Abstract
DsRBDs often bind dsRNAs with some specificity, yet the basis for this specificity is poorly understood. Rnt1p, the major RNase III in Saccharomyces cerevisiae, cleaves RNA substrates containing hairpins capped by A/uGNN tetraloops, using its dsRBD to recognize the conserved fold of these tetraloops. However, the identification of a Rnt1p substrate capped by an AAGU tetraloop raised the question of whether Rnt1p binds to this non-canonical substrate differently than to A/uGNN tetraloops. The solution structure of Rnt1p dsRBD in complex with an AAGU-capped hairpin reveals that the tetraloop undergoes a structural rearrangement upon binding to Rnt1p dsRBD to adopt a backbone conformation that is essentially the same as the AGAA tetraloop, and indicates that a conserved recognition mode is used for all Rnt1p substrates. Comparison of free and RNA-bound Rnt1p dsRBD reveals that tetraloop-specific binding requires a conformational change in helix α1. Our findings provide a unified model of binding site selection by this dsRBD.
INTRODUCTION
Eukaryotic members of the RNase III family of endoribonucleases cleave double-stranded RNA (dsRNA) targets involved in a variety of gene expression pathways [1, 2], including the maturation of precursor ribosomal RNA (rRNA) [3–5], small nuclear RNA (snRNA) and small nucleolar RNA (snoRNA) processing [1, 2], RNA interference (RNAi) and microRNA (miRNA) processing [6–8]. Rnt1p, the only non-mitochondrial RNase III present in S. cerevisiae, plays an essential role in the processing of rRNA, snRNAs, and snoRNAs [3, 5, 9, 10] in budding yeast. Rnt1p is also important for mRNA quality control, cleaving intronic sequences of unspliced pre-mRNAs [11]. A Rnt1p target site in the mRNA coding for the essential telomerase protein Est1p has been proposed to be important for maintenance of telomere length through regulation of Est1p expression [12]. Several studies have indicated that Rnt1p may play a role in transcription termination by cleavage of nascent transcripts [13–16]. Drosha and Dicer, other members of the RNAse III family, are involved in miRNA processing and RNAi [7, 8]. Although the RNAi pathway has been evolutionally lost in S. cerevisiae, it has been found in closely related yeast species such as S. castellii and Kluyveromyces polysporus. Introduction of S. castellii Dicer and Argonaute into S. cerevisiae resulted in a functional RNAi pathway [17]. Further, the budding yeast Dicers are more closely related to Rnt1p than to canonical Dicer, highlighting the importance of this representative of the RNase III family of enzymes.
All RNase III enzymes contain one or two conserved endonuclease domains (endoND). Two endoNDs form an intra- or inter-molecular dimer to create a large catalytic valley for Mg2+-dependent catalysis [18–24]. Most RNase III enzymes also have one or more double-stranded RNA binding domains (dsRBD). The N-terminal region of RNase III enzymes is variable across the family, and may include one or more additional domains with different functions. Rnt1p, like the bacterial RNase III enzymes, contains one endonuclease domain and one double-stranded RNA binding domain (dsRBD). However, Rnt1p also has an N-terminal domain unique to yeast RNase IIIs whose function is uncertain, but which may be required for the stabilization of Rnt1p homodimers [25]. RNase IIIs found in budding yeasts have a domain structure similar to that of Rnt1p, while most Drosha and Dicer enzymes have one or two dsRBDs, two endoNDs and an N-terminal accessory domain [20, 26].
The dsRBD is the second most abundant RNA binding domain. This domain specifically recognizes dsRNA [27–30] and has a conserved αβββα fold [28, 29, 31–34]. The first crystal structure of a dsRBD/dsRNA complex revealed that helix α1, β3-α2 loop and β1-β2 loop interact with the sugar-phosphate backbone of successive minor, major and minor grooves, respectively, along one face of an RNA helix, without any apparent base pair specificity [31]. The recognition of dsRNA by dsRBDs plays an important role in the catalytic cleavage or modification of dsRNAs by many RNAses [16, 18–20, 22, 24, 33] and RNA modification enzymes such as ADAR [35, 36]. Based on the structures of bacterial RNase III/dsRNA complexes [37] the dsRBDs are thought to contribute primarily to specificity of binding to dsRNA but not to target site selection [21, 38], although there are two base contacts that have recently been proposed to be sequence specific [36]. In contrast, Rnt1p dsRNA substrates are capped by A/uGNN tetraloops located 14–16 bp away from the cleavage site [39, 40], and specificity for these substrates resides in the dsRBD [33, 39–42]. Structural studies have revealed that A/uGNN tetraloops adopt a conserved fold [33, 43, 44], the shape of which is recognized on the minor groove side by Rnt1p dsRBD [33]. Surprisingly, the dsRBD has no direct contacts to the conserved A and G bases which point into the major groove, but rather its helix α1 fits snugly into the minor groove side of the tetraloop and top of the stem, interacting with the sugar-phosphate backbone and non-conserved 3′ bases. To date, this is the only known example of dsRBD binding specificity through terminal loop recognition. Rnt1p dsRBD is also unusual in containing an additional helix α3 that has been proposed to contribute to recognition of the tetraloop indirectly by stabilizing helix α1 [33, 45].
