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For the slowest stimulus speed (5° · s−1), pursuit gain was closest to unity and progressively declined for faster stimulus speeds (10° · s−1 and 30° · s−1).
As seen in Table 2, tumour 2B had the highest T/B ratio among the cold tumours, i.e. closest to unity, and tumours 9A and 9D had the lowest T/B ratios among the hot tumours, i.e. closest to unity.
The isotherm giving an R 2 value closest to unity was deemed to provide the best fit.
By comparing the values of R 2 which is closest to unity, the values of R2 for the adsorption process yielded excellent fits in the following order: pseudo-second order > pseudo-first order > Elovich (Table 9).
The dispersion was checked for every run and the model having a quota between Pearson Chi-Square and the number of the degrees of freedom closest to unity was chosen.
Beyond the burst release, the drug release from both C-GP and C-GP-PEG formulations seemed to follow Higuchi's kinetics for diffusion controlled release since the correlation coefficient for this profile was the closest to unity.
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The representativity factor became closer to unity.
Markstein numbers are probably close to unity.
Good agreement was found at equivalence ratios close to unity.
B is close to unity with the average B value being calculated to be 0.9867.
It is shown that the SDelta can achieve a local minimum condition number close to unity.
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Justyna Jupowicz-Kozak
CEO of Professional Science Editing for Scientists @ prosciediting.com