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N Go

Publications and source records attributed to N Go.

At least 55 records · Page 3Linked to original sources
PubMed1990

Deoxymyoglobin studied by the conformational normal mode analysis. I. Dynamics of globin and the heme-globin interaction.

Dynamic properties of deoxymyoglobin are studied theoretically by the analysis of conformational fluctuations. Root-mean-square atomic fluctuations and distance fluctuations between different segments reveal the mechanical construction of the molecule. Eight alpha-helices behave as relatively rigid bodies and corner regions are more flexible, showing larger fluctuations. More particularly, corner regions EF and GH are specific in that flanking alpha-helices extend their rigidity up to a point in the corner region and the two rigid segments are connected flexibly at that point. The FG corner is exceptional. A segment from the F helix to the beginning of the G helix, in which the FG corner is included, becomes relatively rigid by means of strong interactions with the heme group. The whole myoglobin molecule is divided into two large units of motion, one extending from the B to the E helix, and the other from the F to the H helix. These two units are connected covalently by the EF corner. However, dynamic interactions between these two units take place mainly through contacts between helices B and G and not through the EF corner. From correlation coefficients between fluctuational motions of residues and the heme group, 55 residues are identified as having strong dynamic interactions with the heme moiety. Among them, 18 residues in the three segments, one consisting of residues from the C helix to the CD corner, a second consisting of the E helix, and a third from the F helix to the beginning of the G helix, are in close contact with the heme group. Twenty-two of the 55 residues are within four residues of the 18 residues in their sequential residue number and are more than 3 A away from the heme group. The other 15 residues are located further in the sequential residue number and are all found in helices A and H. They are more than 6 A away from the heme group. By the use of correlation coefficients of fluctuations between residues, it is found that dynamic interaction with the heme group is transmitted to the A helix and the beginning of the H helix in the direction Leu(E15)----[Val(All) and Trp(A12)]. The transmission to the C-terminal end of the H helix is mediated by a long segment, from the end of the EF corner to the beginning of the G helix, that lies on the heme group and has close contacts over a wide range.(ABSTRACT TRUNCATED AT 400 WORDS)

Amino Acid Sequence↗
PubMed1990

Deoxymyoglobin studied by the conformational normal mode analysis. II. The conformational change upon oxygenation.

The conformational change taking place in myoglobin concomitantly with the observed geometrical change at the heme-His(F8) linkage upon oxygenation is studied by normal mode analysis, which is based on the quadratic approximation of the conformational energy function. The heme-globin interaction energy increases for this change by 8.114 kcal/mol when both the heme group and the globin molecule are held rigid. When they are permitted flexibility, the interaction energy relaxes by 7.038 kcal/mol, and the difference (1.076 kcal/mol) is distributed as strain energy within the molecule. This increase is the work necessary for the heme group to move against the force exerted by the globin. If the force is assumed to be invariable during this move, the work is small, 0.276 kcal/mol, meaning that the force is strongly variable. Furthermore, this means that the heme group is located near the equilibrium point of the potential energy of the heme-globin interaction. The change in the localized strain energy stored in the force field at the linkage between the heme and the imidazole of HisF8 is estimated to be of the same order of magnitude as the distributed energy. The largest atomic displacements are observed at the region from the F helix to the beginning of the G helix, and secondary large displacements occur at several regions, i.e, the A helix, from the C helix to the CD corner, the E helix, and the C-terminal side of the H helix. All of these regions have strong dynamic interactions with the heme group, either directly or indirectly. Their secondary structures show complex deformations. In other parts, relatively rigid segments undergo rotational and/or bending changes in a way consistent with the large changes described above and close atomic packing within the molecule. The calculated conformational change is decomposed to vibrational normal modes of deoxymyoglobin. The magnitude of the conformational change, measured by the mass-weighted mean-square atomic displacement, is accounted for up to 92.0% by the 151 normal modes with frequencies lower than 40 cm-1. In descending order of contribution, the first six modes, each of which has a frequency lower than 12 cm-1, account for up to 57.4%. This means that the functionally important conformational change can well be expressed in terms of a relatively small number of collective low frequency normal modes.

Calorimetry↗
PubMed1990

Normal mode analysis of human lysozyme: study of the relative motion of the two domains and characterization of the harmonic motion.

