Stability of XGCGCp, GCGCYp, and XGCGCYp helixes: an empirical estimate of the energetics of hydrogen bonds in nucleic acids

The stabilizing effects of dangling ends and terminal base pairs on the core helix GCGC are reported. Enthalpy and entropy changes of helix formation were measured spectrophotometrically for AGCGCU, UGCGCA, GGCGCCp, CGCGCGp, and the corresponding pentamers XGCGCp and GCGCYp containing the GCGC core plus a dangling end. Each 5' dangling end increases helix stability at 37 degrees C roughly 0.2 kcal/mol and each 3' end from 0.8 to 1.7 kcal/mol. The free energy increments for dangling ends on GCGC are similar to the corresponding increments reported for the GGCC core [Freier, S. M., Alkema, D., Sinclair, A., Neilson, T., & Turner, D. H. (1985) Biochemistry 24, 4533-4539], indicating a nearest-neighbor model is adequate for prediction of stabilization due to dangling ends. Nearest-neighbor parameters for prediction of the free energy effects of adding dangling ends and terminal base pairs next to G.C pairs are presented. Comparison of these free energy changes is used to partition the free energy of base pair formation into contributions of "stacking" and "pairing". If pairing contributions are due to hydrogen bonding, the results suggest stacking and hydrogen bonding make roughly comparable favorable contributions to the stability of a terminal base pair. The free energy increment associated with forming a hydrogen bond is estimated to be -1 kcal/mol of hydrogen bond.     

Sequence dependence for the energetics of dangling ends and terminal base pairs in ribonucleic acid

Stability increments of terminal unpaired nucleotides (dangling ends) and terminal base pairs on the core helixes AUGCAU and UGCGCA are reported. Enthalpy, entropy, and free energy changes of helix formation were measured spectrophotometrically for 18 oligoribonucleotides containing the core sequences. The results indicate 3' dangling purines add more stability than 3' dangling pyrimidines. In most cases, the additional stability from a 3' dangling end on an AU base pair is less than that on a GC base pair [Freier, S.M., Burger, B.J., Alkema, D., Neilson, T., & Turner, D.H. (1985) Biochemistry 22, 6198-6206]. The sequence dependence provides a test for the importance of dangling ends for various RNA interactions. Correlations are suggested with codon context effects and with the three-dimensional structure of yeast phenylalanine transfer RNA. In the latter case, all terminal unpaired nucleotides having stability increments more favorable than -1 kcal/mol are stacked on the adjacent base pair. All terminal unpaired nucleotides having stability increments less favorable than -0.3 kcal/mol are not stacked on the adjacent base pair. In several cases, this lack of stacking is associated with a turn in the sugar-phosphate backbone. This suggests stability increments measured on oligoribonucleotides may be useful for predicting tertiary structure in large RNA molecules. Comparison of the stability increments for terminal dangling ends and base pairs, and of terminal GC and AU base pairs, indicates the free energy increment associated with forming a hydrogen bond can be about -1 kcal/mol of hydrogen bond.     

The dynamic structural basis of differential enhancement of conformational stability by 5'- and 3'-dangling ends in RNA

Unpaired bases at the end of an RNA duplex (dangling ends) can stabilize the core duplex in a sequence-dependent manner and are important determinants of RNA folding, recognition, and functions. Using 2-aminopurine as a dangling end purine base, we have employed femtosecond time-resolved fluorescence spectroscopy, combined with UV optical melting, to quantitatively investigate the physical and structural nature of the stacking interactions between the dangling end bases and the terminal base pairs. A 3'-dangling purine base has a large subpopulation that stacks on the guanine base of the terminal GC or UG pair, either intrastrand or cross-strand depending on the orientation of the pair, thus providing stabilization of different magnitudes. On the contrary, a 5'-dangling purine base only has a marginal subpopulation that stacks on the purine of the same strand (intrastrand) but has little cross-strand stacking. Thus a 5'-dangling purine does not provide significant stabilization. These stacking structures are not static, and a dangling end base samples a range of stacked and unstacked conformations with respect to the terminal base pair. Femtosecond time-resolved anisotropy decay reveals certain hindered base conformational dynamics that occur on the picosecond to nanosecond time scales, which allow the dangling base to sample these substates. When the dangling purine is opposite to a U and is able to form a potential base pair at the end of the duplex, there is an interplay of base stacking and hydrogen-bonding interactions that depends on the orientation of the base pair relative to the adjacent GC pair. By resolving these populations that are dynamically exchanging on fast time scales, we elucidated the correlation between dynamic conformational distributions and thermodynamic stability.     

