A "structural" water molecule in the family of fatty acid binding proteins

A single water molecule (w135), buried within the structure of rat intestinal fatty acid binding protein (I-FABP), is investigated by NMR, molecular dynamics simulations, and analysis of known crystal structures. An ordered water molecule was found in structurally analogous position in 24 crystal structures of nine different members of the family of fatty acid binding proteins. There is a remarkable conservation of the local structure near the w135 binding site among different proteins from this family. NMR cross-relaxation measurements imply that w135 is present in the I-FABP:ANS (1-sulfonato-8-(1')anilinonaphthalene) complex in solution with the residence time of >300 ps. Mean-square positional fluctuations of w135 oxygen observed in MD simulations (0.18 and 0.13 A2) are comparable in magnitude to fluctuations exhibited by the backbone atoms and result from highly constrained binding pocket as revealed by Voronoi volumes (averages of 27.0 +/- 1.8 A3 and 24.7 +/- 2.2 A3 for the two simulations). Escape of w135 from its binding pocket was observed only in one MD simulation. The escape process was initiated by interactions with external water molecules and was accompanied by large deformations in beta-strands D and E. Immediately before the release, w135 assumed three distinct states that differ in hydrogen bonding topology and persisted for about 15 ps each. Computer simulations suggest that escape of w135 from the I-FABP matrix is primarily determined by conformational fluctuations of the protein backbone and interactions with external water molecules.     

Structure and dynamics of the fatty acid binding cavity in apo rat intestinal fatty acid binding protein.

The structure and dynamics of the fatty acid binding cavity in I-FABP (rat intestinal fatty acid binding protein) were analyzed. In the crystal structure of apo I-FABP, the probe occupied cavity volume and surface are 539+/-8 A3 and 428 A2, respectively (1.4 A probe). A total of 31 residues contact the cavity with their side chains. The side-chain cavity surface is partitioned according to the residue type as follows: 36-39% hydrophobic, 21-25% hydrophilic, and 37-43% neutral or ambivalent. Thus, the cavity surface is neither like a typical protein interior core, nor is like a typical protein external surface. All hydrophilic residues that contact the cavity-with the exception of Asp74-are clustered on the one side of the cavity. The cavity appears to expand its hydrophobic surface upon fatty acid binding on the side opposite to this hydrophilic patch. In holo I-FABP the fatty acid chain interactions with the hydrophilic side chains are mediated by water molecules. Molecular dynamics (MD) simulation of fully solvated apo I-FABP showed global conformational changes of I-FABP, which resulted in a large, but seemingly transient, exposure of the cavity to the external solvent. The packing density of the side chains lining the cavity, studied by Voronoi volumes, showed the presence of two distinctive small hydrophobic cores. The MD simulation predicts significant structural perturbations of the cavity on the subnanosecond time scale, which are capable of facilitating exchange of I-FABP internal water.     

Water dynamics in the large cavity of three lipid-binding proteins monitored by (17)O magnetic relaxation dispersion

Intracellular lipid-binding proteins contain a large binding cavity filled with water molecules. The role played by these water molecules in ligand binding is not well understood, but their energetic and dynamic properties must be important for protein function. Here, we use the magnetic relaxation dispersion (MRD) of the water 17O resonance to investigate the water molecules in the binding cavity of three different lipid-binding proteins: heart fatty acid-binding protein (H-FABP), ileal lipid-binding protein (I-LBP) and intestinal fatty acid-binding protein (I-FABP). Whereas about half of the crystallographically visible water molecules appear to be expelled by the ligand, we find that ligand binding actually increases the number of water molecules within the cavity. At 300 K, the water molecules in the cavity exchange positions on a time-scale of about 1ns and exchange with external water on longer time-scales (0.01-1 micros). Exchange of water molecules among hydration sites within the cavity should be strongly coupled to ligand motion. Whereas a recent MD simulation indicates that the structure of the cavity water resembles a bulk water droplet, the present MRD results show that its dynamics is more than two orders of magnitude slower than in the bulk. These findings may have significant implications for the strength, specificity and kinetics of lipid binding.     

