Concentration Dependent Ion-Protein Interaction Patterns Underlying Protein Oligomerization Behaviours

Salts and proteins comprise two of the basic molecular components of biological materials. Kosmotropic/chaotropic co-solvation and matching ion water affinities explain basic ionic effects on protein aggregation observed in simple solutions. However, it is unclear how these theories apply to proteins in complex biological environments and what the underlying ionic binding patterns are. Using the positive ion Ca²⁺ and the negatively charged membrane protein SNAP25, we studied ion effects on protein oligomerization in solution, in native membranes and in molecular dynamics (MD) simulations. We find that concentration-dependent ion-induced protein oligomerization is a fundamental chemico-physical principle applying not only to soluble but also to membrane-anchored proteins in their native environment. Oligomerization is driven by the interaction of Ca²⁺ ions with the carboxylate groups of aspartate and glutamate. From low up to middle concentrations, salt bridges between Ca²⁺ ions and two or more protein residues lead to increasingly larger oligomers, while at high concentrations oligomers disperse due to overcharging effects. The insights provide a conceptual framework at the interface of physics, chemistry and biology to explain binding of ions to charged protein surfaces on an atomistic scale, as occurring during protein solubilisation, aggregation and oligomerization both in simple solutions and membrane systems.

Computer simulations suggest direct and stable tip to tip interaction between the outer membrane channel TolC and the isolated docking domain of the multidrug RND efflux transporter AcrB

One way by which bacteria achieve antibiotics resistance is preventing drug access to its target molecule for example through an overproduction of multi-drug efflux pumps of the resistance nodulation division (RND) protein super family of which AcrAB-TolC in Escherichia coli is a prominent example. Although representing one of the best studied efflux systems, the question of how AcrB and TolC interact is still unclear as the available experimental data suggest that either both proteins interact in a tip to tip manner or do not interact at all but are instead connected by a hexamer of AcrA molecules. Addressing the question of TolC-AcrB interaction, we performed a series of 100 ns - 1 µs-molecular dynamics simulations of membrane-embedded TolC in presence of the isolated AcrB docking domain (AcrB(DD)). In 5/6 simulations we observe direct TolC-AcrB(DD) interaction that is only stable on the simulated time scale when both proteins engage in a tip to tip manner. At the same time we find TolC opening and closing freely on extracellular side while remaining closed at the inner periplasmic bottleneck region, suggesting that either the simulated time is too short or additional components are required to unlock TolC.

Molecular Dynamics Computer Simulations of Multidrug RND Efflux Pumps

Over-expression of multidrug efflux pumps of the Resistance Nodulation Division (RND) protein super family counts among the main causes for microbial resistance against pharmaceuticals. Understanding the molecular basis of this process is one of the major challenges of modern biomedical research, involving a broad range of experimental and computational techniques. Here we review the current state of RND transporter investigation employing molecular dynamics simulations providing conformational samples of transporter components to obtain insights into the functional mechanism underlying efflux pump-mediated antibiotics resistance in Escherichia coli and Pseudomonas aeruginosa.

Unilateral access regulation: ground state dynamics of the Pseudomonas aeruginosa outer membrane efflux duct OprM

Acting as an efflux duct in the MexA-MexB-OprM multidrug efflux pump, OprM plays a major role in the antibiotic resistance capability of Pseudomonas aeruginosa, trafficking substrates through the outer cell membrane. Whereas the available crystal structures showed restricted OprM access on both ends, the underlying gating mechanism is not yet fully understood. To gain insight into the functional mechanism of OprM access regulation, we conducted a series of five independent, unbiased molecular dynamics simulations, computing 200 ns dynamics samples of the wild-type protein in a phospholipid membrane/150 mM NaCl water environment. On the extracellular side, OprM opens and closes freely under the simulated conditions, suggesting the absence of a gating mechanism on this side of the isolated protein. On the periplasmic side, we observe an opening of the tip regions at Val408 and to a lesser degree Asp416 located 1.5 nm further into the channel, leading to OprM end conformations being up to 3 and 1.4 times, respectively, more open than the asymmetric crystal structure. If our simulations are correct, our findings imply that periplasmic gating involves only the Asp416 region and that in vivo additional components, absent in our simulation, might be required for periplasmic gating if the observed opening trend near Asp416 is not negligible. In addition to that ,we identified in each monomer a previously unreported sodium binding site in the channel interior coordinated by Asp171 and Asp230 whose functional role remains to be investigated.

