Effect of sequence mutations on the higher order structure of the yeast 5 S rRNA.

Mutant yeast ribosomal 5 S RNAs were probed by enzymatic cleavage and chemical reactivity to define further the higher order structure. Mutations that destabilized helix IV resulted in an altered tertiary structure in which a reduced reactivity to ethylnitrosourea at U90 and G91 could be correlated with greater enzymatic and Fe(II)-EDTA cleavages in helices II and V. The results provide direct evidence for, and a further definition of, a structural juxtaposition between helix II and the end of helix IV and indicate that, in contrast to earlier suggestions, the remaining tertiary structure is sufficiently stable to prevent "pseudoknot-like" interactions between helices III and IV. The data are fully consistent with the "lollipop" model of the tertiary structure.     

Computer graphics program to reveal the dependence of the gross three-dimensional structure of the B-DNA double helix on primary structure.

Programs are presented to plot the gross three-dimensional structure of the DNA double helix with the base sequence as input information. The rules that determine the overall structure of the double helix are those that predict the dependence of local helix parameters (specifically, helix twist angle and relative basepair roll angle) on sequence. For this purpose, the user can select either the Calladine-Dickerson parameters or the Tung-Harvey parameters. These programs can be used as tools to investigate the variation of DNA tertiary structure with sequence, which may play an important role in the sequence-specific recognition of DNA by proteins.     

Helix capping in the GCN4 leucine zipper.

Capping interactions associated with specific sequences at or near the ends of alpha-helices are important determinants of the stability of protein secondary and tertiary structure. We investigate here the role of the helix-capping motif Ser-X-X-Glu, a sequence that occurs frequently at the N termini of alpha helices in proteins, on the conformation and stability of the GCN4 leucine zipper. The 1.8 A resolution crystal structure of the capped molecule reveals distinct conformations, packing geometries and hydrogen-bonding networks at the amino terminus of the two helices in the leucine zipper dimer. The free energy of helix stabilization associated with the hydrogen-bonding and hydrophobic interactions in this capping structure is -1.2 kcal/mol, evaluated from thermal unfolding experiments. A single cap thus contributes appreciably to stabilizing the terminated helix and thereby the native state. These results suggest that helix capping plays a further role in protein folding, providing a sensitive connector linking alpha-helix formation to the developing tertiary structure of a protein.     

Localization of the structural change induced in tRNA fMET (Escherichia coli) by acidic pH.

We have compared the molecular mechanism of thermal unfolding for native tRNA fMet (Escherichia coli) and the denatured species produced by annealing at pH 4.3. Relaxation kinetic measurements reveal that the transitions assigned to melting of TphiC, anticodon, and acceptor stem helices at neutral pH remain essentially unaltered at pH 4.3, but the transition corresponding to coupled melting of tertiary structure and dihydrouridine helix is greatly affected. The Tm of this region is more than 20 degrees higher at pH 4.3 and it has a larger enthalpy formation than in the native state. The transition dynamics are also considerably changed. In contrast to the native structure, tRNA fMet1 and tRNA fMet3 have similar tertiary structure stabilities at pH 4.3. We conclude that the structural difference between native and acid-denatured forms is localized in the tertiary structure-dihydrouridine helix cooperative interaction region of the molecule.     

Structure of a B-DNA decamer with a central T-A step: C-G-A-T-T-A-A-T-C-G.

The X-ray crystal structure analysis of the decamer C-G-A-T-T-A-A-T-C-G has been carried out to a resolution of 1.5 A. The crystals are space group P2(1)2(1)2(1), cell dimensions a = 38.60 A, b = 39.10 A, c = 33.07 A. The structure was solved by molecular replacement and refined with X-PLOR and NUCLSQ. The final R factor for a model with 404 DNA atoms, 108 water molecules and one magnesium hexahydrate cation is 15.7%. The double helix is essentially isostructural with C-G-A-T-C-G-A-T-C-G, with closely similar local helix parameters. The structure of the T-T-A-A center differs from that found in C-G-C-G-T-T-A-A-C-G-C-G in that the minor groove in our decamer is wide at the central T-A step rather than narrow, and the twist angle of the T-A step is small (31.1 degrees) rather than large. Whereas the tetrad model provides a convenient framework for discussing local DNA helix structure, it cannot be the entire story. The articulated helix model of DNA structure proposes that certain sequence regions of DNA show preferential twisting or bending properties, whereas other regions are less capable of deformation, in a manner that may be useful in sequence recognition by drugs and protein. Further crystal structure analyses should help to delineate the precise nature of sequence-dependent articulation in the DNA double helix.     

