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G N Phillips

Publications and source records attributed to G N Phillips.

At least 55 records · Page 3Linked to original sources

Visualization of dynamic simulations of muscle thin filaments.

Following a novel computational formalism, the thin filament of muscle can be modeled by a computational machine containing a large number of finite automata that have one-to-one correspondence with the constituent protein molecules. Computer graphics can be used to visualize the correspondence between the states of finite automata and the configurations of protein molecules according to the structural data. The dynamic simulation of the muscle filament that corresponds to the concurrent state transitions of finite automata can be represented as a sequence of video images. The kinetic and structural knowledge of individual protein molecules is, therefore, integrated into a coherent and functional system. This type of computation and visualization can also be useful for the investigation of molecular structure, function, and interaction in various complex biological systems.

Actin Cytoskeleton↗

XRayView: a teaching aid for X-ray crystallography.

A software package, XRayView, has been developed that uses interactive computer graphics to introduce basic concepts of x-ray diffraction by crystals, including the reciprocal lattice, the Ewald sphere construction, Laue cones, the wavelength dependence of the reciprocal lattice, primitive and centered lattices and systematic extinctions, rotation photography. Laue photography, space group determination and Laue group symmetry, and the alignment of crystals by examination of reciprocal space. XRayView is designed with "user-friendliness" in mind, using pull-down menus to control the program. Many of the experiences of using real x-ray diffraction equipment to examine crystalline diffraction can be simulated. Exercises are available on-line to guide the users through many typical x-ray diffraction experiments.

Biophysics↗

Crystal structure of photolysed carbonmonoxy-myoglobin.

Myoglobin is a globular haem protein that reversibly binds ligands such as O2 and CO. Single photons of visible light can break the covalent bond between CO and the haem iron in carbon-monoxy-myoglobin (MbCO) and thus form an unstable intermediate, Mb*CO, with the CO inside the protein. The ensuing rebinding process has been extensively studied as a model for the interplay of dynamics, structure and function in protein reactions. We have used X-ray crystallography at liquid-helium temperatures to determine the structure of Mb*CO to a resolution of 1.5 A. The photodissociated CO lies on top of the haem pyrrole ring C. Comparison with the CO-bound and unligated myoglobin structures reveals that on photodissociation of the CO, the haem 'domes', the iron moves partially out of the haem plane, the iron-proximal histidine bonds is compressed, the F helix is strained and the distal histidine swings towards the outside of the ligand-binding pocket.

Animals↗

Nitric oxide recombination to double mutants of myoglobin: role of ligand diffusion in a fluctuating heme pocket.

Picosecond recombination of nitric oxide to the double mutants of myoglobin, His64Gly-Val68Ala and His64Gly.Val68Ile, at E7 and E11, has been studied experimentally and by computation. It is shown that distal residues have a profound effect on NO recombination. Recombination in the mutants may be explained in terms of fluctuating free volume and structure of the heme pocket. The double mutants provide insight into the effects of free volume and steric hindrance on rates of ligand rebinding following photolysis. Water molecules of the first solvation shell replace surface residues deleted by mutation and can block apparent holes in the protein structure. Thus, water molecules extend the time required for ligands to escape significantly to a nanosecond time scale, which is much longer than would be expected for an open heme pocket. Both nearly exponential (G64A68) and markedly nonexponential (native and G64I68) kinetics are observed, a result at variance with expectation from the model of Petrich et al. [Petrich, J.W., Lambry, J.C., Kuczera, K., Karplus, M., Poyart, C., & Martin, J.L. (1991) Biochemistry 30, 3975-3987], which attributes nonexponential kinetics to proximal effects.

Amino Acid Sequence↗

Coiled-coil packing in spermine-induced tropomyosin crystals. A comparative study of three forms.

