Dynamics of fd coat protein in the bacteriophage

The dynamics of the coat protein in fd bacteriophage are described with solid-state 15N and 2H NMR experiments. The virus particles and the coat protein subunits are immobile on the time scales of the 15N chemical shift anisotropy (10(3) Hz) and 2H quadrupole (10(6) Hz) interactions. Previously we have shown that the Trp-26 side chain is immobile, that the two Tyr and three Phe side chains undergo only rapid twofold jump motions about their C beta-C gamma bond axis [Gall, C. M., Cross, T. A., DiVerdi, J. A., & Opella, S. J. (1982) Proc. Natl. Acad. Sci. U.S.A. 79, 101-105], and that most of the backbone peptide linkages are highly constrained but do undergo rapid small amplitude motions [Cross, T. A., & Opella, S. J. (1982) J. Mol. Biol. 159, 543-549] in the coat protein subunits in the virus particles. In this paper, we demonstrate that the four N-terminal residues of the coat protein subunits are highly mobile, since both backbone and side-chain sites of these residues undergo large amplitude motions that are rapid on the time scales of the solid-state NMR experiments. In addition, the dynamics of the methyl-containing aliphatic residues Ala, Leu, Val, Thr, and Met are analyzed. Large amplitude jump motions are observed in nearly all of these side chains even though, with the exception of the N-terminal residue Ala-1, their backbone peptide linkages are highly constrained. The established information about the dynamics of the structural form of fd coat protein in the virus particle is summarized qualitatively.(ABSTRACT TRUNCATED AT 250 WORDS)     

Comparison of the dynamics of the membrane-bound form of fd coat protein in micelles and in bilayers by solution and solid-state nitrogen-15 nuclear magnetic resonance spectroscopy

Solid-state and solution 15N nuclear magnetic resonance experiments on uniformly and specifically 15N labeled coat protein in phospholipid bilayers and in detergent micelles are used to describe the dynamics of the membrane-bound form of the protein. The residues in the N- and C-terminal portions of the coat protein in both phospholipid bilayers and in detergent micelles are mobile, while those in the hydrophobic midsection are immobile. There is evidence for a gradient of mobility in the C-terminal region of the coat protein in micelles; at 25 degrees C only the last two residues are mobile on the 10(9)-Hz timescale, while the last six to eight residues appear to be mobile on slower timescales and highly mobile at higher temperatures. Since all of the C-terminal residues are immobile in the virus particles, the mobility of these residues in the membrane-bound form of the protein may be important for the formation of protein-DNA interactions in the assembly process.     

Structure and dynamics of the Pf1 filamentous bacteriophage coat protein in micelles

The major coat protein of filamentous bacteriophage adopts its membrane-bound conformation in detergent micelles. High-resolution 1H and 15N NMR experiments are used to characterize the structure and dynamics of residues 30-40 in the hydrophobic midsection of Pf1 coat protein in sodium dodecyl sulfate micelles. Uniform and specific-site 15N labels enable the immobile backbone sites to be identified by their 1H/15N heteronuclear nuclear Overhauser effect and allow the assignment of 1H and 15N resonances. About one-third of the amide N-H protons in the protein undergo very slow exchange with solvent deuterons, which is indicative of sites in highly structured environments. The combination of results from 1H/15N heteronuclear correlation, 1H homonuclear correlation, and 1H homonuclear Overhauser effect experiments assigns the resonances to specific residues and demonstrates that residues 30-40 of the coat protein have a helical secondary structure.     

