Selection for thermodynamically stable DNA tetraloops using temperature gradient gel electrophoresis reveals four motifs: d(cGNNAg), d(cGNABg),d(cCNNGg), and d(gCNNGc)

Hairpins play important roles in the function of DNA, forming cruciforms and affecting processes such as replication and recombination. Temperature gradient gel electrophoresis (TGGE) and in vitro selection have been used to isolate thermodynamically stable DNA hairpins from a six-nucleotide random library. The TGGE-selection process was optimized such that known stable DNA tetraloops were recovered, and the selection appears to be exhaustive. In the selection, four families of exceptionally stable DNA loops were identified: d(cGNNAg), d(cGNABg), d(cCNNGg), and d(gCNNGc). (Lowercase denotes the closing base pair; N = A, C, G, or T; and B = C, G, or T.) It appears that the known stable d(cGNAg) triloop motif can be embedded into a tetraloop, with the extra nucleotide inserted into either the middle of the loop, d(cGNNAg), or at the 3'-end of the loop, d(cGNABg). For d(cGNNAg) and d(cGNABg), a CG closing base pair was strongly preferred over a GC, with DeltaDeltaG degrees (37) approximately 2 kcal/mol. Members of the two families, d(cCNNGg) and d(gCNNGc), are similar in stability. The loop sequences and closing base pairs identified for exceptionally stable DNA tetraloops show many similarities to those known for exceptionally stable RNA tetraloops. These data provide an expanded set of thermodynamic rules for the formation of tetraloops in DNA.     

Effects of osmolytes on stable UUCG tetraloops and their preference for a CG closing base pair

Osmolytes have the potential to affect the stability of secondary structure motifs and alter preferences for conserved nucleic acid sequences in the cell. To contribute to the understanding of the in vivo function of RNA we observed the effects of different classes of osmolytes on the UNCG tetraloop motif. UNCG tetraloops are the most common and stable of the RNA tetraloops and are nucleation sites for RNA folding. They also have a significant thermodynamic preference for a CG closing base pair. The thermal denaturation of model hairpins containing UUCG loops was monitored using UV-Vis spectroscopy in the presence of osmolytes with different chemical properties. Interestingly, all of the osmolytes tested destabilized the hairpins, but all had little effect on the thermodynamic preference for a CG base pair, except for polyethylene glycol (PEG) 200. PEG 200 destabilized the loop with the CG closing base pair relative to the loop with a GC closing base pair. The destabilization was linear with increasing concentrations of PEG 200, and the slope of this relationship was not perturbed by changes in the hairpin stem outside of the closing pair. This result suggests that in the presence of PEG 200, the UUCG loop with a GC closing base pair may retain some preferential interactions with the cosolute that are lost in the presence of the CG closing base pair. These results reveal that relatively small structural changes may influence how osmolytes tune the stability, and thus the function of a secondary structure motif in vivo.     

Isolation and characterization of a family of stable RNA tetraloops with the motif YNMG that participate in tertiary interactions

RNA is known to fold into a variety of structural elements, many of which have sufficient sequence complexity to make the thermodynamic study of each possible variant impractical. We previously reported a method for isolating stable and unstable RNA sequences from combinatorial libraries using temperature gradient gel electrophoresis (TGGE). This method was used herein to analyze a six-nucleotide RNA hairpin loop library. Three rounds of in vitro selection were performed using TGGE, and unusually stable RNAs were identified by cloning and sequencing. Known stable tetraloops were found, including sequences belonging to the UNCG motif closed by a CG base pair, and the CUUG motif closed by a GC base pair. In addition, unknown tetraloops were found that were nearly as stable as cUNCGg, including sequences related through substitution of the U with a C (Y), the C with an A (M), or both. These substitutions allow hydrogen bonding and stacking interactions in the UNCG loop to be maintained. Thermodynamic analysis of YNMG and variant loops confirmed optimal stability with Y at position 1 and M at position 3. Similarity in structure and stability among YNMG loops was further supported by deoxyribose substitution, CD, and NMR experiments. A conserved tertiary interaction in 16S rRNA exists between a YAMG loop at position 343 and two adenines in the loop at position 159 (Escherichia coli numbering). NMR and functional group substitution experiments suggest that YNAG loops in particular have enhanced flexibility, which allows the tertiary interaction to be maintained with diverse loop sequences at position 159. Taken together, these results support the existence of an extended family of UNCG-like tetraloops with the motif cYNMGg that are thermodynamically stable and structurally similar and can engage in tertiary interactions in large RNA molecules.     

