Folding of a DNA hairpin loop structure in explicit solvent using replica-exchange molecular dynamics simulations

Hairpin loop structures are common motifs in folded nucleic acids. The 5'-GCGCAGC sequence in DNA forms a characteristic and stable trinucleotide hairpin loop flanked by a two basepair stem helix. To better understand the structure formation of this hairpin loop motif in atomic detail, we employed replica-exchange molecular dynamics (RexMD) simulations starting from a single-stranded DNA conformation. In two independent 36 ns RexMD simulations, conformations in very close agreement with the experimental hairpin structure were sampled as dominant conformations (lowest free energy state) during the final phase of the RexMDs ( approximately 35% at the lowest temperature replica). Simultaneous compaction and accumulation of folded structures were observed. Comparison of the GCA trinucleotides from early stages of the simulations with the folded topology indicated a variety of central loop conformations, but arrangements close to experiment that are sampled before the fully folded structure also appeared. Most of these intermediates included a stacking of the C(2) and G(3) bases, which was further stabilized by hydrogen bonding to the A(5) base and a strongly bound water molecule bridging the C(2) and A(5) in the DNA minor groove. The simulations suggest a folding mechanism where these intermediates can rapidly proceed toward the fully folded hairpin and emphasize the importance of loop and stem nucleotide interactions for hairpin folding. In one simulation, a loop motif with G(3) in syn conformation (dihedral flip at N-glycosidic bond) accumulated, resulting in a misfolded hairpin. Such conformations may correspond to long-lived trapped states that have been postulated to account for the folding kinetics of nucleic acid hairpins that are slower than expected for a semiflexible polymer of the same size.     

A shorter peptide model from staphylococcal nuclease for the folding-unfolding equilibrium of a beta-hairpin shows that unfolded state has significant contribution from compact conformational states

It is important to understand the conformational features of the unfolded state in equilibrium with folded state under physiological conditions. In this paper, we consider a short peptide model LMYKGQPM from staphylococcal nuclease to model the conformational equilibrium between a hairpin conformation and its unfolded state using molecular dynamics simulation under NVT conditions at 300K using GROMOS96 force field. The free energy landscape has overall funnel-like shape with hairpin conformations sampling the minima. The "unfolded" state has a higher free energy of approximately 12kJ/mol with respect to native hairpin minimum and occupies a plateau region. We find that the unfolded state has significant contributions from compact conformations. Many of these conformations have hairpin-like topology. Further, these compact conformational forms are stabilized by hydrophobic interactions. Conversion between native and non-native hairpins occurs via unfolded states. Frequent conversions between folded and unfolded hairpins are observed with single exponential kinetics. We compare our results with the emerging picture of unfolded state from both experimental and theoretical studies.     

Site-specific variations in RNA folding thermodynamics visualized by 2-aminopurine fluorescence

The fluorescent base analogue 2-aminopurine (2-AP) is commonly used to study specific conformational and protein binding events involving nucleic acids. Here, combinations of steady-state and time-resolved fluorescence spectroscopy of 2-AP were employed to monitor conformational transitions within a model hairpin RNA from diverse structural perspectives. RNA substrates adopting stable, unambiguous secondary structures were labeled with 2-AP at an unpaired base, within the loop, or inside the base-paired stem. Steady-state fluorescence was monitored as the RNA hairpins made the transitions between folded and unfolded conformations using thermal denaturation, urea titration, and cation-mediated folding. Unstructured control RNA substrates permitted the effects of higher-order RNA structures on 2-AP fluorescence to be distinguished from stimulus-dependent changes in intrinsic 2-AP photophysics and/or interactions with adjacent residues. Thermodynamic parameters describing local conformational changes were thus resolved from multiple perspectives within the model RNA hairpin. These data provided energetic bases for construction of folding mechanisms, which varied among different folding-unfolding stimuli. Time-resolved fluorescence studies further revealed that 2-AP exhibits characteristic signatures of component fluorescence lifetimes and respective fractional contributions in different RNA structural contexts. Together, these studies demonstrate localized conformational events contributing to RNA folding and unfolding that could not be observed by approaches monitoring only global structural transitions.     

