Open Access Article
E.
De Santis‡
*a,
A. A.
Edwards
a,
B. D.
Alexander
b,
S. J.
Holder
*c,
A.-S.
Biesse-Martin
de,
B. V.
Nielsen
b,
D.
Mistry
f,
L.
Waters
f,
G.
Siligardi
g,
R.
Hussain
g,
S.
Faure
de and
C.
Taillefumier
*de
aMedway School of Pharmacy, Universities of Kent and Greenwich at Medway, Central Avenue, Chatham Maritime, Kent ME4 4TB, UK. E-mail: emiliana.de.santis@npl.co.uk
bSchool of Science, University of Greenwich, Central Avenue, Chatham Maritime, Kent ME4 4TB, UK
cFunctional Materials Group, School of Physical Sciences, University of Kent, Canterbury, CN2 7NZ, UK. E-mail: S.J.Holder@kent.ac.uk
dUniversité Clermont Auvergne, Université Blaise Pascal, Institut de Chimie de Clermont-Ferrand, BP 10448, F-63000 Clermont-Ferrand, France. E-mail: claude.taillefumier@univ-bpclermont.fr
eCNRS, UMR 6296, ICCF, F-63178 Aubière Cedex, France
fDivision of Pharmacy and Pharmaceutical Sciences, University of Huddersfield, Queensgate, Huddersfield, HD1 3DE, UK
gDiamond Light Source Ltd, Diamond House, Harwell Science and Innovation Campus, Didcot, Oxfordshire OX11 0DE, UK
First published on 2nd November 2016
We describe the qualitative and quantitative analysis of the complexation properties towards cations of a cyclic peptoid hexamer composed of alternating α- and β-peptoid monomers, which bear exclusively chiral (S)-phenylethyl side chains (spe) that have no noticeable chelating properties. The binding of a series of monovalent and divalent cations was assessed by 1H NMR, circular dichroism, fluorescence and molecular modelling. In contrast to previous studies on cations binding by 18-membered α-cyclopeptoid hexamers, the 21-membered cyclopeptoid cP1 did not complex monovalent cations (Na+, K+, Ag+) but showed selectivity for divalent cations (Ca2+, Ba2+, Sr2+ and Mg2+). Hexacoordinated C-3 symmetrical complexes were demonstrated for divalent cations with ionic radii around 1 Å (Ca2+ and Ba2+), while 5-coordination is preferred for divalent cations with larger (Ba2+) or smaller ionic radii (Mg2+).
In the realm of peptidomimetics, α-peptoids (poly-N-substituted glycines) are particularly attractive architectures that were previously shown to bind metal ions forming metallopeptoids.4 Peptoid synthesis is straightforward and an extremely high diversity of side chains is accessible.5 Their head to tail macrocyclisation is also particularly facile due to the inherent flexibility of the peptoid backbone.6 This also applies to the formation of cyclic β-peptoids7 and analogous cyclic alternated α,β-peptoids.8
Cyclic α-peptoids with 3,9 4, 6, 8 and 10 residues have been shown to bind cations, particularly from the first group alkali metals with selectivity depending on the ring size.10 For example, 18-membered cyclohexamers showed a peak of selectivity for Na+ and metallated structures could be characterised in the solid state.10a,d These include the formation of the first supramolecular 1D metal–organic framework (MOF) based on a cyclic peptoid.10d In this MOF triggered by Na+, N-methoxyethyl coordinating side chains participate to generate the supramolecular assembly. Recently, binding of Gd3+ cations was also demonstrated by cyclic α-hexapeptoids characterized by the presence of six N-carboxyethyl side chains or three N-methoxyethyl and three carboxyethyl side chains in alternation.11 Interestingly, these side chains, which confer aqueous solubility to the complexes, do not appear to have any effective role in Gd3+ coordination.
Herein we present the first reported metal binding ability of a cyclic α,β-peptoid hexamer towards a selection of metal cations. The 21-membered cyclopeptoid cP1 is characterised by six chiral (S)-1-phenylethyl side chains (spe) that lack coordinating sites, so the binding was therefore envisaged via the backbone amides (Fig. 1).
