ASTM E2729-2016 Standard Practice for Rectification of Spectrophotometric Bandpass Differences《光谱光度测量的带通差异调整的标准实施规程》.pdf
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1、Designation: E2729 09 (Reapproved 2015)E2729 16Standard Practice forRectification of Spectrophotometric Bandpass Differences1This standard is issued under the fixed designation E2729; 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.1. Scope1.1 This standard outlines the methods that can be used to deconvolve, at least partially, the spectral bandp
3、ass differences ofraw spectral data acquired by abridged spectrophotometry. Such differences are introduced because the spectral passband must beof significant bandwidth to allow sufficient energy to reach the detector. On the other hand, the spectral data that should be beingreported is that of a v
4、irtual 1-nm bandwidth spectrum in order to be useful in the CIE method of tristimulus integration whichinvolves 1-nm summation.1.2 The standard establishes practices for whether, when, and how a bandpass rectification should be made to any reflectanceor transmittance spectrum acquired by abridged sp
5、ectrophotometry.1.3 It is applicable where the shape of the passband is triangular and the bandwidth is equal to the measurement interval betweenpassbands. Information is provided in Section 7 for users when that condition is not satisfactorily met.1.4 This standard does not purport to address all o
6、f the safety concerns, if any, associated with its use. It is the responsibilityof the user of this standard to establish appropriate safety and health practices and determine the applicability of regulatorylimitations prior to use.2. Referenced Documents2.1 ASTM Standards:2E284 Terminology of Appea
7、ranceE308 Practice for Computing the Colors of Objects by Using the CIE System3. Terminology3.1 DefinitionsFor definition of terms used in this practice, refer to Terminology E284.3.2 Definitions of Terms Specific to This Standard:3.2.1 virtual 1-nm bandwidth spectrum, nspectral data that have been
8、corrected by numerical methods so as to match asclosely as possible a spectrum from the same source but with a putative bandwidth of 1 nm.4. Summary of Practice4.1 The practice assumes that the shape of the passband is triangular and that the bandwidth is equal to the measurement intervalbetween pas
9、sbands. This condition is thought to be met by a majority of commercial instruments in use in spectrophotometry andspectrocolorimetry. Under those conditions, the methods of Section 6 are to be utilized to rectify the raw reflectance ortransmittance data for its bandpass differences immediately upon
10、 the return of the data to the host computer program from theacquiring instrument, or before presentation of the data to the user.5. Significance and Use5.1 Failure to make such a rectification introduces differences from the true value of the spectrum of about 0.02 to 0.4 E*abunits. All users are r
11、equired to make a rectification of such bandpass differences. It is especially incumbent upon writers ofcomputer programs whose function it is to acquire such spectra from instruments to see that a competent rectification is1 This practice is under the jurisdiction of ASTM Committee E12 on Color and
12、 Appearance and is the direct responsibility of Subcommittee E12.04 on Color andAppearance Analysis.Current edition approved April 1, 2015Aug. 1, 2016. Published April 2015August 2016. Originally approved in 2009. Last previous edition approved in 20092015 asE2729 09. 09 (2015). DOI: 10.1520/E2729-0
13、9R15.10.1520/E2729-16.2 For referencedASTM standards, visit theASTM website, www.astm.org, or contactASTM Customer Service at serviceastm.org. For Annual Book of ASTM Standardsvolume information, refer to the standards Document Summary page on the ASTM website.This document is not an ASTM standard a
14、nd is intended only to provide the user of an ASTM standard an indication of what changes have been made to the previous version. Becauseit may not be technically possible to adequately depict all changes accurately, ASTM recommends that users consult prior editions as appropriate. In all cases only
15、 the current versionof the standard as published by ASTM is to be considered the official document.Copyright ASTM International, 100 Barr Harbor Drive, PO Box C700, West Conshohocken, PA 19428-2959. United States1implemented in the program before any additional processing of the spectrum, or calcula
16、tions involving the spectrum areaccomplished, or before the spectrum is made available to a user.5.2 Legacy measuring systems are explicitly exempted from any requirements for retrofitting of hardware or software and maycontinue to utilize previously accepted methods of making the bandwidth rectific
17、ation.6. Methodology6.1 The First and Last PassbandsIn the first and last passband being rectified, no correction is called for. The correctedspectral value Rs, should be set equal to the measured spectral value Rm,.Rs,15Rm,1 (1)Rs,n 5Rm,nwhere the subscripts 1 and n refer to the wavelength index of
18、 the first and last passbands being corrected.6.2 The Second and Next-to-last PassbandsThe second and next-to-last passbands being rectified are subject to the followingcorrection:Rs,2520.10Rm,111.21Rm,220.12Rm,310.01Rm,4 (2)Rs,n21520.10Rm,n11.21Rm,n2120.12Rm,n2210.01Rm,n23where the second subscript
19、 refers to the wavelength index of the bandpass considered.6.3 The Remaining Interior PassbandsThe remaining interior passbands are subject to the following five-point rectification:Rs,i 50.01Rm,i2220.12Rm,i2111.22Rm,i 20.12Rm,i1110.01Rm,i12 (3)where the subscript i is the wavelength index of the pa
20、ssband being corrected and varies over the range of 3 to n2.7. Applicable Bandpass Shapes7.1 The coefficients of the foregoing rectification equations have been calculated under the assumption that the passbands arespaced at equal intervals. The interval is assumed to be equal to the full-width half
21、-height of the passbands. Further, assumptionis made that the passbands are triangular in shape and that the reflectance, or transmittance, functions may be characterized by aquadratic function in the range of any passband. These assumptions are believed to be true for most instruments, materials, a
22、ndmeasurements known to the Subcommittee with jurisdiction for this practice. Accordingly, the above correction is among the bestpractices for making a rectification of bandpass differences.7.2 While the underlying theory leading to the rectification equations is based on triangular passbands, some
23、related bandpassshapes may be adequately rectified by the methods of this practice. This is true of Gaussian and Lorentzian function band shapes,and may be true of instruments with concave diffraction gratings imaged on diode arrays with more pixels than wavelengths beingreported. Those passbands ar
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