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Structure and function of cytochromes P450: a comparative analysis of three crystal structures.

BACKGROUND: Cytochromes P450 catalyze the oxidation of a variety of hydrophobic substrates. Sequence identities between P450 families are generally low (10-30%), and consequently, the structure-function correlations among P450s are not clear. The crystal structures of P450terp and the hemoprotein domain of P450BM-3 were recently determined, and are compared here with the previously available structure of P450cam. RESULTS: The topology of all three enzymes is quite similar. The heme-binding core structure is well conserved, except for local differences in the I helices. The greatest variation is observed in the substrate-binding regions. The structural superposition of the proteins permits an improved sequence alignment of other P450s. The charge distribution in the three structures is similarly asymmetric and defines a molecular dipole. CONCLUSIONS: Based on this comparison we believe that all P450s will be found to possess the same tertiary structure. The ability to precisely predict other P450 substrate-contact residues is limited by the extreme structural heterogeneity in the substrate-recognition regions. The central I-helix structures of P450terp and P450BM-3 suggest a role for helix-associated solvent molecules as a source of catalytic protons, distinct from the mechanism for P450cam. We suggest that the P450 molecular dipole might aid in both redox-partner docking and proton recruitment for catalysis.

Amino Acid Sequence↗

Free-energy calculations highlight differences in accuracy between X-ray and NMR structures and add value to protein structure prediction.

BACKGROUND: While X-ray crystallography structures of proteins are considerably more reliable than those from NMR spectroscopy, it has been difficult to assess the inherent accuracy of NMR structures, particularly the side chains. RESULTS: For 15 small single-domain proteins, we used a molecular mechanics-/dynamics-based free-energy approach to investigate native, decoy, and fully extended alpha conformations. Decoys were all less energetically favorable than native conformations in nine of the ten X-ray structures and in none of the five NMR structures, but short 150 ps molecular dynamics simulations on the experimental structures caused them to have the lowest predicted free energy in all 15 proteins. In addition, a strong correlation exists (r(2) = 0.86) between the predicted free energy of unfolding, from native to fully extended conformations, and the number of residues. CONCLUSIONS: This work suggests that the approximate treatment of solvent used in solving NMR structures can lead NMR model conformations to be less reliable than crystal structures. This conclusion was reached because of the considerably higher calculated free energies and the extent of structural deviation during aqueous dynamics simulations of NMR models compared to those determined by X-ray crystallography. Also, the strong correlation found between protein length and predicted free energy of unfolding in this work suggests, for the first time, that a free-energy function can allow for identification of the native state based on calculations on an extended state and in the absence of an experimental structure.

Crystallography, X-Ray↗

Recognition of tertiary structure in tRNAs by Rh(phen)2phi3+, a new reagent for RNA structure-function mapping.

With photoactivation Rh(phen)2phi3+ promotes strand cleavage at sites of tertiary interaction in tRNA. The rhodium complex, which binds double-helical DNA by intercalation in the major groove, yields no cleavage in double-helical regions of the RNA or in unstructured single-stranded regions. Instead, Rh(phen)2phi3+ appears to target regions which are structured so that the major groove is open and accessible for stacking with the complex, as occurs where bases are triply bonded. So as to examine the specificity of this novel reagent and to evaluate its use in probing structural changes in RNAs, cleavage studies have been conducted on two structurally characterized tRNAs, tRNA(Phe) and tRNA(Asp) from yeast, the unmodified yeast tRNA(Phe) transcript, and a chemically modified tRNA(Phe), as well as on a series of tRNA(Phe) mutants. On tRNA(Phe) strong cleavage is observed at residues G22, G45, U47, psi 55, and U59; weaker cleavage is observed at A44, m7G46, and C48. On tRNA(Asp) cleavage is found at residues A21 through G26, psi 32, and U48, with minor cleavage apparent at A44, G45, A46, psi 55, U59, and U60. There is a striking similarity in cleavage observed on these tRNAs, and the sites of cleavage mark regions of tertiary folding. Cleavage on the unmodified tRNA(Phe) transcript resembles closely that found on native yeast tRNA(Phe), but additional sites, primarily in the anticodon loop and stem, are evident. The results indicate that globally the structures containing or lacking the modified bases appear to be the same; the differences in cleavage observed may reflect a loosening or alteration in the structure due to the absence of the modified bases. Cleavage results on mutants of tRNA(Phe) illustrate Rh(phen)2phi3+ as a sensitive probe in characterizing tRNA tertiary structure. Results are consistent with other assays for structural or functional changes. Uniquely, Rh(phen)2phi3+ appears to target directly sites of tertiary interaction. Cleavage results on mutants which involve base changes within the triply bounded region of the molecule indicate that it is the structure of the triply bonded array rather than the individual nucleotides which are being targeted. Chemical modification to promote selective depurination of the third base (m7G46) involved in the triple in the folded, native tRNA leads to the reduction of cleavage by the metal complex; this result shows directly the importance of the stacked triple base structure for recognition by the metal complex.(ABSTRACT TRUNCATED AT 400 WORDS)

2,2'-Dipyridyl↗

1.67-A X-ray structure of the B2 immunoglobulin-binding domain of streptococcal protein G and comparison to the NMR structure of the B1 domain.

