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Continuum Solvent Non-Electrostatics

Abstract

Rules for implicit solvation

3. Electrostatics are only part of the free energy of solvation

Consequence:

You also need to somehow account for cavitation, dispersion, solvent structural changes etc.

Tools:

You can always make electrostatics better at the same time

How to account for non-electrostatic terms

  • (worst) You could ignore them completely, though this would only really be valid for systems where electrostatic effects will dominate
  • Attempt to compute them separately e.g. one property, one calculation
  • (best) Assume proportionality to the solvent-accessible surface area and parameterise microscopic surface tensions
    • Continuum solvation is inherently semiempirical, so parameterisation should not be feared.

First solvation-shell contributions

One way to approximate the Solvent Accessible Surface Area (SASA) is to “roll a ball” over the surface of the molecule and the volume it takes up defines the

image

Where:

  • \(\sum\limits_k^{atoms}=\) Adding up the influence of each atom \(k\)
  • \(A_k=\) Surface area exposed of the atom \(k\)
  • \(\sigma_k=\) A characteristic surface tension, based on atomic number
  • \(\sum\limits_{k'}^{atoms}\sigma_{kk'}(R)=\) A modifier for the interaction of functional groups
    • \(\sum\limits_{k'}^{atoms}=\) Adding up the influence of each other atom (\(k'\))
    • \(\sigma_{kk'}(R)=\) looks at the distance between the two atoms (\(k\) and \(k'\)) and modifies the value of \(\sigma\)
\[ G_{CDS}=\sum\limits_k^{atoms}A_k\bigg(\sigma_k+\sum\limits_{k'}^{atoms}\sigma_{kk'}(R)\bigg) \]

The value of \(\sigma_{kk'}\) varies over distance, which will result in a gradual switching behaviour. In the figure below, the short distances might represent a ketone (the switch is on) and the longer distance might represent an ether (the switch is off)

image

Microscopic surface tensions

This simple equation shows the non-electrostatic solvation energy \(G_{CDS}\) is equal to the sum of the exposed surface area of each atom \(A_k\) times some proportionality constant \(\sigma_k\).

\[ G_{CDS}=\sum\limits_kA_k\sigma_k \]

E.g. 1. SMx universal solvation model

These are universal, because the surface tension (\(\sigma_k\)) will change based on the solvent

  • Surface tensions are treated as functions, rather than parameters
  • The value arrives from running over a series of descriptors (\(\sum_j^{descr}\)) and taking a parameter associated with that descriptor (\(\hat{\sigma}_{Z_i}\)) and multiplying it with the descriptor (\(\xi_j\)$)
\[ \sigma_i=\sum\limits_j^{descr}\hat{\sigma}_{Z_i}\xi_j \]

The descriptors could be (incomplete list):

  • \(n=\) solvent index of refraction (is a direct measure of polarisability of the solvent)
  • \(\gamma=\) solvent macroscopic surface tension (how hard it is to cavitate the solvent)
  • \(\alpha=\) Abraham h-bonding acidity (the ability of the solvent to h-bond as a proton donor)
  • \(\beta=\) Abraham h-bonding basicity (the ability of the solvent to h-bond as a proton acceptor)

To create these parameters

Take the experimental data, subtract the electrostatics to get the \(G_{CDS}\), we know the surface area, since we can calculate it, which leaves the unknown parameters.

After doing a big multilinear regression, we can determine the universal parameters of the solvent

\[ \Delta G_{aq,\:expt}-\Delta G_{ENP}=G_{CDS}=\sum\limits_kA_k\sigma_k \]

The result

SM8 has about 72 parameters for 2500 data (H, C, N, O, F, S, P, Cl, Br based compounds) in 91 solvents.

There is a mean error of \(\sim\pm0.6\:kcal\:mol^{-1}\) for neutral species and \(\pm3-6\:kcal\:mol^{-1}\) for ions (depending on the solvent)

Examples of solvent descriptors

\(\ce{H2O}\) \(\ce{C6H6}\) \(\ce{CH2Cl2}\)
Dielectric constant (\(\varepsilon\)) 78.36 2.27 8.93
Abraham h-bonding acidity (\(\alpha\)) 0.82 0.00 0.10
Abraham h-bonding basicity (\(\beta\)) 0.38 0.141 0.05
Refractive index (\(n\)) 1.33 1.50 1.42
Surface tension (\(cal\cdot mol^{-1}\cdot\unicode{x212B}^{-2}\)) 104.71 40.62 39.15
Carbon aromaticity 0.00 1.00 0.00
Electronegative halogenicity 0.00 0.00 0.67

SM8 Performance

Mean unsigned errors (kcal/mol) for SM8 compared to other models

Solute Class Data N SM8 IEFPCM (G03/UA0) C-PCM GAMESS PB Jaguar All Equal to Mean2
Aqueous neutrals 274 0.5 4.9 1.6 0.9 2.7
Non-aqueous neutrals 666 0.6 6.0 2.8 2.3 1.5
Aqueous ions 112 3.2 12.4 8.4 4.0 8.6
Non-aqueous ions 220 4.9 8.4 8.4 8.1 8.6

  1. Benzene’s \(\pi\) cloud can actually accept a proton to some extent. 

  2. Assumes no difference in atom types.