Briefly, the linear precursor was composed of (S)-N-(1-phenylethyl)glycine and (S)-N-(1-phenylethyl)-β-alanine monomers in alternation and was synthesised by a solution-phase submonomer approach.12 The C-terminal tBu-capping group of the synthesised linear peptoid was cleaved using trifluoroacetic acid and subsequent HATU-mediated cyclisation led to cP1 in 64% yield (see ESI† for details).
| Cation | Ionic radiusa (Å) | Charge density (charge Å−2) | log Ka b |
|
|---|---|---|---|---|
a Ionic radius for coordination number VI.15a
b log ka values for Mn+ + nClO4− → Mn+(ClO4−)n in CH3CN.
|
||||
| +1 | Na | 1.02 | 0.076 | 0.91, 1.0015b |
| Ag | 1.15 | 0.060 | — | |
| K | 1.38 | 0.042 | 1.23, 1.5215b,c | |
| +2 | Mg | 0.72 | 0.307 | 2.26, 2.3715d |
| Zn | 0.74 | 0.291 | 1.6815e | |
| Fe | 0.78 | 0.262 | — | |
| Ca | 1.00 | 0.159 | 2.44, 2.7415d | |
| Sr | 1.18 | 0.114 | 2.5815d | |
| Ba | 1.35 | 0.087 | 2.6915d | |
| +3 | Fe | 0.55 | 0.789 | — |
![]() | ||
| Fig. 2 Binding of cP1 with perchlorate salts of divalent cations. Qualitative 1H NMR spectra of cP1 alone and in the presence of perchlorate salts at a molar ratio (metal/cP1) of 2. | ||
The 1H NMR spectrum of cyclopeptoid cP1 alone is characterised by a number of benzylic proton resonances between 5 and 6 ppm. This is indicative of the simultaneous presence of cis and trans amides along the backbone. According to literature, for pe side chains, 1H NMR resonances between 5.5 and 6 ppm are associated with benzylic protons on cis amides and those around 5 ppm are from benzylic protons on trans amides.17 The average amide cis/trans ratio was estimated to 75
:
25 in CD3CN (Fig. 2, 3 and S2†). The addition of a molar excess of metal ion typically resulted in a decrease of the signal around 6 ppm thus indicating an increased population of all-trans conformers. At the saturation point, no further changes of the 1H NMR spectrum and the cis/trans ratio were observed. To confirm this, a step-wise titration of strontium perchlorate into cP1 was performed in CD3CN (Fig. 3 and S3†). A simplification of the 1H NMR spectrum was observed in the region between 5 and 6 ppm. Specifically, increasing the molar ratio (Sr2+/cP1) from 0 to 3 determined a stepwise decrease of the peak around 5.8 ppm with a corresponding increase in the signal around 5 ppm (Fig. 3). This suggested that once the metal complex was formed, the cyclopeptoid cP1 adopted an all-trans conformation. A plot integration of peaks around 5.8 ppm versus the molar ratio clearly indicated that no further changes in the 1H NMR spectrum were observed after a 1
:
1 stoichiometry was reached. The 1H NMR spectrum of the Sr2+/cP1 complex showed a single set of signals for each α- and β-monomer which therefore was indicative of a discrete conformation with a 3-fold rotational symmetry. NMR temperature studies and 2D experiments enabled full proton assignment of the metal complex (Fig. S4 and Table S1†). Notably, the 1H NMR spectrum for the Ca2+/cP1 complex is very similar to that of the Sr2+/cP1 complex thus also indicative of a 3-fold symmetry (Fig. 2). In contrast the spectra for the Ba2+/cP1 and Mg2+/cP1 complexes, whilst simpler than that of the peptoid cP1 alone, are distinct from those of Sr2+/cP1 and Ca2+/cP1 complexes. For all of the metal complexes the cis to trans conversion was complete upon addition of an excess of metal. A cis to trans isomerisation was previously observed in cyclic α-peptoid binding cations.10a,18
The CD spectrum of cP1 is characterised by two negative maxima at 203 and 222 nm (Fig. 4). Similar CD spectra observed for α-peptoids in CH3CN have been assigned to helical conformations.21 However, due to the cyclic nature of the α,β-peptoid cP1, a helical conformation is unlikely and the spectrum may instead arise from a twisted-like conformation. Based on these observations and the complexity of the 1H NMR spectra at room temperature, the CD spectrum of cylopeptoid cP1 is likely to indicate the presence of multiple conformers rather than one dominant species and the [θ]203 nm of 268 × 103 is therefore taken to be indicative of this. In this case, this dynamic behaviour may be due to the intrinsic flexibility of the backbone derived from the presence of β-residues and the cis/trans isomerism of tertiary amides.
