Conformational dynamics of M2 helices in KirBac channels: helix flexibility in relation to gating via molecular dynamics simulations

KirBac1.1 and 3.1 are bacterial homologues of mammalian inward rectifier K channels. We have performed extended molecular dynamics simulations (five simulations, each of >20 ns duration) of the transmembrane domain of KirBac in two membrane environments, a palmitoyl oleoyl phosphatidylcholine bilayer and an octane slab. Analysis of these simulations has focused on the conformational dynamics of the pore-lining M2 helices, which form the cytoplasmic hydrophobic gate of the channel. Principal components analysis reveals bending of M2, with a molecular hinge at the conserved glycine (Gly134 in KirBac1.1, Gly120 in KirBac3.1). More detailed analysis reveals a dimer-of-dimers type motion. The first two eigenvectors describing the motions of M2 correspond to helix kink and swivel motions. The conformational flexibility of M2 seen in these simulations correlates with differences in M2 conformation between that seen in the X-ray structures of closed channels (KcsA and KirBac) in which the helix is undistorted, and in open channels (e.g. MthK) in which the M2 helix is kinked. Thus, the simulations, albeit on a time scale substantially shorter than that required for channel gating, suggest a gating model in which the intrinsic flexibility of M2 about a molecular hinge is coupled to conformational transitions of an intracellular 'gatekeeper' domain, the latter changing conformation in response to ligand binding.     

Proline-induced hinges in transmembrane helices: possible roles in ion channel gating

A number of ion channels contain transmembrane (TM) alpha-helices that contain proline-induced molecular hinges. These TM helices include the channel-forming peptide alamethicin (Alm), the S6 helix from voltage-gated potassium (Kv) channels, and the D5 helix from voltage-gated chloride (CLC) channels. For both Alm and KvS6, experimental data implicate hinge-bending motions of the helix in an aspect of channel gating. We have compared the hinge-bending motions of these TM helices in bilayer-like environments by multi-nanosecond MD simulations in an attempt to describe motions of these helices that may underlie possible modes of channel gating. Alm is an alpha-helical channel-forming peptide, which contains a central kink associated with a Gly-x-x-Pro motif in its sequence. Simulations of Alm in a TM orientation for 10 ns in an octane slab indicate that the Gly-x-x-Pro motif acts as a molecular hinge. The S6 helix from Shaker Kv channels contains a Pro-Val-Pro motif. Modeling studies and recent experimental data suggest that the KvS6 helix may be kinked in the vicinity of this motif. Simulations (10 ns) of an isolated KvS6 helix in an octane slab and in a POPC bilayer reveal hinge-bending motions. A pattern-matching approach was used to search for possible hinge-bending motifs in the TM helices of other ion channel proteins. This uncovered a conserved Gly-x-Pro motif in TM helix D5 of CLC channels. MD simulations of a model of hCLC1-D5 spanning an octane slab suggest that this channel also contains a TM helix that undergoes hinge-bending motion. In conclusion, our simulations suggest a model in which hinge-bending motions of TM helices may play a functional role in the gating mechanisms of several different families of ion channels.     

Structure and dynamics of K channel pore-lining helices: a comparative simulation study

Isolated pore-lining helices derived from three types of K-channel have been analyzed in terms of their structural and dynamic features in nanosecond molecular dynamics (MD) simulations while spanning a lipid bilayer. The helices were 1) M1 and M2 from the bacterial channel KcsA (Streptomyces lividans), 2) S5 and S6 from the voltage-gated (Kv) channel Shaker (Drosophila melanogaster), and 3) M1 and M2 from the inward rectifier channel Kir6.2 (human). In the case of the Kv and Kir channels, for which x-ray structures are not known, both short and long models of each helix were considered. Each helix was incorporated into a lipid bilayer containing 127 palmitoyloleoylphosphatidylcholine molecules, which was solvated with approximately 4000 water molecules, yielding approximately 20, 000 atoms in each system. Nanosecond MD simulations were used to aid the definition of optimal lengths for the helix models from Kv and Kir. Thus the study corresponds to a total simulation time of 10 ns. The inner pore-lining helices (M2 in KcsA and Kir, S6 in Shaker) appear to be slightly more flexible than the outer pore-lining helices. In particular, the Pro-Val-Pro motif of S6 results in flexibility about a molecular hinge, as was suggested by previous in vacuo simulations (, Biopolymers. 39:503-515). Such flexibility may be related to gating in the corresponding intact channel protein molecules. Analysis of H-bonds revealed interactions with both water and lipid molecules in the water/bilayer interfacial region. Such H-bonding interactions may lock the helices in place in the bilayer during the folding of the channel protein (as is implicit in the two-stage model of membrane protein folding). Aromatic residues at the extremities of the helices underwent complex motions on both short (<10 ps) and long (>100 ps) time scales.     