A normal mode analysis of human lysozyme has been carried out at room temperature. Human lysozyme is an enzyme constituted of two domains separated by an active site cleft, the motion of which is thought to be relevant for biological function. This motion has been described as a hinge bending motion. McCammon et al. have determined the characteristics of the hinge bending motion but they assumed a prior knowledge of the hinge axis. In this work we propose a method which is free from this assumption and determines the hinge axis and root mean square (rms) rotation angle which give the best agreement with the pattern of changes in all the distances between nonhydrogen atoms in the two domains, obtained by the normal mode analysis. The hinge axis we found is notably different from the one previously determined and goes, roughly, through the C alpha 55 and C alpha 76, i.e., it is located at the base of the beta-sheet of the second domain. The rms value for the rotation angle is also twice as large as the previous one: 3.37 degrees. It is shown that this hinge bending motion provides a fairly good approximation of the dynamics of human lysozyme and that the normal mode with the lowest frequency has a dominating contribution to this hinge bending motion. A study of the accessible surface area of the residues within the cleft reveals that the motion does not result in a better exposure to the solvent of these residues. A characterization of the thermally excited state (under the hypothesis of the harmonicity of the potential energy surface) has been done using the concept of topology of atom packing. Under this hypothesis the thermal fluctuations result only in a small change of the topology of atom packing, leading therefore to nearly elastic deformations of the protein.

Humans↗
PubMed1990

A theorem on amplitudes of thermal atomic fluctuations in large molecules assuming specific conformations calculated by normal mode analysis.

An exact theorem is proved and its implication is discussed. The theorem states that, if a large molecule, typically biological macromolecules such as proteins, undergoes small-amplitude conformational fluctuations around its native conformation in such a way that within the range of conformational fluctuations at thermal equilibrium the conformational energy surface can be approximated by a multidimensional parabola, then the mass-weighted mean-square displacement of constituent atoms is given by the sum of the contributions from each normal mode of conformational vibration, which in turn is proportional to the inverse of the square of its frequency. This theorem provides a firm theoretical basis for the fact hitherto empirically recognized in the conformational dynamics of, for instance, native proteins that very-low-frequency normal modes make dominant contributions to the conformational fluctuations at thermal equilibrium. Discussion is given on the implication of this theorem, especially on the importance of the concept of the low-frequency normal modes, even in the case where the basic assumption of the harmonicity of the energy surface does not hold.

DNA↗
PubMed1990

Refinement of protein dynamic structure: normal mode refinement.

An x-ray crystallographic refinement method, referred to as the normal mode refinement, is proposed. The Debye-Waller factor is expanded in terms of the effective normal modes whose amplitudes and eigenvectors are experimentally determined by the crystallographic refinement. In contrast to the conventional method, the atomic motions are treated generally as anisotropic and concerted. This method is assessed by using the simulated x-ray data given by a Monte Carlo simulation of human lysozyme. In this article, we refine the dynamic structure by fixing the average static structure to exact coordinates. It is found that the normal mode refinement, using a smaller number of variables, gives a better R factor and more information on the dynamics (anisotropy and collectivity in the motion).

Mathematics↗
PubMed1990

The differences in conformation between alpha-human atrial natriuretic polypeptide, alpha-hANP, and its derivative, Met(O)-alpha-hANP, in solution.

The differences in conformation between alpha-human atrial natriuretic polypeptide (alpha-hANP) and its inactive analog, Met(O)-alpha-hANP, have been analyzed by nuclear magnetic resonance spectroscopy. All proton resonances for both peptides were assigned by means of the sequential assignment procedure. The three-dimensional structure of alpha-hANP in solution had previously been determined by distance geometry calculation using distance constraints derived from nuclear Overhauser effects (NOEs). Here, the three-dimensional structure of Met(O)-alpha-hANP was determined. The conformational differences between these two molecules were as follows: three segments of alpha-hANP, Ser1-Cys7, Arg11-Ala17 and Gln18-Tyr28, have some ordered structures. In Met(O)-alpha-hANP the Gln18-Tyr28 region has a similar conformation, while the remaining two regions do not have the ordered structure found in alpha-hANP. It is suggested that the conserved conformation of the Gln18-Tyr28 region is required for binding to the ANP receptor and that the slight biological activity of Met(O)-alpha-hANP is due to loss of the ordered structures evoked in the Ser1-Cys7 and Arg11-Ala17 regions of alpha-hANP.

Amino Acid Sequence↗
PubMed1989

Solution conformation of conotoxin GI determined by 1H nuclear magnetic resonance spectroscopy and distance geometry calculations.

