Stabilities of consecutive A.C, C.C, G.G, U.C, and U.U mismatches in RNA internal loops: Evidence for stable hydrogen-bonded U.U and C.C.+ pairs.

The stability and structure of RNA duplexes with consecutive A.C, C.A, C.C, G.G, U.C, C.U, and U.U mismatches were studied by UV melting, CD, and NMR. The results are compared to previous results for GA and AA internal loops [SantaLucia, J., Kierzek, R., & Turner, D. H. (1990) Biochemistry 29, 8813-8819; Peritz, A., Kierzek, R., & Turner, D.H. (1991) Biochemistry 30, 6428-6436)]. The observed order for stability increments of internal loop formation at pH 7 is AG = GA approximately UU greater than GG greater than or equal to CA greater than or equal to AA = CU = UC greater than or equal to CC greater than or equal to AC. The results suggest two classes for internal loops with consecutive mismatches: (1) loops that stabilize duplexes and have strong hydrogen bonding and (2) loops that destabilize duplexes and may not have strong hydrogen bonding. Surprisingly, rCGCUUGCG forms a very stable duplex at pH 7 in 1 M NaCl with a TM of 44.8 degrees C at 1 x 10(-4) M and a delta G degrees 37 of -7.2 kcal/mol. NOE studies of the imino protons indicate hydrogen bonding within the U.U mismatches in a wobble-type structure. Resonances corresponding to the hydrogen-bonded uridines are located at 11.3 and 10.4 ppm. At neutral pH, rCGCCCGCG is one of the least stable duplexes with a TM of 33.2 degrees C and delta G degrees 37 of -5.1 kcal/mol. Upon lowering the pH to 5.5, however, the TM increases by 12 degrees C, and delta G degrees 37 becomes more favorable by 2.5 kcal/mol. The pH dependence of rCGCCCGCG may be due to protonation of the internal loop C's, since no changes in thermodynamic parameters are observed for rCGCUUGCG between pH 7 and 5.5. Furthermore, two broad imino proton resonances are observed at 10.85 and 10.05 ppm for rCGCCCGCG at pH 5.3, but not at pH 6.5. This is also consistent with C.C+ base pairs forming at pH 5.5. rCGCCAGCG and rGGCACGCC have a small pH dependence, with TM increases of 5 and 3 degrees C, respectively, upon lowering the pH from 7 to 5.5. rCGCCUGCG and rCGCUCGCG also show little pH dependence, with TM increases of 0.8 and 1.4 degrees C, respectively, upon lowering the pH to 5.5.(ABSTRACT TRUNCATED AT 400 WORDS)     

Nearest-neighbor thermodynamics and NMR of DNA sequences with internal A.A, C.C, G.G, and T.T mismatches

Thermodynamic measurements are reported for 51 DNA duplexes with A.A, C.C, G.G, and T.T single mismatches in all possible Watson-Crick contexts. These measurements were used to test the applicability of the nearest-neighbor model and to calculate the 16 unique nearest-neighbor parameters for the 4 single like with like base mismatches next to a Watson-Crick pair. The observed trend in stabilities of mismatches at 37 degrees C is G.G > T.T approximately A.A > C.C. The observed stability trend for the closing Watson-Crick pair on the 5' side of the mismatch is G.C >/= C.G >/= A.T >/= T.A. The mismatch contribution to duplex stability ranges from -2.22 kcal/mol for GGC.GGC to +2.66 kcal/mol for ACT.ACT. The mismatch nearest-neighbor parameters predict the measured thermodynamics with average deviations of DeltaG degrees 37 = 3.3%, DeltaH degrees = 7. 4%, DeltaS degrees = 8.1%, and TM = 1.1 degrees C. The imino proton region of 1-D NMR spectra shows that G.G and T.T mismatches form hydrogen-bonded structures that vary depending on the Watson-Crick context. The data reported here combined with our previous work provide for the first time a complete set of thermodynamic parameters for molecular recognition of DNA by DNA with or without single internal mismatches. The results are useful for primer design and understanding the mechanism of triplet repeat diseases.     

Thermodynamics of single mismatches in RNA duplexes

The thermodynamic properties and structures of single mismatches in short RNA duplexes were studied in optical melting and imino proton NMR experiments. The free energy increments at 37 degrees C measured for non-GU single mismatches range from -2.6 to 1.7 kcal/mol. These increments depend on the identity of the mismatch, adjacent base pairs, and the position in the helix. UU and AA mismatches are more stable close to a helix end, but GG mismatch stability is essentially unaffected by the position in the helix. Approximations are suggested for predicting stabilities of single mismatches in short RNA duplexes.     