Thermodynamic parameters for loop formation in RNA and DNA hairpin tetraloops.

We determined the melting temperatures (Tm) and thermodynamic parameters of 15 RNA and 19 DNA hairpins at 1 M NaCl, 0.01 M sodium phosphate, 0.1 mM EDTA, at pH 7. All these hairpins have loops of four bases, the most common loop size in 16S and 23S ribosomal RNAs. The RNA hairpins varied in loop sequence, loop-closing base pair (A.U, C.G, or G.C), base sequence of the stem, and stem size (four or five base pairs). The DNA hairpins varied in loop sequence, loop-closing base pair (C.G, or G.C), and base sequence of the four base-pair stem. Thermodynamic properties of a hairpin may be represented by nearest-neighbor interactions of the stem plus contributions from the loop. Thus, we obtained thermodynamic parameters for the formation of RNA and DNA tetraloops. For the tetraloops we studied, a free energy of loop formation (at 37 degrees C) of about +3 kcal/mol is most common for either RNA or DNA. There are extra stable loops with delta G degrees 37 near +1 kcal/mol, but the sequences are not necessarily the same for RNA and DNA. The closing base pair is also important; changing from C.G to G.C lowered the stability of several tetraloops in both RNA and DNA. These values will be useful in predicting RNA and DNA secondary structures.     

Structural and thermodynamic signatures that define pseudotriloop RNA hairpins

Pseudotriloop (PTL) structures in RNAs have been recognized as essential elements in RNA folding and recognition of proteins. PTL structures are derived from hexaloops by formation of a cross–loop base pair leaving a triloop and 3′ bulged out residue. Despite their common presence and functional importance, insufficient structural and thermodynamic data are available that can be used to predict formation of PTLs from sequence alone. Using NMR spectroscopy and UV-melting data we established factors that contribute to the formation and stability of PTL structures derived from hepatitis B virus and human foamy virus. The NMR data show that, besides the cross–loop base pair, also a 3′ pyrimidine bulge and a G–C loop-closing base pair are primary determinants of PTL formation. By changing the G–C closing base pair into C–G, the PTL switches into a hexaloop. Comparison of these rules with regular triloop hairpins and PTLs from other sources is discussed as well as the conservation of a PTL in human foamy virus and other spumaretroviruses.     

A thermodynamic study of unusually stable RNA and DNA hairpins.

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.     

High-throughput thermal stability assessment of DNA hairpins based on high resolution melting

On the basis of high-resolution melting, a high-throughput approach to measure melting temperatures (T_ms) of short DNA hairpins was developed. With this method, T_ms of thousands of triloop, tetraloop, and pentaloop hairpins involving various loop sequences and various closing base pairs (cbp) were obtained in hours. The stability of triloop hairpins decreased with the change of cbp (5′–3′) in the order of c-g > g-c > t-a ≥ a-t, showing that the cbp of 5′-Pyr-Pur-3′ (Pyr = pyrimidine, Pur = purine) contributed more stability than 5′-Pur-Pyr-3′. For tetraloop hairpins, GNNA, GNAB, and CNNG (N = A, G, C, or T; B = G, C, or T) were found to be highly stable irrespective of the cbp type. TNNA was also stable in both g-c and a-t families, while CGNA only in the c-g family. Pentaloop hairpins of cTGNAGg, cGNYNAg (Y = T or C) and cCGNNAg were exceptionally stable motifs. In most cases, pyrimidine-rich loops were more favorable to stabilize the whole structure than purine-rich ones. The present approach showed a good performance in assessing the thermal stability of large amounts of DNA hairpins comprehensively. These data are useful to understand the sequence dependence of the stability of DNA secondary structures and promising to improve the structure simulation by consummating basic databases.     