Consistently with 1H NMR data, no binding was observed with sodium and potassium cations as indicated by the lack of spectral changes in the far UV CD, which was also reported for silver, zinc and iron(II) (Fig. S6†). This was further confirmed for sodium and zinc by quantitative CD titrations in the far UV region (Fig. S7†). CD in the near UV and fluorescence spectroscopy also showed no significant spectral changes upon addition of sodium perchlorate to cP1 (Fig. S8†). In contrast, a significant change to the spectral features in the far UV was observed upon addition of perchlorate salts of Ba2+, Ca2+, Fe3+, Mg2+ and Sr2+ thus indicating metal complex formation (Fig. 4, S8 and S9†). Spectroscopic studies by fluorescence and in the near UV by CD showed significant changes upon addition of magnesium perchlorate to cP1 further supporting the metal binding (Fig. S8†).
Nearly identical spectral features were observed for cylopeptoid cP1 in the presence of Ca2+ or Sr2+. The CD spectra of these metal complexes were characterised by one negative maximum around 208 nm which was red shifted in comparison to the free cylopeptoid cP1. The CD spectrum in the presence of Ba2+ has two maxima (negative circa 204 nm, positive circa 227 nm). The CD spectrum of the Ba2+ complex has greater [θ] and the negative maximum is only marginally red shifted relative to cP1 and the corresponding Ca2+/Sr2+ complexes. The Mg2+/cP1 complex was characterised by a negative maximum at 198 nm and a positive maximum centred at 222 nm with a component at 216 nm. The CD spectrum in the presence of Fe3+ has two negative maxima (circa 197 nm and circa 210 nm) and shows similarity to the Mg2+ profile based on the blue shift of the negative maxima relative to cP1.
The similarity in appearance of the Sr2+/cP1 and Ca2+/cP1 CD spectra agrees well with the similarity of their 1H NMR spectra. The differences between the CD spectra of these two metal complexes and those with barium and magnesium were also reflected in their 1H NMR spectra suggesting distinct conformational differences. Notably, all metal complexes were found to have increased [θ] relative to cP1 alone which was also consistent with the 1H NMR observation of a conformational shift to population of all-trans isomers i.e. increased ordering of the conformational preference of cP1.
