Heterogeneity in iota-carrageenan molecular structure: insights for polymorph II-->III transition in the presence of calcium ions

Iota-carrageenan is used in pharmaceutical and food applications due to its ability to complex with other hydrocolloids and proteins. Six distinct cation dependent allomorphs, consistent with its versatile functionality, have so far been observed in the solid state. In this contribution, X-ray structural details of calcium iota-carrageenan (form III) are reported. The polysaccharide retains the half-staggered, parallel, 3-fold, right-handed double helix stabilized by interchain hydrogen bonds from O-2H and O-6H in the Galp units. Results show that there are four helices, rather than one in I or three in II, organized in a larger pseudo-trigonal unit cell of dimensions a=27.44, c=13.01 A, and gamma=120 degrees . The four helices have similar core structures, but their sulfate group orientations are quite different. Fifteen calcium ions and 64 water molecules hold the helices together and promote helix-helix interactions. The results portray how the helices would shuffle around in an orchestrated manner to yield calcium iota-carrageenan III from II.     

Refined structure of southern bean mosaic virus at 2.9 A resolution

The T = 3 capsid of southern bean mosaic virus is analyzed in detail. The beta-sheets of the beta-barrel folding motif that form the subunits show a high degree of twist, generated by several beta-bulges. Only 34 water molecules were identified in association with the three quasi-equivalent subunits, most of them on the external viral surface. Subunit contacts related by quasi-3-fold axes are similar, are dominated by polar interactions and have almost identical calcium binding sites. There is no metal ion on the quasi-3-fold axis, as previously reported. Subunits related by quasi-2-fold and icosahedral 2-fold axes have different contacts but nevertheless display almost identical interactions between the antiparallel helices alpha A. A dipole-dipole type interaction between these helices may produce an energetically stable hinge that allows two types of dimers in a T = 3 assembly. The temperature factor distribution, the hydrogen-bonding pattern, and the contacts across the icosahedral 2-fold axes suggest that one of the dimer types is present in the intact virion and probably also in solution; the other is produced only during capsid assembly. Interactions along the 5-fold axes are mainly polar and possibly form an ion channel. The beta-sheet structures of the three subunits can be superimposed with considerable precision. Significant relative distortions between quasi-equivalent subunits occur mainly in helices and loops. The two dimeric forms and the subunit distortions are the consequence of the non-equivalent subunit environments in the capsid.     

Unmasking the annexin I interaction from the structure of Apo-S100A11

S100A11 is a homodimeric EF-hand calcium binding protein that undergoes a calcium-induced conformational change and interacts with the phospholipid binding protein annexin I to coordinate membrane association. In this work, the solution structure of apo-S100A11 has been determined by NMR spectroscopy to uncover the details of its calcium-induced structural change. Apo-S100A11 forms a tight globular structure having a near antiparallel orientation of helices III and IV in calcium binding site II. Further, helices I and IV, and I and I', form a more closed arrangement than observed in other apo-S100 proteins. This helix arrangement in apo-S100A11 partially buries residues in helices I (P3, E11, A15), III (V55, R58, M59), and IV (A86, C87, S90) and the linker (A45, F46), which are required for interaction with annexin I in the calcium-bound state. In apo-S100A11, this results in a "masked" binding surface that prevents annexin I binding but is uncovered upon calcium binding.     

Amide exchange shows calcium-induced conformational changes are transmitted to the dimer interface of S100B