Electron microscope images of highly ordered spermine-induced microcrystals of tropomyosin have been analyzed to determine the packing of the molecular filaments. Negatively stained microcrystals terminate in a distinctive "double fringe", which reveals the location of the molecular ends. This information, together with the symmetry of the structure in projection, shows that the microcrystals can be accounted for by a packing scheme of four layers of molecules in the unit cell. Knowing the position of the symmetry elements relating the layers then allows the three-dimensional space group of the microcrystals to be established as C222(1). Using cryo-electron microscopy and simulation studies, the run of the filaments and their packing in the C222(1) form have been shown to be related to those in the spermine-induced C2 crystal of tropomyosin whose structure has been solved to 9 A by X-ray crystallography. This result allows us to infer the location of the molecular ends in the C2 crystal as well, and this inference has been confirmed by analysis of thin sections of the C2 crystal. The C222(1) microcrystal has also been shown to be closely related to the classical divalent cation tropomyosin paracrystal. Based on knowledge of the molecular packing in the divalent cation paracrystal, the polarity of the molecules has been deduced in the other two crystal forms. The tropomyosin filament packing in all these forms may be accounted for by coiled-coil close packing and specific cationic bridging of negatively charged zones on the molecule. Taken together the results reveal a hierarchy of interactions in these close-packed crystalline forms, whose principles may apply to the packing in other fibrous proteins. This study also shows the usefulness of co-ordinating results from cryo-electron microscopy with negative staining in the structure analysis of such ordered arrays, and how these findings can complement the results of low resolution X-ray crystallographic studies.

Animals↗

Analysis of diffuse scattering from yeast initiator tRNA crystals.

Yeast initiator tRNA crystals exhibit strong X-ray diffuse scattering. This scattering can be used to extract information about lattice-coupled and intramolecular motions in the crystals. The amplitudes and correlation distances of these motions can be estimated by calculating the diffuse scattering and comparing the results with the observed scattering. Results indicate that both anisotropic, lattice-coupled motions as well as short-range correlated local disorder in the anticodon arm contribute to the overall disorder in the crystals. These types of motions can be correlated with aspects of tRNA function. This additional information complements the results from analysis of crystallographic data and provides a more detailed picture of the structure and dynamics of the molecule. The degree to which the methodology presented here can account for the observed diffuse scattering from tRNA represents a significant step forward in the ability to use this conventionally discarded information, and encourages the ultimate extension of these ideas to a wide variety of macromolecular systems.

Journal Article↗

Structural determinants of the stretching frequency of CO bound to myoglobin.

In order to assess the relative importance of polar versus steric interactions, infrared spectra and overall CO binding properties were measured at room temperature for 41 different recombinant myoglobins containing mutations at His64(E7), Val68(E11), Phe43(CD1), Arg45(CD3), Phe46(CD4), and Leu29(B10). The results were compared to the crystal structures of wild-type, Phe29, Val46, Ala68, Phe68, Gln64, Leu64, and Gly64 sperm whale CO-myoglobin and that of Thr68 pig CO-myoglobin. As observed in several previous studies, replacement of the distal histidine (His64) with aliphatic amino acids results in the appearance of a single IR band in the 1960-1970-cm-1 region and in large increases in CO affinity (KCO). More complex behavior is observed for Gly, Ala, Gln, Met, and Trp substitutions at position 64, but in each case there is a net increase in the intensity of this high-frequency component. Replacement of Val68 with Ala, Leu, Ile, and Phe produces little effect on the IR spectrum, whereas these mutations cause 20-fold changes in KCO, presumably due to steric effects. Replacement of Val68 with Thr decreases KCO 4-5-fold, whereas the position of the major IR band increases from 1945 to 1961 cm-1. Replacement of Val68 with Asn also causes a large decrease in KCO, but in this case, the peak position of the major IR band decreases from 1945 to 1916 cm-1. Nine replacements were made in the CD corner at positions 43, 45, and 46. All of the resultant mutants show increased stretching frequencies that can be correlated with movement of the imidazole side chain of His64 away from the bound ligand. All five substitutions at position 29 cause changes in the IR spectra. The Leu29-->Phe mutation had the largest effect, producing a single band centered at 1932 cm-1. Together these data demonstrate that there is little direct correlation between affinity, vCO, and Fe-C-O geometry. The major factor governing vCO appears to be the electrostatic potential surrounding the bound ligand and not steric hindrance. The presence of positive charges from proton donors, such as N epsilon of His64 and N delta of Asn68, cause a decrease in the bond order and stretching frequency of bound CO. In contrast, the negative portion of the Thr68 dipole points directly toward the bound ligand and increases the C-O bond order and stretching frequency. Movement of His64 away from the bound ligand or replacement of this residue with aliphatic amino acids prevents hydrogen-bonding interactions, causing vCO to increase.(ABSTRACT TRUNCATED AT 250 WORDS)

