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N Go

Publications and source records attributed to N Go.

At least 73 records · Page 4Linked to original sources
PubMed1986

Conformations of cyclo(L-orD-Phe-L-Pro-Aca) and cyclo(L-Pro-L- or D-Phe-Aca). Cyclized dipeptide models for specific types of beta-bends.

Conformational analyses on four cyclic model peptides of the beta-bend, cyclo(L- or D-Phe-L-Pro-epsilon-aminocaproyl(Aca] and cyclo(L-Pro-L- or D-Phe-Aca), were carried out both experimentally and theoretically. Cyclo(D-Phe-L-Pro-Aca) was shown to exist as a single conformer taking the type II' beta-bend. The comparison of its CD spectra with those of cyclo(L-Ala-L-Ala-Aca) revealed that type I and II' beta-bends, both with alpha-helix-like CD spectra, can be distinguished. Cyclo(L-Phe-L-Pro-Aca) was shown to exist as a single conformer with a cis L-Phe-L-Pro peptide bond, taking the type VI beta-bend. Its CD spectrum has thus been observed for the first time for the bend containing a cis peptide bond. Cyclo(L-Pro-L-Phe-Aca) was shown to exist as a mixture of two conformers, the major one taking the type I beta-bend with a trans Aca-L-Pro peptide bond and the minor one with a cis Aca-L-Pro peptide bond. Cyclo(L-Pro-D-Phe-Aca) was suggested to exist as a mixture of two conformers, the major one taking the type II beta-bend with a trans Aca-L-Pro peptide bond and the minor one with a cis Aca-L-Pro peptide bond.

Dipeptides↗
PubMed1985

Calculation of protein conformations by proton-proton distance constraints. A new efficient algorithm.

We have developed a method to determine the three-dimensional structure of a protein molecule from such a set of distance constraints as can be determined by nuclear magnetic resonance studies. The currently popular methods for distance geometry based on the use of the metric matrix are applicable only to small systems. The method developed here is applicable to large molecules, such as proteins, with all atoms treated explicitly. This method works in the space of variable dihedral angles and determines a three-dimensional structure by minimization of a target function. We avoid difficulties hitherto inherent in this type of approach by two new devices: the use of variable target functions; and a method of rapid calculation of the gradient of the target functions. The method is applied to the determination of the structures of a small globular protein, bovine pancreatic trypsin inhibitor, from several artificial sets of distance constraints extracted from the X-ray crystal structure of this molecule. When a good set of constraints was available for both short- and long-range distances, the crystal structure was regenerated nearly exactly. When some ambiguities, such as those expected in experimental information, are allowed, the protein conformation can be determined up to a few local deformations. These ambiguities are mainly associated with the low resolving power of the short-range information.

Aprotinin↗
PubMed1985

Induced fitting between a complex of four nucleotides and the cognate amino acid.

The conformation of the hydrogen-bonded complex of a trinucleoside diphosphate (anticodon bases), a nucleic acid base (discriminator base), and an amino acid is investigated. This complex has been named C4N (complex of the four nucleotides) by one of the authors. Concerning the aminoacylation of tRNA and the genetic code, it has been proposed that C4N accepts the cognate protein amino acid by the lock-and-key relationship. The purpose of the calculation is to investigate the conformational and energetic properties of C4N from the energy minimum principle. The calculation is carried out by using the empirical potential functions. Glycine, glutamine, and valine are taken as typical cases. The formation energies are estimated. It is shown that some conformational changes are induced in the anticodon trinucleoside diphosphate by the binding of the discriminator base. Conformational changes of C4N and the amino acid are also induced by the binding of the amino acid to C4N.

Amino Acids↗
PubMed1984

The consistency principle in protein structure and pathways of folding.

It is pointed out that various energy terms contributing to stabilize the native state of globular proteins are consistent in the first approximation with each other in the native state. This means that each energy term is individually minimized at the minimum point of the total energy. I proposed (1) to call this fact "the consistency principle in protein structure." The fair success of various methods of prediction of the secondary structures in globular proteins from their amino acid sequence is often interpreted as indicating the dominance of the short-range interactions in determining the local structures of the polypeptide chains. Partly from such a point of view, the hierarchic condensation model has been popular for the process of protein folding. However the consistency principle indicates that the short-range interactions are just one type of intramolecular interaction which contributes to stabilization of the native structure together with other mutually consistent types of intramolecular interactions. Therefore the hierarchic condensation model is not necessarily a unique model of protein folding. Roles of a possible nonspecific globular state, stabilized by nonspecific long-range intramolecular interactions, in the folding process are discussed. It is expected that this nonspecific globular state is observed either as an equilibrium or a kinetic intermediate state between the unfolded and the folded native states. Observation as a kinetic intermediate state is expected to occur in experiments done under strongly refolding conditions. In this case the polypeptide chain in the unfolded state collapses into a nonspecific globule by the action of nonspecific long-range intramolecular interactions. Two possible mechanisms of the transition from the nonspecific globular state to the specific native folded state are discussed. In an experiment done under weakly refolding conditions, folding is expected to occur according to the embryo-nucleus model. This model is a refined version of the hierarchic condensation model. Refinement is done by taking into account the fact that the intermediate structures assumed in the hierarchic condensation model are unstable against both the native folded state and the unfolded state. A nucleus is an ordered structure of a certain size. Ordered structures of a size larger than a nucleus tend to fold further to become the native specific globule. Ordered structures of a size smaller than a nucleus tend to unfold. Embryos are intrinsically unstable ordered structures smaller than a nucleus. Folding occurs when embryos grow in size to become a nucleus.(ABSTRACT TRUNCATED AT 400 WORDS)

Drug Stability↗
PubMed1983

Conformational change of a globular protein elucidated at atomic resolution. Theoretical and nuclear magnetic resonance study.

