computational chemistry study of reactions, equilibrium and kinetics of chemical co2 absorption
TRANSCRIPT
i n t e r n a t i o n a l j o u r n a l o f g r e e n h o u s e g a s c o n t r o l 1 ( 2 0 0 7 ) 1 5 1 – 1 5 7
Computational chemistry study of reactions, equilibriumand kinetics of chemical CO2 absorption
Eirik F. da Silva a,b,*, Hallvard F. Svendsen a
aThe Norwegian University of Science and Technology (NTNU), NO-7491 Trondheim, Norwayb SINTEF Materials and Chemistry, NO-7465 Trondheim, Norway
a r t i c l e i n f o
Article history:
Received 7 August 2006
Received in revised form
22 November 2006
Accepted 26 January 2007
Published on line 13 March 2007
Keywords:
CO2 absorption
Solvents
Reaction mechanism
Computational chemistry
a b s t r a c t
The chemical reactions involved in CO2 absorption in amine systems are studied. For each
mechanism, available experimental data are considered and quantum mechanical calcula-
tions carried out. Base-catalyzed bicarbonate formation is found to be a likely mechanism
for all amine bases, not only tertiary amines. Direct formation of bicarbonate species from
carbamate species is found to be unlikely. The carbamate formation has been proposed to
take place through a single-step termolecular reaction, or through a two step mechanism
with a zwitterionic intermediate. Quantum mechanical calculations suggest that if there is
such a zwitterionic intermediate, it is likely to be short-lived.
Quantum mechanical calculations together with solvation models are shown to predict
the base strength and carbamate stability of different amine solvents with a useful degree of
accuracy. Solvent effects and electron donation and withdrawal through bonds are identi-
fied as important factors in determining the overall reactivity of different amine solvents.
Results suggest a strong correlation between the carbamate stability and base strength of
amine solvents and their reaction kinetics.
# 2007 Elsevier Ltd. All rights reserved.
avai lab le at www.sc iencedi rec t .com
journal homepage: www.e lsev ier .com/ locate / i jggc
1. Introduction
There is at present great interest both in finding optimal
solvents for CO2 absorption and in finding the optimal process
conditions for a given solvent. Detailed understanding of the
chemistry is of great value in accomplishing both of these
tasks. For simple aliphatic amines, the species formed are
known and the overall reactions are reasonably well under-
stood (Versteeg et al., 1996). There is, however, uncertainties
regarding some mechanisms that have not been resolved by
experimental work (Versteeg et al., 1996). Quantum mechan-
ical calculations can be used to directly study a given reaction
mechanism, thereby providing new insight into which
reaction mechanisms are most likely.
Over the years a number of different amine solvents have
been studied in the context of CO2 absorption. Kinetic and
* Corresponding author.E-mail address: [email protected] (E.F. da Silva).
1750-5836/$ – see front matter # 2007 Elsevier Ltd. All rights reserveddoi:10.1016/S1750-5836(07)00022-9
equilibrium data have been reported and in many cases there
is a good understanding of the chemistry. There has, however,
been a limited understanding of the relationship between the
molecular structure of the solvent and chemical equilibrium.
2. Computational chemistry
Quantum mechanics offers the possibility of calculating a
large number of chemical properties from first principles, with
little or no experimental input. As availability of computa-
tional resources has increased, the application of quantum
mechanical calculations has grown. Such calculations are
today successfully used to study and predict molecular
structure, reaction mechanisms, thermodynamics and spec-
troscopic properties. A general presentation on main the
.
Fig. 1 – Species formed in solution.
i n t e r n a t i o n a l j o u r n a l o f g r e e n h o u s e g a s c o n t r o l 1 ( 2 0 0 7 ) 1 5 1 – 1 5 7152
applications of quantum mechanics and other forms of
computational chemistry can be found in the textbook
‘‘Essentials of computational chemistry’’ (Cramer, 2002).
The computation time for quantum mechanical calcula-
tions increases with the quality of calculations and the size of
the system. Such calculations are therefore quite successful in
calculating gas phase reaction energies (examples are work by
Smith and Radom, 1993; East et al., 1997; da Silva, 2005).