Animals↗

His64(E7)-->Tyr apomyoglobin as a reagent for measuring rates of hemin dissociation.

To develop an assay for hemin dissociation, His64(E7) was replaced by Tyr in sperm whale myoglobin producing a holoprotein with a distinct green color due to an intense absorption band at 600 nm. Val68(E11) was replaced by Phe in the same protein to increase its stability. When excess Tyr64-Val68 apoglobin is mixed with either metmyoglobin or methemoglobin, the solution turns from brown to green, and the absorbance changes can be used to measure complete time courses for hemin dissociation from either holoprotein. This assay has been used to measure rates of hemin dissociation from native metmyoglobin, four myoglobin mutants (Ala64(E7), Ala68(E11), Phe68(E11), and Glu45(CD3)), native methemoglobin, valence hybrid hemoglobins, and two mutant hemoglobins ((alpha(Gly-E7)beta(native))2, and (alpha(native)beta(Gly-E7))2). Two kinetic phases were observed for hemin dissociation from native human hemoglobin at pH 7.0 and 37 degrees C. Valence and mutant hybrid hemoglobins were used to assign the faster phase (k = 7.8 +/- 2.0 h-1) to hemin dissociation from ferric beta subunits and the slower (k = 0.6 +/- 0.15 h-1) to dissociation from alpha subunits. The corresponding rate for wild-type metmyoglobin is 0.007 +/- 0.004 h-1.

Animals↗

Cross-validation tests of time-averaged molecular dynamics refinements for determination of protein structures by X-ray crystallography.

Time-averaged structure-factor restraints have been used in two molecular dynamics refinement schemes to define ensembles of conformations for myoglobin that fit the experimentally measured Bragg scattering from P6 crystals. The geometries of the structures have been maintained to the same currently acceptable limits in all cases. Free R value analysis was used to assess the validity of the two approaches. In the first scheme, where atoms have no B values, the decrease in R value was found to be spurious as judged by a concomitant increase in the free R value. The other scheme, however, which retains individual B values, was found to yield both low R values and low free R values; thus, here the additional variables introduced by modeling the protein in terms of an evolving ensemble of states do not overfit the data. For comparison, refinements were also carried out on the system using several other techniques for isotropic and anisotropic crystallographic refinement. The time-averaged refinements with B values compare quite favorably with the standard methods, but yield additional information about substates of the system. Hence, correctly applied time-averaged refinements can yield accurate models for protein molecules; moreover, by essentially relaxing the harmonic approximation from the refinement process, these refinements allow a more detailed description of the motions of complex molecules, such as proteins, to be determined from X-ray crystallographic data.

Journal Article↗

Stabilization of myoglobin by multiple alanine substitutions in helical positions.

