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Biophys J, November 2002, p. 2812-2825, Vol. 83, No. 5


and
*Department of Biochemistry and Biophysics, Arrhenius Laboratories,
Stockholm University, S-106 91 Stockholm, Sweden;
Structural Biochemistry, Department of Biotechnology,
Stockholm Center for Physics, Astronomy, and Biotechnology, The Royal
Institute of Technology, S-106 91 Stockholm, Sweden; and
Department of Medical Biophysics, Karolinska Institute,
S-171 77 Stockholm, Sweden
Tyrosine ring dynamics of the gastrointestinal hormone
motilin was studied using two independent physical methods:
fluorescence polarization anisotropy decay and NMR relaxation. Motilin,
a 22-residue peptide, was selectively 13C labeled in the
ring
-carbons of the single tyrosine residue. To eliminate effects
of differences in peptide concentration, the same motilin sample was
used in both experiments. NMR relaxation rates of the tyrosine ring
C
-H
vectors, measured at four magnetic
field strengths (9.4, 11.7, 14.1, and 18.8 Tesla) were used to map the
spectral density function. When the data were analyzed using dynamic
models with the same number of components, the dynamic parameters from
NMR and fluorescence are in excellent agreement. However, the estimated
rotational correlation times depend on the choice of dynamic model. The
correlation times estimated from the two-component model-free approach
and the three-component models were significantly different (1.7 ns and
2.2 ns, respectively). Various earlier studies of protein dynamics by
NMR and fluorescence were compared. The rotational correlation times
estimated by NMR for samples with high protein concentration were on
average 18% longer for folded monomeric proteins than the
corresponding times estimated by fluorescence polarization anisotropy
decay, after correction for differences in viscosity due to temperature
and D2O/H2O ratio.
Biophys J, November 2002, p. 2812-2825, Vol. 83, No. 5
© 2002 by the Biophysical Society 0006-3495/02/11/2812/14 $2.00
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