Electrophoretic mobility is a reporter of hairpin structure in single-stranded DNA oligomers

The electrophoretic mobilities of 24 single-stranded DNA oligomers, each containing 26 nucleotide residues, have been measured in polyacrylamide gels and in free solution. The mobilities observed at 20 degrees C differed by approximately 20% in polyacrylamide gels and by approximately 10% in free solution, even though the oligomers contained the same number of bases. Increasing the temperature or adding urea to the solution equalized the mobilities of the oligomers, suggesting that the variable mobilities observed at 20 degrees C are due to the formation of stable secondary structures, most likely hairpins. Thermal melting profiles were measured for eight oligomers in 40 mM Tris acetate buffer. The observed melting temperatures of most oligomers correlated roughly with the mobilities observed at 20 degrees C; however, one oligomer was much more stable than the others. The melting temperatures of four of the oligomers were close to the values predicted by DINAMelt [Markham, N. R., and Zuker, M. (2005) Nucleic Acids Res. 33, W577-W581]; melting temperatures of the other oligomers differed significantly from the predicted values. Thermal melting profiles were also measured for two oligomers as a function of the Tris acetate buffer concentration. The salt concentration dependence of the melting temperatures suggests that 0.15 Tris+ ion per phosphate is released upon denaturation. Because the apparent number of Tris+ ions released is greater than that observed by others for the release of Na+ ions from similar hairpins, the results suggest that DNA hairpins (and, presumably, duplexes) bind more Tris+ ions than Na+ ions in solution.     

Thermal stability of RNA hairpins containing a four-membered loop and a bulge nucleotide

Fourteen RNA hairpins containing a four-membered loop and a bulge nucleotide were synthesized and their thermal stabilities determined. The combined contribution of a four-membered loop and bulge A to the free energy of a hairpin is calculated to be 9.3 kcal/mol at 37 degrees C and successfully predicts the stability of an independent RNA hairpin. The introduction of a bulge nucleotide to the helical stem of an RNA hairpin destabilizes the molecule in a sequence-dependent manner. The individual thermodynamic contributions of a four-membered loop and bulge A, G, and U residues to the stability of an RNA hairpin loop are presented.     

Characterization of RNA hairpin loop stability.

Fifteen RNA hairpins that share the same stem sequence and have homopolymer loops of A, C and U residues which vary in length from three to nine nucleotides were synthesized and their thermal stabilities determined. Tm varies as a function of loop size but is almost independent of loop composition. Loops of four or five nucleotides are found to be the most stable loop size. This is consistent with the observation that four-membered loops are the most prevalent loop size in 16S-like RNAs. The contribution of each loop to hairpin stability was calculated by subtracting the known contribution of the helical stem. These data should be useful for predicting the stability of other hairpins.     

Analysis of melting transitions of the DNA hairpins formed from the oligomer sequences d[GGATAC(X)4GTATCC] (X = A, T, G, C)

Optical melting transitions of the short DNA hairpins formed from the self-complementary DNA oligomers d[GGATACX4GTATCC] where X = A, T, G, or C measured in 100 mM NaCl are presented. A significant dependence of the melting transitions on loop sequence is observed and transition temperatures, tm, of the hairpins vary from 58.3 degrees C for the T4 loop hairpin to 55.3 degrees C for the A4 loop. A nearest-neighbor sequence-dependent theoretical algorithm for calculating melting curves of DNA hairpins is presented and employed to analyze the experimental melting transitions. Experimental melting curves were fit by adjustment of a single theoretical parameter, Fend(n), the weighting function for a hairpin loop comprised of n single-strand bases. Empirically determined values of Fend(n) provide an evaluation of the free-energy of hairpin loop formation and stability. Effects of heterogeneous nearest-neighbor sequence interactions in the duplex stem on hairpin loop formation were investigated by evaluating Fend(n) in individual fitting procedures using two of the published sets of nearest-neighbor stacking interactions in DNA evaluated in 100 mM NaCl and given by Wartell and Benight, 1985. In all cases, evaluated values of Fend(n) were obtained that provided exact theoretical predictions of the experimental transitions. Results of the evaluations indicate: (1) Evaluated free-energies of hairpin loop formation are only slightly dependent on loop sequences examined. At the transition temperature, Tm, the free-energy of forming a loop of four bases is approximately equal for T4, G4, or C4 loops and varies from 3.9 to 4.8 kcal/mole depending on the set of nearest-neighbor interactions employed in the evaluations. This result suggests, in light of the observed differences in stability between the T4, G4, and C4 loop hairpins, that sequence-dependent interactions between base residues of the loop are most likely not the source of the enhanced stability of a T4 loop.(ABSTRACT TRUNCATED AT 400 WORDS)     

Perturbation of DNA hairpins containing the EcoRI recognition site by hairpin loops of varying size and composition: physical (NMR and UV) and enzymatic (EcoRI) studies.