S100B is a 21 kDa member of the S100 calcium-binding protein family. This protein comprises a symmetric homodimer with each subunit having two EF-hands arranged from four alpha-helices (I-IV). S100B binds calcium and undergoes a conformation change leading to the exposure of hydrophobic surface residues that enable the protein to interact with biological target molecules. The most significant structural change that occurs during calcium binding results in a change in the orientation of helix III with respect to helices II and IV. In this work, the calcium-sensitive conformational change has been studied by utilizing fast 1H-15N HSQC experiments and water-transfer methods to follow the amide exchange in apo-S100B and Ca-S100B at 35 degrees C. In apo-S100B, the protection factors are 2-3 orders of magnitude lower for helix III than for helix I, II, or IV. In addition, the exchange stability measured here for the dimer interface helices (I, I', IV, and IV'), in the absence of calcium, is similar to the stability obtained from chemical denaturation experiments. When calcium binds, significant decreases in the protection factors for helices I and IV indicate a modification in the stability of the dimer interface has occurred. In contrast, helix II protection factors increase slightly, which is consistent with a decreased level of surface exposure of this helix. These data have been compared with those of the monomeric S100 protein, calbindin D9k, to illustrate that upon calcium binding there is a balance maintained between the amide exchange rates in helices II and III, although largely the rates are dissimilar for each of these proteins. This distinguishing feature may be important for the calcium-induced conformational change in S100B, where calcium binding is transmitted to the dimer-forming helices.     

Structural understanding of the transmembrane domains of inositol triphosphate receptors and ryanodine receptors towards calcium channeling.

Inositol 1,4,5-triphosphate receptors (Insp(3)Rs) and ryanodine receptors (ryRs) act as cationic channels transporting calcium ions from the endoplasmic reticulum to cytosol by forming tetramers and are proteins localized to the endoplasmic reticulum (ER). Despite the absence of classical calcium-binding motifs, calcium channeling occurs at the transmembrane domain. We have investigated putative calcium binding motifs in these sequences. Prediction methods indicate the presence of six transmembrane helices in the C-terminal domain, one of the three domains conserved between Insp(3)R and ryR receptors. The recently identified crystal structure of the K(+) channel, which also forms tetramers, revealed that two transmembrane helices, an additional pore helix and a selectivity filter are responsible for selective K(+) ion channeling. The last three TM helices of Insp(3)R and ryR are particularly well conserved and we found analogous pore helix and selectivity filter motif in these sequences. We obtained a three-dimensional structural model for the transmembrane tetramer by extrapolating the distant structural similarity to the K(+) channels.     

Helix packing of leucine-rich peptides: a parallel leucine ladder in the structure of Boc-Aib-Leu-Aib-Aib-Leu-Leu-Leu-Aib-Leu-Aib-OMe.

The packing of peptide helices in crystals of the leucine-rich decapeptide Boc-Aib-Leu-Aib-Aib-Leu-Leu-Leu-Aib-Leu-Aib-OMe provides an example of ladder-like leucylleucyl interactions between neighboring molecules. The peptide molecule forms a helix with five 5----1 hydrogen bonds and two 4----1 hydrogen bonds near the C terminus. Three head-to-tail NH ... O = C hydrogen bonds between helices form continuous columns of helices in the crystal. The helicial columns associate in an antiparallel fashion, except for the association of Leu ... Leu side chains, which occurs along the diagonal of the cell where the peptide helices are parallel. The peptide, with formula C56H102N10O13, crystallizes in space group P2(1)2(1)2(1) with Z = 4 and cell parameters a = 16.774(3) A, b = 20.032(3) A and c = 20.117(3) A; overall agreement factor R = 10.7% for 2014 data with magnitude of F(obs) greater than 3 sigma (F); resolution 1.0 A.     

Structural and motional changes induced in apo-S100A1 protein by the disulfide formation between its Cys 85 residue and beta-mercaptoethanol

Recently, we have shown (Goch, G., Vdovenko, S., Koz?owska, H., and Bierzyński, A. (2005) FEBS J. 272, 2557-2565) that the chemical modification of Cys 85 residue of S100A1 protein by disulfide bond formation with small thiols such as glutathione, cysteine, or beta-mercaptoethanol (betaME) leads to a dramatic increase of the protein affinity for calcium. Therefore, the biological function of S100A1 as a calcium signal transmitter is probably regulated by the redox potential within the cell. Systematic, structural studies of various mixed disulfides of S100A1 in the apo and holo states are necessary to elucidate the mechanism of this phenomenon. Using NMR methods we have determined the structure of apo-S100A1-betaME and, on the basis of 15N nuclear magnetic relaxation data, we have characterized the structural dynamics of both: modified and unmodified molecules of apo-S100A1. The following effects of betaME modification have been observed: (1) Helices IV and IV' of two protein subunits are elongated by five residues (85-89). (2) Conformation of the calcium binding N-terminal loops is dramatically changed, and structural flexibility of the N-loops as well as C-loops markedly increases. (3) The angle between helices I and IV increases by approximately 20 degrees and between helices IV and IV' decreases by approximately 35 degrees . All these observations lead to the conclusion that betaME modification of apo-S100A1 makes its structure more similar to that of holo-S100A1, so that it becomes much better adjusted for calcium coordination.     