A spin label study of the thermal unfolding of secondary and tertiary structure in E. colic transfer RNAs.

The molecular mechanism of thermal unfolding of E. coli tRNAGlu, tRNAfMet and tRNAPhe (in 0.02M Tris-HC1, pH 7.5. 10 MM Mg C12) has been examined by the spin-labeling technique. The rate of tumbling of the spin label has been measured as a function of temperature for ten different selectively spin-labeled tRNAs. Only spin labels at position s4U-8 were able to probe the tertiary structure. Evidences are presented which support the hypothesis that the thermal denaturation of the three species of tRNAs studied is sequential. The unfolding process occurs in three discrete stages. The first step (30 degrees-32 degrees) could either be assigned to a localized reorganization of the cold-denatured structure or to a "transient" melting, followed by the simultaneous disruption of the tertiary structure and part of the hU helix. This transition is observed even in the absence of magnesium. The second step (50 degrees-54 degrees) involves the melting of the anticodon and miniloop regions. The last step occurs above 65 degrees where the t psi c and amino acid acceptor stems, forming one continuous double helix, melt. A simple dynamic model is considered for tRNA function in protein biosynthesis.     

Eukaryotic DNAs in solution contain characteristic components of tertiary structure.

For natural eukaryotic DNA in solution, we suggest the existence of secondary-helix components superponed to parts of the DNA double helices. In a previous report we found, for calf thymus DNA in solution and of different mean molar mass Mr, an electrostatically driven rise of the hydrodynamically operative contour length of the double helix. This result was derived from Mr-dependent systematic deviations from the almost but not exactly linear plots of intrinsic viscosity [eta] as a function of 1/cs1/2 (cs = Na+ concentration) accurately determined by a titration technique [K.G. and K.E.R., Nucl. Acids Res. 8, 2807 (1980)]. In order to discriminate between DNA elongation contributions caused by secondary or by tertiary structure effects, respective measurements have now been extended to different temperatures for two eukaryotic and two prokaryotic DNA species. The slope of the curves obtained for the (apparent) gradual elongation effect as a function of temperature is negative for the eukaryotic DNAs investigated and is smaller and positive for the prokaryotic species, thus revealing different underlying main elongation mechanisms. We propose that, for the eukaryotic DNA samples, an electrostatically driven partial abolition of tertiary structure components is responsible for the prevailing part of the DNA elongation effect measured. (A helix elongation of this type may be the result of an abolition of an apparent helix shortening as realized in a very high degree on formation of nucleosome chains or in a less degree by DNA molecules with a respective evolutionarily fitted tertiary structure). For the smaller effects of prokaryotic DNA species something like a base breathing seems to dominate. Recent literature results support such an interpretation.     

Molecular dynamics of individual alpha-helices of bacteriorhodopsin in dimyristol phosphatidylocholine. I. Structure and dynamics.

Understanding the role of the lipid bilayer in membrane protein structure and dynamics is needed for tertiary structure determination methods. However, the molecular details are not well understood. Molecular dynamics computer calculations can provide insight into these molecular details of protein:lipid interactions. This paper reports on 10 simulations of individual alpha-helices in explicit lipid bilayers. The 10 helices were selected from the bacteriorhodopsin structure as representative alpha-helical membrane folding components. The bilayer is constructed of dimyristoyl phosphatidylcholine molecules. The only major difference between simulations is the primary sequence of the alpha-helix. The results show dramatic differences in motional behavior between alpha-helices. For example, helix A has much smaller root-mean-squared deviations than does helix D. This can be understood in terms of the presence of aromatic residues at the interface for helix A that are not present in helix D. Additional motions are possible for the helices that contain proline side chains relative to other amino acids. The results thus provide insight into the types of motion and the average structures possible for helices within the bilayer setting and demonstrate the strength of molecular simulations in providing molecular details that are not directly visualized in experiments.     

Exendin-4 and glucagon-like-peptide-1: NMR structural comparisons in the solution and micelle-associated states.

