Thermodynamic examination of 1- to 5-nt purine bulge loops in RNA and DNA constructs

Bulge loops are common features of RNA structures that are involved in the formation of RNA tertiary structures and are often sites for interactions with proteins and ions. Minimal thermodynamic data currently exist on the bulge size and sequence effects. Using thermal denaturation methods, thermodynamic properties of 1- to 5-nt adenine and guanine bulge loop constructs were examined in 10 mM MgCl₂ or 1 M KCl. The ΔG37∘ loop parameters for 1- to 5-nt purine bulge loops in RNA constructs were between 3.07 and 5.31 kcal/mol in 1 M KCl buffer. In 10 mM magnesium ions, the ΔΔG° values relative to 1 M KCl were 0.47–2.06 kcal/mol more favorable for the RNA bulge loops. The ΔG37∘ loop parameters for 1- to 5-nt purine bulge loops in DNA constructs were between 4.54 and 5.89 kcal/mol. Only 4- and 5-nt guanine constructs showed significant change in stability for the DNA constructs in magnesium ions. A linear correlation is seen between the size of the bulge loop and its stability. New prediction models are proposed for 1- to 5-nt purine bulge loops in RNA and DNA in 1 M KCl. We show that a significant stabilization is seen for small bulge loops in RNA in the presence of magnesium ions. A prediction model is also proposed for 1- to 5-nt purine bulge loop RNA constructs in 10 mM magnesium chloride.     

Thermodynamic examination of the pyrophosphate sensor helix in the thiamine pyrophosphate riboswitch

Riboswitches are functional mRNA that control gene expression. Thiamine pyrophosphate (TPP) binds to thi-box riboswitch RNA and allosterically inhibits genes that code for proteins involved in the biosynthesis and transport of thiamine. Thiamine binding to the pyrimidine sensor helix and pyrophosphate binding to the pyrophosphate sensor helix cause changes in RNA conformation that regulate gene expression. Here we examine the thermodynamic properties of the internal loop of the pyrophosphate binding domain by comparing the wild-type construct (RNA WT) with six modified 2 × 2 bulged RNA and one 2 × 2 bulged DNA. The wild-type construct retains five conserved bases of the pyrophosphate sensor domain, two of which are in the 2 × 2 bulge (C65 and G66). The RNA WT construct was among the most stable (ΔG°₃₇ = −7.7 kcal/mol) in 1 M KCl at pH 7.5. Breaking the A•G mismatch of the bulge decreases the stability of the construct ∼0.5–1 kcal/mol, but does not affect magnesium binding to the RNA WT. Guanine at position 48 is important for RNA–Mg²⁺ interactions of the TPP-binding riboswitch at pH 7.5. In the presence of 9.5 mM magnesium at pH 5.5, the bulged RNA constructs gained an average of 1.1 kcal/mol relative to 1 M salt. Formation of a single A+•C mismatch base pair contributes about 0.5 kcal/mol at pH 5.5, whereas two tandem A+•C mismatch base pairs together contribute about 2 kcal/mol.     

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.     

Non-nearest-neighbor dependence of the stability for RNA group II single-nucleotide bulge loops

Thirty-one RNA duplexes containing single-nucleotide bulge loops were optically melted in 1 M NaCl, and the thermodynamic parameters ΔH°, ΔS°, ΔG°(37), and T(M) for each sequence were determined. The bulge loops were of the group II variety, where the bulged nucleotide is identical to one of its nearest neighbors, leading to ambiguity as to the exact position of the bulge. The data were used to develop a model to predict the free energy of an RNA duplex containing a single-nucleotide bulge. The destabilization of the duplex by the bulge was primarily 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. Since there is an ambiguity of the bulge position for group II bulges, several different stem combinations are possible. The destabilization of group II bulge loops is similar to the destabilization of group I bulge loops, if the second least stable stem is used to predict the influence of the group II bulge. In-line structure probing of the group II bulge loop embedded in a hairpin indicates that the bulged nucleotide is the one positioned farther from the hairpin loop.     

