Residual dipolar coupling TOCSY for direct through space correlations of base protons and phosphorus nuclei in RNA

RNA structure determination by NMR

This chapter reviews the methodologies for RNA structure determination by liquid-state nuclear magnetic resonance (NMR). The routine production of milligram quantities of isotopically labeled RNA remains critical to the success of NMR-based structure studies. The standard method for the preparation of isotopically labeled RNA for structural studies in solution is in vitro transcription from DNA oligonucleotide templates using T7 RNA polymerase and unlabeled or isotopically labeled nucleotide triphosphates (NTPs). The purification of the desired RNA can be performed by either denaturing polyacrylamide gel electrophoresis (PAGE) or anion-exchange chromatography. Our basic strategy for studying RNA in solution by NMR is outlined. The topics covered include RNA resonance assignment, restraint collection, and the structure calculation process. Selected examples of NMR spectra are given for a correctly folded 30 nucleotide-containing RNA.

13C-detection in RNA bases: revealing structure-chemical shift relationships

The chemical shifts of the unprotonated carbons in the proton-deficient nucleobases of RNA are rarely reported, despite the valuable information that they contain about base-pairing and base-stacking. We have developed 13C-detected 2D-experiments to identify the unprotonated 13C in the RNA bases and have assigned all the base nuclei of uniformly 13C,15N-labeled HIV-2 TAR-RNA. The 13C chemical shift distributions revealed perturbations correlated with the base-pairing and base-stacking properties of all four base-types. From this work, we conclude that the information contained in the chemical shift perturbations within the base rings can provide valuable restraint information for solving RNA structures, especially in conformational averaged regions, where NOE-based information is not available.

Accurate measurement of 15N-13C residual dipolar couplings in nucleic acids

New 3D HCN quantitative J (QJ) pulse schemes are presented for the precise and accurate measurement of one-bond 15N1/9-13C1', 15N1/9-13C6/8, and 15N1/9-13C2/4 residual dipolar couplings (RDCs) in weakly aligned nucleic acids. The methods employ 1H-13C multiple quantum (MQ) coherence or TROSY-type pulse sequences for optimal resolution and sensitivity. RDCs are obtained from the intensity ratio of H1'-C1'-N1/9 (MQ-HCN-QJ) or H6/8-C6/8-N1/9 (TROSY-HCN-QJ) correlations in two interleaved 3D NMR spectra, with dephasing intervals of zero (reference spectrum) and approximately 1/(2J(NC)) (attenuated spectrum). The different types of 15N-13C couplings can be obtained by using either the 3D MQ-HCN-QJ or TROSY-HCN-QJ pulse scheme, with the appropriate setting of the duration of the constant-time 15N evolution period and the offset of two frequency-selective 13C pulses. The methods are demonstrated for a uniformly 13C, 15N-enriched 24-nucleotide stem-loop RNA sequence, helix-35psi, aligned in the magnetic field using phage Pf1. For measurements of RDCs systematic errors are found to be negligible, and experiments performed on a 1.5 mM helix-35psi sample result in an estimated precision of ca. 0.07 Hz for 1D(NC), indicating the utility of the measured RDCs in structure validation and refinement. Indeed, for a complete set of 15N1/9-13C1', 15N1/9-13C6/8, and 15N1/9-13C2/4 dipolar couplings obtained for the stem nucleotides, the measured RDCs are in excellent agreement with those predicted for an NMR structure of helix-35psi, refined using independently measured observables, including 13C-1H, 13C-13C and 1H-1H dipolar couplings.

NMR spectroscopy of RNA

NMR spectroscopy is a powerful tool for studying proteins and nucleic acids in solution. This is illustrated by the fact that nearly half of all current RNA structures were determined by using NMR techniques. Information about the structure, dynamics, and interactions with other RNA molecules, proteins, ions, and small ligands can be obtained for RNA molecules up to 100 nucleotides. This review provides insight into the resonance assignment methods that are the first and crucial step of all NMR studies, into the determination of base-pair geometry, into the examination of local and global RNA conformation, and into the detection of interaction sites of RNA. Examples of NMR investigations of RNA are given by using several different RNA molecules to illustrate the information content obtainable by NMR spectroscopy and the applicability of NMR techniques to a wide range of biologically interesting RNA molecules.

NMR structure of the 101-nucleotide core encapsidation signal of the Moloney murine leukemia virus

The full length, positive-strand genome of the Moloney Murine Leukemia Virus contains a "core encapsidation signal" that is essential for efficient genome packaging during virus assembly. We have determined the structure of a 101-nucleotide RNA that contains this signal (called mPsi) using a novel isotope-edited NMR approach. The method is robust and should be generally applicable to larger RNAs. mPsi folds into three stem loops, two of which (SL-C and SL-D) co-stack to form an extended helix. The third stem loop (SL-B) is connected to SL-C by a flexible, four-nucleotide linker. The structure contains five mismatched base-pairs, an unusual C.CG base-triple platform, and a novel "A-minor K-turn," in which unpaired adenosine bases A340 and A341 of a GGAA bulge pack in the minor groove of a proximal stem, and a bulged distal uridine (U319) forms a hydrogen bond with the phosphodiester of A341. Phylogenetic analyses indicate that these essential structural elements are conserved among the murine C-type retroviruses.

Stem of SL1 RNA in HIV-1: structure and nucleocapsid protein binding for a 1 x 3 internal loop

The 5'-leader of HIV-1 RNA controls many viral functions. Nucleocapsid (NC) domains of gag-precursor proteins select genomic RNA for packaging by binding several sites in the leader. One is likely to be a stem defect in SL1 that can adopt either a 1 x 3 internal loop, SL1i (including G247, A271, G272, G273) or a 1 x 1 internal loop (G247 x G273) near a two-base bulge (A269-G270). It is likely that these two conformations are both present and exchange readily. A 23mer RNA construct described here models SL1i and cannot slip into the alternate form. It forms a 1:1 complex with NCp7, which interacts most strongly at G247 and G272 (K(d) = 140 nM). This demonstrates that a linear G-X-G sequence is unnecessary for high-affinity binding. The NMR-based structure shows an easily broken G247:A271 base pair. G247 stacks on both of its immediate neighbors and A271 on its 5'-neighbor; G272 and G273 are partially ordered. A bend in the helix axis between the SL1 stems on either side of the internal loop is probable. An important step in maturation of the virus is the transition from an apical loop-loop interaction to a dimer involving intermolecular interactions along the full length of SL1. A bend in the stem may be important in relieving strain and ensuring that the strands do not become entangled during the transition. A stem defect with special affinity for NCp7 may accelerate the rate of the dimer transformation. This complex could become an important target for anti-HIV drug development, where a drug could exert its action near a high-energy intermediate on the pathway for maturation of the dimer.

Sensitive through-space dipolar correlations between nuclei of small organic molecules by partial alignment in a deuterated liquid solvent

Through-space residual dipolar correlations in NMR spectra can be measured between nuclei of small organic molecules by partially aligning them with respect to the magnetic field in a pure deuterated liquid solvent, 4-pentyl-4'-cyanobiphenyl. A simple temperature change of this liquid phase enables spectra to be compared between samples under isotropic tumbling conditions and weakly oriented anisotropic states. This should provide access of a number of small nonpolar molecules to more sensitive through-space nuclear correlations than possible through NOE experiments, depending on the net orientation of specific nuclear pairs with respect to the magnetic field and the specific coherence transfers employed.