Porter domain opening and closing motions in the multi-drug efflux transporter AcrB

Acriflavine resistance protein B acts as the active transporter in the multi-drug efflux pump Acriflavine resistance proteins A / B - Tolerance to colicins protein in Escherichia coli. Within the same reaction cycle intermediate all Acriflavine resistance protein B X-ray structures display highly similar conformations of the substrate-recruiting and transporting porter domain. To assess if this structural homogeneity is an intrinsic feature of Acriflavine resistance protein B or stems from other causes we performed a series of six independent, unbiased 100 ns molecular dynamics simulations of membrane-embedded, asymmetric, substrate-free wild type Acriflavine resistance protein B in a 150 mM NaCl solution. We find the porter domain more flexible than previously assumed displaying clear opening and closing motions of the proximal binding pocket (L and T-state) and the exit of the drug transport channels (O-intermediate). Concurrently the hydrophobic binding pocket favors a closed conformation in all three protomers. Our findings suggest that the conformational homogeneity seen in the crystal structures is likely an effect of bound but structurally unresolved substrate. Our simulations further imply that each of the known three reaction cycle intermediates occurs in at least two variants, the Thr676 loop independently regulates porter domain access and likely plays a key role in substrate transport. On a 100 ns time scale we find no evidence supporting the proposed LLL resting state in the absence of substrate. If the proximal binding pocket dynamics have an inhibiting effect on Acriflavine resistance protein B pump activity lowering the life time of substrate-accessible conformations, the observed dynamics could provide a structural explanation for the Acriflavine resistance protein B activity-enhancing effect of the adaptor protein Acriflavine resistance protein A stabilizing PC1 and PC2 subdomain orientations.

Locked on one side only: ground state dynamics of the outer membrane efflux duct TolC

Playing a major role in the expulsion of antibiotics and the secretion of cell toxins in conjunction with inner membrane transporters of three protein superfamilies, the outer membrane channel TolC occurs in at least two states blocking or permitting the passage of substrates. The details of the underlying gating mechanism are not fully understood. Addressing the questions of extracellular access control and periplasmic gating mechanism, we conducted a series of independent, unbiased 150-300 ns molecular dynamics simulations of wild-type TolC in a phospholipid membrane/150 mM NaCl water environment. We find that TolC opens and closes freely on the extracellular side, suggesting the absence of a gating mechanism on this side in the isolated protein. On the periplasmic side, we observe the outer periplasmic bottleneck region adopting in all simulations a conformation more open than the TolC wild-type crystal structures until in one run the successive binding of two sodium ions induces the transition to a conformation more closed than any of the available TolC X-ray structures. Concurrent with a heightened sodium residence probability near Asp374, the inner periplasmic bottleneck region at Asp374 remains closed throughout the simulations unless all NaCl is removed from the system, inducing a reopening of the outer and inner bottleneck. Our findings suggest that TolC is locked only on the periplasmic side in a sodium-dependent manner.

