International
Tables for
Crystallography
Volume F
Crystallography of biological macromolecules
Edited by M. G. Rossmann and E. Arnold

International Tables for Crystallography (2006). Vol. F. ch. 19.7, pp. 466-467   | 1 | 2 |

Section 19.7.5. NMR studies of rate processes and conformational equilibria in three-dimensional macromolecular structures

K. Wüthricha

a Institut für Molekularbiologie und Biophysik, Eidgenössische Technische Hochschule-Hönggerberg, CH-8093 Zürich, Switzerland

19.7.5. NMR studies of rate processes and conformational equilibria in three-dimensional macromolecular structures

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Similar to the aforementioned hydration studies, information on intramolecular rate processes in macromolecular structures cannot usually be obtained from the standard protocol for NMR structure determination (Fig. 19.7.2.1[link]), but results from additional experiments. The complementarity of such NMR information to crystallographic data is well illustrated by the `ring flips' of phenylalanine and tyrosine (Wüthrich, 1986[link]). The observation of these ring-flipping motions in the basic pancreatic trypsin inhibitor (BPTI) (Wüthrich & Wagner, 1975[link]) was a genuine surprise for the following reasons. In the refined X-ray crystal structure of BPTI, the aromatic rings of phenylalanine and tyrosine are among the side chains with the smallest temperature factors. For each ring, the relative values of the B factors increase toward the periphery, so that the largest positional uncertainty is indicated for carbon atom 4 on the symmetry axis through the Cβ—C1 bond, rather than for the carbon atoms 2, 3, 5 and 6 (Fig. 19.7.5.1[link]), which undergo extensive movements during the ring flips. Theoretical studies then showed that the crystallographic B factors sample multiple rotation states about the Cα—Cβ bond, whereas the ring flips about the Cβ—C1 bond seen by NMR are very rapid 180° rotations connecting two indistinguishable equilibrium orientations of the ring. The B factors do not manifest these rotational motions because the populations of all non-equilibrium rotational states about the Cβ—C1 bond are vanishingly small. The ring-flip phenomenon is now a well established feature of globular proteins, manifesting ubiquitous low-frequency internal motions with activation energies of 60–100 kJ mol−1, amplitudes of [\lower2pt\hbox{${\buildrel \displaystyle \gt \over \sim}$} 1.0] Å and activation volumes of about 50 Å3 (Wagner, 1980[link]), and involving concerted displacement of numerous groups of atoms (Fig. 19.7.5.1[link]).

[Figure 19.7.5.1]

Figure 19.7.5.1| top | pdf |

180° ring flips of tyrosine and phenylalanine about the Cβ—C1 bond. On the left, the atom numbering is given and the [\chi^{2}] rotation axis is identified with an arrow. The drawing on the right presents a view along the Cβ—C1 bond of a flipping ring in the interior of a protein, where the broken lines indicate a transient orientation of the ring plane during the flip. The circles represent atom groups near the ring, and arrows indicate movements of atom groups during the ring flip (Wüthrich, 1986[link]).

References

First citation Qian, Y. Q., Billeter, M., Otting, G., Müller, M., Gehring, W. J. & Wüthrich, K. (1989). The structure of the Antennapedia homeodomain determined by NMR spectroscopy in solution: comparison with prokaryotic repressors. Cell, 59, 573–580.Google Scholar
First citation Wagner, G. (1980). Activation volumes for the rotational motion of interior aromatic rings in globular proteins determined by high resolution 1H NMR at variable pressure. FEBS Lett. 112, 280–284.Google Scholar
First citation Wüthrich, K. (1986). NMR of proteins and nucleic acids. New York: Wiley.Google Scholar
First citation Wüthrich, K. & Wagner, G. (1975). NMR investigations of the dynamics of the aromatic amino acid residues in the basic pancreatic trypsin inhibitor. FEBS Lett. 50, 265–268.Google Scholar








































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