Protein Free Energy Landscapes Remodeled by Ligand Binding

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Presentation transcript:

Protein Free Energy Landscapes Remodeled by Ligand Binding Troy C. Messina, David S. Talaga  Biophysical Journal  Volume 93, Issue 2, Pages 579-585 (July 2007) DOI: 10.1529/biophysj.107.103911 Copyright © 2007 The Biophysical Society Terms and Conditions

Figure 1 Glucose modulated fluorescence in GGBP. Contour plots representing the isotropic fluorescence lifetime distributions from globally regularized fitting of a glucose titration at 35°C. The solid symbols represent the parameters from a discrete three-exponential global fit to the same data set, but also including the parallel and perpendicular fluorescence components. The size of the symbols represents the relative amplitude changes of the components. Quantitative populations for all data appear in Fig. 2. Two lifetime distributions (∼1.5 and 4.5ns) are nearly constant with glucose concentration, whereas a third lifetime shifts from ∼250 to 400ps with increasing glucose. Biophysical Journal 2007 93, 579-585DOI: (10.1529/biophysj.107.103911) Copyright © 2007 The Biophysical Society Terms and Conditions

Figure 2 Discrete least-squares data fit. Fluorescence lifetime populations as a function of glucose concentration at 35°C resulting from global least-squares fitting. The inset shows the third lifetime, which is fit locally to each glucose concentration. This lifetime showed isotherm-type behavior with a binding constant of ∼0.2μM. Biophysical Journal 2007 93, 579-585DOI: (10.1529/biophysj.107.103911) Copyright © 2007 The Biophysical Society Terms and Conditions

Figure 3 Fluorescence of three GGBP conformations. The three structures on the right side of the figure illustrate the placement of the acrylodan fluorescent probe on GGBP. The blue and red surface regions emphasize the type of conformational change by their relative alignment. The structures were created from molecular dynamics simulations of 2GBP from the Protein Data Bank and exhibit the closed (top), open (center), and twisted (bottom) structures of GGBP. The graphs directly to the left of the structures show the dependence of the population of each contribution on glucose concentration ([g]=0.0, 0.0, 0.2, 0.5, 1.0, 1.3, 2.5, 4.5, 6.0, 10.0, 45.0μM) and temperature (T=5, 10, 15, 20, 25, 30, 35°C). The population of the open form can be seen to decrease with increasing [g] whereas the population of the closed and twisted forms increases. Biophysical Journal 2007 93, 579-585DOI: (10.1529/biophysj.107.103911) Copyright © 2007 The Biophysical Society Terms and Conditions

Figure 4 Six-state model for GGBP. A model based on the time-correlated fluorescence analysis described in this article. The open (O±), closed (C±), and twisted (T±) structures each exhibit spectroscopically distinguishable apo-GGBP (O⊝, C⊝, T⊝) and holo-GGBP (O⊕, C⊕, T⊕) states. Biophysical Journal 2007 93, 579-585DOI: (10.1529/biophysj.107.103911) Copyright © 2007 The Biophysical Society Terms and Conditions

Figure 5 Free energies of GGBP. (a) Free energy difference between glucose-free and glucose-bound conformations. The apparent free energy is calculated as 〈ΔG〉=−RT ln(Kd). (Inset) The apparent binding constant, Kd, as a function of temperature. (b) The free energy difference between conformational states of apo-GGBP (upper two traces) shows a lower temperature dependence than that of holo-GGBP (lower two traces). Biophysical Journal 2007 93, 579-585DOI: (10.1529/biophysj.107.103911) Copyright © 2007 The Biophysical Society Terms and Conditions