RNA hairpin loop stability depends on closing base pair.

Thermodynamic parameters are reported for hairpin formation in 1 M NaCl by RNA sequences of the type GGXAUAAUAYCC, where X and Y are CG, GC, AU, UA, GU, or UG. A nearest neighbor analysis of the data indicates the free energy change for loop formation at 37 degrees C, delta degrees Gl,37, averages 3.4 kcal/mol for hairpin loops closed with C.G, G.C, and G.U pairs. In contrast, delta G degree l,37 averages 4.6 kcal/mol for loops closed with A.U, U.A, or U.G pairs. Thus the stability of an RNA hairpin depends on the closing base pair. The hairpin with a GA mismatch that is formed by GGCGUAAUAGCC is more stable than the corresponding hairpin with an AA mismatch. Thus hairpin stability also depends on loop sequence. These effects are not included in current algorithms for prediction of RNA structure from sequence.     

Use of ultra stable UNCG tetraloop hairpins to fold RNA structures: thermodynamic and spectroscopic applications.

RNA molecules of > 20 nucleotides have been the focus of numerous recent NMR structural studies. Several investigators have used the UNCG family of hairpins to ensure proper folding. We show that th UUCG hairpin has a minimum requirement of a two base-pair stem. Hairpins with a CG loop closing base pair and an initial 5'CG or 5'GC base pair have a melting temperature approximately 55 degrees C in 10 mM sodium phosphate. The high stability of even such small hairpins suggests that the hairpin can serve as a nucleation site for folding. For high resolution NMR work, the UNCG loop family (UACG in particular) provides excellent spectroscopic markers in one-dimensional exchangeable spectra, in two-dimensional COSY spectra and in NOESY spectra that clearly define it as forming a hairpin. This allows straightforward initiation of chemical shift assignments.     

Multinuclear NMR studies of DNA hairpins. 2. Sequence-dependent structural variations

The solution conformation of three related DNA hairpins, each with five bases in the loop, is investigated by proton and phosphorus 2D NMR methods. The sequences of the three oligomers are d(CGCGTTGTTCGCG), d(CGCGTTTGTCGCG), and d(CTGCTCTTGTTGAGCAG). One pair of hairpins shares the same stem sequence but differs in the loop, and the appearance of an unusual phosphate torsion in the stem is found to depend on the sequence in the loop of the hairpin. The second pair of hairpins shares the same loop region but differs in the stem sequence in that the base pair which closes the loop is a C-G or G-C pair. The pattern of NOEs reveals that the stacking arrangement in the loop region depends on the base pair that closes the stem. These results suggest that hairpin loop conformation and dynamics are sensitive to small changes in the loop and adjacent stem sequences. These findings are discussed in relation to sequence-dependent thermodynamic changes that have been observed in RNA hairpins.     

Parallel-stranded DNA with mixed AT/GC composition: role of trans G.C base pairs in sequence dependent helical stability