X-ray structures of U2 snRNA-branchpoint duplexes containing conserved pseudouridines

A pseudouridine-modified region of the U2 small nuclear (sn)RNA anneals with the intronic branchpoint sequence and positions a bulged adenosine to serve as the nucleophile in the first chemical step of pre-mRNA splicing. We have determined three X-ray structures of RNA oligonucleotides containing the pseudouridylated U2 snRNA and the branchpoint consensus sequences. The expected adenosine branchpoint is extrahelical in a 1.65 A resolution structure containing the mammalian consensus sequence variant and in a 2.10 A resolution structure containing a shortened Saccharomyces cerevisiae consensus sequence. The adenosine adjacent to the expected branchpoint is extrahelical in a third structure, which contains the intact yeast consensus sequence at 1.57 A resolution. The hydration and base stacking interactions mediated by the U2 snRNA pseudouridines correlate with the identity of the unpaired adenosine. The expected adenosine bulge is associated with a well-stacked pseudouridine, which is linked via an ordered water molecule to a neighboring nucleotide. In contrast, the bulge of the adjacent adenosine shifts the base stacking and disrupts the water-mediated interactions of the pseudouridine. These structural differences may contribute to the ability of the pseudouridine modification to promote the bulged conformation of the branch site adenosine and to enhance catalysis by snRNAs. Furthermore, iodide binding sites are identified adjacent to the unconventional bulged adenosine, and the structure of the mammalian consensus sequence variant provides a high-resolution view of a hydrated magnesium ion bound in a similar manner to a divalent cation binding site of the group II intron.     

Conservation of helical structure contributes to functional metal ion interactions in the catalytic domain of ribonuclease P RNA

Like protein enzymes, catalytic RNAs contain conserved structure motifs important for function. A universal feature of the catalytic domain of ribonuclease P RNA is a bulged-helix motif within the P1-P4 helix junction. Here, we show that changes in bulged nucleotide identity and position within helix P4 affect both catalysis and substrate binding, while a subset of the mutations resulted only in catalytic defects. We find that the proximity of the bulge to sites of metal ion coordination in P4 is important for catalysis; moving the bulge distal to these sites and deleting it had similarly large effects, while moving it proximal to these sites had only a moderate effect on catalysis. To test whether the effects of the mutations are linked to metal ion interactions, we used terbium-dependent cleavage of the phosphate backbone to probe metal ion-binding sites in the wild-type and mutant ribozymes. We detect cleavages at specific sites within the catalytic domain, including helix P4 and J3/4, which have previously been shown to participate directly in metal ion interactions. Mutations introduced into P4 cause local changes in the terbium cleavage pattern due to alternate metal ion-binding configurations with the helix. In addition, a bulge deletion mutation results in a 100-fold decrease in the single turnover cleavage rate constant at saturating magnesium levels, and a reduced affinity for magnesium ions important for catalysis. In light of the alternate terbium cleavage pattern in P4 caused by bulge deletion, this decreased ability to utilize magnesium ions for catalysis appears to be due to localized structural changes in the ribozyme's catalytic core that weaken metal ion interactions in P4 and J3/4. The information reported here, therefore, provides evidence that the universal conservation of the P4 structure is based in part on optimization of metal ion interactions important for catalysis.     

Thermodynamic parameters based on a nearest-neighbor model for DNA sequences with a single-bulge loop

All 64 possible thermodynamic parameters for a single-bulge loop in the middle of a sequence were derived from optical melting studies. The relative stability of a single bulge depended on both the type of bulged base and its flanking base pairs. The contribution of the single bulge to helix stability ranged from 3.69 kcal/mol for a TAT bulge to -1.05 kcal/mol for an ACC bulge. Thermodynamics for 10 sequences with a GTG bulge were determined to test the applicability of the nearest-neighbor model to a single-bulge loop. Thermodynamic parameters for the GTG bulge and Watson-Crick base pairs predict, DeltaH degrees, DeltaS degrees, and T(M)(50 microM) values with average deviations of 3.0%, 4.3%, 4.7%, and 0.9 degrees C, respectively. The prediction accuracy was within the limits of what can be expected for a nearest-neighbor model. This certified that the thermodynamics for single-bulge loops can be estimated adequately using a nearest-neighbor model.     

The Influence of Monovalent Cation Size on the Stability of RNA Tertiary Structures

Many RNA tertiary structures are stable in the presence of monovalent ions alone. To evaluate the degree to which ions at or near the surfaces of such RNAs contribute to stability, the salt-dependent stability of a variety of RNA structures was measured with each of the five group I cations. The stability of hairpin secondary structures and a pseudoknot tertiary structure are insensitive to the ion identity, but the tertiary structures of two other RNAs, an adenine riboswitch and a kissing loop complex, become more stable by 2-3 kcal/mol as ion size decreases. This "default" trend is attributed to the ability of smaller ions to approach the RNA surface more closely. The degree of cation accumulation around the kissing loop complex was also inversely proportional to ion radius, perhaps because of the presence of sterically restricted pockets that can be accessed only by smaller ions. An RNA containing the tetraloop-receptor motif shows a strong (up to ∼ 3 kcal/mol) preference for Na⁺ or K⁺ over other group I ions, consistent with the chelation of K⁺ by this motif in some crystal structures. This RNA reverts to the default dependence on ion size when a base forming part of the chelation site is mutated. Lastly, an RNA aptamer for cobinamide, which was originally selected in the presence of high concentrations of LiCl, binds ligand more strongly in the presence of Li⁺ than other monovalent ions.On the basis of these trends in RNA stability with group I ion size, it is argued that two features of RNA tertiary structures may promote strong interactions with ions at or near the RNA surface: negative charge densities that are higher than that in secondary structures, and the occasional presence of chelation sites, which are electronegative pockets that selectively bind ions of an optimum size.     

