E.V. Ivanov, D.V. Batov / Thermochimica Acta 620 (2015) 59–64
61
Table 2
found to be the following: 2.61 (s, 3Н, Me), 5.14 (d, 1H, CH, J = 8.2),
o
2
Standard molar enthalpies of dissolution, ꢀsolH , of the studied glycoluril-
derivatives in water at different temperatures, T, and p = 99.6 kPa.
5
1
.20 (d, 1H, CH, J = 8.2), 7.25 (s, 1H, NH), 7.27 (s, 1H, NH), 7.44 (s,
H, NH) for 2-MMGU and 2.61 (s, 6H, 2Me), 5.10 (s, 2H, 2CH), 7.52
a
T/K
m/{mol (kg H2O)−
}
1
b
Nc
ꢀsolHo ± ıH /(kJ mol−1)d
(
s, 2H, 2NH) for 2,6-DMGU. These results, being presented graph-
ically (in the form of spectrograms) as a Supplementary material
Figs. S1 and S2), are in good agreement with those existing in the
literature [1,5,12]. As for 2,4,6-TMGU, we have presented here the
2
2
-Monomethylglycoluril
(
278.15
0.0057–0.0091
0.0075–0.0109
0.0136–0.0154
0.0117–0.0141
0.0125–0.0145
0.0103–0.0153
4
5
4
4
4
5
23.00 ± 0.04
23.05 ± 0.03
23.44 ± 0.06
24.00 ± 0.08
24.76 ± 0.08
25.19 ± 0.08
2
79.15
288.15
98.15
1
13
relevant H NMR and C NMR data for this glycoluril-derivative in
DMSO-d6 at T = 300 K for the first time (earlier [4], the data on ı in
CDCl3 at the same temperature were published only). The results
also were provided as a Supplementary material, in the form of
detailed NMR-spectrograms (see Figs. 3S and 4S).
2
308.15
313.15
2
,6-Dimethylglycoluril
278.15
0.0062–0.0075
0.0052–0.0055
0.0050–0.0059
0.0101–0.0109
0.0043–0.0068
0.0048–0.0050
4
4
4
4
4
4
11.92 ± 0.04
12.02 ± 0.04
12.94 ± 0.12
13.88 ± 0.06
14.93 ± 0.03
15.40 ± 0.09
In Table 1, data on melting point, Tmp, and standard molar
279.15
288.15
o
2
enthalpy of the fusion (melting), ꢀfusH , for the investigated
2
3
3
98.15
08.15
13.15
glycoluril-derivatives are shown together with values, being found
in other sources. The results of thermal analysis of the samples were
derived from heating curves in the melting region using a mul-
tipurpose differential scanning calorimeter DSC 204 F1 Phoenix
2
2
2
,4,6-Trimethylglycoluril
78.15
79.15
0.0077–0.0095
5
4
5
4
5
4
3.28 ± 0.06
3.40 ± 0.06
4.63 ± 0.09
5.91 ± 0.13
7.32 ± 0.08
7.98 ± 0.06
(
Netzsch-Gerätebau GmbH, Germany). As follows from data of
0.0066–0.0073
0.0048–0.0071
0.0058–0.0086
0.0051–0.0078
0.0049–0.0075
Table 1, our values of Tmp are in fairly good agreement with the
results reported by other authors, perhaps, with the exception of
the quantity for 2,4,6-TMGU. We believe that it may be mainly
due to differences in details of the experimental procedure. Unfor-
tunately, there is no information on ways of the preparing and
thermal testing the 2,4,6-TMGU sample in the work [4], whereas
288.15
298.15
3
3
08.15
13.15
a
The expanded uncertainties, U, do not exceed: U(m) = ± 0.0001 mol kg−1
,
U(T) = ± 0.001 K and U(p) = ± 0.8 kPa (level of confidence = 0.95).
b
c
m
2
The molality range in which the ꢀsolH values were averaged.
