Experimental and theoretical studies of the effects of deoxyribose substitutions on the stability of the UUCG tetraloop

Measuring thermodynamic preferences to form non-native conformations in nucleic acids using ultraviolet melting

Thermodynamic preferences to form non-native conformations are crucial for understanding how nucleic acids fold and function. However, they are difficult to measure experimentally because this requires accurately determining the population of minor low-abundance (<10%) conformations in a sea of other conformations. Here, we show that melting experiments enable facile measurements of thermodynamic preferences to adopt nonnative conformations in DNA and RNA. The key to this "delta-melt" approach is to use chemical modifications to render specific minor non-native conformations the major state. The validity and robustness of delta-melt is established for four different non-native conformations under various physiological conditions and sequence contexts through independent measurements of thermodynamic preferences using NMR. Delta-melt is faster relative to NMR, simple, and cost-effective and enables thermodynamic preferences to be measured for exceptionally low-populated conformations. Using delta-melt, we obtained rare insights into conformational cooperativity, obtaining evidence for significant cooperativity (1.0 to 2.5 kcal/mol) when simultaneously forming two adjacent Hoogsteen base pairs. We also measured the thermodynamic preferences to form G-C⁺ and A-T Hoogsteen and A-T base open states for nearly all 16 trinucleotide sequence contexts and found distinct sequence-specific variations on the order of 2 to 3 kcal/mol. This rich landscape of sequence-specific non-native minor conformations in the DNA double helix may help shape the sequence specificity of DNA biochemistry. Thus, melting experiments can now be used to access thermodynamic information regarding regions of the free energy landscape of biomolecules beyond the native folded and unfolded conformations.

RNA Structural Dynamics As Captured by Molecular Simulations: A Comprehensive Overview

With both catalytic and genetic functions, ribonucleic acid (RNA) is perhaps the most pluripotent chemical species in molecular biology, and its functions are intimately linked to its structure and dynamics. Computer simulations, and in particular atomistic molecular dynamics (MD), allow structural dynamics of biomolecular systems to be investigated with unprecedented temporal and spatial resolution. We here provide a comprehensive overview of the fast-developing field of MD simulations of RNA molecules. We begin with an in-depth, evaluatory coverage of the most fundamental methodological challenges that set the basis for the future development of the field, in particular, the current developments and inherent physical limitations of the atomistic force fields and the recent advances in a broad spectrum of enhanced sampling methods. We also survey the closely related field of coarse-grained modeling of RNA systems. After dealing with the methodological aspects, we provide an exhaustive overview of the available RNA simulation literature, ranging from studies of the smallest RNA oligonucleotides to investigations of the entire ribosome. Our review encompasses tetranucleotides, tetraloops, a number of small RNA motifs, A-helix RNA, kissing-loop complexes, the TAR RNA element, the decoding center and other important regions of the ribosome, as well as assorted others systems. Extended sections are devoted to RNA-ion interactions, ribozymes, riboswitches, and protein/RNA complexes. Our overview is written for as broad of an audience as possible, aiming to provide a much-needed interdisciplinary bridge between computation and experiment, together with a perspective on the future of the field.

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.

Propensities for loop structures of RNA & DNA backbones

RNA oligonucleotides exhibit a large tendency to bend and form a loop conformation which is a major motif contributing to their complex three-dimensional structure. This is in contrast to DNA molecules that predominantly form the double-helix structure. In this paper we investigate by molecular dynamics simulation, as well as, by its combination with the replica-exchange method, the propensity of RNA chains containing the GCUAA pentaloop to form spontaneously a hairpin conformation. The results were then compared with those of analogous hybrid oligonucleotides in which the ribose groups in the loop-region were substituted by deoxyriboses. We find that the RNA oligomers exhibit a marginal excess stability to form loop structures. The equilibrium constant for opening the loop to an extended conformation is twice as large in the hybrid than it is in the RNA chain. Analyses of the hydrogen bonds indicate that the excess stability for forming a hairpin is a result of hydrogen bonds the 2'-hydroxyls in the loop region form with other groups in the loop. Of these hydrogen bonds, the most important is the hydrogen bond donated from the 2'-OH at the first position of the loop to N7 of adenine at the forth position. RNA and DNA backbones are characterized by different backbone dihedral angles and sugar puckering that can potentially facilitate or hamper the hydrogen bonds involving the 2'-OH. Nevertheless, the sugar puckerings of all the pentaloop nucleotides were not significantly different between the two chains displaying the C3'-endo conformation characteristic to the A-form double helix. All of the other backbone dihedrals also did not show any considerable difference in the loop-region except of the δ-dihedral. In this case, the RNA loop exhibited bimodal distributions corresponding to, both, the RNA and DNA backbones, whereas the loop of the hybrid chain behaved mostly as that of a DNA backbone. Thus, it is possible that the behavior of the δ-dihedrals in the loop-region of the RNA adopts conformations that facilitate the intra-nucleotide hydrogen bondings of the 2'-hydroxyls, and consequently renders loop structures in RNA more stable.

