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When the oscillations were compared with ones calculated using the Francis model, the phase lines of the modeled GWs showed agreement with those of the observed oscillations.
The enthalpy porosity method is used to model the phase change in PCM.
In such a model, the phase interactions were taken into account.
In the homogeneous model, the phase holdup is calculated directly by the cumulative production of each phase, whereas in the drift-flux model, the phase holdup is calculated by drift-flux correlations.
In the Wiener phase noise model, the phase changes are mutually independent, zero-mean Gaussian random variables.
The optimum value increases with increasing because more DCT coefficients are needed to model the phase fluctuations when gets larger.
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A single region (continuum) formulation based on the enthalpy method is adopted to model the phase-change problem.
Peleg and Friedlander [12] modeled the phase perturbation using a polynomial phase with constant magnitude.
The first-order phase noise models the phase instabilities of an oscillator signal that results from a phase-locked loop (PLL) circuit.
By modeling the phase of human host infection, we showed that transporter transcript expression profiles of recently transformed schistosomula have two opposing responses to increased glucose concentrations.
Using a two-phase model, the amorphous phase CTE was deduced for the semicrystalline materials.
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