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In Figure 2, the obtained GGA frequency shifts of both LO and TO modes were fitted by second-degree polynomials, with a strong positive curvature.
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The distributions of projections along the modes were fit to a Gaussian mixture model through an expectation maximization algorithm.
Data points of the higher A 1 g 2 and the E g 2 mode were fitted with a spline interpolation.
A Max well model with three viscoelastic modes and an equilibrium mode was fitted to the mean of all samples.
Longitudinal models were fit on data from households that completed more than one survey of the same mode.
Although different working-resting modes that were fit for different degenerated models have been predicted in the current study, the external load sustained by the lumbar spine in working and exercising conditions differed.
Therefore 3 parameters representing the mode (peak year) and maximum (peak incidence) and end year of incidence were fitted.
Modes can be fitted readily to recordings of such real objects being struck, and each mode has intuitive control parameters, amplitude frequency, and damping.
The developed mixed mode isotherm was fitted with protein adsorption data obtained for five different proteins on four different mixed mode adsorbents by 96-well microtitre plate high throughput batch experiments on a robotic workstation.
The data were fit to Michaelis Menten equation for the best inhibition mode (competitive, uncompetitive, and noncompetitive) using SigmaPlot.
Sensograms were fit globally with BIAcore T200 analysis using 1 1 Langumuir binding mode.
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