Bioinformatics and molecular dynamics simulation study of L1 stalk non-canonical rRNA elements: kink-turns, loops, and tetraloops

The L1 stalk is a prominent mobile element of the large ribosomal subunit. We explore the structure and dynamics of its non-canonical rRNA elements, which include two kink-turns, an internal loop, and a tetraloop. We use bioinformatics to identify the L1 stalk RNA conservation patterns and carry out over 11.5 μs of MD simulations for a set of systems ranging from isolated RNA building blocks up to complexes of L1 stalk rRNA with the L1 protein and tRNA fragment. We show that the L1 stalk tetraloop has an unusual GNNA or UNNG conservation pattern deviating from major GNRA and YNMG RNA tetraloop families. We suggest that this deviation is related to a highly conserved tertiary contact within the L1 stalk. The available X-ray structures contain only UCCG tetraloops which in addition differ in orientation (anti vs syn) of the guanine. Our analysis suggests that the anti orientation might be a mis-refinement, although even the anti interaction would be compatible with the sequence pattern and observed tertiary interaction. Alternatively, the anti conformation may be a real substate whose population could be pH-dependent, since the guanine syn orientation requires protonation of cytosine in the tertiary contact. In absence of structural data, we use molecular modeling to explore the GCCA tetraloop that is dominant in bacteria and suggest that the GCCA tetraloop is structurally similar to the YNMG tetraloop. Kink-turn Kt-77 is unusual due to its 11-nucleotide bulge. The simulations indicate that the long bulge is a stalk-specific eight-nucleotide insertion into consensual kink-turn only subtly modifying its structural dynamics. We discuss a possible evolutionary role of helix H78 and a mechanism of L1 stalk interaction with tRNA. We also assess the simulation methodology. The simulations provide a good description of the studied systems with the latest bsc0χOL3 force field showing improved performance. Still, even bsc0χOL3 is unable to fully stabilize an essential sugar-edge H-bond between the bulge and non-canonical stem of the kink-turn. Inclusion of Mg(2+) ions may deteriorate the simulations. On the other hand, monovalent ions can in simulations readily occupy experimental Mg(2+) binding sites.

Ribose 2'-Hydroxyl Groups Stabilize RNA Hairpin Structures Containing GCUAA Pentaloop

The chemical structure of RNA and DNA is very similar; however, the three-dimensional conformation of these two nucleic acids is very different. Whereas the DNA adopts a repetitive structure of a double-stranded helix, RNA is primarily single stranded with a complex three-dimensional structure in which the hairpin is the most common secondary structure. Apart from the difference between uracil and thymine, the difference in the chemical structure between RNA and DNA is the presence of a hydroxyl group at position 2' of the sugar (ribose) instead of a hydrogen (deoxyribose). In this paper, we present molecular dynamics simulations addressing the contribution of 2'-hydroxyls to the stability of a GCUAA pentaloop motif. The results indicate that the 2'-hydroxyls stabilize the hairpin conformation of the GCUAA pentaloop relative to an analogous oligonucleotide in which the ribose sugars in the loop region were substituted with deoxyriboses. The magnitude of the stabilization was found to be 23.8 ± 4.1 kJ/mol using an alchemical mutations free energy method and 4.2 ± 6.5 kJ/mol using potential of mean force calculations. The latter indicates that in addition to its larger thermodynamic stability the RNA hairpin is also kinetically more stable. We find that the excess stability is a result of intrahairpin hydrogen bonds in the loop region between the 2'-hydroxyls and sugars, bases, and phosphates. The hydrogen bonds with the sugars and phosphates involve predominantly interactions with adjacent nucleotides. However, the hydrogen bonds with the bases involve also interactions between groups on opposite sides of the loop or with the middle base of the loop and are therefore likely to contribute significantly to the stability of the loop. Of these hydrogen bonds, the most frequent is observed between the 2'-hydroxyl at the first position of the pentaloop with N6/N7 of adenine at the forth position, as well as between the 2'-hydroxyl at position -1 with N6 of adenine at the fifth position. Our results contribute to the notion that one of the important roles of the ribose sugars in RNA is to facilitate hairpin formation.