Sequence dependence for the energetics of terminal mismatches in ribooligonucleotides

Stability increments of terminal mismatches on the core helixes AUGCAU and UGCGCA are reported. Enthalpy, entropy, and free energy changes of helix formation were measured spectrophotometrically for 15 oligoribonucleotides containing the core sequences and various mismatches. Free energy increments for mismatches in this series range from -0.5 to -1.1 kcal/mol. These increments for mismatches on AU base pairs are smaller than those measured previously on GC base pairs [Freier, S.M., Kierzek, R., Caruthers, M.H., Neilson, T., & Turner, D.H. (1986) Biochemistry 25, 3209-3213]. The terminal GU mismatches in the sequences GAUGCAUUp and UAUGCAUGp add approximately the same stability increment as the corresponding terminal AU mismatch. The stability increments for pyrimidine-pyrimidine and pyrimidine-purine mismatches can be approximated within 0.3 kcal/mol by adding the stability increments for the corresponding 3' and 5' unpaired nucleotides (dangling ends). Stability increments for purine-purine mismatches are approximated well by the stability increment for the corresponding 3' dangling end made more favorable by 0.2 kcal/mol. These approximations are used to provide a table of stability increments for all 48 possible sequences of mismatches.     

Effects of flanking G . C base pairs on internal Watson-Crick, G . U, and nonbonded base pairs within a short ribonucleic acid duplex

A series of pentaribonucleotides, ApGpXpGpU (where X identical to A, G, C, or U), was synthesized to investigate the effects of flanking G . C pairs on internal Watson-Crick, G . U, and nonbonded base pairs. Sequences ApGpApCpU (Tm = 26 degrees C) and ApGpCpCpU (Tm = 25 degrees C) were each found to form a duplex with non-base-paired internal residues that stacked with the rest of the sequence but were not looped out. ApGpGpCpU also forms a duplex (Tm = 30 degrees C) but with dangling terminal nonbonded adenosines rather than internal nonbonded guanosines. ApGpUpCpU prefers a stacked single-strand conformation. In addition, contribution to duplex stability from an internal A . U or G . C base pair is enhanced by 6 degrees C when flanked by G . C base pairs as compared to A . U base pairs. G . C base pairs flanking an internal G . U base pair were found to be more tolerant to the altered conformation of a G . U pair and result in an increase to stability comparable with that found for an internal A . U base pair.     

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 double- and triple-helical aggregates formed by self-complementary oligoribonucleotides of the type rAxUy

The thermal denaturation of a series of oligoribonucleotides of the form rAxUy (x = 5 or 7 and y = 3-11) has been characterized by means of IR spectroscopy, UV spectroscopy, and DSC. IR spectra proved the occurrence of double- and triple-helical regions at various contents of uracil residues in the nucleotide. From DSC measurements transition enthalpies, entropies, and free enthalpies were derived. The effect of fraying in terminal base pairs of symmetrical nucleotides (x = y) was quantified. Thermodynamic excess parameters due to dangling ends (5'A and 3'U), terminal AU base pairs, and UAU base triplets were obtained by comparing DSC results from different nucleotides. Empirical values for contributions of base stacking and pairing to the stability of terminal AU base pairs have been estimated: for nucleotides under study with a high degree of fraying at the ends of the helix the major stabilization effect comes from base stacking. The size of the cooperative unit lambda in most nucleotides under study is larger than 1; i.e., in these cases intermolecular cooperation takes place. Through deconvolution of DSC data maximum populations of intermediate states FI,max were obtained. On the basis of these results all nucleotides under study were proved to melt in multistate manner. FI,max increases with the number of base pairs, decreases through dangling ends, and shows approximately constant values for triple-helical aggregates of the series rA5Uy as well as rA7Uy.     

