A heuristic approach to predicting the tertiary structure of bovine somatotropin

A combination of a heuristic approach and energy minimization was used to predict the three-dimensional structure of bovine somatotropin (bSt), also known as bovine growth hormone, a protein of 191 amino acids. The starting points for energy minimizations were generated from the following two types of inputs: (a) the amino acid sequence and (b) the heuristic inputs, which were derived according to physical, chemical, and biological principles by piecing together all useful information available. The predicted 3-D structure of the bSt molecule has all the features observed in four-helix bundle proteins. The four alpha-helices in bSt are intimately packed to form an assembly with an approximately square cross section. All the adjacent alpha-helices are antiparallel, with a somewhat tilted angle between each of the adjacent pairs so that the assembly of the four helices looks like a left-handed twisted bundle. There are two disulfide bonds in the bSt structure: one "hooking" the middle of a long loop with helix 4 so as to pull the long loop onto the surface of the helix bundle and the other "hooking" the C-terminal segment with the same helix so as to force the C-terminal segment to bend toward the helix bundle. As a consequence, a considerable part of the surface of the four-helix bundle is closely packed or intimately embraced by the loop segments. The predicted bSt structure has a hydrophobic core and a hydrophilic exterior surface. The energetic analysis of the predicted bSt structure indicates that the interaction between helices and loops plays a dominant role in stabilizing the four-helix bundle structure from the viewpoint of both electrostatic and nonbonded interactions. A technique called FOLD was meanwhile developed, by which one can fold a polypeptide chain into any shape as desired. This tool proved to be very useful during the heuristic model-building process.     

Proline-induced distortions of transmembrane helices

Proline residues in the transmembrane (TM) alpha-helices of integral membrane proteins have long been suspected to play a key role for helix packing and signal transduction by inducing regions of helix distortion and/or dynamic flexibility (hinges). In this study we try to characterise the effect of proline on the geometric properties of TM alpha-helices. We have examined 199 transmembrane alpha-helices from polytopic membrane proteins of known structure. After examining the location of proline residues within the amino acid sequences of TM helices, we estimated the helix axes either side of a hinge and hence identified a hinge residue. This enabled us to calculate helix kink and swivel angles. The results of this analysis show that proline residues occur with a significant concentration in the centre of sequences of TM alpha-helices. In this location, they may induce formation of molecular hinges, located on average about four residues N-terminal to the proline residue. A superposition of proline-containing TM helices structures shows that the distortion induced is anisotropic and favours certain relative orientations (defined by helix kink and swivel angles) of the two helix segments.     

Electrostatic stabilization in four-helix bundle proteins.

Charge substitutions generated by site-directed mutagenesis at the termini of adjacent anti-parallel alpha-helices in a four-helix bundle protein were used to determine a precise value for the contribution of indirect charge-charge interactions to overall protein stability, and to simulate the electrostatic effects of alpha-helix macrodipoles. Thermodynamic double mutant cycles were constructed to measure the interaction energy between such charges on adjacent anti-parallel helices in the four-helix bundle cytochrome b562 from Escherichia coli. Previously, theoretical calculations of helix macrodipole interactions using modeled four-helix bundle proteins have predicted values ranging over an order of magnitude from 0.2 to 2.5 kcal/mol. Our system represents the first experimental evidence for electrostatic interactions such as those between partial charges due to helix macrodipole charges. At the positions mutated, we have measured a favorable interaction energy of 0.6 kcal/mol between opposite charges simulating an anti-parallel helix pair. Pairs of negative or positive charges simulating a parallel orientation of helices produce an unfavorable interaction of similar magnitude. The interaction energies show a strong dependence upon ionic strength, consistent with an electrostatic effect. Indirect electrostatic contacts do appear to confer a limited stabilization upon the association of anti-parallel packing of helices, favoring this orientation by as much as 1 kcal/mol at 20 mM K phosphate.     