β‐Hairpin folding and stability: molecular dynamics simulations of designed peptides in aqueous solution

The structural properties of a 10‐residue and a 15‐residue peptide in aqueous solution were investigated by molecular dynamics simulation. The two designed peptides, SYINSDGTWT and SESYINSDGTWTVTE, had been studied previously by NMR at 278 K and the resulting model structures were classified as 3:5 β‐hairpins with a type I + G1 β‐bulge turn. In simulations at 278 K, starting from the NMR model structure, the 3:5 β‐hairpin conformers proved to be stable over the time period evaluated (30 ns). Starting from an extended conformation, simulations of the decapeptide at 278 K, 323 K and 353 K were also performed to study folding. Over the relatively short time scales explored (30 ns at 278 K and 323 K, 56 ns at 353 K), folding to the 3:5 β‐hairpin could only be observed at 353 K. At this temperature, the collapse to β‐hairpin‐like conformations is very fast. The conformational space accessible to the peptide is entirely dominated by loop structures with different degrees of β‐hairpin character. The transitions between different types of ordered loops and β‐hairpins occur through two unstructured loop conformations stabilized by a single side‐chain interaction between Tyr2 and Trp9, which facilitates the changes of the hydrogen‐bond register. In agreement with previous experimental results, β‐hairpin formation is initially driven by the bending propensity of the turn segment. Nevertheless, the fine organization of the turn region appears to be a late event in the folding process. Copyright © 2004 European Peptide Society and John Wiley & Sons, Ltd.     

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

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

Structural characterization of three RNA hexanucleotide loops from the internal ribosome entry site of polioviruses.

Structural characteristics of three RNA hairpins from the internal ribosome entry site of poliovirus mRNAs have been determined in solution by NMR. Complete proton, phosphorus and carbon resonance assignments were made for the three 16 nt hairpins. The loop sequences, 5'-AAUCCA , AAACCA and GAACCA, have been shown to be essential for viral mRNA translation. NOESY spectra for the three oligomers were very similar indicating a common three dimensional structure. Stems were A-type duplexes with C3'-endo sugar pucker. In the loops, sequential base stacking interactions were detected for all bases except between U8/A8 and C9, indicating a turn in the phosphodiester backbone at this point. Only one nucleotide, U8/A8, had a sugar pucker which deviated appreciably from C3'-endo. The final base in the loop, A11, exhibited an unusual gauche (-) gamma angle. An ensemble of 10 structures calculated for one hairpin using restrained molecular dynamics shows that the first three bases of the loop are turned so as to be exposed to the exterior of the molecule, while the remaining three bases are in an orientation approximating a continuation of the stem helix. Structure calculations and NMR relaxation measurements indicate that the loop apex is subject to considerable local dynamics.     

To be folded or to be unfolded?

The lack of ordered structure in “natively unfolded” proteins raises a general question: Are there intrinsic properties of amino acid residues that are responsible for the absence of fixed structure at physiological conditions? In this article, we demonstrate that the competence of a protein to be folded or to be unfolded may be determined by the property of amino acid residues to form a sufficient number of contacts in a globular state. The expected average number of contacts per residue calculated from the amino acid sequence alone (using the average number of contacts for 20 amino acid residues in globular proteins) can be used as one of the simple indicators of natively unfolded proteins. The prediction accuracy for the sets of 80 folded and 90 natively unfolded proteins reaches 89% if the expected average number of contacts is used as a parameter and 83% in the case of hydrophobicity. An optimal set of artificial parameters for 20 amino acid residues obtained by Monte Carlo algorithm to maximally separate the sets of 90 natively unfolded and 80 folded proteins demonstrates the upper limit for prediction accuracy, which is 95%.     