Exendin-4, a 39 amino acid peptide originally isolated from the oral secretions of the lizard Heloderma suspectum, has been shown to share certain activities with glucagon-like-peptide-1 (GLP-1), a 30 amino acid peptide. We have determined the structuring preferences of exendin-4 and GLP-1 by NMR in both the solution and dodecylphosphocholine (DPC) micelle-associated states. Based on both chemical shift deviations and the pattern of intermediate range NOEs, both peptides display significant helicity from residue 7 to residue 28 with greater fraying at the N-terminus. Thornton and Gorenstein [(1994) Biochemistry 33, 3532-3539] reported that the presence of a flexible, helix-destabilizing, glycine at residue 16 in GLP-1 was an important feature for membrane and receptor binding. Exendin-4 has a helix-favoring glutamate as residue 16. In the micelle-associated state, NMR data indicate that GLP-1 is less helical than exendin-4 due to the presence of Gly16; chemical shift deviations along the peptide sequence suggest that Gly16 serves as an N-cap for a second, more persistent, helix. In 30 vol-% trifluoroethanol (TFE), a single continuous helix is evident in a significant fraction of the GLP-1 conformers present. Exendin-4 has a more regular and less fluxional helix in both media and displays stable tertiary structure in the solution state. In the micelle-bound state of exendin-4, a single helix (residues 11-27) is observed with residues 31-39 completely disordered and undergoing rapid segmental motion. In aqueous fluoroalcohol or aqueous glycol, the Leu21-Pro38 span of exendin-4 forms a compact tertiary fold (the Trp-cage) which shields the side chain of Trp25 from solvent exposure and produces ring current shifts as large as 3 ppm. This tertiary structure is partially populated in water and fully populated in aqueous TFE. The Leu21-Pro38 segment of exendin-4 may be the smallest protein-like folding unit observed to date. When the Trp-cage forms, fraying of the exendin-4 helix occurs exclusively from the N-terminus; backbone NHs for the C-terminal residues of the helix display H/D exchange protection factors as large as 10(5) at 9 degrees C. In contrast, no tertiary structure is evident when exendin-4 binds to DPC micelles. An energetically favorable insertion of the tryptophan ring into the DPC micelle is suggested as the basis for this change. With the exception of exendin-4 in media containing fluoro alcohol cosolvents, NMR structure ensembles generated from the NOE data do not fully reflect the conformational averaging present in these systems. Secondary structure definition from chemical shift deviations may be the most appropriate treatment for peptides that lack tertiary structure.     

Transfer RNA splicing in Saccharomyces cerevisiae. Secondary and tertiary structures of the substrates

Secondary and tertiary structures of four yeast tRNA precursors that contain introns have been elucidated using limited digestion with a variety of single-strand- and double-strand-specific nucleases. The pre-tRNAs, representing the variety of intron sizes and potential structures, were: pre-tRNALeuCAA, pre-tRNALeuUAG, pre-tRNAIleUAU, and pre-tRNAPro-4UGG. Conventional tRNA cloverleaf structure is maintained in these precursors except that the anticodon loop is interrupted by the intron. The intron contains a sequence which is complementary to a portion of the anticodon loop and allows the formation of a double helix often extending the anticodon stem. The 5' and 3' splicing cleavage sites are located at either end of this helix and are single-stranded. The intron is the most sensitive region to nuclease cleavage, suggesting that it is on the surface of the molecule and available for interaction with the splicing endonuclease. Absence of Mg2+ or spermidine renders the dihydrouridine and T psi C loops of these precursors highly sensitive to nuclease digestion. These ionic effects mimic those observed for tRNAPhe and suggest that the tRNA portion of these precursors has native tRNA structure. We propose consensus secondary and tertiary structures which may be of significance to eventual understanding of the mechanism of yeast tRNA splicing.     

Spectroscopically and kinetically distinct conformational populations of sol-gel-encapsulated carbonmonoxy myoglobin. A comparison with hemoglobin

We have used sol-gel encapsulation protocols to trap kinetically and spectroscopically distinct conformational populations of native horse carbonmonoxy myoglobin. The method allows for direct comparison of functional and spectroscopic properties of equilibrium and non-equilibrium populations under the same temperature and viscosity conditions. The results implicate tertiary structure changes that include the proximal heme environment in the mechanism for population-specific differences in the observed rebinding kinetics. Differences in the resonance Raman frequency of nu(Fe-His), the iron-proximal histidine stretching mode, are attributed to differences in the positioning of the F helix. For myoglobin, the degree of separation between the F helix and the heme is assigned as the conformational coordinate that modulates both this frequency and the innermost barrier controlling CO rebinding. A comparison with the behavior of encapsulated derivatives of human adult hemoglobin indicates that these CO binding-induced conformational changes are qualitatively similar to the tertiary changes that occur within both the R and T quaternary states. Protein-specific differences in the time scale for the proposed F helix relaxation are attributed to variations in the intra-helical hydrogen bonding patterns that help stabilize the position of the F helix.     

