[CP2K-user] [CP2K:17037] Simulating liquid DMSO

Thomas Kühne tkuehne at gmail.com
Wed May 25 19:16:10 UTC 2022


Dear Henrique Junior, 

if these are subsequent step separated by 0.5fs than this looks all very reasonable to me. 
The atoms don’t move a hell a lot within half a femtosecond. 

Best, 
Thomas Kühne

> Am 27.04.2022 um 21:22 schrieb Henrique Junior <henriquecsj at gmail.com>:
> 
> Hi everyone, I hope you are all doing fine.
> 
> CP2K is completely new for me, and it is proving to be a challenge. I am attempting to simulate liquid DMSO (a simple molecule with 10 atoms) just as a test. So far, I have tried to build my input based on tutorials simulating liquid water and tweaking it for DMSO.
> 
> The calculation is running fine and converging quite smoothly but looking at the DMSO-pos-1.xyz file that’s being generated I can see that the atoms are barely shaking. I’m attaching (and showing below) my input and the xyz file. Any help would be much appreciated.
> 
> Thanks in advance.
> 
> Vvvvvvvvvvvvvvvvvvvvvvvvvv INPUT vvvvvvvvvvvvvvvvvvvvvvvvvv
> 
> &GLOBAL
>   PROJECT DMSO
>   RUN_TYPE MD             
> &END GLOBAL
> 
> &FORCE_EVAL
>   METHOD Quickstep
>   &DFT
>     BASIS_SET_FILE_NAME GTH_BASIS_SETS
>     POTENTIAL_FILE_NAME GTH_POTENTIALS            
>     CHARGE 0
>     MULTIPLICITY 1
> 
>     &MGRID
>        CUTOFF [Ry] 400 
>     &END
> 
>     &QS
>        METHOD GPW 
>        EPS_DEFAULT 1.0E-10 
>        EXTRAPOLATION ASPC 
>     &END
> 
>     &POISSON
>        PERIODIC XYZ ! the default, gas phase systems should have 'NONE' and a wavelet solver
>     &END
> 
>     &PRINT
>        &E_DENSITY_CUBE OFF
>        &END E_DENSITY_CUBE
>        &MO_CUBES
>           NLUMO 4
>           NHOMO 4
>           WRITE_CUBE .FALSE.
>           &EACH
>             MD 10
>           &END
>        &END
>     &END
> 
>     &SCF                              
>       SCF_GUESS ATOMIC 
>       MAX_SCF 500
>       EPS_SCF 1.0E-6 
>       &OT
>         PRECONDITIONER FULL_SINGLE_INVERSE
>         MINIMIZER DIIS
>       &END OT
>       &OUTER_SCF ! repeat the inner SCF cycle 10 times
>         MAX_SCF 10
>         EPS_SCF 1.0E-6
>       &END
>       &PRINT
>         &RESTART OFF
>       &END
>       &END
>     &END SCF
> 
>     &XC
>       &XC_FUNCTIONAL 
>          &PBE
>          &END
>       &END XC_FUNCTIONAL
>       ! adding Grimme's D3 correction (by default without C9 terms) 
>       &VDW_POTENTIAL
>          POTENTIAL_TYPE PAIR_POTENTIAL 
>          &PAIR_POTENTIAL
>             PARAMETER_FILE_NAME dftd3.dat
>             TYPE DFTD3
>             REFERENCE_FUNCTIONAL PBE
>             R_CUTOFF [angstrom] 16
>          &END
>       &END VDW_POTENTIAL
>     &END XC
>   &END DFT
>  
>   &SUBSYS
>     &CELL 
>       ABC [angstrom] 9.0 9.0 9.0
>     &END CELL
> 
>     &TOPOLOGY
>       COORD_FILE_NAME DMSOcaixa.xyz
>       COORD_FILE_FORMAT XYZ
>     &END
> 
>     &KIND H                              
>       BASIS_SET DZVP-MOLOPT-SR-GTH         
>       POTENTIAL GTH-PBE-q1             
>     &END KIND
>     &KIND C
>       BASIS_SET DZVP-MOLOPT-SR-GTH
>       POTENTIAL GTH-PBE-q4
>     &END KIND
>     &KIND O
>       BASIS_SET DZVP-MOLOPT-SR-GTH
>       POTENTIAL GTH-PBE-q6
>     &END KIND
>     &KIND S
>       BASIS_SET DZVP-MOLOPT-SR-GTH
>       POTENTIAL GTH-PBE-q6
>     &END KIND
>   &END SUBSYS
> &END FORCE_EVAL
> 
> ! how to propagate the system, selection via RUN_TYPE in the &GLOBAL section
> &MOTION
>   &PRINT
>     &TRAJECTORY
>       &EACH
>         MD 1
>       &END EACH
>     &END TRAJECTORY
>     &VELOCITIES OFF
>     &END VELOCITIES
>     &FORCES OFF
>     &END FORCES
>     &RESTART_HISTORY
>       &EACH
>         MD 500
>       &END EACH
>     &END RESTART_HISTORY
>     &RESTART
>       BACKUP_COPIES 3
>       &EACH
>         MD 1
>       &END EACH
>     &END RESTART
>   &END PRINT
>  &GEO_OPT
>    OPTIMIZER BFGS ! Good choice for 'small' systems (use LBFGS for large systems)
>    MAX_ITER  100
>    MAX_DR    [bohr] 0.003 ! adjust target as needed
>    &BFGS
>    &END
>  &END
>  &MD
>    ENSEMBLE NVT  ! sampling the canonical ensemble, accurate properties might need NVE
>    TEMPERATURE [K] 300
>    TIMESTEP [fs] 0.5
>    STEPS 1000
>    # GLE thermostat as generated at http://epfl-cosmo.github.io/gle4md 
>    # GLE provides an effective NVT sampling.
>    &THERMOSTAT
>      REGION MASSIVE
>      TYPE GLE
>      &GLE
>        NDIM 5
>        A_SCALE [ps^-1] 1.00
>        A_LIST    1.859575861256e+2   2.726385349840e-1   1.152610045461e+1  -3.641457826260e+1   2.317337581602e+2
>        A_LIST   -2.780952471206e-1   8.595159180871e-5   7.218904801765e-1  -1.984453934386e-1   4.240925758342e-1
>        A_LIST   -1.482580813121e+1  -7.218904801765e-1   1.359090212128e+0   5.149889628035e+0  -9.994926845099e+0
>        A_LIST   -1.037218912688e+1   1.984453934386e-1  -5.149889628035e+0   2.666191089117e+1   1.150771549531e+1
>        A_LIST    2.180134636042e+2  -4.240925758342e-1   9.994926845099e+0  -1.150771549531e+1   3.095839456559e+2
>      &END GLE
>    &END THERMOSTAT
>  &END
> &END
> 
> 
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> <DMSO.inp><DMSO-pos-1.xyz>



==============================
Thomas D. Kühne
Dynamics of Condensed Matter
Chair of Theoretical Chemistry
University of Paderborn
Warburger Str. 100
D-33098 Paderborn
Germany
thomas.kuehne at upb.de
+49/(0)5251/60-5726

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