Determining reaction energies in solution directly from
quantum mechanical calculations is, however, a very challen-
ging task. In a solution, there are very large numbers of
molecules interacting and experimentally observed properties
represent averages over large ensembles, accurate calcula-
tions on such large systems are extremely time-consuming. A
widely used approach to calculate reaction energies in
solution is to first calculate reaction energies in gas phase
and then calculate the solvation energy with some form of
solvation model (Cramer, 2002). Solvation models are based on
some simplified representation of the solvent, common forms
are continuum models, where the solvent is represented as a
dielectric continuum, and explicit models where solvent
molecules are usually given a simplified molecular mechanics
representation (some form of ball-and-stick model with fixed
charges). Orozco and Luque (2000) provide a broad review of
solvation models. In calculations, where quantum mechanical
calculations and solvation models are combined, the solvation
models are usually expected to be the main source of
uncertainty.
Fig. 2 – Transition state of bicarbonate formation.
3. Methods
In the present work, reaction mechanisms are studied by
calculations in vacuum, solvent molecules are added to
capture their direct contribution to reactions. This is quali-
tative approach, intended to address the likelihood of a
reaction taking place. These calculations were carried at the
Hartree-Fock level in the Spartan 04 program.
For the calculation of basicity in solution (pKa of the
conjugate base of a amine) a combination of quantum
mechanical gas phase energies and a continuum solvation
model is utilized. Gas phase energies were calculated at the
B3LYP/6-311++G(d,p) level, while the zero-point energy and
thermal corrections were calculated at the HF/6-31G(d) level.
This level of theory has been shown to be reasonably accurate
for the calculation of gas phase basicities (da Silva, 2005).
Solvation energies were calculated with the SM 5.42 R model
(Li et al., 1999) on HF/6-31G(d) level geometries. The reported
mean absolute error for neutral solutes for this model is
0.46 kcal/mol, while it is 3.8 kcal/mol for ions (Li et al., 1999).
The present basicity calculations are an extension to pre-
viously published work by the present authors (da Silva and
Svendsen, 2003). Gas phase energies were calculated in
Gaussian98 (Frisch et al., 1998) while solvation energies were
calculated in the Gamesol program (Xidos et al., 2002).
Many of the amines in the present study are highly flexible
molecules that may take on a number of conformers in
aqueous solution. As in our previous work, the overall
approach has been to assume that conformers identified as
the most stable in the gas phase, are also the most stable in
solution. While it is a reasonable assumption, it does add a
layer of uncertainty to the results.
4. Reaction mechanisms
4.1. Bicarbonate formation
CO2 reacts in aqueous amine systems to form either
bicarbonate or carbamate. These species are shown in
Fig. 1. The R groups in NR2 can be a proton or any form of
substituent group.
The formation of bicarbonate from CO2 and water is a well
known reaction in chemistry. There are three (related)
mechanisms for this reaction.
CO2 þH2OÐH2CO3 (1)
CO2 þOH�ÐHCO�3 (2)
H2CO3 þOH�ÐHCO�3 þH2O (3)
Bicarbonate can again be deprotonated by a base molecule
(B).
HCO�3 þ BÐCO�23 þ BHþ (4)
The base molecule is usually an amine molecule or a
hydroxyl ion (OH�). By itself bicarbonate formation is,
however, a rather slow reaction. It has been observed that
this reaction proceeds more quickly in the presence of amine
molecules, an effect beside the direct effect of the amines as
bases (Donaldsen and Nguyen, 1980). It is also known that
Fig. 3 – Mechanism of catalyzed bicarbonate formation.
Fig. 4 – Zwitterion mechanism. Water as base molecule.
Fig. 6 – Ethanolamine carbamate interacting with a water
molecule.
i n t e r n a t i o n a l j o u r n a l o f g r e e n h o u s e g a s c o n t r o l 1 ( 2 0 0 7 ) 1 5 1 – 1 5 7 153
Brønsted bases can act to catalyze the formation of bicarbo-
nate (Sharma and Danckwerts, 1963).
Calculations for this mechanism were performed with one
water molecule and one CO2 molecule in the presence of an
Ethanolamine molecule. The determined transition-state
geometry at the HF/6-31G(d,p) level is shown in Fig. 2.
