 
 
 
 
 
   In this section, you will examine the minimization and equilibration of ubiquitin in a water box with periodic boundary conditions.
 
 1-3-box.  Here, you will find a configuration file for the minimization and equilibration of ubiquitin in a water box.  All output files for the minimization and equilibration of your ubiquitin in a water box system will be placed in this directory.
1-3-box.  Here, you will find a configuration file for the minimization and equilibration of ubiquitin in a water box.  All output files for the minimization and equilibration of your ubiquitin in a water box system will be placed in this directory. 
The configuration file contains some commands which are different than the water sphere configuration file. Here, these differences are pointed out and explained.
 ,
,  , or
, or  value being specified by each.  For instance, cellBasisVector1 is
 value being specified by each.  For instance, cellBasisVector1 is  Å,
Å,  Å,
Å,  Å.  With each vector perpendicular, a rectangular 3-D box is formed.
Å.  With each vector perpendicular, a rectangular 3-D box is formed.
Particle Mesh Ewald (PME) is a useful method for dealing with electrostatic interactions in a system when periodic boundary conditions are present. The Ewald sum is an efficient way of calculating long range forces in a periodic system. The particle mesh is a 3-D grid created in the system over which the system charge is distributed. From this charge, potentials and forces on atoms in the system are determined. As a result, your grid size should be chosen such that it is fine enough to accurately represent the configuration of your system.
Alternatively, one can define the PME grid sizes manually, using PMEGridSizeX, PMEGridSizeY, and PMEGridSizeZ.  These set the size of the PME grid along 
cellBasisVector1, 2 and 3, respectively (not the  ,
,  , and
, and  directions as implied).  For speed in computing Fast Fourier Transforms, PMEGridSizeX should be chosen 
so that it can be factorized by 2, 3, or 5. If your cellBasisVector1 = (60, 0, 0), a good choice for PMEGridSizeX might be 64, since 60 Å / 64 = 0.9375 Å and
 directions as implied).  For speed in computing Fast Fourier Transforms, PMEGridSizeX should be chosen 
so that it can be factorized by 2, 3, or 5. If your cellBasisVector1 = (60, 0, 0), a good choice for PMEGridSizeX might be 64, since 60 Å / 64 = 0.9375 Å and 
 . Note that since cellBasisVector is defined with slightly different values in each direction, the size of the mesh spacing (in length) will be different in each direction.
. Note that since cellBasisVector is defined with slightly different values in each direction, the size of the mesh spacing (in length) will be different in each direction.  
Note also that when using the PME method, the command cutoff dictates the separation between long and short range forces for the method; it does not simply turn off interactions.
 cross sectional area constant while varying the
 cross sectional area constant while varying the  dimension; uses values yes and no.
 dimension; uses values yes and no.
The following are specifications for the Langevin piston which NAMD allows you to specify.
Note that the commands which specify spherical boundary conditions have been completely removed, since this simulation is using periodic boundary conditions.
 
 
 
 
 
 
 