Evaluation of parameters critical for observing nucleic acids inside living Xenopus laevis oocytes by in-cell NMR spectroscopy

In-cell NMR spectroscopy of proteins in different cellular environments is a well-established technique that, however, has not been applied to nucleic acids so far. Here, we show that isotopically labeled DNA and RNA can be observed inside the eukaryotic environment of Xenopus laevis oocytes by in-cell NMR spectroscopy. One limiting factor for the observation of nucleic acids in Xenopus oocytes is their reduced stability. We demonstrate that chemical modification of DNA and RNA can protect them from degradation and can significantly enhance their lifetime. Finally, we show that the imino region of the NMR spectrum is devoid of any oocyte background signals enabling the detection even of isotopically nonlabeled molecules.

High-resolution NMR structure of an RNA model system: the 14-mer cUUCGg tetraloop hairpin RNA

We present a high-resolution nuclear magnetic resonance (NMR) solution structure of a 14-mer RNA hairpin capped by cUUCGg tetraloop. This short and very stable RNA presents an important model system for the study of RNA structure and dynamics using NMR spectroscopy, molecular dynamics (MD) simulations and RNA force-field development. The extraordinary high precision of the structure (root mean square deviation of 0.3 A) could be achieved by measuring and incorporating all currently accessible NMR parameters, including distances derived from nuclear Overhauser effect (NOE) intensities, torsion-angle dependent homonuclear and heteronuclear scalar coupling constants, projection-angle-dependent cross-correlated relaxation rates and residual dipolar couplings. The structure calculations were performed with the program CNS using the ARIA setup and protocols. The structure quality was further improved by a final refinement in explicit water using OPLS force field parameters for non-bonded interactions and charges. In addition, the 2'-hydroxyl groups have been assigned and their conformation has been analyzed based on NOE contacts. The structure currently defines a benchmark for the precision and accuracy amenable to RNA structure determination by NMR spectroscopy. Here, we discuss the impact of various NMR restraints on structure quality and discuss in detail the dynamics of this system as previously determined.

RNA phosphodiester backbone dynamics of a perdeuterated cUUCGg tetraloop RNA from phosphorus-31 NMR relaxation analysis

We have analyzed the relaxation properties of all (31)P nuclei in an RNA cUUCGg tetraloop model hairpin at proton magnetic field strengths of 300, 600 and 900 MHz in solution. Significant H, P dipolar contributions to R (1) and R (2) relaxation are observed in a protonated RNA sample at 600 MHz. These contributions can be suppressed using a perdeuterated RNA sample. In order to interpret the (31)P relaxation data (R (1), R (2)), we measured the (31)P chemical shift anisotropy (CSA) by solid-state NMR spectroscopy under various salt and hydration conditions. A value of 178.5 ppm for the (31)P CSA in the static state (S (2) = 1) could be determined. In order to obtain information about fast time scale dynamics we performed a modelfree analysis on the basis of our relaxation data. The results show that subnanosecond dynamics detected around the phosphodiester backbone are more pronounced than the dynamics detected for the ribofuranosyl and nucleobase moieties of the individual nucleotides (Duchardt and Schwalbe, J Biomol NMR 32:295-308, 2005; Ferner et al., Nucleic Acids Res 36:1928-1940, 2008). Furthermore, the dynamics of the individual phosphate groups seem to be correlated to the 5' neighbouring nucleobases.