Parallel-stranded (ps) DNAs with mixed AT/GC content comprising G.C pairs in a varying sequence context have been investigated. Oligonucleotides were devised consisting of two 10-nt strands complementary either in a parallel or in an antiparallel orientation and joined via nonnucleotide linkers so as to form 10-bp ps or aps hairpins. A predominance of intramolecular hairpins over intermolecular duplexes was achieved by choice of experimental conditions and verified by fluorescence determinations yielding estimations of rotational relaxation times and fractional base pairing. A multistate mode of ps hairpin melting was revealed by temperature gradient gel electrophoresis (TGGE). The thermal stability of the ps hairpins with mixed AT/GC content depends strongly on the specific sequence in a manner peculiar to the ps double helix. The thermodynamic effects of incorporating trans G.C base pairs into an AT sequence are context-dependent: an isolated G. C base pair destabilizes the duplex whereas a block of > or =2 consecutive G.C base pairs exerts a stabilizing effect. A multistate heterogeneous zipper model for the thermal denaturation of the hairpins was derived and used in a global minimization procedure to compute the thermodynamic parameters of the ps hairpins from experimental melting data. In 0.1 M LiCl at 3 degrees C, the formation of a trans G.C pair in a GG/CC sequence context is approximately 3 kJ mol(-)(1) more favorable than the formation of a trans A.T pair in an AT/TA sequence context. However, GC/AT contacts contribute a substantial unfavorable free energy difference of approximately 2 kJ mol(-)(1). As a consequence, the base composition and fractional distribution of isolated and clustered G.C base pairs determine the overall stability of ps-DNA with mixed AT/GC sequences. Thus, the stability of ps-DNA comprising successive > or =2 G.C base pairs is greater than that of ps-DNA with an alternating AT sequence, whereas increasing the number of AT/GC contacts by isolating G.C base pairs exerts a destabilizing effect on the ps duplex. Molecular modeling of the various helices by force field techniques provides insight into the structural basis for these distinctions.     

Role of the closing base pair for d(GCA) hairpin stability: free energy analysis and folding simulations

Hairpin loops belong to the most important structural motifs in folded nucleic acids. The d(GNA) sequence in DNA can form very stable trinucleotide hairpin loops depending, however, strongly on the closing base pair. Replica-exchange molecular dynamics (REMD) were employed to study hairpin folding of two DNA sequences, d(gcGCAgc) and d(cgGCAcg), with the same central loop motif but different closing base pairs starting from single-stranded structures. In both cases, conformations of the most populated conformational cluster at the lowest temperature showed close agreement with available experimental structures. For the loop sequence with the less stable G:C closing base pair, an alternative loop topology accumulated as second most populated conformational state indicating a possible loop structural heterogeneity. Comparative-free energy simulations on induced loop unfolding indicated higher stability of the loop with a C:G closing base pair by ~3 kcal mol(-1) (compared to a G:C closing base pair) in very good agreement with experiment. The comparative energetic analysis of sampled unfolded, intermediate and folded conformational states identified electrostatic and packing interactions as the main contributions to the closing base pair dependence of the d(GCA) loop stability.     

Structure of an RNA hairpin from HRV-14.

The 5' noncoding region of the picornaviral genome begins with a cloverleaf which is required for viral replication, due at least in part to an interaction with the viral RNA polymerase as part of a fusion with the predominant viral protease. The necessary region of the cloverleaf has previously been narrowed to a highly conserved stem-loop. The solution structure of a 14-nucleotide RNA hairpin, which is part of the conserved stem-loop from human rhinovirus isotype 14, is presented here. The secondary structure of the hairpin is identical to predictions: a five base pair stem is bounded by a triloop with sequence UAU. However, the fold of the triloop is novel, with stacking of the second loop base onto the closing base pair of the stem, and deviations from A form geometry are introduced into the stem regions bordering the triloop, particularly on the 3' side. These deviations and the associated triloop structure could help to explain the distinct sequence conservation and mutational analysis data observed for the stem region of the hairpin, as compared to a second sequentially similar stem in the intact stem-loop.     