Structural and dynamic roles of permanent water molecules in ligand molecular recognition by chicken liver bile acid binding protein

Chicken liver bile acid binding protein (cL-BABP) crystallizes with water molecules in its binding site. To obtain insights on the role of internal water, we performed two 100 ns molecular dynamics (MD) simulations in explicit solvent for cL-BABP, as apo form and as a complex with two molecules of cholic acid, and analyzed in detail the dynamics properties of all water molecules. The diffusion coefficients of the more persistent internal water molecules are significantly different from the bulk, but similar between the two protein forms. A different number of molecules and a different organization are observed for apo- and holo-cL-BABP. Most water molecules identified in the binding site of the apo-crystal diffuse to the bulk during the simulation. In contrast, almost all the internal waters of the holo-crystal maintain the same interactions with internal sidechains and ligands, which suggests they have a relevant role in protein-ligand molecular recognition. Only in the presence of these water molecules we were able to reproduce, by a classical molecular docking approach, the structure of the complex cL-BABP::cholic acid with a low ligand root mean square deviation (RMSD) with respect to its reference positioning. Literature data reported a conserved pattern of hydrogen bonds between a single water molecule and three amino acid residues of the binding site in a series of crystallized FABP. In cL-BABP, the interactions between this conserved water molecule and the three residues are present in the crystal of both apo- and holo-cL-BABP but are lost immediately after the start of molecular dynamics. Copyright (c) 2008 John Wiley & Sons, Ltd.     

Dynamics of hydration in hen egg white lysozyme

We investigate the hydration dynamics of a small globular protein, hen egg-white lysozyme. Extensive simulations (two trajectories of 9 ns each) were carried out to identify the time-scales and mechanism of water attachment to this protein. The location of the surface and integral water molecules in lysozyme was also investigated. Three peculiar temporal scales of the hydration dynamics can be discerned: two among these, with sub-nanosecond mean residence time, tau(w), are characteristic of surface hydration water; the slower time-scale (tau(w) approximately 2/3 ns) is associated with buried water molecules in hydrophilic pores and in superficial clefts. The computed tau(w) values in the two independent runs fall in a similar range and are consistent with each other, thus adding extra weight to our result. The tau(w) of surface water obtained from the two independent trajectories is 20 and 24 ps. In both simulations only three water molecules are bound to lysozyme for the entire length of the trajectories, in agreement with nuclear magnetic relaxation dispersion estimates. Locations other than those identified in the protein crystal are found to be possible for these long-residing water molecules. The dynamics of the hydration water molecules observed in our simulations implies that each water molecule visits a multitude of residues during the lifetime of its bound with the protein. The number of residues seen by a single water molecule increases with the time-scale of its residence time and, on average, is equal to one only for the water molecules with shorter residence time. Thus, tau(w) values obtained from inelastic neutron scattering and based on jump-diffusion models are likely not to account for the contribution of water molecules with longer residence time.     

The interaction of lipophilic drugs with intestinal fatty acid-binding protein

Intestinal fatty acid-binding protein (I-FABP) is a small protein that binds long-chain dietary fatty acids in the cytosol of the columnar absorptive epithelial cells (enterocytes) of the intestine. The binding cavity of I-FABP is much larger than is necessary to bind a fatty acid molecule, which suggests that the protein may be able to bind other hydrophobic and amphipathic ligands such as lipophilic drugs. Herein we describe the binding of three structurally diverse lipophilic drugs, bezafibrate, ibuprofen (both R- and S-isomers) and nitrazepam to I-FABP. The rank order of affinity for I-FABP determined for these compounds was found to be R-ibuprofen approximately bezafibrate > S-ibuprofen > nitrazepam. The binding affinities were not directly related to aqueous solubility or partition coefficient of the compounds; however, the freely water-soluble drug diltiazem showed no affinity for I-FABP. Drug-I-FABP interaction interfaces were defined by analysis of chemical shift perturbations in NMR spectra, which revealed that the drugs bound within the central fatty acid binding cavity. Each drug participated in a different set of interactions within the cavity; however, a number of common contacts were observed with residues also involved in fatty acid binding. These data suggest that the binding of non-fatty acid lipophilic drugs to I-FABP may increase the cytosolic solubility of these compounds and thereby facilitate drug transport from the intestinal lumen across the enterocyte to sites of distribution and metabolism.     