Three ways in, one way out: water dynamics in the trans-membrane domains of the inner membrane translocase AcrB

Powered by proton-motive force, the inner membrane translocase AcrB is the engine of the AcrAB-TolC efflux pump in Escherichia coli. As proton conduction in proteins occurs along hydrogen-bonded networks of polar residues and water molecules, knowledge of the protein-internal water distribution and water-interacting residues allows drawing conclusions to possible pathways of proton conduction. Here, we report a series of 6× 50 ns independent molecular dynamics simulations of asymmetric AcrB embedded in a phospholipid/water environment. Simulating each monomer in its proposed protonation state, we calculated for each trans-membrane domain the average water distribution, identified residues interacting with these waters and quantified each residue's frequency of water hydrogen bond contact. Combining this information we find three possible routes of proton transfer connecting a continuously hydrated region of known key residues in the TMD interior to bulk water by one cytoplasmic and up to three periplasm water channels in monomer B and A. We find that water access of the trans-membrane domains is regulated by four groups of residues in a combination of side chain re-orientations and shifts of trans-membrane helices. Our findings support a proton release event via Arg971 during the C intermediate or in the transition to A, and proton uptake occurring in the A or B state or during a so far unknown intermediate in between B and C where cytoplasmic water access is still possible. Our simulations suggest experimentally testable hypotheses, which have not been investigated so far.

dxTuber: detecting protein cavities, tunnels and clefts based on protein and solvent dynamics

Empty space in a protein structure can provide valuable insight into protein properties such as internal hydration, structure stabilization, substrate translocation, storage compartments or binding sites. This information can be visualized by means of cavity analysis. Numerous tools are available depicting cavities directly or identifying lining residues. So far, all available techniques base on a single conformation neglecting any form of protein and cavity dynamics. Here we report a novel, grid-based cavity detection method that uses protein and solvent residence probabilities derived from molecular dynamics simulations to identify (I) internal cavities, (II) tunnels or (III) clefts on the protein surface. Driven by a graphical user interface, output can be exported in PDB format where cavities are described as individually selectable groups of adjacent voxels representing regions of high solvent residence probability. Cavities can be analyzed in terms of solvent density, cavity volume and cross-sectional area along a principal axis. To assess dxTuber performance we performed test runs on a set of six example proteins representing the three main classes of protein cavities and compared our findings to results obtained with SURFNET, CAVER and PyMol.

Computer simulation of antimicrobial peptides

Naturally occurring and synthetic peptides may be a novel class of clinically useful antibiotics. A large body of experimental data on structure function relationships for such peptides is available, but the molecular mechanism of their action remains elusive in most cases. Computer simulations can give detailed insights into the interactions between peptides and lipid bilayers, at least one crucial step in the antimicrobial mechanism. Here we review recent simulations of antimicrobial peptides and discuss potential future contributions of computer simulations in understanding and ultimately designing antimicrobial peptides.

The distribution and conformation of very long-chain plant wax components in a lipid bilayer

Plant wax contains long-chain alkanes and related components which are transported to the surface of the plant by specialized ABC transporter proteins. Here, we determine the distribution and conformation of three wax components, nonacosane, nonacosan-15-one, and nonacosan-15-ol, using unbiased and umbrella sampling molecular dynamics simulations. The molecules all partitioned to the center of the bilayer, with a free-energy difference of -70 kJ/mol between bulk water and the center of the bilayer for the alkane and -55 kJ/mol for the two more-polar molecules. All of the wax molecules were highly mobile in the bilayer, freely moving between opposite leaflets on a time scale of a few nanoseconds. Nonacosan-15-one and nonacosan-15-ol folded double to expose their hydrophilic group to the solvent, whereas nonacosane alternated between orientations spanning the full bilayer and orientations in the center of the bilayer.

Setting up and running molecular dynamics simulations of membrane proteins

Molecular dynamics simulations have become a popular and powerful technique to study lipids and membrane proteins. We present some general questions and issues that should be considered prior to embarking on molecular dynamics simulation studies of membrane proteins and review common simulation methods. We suggest a practical approach to setting up and running simulations of membrane proteins, and introduce two new (related) methods to embed a protein in a lipid bilayer. Both methods rely on placing lipids and the protein(s) on a widely spaced grid and then 'shrinking' the grid until the bilayer with the protein has the desired density, with lipids neatly packed around the protein. When starting from a grid based on a single lipid structure, or several potentially different lipid structures (method 1), the bilayer will start well-packed but requires more equilibration. When starting from a pre-equilibrated bilayer, either pure or mixed, most of the structure of the bilayer stays intact, reducing equilibration time (method 2). The main advantages of these methods are that they minimize equilibration time and can be almost completely automated, nearly eliminating one time consuming step in MD simulations of membrane proteins.