Hairpin structures in synthetic oligodeoxynucleotides: sequence effects on the duplex-to-hairpin transition

We have synthesized and examined a number of fully and partly self-complementary palindromic oligodeoxynucleotides for their ability to assume in solution a unimolecular hairpin structure. The main results obtained by a combined optical and electrophoresis investigation show that: (i) DNA folding needs not be driven by mismatched base pairings over the dyad; fully self-complementary palindromic duplexes, comprising regular (CG)n DNA fragments, possess a considerable intrinsic propensity to make intramolecular base pairings; (ii) The duplex-hairpin interconversion is, in general, a slow process independent of the length and base composition of the palindrome; (iii) The palindromic sequences energetically least favored to form hairpin structures consist of C:G base pairs around the dyad axis and of T:A blocks in the arms of the inverted repeat; (IV) The base composition of the stem strongly influences the hairpin thermal stability. For instance, the substitution of one C:G with one A:T base pair in the stem helix of d(CG)7 diminishes the stability of the hairpin by 9 degrees C. It is found that the stability of the stem helix, in hairpins of defined sequence and with the same loop length, decreases in the order alternating-CG greater than homo-CG greater than AC(GT) greater than alternating-AT, i.e. as in polynucleotides. The thermodynamic parameters for the hairpin-coil transition are reported.     

Solution structure of a GAAG tetraloop in helix 6 of SRP RNA from Pyrococcus furiosus

The NMR structure of a 12-mer RNA derived from the helix 6 of SRP RNA from Pyrococcus furiosus, whose loop-closing base pair is U.G, was determined, and the structural and thermodynamic properties of the RNA were compared with those of a mutant RNA with the C:G closing base pair. Although the structures of the two RNAs are similar to each other and adopt the GNRR motif the conformational stabilities are significantly different to each other It was suggested that weaker stacking interaction of the GAAG loop with the U:G closing base pair in 12-mer RNA causes the lower conformational stability.     

Preference for ribose over deoxyribose in loop-closing base pairs of extra stable nucleic acid hairpins

We have investigated the effect of switching ribose to deoxyribose at the closing base-pair of an extra-stable RNA hairpin. Specifically, we studied the sequence 5'-GGAC(UUCG)GUCC, a dodecanucleotide that folds into a well-characterized, "extra stable" RNA hairpin structure. Recently, we showed that hairpins containing a 2',5'-linked (UUCG) loop instead of the native 3',5'-linked loop also exhibit extra-stability (Hannoush and Damha, J. Am. Chem. Soc., 2001, 123, 12368-12374). In this article, we show that the ribose units located at the loop-closing positions (i.e., rC4 and rG9) contribute significantly to the stabilization of RNA hairpins, particularly those containing the 3',5'-UUCG loop. Interestingly, the requirement of rC4 and rG9 is more relaxed for DNA hairpins containing the 2',5'-UUCC loop and, in fact, they may be replaced altogether (ribose--> deoxyribose) without affecting stability. The results broaden our understanding of the behavior of highly stable (UUCG) hairpin loops and how they respond to structural perturbation of the loop-closing base pairs.     

MS2 RNA has a potential to form an unusually large number of stable hairpins

Several long nucleotide sequences were analysed to find out if any of them are unusual in terms of the possible formation of “hairpins” (pairs of complementary runs of nucleotides forming double-stranded structures) as compared to random sequences. The RNA of MS2 bacteriophage has more potential hairpins with short loops (up to 10 bases in a loop) than found in random sequences with the same length and base composition. Other analyzed nucleotide sequences (SV40, φX174, Fd and 16S rRNA) behaved very much as their corresponding random ones. Most of the extra hairpins of the MS2 RNA are estimated to be thermodynamically stable. These potential hairpins might play some role in the function of the MS2 RNA.     