Conformationally restricted nucleotides as a probe of structure-function relationships in RNA

We introduce the use of commercially available locked nucleic acids (LNAs) as a functional probe in RNA. LNA nucleotides contain a covalent linkage that restricts the pseudorotation phase of the ribose to C3'-endo (A-form). Introduction of an LNA at a single site thus allows the role of ribose structure and dynamics in RNA function to be assessed. We apply LNA probing at multiple sites to analyze self-cleavage in the lead-dependent ribozyme (leadzyme), thermodynamic stability in the UUCG tetraloop, and the kinetics of recognition of U1A protein by U1 snRNA hairpin II. In the leadzyme, locking a single guanosine residue into the C3'-endo pucker increases the catalytic rate by a factor of 20, despite the fact that X-ray crystallographic and NMR structures of the leadzyme ground state reported a C2'-endo conformation at this site. These results strongly suggest that a conformational change at this position is critical for catalytic function. Functional insights obtained in all three systems demonstrate the highly general applicability of LNA probing in analysis of the role of ribose orientation in RNA structure, dynamics, and function.

NMR and MD studies of the temperature-dependent dynamics of RNA YNMG-tetraloops

In a combined NMR/MD study, the temperature-dependent changes in the conformation of two members of the RNA YNMG-tetraloop motif (cUUCGg and uCACGg) have been investigated at temperatures of 298, 317 and 325 K. The two members have considerable different thermal stability and biological functions. In order to address these differences, the combined NMR/MD study was performed. The large temperature range represents a challenge for both, NMR relaxation analysis (consistent choice of effective bond length and CSA parameter) and all-atom MD simulation with explicit solvent (necessity to rescale the temperature). A convincing agreement of experiment and theory is found. Employing a principle component analysis of the MD trajectories, the conformational distribution of both hairpins at various temperatures is investigated. The ground state conformation and dynamics of the two tetraloops are indeed found to be very similar. Furthermore, both systems are initially destabilized by a loss of the stacking interactions between the first and the third nucleobase in the loop region. While the global fold is still preserved, this initiation of unfolding is already observed at 317 K for the uCACGg hairpin but at a significantly higher temperature for the cUUCGg hairpin.

Base-specific spin-labeling of RNA for structure determination

To facilitate the measurement of intramolecular distances in solvated RNA systems, a combination of spin-labeling, electron paramagnetic resonance (EPR), and molecular dynamics (MD) simulation is presented. The fairly rigid spin label 2,2,5,5-tetramethyl-pyrrolin-1-yloxyl-3-acetylene (TPA) was base and site specifically introduced into RNA through a Sonogashira palladium catalyzed cross-coupling on column. For this purpose 5-iodo-uridine, 5-iodo-cytidine and 2-iodo-adenosine phosphoramidites were synthesized and incorporated into RNA-sequences. Application of the recently developed ACE chemistry presented the main advantage to limit the reduction of the nitroxide to an amine during the oligonucleotide automated synthesis and thus to increase substantially the reliability of the synthesis and the yield of labeled oligonucleotides. 4-Pulse Electron Double Resonance (PELDOR) was then successfully used to measure the intramolecular spin-spin distances in six doubly labeled RNA-duplexes. Comparison of these results with our previous work on DNA showed that A- and B-Form can be differentiated. Using an all-atom force field with explicit solvent, MD simulations gave results in good agreement with the measured distances and indicated that the RNA A-Form was conserved despite a local destabilization effect of the nitroxide label. The applicability of the method to more complex biological systems is discussed.

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.

Structure and dynamics of an RNA tetraloop: a joint molecular dynamics and NMR study

Molecular dynamics simulations of the RNA tetraloop 5'-CGCUUUUGCG-3' with high melting temperature and significant conformational heterogeneity in explicit water solvent are presented and compared to NMR studies. The NMR data allow for a detailed test of the theoretical model, including the quality of the force field and the conformational sampling. Due to the conformational heterogeneity of the tetraloop, high temperature (350 K) and locally enhanced sampling simulations need to be invoked. The Amber98 force field leads to a good overall agreement with experimental data. Based on NMR data and a principal component analysis of the 350 K trajectory, the dynamic structure of the tetraloop is revealed. The principal component free energy surface exhibits four minima, which correspond to well-defined conformational structures that differ mainly by their base stacking in the loop region. No correlation between the motion of the sugar rings and the stacking dynamics of the loop bases is found.

