Search PubMed⌕ Search

SEARCH · Search PubMed

Results for “Secondary structure”

Search indexed PubMed citations on genomics, clinical trials, systematic reviews and public health. Explore titles, authors and supplied subject terms, then open the PubMed record.

Quote a phrase for an exact phrase match. Source license links do not imply unrestricted reuse.

At least 973 records · Page 54Linked to original sources
PubMed2005

STARS: statistics on inter-atomic distances and torsion angles in protein secondary structures.

UNLABELLED: A graphics package has been developed for performing statistics on interatomic distances and torsion angles in protein secondary structures (STARS) from a protein crystal structure database. It allows one to obtain both the graphical view and the text format of distributions of the distances and angles for atoms located in 10 types of protein secondary structures. STARS will facilitate assignment of ambiguous NOESY peaks, structure determination by nuclear magnetic resonance, structure validation and comparison of protein folds. AVAILABILITY: All data, documents and execute files are freely downloadable at http://stars.zhengyuhome.com. The software works appropriately on Windows system, without any compilation or installation. CONTACT: dbsydw@nus.edu.sg.

Computer Graphics↗
PubMed1987

Stabilization of acetylcholine receptor secondary structure by cholesterol and negatively charged phospholipids in membranes.

Fourier-transform infrared (FTIR) spectroscopy was used to study the secondary structure of purified Torpedo californica nicotinic acetylcholine receptor (AChR) in reconstituted membranes. Functional studies have previously demonstrated that the ion channel activity requires the presence of both sterol and negatively charged phospholipids in membranes. The present studies are designed to test the hypothesis that the alpha-helical structure of AChR may be stabilized by specific lipid molecules (sterol and/or negatively charged phospholipids) and that these alpha-helices may be responsible for the formation of a potential ion channel. FTIR data show statistically significant (p less than 0.005) spectral changes due to cholesterol and negatively charged phospholipids, respectively. On the basis of standard curves describing the relationship between the spectral properties and the secondary structural contents of water-soluble proteins, the observed spectral change at 931 cm-1 can be interpreted as an apparent change in the alpha-helix content from about 17% in the absence of sterols to about 20% in the presence of sterols, suggesting that protein-sterol interactions increase the helical structure of the AChR molecule. Similarly, the spectral change at 988 cm-1 can be interpreted as an apparent increase of beta-sheet content in the AChR molecule from about 20% to about 24% due to the presence of negatively charged phospholipids. Functional AChR in membranes thus appears to be correlated with higher alpha-helical and beta-sheet contents. It is concluded that one role of specific interactions between membrane protein and lipid molecules may be to maintain specific secondary structures necessary to support the ion channel function of AChR.

Animals↗
PubMed2003

Accurate and automated classification of protein secondary structure with PsiCSI.

PsiCSI is a highly accurate and automated method of assigning secondary structure from NMR data, which is a useful intermediate step in the determination of tertiary structures. The method combines information from chemical shifts and protein sequence using three layers of neural networks. Training and testing was performed on a suite of 92 proteins (9437 residues) with known secondary and tertiary structure. Using a stringent cross-validation procedure in which the target and homologous proteins were removed from the databases used for training the neural networks, an average 89% Q3 accuracy (per residue) was observed. This is an increase of 6.2% and 5.5% (representing 36% and 33% fewer errors) over methods that use chemical shifts (CSI) or sequence information (Psipred) alone. In addition, PsiCSI improves upon the translation of chemical shift information to secondary structure (Q3 = 87.4%) and is able to use sequence information as an effective substitute for sparse NMR data (Q3 = 86.9% without (13)C shifts and Q3 = 86.8% with only H(alpha) shifts available). Finally, errors made by PsiCSI almost exclusively involve the interchange of helix or strand with coil and not helix with strand (<2.5 occurrences per 10000 residues). The automation, increased accuracy, absence of gross errors, and robustness with regards to sparse data make PsiCSI ideal for high-throughput applications, and should improve the effectiveness of hybrid NMR/de novo structure determination methods. A Web server is available for users to submit data and have the assignment returned.

Automation↗
PubMed1996

Secondary structure changes and peptic hydrolysis of beta-lactoglobulin induced by diols.