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   

Influence of N6-isopentenyladenosine (i(6)A) on thermal stability of RNA duplexes.

The thermodynamic stability of self-complementary oligoribonucleotides containing N6-isopentenyladenosine (i(6)A) or N6-isopentanyladenosine (p(6)A) was determined. The base pairs i(6)A.U and p(6)A.U were placed in either an internal (separated and tandem) and a terminal position within the duplex, or unpaired i(6)A and p(6)A as a 3'-dangling ends. The thermal unfolding of the oligomers was determined by means of UV melting profiles and the thermodynamic parameters: enthalpy (DeltaH degrees ), entropy (DeltaS degrees) and free energy (DeltaG degrees (37)) as well as the melting temperature (T(m)) were calculated. Both modified nucleosides destabilized the duplexes, however, the effect depended on the position of the modified adenosine within the duplex. The similarity of the behavior of oligomers containing i(6)A and p(6)A suggests a negligible effect of the double bond on the thermal stability. The largest destabilization was observed when derivatives of adenosine were placed in an internal position. The effect of 3'-dangling ends suggests that the presence of the N6-isopentenyl- or N6-isopentanyl substitutent affects hydrogen bonding rather than stacking within duplex.     

Identification and assignment of base pairs in three helical stems of Torulopsis utilis ribosomal 5S RNA and its RNase T1 and RNase T2 cleaved fragments via 500-MHz proton homonuclear overhauser enhancements

Imino proton resonances in the downfield region (10-14 ppm) of the 500-MHz 1H NMR spectrum of Torulopsis utilis 5S RNA are identified (A X U, G X C, or G X U) and assigned to base pairs in helices I, IV, and V via analysis of homonuclear Overhauser enhancements (NOE) from intact T. utilis 5S RNA, its RNase T1 and RNase T2 digested fragments, and a second yeast (Saccharomyces cerevisiae) 5S RNA whose nucleotide sequence differs at only six residues from that of T. utilis 5S RNA. The near-identical chemical shifts and NOE behavior of most of the common peaks from these four RNAs strongly suggest that helices I, IV, and V retain the same conformation after RNase digestion and that both T. utilis and S. cerevisiae 5S RNAs share a common secondary and tertiary structure. Of the four G X U base pairs identified in the intact 5S RNA, two are assigned to the terminal stem (helix I) and the other two to helices IV and V. Seven of the nine base pairs of the terminal stem have been assigned. Our experimental demonstration of a G X U base pair in helix V supports the 5S RNA secondary structural model of Luehrsen and Fox [Luehrsen, K. R., & Fox, G.E. (1981) Proc. Natl. Acad. Sci. U.S.A. 78, 2150-2154]. Finally, the base-pair proton peak assigned to the terminal G X U in helix V of the RNase T2 cleaved fragment is shifted downfield from that in the intact 5S RNA, suggesting that helices I and V may be coaxial in intact T. utilis 5S RNA.     

Proton NMR study and conformational analysis of d(CGT), d(TCG) and d(CGTCG) in aqueous solution. The effect of a dangling thymidine and of a thymidine mismatch on DNA mini-duplexes

Proton NMR studies of d(CGT), d(TCG) and d(CGTCG) were carried out at 300 and 500 MHz. The temperature and concentration dependence of the chemical shifts of various resonances indicates duplex formation only in the cases of d(TCG) and d(CGTCG). It is concluded that d(TCG) forms a mini-duplex stabilized by a 5'-dangling thymine base. Thermodynamic parameters of the duplex-to-coil equilibrium of the d(TCG) duplex are: delta H0 = -22.3 kcal/mol and delta S0 = -70 cal/mol. K, which correspond to approximately 40% duplex formation at 0 degrees C in a 2 mM nucleotide solution. Comparison of these data with thermodynamic parameters given earlier [Borer, P.N., Dengler, B., Tinoco, I. and Uhlenbeck, O.C. (1974) J. Mol. Biol. 86, 843-853] leads to the conclusion that the dangling base stabilization observed here is approximately equivalent to the stabilization caused by one or two additional A . T base pairs. The chemical shift behaviour of various resonances in d(CGTCG) indicates duplex formation without looping out of the thymine bases. The T X T mismatch does not seem to disturb the helical structure to a large extent. Analysis of the vicinal proton-proton coupling constants of the three compounds yielded geometrical data for the sugar rings. The data are interpreted in terms of N and S pseudorotational ranges. It is shown that a distinct conformation-transmission effect is exerted by the guanosine residues in a 5'----3' direction.     