Bundles of amphipathic transmembrane alpha-helices as a structural motif for ion-conducting channel proteins: studies on sodium channels and acetylcholine receptors

Channel proteins are transmembrane symmetric (or pseudosymmetric) oligomers organized around a central ionic pore. We present here a molecular model of the pore forming structures of two channel proteins with different primary structures and oligomeric size: the voltage-sensitive sodium channel and the nicotinic cholinergic receptor. We report low-energy arrangements of alpha-helical bundles calculated by semiempiricial potential energy functions and optimization routines and further refined using molecular dynamics. The ion-conducting pore is considered to be a symmetric or pseudosymmetric homooligomer of 3-5 amphipathic alpha-helices arranged such that the polar residues line a central hydrophilic pathway and the apolar residues face the hydrophobic bilayer interior. The channel lining exposes either charged (Asp, Glu, Arg, Lys) or polar-neutral (Ser, Thr) residues. A bundle of four parallel helices constrained to C4 symmetry, the helix axis aligned with the symmetry axis, and the helices constrained to idealized dihedral angles, produces a structure with a pore of the size inferred for the sodium channel protein (area approximately 16 A2). Similarly, a pentameric array optimized with constraints to maintain C5 symmetry and backbone torsions characteristic of alpha-helices adopts a structure that appears well suited to form the lining of the nicotinic cholinergic receptor (pore area approximately 46 A2). Thus, bundles of amphipathic alpha-helices satisfy the structural, energetic, and dynamic requirements to be the molecular structural motif underlying the function of ionic channels.     

Insights into dimerization and four-helix bundle formation found by dissection of the dimer interface of the GrpE protein from Escherichia coli

The GrpE heat shock protein from Escherichia coli has a homodimeric structure. The dimer interface encompasses two long alpha-helices at the NH(2)-terminal end from each monomer (forming a "tail"), which lead into a small four-helix bundle from which each monomer contributes two short sequential alpha-helices in an antiparallel topological arrangement. We have created a number of different deletion mutants of GrpE that have portions of the dimer interface to investigate requirements for dimerization and to study four-helix bundle formation. Using chemical crosslinking and analytical ultracentrifugation techniques to probe for multimeric states, we find that a mutant containing only the long alpha-helical tail portion (GrpE1-88) is unable to form a dimer, most likely due to a decrease in alpha-helical content as determined by circular dichroism spectroscopy, thus one reason for a dimeric structure for the GrpE protein is to support the tail region. Mutants containing both of the short alpha-helices (GrpE1-138 and GrpE88-197) are able to form a dimer and presumably the four-helix bundle at the dimer interface. These two mutants have equilibrium constants for the monomer-dimer equilibrium that are very similar to the full-length protein suggesting that the tail region does not contribute significantly to the stability of the dimer. Interestingly, one mutant that contains just one of the short alpha-helices (GrpE1-112) exists as a tetrameric species, which presumably is forming a four-helix bundle structure. A proposed model is discussed for this mutant and its relevance for factors influencing four-helix bundle formation.     

Serine and threonine residues bend alpha-helices in the chi(1) = g(-) conformation

The relationship between the Ser, Thr, and Cys side-chain conformation (chi(1) = g(-), t, g(+)) and the main-chain conformation (phi and psi angles) has been studied in a selection of protein structures that contain alpha-helices. The statistical results show that the g(-) conformation of both Ser and Thr residues decreases their phi angles and increases their psi angles relative to Ala, used as a control. The additional hydrogen bond formed between the O(gamma) atom of Ser and Thr and the i-3 or i-4 peptide carbonyl oxygen induces or stabilizes a bending angle in the helix 3-4 degrees larger than for Ala. This is of particular significance for membrane proteins. Incorporation of this small bending angle in the transmembrane alpha-helix at one side of the cell membrane results in a significant displacement of the residues located at the other side of the membrane. We hypothesize that local alterations of the rotamer configurations of these Ser and Thr residues may result in significant conformational changes across transmembrane helices, and thus participate in the molecular mechanisms underlying transmembrane signaling. This finding has provided the structural basis to understand the experimentally observed influence of Ser residues on the conformational equilibrium between inactive and active states of the receptor, in the neurotransmitter subfamily of G protein-coupled receptors.     