Beta-hairpin folding simulations in atomistic detail using an implicit solvent model

We have used distributed computing techniques and a supercluster of thousands of computer processors to study folding of the C-terminal beta-hairpin from protein G in atomistic detail using the GB/SA implicit solvent model at 300 K. We have simulated a total of nearly 38 micros of folding time and obtained eight complete and independent folding trajectories. Starting from an extended state, we observe relaxation to an unfolded state characterized by non-specific, temporary hydrogen bonding. This is followed by the appearance of interactions between hydrophobic residues that stabilize a bent intermediate. Final formation of the complete hydrophobic core occurs cooperatively at the same time that the final hydrogen bonding pattern appears. The folded hairpin structures we observe all contain a closely packed hydrophobic core and proper beta-sheet backbone dihedral angles, but they differ in backbone hydrogen bonding pattern. We show that this is consistent with the existing experimental data on the hairpin alone in solution. Our analysis also reveals short-lived semi-helical intermediates which define a thermodynamic trap. Our results are consistent with a three-state mechanism with a single rate-limiting step in which a varying final hydrogen bond pattern is apparent, and semi-helical off-pathway intermediates may appear early in the folding process. We include details of the ensemble dynamics methodology and a discussion of our achievements using this new computational device for studying dynamics at the atomic level.     

Bergerac-SH3: "frustation" induced by stabilizing the folding nucleus

The influence of an inserted exogenous independent folding element on the thermodynamics and folding properties of SH3 domain from alpha-spectrin has been investigated by creating a fused form between this small all-beta domain and a stable beta-hairpin (BH19). NMR analysis of synthetic peptides shows that insertion of BH19 nucleates formation of the original natural beta-hairpin (distal loop) that is part of the SH3 folding nucleus. The resulting protein (Bergerac-SHH) is more stable, folds faster and contains an elongated hairpin protruding from the globular domain as determined by 2D-NMR. "Protein engineering" analysis of the inserted region shows that it is folded in the transition state. Interestingly, stabilisation by insertion of the distal loop region results in the appearance of a compact intermediate revealed by a curved chevron plot at low denaturant concentration. This effect is eliminated at low salt concentrations by a single mutation of a hydrophobic residue within BH19 sequence, which is most probably involved in non-native interactions. Local stabilisation by enlargement and reinforcement of the folding nucleus, global compaction by the addition of salt and non-native interactions are shown to contribute to the observed deviation from the two-state behaviour.     

Nuclear magnetic resonance titration curves of histidine ring protons. Ribonuclease S-peptide and S-proteins.

The histidine C-2 proton NMR titration curves of ribonuclease S-peptide (residues 1 to 20) and S-protein (residues 21 to 124) are reported. Although S-protein contains 3 histidine residues, four discrete resonances are observed to titrate. One of these arises from the equivalent histidine residues of unfolded S-protein. The variation in area of the four resonances indicate that there is a reversible pH-dependent equilibrium between the folded and unfolded forms of S-protein, with some unfolded material being present at most pH values. Two of the resonances of the folded S-protein can be assigned to 2 of the histidine residues, 48 and 105, from the close similarity of their titration curves to those in ribonuclease. These similarities indicate a homology of portions of the folded conformation of S-protein to that of ribonuclease in solution. These results indicate that the complete amino acid sequence is not required to produce a folded conformation similar to the native globular protein, and they appear to eliminate the possibility that proteins fold from their NH2 terminus during protein synthesis. The low pH inflection present in the titration curve assigned to histidine residue 48 in ribonuclease is absent from this curve in S-protein. This is consistent with our previous conclusion that this inflection arises from the interaction of histidine 48 with aspartic acid residue 14, which is also absent in S-protein. The third titrating resonance of native S-protein is assigned to the remaining histidine residue at position 119. The properties of this resonance are not identical with either of the titration curves of the active site histidine residues 12 and 119 of ribonuclease. The resonance assigned to histidine 119 is the only one significantly affected on the addition of sodium phosphate to S-protein, indicating that some degree of phosphate binding occurs. In both the absence and presence of phosphate this curve also lacks the low pH inflection observed in the histidine 119 NMR titration curve in ribonuclease. This difference presumably arise from a conformational between ribonuclease and the folded S-protein involving a carboxyl group.     

