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Oligonucleotides modeled on a proposed base-triple domain in the P4/P6 region of the self-splicing group I intron have been characterized by NMR. The NMR data indicate that single-stranded nucleotides in this domain are in the minor groove of an adjacent helix within hydrogen bonding distance of 2'-hydroxyl groups in an interaction we term a nucleoside triple. Oligonucleotides containing the two most frequently occurring sequences among group I introns in the P4/P6 region formed nucleoside triples in the minor groove, whereas oligonucleotides containing sequences which are not conserved did not form triples. Surprisingly, the structures of the nucleoside triples in the oligonucleotides containing the two most frequently occurring sequences are different. If this difference were maintained in the context of the whole intron, it would suggest that the triples are not directly involved in catalysis, but rather that the nucleoside triples function by aligning the helical domains within the catalytic core of the intron.

About 70% of the RNA tetra-loop sequences identified in ribosomal RNAs from different organisms fall into either (UNCG) or (GNRA) families (where N = A, C, G, or U; and R = A or G). RNA hairpins with these loop sequences form unusually stable tetra-loop structures. We have studied the RNA hairpin GGAC(UUCG)GUCC and several sequence variants to determine the effect of changing the loop sequence and the loop-closing base pair on the thermodynamic stability of (UNCG) tetra-loops. The hairpin GGAG(CUUG)CUCC with the conserved loop G(CUUG)C was also unusually stable. We have determined melting temperatures (Tm), and obtained thermodynamic parameters for DNA hairpins with sequences analogous to stable RNA hairpins with (UNCG), C(GNRA)G, C(GAUA)G, and G(CUUG)C loops. DNA hairpins with (TTCG), (dUdUCG), and related sequences in the loop, unlike their RNA counterparts, did not form unusually stable hairpins. However, DNA hairpins with the consensus loop sequence C(GNRA)G were very stable compared to hairpins with C(TTTT)G or C(AAAA)G loops. The C(GATA)G and G(CTTG)C loops were also extra stable. The relative stabilities of the unusually stable DNA hairpins are similar to those observed for their RNA analogs.

The relaxation lifetimes of imino protons from individual base pairs were measured in (I) a perfect helix, d(C-G-C-G-A-A-T-T-C-G-C-G), (II) this helix with a G . C base pair replaced with a G . T base pair, d(C-G-T-G-A-A-T-T-C-G-C-G), and (III) the perfect helix with an extra adenine base in a mismatch, d(C-G-C-A-G-A-A-T-T-C-G-C-G). The lifetimes were measured by saturation recovery proton nuclear magnetic resonance experiments performed on the imino protons of these duplexes. The measured lifetimes of the imino protons were shown to correspond to chemical exchange lifetimes at higher temperatures and spin-lattice relaxation times at lower temperatures. Comparison of the lifetimes in these duplexes showed that the destabilizing effect of the G . T base pair in II affected the opening rate of only the nearest-neighbor base pairs. For helix III, the extra adenine affected the opening rates of all the base pairs in the helix and thus was a larger perturbation for opening of the base pairs than the G . T base pair. The temperature dependence of the exchange rates of the imino proton in the perfect helix gives values of 14-15 kcal/mol for activation energies of A . T imino protons. These relaxation rates were shown to correspond to exchange involving individual base pair opening in this helix, which means that one base-paired imino proton can exchange independent of the others. For the other two helices that contain perturbations, much larger activation energies for exchange of the imino protons were found, indicating that a cooperative transition involving exchange of at least several base pairs was the exchange mechanism of the imino protons. The effects of a perturbation in a helix on the exchange rates and the mechanisms for exchange of imino protons from oligonucleotide helices are discussed.

The lifetime for opening of individual base pairs in a DNA (dCA5G + dCT5G), and RNA (rCA5G + rCU5G), and a hybrid DNA-RNA (rCA5G + dCT5G) helix have been measured by proton nuclear magnetic resonance. The lifetimes were obtained by saturation recovery experiments performed on the hydrogen-bonding imino protons of the Watson-Crick base pairs. In these oligonucleotide helices the observed relaxation rates were dominated by exchange with water, with the magnetic spin-lattice relaxation time of the imino protons possibly being important only at the lowest temperatures in the DNA helix. It was shown that three interior base pairs in the DNA heptamer dCA5G + dCT5G were in the open-limited region, which means that these imino protons exchange every time the base pair opens. The lifetime of the terminal G X C base pairs in the DNA helix are much shorter than the interior A X T base pairs. The pH dependence of the terminal base pairs indicated that the ends of the helix open and close many times before exchange of the imino protons with water takes place. The temperature dependence of the lifetimes of the interior A X T imino protons in the DNA helix showed that these protons exchange only when the double helix has dissociated into single strands. Thus, these lifetimes measure the rate for dissociation of the double helix. The activation energy for this process was found to be 47 kcal/mol. Comparison of the lifetimes of the interior protons in the DNA, RNA, and hybrid helices showed that the rates of dissociation of the RNA and hybrid helices are very similar at 5 degrees C, whereas the rate for the DNA helix was approximately 1 order of magnitude smaller than that for the other two helices. The reasons for the differences in the kinetics of the three helices are discussed, as are the general dynamics of oligonucleotide helices in solution.