Strong electrostatic loop-helix interactions in bundle motif protein structures.

Based on CHARMM potential (Brooks et al., 1983) an energetic analysis has been carried out for four typical 4-alpha-helix bundle proteins, i.e., methemerythrin, cytochrome b-562, cytochrome c', and bovine somatotropin. The bovine somatotropin possesses long loops, but all the other three proteins have short loops. It was found that in all these four 4-alpha-helix bundle motif structures the interaction between loops and helices was much stronger than the interaction among the four helices themselves. Particularly for the electrostatic interaction energy, the loop-helix interaction is overwhelmingly stronger than the interhelix interaction although the latter involves the favorable helix dipole interaction due to the antiparallel arrangement of neighboring alpha-helices. The present study indicates that such a conclusion holds true regardless of what loops, long or short, are in the 4-alpha-helix bundle protein, and also regardless of which empirical potential, ECEPP or CHARMM, is used for calculations although in CHARMM the electrostatic energy is much more heavily emphasized than in ECEPP. Therefore, no appropriate conclusion can be drawn in arguing whether the dipole interaction among the four alpha-helices play a stabilizing role or destabilizing role for a 4-alpha-helix bundle protein without taking into consideration the effect of interaction between helices and loops. The calculated results reported here provide, from a different point of view, insights that might be useful for revealing the essence of the driving forces during the folding of proteins.     

Three-dimensional solution structure of the calcium-signaling protein apo-S100A1 as determined by NMR.

S100A1, a member of the S100 protein family, is an EF-hand containing Ca(2+)-binding protein (93 residues per subunit) with noncovalent interactions at its dimer interface. Each subunit of S100A1 has four alpha-helices and a small antiparallel beta-sheet consistent with two helix-loop-helix calcium-binding domains [Baldiserri et al. (1999) J. Biomol. NMR 14, 87-88]. In this study, the three-dimensional structure of reduced apo-S100A1 was determined by NMR spectroscopy using a total of 2220 NOE distance constraints, 258 dihedral angle constraints, and 168 backbone hydrogen bond constraints derived from a series of 2D, 3D, and 4D NMR experiments. The final structure was found to be globular and compact with the four helices in each subunit aligning to form a unicornate-type four-helix bundle. Intermolecular NOE correlations were observed between residues in helices 1 and 4 from one subunit to residues in helices 1' and 4' of the other subunit, respectively, consistent with the antiparallel alignment of the two subunits to form a symmetric X-type four-helix bundle as found for other members of the S100 protein family. Because of the similarity of the S100A1 dimer interface to that found for S100B, it was possible to calculate a model of the S100A1/B heterodimer. This model is consistent with a number of NMR chemical shift changes observed when S100A1 is titrated into a sample of (15)N-labeled S100B. Helix 3 (and 3') of S100A1 was found to have an interhelical angle of -150 degrees with helix 4 (and 4') in the apo state. This crossing angle is quite different (>50 degrees ) from that typically found in other EF-hand containing proteins such as apocalmodulin and apotroponin C but more similar to apo-S100B, which has an interhelical angle of -166 degrees. As with S100B, it is likely that the second EF-hand of apo-S100A1 reorients dramatically upon the addition of Ca(2+), which can explain the Ca(2+) dependence that S100A1 has for binding several of its biological targets.     

Visualization of alpha-helices in a 6-angstrom resolution cryoelectron microscopy structure of adenovirus allows refinement of capsid protein assignments

The structure of adenovirus was determined to a resolution of 6 A by cryoelectron microscopy (cryoEM) single-particle image reconstruction. Docking of the hexon and penton base crystal structures into the cryoEM density established that alpha-helices of 10 or more residues are resolved as rods. A difference map was calculated by subtracting a pseudoatomic capsid from the cryoEM reconstruction. The resulting density was analyzed in terms of observed alpha-helices and secondary structure predictions for the additional capsid proteins that currently lack atomic resolution structures (proteins IIIa, VI, VIII, and IX). Protein IIIa, which is predicted to be highly alpha-helical, is assigned to a cluster of helices observed below the penton base on the inner capsid surface. Protein VI is present in approximately 1.5 copies per hexon trimer and is predicted to have two long alpha-helices, one of which appears to lie inside the hexon cavity. Protein VIII is cleaved by the adenovirus protease into two fragments of 7.6 and 12.1 kDa, and the larger fragment is predicted to have one long alpha-helix, in agreement with the observed density for protein VIII on the inner capsid surface. Protein IX is predicted to have one long alpha-helix, which also has a strongly indicated propensity for coiled-coil formation. A region of density near the facet edge is now resolved as a four-helix bundle and is assigned to four copies of the C-terminal alpha-helix from protein IX.     