Structure and Dynamics of the Membrane-Bound Form of Pf1 Coat Protein: Implications of Structural Rearrangement for Virus Assembly

The three-dimensional structure of the membrane-bound form of the major coat protein of Pf1 bacteriophage was determined in phospholipid bilayers using orientation restraints derived from both solid-state and solution NMR experiments. In contrast to previous structures determined solely in detergent micelles, the structure in bilayers contains information about the spatial arrangement of the protein within the membrane, and thus provides insights to the bacteriophage assembly process from membrane-inserted to bacteriophage-associated protein. Comparisons between the membrane-bound form of the coat protein and the previously determined structural form found in filamentous bacteriophage particles demonstrate that it undergoes a significant structural rearrangement during the membrane-mediated virus assembly process. The rotation of the transmembrane helix (Q16-A46) around its long axis changes dramatically (by 160°) to obtain the proper alignment for packing in the virus particles. Furthermore, the N-terminal amphipathic helix (V2-G17) tilts away from the membrane surface and becomes parallel with the transmembrane helix to form one nearly continuous long helix. The spectra obtained in glass-aligned planar lipid bilayers, magnetically aligned lipid bilayers (bicelles), and isotropic lipid bicelles reflect the effects of backbone motions and enable the backbone dynamics of the N-terminal helix to be characterized. Only resonances from the mobile N-terminal helix and the C-terminus (A46) are observed in the solution NMR spectra of the protein in isotropic q > 1 bicelles, whereas only resonances from the immobile transmembrane helix are observed in the solid-state ¹H/¹⁵N-separated local field spectra in magnetically aligned bicelles. The N-terminal helix and the hinge that connects it to the transmembrane helix are significantly more dynamic than the rest of the protein, thus facilitating structural rearrangement during bacteriophage assembly.     

Structure and dynamics of a membrane protein in micelles from three solution NMR experiments

Three solution NMR experiments on a uniformly ¹⁵N labeled membrane protein in micelles provide sufficient information to describe the structure, topology, and dynamics of its helices, as well as additional information that characterizes the principal features of residues in terminal and inter-helical loop regions. The backbone amide resonances are assigned with an HMQC-NOESY experiment and the backbone dynamics are characterized by a ¹H-¹⁵N heteronuclear NOE experiment, which clearly distinguishes between the structured helical residues and the more mobile residues in the terminal and interhelical loop regions of the protein. The structure and topology of the helices are described by Dipolar waves and PISA wheels derived from experimental measurements of residual dipolar couplings (RDCs) and residual chemical shift anisotropies (RCSAs). The results show that the membrane-bound form of Pf1 coat protein has a 20-residue trans-membrane hydrophobic helix with an orientation that differs by about 90° from that of an 8-residue amphipathic helix. This combination of three-experiments that yields Dipolar waves and PISA wheels has the potential to contribute to high-throughput structural characterizations of membrane proteins.     

Structure of the coat protein in Pf1 bacteriophage determined by solid-state NMR spectroscopy

The atomic resolution structure of Pf1 coat protein determined by solid-state NMR spectroscopy of magnetically aligned filamentous bacteriophage particles in solution is compared to the structures previously determined by X-ray fiber and neutron diffraction, the structure of its membrane-bound form, and the structure of fd coat protein. These structural comparisons provide insights into several biological properties, differences between class I and class II filamentous bacteriophages, and the assembly process. The six N-terminal amino acid residues adopt an unusual "double hook" conformation on the outside of the bacteriophage particle. The solid-state NMR results indicate that at 30 degrees C, some of the coat protein subunits assume a single, fully structured conformation, and some have a few mobile residues that provide a break between two helical segments, in agreement with structural models from X-ray fiber and neutron diffraction, respectively. The atomic resolution structure determined by solid-state NMR for residues 7-14 and 18-46, which excludes the N-terminal double hook and the break between the helical segments, but encompasses more than 80% of the backbone including the distinct kink at residue 29, agrees with that determined by X-ray fiber diffraction with an RMSD value of 2.0 A. The symmetry and distance constraints determined by X-ray fiber and neutron diffraction enable the construction of an accurate model of the bacteriophage particle from the coordinates of the coat protein monomers.     

