Spatial sequestration of molecules is a prerequisite for the complexity of biological systems, enabling the occurrence of numerous, often non-compatible chemical reactions and processes in one cell at the same time. Inspired by this compartmentalization concept, chemists design and synthesize artificial nanocontainers (capsules and cages) and use them to mimic the biological complexity and for new applications in recognition, separation, and catalysis. Here, we report the formation of large closed-shell species by interactions of well-known polyphenolic macrocycles with anions. It has been known since many years that C-alkyl resorcin[4]arenes (R4C) and C-alkyl pyrogallol[4]arenes (P4C) narcissistically self-assemble in nonpolar solvents to form hydrogen-bonded capsules. Here, we show a new interaction model that additionally involves anions as interacting partners and leads to even larger capsular species. Diffusion-ordered spectroscopy and titration experiments indicate that the anion-sealed species have a diameter of >26 Å and suggest stoichiometry (M)6(X-)24 and tight ion pairing with cations. This self-assembly is effective in a nonpolar environment (THF and benzene but not in chloroform), however, requires initiation by mechanochemistry (dry milling) in the case of non-compatible solubility. Notably, it is common among various polyphenolic macrocycles (M) having diverse geometries and various conformational lability.
Spatial sequestration of molecules is a prerequisite for the complexity of biological systems, enabling the occurrence of numerous, often non-compatible chemical reactions and processes in one cell at the same time. Inspired by this compartmentalization concept, chemists design and synthesize artificial nanocontainers (capsules and cages) and use them to mimic the biological complexity and for new applications in recognition, separation, and catalysis. Here, we report the formation of large closed-shell species by interactions of well-known polyphenolic macrocycles with anions. It has been known since many years that C-alkyl resorcin[4]arenes (R4C) and C-alkyl pyrogallol[4]arenes (P4C) narcissistically self-assemble in nonpolar solvents to form hydrogen-bonded capsules. Here, we show a new interaction model that additionally involves anions as interacting partners and leads to even larger capsular species. Diffusion-ordered spectroscopy and titration experiments indicate that the anion-sealed species have a diameter of >26 Å and suggest stoichiometry (M)6(X-)24 and tight ion pairing with cations. This self-assembly is effective in a nonpolar environment (THF and benzene but not in chloroform), however, requires initiation by mechanochemistry (dry milling) in the case of non-compatible solubility. Notably, it is common among various polyphenolic macrocycles (M) having diverse geometries and various conformational lability.
Complexity
requires spatial organization. To perform various chemical
reactions or physical processes (recognition, separation, and catalysis),
nature has evolved compartmentalization strategies that utilize tailored
protein cavities or various cellular containers. Chemists, inspired
by nature, utilize synthetic building blocks to construct synthetic
organizational systems like capsules and cages. Hexameric capsules
(R4C)6(H2O)8 and (PC)6 (Figure a,b) are one of the
largest and, at the same time, the easiest to obtain artificial capsules
based on hydrogen bonds.[1,2] They spontaneously form
by interactions between polyphenolic macrocycles [C-alkyl resorcin[4]arenes
(RC) or C-alkyl
progallol[4]arenes (PC) Figure a,b], enclosing
>1000 Å3of the internal space. These hexameric
capsules
(found in the solid state[1,2] and low-polarity solvents[3]) have unique encapsulation properties,[4] exhibit high-fidelity self-sorting,[5] and amazing enzyme-like catalytic activity.[6−8] They are nowadays considered the classics of supramolecular chemistry.[6d,9−12] After many years of extensive studies, it seems that these macrocycles
carry no mysteries. However, our recent studies performed for related
compounds ([5]arenes[13]) demonstrated a
new interaction model that has not been known before for polyphenolic
macrocycles. It has been found that [5]arenes are capable of forming
capsules via hydrogen bonds between hydroxyl groups (OH) and anions.[14] These findings inspired us to re-visit interactions
between a series of well-known [4]arenes and anions to explore the
universal character of such interactions and test the possibility
of the formation of new capsular structures using old building blocks.