Thermodynamic and structural properties of pentamer DNA.DNA, RNA.RNA, and DNA.RNA duplexes of identical sequence

Four pentamers with the general sequence 5'CU(T)GU(T)G/5'CACAG have been prepared by chemical synthesis in order to generate duplex structures with common sequences. The four duplexes studied include the DNA.DNA duplex (5'dCACAG/5'dCTGTG) and the RNA.RNA duplex (5'rCUGUG/5'rCACAG) as well as the two corresponding DNA.RNA heteroduplexes (5'rCUGUG/5'dCACAG and 5'CACAG/5'dCTGTG). The measured entropy, enthalpy, and free energy changes upon melting are reported for each pentamer and compared to the predicted values where possible. Results show that the two DNA.RNA heteroduplexes are destabilized (delta G degrees 25 = -4.2 +/- 0.4 kcal/mol) relative to either the DNA.DNA duplex (delta G degrees 25 = -4.8 +/- 0.5 kcal/mol) or the RNA.RNA duplex (delta G degrees 25 = -5.8 +/- 0.6 kcal/mol). Circular dichroism spectra indicate that the RNA and the two heteroduplexes adopt an A-form conformation, while the DNA conformation is B-form. Imino proton NMR spectra also show that the heteroduplex structures resemble the RNA.RNA duplex.     

Effects of site-specific substitution of 5-fluorouridine on the stabilities of duplex DNA and RNA.

The effects of 5-fluorouridine (FUrd) and 5-fluorodeoxyuridine (FdUrd) substitution on the stabilities of duplex RNA and DNA have been studied to determine how FUrd substitution in nucleic acids may alter the efficiency of biochemical processes that require complementary base pairing for molecular recognition. The parent sequence, 5'-GCGAAUUCGC, contains two non-equivalent uridines. Eight oligonucleotides (four RNA and four DNA) were prepared with either zero, one or two Urd substituted by FUrd. The stability of each self-complementary duplex was determined by measuring the absorbance at 260 nm as a function of temperature. Tm values were calculated from the first derivative of the absorbance versus temperature profiles and values for delta H0 and delta S0 were calculated from the concentration dependence of the Tm. Individual absorbance versus temperature curves were also analyzed by a parametric approach to calculate thermodynamic parameters for the duplex to single-stranded transition. Analysis of the thermodynamic parameters for each oligonucleotide revealed that FUrd substitution had sequence-dependent effects in both A-form RNA and B-form DNA duplexes. Conservation of helix geometry in FUrd-substituted duplexes was determined by CD spectroscopy. FUrd substitution at a single site in RNA stabilized the duplex (delta delta G37 = 0.8 kcal/mol), largely due to more favorable stacking interactions. FdUrd substitution at a single site in DNA destabilized the duplex (delta delta G37 = 0.3 kcal/mol) as a consequence of less favorable stacking interactions. All duplexes melt via single cooperative transitions.     

Purine-purine mismatches in RNA helices: evidence for protonated G.A pairs and next-nearest neighbor effects.

Thermodynamic parameters are presented for 12 different RNA duplexes containing A.A, A.G, G.A and G.G mismatches flanked by C-G base pairs. UV melting studies were conducted under three different buffer conditions in order to evaluate the effects of salt concentration and pH on the stability of each mismatch-containing duplex. The main findings are: (i) the mismatches have a wide range of effects on duplex stability, decreasing delta G degrees 37 of denaturation by approximately 0-7 kcal/mol; (ii) the nearest-neighbor assumption commonly used to calculate helix stability breaks down for G.A mismatches; and (iii) G.A mismatches separated by 2 bp form a protonated structure.     

