Abstract

Selective stable isotope labeling has transformed structural and dynamics analysis of RNA by NMR spectroscopy. These methods can remove 13C-13C dipolar couplings that complicate 13C relaxation analyses. While these phenomena are well documented for sites with adjacent 13C nuclei (e.g. ribose C1′), less is known about so-called isolated sites (e.g. adenosine C2). To investigate and quantify the effects of long-range (> 2 Å) 13C-13C dipolar interactions on RNA dynamics, we simulated adenosine C2 relaxation rates in uniformly [U-13C/15N]-ATP or selectively [2-13C]-ATP labeled RNAs. Our simulations predict non-negligible 13C-13C dipolar contributions from adenosine C4, C5, and C6 to C2 longitudinal (R1) relaxation rates in [U-13C/15N]-ATP labeled RNAs. Moreover, these contributions increase at higher magnetic fields and molecular weights to introduce discrepancies that exceed 50%. This will become increasingly important at GHz fields. Experimental R1 measurements in the 61 nucleotide human hepatitis B virus encapsidation signal ε RNA labeled with [U-13C/15N]-ATP or [2-13C]-ATP corroborate these simulations. Thus, in the absence of selectively labeled samples, long-range 13C-13C dipolar contributions must be explicitly taken into account when interpreting adenosine C2 R1 rates in terms of motional models for large RNAs.

Highlights

  • RNAs are important macromolecules that function in a wide range of cellular roles (Cech and Steitz 2014; Mortimer et al 2014; Sharp 2009)

  • We recently showed that purine C8 may experience non-negligible dipolar contributions to R­ 1 relaxation from non-adjacent coupling partners (Nam et al 2020)

  • We demonstrate that the removal of long-range 13C-13C dipolar coupling partners reveals discrepancies in measured adenosine C2 ­R1 values between uniformly and selectively labeled samples

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Summary

Introduction

RNAs are important macromolecules that function in a wide range of cellular roles (Cech and Steitz 2014; Mortimer et al 2014; Sharp 2009). RNAs are dynamic and can sample numerous conformations on various time scales that might be important for function (Zhao et al 2017; Marušič et al 2019). Three commonly measured dynamics parameters are the longitudinal (­ R1) and transverse ­(R2) relaxation rates and the heteronuclear Overhauser effect (hNOE) (Marušič et al 2019; Palmer 2004; Wagner 1993). The ­R1 rate measures the return of the longitudinal magnetization to thermal equilibrium whereas R­ 2 measures the decay of transverse magnetization, and the hNOE measures the change in heteronuclear spin magnetization in response to saturating proton spins (Yamazaki et al 1994; Peng and Wagner 1992; Abragam 1961)

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