The structure of the B2 immunoglobulin-binding domain of streptococcal protein G has been determined at 1.67-A resolution using a combination of single isomorphous replacement (SIR) phasing and manual fitting of the coordinates of the NMR structure of B1 domain of streptococcal protein G [Gronenborn, A. M., et al. (1991) Science 253, 657-661]. The final R value was 0.191 for data between 8.0 and 1.67 A. The structure described here has 13 residues preceding the 57-residue Ig-binding domain and 13 additional residues following it, for a total of 83 residues. The 57-residue binding domain is well-determined in the structure, having an average B factor of 18.0. Only residues 8-77 could be located in the electron density maps, with the ends of the structure fading into disorder. Like the B1 domain, the B2 domain consists of four beta-strands and a single helix lying diagonally across the beta-sheet, with a -1, +3 chi, -1 topology. This small structure is extensively hydrogen-bonded and has a relatively large hydrophobic core. These structural observations may account for the exceptional stability of protein G. A comparison of the B2 domain X-ray structure and the B1 domain NMR structure showed minor differences in the turn between strands and two and a slight displacement of the helix relative to the sheet. Hydrogen bonds between crystallographically related molecules account for most of these differences.

Amino Acid Sequence↗

Structure and thermodynamics of nonalternating C.G base pairs in Z-DNA: the 1.3-A crystal structure of the asymmetric hexanucleotide d(m5CGGGm5CG).d(m5CGCCm5CG).

We have solved the single-crystal X-ray structure of the complementary hexanucleotides d(m5-CGGGm5CG) and d(m5CGCCm5CG). The hexamer duplex was crystallized as Z-DNA, but contains a single C.G base pair that does not follow the alternating pyrimidine/purine rule for Z-DNA formation. This is the first crystal structure which serves to illustrate the structural consequences of placing a cytosine in the sterically disfavored syn conformation. In addition, since these sequences are not self-complementary, the individual strands of this asymmetric hexamer are unique in sequence and therefore distinguishable in the crystal lattice. Nevertheless, the crystal of this duplex is isomorphous with other Z-DNA hexamer structures. The asymmetry of this hexamer sequence required that the structure be solved using two unique models, which are distinguished by the orientation of hexanucleotides in the crystal lattice. In one model (the GG model) the cytosine in the syn conformation is packed against the terminal guanine base of a symmetry-related hexamer, while in the alternative model (the CC model) this cytosine sits exposed in a solvent channel of the lattice. We find that neither model alone can completely account for the observed electron densities. The two models ultimately were refined together. A composite structure consisting of 65% GG model and 35% CC model refined to an R-factor of 19.3%, which was significantly lower than refinements using either model alone. A detailed analysis of these two structures shows that, in spite of the out-of-alternation C.G base pair, the features characteristic of Z-DNA have been maintained. Both models, however, show significant local structural adjustments to accommodate the single cytosine base which is forced to adopt the syn conformation in each hexamer. In general, it appears that in order to relieve the energetically unfavorable steric contacts between the cytosine base in the syn conformation and the deoxyribose sugar, the base is forced into a highly buckled conformation, and that this large buckle in turn alters the conformation of neighboring residues. This unusual conformation also significantly weakens base-stacking interactions between the cytosine in syn and the adjacent residues in the helix and affects the exposure of the bases to solvent. We conclude that this crystal structure provides a molecular rationale for why nonalternating bases are energetically disfavored in Z-DNA.

Base Composition↗

Solution structure of the EcoRI DNA sequence: refinement of NMR-derived distance geometry structures by NOESY spectrum back-calculations.

