1、Designation: B567 98 (Reapproved 2009a)Standard Test Method forMeasurement of Coating Thickness by the Beta BackscatterMethod1This standard is issued under the fixed designation B567; 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 () indicates an editorial change since the last revision or reapproval.This standard has been approved for use by agencies of the Department of Defense.1. Scope1.1 This test method covers
3、the beta backscatter gages forthe nondestructive measurement of metallic and nonmetalliccoatings on both metallic and nonmetallic substrate materials.1.2 The test method measures the mass of coating per unitarea, which can also be expressed in linear thickness unitsprovided that the density of the c
4、oating is known.1.3 The test method is applicable only if the atomic numbersor equivalent atomic numbers of the coating and substratediffer by an appropriate amount (see 6.2).1.4 Beta backscatter instruments employ a number of dif-ferent radioactive isotopes. Although the activities of theseisotopes
5、 are normally very low, they can present a hazard ifhandled incorrectly. This standard does not purport to addressthe safety issues and the proper handling of radioactivematerials. It is the responsibility of the user to comply withapplicable State and Federal regulations concerning the han-dling an
6、d use of radioactive material. Some States requirelicensing and registration of the radioactive isotopes.1.5 The values stated in SI units are to be regarded asstandard. No other units of measurement are included in thisstandard.1.6 This standard does not purport to address all of thesafety concerns
7、, if any, associated with its use. 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. Terminology2.1 Descriptions of Terms:2.1.1 activitythe nuclei of all radioisotopes
8、are unstableand tend to change into a stable condition by spontaneouslyemitting energy or particles, or both. This process is known asradioactive decay. The total number of disintegrations during asuitably small interval of time divided by that interval of timeis called “activity.” Therefore, in bet
9、a backscatter measure-ments, a higher activity corresponds to a greater emission ofbeta particles. The activity of a radioactive element used in betabackscatter gages is generally expressed in microcuries (1Ci = 3.7 3 104disintegrations per second).2.1.2 aperturethe opening of the mask abutting the
10、testspecimen. It determines the size of the area on which thecoating thickness is measured. This mask is also referred to asa platen, an aperture plate, a specimen support, or a specimenmask.2.1.3 backscatterwhen beta particles pass through matter,they collide with atoms. Among other things, this in
11、teractionwill change their direction and reduce their speed. If thedeflections are such that the beta particle leaves the body ofmatter from the same surface at which it entered, the betaparticle is said to be backscattered.2.1.4 backscatter coeffcientthe backscatter coefficient ofa body, R, is the
12、ratio of the number of beta particlesbackscattered to that entering the body. R is independent of theactivity of the isotope and of the measuring time.2.1.5 backscatter count:2.1.5.1 absolute backscatter countthe absolute backscat-ter count, X, is the number of beta particles that are backscat-tered
13、 during a finite interval of time and displayed by theinstrument. X will, therefore, depend on the activity of thesource, the measuring time, the geometric configuration of themeasuring system, and the properties of the detector, as well asthe coating thickness and the atomic numbers of the coatinga
14、nd substrate materials. X0is the count produced by theuncoated substrate, and Xs, that of the coating material. Toobtain these values, it is necessary that both these materials areavailable with a thickness greater than the saturation thickness(see 2.1.12).2.1.5.2 normalized backscatterthe normalize
15、d backscat-ter, xn, is a quantity that is independent of the activity of thesource, the measuring time, and the properties of the detector.The normalized backscatter is defined by the equation:xn5X 2 X0Xs2 X0where:1This test method is under the jurisdiction ofASTM Committee B08 on Metallicand Inorga
16、nic Coatings and is the direct responsibility of Subcommittee B08.10 onTest Methods.Current edition approved Sept. 1, 2009. Published December 2009. Originallyapproved in 1972. Last previous edition approved in 2009 as B567 98 (2009).DOI: 10.1520/B0567-98R09.1Copyright ASTM International, 100 Barr H
17、arbor Drive, PO Box C700, West Conshohocken, PA 19428-2959, United States.X0= count from the substrate,Xs= count from the coating material, andX = count from the coated specimen, and each count is forthe same interval of time.Because X is always $X0and # Xs, xncan only take valuesbetween 0 and 1. (F
18、or reasons of simplicity, it is oftenadvantageous to express the normalized count as a percentageby multiplying xnby 100.)2.1.5.3 normalized backscatter curvethe curve obtainedby plotting the coating thickness as a function of xn.2.1.6 beta particlesbeta particles or beta rays are high-speed electro
19、ns that are emitted from the nuclei of materialsundergoing a nuclear transformation. These materials arecalled beta-emitting isotopes, beta-emitting sources, or betaemitters.2.1.7 coating thicknessin this test method, coating thick-ness refers to mass per unit area as well as geometricalthickness.2.