Helix Capping in RNA Structure

Helices are an essential element in defining the three-dimensional architecture of structured RNAs. While internal basepairs in a canonical helix stack on both sides, the ends of the helix stack on only one side and are exposed to the loop side, thus susceptible to fraying unless they are protected. While coaxial stacking has long been known to stabilize helix ends by directly stacking two canonical helices coaxially, based on analysis of helix-loop junctions in RNA crystal structures, herein we describe helix capping, topological stacking of a helix end with a basepair or an unpaired nucleotide from the loop side, which in turn protects helix ends. Beyond the topological protection of helix ends against fraying, helix capping should confer greater stability onto the resulting composite helices. Our analysis also reveals that this general motif is associated with the formation of tertiary structure interactions. Greater knowledge about the dynamics at the helix-junctions in the secondary structure should enhance the prediction of RNA secondary structure with a richer set of energetic rules and help better understand the folding of a secondary structure into its three-dimensional structure. These together suggest that helix capping likely play a fundamental role in driving RNA folding.     

Folding topology of the disulfide-bonded dimeric DNA-binding domain of the myogenic determination factor MyoD.

The myogenic determination factor MyoD is a member of the basic-helix-loop-helix (bHLH) protein family. A 68-residue fragment of MyoD encompassing the entire bHLH region (MyoD-bHLH) is sufficient for protein dimerization, sequence-specific DNA binding in vitro, and conversion of fibroblasts into muscle cells. The circular dichroism spectrum of MyoD-bHLH indicates the presence of significant alpha-helical secondary structure; however, the NMR spectrum lacks features of a well-defined tertiary structure. There is a naturally occurring cysteine at residue 135 in mouse MyoD that when oxidized to a disulfide induces MyoD-bHLH to form a symmetric homodimer with a defined tertiary structure as judged by sedimentation equilibrium ultracentrifugation and NMR spectroscopy. Oxidized MyoD-bHLH retains sequence-specific DNA-binding activity, albeit with an apparent 100-1000-fold decrease in affinity. Here, we report the structural characterization of the oxidized MyoD-bHLH homodimer by NMR spectroscopy. Our findings indicate that the basic region is unstructured and flexible, while the HLH region consists of two alpha-helices of unequal length connected by an as yet undetermined loop structure. Qualitative examination of interhelical NOEs suggests several potential arrangements for the two helix 1/helix 2 pairs in the symmetric oxidized dimer. These arrangements were evaluated for whether they could incorporate the disulfide bond, satisfy loop length constraints, and juxtapose the two basic regions. Only a model that aligns helix 1 parallel to helix 1' and antiparallel to helix 2 was consistent with all constraints. Thus, an antiparallel four-helix bundle topology is proposed for the symmetric dimer. This topology is hypothesized to serve as a general model for other bHLH protein domains.     

Structure of Ustilago maydis killer toxin KP6 alpha-subunit. A multimeric assembly with a central pore.

Ustilago maydis is a fungal pathogen of maize, some strains of which secrete killer toxins. The toxins are encoded by double-stranded RNA viruses in the cell cytoplasm. The U. maydis killer toxin KP6 contains two polypeptide chains, alpha and beta, having 79 and 81 amino acids, respectively, both of which are necessary for its killer activity. The crystal structure of the alpha-subunit of KP6 (KP6alpha) has been determined at 1.80-A resolution. KP6alpha forms a single domain structure that has an overall shape of an ellipsoid with dimensions 40 A x 26 A x 21 A and belongs to the alpha/beta-sandwich family. The tertiary structure consists of a four-stranded antiparallel beta-sheet, a pair of antiparallel alpha-helices, a short strand along one edge of the sheet, and a short N-terminal helix. Although the fold is reminiscent of toxins of similar size, the topology of KP6alpha is distinctly different in that the alpha/beta-sandwich motif has two right-handed betaalphabeta split crossovers. Monomers of KP6alpha assemble through crystallographic symmetries, forming a hexamer with a central pore lined by hydrophobic N-terminal helices. The central pore could play an important role in the mechanism of the killing action of the toxin.     

