Biomedical subjects

Ran Friedman

Publications and source records attributed to Ran Friedman.

10 recordsLinked to original sources

PubMed2006

A molecular dynamics study and free energy analysis of complexes between the Mlc1p protein and two IQ motif peptides.

The Mlc1p protein from the budding yeast Saccharomyces cerevisiae is a Calmodulin-like protein, which interacts with IQ-motif peptides located at the yeast's myosin neck. In this study, we report a molecular dynamics study of the Mlc1p-IQ2 protein-peptide complex, starting with its crystal structure, and investigate its dynamics in an aqueous solution. The results are compared with those obtained by a previous study, where we followed the solution structure of the Mlc1p-IQ4 protein-peptide complex by molecular dynamics simulations. After the simulations, we performed an interaction free-energy analysis using the molecular mechanics Poisson-Boltzmann surface area approach. Based on the dynamics of the Mlc1p-IQ protein-peptide complexes, the structure of the light-chain-binding domain of myosin V from the yeast S. cerevisiae is discussed.

Amino Acid Motifs↗

PubMed2006

Molecular dynamics study of a calmodulin-like protein with an IQ peptide: spontaneous refolding of the protein around the peptide.

The Calmodulin (CaM) is a small (16.7 kDa), highly acidic protein that is crucial to all eukaryotes by serving as a prototypical calcium sensor. In the present study, we investigated, through molecular dynamics simulations, the dynamics of a complex between the Mlc1p protein, which is a CaM-like protein, and the IQ4 peptide. This protein-peptide interaction is of high importance because IQ motifs are widely distributed among different kinds of CaM-binding proteins. The Mlc1p-IQ4 complex, which had been resolved by crystallography to 2.1 A, confers to a Ca(+2)-independent stable structure. During the simulations, the complex undergoes a complicated modulation process, which involves bending of the angles between the alpha-helices of the protein, breaking of the alpha-helical structure of the IQ4 peptide into two sections, and formation of new contact points between the protein and the peptide. The dynamics of the process consist of fast sub picosecond events and much slower ones that take a few nanoseconds to completion. Our study expands the information embedded in the crystal structure of the Mlc1p-IQ4 complex by describing its dynamic behavior as it evolves from the crystal structure to a form stable in solution. The article shows that careful application of molecular dynamics simulations can be used for extending the structural information presented by the crystal structure, thereby revealing the dynamic configuration of the protein in its physiological environment.

Algorithms↗

PubMed2006

A molecular dynamics study of the effect of Ca2+ removal on calmodulin structure.

Calmodulin is a small (148 residues), ubiquitous, highly-conserved Ca(2+) binding protein serving as a modulator of many calcium-dependent processes. In this study, we followed, by means of molecular dynamics, the structural stability of the protein when one of its four bound Ca(2+) ions is removed, and compared it to a simulation of the fully Ca(2+) bound protein. We found that the removal of a single Ca(2+) ion from the N-lobe of the protein, which has a lower affinity for the ion, is sufficient to initiate a considerable structural rearrangement. Although the overall structure of the fully 4 Ca(2+) bound protein remained intact in the extended conformation, the Ca(2+)-removed protein changed its conformation into a compact state. The observation that the 3 Ca(2+) loaded protein assumes a compacted solution state is in accord with experimental observation that the NSCP protein, which binds only three Ca(2+) ions, is natively in a compact state. Examination of the folding dynamics reveals a cooperation between the C-lobe, N-lobe, and the interdomain helix that enable the conformation change. The forces driving this conformational change are discussed.

Animals↗

PubMed2006

The mechanism of proton transfer between adjacent sites on the molecular surface.

The surface of a protein, or a membrane, is spotted with a multitude of proton binding sites, some of which are only few A apart. When a proton is released from one site, it propagates through the water by a random walk under the bias of the local electrostatic potential determined by the distribution of the charges on the protein. Eventually, the released protons are dispersed in the bulk, but during the first few nanoseconds after the dissociation, the protons can be trapped by encounter with nearby acceptor sites. While the study of this reaction on the surface of a protein suffers from experimental and theoretical difficulties, it can be investigated with simple model compounds like derivatives of fluorescein. In the present study, we evaluate the mechanism of proton transfer reactions that proceed, preferentially, inside the Coulomb cage of the dye molecules. Kinetic analysis of the measured dynamics reveals the role of the dimension of the Coulomb cage on the efficiency of the reaction and how the ordering of the water molecules by the dye affects the kinetic isotope effect.

