Solution structure of a DNA three-way junction containing two unpaired thymidine bases. Identification of sequence features that decide conformer selection

The solution structure of a DNA three-way junction (3H) containing two unpaired thymidine bases at the branch site (3HT2), was determined by NMR. Arms A and B of the 3HT2 form a quasi-continuous stacked helix, which is underwound at the junction and has an increased helical rise. The unstacked arm C forms an acute angle of approximately 55 degrees with the unique arm A. The stacking of the unpaired thymidine bases on arm C resembles the folding of hairpin loops. From this data, combined with the reported stacking behavior of 23 other 3HS2 s, two rules are derived that together correctly reproduce their stacking preference. These rules predict, from the sequence of any 3HS2, its stacking preference. The structure also suggests a plausible mechanism for structure-specific recognition of branched nucleic acids by proteins.     

Helical stacking in DNA three-way junctions containing two unpaired pyrimidines: proton NMR studies.

The proton NMR spectra of DNA three-way junction complexes (TWJ) having unpaired pyrimidines, 5'-TT- and 5'-TC- on one strand at the junction site were assigned from 2D NOESY spectra acquired in H2O and D2O solvents and homonuclear 3D NOESY-TOCSY and 3D NOESY-NOESY in D2O solvent. TWJ are the simplest branched structures found in biologically active nucleic acids. Unpaired nucleotides are common features of such structures and have been shown to stabilize junction formation. The NMR data confirm that the component oligonucleotides assemble to form conformationally homogeneous TWJ complexes having three double-helical, B-form arms. Two of the helical arms stack upon each other. The unpaired pyrimidine bases lie in the minor groove of one of the helices and are partly exposed to solvent. The coaxial stacking arrangement deduced is different from that determined by Rosen and Patel (Rosen, M.A., and D.J. Patel. 1993. Biochemistry. 32:6576-6587) for a DNA three-way junction having two unpaired cytosines, but identical to that suggested by Welch et al. (Welch, J. B., D. R. Duckett, D. M. J. Lilley. 1993. Nucleic Acids Res. 21:4548-4555) on the basis of gel electrophoretic studies of DNA three-way junctions containing unpaired adenosines and thymidines.     

Refinement of the solution structure of a branched DNA three-way junction.

We have refined the structure of the DNA Three-Way Junction complex, TWJ-TC, described in the companion paper by quantitative analysis of two 2D NOESY spectra (mixing times 60 and 200 ms) obtained in D2O solution. NOESY crosspeak intensities extracted from these spectra were used in two kinds of refinement procedure: 1) distance-restrained energy minimization (EM) and molecular dynamics (MD) and 2) full relaxation matrix back calculation refinement. The global geometry of the refined model is very similar to that of a published, preliminary model (Leontis, 1993). Two of the helical arms of the junction are stacked. These are Helix 1, defined by basepairs S1-G1/S3-C12 through S1-C5/S3-G8 and Helix 2, which comprises basepairs S1-C6/S2-G5 through S1-G10/S2-G1. The third helical arm (Helix 3), comprised of basepairs S2-C6/S3-G5 through S2-C10/S3-G1 extends almost perpendicularly from the axis defined by Helices 1 and 2. The bases S1-C5 and S1-C6 of Strand 1 are continuously stacked across the junction region. The conformation of this strand is close to that of B-form DNA along its entire length, including the S1-C5 to S1-C6 dinucleotide step at the junction. The two unpaired bases S3-T6 and S3-C7 lie outside of the junction along the minor groove of Helix 1 and largely exposed to solvent. Analysis of the refined structure reveals that the glycosidic bond of S3-T6 exists in the syn conformation, allowing the methyl group of this residue to contact the hydrophobic surface of the minor groove of Helix 1, at S3-G11.(ABSTRACT TRUNCATED AT 250 WORDS)     

Solution conformation of a bulged adenosine base in an RNA duplex by relaxation matrix refinement

Bulges are common structural motifs in RNA secondary structure and are thought to play important roles in RNA-protein and RNA-drug interactions. Adenosine bases are the most commonly occurring unpaired base in double helical RNA secondary structures. The solution conformation and dynamics of a 25-nucleotide RNA duplex containing an unpaired adenosine, r(GGCAGAGUGCCGC): r(GCGGCACCUGCC) have been studied by NMR spectroscopy and MORASS iterative relaxation matrix structural refinement. The results show that the bulged adenosine residue stacks into the RNA duplex with little perturbation around the bulged region. Most of the bases in the RNA duplex adopt C(3)'-endo conformation, exhibiting the N-type sugar pucker as found in the A form helices. The sugars of the bulged residue and the 5' flanking residue to it are found to exhibit C(2)'-endo conformation. None of the residues are in syn conformation.     

