ASTM E2729-2009(2015) 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践规程》.pdf
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1、Designation: E2729 09 (Reapproved 2015)Standard 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, 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.1. Scope1.1 This standard outlines the methods that can be used todeconvolve, at least partially, the spectral bandpass diffe
3、rencesof raw spectral data acquired by abridged spectrophotometry.Such differences are introduced because the spectral passbandmust be of significant bandwidth to allow sufficient energy toreach the detector. On the other hand, the spectral data thatshould be being reported is that of a virtual 1-nm
4、 bandwidthspectrum in order to be useful in the CIE method of tristimulusintegration which involves 1-nm summation.1.2 The standard establishes practices for whether, when,and how a bandpass rectification should be made to anyreflectance or transmittance spectrum acquired by abridgedspectrophotometr
5、y.1.3 It is applicable where the shape of the passband istriangular and the bandwidth is equal to the measurementinterval between passbands. Information is provided in Section7 for users when that condition is not satisfactorily met.1.4 This standard does not purport to address all of thesafety conc
6、erns, 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. Referenced Documents2.1 ASTM Standards:2E284 Terminology of AppearanceE308 Prac
7、tice for Computing the Colors of Objects by Usingthe CIE System3. Terminology3.1 DefinitionsFor definition of terms used in thispractice, refer to Terminology E284.3.2 Definitions of Terms Specific to This Standard:3.2.1 virtual 1-nm bandwidth spectrum, nspectral datathat have been corrected by nume
8、rical methods so as to matchas closely as possible a spectrum from the same source but witha putative bandwidth of 1 nm.4. Summary of Practice4.1 The practice assumes that the shape of the passband istriangular and that the bandwidth is equal to the measurementinterval between passbands. This condit
9、ion is thought to be metby a majority of commercial instruments in use in spectropho-tometry and spectrocolorimetry. Under those conditions, themethods of Section 6 are to be utilized to rectify the rawreflectance or transmittance data for its bandpass differencesimmediately upon the return of the d
10、ata to the host computerprogram from the acquiring instrument, or before presentationof the data to the user.5. Significance and Use5.1 Failure to make such a rectification introduces differ-ences from the true value of the spectrum of about 0.02 to 0.4E*abunits. All users are required to make a rec
11、tification ofsuch bandpass differences. It is especially incumbent uponwriters of computer programs whose function it is to acquiresuch spectra from instruments to see that a competent rectifi-cation is implemented in the program before any additionalprocessing of the spectrum, or calculations invol
12、ving thespectrum are accomplished, or before the spectrum is madeavailable to a user.5.2 Legacy measuring systems are explicitly exempted fromany requirements for retrofitting of hardware or software andmay continue to utilize previously accepted methods of makingthe bandwidth rectification.6. Metho
13、dology6.1 The First and Last PassbandsIn the first and lastpassband being rectified, no correction is called for. Thecorrected spectral value Rs,should be set equal to themeasured spectral value Rm,.Rs,15 Rm,1(1)Rs,n5 Rm,n1This practice is under the jurisdiction of ASTM Committee E12 on Color andApp
14、earance and is the direct responsibility of Subcommittee E12.04 on Color andAppearance Analysis.Current edition approved April 1, 2015. Published April 2015. Originallyapproved in 2009. Last previous edition approved in 2009 as E2729 09. DOI:10.1520/E2729-09R15.2For referenced ASTM standards, visit
15、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 onthe ASTM website.Copyright ASTM International, 100 Barr Harbor Drive, PO Box C700, West Conshohocken, PA 19428-2959.
16、 United States1where the subscripts 1 and n refer to the wavelength index ofthe first and last passbands being corrected.6.2 The Second and Next-to-last PassbandsThe secondand next-to-last passbands being rectified are subject to thefollowing correction:Rs,2520.10Rm,111.21Rm,22 0.12Rm,310.01Rm,4(2)R
17、s,n21520.10Rm,n11.21Rm,n212 0.12Rm,n2210.01Rm,n23where the second subscript refers to the wavelength index ofthe bandpass considered.6.3 The Remaining Interior PassbandsThe remaining in-terior passbands are subject to the following five-point rectifi-cation:Rs,i5 0.01Rm,i222 0.12Rm,i2111.22Rm,i2 0.1
18、2Rm,i1110.01Rm,i12(3)where the subscript i is the wavelength index of the passbandbeing corrected and varies over the range of 3 to n2.7. Applicable Bandpass Shapes7.1 The coefficients of the foregoing rectification equationshave been calculated under the assumption that the passbandsare spaced at e
19、qual intervals. The interval is assumed to beequal to the full-width half-height of the passbands. Further,assumption is made that the passbands are triangular in shapeand that the reflectance, or transmittance, functions may becharacterized by a quadratic function in the range of anypassband. These
20、 assumptions are believed to be true for mostinstruments, materials, and measurements known to the Sub-committee with jurisdiction for this practice. Accordingly, theabove correction is among the best practices for making arectification of bandpass differences.7.2 While the underlying theory leading
21、 to the rectificationequations is based on triangular passbands, some relatedbandpass shapes may be adequately rectified by the methods ofthis practice. This is true of Gaussian and Lorentzian functionband shapes, and may be true of instruments with concavediffraction gratings imaged on diode arrays
22、 with more pixelsthan wavelengths being reported. Those passbands are trap-ezoidal in shape.7.3 If the user has specific knowledge as to departures fromthe above assumptions with respect to his particular measure-ment conditions, he may calculate a set of correction coeffi-cients fitting his own cas
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