A genome-wide search in S. cerevesiae for snoRNA substrates of Rnt1p identified the non-canonical snoRNA substrate snR48 [46]. Unlike most Rnt1p substrates, snR48 contains an Rnt1p recognition site consisting of an AAGU capped hairpin. It was proposed that the AAGU tetraloop adopts a different fold from the canonical fold of AGNN tetraloops [47, 48], and that Rnt1p distinguishes between these two different ‘classes’ of tetraloop-hairpin substrates using different networks of protein-RNA interactions. To investigate the molecular basis for the recognition of the AAGU hairpin and to gain further understanding of substrate-specific recognition by Rnt1p, we determined the NMR solution structure of Rnt1p dsRBD in complex with a dsRNA hairpin capped by an AAGU tetraloop and investigated in vitro and in vivo cleavage and dsRBD binding. We find that when in complex with the dsRBD the AAGU tetraloop undergoes a structural rearrangement to adopt a backbone fold and interactions that are essentially the same as those in the complex of the dsRBD with an AGAA hairpin. Comparison of the structures of the complexes to previously determined solution and crystal structures of the free dsRBD showed that the dsRBD helix α1 undergoes a conformational change upon binding to both AAGU and AGAA tetraloops. Taken together, our results provide new insights into substrate-specific recognition by dsRBDs and provide a structural framework for a conserved general mode of RNA substrate recognition by Rnt1p.
RESULTS
The AAGU hairpin binds to and is efficiently cleaved by Rnt1p in the context of snR47 stem sequence
We investigated, using NMR spectroscopy, the interaction of Rnt1p dsRBD with a 32 nt RNA hairpin containing a 14 bp stem and capped by the AAGU tetraloop (AAGU hairpin) found in the snoRNA snR48 precursor (see Fig 3A). To facilitate comparisons between this complex (dsRBD/AAGU) and one with a canonical A/uGNN tetraloop, we used the same stem sequence as in the previously determined structure of a Rnt1p dsRBD-snR47h complex (dsRBD/AGAA), where the hairpin sequence was derived from the snoRNA snR47 precursor [33]. The two base pairs below the tetraloop are the same for snR47 and snR48, but otherwise the stem sequences differ, except for the 1st and 4th base pair in our hairpins. Complex formation was initially monitored by chemical shift changes observed in the 1H-15N HSQC spectra of the dsRBD upon the addition of AAGU (Figure S1). The dsRBD is at or near fast exchange with the hairpin on the NMR timescale, but the complex is saturated at a small excess of RNA, as observed for the dsRBD/AGAA complex, and amide chemical shift changes are very similar [33].
Figure 3.
Solution structure of the Rnt1p dsRBD/AAGU complex. (A) Sequence and secondary structure of the AAGU hairpin used in the NMR studies. (B) Superposition of the 16 lowest energy structures, showing all heavy atoms. The dsRBD is magenta and the AAGU hairpin is green. (C) Lowest energy structure of the complex. The RNA is shown as solvent-accessible surface and the protein as ribbons with the amino acids at the protein-RNA interface shown as ball-and-sticks, with oxygen red and nitrogen blue. The nucleotides in the AAGU tetraloop are colored 5′ to 3′ red (A), blue (A), orange (G) and cyan (U). See also Figure S1.
To compare the relative binding affinity of Rnt1p dsRBD to AGAA and AAGU hairpins, a series of 1H-15N HSQC spectra of the dsRBD were acquired at various ratios of added AGAA, AAGU, and UUCG hairpins, under high salt conditions. Previous studies have shown that the dsRBD does not specifically recognize a UUCG-capped hairpin [39], so this hairpin was used as a comparison for non-specific binding of the dsRBD to double stranded RNA. Apparent Kd values calculated from global fitting of the HSQC titration data, assuming a one-site binding model, are 34.1±2.9, 30.1±3.8, and 280±24.6 μM for the AAGU, AGAA, and UUCG hairpins, respectively (Figure 1A,B,C). These values indicate that under the NMR conditions Rnt1p dsRBD binds with the same affinity to both the AAGU and AGAA hairpins. In contrast, non-specific binding to dsRNA capped by a UUCG tetraloop is about an order of magnitude weaker. This result is consistent with gel shift assays using full-length Rnt1p, which show it binds with a 5–10 fold weaker affinity to non AGNN-containing tetraloops than to canonical tetraloop containing substrates [39, 40].
Figure 1.
snR47-derived dsRNA capped by an AAGU tetraloop binds to the Rnt1p dsRBD. (A-C) HSQC titration curves showing 15N and 1H chemical shift change Δδ(N,H) = [(Δδ(HN)2+ (Δδ(NH)/4)2] ½ as a function of the concentration ratio for the titration of dsRBD with the (A) AAGU, (B) AGAA, and (C) UUCG hairpins. The continuous lines show the curves for all amides with chemical shifts changes >0.05 ppm fitted globally to a one-site binding model.