A conserved RNA pseudoknot in a putative molecular switch domain of the 3'-untranslated region of coronaviruses is only marginally stable

The 3'-untranslated region (UTR) of the group 2 coronavirus mouse hepatitis virus (MHV) genome contains a predicted bulged stem-loop (designated P0ab), a conserved cis-acting pseudoknot (PK), and a more distal stem-loop (designated P2). Base-pairing to create the pseudoknot-forming stem (P1(pk)) is mutually exclusive with formation of stem P0a at the base of the bulged stem-loop; as a result, the two structures cannot be present simultaneously. Herein, we use thermodynamic methods to evaluate the ability of individual subdomains of the 3' UTR to adopt a pseudoknotted conformation. We find that an RNA capable of forming only the predicted PK (58 nt; 3' nucleotides 241-185) adopts the P2 stem-loop with little evidence for P1(pk) pairing in 0.1 M KCl and the absence of Mg(2+); as Mg(2+) or 1 M KCl is added, a new thermal unfolding transition is induced and assignable to P1(pk) pairing. The P1(pk) helix is only marginally stable, ΔG(25) ≈ 1.2 ± 0.3 kcal/mol (5.0 mM Mg(2+), 100 mM K(+)), and unfolded at 37°C. Similar findings characterize an RNA 5' extended through the P0b helix only (89 nt; 294-185). In contrast, an RNA capable of forming either the P0a helix or the pseudoknot (97 nt; 301-185) forms no P1(pk) helix. Thermal unfolding simulations are fully consistent with these experimental findings. These data reveal that the PK forms weakly and only when the competing double-hairpin structure cannot form; in the UTR RNA, the double hairpin is the predominant conformer under all solution conditions.     

Crystal structure of the leadzyme at 1.8 A resolution: metal ion binding and the implications for catalytic mechanism and allo site ion regulation

The leadzyme is a small ribozyme, derived from in vitro selection, which catalyzes site specific, Pb(2+)-dependent RNA cleavage. Pb(2+) is required for activity; Mg(2+) inhibits activity, while many divalent and trivalent ions enhance it. The leadzyme structure consists of an RNA duplex interrupted by a trinucleotide bulge. Here, crystal structures determined to 1.8 A resolution, both with Mg(2+) as the sole divalent counterion and with Mg(2+) and Sr(2+) (which mimics Pb(2+) with respect to binding but not catalysis), reveal the metal ion interactions with both the ground state and precatalytic conformations of the leadzyme. Mg(H(2)O)(6)(2+) ions bridge complementary strands of the duplex at multiple locations by binding tandem purines of one RNA strand in the major groove. At one site, Mg(H(2)O)(6)(2+) ligates the phosphodiester backbone of the trinucleotide bulge in the ground state conformation, but not in the precatalytic conformation, suggesting (a) Mg(2+) may inhibit leadzyme activity by stabilizing the ground state and (b) metal ions which displace Mg(2+) from this site may activate the leadzyme. Binding of Sr(2+) to the presumed catalytic Pb(2+) site in the precatalytic leadzyme induces local structural changes in a manner that would facilitate alignment of the catalytic ribose 2'-hydroxyl with the scissile bond for cleavage. These data support a model wherein binding of a catalytic ion to a precatalytic conformation of the leadzyme, in conjunction with the flexibility of the trinucleotide bulge, may facilitate structural rearrangements around the scissle phosphodiester bond favoring configurations that allow bond cleavage.     