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.     

Self-assembly of a simple membrane protein: coarse-grained molecular dynamics simulations of the influenza M2 channel

The transmembrane (TM) domain of the M2 channel protein from influenza A is a homotetrameric bundle of α-helices and provides a model system for computational approaches to self-assembly of membrane proteins. Coarse-grained molecular dynamics (CG-MD) simulations have been used to explore partitioning into a membrane of M2 TM helices during bilayer self-assembly from lipids. CG-MD is also used to explore tetramerization of preinserted M2 TM helices. The M2 helix monomer adopts a membrane spanning orientation in a lipid (DPPC) bilayer. Multiple extended CG-MD simulations (5 × 5 μs) were used to study the tetramerization of inserted M2 helices. The resultant tetramers were evaluated in terms of the most populated conformations and the dynamics of their interconversion. This analysis reveals that the M2 tetramer has 2× rotationally symmetrical packing of the helices. The helices form a left-handed bundle, with a helix tilt angle of ∼16°. The M2 helix bundle generated by CG-MD was converted to an atomistic model. Simulations of this model reveal that the bundle's stability depends on the assumed protonation state of the H37 side chains. These simulations alongside comparison with recent x-ray (3BKD) and NMR (2RLF) structures of the M2 bundle suggest that the model yielded by CG-MD may correspond to a closed state of the channel.     

Picosecond timescale rigid-helix and side-chain motions in deoxymyoglobin

The contribution of rigidbody motions to the atomic trajectories in a 100 ps molecular dynamics simulation of deoxymyoglobin is examined. Two typesof rigid-body motions are considered: one in which the helices are rigid units and one in which the side-chains are rigid units. Using a quaternionbased algorithm, fits of the rigid reference structures are made to each time frame of the simulation to derive trajectories of the rigid-body motions. The fitted trajectories are analysed in terms of atomic position fluctuations, mean-square displacements as a function of time, velocity autocorrelation functions and densities of states. The results are compared with the corresponding quantities calculated from the full trajectory. The relative contribution of the rigid helix motions to the helix atom dynamics depends on which quantity is examined and on which subset of atoms is chosen: rigid-helix motions contribute 86% of the rms helix backbone atomic position fluctuations, but 30% of the helix,: atom (backbone and side-chain) mean square displacements and only 1.1% of total kinetic energy. Only very low-frequency motions contribute to the rigid-helix dynamics; the rigid-body analysis allows characteristic rigid-helix vibrations to be identified and described. Treating the side-chains as rigid bodies is foundto be an excellent approximation to both their diffusive and vibrationalmean-square displacements: 96% of side-chain atom mean-square displacements originate from rigid side-Chain motions. However, the errors in theside-chain atomic positional fits are not always small. An analysis is madeof factors contributing to the positional error for different types of side-chain. © Wiley-Liss, Inc.     

Computer simulation of the interaction of non-steroidal anti-inflammatory drugs: indoprofen and NS398 with cyclooxygenase

