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Before the fabrication of the models, the computed tomography (CT) data were manipulated to add a series of rulers and markers to the models.
For both combustion models the computed frequency of the thermoacoustic oscillation is close to the experimental value, whereas its amplitude is significantly overestimated by about 15 dB in comparison to measurements.
For the reduced fixed-point models, the computed values are saturated to the maximum representable number on overflow, or to the minimum on underflow; the same input is applied to both models.
To determine the plausibility of the existing models, the computed steady state profiles were compared to the experimentally observed expression profiles.
Although for all models the computed energies and intensities of the electronic transitions are overestimated, both the (N3 /OH–)- and (N3 /OH /H2O -Fe(III)CDO models are predicted to exhibit traN3 /OH /H2O -FeIII CDOant N3– → Fe CT character in the visible spectral region.
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In order to confirm the appropriate turbulence model, the computed results are validated against indigenous experimental data.
For the Laub and Loomis model, the computed maximum allowed variation is tighter than what was obtained with previous multiparametric analysis methods.
Before starting the Latent period, the model computed the duration for each of the subsequent four stages of illness.
When an individual enters the Latent period, the model computed the duration for each of the subsequent four stages of illness.
For an overall comparison of the different models, we computed the sum of the city-specific AIC values.
JC derived the model, computed the real data, run simulation studies, and participated in the writing of the Methods section.
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Justyna Jupowicz-Kozak
CEO of Professional Science Editing for Scientists @ prosciediting.com