Hairpin structures in DNA containing arabinofuranosylcytosine. A combination of nuclear magnetic resonance and molecular dynamics

Nuclear magnetic resonance (NMR) and model-building studies were carried out on the hairpin form of the octamer d(CGaCTAGCG) (aC = arabinofuranosylcytosine), referred to as the TA compound. The nonexchangeable protons of the TA compound were assigned by means of nuclear Overhauser effect spectroscopy (NOESY) and correlated spectroscopy (COSY). From a detailed analysis of the coupling data and of the NOESY spectra the following conclusions are reached: (i) The hairpin consists of a stem of three Watson-Crick type base pairs, and the two remaining residues, T(4) and dA(5), participate in a loop. (ii) All sugar rings show conformational flexibility although a strong preference for the S-type (C2'-endo) conformer is observed. (iii) The thymine does not stack upon the 3' side of the stem as expected, but swings into the minor groove. (This folding principle of the loop involves an unusual alpha t conformer in residue T(4).) (iv) At the 5'-3' loop-stem junction a stacking discontinuity occurs as a consequence of a sharp turn in that part of the backbone, caused by the unusual beta + and gamma t torsion angles in residue dG(6). (v) The A base slides over the 5' side of the stem to stack upon the aC(3) residue at the 3' side of the stem in an antiparallel fashion. On the basis of J couplings and a set of approximate proton-proton distances from NOE cross peaks, a model for the hairpin was constructed. This model was then refined by using an iterative relaxation matrix approach (IRMA) in combination with restrained molecular dynamics calculations. The resulting final model satisfactorily explains all the distance constraints.     

Molecular dynamics simulation reveals a surface salt bridge forming a kinetic trap in unfolding of truncated Staphylococcal nuclease

Surface salt bridges are ubiquitous in globular proteins. Their contribution to protein stability has been extensively debated in the past decade. Here, molecular dynamics simulations are performed starting from a non-equilibrium state of Staphylococcal nuclease (SNase) with C-terminal truncation (SNaseDelta). The results indicate a key role in the unfolding of the surface salt bridge between arginine 105 and glutamate 135. Experimentally, SNaseDelta is known to be partially unfolded. However, in simulations over 1 ns at 300 K and over 500 ps at 400 K, SNaseDelta remains stable in the native-like folded conformation, the salt bridge hindering unfolding. When the potential function is altered so as to selectively weaken the salt bridge, which then breaks rapidly at 430 K, the protein starts to unfold. The results suggest that breaking of this salt bridge presents a significant barrier to the unfolding transition of SNaseDelta from a native-like state to the unfolded state. Potential of mean force calculations indicate that the barrier height for this transition is approximately 7 kcal/mol.     

H-bond stability in the tRNA(Asp) anticodon hairpin: 3 ns of multiple molecular dynamics simulations.

Multiple molecular dynamics trajectories of the solvated and neutralized 17-residue tRNA(Asp) anticodon hairpin were generated for a total of 3 ns. Explicit treatment of all long-ranged electrostatic interactions by the particle mesh Ewald algorithm, as implemented in the AMBER MD software package, effected a degree of structural stabilization not previously achieved by use of a long 16-A solvent interaction truncation scheme. The increased stability of this multiple molecular dynamics set was appropriate for an in-depth analysis of the six 500-ps-long trajectories and allowed the characterization of a number of key structural interactions. The dynamical behavior of the standard Watson-Crick base pairs, the noncanonical G30-U40 "wobble" base pair, and the psi 32-C38 pseudo-base pair is presented as well as that of two C--H... O hydrogen bonds found to contribute to the array of tertiary interactions that stabilize the seven-nucleotide native loop conformation. The least mobile residue in the loop is U33, which forms the U-turn motif and which participates in several hydrogen-bonding interactions, whereas the most mobile residue is the apical residue G34 at the wobble position, a factor undoubtedly important in its biological function. The set of multiple molecular dynamics trajectories obtained does not converge on a 500-ps time scale to a unique dynamical model but instead describes an ensemble of structural microstates accessible to the system under the present simulation protocol, which is the result of local structural heterogeneity rather than of global conformational changes.     

