METAGUI A VMD EXTENSION TO ANALYZE AND VISUALIZE METADYNAMICS SIMULATIONS
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1 METAGUI A VMD EXTENSION TO ANALYZE AND VISUALIZE METADYNAMICS SIMULATIONS Alessandro Laio SISSA & DEMOCRITOS, Trieste Coworkers: Xevi Biarnes Fabio Pietrucci Fabrizio Marinelli
2 Metadynamics (Laio A. and Parrinello M., 2002). Filling the free energy wells with computational sand choose a collective variable s(x) (in the example s(x)=x) Bias the dynamics with a potential of the form V G ( s( x), t) = w t dt'exp s ( x) s( x( t') ) 2δs 0 2 V G (s,t) for large t is an approximation of F(s) 2 Other methods based on similar ideas: Taboo search: Cvijovic, D.; Klinowski, J. Local elevation: T. Huber, A.E. Torda and W.F. van Gunsteren Adaptive force bias: E. Darve and A. Pohorille Wang and Landau
3 Limitations " It is difficult to know in advance all the relevant variables " If one is forgotten histeresis!!! " Even if you know all: the filling speed decreases exponentially with the dimensionality of the free energy.
4 Bias-exchange metadynamics Run several metadynamics each biasing a different collective variable: Replica 1: collective variable a, bias potential V a (x,t) Replica 2: collective variable b, bias potential V b (x,t) Replica 3:. Attempt swapping the coordinates between the two replicas. Accept the move with a probability P=min[1,exp(-β(V a (x b,t)+v b (x a,t)-v a (x a,t)+v b (x b,t))] Parallelel reconstruction of F(s) in a virtually unlimited number of CVs The accuracy of each F(s) is greatly enhanced by the jumps in CV space due to the exchanges. S. Piana and AL, JPCB, 111, 4553 (2007) Related works: Replica exchange on proteins: Sugita, Y.; Okamoto, Y. Chem. Phys. Lett. 314, (1999). Replica exchange+ metadynamics: G. Bussi, F.L. Gervasio, AL and M. Parrinello, JACS 128, (2006)
5 Bias Exchange Metadyn. 6 replicas 6 Collective Variable 6 Bias Potential (1D) Piana and Laio, J Phys Chem B 2007 Marinelli et al, PLoS Comp Biol XYZ 6 COLVAR 6 HILLS
6 From NR one-dimensional free energies To an NR-dimensional free energy hypersurface
7 Select a subset of the biased CVs for the analysis Divide the CV space in hypercubes Collective variable 1 Collective variable 2
8 The structures belonging to each hypercube define a microstate Collective variable 1 Collective variable 2
9 The structures belonging to each hypercube define a microstate Structures belonging to a microstate MUST be similiar Collective variable 1 Collective variable 2
10 BIASED POPULATIONS (n α ) to be corrected by the metadynamics bias (V α ) Combine different estimates of p α by WHAM: Marinelli et al, PLoS Comp Biol 2009
11 Free energy of the microstates: test on 3ALA Cluster analysis in the 6- dimensional CV space: ~ clusters. For each cluster we compute the free energy from the 1800 ns of normal MD and by the WHAM procedure on the biasexchange results
12 Transition Rate Matrix Ø Eigenvalues How many relevant basins? Ø Eigenvectors Which microstates belong to a basin? Marinelli et al, PLOS Comp Biol 2009
13 Ø Metadynamics output files Ø Coordinates Trajectories (XYZ) 1)Find the microstates Ø Collective Variables Trajectories Ø Time dependent Bias Potentials Collective variable 1 Collective variable 2
14 Ø Metadynamics output files Ø Coordinates Trajectories (XYZ) 2)Check their structural consistency Ø Collective Variables Trajectories Ø Time dependent Bias Potentials Collective variable 1 Collective variable 2
15 Ø Metadynamics output files Ø Coordinates Trajectories (XYZ) 3) Compute their free energy by WHAM 4) Find the kinetic basins Ø Collective Variables Trajectories Ø Time dependent Bias Potentials
16 1) Structural clustering of the trajectories VMD (TCL/TK) + FORTRAN90 2) Compute the free energy hypersurface 3) Identify the main basins 4) Interactively explore the structures of the system Biarnés et al, CPC 2011
17 Ø METAGUI simplifies the analysis of metadynamics simulations, and directly connects CV based results onto 3D structures. Ø ex. 2D Free Energy Surface of an enzymatic reaction --> click at any point and show the structure. bond 2 cleavage bond 1 formation