Molecular dynamics study of water penetration in staphylococcal nuclease

The ionization properties of Lys and Glu residues buried in the hydrophobic core of staphylococcal nuclease (SN) suggest that the interior of this protein behaves as a highly polarizable medium with an apparent dielectric constant near 10. This has been rationalized previously in terms of localized conformational relaxation concomitant with the ionization of the internal residue, and with contributions by internal water molecules. Paradoxically, the crystal structure of the SN V66E variant shows internal water molecules and the structure of the V66K variant does not. To assess the structural and dynamical character of interior water molecules in SN, a series of 10-ns-long molecular dynamics (MD) simulations was performed with wild-type SN, and with the V66E and V66K variants with Glu66 and Lys66 in the neutral form. Internal water molecules were identified based on their coordination state and characterized in terms of their residence times, average location, dipole moment fluctuations, hydrogen bonding interactions, and interaction energies. The locations of the water molecules that have residence times of several nanoseconds and display small mean-square displacements agree well with the locations of crystallographically observed water molecules. Additional, relatively disordered water molecules that are not observed crystallographically were found in internal hydrophobic locations. All of the interior water molecules that were analyzed in detail displayed a distribution of interaction energies with higher mean value and narrower width than a bulk water molecule. This underscores the importance of protein dynamics for hydration of the protein interior. Further analysis of the MD trajectories revealed that the fluctuations in the protein structure (especially the loop elements) can strongly influence protein hydration by changing the patterns or strengths of hydrogen bonding interactions between water molecules and the protein. To investigate the dynamical response of the protein to burial of charged groups in the protein interior, MD simulations were performed with Glu66 and Lys66 in the charged state. Overall, the MD simulations suggest that a conformational change rather than internal water molecules is the dominant determinant of the high apparent polarizability of the protein interior.     

Simulations of apo and holo-fatty acid binding protein: structure and dynamics of protein, ligand and internal water.

Two molecular dynamics simulations of 5 ns each have been carried out for rat intestinal fatty acid binding protein, in apo-form and with bound palmitate. The fatty acid and a number of water molecules are encapsulated in a large interior cavity of the barrel-shaped protein. The simulations are compared to experimental data and analyzed in terms of root mean square deviations, atomic B-factors, secondary structure elements, hydrogen bond patterns, and distance constraints derived from nuclear Overhauser experiments. Excellent agreement is found between simulated and experimental solution structures of holo-FABP, but a number of differences are observed for the apo-form. The ligand in holo-FABP shows considerable displacement after about 1.5 ns and displays significant configurational entropy. A novel computational approach has been employed to identify internal water and to capture exchange pathways. Orifices in the portal and gap regions of the protein, discussed in the experimental literature, have been confirmed as major openings for solvent exchange between the internal cavity and bulk water. A third opening on the opposite side of the barrel experiences significant exchange but it does not provide a pathway for further passage to the central cavity. Internal water is characterized in terms of density distributions, interaction energies, mobility, protein contact times, and water molecule coordination. A number of differences are observed between the apo and holo-forms and related to differences in the protein structure. Solvent inside apo-FABP, for example, shows characteristics of a water droplet, while solvent in holo-FABP benefits from interactions with the ligand headgroup and slightly stronger interactions with protein residues.     

Water molecules and hydrogen-bonded networks in bacteriorhodopsin--molecular dynamics simulations of the ground state and the M-intermediate

Protein crystallography provides the structure of a protein, averaged over all elementary cells during data collection time. Thus, it has only a limited access to diffusive processes. This article demonstrates how molecular dynamics simulations can elucidate structure-function relationships in bacteriorhodopsin (bR) involving water molecules. The spatial distribution of water molecules and their corresponding hydrogen-bonded networks inside bR in its ground state (G) and late M intermediate conformations were investigated by molecular dynamics simulations. The simulations reveal a much higher average number of internal water molecules per monomer (28 in the G and 36 in the M) than observed in crystal structures (18 and 22, respectively). We found nine water molecules trapped and 19 diffusive inside the G-monomer, and 13 trapped and 23 diffusive inside the M-monomer. The exchange of a set of diffusive internal water molecules follows an exponential decay with a 1/e time in the order of 340 ps for the G state and 460 ps for the M state. The average residence time of a diffusive water molecule inside the protein is approximately 95 ps for the G state and 110 ps for the M state. We have used the Grotthuss model to describe the possible proton transport through the hydrogen-bonded networks inside the protein, which is built up in the picosecond-to-nanosecond time domains. Comparing the water distribution and hydrogen-bonded networks of the two different states, we suggest possible pathways for proton hopping and water movement inside bR.     