Secondary structure of filamentous bacteriophage coat protein is preserved in lipid environments

1H nuclear magnetic resonance experiments have shown that the amide hydrogens of residues 30 to 40 of bacteriophage Pf1 coat protein in micelles undergo very slow exchange with solvent deuterons. The amide 1H resonances from these residues were used to monitor the structural stability of the membrane-spanning helix of the coat protein during the transition of the coat protein from its structural form, in the virus particle, to the membrane-bound form, in micelles. The helix was found to remain folded on the 10(-3) second time-scale of the experiment, which indicates that no major disruption or rearrangement of the central part of the protein structure occurs during the process of coat protein solubilization by detergent. The results also suggest that a helical peptide can associate with lipids without reorganization of its secondary structure. However, a general model for the insertion of proteins into membranes cannot be established from these results, because the mechanism of the detergent solubilization process may differ somewhat from that of the membrane insertion process.     

Molecular dynamics simulation of Pf1 coat protein.

The results of molecular dynamics simulations of Pf1 coat protein are described and compared to experimental NMR data on both the membrane bound and structural forms of this viral coat protein. Molecular dynamics simulations of the 46 residue coat protein and related model sequences were performed according to a simple protocol. The simulations were initiated with the polypeptides in a completely uniform alpha helical conformation in a dielectric continuum (epsilon = 2) and the motions of individual residues were followed as a function of time by monitoring the angular fluctuations of amide NH bond vectors. The simulations of Pf1 coat protein were able to identify the same mobile and structured segments found in experimental NMR studies of the membrane bound form of the protein (Shon, K.-J., Y. Kim, L. A. Colnago, and S. J. Opella. 1991. Science (Wash. DC). 252:1303-1305). Significantly, in addition to mobile amino and carboxyl terminal regions, a mobile internal loop was found that connects the rigid hydrophobic and amphipathic helices in the protein. NMR experiments show that this mobile loop is present in both the viral and membrane bound forms of the protein and that it plays a role in viral assembly (Nambudripad, R., W. Stark, S. J. Opella, and L. Makowski. 1991. Science (Wash. DC) 252:1305-1308). The results of simulations of several alanine based 46 residue polypeptides with some of the charged residues present in the Pf1 coat protein sequence suggest that interactions between the Asp 14 and Asp 18 sidechains and the peptide backbone are responsible for the formation of the mobile loop.(ABSTRACT TRUNCATED AT 250 WORDS)     

Calcium- and membrane-induced changes in the structure and dynamics of three helical hairpins in annexin B12

Annexins are a family of soluble proteins that can undergo reversible Ca(2+)-dependent interaction with the interfacial region of phospholipid membranes. The helical hairpins on the convex face of the crystal structure of soluble annexins are proposed to mediate binding to membranes, but the mechanism is not defined. For this study, we used a site-directed spin labeling (SDSL) experimental approach to investigate Ca(2+) and membrane-induced structural and dynamic changes that occurred in the helical hairpins encompassing three of the four D and E helices of annexin B12. Electron paramagnetic resonance (EPR) parameters were analyzed for the soluble and Ca(2+)-dependent membrane-bound states of the following nitroxide scans of annexin B12: a continuous 24-residue scan of the D and E helices in the third repeat (residues 219-242) and short scans encompassing the D-E loop regions of the first repeat (residues 68-74) and the fourth repeat (300-305). EPR mobility and accessibility parameters of most sites were similar when the protein was in solution or in the membrane-bound state, and both sets of data were consistent with the crystal structure of the protein. However, membrane-induced changes in mobility and accessibility were observed in all three loop regions, with the most dramatic changes noted at sites corresponding to the highly conserved serine and glycine residues in the loops. EPR accessibility parameters clearly established that nitroxide side chains placed at these sites made direct contact with the bilayer. EPR mobility parameters showed that these sites were very mobile in solution, but immobilized on the EPR time scale in the membrane-bound state. Since the headgroup regions of bilayer phospholipids are relatively mobile in the absence of annexins, Ca(2+)-dependent binding of annexin B12 appears to form a complex in which the mobility of the D-E loop region of the protein and the headgroup region of the phospholipid are highly constrained. Possible biological consequences of annexin-induced restriction of membrane mobility are discussed.     

