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1.
Figure 2

Figure 2. From: An Extended Guinier Analysis for Intrinsically Disordered Proteins.

Parameterizing α in terms of ν. We plot the relation between α and ν for implict solvent simulations with the ABSINTH model[] for a variety of sequences (see legend). Note that each data point corresponds to a single temperature from the replica exchange simulations of each protein.

Wenwei Zheng, et al. J Mol Biol. ;430(16):2540-2553.
2.
Figure 6

Figure 6. From: An Extended Guinier Analysis for Intrinsically Disordered Proteins.

Correlations between correction coefficient α and structural descriptors. Descriptors include mean squared radius of gyration (a), mean asphericity 〈δ*〉 (b), variance of squared radius of gyration (c) or variance of asphericity σ(δ*) (d) for a series of ensembles selected by fixing the other three valuables. Legends show the corresponding fixed and 〈δ*〉 for the ensembles used.

Wenwei Zheng, et al. J Mol Biol. ;430(16):2540-2553.
3.
Figure 3

Figure 3. From: An Extended Guinier Analysis for Intrinsically Disordered Proteins.

Fit of different models to low-q experimental data. The fit of SAXS data for R17 (black) obtained in 0.58M GdmCl using different approximations, including Guinier analysis (blue, with qmaxRg = 1.1), Debye's equation (red, with qmaxRg = 2.0), and extended Guinier analysis (cyan, with qmaxRg = 2.0). Vertical black lines indicate different values of qRg, using the Rg determined by ensemble fitting, as labelled on top axis.

Wenwei Zheng, et al. J Mol Biol. ;430(16):2540-2553.
4.
Figure 4

Figure 4. From: An Extended Guinier Analysis for Intrinsically Disordered Proteins.

Testing using all-atom MD simulations with explicit solvent. The Rg-s determined from Guinier analysis (blue), Debye's equation (red), and extended Guinier analysis (cyan) are compared with reference values obtained directly from the simulation trajectories. The three columns show the results for fitting ranges qmaxRg = 1.1, 1.3 and 2.0, respectively. In (a) we compare Rg from analysis to the true simulation Rg, and in (b) the scaling exponent ν from analysis with that calculated from the internal distance scaling in the simulations. In (c), we summarize the deviation of inferred Rg from the true value using χ2, RMSE and MSRE.

Wenwei Zheng, et al. J Mol Biol. ;430(16):2540-2553.
5.
Figure 1

Figure 1. From: An Extended Guinier Analysis for Intrinsically Disordered Proteins.

Investigation of fourth order correction term to the Guinier approximation. a) Magnitude of the correction term to Guinier analysis, as a function of . The blue lines show the curve for individual configurations in the ensemble whereas red lines show the ensemble averaged values. Dashed lines show the best fit linear curve with slope α (fitting between 0 ≤ < 4). Legends show the polymer scaling exponent ν determined from internal distance scaling with sequence separation for each ensemble. b) The fitted slope α of curves in (a) plotted as a function of ν. Left column shows R17, middle column ACTR and right column poly-Val.

Wenwei Zheng, et al. J Mol Biol. ;430(16):2540-2553.
6.
Figure 5

Figure 5. From: An Extended Guinier Analysis for Intrinsically Disordered Proteins.

Testing on experimental data for different proteins and denaturation conditions. We show a comparison between the Rg extracted from (a) Guinier analysis, (b), Debye's equation and (c) extended Guinier analysis on different experimental data sets including R17 and ACTR in different denaturant conditions. The corresponding scaling exponent, ν, from extended Guinier analysis is shown in (d). The reference values (grey shaded regions) are from ensembles fitted to both FRET and SAXS experimental data from Ref. []. e) Errors estimated using χ2, RMSE and MSRE for using Guinier analysis with qmaxRg = 1.3 (blue), Debye's equation with qmaxRg = 2.0 (red) and extended Guinier analysis with qmaxRg = 2.0 (cyan). Color code is shown in the legend: qmaxRg used for fitting in (a), (b), (c) and (d); or the method used for interpreting data in (e).

Wenwei Zheng, et al. J Mol Biol. ;430(16):2540-2553.

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