Efficient search on energy minima for structure prediction of nucleic acid motifs

Structure prediction of non-canonical motifs such as mismatches, extra unmatched nucleotides or internal and hairpin loop structures in nucleic acids is of great importance for understanding the function and design of nucleic acid structures. Systematic conformational analysis of such motifs typically involves the generation of many possible combinations of backbone dihedral torsion angles for a given motif and subsequent energy minimization (EM) and evaluation. Such approach is limited due to the number of dihedral angle combinations that grows very rapidly with the size of the motif. Two conformational search approaches have been developed that allow both an effective crossing of barriers during conformational searches and the computational demand grows much less with system size then search methods that explore all combinations of backbone dihedral torsion angles. In the first search protocol single torsion angles are flipped into favorable states using constraint EM and subsequent relaxation without constraints. The approach is repeated in an iterative manner along the backbone of the structural motif until no further energy improvement is obtained. In case of two test systems, a DNA-trinucleotide loop (sequence: GCA) and a RNA tetraloop (sequence: UUCG), the approach successfully identified low energy states close to experiment for two out of five start structures. In the second method randomly selected combinations of up to six backbone torsion angles are simultaneously flipped into preset ranges by a short constraint EM followed by unconstraint EM and acceptance according to a Metropolis acceptance criterion. This combined stochastic/EM search was even more effective than the single torsion flip approach and selected low energy states for the two test cases in between two and four cases out of five start structures.

Hinge-like motions in RNA kink-turns: the role of the second a-minor motif and nominally unpaired bases

Kink-turn (K-turn) motifs are asymmetric internal loops found at conserved positions in diverse RNAs, with sharp bends in phosphodiester backbones producing V-shaped structures. Explicit-solvent molecular dynamics simulations were carried out for three K-turns from 23S rRNA, i.e., Kt-38 located at the base of the A-site finger, Kt-42 located at the base of the L7/L12 stalk, and Kt-58 located in domain III, and for the K-turn of human U4 snRNA. The simulations reveal hinge-like K-turn motions on the nanosecond timescale. The first conserved A-minor interaction between the K-turn stems is entirely stable in all simulations. The angle between the helical arms of Kt-38 and Kt-42 is regulated by local variations of the second A-minor (type I) interaction between the stems. Its variability ranges from closed geometries to open ones stabilized by insertion of long-residency waters between adenine and cytosine. The simulated A-minor geometries fully agree with x-ray data. Kt-58 and Kt-U4 exhibit similar elbow-like motions caused by conformational change of the adenosine from the nominally unpaired region. Despite the observed substantial dynamics of K-turns, key tertiary interactions are stable and no sign of unfolding is seen. We suggest that some K-turns are flexible elements mediating large-scale ribosomal motions during the protein synthesis cycle.

Dynamics and Stability of GCAA Tetraloops with 2-Aminopurine and Purine Substitutions

The contributions of various interactions in the GGCGCAAGCC hairpin containing a GCAA tetraloop were studied by computer simulations using the substitutions of functional groups. The guanosine (G) in the first tetraloop position or in the C-G closing base pair was replaced by 2-aminopurine (AP), and the individual tetraloop's adenosines (A) were replaced by purine (PUR). These substitutions eliminated particular hydrogen bonds thought to stabilize the GCAA tetraloop. For each substitution, molecular dynamics (MD) simulations were carried out in an aqueous solution with sodium counterions, using the CHARMM27 force field. The MD simulations showed that the substitutions in the first (G-->AP) and the third (A-->PUR) position of the GCAA tetraloop did not significantly influence the conformation of the hairpin. A long-lived bridging water molecule observed in the GCAA loop was present in both modified loops. The substitutions made in the last loop position (A-->PUR) or in the C-G base pair closing the tetraloop (G-->AP) to some extent influenced the loop structure and dynamics. These loops did not display the long-lived bridging water molecules. When the second A in the GCAA loop was replaced by PUR, the first A in the loop was observed in the anti or in the syn orientation about the glycosyl bond. The G to AP substitution in C-G base pair led to a change of their arrangement from the Watson-Crick to wobble. The MD simulations of the hairpin with C-AP wobble closing base pair showed increased conformational dynamics of the hairpin. The changes of hairpin formation free energy associated with the substitutions of individual bases were calculated by the free energy perturbation method. Our theoretical estimates suggest a larger destabilization for the G to AP substitutions in GCAA loop than for the substitutions of individual A's by PUR, which is in accordance with experimental tendency. The calculations predicted a similar free energy change for G to AP substitutions in the GCAA tetraloop and in the C-G closing base pair.

