Showing posts with label AFM. Show all posts
Showing posts with label AFM. 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.


Wednesday, January 31, 2018

When solvent breaks a protein: protein unfolding under shear

Proteins break under the action of different perturbations, the temperature, chemicals, mechanical forces. Fluid flow too, in special condition, unfolds a protein. In some biological processes, the fluid induced perturbation is even functional. That is the case of blood coagulation where the long chain of the von Willibrend factor unrolls and extends under the action of blood shear flow caused by a vessel injury. Other proteins, known as catch-bonds, use the tensile force to strength the binding with their substrate via a sort of allosteric conformational change. It is therefore intriguing to understand in which conditions a protein unfolds in shear flow, and the molecular mechanism of the process. We have dedicated a recent paper to this by exploiting the power of the lattice Boltzmann MD technique. Surf it here.


Monday, December 9, 2013

Unfolding is a crack!

The atomic force microscopy and other single molecule techniques have inspired a body of theoretical work aimed to detail the unfolding process of proteins.
A related intriguing question is: at which extent the unfolding due to a perturbative external mechanical force overlaps with the temperature (or chemically) induced process? There is not reason to think the two processes to be identical, and in principle a thermostable protein could lacks resistance along the pulling direction. However, it is tempting to follow the unfolding mechanism in different cases (temperature, chemical, and force induced) and see whether or not they can be mapped onto a similar problem-class.
I cite here a very interesting work by de Graff, Shannon, Farrel, Williams and Thorpe appeared in Biophysical Journal in 2011, see the pdf here. They used a simplified, but realistic enough, model to describe force induced unfolding of a protein as the crack propagation in a network. The model describes the protein matrix as a network of interactions between rigid units, and these interactions can break as effect of the applied external force mimicking the pulling of the protein's terminals. The progress of the cracking is followed and successfully compared to the unfolding processes caused by external force and generated by molecular dynamics simulations at the atomistic resolution. The great advantage of the model introduced by Thorpe and coworker is the computational cost, quite low as compared to the cpu-time required to perform atomistic simulations. The dissolution of a connected rigid network induced by progressively scaled interactions has been previously used to model thermal denaturation. In particular some investigations were devoted to thermophilic proteins and their thermal stability, see Rader, PhysBio(2009) and Rodestock&Gohlke, Protein(2010). The authors showed that in the matrix of thermophilic proteins the dissolution process of the network is more difficult to occur as effect of a more robust connectivity of the rigid motifs. The idea to compare temperature and force unfolding path echoes also in other recent papers, more or less innovative, see Srivastava&Granek, PhysRevLett(2013) and Prasanth&Andricioaei, NatureComm(2012).




Unfolding pathway of barnase protein. de Graff et al, Biophy J (2011),  101, 736.