Structured pathway across the transition state for peptide folding revealed by molecular dynamics simulations

Small globular proteins and peptides commonly exhibit two-state folding kinetics in which the rate limiting step of folding is the surmounting of a single free energy barrier at the transition state (TS) separating the folded and the unfolded states. An intriguing question is whether the polypeptide chain reaches, and leaves, the TS by completely random fluctuations, or whether there is a directed, stepwise process. Here, the folding TS of a 15-residue β-hairpin peptide, Peptide 1, is characterized using independent 2.5 μs-long unbiased atomistic molecular dynamics (MD) simulations (a total of 15 μs). The trajectories were started from fully unfolded structures. Multiple (spontaneous) folding events to the NMR-derived conformation are observed, allowing both structural and dynamical characterization of the folding TS. A common loop-like topology is observed in all the TS structures with native end-to-end and turn contacts, while the central segments of the strands are not in contact. Non-native sidechain contacts are present in the TS between the only tryptophan (W11) and the turn region (P7-G9). Prior to the TS the turn is found to be already locked by the W11 sidechain, while the ends are apart. Once the ends have also come into contact, the TS is reached. Finally, along the reactive folding paths the cooperative loss of the W11 non-native contacts and the formation of the central inter-strand native contacts lead to the peptide rapidly proceeding from the TS to the native state. The present results indicate a directed stepwise process to folding the peptide.     

Characterization of a partially folded intermediate of stem bromelain at low pH.

Equilibrium studies on the acid included denaturation of stem bromelain (EC 3.4.22.32) were performed by CD spectroscopy, fluorescence emission spectroscopy and binding of the hydrophobic dye, 1-anilino 8-naphthalene sulfonic acid (ANS). At pH 2.0, stem bromelain lacks a well defined tertiary structure as seen by fluorescence and near-UV CD spectra. Far-UV CD spectra show retention of some native like secondary structure at pH 2.0. The mean residue ellipticities at 208 nm plotted against pH showed a transition around pH 4.5 with loss of secondary structure leading to the formation of an acid-unfolded state. With further decrease in pH, this unfolded state regains most of its secondary structure. At pH 2.0, stem bromelain exists as a partially folded intermediate containing about 42.2% of the native state secondary structure Enhanced binding of ANS was observed in this state compared to the native folded state at neutral pH or completely unfolded state in the presence of 6 m GdnHCl indicating the exposure of hydrophobic regions on the protein molecule. Acrylamide quenching of the intrinsic tryptophan residues in the protein molecule showed that at pH 2.0 the protein is in an unfolded conformation with more tryptophan residues exposed to the solvent as compared to the native conformation at neutral pH. Interestingly, stem bromelain at pH 0.8 exhibits some characteristics of a molten globule, such as an enhanced ability to bind the fluorescent probe as well as considerable retention of secondary structure. All the above data taken together suggest the existence of a partially folded intermediate state under low pH conditions.     

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)     

Loop and stem dynamics during RNA hairpin folding and unfolding

2-Aminopurine (2AP) is a fluorescent adenine analog that probes mainly base stacking in nucleic acids. We labeled the loop or the stem of the RNA hairpin gacUACGguc with 2AP to study folding thermodynamics and kinetics at both loci. Thermal melts and fast laser temperature jumps detected by 2AP fluorescence monitored the stability and folding/unfolding kinetics. The observed thermodynamic and kinetic traces of the stem and loop mutants, though strikingly different at a first glance, can be fitted to the same free-energy landscape. The differences between the two probe locations arise because base stacking decreases upon unfolding in the stem, whereas it increases in the loop. We conclude that 2AP is a conservative adenine substitution for mapping out the contributions of different RNA structural elements to the overall folding process. Molecular dynamics (MD) totaling 0.6 μsec were performed to look at the conformations populated by the RNA at different temperatures. The combined experimental data, and MD simulations lead us to propose a minimal four-state free-energy landscape for the RNA hairpin. Analysis of this landscape shows that a sequential folding model is a good approximation for the full folding dynamics. The frayed state formed initially from the native state is a heterogeneous ensemble of structures whose stem is frayed either from the end or from the loop.     

