 8 Measurement uncertainty.6 9 Test report6 Annex A (informative) Eddy current generation in a metallic conductor .7 Annex B (normative) Test for edge effect10 Bibliography .11 ISO 2360:2003(E) iv ISO 2003 All rights reserved Foreword ISO (the International Organization for S

10、tandardization) is a worldwide federation of national standards bodies (ISO member bodies). The work of preparing International Standards is normally carried out through ISO technical committees. Each member body interested in a subject for which a technical committee has been established has the ri

11、ght to be represented on that committee. International organizations, governmental and non-governmental, in liaison with ISO, also take part in the work. ISO collaborates closely with the International Electrotechnical Commission (IEC) on all matters of electrotechnical standardization. Internationa

12、l Standards are drafted in accordance with the rules given in the ISO/IEC Directives, Part 2. The main task of technical committees is to prepare International Standards. Draft International Standards adopted by the technical committees are circulated to the member bodies for voting. Publication as

13、an International Standard requires approval by at least 75 % of the member bodies casting a vote. Attention is drawn to the possibility that some of the elements of this document may be the subject of patent rights. ISO shall not be held responsible for identifying any or all such patent rights. ISO

14、 2360 was prepared by Technical Committee ISO/TC 107, Metallic and other inorganic coatings, Subcommittee SC 2, Test methods. This third edition cancels and replaces the second edition (ISO 2360:1982), which has been technically revised. INTERNATIONAL STANDARD ISO 2360:2003(E) ISO 2003 All rights re

15、served 1 Non-conductive coatings on non-magnetic electrically conductive basis materials Measurement of coating thickness Amplitude-sensitive eddy current method 1 Scope This International Standard describes a method for non-destructive measurements of the thickness of non- conductive coatings on no

16、n-magnetic, electrically conductive (generally metallic) basis materials, using amplitude-sensitive eddy current instruments. NOTE This method can also be used to measure non-magnetic metallic coatings on non-conductive basis materials. The method is particularly applicable to measurements of the th

17、ickness of most oxide coatings produced by anodizing, but is not applicable to all conversion coatings, some of which are too thin to be measured by this method (see Clause 6). Although theoretically, the method can be used for measurements of the thickness of coatings on magnetic basis materials, i

18、ts use for this application is not recommended. In such cases, the magnetic method specified in ISO 2178 should be used. 2 Principle An eddy current probe (or integrated probe/instrument) is placed on the surface of the coating(s) to be measured, and the thickness is read from the instruments readou

19、t. 3 Apparatus 3.1 Probe, containing an eddy current generator and detector linked to a system capable of measuring and displaying the changes in amplitude, normally as a direct readout of coating thickness. The system may also be able to measure phase changes. NOTE 1 The probe and measuring system/

20、display may be integrated into a single instrument. NOTE 2 Factors affecting measurement accuracy are discussed in Clause 5. 4 Sampling Sampling depends on the specific application and coating to be tested. The area, location and number of test specimens shall be agreed between interested parties an

21、d shall be included in the test report (see Clause 9). ISO 2360:2003(E) 2 ISO 2003 All rights reserved 5 Factors affecting measurement uncertainty 5.1 Coating thickness A measurement uncertainty is inherent in the method. For thin coatings, this measurement uncertainty (in absolute terms) is constan

22、t, independent of the coating thickness and, for a single measurement, is at least 0,5 m. For coatings thicker than 25 m, the uncertainty becomes relative to the thickness and is approximately a constant fraction of that thickness. For measuring coating thicknesses of 5 m or less, the average of sev

23、eral measurements shall be taken. It may not be possible to obtain the measurement uncertainty specified in Clause 8 when measuring coatings of less than 3 m in thickness. 5.2 Electrical properties of the basis materials Measurements using eddy current instruments can be affected by the electrical c

24、onductivity of the basis metal, which is a function of the composition and heat treatment of the material. The influence of electrical conductivity on the measurement varies considerably with the make and type of instrument. 5.3 Basis metal thickness For each instrument there is a critical minimum b

25、asis metal thickness above which measurements are not affected by an increase in thickness. Since this thickness depends on both the eddy current generation frequency of the probe system and the electrical properties of the basis material its value should be determined experimentally, unless otherwi

26、se specified by the manufacturer. An explanation of Eddy current generation and the calculation of the required minimum basis material thickness, dmin, is given in Annex A. However, in the absence of any other information, the required minimum basis material thickness, dmin, can be estimated from th

27、e equation: dmin = 2,5 0 where 0 is the standard penetration depth of the basis material (see A.1). 5.4 Edge effects Eddy current instruments can be sensitive to abrupt changes in surface contour of test specimen. Therefore measurements made too near to an edge or corner may not be valid unless the

28、instrument has been specifically calibrated for such measurements (see 6.2.4 and Annex B). NOTE When compared with the phase-sensitive method of ISO 21968, the amplitude-sensitive eddy current instruments can be substantially more heavily affected by edge effects. 5.5 Surface curvature Measurements