Conformational analysis of conotoxin GI, one of the neurotoxic peptides produced by a marine snail, genus Conus, was performed by a combination of nuclear magnetic resonance spectroscopy (NMR) and distance geometry calculations. The resulting conformers on minimization of the target function were classified into two groups. The difference in the structures of the conformers is mainly due to the difference in the orientation of the side chain of the tyrosyl residue. The results show that the solution structure of conotoxin GI satisfies the conformational requirements for the biological activity of an antagonist toward nicotinic cholinergic receptors elucidated in a series of studies on alkaloids. The structure is discussed on the basis of the results of comparison of the atomic arrangements of the active sites of snake venom peptides and molecular models based on the results of secondary structure prediction.

Amino Acid Sequence↗
PubMed1989

Structural basis of hierarchical multiple substates of a protein. I: Introduction.

A computer experiment of protein dynamics is carried out, which consists of two steps: (1) A Monte Carlo simulation of thermal fluctuations in the native state of a globular protein, bovine pancreatic trypsin inhibitor; and (2) a simulation of the quick freezing of fluctuating conformations into energy minima by minimization of the energy of a number of conformations sampled in the Monte Carlo simulation. From the analysis of results of the computer experiment is obtained the following picture of protein dynamics: multiple energy minima exist in the native state, and they are distributed in clusters in the conformational space. The dynamics has a hierarchical structure which has at least two levels. In the first level, dynamics is restricted within one of the clusters of minima. In the second, transitions occur among the clusters. Local parts of a protein molecule, side chains and local main chain segments, can take multiple locally stable conformations in the native state. Many minima result from combinations of these multiple local conformations. The hierarchical structure in the dynamics comes from interactions among the local parts. Protein molecules have two types of flexibility, each associated with elastic and plastic deformations, respectively.

Animals↗
PubMed1989

Structural basis of hierarchical multiple substates of a protein. II: Monte Carlo simulation of native thermal fluctuations and energy minimization.

Conformational fluctuations in a globular protein, bovine pancreatic trypsin inhibitor, in the time range between picoseconds and nanoseconds are studied by a Monte Carlo simulation method. Multiple energy minima are derived from sampled conformations by minimizing their energy. They are distributed in clusters in the conformational space. A hierarchical structure is observed in the simulated dynamics. In the time range between 10(-14) and 10(-10) seconds dynamics is well represented by a superposition of vibrational motions within an energy well with transitions among minima within each cluster. Transitions among clusters take place in the time range of nanoseconds or longer.

Animals↗
PubMed1989

Structural basis of hierarchical multiple substates of a protein. III: Side chain and main chain local conformations.

An analysis is carried out of differences in the minimum energy conformations obtained in the previous paper by energy minimization starting from conformations sampled by a Monte Carlo simulation of conformational fluctuations in the native state of a globular protein, bovine pancreatic trypsin inhibitor. Main conformational differences in each pair of energy minima are found usually localized in several side chains and in a few local main chain segments. Such side chains and local main chain segments are found to take a few distinct local conformations in the minimum energy conformations. Energy minimum conformations can thus be described in terms of combinations of these multiple local conformations.

Amino Acid Sequence↗
PubMed1989

Structural basis of hierarchical multiple substates of a protein. IV: Rearrangements in atom packing and local deformations.

Differences in atom packing are studied in the minimum energy conformations derived from the record of the Monte Carlo simulation of conformational fluctuation in the native state of a globular protein, bovine pancreatic trypsin inhibitor. It is found that local deformations observed among the minima which are found in the previous paper are accompanied by rearrangement of atom packing. Spatial locations of the local deformations in the three-dimensional folded structure are also studied. It is found that the local deformations are distributed in space in several clusters in the folded structure. The size and location of the clusters characterize the respective fluctuations of the first and the second levels observed in the simulation. In the fluctuations of the first level local deformations, each of which usually involves a few side chains and one main chain local segment, are thermally exited independently of each other near the surface of the molecule. The observed fluctuation of the second level involves a cooperative deformation involving many side chains and local main chain segments all in one cluster, which goes though the core of the molecule. The collective local deformations observed both in the first and second levels are plastic in the sense that they are accompanied with rearrangement of atom packing.

Amino Acid Sequence↗
PubMed1989

Structural basis of hierarchical multiple substates of a protein. V: Nonlocal deformations.

