2015.01.25: I have summarized discussion of this and related issues in this paper. I have also made some changes in the post to reflect what I have learned since I wrote it.
The problem
Thermodynamics involving ionizable functional group at constant pH require special considerations. Robert Alberty has written extensively on this topic (example) but I confess I had some trouble relating the work to quantum chemical calculations. This post aims to do just that.
Let's say you want to compute the standard free energy change at pH 7 for this equilibrium
where molecule $\mathrm{B}$ can be converted to an acid $\mathrm{HA}$, which is in equilibrium with it conjugate base and thus pH-dependent.
The apparent equilibrium constant ($K^\prime$) is
How to compute the corresponding standard free energy change?:
The Solution
$K^\prime$ can be rewritten as
where
and
Thus,
where
Thus
where
Here $\mathrm{\overline{HA}}$ refers to "$\text{HA and A}$"
An example
How do you compute the standard free energy change in aqueous solution at pH 7 using QM for this reaction?:
First you optimize each molecule and perform the vibrational analysis to get the free energies. You can account for solvation effects using a method like PCM or COSMO. $\mathrm{HCOOH}$ and $\mathrm{NH_3}$ are acids and basis, respectively so you will also need the energies for $\mathrm{HCOO^-}$ and $\mathrm{NH_4^+}$
Most QM programs assume the molecules are in the gas phase when computing the Gibbs free energies so the standard state is 1 bar. The free energies must be corrected for the solution standard state of 1 M:
where $V$ is the molar volume of an ideal at gas at your chosen temperature. The exception is water since that is also the solvent. Here the standard state is 55.34 M at 25C.
$G^{\prime\circ}(\mathrm{HCOO^-})$ and is then computed using Eq (1). $G^{\circ}(\mathrm{H^+})$ is usually taken from the literature though estimates vary between -265.8 and -268.6 kcal/mol.
$G^{\prime\circ}(\mathrm{\overline{HCOOH}})$ can then be computed using Eq (3). The electronic energy component of $G^{\circ}(\mathrm{X})$ can be quite large in magnitude and give some numerical problems when computing the exponential function so Eq (3) and be rewritten as
Following a derivation similar to the one at the beginning of this post,
and $G^{\prime\circ}(\mathrm{\overline{NH_3}})$ is computed by Eq (3)
Finally, we put everything together
Another way
If you happen to know the pKa values (e.g. from experiment) of the ionizable species you can use this expression
$\Delta G^{\prime\circ}=\Delta A^{\circ}-RT\ln \left( 1+10^{\mathrm{pH}- pK_{a,\mathrm{HCOOH}}} \right)-RT\ln \left( 1+10^{ pK_{a,\mathrm{NH_4^+}}-\mathrm{pH}} \right)$
where
$\Delta G^{\circ}=G^{\circ}(\mathrm{HCOOH})+G^{\circ}(\mathrm{NH_3})- G^\circ(\mathrm{\text{HC(=O)-}NH_2})-G^\circ(\mathrm{H_2O})$
This work is licensed under a Creative Commons Attribution 4.0
The problem
Thermodynamics involving ionizable functional group at constant pH require special considerations. Robert Alberty has written extensively on this topic (example) but I confess I had some trouble relating the work to quantum chemical calculations. This post aims to do just that.
Let's say you want to compute the standard free energy change at pH 7 for this equilibrium
$\mathrm{B \rightleftharpoons HA}$
where molecule $\mathrm{B}$ can be converted to an acid $\mathrm{HA}$, which is in equilibrium with it conjugate base and thus pH-dependent.