The three-dimensional solution structure of Ca(2+)-bound S100A1 as determined by NMR spectroscopy

S100A1 is an EF-hand-containing Ca(2+)-binding protein that undergoes a conformational change upon binding calcium as is necessary to interact with protein targets and initiate a biological response. To better understand how calcium influences the structure and function of S100A1, the three-dimensional structure of calcium-bound S100A1 was determined by multidimensional NMR spectroscopy and compared to the previously determined structure of apo. In total, 3354 nuclear Overhauser effect-derived distance constraints, 240 dihedral constraints, 160 hydrogen bond constraints, and 362 residual dipolar coupling restraints derived from a series of two-dimensional, three-dimensional, and four-dimensional NMR experiments were used in its structure determination (>21 constraints per residue). As with other dimeric S100 proteins, S100A1 is a symmetric homodimer with helices 1, 1', 4, and 4' associating into an X-type four-helix bundle at the dimer interface. Within each subunit there are four alpha-helices and a short antiparallel beta-sheet typical of two helix-loop-helix EF-hand calcium-binding domains. The addition of calcium did not change the interhelical angle of helices 1 and 2 in the pseudo EF-hand significantly; however, there was a large reorientation of helix 3 in the typical EF-hand. The large conformational change exposes a hydrophobic cleft, defined by residues in the hinge region, the C terminus, and regions of helix 3, which are important for the interaction between S100A1 and a peptide (TRTK-12) derived from the actin-capping protein CapZ.     

Collagen: the organic matrix of bone

Collagen is the principal organic matrix in bone. The triple helical region of the molecule is 1014 amino acids long. In fibrils these molecules are staggered axially by integers of 234 residues or 68 nm (D). This axial shift occurs by self-assembly and can be understood in terms of a periodicity in the occurrence of apolar and polar residues in the amino acid sequence. Because the molecular length L = 4.47 D, there are gaps 1.5 X 36.5 nm regularly arrayed throughout the fibrils. The three-dimensional molecular arrangement is a quasi-hexagonal lattice with three distinct values for the principal interplanar spacings. Analysis of the intensity distribution in the medium-angle X-ray diffraction patterns from tendons has produced the following picture of the molecular arrangement in fibrils (Fraser et al. 1983). The molecular helices have a coherent length of 32 nm and are tilted parallel to a specific place within the lattice. A regular azimuthal interaction exists between these helices. This crystalline region could be the overlap region with a non-crystalline gap region. However, the gap is still regular axially and the molecular helices retain their structure; their lateral packing is perturbed although they retain a 'gap'. Neutron and X-ray scattering experiments have shown that calcium hydroxyapatite crystals occur in the gap and are nucleated at a specific though unknown location within the gap. The c-axis of the apatite crystals is parallel to the fibril axis and its length c = 0.688 nm is close to the axial periodicity in a protein with an extended beta-conformation. If the telopeptides at the end of a collagen molecule do have this conformation they would either have a highly heterogeneous conformation or exist in a folded manner because the overall length of the telopeptides is shorter than a regular collagen repeat of 0.029 nm would allow.     