Stability and structure of three-way DNA junctions containing unpaired nucleotides.

Non-paired nucleotides stabilize the formation of three-way helical DNA junctions. Two or more unpaired nucleotides located in the junction region enable oligomers ten to fifteen nucleotides long to assemble, forming conformationally homogeneous junctions, as judged by native gel electrophoresis. The unpaired bases can be present on the same strand or on two different strands. Up to five extra bases on one strand have been tested and found to produce stable junctions. The formation of stable structures is favored by the presence of a divalent cation such as magnesium and by high monovalent salt concentration. The order-disorder transition of representative three-way junctions was monitored optically in the ultraviolet and analyzed to quantify thermodynamically the stabilization provided by unpaired bases in the junction region. We report the first measurements of the thermodynamics of adding an unpaired nucleotide to a nucleic acid three-way junction. We find that delta delta G degrees (37 degrees C) = +0.5 kcal/mol for increasing the number of unpaired adenosines from two to three. Three-way junctions having reporter arms 40 base-pairs long were also prepared. Each of the three reporter arms contained a unique restriction site 15 base-pairs from the junction. Asymmetric complexes produced by selectively cleaving each arm were analyzed on native gels. Cleavage of the double helical arm opposite the strand having the two extra adenosines resulted in a complex that migrated more slowly than complexes produced by cleavage at either of the other two arms. It is likely that the strand containing the unpaired adenosines is kinked at an acute angle, forming a Y-shaped, rather than a T-shaped junction.     

Structures of bulged three-way DNA junctions.

We have studied a series of three-way DNA junctions containing unpaired bases on one strand at the branch-point of the junctions. The global conformation of the arms of the junctions has been analysed by means of polyacrylamide gel electrophoresis, as a function of conditions. We find that in the absence of added metal ions, all the results for all the junctions can be accounted for by extended structures, with the largest angle being that between the arms defined by the strand containing the extra bases. Upon addition of magnesium (II) or hexamine cobalt (III) ions, the electrophoretic patterns change markedly, indicative of ion-dependent folding transitions for some of the junctions. For the junction lacking the unpaired bases, the three inter-arm angles appear to be quite similar, suggesting an extended structure. However, the addition of unpaired bases permits the three-way junction to adopt a significantly different structure, in which one angle becomes smaller than the other two. These species also exhibit marked protection against osmium addition to thymine bases at the point of strand exchange. These results are consistent with a model in which two of the helical arms undergo coaxial stacking in the presence of magnesium ions, with the third arm defining an angle that depends upon the number of unpaired bases.     

Global structure of a DNA three-way junction by solution NMR: towards prediction of 3H fold

Three-way junctions (3H) are the simplest and most commonly occurring branched nucleic acids. They consist of three double helical arms (A to C), connected at the junction point, with or without a number of unpaired bases in one or more of the three different strands. Three-way junctions with two unpaired bases in one strand (3HS2) have a high tendency to adopt either of two alternative stacked conformations in which two of the three arms A, B and C are coaxially stacked, i.e. A/B-stacked or A/C-stacked. Empirical stacking rules, which successfully predict for DNA 3HS2 A/B-stacking preference from sequence, have been extended to A/C-stacked conformations. Three novel DNA 3HS2 sequences were designed to test the validity of these extended stacking rules and their conformational behavior was studied by solution NMR. All three show the predicted A/C-stacking preference even in the absence of multivalent cations. The stacking preference for both classes of DNA 3HS2 can thus be predicted from sequence. The high-resolution NMR solution structure for one of the stacked 3HS2 is also reported. It shows a well-defined local and global structure defined by an extensive set of classical NMR restraints and residual dipolar couplings. Analysis of its global conformation and that of other representatives of the 3H family, shows that the relative orientations of the stacked and non-stacked arms, are restricted to narrow regions of conformational space, which can be understood from geometric considerations. Together, these findings open up the possibility of full prediction of 3HS2 conformation (stacking and global fold) directly from sequence.     

Relative stabilities of DNA three-way, four-way and five-way junctions (multi-helix junction loops): unpaired nucleotides can be stabilizing or destabilizing.

