The length of the dicarboxylic acids was such that proto-
nation at one of the ‘interior’ faces preorganised the proto-
nation of the second ‘interior’ face (especially in the case of the
more rigid TFTA) such that the intramolecular cooperativity
led to cavity-specific recognition of the dicarboxylic acids.
This left the smaller mono-functional TFA to satisfy the
requirement for protonation and anion complexation at the
‘exterior’ faces.
Further characterisation of the acid–porphyrin host–guest
complexes was provided by nano-ESI mass spectrometry. Two
peaks were recorded for 1 at 902 and 1803 m/z for the 2+ and
1+ charge states (Fig. S17, ESIw). Peaks corresponding to the
freebase dimer 1 were again recorded in the presence of TFA
together with additional signals (Fig. S18, ESIw). In this case,
no signals were observed for the 1ꢀTFA4 complex unlike the
assemblies characterised by NMR spectroscopy (Fig. 2). How-
ever, under the same conditions, the MS results of the dimer
with HFGA and TFTA (with TFA to cap the ‘exterior’ faces)
were able to support the NMR characterisation. The spectrum
of the acid–porphyrin dimer with HFGA (1ꢀHFGA) was
dominated by a peak at 1022 m/z, assigned to the 2+ charge
state of the complex (Fig. S19, ESIw). The equivalent
experiment with TFTA generated a spectrum for 1ꢀTFTA
also dominated by the diprotonated state of the host–
guest complex at 1021 m/z (Fig. S20, ESIw). These two
results with the diacids are consistent with the structures
shown in Scheme 3 in the absence of the exterior bound
TFA molecules.
Scheme 3 Two schematic representations of the 1ꢀHFGA–TFA2 (left)
and 1ꢀTFTA–TFA2 (right) porphyrin dimer complexes.
strong bonds with the carboxylates of the acids, and stacking
interactions operate in the cavity between two neighbouring
aromatic groups bound to the two ‘interior’ faces of the
porphyrins. In the protonation mechanism5 the plane of one
porphyrin must distort in order to accommodate the extra
protons, and the additional distance required to form the
(weak) interaction with the carboxylate anion creates a micro-
environment that inhibits protonation with the second porphyrin
of the dimer.
The monometallation of 1 can be achieved by adding less
than one equivalent of a zinc salt but this typically leads to
a mixture of the freebase, mono-zinc, and di-zinc dimers
which are extremely difficult to separate chromatographically.
In our previous work5 we identified the significance of the
role of the anion in the zinc metallation of porphyrins. The
1ꢀPFBA2 system offered the opportunity to investigate
the potential for selectively mono-metallating the dimer by
directing the metallation using the PFBA to ‘activate’ a single
porphyrin core (Fig. S11 and S12, ESIw). Unfortunately,
the lability of the acid–porphyrin complex resulted in scram-
bling of the Zn metallation that ultimately led to the same
unsatisfactory mixture of products according to our NMR
spectroscopy.
In conclusion, we have exploited the restricted cavity of the
freebase porphyrin dimer 1 and its unique capacity for proto-
nation and anion complexation to selectively accommodate
diacid guests into the core whilst using NMR spectroscopy
together with the diamagnetic ring currents of the porphyrins
to better understand the complexation behaviour of (fluori-
nated) acids. The use of nano-ESI mass spectrometry (not
previously reported for comparable complexes) provided an
additional technique for characterisation of more elaborate
complexes using these ‘weak’ interactions. The lability of the
complexation has directed us to explore the cavity of analogous
cyclic hosts as potential ‘reaction centres’.
In order to establish the competitive binding preference of a
mixture of acids, 1 was challenged with a 1 : 1 mixture of TFA
and PFBA. Only a mixture of complexes was identified in
solution, with no preference for the acids for the ‘interior’ or
‘exterior’ faces of the host (Fig. S13, ESIw).
We thank the EPSRC for financial support (studentship
for MJW).
In contrast, mixtures of TFA and dicarboxylic acids such as
HFGA or TFTA did show site-specific preference, and the
complexes (Scheme 3) were characterised by 1H (Fig. S14 and
S15, ESIw) and 19F NMR spectroscopy. For example, a single
peak (indicative of symmetry) was identified for the TFTA
ligand of the 1ꢀTFTA–TFA2 complex at ꢁ148.6 ppm in the
19F NMR spectrum (Fig. S16, ESIw), compared to the chemical
shift of ‘free’ acid at ꢁ141.3 ppm. One single TFA resonance
was observed at ꢁ78.2 ppm. The chemical shift implies that the
anions were bound to the ‘exterior’ faces of the complex whilst
the absence of a second resonance at 253 K (Fig. S3, ESIw)
suggests one chemical environment and assembly symmetry.
Similar structural features were identified for 1ꢀHFGA–TFA2.
Notes and references
1 (a) H. L. Anderson and J. K. M. Sanders, J. Chem. Soc., Perkin
Trans. 1, 1995, 2223–2229; (b) H. L. Anderson, S. Anderson and
J. K. M. Sanders, J. Chem. Soc., Perkin Trans. 1, 1995, 2231–2245;
(c) S. Anderson, H. L. Anderson and J. K. M. Sanders, J. Chem.
Soc., Perkin Trans. 1, 1995, 2247–2254.
2 (a) C. J. Walter, H. L. Anderson and J. K. M. Sanders, J. Chem.
Soc., Chem. Commun., 1993, 5, 458–460; (b) L. G. Mackay,
R. S. Wylie and J. K. M. Sanders, J. Am. Chem. Soc., 1994, 116,
3141–3142.
3 J. C. Hawley, N. Bampos and J. K. M. Sanders, Chem.–Eur. J.,
2003, 9, 5211–5222.
4 Y. Mizuno and T. Aida, Chem. Commun., 2003, 20–21.
5 M. J. Webb and N. Bampos, Chem. Sci., 2012, 3, 2351–2366.
c
9360 Chem. Commun., 2012, 48, 9358–9360
This journal is The Royal Society of Chemistry 2012