The Osmolyte TMAO Stabilizes Native RNA Tertiary Structures in the Absence of Mg: Evidence for a Large Barrier to Folding from Phosphate Dehydration

The stabilization of RNA tertiary structures by ions is well known, but the neutral osmolyte trimethylamine oxide (TMAO) can also effectively stabilize RNA tertiary structure. To begin to understand the physical basis for the effects of TMAO on RNA, we have quantitated the TMAO-induced stabilization of five RNAs with known structures. So-called m values, the increment in unfolding free energy per molal of osmolyte at constant KCl activity, are ∼ 0 for a hairpin secondary structure and between 0.70 and 1.85 kcal mol^− 1m^− 1 for four RNA tertiary structures (30-86 nt). Further analysis of two RNAs by small-angle X-ray scattering and hydroxyl radical probing shows that TMAO reduces the radius of gyration of the unfolded ensemble to the same endpoint as seen in titration with Mg²⁺ and that the structures stabilized by TMAO and Mg²⁺ are indistinguishable. Remarkably, TMAO induces the native conformation of a Mg²⁺ ion chelation site formed in part by a buried phosphate, even though Mg²⁺ is absent. TMAO interacts weakly, if at all, with KCl, ruling out the possibility that TMAO stabilizes RNA indirectly by increasing salt activity. TMAO is, however, strongly excluded from the vicinity of dimethylphosphate (unfavorable interaction free energy, + 211 cal mol^− 1m^− 1 for the potassium salt), an ion that mimics the RNA backbone phosphate. We suggest that formation of RNA tertiary structure is accompanied by substantial phosphate dehydration (loss of 66-173 water molecules in the RNA structures studied) and that TMAO works principally by reducing the energetic penalty associated with this dehydration. The strong parallels we find between the effects of TMAO and Mg²⁺ suggest that RNA sequence is more important than specific ion interactions in specifying the native structure.     

X-ray crystallographic observation of "in-line" and "adjacent" conformations in a bulged self-cleaving RNA/DNA hybrid

The RNA strand in an RNA/DNA duplex with unpaired ribonucleotides can undergo self-cleavage at bulge sites in the presence of a variety of divalent metal ions (Hüsken et al., Biochemistry, 1996, 35:16591-16600). Transesterification proceeds via an in-line mechanism, with the 2'-OH of the bulged nucleotide attacking the 3'-adjacent phosphate group. The site-specificity of the reaction is most likely a consequence of the greater local conformational freedom of the RNA backbone in the bulge region. A standard A-form backbone geometry prohibits formation of an in-line arrangement between 2'-oxygen and phosphate. However, the backbone in the region of an unpaired nucleotide appears to be conducive to an in-line approach. Therefore, the bulge-mediated phosphoryl transfer reaction represents one of the simplest RNA self-cleavage systems. Here we focus on the conformational features of the RNA that underlie site-specific cleavage. The structures of an RNA/DNA duplex with single ribo-adenosyl bulges were analyzed in two crystal forms, permitting observation of 10 individual conformations of the RNA bulge moiety. The bulge geometries cover a range of relative arrangements between the 2'-oxygen of the bulged nucleotide and the P-O5' bond (including adjacent and near in-line) and give a detailed picture of the conformational changes necessary to line up the 2'-OH nucleophile and scissile bond. Although metal ions are of crucial importance in the catalysis of analogous cleavage reactions by ribozymes, it is clear that local strain or conformational flexibility in the RNA also affect cleavage selectivity and rate (Soukup & Breaker, RNA, 1999, 5:1308-1325). The geometries of the RNA bulges frozen out in the crystals provide snapshots along the reaction pathway prior to the transition state of the phosphoryl transfer reaction.     

Structural probing and damage selection of citrulline- and arginine-specific RNA aptamers identify base positions required for binding.

In a recent study, an RNA aptamer for the specific recognition of the amino acid L-arginine was evolved from an in vitro selected L-citrulline binding parent sequence [M. Famulok (1994) J. Am. Chem. Soc. 116, 1698-1706]. We have now carried out a structural analysis of these aptamers by using chemical modification experiments. Footprinting experiments and a damage selection approach were performed to identify those positions protected from modification in the presence of the amino acids and modifications that interfere with the binding of the ligand. It is shown that of the two bulged regions present in both aptamers one can be modified without loss of binding activity whereas in the other bulge nearly every position is shown to be involved in the recognition of the ligands. This might be indicative for non-canonical base pairing to occur within the non-Watson-Crick paired regions which might be stabilized by the complexed amino acid. Binding to the cognate amino acid significantly enhances the conformational stability of the RNA. We also tested the sensitivity of both aptamers towards lead (II) ion induced cleavage and identified a hypersensitive cleavage site within the invariant bulged region. Lead cleavage is inhibited by the complexed amino acid, indicating a conformational change of the aptamer upon ligand binding. NMR titration data obtained with both aptamers and their cognate ligands confirm the proposed conformational changes and indicate the formation of a 1:1 complex of RNA:amino acid.     