Previously, Rnt1p was reported to require a defined sequence in the stem region of snR48-derived AAGU hairpin substrates for optimal cleavage [46, 48]. To confirm that the snR47-AAGU hybrid hairpin is a good substrate for Rnt1p, we performed Rnt1p cleavage assays with substrates derived from snR47, capped by AGAA, AAGU, or UUCG tetraloops (snR47-AGAA, snR47-AAGU, and snR47-UUCG, respectively) (Figure 2A), under single-turnover conditions (Figure 2B). Both snR47-AAGU and snR47-AGAA showed specific cleavage, while snR47-UUCG was almost unreactive over the assayed reaction time. The fact that the snR47-UUCG substrate shows only a 10-fold reduction of binding (Fig. 1C) but is almost completely refractory to Rnt1p cleavage confirms that, as shown previously [39, 40], the differences in binding affinity between different tetraloop-containing stems are not sufficient to explain the strong cleavage discrimination between these substrates. SnR47-AAGU also shows more additional cleavage products than snR47-AGAA. One corresponds to an intermediate cleaved in one strand only (band below substrate band in Figure 2B), and the others correspond to some alternate cleavage sites. In vivo, cleavage at any of these alternative sites would still be expected to result in correct subsequent processing, because each of these cleaved intermediates are expected to be used at similar efficiencies by the Rat1p exonuclease [49]. Overall, cleavage of the snR47-AAGU substrate occurred at a slightly slower rate than for snR47-AGAA, but the relative cleavage rates for this non-canonical substrate is comparable to the previously reported relative rates for canonical Rnt1p substrates containing AGAA and UGAA tetraloops [43]. These results indicate that the AAGU tetraloop in the context of the snR47 stem sequence is sufficient to support cleavage at a rate comparable to A/uGNN-tetraloop hairpin substrates.
Figure 2.
dsRNA capped by an AAGU tetraloop is an efficient substrate for Rnt1p. (A) Sequence of snR47-derived RNA substrates, where NNNN is AGAA, AAGU, or UUCG with the Rnt1p cleavage site indicated by arrows. (B and C) Single-turnover cleavage kinetics for snR47-AGAA, snR47-AAGU, and snr47-UUCG. (B) Phophorimages of polyacrylamide gels of RNA from the cleavage reactions. Bands corresponding to the full-length substrate (Su) and the cleavage product (Pr) are indicated. (C) Plot of fraction of substrate cleaved vs time. (D) Northern blot analysis of snR47 snoRNA expression carrying normal and mutant tetraloop sequences. Strains expressing snR47 with the wild-type (AGAA), AAGU, or UUCG loop sequences and a strain inactivated for Rnt1p (Rnt1Δ) were analyzed. MW, molecular weight marker (MspI digested pBR322); P, unprocessed precursor; M, mature snR47 snoRNA. (E) Primer extension analysis of snR47 snoRNA expression carrying normal and mutant tetraloop sequences. Legends are as in D.
To further investigate the ability of Rnt1p to recognize and process a substrate carrying an AAGU tetraloop, we analyzed the processing of snR47 mutant derivatives with different types of tetraloops in vivo. We introduced AAGU in place of AGAA in the stem-loop sequence upstream from the snR47 [9] chromosomal locus by homologous recombination (see Experimental Procedures). As controls for inefficient processing and complete loss of Rnt1p function, we generated a strain carrying a UUCG tetraloop and used a strain inactivated for Rnt1p (rnt1Δ), respectively. As shown by Northern blot in Figure 2D, the AAGU mutant snoRNA precursor was processed as efficiently as the wild-type precursor in vivo, showing high levels of mature snoRNA and no apparent unprocessed precursor accumulation. In contrast, samples extracted from the UUCG tetraloop mutant or from the rnt1Δstrain exhibited little or no mature snoRNA and a strong accumulation of unprocessed precursors (P, Figure 2D). Primer extension analysis of the wild-type (AGAA), AAGU or UUCG mutant strains confirmed the efficient 5′-end processing of the AAGU mutant and the strong processing defect of the UUCG mutant (Figure 2E). These results indicate that a hairpin capped by a AAGU tetraloop sequence can serve as an efficient recognition site for Rnt1p in vivo, even when placed on a substrate stem that normally contains a canonical AGNN tetraloop. In conclusion, AAGU tetraloop hairpins can be efficiently recognized by Rnt1p in vitro and in vivo, regardless of the stem sequence that they cap.
Overview of the solution structure of Rnt1p dsRBD/AAGU hairpin complex
Protein and RNA resonances in the Rnt1p dsRBD/AAGU complex were assigned following previously established protocols [50]. The protein-RNA interface was well defined by 43 intermolecular NOEs assigned from 2D filtered/edited NOESY [51] (Figure S1). The structure of the dsRBD-AAGU complex has backbone RMSDs to the mean of 0.55±0.11Å and 0.64±0.15Å for the dsRBD and AAGU hairpin, respectively (Figure 3A) (Table 1). The dsRBD adopts the standard α1β1β2β3 α2 fold [27] with the additional helix α3 packed against and stabilizing the C-terminal end of helix α1, as previously observed [33, 45]. The dsRBD binds to one face of the RNA and interacts primarily with the sugar-phosphate backbone in three successive regions: the tetraloop minor groove and top two base pairs with helix α1, the stem major groove with the N-terminal end of helix α2 and the β3-α2 loop, and the stem minor groove with the β1-β2 loop (Figure 3B). All of the bases in the tetraloop are in the anti conformation, and the RNA stem forms an A-form helix.
Table 1.