29、are affected by the curvature of the test specimen. This influence of curvature varies considerably with the make and type of instrument and probe, but always becomes more pronounced as the radius of curvature decreases. Measurements made on curved test specimens might not, therefore, be valid unles

30、s the instrument is specifically calibrated for the surface curvature in question, or a special probe, which compensates for surface influence, is used. ISO 2360:2003(E) ISO 2003 All rights reserved 3 5.6 Surface roughness Measurements are influenced by the surface topography of the basis material a

31、nd of the coating. Rough surfaces can cause both systematic and random errors. Random errors can be reduced by making multiple measurements, each measurement being made at a different location, and then calculating the average value of that series of measurements. If the basis material is rough, the

32、 zero of the instrument shall be checked at several locations on a typical sample of the uncoated, rough, basis material. If no typical uncoated basis material is available, the coating of the test specimen shall be stripped, at least over part of its area, with a chemical solution that does not att

33、ack the basis material. NOTE When compared with the phase-sensitive method of ISO 21968, the amplitude-sensitive eddy current measurement can be more heavily affected by basis material roughness. 5.7 Lift-off effect If the probe is not placed directly on the coating, the gap between probe and coatin

34、g (“lift-off”) affects the measurement of the coating thickness. The measured thickness will be equal to the coating thickness plus the additional “lift-off” gap. Lift-off can be produced unintentionally, e.g., by the presence of foreign particles between the probe and the coating. The probe tip sha

35、ll be checked frequently for cleanliness. 5.8 Probe pressure The pressure with which the probe is applied to the test specimen affects the instrument readings and shall therefore be made constant. This pressure effect is more noticeable when the coatings are soft. Most commercially-available instrum

36、ents are supplied with constant pressure probes. 5.9 Probe tilt Unless otherwise instructed by the manufacturer, the probe shall be applied perpendicularly to the coating surface as tilting the probe away from the perpendicular can cause measurement errors. The possibility of tilt occurring inadvert

37、ently can be minimized by probe design or by the use of a probe- holding jig. 5.10 Temperature effects Because temperature changes affect the characteristics of the probe, it should be used under approximately the same temperature conditions as those used for calibration unless the probe has built-i

38、n temperature compensation. Most metals change their electrical conductivity with temperature. Because the measured coating thickness is influenced by changes in the electrical conductivity of the basis metal, large temperature changes should be avoided. 5.11 Intermediate coatings The presence of an

39、 intermediate coating can affect the measurement of the coating thickness if the electrical characteristics of that intermediate coating differ from that of the coating or basis material. If a difference does exist then the measurements will, in addition, be affected by an intermediate coating thick

40、ness of less than ISO 2360:2003(E) 4 ISO 2003 All rights reserved dmin. If the thickness is greater than dmin then the intermediate coating, if non-magnetic, can be treated as the basis material. It has been found that some instruments having probe systems operating with multiple frequencies can mea

41、sure both top and intermediate coatings. 6 Procedure 6.1 Calibration of instruments 6.1.1 General Before use, each instrument shall be calibrated in accordance with the manufacturers instructions, using suitable calibration standards. Particular attention shall be paid to the description given in Cl

42、ause 3 and to the factors described in Clause 5. In order to minimize conductivity changes due to temperature variations, at the time of calibration the instrument and the calibration standards shall be at a temperature close to the temperature of the items to be measured. NOTE Calibration checks sh

43、ould also be carried out as necessary during the determinations to avoid instrument drift. 6.1.2 Calibration standards Instrument calibration shall be made using at least two standards of different and known thicknesses. One of these standards may be of the uncoated basis material. NOTE 1 Such stand

44、ards should have their thicknesses traceable to a certifiable source. The electrical conductivity and magnetic permeability of both coating and basis materials shall be identical to those properties of the parts to be measured. NOTE 2 As calibration standards are subject to wear and deterioration wi

45、th time and use, they should be recalibrated and/or replaced periodically at time intervals established locally or after consultation with the manufacturer. 6.1.3 Verification The electrical properties of the basis material of the calibration standards shall be similar to those of the basis material

46、 of the test specimen. NOTE To confirm their suitability, the readings obtained with the basis material of the uncoated calibration standard and with that of the test specimen should be compared. If the basis material thickness exceeds the critical thickness, as defined in 5.3, the thickness measure

47、ment is not affected by the thickness of the basis material. If the critical thickness is not exceeded, the thickness of the basis material for the test and for the calibration shall be the same. If, under practical conditions, this is not possible then it may be possible to back either the standard

48、 or the test specimen with a sufficient thickness of a material having similar electrical properties to make the readings independent of the basis material thickness. If this method is used, tests shall be undertaken to confirm that it is acceptable and to establish the presence of any additional er

49、rors. If the curvature of the coated surface to be measured is such as to preclude calibration on a flat surface, the standards used for calibration shall have the same radii of curvature as the specimen to be measured, unless a special probe that compensates for the curvature influence is used. ISO 2360:2003(E) ISO 2003 All rights reserved 5 6.2 Determination 6.2.1 General Operate each instrument in accordance with the manufacturers instructions, giving appropriate attention to the factors given in Clause 5. Check the

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