This transition state is consistent with the mechanism
proposed by Donaldsen and Nguyen (1980) (Fig. 3):
This reaction may be written in the following form:
CO2 þH2Oþ BÐHCO�3 þ BHþ (5)
At the HF/6-31G(d,p) level, the barrier to bicarbonate
formation with Ethanolamine as a base was found to be
29.5 kcal/mol. For the bicarbonate formation in water a
reaction-barrier of 42.5 kcal/mol has been reported with the
same type of calculation at the same level of theory (Nguyen
et al., 1997). While neither of these calculations is quantitative
in nature, the results do suggest that the presence of
Ethanolamine significantly lowers the reaction barrier.
While this mechanism is usually mentioned in the context
of tertiary amines, it is probably not unique to this class of
molecules. The calculations suggest that this reaction will take
place as long as the base functionality is of appropriate
strength and accessible to the solvent water molecules.
4.2. Carbamate formation
The carbamate formation is one of the main reactions of CO2
absorption. Two mechanisms have been proposed for this in
the literature. One is the zwitterion mechanism originally
proposed by Caplow (1968) (Fig. 4).
In this mechanism, CO2 forms a bond to the amine
functionality in a first step. In a second step, an amine-proton
is transferred to a base molecule. Crooks and Donnellan (1989)
proposed the following single-step mechanism (Fig. 5).
Fig. 5 – Single-step carbamate formation mechanism.
Here, B is a base molecule. In this mechanism, the bonding
between amine and CO2 and the proton transfer take place
simultaneously.
The present authors have in previous work concluded that
experimental data can be accounted for by both mechanisms
(da Silva and Svendsen, 2004). Quantum mechanical calcula-
tions suggest that any zwitterion species is likely to be
unstable (da Silva and Svendsen, 2004; Ohno et al., 1999). This
suggests three possible mechanisms, depending on the nature
of the zwitterion. The zwitterion may be an entirely transient
state (giving a single-step mechanism), it may be a short-lived
species or it may be a transition state. The overall reaction may
in general be written in the following form:
CO2 þAmþ BÐAmCO�2 þ BHþ (6)
4.3. Carbamate as reaction intermediate
It has been suggested that carbamate undergoes a direct
hydrolysis reaction (Smith and Quinn, 1979), meaning a direct
reaction with water to form bicarbonate and amine. In
quantum mechanical, calculations no reaction path or
transition-state was found for such a mechanism. Fig. 6
shows a HF/3-21G(d) geometry of a water molecule interacting
with a carbamate species. Other forms of interaction were also
considered, but the general conclusion from the calculations is
that the carbamate CO2-group carbon is unlikely to participate
in any reaction except reversal back to CO2 and amine.
It is known that in a CO2–water–amine system there may be
shifts in concentration between carbamate and bicarbonate
species. Such shifts can, however, readily be accounted for by
reactions (1)–(6), all of which are reversible.
4.4. Alcohol-group bonding to CO2
It has been suggested that at very high pH values, CO2 can
bond to alcohol-groups (Jørgensen and Faurholt, 1954).
Calculations at the HF/3-21G(d) level with Ethanolamine as
reactant and base suggest a mechanism analog to that of
carbamate formation (Fig. 7):
Fig. 7 – CO2 bonding to alcohol groups. Fig. 8 – General reaction with CO2.
i n t e r n a t i o n a l j o u r n a l o f g r e e n h o u s e g a s c o n t r o l 1 ( 2 0 0 7 ) 1 5 1 – 1 5 7154
This reaction is, however, in general not expected to play a
significant role in industrial CO2 absorption processes as the
pH of the system is usually not high enough for this reaction to
take place (Versteeg et al., 1996).