Helix geometry in proteins

In this report we describe a general survey of all helices found in 57 of the known protein crystal structures, together with a detailed analysis of 48 alpha-helices found in 16 of the structures that are determined to high resolution. The survey of all helices reveals a total of 291 alpha-helices, 71 3(10)-helices and no examples of pi-helices. The conformations of the observed helices are significantly different from the "ideal" linear structures. The mean phi, psi angles for the alpha- and 3(10)-helices found in proteins are, respectively, (-62 degrees, -41 degrees) and (-71 degrees, -18 degrees). A computer program, HBEND, is used to characterize and to quantify the different types of helix distortion. alpha-Helices are classified as regular or irregular, linear, curved or kinked. Of the 48 alpha-helices analysed, only 15% are considered to be linear; 17% are kinked, and 58% are curved. The curvature of helices is caused by differences in the peptide hydrogen bonding on opposite faces of the helix, reflecting carbonyl-solvent/side-chain interactions for the exposed residues, and packing constraints for residues involved in the hydrophobic core. Kinked helices arise either as a result of included proline residues, or because of conflicting requirements for the optimal packing of the helix side-chains. In alpha-helices where there are kinks caused by proline residues, we show that the angle of kink is relatively constant (approximately 26 degrees), and that there is minimal disruption of the helix hydrogen bonding. The proline residues responsible for the kinks are highly conserved, suggesting that these distortions may be structurally/functionally important.     

Identification of a stability determinant on the edge of the Tet repressor four-helix bundle dimerization motif

Isofunctional tetracycline repressor (TetR) proteins isolated from different bacteria show a sequence identity between 38 and 88% of the residues. Their active state is a homodimer formed by a four-alpha-helix bundle as the main interaction motif. We utilize this sequence variation of isofunctional proteins to determine residues contributing to the stability of the four-helix bundle. The thermodynamic stabilities of two TetR proteins with 63% sequence identity were determined by urea-induced reversible denaturation followed by fluorescence and circular dichroism. Both methods yield identical results. The deltaG(o)U (H2O) values are 60 and 75 kJ x mol(-1). We have constructed TetR hybrid proteins derived from these wild types to identify the determinant leading to the 15 kJ x mol(-1) stability difference. Successive size reduction of the exchanged portion yielded two single residues affecting the overall protein stability. The P184Q exchange leads to a more stable protein, whereas the G181D exchange located at the solvent's exposed edge of the four-helix bundle is solely responsible for the reduced stability. Additional mutants based on crystal structures of TetR do not reveal any hint for steric interference of the Asp181 side chain with neighboring residues. Thus, this is an example for the role played by surface-exposed turn residues for the stability of four-helix bundles. We assume that the larger conformational flexibility of Gly and the reduction of the negative surface charge could favor formation of the turn on the edge of the four-helix bundle.     

Molecular Dynamics Simulations of Homo-oligomeric Bundles Embedded Within a Lipid Bilayer

