Paper
NJC
referenced internally for the 1H NMR using the solvent residual
peak of CD2Cl2 (d = 5.31 ppm). The UV/Vis absorption spectra
were measured on an MCS 400 diode-array spectrometer from
Carl Zeiss Jena with a resolution of 1 nm in 2 mm quartz cells.
Spectral analyses were performed with Aspect Plus (version
1.76, Carl Zeiss Jena). All spectroscopic data are available in
Tables S1 and S2 in the ESI.†
Acknowledgements
Financial support by the Deutsche Forschungsgemeinschaft
(DFG SP 392/45-1) is gratefully acknowledged. The authors
thank J. Kronawitt for her experimental work and Dr A. Seifert
for the fruitful discussions.
Notes and references
General synthesis of tri-n-alkylmethylammonium ILs/LTMSs
1 J. P. Hallett and T. Welton, Chem. Rev., 2011, 111, 3508–3576.
2 J. G. Huddleston, A. E. Visser, W. M. Reichert, H. D. Willauer,
G. A. Broker and R. D. Rogers, Green Chem., 2001, 3, 156–164.
3 P. Wasserscheid, M. Sesing and W. Korth, Green Chem.,
2002, 4, 134–138.
4 C. Reichardt, Green Chem., 2005, 7, 339–351.
5 A. J. Carmichael and K. R. Seddon, J. Phys. Org. Chem., 2000,
13, 591–595.
The ILs/LTMS were synthesized from the respective chloride
salt according to established literature procedures.38–42 In
general, tri-n-butylmethylammonium chloride (5 g) was dis-
solved in water (150 mL) and a solution of equimolar silver
salt (AgNO3, AgCF3CO2, AgCF3SO3, AgN(CN)2 [freshly synthe-
sized]); sodium salt (NaBF4) or lithium salt (LiNtf2) was added
dropwise. For the synthesis of tri-n-octylmethylammonium
ILs/LTMS tri-n-octylmethylammonium chloride was dissolved
in a H2O/DCM solution (50 : 50% v/v). When using silver salts,
the formed solid was filtered and the solvent removed by rotary
distillation. Insoluble products that were generated by using
sodium salts were filtered off and washed several times with the
reaction solvent. All the products were dried as described above
and characterized via NMR spectroscopy, IR spectroscopy,
quantitative elemental analysis and DSC measurements.
¨
6 H. Weingartner, Angew. Chem., Int. Ed., 2008, 47, 654–670.
´
´
7 J. Catalan, J. Palomar, C. Dıaz and J. L. G. de Paz, J. Phys.
Chem. A, 1997, 101, 5183–5189.
´
´
´
´
8 J. Catalan, C. Dıaz, V. Lopez, P. Perez, J.-L. G. De Paz and
´
J. G. Rodrıguez, Liebigs Ann., 1996, 11, 1785–1794.
9 R. Lungwitz, M. Friedrich, W. Linert and S. Spange, New
J. Chem., 2008, 32, 1493–1499.
10 V. Selvamani, V. Suryanarayanan, D. Velayutham and
S. Gopukumar, J. Solid State Electrochem., 2016, 20, 2283–2293.
11 N. Terasawa and K. Asaka, Sens. Actuators B Chem., 2014,
193, 851–856.
Methodology for determination of the empirical polarity
parameters (theoretical background see ref. 19)
´
The innovation of the Catalan scale in comparison to the
12 N. L. Nguyen and D. Rochefort, Electrochim. Acta, 2014, 147,
96–103.
Kamlet–Taft scale is the differentiation between solvent polarity
and polarizability. Therefore, it is necessary to use dyes which
are unaffected by hydrogen bonds and respond in different
degrees to polarity and polarizability. The chromophore pair
Th and BMN have been developed by us as appropriate dyes
for this.
´
13 U. Domanska and M. Wlazło, Fuel, 2014, 134, 114–125.
14 B. Qiu, B. Lin, L. Qiu and F. Yan, J. Mater. Chem., 2011, 22,
1040–1045.
15 V. Kumar, V. S. Parmar and S. V. Malhotra, Biochimie, 2010,
92, 1260–1265.
´
The Catalan acidity parameter (SA) can be calculated by the
´
16 W. L. Hough, M. Smiglak, H. Rodrıguez, R. P. Swatloski,
sole use of eqn (12). For this purpose, the UV/Vis absorption
S. K. Spear, D. T. Daly, J. Pernak, J. E. Grisel, R. D. Carliss,
M. D. Soutullo, J. H. Davis and R. D. Rogers, New J. Chem.,
2007, 31, 1429–1436.
˜
˜
maxima vmax of the Fe indicator are measured in the ILs. Dv
values are used in 10ꢀ3 cmꢀ1
v Fe solv: ꢁ 10ꢀ3 cmꢀ1 ꢀ 16:255
ꢀ3:62047
Þ
~ð Þð
17 B. S. Sekhon, Ars Pharm., 2013, 54, 37–44.
18 S. Spange, R. Lungwitz and A. Schade, J. Mol. Liq., 2014, 192,
137–143.
SA ¼
(12)
The SB parameter can be determined by simultaneous use of
19 A. Schade, N. Behme and S. Spange, Chem. – Eur. J., 2014,
20, 2232–2243.
20 L. Cammarata, S. G. Kazarian, P. A. Salter and T. Welton,
Phys. Chem. Chem. Phys., 2001, 3, 5192–5200.
˜
ABF and DMeABF. vmax (DMeABF) is not affected by the solvent
basicity. Therefore, the SB paramꢀe3ter can be calculated by
eqn (13), where Dv values are in 10 cmꢀ1
.
˜
~
~
DvðABFÞ ꢀ DvðDMeABFÞðsolv:Þ ꢀ 2:84647
SB ¼
(13)
¨
21 K. Bica, M. Deetlefs, C. Schroder and K. R. Seddon, Phys.
ꢀ3:62047
Chem. Chem. Phys., 2013, 15, 2703–2711.
22 P. G. Jessop, D. A. Jessop, D. Fu and L. Phan, Green Chem.,
2012, 14, 1245–1259.
23 C. Chiappe, C. S. Pomelli and S. Rajamani, J. Phys. Chem. B,
2011, 115, 9653–9661.
The solvent polarity SdP and polarizability SP can be separately
calculated from eqn (14) and (15) using the UV/Vis absorption
maxima of Th and BMN measured in the particular IL.
˜
˜
SP = 0.387vmax(Th)(solv.) ꢀ 0.605vmax(BMN)(solv.) + 8.500
24 L. P. Novaki and O. A. El Seoud, Ber. Bunsenges. Phys. Chem.,
1996, 100, 648–655.
(14)
˜
˜
¨
SdP = 0.556vmax(BMN)(solv.) ꢀ 0.980vmax(BMN)(solv.) + 3.791
25 T. Cremer, C. Kolbeck, K. R. J. Lovelock, N. Paape, R. Wolfel,
(15)
P. S. Schulz, P. Wasserscheid, H. Weber, J. Thar, B. Kirchner,
New J. Chem.
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