We have applied computer simulation technique to study interaction of two anti-inflammatory drugs (NSAIDs) indoprofen and NS398 with cyclooxygenase (COX-1 and COX-2) enzymes. We have also investigated conformational flexibility of the two drugs by systematic search and simulated annealing molecular dynamics (SAMD) methods. Both the drugs were docked in the cyclooxygenase channel using in house docking program IMF1. The complexes were energy minimised by molecular mechanics (MM) method. These were heated for 30 picoseconds (ps), equilibrated for 110 ps at 300K and subjected to 'production simulation' for 110 ps by molecular dynamics (MD) method using Sanderís module of AMBER 5.0 package and united atom force field mostly from PARM96.DAT. Integration was carried out with time step of 0.001 ps, distance dependent di-electric constant with scaling factor 2.0 for 1-4 interaction and cut-off distance for non-bonded pair-list equal to 8A. The non-bonded pair-list was upgraded after every 20 cycles. The coordinate output from MD trajectories is analysed using analysis package of AMBER 5.0, MOLMOL, P-CURVES 3.0 and in house packages: ANALMD, ANALP1. We have observed perturbative changes in COX-1 and COX-2 structures due to indoprofen and NS398. In case of indoprofen specific changes between COX-1 and COX-2 were noted in helix D, H6, S6 and helix H8 in the cyclooxygenase cavity. In case of NS398 these were in helix B in membrane binding domain, helix H6, S8 and S10 in cyclooxygenase cavity and helices H14-H16 in small lobe close to haem binding region. Implications of these results in enzyme selectivity by NSAIDs is discussed here.     

Dynamics and relative stabilities of parallel- and antiparallel-stranded DNA duplexes.

The dynamics and stability of four DNA duplexes are studied by means of molecular dynamics simulations. The four molecules studied are combinations of 4, 15 bases long, single-stranded oligomers, F1, F2, F3, and F4. The sequence of these single strand oligomers are chosen such that F1-F2 and F3-F4 form parallel (ps) DNA double helices, whereas F1-F4 and F2-F3 form antiparallel-stranded (aps) DNA double helices. Simulations were done at low (100 K) and room (300 K) temperatures. At low temperatures the dynamics are quasi-harmonic and the analysis of the trajectories gives good estimates of the low frequency vibrational modes and density of states. These are used to estimate the linear (harmonic) contribution of local fluctuations to the configurational entropy of the systems. Estimates of the differences in enthalpy between ps and aps duplexes show that aps double helices are more stable than the corresponding ps duplexes, in agreement with experiments. At higher temperatures, the distribution of the fluctuations around the average structures are multimodal and estimates of the configurational entropy cannot be obtained. The multi-basin, nonlinear character of the dynamics at 300 K is established using a novel method which extracts large amplitude nonlinear motions from the molecular dynamics trajectories. Our analysis shows that both ps DNA exhibit much larger fluctuations than the two aps DNA. The large fluctuations of ps DNA are explained in terms of correlated transitions in the beta, epsilon, and zeta backbone dihedral angles.     

Pores formed by the nicotinic receptor m2delta Peptide: a molecular dynamics simulation study

The M2delta peptide self-assembles to form a pentameric bundle of transmembrane alpha-helices that is a model of the pore-lining region of the nicotinic acetylcholine receptor. Long (>15 ns) molecular dynamics simulations of a model of the M2delta(5) bundle in a POPC bilayer have been used to explore the conformational dynamics of the channel assembly. On the timescale of the simulation, the bundle remains relatively stable, with the polar pore-lining side chains remaining exposed to the lumen of the channel. Fluctuations at the helix termini, and in the helix curvature, result in closing/opening transitions at both mouths of the channel, on a timescale of approximately 10 ns. On average, water within the pore lumen diffuses approximately 4x more slowly than water outside the channel. Examination of pore water trajectories reveals both single-file and path-crossing regimes to occur at different times within the simulation.     

Comparison of simulated and experimentally determined dynamics for a variant of the Lacl DNA-binding domain, Nlac-P.

Recent advances in the experimentally determined structures and dynamics of the domains within LacI provide a rare context for evaluating dynamics calculations. A 1500-ps trajectory was simulated for a variant of the LacI DNA-binding domain, which consists of the first three helices in LacI and the hinge helix of the homologous PurR. Order parameters derived from dynamics simulations are compared to those obtained for the LacI DNA-binding domain with 15N relaxation NMR spectroscopy (Slijper et al., 1997. Biochemistry. 36:249-254). The MD simulations suggest that the unstructured loop between helices II and III does not exist in a discrete state under the conditions of no salt and neutral pH, but occupies a continuum of states between the DNA-bound and free structures. Simulations also indicate that the unstructured region between helix III and the hinge helix is very mobile, rendering motions of the hinge helix essentially independent of the rest of the protein. Finally, the alpha-helical hydrogen bonds in the hinge helix are broken after 1250 ps, perhaps as a prelude to helix unfolding.     

