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Environment

VeloxChem implements both implicit (CPCM and SMD) and explicit (polarizable embedding) solvation models. Furthermore, hydrostatic pressure can be modeled with GOSTSHYP.

Implicit solvation

Implicit solvation models describe the effect of a surrounding liquid environment by replacing the explicit solvent molecules with a continuous dielectric medium that interacts self‑consistently with the electronic structure of the solute. Tomasi et al. (2005)

A separation is made between equilibrium and non-equilibrium solvation. In the former case, the timescale is such that both nuclear and electronic relaxations take place in the environment, such as in molecular structure optimizations. In the latter case, only electrons are fully equilibrated with the time-dependent solute charge density, such as in UV/vis spectrum simulations.

CPCM

In the conductor‑like polarizable continuum model (CPCM), the solute is placed inside a cavity defined by its molecular surface, and the reaction field is obtained by solving surface‑charge equations that approximate the dielectric screening of a perfect conductor and are subsequently scaled to represent the desired solvent permittivity.

VeloxChem implements the CPCM model for:

  • SCF energies

  • gradients (structure optimizations)

  • linear response (UV/vis spectra and more)

Python script

In CPCM, the induced charge density on the cavity (due to the presence of the solute) is represented on a surface grid and discretized as Gaussian charges centred at the grid points. The converged grid charges can be visualized using the CPCM driver.

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Text file

@jobs
task: scf
@end

@method settings
basis: def2-svp
xcfun: b3lyp
solvation model: cpcm
cpcm epsilon : 78.39
@end

@molecule
charge: 0
multiplicity: 1
xyz:
...
@end

SMD

The solvation model based on density (SMD) combines a self‑consistent reaction‑field description of the electrostatic polarization with empirically parametrized terms for cavitation, dispersion, and solvent–solute interactions based on the solute’s electron density, enabling accurate free‑energy predictions across a wide range of solvents. For further details, see Marenich et al. (2009).

In Veloxchem, the electrostatic contribution is determined using the CPCM model.

Python script

Text file

@jobs
task: scf
@end

@method settings
basis: def2-svp
xcfun: b3lyp
solvation model: smd
smd solvent : water
@end

@molecule
charge: 0
multiplicity: 1
xyz:
...
@end

Explicit solvation

An explicit representation of the environment is available with the polarizable embedding (PE) model. Molecules in the environment are represented by site charges and polarizabilities. VeloxChem supports the PE model for:

  • SCF energies

  • linear response (UV/vis spectra and more)

The PE model is invoked in input files by giving the name of the associated potential file.

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Python script

Text file

@jobs
task: scf
@end

@method settings
basis: aug-cc-pvdz
potfile: solvent.pot
@end

@molecule
charge: 0
multiplicity: 1
xyz:
C        4.3399560215    0.0305428946    0.0828144786
C        4.4095576538    1.3683610158   -0.3235192595
H        3.5134027643    1.9937601903   -0.3924032993
N        5.5723395543    1.9197433737   -0.6488743924
C        6.6935279309    1.1757794133   -0.5864329168
H        7.6224068215    1.6875951052   -0.8616425839
C        6.7276910108   -0.1635918452   -0.2107845581
H        7.6695032300   -0.7162266137   -0.1924428573
C        5.5097537075   -0.7720747162    0.1336293537
C        5.1009824698   -2.0878240657    0.5406435604
H        5.7372998568   -2.9570654838    0.6892873628
C        3.7438801169   -2.0443763598    0.7226497610
H        3.0543062251   -2.8214265706    1.0462619034
N        3.2609508451   -0.7683360554    0.4549835483
C        1.9260075376   -0.3749845510    0.5283176588
S        0.6782993391   -1.3889716576   -0.1542613778
C        1.4061153730    0.7824770017    1.0601625728
H        2.0181143215    1.5416160613    1.5454703546
C       -0.0068851194    0.8477465652    0.9398680126
H       -0.6059313977    1.6741214421    1.3245241162
C       -0.5667478467   -0.2580211398    0.3294429618
C       -1.9604337493   -0.5533359638    0.0792123648
C       -2.5277285148   -1.7535587315   -0.3270277748
H       -1.9416881983   -2.6565543003   -0.5031604314
C       -3.9321104260   -1.6831753283   -0.4684223853
H       -4.5766877637   -2.5081858439   -0.7717042735
S       -3.1787442841    0.6764078755    0.2764099378
C       -4.4390511633   -0.4347565024   -0.1731766944
C       -5.8556810641   -0.0499048614   -0.2240721981
O       -6.7574530303   -0.7927799637   -0.5363405829
O       -6.0328437022    1.2420382988    0.1214233024
C       -7.3762795865    1.7182783197    0.1021539149
H       -8.0044633860    1.1450501374    0.8009438574
H       -7.3321515876    2.7714270760    0.4053723170
H       -7.8085678845    1.6284781442   -0.9060973811
@end

Non-polarizable embedding

Potential file

The potential file named solvent_npe.pot in this example takes the following form, where all water molecules are treated as non-polarizable.

Polarizable embedding

The following potential file solvent_pe.pot contains most water molecules treated as polarizable and others as non-polarizable.

The polarizability components are listed in the order xx, xy, xz, yy, yz, zz.

Hydrostatic pressure

Hydrostatic pressure on molecular systems can be modeled using GOSTSHYP (Gaussians On Surface Tesserae Simulate HYdrostatic Pressure). In the model, the molecule subject to pressure is placed inside a cavity, similar to the one employed in CPCM. The pressure is induced via a collection of confining Gaussian potentials that are centered on the cavity surface, from which the force on the electron density is derived. Taking the cavity surface area into account, a mechanical pressure on the system is defined as force divided by area. The user inputs the desired pressure and units. Scheurer et al. (2021)

VeloxChem implements the GOSTSHYP model for:

  • SCF energies

  • Gradients (structure optimizations)

  • Linear response (UV/vis spectra and more)

Python script

References
  1. Tomasi, J., Mennucci, B., & Cammi, R. (2005). Quantum Mechanical Continuum Solvation Models. Chem. Rev., 105(8), 2999–3094. 10.1021/cr9904009
  2. Marenich, A. V., Cramer, C. J., & Truhlar, D. G. (2009). Universal Solvation Model Based on Solute Electron Density and on a Continuum Model of the Solvent Defined by the Bulk Dielectric Constant and Atomic Surface Tensions. J. Phys. Chem. B, 113(18), 6378–6396. 10.1021/jp810292n
  3. Scheurer, M., Dreuw, A., Epifanovsky, E., Head-Gordon, M., & Stauch, T. (2021). Modeling Molecules under Pressure with Gaussian Potentials. Journal of Chemical Theory and Computation, 17(1), 583–597. 10.1021/acs.jctc.0c01212