Accurate nucleic acid concentrations by nuclear magnetic resonance.

Determination of the concentration of biochemical samples often yields values with uncertainties of 10-20% or more. This paper details a protocol for use with 500- to 600-MHz NMR spectrometers to measure approximately 1mM concentrations within +/-1-3% accuracy. With suitable precautions, all compounds have equal NMR "absorption coefficients" for protons. About 2mg of sample are needed for proteins and nucleic acids with MW=5000, although less accurate determinations could be made with smaller amounts. The technique utilizes standardized internal reference reagent compounds, cacodylic acid or 3-(trimethylsilyl)propionic-2,2,3,3-d(4) acid sodium salt. Spectra were signal-averaged using long interpulse delays so that integrals of nonexchangeable protons could be quantified relative to the reference standard. Accurate determinations require careful optimization of the homogeneity of the magnetic field and meticulous attention to sample preparation and spectral processing. The main source of error is usually the accuracy of micropipets. If sample preparation errors could be eliminated, the lower limit of accuracy with the current generation of NMR spectrometers is probably near 0.4%. However, this would require >99.5% sample purity. Methods are described to establish the concentration of the standards, and applications are illustrated with DNA mono- and oligonucleotides. Similar procedures should apply to proteins, polysaccharides, and other biomolecules, with about the same accuracy and precision.

Structure of SL4 RNA from the HIV-1 packaging signal.

The NMR-based structure is described for an RNA model of stem-loop 4 (SL4) from the HIV-1 major packaging domain. The GAGA tetraloop adopts a conformation similar to the classic GNRA form, although there are differences in the details. The type II tandem G.U pairs have a combination of wobble and bifurcated hydrogen bonds where the uracil 2-carbonyl oxygen is hydrogen-bonded to both G,H1 and G,H2. There is the likelihood of a Na(+) ion coordinated to the four carbonyl oxygens in the major groove for these G.U pairs and perhaps to the N7 lone pairs of the G bases as well. A continuous stack of five bases extends over nearly the whole length of the stem to the base of the loop in the RNA 16mer: C15/U14/G13/G5/C6. There is no evidence for a terminal G.A pair; instead, G1 appears quite unrestrained, and A16 stacks on both C15 and G2. Residues G2 through G5 exhibit broadened resonances, especially G3 and U4, suggesting enhanced mobility for the 5'-side of the stem. The structure shows G2/G3/U4 stacking along the same strand, nearly isolated from interaction with the other bases. This is probably an important factor in the signal broadening and apparent mobility of these residues and the low stability of the 16mer hairpin against thermal denaturation.

Three-dimensional folding of an RNA hairpin required for packaging HIV-1.

An NMR-based structure is presented for a 20 mer hairpin model of the SL3 stem-loop from the HIV-1 packaging signal. The stem has an A-family structure. However, the GGAG tetraloop appears to be flexible with the second (G10) and fourth (G12) bases extruded from the normal stacking arrangement. The A-base (A11) occupies a cavity large enough for it to jump rapidly between stacking upon G9 (in the loop) and G13 (from the base-pair adjacent to the loop). The H-bonding loci of G10, A11, and G12 are unoccupied in the free RNA structure. The loop should be easily adaptable to binding by the HIV-1 nucleocapsid protein or loop receptors.

Structure determination of [d(ATATATAUAT)]2 via two-dimensional NOE spectroscopy and molecular dynamics calculations.

Proton homonuclear two-dimensional (2D) NOE spectra were obtained for the decamer [d(ATATATAUAT)]2 as a function of mixing time, and proton resonance assignments were made. Quantitative assessment of the 2D NOE cross-peak intensities was used in conjunction with the program MARDIGRAS, which entails a complete relaxation matrix analysis of the 2D NOE peak intensities, to obtain a set of upper and lower bound interproton distance constraints. The analysis with MARDIGRAS was carried out using three initial models: A-DNA, B-DNA and Z-DNA. The distance constraints determined were essentially the same regardless of initial structure. These experimental structural constraints were used with restrained molecular dynamics calculations to determine the solution structure of the decamer. The molecular dynamics program AMBER was run using A-DNA or B-DNA as starting model. The root-mean-square (rms) difference between these two starting models is 0.504 nm. The two starting models were subjected to 22.5 ps of restrained molecular dynamics calculations. The coordinates of the last 10.5 ps of the molecular dynamics runs were averaged to give two final structures. MDA and MDB. The rms difference between these two structures is 0.09 nm, implying convergence of the two molecular dynamics runs. The 2D NOE spectral intensities calculated for the derived structures are in good agreement with experimental spectra, based on sixth-root residual index analysis of intensities. A detailed examination of the structural features suggests that while the decamer is in the B-family of DNA structures, many torsion angle and helical parameters alternate from purine to pyrimidine, with kinks occurring at the U-A steps.