Localization and rearrangement modulation of the N-terminal arm of the membrane-bound major coat protein of bacteriophage M13

During infection the major coat protein of the filamentous bacteriophage M13 is in the cytoplasmic membrane of the host Escherichia coli. This study focuses on the configurational properties of the N-terminal part of the coat protein in the membrane-bound state. For this purpose X-Cys substitutions are generated at coat protein positions 3, 7, 9, 10, 11, 12, 13, 14, 15, 17, 19, 21, 22, 23 and 24, covering the N-terminal protein part. All coat protein mutants used are successfully produced in mg quantities by overexpression in E. coli. Mutant coat proteins are labeled and reconstituted into mixed bilayers of phospholipids. Information about the polarity of the local environment around the labeled sites is deduced from the wavelength of maximum emission using AEDANS attached to the SH groups of the cysteines as a fluorescent probe. Additional information is obtained by determining the accessibility of the fluorescence quenchers acrylamide and 5-doxyl stearic acid. By employing uniform coat protein surroundings provided by TFE and SDS, local effects of the backbone of the coat proteins or polarity of the residues could be excluded. Our data suggest that at a lipid to protein ratio around 100, the N-terminal arm of the protein gradually enters the membrane from residue 3 towards residue 19. The hinge region (residues 17-24), connecting the helical parts of the coat protein, is found to be more embedded in the membrane. Substitution of one or more of the membrane-anchoring amino acid residues lysine 8, phenylalanine 11 and leucine 14, results in a rearrangement of the N-terminal protein part into a more extended conformation. The N-terminal arm can also be forced in this conformation by allowing less space per coat protein at the membrane surface by decreasing the lipid to protein ratio. The influence of the phospholipid headgroup composition on the rearrangement of the N-terminal part of the protein is found to be negligible within the range thought to be relevant in vivo. From our experiments we conclude that membrane-anchoring and space-limiting effects are key factors for the structural rearrangement of the N-terminal protein part of the coat protein in the membrane.     

Protein hot spots: the islands of stability

Understanding the structural basis of protein-protein interactions (PPIs) may shed light on the organization and functioning of signal transduction and metabolic networks and may assist in structure-based design of ligands (drugs) targeting protein-protein interfaces. The residues at the bimolecular interface, designated as the hot spots, contribute most of the free binding energy of PPI. To date, there is no conclusive atomistic explanation for the unique functional properties of the hot spots. We hypothesized that backbone compliance may play a role in protein-protein recognition and in the mechanism of binding of small-molecule compounds to protein surfaces. We used a steered molecular dynamics simulation to explore the compliance properties of the backbone of surface-exposed residues in several model proteins: interleukin-2, mouse double minute protein 2 and proliferating cell nuclear antigen. We demonstrated that protein surfaces exhibit distinct patterns in which highly immobile residues form defined clusters ("stability patches") alternating with areas of moderate to high mobility. These "stability patches" tend to localize in functionally important regions involved in protein-protein recognition. We propose a mechanism by which the distinct structural organization of the hot spots may contribute to their role in mediating PPI and facilitating binding of structurally diverse small-molecule compounds to protein surfaces.     

Fluorescence determination of tryptophan side-chain accessibility and dynamics in triple-helical collagen-like peptides

We report tryptophan fluorescence measurements of emission intensity, iodide quenching, and anisotropy that describe the environment and dynamics at X and Y sites in stable collagen-like peptides of sequence (Gly-X-Y)(n). About 90% of tryptophans at both sites have similar solvent exposed fluorescence properties and a lifetime of 8.5-9 ns. Analysis of anisotropy decays using an associative model indicates that these long lifetime populations undergo rapid depolarizing motion with a 0.5 ns correlation time; however, the extent of fast motion at the Y site is considerably less than the essentially unrestricted motion at the X site. About 10% of tryptophans at both sites have a shorter ( approximately 3 ns) lifetime indicating proximity to a protein quenching group; these minor populations are immobile on the peptide surface, depolarizing only by overall trimer rotation. Iodide quenching indicates that tryptophans at the X site are more accessible to solvent. Side chains at X sites are more solvent accessible and considerably more mobile than residues at Y sites and can more readily fluctuate among alternate intermolecular interactions in collagen fibrils. This fluorescence analysis of collagen-like peptides lays a foundation for studies on the structure, dynamics, and function of collagen and of triple-helical junctions in gelatin gels.     

