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A global model including all the loop elements and the essential physical processes has been designed, with a sole control parameter for fitting experiments and simulations.
Once the key regions of separation distance and indentation are detected, the physical parameters describing the relevant interactions operating in these regions are extracted making use of regression procedure for fitting experiments to theory.
These observations indicate that the no-nucleotide structure identified by our flexible fitting experiments is at least transiently stable.
Rigid-body fitting experiments using fragments of kinesin X-ray structures indicate that the upper subdomain rotates by much less (∼11°) than the N-terminal subdomain.
The kinetic parameters and rate expressions used in the fitting experiments together with PySCeS and SBML formatted models [ 28] are available in Table 1 or in the Supplementary information.
For the kinetic fitting experiments described in this study, non-linear least squares regression with the Levenberg Marquardt algorithm from SciPy (http://www.scipy.org) was used to fit data to models of the yeast Grx1 and Grx2 systems [ 26].
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We show a fitting experiment comparing the proposed initialization framework with the Viola-Jones face detection framework.
We see evidence of this high heterogeneity with our model-fitting experiments, which always favor the most parameter-rich models (Table 2).
SBSIVisual provides a report view of a parameter-fitting experiment, showing plots of cost function value versus search iteration, and overlays of simulation traces and experimental data.
Figure 3 GAAM fitting initialization experiment.
using a central composite design (CCD), which is a response surface methodology (RS M, was used for the model fitting and experiment optimization of response parameters.
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