Structural statistics of Rnt1p dsRBD/AAGU hairpin complex
| Distance and dihedral restraints | Protein | RNA | |
|---|---|---|---|
| Total NOE restraints | 2095 | 695 | |
| Intraresidue | 842 | 243 | |
| Sequential | 498 | 325 | |
| Medium (i+2 to i+4) | 405 | 10 | |
| Long range (> i+4) | 350 | 117 | |
| Intermolecular NOE restraints | 45 | ||
| Hydrogen bond restraints | 80 | 72 | |
| RDC restraints | 83 | ||
| Dihedral angle restraints | 148 | 225 | |
| Structure statistics | |||
| (16 lowest energy structures) | |||
| No. of NOE violations>0.2Å | 0.125±0.22 | ||
| No. of NOE violations>0.5Å | 0 | ||
| No. of Dihedral violations>5º | 0 | ||
| No. of RDC violations>2(Hz) | 0 | ||
| RMSD of RDC, Hz | 0.4723±0.036 | ||
| RMSD from ideal covalent geometry | |||
| Bond lengths (Å) | 0.00337±0.00004 | ||
| Bond angles (°) | 0.757±0.004 | ||
| Impropers (°) | 0.364±0.011 | ||
| RMSD from the mean structure (Å) | Backbone | Heavy atoms | |
| Protein (366–448) | 0.55±0.11 | 0.90±0.12 | |
| RNA (3–14,19–30) | 0.65±0.15 | 0.61±0.12 | |
| Complex (3–14,19–30,366–448) | 0.61±0.11 | 0.80±0.11 | |
| Ramachandran statistics | |||
| Most favored regions | 59.5% | ||
| Additional allowed regions | 32.7% | ||
| Generously allowed regions | 5.8% | ||
| Disallowed regions | 1.9% | ||
Analysis of RDCs indicates that the dsRBD adopts the same conformation in both the AAGU and AGAA complexes
We compared the structures of dsRBDs in the dsRBD/AAGU and dsRBD/AGAA complexes using residual dipolar couplings (RDCs) [52, 53]. Structure calculations for the dsRBD/AAGU complex included 83 1H-15N RDCs in the final refinement step. For comparison purposes, we measured and analyzed a comparable set of 81 RDCs for the dsRBD/AGAA complex that had been previously determined and refined with 43 RDCs [33], and re-calculated the structure. We first evaluated the quality of the structures by back-calculating the RDCs from the RDC-refined dsRBD/AAGU and dsRBD/AGAA structures using the program PALES [54] (Figure 4A,B). The Q quality factors (Q) are 11.5% and 9.4% for dsRBD/AAGU and dsRBD/AGAA respectively, indicating an excellent agreement between the structures and their RDC data [53]. We next evaluated how similar the structures of the dsRBDs in the two complexes were to each other by back-calculating the set of RDCs for each complex using the structures of the other complex. Results for the lowest energy structure in each structure ensemble are shown in Figure 4C,D. R factors for the back-calculated dsRBD/AGAA and dsRBD/AAGU complexes are 0.98 and Q factors are <20% for both cases. Similar results are observed for each set of individual structures in the structure ensembles (Figure S2). These values indicate that the dsRBD conformations in the two complexes are highly similar. The dsRBDs in the two complexes have an RMSD between the two ensembles of 1.18 +/− 0.32Å for all heavy atoms (Figure 4E), which is within experimental error of the pairwise RMSDs of each ensemble.
Figure 4.
Correlation plots between experimental and back-calculated RDCs for the dsRBD/AAGU and dsRBD/AGAA hairpin complexes. (A) dsRBD/AAGU hairpin vs itself. (B) dsRBD/AGAA hairpin vs itself (C) dsRBD/AAGU hairpin vs dsRBD/AGAA hairpin (D) dsRBD/AGAA hairpin vs dsRBD AAGU hairpin. R factors, RMSD, and Q values (for C and D) are shown with the plots. Residues in (C) and (D) are shown as following: α1 (367–378), L1 (379–385), β1 (386–390), L2 (391–399), β2 (400–405), L3 (406–411), β3 (412–417), L4 (418–420), α2 (421–432), L5 (433–434) and α3 (435–448). (E) Superpositions of the ensembles of 16 lowest energy structures of the dsRBD in the dsRBD/AAGU hairpin (magenta) and dsRBD/AGAA hairpin (gold) complexes. The structures were aligned using the secondary structure elements, α1, β1, β2, β3, α2, and α3. See also Figure S2.
The AAGU tetraloop in the complex adopts a backbone fold similar to that of the AGAA tetraloop
The solution structure of the free AAGU tetraloop is substantially different from the A/uGNN fold [48] (Fig 5C) (see below). Surprisingly however, in the dsRBD/AAGU complex, the backbone fold and shape of the minor groove of the tetraloop is highly similar to that of the AGAA tetraloop (Figure 5A,B), with an RMSD for all backbone heavy atoms of 1.06 Å for the lowest energy structures (Figure 5B). As is the case for the AGNN tetraloops [33], the first two bases in the AAGU tetraloop, A15 and A16, stack on each other and point into the major groove away from the Rnt1p dsRBD helix α1 in the minor groove. The last two bases, G17 and U18 on the 3′ side, point into the minor groove and their backbones interact with helix α1 of the dsRBD (Figure 6). While all point into the minor groove, the positions of these bases, which are not conserved in AGNN tetraloops, differ somewhat among tetraloops.
Figure 5.
Comparison of the structures of the AAGU and AGAA tetraloops in the free and dsRBD bound states. Stereoviews are shown. (A) Superposition of the ensemble structures (16 lowest energy) of the dsRBD-bound AAGU (green) and dsRBD-bound AGAA (gray) tetraloops and the four stem base pairs below the tetraloops. The structures were aligned using residues 11–22. Superpositions of lowest energy structures of (B) dsRBD-bound AAGU tetraloop and dsRBD-bound AGAA tetraloop (RMSD 0.975Å). Nucleotides for dsRBD-bound AAGU are shown in red (A), orange (G), dark blue (C), and cyan (U); (C) Free AAGU tetraloop (gold) and dsRBD-bound AAGU (green) tetraloop (RMSD 1.64); (D) Free AGAA tetraloop (blue) and dsRBD-bound AGAA (gray) tetraloop (RMSD 0.99Å). Superimpositions for B–D include the tetraloops and closing base pair. RMSDs are for backbone heavy atoms. See also Figure S3.
