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Association and dissociation rates were determined using a bivalent analyte model for curve fitting.
In this paper, a computationally efficient engineering model for curve squeal in the time-domain is proposed.
In the present paper, a previously developed engineering time-domain model for curve squeal is extended to include the effects of the contact angle and spin creepage.
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Xiang, Y., Wei, H. & Ming, P. A generalized Peierls Nabarro model for curved dislocations and core structures of dislocation loops in Al and Cu.
In this paper, we present a generalized Peierls Nabarro model for curved dislocations.
We extend a recently introduced method for numerically solving partial differential equations on implicit surfaces [M. Bertalmío, L.T. Cheng, S. Osher, G. Sapiro. Variational problems and partial differential equations on implicit surfaces, J. Comput. Phys. 174 (20012001) 759 780] to fourth order PDEs including the Cahn Hilliard equation and a lubrication model for curved surfaces.
Like many other deformable models such as snakes and active contours (Kass et al., 1987; Xu and Prince, 1998), we define an energy model for a curve and seek the curve that minimizes energy.
This background activity was then accounted for by including a constant term in the model used for curve fitting.
Baty and Delignette-Muller [ 4] found that Baranyi was the best curve-fitting model for most curves, although they noted that the intermodel variability was frequently minor comparing to the imprecision of the parameter estimates, due to the low quantity and quality of the data used to build the growth curves.
They tried to fit the experimental data to fixed-bed model for breakthrough curve.
The advantages of the unified state model for load curve smoothing control primarily include three parts.
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