We have investigated loop-induced structural perturbation of the stem structure in hairpins d(GAATTCXnGAATTC) (X = A, T and n = 3, 4, 5 and 6) that contain an EcoRI restriction site in close proximity to the hairpin loop. Oligonucleotides containing either a T3 or a A3 loop were not hydrolyzed by the restriction enzyme and also showed only weak binding to EcoRI in the absence of the cofactor Mg2+. In contrast, hairpins with larger loops are hydrolyzed by the enzyme at the scission site next to the loop although the substrate with a A4 loop is significantly more resistant than the oligonucleotide containing a T4 loop. The hairpin structures with 3 loop residues were found to be thermally most stable while larger hairpin loops resulted in structures with lower melting temperatures. The T-loop hairpins are thermally more stable than the hairpins containing the same number of A residues in the loop. As judged from proton NMR spectroscopy and the thermodynamic data, the base pair closest to the hairpin loop did form in all cases studied. The hairpin loops did, however, affect the conformation of the stem structure of the hairpins. From 31P and 1H NMR spectroscopy we conclude that the perturbation of the stem structure is stronger for smaller hairpin loops and that the extent of the perturbation is limited to 2-3 base pairs for hairpins with T3 or A4 loops. Our results demonstrate that hairpin loops modulate the conformation of the stem residues close to the loop and that this in turn reduces the substrate activity for DNA sequence specific proteins.     

Interactions of hairpin oligo-2'-O-methylribonucleotides containing methylphosphonate linkages with HIV TAR RNA

Methylphosphonate-modified oligo-2'-O-methylribonucleotides 15-20 nucleotides (nt) in length were prepared whose sequences are complementary to the 5' and 3' sides of the upper hairpin of HIV trans-acting response element (TAR) RNA. These anti-TAR oligonucleotides (ODNs) form stable hairpins whose melting temperatures (Tm) range from 55 degrees C to 80 degrees C. Despite their rather high thermal stabilities, the hairpin oligo-2'-O-methylribonucleotides formed very stable complexes with TAR RNA, with dissociation constants in the nanomolar concentration range at 37 degrees C. The affinities of the hairpin oligomers for TAR RNA were influenced by the positions of the methylphosphonate linkages. The binding affinity was reduced approximately 17-fold by the presence of two methylphosphonate linkages in the TAR loop complementary region (TLCR) of the oligomer, whereas methylphosphonate linkages outside this region increased binding affinity approximately 3-fold. The configurations of the methylphosphonate linkages in the TLCR also affected binding affinity, with the RpRp isomer showing significantly higher binding than the SpSp isomer. In addition to serving as probes of the interactions between the oligomer and TAR RNA, the presence of the methylphosphonate linkages in combination with the hairpin structure increases the resistance of these oligomers to degradation by exonucleases found in mammalian serum. The combination of high binding affinity and nuclease resistance of the hairpin ODNs containing methylphosphonate linkages suggests their potential utility as antisense compounds.     

A test of the model to predict unusually stable RNA hairpin loop stability

To investigate the accuracy of a model [Giese et al., 1998, Biochemistry37:1094-1100 and Mathews et al., 1999, JMol Biol 288:911-940] that predicts the stability of RNA hairpin loops, optical melting studies were conducted on sets of hairpins previously determined to have unusually stable thermodynamic parameters. Included were the tetraloops GNRA and UNCG (where N is any nucleotide and R is a purine), hexaloops with UU first mismatches, and the hairpin loop of the iron responsive element, CAGUGC. The experimental values for the GNRA loops are in excellent agreement (deltaG degrees 37 within 0.2 kcal/mol and melting temperature (TM) within 4 degrees C) with the values predicted by the model. When the UNCG hairpin loops are treated as tetraloops, and a bonus of 0.8 kcal/mol included in the prediction to account for the extra stable first mismatch (UG), the measured and predicted values are also in good agreement (deltaG degrees 37 within 0.7 kcal/mol and TM within 3 degrees C). Six hairpins with unusually stable UU first mismatches also gave good agreement with the predictions (deltaG degrees 37 within 0.5 kcal/mol and TM within 8 degrees C), except for hairpins closed by wobble base pairs. For these hairpins, exclusion of the additional stabilization term for UU first mismatches improved the prediction (AG degrees 37 within 0.1 kcal/mol and TM within 3 degrees C). Hairpins with the iron-responsive element loop were not predicted well by the model, as measured deltaG degrees 37 values were at least 1 kcal/mol greater than predicted.     

