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The flame thermo-acoustic behavior was described using the flame transfer function concept.
In the HTC, which existed in 2 consecutive versions, the dog's herding behavior was described using predefined scales typically consisting of 6 classes within each trait.
The aging behavior was described using Struik's aging model by allowing the initial conditions to depend on each sample's previous history.
Under these experimental conditions, the hydrodynamic behavior was described using the Reynolds-averaged Navier Stokes equations and the κ ɛ turbulence model as well as the wall functions based on the universal distribution of velocities for the near-wall region.
This behavior was described using a saturating mathematical expression, which included a phase-function specific fitted power (ρ2) on the dimensionless scattering term; while the fitted values for this parameter were relatively close to unity (range=[1.018 1.152], see Table 1) the model fit quality was significantly increased by fitting the parameter.
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The fluid behavior is described using the perturbed velocity potential.
FSMs are actors whose behavior is described using a finite set of states and transitions between the states.
Binding behavior of MIP was described using Freundlich isotherm.
These phenomena, which are crucial to the subgrade behavior, can be described using FEM models.
This behavior can be described using the well known Beer Lambert law 34, which states that (11) where A λ is the material's absorbance at a specific wavelength, λ, of incoming light, I0 is the intensity of the light before it passes through the sample, and I1 is the intensity of light that remains after passing through the sample.
Physicists have long hoped that these collective behaviors could be described using the ideas and methods of statistical mechanics.
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