The synthesis and properties of oligodeoxyribonucleotides containing N6-methoxyadenine.

Oligodeoxyribonucleotides containing N6-methoxyadenine (M) have been synthesized. The order of stability of duplexes consisting of synthesized oligodeoxyribonucleotides, 5'd(CCTGGTAXCAGGTCC)3'-5'd(GGACCTGNTACCAGG)3' (X = M, A, G. N = A, G, T, C), was M: A (Tm = 52 degrees C) greater than M: T (50 degrees C) greater than M: G (48 degrees C) greater than M: C (46 degrees C) observed by thermal denaturation in a buffer of 0.01 M Na cacodylate, and 0.1 M NaCl at pH 7.0. The Tms are within a range of 6 degrees of difference, which is smaller than those of Tms of the duplexes containing A:N pairs (11 degrees) and G:N pairs (11 degrees). DNA replication study on a template-primer system, 5'd(32p-CAGCTTTCGC)3' 3'd(GTCGAAAGCGMAGTCG)5', showed that TTP and dCTP were incorporated into DNA strands at a site opposite to M by Klenow DNA polymerase, but dATP and dGTP were not.     

Effects of internal nonbonded bases and a G.U base pair on the stability of a short ribonucleic acid helix.

Proton nuclear magnetic resonance has been used to examine the effect of both noncomplementary and G.U oppositions in the duplexes formed by the synthetic pentaribonucleotides CpApApUpG, CpApUpUpG, CpApGpUpG, and CpApCpUpG. The lack of any sigmoidal behavior in the chemical shift vs. temperature plots of the base protons in the individual pentaribonucleotides indicates that duplexes with noncomplementary base oppositions of the type: formula: (see text), (where X = A, U, G, or C) do not form. Variable temperature spectra of the mixture of CpApGpUpG and CpApUpUpG were recorded over the range of 70--10 degrees C. The chemical shift vs. temperature plot of the purine aromatic protons displayed sigmoidal curves. This demonstrated both duplex formation and the presence of a G.U. base pair. The average Tm of the duplex was found to be 23.4 +/- 2.0 degrees C. This is similar to that of the duplex formed by CpApUpG (24.0 +/- 1.0 degrees C) but less than the Tm of the following duplexes: CpApApUpG:CpApUpUpG (Tm = 28.5 +/- 2.1 degrees C), CpApGpUpG:CpApCpUpG (Tm = 38.4 +/- 0.6 degrees C) and CpApUpApUpG (Tm = 41.5 +/- 1.1 degrees C). The G.U base pair has a Tm (20.0 degrees C) significantly lower than the rest of the duplex (24 +/- 1 degree C) and is a region of local instability within the double helix. This 1H NMR study is the first to investigate both the formation and relative stability of an internal G.U. base pair neighboring regular Watson--Crick base pairs.     

Thermodynamic and spectroscopic study of bulge loops in oligoribonucleotides

Thermodynamic parameters for bulge loops of one to three nucleotides in oligoribonucleotide duplexes have been measured by optical melting. The results indicate bulges Bn of An and Un have similar stabilities in the duplexes, GCGBmGCG + CGCCGC. The stability increment for a bulge depends on more than its adjacent base pairs. For example, the stability increment for a bulge is affected more than 1 kcal/mol by changing two nonadjacent base pairs or by adding terminal unpaired nucleotides (dangling ends) three base pairs away. Thus a nearest-neighbor approximation for helixes with bulges is oversimplified. Many of the non-self-complementary strands used in this study were observed to form homoduplexes. Such duplexes with GA mismatches were particularly stable.     