Binding Sites↗

PubMed2005

Fatty acid binding proteins: same structure but different binding mechanisms? Molecular dynamics simulations of intestinal fatty acid binding protein.

Fatty acid binding proteins (FABPs) carry fatty acids (FAs) and other lipids in the cellular environment, and are thus involved in processes such as FA uptake, transport, and oxidation. These proteins bind either one or two ligands in a binding site, which appears to be inaccessible from the bulk. Thus, the entry of the substrate necessitates a conformational change, whose nature is still unknown. A possible description of the ligand binding process is given by the portal hypothesis, which suggests that the FA enters the protein through a dynamic area known as the portal region. On the other hand, recent simulations of the adipocyte lipid binding protein (ALBP) suggested a different entry site (the alternative portal). In this article, we discuss molecular dynamics simulations of the apo-intestinal-FABP (I-FABP) in the presence of palmitate molecule(s) in the simulation box. The simulations were carried out to study whether the FA can enter the protein during the simulations (as in the ALBP) and where the ligand entry site is (the portal region, the alternative portal or a different domain). The analysis of the simulations revealed a clear difference between the ALBP and the I-FABP. In the latter case, the palmitate preferentially adsorbed to the portal region, which was more mobile than the rest of the protein. However, no ligand entry was observed in the multi-nanosecond-long simulations, in contrast to ALBP. These findings suggest that, although the main structural motif of the FABPs is common, the fine details of each individual protein structure grossly modulate its reactivity.

Adsorption↗

PubMed2005

Application of classical molecular dynamics for evaluation of proton transfer mechanism on a protein.

Proton transfer reactions on surfaces are prevalent in biology, chemistry and physics. In the present study, we employed classical Molecular Dynamics simulations to search for the presence of transient configurations that enable proton transfer, or proton sharing, between adjacent carboxylate groups on the protein surface. The results demonstrate that, during random fluctuations of the residues on the surface, there are repeated situations in which nearby carboxylates either share a common proton through a hydrogen bond, or are connected by a few water molecules that form conducting networks. These networks do not extend out of the common Coulomb cage of the participating residues and the lifetimes of the bridged structures are sufficiently long to allow passage of a proton between the carboxylates. The detection of domains capable of supporting a rapid proton transfer on a protein supports the notion that clusters of carboxylates are the operative elements of proton collecting antennae, as in bacteriorhodopsin, cytochrome c oxidase or the photosynthetic reaction center.

Aspartic Acid↗

PubMed2005

The mechanism of proton transfer between adjacent sites exposed to water.

The surface of a protein, or a membrane, is spotted with a multitude of proton-binding sites, some of which are only a few angstroms apart. When a proton is released from one site, it propagates through the water by a random walk under the bias of the local electrostatic potential determined by the distribution of the charges on the protein. Some of the released protons disperse into the bulk, but during the first few nanoseconds, the released protons can be trapped by encounter with nearby acceptor sites. This process resembles a scenario which corresponds with the time-dependent Debye-Smoluchowski equation. In the present study, we investigated the mechanism of proton transfer between sites that are only a few angstroms apart, using as a model the proton exchange between sites on a small molecule, fluorescein, having two, spectrally distinguishable, proton-binding sites. The first site is the oxyanion on the chromophore ring structure. The second site is the carboxylate moiety on the benzene ring of the molecule. Through our experiments, we were able to reconstruct the state of protonation at each site and the velocity of proton transfer between them. The fluorescein was protonated by a few nanosecond long proton pulse under specific conditions that ensured that the dye molecules would be protonated only by a single proton. The dynamics of the protonation of the chromophore were measured under varying initial conditions (temperature, ionic strength, and different solvents (H(2)O or D(2)O)), and the velocity of the proton transfer between the two sites was extracted from the overall global analysis of the signals. The dynamics of the proton transfer between the two proton-binding sites of the fluorescein indicated that the efficiency of the site-to-site proton transfer is very sensitive to the presence of the screening electrolyte and has a very high kinetic isotope effect (KIE = 55). These two parameters clearly distinguish the mechanism from proton diffusion in bulk water. The activation energy of the reaction (E(a) = 11 kcal mol(-1)) is also significantly higher than the activation energy for proton dissociation in bulk water (E(a) approximately 2.5 kcal mol(-1)). These observations are discussed with respect to the effect of the solute on the water molecules located within the solvation layer.