Insights into nucleic acid conformational dynamics from massively parallel stochastic simulations

The helical hairpin is one of the most ubiquitous and elementary secondary structural motifs in nucleic acids, capable of serving functional roles and participating in long-range tertiary contacts. Yet the self-assembly of these structures has not been well-characterized at the atomic level. With this in mind, the dynamics of nucleic acid hairpin formation and disruption have been studied using a novel computational tool: large-scale, parallel, atomistic molecular dynamics simulation employing an inhomogeneous distributed computer consisting of more than 40,000 processors. Using multiple methodologies, over 500 micro s of atomistic simulation time has been collected for a large ensemble of hairpins (sequence 5'-GGGC[GCAA]GCCU-3'), allowing characterization of rare events not previously observable in simulation. From uncoupled ensemble dynamics simulations in unperturbed folding conditions, we report on 1), competing pathways between the folded and unfolded regions of the conformational space; 2), observed nonnative stacking and basepairing traps; and 3), a helix unwinding-rewinding mode that is differentiated from the unfolding and folding dynamics. A heterogeneous transition state ensemble is characterized structurally through calculations of conformer-specific folding probabilities and a multiplexed replica exchange stochastic dynamics algorithm is used to derive an approximate folding landscape. A comparison between the observed folding mechanism and that of a peptide beta-hairpin analog suggests that although native topology defines the character of the folding landscape, the statistical weighting of potential folding pathways is determined by the chemical nature of the polymer.     

Prediction of natively unfolded regions in protein chain

We have shown that the ability of a protein to be in globular or in natively unfolded state (under native conditions) may be determined (besides low overall hydrophobicity and a large net charge) by such a property as the average environment density, the average number of residues enclosed at the given distance. A statistical scale of the average number of residues enclosed at the given distance for 20 types of amino acid residues in globular state has been created on the basis of 6626 protein structures. Using this scale for separation of 80 globular and 90 natively unfolded proteins we fail only in 11% of proteins (compared with 17% of errors which are observed if to use hydrophobicity scale). The present scale may be used both for prediction of form (folded or unfolded) of the native state of protein and for prediction of natively unfolded regions in protein chains. The results of comparison of our method of predicting natively unfolded regions with the other known methods show that our method has the highest fraction of correctly predicted natively unfolded regions (that is 87% and 77% if to make averaging over residues and over proteins correspondingly).     

A conserved hairpin structure in Alfamovirus and Bromovirus subgenomic promoters is required for efficient RNA synthesis in vitro

The coat protein gene in RNA 3 of alfalfa mosaic virus (AMV; genus Alfamovirus, family Bromoviridae) is translated from the subgenomic RNA 4. Analysis of the subgenomic promoter (sgp) in minus-strand RNA 3 showed that a sequence of 37 nt upstream of the RNA 4 start site (nt +1) was sufficient for full sgp activity in an in vitro assay with the purified viral RNA-dependent RNA-polymerase (RdRp). The sequence of nt -6 to -29 could be folded into a potential hairpin structure with a loop represented by nt -16, -17, and -18, and a bulge involving nt -23. By introducing mutations that disrupted base pairing and compensatory mutations that restored base pairing, it was shown that base pairing in the top half of the putative stem (between the loop and bulge) was essential for sgp activity, whereas base pairing in the bottom half of the stem was less stringently required. Deletion of the bulged residue A-23 or mutation of this residue into a C strongly reduced sgp activity, but mutation of A-23 into U or G had little effect on sgp activity. Mutation of loop residues A-16 and A-17 affected sgp activity, whereas mutation of U-18 did not. Using RNA templates corresponding to the sgp of brome mosaic virus (BMV; genus Bromovirus, family Bromoviridae) and purified BMV RdRp, evidence was obtained indicating that also in BMV RNA a triloop hairpin structure is required for sgp activity.