A powerful method of conformational energy minimization which uses both first and second derivatives of the energy function is applied both to a small globular protein, bovine pancreatic trypsin inhibitor (BPTI), consisting of 58 amino acid residues and to its chemical derivative obtained by carboxamidomethylation of cysteinyl residues of the 14-38 disulphide bond. Conformational fluctuations are also calculated from the second derivative matrix obtained at the respective minimum energy conformations. Appreciable conformational changes upon chemical modification are observed only in the vicinity of the site of the modification. The nuclear magnetic resonance data on both BPTI and the modified BPTI are analyzed to compare with the calculated conformational changes upon chemical modification. Good correlations are found between the theoretically predicted and experimentally deduced conformational changes. The theoretical method employed here has a general application for the calculation of small conformational changes of globular proteins upon their chemical modification or an amino acid substitution.

Aprotinin↗
PubMed1983

Dynamics of a small globular protein in terms of low-frequency vibrational modes.

Normal modes of low-frequency vibrations are calculated for a small globular protein, bovine pancreatic trypsin inhibitor. In modes with frequencies below 120 cm-1 the protein molecule behaves like a continuous elastic body. Most modes with frequencies above 50 cm-1 are shown to behave harmonically within the range of thermal fluctuations at room temperature. Those with frequencies below 50 cm-1 show some anharmonicity. Magnitudes of displacements of atoms are mainly determined by the modes with frequencies below 30 cm-1. These very-low-frequency modes contribute significantly to the entropy of the system. The dynamic structure of the globular protein is described as a superposition of harmonic high-frequency motions and coupled anharmonic low-frequency motions of collective variables corresponding to the normal modes of vibration.

Animals↗
PubMed1983

Randomness of the process of protein folding.

How specific or definite are pathways of folding and unfolding in globular proteins? In order to study this question, computer simulation of the folding-unfolding transition was carried out in a two-dimensional lattice model of proteins in which it is assumed that strongly specific intramolecular interactions contribute to the stability of the native conformation. This specificity of the interactions should tend to make the pathways of folding and unfolding more definite than reality. Yet, the analysis of the record of simulation indicated the process of transition to be stochastic rather than definite. This poses a fundamental problem of how to describe the pathways of folding and unfolding transition. It is argued that the description should consist of (i) a definition of intermediate states in terms of characteristic conformational features and (ii) stochastic rules of transitions between these intermediate states. The simplest would be the case in which the transitions occur as a markoffian process.

Kinetics↗
PubMed1983

Markoffian description of the process of protein folding.

A long record of computer simulation of folding-unfolding transition in a two-dimensional lattice model of protein as monitored by one conformational order parameter was studied to see if it could be approximated by a markoffian process. For this purpose the normalized time correlation functions of the order parameter were calculated (i) directly from the record of simulation and (ii) by assuming the markoffian behavior of the record. Both of them can be well approximated by a sum of two simple exponential terms. The relaxation time of the slow relaxing term, which corresponds to the overall folding-unfolding transition, becomes very short when the markoffian assumption is made. From this observation we conclude that intermediate states defined by one more-or-less arbitrarily chosen conformational parameter are, in general, collections of very heterogeneous conformations and therefore transitions between them cannot be markoffian. This indicates the importance of multi-parameter observation of dynamic process of folding. Characteristic features of the method of trapping disulfide intermediates are discussed.

Computers↗
PubMed1983

Theoretical and experimental approach to recognition of amino acid by tRNA.

The C4N model concludes that the pocket on the complex of the anticodon bases and the discriminator base on a tRNA can accept the corresponding protein amino acid. A theoretical molecular computation by using the energy minimum principle is carried out to find the energy-refined C4N conformation. The results for Gln and Val suggest that not only the lock and key relationship but the induced fitting effect occurs. Some experiments to detect the interaction between the polynucleotides and the amino acid are being attempted.

Amino Acids↗
PubMed1981

Monte Carlo simulation study of thermal fluctuations and conformational energy surface of a small protein, basic pancreatic trypsin inhibitor.

The conformation energy surface of a small protein, basic pancreatic trypsin inhibitor, is studied to characterize small-amplitude thermal fluctuations in the protein molecule. In order to see the shape of the conformational energy surface near the energy minimum point, the thermal equilibrium of the molecule is stimulated by the Monte Carlo method of Metropolis et al. From the sample of the equilibrium population, which reflects the shape of the energy surface, orthogonal directions are generated in the conformational space, and the conformational energy is actually calculated along these directions. All energy profiles along these directions are found to be approximately a parabola within the range of thermal fluctuations, which suggests the possibility of harmonic approximation to the conformational energy surface of the globular protein.

Aprotinin↗