Deuterium/hydrogen exchange factors measured by solution nuclear magnetic resonance spectroscopy as indicators of the structure and topology of membrane proteins

Deuterium/hydrogen exchange factors (chi) were measured for the backbone amide sites of the membrane-bound forms of the 50-residue fd coat protein and the 23-residue magainin2 peptide in lipid micelles by solution nuclear magnetic resonance spectroscopy. By combining kinetic and thermodynamic effects, deuterium/hydrogen exchange factors overcome the principal limitations encountered in the measurements of kinetic protection factors and thermodynamic fractionation factors for membrane proteins. The magnitudes of the exchange factors can be correlated with the structure and topology of membrane-associated polypeptides. In fd coat protein, residues in the transmembrane helix have exchange factors that are substantially smaller than those in the amphipathic surface helix or the loop connecting the two helices. For the amphipathic helical peptide, magainin2, the exchange factors of residues exposed to the solvent are appreciably larger than those that face the hydrocarbon portion of membrane bilayers. These examples demonstrate that deuterium/hydrogen exchange factors can be measured by solution NMR spectroscopy and used to identify residues in transmembrane helices as well as to determine the polarity of amphipathic helices in membrane proteins.     

Backbone dynamics of complement control protein (CCP) modules reveals mobility in binding surfaces

The regulators of complement activation (RCA) are critical to health and disease because their role is to ensure that a complement-mediated immune response to infection is proportionate and targeted. Each protein contains an uninterrupted array of from four to 30 examples of the very widely occurring complement control protein (CCP, or sushi) module. The CCP modules mediate specific protein-protein and protein-carbohydrate interactions that are key to the biological function of the RCA and, paradoxically, provide binding sites for numerous pathogens. Although structural and mutagenesis studies of CCP modules have addressed some aspects of molecular recognition, there have been no studies of the role of molecular dynamics in the interaction of CCP modules with their binding partners. NMR has now been used in the first full characterization of the backbone dynamics of CCP modules. The dynamics of two individual modules-the 16th of the 30 modules of complement receptor type 1 (CD35), and the N-terminal module of membrane cofactor protein (CD46)-as well as their solution structures, are compared. Although both examples share broadly similar three-dimensional structures, many structurally equivalent residues exhibit different amplitudes and timescales of local backbone motion. In each case, however, regions of the module-surface implicated by mutagenesis as sites of interactions with other proteins include several mobile residues. This observation suggests further experiments to explore binding mechanisms and identify new binding sites.     

Local and global dynamics of the G protein-coupled receptor CXCR1

The local and global dynamics of the chemokine receptor CXCR1 are characterized using a combination of solution NMR and solid-state NMR experiments. In isotropic bicelles (q = 0.1), only 13% of the expected number of backbone amide resonances is observed in (1)H/(15)N HSQC solution NMR spectra of uniformly (15)N-labeled samples; extensive deuteration and the use of TROSY made little difference in the 800 MHz spectra. The limited number of observed amide signals is ascribed to mobile backbone sites and assigned to specific residues in the protein; 19 of the signals are from residues at the N-terminus and 25 from residues at the C-terminus. The solution NMR spectra display no evidence of local backbone motions from residues in the transmembrane helices or interhelical loops of CXCR1. This finding is reinforced by comparisons of solid-state NMR spectra of both magnetically aligned and unoriented bilayers containing either full-length or doubly N- and C-terminal truncated CXCR1 constructs. CXCR1 undergoes rapid rotational diffusion about the normal of liquid crystalline phospholipid bilayers; reductions in the frequency span and a change to axial symmetry are observed for both carbonyl carbon and amide nitrogen chemical shift powder patterns of unoriented samples containing (13)C- and (15)N-labeled CXCR1. In contrast, when the phospholipids are in the gel phase, CXCR1 does not undergo rapid global reorientation on the 10(4) Hz time scale defined by the carbonyl carbon and amide nitrogen chemical shift powder patterns.     