General architecture of the alpha-helical globule

A model is presented for the arrangement of alpha-helices in globular proteins. In the model, helices are placed on certain ribs of "quasi-spherical" polyhedra. The polyhedra are chosen so as to allow the close packing of helices around a hydrophobic core and to stress the collective interactions of the individual helices. The model predicts a small set of stable architectures for alpha-helices in globular proteins and describes the geometries of the helix packings. Some of the predicted helix arrangements have already been observed in known protein structures; others are new. An analysis of the three-dimensional structures of all proteins for which co-ordinates are available shows that the model closely approximates the arrangements and packing of helices actually observed. The average deviations of the real helix axes from those in the model polyhedra is +/- 20 degrees in orientation and +/- 2 A in position (1 A = 0.1 nm). We also show that for proteins that are not homologous, but whose helix arrangements are described by the same polyhedron, the root-mean-square difference in the position of the C alpha atoms in the helices is 1.6 to 3.0 A.     

Design and synthesis of the pseudo-EF hand in calbindin D9K: effect of amino acid substitutions in the alpha-helical regions

A series of 37-residue analogues of the pseudo-EF hand in bovine calbindin D9K has been synthesized by the solid phase method. In the presence of calcium an alpha-helical induction of up to 44% was observed for the peptide with the native sequence with a Kd for calcium binding of 0.35 mM. A number of amino acid substitutions have been carried out to study the packing of the two alpha-helices based on the crystal structure of the entire protein. Three strategies were employed: (1) replacement of the Leu residues, which in the crystal structure do not contribute to the hydrophobic interaction between the two helices, by Gln or Ala in order to control the orientation of the helix packing, (2) stabilization of the individual helix by introducing a Glu-...Lys+ salt bridge or by changing the N-terminal charge to compensate for the helix dipole moment, and (3) introduction of a disulfide bond between the two helices to help the packing of the helices. The mutants with the substitution of (Leu-30, Leu-32) to (Gln-30, Gln-32), (Gln-30, Ala-32), and (Ala-30,Ala-32) designed based on the strategy 1 do not show any affinity for calcium and have low alpha-helicity. The Leu-30 to Lys-30 mutant designed to form a salt bridge between the side chains of Glu-26 and Lys-30 has an apparent Kd for calcium of 6.8 mM. Kd of the N-terminal acetylated and succinylated mutants are 0.41 and 0.45 mM, respectively, and no increase in the alpha-helix content relative to that of the natural sequence peptide is observed. The disulfide containing mutants, namely Tyr-13, Leu-31 to Cys-13, Cys-31 and Tyr-13, Leu-31 to Cys-13, hCys-31, show apparent Kd values of 0.93 and 2.1 mM, respectively. The former mutant shows the highest alpha-helix content among the peptides studied in the presence and absence of calcium. While it is difficult to construct an isolated and rigid helix-loop-helix motif with peptides of this size, introduction of a disulfide bond proved to be effective for this purpose.     

Parallel helix bundles and ion channels: molecular modeling via simulated annealing and restrained molecular dynamics.

A parallel bundle of transmembrane (TM) alpha-helices surrounding a central pore is present in several classes of ion channel, including the nicotinic acetylcholine receptor (nAChR). We have modeled bundles of hydrophobic and of amphipathic helices using simulated annealing via restrained molecular dynamics. Bundles of Ala20 helices, with N = 4, 5, or 6 helices/bundle were generated. For all three N values the helices formed left-handed coiled coils, with pitches ranging from 160 A (N = 4) to 240 A (N = 6). Pore radius profiles revealed constrictions at residues 3, 6, 10, 13, and 17. A left-handed coiled coil and a similar pattern of pore constrictions were observed for N = 5 bundles of Leu20. In contrast, N = 5 bundles of Ile20 formed right-handed coiled coils, reflecting loosened packing of helices containing beta-branched side chains. Bundles formed by each of two classes of amphipathic helices were examined: (a) M2a, M2b, and M2c derived from sequences of M2 helices of nAChR; and (b) (LSSLLSL)3, a synthetic channel-forming peptide. Both classes of amphipathic helix formed left-handed coiled coils. For (LSSLLSL)3 the pitch of the coil increased as N increased from 4 to 6. The M2c N = 5 helix bundle is discussed in the context of possible models of the pore domain of nAChR.     

