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Table 6 Upper part: Results of the pairwise comparisons by fitting Eqs.
Fitting eqs.
The cited quantities ξ r, A i, β i, p i can be related to reality by fitting eqs. 5 and 6 to experimental data.
These are then interpolated across the DCS timepoints and used in fitting Eqs.
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We estimate ten temperatures for an interference fringe image by fitting Eq. (1) to the observed ten fringes.
The thick lines are regression lines computed by fitting Eq. (2) to the average energy release rates.
Finally, the B value was acquired by fitting Eq. (1) to the envelope using a least-squares method.
For each band, we estimated coda Q by fitting Eq. (1) and averaging over three components at each station using the logarithmic value of (Q_{text{C}}^{ - 1}).
The average noise component that remains after fitting Eq. (4) to the radial residuals of the detected limb points is small enough to be negligible relative to σ.
We obtained the parameters (lambda = 10.37), (mu = 2.03) and (sigma = 1.12) by fitting Eq. (3) to the book's cumulative sales, the fit being shown in Fig. 10(C), trailing closely the real sales pattern ((R^{2}=0.99)).
We extract the relative permittivities (epsilon_{mathrm{r}}) from Eq. (2) and the loss tangent tanδ from fitting Eq. (5) to the measured (Q_{mathrm{i}}(nu)) for each coaxial cable (Table 2).
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