4.5. Other reactions
The amines are organic bases that may undergo the following
reaction:
BþH2OÐBHþ þOH� (7)
Finally, there is the self-dissociation of water:
H2OÐHþ þOH� (8)
Table 1 – Experimental and calculated basicity data
No. Compound Acronym Exp
1 Ammonia
2 Methylamine
3 Dimethylamine
4 Trimethylamine
5 Piperidine
6 Piperazine
7 Morpholine
8 Pyrrolidine
9 Ethyleneamine
10 2,2,6,6 Tetramethyl-4-piperidinol TMP
11 Ethanolamine MEA
12 2-Amino-2-methylpropanol AMP
13 1-Amino-2-Propanol MIPA
14 N-N-Butylethanolamine BEA
15 2-Methylaminoethanol MMEA
16 3-Amino-1-propanol MPA
17 Ethylenediamine EDA
18 Diethanolamine DEA
19 Diisopropanolamine DIPA
20 N-Methyldiethanolamine MDEA
21 Diglycolamine DGA
22 Triethanolamine TEA
23 o-Methylhydroxylamine
24 Ethanimidamine
25 Diethylaminoethanol DEMEA
26 N-(2-hydroxyethyl) ethylenediamine AEEA
27 Diethanoltriamine DETA
28 N,N-Dimethylethanolamine DMMEA
29 2-Diisopropylaminoethanol DIPMEA
a Relative gas phase protonation energies. Energies calculated at B3LYP/6
calculated at HF/6-31G(d) level.b Solvation energy of amine. Calculation is SM 5.42R/HF/6-31G(d)//HF/6-3c Solvation energy of protonated amine. Calculation is SM 5.42R/HF/6-31d Relative protonation energies (basicity) in solution.e First protonation constant: 1, Pearson (1986); 2, Perrin (1965); 3, Hoff (2
4.6. Reaction summary
It is noteworthy that all the reviewed reactions with the CO2
molecule can be summarized as a nucleophile attack on the
CO2-carbon (Fig. 8).
B is again a base molecule and AH is any molecule with a
free-electron pair and a hydrogen atom on the same site.
5. Equilibrium constants and structure
In Table 1, experimental basicity data are shown together with
calculated values for gas phase basicity, solvation energies
tl pKa at 25 8C DGpga DGs
b DGs(H+)c DGps
d
9.31 0.0 �4.9 �87.2 0.0
10.652 10.2 �5.1 �76.4 �0.9
10.82 17.9 �3.8 �67.1 �1.1
9.82 22.2 �3.0 �59.4 �3.7
11.122 24.2 �4.3 �61.7 �0.8
9.832e 23.3 �9.0 �66.2 �1.9
8.4922 17.0 �7.2 �67.7 �4.8
11.32 23.6 �6.0 �63.9 �0.9
10.782 14.3 �4.9 �72.7 �0.2
10.052 29.7 �5.6 �56.2 �2.0
9.52 16.2 �9.0 �70.7 �4.4
9.722 23.6 �7.0 �64.0 �1.7
9.462 17.9 �8.4 �70.3 �2.5
9.93 27.6 �6.3 �60.2 �0.9
9.82 23.0 �7.4 �64.6 �2.2
10.02 23.4 �9.2 �67.6 �0.5
9.922 22.7 �9.3 �69.3 0.4
8.962 28.2 �12.9 �61.5 �5.5
8.892 31.8 �10.7 �57.3 �3.9
8.522 32.2 �11.2 �56.6 �4.7
9.462 26.6 �11.3 �66.0 �1.0
7.762 32.7 �17.9 �60.0 �3.0
4.62 �3.3 �4.8 71.9 �13.7
12.42 31.4 �10.0 �65.6 4.7
9.752 31.6 �4.6 �52.8 �2.5
9.822e 28.6 �11.1 �64.6 �0.2
9.82 32.6 �11.1 �61.0 0.2
9.232 27.0 �6.0 �57.7 �3.6
9.972 34.7 �2.9 �48.1 �2.4
-311++G(d,p) level with thermal corrections and zero-point energies
1G(d) level.
G(d)//HF/6-31G(d) level.
003).
Fig. 9 – Calculated basicity vs. experimental basicity. Gray
crosshairs are flexible amines, with potential uncertainty
in conformer form, while black crosshairs are rigid
molecules.
Fig. 10 – Plot of logarithm of experimental reaction rate vs.
calculated carbamate stability (da Silva and Svendsen,
2006).
i n t e r n a t i o n a l j o u r n a l o f g r e e n h o u s e g a s c o n t r o l 1 ( 2 0 0 7 ) 1 5 1 – 1 5 7 155
and basicity in solution. The computational results are only
used to predict basicites, and basicity results are shown as
values relative to ammonia. For the solvation energies of the
amines and their protonated forms the absolute values are
shown (more negative values indicating higher solvability).