Os ligating Sr2+) and 6 co-ordinate species (6 C
Os ligating Sr2+) with the 4 co-ordinate systems possessing consistently higher heats of formation (ΔHf ∼ 275 kJ mol) than the 6 coordinate. At least two distinct co-ordination patterns involving 6 carbonyl co-ordination were observed, one with ΔHf values circa 220 kJ mol−1 involving two C
Os binding from above and four C
Os binding from below the Sr2+ cation, relative to the plane of the ring. In contrast, the conformers approaching C3 symmetric arrangement of C
Os about the Sr2+ (3 above and 3 below the plane of the ring) gave significantly lower ΔHf values, from ∼212 kJ mol−1 down to ∼192 kJ mol−1. Since C3 symmetry was confirmed by 1H NMR system with the lowest ΔHf was chosen to investigate the arrangement of ethylphenyl groups about the ring. Since the ethylphenyl groups displayed full unhindered rotation about the N–C bond this was an extensive conformational space. To facilitate the search a simple system of varying the arrangements of the ethylphenyl groups about the ring was adopted; in essence systematically changing the C–N–C–C dihedral angles to facilitate various conformational starting structures based upon the relative orientation of the phenyl group ‘above’ (up or u) or ‘below’ (down or d) the plane of the ring relative to the other groups. This analysis revealed a relatively flat potential energy surface about these conformers (Fig. S21†) with minimum energy conformers possessing ΔHf values from ∼180 to ∼196 kJ mol−1. However the conformations starting from the alternating ethylphenyl (ududud) starting point all gave lower heats of formation than any of the other arrangements. Two minimum energy conformers possessed C3 symmetry, one with ΔHf = 184.6 kJ mol−1 and one with ΔHf = 180.1 kJ mol−1. The geometries of these two conformers were then optimised using PM6 with the COSMO solvation model inherent in MOPAC. The former conformer did not give a vibrational spectrum without negative frequencies. The latter conformer with further optimisation gave rise to a Sr2+/cP1 complex with three-fold symmetry (C3) about the cyclic axis (Fig. 5 and S10†) with a vibrational spectrum free of negative frequencies. A similar procedure was adopted for the Ba2+ complex giving a Ba2+/cP1 complex with three-fold symmetry (C3) about the cyclic axis. This is in excellent agreement with the NMR spectra (Fig. 2). The average metal–O bond lengths were 2.49 (SD = ±0.05) Å for Sr–O and 2.35 (SD = ±0.04) Å for Ba–O.
![]() | ||
| Fig. 5 Minimum energy conformations for metal complexes predicted by PM6 (COSMO) calculations. Hydrogens are omitted for clarity. The Ca2+/cP1 complex is nearly identical to the Sr2+/cP1 complex (see ESI†). | ||
In contrast, the lowest energy conformers for both Mg2+/cP1 and Fe3+/cP1 complexes involved only 5 of the 6 carbonyls coordinating to the metal centre. For these complexes the average metal–O bond lengths for the 5 bonding carbonyls were 1.98 (SD = ±0.03) Å for Mg2+/cP1 and 1.91 (SD = ±0.06) Å for Fe3+/cP1 (Fig. 5 and S11a, c†). Consequently, these complexes possessed no symmetry beyond their identity; again, this is in accordance with the results from the 1H NMR for the Mg2+/cP1 complex (Fig. 2). Replacing the Mg2+ and Fe3+ ions in the sites of the Ca2+ or Sr2+ ions of the C3 symmetrical complexes and optimising the geometry led to stable symmetrical C3 complexes of these metals (Fig. S11b and d†) but their energies were significantly higher (Table S2†) than those illustrated in Fig. 5. Similarly transposing the Ca2+/cP1 and Sr2+/cP1 complexes into those with Mg2+ or Fe3+ led to rearrangement of the cyclic peptoid cP1 to facilitate 6 coordinate carbonyl binding once again. It is uncertain as to whether the metal complexes with Mg2+ and Fe3+ shown in Fig. 5 are absolutely the lowest energy conformers due to the range of conformational possibilities available to these complexes however they are significantly lower in energy than any 6 coordinate species found.
The Ba2+/cP1 complex also showed 5 coordinate carbonyl binding but unusually the cation itself was displaced from the plane of the peptoid resulting in close contacts with three of the phenyl groups (Fig. 5 and S12†). Thus average metal–O bond lengths for 3 of the bonding carbonyls were 2.76 (SD = ±0.03) Å and for the other two = 2.56 (SD = ±0.01), with the average C–Ba distance for the three coordinating phenyls being 2.74 (SD = ±0.12) Å. Again, this lack of symmetry was mirrored in the 1H NMR and support for the phenyl coordination comes from the appearance of an upfield shifted aromatic resonance at 6.51 ppm.