The addition of ethylene glycol, and 1,2- and 1,3-propanediol, decreases the bulk dielectric constant of the medium, and according to CD measurements, increases significantly the proportion of helical structure in beta-lactoglobulin. The medium-induced folding changes followed by limited peptic hydrolysis show that the cleavage of beta-lactoglobulin by pepsin is triggered by structural transformations induced by ethylene glycol only and not by 1, 2- and 1, 3-propanediol. Density measurements, at constant chemical potential and constant molality, demonstrate that all diols are present in the immediate domain of the protein. They are engaged in hydrophobic interactions with the amino acids of beta-lactoglobulin core inducing the formation of additional alpha-helices.

Alcohols↗
PubMed1997

Thermodynamic model of secondary structure for alpha-helical peptides and proteins.

A thermodynamic model describing formation of alpha-helices by peptides and proteins in the absence of specific tertiary interactions has been developed. The model combines free energy terms defining alpha-helix stability in aqueous solution and terms describing immersion of every helix or fragment of coil into a micelle or a nonpolar droplet created by the rest of protein to calculate averaged or lowest energy partitioning of the peptide chain into helical and coil fragments. The alpha-helix energy in water was calculated with parameters derived from peptide substitution and protein engineering data and using estimates of nonpolar contact areas between side chains. The energy of nonspecific hydrophobic interactions was estimated considering each alpha-helix or fragment of coil as freely floating in the spherical micelle or droplet, and using water/cyclohexane (for micelles) or adjustable (for proteins) side-chain transfer energies. The model was verified for 96 and 36 peptides studied by 1H-nmr spectroscopy in aqueous solution and in the presence of micelles, respectively ([set 1] and [set 2]) and for 30 mostly alpha-helical globular proteins ([set 3]). For peptides, the experimental helix locations were identified from the published medium-range nuclear Overhauser effects detected by 1H-nmr spectroscopy. For sets 1, 2, and 3, respectively, 93, 100, and 97% of helices were identified with average errors in calculation of helix boundaries of 1.3, 2.0, and 4.1 residues per helix and an average percentage of correctly calculated helix-coil states of 93, 89, and 81%, respectively. Analysis of adjustable parameters of the model (the entropy and enthalpy of the helix-coil transition, the transfer energy of the helix backbone, and parameters of the bound coil), determined by minimization of the average helix boundary deviation for each set of peptides or proteins, demonstrates that, unlike micelles, the interior of the effective protein droplet has solubility characteristics different from that for cyclohexane, does not bind fragments of coil, and lacks interfacial area.

Enzymes↗
PubMed1998

Molecular simulation of the primary and secondary structures of the Abeta(1-42)-peptide of Alzheimer's disease.

The major protein constituent of the deposits of Alzheimer's disease is the so-called amyloid beta-peptide (Abeta) which was derived from proteolysis of a large transmembrane amyloid precursor protein. Some physicochemical and biological properties of the Abeta(1-42) peptide are described in this paper. Three functional areas of the soluble Abeta(1-42) peptide were found: (i) a lipophilic region in the middle of the peptide (Lys16 to Ala21), (ii) a second lipophilic core at the end (Lys28 to Val40), and (iii) polarized and charged, solvent-exposed areas. Using molecule coordinates found experimentally by NMR-solution spectroscopy, subsequent Gasteiger-MM+ geometry optimization led to the result that the first lipophilic core has an alpha-helical structure which is stabilized by intramolecular hydrogen-bonding forces. The result is a loop-like molecule. The second lipophilic core has a beta-sheet structure, and is able to form long-ranged, noncovalent, mainly hydrophobic forces with other beta-sheets of Abeta peptides. The beta-strands run in an antiparallel direction. The aggregates are highly stable and ordered. The negatively charged, solvent-exposed residues are potential sites for a crosslinking with membrane-bound receptors. A perspective in drug research is the development of drugs that bind to individual beta-sheets by noncovalent interactions, blocking the associations between the individual Abeta peptides and preventing the formation of amyloid aggregates.

Alzheimer Disease↗
PubMed1998

Two-dimensional mid-IR and near-IR correlation spectra of ribonuclease A: using overtones and combination modes to monitor changes in secondary structure.