Conformational dynamics of free and catalytically active thermolysin are indistinguishable by hydrogen/deuterium exchange mass spectrometry

Conformational dynamics are thought to be a prerequisite for the catalytic activity of enzymes. However, the exact relationship between structural fluctuations and function is not well understood. In this work hydrogen/deuterium exchange (HDX) and electrospray ionization mass spectrometry (ESI-MS) are used for exploring the conformational dynamics of thermolysin. Amide HDX reflects the internal mobility of proteins; regions that undergo frequent unfolding-refolding show faster exchange than segments that are highly stable. Thermolysin is a zinc protease with an active site that is located between two lobes. Substrate turnover is associated with hinge bending that leads to a closed conformation. Product release regenerates the open form, such that steady-state catalysis involves a continuous closing/opening cycle. HDX/ESI-MS with proteolytic peptide mapping in the absence of substrate shows that elements in the periphery of the two lobes are most mobile. A comparison with previous X-ray data suggests that these peripheral regions undergo quite pronounced structural changes during the catalytic cycle. In contrast, active site residues exhibit only a moderate degree of backbone flexibility, and the central zinc appears to be in a fairly rigid environment. The presence of both rigid and moderately flexible elements in the active site may reflect a carefully tuned balance that is required for function. Interestingly, the HDX behavior of catalytically active thermolysin is indistinguishable from that of the free enzyme. This result is consistent with the view that catalytically relevant motions preexist in the resting state and that enzyme function can only be performed within the limitations given by the intrinsic dynamics of the protein. The data presented in this work indicate the prevalence of stochastic elements in the function of thermolysin, rather than supporting a deterministic mechanism.     

(1)H/(15)N heteronuclear NMR spectroscopy shows four dynamic domains for phospholamban reconstituted in dodecylphosphocholine micelles

We report the backbone dynamics of monomeric phospholamban in dodecylphosphocholine micelles using (1)H/(15)N heteronuclear NMR spectroscopy. Phospholamban is a 52-amino acid membrane protein that regulates Ca-ATPase in cardiac muscle. Phospholamban comprises three structural domains: a transmembrane domain from residues 22 to 52, a connecting loop from 17 to 21, and a cytoplasmic domain from 1 to 16 that is organized in an "L"-shaped structure where the transmembrane and the cytoplasmic domain form an angle of approximately 80 degrees (Zamoon et al., 2003; Mascioni et al., 2002). T(1), T(2), and (1)H/(15)N nuclear Overhauser effect values measured for the amide backbone resonances were interpreted using the model-free approach of Lipari and Szabo. The results point to the existence of four dynamic domains, revealing the overall plasticity of the cytoplasmic helix, the flexible loop, and part of the transmembrane domain (residues 22-30). In addition, using Carr-Purcell-Meiboom-Gill-based experiments, we have characterized phospholamban dynamics in the micros-ms timescale. We found that the majority of the residues in the cytoplasmic domain, the flexible loop, and the first ten residues of the transmembrane domain undergo dynamics in the micros-ms range, whereas minimal dynamics were detected for the transmembrane domain. Hydrogen/deuterium exchange factors measured at different temperatures support the existence of slow motion in both the loop and the cytoplasmic helix. We propose that these dynamic properties are critical factors in the biomolecular recognition of phospholamban by Ca-ATPase and other interacting proteins such as protein kinase A and protein phosphatase 1.     