An alternating sheared AA pair and elements of stability for a single sheared purine-purine pair flanked by sheared GA pairs in RNA

A previous NMR structure of the duplex 5'GGU GGA GGCU/PCCG AAG CCG5' revealed an unusually stable RNA internal loop with three consecutive sheared GA pairs. Here, we report NMR studies of two duplexes, 5'GGU GGA GGCU/PCCA AAG CCG5' (replacing the UG pair with a UA closing pair) and 5'GGU GAA GGCU/PCCG AAG CCG5' (replacing the middle GA pair with an AA pair). An unusually stable loop with three consecutive sheared GA pairs forms in the duplex 5'GGU GGA GGCU/PCCA AAG CCG5'. The structure contrasts with that reported for this loop in the crystal structure of the large ribosomal subunit of Deinococcus radiodurans [Harms, J., Schluenzen, F., Zarivach, R., Bashan, A., Gat, S., Agmon, I., Bartels, H., Franceschi, F., and Yonath, A. (2001) Cell 107, 679-688]. The middle AA pair in the duplex 5'GGU GAA GGCU/PCCG AAG CCG5' rapidly exchanges orientations, resulting in alternative base stacking and pseudosymmetry with exclusively sheared pairs. The U GAA G/G AAG C internal loop is 2.1 kcal/mol less stable than the U GGA G/G AAG C internal loop at 37 degrees C. Structural, energetic, and dynamic consequences upon functional group substitutions within related 3 x 3 and 3 x 6 internal loops are also reported.     

Thermodynamic characterization of single mismatches found in naturally occurring RNA

Many naturally occurring RNA structures contain single mismatches. However, the algorithms currently used to predict RNA structure from sequence rely on a minimal set of data for single mismatches, most of which occur rather infrequently in nature. As a result, several approximations and assumptions are used to predict the stability of RNA duplexes containing the most common single mismatches. Therefore, the relative frequency of single mismatches was determined by compiling and searching a database of 955 RNA secondary structures. Thermodynamic parameters for duplex formation, derived from optical melting experiments, are reported for 28 oligoribonucleotides containing frequently occurring single mismatches. These data were then combined with previous data to construct a dataset of 64 single mismatches, including the 30 most common in the database. Because of this increase in experimental thermodynamic parameters for single mismatches that occur frequently in nature, more accurate free energy calculations have resulted. To improve the prediction of the thermodynamic parameters for duplexes containing single mismatches that have not been experimentally measured, single mismatch-specific nearest neighbor parameters were derived. The free energy of an RNA duplex containing a single mismatch that has not been thermodynamically characterized can be calculated by: DeltaG degrees 37,single mismatch = DeltaG degrees 37,mismatch nt + DeltaG degrees 37,mismatch-NN interaction + DeltaG degrees 37,AU/GU. Here, DeltaG degrees 37,mismatch is -0.4, -2.1, and -0.3 kcal/mol for A.G, G.G, and U.U mismatches, respectively; DeltaG degrees 37,mismatch-NN interaction is 0.7, -0.5, 0.4, -0.4, and -1.0 kcal/mol for 5'YRR3'/3'RRY5', 5'RYY3'/3'YYR5', 5'YYR3'/3'RYY5', 5'YRY3'/3'RYR5', and 5'RRY3'/3'YYR5' mismatch-nearest neighbor combinations, respectively, when A and G are categorized as purines (R) and C and U are categorized as pyrimidines (Y); and DeltaG degrees 37,AU/GU is a penalty of 1.2 kcal/mol for replacing a G-C base pair with either an A-U or G-U base pair. Similar predictive models were also derived for DeltaH degrees single mismatch and DeltaS degrees single mismatch. These new predictive models, in conjunction with the reported thermodynamics for frequently occurring single mismatches, should allow for more accurate calculations of the free energy of RNA duplexes containing single mismatches and, furthermore, allow for improved prediction of secondary structure from sequence.     

Free energy contributions of G.U and other terminal mismatches to helix stability

Thermodynamic parameters of helix formation were measured spectroscopically for seven hexaribonucleotides containing a GC tetramer core and G.U or other terminal mismatches. The free energies of helix formation are compared with those for the tetramer core alone and with those for the hexamer with six Watson-Crick base pairs. In 1 M NaCl, at 37 degrees C, the free energy of a terminal G.U mismatch is about equal to that of the corresponding A.U pair. Although other terminal mismatches studied add between -1.0 and -1.6 kcal/mol to delta G0 37 for helix formation, all are less stable than the corresponding Watson-Crick pairs. Comparisons of the stability increments for terminal G.U mismatches and G.C pairs suggest when stacking is weak the additional hydrogen bond in the G.C pair adds roughly -1 kcal/mol to the favorable free energy of duplex formation.     

