Abstract:Mechanical stretching of the I27 domain of titin and of its double and triple repeats are studied through molecular dynamics simulations of a Go-like model with Lennard-Jones contact interactions. We provide a thorough characterization of the system and correlate the sequencing of the folding and unraveling events with each other and with the contact order. The roles of cantilever stiffness and pulling rate are studied. Unraveling of tandem titin structures has a serial nature. The force-displacement curves in… Show more
“…1BDD͔͒. 15 Very briefly, the protein a͒ model is coarse grained so that each amino acid is represented by individual beads located at the C ␣ atoms. Consecutive beads along the chain interact through an anharmonic potential given by…”
Section: A Protein a Using Go-type Modelmentioning
We have studied the efficiency of parallel tempering simulations for a variety of systems including a coarse-grained protein, an atomistic model polypeptide, and the Lennard-Jones fluid. A scheme is proposed for the optimal allocation of temperatures in these simulations. The method is compared to the existing empirical approaches used for this purpose. Accuracy associated with the computed thermodynamic quantities such as specific heat is also computed and their dependence on the trial-exchange acceptance rate is reported.
“…1BDD͔͒. 15 Very briefly, the protein a͒ model is coarse grained so that each amino acid is represented by individual beads located at the C ␣ atoms. Consecutive beads along the chain interact through an anharmonic potential given by…”
Section: A Protein a Using Go-type Modelmentioning
We have studied the efficiency of parallel tempering simulations for a variety of systems including a coarse-grained protein, an atomistic model polypeptide, and the Lennard-Jones fluid. A scheme is proposed for the optimal allocation of temperatures in these simulations. The method is compared to the existing empirical approaches used for this purpose. Accuracy associated with the computed thermodynamic quantities such as specific heat is also computed and their dependence on the trial-exchange acceptance rate is reported.
“…Its scenario is defined in terms of the last average distance, d u , at which contacts are still holding when the C-terminus is moving at a constant speed and the N-terminus is attached to an elastic anchor. We have already established that stretching at "room temperature" proceeds in a way that is unrelated to folding [16,9]. It is only in the entropic limit, when stretching is governed exclusively by the sequential distance that stretching is approximately reverse to folding at optimality [23].…”
Section: Between Strands B-e (Open Triangles) and B-g (Open Circles)mentioning
confidence: 99%
“…Mechanical stretching of this protein has been extensively studied in experiments involving atomic force microscopy [11][12][13] and there is also some information about its folding [14,15]. Furthermore, we have already studied it undergoing both processes through molecular dynamics simulations within the topology based model [9,[16][17][18].…”
mentioning
confidence: 99%
“…The broken line corresponds to the distance of 1.5σ ij that is considered as a qualitative treshold for the amino acids staying or not staying in a contact [8,16]. It is seen that the treshold line is being crossed repeatedly due to thermal fluctuations.…”
Thermal unfolding of proteins is compared to folding and mechanical stretching in a simple topology-based dynamical model. We define the unfolding time and demonstrate its low-temperature divergence. Below a characteristic temperature, contacts break at separate time scales and unfolding proceeds approximately in a way reverse to folding. Features in these scenarios agree with experiments and atomic simulations on titin.
“…In the following we will present and discuss Molecular Dynamics (MD) simulation results in which we can perform a quasi-fixed stretch treatment. In these simulations (similar to what has been done for protein-like polymers [27,28]) the two ends of the polymer are tethered by springs to two fixed points in space so its end-to-end vector can vary only little. The two fixed points are chosen such that a line connecting them is along the z-direction.…”
A new formula for the force vs extension relation is derived from the discrete version of the so called worm like chain model. This formula correctly fits some recent experimental data on polymer stretching and some numerical simulations with pairwise repulsive potentials. For a more realistic Lennard-Jones potential the agreement with simulations is found to be good when the temperature is above the θ temperature. For lower temperatures a plateau emerges, as predicted by some recent experimental and theoretical results, and our formula gives good results only in the high force regime. We briefly discuss how other kinds of self-interactions are expected to affect the elasticity of the polymer.
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