1、Designation: E2847 131Standard Test Method forCalibration and Accuracy Verification of Wideband InfraredThermometers1This standard is issued under the fixed designation E2847; the number immediately following the designation indicates the year oforiginal adoption or, in the case of revision, the yea
2、r 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.1NOTETitle corrected editorially in September 2013.1. Scope1.1 This test method covers electronic instruments intendedfor mea
3、surement of temperature by detecting the intensity ofthermal radiation exchanged between the subject of measure-ment and the sensor.1.2 The devices covered by this test method are referred toas infrared thermometers in this document.1.3 The infrared thermometers covered in this test methodare instru
4、ments that are intended to measure temperaturesbelow 1000C, measure thermal radiation over a wide band-width in the infrared region, and are direct-reading in tempera-ture.1.4 This guide covers best practice in calibrating infraredthermometers. It addresses concerns that will help the userperform mo
5、re accurate calibrations. It also provides a structurefor calculation of uncertainties and reporting of calibrationresults to include uncertainty.1.5 Details on the design and construction of infraredthermometers are not covered in this test method.1.6 This test method does not cover infrared thermo
6、metryabove 1000C. It does not address the use of narrowbandinfrared thermometers or infrared thermometers that do notindicate temperature directly.1.7 The values stated in SI units are to be regarded as thestandard. The values given in parentheses are for informationonly.1.8 The values stated in inc
7、h-pound units are to be regardedas standard. The values given in parentheses are mathematicalconversions to SI units that are provided for information onlyand are not considered standard.2. Referenced Documents2.1 ASTM Standards:2E344 Terminology Relating to Thermometry and Hydrom-etryE1256 Test Met
8、hods for Radiation Thermometers (SingleWaveband Type)E2758 Guide for Selection and Use of Wideband, LowTemperature Infrared Thermometers3. Terminology3.1 Definitions of Terms Specific to This Standard:3.1.1 cavity bottom, nthe portion of the cavity radiationsource forming the end of the cavity.3.1.1
9、.1 DiscussionThe cavity bottom is the primary areawhere an infrared thermometer being calibrated measuresradiation.3.1.2 cavity radiation source, na concave shaped geom-etry approximating a perfect blackbody of controlled tempera-ture and defined emissivity used for calibration of radiationthermomet
10、ers.3.1.2.1 DiscussionA cavity radiation source is a subset ofthermal radiation sources.3.1.2.2 DiscussionTo be a cavity radiation source ofpractical value for calibration, at least 90 % of the field-of-viewof a radiation thermometer is expected to be incident on thecavity bottom. In addition, the r
11、atio of the length of the cavityversus the cavity diameter is expected to be greater than orequal to 5:1.3.1.3 cavity walls, nthe inside surfaces of the concaveshape forming a cavity radiation source.3.1.4 customer, nthe individual or institution to whom thecalibration or accuracy verification is be
12、ing provided.3.1.5 distance-to-size ratio (D:S), nsee field-of-view.1This practice is under the jurisdiction ofASTM Committee E20 on TemperatureMeasurement and is the direct responsibility of Subcommittee E20.02 on RadiationThermometry.Current edition approved May 1, 2013. Published July 2013. Origi
13、nally approvedin 2011. Last previous edition approved in 2011 as E284711. DOI: 10.1520/E2847131.2For 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 Docume
14、nt Summary page onthe ASTM website.Copyright ASTM International, 100 Barr Harbor Drive, PO Box C700, West Conshohocken, PA 19428-2959. United States13.1.6 effective emissivity, nthe ratio of the amount ofenergy over a given spectral band exiting a thermal radiationsource to that predicted by Plancks
15、 Law at a given tempera-ture.3.1.7 field-of-view, na usually circular, flat surface of ameasured object from which the radiation thermometer re-ceives radiation. (1)33.1.7.1 DiscussionMany handheld infrared thermometersmanufacturers include distance-to-size ratio (D:S) in theirspecifications. Distan
16、ce-to-size ratio relates to the followingphysical situation: at a given distance (D), the infrared ther-mometer measures a size (S) or diameter, and a certainpercentage of the thermal radiation received by the infraredthermometer is within this size. Field-of-view is a measure ofthe property describ
17、ed by distance-to-size ratio. (1)3.1.8 flatplate radiation source, na planar surface ofcontrolled temperature and defined emissivity used for calibra-tions of radiation thermometers.3.1.8.1 DiscussionA flatplate radiation source is a subsetof thermal radiation sources.3.1.9 measuring temperature ran