Conformations of duplex structures formed by oligodeoxynucleotides covalently linked to the intercalator 2-methoxy-6-chloro-9-aminoacridine

A family of covalent complexes between oligonucleotides and derivatives of the intercalating agent 9-amino acridine has been synthesized (Asseline, U., Thuong, N.T. and Helene, C. (1983) C.R.Acad. Sci. (Paris) 297 (III), 369-372) and studied (Lancelot, G., Asseline, U., Thuong, N.T., and Helene, C. (1985) Biochemistry 24, 2521-2529; Lancelot, G., Asseline, U., Thuong, N.T., and Helene, C. (1985) J. Biomol. Str. Dyn. 3, 913-921) with a view to understand nucleic acid-nucleic acid recognition. In order to understand the nature of interactions between the intercalator and the oligonucleotides in such complexes and the sensitivity of such interactions to the polymorphic form of the DNA, we have carried out molecular mechanics simulations on duplex deoxyoligonucleotides d(A)6.d(T)6 (A and B forms) and d(TATC).d(GATA) (B form) covalently bound to 2-methoxy-6-chloro-9-aminoacridine through a pentamethylene linker chain. Structures in which the acridine derivative is end stacked (at the 3' and 5' ends) and in which the dye is intercalated between the terminal base pairs (at both the ends) and between second and third base pairs from the 3' end are all of reasonably low energy in both A and B forms of DNA. Our studies on 3' end complexes find that in the B form, intercalation of the dye between the second and third base pairs is preferred over the other two modes of binding, while in the A form, intercalation between the terminal base pairs is preferred. In the 5' end A and B form complexes, outside stacking and intercalation between the terminal base pairs are preferred, respectively. Our calculations suggest the possibility that the presence of the dye attached covalently to the DNA can induce conformational transitions in the DNA. For example, intercalation of the dye two base pairs from the end could induce an A----B transition.     

An estimate of the nearest neighbor base-pair content of 5S RNA using CD and absorption spectroscopy.

We analyzed the CD and uv absorption spectra of 5S RNA from Escherichia coli using the method developed in the preceding paper. The analysis of spectra of 5S RNA at 20 degrees C in 0.1M NaClO4, 2.5 mM Na+ (phosphate), pH 7.0, and 0.5 mM MgSO4 gave 7 +/- 3.6 A.U base pairs, 25 +/- 3.6 G.C base pairs, and 7.5 +/- 3.6 G.U base pairs. Estimates of nearest neighbor base pairs were more consistent with the Pieler-Erdmann and the Gewirth-Moore secondary structure models than with the Fox-Woese or the Burns-Luoma-Marshall models. We also examined the structure of 5S RNA as a function of temperature. The melting profile exhibited two transitions--one at about 35 degrees C and one above 50 degrees C. Our spectral data showed that helices I and II were stable during the first transition, and agreed with other data that helix III was the most likely helix to have melted. The results from this in-depth study of 5S RNA indicate that our method of analysis should be useful for studying the secondary structures of other small, unmodified RNAs.     

Consecutive terminal GU pairs stabilize RNA helices

Consecutive GU pairs at the ends of RNA helices provide significant thermodynamic stability between -1.0 and -3.8 kcal/mol at 37 °C, which is equivalent to approximately 2 orders of magnitude in the value of a binding constant. The thermodynamic stabilities of GU pairs depend on the sequence, stacking orientation, and position in the helix. In contrast to GU pairs in the middle of a helix that may be destabilizing, all consecutive terminal GU pairs contribute favorable thermodynamic stability. This work presents measured thermodynamic stabilities for 30 duplexes containing two, three, or four consecutive GU pairs at the ends of RNA helices and a model to predict the thermodynamic stabilities of terminal GU pairs. Imino proton NMR spectra show that the terminal GU nucleotides form hydrogen-bonded pairs. Different orientations of terminal GU pairs can have different conformations with equivalent thermodynamic stabilities. These new data and prediction model will help improve RNA secondary structure prediction, identification of miRNA target sequences with GU pairs, and efforts to understand the fundamental physical forces directing RNA structure and energetics.     