Thermodynamics of RNA internal loops with a guanosine-guanosine pair adjacent to another noncanonical pair

Thermodynamic parameters measured by optical melting are reported for formation of RNA duplexes containing tandem noncanonical pairs with at least one guanosine-guanosine (GG) pair. For selected sequences, imino proton NMR provides evidence that the desired duplex forms and that the structure of a GG pair adjacent to a noncanonical pair depends on context. A GG pair next to a different noncanonical pair is more stable than expected from measurements of adjacent GG pairs. This is likely due to an unfavorable stacking interaction between adjacent GG pairs, where areas of high negative charge probably overlap. The results suggest a model where tandem noncanonical pairs closed by two GC pairs are assigned the following free energy increments at 37 degrees C: 0.8 kcal/mol for adjacent GG pairs, 1.0 kcal/mol for GG next to UU, and -0.3 kcal/mol for all others. These values are adjusted by 0.65 kcal/mol for each closing AU pair.     

Thermodynamics of internal C.T mismatches in DNA.

Thermodynamics of 23 oligonucleotides with internal single C.T mismatches were obtained by measuring UV absorbance as a function of temperature. Results from these 23 duplexes were combined with three measurements from the literature to derive nearest-neighbor thermodynamic parameters for seven linearly independent trimer sequences with internal C.T mismatches. The data show that the nearest-neighbor model is adequate for predicting thermodynamics of oligonucleotides with internal C.T with average deviations for Delta G degrees37, Delta H degrees, Delta S degrees and T m of 6.4%, 9.9%, 10.6%, and 1.9 degreesC respectively. C.T mismatches destabilize the duplex in all sequence contexts. The thermodynamic contribution of C. T mismatches to duplex stability varies weakly depending on the orientation of the mismatch and its context and ranges from +1.02 kcal/mol for GCG/CTC and CCG/GTC to +1.95 kcal/mol for TCC/ATG.     

Pyrimidine.pyrimidine base-pair mismatches in DNA. A nuclear magnetic resonance study of T.T pairing at neutral pH and C.C pairing at acidic pH in dodecanucleotide duplexes

Structural features of pyrimidine.pyrimidine mismatches in the interior of oligonucleotide duplexes have been investigated by high resolution two-dimensional proton nuclear magnetic resonance (n.m.r.) spectroscopy. These studies were conducted on the self-complementary d(C-G-C-T-A-G-C-T-T-G-C-G) duplex (designated T.T 12-mer) and the self-complementary d(C-G-C-C-A-G-C-T-C-G-C-G) duplex (designated C.C 12-mer) containing T.T and C.C pairs located at identical positions four base-pairs from either end of the duplex. Proton n.m.r. studies on the T.T 12-mer duplex were undertaken in the neutral pH range, while studies on the C.C 12-mer duplex were recorded at acidic pH. The proton spectra narrowed considerably on lowering the pH below neutrality for the C.C 12-mer duplex. Two-dimensional nuclear Overhauser enhancement spectroscopy (NOESY) data sets have been recorded on the T.T 12-mer and C.C 12-mer duplexes in high salt H2O and D2O solution. The magnitude of the NOE crosspeaks and the directionality of the NOE connectivities demonstrate that both duplexes are right-handed with all bases, including those at the mismatch site, adopting an anti configuration about the glycosidic bond. The observed base and sugar proton chemical shifts suggest structural similarities for the trinucleotide segments centered about the T.T and C.C mismatches. A NOE is detected between the resolved imino protons of T4 and T9 at the mismatch site, consistent with formation of a stacked "wobble" T4(anti).T9(anti) pair in the T.T 12-mer duplex. A comparison of the imino proton chemical shift and NOE data suggests that the imino-carbonyl hydrogen bonds in the wobble T.T mismatch are weaker than the corresponding imino-carbonyl hydrogen bonds in the wobble G.T mismatch. The 4-amino protons of C4 and C9 at the mismatch site in the C.C 12-mer duplex do not exhibit the pattern of hydrogen-bonded and exposed protons separated by approximately 1.5 parts per million characteristic of cytidine amino protons involved in Watson-Crick G.C pairing. The experimental data are insufficient to differentiate between wobble C(anti).C+(anti) and other pairing possibilities for the mismatch in the C.C 12-mer duplex at acidic pH.     

