Two-Protonic Acid Ionic Liquid and Esterification
C
As one can see in Fig. S3 (see Supplementary Material), the
þ
complete deprotonation of the sulfuric acid likely occurs by
TMDP under our reaction conditions.
protons of .NH2 disappeared in D O due to fast hydrogen
2
exchange with the deuterium of D O.
2
The carbons of new IL are detected at 43.57, 35.64, 32.95,
8.57, and 22.76 ppm and 44.15, 34.97, 32.76, 28.37, 22.29 ppm
Physical Properties of [TMDPH ][SO ]
2
4
2
in DMSO-d and D O, respectively (see Supplementary Mate-
The bulk amount of [TMDPH ][SO ] could be liquefied at
2
4
6
2
,
1108C in an oil bath (mp 74–758C). The ionic conduction
rial, Figs S4 and S5).
The 2D COSY spectra of new IL displayed correlations
ꢀ1
value (s) of new IL was 1.82 ꢁ 0.04 mS cm at 858C. The total
water content of [TMDPH ][SO ] was determined 0.18 ꢁ 0.02
þ
2
4
between the acidic protons of .NH at 8.46 and 8.17 ppm with
2
wt-% under ambient humidity and temperature. Although
[TMDPH ][SO ] was soluble in water, dimethyl sulfoxide,
0
0
the equatorial and axial protons of C2, C2 , C6, C6 at 3.23 and
2
2 4
.82 ppm, respectively (see Supplementary Material, Fig. S6).
The reaction of TMDP and sulfuric acid was also carried out
in CH Cl at a ratio of 1 : 1 at room temperature overnight, which
gave a white solid. The H and C NMR spectra of the TMDP
and sulfuric acid at a ratio of 1 : 1 were recorded in DMSO-d6
methanol, and acetic acid, it was immiscible with ethanol,
acetonitrile, ethyl acetate, acetone, chloroform, dichlor-
omethane, and n-hexane at room temperature.
2
2
1
13
Thermal Behaviour of [TMDPH ][SO ]
2
4
(see Supplementary Material, Fig. S7). One and two equi-
valent(s) of sulfuric acid (98 %) was then directly added to the
NMR tube containing TMDP and sulphuric acid at a ratio of 1 : 1
The thermal behaviour of [TMDPH
][SO ] was investigated by
4
2
a differential scanning calorimetry (DSC) plot in two cycles
over temperature ranges of 30–300 and 30–5008C (see Sup-
plementary Material, Fig. S12). DSC of pure TMDP has been
1
in DMSO-d , and the H NMR spectra were recorded (see
Supplementary Material, Fig. S8).
6
[
26]
The single peak of water at 3.92 ppm moved to the downfield
region, and a broadened multiplet and singlet signal were
observed at 4.45–4.43 and 6.96 ppm, respectively (see Figs
S7a, S8a, and S8b, Supplementary Material). The C NMR
spectra showed negligible shifts before and after adding sulfuric
1
acid. The H NMR spectrum of sulfuric acid was also investi-
previously reported in the literature, and it displays two sharp
and one broad endothermic peak centred at 58, 110, and 3328C.
The peaks at 52.3 and 332.58C were attributed to the melting and
boiling points of TMDP, respectively. The second endothermic
broad peak at a range of 76–1578C was attributed to the
desorption of trapped moisture in TMDP.
1
3
gated, which showed a relatively sharp singlet at 7.13 ppm in
DMSO-d (see Supplementary Material, Fig. S9).
Under a nitrogen atmosphere and at a range of 30–3008C,
three sharp and one weak endothermic peak(s) were displayed
on the DSC curve of [TMDPH ][SO ], and no exothermic peak
2 4
6
1
The H NMR spectrum of new IL did not show any peaks at a
region of 4.38–5.25. Moreover, no sharp or broadened peak was
detected at a range of 4.0 to 8.5 ppm and above 9.5 ppm.
Therefore, the existence of excess sulfuric acid or formation
of an acidic anion, namely hydrogen sulfate, could be excluded.