Overall, the semi-empirical modelling largely agrees with the CD spectra in that the spectra for Ca2+/cP1 and Sr2+/cP1 complexes are virtually identical in line with identical predicted conformations. The maxima for the complexes of Ba2+, Mg2+ and Fe3+ are distinct from those of Ca2+ and Sr2+. However, whereas the negative maxima occur at similar positions for Mg2+/cP1 and Fe3+/cP1 (circa 197 nm) that of the Ba2+/cP1 complex is unique (circa 204 nm) which is in line with the distinct conformation predicted by modelling. Interestingly the CD spectrum of the Fe3+/cP1 complex appears to consist of at least one more distinct peak at circa 210 nm; one possibility for this is that this peak arises from a certain proportion of the complexes in solution adopting the higher energy 6-coordinate C3 symmetry in equilibrium with the predominately 5-coordinate species.
980) at 230 nm as a function of the Sr2+ concentration yielded a dissociation constant (Kd) of 11.9 ± 0.5 μM when fitted to the Hill equation (R2 = 0.99) (Fig. 6B).22 It is of note that the value of the Kd was independent of the wavelength selected and the maximum at 231 nm was chosen due to the absence of any significant wavelength shift. The Kd was of the same order of magnitude as that previously reported for an α-peptoid hexamer with benzyloxyethyl (be) side chains which was shown to bind monovalent cations by quantitative 1H NMR.10a This similarity indicated that the α,β-peptoid backbone retained the ability to bind metal ions in the presence of the more flexible β-residues and different side chains, albeit with a different cation selectivity. No binding to the monovalent cations investigated was observed for cP1.
A Yoe–Jones plot23 where the differential molar ellipticity at the positive and negative maxima was plotted versus the molar ratio (Sr2+/cP1) gave a stoichiometric point of 1.6 as indicated by the projection of the inflection point on the x-axis (Fig. S13†). This was not consistent with the stoichiometry obtained by 1H NMR and may be rationalised on the basis of the higher sensitivity of CD to subtle conformational changes. Specifically, 1H NMR indicated changes to the cis/trans isomerisation up to a Sr2+/cP1 molar ratio of 1 indicating a 1
:
1 stoichiometry. Any further structural rigidification, which does not alter the cis/trans ratio or does not modify significantly the ring conformation would not be detected by 1H NMR. By contrast, these would be detected by CD (as an increased signal intensity) and may give rise to the higher stoichiometry observed in comparison to 1H NMR.
Interestingly, when looking at the intensity and wavelength position of the negative maximum at 207, whilst the intensity increases up to a molar ratio of 2, a significant wavelength shift only occurs up to a molar ratio of 1 (Fig. 6A and S14†). Based on these observations and supported by the PM6 calculation showing the 1
:
1 complex as the most favourable, it is reasonable to assume that the complex is characterised by a 1
:
1 stoichiometry and any further change in intensity of the CD signal is likely to result from further structural rigidification and an increased population of metal complexes. A similar trend was also observed for the other metal complexes (Fig. S14†) for which similar binding affinity was observed between each metal and cP1 (Table 2 and Fig. S15–S18†).
| Complex | K d (μM) | Stoichiometry (Mtn+/cP1) | |
|---|---|---|---|
| >210 nm | <210 nm | ||
| Sr2+/cP1 | 11.9 ± 0.5 | 1.6 | 1.6 |
| Mg2+/cP1 | 12 ± 0.2 | 1.5 | 1.5 |
| Ca2+/cP1 | 8.2 ± 0.3 | 1.1 | 1.04 |
| Ba2+/cP1 | 12.7 ± 8.6 | 1.1 | 1.2 |
| Fe3+/cP1 | 1.2 ± 0.9 | — | 1.5 |
The Mg2+/cP1 complex gave a Kd of 12 ± 0.2 μM by CD and this was largely comparable with that calculated by isothermal titration calorimetry (ITC),24 which yielded a Kd of the same order of magnitude (2.3 μM) (Fig. 6C). ITC also showed that the binding event was endothermic, as indicated by the positive values for the heat exchange and the enthalpy value (ΔHcal) of 6902 cal mol−1 with an entropic contribution (ΔScal) of 49.2 cal mol−1. Using ITC, the projection of the mid-point of the titration curve on the x axis provided the stoichiometry of the binding which was found to be close to 1
:
1 (metal/peptoid) suggesting an approximately equimolecular interaction. This stoichiometry was consistent with that deduced by CD and with the PM6 calculations for the Mg2+/cP1 complex. Unfortunately, quantitative studies by 1H NMR were hampered by the significant signal overlap (Fig. S19†).