Thermodynamics-structure relationship of single mismatches in RNA/DNA duplexes

Thermodynamics of 66 RNA/DNA duplexes containing single mismatches were measured by UV melting methods. Stability enhancements for rG. dT mismatches were the largest of all mismatches examined here, while rU.dG mismatches were not as stable. The methyl group on C5 of thymine enhanced the stability by 0.12 approximately 0.53 kcal mol(-)(1) depending on the identity of adjacent Watson-Crick base pairs, whereas the 2'-hydroxyl group in ribouridine stabilized the duplex by approximately 0.6 kcal mol(-)(1) regardless of the adjacent base pairs. Stabilities induced by the methyl group in thymine, the 2'-hydroxyl group of ribouridine, and an nucleotide exchange at rG.dT and rU.dG mismatches were found to be independent of each other. The order for the mismatch stabilities is rG.dT > rU. dG approximately rG.dG > rA.dG approximately rG.dA approximately rA. dC > rA.dA approximately rU.dT approximately rU.dC > rC.dA approximately rC.dT, although the identity of the adjacent base pairs slightly altered the order. The pH dependence stability and structural changes were suggested for the rA.dG but not for rG.dA mismatches. Comparisons of trinucleotide stabilities for G.T and G.U pairs in RNA, DNA, and RNA/DNA duplexes indicate that stable RNA/DNA mismatches exhibit a stability similar to RNA mismatches while unstable RNA/DNA mismatches show a stability similar to that of DNA mismatches. These results would be useful for the design of antisense oligonucleotides.     

Effect of thiazole orange doubly labeled thymidine on DNA duplex formation

Nucleic acid oligonucleotides are widely used in hybridization experiments for specific detection of complementary nucleic acid sequences. For design and application of oligonucleotides, an understanding of their thermodynamic properties is essential. Recently, exciton-controlled hybridization-sensitive fluorescent oligonucleotides (ECHOs) were developed as uniquely labeled DNA oligomers containing commonly one thymidine having two covalently linked thiazole orange dye moieties. The fluorescent signal of an ECHO is strictly hybridization-controlled, where the dye moieties have to intercalate into double-stranded DNA for signal generation. Here we analyzed the hybridization thermodynamics of ECHO/DNA duplexes, and thermodynamic parameters were obtained from melting curves of 64 ECHO/DNA duplexes measured by ultraviolet absorbance and fluorescence. Both methods demonstrated a substantial increase in duplex stability (ΔΔG°(37) ～ -2.6 ± 0.7 kcal mol(-1)) compared to that of DNA/DNA duplexes of the same sequence. With the exception of T·G mismatches, this increased stability was mostly unaffected by other mismatches in the position opposite the labeled nucleotide. A nearest neighbor model was constructed for predicting thermodynamic parameters for duplex stability. Evaluation of the nearest neighbor parameters by cross validation tests showed higher predictive reliability for the fluorescence-based than the absorbance-based parameters. Using our experimental data, a tool for predicting the thermodynamics of formation of ECHO/DNA duplexes was developed that is freely available at http://genome.gsc.riken.jp/echo/thermodynamics/ . It provides reliable thermodynamic data for using the unique features of ECHOs in fluorescence-based experiments.     

Thermodynamics of RNA duplexes with tandem mismatches containing a uracil-uracil pair flanked by C.G/G.C or G.C/A.U closing base pairs

The thermodynamics governing the denaturation of RNA duplexes containing 8 bp and a central tandem mismatch or 10 bp were evaluated using UV absorbance melting curves. Each of the eight tandem mismatches that were examined had one U-U pair adjacent to another noncanonical base pair. They were examined in two different RNA duplex environments, one with the tandem mismatch closed by G.C base pairs and the other with G.C and A.U closing base pairs. The free energy increments (Delta Gdegrees(loop)) of the 2 x 2 loops were positive, and showed relatively small differences between the two closing base pair environments. Assuming temperature-independent enthalpy changes for the transitions, (Delta Gdegrees(loop)) for the 2 x 2 loops varied from 0.9 to 1.9 kcal/mol in 1 M Na(+) at 37 degrees C. Most values were within 0.8 kcal/mol of previously estimated values; however, a few sequences differed by 1.2-2.0 kcal/mol. Single strands employed to form the RNA duplexes exhibited small noncooperative absorbance increases with temperature or transitions indicative of partial self-complementary duplexes. One strand formed a partial self-complementary duplex that was more stable than the tandem mismatch duplexes it formed. Transitions of the RNA duplexes were analyzed using equations that included the coupled equilibrium of self-complementary duplex and non-self-complementary duplex denaturation. The average heat capacity change (DeltaC(p)) associated with the transitions of two RNA duplexes was estimated by plotting DeltaH degrees and DeltaS degrees evaluated at different strand concentrations as a function of T(m) and ln T(m), respectively. The average DeltaC(p) was 70 +/- 5 cal K(-)(1) (mol of base pairs)(-)(1). Consideration of this heat capacity change reduced the free energy of formation at 37 degrees C of the 10 bp control RNA duplexes by 0.3-0.6 kcal/mol, which may increase Delta Gdegrees(loop) values by similar amounts.     