Effects of base substitutions in an RNA hairpin from molecular dynamics and free energy simulations

Contributions of individual interactions in the GGCGCAAGCC hairpin containing a GCAA tetraloop were studied by computer simulations using base substitutions. The G in the first tetraloop position was replaced by inosine (I) or adenosine (A), and the G in the C-G basepair closing the tetraloop was replaced by I. These substitutions eliminate particular hydrogen bonds proposed in the nuclear magnetic resonance model of the GCAA tetraloop. Molecular dynamics simulations of the GCAA tetraloop in aqueous solvent displayed a well-defined hydrogen pattern between the first and last loop nucleotides (G and A) stabilized by a bridging water molecule. Substitution of G-->I in the basepair closing the tetraloop did not significantly influence the loop structure and dynamics. The ICAA loop maintained the overall structure, but displayed variation in the hydrogen-bond network within the tetraloop itself. Molecular dynamics simulations of the ACAA loop led to conformational heterogeneity of the resulting structures. Changes of hairpin formation free energy associated with substitutions of individual bases were calculated by the free energy perturbation method. The calculated decrease of the hairpin stability upon G-->I substitution in the C-G basepair closing the tetraloop was in good agreement with experimental thermodynamic data. Our theoretical estimates for G-->I and G-->A mutations located in the tetraloop suggest larger loop destabilization than corresponding experimental results. The extent of conformational sampling of the structures resulting from base substitutions and its impact on the calculated free energy was discussed.

Sequence context dependence of tandem guanine:adenine mismatch conformations in RNA: a continuum solvent analysis

Guanine:adenine (G:A) mismatches and in particular tandem G:A (tG:A) mismatches are frequently observed in biological RNA molecules and can serve as sites for tertiary interaction, metal binding and protein recognition. Depending on the surrounding sequence tG:A mismatches can adopt different basepairing topologies. In the sequence context (5'-) GGAC (tandem G:A in bold) a face-to-face (imino or Watson-Crick-like) pairing is preferred whereas in the CGAG context, G and A adopt a sheared arrangement. Systematic conformational searches with a generalized Born continuum model and molecular dynamics simulations including explicit water molecules and ions have been used to generate face-to-face and sheared tG:A mismatches in both CGAG and GGAC sequence contexts. Conformations from both approaches were evaluated using the same force field and a Poisson-Boltzmann continuum solvent model. Although the substate analysis predicted the sheared arrangement to be energetically preferred in both sequence contexts, a significantly greater preference of the sheared form was found for the CGAG context. In agreement with the experimental observation, the analysis of molecular dynamics trajectories indicated a preference of the sheared form in the case of the CGAG-context and a favorization of the face-to-face form in the case of the GGAC context. The computational studies allowed to identify energetic contributions that stabilize or destabilize the face-to-face and sheared tandem mismatch topologies. The calculated nonpolar solvation and Lennard-Jones packing interaction were found to stabilize the sheared topology independent of the sequence context. Electrostatic contributions are predicted to make the most significant contribution to the sequence context dependence on the structural preference of tG:A mismatches.

