Showing posts with label hydrodynamics. Show all posts
Showing posts with label hydrodynamics. Show all posts

Thursday, December 13, 2018

The force, the heat and the shear. Three weaknesses for three perturbations!

Shear unfolding chapter two. Same question: Can proteins unfold in shearing fluid flows, and to what extent? How do the tensile forces exerted by the solvent affect the protein compared to other types of external perturbations such as thermal denaturation, or directional pulling forces used in optic/magnetic tweezers or atomic force microscopy (AFM) experiments? Before the answer: conventional all-atom molecular dynamics simulations often require too much computational effort, hence, we have developed an original methodology using Lattice Boltzmann Molecular Dynamics (LBMD) and the Optimized Potential for Efficient peptide folding Prediction (OPEP) coarse-grained model to inquire the unfolding features of a small Cold Shock Protein subjected to three different perturbations: shear flow, heat shock and pulling force. Since the implicit-solvent OPEP model inherently lacks hydrodynamics, the Lattice Boltzmann framework allowed us to realistically simulate the flow interaction with the protein, while retaining good computational efficiency with respect to explicit-solvent approaches. Here the answer: The direct comparison of the unfolding mechanisms evidenced that the three perturbations act on different weaknesses of the protein, and thus lead on average to very different unfolding pathways. Funny enough, for this small globular protein shear flow acts more similarly to thermal excitation then a direct mechanical force. Our results suggest that the interpretation of experimental studies that rely on force-spectroscopy techniques to investigate natural shear-activated systems, such as the von Willebrand factor or the bacterial adhesin FimH, is not straightforward. The paper is out here.


Sunday, May 25, 2014

Unfolding Under Shear

What does it happen to a protein in fluid shear flow? According to some studies, a protein could be forced to unfold. However there is not agreement on the necessary strength, or more technically, on the magnitude of the shear rate that could cause the unfolding to happen. Jaspe and Hagen for example estimated that only an extraordinary value of the shear rate (107 s-1) is effective for unfolding globular proteins, read their work in Biophys. J.(2006)  here.

In our group we have recently combined an effective coarse-grained model for simulating protein motion with an engine for considering hydrodynamic interactions. A first glance to this coupling is presented in a recent review in ChemSocRev(2014), see here. We also presented the preliminary results of an investigation aimed to understand how shear flow acts on the stability of proteins. We actually show the unfolding process of a simple β-hairpin peptide under laminar shear flow. We have used a very strong shear rate, 1010s-1, and the unfolding occurs in about 10 ns. We are now checking how the unfolding rate changes by decreasing the shear rate.

Fig.9 in Sterpone et al, Chem.Soc.Rev. (2014) DOI:10.1039/C4CS00048J.  Unfolding of β-hairpin under shear.