All of the information concerning the trajectory of these times was collected every 5 ps. The equilibration of the trajectory was checked by monitoring the equilibration of the quantities, such as the RMSD of non-hydrogen atoms with respect to the initial structure. Fludarabine solubility dmso Analysis of the total energy, potential energy and kinetic energy were all obtained using GROMACS software. RMSD values between final and LY3039478 nmr template structures also helped to identify the common segments, which corresponds to the structurally conserved region. The average structure of the entire trajectory was also determined using the g_rms algorithm [68]. The first 10 ns of the trajectory

were not used to determine the average structures. All of the water molecules were removed from the selected structures to proceed with the docking simulations in the next step. Molecular docking By using the structures of PbMLS-interacting proteins determined by MD as described above, a global search find more of protein-protein interactions was performed using GRAMM-X software [69]. The Protein-Protein Docking Web Server v.1.2.0 was used to perform rigid docking. Simulations were performed with no pre-conceived bias toward specific residue interactions, and the best model-structure of each complex (PbMLS + PbMLS-interacting proteins) was selected. Refinement of MD MD simulations of the complexes were performed to improve the

orientation of their side chains and to minimize the high-magnitude repulsive interactions between atoms. Short simulations were performed for the complexes defined by the GRAMM-X software, again using GROMACS software, with the same force field and solvent model Reverse transcriptase previously used to define the 3D-structures of each protein. The system was defined by a cubic box with periodic boundary conditions, and a 9 Å cut-off for non-bond interactions was used for electrostatic interactions treated by the Particle Mesh Ewald method. Overlapping water molecules were deleted, and the systems were neutralized by adding counter ions. Initially, the

system was subjected to minimization using steepest descent energy. The simulations were completed when the tolerance of 1000 kJ/mol was no longer exceeded. After minimization, the system was subjected to a 100 ps simulation in the NVT ensemble and then was immediately subjected to a 100 ps simulation in the NPT ensemble. For both stages, T = 300 K, and the thermostat relaxation constant = 0.1 ps; additionally, a Berendsen thermostat, 1 atm pressure, a time-step of 2 fs and position restraint of the complex were used. After that step, the system was subjected to an MD run in the NPT ensemble. The simulations were performed for 1 ns with a constant temperature of 300 K, 1 atm pressure, a time-step of 2 fs and without any restriction on the complex conformations.