Using molecular dynamics simulations, we studied the structure, interhelix interactions, and dynamics of transmembrane proteins. Specifically, we investigated homooligomeric helical bundle systems consisting of synthetic α-helices with either the sequence Ac-(LSLLLSL)₃-NH₂ (LS2) or Ac-(LSSLLSL)₃-NH₂ (LS3). The LS2 and LS3 helical peptides are designed to have amphipathic characteristics that form ion channels in membrane. We simulated bundles containing one to six peptides that were embedded in palmitoyl-oleoyl-phosphatidylcholine (POPC) lipid bilayer and placed between two lamellae of water. We aim to provide a fundamental understanding of how amphipathic helical peptides interact with each other and their dynamical behaviors in different homooligomeric states. To understand structural properties, we examined the helix lengths, tilt angles of individual helices and the entire bundle, interhelix distances, interhelix cross-angles, helix hydrophobic-to-hydrophilic vector projections, and the average number of interhelix hydrophilic (serine–serine) contacts lining the pore of the transmembrane channel. To analyze dynamical properties, we calculated the rotational autocorrelation function of each helix and the cross-correlation of the rotational velocity between adjacent helices. The observed structural and dynamical characteristics show that higher order bundles containing four to six peptides are composed of multiple lower order bundles of one to three peptides. For example, the LS2 channel was found to be stable in a tetrameric bundle composed of a “dimer of dimers.” In addition, we observed that there is a minimum of two strong hydrophilic contacts between a pair of adjacent helices in the dimer to tetramer systems and only one strong hydrophilic interhelix contact in helix pairs of the pentamer and hexamer systems. We believe these results are general and can be applied to more complex ion channels, providing insight into ion channel stability and assembly.     

Molecular Dynamics Simulations of Homo-oligomeric Bundles Embedded Within a Lipid Bilayer

Using molecular dynamics simulations, we studied the structure, interhelix interactions, and dynamics of transmembrane proteins. Specifically, we investigated homooligomeric helical bundle systems consisting of synthetic α-helices with either the sequence Ac-(LSLLLSL)₃-NH₂ (LS2) or Ac-(LSSLLSL)₃-NH₂ (LS3). The LS2 and LS3 helical peptides are designed to have amphipathic characteristics that form ion channels in membrane. We simulated bundles containing one to six peptides that were embedded in palmitoyl-oleoyl-phosphatidylcholine (POPC) lipid bilayer and placed between two lamellae of water. We aim to provide a fundamental understanding of how amphipathic helical peptides interact with each other and their dynamical behaviors in different homooligomeric states. To understand structural properties, we examined the helix lengths, tilt angles of individual helices and the entire bundle, interhelix distances, interhelix cross-angles, helix hydrophobic-to-hydrophilic vector projections, and the average number of interhelix hydrophilic (serine–serine) contacts lining the pore of the transmembrane channel. To analyze dynamical properties, we calculated the rotational autocorrelation function of each helix and the cross-correlation of the rotational velocity between adjacent helices. The observed structural and dynamical characteristics show that higher order bundles containing four to six peptides are composed of multiple lower order bundles of one to three peptides. For example, the LS2 channel was found to be stable in a tetrameric bundle composed of a “dimer of dimers.” In addition, we observed that there is a minimum of two strong hydrophilic contacts between a pair of adjacent helices in the dimer to tetramer systems and only one strong hydrophilic interhelix contact in helix pairs of the pentamer and hexamer systems. We believe these results are general and can be applied to more complex ion channels, providing insight into ion channel stability and assembly.     

Dramatic structural and thermodynamic consequences of repacking a protein's hydrophobic core

BACKGROUND: Rop is an RNA binding, dimeric, four-helix bundle protein with a well-defined, regular hydrophobic core ideally suited for redesign studies. A family of Rop variants in which the hydrophobic core was systematically redesigned has previously been created and characterized. RESULTS: We present a structural and thermodynamic analysis of Ala2Ile2-6, a variant of Rop with an extensively redesigned hydrophobic core. The structure of Ala2Ile2-6 reveals a completely new fold formed by a conformational "flip" of the two protomers around the dimeric interface. The free-energy profile of Ala2Ile2-6 is also very different from that of wild-type Rop. Ala2Ile2-6 has a higher melting temperature than Rop, but undergoes a slightly smaller free-energy change on unfolding. CONCLUSIONS: The structure of Ala2Ile2-6, along with molecular modeling results, demonstrate the importance of tight packing of core residues and the adoption of favorable core side chain rotamer values in determining helix-helix interactions in the four-helix bundle fold. Structural disorder at the N and C termini of Ala2Ile2-6 provides a basis for the large differences in the enthalpy and entropy of Ala2Ile2-6 folding compared with wildtype Rop.     

