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Figure S6, tabulated data of the fitted linear optical parameters of the coupled oscillator model.
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The F test of lack of fit describes the variation of the data scattering the fitted model.
In order to assess if the model is appropriate, Fig. 11 a and b display the histogram of the current data and the fitted densities of the GW-N, N, GW-LL, GW-Gu, GW-LN, EWE and WE models.
Additionally, the lack of fit (LOF), which is a variation of the data around the fitted model, was also used to determine the adequacy of the model fit.
Figure 7 displays the histogram of the data and the fitted GEW, BXIIG, BLN and EWP densities.
The survival curves show a good fit of the data, since the fitted models are both within the 95% confidence interval.
Data of the fit indices in Table 2 demonstrate that the lower and higher-order scales of the PedsQL™ 4.0 adolescent self-report and parent proxy-report have good-to-excellent fit within the indices mentioned above.
The histogram of the data and the plots of the fitted densities for some models are displayed in Fig. 6.
Model fits were tested by the Hosmer Lemeshow χ test with the data grouped in percentiles of the fitted values.
The leaching data of nickel fitted the "Ginstling Brounsthein" equation while for cobalt a mixed kinetic model consisting of "spherical geometry" and the "Ginstling Brounsthein" equation was followed.
Most of the fitted data fell within ±20% of the experimental values.
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