The solution structure of the self-complementary DNA duplex [d(CGCGAATTCGCG)]2, which contains the EcoRI restriction site sequence GAATTC at the center, has been studied by two-dimensional nuclear magnetic resonance spectroscopy. Time-dependent nuclear Overhauser effect spectra were used to obtain the initial cross-relaxation rates between 155 pairs of protons. These initial cross-relaxation rates were converted into interproton distances and entered into a distance (bounds) matrix. A distance geometry algorithm (DSPACE) was used to create embedded starting structures and to refine these structures until they showed good agreement with the distance matrix; symmetry constraints were included in the refinement procedure, making the two strands in the refined distance geometry structures virtually identical and significantly improving the agreement with the distance matrix. The NOESY spectrum for one of these distance geometry structures was then calculated from the explicit coordinates by numerically integrating all the z-magnetization transfer pathways among neighboring protons within a specified radius. Distances in this distance geometry structure that did not agree with the experimental NOESY time course were then adjusted accordingly. This process was iterated until a good agreement between calculated and experimental NOESY spectra was reached. The final structure, which generates good agreement with the experimental NOESY spectrum, displays kinks at the C3-G4 base step and at the A6-T7 base step that appear to be similar to those reported for the EcoRI restriction site DNA bound to its endonuclease. The solution structure is not the same as the crystal structure of this DNA duplex.

Base Sequence↗

Chloroplastic aspartate aminotransferase from Arabidopsis thaliana: an examination of the relationship between the structure of the gene and the spatial structure of the protein.

A clone encoding a plastid isoenzyme of aspartate amino-transferase (AAT5) was isolated from an Arabidopsis genomic library and its complete sequence determined. The gene for AAT5 (asp5) contains an open reading frame of 2447 bp comprising 11 exons separated by introns ranging in length from 74 to 207 bp. The upstream regulatory region contains a putative TATA box and multiple copies of two sequence motifs, CTCTT and AAAGAT, previously associated with nodule-specific gene activity in legumes. The deduced primary amino acid sequence of the protein product of asp5 was used to generate a three-dimensional structure of the AAT5 protein by using the computer program Sybyl: Biopolymer Composer and known AAT structures on the protein databases. Both the mature protein and its precursor protein containing a putative N-terminal transit peptide were modelled. The resulting structure of the precursor protein indicated that the transit peptide might also inhibit dimerization of the protein until after its translocation across the chloroplast membrane. The derived structure of the mature protein was then analysed in terms of its component elements of secondary structure, and the positions on the polypeptide back-bone corresponding to intron insertion sites were determined. It is observed that the introns tend to map to regions between structural subdomains of the protein and also map to sites on the surface of the molecule. The asp5 gene in Arabidopsis is thus consistent with Gilbert's exon-shuffling theory of gene evolution [Gilbert (1985) Science 228, 823-824]. A high degree of conservation of intron insertion sites between AAT genes from different plants and animals is observed, particularly within the part of the gene encoding a large beta-sheet structure that forms the structural and functional core of the protein. This beta-sheet structure is thus believed to compromise an ancient and very highly conserved moiety of the molecule.

Amino Acid Sequence↗

Accuracy of a structural homology model for a class II histocompatibility protein, HLA-DR1: comparison to the crystal structure.

Structural homology modeling is used to test the accuracy by which a Class I major histocompatibility complex (MHC) could be used to model a Class II MHC. The crystal structure of HLA-aw68 served as a reference molecule to model HLA-DR1. The resulting model was compared to the recently released crystal structure by Brown et al. (Nature, Vol. 364, p. 33-39 (1993)). The overall tertiary structure motif (two alpha-helices and a beta-sheet forming a peptide binding cleft) was maintained. However, significant deviations in the secondary structure elements were found between the model and the DR1 crystal structure. These deviations were consistent with the differences between Class I and Class II crystal structures. In regions where the model and DR1 crystals structures are most similar, side chain orientations are also similar. Specific peptide-MHC interactions are discussed and compared with the crystal structure results.

Amino Acid Sequence↗

The three-dimensional structure of the ligand-binding domain of a wild-type bacterial chemotaxis receptor. Structural comparison to the cross-linked mutant forms and conformational changes upon ligand binding.

The three-dimensional structures of the ligand-binding domain of the wild-type Salmonella typhimurium aspartate receptor have been determined in the absence (apo) and presence of bound aspartate (complex) and compared to a cross-linked mutant containing a cysteine at position 36 which does not change signaling behavior of the intact receptor. The structures of the wild-type forms were determined in order to assess the effects of cross-linking on the structure and its influence on conformational changes upon ligand binding. As in the case of the cross-linked mutant receptor, the non-cross-linked ligand-binding domain is dimeric and is composed of 4-alpha-helical bundle monomer subunits related by a crystallographic 2-fold axis in the unbound form and by a non-crystallographic axis in the aspartate-bound form. A comparative study between the non-cross-linked and cross-linked structures has led to the following observations: 1) The long N-terminal helices of the individual subunits in the cross-linked structures are bent toward each other to accommodate the disulfide bond. 2) The rest of the subunit conformation is very similar to that of the wild-type. 3) The intersubunit angle of the cross-linked apo structure is larger by about 13 degrees when compared to the wild-type apo structure. 4) The nature and magnitude of the aspartate-induced conformational changes in the non-cross-linked wild-type structures are very similar to those of the cross-linked structures.