Effects of magnesium ions on the stabilization of RNA oligomers of defined structures

Optical melting was used to determine the stabilities of 11 small RNA oligomers of defined secondary structure as a function of magnesium ion concentration. The oligomers included helices composed of Watson-Crick base pairs, GA tandem base pairs, GU tandem base pairs, and loop E motifs (both eubacterial and eukaryotic). The effect of magnesium ion concentration on stability was interpreted in terms of two simple models. The first assumes an uptake of metal ion upon duplex formation. The second assumes nonspecific electrostatic attraction of metal ions to the RNA oligomer. For all oligomers, except the eubacterial loop E, the data could best be interpreted as nonspecific binding of metal ions to the RNAs. The effect of magnesium ions on the stability of the eubacterial loop E was distinct from that seen with the other oligomers in two ways. First, the extent of stabilization by magnesium ions (as measured by either change in melting temperature or free energy) was three times greater than that observed for the other helical oligomers. Second, the presence of magnesium ions produces a doubling of the enthalpy for the melting transition. These results indicate that magnesium ion stabilizes the eubacterial loop E sequence by chelating the RNA specifically. Further, these results on a rather small system shed light on the large enthalpy changes observed upon thermal unfolding of large RNAs like group I introns. It is suggested that parts of those large enthalpy changes observed in the folding of RNAs may be assigned to variations in the hydration states and types of coordinating atoms in some specifically bound magnesium ions and to an increase in the observed cooperativity of the folding transition due to the binding of those magnesium ions coupling the two stems together. Brownian dynamic simulations, carried out to visualize the metal ion binding sites, reveal rather delocalized ionic densities in all oligomers, except for the eubacterial loop E, in which precisely located ion densities were previously calculated.     

Melting studies of short DNA hairpins: Influence of loop sequence and adjoining base pair identity on hairpin thermodynamic stability

Spectroscopic and calorimetric melting studies of 28 DNA hairpins were performed. These hairpins form by intramolecular folding of 16 base self‐complementary DNA oligomer sequences. Sequence design dictated that the hairpin structures have a six base pair duplex linked by a four base loop and that the first five base pairs in the stem are the same in every molecule. Only loop sequence and identity of the duplex base pair closing the loop vary for the set of hairpins. For these DNA samples, melting studies were carried out to investigate effects of the variables on hairpin stability. Stability of the 28 oligomers was ascertained from their temperature‐induced melting transitions in buffered 115 mM Na⁺ solvent, monitored by ultraviolet absorbance and differential scanning calorimetry (DSC). Experiments revealed the melting temperatures of these molecules range from 32.4 to 60.5°C and are concentration independent over strand concentrations of 0.5 to 260 μM; thus, as expected for hairpins, the melting transitions are apparently unimolecular. Model independent thermodynamic transition parameters, ΔH_cal, ΔS_cal, and ΔG_cal, were determined from DSC measurements. Model dependent transition parameters, ΔH_vH, ΔS_vH, and ΔG_vH were estimated from a van't Hoff (two‐state) analysis of optical melting transitions. Results of these studies reveal a significant sequence dependence to DNA hairpin stability. Thermodynamic parameters evaluated by either procedure reveal the transition enthalpy, ΔH_cal (ΔH_vH) can differ by as much as 20 kcal/mol depending on sequence. Similarly, values of the transition entropy ΔS_cal (ΔS_vH) can differ by as much as 60 cal/Kmol (eu) for different molecules. Differences in free energies ΔG_cal (ΔG_vH) are as large as 4 kcal/mol for hairpins with different sequences. Comparisons between the model independent calorimetric values and the thermodynamic parameters evaluated assuming a two‐state model reveal that 10 of the 28 hairpins display non‐two‐state melting behavior. The database of sequence‐dependent melting free energies obtained for the hairpins was employed to extract a set of n‐n (nearest‐neighbor) sequence dependent loop parameters that were able to reproduce the input data within error (with only two exceptions). Surprisingly, this suggests that the thermodynamic stability of the DNA hairpins can in large part be reasonably represented in terms of sums of appropriate nearest‐neighbor loop sequence parameters. © 1999 John Wiley & Sons, Inc. Biopoly 50: 425–442, 1999     

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.     

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.     

