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Standard Reference Material 2881 - National Institute of Standards ...

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Concentration <strong>of</strong> total polymer to retinoic was held about at the three-quarter point in therange <strong>of</strong> linearity found by Goldschmidt and Guttman. 18 This range was re-checked inpreliminary experiments. In addition, the silver triflouroacetate concentration from the aboverecipe was found to work well for the linear range as long as there was a molar excess <strong>of</strong> silver.This was checked by making measurements at concentrations <strong>of</strong> silver triflouroacetate rangingfrom 25 % to 200 % <strong>of</strong> that value using the 10:70:20 <strong>of</strong> OctylB:ButylA:OctylC gravimetricmixture employed in the instrument optimization experiments 2 and described in section 3.4.Within the noise limits <strong>of</strong> the repeatability <strong>of</strong> the experiment there was no change <strong>of</strong> ratio <strong>of</strong>OctylB/Butyl A or OctylC/ButylA either as a function <strong>of</strong> silver triflouroacetate concentration oras a function <strong>of</strong> the time the experiment was done.8. Data Analysis MethodsThe data for one set <strong>of</strong> linearity experiments require up to two days to collectyielding 35 sets <strong>of</strong> data to analyze. Without automated data analysis methods this canlead to a severe bottleneck in standards production. The automated data analysis programmust identify the peaks (as many as 80 or 100 for a mixture <strong>of</strong> two narrow distributionpolymers), determine the area under each peak, and for these experiments sort the peaksinto series which are identifiable by end group <strong>of</strong> polymer, sum the total area attributableto each series, determine the MMD and the MMD moments <strong>of</strong> each series and computethe apparent gravimetric mass attributable to each series. Since there are five repeats ateach point the programs must also be able to handle these and any other requiredstatistics automatically.The transformation <strong>of</strong> the data time-<strong>of</strong>-flight to mass was done using the BrukerDaltonics Xmass program (version 5.1.0). Peak picking and peak integration wereperformed using the MassSpectator FORTRAN computer code 3-5 developed at NISTfor standards production. MassSpectator makes no assumptions about peak shape andrequires no smoothing or preprocessing <strong>of</strong> the data, a process which has been shown todistort peak area. 3 The algorithm is based on a time-series segmentation routine that25

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