We introduce near-IR spectroscopy as an ancillary tool for monitoring structural changes of proteins in aqueous solution using ribonuclease A (RNase A) as a model protein. The thermal unfolding of RNase A results in clear spectral changes in the near-IR and the mid-IR regions. In the near-IR the most pronounced changes are observed in the spectral region between 4820 and 4940 cm-1. The strong N-H combination band found at 4867 cm-1 in the spectrum of native RNase A shifts to 4878 cm-1 upon thermal unfolding. Hydrogen-deuterium exchange experiments that validate the N-H character of this mode can also be used to estimate the number of unexchanged amide protons after exposure to D2O. The transition profiles and temperatures derived from the temperature dependence of the N-H combination mode were found to be practically identical with those derived from the temperature dependence of the C = O amide I band in the mid-IR region, demonstrating that the near-IR region can be used as a conformation-sensitive monitor for the thermally induced unfolding of proteins in H2O solution. A 2-dimensional correlation analysis was applied to the mid-IR and near-IR spectra of RNase A to establish correlations between IR bands in both regions. The correlation analysis demonstrates that the thermal unfolding of RNase A is not a completely cooperative process; rather it begins with some changes in beta-sheet structure, followed by the loss of alpha-helical structures, and then ending with the unfolding of the remaining beta-sheets.

Amides↗
PubMed2001

Differences in secondary structure of HAV-synthetic peptides induced by the sequential order of T- and B-cell epitopes.

The present study was undertaken to examine the structural features of two peptide constructs designed on the basis of linear combination of B and T-cell epitopes in different orientations (BT and TB) that may be important to explain the differences in the elicited antihepatitis A virus immune response and in the interaction with biological model membranes. A CD study was carried out and the corresponding quantitative analysis of the experimental data was done using deconvolution computer programs. Moreover, fluorescence experiments were performed to analyze differences in the fluorescence emission spectra of both molecules. The main conformational difference by CD studies was obtained working in aqueous medium. Although the TB sequence adopted a preferably random coil structure, the BT peptide was best fitted with beta-type structures. These results are further supported by fluorescence studies. These findings have relevance for the design of synthetic immunopeptides.

Amino Acid Sequence↗
PubMed2000

CIDEP effects of intramolecular quenching of singlet and triplet excited states by nitroxide radicals in oligopeptides: a potentially useful new method for investigating peptide secondary structures in solution.

Two hexapeptides, each bearing one photoactive alpha-amino acid (Bin or Bpa) and one nitroxide-containing TOAC residue, have been synthesized and fully characterized. FT-IR absorption measurements indicate that a 3(10)-helical conformation is adopted by these peptides in solution. As two amino acid units separate the photoactive residue from TOAC in the peptide sequences, the two moieties face each other at a distance of about 6 A after one complete turn of the ternary helix. Irradiation by a light pulse from an excimer laser populates the excited states localized on the chromophores. An intramolecular interaction between the singlet (Bin) or triplet (Bin and Bpa) excited states and the doublet state of the TOAC nitroxide makes a spin-selective decay pathway possible, that produces transient spin polarization. In addition, in order to determine whether the intramolecular exchange interaction occurs through-bond or through-space, we have prepared linear and cyclic TOAC-Bin dipeptide units. A CIDEP study revealed that a through-space intramolecular interaction is operative. The observation of spin polarization makes the two helical hexapeptides suitable models to test the possibility of application of this novel technique to conformational studies of peptides in solution.

Cyclic N-Oxides↗
PubMed2001

Raman spectroscopy of secondary structure of elastinlike polymer poly(GVGVP).

Raman spectra of the elastinlike polypentapeptide poly(GVGVP) were measured in H(2)O and D(2)O as solutions and, after increasing the temperature, as suspensions and sediments. In addition, spectra of the polypentapeptide in the solutions of increasing concentration and in the solid state were also investigated by gradually evaporating the water. Significant changes in band frequencies, intensities, and shapes were found for selected Raman bands in the measured spectra, particularly for the C-H stretching, the glycine CH(2) wagging, and some amide vibrations. The C-H stretching vibrations are influenced predominantly by the presence of water, the glycine CH(2) wagging vibrations are associated with conformational transitions. Three possible types of poly(GVGVP)s in the presence of water were indicated: polymer chains in a relatively extended state in the solution, a beta-spiral structure in the suspension, and irregularly bent chains in the sediment.

Elastin↗
PubMed2005

Synthesis and secondary structure of oligo(alpha-isobutyl beta,L-aspartate)s.