Molecular dynamics simulation of the M2 helices within the nicotinic acetylcholine receptor transmembrane domain: structure and collective motions

Multiple nanosecond duration molecular dynamics simulations were performed on the transmembrane region of the Torpedo nicotinic acetylcholine receptor embedded within a bilayer mimetic octane slab. The M2 helices and M2-M3 loop regions were free to move, whereas the outer (M1, M3, M4) helix bundle was backbone restrained. The M2 helices largely retain their hydrogen-bonding pattern throughout the simulation, with some distortions in the helical end and loop regions. All of the M2 helices exhibit bending motions, with the hinge point in the vicinity of the central hydrophobic gate region (corresponding to residues alphaL251 and alphaV255). The bending motions of the M2 helices lead to a degree of dynamic narrowing of the pore in the region of the proposed hydrophobic gate. Calculations of Born energy profiles for various structures along the simulation trajectory suggest that the conformations of the M2 bundle sampled correspond to a closed conformation of the channel. Principal components analyses of each of the M2 helices, and of the five-helix M2 bundle, reveal concerted motions that may be relevant to channel function. Normal mode analyses using the anisotropic network model reveal collective motions similar to those identified by principal components analyses.     

A high resolution structure of the putative hinge region in M2 channel-lining segments of the nicotinic acetylcholine receptor

Transmembrane peptide helices play key roles in signal transduction across cell membranes, yet little is known about their high-resolution structure or the role membrane composition plays in their association, structure, dynamics and ultimately their performance. Using magic angle spinning (MAS) homonuclear dipolar recoupling experiments, the backbone structure at positions L10, L11, and A12 of the M2 ion channel peptide was determined in two lipid systems. Their measurements are in agreement with M2 forming transmembrane helices, but the torsion angles vary considerably from common α−helical values. These measurements show remarkable agreement with a previous computational model of M2 peptides forming a pore domain in which their helices are kinked near the central leucine, L11 [R. Sankararamakrishnan, C. Adcock, M.S.P. Sansom, The pore domain of the nicotinic acetylcholine receptor: Molecular modeling, pore dimensions, and electrostatics, Biophys. J. 71 (1996) 1659-1671]. The generation of high resolution data for transmembrane helices is of critical importance in refining structures for membrane protein and developing models of helix packing interactions.     

Molecular modeling of c-erbB2 receptor dimerization: Coiled-coil structure of wild and oncogenic transmembrane domains—Stabilization by interhelical hydrogen bonds in the oncogenic form

Dimerization models of c-erbB2 transmembrane domains (Leu651-Ile675) are studied by molecular mechanics and molecular dynamics simulations. Both wild and Glu mutated transmembrane helices exhibit the same relative orientation for favorable associations and dimerize preferentially in left-handed coiled-coil structures. The mutation point 659 belongs to the interfacing residues, and in the transforming domain, symmetric hydrogen bonds between Glu carboxylic groups stabilize the dimeric structure. The same helix packing found for the wild dimers, except side-chain—side-chain hydrogen bonds, suggests that the transmembrane domains dimerize according to similar process. Structural and energetical characterization of the models are presented. © 1997 John Wiley & Sons, Inc. Biopoly 42: 157–168, 1997     

Sequence context strongly modulates association of polar residues in transmembrane helices