Oligoribonucleotide binding to baker's yeast initiator tRNA was measured by equilibrium dialysis in order to determine which regions of the tRNA were free to bind complementary oligomers and which were involved in secondary and tertiary structure. Association constants of trinucleoside diphosphates and tetranucleoside triphophates complementary to the single-stranded regions of the cloverleaf structure of yeast tRNAfMet were measured at o degrees in 1.0 M NaCl, and 0.01 M MgCl2. The only regions of the tRNA whose complementary oligomers bound to the tRNA were the amino acid acceptor end and the five nucleotides at the 5' end of the anticodon loop. These results differ from those for the other tRNAs studied by this technique; usually oligomers complementary to the dihydrouracil loop bind to the tRNA. The sequence of yeast tRNAfMet and other eucaryotic initiators is unusual. The "TpsiC loop" contains the sequence A-U-C instead of T-psi-C, yet the binding pattern to the THE TpsiC LOOP IS LIKE THAT FOR OTHER TRNAs; no oligomers bind.

The structures and hydrogen exchange properties of the mismatched DNA oligonucleotide duplexes d(CCCAGGG)2 and d(CCCTGGG)2 have been studied by high-resolution nuclear magnetic resonance. Both the adenine-adenine and thymine-thymine mismatches are intercalated in the duplexes. The structures of these self-complementary duplexes are symmetric, with the two strands in equivalent positions. The evidence indicates that these mismatches are not stably hydrogen bonded. The mismatched bases in both duplexes are in the anti conformation. The mismatched thymine nucleotide in d(CCCTGGG)2 is intercalated in the duplex with very little distortion of the bases or sugar-phosphate backbone. In contrast, the bases of the adenine-adenine mismatch in d(CCCAGGG)2 must tilt and push apart to reduce the overlap of the amino groups. The thermodynamic data show that the T-T mismatch is less destabilizing than the A-A mismatch when flanked by C-G base pairs in this sequence, in contrast to their approximately equal stabilities when flanked by A-T base pairs in the sequence d(CAAAXAAAG.CTTTYTTTG) where X and Y = A, C, G, and T [Aboul-ela, F., Koh, D., & Tinoco, I., Jr. (1985) Nucleic Acids Res. 13, 4811]. Although the mechanism cannot be determined conclusively from the limited data obtained, exchange of the imino protons with solvent in these destabilized heteroduplexes appears to occur by a cooperative mechanism in which half the helix dissociates.

The conformations of dinucleoside phosphates have been reexamined by semiempirical potential energy calculations. Conformations I, II, and III, proposed by Lee & Tinoco [Lee, C. H., & Tinoco, I., Jr. (1977) Biochemistry 16, 5403], are possible species after refinement of their structures by potential energy minimization. These three conformers can represent three types of dinucleoside phosphate species in solution. Dhingra et al. [Dhingra, M. M., Sarma, R. H., Giessner-Prettre, C., & Pullman, B. (1978) Biochemistry 17, 5815] had concluded that conformations of type II and III were unlikely or impossible. They favored conformations g-g- (equivalent to I), g+g+,g+t, and tg+; the last three conformations have little stacking and are calculated to be energetically less favorable by more than 5 kcal/mol. Common structures of the types I, II, and III are found for dinucleoside phosphates with different purine-pyrimidine sequences. The sequence dependence of the potential energy of these three conformers has been calculated. The experimental nuclear magnetic resonance data of dinucleoside phosphates are consistent with these three conformations.

The kinetics of U-U-C-A binding to the dodecanucleotide (A-Cm-U-Gm-A-A-Y-A-psi-m5C-U-Gp) isolated from the anticodon region of yeast tRNA-Phe are similar to the kinetics of binding of U-U-C-A to intact tRNA-Phe. A large enhancement in binding constant over that predicted for U-U-C-A-U-G-A-A is observed for both the complexes of dodecanucleotide and tRNA-Phe with U-U-C-A. This strongly suggests that both the anticodon loop in tRNA-Phe and the dodecanucleotide can form four base pairs with U-U-C-A. Furthermore, the enhanced stability cannot be attributed to a special conformation of the anticodon loop, but instead the anticodon loop is probably flexible. A likely explanation for the increased binding is the effect of non-base-paired ends. This increased thermodynamic stability comes from a larger entropy gain rather than a larger enthalpy decrease.