Competition binding and UV melting studies of a DNA model system consisting of three, four or five mutually complementary oligonucleotides demonstrate that unpaired bases at the branch point stabilize three- and five-way junction loops but destabilize four-way junctions. The inclusion of unpaired nucleotides permits the assembly of five-way DNA junction complexes (5WJ) having as few as seven basepairs per arm from five mutually complementary oligonucleotides. Previous work showed that 5WJ, having eight basepairs per arm but lacking unpaired bases, could not be assembled [Wang, Y.L., Mueller, J.E., Kemper, B. and Seeman, N.C. (1991) Biochemistry, 30, 5667-5674]. Competition binding experiments demonstrate that four-way junctions (4WJ) are more stable than three-way junctions (3WJ), when no unpaired bases are included at the branch point, but less stable when unpaired bases are present at the junction. 5WJ complexes are in all cases less stable than 4WJ or 3WJ complexes. UV melting curves confirm the relative stabilities of these junctions. These results provide qualitative guidelines for improving the way in which multi-helix junction loops are handled in secondary structure prediction programs, especially for single-stranded nucleic acids having primary sequences that can form alternative structures comprising different types of junctions.     

The stereochemistry of a four-way DNA junction: a theoretical study.

The stereochemical conformation of the four-way helical junction in DNA (the Holliday junction; the postulated central intermediate of genetic recombination) has been analysed, using molecular mechanical computer modelling. A version of the AMBER program package was employed, that had been modified to include the influence of counterions and a global optimisation procedure. Starting from an extended planar structure, the conformation was varied in order to minimise the energy, and we discuss three structures obtained by this procedure. One structure is closely related to a square-planar cross, in which there is no stacking interaction between the four double helical stems. This structure is probably closely similar to that observed experimentally in the absence of cations. The remaining two structures are based on related, yet distinct, conformations, in which there is pairwise coaxial stacking of neighbouring stems. In these structures, the four DNA stems adopt the form of two quasi-continuous helices, in which base stacking is very similar to that found in standard B-DNA geometry. The two stacked helices so formed are not aligned parallel to each other, but subtend an angle of approximately 60 degrees. The strands that exchange between one stacked helix and the other are disposed about the smaller angle of the cross (i.e. 60 degrees rather than 120 degrees), generating an approximately antiparallel alignment of DNA sequences. This structure is precisely the stacked X-structure proposed on the basis of experimental data. The calculations indicate distortions from standard B-DNA conformation that are required to adopt the stacked X-structure; a widening of the minor groove at the junction, and reorientation of the central phosphate groups of the exchanging strands. An important feature of the stacked X-structure is that it presents two structurally distinct sides. These may be recognised differently by enzymes, providing a rationalisation for the points of cleavage by Holliday resolvases.     

Solution structure of a five-adenine bulge loop within a DNA duplex.

The three-dimensional solution structure of a DNA molecule of the sequence 5'-d(GCATCGAAAAAGCTACG)-3' paired with 5'-d(CGTAGCCGATGC)-3' containing a five-adenine bulge loop (dA(5)-bulge) between two double helical stems was determined by 2D (1)H and (31)P NMR, infrared, and Raman spectroscopy. The DNA in both stems adopt a classical B-form double helical structure with Watson-Crick base pairing and C2'-endo sugar conformation. In addition, the two dG/dC base pairs framing the dA(5)-bulge loop are formed and are stable at least up to 30 degrees C. The five adenine bases of the bulge loop are localized at intrahelical positions within the double helical stems. Stacking on the double helical stem is continued for the first four 5'-adenines in the bulge loop. The total rise (the height) of these four stacked adenines roughly equals the diameter of the double helical stem. The stacking interactions are broken between the last of these four 5'-adenines and the fifth loop adenine at the 3'-end. This 3'-adenine partially stacks on the other stem. The angle between the base planes of the two nonstacking adenines (A10 and A11) in the bulge loop reflects the kinking angle of the global DNA structure. The neighboring cytosines opposite the dA(5)-bulge (being parts of the bulge flanking base pairs) do not stack on one another. This disruption of stacking is characterized by a partial shearing of these bases, such that certain sequential NOEs for this base step are preserved. In the base step opposite the loop, an extraordinary hydrogen bond is observed between the phosphate backbone of the 5'-dC and the amino proton of the 3'-dC in about two-thirds of the conformers. This hydrogen bond probably contributes to stabilizing the global DNA structure. The dA(5)-bulge induces a local kink into the DNA molecule of about 73 degrees (+/-11 degrees ). This kinking angle and the mutual orientation of the two double helical stems agree well with results from fluorescence resonance energy transfer measurements of single- and double-bulge DNA molecules.     