Figure 6.
Interactions between the Rnt1p dsRBD and RNA. Steroviews of (A) the lowest energy structure of the dsRBD/AAGU complex and (B) helix α1 and side chain interactions in the tetraloop and top three base pairs. The dsRBD helix α, the β1-β2 loop, and β3-α2 loop are red and the rest of the dsRBD is magenta, the amino acids side chains that interact with RNA are shown in gray sticks, oxygen is red and nitrogen is blue. The RNA is green sticks with oxygens in red. Potential direct and water-mediated hydrogen bonds are indicated by blue dashed lines between heavy atoms. A hydrophobic interaction between Ala395 methyl and A4 H2 is shown with green dashed line. The interaction surfaces of dsRBD are shown in red. See also Figure S4.
Although the backbone fold is the same for the AGAA and AAGU tetraloops in complex with the dsRBD, the second base (A16) is in the anti conformation and its position is quite different from that of the syn G in the AGAA tetraloop. The syn conformation positions the G amino group within hydrogen bonding distance to one of the non-bridging oxygen atoms on its 5′ phosphate group, and therefore presumably stabilizes its stacking on the A (or U). An A in the second position does not have a proton donor at the same position as the G, and therefore cannot hydrogen bond to the backbone even in the syn conformation. Thus, in the complex, the stabilization conferred by a hydrogen bond to the backbone from a syn G at position 2 of the tetraloop does not appear to be required for the AAGU tetraloop to adopt the same backbone conformation as an AGAA tetraloop.
In the free AAGU tetraloop the first two As (A15 and A16) stack on each other and point into the major groove and the backbone turns after the second A, as is the case for the bound AAGU tetraloop, however the position of the backbone before the turn is substantially different (Figure 5C). On the 3′ side of the loop, the Watson-Crick face of G17 points into the minor groove and the base is nearly co-planar with A16, while U18 points up above G17 and out into the major groove [48]. In contrast, in the dsRBD/AAGU complex, the base of U18 is in the minor groove, and the positions of both G17 and U18 are significantly different, with the base of G17 pointing into the minor groove from near the top of the tetraloop and U18 below G17. Thus, the AAGU tetraloop in the hairpin undergoes a large conformational change upon binding to the dsRBD, to a conformation that presents a minor groove surface and backbone contacts to helix α1 that are highly similar to those in the AGAA tetraloop.
Since the dsRBD has the same binding affinity for the two hairpins, but the AAGU tetraloop undergoes a larger conformational change, we measured the binding by isothermal titration calorimetry (Figure S3). Although the two complexes have the same ΔG, the dsRBD/AAGU complex has larger negative values for both ΔH and ΔS. For dsRBD/AAGU and dsRBD/AGAA, ΔH = −1.42 × 104 vs −0.91 × 104 kcal/mole and ΔS = −21.8 and −3.94 kcal/moleK, respectively. These results indicate that while the AAGU/dsRBD complex undergoes a larger change in enthalpy upon complex formation, this is offset by a compensatory decrease in entropy.
Comparison of the protein-RNA interfaces in the Rnt1p dsRBD/AAGU and dsRBD/AGAA complexes
In both the dsRBD/AAGU and dsRBD/AGAA complexes, the β1-β2 loop contacts the stem minor groove of base pairs 2–5, the N-terminal end of helix α2 inserts into the major groove between base pairs 5–10, and helix α1 specifically recognizes the minor groove of the tetraloop and top two base pairs (Figure 3 and 6 and Table S1). Almost all of the contacts are to the phosphodiester backbone. Detailed comparison of the dsRBD/AAGU and dsRBD/AGAA complexes shows that the interactions between the protein and RNA stem are nearly identical (Figure 6 and S4). In the minor groove of the three base pairs adjacent to the tetraloop, the D367 side chain carboxyl group interacts with A20 2′OH and A21 2′OH through potential direct or water-mediated hydrogen bonds, and the side chain of K371 forms potential hydrogen bonds to A20 2′OH and A21O4′ for both complexes. On the 3′ side of the tetraloops, the guanidinium group of the R372 stacks onto the ring of the base G17 (in the AAGU tetraloop) or A17 (in the AGAA tetraloop) in the complexes (Figure 6 and S4). On the 5′ side of the tetraloop, the non-polar side chain of M368 stacks onto the A15 ribose and its sulfur group forms a potential water-mediated hydrogen bond with C14 O2. In the dsRBD/AGAA complex, R372 guanidinium group and S376 OH form hydrogen bonds with the 2′OH of A17 and A18 respectively (Figure S4), while in the AAGU complex the R372 guanidinium group forms a hydrogen bond with 2′OH of A15 and G17, and S376 OH forms a hydrogen bond with the 2′OH of U18 (Figure 6B). These small differences can be attributed to the difference in sequence at these positions. Neither the tetraloop sequence nor the top two base pairs are conserved, and consistent with this, no specific contacts to the bases were observed. Mutation of M368, which has a potential interaction with C14 O2, to alanine, does not affect binding [55]. Thus, the dsRBD recognizes the A/uGNN and AAGU tetraloops in the same way, by shape specific binding.