Interaction of DNA hairpin loops and a complementary strand by a triplet of base pairs

Hypothesis of non-enzymatic recognition of primordial tRNA and mRNA precursors is experimentally approached. DNA hairpins containing a different number of deoxyguanosine residues in the loop are analyzed for their binding ability to a chemically fixed single-strand of oligo(dC). In presence of small Mg2+ concentration a hairpin with five dG residues in the loop is adsorbed to affinity matrix. Comparison of elution temperatures of hairpin oligonucleotides with those of single-stranded oligoguanylic acids with length of the loop indicates, that smallest loop able to bind forms a triplet of base pairs.     

Oligodeoxynucleotide folding in solution: loop size and stability of B-hairpins

The secondary structures of the synthetic DNA fragments d(CGCGCGTTTTTCGCGCG) (T5), d(CGCGCGAAAAACGCGCG) (A5), d(CGCGCGTACGCGCG) (TA), and d(CGCGCGATCGCGCG) (AT) were investigated in a combined electrophoretic and spectroscopic study. All the oligomers exist, at low temperature and over a wide range of ionic strength (0.5-100 mM salt) and of nucleotide concentration [0.1-2.0 mM (phosphate)], as a mixture of two slowly interconverting species, identified as the dimeric duplex and the monomeric hairpin structure. The thermodynamic parameters for hairpin denaturation of T5, A5, TA, and AT and for duplex denaturation of d(CGCGCG) show that (a) the hairpins are more stable than the reference hexamer duplex at all accessible nucleotide concentrations; (b) the loop contributes favorably to the enthalpy change of hairpin denaturation in the four DNA fragments; (c) the base composition of the loop (A vs T) and the size of the loop (A5/T5 vs TA/AT) do not appreciably influence the enthalpic contents of the hairpins; (d) hairpins TA and AT, with two AT bases intervening in the CG self-complementary part of the molecule, exhibit a markedly higher thermal stability than hairpins T5 and A5, which is entropic in origin. These findings are consistent with the presence of two-residue loops in the tetradecamers TA and AT.     

On loop folding in nucleic acid hairpin-type structures

In a series of studies, combining NMR, optical melting and T-jump experiments, it was found that DNA hairpins display a maximum stability when the loop part of the molecule comprises four or five nucleotide residues. This is in contrast with the current notion based on RNA hairpin studies, from which it had been established that a maximum hairpin stability is obtained for six or seven residues in the loop. Here we present a structural model to rationalize these observations. This model is based on the notion that to a major extent base stacking interactions determine the stability of nucleic acid conformations. The model predicts that loop folding in RNA is characterized by an extension of the base stacking at the 5'-side of the double helix by five or six bases; the remaining gap can then easily be closed by two nucleotides. Conversely, loop folding in DNA is characterized by extending base stacking at the 3'-side of the double helical stem by two or three residues; again bridging of the remaining gap can then be achieved by one or two nucleotides. As an example of loop folding in RNA the anticodon loop of yeast tRNAPhe is discussed. For the DNA hairpin formed by d(ATCCTAT4TAGGAT) it is shown that the loop structure obtained from molecular mechanics calculations obeys the above worded loop folding principles.     

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.     

A semiflexible polymer model applied to loop formation in DNA hairpins

A statistical mechanical "zipper" model is applied to describe the equilibrium melting of short DNA hairpins with poly(dT) loops ranging from 4 to 12 bases in the loop. The free energy of loop formation is expressed in terms of the persistence length of the chain. This method provides a new measurement of the persistence length of single-stranded DNA, which is found to be approximately 1.4 nm for poly(dT) strands in 100 mM NaCl. The free energy of the hairpin relative to the random coil state is found to scale with the loop size with an apparent exponent of > or = 7, much larger than the exponent of approximately 1.5-1.8 expected from considerations of loop entropy alone. This result indicates a strong dependence of the excess stability of the hairpins, from stacking interactions of the bases within the loop, on the size of the loop. We interpret this excess stability as arising from favorable hydrophobic interactions among the bases in tight loops and which diminish as the loops get larger. Free energy profiles along a generalized reaction coordinate are calculated from the equilibrium zipper model. The transition state for hairpin formation is identified as an ensemble of looped conformations with one basepair closing the loop, and with a lower enthalpy than the random coil state. The equilibrium model predicts apparent activation energy of approximately -11 kcal/mol for the hairpin closing step, in remarkable agreement with the value obtained from kinetics measurements.     