Structures of helical junctions in nucleic acids

Our knowledge of the architectural principles of nucleic acid junctions has seen significant recent advances. The conformation of DNA junctions is now well understood, and this provides a new basis for the analysis of important structural elements in RNA. The most significant new data have come from X-ray crystallography of four-way DNA junctions; incidentally showing the great importance of serendipity in science, since none of the three groups had deliberately set out to crystallise a junction. Fortunately the results confirm, and of course extend, the earlier conformational studies of DNA junctions in almost every detail. This is important, because it means that these methods can be applied with greater confidence to new systems, especially in RNA. Methods like FRET, chemical probing and even the humble polyacrylamide gel can be rapid and very powerful, allowing the examination of a large number of sequence variants relatively quickly. Molecular modelling in conjunction with experiments is also a very important component of the general approach. Ultimately crystallography provides the gold standard for structural analysis, but the other, simple approaches have considerable value along the way. At the beginning of this review I suggested two simple folding principles for branched nucleic acids, and it is instructive to review these in the light of recent data. In brief, these were the tendency for pairwise coaxial stacking of helical arms, and the importance of metal ion interactions in the induction of folding. We see that both are important in a wide range of systems, both in DNA and RNA. The premier example is the four-way DNA junction, which undergoes metal ion-induced folding into the stacked X-structure that is based on coaxial stacking of arms. As in many systems, there are two alternative ways to achieve this depending on the choice of stacking partners. Recent data reveal that both forms often exist in a dynamic equilibrium, and that the relative stability of the two conformers depends upon base sequence extending a significant distance from the junction. The three-way junction has provided a good test of the folding principles. Perfect three-way (3H) DNA junctions seem to defy these principles in that they appear reluctant to undergo coaxial stacking of arms, and exhibit little change in conformation with addition of metal ions. Modelling suggests that such a junction is stereochemically constrained in an extended conformation. However, upon inclusion of a few additional base pairs at the centre (to create a 3HS2 junction for example) the additional stereochemical flexibility allows two arms to undergo coaxial stacking. Such a junction exhibits all the properties consistent with the general folding principles, with ion-induced folding into a form based on pairwise coaxial stacking of arms in one of two different conformers. The three-way junction is therefore very much the exception that proves the rule. It is instructive to compare the folding of corresponding species in DNA and RNA, where we find both similarities and differences. The RNA four-way junction can adopt a structure that is globally similar to the stacked X-structure (Duckett et al. 1995a), and the crystal structure of the DNAzyme shows that the stacked X-conformation can include one helical pair in the A-conformation (Nowakowski et al. 1999). However, modelling suggests that the juxtaposition of strands and grooves will be less satisfactory in RNA, and the higher magnesium ion concentration required to fold the RNA junction indicates a lower stability of the antiparallel form. Perhaps the biggest difference between the properties of the DNA and RNA four-way junctions is the lack of an unstacked structure at low salt concentrations for the RNA species. This clearly reflects a major difference in the electrostatic interactions in the RNA junction. In general the folding of branched DNA provides some good indications on the likely folding of the corresponding RNA species, but caution is required in making the extrapolation because the two polymers are significantly different. A number of studies point to the flexibility and malleability of branched nucleic acids, and this turns out to have particular significance in their interactions with proteins. Proteins such as the DNA junction-resolving enzymes exhibit considerable selectivity for the structure of their substrates, which is still not understood at a molecular level. Despite this, it appears to be universally true that these proteins distort the global, and in some cases at least the local, structure of the junctions. The somewhat perplexing result is that the proteins appear to distort the very property that they recognise. In general it seems that four-way DNA junctions are opened to one extent or another by interaction with proteins. (ABSTRACT TRUNCATED)     

RNA2D3D: A program for Generating,Viewing, and Comparing 3-Dimensional Models of RNA

Abstract

Using primary and secondary structure information of an RNA molecule, the program RNA2D3D automatically and rapidly produces a first-order approximation of a 3-dimensional conformation consistent with this information. Applicable to structures of arbitrary branching complexity and pseudoknot content, it features efficient interactive graphical editing for the removal of any overlaps introduced by the initial generating procedure and for making conformational changes favorable to targeted features and subsequent refinement. With emphasis on fast exploration of alternative 3D conformations, one may interactively add or delete base-pairs, adjacent stems can be coaxially stacked or unstacked, single strands can be shaped to accommodate special constraints, and arbitrary subsets can be defined and manipulated as rigid bodies. Compaction, whereby base stacking within stems is optimally extended into connecting single strands, is also available as a means of strategically making the structures more compact and revealing folding motifs. Subsequent refinement of the first-order approximation, of modifications, and for the imposing of tertiary constraints is assisted with standard energy refinement techniques. Previously determined coordinates for any part of the molecule are readily incorporated, and any part of the modeled structure can be output as a PDB or XYZ file. Illustrative applications in the areas of ribozymes, viral kissing loops, viral internal ribosome entry sites, and nanobiology are presented.     