Water and ion binding around RNA and DNA (C,G) oligomers

The dynamics, hydration, and ion-binding features of two duplexes, the A(r(CG)(12)) and the B(d(CG)(12)), in a neutralizing aqueous environment with 0.25 M added KCl have been investigated by molecular dynamics (MD) simulations. The regular repeats of the same C=G base-pair motif have been exploited as a statistical alternative to long MD simulations in order to extend the sampling of the conformational space. The trajectories demonstrate the larger flexibility of DNA compared to RNA helices. This flexibility results in less well defined hydration patterns around the DNA than around the RNA backbone atoms. Yet, 22 hydration sites are clearly characterized around both nucleic acid structures. With additional results from MD simulations, the following hydration scale for C=G pairs can be deduced: A-DNA相似文献   

Water and urea interactions with the native and unfolded forms of a beta-barrel protein

A fundamental understanding of protein stability and the mechanism of denaturant action must ultimately rest on detailed knowledge about the structure, solvation, and energetics of the denatured state. Here, we use (17)O and (2)H magnetic relaxation dispersion (MRD) to study urea-induced denaturation of intestinal fatty acid-binding protein (I-FABP). MRD is among the few methods that can provide molecular-level information about protein solvation in native as well as denatured states, and it is used here to simultaneously monitor the interactions of urea and water with the unfolding protein. Whereas CD shows an apparently two-state transition, MRD reveals a more complex process involving at least two intermediates. At least one water molecule binds persistently (with residence time >10 nsec) to the protein even in 7.5 M urea, where the large internal binding cavity is disrupted and CD indicates a fully denatured protein. This may be the water molecule buried near the small hydrophobic folding core at the D-E turn in the native protein. The MRD data also provide insights about transient (residence time <1 nsec) interactions of urea and water with the native and denatured protein. In the denatured state, both water and urea rotation is much more retarded than for a fully solvated polypeptide. The MRD results support a picture of the denatured state where solvent penetrates relatively compact clusters of polypeptide segments.     

Molecular dynamics study of conformational changes in human serum albumin by binding of fatty acids

Human serum albumin (HSA) binds with fatty acids under normal physiologic conditions. To date, there is little published information on the tertiary structure of HSA-fatty acid complex in aqueous solution. In the present study, we used molecular dynamics (MD) simulations to elucidate possible structural changes of HSA brought about by the binding of fatty acids. Both unliganded HSA and HSA-fatty acid complex models for MD calculations were constructed based on the X-ray crystal structures. Five myristates (MYRs) were bound in the HSA-fatty acid complex model. In the present MD study, the motion of domains I and III caused by the binding of MYR molecules increased the radius of gyration of HSA. Root-mean-square fluctuations from the MD simulations revealed that the atomic fluctuations of the specific amino acids at drug-binding site I that can regulate the drug-binding affinity were increased by the binding of MYR molecules. Primary internal motions, characterized by the first three principal components, were observed mainly at domains I and III in the principal component analysis for trajectory data. The directional motion projected on the first principal component of unliganded HSA was conserved in HSA-MYR complex as the third principal directional motion with higher frequency. However, the third principal directional motion in unliganded HSA turned into the first principal directional motion with lower frequency in the HSA-MYR complex. Thus, the present MD study provides insights into the possible conformational changes of HSA caused by the binding of fatty acids.     

Mechanism of Interaction between the General Anesthetic Halothane and a Model Ion Channel Protein, III: Molecular Dynamics Simulation Incorporating a Cyanophenylalanine Spectroscopic Probe