In Fig. 9, basicites from computational chemistry calcula-
tions are plotted against experimental values. In the plotted
results, piperazine is given it’s experimental pKa value and all
calculated values are relative to this value. The grey line
indicates the theoretical relationship between calculated and
experimental values, i.e. if the model had been perfect all
points should fall on this line. While most of the amines in the
study are of direct relevance to CO2 absorption, o-methylhy-
droxylamine (lowest pKa in plot) and ethanimidamine (highest
pKa in the plot) are mainly included to show the overall
robustness of the predictions. While the calculations are not
entirely accurate, they are capable of predicting if a base is
very strong or very weak.
Fig. 10 shows a previously published plot (da Silva and
Svendsen, 2006) of calculated carbamate stabilities versus the
logarithm of experimental reaction rates (second-order rate
constant). There is very little reliable experimental data
available on the equilibrium constants of carbamate forma-
tion and logarithm of the rate of reaction was chosen as a
proxy variable for carbamate stability. The underlying
assumption is that the rate of reaction increases proportion-
ally with increasing stability of the carbamate species. The
calculated energy (DGc2s) is for the reaction given in Eq. (6),
where the base molecule is a second amine molecule.
Both Figs. 9 and 10 show fairly good correlation between
modeled values and experimental data. While not entirely
accurate, the models give a good qualitative picture of the
relationship between molecular structure and the stability of
different species formed.
The contributions to stability of species in solution can be
separated into stability through bonds, steric repulsion
between non-bonded groups, intramolecular hydrogen bond-
ing and solvation effects. The stabilizing effect of the solvent
depends on the accessibility of the solute surface to the
solvent, this is of particular importance for ions. Examples of
this can be seen in Table 1; ammonia is a relatively weak base
in gas phase, but protonated ammonia has a high degree of
solvent stabilization resulting in fairly strong basicity in
solution. Triethanolamine is on the other hand, a strong base
in the gas phase, but as a tertiary amine it has a congested
amine functionality resulting in low solvability for the
protonated form and relatively low basicity.
Alcohol groups in the molecular structure tend to reduce
the basicity of amines, while alkane groups tend to increase
the basicity. By adding an alcohol group to ethyleneamine
ethanolamine is formed, the addition of this groups leads to a
drop in base strength of over 1 pKa unit. Ethylamine, having a
methyl group more than methylamine, has a somewhat
higher pKa. These effects are mainly due to stabilization
through bonds.
There has in the literature on CO2 absorption been a
tendency to only consider sterical hindrance when discussing
differences in reactivity towards CO2 between different
solvents. While sterical hindrance may play a role in affecting
reactivity, other effects such as electron donation through
bonds and solvation effects are in many cases likely to be at
least as important in accounting for overall reactivity. This
conclusion is in part supported by the breakdown of
contributions to stability in the computational chemistry
models. Experimental data also show large variations in
i n t e r n a t i o n a l j o u r n a l o f g r e e n h o u s e g a s c o n t r o l 1 ( 2 0 0 7 ) 1 5 1 – 1 5 7156
activity towards CO2 between amines that are not sterically
hindered.
6. Reaction kinetics
The kinetics of CO2 in aqueous amine systems is of great
importance in determining the viability of a given solvent. Fast
kinetics is by itself preferable as a given degree of CO2
separation can be achieved with a smaller absorption column
than would be the case with slower kinetics. General insight
into differences in kinetics between different amines is
therefore of importance in solvent selection.
We suggest that that there is a simple overall correlation
between the kinetics and the free energy for the main
reactions of CO2 absorption, these reactions being carbamate
formation and bicarbonate formation. The kinetics of carba-
mate formation is significantly faster than that of bicarbonate
formation (Versteeg et al., 1996), and for a carbamate forming
system we would therefore expect the carbamate formation
kinetics to dominate. The results in Fig. 10 do strongly suggest
such a correlation between overall kinetics and free energy for
carbamate formation. For amines that do not form carbamate
the main reaction is bicarbonate formation, the free energy of
reaction is in this case a function of the base strength of the
amine. In Fig. 11, the base strength of tertiary amines (that do
not form carbamate) are plotted against kinetic data (second-
order rate constants, data from Versteeg et al., 1996). Again a
fairly strong correlation can be seen between the free energy of
reaction and rate of reaction. These observed correlations
between free energies of reaction and kinetics, suggest that
reaction kinetics can be predicted from equilibrium data.