We have carried out a series of multiple Xaa-->Ala changes at nonadjacent surface positions in the sequence of sperm whale myoglobin. Although the corresponding single substitutions do not increase the thermal stability of the protein, multiple substitutions enhance the stability of the resulting myoglobins. The effect observed is an increase in the observed Tm (midpoint unfolding temperature) relative to that predicted from assuming additivity of the free energy changes corresponding to single mutations. The stabilization occurs in the presence of urea, as measured by the dependence of the unfolding temperature on urea concentration. The sites that have been altered occur in different helices and are not close in sequence or in the native structure of myoglobin. The observed effect is consistent with a role of multiple alanines in residual interactions in the unfolded state of the mutant proteins.

Alanine↗

The closed conformation of a highly flexible protein: the structure of E. coli adenylate kinase with bound AMP and AMPPNP.

The structure of E. coli adenylate kinase with bound AMP and AMPPNP at 2.0 A resolution is presented. The protein crystallizes in space group C2 with two molecules in the asymmetric unit, and has been refined to an R factor of 20.1% and an Rfree of 31.6%. In the present structure, the protein is in the closed (globular) form with the large flexible lid domain covering the AMPPNP molecule. Within the protein, AMP and AMPPNP, and ATP analog, occupy the AMP and ATP sites respectively, which had been suggested by the most recent crystal structure of E. coli adenylate kinase with Ap5A bound (Müller and Schulz, 1992, ref. 1) and prior fluorescence studies (Liang et al., 1991, ref. 2). The binding of substrates and the positions of the active site residues are compared between the present structure and the E. coli adenylate kinase/Ap5A structure. We failed to detect a peak in the density map corresponding to the Mg2+ ion which is required for catalysis, and its absence has been attributed to the use of ammonium sulfate in the crystallization solution. Finally, a comparison is made between the present structure and the structure of the heavy chain of muscle myosin.

Adenosine Monophosphate↗

A cellular automaton model for the regulatory behavior of muscle thin filaments.

Regulation of skeletal muscle contraction is achieved through the interaction of six different proteins: actin, myosin, tropomyosin, and troponins C, I, and T. Many experiments have been performed on the interactions of these proteins, but comparatively less effort has been spent on attempts to integrate the results into a coherent description of the system as a whole. In this paper, we present a new way of approaching the integration problem by using a cellular automaton. We assign rate constants for state changes within each constituent molecule of the muscle thin filament as functions of the states of its neighboring molecules. The automaton shows how the interactions among constituent molecules give rise to the overall regulatory behavior of thin filaments as observed in vitro and is extendable to in vivo measurements. The model is used to predict myosin binding and ATPase activity, and the result is compared with various experimental data. Two important aspects of regulation are revealed by the requirement that the model fit the experimental data: (1) strong interactions must exist between two successively bound myosin heads, and (2) the cooperative binding of calcium to the thin filament can be attributed in a simple way to the interaction between neighboring troponin-tropomyosin units.

Actin Cytoskeleton↗

A global model of the protein-solvent interface.

The solvent structure and dynamics around myoglobin is investigated at the microscopic level of detail by computer simulation. We analyze a molecular dynamics trajectory in terms of solvent mobility and probability distribution. Local events, occurring in the protein-solvent interfacial region, which are often masked by other approaches are thus revealed. Specifically, the local solvent mobility is greatly enhanced for certain locations at the protein surface and in its interior. In addition, a strong correlation between the solvent mobility and density emerges on both global and local scales. We propose a simple model where the solvent distribution measured perpendicularly to the protein surface is utilized to reconstruct the simulated network of hydration within 6 A from the protein surface with a relative error of only 17%. The global precision of this solvation model matches results obtained with more complicated models usually used in refinement procedures in x-ray and neutron experiments but with far fewer parameters. The dramatically improved correspondence between observed and calculated x-ray intensities at low resolution relative to other methods both confirms the validity of the approach used in the MD (molecular dynamics) simulations and allows the results of this study to be implemented in solvent studies on real systems.

Biophysical Phenomena↗

High-resolution crystal structures of distal histidine mutants of sperm whale myoglobin.