Nuclear magnetic resonance spectroscopy and molecular modeling reveal that different hydrogen bonding patterns are possible for G.U pairs: one hydrogen bond for each G.U pair in r(GGCGUGCC)(2) and two for each G.U pair in r(GAGUGCUC)(2)

G.U pairs occur frequently and have many important biological functions. The stability of symmetric tandem G.U motifs depends both on the adjacent Watson-Crick base pairs, e.g., 5'G > 5'C, and the sequence of the G.U pairs, i.e., 5'-UG-3' > 5'-GU-3', where an underline represents a nucleotide in a G.U pair [Wu, M., McDowell, J. A., and Turner, D. H. (1995) Biochemistry 34, 3204-3211]. In particular, at 37 degrees C, the motif 5'-CGUG-3' is less stable by approximately 3 kcal/mol compared with other symmetric tandem G.U motifs with G-C as adjacent pairs: 5'-GGUC-3', 5'-GUGC-3', and 5'-CUGG-3'. The solution structures of r(GAGUGCUC)(2) and r(GGCGUGCC)(2) duplexes have been determined by NMR and restrained simulated annealing. The global geometry of both duplexes is close to A-form, with some distortions localized in the tandem G.U pair region. The striking discovery is that in r(GGCGUGCC)(2) each G.U pair apparently has only one hydrogen bond instead of the two expected for a canonical wobble pair. In the one-hydrogen-bond model, the distance between GO6 and UH3 is too far to form a hydrogen bond. In addition, the temperature dependence of the imino proton resonances is also consistent with the different number of hydrogen bonds in the G.U pair. To test the NMR models, U or G in various G.U pairs were individually replaced by N3-methyluridine or isoguanosine, respectively, thus eliminating the possibility of hydrogen bonding between GO6 and UH3. The results of thermal melting studies on duplexes with these substitutions support the NMR models.     

Molecular recognition in purine-rich internal loops: thermodynamic,structural, and dynamic consequences of purine for adenine substitutions in 5'(rGGCAAGCCU)2

The contribution of amino groups to the thermodynamics, structure, and dynamics of tandem A.A mismatches is investigated by substitution of purine (P) for adenine (A) within the RNA duplex, 5'(rGGCAAGCCU)(2), to give 5'(rGGCPAGCCU)(2), 5'(rGGCAPGCCU)(2), and 5'(rGGCPPGCCU)(2). The 5'(rGGCAAGCCU)(2) duplex has sheared A(anti).A(anti) (A.A trans Hoogsteen/Sugar-edge) pairs in which the A5 amino group is involved in hydrogen bonds but the A4 amino group is not [Znosko, B. M., Burkard, M. E., Schroeder, S. J., Krugh, T. R., and Turner, D. H. (2002) Biochemistry 41, 14969-14977]. In comparison to 5'(rGGCAAGCCU)(2), replacing the amino group of A4 with a hydrogen stabilizes the duplex by 1.3 kcal/mol, replacement of the A5 amino group destabilizes the duplex by 0.6 kcal/mol, and replacement of both A4 and A5 amino groups destabilizes the duplex by 0.8 kcal/mol. In NMR structures, the P.A noncanonical pairs of the 5'(rGGCPAGCCU)(2) duplex have a sheared anti-anti structure (P.A trans Hoogsteen/Sugar-edge) with P4.A5 interstrand hydrogen bonding and A5 bases that interstrand stack, similar to the structure of 5'(rGGCAAGCCU)(2). In contrast, the A.P pairs of the 5'(rGGCAPGCCU)(2) duplex have a face-to-face conformation (A.P trans Watson-Crick/Watson-Crick) with intrastrand stacking resembling typical A-form geometry. Although the P5 bases in 5'(rGGCPPGCCU)(2) are involved in an interstrand stack, the loop region is largely undefined. The results illustrate that both hydrogen-bonded and non-hydrogen-bonded amino groups play important roles in determining the thermodynamic, structural, and dynamic characteristics of purine rich internal loops.     