The oligo(beta-peptide)s, hexa(alpha-isobutyl beta,L-aspartate) (Hex-AIBLA) and octa(alpha-isobutyl beta,L-aspartate) (Oct-AIBLA), were synthesized in solution by using standard coupling methods. Powder x-ray diffraction showed that the octamer crystallized in the two helical crystal forms known to exist in the homologous poly(beta-peptide), whereas the hexamer seemed to adopt an extended conformation. Both CD and 1H-NMR spectra of Oct-AIBLA in MeOH revealed the presence of a regularly folded conformation in this solvent, presumably the 3(14) helix. The helix-to-coil transition of Oct-AIBLA was observed to take place upon heating in both MeOH and CHCl3, in the second case associated with a not-well-defined aggregation-disaggregation process. The spectroscopic evidence obtained on the presence of folded structures in Hex-AIBLA were much weaker than for the octamer.

Circular Dichroism↗
PubMed1992

A molecular thermodynamic approach to predict the secondary structure of homopolypeptides in aqueous systems.

Under physiological conditions, many polypeptide chains spontaneously fold into discrete and tightly packed three-dimensional structures. The folded polypeptide chain conformation is believed to represent a minimum Gibbs energy of the system, governed by the weak interactions that operate between the amino acid residues and between the residues and the solvent. A semiempirical molecular thermodynamic model is proposed to represent the Gibbs energy of folding of aqueous homopolypeptide systems. The model takes into consideration both the entropy contribution and the enthalpy contribution of folding homopolypeptide chains in aqueous solutions. The entropy contribution is derived from the Flory-Huggins expression for the entropy of mixing. It accounts for the entropy loss in folding a random-coiled polypeptide chain into a specific polypeptide conformation. The enthalpy contribution is derived from a molecular segment-based Non-Random Two Liquid (NRTL) local composition model [H. Renon and J. M. Prausnitz (1968) AIChE J., Vol. 14, pp. 135-142; C.-C. Chen and L. B. Evans (1986) AIChE J., Vol. 32, pp. 444-454], which takes into consideration of the residue-residue, residue-solvent, and solvent-solvent binary physical interactions along with the local compositions of amino acid residues in aqueous homopolypeptides. The UNIFAC group contribution method [A. Fredenslund, R. L. Jones, and J. M. Prausnitz (1975) AIChE J., 21, 1086-1099; A. Fredenslund, J. Gmehling, and P. Rasmussen (1977) Vapor-Liquid Equilibrium Using UNIFAC, Elsevier Scientific Publishing Company, Amsterdam], developed originally to estimate the excess Gibbs energy of solutions of small molecules, was used to estimate the NRTL binary interaction parameters. The model yields a hydrophobicity scale for the 20 amino acid side chains, which compares favorably with established scales [Y. Nozaki and C. Tanford (1971) Journal of Biological Chemistry, Vol. 46, pp. 2211-2217; E. B. Leodidis and T. A. Hatton (1990) Journal of Physical Chemistry, Vol. 94, pp. 6411-6420]. In addition, the model generates qualitatively correct thermodynamic constants and it accurately predicts thermodynamically favorable folding of a number of aqueous homopolypeptides from random-coiled states into alpha-helices. The model further facilitates estimation of the Zimm-Bragg helix growth parameter s and the nucleation parameter sigma for amino acid residues [B. H. Zimm and J. K. Bragg (1959) Journal of Chemical Physics, Vol. 31, pp. 526-535]. The calculated values of the two parameters fall into the ranges suggested by Zimm and Bragg.

Models, Molecular↗
PubMed2003

beta-Hairpins, alpha-helices, and the intermediates among the secondary structures in the energy landscape of a peptide from a distal beta-hairpin of SH3 domain.

Energy landscape of a peptide, extracted from a distal beta-hairpin of src SH3 domain, in explicit water was obtained with the multicanonical molecular dynamics. A variety of beta-hairpins with various strand-strand hydrogen bonds were found in the energy landscape at 300 K. There was no energy barrier between random-coil and hairpins. Thus, the peptide conformation can easily change from the random-coil to the hairpins in the thermal fluctuations at 300 K. The landscape also included two clusters of alpha-helices, among which an energy barrier existed, and besides, these helix clusters were separated from the other conformations. Thus, the free-energy barrier exists among the helices and the other conformations. Intermediate clusters were found between the helix and the hairpin clusters. The current study showed that the isolated state of this peptide in water fluctuates among random-coil, beta-hairpin, and alpha-helix. In SH3 domain, which has a topology of mainly beta-protein, the whole-protein folding may proceed when the segment is folded in the beta-hairpin and the other parts of the protein are coupled with the beta-hairpin in an energetically or kinetically favorite way.

Algorithms↗