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PubMedDate not supplied

[Taking account of macromolecule conformation dynamics in the analysis of luminescent probe signals].

A mathematical model of electron excitation energy transport between molecular probes sorbed on the polymeric chain in solution was proposed. The kinetics of the process was described in terms of the conception of stochastic changes in macromolecule conformation. The results of computer simulation and the analytical expressions obtained in the framework of the perturbation theory for the cases of low transfer rate and/or fast conformation motion of the macrochain are presented. A channel of nonlinear deactivation as a result of binary annihilation of closely-spaced excited centers was considered. Expressions for the effective rate of mutual quenching and delayed annihilation fluorescence of the probe were obtained. Time dependencies of typical luminescent signals and parameteric curves of relative fluorescence quantum yield are presented.

Electron Transport↗
PubMed1996

Conformational dynamics in cytochrome P450-substrate interactions.

There now are four known cytochrome P450 crystal structures. Two of these, P450cam and P450eryF, are substrate-bound while P450terp and the heme domain of P450BM-3 are substrate-free. Here we describe a preliminary analysis of the P450BM-3 heme domain complexed with the 16-carbon fatty acid substrate, palmitoleic acid. A comparison of the substrate-free and -bound structures shows that a large conformational change in the substrate access channel accompanies substrate binding. This new information, together with the substrate-bound structures of P450cam and P450eryF, reveals which regions of P450 are the most important in controlling the dynamics of substrate binding and recognition.

Bacterial Proteins↗
PubMed2005

Mosaic energy landscapes of liquids and the control of protein conformational dynamics by glass-forming solvents.

Using recent advances in the Random First-Order Transition (RFOT) Theory of glass-forming liquids, we explain how the molecular motions of a glass-forming solvent distort the protein's boundary and slave some of the protein's conformational motions. Both the length and time scales of the solvent imposed constraints are provided by the RFOT theory. Comparison of the protein relaxation rate to that of the solvent provides an explicit lower bound on the size of the conformational space explored by the protein relaxation. Experimental measurements of slaving of myoglobin motions indicate that a major fraction of functionally important motions have significant entropic barriers.

Chemistry, Physical↗
PubMed2004

Conformational dynamics of the GdmHCl-induced molten globule state of creatine kinase monitored by hydrogen exchange and mass spectrometry.

Our understanding of the mechanism of protein folding can be improved by the characterization of folding intermediate states. Intrinsic tryptophan fluorescence measurements of equilibrium GdmHCl-induced unfolding of MM-CK allow for the construction of a "phase diagram", which shows the presence of five different conformational states, including three partially folded intermediates. However, only three states are detected by using pulsed-labeled H-D exchange analyzed by electrospray ionization mass spectrometry. One of them is the native state, and the two other species are present in proportions strongly dependent on the GdmHCl concentration and denaturation time. The low-mass peak is due to a largely exchange-incompetent state, which has gained only approximately 10 deuteriums more than the native protein. This population of MM-CK molecules has undergone a small conformational change induced by low GdmHCl concentrations. However, this limited change is in itself not sufficient to inactivate the enzyme or is easily reversible. The high-mass peak corresponds to a population of MM-CK that is fully deuterated. The comparison of fluorescence, activity, and H-D exchange measurements shows that the maximally populated intermediate at 0.8 M GdmHCl has the characteristics of a molten globule. It has no activity; it has 55% of its native alpha-helices and a maximum fluorescence emission wavelength of approximately 341 nm, and it binds ANS strongly. However, no protection against exchange is detected under the conditions used in this work. This paradox, the presence of significant residual secondary and tertiary structures detected by optical probes and the total deuteration of its amide protons detected by H-D exchange and mass spectrometry, could be explained by a highly dynamic MM-CK molten globule.

Animals↗
PubMed1996

[Amyloidosis, protein conformation dynamics and neurologic diseases].