The infrared spectrum of new IL is shown in Figure S10 (see
was observed. The first sharp peak was assigned to the melting
of the IL which began at 85.28C and ended at 111.78C with a
ꢀ1
latent heat of fusion of 140.8 J g , which was in good agree-
ment with the obtained melting point achieved using an open
capillary tube in a B u¨ chi B-545 apparatus (mp 74–758C). The
second endothermic sharp peak was observed in the range
131.3–175.58C centred at 160.28C, which was assigned to the
dehydration and degassing of the IL with a latent heat of
ꢀ1
Supplementary Material). The broadened peak at 3407 cm
can be attributed to the N–H vibration mode at the .NH
þ
2
ꢀ1
groups. Two bands at 3034, 2923, and 1321 cm were assigned
to the symmetric, antisymmetric stretching vibrational, and
wagging mode of methylene groups in the piperidinium rings,
respectively. All absorption peaks at a range of 2848 to
ꢀ1
evaporation of 38.0 J g . Two sharp peaks were observed at a
range of 248.2 to 294.78C, which were assigned as the boiling
point decomposition of [TMDPH ][SO ] due to an appreciable
2 4
ꢀ1
2
shift towards this region are probably due to the strong interac-
524 cm were assigned to the N–H stretching band and their
loss of weight, a remarkable change in heat capacity of the
sample, and an exothermic baseline shift. The latent heat of
evaporation and decomposition of the [TMDPH ][SO ] were
þ
tions between .NH and the sulfate anion through hydrogen
2
2
4
[
bonding. The deformation vibration modes of .NH at 1616
28]
þ
ꢀ1
276.3 and 187.0 J g , respectively. There was no exothermic
and endothermic peak in the second cycle at a range of 30–
5008C, which supports the evaporation/decomposition of the
2
ꢀ
1
[28]
and 1462 cm are characteristic of secondary amine salts.
The asymmetric and symmetric SO2 stretching vibrations
ꢀ1
appeared at 1215, 1151, and 1029 cm , respectively. The
[TMDPH
Moreover, the thermal stability of [TMDPH ][SO ] was
2 4
2 4
][SO ] below 3008C in the first cycle.
ꢀ
1
sharp bands at 877 and 577 cm , as well as a medium band at
ꢀ
1
87 cm , were assigned to the S–O stretching modes and SO
4
bending, respectively.
studied in a temperature range from 30 to 8008C under a nitrogen
atmosphere through thermogravimetric analysis/differential
thermal analysis (TGA/DTA) (see Supplementary Material,
Fig. S13). Three peaks were observed on the DTA curve, and
2
[
29]
Electrospray ionisation–mass spectrometry (ESI-MS) analy-
ses in the negative and positive ionisation modes were conducted
on the sample. Both negative and positive ion modes of analysis
[TMDPH ][SO ] started to decompose at 2708C, which was in
2 4
gave sensitive and good spectra data. The positive ionisation
þ
good agreement with the result of DSC. The thermal decompo-
sition was mainly completed at 4508C. The first peak was
observed below 2008C with a maximum mass loss of 6.1 %;
this loss was related to the removal and evaporation of the
trapped and adsorbed moisture in [TMDPH ][SO ]. The second
2 4
and third peaks showed a maximum mass loss of 31.5 and
34.4 % at 250–290 and 290–3308C, respectively, which were
spectrum of the new ILrecordedprominent [Mþ EtOH þ NH ]
4
þ
and [M þ EtOH þ CO þ NH ] peaks (where M corresponds to
2
4
TMDP) at m/z 274.2753 and 318.3014, respectively (see Supple-
mentary Material, Fig. S11-A). Moreover, the negative ionisation
spectrum of the new IL displayed a weak ion at m/z 339.2005
ꢀ
assigned to [M þ H þ SO þ CH OH] (see Supplementary
4
3
Material, Fig. S11-B).
Based on our results, structure II was demonstrated for the
related to the total decomposition of [TMDPH
and TGA/DTA results showed that [TMDPH
mally stable up to 2708C, probably owing to the strong
2
][SO
4
]. The DSC
][SO
] is ther-
2
4
new IL evidencing it to be [TMDPH ][SO ], and indicate that
2
4