With regard to the divalent cations, between each other the charge density is not the only criterion to be considered, as their difference in size also plays a significant role in their binding selectivity. The divalent cations with the smallest ionic radii (Mg2+, Zn2+ and Fe2+) bind to cP1 only if the associated charge density is very high. Thus, the hard Mg2+ cation binds to cP1 whereas the Zn2+ and Fe2+ cations having slightly lower charge density do not bind (Table 1). For the other divalent cations tested (Ca2+, Sr2+ and Ba2+), even though their charge density is lower, they have ionic radii ≥1 Å, thus are more adapted to the cavity size, which facilitate their complexation to cP1. Size of the cations also appears to influence the final conformation of the complexes i.e. when the cation radius is too large or too small the binding is 5 coordinate and 6 coordinate only obtainable for a specific range of ionic radii. Despite these observations, the case for the role of the ionic radius and charge density in predicting binding is not clear cut. It would appear that a number of factors involving size, charge density, enthalpy and entropy play a part for all of the species involved, namely the cation, anion, acetonitrile and peptoid. Surprisingly a clear correlation between the occurrence of binding is observed with the association constants of the metal perchlorates in acetonitrile (Table 1, Fig. 7). The metal perchlorates with low association constants in acetonitrile (log
Ka < circa 2) are not bound whereas all of the salts possesing Ka values roughly an order of magnitude larger were observed to bind.
![]() | ||
| Fig. 7 The average Ka for Mn+ + nClO4− → Mn+(ClO4−)n in CH3CN for the metal cations illustrating binding and non-binding regimes. | ||
The Ka values of the salts in acetonitrile can be taken as an indication of the free energy change in solvating the ions. A high dissociation (low association) is a reflection of the affinity of the salts for acetonitrile. The low dissociation constants (high association) indicate a lower free energy change upon solvation i.e. the solvation energy for the non-binding salts is higher than that of the binding salts. Thus, there is a larger thermodynamic penalty being paid by taking the non-binding salts out of acetonitrile into the macrocyclic complex and consequently the overall free energy change is positive. Since the binding salts are highly associated in acetonitrile it can be taken that the free energy penalty in removing them from the coordination/solvation sphere of acetonitrile is lower and a negative free energy results from this process. This is by no means a conclusive correlation or interpretation of binding selectivity but the correlation between Ka and binding is striking.