Distances between centers of gravity of individual residues are compared among the minimum energy conformations derived from the record of the Monte Carlo simulation of conformational fluctuations in the native state of a globular protein, bovine pancreatic trypsin inhibitor. It is found that local deformations originating from the multiplicity of local conformations cause deformations of the whole structure of the molecule in various ways, which can be classified into two types. Type 1: When a local deformation occurs in a region consisting of a few residues near the surface of the molecule, the whole shape of the molecule responds by deforming elastically. The magnitude of this deformation is in the range of thermal fluctuations calculated by the harmonic approximation around a single minimum. Type 2: We have observed one case belonging to the second type in which local deformations occur cooperatively in an extended region. This region goes across the whole molecule and divide the remaining parts into two. Atom packing changes in and around the extended region of local deformations. For this reason deformation in this region is plastic. Relative location and orientation between the divided two parts change very much. Deformation of the whole shape in this case, associated with the plastic deformation in an extended region, demonstrates that protein molecules have a flexibility beyond the harmonic limit.

Amino Acid Sequence↗
PubMed1988

Tertiary structure of mouse epidermal growth factor determined by two-dimensional 1H NMR.

The tertiary structure of mouse epidermal growth factor (EGF) in solution (28 degrees C, pH 2.0) was studied by two-dimensional NMR spectroscopy. Proton-proton distance constraints derived from NOESY spectra were used to construct a mechanical molecular model of mouse EGF, which was subsequently checked by means of a preliminary distance geometry calculation. The chain-folds in the two structural domains of mouse EGF were very similar to those previously reported (Montelione et al. (1987) Proc. Natl. Acad. Sci. U.S. 84, 5226-5230). However, the relative orientations of the two domains were different. Because we could assign much more inter-domain NOEs, the relative orientations of the two domains were well determined in our model. The hollow between the two domains may function as a binding site for the EGF receptor.

Animals↗
PubMed1988

The conformation of alpha-human atrial natriuretic polypeptide in solution.

The three-dimensional structure of alpha-human ANP in solution was determined through the combined use of nuclear magnetic resonance spectroscopy and distance geometry. The results are based on distance constraints determined by nuclear Overhauser effect measurements and one disulfide bond. The structure is as follows. Three separate regions, which are Ser1-Cys7, Arg11-Ile15, and Gln18-Tyr28 each have some ordered structure. The remaining parts in the sequences of Gly9-Gly10 and Gly16-Ala17 act as hinges. And the C-terminal part is folded back toward the cyclic moiety. The conformation of alpha-hANP reported here is expected to give a better understanding of the relationships between its biological activities and three-dimensional structure.

Amino Acid Sequence↗
PubMed1987

Protein structures in solution by nuclear magnetic resonance and distance geometry. The polypeptide fold of the basic pancreatic trypsin inhibitor determined using two different algorithms, DISGEO and DISMAN.

A set of conformational restraints derived from nuclear magnetic resonance (n.m.r.) measurements on solutions of the basic pancreatic trypsin inhibitor (BPTI) was used as input for distance geometry calculations with the programs DISGEO and DISMAN. Five structures obtained with each of these algorithms were systematically compared among themselves and with the crystal structure of BPTI. It is clear that the protein architecture observed in single crystals of BPTI is largely preserved in aqueous solution, with local structural differences mainly confined to the protein surface. The results confirm that protein conformations determined in solution by combined use of n.m.r. and distance geometry are a consequence of the experimental data and do not depend significantly on the algorithm used for the structure determination. The data obtained further provide an illustration that long intramolecular distances in proteins, which are comparable with the radius of gyration, are defined with high precision by relatively imprecise nuclear Overhauser enhancement measurements of a large number of much shorter distances.

Algorithms↗
PubMed1987

Normal modes of vibration in bovine pancreatic trypsin inhibitor and its mechanical property.

The normal mode analysis of conformational fluctuation is carried out for a small globular protein, bovine pancreatic trypsin inhibitor. Results are analyzed mainly to reveal the mechanical construction of the protein molecule. We take dihedral angles, including peptide omega angles, as independent variables for the normal mode analysis. There are 306 such angles in this molecule. Motions in modes with frequencies lower than 120 cm-1 are shown to involve atoms in the whole protein molecule, and spatial change of displacement vectors is continuous, i.e., those of atoms near in space are similar. To quantitate the observation of the continuity, a correlation function of direction vectors of atomic displacements is calculated. From this function we define a quantity that is interpreted as the wave length of an equivalent elastic plane wave. From this quantity we deduce effective Young's modulus for each mode. For the mode with the lowest frequency 4.4 cm-1, it turned out to be 0.8 x 10(9) dyn cm-2, the value two orders of magnitude softer than, for instance, alpha-helices. Prompted by this observation, the four lowest frequency modes and also the harmonic motions in the thermal equilibrium are analyzed further mainly to detect relatively rigid structural elements in the molecule. From this analysis emerges a mechanical picture of the protein molecule that is made up of relatively rigid elements held together by very soft parts.

Animals↗