C4Im3S dissolved homogeneously in [C4mim][Tf2N] without
disruption of the hydration state.
There was an obvious liquid–liquid phase separation
between the IL phase and aqueous ZI phase upon adding
further water to the mixture (>1 : 8). We determined the
water content of the separated IL phase of the mixture
(the molar ratio of C4Im3S, [C4mim][Tf2N], and water was
1 : 1 : 9) by the Karl–Fischer titration method. The water
content was 1.8 wt%, indicating that most C4Im3S had
transferred to the aqueous phase. After the phase separation,
we found that all cyt.c had transferred from the IL phase to
the aqueous ZI phase. This result clearly shows that the
recycling of [C4mim][Tf2N] and the re-extraction of cyt.c were
both facilitated by simple addition of excess water. This is the
basis for a novel reaction–extraction process for bio-related
polymers.
Fig. 4 DSC profiles of C4Im3S after mixing with differing amounts
of water.
In conclusion, we have demonstrated that the saturated
water content of hydrophobic [C4mim][Tf2N] is controlled
accurately up to 17.8 wt% by mixing with C4Im3S in suitable
proportions. The drastic change in the saturated water content
of the hydrophobic [C4mim][Tf2N] involves water molecules
bound strongly to the C4Im3S (8 water molecules per C4Im3S).
This study was supported by a Grant-in-Aid for Scientific
Research from the Japan Society for the Promotion of Science
(No. 21225007).
stabilisation of cyt.c in [C4mim][Tf2N] are accomplished by
adding the C4Im3S–water mixture.
Since hydrophobic [C4mim][Tf2N] has no capability to
dissolve cyt.c, it is plausible that the hydration state of
C4Im3S affects the stable dissolution of cyt.c. Nikawa et al.
analysed the hydrated state of choline dihydrogenphosphate-
type ILs by means of differential scanning calorimetric (DSC)
measurement, and found that the superior hydrated state of the
IL facilitated the stable dissolution of proteins.18 Accordingly,
we also analysed the hydration state of C4Im3S after mixing
with different amounts of water. Fig. 4 shows typical DSC
heating curves of C4Im3S after mixing with differing amounts
of water (the heating rate was 5 1C minÀ1). C4Im3S formed a
homogeneous solution when more than 6 water molecules were
added per C4Im3S molecule. In DSC heat-flow profiles of the
mixture (the mole fraction of C4Im3S to water was 1 : 6), there
was no endothermic peak due to melting of water. This implies
that the added water in the solution exists as non-freezing water
which interacted strongly with C4Im3S. In the case of the
C4Im3S–water mixture with a molar ratio of 1 : 8, both
exothermic and endothermic peaks were observed, at around
À50 1C and À20 1C, respectively. These peaks are characteristic
of freezing bound water, which is often seen in biocompatible
polymers.19,20 In the case of C4Im3S–water mixtures with a
molar ratio exceeding 1 : 10, the exothermic peak disappeared
completely, and only an endothermic peak was observed. This
endothermic peak is known to be derived from ‘‘free’’ water
molecules that do not interact strongly with the ions. These
results indicate that C4Im3S forms a ‘‘hydrated ZI’’, in which
water molecules interact strongly with C4Im3S when 6 to
8 water molecules are added for each C4Im3S molecule. The
[C4mim][Tf2N]–C4Im3S–water mixture formed a clear homo-
geneous solution. This result suggests that the hydration state
of C4Im3S would be maintained in the hydrophobic
[C4mim][Tf2N]. To check this, we measured the DSC of the
hydrated C4Im3S–[C4mim][Tf2N] mixture (the molar ratio
of C4Im3S, [C4mim][Tf2N], and water was 1 : 1 : 8). The
endothermic peak derived from freezing bound water was also
observed in this mixture (see ESI,w Fig. S1). It is apparent that
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11222 Chem. Commun., 2012, 48, 11220–11222
This journal is The Royal Society of Chemistry 2012