A homology model of the pore domain of a voltage-gated calcium channel is consistent with available SCAM data

In the absence of x-ray structures of calcium channels, their homology models are used to rationalize experimental data and design new experiments. The modeling relies on sequence alignments between calcium and potassium channels. Zhen et al. (2005. J. Gen. Physiol. doi:10.1085/jgp.200509292) used the substituted cysteine accessibility method (SCAM) to identify pore-lining residues in the Ca_v2.1 channel and concluded that their data are inconsistent with the symmetric architecture of the pore domain and published sequence alignments between calcium and potassium channels. Here, we have built K_v1.2-based models of the Ca_v2.1 channel with 2-(trimethylammonium)ethyl methanethiosulfonate (MTSET)-modified engineered cysteines and used Monte Carlo energy minimizations to predict their energetically optimal orientations. We found that depending on the position of an engineered cysteine in S6 and S5 helices, the ammonium group in the long flexible MTSET-modified side chain can orient into the inner pore, an interface between domains (repeats), or an interface between S5 and S6 helices. Different local environments of equivalent positions in the four repeats can lead to different SCAM results. The reported current inhibition by MTSET generally decreases with the predicted distances between the ammonium nitrogen and the pore axis. A possible explanation for outliers of this correlation is suggested. Our calculations rationalize the SCAM data, validate one of several published sequence alignments between calcium and potassium channels, and suggest similar spatial dispositions of S5 and S6 helices in voltage-gated potassium and calcium channels.     

A structural model for the catalytic cycle of Ca(2+)-ATPase

Ca(2+)-ATPase is responsible for active transport of calcium ions across the sarcoplasmic reticulum membrane. This coupling involves an ordered sequence of reversible reactions occurring alternately at the ATP site within the cytoplasmic domains, or at the calcium transport sites within the transmembrane domain. These two sites are separated by a large distance and conformational changes have long been postulated to play an important role in their coordination. To characterize the nature of these conformational changes, we have built atomic models for two reaction intermediates and postulated the mechanisms governing the large structural changes. One model is based on fitting the X-ray crystallographic structure of Ca(2+)-ATPase in the E1 state to a new 6 A structure by cryoelectron microscopy in the E2 state. This fit indicates that calcium binding induces enormous movements of all three cytoplasmic domains as well as significant changes in several transmembrane helices. We found that fluorescein isothiocyanate displaced a decavanadate molecule normally located at the intersection of the three cytoplasmic domains, but did not affect their juxtaposition; this result indicates that our model likely reflects a native E2 conformation and not an artifact of decavanadate binding. To explain the dramatic structural effect of calcium binding, we propose that M4 and M5 transmembrane helices are responsive to calcium binding and directly induce rotation of the phosphorylation domain. Furthermore, we hypothesize that both the nucleotide-binding and beta-sheet domains are highly mobile and driven by Brownian motion to elicit phosphoenzyme formation and calcium transport, respectively. If so, the reaction cycle of Ca(2+)-ATPase would have elements of a Brownian ratchet, where the chemical reactions of ATP hydrolysis are used to direct the random thermal oscillations of an innately flexible molecule.     

ATP-AMP phosphotransferase from Paracoccus denitrificans

1H NMR is used to study the solution structure of vitamin-D-induced bovine intestinal calcium-binding protein. The study of the native protein is aided by the recently published crystal structure; it is shown that the conformations of the molecule in the crystal and in solution are very similar. The effect of pH and temperature on the native structure is described. The structure of the apo protein is then described, and the effect of pH and temperature on its fold is outlined. A comparison between apo and native protein folds is made which indicates that the folds are very similar. The two folds are related by a calcium titration, which indicates that the protein binds two calcium ions sequentially. Both steps in the Ca2+ titration occur under conditions of slow exchange (kex 80 s-1). The effect of binding Ca2+ ions is to cause twisting motions of helices, with the helices acting as rods, relaying the conformational change induced by Ca2+ binding to the linker regions of the protein.     