Polar residues are capable of mediating the association of membrane-embedded helices through the formation of side-chain/side-chain inter-helical hydrogen bonds. However, the extent to which native van der Waals packing of the residues surrounding the polar locus can enhance, or interfere with, the interaction of polar residues has not yet been studied. We examined the propensities of four polar residues (aspartic acid, asparagine, glutamic acid, and glutamine) to promote self-association of transmembrane (TM) domains in several biologically derived sequence environments, including (i). four naturally occurring TM domains that contain a Glu or Gln residue (Tnf5/CD40 ligand, C79a/Ig-alpha, C79b/Ig-beta, and Fut3/alpha-fucosyltransferase); and (ii). variants of bacteriophage M13 major coat protein TM segment with Asp and Asn at interfacial and non-interfacial positions. Self-association was quantified by the TOXCAT assay, which measures TM helix self-oligomerization in the Escherichia coli inner membrane. While an appropriately placed polar residue was found in several cases to significantly stabilize TM helix-helix interactions through the formation of an interhelical hydrogen bond, in other cases the strongly polar residues did not enhance the association of the two helices. Overall, these results suggest that an innate structural mechanism may operate to control non-specific association of membrane-embedded polar residues.     

Structure and dynamics of the pore-lining helix of the nicotinic receptor: MD simulations in water, lipid bilayers, and transbilayer bundles

Multiple nanosecond duration molecular dynamics simulations on the pore-lining M2 helix of the nicotinic acetylcholine receptor reveal how its structure and dynamics change as a function of environment. In water, the M2 helix partially unfolds to form a molecular hinge in the vicinity of a central Leu residue that has been implicated in the mechanism of ion channel gating. In a phospholipid bilayer, either as a single transmembrane helix, or as part of a pentameric helix bundle, the M2 helix shows less flexibility, but still exhibits a kink in the vicinity of the central Leu. The single M2 helix tilts relative to the bilayer normal by 12 degrees, in agreement with recent solid state NMR data (Opella et al., Nat Struct Biol 6:374-379, 1999). The pentameric helix bundle, a model for the pore domain of the nicotinic receptor and for channels formed by M2 peptides in a bilayer, is remarkably stable over a 2-ns MD simulation in a bilayer, provided one adjusts the pK(A)s of ionizable residues to their calculated values (when taking their environment into account) before starting the simulation. The resultant transbilayer pore shows fluctuations at either mouth which transiently close the channel. Proteins 2000;39:47-55.     

A high resolution structure of the putative hinge region in M2 channel-lining segments of the nicotinic acetylcholine receptor

Transmembrane peptide helices play key roles in signal transduction across cell membranes, yet little is known about their high-resolution structure or the role membrane composition plays in their association, structure, dynamics and ultimately their performance. Using magic angle spinning (MAS) homonuclear dipolar recoupling experiments, the backbone structure at positions L10, L11, and A12 of the M2 ion channel peptide was determined in two lipid systems. Their measurements are in agreement with M2 forming transmembrane helices, but the torsion angles vary considerably from common alpha-helical values. These measurements show remarkable agreement with a previous computational model of M2 peptides forming a pore domain in which their helices are kinked near the central leucine, L11 [R. Sankararamakrishnan, C. Adcock, M.S.P. Sansom, The pore domain of the nicotinic acetylcholine receptor: Molecular modeling, pore dimensions, and electrostatics, Biophys. J. 71 (1996) 1659-1671]. The generation of high resolution data for transmembrane helices is of critical importance in refining structures for membrane protein and developing models of helix packing interactions.     

Molecular dynamics simulations of isolated transmembrane helices of potassium channels

In the middle of the S6 helix in voltage-gated potassium channels there is a highly conserved Pro-Val-Pro motif, while the equivalent M2 helix of inward rectifier potassium channels contains a conserved glycine residue in a comparable position. The structural implications of these conserved motifs are of interest given the evidence that S6 and M2 are components of the lining of their respective pores. Multiple sequence alignment and TM helix prediction methods were used to define consensus regions for S6 and M2. Ensembles of 50 structures for each helix were generated by simulated annealing and restrained molecular dynamics. Time-dependent fluctuations of S6 and M2 were investigated by long time scale molecular dynamics simulations on representative members of each ensemble carried out in vacuo in the presence and absence of a hydrophobic potential that mimics a lipid bilayer. The results are discussed in terms of the structural basis of the kink in S6 and M2 and of a putative functional role for flexible helices as “molecular swivels.” © 1996 John Wiley & Sons, Inc.     

