Nuclear Magnetic Resonance (NMR) Spectroscopy for Monitoring Molecular Dynamics in Solution

Biological macromolecules exhibit a wide range of dynamic motions. Analysis of relaxation rates of NMR signals allows these motions to be characterized throughout a macromolecule at an atomic level of detail.

Keywords: NMR; heteronuclear; relaxation; dynamics; model-free

Figure 1. Motion of a single bond vector expressed as autocorrelation and spectral density functions. The time domain of the autocorrelation function, C(t), and the frequency domain of the spectral density function, J(), interconvert upon a real Fourier transformation. In both panels, the motion shown results from an overall rotational correlation time of 4 ns, an internal correlation time of 100 ps, and an order parameter (S2) of 0.5. (a) The blue line corresponds to the autocorrelation function for overall tumbling; the red line corresponds to internal reorientation in the molecular frame. The dashed line corresponds to the composite autocorrelation function resulting from both overall and internal motions. Functions are normalized to a value of 1 at time zero. (b) The spectral density function, J(), is decomposed into its overall and internal components, shown in blue and red, respectively. Vertical lines are drawn at frequencies sampled by 15N and/or 13C relaxation at a field strength corresponding to a 1H frequency of 600 MHz. Short and long dashed lines correspond to frequencies probed by 15N and 13C relaxation, respectively. Green lines are drawn at the zero and 1H frequencies, and are sampled by both nuclei.
Figure 2. Model-free order parameters for backbone and side-chain bond vectors in the human ubiquitin protein. Backbone amide S2 values are derived from 15N relaxation and are shown as solid circles. Methyl side-chain order parameters are derived from 13C relaxation and are shown as open circles and triangles. Each methyl side-chain order parameter corresponds to the threefold symmetry axis, which extends from the C–CH3 bond vector (see Lee and Wand, (1999); Lee et al., 1999).
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 References
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 Further Reading
    Engelke J and Rüterjans H (1998) Dynamics of -CH and -CH2 groups of amino acid side chains in proteins. Journal of Biomolecular NMR 11: 165–183.
    Fischer MWF, Zeng L, Pang Y et al. (1997) Experimental characterization of models for backbone picosecond dynamics in proteins. Quantification of NMR auto- and cross-correlation relaxation mechanisms involving different nuclei of the peptide plane. Journal of the American Chemical Society 119: 12629–12642.
    Lee LK, Rance M, Chazin WJ and Palmer AG (1997) Rotational diffusion anisotropy of proteins from simultaneous analysis of 15N and 13C nuclear spin relaxation. Journal of Biomolecular NMR 9: 287–298.
    LeMaster DM (1999) NMR relaxation order parameter analysis of the dynamics of protein side chains. Journal of the American Chemical Society 121: 1726–1742.
    Lipari G and Szabo A (1982) Model-free approach to the interpretation of nuclear magnetic resonance relaxation in macromolecules. 2. Analysis of experimental results. Journal of the American Chemical Society 104: 4559–4570.
    Loria JP, Rance M and Palmer AG (1999) A relaxation-compensated Carr–Purcell–Meiboom–Gill sequence for characterizing chemical exchange by NMR spectroscopy. Journal of the American Chemical Society 121: 2331–2332.
    Peng JW and Wagner G (1994) Investigation of protein motions via relaxation measurements. Methods in Enzymology 239: 563–596.
    Schneider DM, Dellwo MJ and Wand AJ (1992) Fast internal main-chain dynamics of human ubiquitin. Biochemistry 31: 3645–3652.
    Schurr JM, Babcock HP and Fujimoto BS (1994) A test of the model-free formulas. Effects of anisotropic rotational diffusion and dimerization. Journal of Magnetic Resonance, Series B 105: 211–224.
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Lee, Andrew L, and Wand, A Joshua(Apr 2001) Nuclear Magnetic Resonance (NMR) Spectroscopy for Monitoring Molecular Dynamics in Solution. In: eLS. John Wiley & Sons Ltd, Chichester. http://www.els.net [doi: 10.1038/npg.els.0003104]