Simulation of the coupling between nucleotide binding and transmembrane domains in the ATP binding cassette transporter BtuCD

The nucleotide-induced structural rearrangements in ATP binding cassette (ABC) transporters, leading to substrate translocation, are largely unknown. We have modeled nucleotide binding and release in the vitamin B(12) importer BtuCD using perturbed elastic network calculations and biased molecular dynamics simulations. Both models predict that nucleotide release decreases the tilt between the two transmembrane domains and opens the cytoplasmic gate. Nucleotide binding has the opposite effect. The observed coupling may be relevant for all ABC transporters because of the conservation of nucleotide binding domains and the shared role of ATP in ABC transporters. The rearrangements in the cytoplasmic gate region do not provide enough space for B(12) to diffuse from the transporter pore into the cytoplasm, which could suggest that peristaltic forces are needed to exclude B(12) from the transporter pore.

Computer simulations of ABC transporter componentsThis paper is one of a selection of papers published in this Special Issue, entitled CSBMCB — Membrane Proteins in Health and Disease

Current computer simulation techniques provide robust tools for studying the detailed structure and functional dynamics of proteins, as well as their interaction with each other and with other biomolecules. In this minireview, we provide an illustration of recent progress and future challenges in computer modeling by discussing computational studies of ATP-binding cassette (ABC) transporters. ABC transporters have multiple components that work in a well coordinated fashion to enable active transport across membranes. The mechanism by which members of this superfamily execute transport remains largely unknown. Molecular dynamics simulations initiated from high-resolution crystal structures of several ABC transporters have proven to be useful in the investigation of the nature of conformational coupling events that may drive transport. In addition, fruitful efforts have been made to predict unknown structures of medically relevant ABC transporters, such as P-glycoprotein, using homology-based computational methods. The various techniques described here are also applicable to gaining an atomically detailed understanding of the functional mechanisms of proteins in general.

Opening and Closing Motions in the Periplasmic Vitamin B12Binding Protein BtuF†

BtuF is the periplasmic binding protein (PBP) in the vitamin B(12) uptake system in Escherichia coli where it is associated with the ABC transporter BtuCD. When the ligand binds, PBPs generally display large conformational changes, commonly termed the Venus flytrap mechanism. BtuF belongs to a group of PBPs that, on the basis of crystal structures, does not appear to display such behavior. Using 480 ns multicopy molecular dynamics simulations of apo and holo forms of the protein, we investigate the dynamics of BtuF. We find BtuF to be more flexible than previously assumed, displaying clear opening and closing motions which are more pronounced in the apo form. The protein behavior is compatible with a PBP functional model that postulates a closed conformation for the ligand-bound state, whereas the empty form fluctuates between open and closed conformations. Elastic network normal-mode analysis suggests that all BtuF-like PBPs are capable of similar opening and closing motions. It also makes the typical Venus flytrap domain motions a likely common means of how PBP-ABC transporter interaction could occur.