X-ray structure of a maquette scaffold

Maquettes are de novo designed mimicries of nature used to test the construction and engineering criteria of oxidoreductases. One type of scaffold used in maquette construction is a four-alpha-helical bundle. The sequence of the four-alpha-helix bundle maquettes follows a heptad repeat pattern typical of left-handed coiled-coils. Initial designs were molten globular due partly to the minimalist approach taken by the designers. Subsequent iterative redesign generated several structured scaffolds with similar heme binding properties. Variant [I(6)F(13)](2), a structured scaffold, was partially resolved with NMR spectroscopy and found to have a set of mobile inter-helical packing interfaces. Here, the X-ray structure of a similar peptide ([I(6)F(13)M(31)](2) i.e. ([CGGG EIWKL HEEFLKK FEELLKL HEERLKKM](2))(2) which we call L31M), has been solved using MAD phasing and refined to 2.8A resolution. The structure shows that the maquette scaffold is an anti-parallel four-helix bundle with "up-up-down-down" topology. No pre-formed heme-binding pocket exists in the protein scaffold. We report unexpected inter-helical crossing angles, residue positions and translations between the helices. The crossing angles between the parallel helices are -5 degrees rather than the expected +20 degrees for typical left-handed coiled-coils. Deviation of the scaffold from the design is likely due to the distribution and size of hydrophobic residues. The structure of L31M points out that four identical helices may interact differently in a bundle and heptad repeats with an alternating [HPPHHPP]/[HPPHHPH] (H: hydrophobic, P: polar) pattern are not a sufficient design criterion to generate left-hand coiled-coils.     

Three-dimensional solution structure of the B domain of staphylococcal protein A: comparisons of the solution and crystal structures.

The three-dimensional solution structure of the recombinant B domain (FB) of staphylococcal protein A, which specifically binds to the Fc portion of immunoglobulin G, was determined by NMR spectroscopy and hybrid distance geometry-dynamical simulated annealing calculations. On the basis of 692 experimental constraints including 587 distance constraints obtained from the nuclear Overhauser effect (NOE), 57 torsion angle (phi, chi 1) constraints, and 48 constraints associated with 24 hydrogen bonds, a total of 10 converged structures of FB were obtained. The atomic root mean square difference among the 10 converged structures is 0.52 +/- 0.10 A for the backbone atoms and 0.98 +/- 0.08 A for all heavy atoms (excluding the N-terminal segment from Thr1 to Glu9 and the C-terminal segment from Gln56 to Ala60, which are partially disordered). FB is composed of a bundle of three alpha-helices, i.e., helix I (Gln10-His19), helix II (Glu25-Asp37), and helix III (Ser42-Ala55). Helix II and helix III are antiparallel to each other, whereas the long axis of helix I is tilted at an angle of about 30 degrees with respect to those of helix II and helix III. Most of the hydrophobic residues of FB are buried in the interior of the bundle of the three helices. It is suggested that the buried hydrophobic residues form a hydrophobic core, contributing to the stability of FB.(ABSTRACT TRUNCATED AT 250 WORDS)     

Packed protein bilayers in the 0.90 A resolution structure of a designed alpha helical bundle.

A 12-residue peptide designed to form an alpha-helix and self-associate into an antiparallel 4-alpha-helical bundle yields a 0.9 A crystal structure revealing unanticipated features. The structure was determined by direct phasing with the "Shake-and-Bake" program, and contains four crystallographically distinct 12-mer peptide molecules plus solvent for a total of 479 atoms. The crystal is formed from nearly ideal alpha-helices hydrogen bonded head-to-tail into columns, which in turn pack side-by-side into sheets spanning the width of the crystal. Within each sheet, the alpha-helices run antiparallel and are closely spaced (9-10 A center-to-center). The sheets are more loosely packed against each other (13-14 A between helix centers). Each sheet is amphiphilic: apolar leucine side chains project from one face, charged lysine and glutamate side chains from the other face. The sheets are stacked with two polar faces opposing and two apolar faces opposing. The result is a periodic biomaterial composed of packed protein bilayers, with alternating polar and apolar interfaces. All of the 30 water molecules in the unit cell lie in the polar interface or between the stacked termini of helices. A section through the sheet reveals that the helices packed at the apolar interface resemble the four-alpha-helical bundle of the design, but the helices overhang parts of the adjacent bundles, and the helix crossing angles are less steep than intended (7-11 degrees rather than 18 degrees).     

