Beilstein J. Org. Chem. 2014, 10, 774–783.
of ada for monomer 4 and two equivalents of ada for dimer 6 in aqueous solution by self-inclusion, are accessible by external
were required to saturate the chemical shifts of the cavity guest molecules while the strength of binding does not seem to
proton, H3, suggesting full binding capacity of all available decrease by the presence of the linker moieties, compared to the
cavities. When the chemical shift changes of H3 [Δδ(CD-Η3] of parent β-CD. In addition to closed configurations of 4 and 6 in
(
Figure 1), the resulting curve nearly coincided with that of the rations are additionally present, which promote intermolecular
curve of monomer 4. The striking similarity of the induced aggregation and can account for the slow Brownian motion of
chemical shift displacements of CD-Η3 for 4 and 6, reveal a the dimer in the aqueous solution. The fact that in DMSO the
similar mode of inclusion, simultaneous and independent for linkers prefer to reside over the cavity indicates that intermedi-
each cavity of 6 and subsequently very similar association ate conformations, between extended and self-included may
constants. Indeed, non-linear fitting of the observed shifts to a exist in water as well.
43] showed that the association constants, as logK, are in the Computational results
of β-CD alone with the same guest [44]. Therefore the strength mer 4 and dimer 6 at the PM3 level of theory for isolated mole-
of the binding did not reveal severe competition from the phen- cules, as well as in the presence of solvent (water) at the
yl groups of the spacers.
PM3(COSMO) level of theory in order to assess solvation
effects. For critical configurations of 4, the PM3 results were
compared against those calculated by DFT at the B3P86/6-
3
1G(d',p') level of theory. The average structural deviation of
the PM3 geometries from those derived at the B3P86/6-
1G(d',p') level was reasonably small, 0.015 Å for bond lengths,
whereas for bond and dihedral angles the average deviation was
.1 and 7.2 degrees, respectively. Several initial geometries
3
2
with a varying degree of phenyl groups’ orientation and prox-
imity to β-CD (stemming mainly from the torsional flexibility
of the aminopropylamino–spacer moiety) were fully optimized
at the PM3(COSMO) and PM3 level of theory. The calculated
geometries were sorted out into three limiting configurations: i)
open, in which the phenyl rings are positioned on the exterior of
β-CD, ii) vicinal, in which two phenyl rings are close to the pri-
mary side rim of β-CD and iii) inclusion, in which one phenyl
ring penetrates inside the β-CD cavity. A gauche–trans (gt)
arrangement of the C5-C6OH moieties in 4 was found to
disfavor the inclusion configuration by more than 10 kJ/mol,
due to the subsequent contraction of the primary entrance of the
β-CD cavity, compared to a gauche–gauche (gg) arrangement.
Figure 1: 1H NMR chemical shift change (Δδ) of CD cavity Η3 signal
of compounds titrated with 1-adamantylamine·HCl (ada) in D2O
(500 MHz, 298 K): a) monomer 4 (1 mM, filled squares, solid line) and
b) dimer 6 (1 mM) (empty squares, dotted line) plotted per cavity vs ½
concentrations of ada.
from the HSQC spectra) and H5, H6’, is evident from the 2D with a mixed inclusion/vicinal configuration (Figure 3c) being
wider side, the phenyl moieties are lifted over the narrow with phenyl groups immersed in both β-CD cavities (Figure 3d)
opening. In both molecules ada is inserted with the amino are the least stable by PM3(COSMO) (in the presence of water),
group protruding from the wider β-CD side (Figure S7).
although highly favorable by PM3 (in the absence of solvent).
This was attributed to insufficient hydration of the primary
In summary, NMR experiments have shown that the com- hydroxy groups due to steric crowding around the primary sides
pounds, although they form intra- and intermolecular complexes of the two β-CD tori. The DFT energies for critical configura-
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