This observed relationship between chemical equilibrium
and kinetics do have implications for the search for solvents
with optimal properties. Ideally, one might want a solvent
with fast kinetics and low reaction energies. Since these
characteristics are inversely proportional the focus should
Fig. 11 – Brønsted plot for tertiary amines in aqueous
solutions. Data from Versteeg et al. (1996).
perhaps be on finding the optimal tradeoff between desired
kinetics and reaction energies.
7. Conclusion
The review of reaction mechanisms suggest that the absorp-
tion of CO2 in aqueous amine systems can be accounted for
with a small set of reactions. Base-catalyzed bicarbonate
formation is found to be a likely mechanism for all amines
with appropriate base strength. It would seem unlikely that
the carbamate species undergo direct conversion to bicarbo-
nate species. Carbamate formation seems likely to proceed
either as a single-step termolecular reaction or through a two
step reaction, with a short-lived zwitterion intermediate.
The strength of amines as bases and the stability of the
carbamate species they form are determined by a number of
factors. Solvent stabilization, electron donation and with-
drawal through bonds, and sterical effects all play a part. In the
literature on CO2 absorption, too much attention has perhaps
been given to sterical effects in explaining variations in
reactivity.
There appears to be strong correlations between carbamate
stability, base strength and the reaction kinetics of different
amine solvents. For carbamate forming solvents, the reaction
kinetics can be estimated from the reaction energy of
carbamate formation. For solvents that do not form carbamate
(mainly tertiary amines) the kinetics can be estimated from
the base strength. The correlation between equilibrium and
kinetics should be taken into account in the search for optimal
solvents for a given absorption process.
r e f e r e n c e s
Caplow, M., 1968. Kinetics of carbamate formation andbreakdown. J. Am. Chem. Soc. 90, 6795–6803.
Cramer, C.C., 2002. Essentials of Computational Chemistry. JohnWiley & Sons, UK.
Crooks, J.E., Donnellan, J.P., 1989. Kinetics and mechanism ofthe reaction between carbon dioxide and amines inaqueous solution. J. Chem. Soc. Perkins Trans. II, 331–333.
da Silva, E.F., 2005. Comparison of quantum mechanical andexperimental gas phase basicities of amines and alcohols. J.Phys. Chem. A 109, 1603–1607.
da Silva, E.F., Svendsen, H.F., 2003. Prediction of the pKa valuesof amines using ab initio methods and free energyperturbations. Ind. Eng. Chem. Res. 42, 4414–4421.
da Silva, E.F., Svendsen, H.F., 2004. Ab Initio study of thereaction of carbamate formation from CO2 andalkanolamines. Ind. Eng. Chem. Res. 43, 3413–3418.
da Silva, E.F., Svendsen, H.F., 2006. Study of the carbamatestability of amines using ab initio methods and free-energyperturbations. Ind. Eng. Chem. Res. 45, 2497–2504.
Donaldsen, T.L., Nguyen, Y.N., 1980. Carbon dioxide reactionkinetics and transport in aqueous amine membranes. Ind.Eng. Chem. Fundam. 19, 260–266.
East, A.L.L., Smith, B.J., Radom, L., 1997. Entropies and freeenergies of protonation and proton-transfer reactions. J.Am. Chem. Soc. 119, 9014–9020.