Deoxyguanosine-deoxyadenosine pairing in the d(C-G-A-G-A-A-T-T-C-G-C-G) duplex: conformation and dynamics at and adjacent to the dG X dA mismatch site

Nuclear magnetic resonance (NMR) has been used to monitor the conformation and dynamics of the d-(C1-G2-A3-G4-A5-A6-T6-T5-C4-G3-C2-G1) self-complementary dodecanucleotide (henceforth called 12-mer GA) that contains a dG X dA purine-purine mismatch at position 3 in the sequence. These results are compared with the corresponding d(C-G-C-G-A-A-T-T-C-G-C-G) dodecamer duplex (henceforth called 12-mer) containing standard Watson-Crick base pairs at position 3 [Patel, D.J., Kozlowski, S.A., Marky, L.A., Broka, C., Rice, J.A., Itakura, K., & Breslauer, K.J. (1982) Biochemistry 21, 428-436]. The dG X dA interaction at position 3 was monitored at the guanosine exchangeable H-1 and nonexchangeable H-8 protons and the nonexchangeable adenosine H-2 proton. We demonstrate base-pair formation between anti orientations of the guanosine and adenosine rings on the basis of nuclear Overhauser effects (NOE) observed between the H-2 proton of adenosine 3 and the imino protons of guanosine 3 (intra base pair) and guanosines 2 and 4 (inter base pair). The dG(anti) X dA(anti) pairing should result in hydrogen-bond formation between the guanosine imino H-1 and carbonyl O-6 groups and the adenosine N-1 and NH2-6 groups, respectively. The base pairing on either side of the dG X dA pair remains intact at low temperature, but these dG X dC pairs at positions 2 and 4 are kinetically destabilized in the 12-mer GA compared to the 12-mer duplex. We have estimated the hydrogen exchange kinetics at positions 4-6 from saturation-recovery measurements on the imino protons of the 12-mer GA duplex between 5 and 40 degrees C. The measured activation energies for imino proton exchange in the 12-mer GA are larger by a factor of approximately 2 compared to the corresponding values in the 12-mer duplex. This implies that hydrogen exchange in the 12-mer GA duplex results from a cooperative transition involving exchange of several base pairs as was previously reported for the 12-mer containing a G X T wobble pair at position 3 [Pardi, A., Morden, K.M., Patel, D.J., & Tinoco, I., Jr. (1982) Biochemistry 21, 6567-6574]. We have assigned the nonexchangeable base protons by intra and inter base pair NOE experiments and monitored these assigned markers through the 12-mer GA duplex to strand transition.(ABSTRACT TRUNCATED AT 400 WORDS)     

Solution conformation of a deoxynucleotide containing tandem G.A mismatched base pairs and 3'-overhanging ends in d(GTGAACTT)2.

We have used 31P and 1H NMR spectroscopy and circular dichroism to define the solution conformation of d(GTGAACTT)2 which contains tandem G.A mismatched base pairs and 3'-overhanging TT ends. Measurements of coupling constants and NOE intensities show that the sugar puckers of the nucleotides are predominantly in the south domain (i.e., near C2'-endo) and that the glycosidic torsion angles are anti. The sequential NOE intensities indicate the presence of a right-handed helix. Analysis of the 31P and 1H NMR spectra of the duplex shows that the tandem mismatch forms a block in which there are unusual backbone torsion angles (i.e., in the BII state), within an otherwise B-like structure. The chemical shift of the N1H of the mismatched guanosine and NOEs between the mismatched base pairs and their nearest neighbors are inconsistent with the imino pairing present in single A.G mismatches or in the X-ray structure of a tandem mismatch [Privé, G. G., et al. (1987) Science 238, 498-503] but the data are consistent with the amino pairing found by Li et al. (1991) [Li, Y., et al. (1991) Proc. Natl. Acad. Sci. U.S.A. 88, 26-30]. The strong base-base stacking both within the tandem G.A block and between the G.A mismatches and their other nearest neighbors offsets the intrinsic destabilizing effects of the mismatch. Further, the 3'-TT overhangs stack onto the ends of the helix and stabilize the duplex against fraying, which accounts for the observed increase in the melting temperature compared with the flush-ended duplex.