Constrained molecular dynamics: Difference between revisions

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== Anderson thermostat ==
== How to ==
Geometric constraints are introduced by defining one or more entries with the STATUS parameter set to 0 in the {{FILE|ICONST}}-file. Constraints can be used within a standard NVT or NpT MD setting introduced by {{TAG|MDALGO}}=1|2|3. Note that fixing geometric parameters related to lattice vectors is not allowed within an NVT simulation (VASP would terminate with an error message). Constraints can be combined with restraints, time-dependent bias potentials ([[:Category:Metadynamics|Metadynamics]]), monitored coordinates and other elements available within the context of MD.       


* For a constrained molecular dynamics run with Andersen thermostat, one has to:
#Set the standard MD-related tags: {{TAG|IBRION}}=0, {{TAG|TEBEG}}, {{TAG|POTIM}}, and {{TAG|NSW}}.
#Set {{TAG|MDALGO}}=1, and choose an appropriate setting for {{TAG|ANDERSEN_PROB}}.
#Define geometric constraints in the {{FILE|ICONST}}-file, and set the STATUS parameter for the constrained coordinates to 0.
#When the free-energy gradient is to be computed, set {{TAG|LBLUEOUT}}=.TRUE.


== References ==
== References ==
<references>
<references>
<ref name="Ryckaert77">[http://dx.doi.org/10.1016/0021-9991(77)90098-5 J. P. Ryckaert, G. Ciccotti, and H. J. C. Berendsen, J. Comp. Phys. 23, 327 (1977).]</ref>
<ref name="Carter89">[http://dx.doi.org/10.1016/S0009-2614(89)87314-2 E. A. Carter, G. Ciccotti, J. T. Hynes, and R. Kapral, Chem. Phys. Lett. 156, 472 (1989).]</ref>
<ref name="Otter00">[http://dx.doi.org/10.1080/00268970009483348 W. K. Den Otter and W. J. Briels, Mol. Phys. 98, 773 (2000).]</ref>
<ref name="Darve02">[http://dx.doi.org/10.1080/08927020211975 E. Darve, M. A. Wilson, and A. Pohorille, Mol. Simul. 28, 113 (2002).]</ref>
<ref name="Fleurat05">[http://dx.doi.org/10.1063/1.1948367 P. Fleurat-Lessard and T. Ziegler, J. Chem. Phys. 123, 084101 (2005).]</ref>
<ref name="Ryckaert77">[http://dx.doi.org/10.1016/0021-9991(77)90098-5 J. P. Ryckaert, G. Ciccotti, and H. J. C. Berendsen, J. Comp. Phys. 23, 327 (1977).]</ref>
<ref name="Ryckaert77">[http://dx.doi.org/10.1016/0021-9991(77)90098-5 J. P. Ryckaert, G. Ciccotti, and H. J. C. Berendsen, J. Comp. Phys. 23, 327 (1977).]</ref>
</references>
</references>

Latest revision as of 06:48, 19 July 2022

Constrained molecular dynamics is performed using the SHAKE algorithm.[1]. In this algorithm, the Lagrangian for the system is extended as follows:

where the summation is over r geometric constraints, is the Lagrangian for the extended system, and λi is a Lagrange multiplier associated with a geometric constraint σi:

with ξi(q) being a geometric parameter and ξi is the value of ξi(q) fixed during the simulation.

In the SHAKE algorithm, the Lagrange multipliers λi are determined in the iterative procedure:

  1. Perform a standard MD step (leap-frog algorithm):
  2. Use the new positions q(tt) to compute Lagrange multipliers for all constraints:
  3. Update the velocities and positions by adding a contribution due to restoring forces (proportional to λk):
  4. repeat steps 2-4 until either |σi(q)| are smaller than a predefined tolerance (determined by SHAKETOL), or the number of iterations exceeds SHAKEMAXITER.

How to

Geometric constraints are introduced by defining one or more entries with the STATUS parameter set to 0 in the ICONST-file. Constraints can be used within a standard NVT or NpT MD setting introduced by MDALGO=1|2|3. Note that fixing geometric parameters related to lattice vectors is not allowed within an NVT simulation (VASP would terminate with an error message). Constraints can be combined with restraints, time-dependent bias potentials (Metadynamics), monitored coordinates and other elements available within the context of MD.


References