Cold denaturation of a synthetic collagen mimetic

Thermal Destabilization of Collagen Matrix Hierarchical Structure by Freeze/Thaw

This study aims to characterize and understand the effects of freezing on collagen structures and functionality. Specifically, thermodynamic destabilization of collagen at molecular- and fibril-levels by combination of low temperatures and freezing were experimentally characterized using modulated differential scanning calorimetry. In order to delineate the effects of sub-zero temperature and water-ice phase change, we hypothesized that the extent of destabilization can be determined based on post-thaw heat induced thermal denaturation of collagen. It is found that thermal denaturation temperature of collagen in hydrogel decreases by 1.4–1.6°C after freeze/thaw while no such decrease is observed in the case of molecular solution. The destabilization is predominantly due to ice formation. Exposure to low temperatures in the absence of ice has only minimal effect. Calorimetry measurements combined with morphological examination of collagen matrices by scanning electron microscopy suggest that freezing results in destabilization of collagen fibrils due to expansion of intrafibrillar space by ice formation. This fibril-level damage can be alleviated by use of cryoprotectant DMSO at concentrations as low as 0.5 M. A theoretical model explaining the change in collagen post-thaw thermal stability by freezing-induced fibril expansion is also proposed.

The unusually stable coiled-coil domain of COMP exhibits cold and heat denaturation in 4-6 M guanidinium chloride

A high thermal stability is observed for the five-stranded alpha-helical coiled-coil domain of cartilage oligomeric matrix protein COMP. It does not unfold in non-denaturing buffer between 0 and 100 degrees C and thermal denaturation is only achieved at high concentrations of guanidinium chloride (4-6 M). In these solutions the protein structure is lost at decreasing (cold denaturation) and increasing temperatures (heat denaturation). In the cold denaturation region, the melting profile showed deviations from the theory of Privalov et al. [P.L. Privalov, V. Griko Yu, S. Venyaminov, V.P. Kutyshenko, Cold denaturation of myoglobin, J. Mol. Biol. 190 (1986) 487-498] probably due to deviations from a two-state mechanism. High thermal stability as well as cold and heat denaturation was also observed for a mutant of the coiled-coil domain of COMP in which glutamine 54 was replaced by isoleucine but it still forms pentamer. The melting temperatures in plain buffer for the heat denaturation of COMP coiled-coil domain and its mutant obtained by extrapolation to zero molar guanidinium chloride concentration are approximately 160 and 220 degrees C, respectively, which groups them among the most stable proteins.

Cooperative equilibrium transitions coupled with a slow annealing step explain the sharpness and hysteresis of collagen folding

Heat and guanidinium-induced denaturation curves of collagen III and its fragments were fitted by theoretical models to explain the extreme sharpness and the hysteresis between unfolding and refolding. It was shown that a recently proposed kinetic model for collagen denaturation does not account for the observed steepness, with physically reasonable values of activation energy and frequency factors in the Arrhenius equation. The extreme slope, which amounts to 0.38 per centigrade for collagen III at the midpoint of its transition, can only be explained by a highly cooperative equilibrium model. The refolding curve is shifted to lower temperatures by 6 degrees C for collagen III and reversible unfolding matching the initial profile of the native protein is observed only after long-time annealing. A simple formalism is proposed by which experimental denaturation and refolding curves are quantitatively described. The transition proceeds via many cooperative steps with slightly different equilibrium constants for unfolding and refolding. Hysteresis and annealing are caused by very slow steps, which are probably connected with a rearrangement of misfolded regions. These slow steps disappear with decreasing size of collagen fragments and hysteresis is not found for collagen model peptides.