Conformational changes in the dsRBD upon binding to target RNA
Since the structure of the free Rnt1p dsRBD has been reported [45], we were able to examine any conformational changes that take place in the dsRBD upon binding to the AAGU hairpin as well as the AGAA hairpin in detail. We acquired a set of RDC data for the free dsRBD in solution. Of the NMR solution and two crystal structures (from one asymmetric unit) reported, the experimental RDCs fit best to the crystal structure chain A (PDB ID 1T4O) (Figure S5), so this structure was used for comparison to our bound complexes. To quantitatively compare the structures of the free and AAGU tetraloop bound dsRBDs, the experimental RDCs from the secondary structure elements β1, β2, β3, α1, and α2 for the dsRBD/AAGU complex were plotted versus the RDCs calculated from the crystal structure (Figure 7A). Helix α3 was excluded from this analysis, since it adopts three different orientations in the solution and two crystal structures [45]. The correlation gives a Q factor of 32%, but when the RDCs from helix α1 are deleted from the analysis, the Q factor decreases to 16%. Similar results were obtained for dsRBD bound to the AGAA hairpin (Figure 7B). When experimental RDCs from helix α1 only are compared (free dsRBD vs dsRBD/AAGU complex and dsRBD/AAGU complex vs dsRBD crystal chain A), poor correlations are obtained (Q = 32% and 49%, respectively) (Figure S5). Taken together, these data indicate that there is a significant change in helix α1 when the dsRBD binds to target RNA, consistent with structural differences observed by direct comparison of the structures as described below.
Figure 7.
Comparison of the structures of free dsRBD (PDB ID 1T4O Chain A) and RNA bound dsRBD. (A and B) Correlation plots between experimental RDCs for the dsRBD secondary structure elements in the (A) dsRBD/AAGU complex vs the RDCs calculated for the structure of the free dsRBD and (B) dsRBD/AGAA complex vs the RDCs calculated for the structure of the free dsRBD. For the correlation plots, the order tensor was determined from secondary structure elements α2,β1,β2,β3. RDC values are shown as black squares (α1) and red circles (α2,β1,β2,β3)). Q factors were calculated for secondary structure elements α1,α2,β1,β2,β3 (black numbers) and for α2,β1,β2,β3 (red numbers). (C) Superposition of the free dsRBD and the dsRBD bound to the AAGU hairpin. Superposition is on the secondary structure elements α2, β1, β2, and β3. (D) Close-up view showing the interaction of α1 with the minor groove of the AAGU tetraloop and comparison to the free dsRBD. The helices are shown as ribbons and the conserved sidechains M368, R372, and S376 in the free and bound dsRBD are shown as sticks. The RNA is shown as a solvent accessible surface. (E) Comparison of the angle of helix α1 in the free and dsRBD bound AAGU complex. The free dsRBD is cyan and the bound dsRBD in the AAGU hairpin complex is magenta. See also Figures S5 and S6.
Comparison of the structures of the free and AAGU hairpin bound dsRBD revealed that all of the regions of the dsRBD that interact with the RNA show significant changes in position between the free and bound dsRBD (Figure 7C). The β1-β2 loop, which inserts into the stem minor groove in the complex, points away approximately 6Å in the free dsRBD. The N-terminal end of helix α2 and the β3-α2 loop also shift to insert into the major groove. Helix α1 rotates about 18° (Figure 7E) and bends slightly from L374 to S376 (Figure 7D) to fit into the convex surface of the tetraloop. In the free dsRBD, helix α1 begins at N369, while in the complex it begins at L366. Side chains of M368, R372, and S376 all shift positions to align along one face of the helix to form van der Waals interactions and hydrogen bonds to 2′OH in the tetraloop minor groove (Figure 7D and 6A). Thus, helix α1 undergoes a change in helix length and bend and rotates 18° when it binds to the dsRNA hairpin substrate.
DISCUSSION
While most dsRBDs bind to dsRNA, the finding that the binding of Rnt1p dsRBD to A/uGNN hairpins is a major determinant of target selection provided the first clear example of a binding specificity for a dsRBD [10, 33, 39, 40]. Structural studies revealed that helix α1 recognizes the specific shape of this broad class of tetraloops [33]. Thus, the discovery of a second class of tetraloops that did not conform to this minimal consensus and had a different free tetraloop structure led to the proposal that Rnt1p bound these substrates in a different way [48]. Comparison of the dsRBD/AAGU structure, reported here, with the dsRBD/AGAA structure revealed that the AAGU hairpin has the same backbone fold in the complex as the AGNN tetraloops, and the dsRBD interactions and RDCs are the same for both complexes. We conclude that a conserved recognition mode is used for all Rnt1p substrates, regardless of their terminal loop sequences.
Conformational analysis of the free Rnt1p dsRBD [45] vs the dsRBD in the dsRBD/AAGU and dsRBD/AGAA [33] complexes revealed that helix α1 has a significant change in conformation upon binding to the tetraloop. We previously compared the structure of Rnt1p dsRBD in complex with the AGAA hairpin to that of a non-specific complex of Xlrpba dsRBD with dsRNA [33]. We noted that the two dsRBDs had a difference of ~15° in the orientation of helix α1, which positions the Rnt1p dsRBD helix α1 to fit perfectly into the minor groove of the AGNN tetraloop and the top of stem without changing the spacing of contacts to the minor groove and major groove, 1 and ½ turns away, respectively. Interestingly, the structure of the free Rnt1p dsRBD is similar to the structure of Xlrpba dsRBD in complex with dsRNA, with an RMSD of 0.41Å (Figure S6 A). Thus, the conformational change in helix α1 may be a key factor in the specific recognition of Rnt1p substrates.