Internal loop/bulge and hairpin loop of the iron-responsive element of ferritin mRNA contribute to maximal iron regulatory protein 2 binding and translational regulation in the iso-iron-responsive element/iso-iron regulatory protein family

Iron-responsive elements (IREs), a natural group of mRNA-specific sequences, bind iron regulatory proteins (IRPs) differentially and fold into hairpins [with a hexaloop (HL) CAGUGX] with helical distortions: an internal loop/bulge (IL/B) (UGC/C) or C-bulge. C-bulge iso-IREs bind IRP2 more poorly, as oligomers (n = 28-30), and have a weaker signal response in vivo. Two trans-loop GC base pairs occur in the ferritin IRE (IL/B and HL) but only one in C-bulge iso-IREs (HL); metal ions and protons perturb the IL/B [Gdaniec et al. (1998) Biochemistry 37, 1505-1512]. IRE function (translation) and physical properties (T(m) and accessibility to nucleases) are now compared for IL/B and C-bulge IREs and for HL mutants. Conversion of the IL/B into a C-bulge by a single deletion in the IL/B or by substituting the HL CG base pair with UA both derepressed ferritin synthesis 4-fold in rabbit reticulocyte lysates (IRP1 + IRP2), confirming differences in IRP2 binding observed for the oligomers. Since the engineered C-bulge IRE was more helical near the IL/B [Cu(phen)(2) resistant] and more stable (T(m) increased) and the HL mutant was less helical near the IL/B (ribonuclease T1 sensitive) and less stable (T(m) decreased), both CG trans-loop base pairs contribute to maximum IRP2 binding and translational regulation. The (1)H NMR spectrum of the Mg-IRE complex revealed, in contrast to the localized IL/B effects of Co(III) hexaammine observed previously, perturbation of the IL/B plus HL and interloop helix. The lower stability and greater helix distortion in the ferritin IL/B-IRE compared to the C-bulge iso-IREs create a combinatorial set of RNA/protein interactions that control protein synthesis rates with a range of signal sensitivities.     

Sequence dependence of the stability of RNA hairpin molecules with six nucleotide loops

Thermodynamic parameters are reported for hairpin formation in 1 M NaCl by RNA sequence of the types GCGXUAAUYCGC and GGUXUAAUYACC with Watson-Crick loop closure, where XY is the set of 10 possible mismatch base pairs. A nearest-neighbor analysis of the data indicates the free energy of loop formation at 37 degrees C varies from 3.1 to 5.1 kcal/mol. These results agree with the model previously developed [Vecenie, C. J., and Serra, M. J. (2004) Biochemistry 43, 11813] to predict the stability of RNA hairpin loops: DeltaG degrees (37L(n) = DeltaG degrees (37i(n) + DeltaG degrees (37MM) - 0.8 (if first mismatch is GA or UU) - 0.8 (if first mismatch is GG and loop is closed on the 5' side by a purine). Here, DeltaG degrees (37i(n) is the free energy for initiating a loop of n nucleotides, and DeltaG degrees (37MM) is the free energy for the interaction of the first mismatch with the closing base pair. Thermodynamic parameters are also reported for hairpin formation in 1 M NaCl by RNA sequence of the types GACGXUAAUYUGUC and GGUXUAAUYGCC with GU base pair closure, where XY is the set of 10 possible mismatch base pairs. A nearest-neighbor analysis of the data indicates the free energy of loop formation at 37 degrees C varies from 3.6 to 5.3 kcal/mol. These results allow the development of a model for predicting the stability of hairpin loops closed by GU base pairs. DeltaG degrees (37L(n) (kcal/mol) = DeltaG degrees (37i(n) - 0.8 (if the first mismatch is GA) - 0.8 (if the first mismatch is GG and the loop is closed on the 5' side by a purine). Note that for these hairpins, the stability of the loops does not depend on DeltaG degrees (37MM). For hairpin loops closed by GU base pairs, the DeltaG degrees (37i(n) values, when n = 4, 5, 6, 7, and 8, are 4.9, 5.0, 4.6, 5.0, and 4.8 kcal/mol, respectively. The model gives good agreement when tested against six naturally occurring hairpin sequences. Thermodynamic values for terminal mismatches adjacent to GC, GU, and UG base pairs are also reported.