Structure based mechanism of the Ca(2+)-induced release of coelenterazine from the Renilla binding protein

The crystal structure of the Ca(2+)-loaded coelenterazine-binding protein from Renilla muelleri in its apo-state has been determined at resolution 1.8 A. Although calcium binding hardly affects the compact scaffold and overall fold of the structure before calcium addition, there are easily discerned shifts in the residues that were interacting with the coelenterazine and a repositioning of helices, to expose a cavity to the external solvent. Altogether these changes offer a straightforward explanation for how following the addition of Ca(2+), the coelenterazine could escape and become available for bioluminescence on Renilla luciferase. A docking computation supports the possibility of a luciferase-binding protein complex.     

Conformational analysis of polynucleotides. I. The favorable left-handed helical model for the poly(8,2''-S-cycloadenylic acid) with high anti conformation.

1) Energy calculations have shown that poly (8,2'-S-cycloadenylic aicd) can form left-handed helices owing to the high anti conformation. 2) Two favorable left-handed helices are characterized by axial translation per residue (Z=4.3 and 3.6A) and by rotations per residue (theta= 40 degrees and -25 degrees). 3) The proposed helical models might be stable in aqueous solution and is well explicable of the optical property of this compound.     

A model for micellar aggregates of a bile salt: crystal structure of sodium taurodeoxycholate monohydrate

Crystals of sodium taurodeoxycholate monohydrate, NaC26H44NO6S X H2O, are trigonal, space group P3(1), with a = 18.393(1), c = 7.097(1)A, V = 2079.3(5)A3, and Z = 3. The structure was solved by direct methods and Fourier techniques and refined by full-matrix least-squares calculations. The final R index is 0.051. The side chair of the anion displays an approximate folded-back conformation. The cyclopentane ring assumes an intermediate conformation between the half-chain and the beta-envelope. The sodium ion shows a distorted octahedral coordination with six oxygen atoms, giving rise to ion-ion and ion-dipole interactions. The molecules form helices, characterized by threefold screw axes, with a radius of about 16 A. The helices are packed in such a way as to be embedded in each other as cog-wheels. The helix found in this crystal structure will be used as a model and checked in the study of the micellar solutions of sodium taurodeoxycholate, following the same strategy satisfactorily employed in the case of sodium deoxycholate.     

An asymmetric conformation of 1,3,5-benzene tricarbonyl [Aib4OMe]3.

Molecules of 1,3,5-benzene tricarbonyl [Aib(4)OMe](3) do not possess any internal symmetry, neither exact nor approximate, in the crystalline state. The Aib(4)OMe moieties each form a 3(10)-helix with an appropriate pair of hydrogen bonds but the sense of rotation is right-handed for two of the helices and left-handed for the third one. The helices are not evenly positioned around the benzene ring, and their helix axes are inclined toward one side of the plane of the benzene ring, giving the molecule the shape of a shallow bowl with an irregular periphery. The molecules are largely surrounded by water and dimethyl sulfoxide (DMSO) solvent molecules that form hydrogen bonds with the CO and NH moieties that protrude from the surfaces of the peptide molecule. The space group is Cc with a = 23.618(4) A, b = 19.708(6) A, c = 17.939(7) A and beta = 100.09(3) degrees.     

Molecular structure of the rhamsan-like exocellular polysaccharide RMDP17 from Sphingomonas paucimobilis.

X-Ray diffraction analysis of the sodium salt of the polysaccharide RMDP17, a 2-deoxy rhamsan analog, reveals that it adopts a gellan-like, half-staggered, threefold, left handed, double helix of pitch 57.4 A. The side chain of the branched polymer is hydrogen bonded to the main chain. Sodium ions, linked to the carboxylate groups, promote the association of helices via water molecules. Two helices of opposite polarity occupy a trigonal unit cell of dimensions a=17.6 and c=28.7 A. The packing arrangement displays a series of hydrogen bonds involving main chain and side chain atoms, as well as some water bridges, between the helices.