Stability of 3' double nucleotide overhangs that model the 3' ends of siRNA

Thermodynamic parameters are reported for duplex formation in 1 M NaCl for 16 RNA sequences, each containing a core tetramer duplex, GGCC, and a 3' overhang consisting of two bases. The results indicate additional double-helical stability is conferred by the double 3' terminal overhang relative to the single 3' terminal overhang. A nearest-neighbor analysis of the data indicates that the free energy contribution at 37 degrees C of the second base in the double 3' terminal overhang varies from 0 to 0.7 kcal/mol. The second base in the 3' double overhang can contribute nearly the same stability to a duplex as a base pair or a 3' dangling overhang. Stability contribution of a dangling base, two nucleotides removed from the 3' end of a duplex, is dependent upon both the identity of the base as well as that of the dangling base that it neighbors. A second dangling base only increases the stability of the duplex when it is neighboring a 3' purine dangling nucleotide. Furthermore, a second dangling pyrimidine provides a greater contribution to duplex stability than a purine. A nearest-neighbor model was developed to predict the influence of 3' double overhang on the stability of duplex formation. The model improves the prediction of free energy and melting temperature when tested against six sequences with different core duplexes.     

Non-nearest-neighbor dependence of the stability for RNA bulge loops based on the complete set of group I single-nucleotide bulge loops

Fifty-nine RNA duplexes containing single-nucleotide bulge loops were optically melted in 1 M NaCl, and the thermodynamic parameters DeltaH degrees, DeltaS degrees, DeltaG 37 degrees, and TM for each sequence were determined. Sequences from this study were combined with sequences from previous studies [Longfellow, C. E., et al. (1990) Biochemistry 29, 278-285; Znosko, B. M., et al. (2002) Biochemistry 41, 10406-10417], thus examining all possible group I single-nucleotide bulge loop and nearest-neighbor sequence combinations. The free energy increments at 37 degrees C for the introduction of a group I single-nucleotide bulge loop range between 1.3 and 5.2 kcal/mol. The combined data were used to develop a model for predicting the free energy of a RNA duplex containing a single-nucleotide bulge. For bulge loops with adjacent Watson-Crick base pairs, neither the identity of the bulge nor the nearest-neighbor base pairs had an effect on the influence of the bulge loop on duplex stability. The proposed model for prediction of the stability of a duplex containing a bulged nucleotide was primarily affected by non-nearest-neighbor interactions. The destabilization of the duplex by the bulge was related to the stability of the stems adjacent to the bulge. Specifically, there was a direct correlation between the destabilization of the duplex and the stability of the less stable duplex stem. The stability of a duplex containing a bulged nucleotide adjacent to a wobble base pair also was primarily affected by non-nearest-neighbor interactions. Again, there was a direct correlation between the destabilization of the duplex and the stability of the less stable duplex stem. However, when one or both of the bulge nearest neighbors was a wobble base pair, the free energy increment for insertion of a bulge loop is dependent upon the position and orientation of the wobble base pair relative the bulged nucleotide. Bulge sequences of the type ((5'UBX)(3'GY)), ((5'GBG)(3'UU)) and ((5'UBU)(3'GG)) are less destabilizing by 0.6 kcal/mol, and bulge sequences of the type ((5'GBX)(3'UY)) and ((5'XBU)(3'YG)) are more destabilizing by 0.4 kcal/mol than bulge loops adjacent to Watson-Crick base pairs.     

Conserved unpaired adenine residues are important for ordered structures of 5S ribosomal RNA. An infrared study of the secondary and tertiary structure of Thermus thermophilus 5S rRNA

An improved set of infrared calibration spectra for the determination of G X C and A X U base pairs leads to 32 +/- 3 G X C (+ G X U) and 4 +/- 1 A X U base pairs for Thermus thermophilus 5S RNA in the presence and absence of Mg2+. These results give further support for the consensus secondary structure of 5S RNA recently proposed by several groups. T. thermophilus 5S RNA shows, in the presence of Mg2+, a distinct two-step thermal melting of its ordered structure. Based on new data about the stacking dependence of infrared intensities of unpaired ribonucleotides the spectral changes of the low-temperature transition should be explained by melting of stacked arrangements of unpaired bases and/or non-standard base pairs. Striking is the reduction in A stacking, which is not related to the melting of A X U base pairs, indicating the importance of the mostly conserved unpaired adenines for the Mg2+ stabilized higher-order structures especially within internal loops of 5S RNA.