The number of independent measurements of ꢀsolH2
ıH is the half-width of a 95% confidential interval for ꢀsolH .
in our case, the most accurate method of measuring tmp was
m
.
o
2
d
o
2
employed. It is worthy of noticing also the fact that the ꢀfus
H
value decreases with sequential increasing the number of methyl
groups on the N(2)-, N(4)-, and N(6)-sited positions in a gly-
coluril’s molecule. Going from 2-MMGU to 2,6-DMGU and further
to 2,4,6-TMGU, this tendency becomes decreasingly pronounced
interaction is to be weaker than the interaction between solute
molecules in their own crystal substance. Indeed, since the stan-
dard state is understood as the state of a hypothetically ideal
solution or gas phase [16,17], the hydration of a solute can be iden-
tified with the condensation of 1 mol of its gaseous (monomeric)
(
see Table 1).
After and before experiments, each glycoluril’s sample was
stored in a light-proof vacuum dessicator over P O5. The water (of
2
natural isotope composition) was deionized and then twice dis-
tilled in a Pyrex-glass apparatus up to electrical conductivity of
1
molecules in an infinitely large amount of a solvent [18].
−
6
−1
.
1
.5 × 10 S cm
o
As the temperature rises, the ꢀsol
H
values become increas-
m
2
2
The molality-dependent molar enthalpies of solution, ꢀsol
H
,
o
ingly positive (see in Table 2). Interestingly, ꢀsol
the same manner as it is observed in the case of changing ꢀfus
H
decreases in
2
of the glycolurils compared were measured using an ampoule-type
o
H
2
sealed microcalorimeter with isothermal shell. The setup was fit-
(Table 1) on going from 2-MMGU to 2,6-DMGU and further to 2,4,6-
3
ted with a 60 cm titanium vessel. The procedure for experimental
TMGU. It would be more “thermodynamically justified”, if a similar
measurements and testing the microcalorimeter were detailed pre-
o
correlation existed between ꢀ H and the molar enthalpy of sub-
m
2
sol
2
viously [13,14]. Four to five measurements of ꢀsol
m were performed at each temperature.
H
at different
o
o
limation, ꢀsub
H
(or hydration, ꢀhydrH ). But, due to the problem
2
2
of decomposition of glycoluril’s samples during their heating, we
o
2
were unable to derive the reliable information on ꢀsub
H
(using
the Knudsen’s effusion mass-spectrometric method [19]).
3
. Results and discussion
Such a distribution in the dissolution enthalpies (Table 2) is not
surprising. Here, the point is that the hydrophobicity of a solute
becomes increasingly pronounced in a sequence of 2-MMGU < 2,6-
DMGU < 2,4,6,8-TMGU (i.e., with the increase in the number of
methyl groups in a glycoluril’s molecule). When the specified
glycoluril-derivatives are subjected to dissolution in water, the
given circumstance should be manifested in the relative strength-
ening of hydrophobic constituent of a solute hydration.
The results of calorimetric measurements indicated that the
m
2
ꢀsol
H
values within the measurement error do not depend on
m at all the temperatures chosen. As a consequence, the values of
o
2
m
ꢀsolH were calculated as average-weighted |ꢀ H |av in the stud-
sol
2
m
2
ied range of m. The procedure for calculating |ꢀ H |av is described
sol
∞
previously [14,15]. The temperature-dependent data on ꢀ
H
sol
2
are tabulated in Table 2.
To understand a situation with enthalpy effects of dissolu-
Data of Table 2 point out the fact that the process of dissolution
tion more clearly, heat capacity changes in the specified process,
of all three glycoluril-derivatives in water is endothermic over
the whole temperature range of interest. A positive sign at ꢀsol
o
p,2
ꢀsol
C
, for all aqueous glycoluril-derivatives under study, must
o
H
2
be considered, too. We have attempted to do it below.
suggests that the total energy released during the formation of
heterocomponent H bonds and from hydrophobic hydration of a
solute (the exothermic contribution) does not replace all of the
energy spent to destroy a glycoluril’s crystal lattice and to form
the cavity in the solvent (the endothermic contribution). The
latter process is accompanied by the disturbance of the hydrogen-
bonded network of water in the nearest environment of the
solute glycoluril-derivative. In other words, the glycoluril–water
1
Here, the point is that the evaporation or sublimation process at standard state
can be identified with the opposite process of condensation where the solute is
postulated to be solvated in its own environment. Hence the sign and quantity of
the standard enthalpy of dissolution are being determined by the difference between
solute–solvent and solute–solute interactions [18].