20、1.8 dead time or resolving timeGeiger-Mller tubesused for counting beta particles have characteristic recoverytimes that depend on their construction and the count rate.After reading a pulse, the counter is unresponsive to successivepulses until a time interval equal to or greater than its dead time
21、has elapsed.2.1.9 energyit is possible to classify beta emitters by themaximum energy of the particles that they release during theirdisintegration. This energy is generally given in mega-electronvolts, MeV.2.1.10 equivalent (or apparent) atomic number theequivalent atomic number of an alloy or comp
22、ound is theatomic number of an element that has the same backscattercoefficient as the material.2.1.11 half-life, radioactivefor a single radioactive decayprocess, the time required for the activity to decrease by half.2.1.12 saturation thicknessthe minimum thickness of amaterial that produces a bac
23、kscatter that is not changed whenthe thickness is increased. (See also Appendix X1.)2.1.13 sealed source or isotopea radioactive sourcesealed in a container or having a bonded cover, the container orcover being strong enough to prevent contact with and disper-sion of the radioactive material under t
24、he conditions of use andwear for which it was designed.2.1.14 source geometrythe spatial arrangement of thesource, the aperture, and the detector with respect to each other.3. Summary of Test Method3.1 When beta particles impinge upon a material, a certainportion of them is backscattered. This backs
25、catter is essentiallya function of the atomic number of the material.3.2 If the body has a surface coating and if the atomicnumbers of the substrate and of the coating material aresufficiently different, the intensity of the backscatter will bebetween two limits: the backscatter intensity of the sub
26、strateand that of the coating. Thus, with proper instrumentation andif suitably displayed, the intensity of the backscatter can beused for the measurement of mass per unit area of the coating,which, if the density remains the same, is directly proportionalto the thickness.3.3 The curve expressing co
27、ating thickness (mass per unitarea) versus beta backscatter intensity is continuous and can besubdivided into three distinct regions, as shown in Fig. 1. Thenormalized count rate, xn, is plotted on the X-axis, and thelogarithm of the coating thickness, on the Y-axis. In the range0#xn#0.35, the relat
28、ionship is essentially linear. In therange 0.35#xn#0.85, the curve is nearly logarithmic; thismeans that, when drawn on semilogarithmic graph paper, as inFig. 1, the curve approximates a straight line. In the range0.85#xn#1, the relationship is nearly hyperbolic.3.4 Radiation other than the beta ray
29、s are emitted orbackscattered by the coating or substrate, and may be includedin the backscatter measurements. Whenever the term backscat-ter is used in this method, it is to be assumed that reference ismade to the total radiation measured.FIG. 1 Normalized BackscatterB567 98 (Reapproved 2009a)24. S
30、ignificance and Use4.1 The thickness or mass per unit area of a coating is oftencritical to its performance.4.2 For some coating-substrate combinations, the beta back-scatter method is a reliable method for measuring the coatingnondestructively.4.3 The test method is suitable for thickness specifica
31、tionacceptance if the mass per unit area is specified. It is notsuitable for specification acceptance if the coating thickness isspecified and the density of the coating material can vary or isnot known.5. Instrumentation5.1 In general, a beta backscatter instrument will comprise:(1) a radiation sou
32、rce (isotope) emitting primarily beta particleshaving energies appropriate to the coating thickness to bemeasured (see Appendix X2), (2) a probe or measuring systemwith a range of apertures that limit the beta particles to the areaof the test specimen on which the coating thickness is to bemeasured,
33、 and containing a detector capable of counting thenumber of backscattered particles (for example, a Geiger-Mller counter (or tube), and (3) a readout instrument wherethe intensity of the backscatter is displayed. The display, in theform of a meter reading or a digital readout can be: (a)proportional
34、 to the count, ( b) the normalized count, or (c) thecoating thickness expressed either in thickness or mass per unitarea units.6. Factors Affecting the Measuring Accuracy6.1 Counting Statistics:6.1.1 Radioactive disintegration takes place randomly.Thus, during a fixed time interval, the number of be