A nitrile-derived amino acid, Phe_CN, has been used as an internal spectroscopic probe to study the binding of an inhalational anesthetic to a model membrane protein. The infrared spectra from experiment showed a blue-shift of the nitrile vibrational frequency in the presence of the anesthetic halothane. To interpret the infrared results and explore the nature of the interaction between halothane and the model protein, all-atom molecular dynamics (MD) simulations have been used to probe the structural and dynamic properties of the protein in the presence and absence of one halothane molecule. The frequency shift analyzed from MD simulations agrees well with the experimental infrared results. Decomposition of the forces acting on the nitrile probes demonstrates an indirect impact on the probes from halothane, namely a change of the protein's electrostatic local environment around the probes induced by halothane. Although the halothane remains localized within the designed hydrophobic binding cavity, it undergoes a significant amount of translational and rotational motion, modulated by the interaction of the trifluorine end of halothane with backbone hydrogens of the residues forming the cavity. This dominant interaction between halothane and backbone hydrogens outweighs the direct interaction between halothane and the nitrile groups, making it a good “spectator” probe of the halothane-protein interaction. These MD simulations provide insight into action of anesthetic molecules on the model membrane protein, and also support the further development of nitrile-labeled amino acids as spectroscopic probes within the designed binding cavity.     

Polyene fatty acid interactions with recombinant intestinal and liver fatty acid-binding proteins. Spectroscopic studies

Binding and proximity relationships of fatty acids with recombinant rat liver fatty acid-binding protein (L-FABP) and intestinal fatty acid-binding protein (I-FABP) were studied with absorption and fluorescence spectroscopy. Protein aromatic amino acids were examined in the absence and presence of bound fatty acid. Second derivative absorbance spectroscopy of the apo- and holoproteins suggested that fatty acid binding altered the conformation of L-FABP, but not of I-FABP. Fatty acid binding also blocked the accessibility of L-FABP tyrosine and I-FABP tryptophan to Stern-Volmer quenching by acrylamide, indicating that these amino acids were present in the fatty acid-binding pocket. Forster energy transfer from I-FABP tryptophan to bound cis-parinaric acid resulted in quenching of tryptophan lifetime and appearance of sensitized lifetime of bound cis-parinaric acid. The calculated donor-acceptor distances were 16.9 +/- 0.6 and 19.2 +/- 0.3 A for I-FABP and L-FABP, respectively. Absorbance spectral shifts and ratios of fluorescence excitation maxima indicated that the parinaric acid microenvironment in the fatty acid-binding site of I-FABP was much less polar than that of L-FABP. Parinaric acids displayed similar rotational correlation time and limiting anisotropy when bound to I-FABP and to L-FABP. These results are consistent with a close proximity of bound fatty acids to the tyrosine and tryptophan residues and with immobilization of the polyene fatty acids in the fatty acid-binding site(s) of L-FABP and I-FABP. The two proteins differ in that only L-FABP has two fatty acid-binding sites and appears to undergo significant conformational change upon fatty acid binding.     

Dynamics, hydration, and motional averaging of a loop-gated artificial protein cavity: the W191G mutant of cytochrome c peroxidase in water as revealed by molecular dynamics simulations

Five molecular dynamics simulations of the W191G cavity mutant of cytochrome c peroxidase in explicit water reveal distinct dynamic and hydration behavior depending on the closed or open state of the flexible loop gating the cavity, the binding of (K+ or small molecule) cations, and the system temperature. The conformational spaces sampled by the loop region and by the cavity significantly reduce upon binding. The largest ordering factor on water dynamics is the presence of the K+ ion occupying the gated cavity. Considerable water exchange occurs for the open-gate cavity when no ligand or cation is bound. In all cases, good correspondence is found between the calculated (ensemble-averaged) location of water molecules and the water sites determined by X-ray crystallography experiments. However, our simulations suggest that these sites do not necessarily correspond to the presence of bound water molecules. In fact, individual water molecules may repeatedly exchange within the cavity volume yet occupy on average these water sites. Four major conclusions emerge. First, it seems misleading to interpret the conformation of protein loop regions in terms of single dominant structures. Second, our simulations support the general picture of Pro 190 cis-trans isomerization as a determinant of the loop-opening mechanism. Third, receptor flexibility is fundamental for ligand binding and molecular recognition, and our results suggest its importance for the docking of small compounds to the artificial cavity. Fourth, after validation against the available experimental data, molecular dynamics simulations can be used to characterize the dynamics and exchange of water molecules and ions, providing atomic level and time-dependent information otherwise inaccessible to experiments.     