18 pubs.acs.org/jacs Multidimensional View of Amyloid Fibril Nucleation in Atomistic 2 Detail Fahimeh Baftizadeh, Xevi Biarnes, Fabio Pietrucci, Fabio Affinito, and Alessandro Laio*, SISSA, Via Bonomea 265, Trieste, Italy Institut Quimic di Sarria Universitat Ramon Llull, Barcelona, Spain Centre Europe en de Calcul Atomique et Mole culaire, EPFL, Lausanne, Switzerland CINECA, Bologna, Italy energy as a function the number of β-strands. Sof Supporting 8 * Information ABSTRACT: Starting from a disordered aggregate, we have simulated the formation of ordered amyloid-like beta structures in a system formed by 18 polyvaline chains in explicit solvent, employing molecular dynamics accelerated by bias-exchange metadynamics. We exploited 8 different collective variables to compute the free energy of hundreds of putative aggregate structures, with variable content of parallel and antiparallel β-sheets and different packing among the sheets. This allowed characterizing in detail a possible nucleation pathway for the formation of amyloid fibrils: first the system forms a relatively large ordered nucleus of antiparallel β-sheets, and then a few parallel sheets start appearing. The relevant nucleation process culminates at this point: when a sufficient number of parallel sheets is formed, the free energy starts to decrease toward a new minimum in which this structure is predominant. The complex nucleation pathway we found cannot be described within classical nucleation theory, namely employing a unique simple reaction coordinate like the total content of β-sheets. 8 collective variables describing parallel and antiparallel packing, etc. 500 ns on 8 replicas incorporating them into macrocycles. Fibril formation is often INTRODUCTION described by a nucleation and growth mechanism, in which the 26 Amyloid fibrils are large protein aggregates characterized by a proteins form intermediate oligomeric aggregates before they 27 high content of β-sheets. Their presence is a hallmark of several organize and grow into ordered fibrils with the characteristic 28 neurodegenerative disorders, including Alzheimer's, Huntington's, 1 cross-beta structure.12 Intraresidue contacts have been mea29 Parkinson's, and prion diseases. The precise pathological role of sured by fluorescence to probe the process of self-assembly fibrillar species is not completely understood. However, amyloid Quasi-elastic light scattering spectroscopy16,17 has also been 31 protofibrils as well as oligomers have been suggested to lead to 2 used for the same scope. Despite all these advances, the exact 32 neuronal cell death. Moreover, interruption of fibril formation energy as a function of three CVs: CV-C is the number of antiparallel β-sheets, CV-Emolecular is the number of parallel β-sheets,fibril andremains CV-H isa matter of assembly of a nascent 33 prevented cell damage, suggesting that the early oligomers in the antiparallel steric zippers. The red isosurface represents3 the region of CV space explored the simulation. The blue debate,during and computer simulations have isosurface played an important 34 fibrillation process are probably toxic. Unlike other protein a free energy of 3.3 kcal/mol per chain and contains the global minimum, a disordered aggregate. The orange isosurface, at 5.8 kcal/mol role in addressing this question. Intermediate-resolution 35 quaternary structures, amyloid fibrils involve a conformation, models with coarse-grained force fields or implicit ights a plateau region (region 2) connected to region 1 and another basin (region 3), which is separated from regions 1 and 2 by asolvent have 36 known as cross-beta structure, that is basically sequence 5 7 been successfully investigated For instance, the aggrega
19 Folding free energy landscape of the GB3 protein Daniele Granata, Carlo Camilloni, Michele Vendruscolo 6 collective variables describing hydrophobic packing, alpha and beta fraction, etc. One CV describing the consistency with experimental chemical shifts. 400 ns on 7 replicas
20 Thanks: Xevi Biarnes Fabio Pietrucci Fabrizio Marinelli Available at:
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