Anions↗

PubMed2005

Molecular dynamics of a protein surface: ion-residues interactions.

Time-resolved measurements indicated that protons could propagate on the surface of a protein or a membrane by a special mechanism that enhanced the shuttle of the proton toward a specific site. It was proposed that a suitable location of residues on the surface contributes to the proton shuttling function. In this study, this notion was further investigated by the use of molecular dynamics simulations, where Na(+) and Cl(-) are the ions under study, thus avoiding the necessity for quantum mechanical calculations. Molecular dynamics simulations were carried out using as a model a few Na(+) and Cl(-) ions enclosed in a fully hydrated simulation box with a small globular protein (the S6 of the bacterial ribosome). Three independent 10-ns-long simulations indicated that the ions and the protein's surface were in equilibrium, with rapid passage of the ions between the protein's surface and the bulk. However, it was noted that close to some domains the ions extended their duration near the surface, thus suggesting that the local electrostatic potential hindered their diffusion to the bulk. During the time frame in which the ions were detained next to the surface, they could rapidly shuttle between various attractor sites located under the electrostatic umbrella. Statistical analysis of the molecular dynamics and electrostatic potential/entropy consideration indicated that the detainment state is an energetic compromise between attractive forces and entropy of dilution. The similarity between the motion of free ions next to a protein and the proton transfer on the protein's surface are discussed.

Amino Acids↗

PubMed2005

Molecular dynamics simulations of the adipocyte lipid binding protein reveal a novel entry site for the ligand.

The adipocyte lipid binding protein (ALBP) binds fatty acids (FA) in a cavity that is inaccessible from the bulk. Therefore, the penetration of the FA necessitates conformational changes whose nature is still unknown. It was suggested that the lipid first enters through a "portal region" which consists of the alphaII helix and the adjacent tight turns. The initial event in the ligand binding must be the interaction of the lipid with the protein surface. To analyze this interaction, we have carried out three molecular dynamics simulations of the apo-ALBP, with a palmitate ion initially located at different positions near the protein surface. The simulation indicated that the ligand could adsorb to the protein in more than one location. Yet, in one case, the ligand managed to penetrate the protein by entering a newly formed cavity some 10 A deep. The entry site is located near the N-terminus, at the junction between the loops connecting the beta-strands. Further progression of the penetration seems to be arrested by the need for desolvation of the COOH end of the headgroup. Evolutionary analysis showed that amino acids in this entry site are well conserved. On the basis of these observations, we suggest that the ligand may enter the protein from a site other than the portal region. Furthermore, the rate-limiting step is proposed to be the desolvation of the FA polar headgroup.

Adipocytes↗

PubMed2003

The role of small intraprotein cavities in the catalytic cycle of bacteriorhodopsin.

The last phase of the proton transfer cycle of bacteriorhodopsin calls for a passage of a proton from D38 to D96. This reaction utilizes a narrow shaft approximately 10-A long that connects the two carboxylates that cross through a very hydrophobic domain. As the shaft is too narrow to be permanently hydrated, there are two alternatives for the proton propagation into the channel. The proton may propagate through the shaft without solvation at the expense of a high electrostatic barrier; alternatively, the shaft will expand to accommodate some water molecules, thus lowering the Born energy for the insertion of the charge into the protein (B. Schätzler, N. A. Dencher, J. Tittor, D. Oesterhelt, S. Yaniv-Checover, E. Nachliel, and G. Gutman, 2003, BIOPHYS: J. 84:671-686). A comparative study of nine published crystal-structures of bacteriorhodopsin identified, next to the shaft, microcavities in the protein whose position and surrounding atoms are common to the reported structures. Some of the cavities either shrink or expand during the photocycle. It is argued that the plasticity of the cavities provides a working space needed for the transient solvation of the shaft, thus reducing the activation energy necessary for the solvation of the shaft. This suggestion is corroborated by the recent observations of Klink et al. (B. U. Klink, R. Winter, M. Engelhard, and I. Chizhov, 2002, BIOPHYS: J. 83:3490-3498) that the late phases of the photocycle (tau >/=1 ms) are strongly inhibited by external pressure.

Bacteriorhodopsins↗