Figure 1
State
of the art: previously known hexameric capsules (a) (R4C)6(H2O)8 (ref (1)), (b) (PC)6 (ref (2)), and (c, d) chloride binding
sites found in proteins (refs (15) and (16)).
State
of the art: previously known hexameric capsules (a) (R4C)6(H2O)8 (ref (1)), (b) (PC)6 (ref (2)), and (c, d) chloride binding
sites found in proteins (refs (15) and (16)).The current studies take additional
inspiration from the analysis
of anion binding sites in proteins (e.g., in chloride-dependent neurotransmiter
sodium symporters[15,16]) in which tyrosine or serine
(the OH-containing amino acids) are frequently found and OH-anion
interactions are common (Figure c,d). There is also a growing appreciation of the strength
of OH-anion interactions in the field of artificial anion receptors.[17] The non-innocent role of anions during encapsulation
of small ammonium cations in dimeric resorcin[4]arene capsules and
during interactions between halogenated resorcin[4]arenes and tetraalkylammonium
cations has also been noticed by the groups of Rissanen, Bayeh, and
Schalley.[18−21] Despite these strong indications, the use of anion-based interactions
to assemble polyphenolic macrocycles has been abandoned. In this study,
we demonstrate that anion-based self-assembly leads to the formation
of large capsular species that possess well-defined structures that
are ion-paired with cations. We also show that it is a common phenomenon
among many polyphenolic macrocycles (M, Figure ), involving those containing
different substitution patterns and having various conformational
lability. Anion-based self-assembly is effective in various media,
although, in the case of non-compatible solubility, its initiation
requires a non-standard approach (we report here the effectiveness
of mechanochemistry).
Figure 2
Chemical structures of the compounds used in this work
and notation
of NMR signals.
Chemical structures of the compounds used in this work
and notation
of NMR signals.
Results and Discussion
Interactions with Anions
in THF
The interactions between
macrocycles (M) and tetraalkylammonium salts which serve
as sources of anions (Alk4NX, Figure ) were first studied in THF-d8. In THF-d8, contrary to
CDCl3 and benzene, all macrocycles are soluble and exist
in monomeric forms, as evidenced from their diffusion coefficients
(D). Upon addition of Alk4NX, the 1H NMR signals of upper-rim protons (OHlateral and
OHcentral for P4C and P4H and
OHlateral and CHcentral for R4C and R4H) experience substantial downfield shifts (Δδmax ≈ +2.5 ppm, Figure a). Although the magnitudes of Δδ values
and the trajectories are different for different macrocycles and salts,
in all cases, the magnitudes of Δδ depend on the type
of anion but remain insensitive to the type of cation, indicating
that the interactions are dominated by anions. DOSY spectra[22] recorded during titrations show a monotonic
increase in the average size of species formed by the macrocycles
with borderline values that are similar for all macrocycles (Figure c). The size of the
species, calculated using the Einstein−Stokes equation from D values reached after addition of 8 equiv of the salt (see Supporting Information), corresponds to hydrodynamic
diameters dH = 23 Å for P4H and R4H and dH = 25 Å
for P4C and R4C, where dH = 2rH. In all titration experiments, the
plateau is reached at amounts of Alk4NX close to 4 equiv
per macrocycle.
Figure 3
1H NMR and DOSY titrations of macrocycles (M) P4H, P4C, R4H, and R4C with Alk4NX salts in [D8]THF: (a)
changes in chemical shifts (Δδ) for OH/CH central, (b)
changes in chemical shifts (Δδ) for OHlateral, and (c) changes of diffusion coefficients (D)
for signals of M and Alk4N+. All titrations
were performed using solutions of analytes, C(M) = 2.5 mM, and titrant, C(M) = 2.5 mM + C(Alk4NX) = 65 mM, at 298
K, 600 MHz.