Membrane protein simulations with a united-atom lipid and all-atom protein model: lipid-protein interactions, side chain transfer free energies and model proteins

We have reparameterized the dihedral parameters in a commonly used united-atom lipid force field so that they can be used with the all-atom OPLS force field for proteins implemented in the molecular dynamics simulation software GROMACS. Simulations with this new combination give stable trajectories and sensible behaviour of both lipids and protein. We have calculated the free energy of transfer of amino acid side chains between water and 'lipid-cyclohexane', made of lipid force field methylene groups, as a hydrophobic mimic of the membrane interior, for both the OPLS-AA and a modified OPLS-AA force field which gives better hydration free energies under simulation conditions close to those preferred for the lipid force field. The average error is 4.3 kJ mol(-1) for water-'lipid-cyclohexane' compared to 3.2 kJ mol(-1) for OPLS-AA cyclohexane and 2.4 kJ mol(-1) for the modified OPLS-AA water-'lipid-cyclohexane'. We have also investigated the effect of different methods to combine parameters between the united-atom lipid force field and the united-atom protein force field ffgmx. In a widely used combination, the strength of interactions between hydrocarbon lipid tails and proteins is significantly overestimated, causing a decrease in the area per lipid and an increase in lipid ordering. Using straight combination rules improves the results. Combined, we suggest that using OPLS-AA together with the united-atom lipid force field implemented in GROMACS is a reasonable approach to membrane protein simulations. We also suggest that using partial volume information and free energies of transfer may help to improve the parameterization of lipid-protein interactions and point out the need for accurate experimental data to validate and improve force field descriptions of such interactions.

Water dynamics simulation as a tool for probing proton transfer pathways in a heptahelical membrane protein

The proton transfer pathway in a heptahelical membrane protein, the light-driven proton pump bacteriorhodopsin (BR), is probed by a combined approach of structural analysis of recent X-ray models and molecular dynamics (MD) simulations that provide the diffusion pathways of internal and external water molecules. Analyzing the hydrogen-bond contact frequencies of the water molecules with protein groups, the complete proton pathway through the protein is probed. Beside the well-known proton binding sites in the protein interior-the protonated Schiff base, Asp85 and Asp96, and the H(5)O(2) (+) complex stabilized by Glu204 and Glu194-the proton release and uptake pathways to the protein surfaces are described in great detail. Further residues were identified, by mutation of which the proposed pathways can be verified. In addition the diffusion pathway of water 502 from Lys216 to Asp96 is shown to cover the positions of the intruding waters 503 and 504 in the N-intermediate. The transiently established water chain in the N-state provides a proton pathway from Asp96 to the Schiff base in the M- to N-transition in a Grotthus-like mechanism, as concluded earlier from time-resolved Fourier transform infrared experiments [le Coutre et al., Proc Nat Acad Sci USA 1995;92:4962-4966].

Dynamics of water molecules in the bacteriorhodopsin trimer in explicit lipid/water environment

Protonated networks of internal water molecules appear to be involved in proton transfer in various integral membrane proteins. High-resolution x-ray studies of protein crystals at low temperature deliver mean positions of most internal waters, but only limited information about fluctuations within such H-bonded networks formed by water and residues. The question arises as to how water molecules behave inside and on the surface of a fluctuating membrane protein under more physiological conditions. Therefore, as an example, long-time molecular dynamics simulations of bacteriorhodopsin were performed with explicit membrane/water environment. Based on a recent x-ray model the bacteriorhodopsin trimer was inserted in a fully solvated 16 x 16 1-palmitoyl-2-oleoyl-sn-glycero-3-phosphocholine (POPC)-bilayer patch, resulting in a system of approximately 84,000 atoms. Unrestrained molecular dynamics calculations of 5 ns were performed using the GROMACS package and force field. Mean water densities were computed to describe the anisotropic distribution of internal water molecules. In the whole protein two larger areas of higher water density are identified. They are located between the central proton binding site, the Schiff base, and the extracellular proton release site. Separated by Arg-82 these water clusters could provide a proton release pathway in a Grotthus-like mechanism as indicated by a continuum absorbance change observed during the photocycle by time-resolved Fourier transform infrared spectroscopy. Residues are identified which are H-bonded to the water clusters and are therefore facilitating proton conduction. Their influence on proton transfer via the H-bonded network as indicated by the continuum absorbance change is predicted. This may explain why several site-directed mutations alter the proton release kinetics without a direct involvement in proton transfer.