Amino Acid Sequence↗

Solution structure of Lqh-8/6, a toxin-like peptide from a scorpion venom--structural heterogeneity induced by proline cis/trans isomerization.

Lqh-8/6 is a minor fraction isolated from the venom of the scorpion Leiurus quinquestriatus hebraeus. Here we describe the purification, amino acid sequencing and solution structure determination by NMR and molecular modeling of this peptide. Lqh-8/6 is a small polypeptide (38 residues) which contains 8 half-cystines and is highly similar to another venom component, chlorotoxin. Standard homonuclear methods were used to sequentially assign the proton NMR spectra and to collect spatial restraints for structure determination. Two populations, identified early in the assignment step, are in slow interconversion on the NMR timescale. The two conformers were shown to originate from a cis/trans peptidyl-prolyl isomerization. Using a distance geometry program and simulated annealing protocol under the NMR restraints we obtained 10 final structures for the major conformation (trans isomer). None of the structures showed NOE violations larger than 0.05 nm, and the rmsd value relative to the mean structure (considering the main chain atoms in well-defined secondary structure) is 0.07 nm. The three-dimensional structure contains a short alpha-helix strapped on a small antiparallel beta-strand and an N-terminal extended fragment. The sequence/structure and structure/function relationships of the new scorpion toxin-like peptide are discussed in the context of the present structure determination. This toxin shows a stable, highly populated cis conformer of a peptidyl-prolyl peptide bond.

Amino Acid Sequence↗

At nonzero temperatures, stacked structures of methylated nucleic acid base pairs and microhydrated nonmethylated nucleic acid base pairs are favored over planar hydrogen-bonded structures: a molecular dynamics simulations study.

The dynamic structure of all ten possible nucleic acid (NA) base pairs and methylated NA base pairs hydrated by a small number of water molecules (from 1 to 16) was determined by using molecular dynamics simulations in the NVE microcanonical and NVT canonical ensembles with the Cornell force field (W. D. Cornell, P. Cieplak, C. I. Bayly, I. R. Gould, K. M. Merz, D. M. Ferguson, D. C. Spellmeyer, T. Fox, J. E. Caldwell, P. Kollman, J. Am. Chem. Soc. 1995, 117, 5179). The presence of one water molecule does not affect the structure of any hydrogen-bonded (H-bonded) nonmethylated base pair. An equal population of H-bonded and stacked structures of adenine...adenine, adenine...guanine and adenine... thymine pairs is reached if as few as two water molecules are present, while obtaining equal populations of these structures in the case of adenine...cytosine, cytosine...thymine, guanine... guanine and guanine...thymine required the presence of four water molecules, and in the case of guanine...cytosine, six. A comparable population of planar, H-bonded and stacked structures for cytosine...cytosine and thymine... thymine base pairs was only obtained if at least eight water molecules hydrated a pair. Methylation of bases changed the situation dramatically and stacked structures were favoured over H-bonded ones even in the absence of water molecules in most cases. Only in the case of methyl cytosine...methyl cytosine, methyl guanine...methyl guanine and methyl guanine...methyl cytosine pairs were two, two or six water molecules, respectively, needed in order to obtain a comparable population of planar, H-bonded and stacked structures. We believe that these results give clear evidence that the preferred stacked structure of NA base pairs in the microhydrated environment, and also apparently in a regular solvent, is due to the hydrophilic interaction of a small number of water molecules. In the case of methylated bases, it is also due to the fact that the hydrogen atoms most suitable for the formation of H-bonds have been replaced by a methyl group. A preferred stacked structure is, thus, not due to a hydrophobic interaction between a large bulk of water molecules and the base pair, as believed.

Base Pairing↗

Predicting RNA structures: the model of the RNA element binding Rev meets the NMR structure.

BACKGROUND: How accurate are the predictions of RNA three-dimensional structures? Assessing this accuracy requires the detailed comparison of the prediction with the experimentally determined structure. Previously, sequence variation in RNA aptamers that bind the Rev protein was used to infer a three-dimensional model of the Rev-binding element (RBE) RNA. Although much of this model has been substantiated by subsequent experimental data, its validity remains to be determined by confronting it with the structure determined by NMR spectroscopy. RESULTS: A series of different criteria such as geometric parameters (root mean square deviation, interproton distances, torsions and puckering), helicoidal parameters (base pairing and base stacking) and stability considerations (conformational energies) have been evaluated to identify common and distinguishing structural characteristics of the model and the NMR structure. CONCLUSIONS: The detailed comparison of the two structures reveals striking structural similarities at both the global and local level that validate the RNA modeling approach that we have used. Analysis of the structural differences and the precision of the model suggest that the limitations of the method are related to the amount of structural information available for modeling.

Binding Sites↗