Frisch, M.J., Trucks, G.W., Schlegel, H.B., Scuseria, G.E., Robb,M.A., Cheeseman, J.R., Zakrzewski, V.G., Montgomery Jr.,J.A., Stratmann, R.E., Burant, J.C., Dapprich, S., Millam, J.M.,
i n t e r n a t i o n a l j o u r n a l o f g r e e n h o u s e g a s c o n t r o l 1 ( 2 0 0 7 ) 1 5 1 – 1 5 7 157
Daniels, A.D., Kudin, K.N., Strain, M.C., Farkas, O., Tomasi,J., Barone, V., Cossi, M., Cammi, R., Mennucci, B., Pomelli, C.,Adamo, C., Clifford, S., Ochterski, J., Petersson, G.A., Ayala,P.Y., Cui, Q., Morokuma, K., Malick, D.K., Rabuck, A.D.,Raghavachari, K., Foresman, J.B., Cioslowski, J., Ortiz, J.V.,Baboul, A.G., Stefanov, B.B., Liu, G., Liashenko, A., Piskorz,P., Komaromi, I., Gomperts, R., Martin, R.L., Fox, D.J., Keith,T., Al-Laham, M.A., Peng, C.Y., Nanayakkara, A.,Challacombe, M., Gill, P.M.W., Johnson, B., Chen, W., Wong,M.W., Andres, J.L., Gonzalez, C., Head-Gordon, M., Replogle,E.S., Pople, J.A., 1998. Gaussian 98, Revision A. 9. Gaussian,Inc., Pittsburgh, PA.
Hoff, K.A., 2003. Unpublished results from work at departmentof Chemical engineering. The Norwegian University ofScience and Engineering.
Jørgensen, E., Faurholt, C., 1954. Reactions between carbondioxide and amino alcohols. Acta Chem. Scand. 8, 1141–1144.
Li, J., Zhu, T., Hawkins, G.D., Winget, P., Daniel, A., Liotard, D.A.,Cramer, C.J., Truhlar, D.G., 1999. Extension of the platformof applicability of the SM5.42R universal solvation model.Theor. Chem. Acc. 103, 9–63.
Nguyen, M.T., Raspoet, G., Vanquickenborn, L.G., Van Duijnen,P.T., 1997. How many water molecules are actively involvedin the neutral hydration of carbon dioxide. J. Phys. Chem.101, 7379–7388.
Ohno, K., Inoue, Y., Yoshida, H., Matsuura, E., 1999. Reaction ofaqueous 2-(N-methylamino)ethanol solutions with carbondioxide. Chemical species and their conformations studiedby vibrational spectroscopy and ab initio theories. J. Phys.Chem. A 103, 4283–4292.
Orozco, M., Luque, J.F., 2000. Theoretical methods for thedescription of the solvent effect in biomolecular systems.Chem. Rev. 100, 4187–4225.
Pearson, R.G., 1986. Ionization potentials and electron affinitiesin aqueous solution. J. Am. Chem. Soc. 108, 6109–6114.
Perrin, D.D., 1965. Supplement 1972. Dissociation Constants ofOrganic Bases in Aqueous Solution. Butterworths, London.
Sharma, M.M., Danckwerts, P.V., 1963. Catalysis by Brønstedbases of the reaction between CO2 and water. Trans.Faraday Soc. 59, 386–395.
Smith, B.J., Radom, L., 1993. Assigning absolute values to protonaffinities: a differentiation between competing scales. J. Am.Chem. Soc. 115, 4885–4888.
Smith, D.R., Quinn, J.A., 1979. The prediction of facilitationfactors for reaction augmented membrane transport. AIChEJ. 25, 197–200.
Spartan 04 Wavefunction Inc. 18401 Von Karman Avenue, Suite370, Irvine, CA 92612.
Versteeg, G.F., van Dijck, L.A.J., van Swaaij, W.P.M., 1996. On thekinetics between CO2 and alkanolamines both in aqueousand non-aqueous solution. An Overview. Chem. Eng.Commun. 144, 113–158.
Xidos, J.D., Li, J., Zhu, T., Hawkins, G.D., Thompson, J.D.,Chuang, Y.-Y., Fast, P.L., Liotard, D.A., Rinaldi, D., Cramer,C.J., Truhlar, D.G, 2002. Gamesol-version 3.1. University ofMinnesota, Minneapolis, based on the General Atomic andMolecular Electronic Structure System (GAMESS) asdescribed in Schmidt, M.W., Baldridge, K.K., Boatz, J.A.,Elbert, S.T., Gordon, M.S., Jensen, J.H., Koseki, S.,Matsunaga, N., Nguyen, K.A., Su, S.J., Windus, T.L., Dupuis,M., Montgomery, J.A., 1993. J. Comp. Chem., 14, 1347.