The abnormal protein which accumulates in the extracellular space in the central nervous system in Alzheimer's disease and prion diseases could result from similar mechanisms. Many studies have demonstrated that the abnormal protein is resistant to proteolytic agents. This resistance is correlated with a modification in the conformation of the protein, inverting the ratio of alpha and beta helix structures. This change in conformation could be the cause of the central nervous system lesions. The mechanism of the modification in conformation could be related to a process of hydrophobisation of the protein resulting from mutation. A hydrophilic amino acid would be replaced by a hydrophobic amino acid or in sporadic forms, modifications in the environment of the peptide may lead to physical and chemical aggressions. Hydrophobisation of the two proteins could later lead to formation of polymers and then insoluble aggregates with the physical and chemical characteristics of the amyloid substance. Polymerisation could be triggered by the formation of protein dimers which would be, in one case, an endogenous protein, PrP, and in the other exogenous proteins coming from the environment.

Alzheimer Disease↗
PubMed2005

Conformational dynamics of amyloid beta-protein assembly probed using intrinsic fluorescence.

Formation of toxic oligomeric and fibrillar structures by the amyloid beta-protein (Abeta) is linked to Alzheimer's disease (AD). To facilitate the targeting and design of assembly inhibitors, intrinsic fluorescence was used to probe assembly-dependent changes in Abeta conformation. To do so, Tyr was substituted in Abeta40 or Abeta42 at position 1, 10 (wild type), 20, 30, 40, or 42. Fluorescence then was monitored periodically during peptide monomer folding and assembly. Electron microscopy revealed that all peptides assembled readily into amyloid fibrils. Conformational differences between Abeta40 and Abeta42 were observed in the central hydrophobic cluster (CHC) region, Leu17-Ala21. Tyr20 was partially quenched in unassembled Abeta40 but displayed a significant and rapid increase in intensity coincident with the maturation of an oligomeric, alpha-helix-containing intermediate into amyloid fibrils. This process was not observed during Abeta42 assembly, during which small decreases in fluorescence intensity were observed in the CHC. These data suggest that the structure of the CHC in Abeta42 is relatively constant within unassembled peptide and during the self-association process. Solvent accessibility of the Tyr ring was studied using a mixed solvent (dimethyl sulfoxide/water) system. [Tyr40]Abeta40, [Tyr30]Abeta42, and [Tyr42]Abeta42 all were relatively shielded from solvent. Analysis of the assembly dependence of the site-specific intrinsic fluorescence data suggests that the CHC is particularly important in controlling Abeta40 assembly, whereas the C-terminus plays the more significant role in Abeta42 assembly.

Alzheimer Disease↗
PubMed1998

NMR detection of slow conformational dynamics in an endonuclease toxin.

The cytotoxic activity of the secreted bacterial toxin colicin E9 is due to a non-specific DNase housed in the C-terminus of the protein. Double-resonance and triple-resonance NMR studies of the 134-amino acid 15N- and 13C/15N-labelled DNase domain are presented. Extensive conformational heterogeneity was evident from the presence of far more resonances than expected based on the amino acid sequence of the DNase, and from the appearance of chemical exchange cross-peaks in TOCSY and NOESY spectra. EXSY spectra were recorded to confirm that slow chemical exchange was occurring. Unambiguous sequence-specific resonance assignments are presented for one region of the protein, Pro65-Asn72, which exists in two slowly exchanging conformers based on the identification of chemical exchange cross-peaks in 3D 1H-1H-15N EXSY-HSQC, NOESY-HSQC and TOCSY-HSQC spectra, together with C alpha and C beta chemical shifts measured in triple-resonance spectra and sequential NH NOEs. The rates of conformational exchange for backbone amide resonances in this stretch of amino acids, and for the indole NH of either Trp22 or Trp58, were determined from the intensity variation of the appropriate diagonal and chemical exchange cross-peaks recorded in 3D 1H-1H-15N NOESY-HSQC spectra. The data fitted a model in which this region of the DNase has two conformers, NA and NB, which interchange at 15 degrees C with a forward rate constant of 1.61 +/- 0.5 s-1 and a backward rate constant of 1.05 +/- 0.5 s-1. Demonstration of this conformational equilibrium has led to a reappraisal of a previously proposed kinetic scheme describing the interaction of E9 DNase with immunity proteins [Wallis et al. (1995) Biochemistry, 34, 13743-13750 and 13751-13759]. The revised scheme is consistent with the specific inhibitor protein for the E9 DNase, Im9, associating with both the NA and NB conformers of the DNase and with binding only to the NB conformer detected because the rate of dissociation of the complex of Im9 and the NA conformer, NAI. is extremely rapid. In this model stoichiometric amounts of Im9 convert, the E9 DNase is converted wholly into the NBI form. The possibility that cis-trans isomerisation of peptide bonds preceding proline residues is the cause of the conformational heterogeneity is discussed. E9 DNase contains 10 prolines, with two bracketing the stretch of amino acids that have allowed the NA [symbol: see text] NB interconversion to be identified, Pro65 and Pro73. The model assumes that one or both of these can exist in either the cis or trans form with strong Im9 binding possible to only one form.