35、ta particlesbackscattered will not always be the same. This gives rise tostatistical errors inherent to radiation counting. In consequence,an estimate of the counting rate based on a short countinginterval (for example, 5 s) may be appreciably different froman estimate based on a longer counting int
36、erval, particularly ifthe counting rate is low. To reduce the statistical error to anacceptable level, it is necessary to use a counting interval longenough to accumulate a sufficient number of counts.6.1.2 At large total counts, the standard deviation (s) willclosely approximate the square root of
37、the total count, that iss5=X; in 95 % of all cases, the true count will be withinX 6 2s. To judge the significance of the precision, it is oftenhelpful to express the standard deviation as a percentage of thecount, that is, 100=X/X, or 100/=X. Thus, a count of100 000 will give a value ten times more
38、 precise than thatobtained with a count of 1000. Whenever possible, a countinginterval should be chosen that will provide a total count of atleast 10 000, which corresponds to a statistical error of 1 % forthe count rate. It should be noted, however, that a 1 % error inthe count rate can correspond
39、to a much larger percentage errorin the thickness measurement, the relative error depending onthe atomic number spread or ratio between coating andsubstrate materials.6.1.3 Direct-reading instruments are also subject to thesestatistical random errors. However, if these instruments do notpermit the d
40、isplay of the actual counting rate or the standarddeviation, the only way to determine the measuring precision isto make a large number of measurements at the same coatedlocation on the same coated specimen, and calculate thestandard deviation by conventional means.NOTE 1The accuracy of a thickness
41、measurement by beta backscatteris generally poorer than the precision described in 5.1, inasmuch as it alsodepends on other factors that are described below. Methods to determinethe random errors of thickness measurements before an actual measure-ment are available from some manufacturers.6.2 Coatin
42、g and Substrate MaterialsBecause the back-scatter intensity depends on the atomic numbers of the sub-strate and the coating, the repeatability of the measurement willdepend to a large degree on the difference between theseatomic numbers; thus, with the same measuring parameters, thegreater this diff
43、erence, the more precise the measurement willbe. As a rule of thumb, for most applications, the difference inatomic numbers should be at least 5. For materials with atomicnumbers below 20, the difference may be reduced to 25 % ofthe higher atomic number; for materials with atomic numbersabove 50, th
44、e difference should be at least 10 % of the higheratomic number. Most plastics and related organic materials (forexample, photoresists) may be assumed to have an equivalentatomic number close to 6. (Appendix X3 gives atomic numbersof commonly used coating and substrate materials.)6.3 Aperture:6.3.1
45、Despite the collimated nature of the sources used incommercial backscatter instruments, the backscatter recordedby the detector is, nearly always, the sum of the backscatterproduced by the test specimen exposed through the apertureand that of the aperture plate(n). It is, therefore, desirable to use
46、a material with a low atomic number for the construction of theplaten and to select the largest aperture possible. Measuringerrors will be increased if the edges of the aperture opening areworn or damaged, or if the test specimen does not properlycontact these edges.6.3.2 Because the measuring area
47、on the test specimen hasto be constant to prevent the introduction of another variable,namely the geometrical dimensions of the test specimen, it isessential that the aperture be smaller than the coated area of thesurface on which the measurement is made.6.4 Coating Thickness:6.4.1 In the logarithmi
48、c range, the relative measuring erroris nearly constant and has its smallest value.6.4.2 In the linear range, the absolute measuring error,expressed in mass per unit area or thickness, is nearly constant,which means that as the coating thickness decreases, therelative measuring error increases. At o
49、r near xn= 0.35, therelative errors of the linear and logarithmic ranges are about thesame. Thus, the relative error at this point may, for mostpractical purposes, be used to calculate the absolute error overthe linear range.6.4.3 In the hyperbolic range, the measuring error is alwayslarge because a small variation in the intensity of the betabackscatter will produce a large variation in the measuredcoating thickness.6.4.4 For instruments that indicate only backscatter countrate and not thickness directly, the count rate is normallyconverted to a thickness by me
