S. Dong et al.
sffiffiffiffiffiffiffiffiffiffiffiffiffiffi sffiffiffiffiffiffiffiffiffiffiffiffiffiffi
(
)
pffiffiffi
Experimental Section
3
4
Að0Þ
Að0Þ
tc ¼ 1:19 ꢀ 10ꢁ9
ꢀ
þ
ꢁ 2 ꢀ DHppð0Þ
Aðþ1Þ
Aðꢁ1Þ
All the experimental procedures and are reported in the Supporting In-
formation.
ð1Þ
Calculated values of the peak-to-peak width of the center
line (DHpp(0)) and the correlation time (tc) by varying the
temperatures are shown in Table S1 in the Supporting Infor-
mation. The sensitivity of the ESR spectrum to the spin-
label mobility is influenced by both the rate and amplitude
of the motion. Consequently, a clear correlation between
ESR spectral shape and conformational status of the triple
helix could be established. In Figure 3, DHpp(0) and tc are
shown with increasing temperatures. The changes of these
values reflect the thermal transition from triple helix to the
unfolded state, which are consistent with the CD spectra.
From 5 to 408C, the tc values decrease almost linearly from
1.21865 to 0.19669 ns and DHpp(0) values also show a linear
decrease from 0.20935 to 0.12818 mT, proving the unfolding
process of the triple helix and the related weakening of the
restricted local structure and spin–spin interactions. The re-
lationship between tc and temperature can be viewed as
ESR melting transition of the triple helix of peptide 9. For
comparative analysis of thermal transitions monitored by
CD and ESR very slow heating rates (128Chꢁ1) were ap-
plied as required for almost equilibrium transitions of CMPs
even at high peptide concentrations.[14b,19]
Acknowledgements
The authors want to thank Prof. Claudio Toniolo (University of Padova,
Italy) for the kind advice in the ESR experiments. This work was in part
supported by the grant from National Natural Science Foundation of
China (No. 30870526).
Keywords:
(2S,4R)-aminoproline
·
collagen
·
ESR
spectroscopy · proteins · site-directed spin labeling
339; b) J. Engel, H. P. Bꢁchinger, in Collagen: Primer in Structure,
Processing and Assembly, Vol. 247 (Eds.: J. Brinckmann, H. Not-
bohm, P. K. Muller), Springer, Heidelberg, 2005, pp. 7–33; c) M.
[3] M. D. Shoulders, K. A. Satyshur, K. T. Forest, R. T. Raines, Proc.
[5] C. S. Klug, J. B. Feix, in Methods in Cell Biology, Vol. 84 (Eds.: J. C.
John, H. W. Detrich III), Academic Press, 2008, pp. 617–658.
[6] M. Kuemin, Y. A. Nagel, S. Schweizer, F. W. Monnard, C. Ochsen-
In the first derivative of tc versus T curve, a transition is
observed from 23.1–31.58C (Figure 3C). Deconvolution of
this temperature excursion curve allows the identification of
two transition temperatures. The first Tm of 23.18C is signifi-
cantly lower than the Tm of 32.28C derived from CD spec-
troscopy. It could be interpreted as a pretransition of mis-
aligned trimeric species present at equilibrium with correctly
registered chains in self-assembled CMPs triple helices. Such
pretransitions of CMP triple helices have been identified by
NMR spectroscopy studies on the dynamics of thermal un-
folding of CMP triple helices.[20] The unfolded monomers re-
align into correctly registered triple helices in a continuous-
equilibrium process. The second transition midpoint Tm of
31.58C is practically identical to the Tm monitored by CD,
which should reflect the transition midpoint of the correctly
aligned triple helices. The normalized thermal unfolding
curve suggests that the exact Tm is at 27.58C. Little fluctua-
tion of the tc values was observed confirming complete un-
folding of triple helix at higher temperatures as also ob-
served in the CD melting curve.
[7] U. Kusebauch, S. A. Cadamuro, H. J. Musiol, L. Moroder, C.
[9] N. Van Eps, L. L. Anderson, O. G. Kisselev, T. J. Baranski, W. L.
[11] C. Dockter, A. Volkov, C. Bauer, Y. Polyhach, Z. Joly-Lopez, G.
[14] a) S. Boudko, S. Frank, R. A. Kammerer, J. Stetefeld, T. Schulthess,
Engel, in Protein Folding Handbook (Eds.: J. Buchner, T. Kiefhab-
er), Wiley-VCH, Weinheim, 2005, pp. 1059–1110.
[16] J. C. McNulty, D. A. Thompson, M. R. Carrasco, G. L. Millhauser,
[18] P. G. Fajer, in Encyclopedia of Analytical Chemistry, Wiley, Chiches-
ter, 2006, pp. 1–37.
[20] a) K. Kawahara, N. Nemoto, D. Motooka, Y. Nishi, M. Doi, S.
Uchiyama, T. Nakazawa, Y. Nishiuchi, T. Yoshida, T. Ohkubo, Y.
The results obtained with the spin-labeled CMP fully con-
firm the usefulness of ESR spectroscopy for measuring the
thermodynamic stability of collagen triple helices. Com-
pared to CD spectroscopy, it could allow the monitoring of
the dynamics of CMP triple helix unfolding similar to very
detailed NMR spectroscopy experiments[20] and thus provide
further insights into collagen structure, stability and folding
dynamics.
Received: August 22, 2013
Published online: November 22, 2013
17682
ꢀ 2013 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim
Chem. Eur. J. 2013, 19, 17679 – 17682