The solution structure of the four-way DNA junction at low-salt conditions: a fluorescence resonance energy transfer analysis.

The four-way DNA (Holliday) junction is an important postulated intermediate in the process of genetic recombination. Earlier studies have suggested that the junction exists in two alternative conformations, depending upon the salt concentration present. At high salt concentrations the junction folds into a stacked X structure, while at low salt concentrations the data indicate an extended unstacked conformation. The stereochemical conformation of the four-way DNA junction at low salt (low alkali ion concentration and no alkaline earth ions) was established by comparing the efficiency of fluorescence resonance energy transfer (FRET) between donor and acceptor molecules attached pairwise in three permutations to the 5' termini of the duplex arms. A new variation of FRET was implemented based upon a systematic variation of the fraction of donor labeled single strands. The FRET results indicate that the structure of the four-way DNA junction at low salt exists as an unstacked, extended, square arrangement of the four duplex arms. The donor titration measurements made in the presence of magnesium ions clearly show the folding of the junction into the X stacked structure. In addition, the FRET efficiency can be measured. The fluorescence anisotropy of the acceptor in the presence of Mg2+ during donor titrations was also measured; the FRET efficiency can be calculated from the anisotropy data and the results are consistent with the folded, stacked X structure.     

Thermodynamics of unpaired terminal nucleotides on short RNA helixes correlates with stacking at helix termini in larger RNAs.

Free energies for stacking of unpaired nucleotides (dangling ends) at the termini of oligoribonucleotide Watson-Crick helixes (DeltaG(0)37,stack) depend on sequence for 3' ends but are always small for 5' ends. Here, these free energies are correlated with stacking at helix termini in a database of 34 RNA structures determined by X-ray crystallography and NMR spectroscopy. Stacking involving GA pairs is considered separately. A base is categorized as stacked by its distance from (相似文献   

RNA2D3D: a program for generating, viewing, and comparing 3-dimensional models of RNA

Using primary and secondary structure information of an RNA molecule, the program RNA2D3D automatically and rapidly produces a first-order approximation of a 3-dimensional conformation consistent with this information. Applicable to structures of arbitrary branching complexity and pseudoknot content, it features efficient interactive graphical editing for the removal of any overlaps introduced by the initial generating procedure and for making conformational changes favorable to targeted features and subsequent refinement. With emphasis on fast exploration of alternative 3D conformations, one may interactively add or delete base-pairs, adjacent stems can be coaxially stacked or unstacked, single strands can be shaped to accommodate special constraints, and arbitrary subsets can be defined and manipulated as rigid bodies. Compaction, whereby base stacking within stems is optimally extended into connecting single strands, is also available as a means of strategically making the structures more compact and revealing folding motifs. Subsequent refinement of the first-order approximation, of modifications, and for the imposing of tertiary constraints is assisted with standard energy refinement techniques. Previously determined coordinates for any part of the molecule are readily incorporated, and any part of the modeled structure can be output as a PDB or XYZ file. Illustrative applications in the areas of ribozymes, viral kissing loops, viral internal ribosome entry sites, and nanobiology are presented.     

Solution structure of a trinucleotide A-T-A bulge loop within a DNA duplex.