The kinetics of double-strand formation were measured by using temperature-jump kinetic techniques for the DNA oligonucleotides dCA5G + dCT5G, the analogous RNA oligonucleotides rCA5G + rCU5G, and the hybrid rCA5G + dCT5G. The DNA oligonucleotides have a faster rate of recombination and a slower rate of dissociation at 12.0 degrees C than the RNA oligonucleotides; the hybrid has about the same recombination rate and a slightly faster dissociation rate than the RNA oligonucleotides. The activation energies for recombination for the DNA and RNA oligonucleotides are both near 0 kcal/mol. The difference in dissociation and recombination activation energies is consistent with the thermodynamic results obtained earlier. The relaxation process is composed of two exponential components for the RNA and hybrid oligonucleotides at temperatures of 12.0 degrees C and lower. One exponential component is observed for these oligonucleotides above 12.0 degrees C and for the DNA oligonucleotides at all temperatures.

The nonexchangeable base protons and the hydrogen-bonding NH--N imino protons were used to study the conformations and the helix--coil transitions in the following oligonucleotides: (I) dCT5G + dCA5G, (II) rCU5G + rCA5G, (III) dCT5 G + rCA5G, (IV) rCU5G + dCA5G. The first three mixtures all form stable double-helical structures at 5 degrees C, whereas IV forms a triple strand with an rCU5G:dCA5G 2:1 ratio. The chemical shifts of the imino protons in the double strands indicate that I, II, and III have different conformations in solution. For example, the hydrogen-bonded proton of one of the C.G base pairs is more deshielded (a 0.4-ppm downfield shift) in helix I than in helix II or III. This implies a significant change in helical parameters, such as the winding angle, the distance between base pairs, or overlap of the bases. The coupling constants of the H1' sugar protons show that helix I has 90% 2'-endo sugar conformation, whereas helix III has greater than 85% 3'-endo conformation for the observed sugar rings. The sugar pucker data are consistent with helix I having B-family geometry; III has A-family geometry. The chemical shifts of the nonexchangeable base protons in system I were followed with increasing temperature. The midpoints for the transitions, Tm's, for all the base protons were 28--30 degrees C; this indicates an all-or-none transition.

The interactions of 4-nitroquinoline 1-oxide (NQO), a potent mutagen and carcinogen, with several self- and non-self-complementary deoxydinucleotides were probed by using absorption spectra of the charge transfer bands and 1H and 13C NMR spectra. Absorption spectra were analyzed by using Benesi-Hildebrand-type equations to yield stoichiometries and equilibrium constants of complex formation. Non-self complementary dimers form weak l:1 complexes [dpTpG:NQO, K(25 degrees C) = 22 M-1] while self-complementary dimers form strong 2:1 complexes [dpCpG)2:NQO, K(25 degrees C) = 2.2 X 10(4) M-2]. A mixture of dpTpG and dpCpA with NQO gives a 2:1 complexes [dpCpG)2:NQO, K(25 degrees C) = 2.2 X 10(4) M-2]. A mixture of dpTpG and dpCpA, K(25 degrees C) = 8.6 X 10(3) M-2]. Analyses of the changes in 13C and 1H NMR chemical shifts with complex formation gave approximate orientations for the intercalation of NQO with self-complementary dimer minihelixes. In the (dpCpG)2:NQO and (dpGpC)2:NQO complexes, the NO2 group of NQO probably lies in the major grove and the NO2, NO containing NQO ring is stacked near the purine imidazole ring. In the (dpTpA)2:NQO and (dpApT)2NQO complexes, the NO2 seems to project into the minor grove and the NQO benzenoid ring is over the purine imidazole ring.

The lifetimes for exchange of the imino protons in the dodecanucleotide d(C-G-C-G-A-A-T-T-C-G-C-G) upon binding of netropsin and/or actinomycin have been measured by proton nuclear magnetic resonance experiments. At high temperature these lifetimes were found to measure the lifetimes for opening of the base pairs in the double helix. Comparison of the opening rates in the dodecamer with those in the complex with netropsin (which binds at the -A-A-T-T- sequence) shows that there is not only a large kinetic stabilization of the A . T base pairs at the binding site but also a significant stabilization of the G . C base pairs adjacent to the netropsin binding site. For the complex with actinomycin, which intercalates at the G-C sites in the double strand, the lifetimes of the base pairs at the binding site increase upon binding of actinomycin, and the A . T base pairs in the central core are slightly kinetically destabilized by the actinomycin binding. The activation energies for exchange of the imino protons were also measured in the complexes and indicate that the mechanism for exchange of the imino protons is individual base-pair opening, where one base pair opens independently of the others. The effects of drug binding on the dynamics of individual base pairs in a double-stranded helix are discussed.