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. 2019 Sep;16(9):1086-1092.
doi: 10.1080/15476286.2018.1536591. Epub 2018 Oct 30.

Observation of preQ1-II riboswitch dynamics using single-molecule FRET

Affiliations

Observation of preQ1-II riboswitch dynamics using single-molecule FRET

Chandani Warnasooriya et al. RNA Biol. 2019 Sep.

Abstract

PreQ1 riboswitches regulate the synthesis of the hypermodified tRNA base queuosine by sensing the pyrrolopyrimidine metabolite preQ1. Here, we use single-molecule FRET to interrogate the structural dynamics of apo and preQ1-bound states of the preQ1-II riboswitch from Lactobacillus rhamnosus. We find that the apo-form of the riboswitch spontaneously samples multiple conformations. Magnesium ions and preQ1 stabilize conformations that sequester the ribosome-binding site of the mRNA within the pseudoknotted structure, thus inhibiting translation initiation. Our results reveal that folding of the preQ1-II riboswitch is complex and provide evidence favoring a conformational selection model of effector binding by riboswitches of this class.

Keywords: RNA dynamics; Riboswitch; conformation selection; smFRET.

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Figures

Figure 1.
Figure 1.
Queuosine biosynthesis, the preQ1-II riboswitch structure and experimental construct for smFRET. (a) The queuosine (Q) base is a hypermodified base that is widespread in prokaryotes and eukaryotes. However, Q is only synthesized de novo in bacteria. Q production starts with GTP and proceeds by several enzymatic steps (arrow) to the last free intermediate preQ1 (7-aminomethyl-7-deazaguanine), which is then inserted into specific tRNAs followed by additional in situ modifications [16]. (b) Ribbon diagram depicting the global HLout pseudoknot fold of the preQ1-II riboswitch from Lactobacillus rhamnosus (Lrh) (PDB entry 4jf2) [13]. The riboswitch comprises three co-axially stacked pairing regions (P1, P2 and P3) with a fourth (P4) flanking the P2-P3 interface. The three-helix junction binds preQ1 to complete P2-P3 coaxial helical stacking. Two nearby Mg2+ ions are shown as purple spheres. The co-crystal structure reveals that the pseudoknot buries the entire Shine-Dalgarno sequence (SDS). The SDS nucleotides are filled (yellow) and preQ1 is drawn as a CPK model (green). Pairing (P) and (J) junction regions are shown in distinct colors. (c) Secondary structure of the wild-type Lrh preQ1-II riboswitch construct used for this investigation based on the known crystal structure in b. The P1 helix is dispensable for effector sensing and was modified to hybridize with a biotinylated DNA oligonucleotide (inset box). The 3´-end comprises the wild-type sequence of the naturally occurring, downstream queT gene that is regulated by the riboswitch. The start codon (AUG) is highlighted. FRET (Dy547) and acceptor (Cy3) labels are depicted as green and red stars.
Figure 2.
Figure 2.
PreQ1 stabilizes preQ1-II riboswitch conformations that sequester the SD sequence into intramolecular core structure. Histograms compiled from hundreds of smFRET traces show the distribution of the FRET values for the riboswitch imaged in the absence of Mg2+. PreQ1 concentration was varied as follows: (a) no preQ1, (b) 0.1 μM, (c) 0.3 μM, (d) 0.5 μM, (e) 1.0 μM and (f) 10 μM. Yellow lines represent individual Gaussian fits; black lines indicate the sum of Gaussians. The fraction of the riboswitch in each FRET state derived from Gaussian fits is shown next to respective individual Gaussian peaks. N equals the number of single-molecule traces compiled.
Figure 3.
Figure 3.
Apo form of the preQ1-II riboswitch imaged in the absence of Mg2+ and preQ1 spontaneously fluctuates between low (~ 0.35) and high (~ 0.7) FRET states. (a) Representative smFRET trace showing fluctuations between the 0.35 and 0.7 FRET states. Observed intensities of donor and acceptor fluorescence and the calculated apparent FRET efficiency are shown in blue, red, and black, respectively. The Hidden Markov Model fit is shown in magenta. (b) Transition density plot (TDP) analysis of 1,277 fluctuations between different FRET states in 126 HMM-idealized FRET traces. The frequency of transitions from the starting FRET value (x axis) to the ending FRET value (y axis) is represented by a heat map. The range of FRET efficiencies from 0 to 1 was separated into 200 bins. The resulting heat map was normalized to the most populated bin in the plot; the lower- and upper-bound thresholds were set to 10% and 100% of the most populated bin.
Figure 4.
Figure 4.
The Lrh preQ1-II riboswitch senses the preQ1 concentration to yield a compact fold. The fraction of the riboswitch in a compact conformation, determined by the area under the 0.7 FRET peak in Fig (2a-f), was plotted as a function of preQ1 concentration and fitted to a hyperbola (red line; y = A*[preQ1]/(EC50+[preQ1])+ B, where EC50 is the half maximal effective concentration of preQ1 and B is the fraction of 0.7 FRET observed in the absence of preQ1).
Figure 5.
Figure 5.
Mg2+ stabilizes Lrh preQ1-II riboswitch conformations that sequester the SD sequence into intramolecular core structure. Histograms compiled from hundreds of smFRET traces show the distribution of the FRET values for the riboswitch imaged in the presence of 0.5 mM Mg2+ (a-b) or 6 mM Mg2+(c-d). Measurements were taken either in the absence (a,c) or the presence of 1 μM preQ1 (b,d). Yellow lines represent individual Gaussian fits; black lines indicate the sum of Gaussians. The fraction of the riboswitch in each FRET state derived from Gaussian fits is shown next to respective individual Gaussian peaks. N equals the number of single-molecule traces compiled.

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