Binding of europium(III) ions to RNA stem loops: role of the primary hydration sphere in complex formation

Understanding the process by which RNA molecules fold into stable structures includes study of the role of site-bound metal ions. Because the alkaline earth metal ions typically associated with RNA structure [most often Mg(II)] do not provide convenient spectroscopic signals, replacement with metal ions having spectroscopically useful properties has been a valuable approach. The luminescence properties of the lanthanide(III) series, in particular europium(III), have made them useful in the study of complexation with biomolecules. We review the physical, chemical, and spectroscopic characteristics of Eu(III) that contribute to its value as a probe of RNA-metal ion interactions, and examples of information obtained from studies of Eu(III) bound to small RNA stem loops. Although Eu(III) has similar site preference to Mg(II), luminescence and isothermal titration calorimetry measurements indicate that Ln(III) loses water molecules from the inner hydration sphere more readily than does Mg(II), resulting in more direct coordination between RNA and the metal ion and very different energetics of binding. In some cases, e.g., a GAAA tetraloop, binding appears to occur by a lock and key process; in the same base sequence containing certain deoxynucleoside substitutions that alter loop structure, binding appears to occur by an induced fit process.

DAPI binding to the DNA minor groove: a continuum solvent analysis

A continuum solvent model based on the generalized Born (GB) or finite-difference Poisson-Boltzmann (FDPB) approaches has been employed to compare the binding of 4'-6-diamidine-2-phenyl indole (DAPI) to the minor groove of various DNA sequences. Qualitative agreement between the results of GB and FDPB approaches as well as between calculated and experimentally observed trends regarding the sequence specificity of DAPI binding to B-DNA was obtained. Calculated binding energies were decomposed into various contributions to solvation and DNA-ligand interaction. DNA conformational adaptation was found to make a favorable contribution to the calculated total interaction energy but did not change the DAPI binding affinity ranking of different DNA sequences. The calculations indicate that closed complex formation is mainly driven by nonpolar contributions and was found to be disfavored electrostatically due to a desolvation penalty that outbalances the attractive Coulomb interaction. The calculated penalty was larger for DAPI binding to GC-rich sequences compared with AT-rich target sequences and generally larger for the FDPB vs the GB continuum model. A radial interaction profile for DAPI at different distances from the DNA minor groove revealed an electrostatic energy minimum a few Angstroms farther away from the closed binding geometry. The calculated electrostatic interaction up to this distance is attractive and it may stabilize a nonspecific binding arrangement.

Modelling ion binding to AA platform motifs in RNA: a continuum solvent study including conformational adaptation

Binding of monovalent and divalent cations to two adenine-adenine platform structures from the Tetrahymena group I intron ribozyme has been studied using continuum solvent models based on the generalised Born and the finite-difference Poisson-Boltzmann approaches. The adenine-adenine platform RNA motif forms an experimentally characterised monovalent ion binding site important for ribozyme folding and function. Qualitative agreement between calculated and experimental ion placements and binding selectivity was obtained. The inclusion of solvation effects turned out to be important to obtain low energy structures and ion binding placements in agreement with the experiment. The calculations indicate that differences in solvation of the isolated ions contribute to the calculated ion binding preference. However, Coulomb attraction and van der Waals interactions due to ion size differences and RNA conformational adaptation also influence the calculated ion binding affinity. The calculated alkali ion binding selectivity for both platforms followed the order K(+) > Na(+) > Rb(+) > Cs(+) > Li(+) (Eisenman series VI) in the case of allowing RNA conformational relaxation during docking. With rigid RNA an Eisenman series V was obtained (K(+) > Rb(+) > Na(+) > Cs(+) > Li(+)). Systematic energy minimisation docking simulations starting from several hundred initial placements of potassium ions on the surface of platform containing RNA fragments identified a coordination geometry in agreement with the experiment as the lowest energy binding site. The approach could be helpful to identify putative ion binding sites in nucleic acid structures determined at low resolution or with experimental methods that do not allow identification of ion binding sites.

