Beilstein J. Org. Chem. 2014, 10, 825–831.
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Table 1: ILGM ratios for the recognition of the three pairs of L-leucine
isomers by templates 1 and 2.
pair of isomers
1
2
Figure 4: ESI-mass spectrum (positive mode) of a 1:1:1 mixture of 1,
protonated L-leucine methyl ester (LeuOMe), and protonated
L-isoleucine trideuteromethyl ester (IleOMe-d3) in a 1:1 mixture of
CH2Cl2/MeOH (m/z = 792.4 LeuOMe–1, m/z = 795.5 IleOMe-d3–1).
L-NleOMe/L-IleOMe
L-IleOMe/L-LeuOMe
L-NleOMe/L-LeuOMe
1.5
0.7
1.0
1.2
0.8
0.9
is tuned in a way that it does not allow detection of such low
molecular mass ions with the necessary accuracy. Hence, we
optimized our ESI conditions using larger and well-detectable These ratios translate into the following relative affinities of our
protonated amino acid esters like protonated phenylalanine receptors:
benzyl ester to make sure that the conditions are mild enough
not to cause dissociation.
Receptor 1: L-NleOMe ≈ L-LeuOMe > L-IleOMe
Having made sure that the method is in principle suitable to Receptor 2: L-LeuOMe ≥ L-NleOMe > L-IleOMe
study the recognition of protonated amino acid derivatives in a
taken into account: non-covalent isotope effects [23] might also cases although the effect is not large enough yet to think about
cause significant differences of the signals’ intensities. There- an application for the separation of the isomers on a larger scale
fore, every experiment has to be repeated with the different via supramolecular transport, for instance. However, these
order of isotope labelling and in addition one should measure results are still promising with regard to the development of a
order to quantify this effect (Figure 5).
leucine which is obviously the most interesting challenge. The
non-covalent isotope effects clearly demonstrate that the ester
group of the amino acid derivative must interact with our
templates, and therefore, these effects tell us something about
within the host–guest complexes (Figure 6).
In fact, the deuterated guests were always bound less good than
the protiated guests. This can be rationalized by assuming
attractive dispersive interaction to play a significant role during
smaller van der Waals volume of the deuterated group [27-32].
In a first approximation, however, the dispersive interactions
get stronger with an increasing size of the volume and conse-
ability to interact via those interactions is weaker [33-35]. This
Figure 5: ESI-mass spectrum (positive mode) of a 1:1:1 mixture of 1,
protonated L-leucine methyl ester (LeuOMe), and protonated L-leucine
trideuteromethyl ester (LeuOMe-d3) in a 1:1 mixture of CH2Cl2/MeOH
(m/z = 792.4 LeuOMe–1, m/z = 795.5 LeuOMe-d3–1).
Table 1 lists the results of the ILGM measurements with regard observation perfectly agrees with the conclusion that the ester
to the affinity of templates 1 and 2 towards L-norleucine, group gets into close contact with the non-polar parts of the
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