The highly conserved distal histidine residue (His64) of sperm whale myoglobin modulates the affinity of ligands. In an effort to fully characterize the effects of mutating residue 64, we have determined the high-resolution crystal structures of the Gly64, Val64, Leu64, Thr64 and Gln64 mutants in several liganded forms. Metmyoglobins with hydrophobic substitutions at residue 64 (Val64 and Leu64) lack a water molecule at the sixth coordination position, while those with polar amino acid residues at this position (wild-type and Gln64) retain a covalently bound water molecule. In the Thr64 mutant, the bound water position is only partially occupied. In contrast, mutating the distal histidine residue to glycine does not cause loss of the coordinated water molecule, because the hydrogen bond from the imidazole side-chain is replaced by one from a well-ordered solvent water molecule. Differences in water structure around the distal pocket are apparent also in the structures of deoxymyoglobin mutants. The water molecule that is hydrogen-bonded to the N epsilon atom of histidine 64 in wild-type deoxymyoglobin is not found in any of the position 64 mutant structures that were determined. Comparison of the carbonmonoxy structures of wild-type, Gly64, Leu64 and Gln64 myoglobins in the P6 crystal form shows that the conformation of the Fe-C-O complex is nearly linear and is independent of the identity of the amino acid residue at position 64. However, the effect of CO binding on the conformation of residue 64 is striking. Superposition of deoxy and carbonmonoxy structures reveals significant displacements of the residue 64 side-chain in the wild-type and Gln64 myoglobins, but no displacement in the Leu64 mutant. These detailed structural studies provide key insights into the mechanisms of ligand binding and discrimination in myoglobin.

Animals↗

Structure of tropomyosin at 9 angstroms resolution.

We have used molecular replacement followed by a highly parameterized refinement to determine the structure of tropomyosin crystals to a resolution to 9 A. The shape, coiled-coil structure and interactions of the molecules in the crystals have been determined. These crystals have C2 symmetry with a = 259.7 A, b = 55.3 A, c = 135.6 A and beta = 97.2 degrees. Because of the unusual distribution of intensity in X-ray diffraction patterns from these crystals, it was possible to solve the rotation problem by inspection of qualitative aspects of the diffraction data and to define unequivocally the general alignment of the molecules along the (332) and (3-32) directions of the unit cell. The translation function was then solved by a direct search procedure, while electron microscopy of a related crystal form indicated the probable location of molecular ends in the asymmetric unit, as well as the anti-parallel arrangement. The structural model we have obtained is much clearer than that obtained previously with crystals of extraordinarily high solvent content and shows the two alpha-helices of the coiled coil over most of the length of the molecules and establishes the coiled-coil pitch at 140(+/- 10) A. Moreover, the precise value of the coiled-coil pitch varies along the molecule, probably in response to local variations in the amino acid sequence, which we have determined by sequencing the appropriate cDNA. The crystals are constructed from layers of tropomyosin filaments. There are two molecules in the crystallographic asymmetric unit and the molecules within a layer are bent into an approximately sinusoidal profile. Molecules in consecutive layers in the crystal lie at an angle relative to one another as found in crystalline arrays of actin and myosin rod. There are three classes of interactions between tropomyosin molecules in the spermine-induced crystals and these give some insights into the molecular interactions between coiled-coil molecules that may have implications for assemblies such as muscle thick filaments and intermediate filaments. In interactions within a layer, the geometry of coiled-coil contacts is retained, whereas in contacts between molecules in adjacent layers the coiled-coil geometry varies and these interactions instead appear to be dominated by the repeating pattern of charged zones along the molecule.

Amino Acid Sequence↗

A novel site-directed mutant of myoglobin with an unusually high O2 affinity and low autooxidation rate.