Proline in alpha-helix: stability and conformation studied by dynamics simulation

Free-energy simulations have been used to estimate the change in the conformational stability of short polyalanine alpha-helices when one of the alanines is replaced by a proline residue. For substituting proline in the middle of the helix the change in free energy of folding (delta delta G degrees) was calculated as 14 kJ/mol (3.4 kcal/mol), in excellent agreement with the one available experimental value. The helix containing proline was found to be strongly kinked; the free energy for reducing the angle of the kink from 40 degrees to 15 degrees was calculated, and found to be small. A tendency to alternate hydrogen bonding schemes was observed in the proline-containing helix. These observations for the oligopeptide agree well with the observation of a range of kink angles (18-35 degrees) and variety of hydrogen bonding schemes, in the rare instances where proline occurs in helices in globular proteins. For substituting proline at the N-terminus of the helix the change in free energy of folding (delta delta G degrees) was calculated as -4 kJ/mol in the first helical position (N1) and +6 kJ/mol in the second helical position (N2). The observed frequent occurrence of proline in position N1 in alpha-helices in proteins therefore has its origin in stability differences of secondary structure. The conclusion reached here that proline may be a better helix former in position N1 than (even) alanine, and thus be a helix initiator may be testable experimentally by measurements of fraction helical conformation of individual residues in oligopeptides of appropriate sequence. The relevance of these results in regards to the frequent occurrence of proline-containing helices in certain membrane proteins is discussed.     

The occurrence of C--H...O hydrogen bonds in alpha-helices and helix termini in globular proteins

A comprehensive database analysis of C--H...O hydrogen bonds in 3124 alpha-helices and their corresponding helix termini has been carried out from a nonredundant data set of high-resolution globular protein structures resolved at better than 2.0 A in order to investigate their role in the helix, the important protein secondary structural element. The possible occurrence of 5 --> 1 C--H...O hydrogen bond between the ith residue CH group and (i - 4)th residue C==O with C...O < or = 3.8 A is studied, considering as potential donors the main-chain Calpha and the side-chain carbon atoms Cbeta, Cgamma, Cdelta and Cepsilon. Similar analysis has been carried out for 4 --> 1 C--H...O hydrogen bonds, since the C--H...O hydrogen bonds found in helices are predominantly of type 5 --> 1 or 4 --> 1. A total of 17,367 (9310 of type 5 --> 1 and 8057 of type 4 --> 1) C--H...O hydrogen bonds are found to satisfy the selected criteria. The average stereochemical parameters for the data set suggest that the observed C--H...O hydrogen bonds are attractive interactions. Our analysis reveals that the Cgamma and Cbeta hydrogen atom(s) are frequently involved in such hydrogen bonds. A marked preference is noticed for aliphatic beta-branched residue Ile to participate in 5 --> 1 C--H...O hydrogen bonds involving methylene Cgamma 1 atom as donor in alpha-helices. This may be an enthalpic compensation for the greater loss of side-chain conformational entropy for beta-branched amino acids due to the constraint on side-chain torsion angle, namely, chi1, when they occur in helices. The preference of amino acids for 4 --> 1 C--H...O hydrogen bonds is found to be more for Asp, Cys, and for aromatic residues Trp, Phe, and His. Interestingly, overall propensity for C--H...O hydrogen bonds shows that a majority of the helix favoring residues such as Met, Glu, Arg, Lys, Leu, and Gln, which also have large side-chains, prefer to be involved in such types of weak attractive interactions in helices. The amino acid side-chains that participate in C--H...O interactions are found to shield the acceptor carbonyl oxygen atom from the solvent. In addition, C--H...O hydrogen bonds are present along with helix stabilizing salt bridges. A novel helix terminating interaction motif, X-Gly with Gly at C(cap) position having 5 --> 1 Calpha--H...O, and a chain reversal structural motif having 1 --> 5 Calpha-H...O have been identified and discussed. Our analysis highlights that a multitude of local C--H...O hydrogen bonds formed by a variety of amino acid side-chains and Calpha hydrogen atoms occur in helices and more so at the helix termini. It may be surmised that the main-chain Calpha and the side-chain CH that participate in C--H...O hydrogen bonds collectively augment the cohesive energy and thereby contribute together with the classical N--H...O hydrogen bonds and other interactions to the overall stability of helix and therefore of proteins.