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The percentage of decolorization efficiency of samples has been calculated for the most intense absorption peak at 432 nm as follows [52]: {text{Efficiency }}%, =, 100, left{ {left( {A_{0} -, A_{text{t}} } right)A_{0} } right} (11 where A 0 and A t are initial absorbance and absorbance after irradiation at various time intervals, respectively.
Deviations from the high SSTs occur as two cold snaps, i.e. short periods of extreme climatic deterioration (Table 2; Fig. 2): (1) SSTs from 26.2 °C to 28.2 °C occur between ~ 17.85 Ma and ~ 17.86 Ma (max. range: 18.02 17.59 Myrs); (2) the lowest SST of 24.1 °C for all samples has been calculated for sample HO 450 (~ 17.81 Ma) (max. range: 17.96 17.55 Myrs).
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Finally, the effective diffusivities and activation energy for the drying process of construction gypsum plaster samples have been calculated.
The lattice parameters a for the spinel samples have been calculated by the Holland-Redfern method using a UnitCell 1997 software [33].
In the present work, the reactivity worth of OSMOSE samples have been calculated using the most recent Monte Carlo N Transport code MCNPX using the most recent nuclear cross-section data library ENDF/B-VII.
The cross-link densities of the NR and SWNT/NR samples have been calculated from uniaxial stress strain measurements, and plotted as the function of the amount of added sulfur.
From Figure 2, the numerical results on the weights of different spectral components of Ga 3d and As 3d for pristine and irradiated samples have been calculated, and the ratio of chemically bonded Ga/As as a function of irradiation fluences is presented in Figure 3.
Instead of using a fixed MC sample size, sampling is continued until either a pre-determined number h of values larger than the observed test statistic t i (i.e. extreme MC samples according to our definition) has been obtained (at MC sample size l, say), or until some maximum number n of MC samples have been calculated.
In these databases, gene coexpression data, which are similarities of expression patterns of gene pairs over a number of samples, have been calculated using publicly available gene expression data produced using the Affymetrix GeneChip system, most of which are stored in primary databases such as GEO, TAIR and NASCArray.
The thickness of the sample has been calculated to be below 1 μm.
The hydrogen content of each sample has been calculated from Equation 2. A Raman confocal microscope (Renishaw 2000, Renishaw, Gloucestershire, UK) has been used in the analysis.
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