We have synthesized an oligodeoxynucleotide duplex, d(G-C-A-T-C-G-A-T-A-G-C-T-A-C-G).d(C-G-T-A-G-C-C-G-A-T-C-G), with a three-base bulge loop (A-T-A) at a central site in the first strand. Nuclear Overhauser experiments (NOESY) in H2O indicate that the GC base pairs flanking the bulge loop are intact between 0 and 25 degrees C. Nuclear Overhauser effects in both H2O and D2O indicate that all bases within the bulge loop are stacked into the helix. These unpaired bases retain an anti conformation about their glycosidic bonds as they stack within the duplex. The absence of normal sequential connectivities between the two cytosine residues flanking the bulge site on the opposite strand indicates a disruption in the geometry of this base step upon insertion of the bulged bases into the helix. This conformational perturbation is more akin to a shearing apart of the bases, which laterally separates the two halves of the molecule, rather than the "wedge" model often invoked for single-base bulges. Using molecular dynamics calculations, with both NOE-derived proton-proton distances and relaxation matrix-calculated NOESY cross peak volumes as restraints, we have determined the solution structure of an A-T-A bulge loop within a DNA duplex. The bulged bases are stacked among themselves and with the guanine bases on either side of the loop. All three of the bulged bases are displaced by 2-3 A into the major groove, increasing the solvent accessibility of these residues. The ATA-bulge duplex is significantly kinked at the site of the lesion, in agreement with previously reported electron microscopy and gel retardation studies on bulge-containing duplexes [Hsieh, C.-H., & Griffith, J. D. (1989) Proc. Natl. Acad. Sci. U.S.A 86, 4833-4837; Bhattacharyya, A., & Lilley, D. M. J. (1989) Nucleic Acids Res. 17, 6821-6840]. Bending occurs in a direction away from the bulge-containing strand, and we find a significant twist difference of 84 degrees between the two base pairs flanking the bulge loop site. This value represents 58% of the twist difference for base pairs four steps apart in B-DNA. These results suggest a structural mechanism for the bending of DNA induced by unpaired bases, as well as accounting for the effect bulge loops may have on the secondary and tertiary structures of nucleic acids.     

Left-handed Helical Polynucleotides with D-Sugar Phosphodiester Backbones

Naturally occurring polynucleotides have right-handed helical confrontations in the solid state¹ and in solution². Poly(dI-dC)poly(dI-dC) was found to form a left-handed helix in spite of the D-sugar backbone. Also, L-adenylyl-(3′–5′)-L-adenosine synthesized by Tazawa et al⁴. takes up the left-handed stacked conformation. We had synthesized a dinucleoside monophosphate, 8,2′-anhydro-8-mercapto-9-β-D-arabinofuranosyladenine phosphoryl-(3′–5′)-8,2′-anhydro-8-mercapto-9-β-D-arabinofuranosyladenine (A^spA^s) (molecular structure Ia; see also ref. 5) and this compound has a left-handed stacked conformation. The two bases in Ia, having the D-sugar backbone, stacked along the left-handed helical axis; these bases are fixed at ?_CN = ?108° (syn-anti region) by the anhydro linkages.     

Insights into the complex 3-D architecture of thylakoid membranes in the unicellular cyanobacterium Cyanothece sp. ATCC 51142

In cyanobacteria and chloroplasts, thylakoids are the complex internal membrane system where the light reactions of oxygenic photosynthesis occur. In plant chloroplasts, thylakoids are differentiated into a highly interconnected system of stacked grana and unstacked stroma membranes. In contrast, in cyanobacteria, the evolutionary progenitors of chloroplasts, thylakoids do not routinely form stacked and unstacked regions, and the architecture of the thylakoid membrane systems is only now being described in detail in these organisms. We used electron tomography to examine the thylakoid membrane systems in one cyanobacterium, Cyanothece sp. ATCC 51142. Our data showed that thylakoids form a complicated branched network with a rudimentary quasi-helical architecture in this organism. A well accepted helical model of grana-stroma architecture of plant thylakoids describes an organization in which stroma thylakoids wind around stacked granum in right-handed spirals. Here we present data showing that the simplified helical architecture in Cyanothece 51142 is lefthanded in nature. We propose a model comparing the thylakoid membranes in plants and this cyanobacterium in which the system in Cyanothece 51142 is composed of non-stacked membranes linked by fret-like connections to other membrane components of the system in a limited left-handed arrangement.Key words: cyanobacteria, Cyanothece 51142, thylakoid membrane, electron tomography, chloroplast     

The three-way DNA junction is a Y-shaped molecule in which there is no helix-helix stacking.

We have studied the structure of a number of three-way DNA junctions that were closely related in sequence to four-way junctions studied previously. We observe that the electrophoretic mobility of the species derived by selective shortening of one arm of a junction are very similar whichever arm is shortened, and that this remains so whether or not magnesium is present in the buffer. This suggests that the angles subtended between the arms of the three-way junctions are similar. All thymine bases located immediately at the junction are reactive to osmium tetroxide, indicating that out-of-plane attack is not prevented by helix-helix stacking, and this is also independent of the presence or absence of metal cations. The results suggest that the three-way junction cannot undergo an ion-induced conformational folding involving helical stacking, but remains fixed in a Y-shaped extended conformation. Thus the three- and four-way junctions are quite different in character in the presence of cations.