Conformational analysis of DNA-trinucleotide-hairpin-loop structures using a continuum solvent model

A number of trinucleotide sequences in DNA can form compact and stable hairpin loops that may have significance for DNA replication and transcription. The conformational analysis of these motifs is important for an understanding of the function and design of nucleic acid structures. Extensive conformational searches have been performed on three experimentally known trinucleotide hairpin loops (AGC, AAA, and GCA) closed by a four-base-pair stem. An implicit solvation model based on the generalized Born method has been employed during energy minimization and conformational search. In addition, energy-minimized conformers were evaluated using a finite-difference Poisson-Boltzmann approach. For all three loop sequences, conformations close to experiment were found as lowest-energy structures among several thousand alternative energy minima. The inclusion of reaction-field contributions was found to be important for a realistic conformer ranking. Most generated hairpin loop structures within approximately 5 kcal x mol(-1) of the lowest-energy structure have a similar topology. Structures within approximately 10 kcal x mol(-1) could be classified into about five structural families representing distinct arrangements of loop nucleotides. Although a large number of backbone torsion angle combinations were compatible with each structural class, some specific patterns could be identified. Harmonic mode analysis was used to account for differences in conformational flexibility of low-energy sub-states. Class-specific differences in the pattern of atomic fluctuations along the sequence were observed; however, inclusion of conformational entropy contributions did not change ranking of structural classes. For an additional loop sequence (AAG) with no available experimental structure, the approach suggests a lowest-energy loop topology overall similar to the other three loop sequences but closed by a different non-canonical base-pairing scheme.

Probing RNA in vivo with methylation guide small nucleolar RNAs

Most box C/D small nucleolar RNAs (snoRNAs) direct the formation of 2'-O-methylated nucleotides in ribosomal RNA and, apparently, other RNAs present in the nucleolar complex. Sites to be modified are selected by a long (>10-nt) antisense guide sequence in the snoRNA and a distance measurement from a box D or D' element that follows the snoRNA guide sequence. Modification of the substrate occurs in the region of complementarity, at a position five nucleotides upstream from box D/D'. Methylation can be targeted to novel sites by expressing a snoRNA with a new guide sequence. In some cases methylation impairs the growth rate of the cell, indicating that a functionally important nucleotide has been altered. With a view to harnessing snoRNA-directed methylation for functional mapping, we have developed a method for constructing libraries of snoRNA genes that, in principle, can introduce methylation point mutations into any rRNA segment of interest. The strategy and procedures are described here, and preliminary results are presented that show the feasibility of using this technology to probe a region of the yeast large subunit rRNA that includes the core of the peptidyltransferase center.

The crystal structure of UUCG tetraloop

All large structured RNAs contain hairpin motifs made of a stem closed by several looped nucleotides. The most frequent loop motif is the UUCG one. This motif belongs to the tetraloop family and has the peculiarity of being highly thermodynamically stable. Here, we report the first crystal structure of two UUCG tetraloops embedded in a larger RNA-protein complex solved at 2.8 A resolution. The two loops present in the asymmetric unit are in a different crystal packing environment but, nevertheless, have an identical conformation. The observed structure is globally close to that obtained in solution by nuclear magnetic resonance. However, subtle differences point to a more detailed picture of the role played by 2'-hydroxyl groups in stabilising this tetraloop.

Experimental and computational studies of the G[UUCG]C RNA tetraloop

In prokaryotic ribosomal RNAs, most UUCG tetraloops are closed by a C-G base-pair. However, this preference is greatly reduced in eukaryotic rRNA species where many UUCG tetraloops are closed by G-C base-pairs. Here, biophysical properties of the C[UUCG]G and G[UUCG]C tetraloops are compared, using experimental and computational methods. Thermal denaturation experiments are used to derive thermodynamic parameters for the wild-type G[UUCG]C tetraloop and variants containing single deoxy substitutions in the loop. A comparison with analogous experiments on the C[UUCG]G motif shows that the two RNA species exhibit similar patterns in response to the substitutions, suggesting that their loop structures are similar. This conclusion is supported by NMR data that suggest that the essential UUCG loop structure is maintained in both tetraloops. However, NMR results show that the G[UUCG]C loop structure is disrupted prior to melting of the stem; this behavior is in contrast to the two-state behavior of the C[UUCG]G molecule. Stochastic dynamics simulations using the GB/SA continuum solvation model, run as a function of temperature, show rare conformational transitions in several G[UUCG]C simulations. These results lead to the conclusion that substitution of a G-C for a C-G closing base-pair increases the intrinsic flexibility of the UUCG loop.