18、ge, ntemperature rangefor which the radiation thermometer is designed. (1)3.1.10 purge, na process that uses a dry gas to remove thepossibility of vapor on a measuring surface.3.1.11 radiance temperature, ntemperature of an ideal (orperfect) blackbody radiator having the same radiance over agiven sp
19、ectral band as that of the surface being measured. (2)3.1.12 thermal radiation source, na geometrically shapedobject of controlled temperature and defined emissivity usedfor calibration of radiation thermometers.3.1.13 usage temperature range, ntemperature range forwhich a radiation thermometer is d
20、esigned to be utilized by theend user.4. Summary of Practice4.1 The practice consists of comparing the readout tempera-ture of an infrared thermometer to the radiance temperature ofa radiation source. The radiance temperature shall correspondto the spectral range of the infrared thermometer under te
21、st.4.2 The radiation source may be of two types. Ideally, thesource will be a cavity source having an emissivity close tounity (1.00). However, because the field-of-view of someinfrared thermometers is larger than typical blackbody cavityapertures, a large-area flatplate source may be used for these
22、calibrations. In either case, the traceable measurement of theradiance temperature of the source shall be known, along withcalculated uncertainties.4.3 The radiance temperature of the source shall be trace-able to a national metrology institute such as the NationalInstitute of Standards and Technolo
23、gy (NIST) in Gaithersburg,Maryland or the National Research Council (NRC) in Ottawa,Ontario, Canada.5. Significance and Use5.1 This guide provides guidelines and basic test methodsfor the accuracy verification of infrared thermometers. Itincludes test set-up and calculation of uncertainties. It isin
24、tended to provide the user with a consistent method, whileremaining flexible in the choice of calibration equipment. It isunderstood that the uncertainty obtained depends in large partupon the apparatus and instrumentation used. Therefore, sincethis guide is not prescriptive in approach, it provides
25、 detailedinstruction in uncertainty evaluation to accommodate thevariety of apparatus and instrumentation that may be em-ployed.5.2 This guide is intended primarily for calibrating handheldinfrared thermometers. However, the techniques described inthis guide may also be appropriate for calibrating o
26、ther classesof radiation thermometers. It may also be of help to thosecalibrating thermal imagers.5.3 This guide specifies the necessary elements of the reportof calibration for an infrared thermometer. The requiredelements are intended as a communication tool to help the enduser of these instrument
27、s make accurate measurements. Theelements also provide enough information, so that the results ofthe calibration can be reproduced in a separate laboratory.6. Sources of Uncertainty6.1 Uncertainties are present in all calibrations. Uncertain-ties are underestimated when their effects are underestima
28、tedor omitted. The predominant sources of uncertainty are de-scribed in Section 10 and are listed in Table 1 and Table X1.1of Appendix X1.6.2 Typically, the most prevalent sources of uncertainties inthis method of calibration are: (1) emissivity estimation of thecalibration source, (2) size-of-sourc
29、e of the infraredthermometer, (3) temperature gradients on the radiation source,(4) improper alignment of the infrared thermometer withrespect to the radiation source, (5) calibration temperature ofthe radiation source, (6) ambient temperature and (7) reflectedtemperature. The order of prevalence of
30、 these uncertaintiesmay vary, depending on use of proper procedure and the typeof thermal radiation source used. Depending on the tempera-ture of the radiation source, the calibration method of theradiation source, the optical characteristics of the infraredthermometer and the detector and filter ch
31、aracteristics of the3The boldface numbers in parentheses refer to a list of references at the end ofthis standard.TABLE 1 Components of UncertaintyUncertainty Component Discussion Evaluation MethodSource UncertaintiesU1Calibration Temperature 10.4 10.4.1U2Source Emissivity 10.5 10.2.3, X2.4 (example
32、)U3Reflected Ambient Radiation 10.6 10.2.2, X2.5 (example)U4Source Heat Exchange 10.7 10.7.1U5Ambient Conditions 10.8 10.8.1U6Source Uniformity 10.9 10.9.1Infrared Thermometer UncertaintiesU7Size-of-Source Effect 10.11 Test Methods E1256U8Ambient Temperature 10.12 Appendix X3U9Atmospheric Absorption
33、 10.13 X2.3U10Noise 10.14 10.14.1U11Display Resolution 10.15 10.15.2E2847 1312infrared thermometer, the contribution of these uncertaintiesmay change significantly in the overall uncertainty budget.7. Apparatus7.1 Thermal Radiation Source:7.1.1 There are two different classes of thermal radiationsou
34、rces which can be used for infrared thermometer calibra-tions: a cavity source and a flatplate source. Some sources maybe considered a hybrid of both categories. Each of thesesources has advantages and disadvantages. The cavity sourceprovides a source of radiation that has a more predictableemissivi