Mutants of sperm whale myoglobin were constructed at position 29 (B10 in helix notation) to examine the effects of distal pocket size on the rates of ligand binding and autooxidation. Leu29 was replaced with Ala, Val, and Phe using the synthetic gene and Escherichia coli expression system of Springer and Sligar (Springer, B. A., and Sligar, S. G. (1987) Proc. Natl. Acad. Sci. U. S. A. 84, 8961-8965). Structures of the ferric forms of Val29 and Phe29, and the oxy form of Phe29 myoglobin were determined to 1.7 A by x-ray crystallography. The ferric mutant proteins are remarkably isomorphous with the wild type protein except in the immediate vicinity of residue 29. Thus, the protein structure in the distal pocket of myoglobin can accommodate either a large "hole" (i.e. Ala or Val) or a large side chain (i.e. Phe) at position 29 without perturbation of tertiary structure. Phe29 oxymyoglobin is also identical to the native oxy protein in terms of overall structure and interactions between the bound O2 and His64, Val68, Phe43, and Ile107. The distance between the nearest side chain atom of residue 29 and the second atom of the bound oxygen molecule is 3.2 A in the Phe29 protein and 4.9 A in native myoglobin. The equilibrium constants for O2 binding to Ala29, Val29, and Leu29 (native) myoglobin are the same, approximately 1.0 x 10(6) M-1 at 20 degrees C, whereas that for the Phe29 protein is markedly greater, 15 x 10(6) M-1. This increase in affinity is due primarily to a 10-fold decrease in the O2 dissociation rate constant for the Phe29 mutant and appears to be the result of stabilizing interactions between the negative portion of the bound O2 dipole and the partially positive edge of the phenyl ring. Increasing the size of residue 29 causes large decreases in the rate of autooxidation of myoglobin: k(ox) = 0.24, 0.23, 0.055, and 0.005 h-1 for Ala29, Val29, Leu29 (native), and Phe29 myoglobin, respectively, in air at 37 degrees C. Thus, the Leu29----Phe mutation produces a reduced protein that is remarkably stable and is expressed in E. coli as 100% MbO2. The selective pressure to conserve Leu29 at the B10 position probably represents a compromise between reducing the rate of autooxidation and maintaining a large enough O2 dissociation rate constant to allow rapid oxygen release during respiration.

Amino Acid Sequence↗

What is the pitch of the alpha-helical coiled coil?

The alpha-helical, coiled-coil protein motif is increasingly recognized in a variety of functional classes of proteins. The pitch of a coiled coil, or rate of winding of the alpha-helices around each other, is a key determinant of both intra- and intermolecular interactions. Experimental measurements of the pitch of parallel two-stranded coiled coils of muscle proteins, and examination of the recently determined structure of another two-stranded coiled coil, the GCN4 transcription factor protein, suggest that the pitch has an average value of about 140 A. This value is consistent with the observed number of residues per turn in alpha-helices of globular proteins, the determinant of the interhelical packing within the coiled-coil motif. An understanding of the structural determinants of this value for the pitch and possible variations will be important in defining the interactions of coiled-coil proteins with other macromolecules.

Protein Structure, Secondary↗

Diffuse x-ray scattering from tropomyosin crystals.

Diffuse scattering analyses are emerging as a technique to extract additional dynamic information from x-ray diffraction data. In fact, when examined carefully, most protein crystals show significant diffuse scattering in addition to the usual Bragg diffraction. This diffuse scattering contains information about the disorder in the crystal that cannot be obtained from the Bragg diffraction data. Diffraction from tropomyosin crystals shows characteristic diffuse scattering streaks that are directly related to motion of the molecules. The structure of tropomyosin to 15 A resolution shows that the limited molecular contacts between molecules allow large conformational fluctuations of up to 8 A amplitude. Models for the three-dimensional motion of tropomyosin have been tested by comparing their predicted diffuse scattering patterns with the experimental data. From the parameters of the successful simulations, we were able to determine the amplitudes, directions, and distances over which the atomic displacements are correlated.

Biophysical Phenomena↗