Seven-helix bundles: molecular modeling via restrained molecular dynamics.

Simulated annealing via restrained molecular dynamics (SA/MD) has been used to model compact bundles of seven approximately (anti)parallel alpha-helices. Seven such helix bundles occur, e.g., in bacteriorhodopsin, in rhodopsin, and in the channel-forming N-terminal domain of Bacillus thuringiensis delta-endotoxin. Two classes of model are considered: (a) those consisting of seven Ala20 peptide chains; and (b) those containing a single polypeptide chain, made up of seven Ala20 helices linked by GlyN interhelix loops (where N = 5 or 10). Three different starting C alpha templates for SA/MD are used, in which the seven helices are arranged (a) on a left-handed circular template, (b) on a bacteriorhodopsin-like template, or (c) on a zig-zag template. The ensembles of models generated by SA/MD are analyzed in terms of their geometry and energetics, and the most stable structures from each ensemble are examined in greater detail. Structures resembling bacteriorhodopsin and structures resembling delta-endotoxin are both represented among the most stable structures. delta-Endotoxin-like structures arise from both circular and bacteriorhodopsin-like C alpha templates. A third helix-packing mode occurs several times among the stable structures, regardless of the C alpha template and of the presence or absence of interhelix loops. It is characterized by a "4 + 1" core, in which four helices form a distorted left-handed supercoil around a central, buried helix. The remaining two helices pack onto the outside of the core. This packing mode is comparable with that proposed for rhodopsin on the basis of two-dimensional electron crystallographic and sequence analysis studies.     

Transmembrane four-helix bundle of influenza A M2 protein channel: structural implications from helix tilt and orientation.

The transmembrane portion of the M2 protein from the Influenza A virus has been studied in hydrated dimyristroylphosphotidylcholine lipid bilayers with solid-state NMR. Orientational constraints were obtained from isotopically labeled peptide samples mechanically aligned between thin glass plates. 15N chemical shifts from single site labeled samples constrain the molecular frame with respect to the magnetic field. When these constraints are applied to the peptide, modeled as a uniform alpha-helix, the tilt of the helix with respect to the bilayer normal was determined to be 33 degrees +/- 3 degrees. Furthermore, the orientation about the helix axis was also determined within an error of +/- 30 degrees. These results imply that the packing of this tetrameric protein is in a left-handed four-helix bundle. Only with such a large tilt angle are the hydrophilic residues aligned to the channel axis.     

NMR solution structure of KP-TerB, a tellurite-resistance protein from Klebsiella pneumoniae

Klebsiella pneumoniae (KP), a Gram-negative bacterium, is a common cause of hospital-acquired bacterial infections worldwide. Tellurium (Te) compounds, although relatively rare in the environment, have a long history as antimicrobial and therapeutic agents. In bacteria, tellurite (TeO(3) (-2)) resistance is conferred by the ter (Te(r)) operon (terZABCDEF). Here, on the basis of 2593 restraints derived from NMR analysis, we report the NMR structure of TerB protein (151 amino acids) of KP (KP-TerB), which is mainly composed of seven alpha-helices and a 3(10) helix, with helices II to V apparently forming a four-helix bundle. The ensemble of 20 NMR structures was well-defined, with a RMSD of 0.32 +/- 0.06 A for backbone atoms and 1.11 +/- 0.07 A for heavy atoms, respectively. A unique property of the KP-TerB structure is that the positively and negatively charged clusters are formed by the N-terminal positively and C-terminal negatively charged residues, respectively. To the best of our knowledge, the protein sequence and structures of KP-TerB are unique.