Conformational change in the AAGU tetraloop upon dsRBD binding
For the AGAA tetraloop, the positions of the bases in the free vs bound are very similar, although there is some change in the backbone on the 3′ side of the loop (Figure 5D). Because the structures of the hairpins capped by AGAA, AGUU, and UGCA tetraloops, which are all substrates for Rnt1p, all had a similar fold with a syn G [43, 44] and this fold was retained in the dsRBD-AGAA complex [33], it was proposed that the dsRBD recognized the conserved shape of the tetraloop. It was therefore surprising to find that for the AAGU hairpin, the positions of the bases and the backbone trajectory both change significantly in the complex (Figure 5C). Thus, it appears that the AAGU tetraloop and helix α1 of the dsRBD co-operatively fold to form a specific complex with a conserved tetraloop fold. In the complexes, these two different tetraloops provide a rare example of two distinct RNA sequences that adopt the same functional fold [56].
While the conformational changes of the free vs bound AAGU tetraloop are larger than for the AGAA tetraloop, both the free and bound tetraloops have features in common that are likely essential for recognition and binding. In all cases, the backbone turns after the second nucleotide, and the position of the backbone in the turn is the same. On the 5′ side of the tetraloop, the first two bases point into the major groove and are stacked on each other. In the complexes, these two bases have no contacts to the dsRBD and the third base is positioned above the binding site. Finally, we note that the ACAA tetraloop has been proposed to have a similar conformation to the AGAA [57]. However, hairpins capped by ACAA are not cleaved by Rnt1p [43]. In the ensemble of ACAA tetraloop structures [57], about half have a backbone conformation at the turn that is very different from the AGAA and AAGU tetraloops, such that the helix α1 would not be able to insert into the minor groove.
Comparison to other dsRBD-RNA complexes
Although the dsRBD is the second most abundant family of RNA recognition motifs, structures of only a few dsRBDs in complex with RNA have been solved. There are now 6 proteins for which the structures of both the free dsRBD and the dsRBD in complex with RNA have been reported. In addition to Rnt1p dsRBD ([33, 45] and this work), these include Staufen dsRBD [28, 32], TAR RNA binding protein 2 (TRBP2) [35], Arabidopsis HYL1 dsRBD [58], ADAR2 dsRBD1 and dsRBD2 [36, 59], and Aquifex aeolicus RNase III [19, 31, 32, 37]. All of the free dsRBDs, with the exception of ADAR2 dsRBD1 and dsRBD2, superimpose well on each other and have virtually the same angle of helix α1 relative to the other secondary structure elements (Figure S6). Furthermore, the conformations of the free and RNA-bound dsRBDs of HYL1, TRBP, Staufen, A. aeolicus RNase III are the same, respectively, indicating that helix α1 does not change its conformation upon binding RNA. Of the complexes solved to date, only the dsRBD of Rnt1p and dsRBDs of ADAR2 have different helix α1 positions in complex with RNA relative to the free dsRBD (Figure S6 I,J). The dsRBDs of ADAR2 have recently been shown to bind dsRNA in a sequence specific manner, with base recognition via the minor groove from one amino acid each on helix α1 and the β1-β2 loop [36]. These two dsRBDs undergo relatively large conformational changes upon RNA binding, similar to Rnt1p. However, in contrast to Rnt1p dsRBD, the position of helix α1 in the free ADAR2 dsRBD1 and dsRBD2 is different compared to Xlrpba and the other dsRBDs (Figure S6).
Rnt1p requires specific tetraloop structures for substrate cleavage both in vivo and in vitro, while A. aeolicus RNase III, the homologue of E. coli RNase III, cleaves dsRNA in vitro with little apparent sequence specificity. Crystal structures of A. aeolicus RNase III in complex with RNA have revealed that, in addition to non-sequence-specific contacts to the backbone, three bases have direct contacts to the dsRBD, two in helix α1 and one in the β1-β2 loop [37]. One of these, Q157, is conserved in all bacterial RNase IIIs and deletion of it abolished cleavage and binding. The equivalent residue in Rnt1p does not contact the RNA. The other two residues, including A. aeolicus RNase III Q161 in helix α1, have been proposed to give rise to sequence specific binding [36]. Of the sequence- or tetraloop-specific dsRBD-RNA complexes solved to date, A. aeolicus RNase III is the only example where there is no significant change in the orientation of the dsRBD helix α1 upon binding to RNA.
In conclusion, our results show that the non-canonical AAGU tetraloop adopts a canonical fold upon binding to the dsRBD and that reorientation of helix α1 plays a major role in substrate-specific recognition. We propose that the Rnt1p dsRBD initially binds non-specifically to dsRNA and scans along the RNA until it reaches an A/uGNN or AAGU tetraloop. Helix α1 is locked into position by the tetraloop fold like a ball in glove, allowing subsequent positioning of the active site of Rnt1p at the cleavage site 14-16 bp away.