Non-nearest-neighbor dependence of stability for group III RNA single nucleotide bulge loops

Thirty-five RNA duplexes containing single nucleotide bulge loops were optically melted and the thermodynamic parameters for each duplex determined. The bulge loops were of the group III variety, where the bulged nucleotide is either a AG/U or CU/G, leading to ambiguity to the exact position and identity of the bulge. All possible group III bulge loops with Watson–Crick nearest-neighbors were examined. The data were used to develop a model to predict the free energy of an RNA duplex containing a group III single nucleotide bulge loop. The destabilization of the duplex by the group III bulge could be modeled so that the bulge nucleotide leads to the formation of the Watson–Crick base pair rather than the wobble base pair. The destabilization of an RNA duplex caused by the insertion of a group III bulge is primarily dependent upon non-nearest-neighbor interactions and was shown to be dependent upon the stability of second least stable stem of the duplex. In-line structure probing of group III bulge loops embedded in a hairpin indicated that the bulged nucleotide is the one positioned further from the hairpin loop irrespective of whether the resulting stem formed a Watson–Crick or wobble base pair. Fourteen RNA hairpins containing group III bulge loops, either 3′ or 5′ of the hairpin loop, were optically melted and the thermodynamic parameters determined. The model developed to predict the influence of group III bulge loops on the stability of duplex formation was extended to predict the influence of bulge loops on hairpin stability.     

RNA recognition by Tat-derived peptides: interaction in the major groove?

Replication of human immunodeficiency virus requires binding of the viral Tat protein to its RNA target sequence TAR; peptides derived from Tat bind to a TAR "contact site" spanning 5 bp and a trinucleotide pyrimidine bulge. We find that high affinity binding requires a U residue in the bulge loop and 2 specific adjacent base pairs. Other bulged RNAs bind in a lower affinity nonspecific manner; sequence-specific binding requires a bulge loop of more than 1 nucleotide. Reaction with diethyl pyrocarbonate indicates that one effect of the bulge is to make the otherwise deep and narrow RNA major groove accessible. A model consistent with these data involves local distortion of A-form geometry at the bulge, which bends the helix and permits protein binding and interactive access in the RNA major groove.     

A Test and Refinement of Folding Free Energy Nearest Neighbor Parameters for RNA Including N6-Methyladenosine

RNA folding free energy change parameters are widely used to predict RNA secondary structure and to design RNA sequences. These parameters include terms for the folding free energies of helices and loops. Although the full set of parameters has only been traditionally available for the four common bases and backbone, it is well known that covalent modifications of nucleotides are widespread in natural RNAs. Covalent modifications are also widely used in engineered sequences. We recently derived a full set of nearest neighbor terms for RNA that includes N⁶-methyladenosine (m⁶A). In this work, we test the model using 98 optical melting experiments, matching duplexes with or without N⁶-methylation of A. Most experiments place RRACH, the consensus site of N⁶-methylation, in a variety of contexts, including helices, bulge loops, internal loops, dangling ends, and terminal mismatches. For matched sets of experiments that include either A or m⁶A in the same context, we find that the parameters for m⁶A are as accurate as those for A. Across all experiments, the root mean squared deviation between estimated and experimental free energy changes is 0.67 kcal/mol. We used the new experimental data to refine the set of nearest neighbor parameter terms for m⁶A. These parameters enable prediction of RNA secondary structures including m⁶A, which can be used to model how N⁶-methylation of A affects RNA structure.     

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.     

Thermodynamic characterization of the Saccharomyces cerevisiae telomerase RNA pseudoknot domain in vitro

Recent structural and functional characterization of the pseudoknot in the Saccharomyces cerevisiae telomerase RNA (TLC1) has demonstrated that tertiary structure is present, similar to that previously described for the human and Kluyveromyces lactis telomerase RNAs. In order to biophysically characterize the identified pseudoknot secondary and tertiary structures, UV-monitored thermal denaturation experiments, nuclear magnetic resonance spectroscopy, and native gel electrophoresis were used to investigate various potential conformations in the pseudoknot domain in vitro, in the absence of the telomerase protein. Here, we demonstrate that alternative secondary structures are not mutually exclusive in the S. cerevisiae telomerase RNA, tertiary structure contributes 1.5 kcal mol(-1) to the stability of the pseudoknot (≈ half the stability observed for the human telomerase pseudoknot), and identify additional base pairs in the 3' pseudoknot stem near the helical junction. In addition, sequence conservation in an adjacent overlapping hairpin appears to prevent dimerization and alternative conformations in the context of the entire pseudoknot-containing region. Thus, this work provides a detailed in vitro characterization of the thermodynamic features of the S. cerevisiae TLC1 pseudoknot region for comparison with other telomerase RNA pseudoknots.