Solution structure and dynamics of the functional domain of Paracoccus denitrificans cytochrome c(552) in both redox states

A soluble and fully functional 10.5 kDa fragment of the 18.2 kDa membrane-bound cytochrome c(552) from Paracoccus denitrificans has been heterologously expressed and (13)C/(15)N-labeled to study the structural features of this protein in both redox states. Well-resolved solution structures of both the reduced and oxidized states have been determined using high-resolution heteronuclear NMR. The overall protein topology consists of two long terminal helices and three shorter helices surrounding the heme moiety. No significant redox-induced structural differences have been observed. (15)N relaxation rates and heteronuclear NOE values were determined at 500 and 600 MHz. Several residues located around the heme moiety display increased backbone mobility in both oxidation states, while helices I, III, and V as well as the two concatenated beta-turns between Leu30 and Arg36 apparently form a less flexible domain within the protein structure. Major redox-state-dependent differences of the internal backbone mobility on the picosecond-nanosecond time scale were not evident. Hydrogen exchange experiments demonstrated that the slow-exchanging amide proton resonances mainly belong to the helices and beta-turns, corresponding to the regions with high order parameters in the dynamics data. Despite this correlation, the backbone amide protons of the oxidized cytochrome c(552) exchange considerably faster with the solvent compared to the reduced protein. Using both differential scanning calorimetry as well as temperature-dependent NMR spectroscopy, a significant difference in the thermostabilities of the two redox states has been observed, with transition temperatures of 349.9 K (76.8 degrees C) for reduced and 307.5 K (34.4 degrees C) for oxidized cytochrome c(552). These results suggest a clearly distinct backbone stability between the two oxidation states.     

Solution structure of the state 1 conformer of GTP-bound H-Ras protein and distinct dynamic properties between the state 1 and state 2 conformers

Ras small GTPases undergo dynamic equilibrium of two interconverting conformations, state 1 and state 2, in the GTP-bound forms, where state 2 is recognized by effectors, whereas physiological functions of state 1 have been unknown. Limited information, such as static crystal structures and (31)P NMR spectra, was available for the study of the conformational dynamics. Here we determine the solution structure and dynamics of state 1 by multidimensional heteronuclear NMR analysis of an H-RasT35S mutant in complex with guanosine 5'-(β, γ-imido)triphosphate (GppNHp). The state 1 structure shows that the switch I loop fluctuates extensively compared with that in state 2 or H-Ras-GDP. Also, backbone (1)H,(15)N signals for state 2 are identified, and their dynamics are studied by utilizing a complex with c-Raf-1. Furthermore, the signals for almost all the residues of H-Ras·GppNHp are identified by measurement at low temperature, and the signals for multiple residues are found split into two peaks corresponding to the signals for state 1 and state 2. Intriguingly, these residues are located not only in the switch regions and their neighbors but also in the rigidly structured regions, suggesting that global structural rearrangements occur during the state interconversion. The backbone dynamics of each state show that the switch loops in state 1 are dynamically mobile on the picosecond to nanosecond time scale, and these mobilities are significantly reduced in state 2. These results suggest that multiconformations existing in state 1 are mostly deselected upon the transition toward state 2 induced by the effector binding.     

Relationships between protein structure and dynamics from a database of NMR-derived backbone order parameters

The amplitude of protein backbone NH group motions on a time-scale faster than molecular tumbling may be determined by analysis of (15)N NMR relaxation data according to the Lipari-Szabo model free formalism. An internet-accessible database has been compiled containing 1855 order parameters from 20 independent NMR relaxation studies on proteins whose three-dimensional structures are known. A series of statistical analyses has been performed to identify relationships between the structural features and backbone dynamics of these proteins. Comparison of average order parameters for different amino acid types indicates that amino acids with small side-chains tend to have greater backbone flexibility than those with large side-chains. In addition, the motions of a given NH group are also related to the sizes of the neighboring amino acids in the primary sequence. The secondary structural environment appears to influence backbone dynamics relatively weakly, with only subtle differences between the order parameter distributions of loop structures and regular hydrogen bonded secondary structure elements. However, NH groups near helix termini are more mobile on average than those in the central regions of helices. Tertiary structure influences are also relatively weak but in the expected direction, with more exposed residues being more flexible on average than residues that are relatively inaccessible to solvent.