Amino Acid Sequence↗
PubMed1985

Effect of B-Z transition and nucleic acid structure on the conformational dynamics of bound ethidium dimer measured by hydrogen deuterium exchange kinetics.

Ethidium dimer is shown to bind by intercalation, almost equally well, to the B and Z form of poly[(dG-m5dC)].poly[(dG-m5dC)], whereas the ethidium monomer shows a strong preference for the B form. The hydrogen-deuterium (H-D) exchange kinetics of the ethidium dimer bound to the B and Z form of poly [(dG-m5dC)].poly[(dG-m5dC)] could then be compared. The kinetics of the H-D exchange were strikingly slower when the dye was bound to Z DNA as compared to B DNA. The exchange kinetics were also modified when ethidium dimer was bound to tRNA and to a triple stranded structure. It is proposed that a dynamic fluctuation at the level of the nucleic acid could modulate the dynamic fluctuation at the level of the bound ligand.

DNA↗
PubMed2005

Conformational dynamics of the ligand-binding domain of inward rectifier K channels as revealed by molecular dynamics simulations: toward an understanding of Kir channel gating.

Inward rectifier (Kir) potassium channels are characterized by two transmembrane helices per subunit, plus an intracellular C-terminal domain that controls channel gating in response to changes in concentration of various ligands. Based on the crystal structure of the tetrameric C-terminal domain of Kir3.1, it is possible to build a homology model of the ATP-binding C-terminal domain of Kir6.2. Molecular dynamics simulations have been used to probe the dynamics of Kir C-terminal domains and to explore the relationship between their dynamics and possible mechanisms of channel gating. Multiple simulations, each of 10 ns duration, have been performed for Kir3.1 (crystal structure) and Kir6.2 (homology model), in both their monomeric and tetrameric forms. The Kir6.2 simulations were performed with and without bound ATP. The results of the simulations reveal comparable conformational stability for the crystal structure and the homology model. There is some decrease in conformational flexibility when comparing the monomers with the tetramers, corresponding mainly to the subunit interfaces in the tetramer. The beta-phosphate of ATP interacts with the side chain of K185 in the Kir6.2 model and simulations. The flexibility of the Kir6.2 tetramer is not changed greatly by the presence of bound ATP, other than in two loop regions. Principal components analysis of the simulated dynamics suggests loss of symmetry in both the Kir3.1 and Kir6.2 tetramers, consistent with "dimer-of-dimers" motion of subunits in C-terminal domains of the corresponding Kir channels. This is suggestive of a gating model in which a transition between exact tetrameric symmetry and dimer-of-dimers symmetry is associated with a change in transmembrane helix packing coupled to gating of the channel. Dimer-of-dimers motion of the C-terminal domain tetramer is also supported by coarse-grained (anisotropic network model) calculations. It is of interest that loss of exact rotational symmetry has also been suggested to play a role in gating in the bacterial Kir homolog, KirBac1.1, and in the nicotinic acetylcholine receptor channel.

Adenosine Triphosphate↗