16 research outputs found

    Solution Structure and Energy Calculation of Bis-Intercalation of Homodimeric Thiazole Orange Dye Derivatives in DNA:  Effects of Modifying the Linker

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    We have used two-dimensional 1H NMR spectroscopy obtained at 750 MHz to determine a high-resolution solution structure of the double-stranded DNA oligonucleotide d(5‘-CGCTAGCG-3‘)2 complexed with the bis-intercalating dye 1,1‘-(5,5,9,9-tetramethyl-5,9-diazatridecamethylene)-bis-4-[3-ethyl-2,3-dihydro(benzo-1,3-thiazolyl)-2-methylidene]quino-linium tetraiodide (TOTO11Et). The determination of the structure was based on a complete relaxation matrix analysis of the NOESY cross-peaks followed by restrained molecular dynamics calculations. Forty final structures were generated for the TOTO11Et complex from A-form and B-form dsDNA starting structures. The root-mean-square (rms) deviation of the coordinates for the 40 structures of the complex was 0.52 Å. A conformational analysis of the deoxyribose rings based on coupling constants obtained from selective DQF-COSY spectra revealed that all ring conformations were almost pure S-type. The structure of the TOTO11Et complex was compared with the structure of a similar DNA complex with a dye containing a shorter linker (TOTOEt). Substantial differences were observed between the two structures because of the difference in the length of the linker. Most prominent was a large difference in the degree of unwinding of the dsDNA part in the two complexes. Unwinding of 73° and 22° relative to the free dsDNA was observed for the complexes with TOTOEt and TOTO11Et, respectively. The AMBER94 force field together with the GB/SA solvation model was used for energy calculations on both of the two complexes. In the calculations, the complex formation was divided into two steps:  (i) unwinding of the free oligonucleotide and (ii) association of the bis-intercalators to the unwound oligonucleotide. The complex formation was in favor of TOTO11Et, mainly because the dsDNA is distorted less in the complex with TOTO11Et than in the complex with TOTOEt

    The Global Conformation of the Hammerhead Ribozyme Determined Using Residual Dipolar Couplings<sup>†</sup>

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    The global structure of the hammerhead ribozyme was determined in the absence of Mg2+ by solution NMR experiments. The hammerhead ribozyme motif forms a branched structure consisting of three helical stems connected to a catalytic core. The 1H-15N and 1H-13C residual dipolar couplings were measured in a set of differentially 15N/13C-labeled ribozymes complexed with an unlabeled noncleavable substrate. The residual dipolar couplings provide orientation information on both the local and the global structure of the molecule. Analysis of the residual dipolar couplings demonstrated that the local structure of the three helical stems in solution is well modeled by an A-form conformation. However, the global structure of the hammerhead in solution in the absence of Mg2+ is not consistent with the Y-shaped conformation observed in crystal structures of the hammerhead. The residual dipolar couplings for the helical stems were combined with standard NOE and J coupling constant NMR data from the catalytic core. The NOE data show formation of sheared G−A base pairs in domain 2. These NMR data were used to determine the global orientation of the three helical stems in the hammerhead. The hammerhead forms a rather extended structure under these conditions with a large angle between stems I and II (∼153°), a smaller angle between stems II and III (∼100°), and the smallest angle between stems I and III (∼77°). The residual dipolar coupling data also contain information on the dynamics of the molecule and were used here to provide qualitative information on the flexibility of the helical domains in the hammerhead ribozyme−substrate complex

    Locked Nucleic Acid (LNA) Recognition of RNA:  NMR Solution Structures of LNA:RNA Hybrids

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    Locked nucleic acids (LNAs) containing one or more 2‘-O,4‘-C-methylene-linked bicyclic ribonucleoside monomers possess a number of the prerequisites of an effective antisense oligonucleotide, e.g. unprecedented helical thermostability when hybridized with cognate RNA and DNA. To acquire a detailed understanding of the structural features of LNA giving rise to its remarkable properties, we have conducted structural studies by use of NMR spectroscopy and now report high-resolution structures of two LNA:RNA hybrids, the LNA strands being d(5‘-CTGATLATGC-3‘) and d(5‘-CTLGATLATLGC-3‘), respectively, TL denoting a modified LNA monomer with a thymine base, along with the unmodified DNA:RNA hybrid. In the structures, the LNA nucleotides are positioned as to partake in base stacking and Watson−Crick base pairing, and with the inclusion of LNA nucleotides, we observe a progressive change in duplex geometry toward an A-like duplex structure. As such, with the inclusion of three LNA nucleotides, the hybrid adopts an almost canonical A-type duplex geometry, and thus it appears that the number of modifications has reached a saturation level with respect to structural changes, and that further incorporations would furnish only minute changes in the duplex structure. We attempt to rationalize the conformational steering induced by the LNA nucleotides by suggesting that the change in electronic density at the brim of the minor groove, introduced by the LNA modification, is causing an alteration of the pseudorotational profile of the 3‘-flanking nucleotide, thus shifting this sugar equilibrium toward N-type conformation
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