Identification of tertiary base pair resonances in the nuclear magnetic resonance spectra of transfer ribonucleic acid.

The low-field hydrogen-bond ring NH proton nuclear magnetic resonance (NMR) spectra of several transfer ribonucleic acids (tRNAs) related to yeast tRNAPhe have been examined in detail. Several resonances are sensitive to magnesium ion and temperature, suggesting that they are derived from tertiary base pairs. These same resonances cannot be attributed to cloverleaf base pairs as shown by experimental assignment and ring current shift calculation of the secondary base pair resonances. The crystal structure of yeast tRNAPhe reveals at least six tertiary base pairs involving ring NH hydrogen bonds, which we conclude are responsible for the extra resonances observed in the low-field NMR spectrum. In several tRNAs with the same tertiary folding potential and dihydrouridine helix sequence as yeast tRNAPhe, the extra resonances from tertiary base pairs are observed at the same position in the spectrum.     

A long-range pseudoknot is required for activity of the Neurospora VS ribozyme.

Four small RNA self-cleaving domains, the hammerhead, hairpin, hepatitis delta virus and Neurospora VS ribozymes, have been identified previously in naturally occurring RNAs. The secondary structures of these ribozymes are reasonably well understood, but little is known about long-range interactions that form the catalytically active tertiary conformations. Our previous work, which identified several secondary structure elements of the VS ribozyme, also showed that many additional bases were protected by magnesium-dependent interactions, implying that several tertiary contacts remained to be identified. Here we have used site-directed mutagenesis and chemical modification to characterize the first long-range interaction identified in VS RNA. This interaction contains a 3 bp pseudoknot helix that is required for tertiary folding and self-cleavage activity of the VS ribozyme.     

Amide proton exchange used to monitor the formation of a stable alpha-helix by residues 3 to 13 during folding of ribonuclease S

We make use of the known exchange rates of individual amide proton in the S-peptide moiety of ribonuclease S (RNAase S) to determine when during folding the alpha-helix formed by residues 3 to 13 becomes stable. The method is based on pulse-labeling with [3H]H2O during the folding followed by an exchange-out step after folding that removes 3H from all amide protons of the S-peptide except from residues 7 to 14, after which S-peptide is separated rapidly from S-protein by high performance liquid chromatography. The slow-folding species of unfolded RNAase S are studied. Folding takes place in strongly native conditions (pH 6.0, 10 degrees C). The seven H-bonded amide protons of the 3-13 helix become stable to exchange at a late stage in folding at the same time as the tertiary structure of RNAase S is formed, as monitored by tyrosine absorbance. At this stage in folding, the isomerization reaction that creates the major slow-folding species has not yet been reversed. Our result for the 3-13 helix is consistent with the finding of Labhardt (1984), who has studied the kinetics of folding of RNAase S at 32 degrees C by fast circular dichroism. He finds the dichroic change expected for formation of the 3-13 helix occurring when the tertiary structure is formed. Protected amide protons are found in the S-protein moiety earlier in folding. Formation or stabilization of this folding intermediate depends upon S-peptide: the intermediate is not observed when S-protein folds alone, and folding of S-protein is twice as slow in the absence of S-peptide. Although S-peptide combines with S-protein early in folding and is needed to stabilize an S-protein folding intermediate, the S-peptide helix does not itself become stable until the tertiary structure of RNAase S is formed.     

The structural flexibility of the preferredoxin transit peptide.

In order to obtain insight into the structural flexibility of chloroplast targeting sequences, the Silene pratensis preferredoxin transit peptide was studied by circular dichroism and nuclear magnetic resonance spectroscopy. In water, the peptide is unstructured, with a minor propensity towards helix formation from Val-9 to Ser-12 and from Gly-30 to Ser-40. In 50% (v/v) trifluoroethanol, structurally independent N- and C-terminal helices are stabilized. The N-terminal helix appears to be amphipathic, with hydrophobic and hydroxylated amino acids on opposite sides. The C-terminal helix comprises amino acids Met-29-Gly-50 and is destabilized at Gly-39. No ordered tertiary structure was observed. The results are discussed in terms of protein import into chloroplasts, in which the possible interactions between the transit peptide and lipids are emphasized.