35、ty. However, the flatplate source can usually be madeless expensively, and can be made with a diameter largeenough to calibrate infrared thermometers with low distance tosize ratios (D:S).7.1.2 Ideally, the size of the thermal radiation source shouldbe specified by the infrared thermometer manufactu
36、rer. Inmany cases, this information may not be available. In thesecases a field-of-view test should be completed as discussed inE1256. The portion of signal incident on the infrared thermom-eter that does not come from the source should be accountedfor in the uncertainty budget.7.1.3 Cavity Source:7
37、.1.3.1 A cavity source can be constructed in several shapesas shown in Fig. 1. In general, a high length-to-diameter ratio(L:D) or radius-to-diameter ratio (R:D) in the spherical casewill result in a smaller uncertainty. A smaller conical angle will also result in a smaller uncertainty.7.1.3.2 The l
38、ocation of a reference or a control probe, orboth, and the thermal conductivity of the cavity walls areimportant considerations in cavity source construction. Ingeneral, a reference or control probe should be as close aspractical to the center of the area where the infrared thermom-eter will typical
39、ly measure, typically the cavity bottom. If thereis a separation between the location of the reference probe andthe cavity surface, cavity walls with a higher thermal conduc-tivity will result in a smaller uncertainty due to temperaturegradients in this region.7.1.3.3 The walls of the cavity source
40、can be treated inseveral different ways. A painted or ceramic surface willgenerally result in higher emissivity than an oxidized metalsurface. By the same measure an oxidized metal surface willgenerally result in higher emissivity than a non-oxidized metalsurface. In some cases, it may be impossible
41、 to paint the cavitysource surface. This is especially true at high temperatures.7.1.3.4 The effective emissivity of the cavity source shall becalculated to determine the radiance temperature of the cavity.Calculation of effective emissivity is beyond the scope of thisstandard. Determination of effe
42、ctive emissivity can be math-ematically calculated or modeled.7.1.4 Flatplate Source:FIG. 1 Cavity ShapesE2847 13137.1.4.1 A flatplate source is a device that consists of apainted circular or rectangular plate. The emissivity is likely tobe less well defined than with a cavity source. This can bepar
43、tially overcome by performing a radiometric transfer (seeScheme II in 7.3.7) to the flatplate source. However, theradiometric transfer should be carried out with an instrumentoperating over a similar spectral band as the infrared thermom-eter under test.7.1.4.2 A cavity source is the preferred radio
44、metric sourcefor infrared thermometer calibrations. The cavity source hastwo main advantages over a flatplate source. First, the cavitysource has better defined emissivity and an emissivity muchcloser to unity due to its geometric shape. Second, along withthe emissvity being closer to unity, the eff
45、ects of reflectedtemperature are lessened. Temperature uniformity on the flat-plate source may be more of a concern as well. However, aflatplate source has a main advantage over a cavity source. Thetemperature controlled flatplate surface can be much largerthan a typical cavity source opening, allow
46、ing for muchsmaller D:S ratios (greater field-of-view).7.2 Aperture:7.2.1 An additional aperture may not be needed for allcalibrations. An aperture is typically used to control scatter. Ifused, the aperture should be temperature-controlled or reflec-tive. An aperture should be used if recommended by
47、 theinfrared thermometer manufacturer. If an aperture is used forcalibration, this information should be stated in the report ofcalibration. The information that shall be included is theaperture distance, the aperture size, and the measuring dis-tance.Apossible configuration for aperture use is show
48、n in Fig.2.7.2.2 In Fig. 2,dapris the aperture distance. The measuringdistance is shown by dmeas.7.3 Transfer Standard:7.3.1 The thermal radiation source shall be calibrated with atransfer standard traceable to a national metrological institutesuch as the National Institute of Standards and Technolo
49、gy(NIST) or National Research Council (NRC). If a referencethermometer (radiometric or contact) is used during the cali-bration of the unit-under-test, this serves as the calibration ofthe radiation source. In this case, the reference thermometershall have a calibration traceable to a national metrologicalinstitute.7.3.2 This calibration of the thermal radiation source maytake place in the calibration laboratory, or it may be done by athird party calibration laboratory. The interval of these checksis determined by the calibration laboratory. The drift r
