In the case of the 24C8 complexes, the resonances due to
NH2, CH2, and ortho aromatic C-H protons were shifted
downfield relative to the free axle, which is indicative of
hydrogen bonding. Thus in solution, a total of eight hydrogen
bonds are responsible for maintaining the [2]pseudorotaxane
structure (see Table 1).
ether used, the association constants are higher for the axles
bearing electron withdrawing CF3 groups (versus OCH3) as
would be expected on a purely electrostatic basis resulting
in increased ion dipole interactions and stronger NH‚‚‚O and
CH‚‚‚O hydrogen bonding. (2) Similar to the trend exhibited
by dibenzylammonium axles9 and contrary to that observed
for bis(pyridinium)ethane cations,3 higher Kassoc were ob-
served with 24C8 than with DB24C8. This can be attributed
to the better ability of aliphatic ether oxygen atoms to engage
in ion-dipole interactions and hydrogen bonding relative to
the aromatic catechol oxygen atoms. (3) For pseudorotaxanes
formed with 24C8, an EWG is more effective when placed
on the anilinium ring than the benzyl ring consistent with
NH‚‚‚O hydrogen bonding being a major contribution to the
overall Kassoc. (4) There appears to be significant π-stacking
involved in binding when DB24C8 is the wheel as indicated
by upfield shifts for meta protons A2 and B2. The π-stacking
is influenced equally by the inclusion of electron withdrawing
groups on either the benzyl or anilinium ring and is
magnified considerably when both rings contain the electron-
withdrawing CF3 (see Figure 3).10 This is reminiscent of the
Table 1. Summary of Changes in Chemical Shift (∆δ in ppm)
of the [2]Pseudorotaxanes Relative to the Free Axlesa
complex
B2
B1
Bn
A1
A2
[1a⊂24C8]+
+0.07
+0.12
+0.09
+0.14
-0.24
-0.13
-0.34
-0.18
+0.26
+0.29
+0.26
+0.28
+0.01
+0.13
-0.04
+0.07
+0.58
+0.55
+0.58
+0.55
+0.76
+0.73
+0.77
+0.72
+0.36
+0.39
+0.25
+0.27
+0.09
+0.11
+0.19
+0.22
-0.03
+0.02
+0.11
+0.09
-0.29
-0.37
-0.16
-0.21
[1b⊂24C8]+
[1c⊂24C8]+
[1d⊂24C8]+
[1a⊂DB24C8]+
[1b⊂DB24C8]+
[1c⊂DB24C8]+
[1d⊂DB24C8]+
a Positive: downfield shift; negative: upfield shift.
For the DB24C8 adducts, the signals due to NH2 and CH2
protons were shifted downfield, but due to the lower basicity
of the aromatic oxygen atoms on the crown ether, there are
not significant aromatic CH‚‚‚O interactions, regardless of
the substituent group on the axle. However, the resonances
due to the hydrogen atoms in meta positions on the CF3-
substituted rings are shifted upfield because of the shielding
generated by the ring current of the catechol rings on the
crown ether, indicating the presence of π-stacking interac-
tions in a fashion similar to that observed in the bis-
(pyridinium)ethane [2]pseudorotaxanes (see Table 1).
Due to the presence of simultaneous equilibria between
protonated/nonprotonated and complexed/uncomplexed spe-
cies, an equation was derived (see the Supporting Informa-
tion) to determine the association constants (Kassoc) from the
measured experimental constant (Kexp), the acidity constant
of the thread (Ka) and the solution concentration of thread
at equilibrium that is nonprotonated, [A]. The concentration
of (A) was calculated from integration and the observed
chemical shift of the uncomplexed peak in the NMR
spectrum. The results are summarized in Table 2.
Figure 3. Bar graph comparing the relative association constants
for the four different axles with 24C8 and DB24C8. For comparison
purposes, the two sets of data have been normalized to 1d+.
trends observed for bis(pyridinium)ethane cations and DB24C8
and is probably a direct result of the observed anti conforma-
tion of the two atom bridge between the aromatic rings.
In a fashion similar to that for the dibenzylammonium
axles,11 the addition of one equivalent of base (triethylam-
mine) to solutions containing the [2]pseudorotaxanes caused
Table 2. Summary of Equilibrium Constantsa
24C8
DB24C8
pKa
Kexp
Kassoc
Kexp
Kassoc
1a
1b
1c
1d
2.7
2.8
4.3
4.3
1163
1274
1569
364
2604
2329
1605
371
655
237
310
84
1100
322
314
85
(8) Perrin, C. L.; Dwyer, T. J. Chem. ReV. 1990, 90, 935-967.
(9) Ashton, P. R.; Bartsch, R. A.; Cantrill, S. J.; Hanes, R. E., Jr.;
Hickingbottom, S. K.; Lowe, J. N.; Preece, J. A.; Stoddart, J. F.; Talanov,
V. S.; Wang, Z.-H. Tetrahedron Lett. 1999, 40, 3661-3664.
(10) (a) Hunter, C. A.; Sanders, J. K. M. J. Am. Chem. Soc. 1990, 112,
5525-5534. (b) Hunter, C. A.; Lawson, K. R.; Perkins, J.; Urch, C. J. J.
Chem. Soc., Perkin Trans. 2 2001, 651-669.
a The values for pKa and Kexp were obtained using 0.01 M solutions in
CD3CN at 25 °C. Kassoc were calculated using the following equation (see
the Supporting Information): Kassoc ) Kexp(1 + (Ka/[A])).
(11) (a) Montalti, M.; Ballardini, R.; Prodi, L.; Balzani, V. Chem.
Commun. 1996, 2011-2012. (b) Ashton, P. R.; Ballardini, R.; Balzani, V.;
Gomez-Lopez, M.; Lawrence, S. E.; Martinez-Diaz, M. V.; Montalti, M.;
Piersanti, A.; Prodi, L.; Stoddart, J. F.; Williams, D. J. J. Am. Chem. Soc.
1997, 119, 10641-10651.
Four general observations can be made regarding the
measured association constants. (1) Regardless of the crown
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