:
1) at 0 °C under Ar, enough iPr2NEt (approx. 5.0 equiv.) was added to turn the mixture slightly basic. HATU (0.48 mmol, 1.2 equiv.) was added and the resulting mixture was stirred for 3 d at rt. The solvents were evaporated under reduced pressure and the residue was taken up in EtOAc (approx. 1/4 of the volume used for cyclization). The organic layer was washed with an equal amount of water and the aqueous layer was extracted with EtOAc (×1). The combined organic layers were dried over MgSO4, filtered and concentrated under reduced pressure. Flash column chromatography in EtOAc until the impurities had passed followed by change to EtOAc/MeOH 97
:
3 yielded cyclic peptoid cP1 (258 mg, 64%) as a colorless solid: Rf (EtOAc/MeOH 97
:
3) = 0.85; mp = 131–133 °C; [α]21D = –156.2 (c 0.74, CHCl3); 1H NMR (400 MHz, acetone-d6): δ 7.84–6.70 (30H, m, PhH), 6.08–5.60 (4.85H, m, NCHCH3), 5.50–5.42 (0.10H, m, NCHCH3), 5.24–4.93 (1.05H, m, NCHCH3), 4.56–3.56 (6H, m, 3 × NCH2C
O), 3.52–2.14 (12H, m, 3 × NCH2CH2C
O and 3 × NCH2CH2C
O), 1.70–1.34 (18H, m, 6 × NCHCH3); 13C NMR (100 MHz, acetone-d6): δ 173.4, 173.2, 173.2, 173.0, 172.9, 172.7, 172.7, 172.4, 172.1, 171.3, 171.2, 170.3, 169.8, 169.7, 169.5, 169.2 (6C, 6 × C
O), 144.0, 143.4, 143.2, 143.0, 142.9, 142.1, 141.8, 141.4, 141.1 (6C, Ph), 130.6, 130.5, 130.3, 130.2, 130.1, 130.0, 129.9, 129.8, 129.2, 129.0, 128.9, 128.8, 128.4, 128.1 (30CH, Ph), 56.8, 55.9, 55.8, 54.7, 54.3, 53.9, 53.5, 53.0, 52.8, 52.3, 51.9 (6CH, 6 × NCHCH3), 47.3, 46.9, 46.6, 46.5, 46.2 (3CH2, 3 × NCH2C
O), 42.5, 42.3, 42.0, 41.8, 40.8, 39.3, 39.1, 37.4, 36.9, 36.0, 35.1, 33.6 (6CH2, 3 × NCH2CH2C
O and 3 × NCH2CH2C
O), 20.1, 19.2, 18.7, 18.3, 18.2, 17.9, 17.8, 17.6, 17.5, 17.4, 17.0 (6CH3, 6 × NCHCH3); IR (ATR): 1647 (C
O, amide), 1495, 1451, 1414, 1377, 1341, 1283, 1234, 1206, 1186, 1074, 1030, 986, 914, 843, 783, 746; HRMS (TOF MS ES+) calcd for C63H72N6O6Na [M + Na]+m/z 1031.5411, found 1031.5417. HPLC (Water (0.1% TFA)/MeCN 20
:
80, flow = 0.80): tr = 15.79 min, purity = 99.5%.
Sr2+/cP1 complex: 1H NMR (500 MHz, CD3CN, 293 K): δ 7.42–7.15 (30H, m, PhH), 5.25 (3H, m, NCHCH3), 5.07 (3H, q, J = 6.5 Hz, NCHCH3), 4.47 (3H, m, 3 × NCH2aC
O), 3.86 (6H, m, 3 × NCH2bC
O, 3 × NCH2aCH2C
O), 3.25 (3H, m, 3 × NCH2bCH2C
O), 2.71 (3H, m, 3 × NCH2CH2aC
O), 2.32 (3H, m, 3 × NCH2CH2bC
O), 1.62, 1.57 and 1.49 (18H, 3xd, J = 6.8 Hz, 6 × NCHCH3); 13C NMR (100 MHz, CD3CN, 293 K): δ 177.1 (3C, 3 × C
O), 171.9 (3C, 3 × C
O), 141.0, 140.1 (6C, Ph), 129.8, 129.6, 128.8, 128.6, 127.9, 127.4 (30CH, Ph), 57.0 (3CH, 3 × NCHCH3), 56.4 (3CH, 3 × NCHCH3), 45.6 (3CH2, 3 × NCH2C
O), 40.3 (3CH2, 3 × NCH2CH2C
O), 35.0 (3CH2, 3 × NCH2CH2C
O), 19.0 (3CH3, 3 × NCHCH3), 18.2 (3CH3, 3 × NCHCH3).
980) into the Hill equation.22
Footnotes |
| † Electronic supplementary information (ESI) available: NMR, CD and fluorescence spectra and additional modelling data. See DOI: 10.1039/c6ob01954d |
| ‡ Currently affiliation is National Physical Laboratory, Hampton road, Teddington, Middlesex, TW11 0LW, UK. |
| This journal is © The Royal Society of Chemistry 2016 |