EXPERIMENTAL PROCEDURES
NMR sample preparation
The Rnt1p dsRBD, consisting of residues 366–453, was expressed as a glutathione transferase (GST) fusion protein and purified essentially as described [33] except for the addition of 1 mM DTT to the gel filtration purification step. Details of the purification are given in the Supplementary Methods. NMR samples were ~ 1 mM dsRBD in 20 mM sodium phosphate, pH 6.5, 150 mM NaCl, 1mM DTT. For NMR binding studies, the 32 nt AGAA (Figure 3A), AAGU, or UUCG hairpins were prepared by in vitro transcription using His6-tagged mutant T7 polymerase (P266L) [60] with a synthetic DNA template and purified on denaturing gels as described [43]. Unlabeled, uniformly 13C,15N-labeled, and A-, U-, G- or C-13C,15N-labeled AAGU hairpins were used for structure determination of the dsRBD/AAGU complex. The dsRBD/AAGU complex was prepared at a 1.1:1 ratio (RNA:protein) by adding the dsRBD to the RNA under dilute conditions followed by concentration in NMR buffer to 1 mM complex.
NMR spectroscopy and structure calculations
All NMR spectra were recorded at 25ºC on Bruker DRX 500 and 600 MHz spectrometers except for 2D NOESY spectra of exchangeable proton resonances of RNA, which were recorded at 10ºC. The assignments of the Rnt1p dsRBD in the complex were derived from the analysis of 3D CBCANH, 3D CBCA(CO)NH, 3D HCCH-TOCSY, 3D HCCH-COSY, 3D 13C-NOESY-HSQC and 3D 15N-NOESY-HSQC experiments [61–63] acquired on 13C,15N-labeled dsRBD in complex with unlabeled AAGU hairpin. The assignments of the AAGU hairpin were derived from 2D HCCH-COSY, 3D HCCH-TOCSY, 2D NOESY, 2D TOCSY [64] and a suite of 2D filtered/edited NOESY [51] using unlabeled dsRBD with 13C,15N-A-, G-, U-, or C-labeled AAGU. Finally, intermolecular NOEs were derived from 2D filtered/edited NOESY experiments as described [51]. One bond 1H-15N RDCs were measured from HSQC-IPAP experiments [65] in the presence and absence of C12E5/Hexanol [66] on a 600 MHz spectrometer. A total of 84, 81 and 83 RDCs were obtained for the free dsRBD, dsRBD/AGAA complex [33], and the dsRBD/AAGU complex, respectively. Structure calculations were performed essentially as described [51], and details are given in the Supplemental Experimental Procedures. For comparison purposes, the dsRBD/AGAA complex was re-refined with the larger set of RDCs (81 vs 43).
Determination of apparent KD from 1H-15N HSQC chemical shift titrations
The AAGU, AGAA and UUCG hairpin were individually titrated into 0.1 mM 15N-labeled dsRBD samples prepared in 500 μl high salt NMR buffer (20 mM sodium phosphate, pH 6.5, 300mM NaCl, 1mM DTT) up to RNA/protein ratios of 2:1 (Figure 1). The higher salt conditions (300mM NaCl), instead of the 150 mM NaCl used for the structure studies, were used in order to minimize non-specific binding. 1H-15N HSQC spectra were recorded for each titration point. The apparent dissociation constant Kd was obtained from changes in weighted chemical shift differences Δδ(N,H) = [(Δδ(HN)2+ (Δδ(NH)/4)2]½, assuming a one-site binding model. The titration curves were fitted globally using following equation:
| [ 67] |
where Δδ(N,H)max is the average chemical shift difference between the free and bound forms and P0, L0 are the total concentration of dsRBD and AAGU hairpin, respectively.
Cleavage kinetics assays
Full-length Rnt1p was expressed with an N-terminal His6-tag in BL-21 (DE3) Gold cells and purified on a GE Healthcare HisTrap Ni2+-affinity column, followed by anion exchange (HiTrap Q) and gel filtration (HiLoad S75) chromatography. Purified Rnt1p was concentrated to ~5 mg/mL. For kinetics assays, 52 nt RNA hairpins snR47-AGAA, snR47-AAGU, or snR47-UUCG (Figure 2A) were 32P end-labeled with T4 polynucleotide kinase. Cleavage reactions were prepared under single-turnover conditions with 25 nM RNA and 1 μM Rnt1p in 20 mM Tris, pH 8.0, 150 mM NaCl at 25°C, and reactions were initiated by adding MgCl2 to a final concentration of 5 mM. 10 μl aliquots were removed at time points of 0.25, 0.5, 1, 2, 4, and 8 minutes, and quenched with 10 μl of formamide gel-loading buffer with 20 mM EDTA. Samples were run on a 10% denaturing polyacrylamide gel (19:1 acrylamide:bisacrylamide), dried, and imaged on a Molecular Imager FX Pro Plus (Bio-Rad). Bands in the gel image corresponding to the uncleaved fraction of the substrate were quantified using ImageJ (NIH). Plotted values are the average of three experiments.
In vivo analysis of tetraloop mutants
Tetraloop mutants (AAGU or UUCG) were inserted into the tetraloop upstream from the snR47 snoRNA gene using the delitto perfetto method [68]. A core KanR-URA3 cassette was inserted between the second and third position of the snR47 snoRNA tetraloop, and double-stranded DNA oligonucleotides were used to excise the core sequence and introduce the AAGU or UUCG sequence. Genomic DNA sequences were confirmed by sequencing. Strains were grown in YPD and harvested, and Northern blot and primer extension analysis were performed as described [9, 55].
Accession numbers
Coordinates and restraints for the 16 lowest energy structures of the Rnt1p dsRBD/AAGU complex have been deposited in the Protein Data Bank, accession number 2LBS and chemical shifts have been deposited in the BioMagResBank, accession number 17574.
Supplementary Material
Acknowledgments
This work was supported by NIH grants GM37254 to J.F. and GM61518 to G.C. The authors thank Qi Zhang for helpful advice.
Footnotes
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