Thermodynamic stability of the 5' dangling-ended DNA hairpins formed from sequences 5'-(XY)2GGATAC(T)4GTATCC-3', where X, Y = A, T, G, C

Expressions for the partition function Q (T) of DNA hairpins are presented. Calculations of Q (T), in conjunction with our previously reported numerically exact algorithm [T. M. Paner, M. Amaratunga, M. J. Doktycz, and A. S. Benight (1990) Biopolymers, 29, 1715-1734], yield a numerical method to evaluate the temperature dependence of the transition enthalpy, entropy, and free energy of a DNA hairpin directly from its optical melting curve. No prior assumptions that the short hairpins melt in a two-state manner are required. This method is then applied in a systematic manner to investigate the stability of the six basepair duplex stem 5'-GGATAC-3' having four-base dangling single-strand ends with the sequences (XY)2, where X, Y = A, T, G, C, on the 5' end and a T4 loop on the 3' end. Results show that all dangling ends of the sample set stabilize the hairpin against melting. Increases in transition temperatures as great as 4.0 degrees C above the blunt-ended control hairpin were observed. The hierarchy of the hairpin transition temperatures is dictated by the identity of the first base of the dangling end adjoining the duplex in the order: purine greater than T greater than C. Calculated melting curves of every hairpin were fit to experimental curves by adjustment of a single parameter in the numerically exact theoretical algorithm. Exact fits were obtained in all cases. Experimental melting curves were also calculated assuming a two-state melting process. Equally accurate fits of all dangling-ended hairpin melting curves were obtained with the two-state model calculation. This was not the case for the melting curve of the blunt-ended hairpin, indicating the presence of a four-base dangling-end drives hairpin melting to a two-state process. Q (T) was calculated as a function of temperature for each hairpin using the theoretical parameters that provided calculated curves in exact agreement with the experimentally obtained optical melting curves. From Q (T), the temperature dependence of the transition enthalpy delta H, entropy delta S, and free energy delta G were calculated for every hairpin providing a quantitative assessment of the effects of dangling ends on hairpin thermodynamics. Comparisons of our results are made with those of the Breslauer group [M. Senior, R. A. Jones, and K. J. Breslauer (1988) Biochemistry 27, 3879-3885] on the T2 5' dangling-ended d(GC)3 duplexes.(ABSTRACT TRUNCATED AT 400 WORDS)     

RNA pseudoknots. Stability and loop size requirements.

The effects of ionic conditions, loop size and loop sequence on the formation of pseudoknots by RNA oligonucleotides have been investigated using biochemical and biophysical methods. An oligonucleotide with the sequence 5' GCGAUUUCUGACCGCUUUUUUGUCAG 3' and oligonucleotides with variations in the sequences of the two loop regions, denoted by bold face type, were studied. Each sequence with the potential to form a pseudoknot can also form two stable hairpins. The pseudoknot structure is stabilized relative to the hairpins by addition of Mg2+. Even in the presence of Mg2+, the pseudoknots formed by the sequences investigated are only marginally more stable (1.5 to 2 kcal mol-1 in free energy at 37 degrees C) than either of the constituent hairpins. The pseudoknot structure is the stable conformation in the presence of Mg2+ when the first loop region is at least three nucleotides and the second is at least four nucleotides. Further deletion of nucleotides from the loop regions stabilizes possible hairpin structures relative to the pseudoknot and equilibria among secondary and tertiary structures result.     

Hairpin formation in synthetic oligonucleotides

The structure and dynamics of the homologous series of the (partly) self-complementary DNA fragments, d(ATCCTATnTAGGAT) n = 0-7, were investigated in a combined NMR, T-jump, and optical melting study. It is shown that all compounds in the series may adopt hairpin like conformations, even for n less than 3, although for these smaller n values this only occurs in significant amounts at relatively low concentrations (approximately 10 microM). The enthalpy change accompanying the hairpin-coil melting transition turns out to depend on the number of intervening thymidines, n. It is shown that this does not mean that the enthalpy of loop closure is significantly different from zero, but that loop formation stabilizes the base pair closing the loop. The results indicate that for DNA the optimal loop consists of four or five residues. The observation that hairpins are formed for n less than 3 and that the stability of DNA hairpins is at its maximum for loop lengths of four to five residues is at variance with earlier findings for RNA. In the latter case the optimal loop size consists of six to seven residues, whereas for less than three intervening residues only, dimer, and no hairpin formation, was observed [17, 20]. A direct comparison with RNA behaviour was made by studying r(AUCCUAUT4UAGGAU), T = ribothymidine. In contrast to its DNA analogue, d(ATCCTAT4TAGGAT), the ribo-fragment forms a dimer as well as a hairpin at low (10 microM) concentrations. With the thermodynamic melting parameters deduced from the present experiments the differences between DNA and RNA melting behaviour can be explained.