Chemistry Reference
In-Depth Information
0.00
200
-0.05
-0.10
0 04060
T /
o
C
150
100
0.0 .2
0.4
0.6
0.8
1.0
α
Fig. 3.56
Conversion dependence of the effective activation energy for demixing of an aqueous
solution of triethylamine that takes place on heating. The inset shows a typical DSC curve of the
process measured at heating rate 1 ᄚC min
−1
the fit appears rather high, 117 3 kJ mol
−1
. The activation energy of diffusion in
liquids is about the same value as those of viscous flow [
148
]. For small spherical
molecules, the latter value is about one third of the vaporization enthalpy [
149
],
i.e., a few tens of kilojoules per mole. The obtained value is more characteristic
of large molecules [
148
]. However, triethylamine in water exists as relatively big
hydrated molecule, (C
2
H
5
)
3
ᄋ 2H
2
O [
150
], the diffusion of which is likely to involve
the breakage and restoration of hydrogen bonds that can create a significant energy
barrier. Note that a solution of triethylamine in water has viscosity that is about four
times larger than that of water [
150
]. It should also be noted that the activation ener-
gies of viscous flow in aqueous solutions of some amino acids have been reported
[
151
] to be around a 100 kJ mol
−1
.
Fig. 3.57
Temperature
dependence of the effective
activation energy derived
from
E
ʱ
versus
ʱ
dependence
(Fig.
3.56
). The
solid line
is
a theoretical fit by means of
Eq. 3.86
250
200
150
100
292
294
296
298
300
302
304
T / K
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