$\mathrm{HA \rightleftharpoons A^- + H^+}$
The apparent equilibrium constant ($K^\prime$) is
$K^\prime=\mathrm{\frac{[HA]+[A^-]}{[B]}}$
How to compute the corresponding standard free energy change?:
$\Delta G^{\prime\circ}=-RT\ln(K^\prime)$
The Solution
$K^\prime$ can be rewritten as
$K^\prime=K+\frac{KK_a}{[\mathrm{H^+}]}$
where
$K=\mathrm{\frac{[HA]}{[B]}}=\exp{(-\Delta G^\circ/RT)}$
and
$K_a=\mathrm{\frac{[A^-][H^+]}{[HA]}}=\exp{(-\Delta G^\circ_a/RT)}$
Thus,
$K^\prime=\exp{(-\Delta G^\circ/RT)} + \exp{(-\Delta G^\circ/RT)}\exp{(-\Delta G^\circ_a/RT)}10^{\mathrm{pH}}$
$=\exp{(-\Delta G^\circ/RT)} + \exp{(-(\Delta G^\circ+\Delta G^\circ_a-RT\ln(10)\mathrm{pH})/RT)}$
$=\frac{\exp{(-G^\circ(\mathrm{HA})/RT)}+\exp{(-G^{\prime\circ}(\mathrm{A^-})/RT)} }{\exp{(-G^\circ(\mathrm{B})/RT)}}$
where
$G^{\prime\circ}(\mathrm{A^-})=G^{\circ}(\mathrm{A^-})+[G^{\circ}(\mathrm{H^+})-RT\ln(10)\mathrm{pH}]$ (1)
Thus
$\Delta G^{\prime\circ}= G^{\prime\circ}(\mathrm{\overline{HA}})-G^\circ(\mathrm{B})$ (2)
where
$G^{\prime\circ}(\mathrm{\overline{HA}})=-RT\ln \left( \exp{(-G^\circ(\mathrm{HA})/RT)}+\exp{(-G^{\prime\circ}(\mathrm{A^-})/RT)} \right)$ (3)
Here $\mathrm{\overline{HA}}$ refers to "$\text{HA and A}$"
An example
How do you compute the standard free energy change in aqueous solution at pH 7 using QM for this reaction?:
$\mathrm{\text{HC(=O)-}NH_2+ H_2O \rightleftharpoons HCOOH + NH_3}$
First you optimize each molecule and perform the vibrational analysis to get the free energies. You can account for solvation effects using a method like PCM or COSMO. $\mathrm{HCOOH}$ and $\mathrm{NH_3}$ are acids and basis, respectively so you will also need the energies for $\mathrm{HCOO^-}$ and $\mathrm{NH_4^+}$
Most QM programs assume the molecules are in the gas phase when computing the Gibbs free energies so the standard state is 1 bar. The free energies must be corrected for the solution standard state of 1 M:
$G^\circ(\mathrm{X}) = G^{\circ,\mathrm{1 bar}}(\mathrm{X})-RT\ln (V^{-1})$
where $V$ is the molar volume of an ideal at gas at your chosen temperature. The exception is water since that is also the solvent. Here the standard state is 55.34 M at 25C.
$G^\circ(\mathrm{H_2O}) = G^{\circ,\mathrm{1 bar}}(\mathrm{H_2O})-RT\ln ((55.34V)^{-1})$
$G^{\prime\circ}(\mathrm{HCOO^-})$ and is then computed using Eq (1). $G^{\circ}(\mathrm{H^+})$ is usually taken from the literature though estimates vary between -265.8 and -268.6 kcal/mol.
$G^{\prime\circ}(\mathrm{\overline{HCOOH}})$ can then be computed using Eq (3). The electronic energy component of $G^{\circ}(\mathrm{X})$ can be quite large in magnitude and give some numerical problems when computing the exponential function so Eq (3) and be rewritten as
$G^{\prime\circ}(\mathrm{\overline{HA}})= G^\circ(\mathrm{HA})-RT\ln \left(1+\exp{(-(G^{\prime\circ}(\mathrm{A^-})-G^\circ(\mathrm{HA}))/RT)} \right)$
Following a derivation similar to the one at the beginning of this post,
$G^{\prime\circ}(\mathrm{NH_4^+})=G^{\circ}(\mathrm{NH_4^+})-[G^{\circ}(\mathrm{H^+})-RT\ln(10)\mathrm{pH}]$
and $G^{\prime\circ}(\mathrm{\overline{NH_3}})$ is computed by Eq (3)
Finally, we put everything together
$\Delta G^{\prime\circ}=G^{\prime\circ}(\mathrm{\overline{HCOOH}})+G^{\prime\circ}(\mathrm{\overline{NH_3}})- G^\circ(\mathrm{\text{HC(=O)-}NH_2})-G^\circ(\mathrm{H_2O}) $
Another way
If you happen to know the pKa values (e.g. from experiment) of the ionizable species you can use this expression
$\Delta G^{\prime\circ}=\Delta A^{\circ}-RT\ln \left( 1+10^{\mathrm{pH}- pK_{a,\mathrm{HCOOH}}} \right)-RT\ln \left( 1+10^{ pK_{a,\mathrm{NH_4^+}}-\mathrm{pH}} \right)$
where
$\Delta G^{\circ}=G^{\circ}(\mathrm{HCOOH})+G^{\circ}(\mathrm{NH_3})- G^\circ(\mathrm{\text{HC(=O)-}NH_2})-G^\circ(\mathrm{H_2O})$
This work is licensed under a Creative Commons Attribution 4.0
No comments:
Post a Comment