Dynamics of water molecules buried in cavities of apolipoprotein E studied by molecular dynamics simulations and continuum electrostatic calculations

Molecular dynamics (MD) simulations of several nanoseconds each were used to monitor the dynamic behavior of the five crystal water molecules buried in the interior of the N-terminal domain of apolipoprotein E. These crystal water molecules are fairly well conserved in several apolipoprotein E structures, suggesting that they are not an artifact of the crystal and that they may have a structural and/or functional role for the protein. All five buried crystal water molecules leave the protein interior in the course of the longest simulations and exchange with water molecules from the bulk. The free energies of binding evaluated from the electrostatic binding free energy computed using a continuum model and estimates of the binding entropy changes represent shallow minima. The corresponding calculated residence times of the buried water molecules range from tens of picoseconds to hundreds of nanoseconds, which denote rather short times as for buried water molecules. Several water exchanges monitored in the simulations show that water molecules along the exit/entrance pathway use a relay of H bonds primarily formed with charged residues which helps either the exit or the entrance from or into the buried site. The exit/entrance of water molecules from/into the sites is permitted essentially by local motions of, at most, two side chains, indicating that, in these cases, complex correlated atomic motions are not needed to open the buried site toward the surface of the protein. This provides a possible explanation for the short residence times.     

A fluorescently labeled intestinal fatty acid binding protein. Interactions with fatty acids and its use in monitoring free fatty acids.

The fatty acid-binding protein from rat intestine (I-FABP) has been covalently modified with the fluorescent compound Acrylodan. Acrylodan was found to label Lys27, one of the few amino acid residues found by x-ray diffraction studies to change orientation upon fatty acid (FA) binding to I-FABP. Binding of FA to this Acrylodan-modified I-FABP (ADIFAB) induces a large shift in fluorescence emission wavelength from 432 to 505 nm. As a consequence, the ratio of emission intensities provides a direct measure of the concentration of FA bound to the protein. Binding of FA is well described by single site equilibrium for FA concentrations below the critical micelle concentration. ADIFAB dissociation constants (Kd) determined at 37 degrees C and at concentrations below the critical micelle concentration for oleate, palmitate, linoleate, arachidonate, and linolenate were, respectively, 0.28, 0.33, 0.97, 1.6, and 2.5 microM. The variation of these Kd values with FA molecular species is highly correlated with the solubility of the FA in water, suggesting that all these FA bind with a similar conformation in the I-FABP binding site. The ADIFAB response together with the measured equilibrium constants allows a direct determination of the concentration of long chain free fatty acid (FFA) in the concentration range, depending upon the FA molecular species, between 1 nM and > 20 microM. As an example of its use as a probe to measure FFA levels, ADIFAB is used here to monitor the time course for FFA release from IgE receptor- and ionomycin-activated rat basophilic leukemia (RBL) cells.     

Molecular dynamics simulations of the Apo-, Holo-, and acyl-forms of Escherichia coli acyl carrier protein

Acyl carrier protein (ACP) is an essential co-factor protein in fatty acid biosynthesis that shuttles covalently bound fatty acyl intermediates in its hydrophobic pocket to various enzyme partners. To characterize acyl chain-ACP interactions and their influence on enzyme interactions, we performed 19 molecular dynamics (MD) simulations of Escherichia coli apo-, holo-, and acyl-ACPs. The simulations were started with the acyl chain in either a solvent-exposed or a buried conformation. All four short-chain (< or = C10) and one long-chain (C16) unbiased acyl-ACP MD simulation show the transition of the solvent-exposed acyl chain into the hydrophobic pocket of ACP, revealing its pathway of acyl chain binding. Although the acyl chain resides inside the pocket, Thr-39 and Glu-60 at the entrance stabilize the phosphopantetheine linker through hydrogen bonding. Comparisons of the different ACP forms indicate that the loop region between helices II and III and the prosthetic linker may aid in substrate recognition by enzymes of fatty acid synthase systems. The MD simulations consistently show that the hydrophobic binding pocket of ACP is best suited to accommodate an octanoyl group and is capable of adjusting in size to accommodate chain lengths as long as decanoic acid. The simulations also reveal a second, novel binding mode of the acyl chains inside the hydrophobic binding pocket directed toward helix I. This study provides a detailed dynamic picture of acyl-ACPs that is in excellent agreement with available experimental data and, thereby, provides a new understanding of enzyme-ACP interactions.