1H NMR and DOSY titrations of macrocycles (M) P4H, P4C, R4H, and R4C with Alk4NX salts in [D8]THF: (a)
changes in chemical shifts (Δδ) for OH/CH central, (b)
changes in chemical shifts (Δδ) for OHlateral, and (c) changes of diffusion coefficients (D)
for signals of M and Alk4N+. All titrations
were performed using solutions of analytes, C(M) = 2.5 mM, and titrant, C(M) = 2.5 mM + C(Alk4NX) = 65 mM, at 298
K, 600 MHz.To suggest a plausible model of
interactions between the macrocycles
and anions, an analysis of the crystallographic database (CCDC) and
a series of DFT calculations were performed (Figure a–d).[31] A plot of electrostatic potential (ESP) of the DFT-optimized pyrogallol
and resorcinol structures indicates the presence of large clusters
of positive ESP along OH-decorated rims, which are responsible for
interactions with negatively charged species. Notably, the positive
ESP is also present for CHcentral in resorcinol (Figure a). In line with
these findings, crystal structures retrieved from CCDC demonstrate
that resorcin[4]arenes or pyrogallol[4]arenes co-crystallized with
Alk4NX are surrounded by anions positioned close to their
upper rims (various modes, see Figure b). However, these CCDC crystal structures were obtained
by crystallization from competitive solvents (alcohols) and represent
non-discrete structures. Using this structural information, experimental D values, and estimated 1:4 stoichiometry, two hypothetical
anion-based discrete structures were constructed: tetramer, (M)4(X–)16 (Figure S115) and hexamer (M)6(X–)24 (Figure e,f). The tetramer was excluded due to its small size, exposed charges,
and electrostatic repulsions. The hexamer with theoretical dH = 23 ÷ 25 Å (the model neglects
counterions and a solvation sphere) corresponds quite well to experimental dH = 23 Å. The internal volume of the hexamer
is 1830 Å3, which is 40% larger than the internal
volume of hydrogen-bonded (PC)6 (1310 Å3).The hexamer
is based on a C4-crown conformation of P4H, and the binding motif involves the formation of trimeric clusters
with anions separated/bridged by OH groups. This binding motif was
inspired by the geometry of coordination hexamers,[23] the geometry of anion–water clusters retrieved from
CCDC, and it is analogous to the one that has been suggested for [5]arenes.[14] The geometry of the binding motif was optimized
using DFT in a vacuum and in THF (continuous solvation model, Figure c,d). In a vacuum,
geometry optimization of the motif leads to its disintegration due
to repulsion between chlorides. On the contrary, in THF, the optimized
structure remains hydrogen-bonded with each chloride held by three
hydrogen bonds with typical distances, Cl···O(H), in
the range of 3.1 ÷ 3.3 Å. The Cl···Cl distances,
which are expected to be repulsive, are 6.2 Å, which are longer
than the shortest distances observed for such interactions in the
solid state (e.g., in dinuclear oligourea/pyrrole foldamers, Cl···Cl
= 3.6 ÷ 4.6 Å)[24] and typical
for H-separated interchloride distances.
Figure 4
Rationale and the suggested
models of anion-based closed-shell
capsules: (a) ESP at the van der Waals surface of resorcinol (DFT
B3LYP/6-31g), (b) X-ray structure of an anion-surrounded resorcinarene
molecule (CCDC 195432), geometry-optimized binding motifs (DFT B3LYP/def2ZVPP,
in THF, PCM solvent model) for (c) pyrogallol and (d) resorcinol,
(e) suggested structure of hexamer (P4H)6(Cl–)24 with the binding motif, external shape,
and internal cavity, and (f) suggested structure of hexamer (R4H)6(Cl–)24 with
the binding motif.
Rationale and the suggested
models of anion-based closed-shell
capsules: (a) ESP at the van der Waals surface of resorcinol (DFT
B3LYP/6-31g), (b) X-ray structure of an anion-surrounded resorcinarene
molecule (CCDC 195432), geometry-optimized binding motifs (DFT B3LYP/def2ZVPP,
in THF, PCM solvent model) for (c) pyrogallol and (d) resorcinol,
(e) suggested structure of hexamer (P4H)6(Cl–)24 with the binding motif, external shape,
and internal cavity, and (f) suggested structure of hexamer (R4H)6(Cl–)24 with
the binding motif.Although the final structure
of anion-based species remains uncertain,
we think that the model of the hexamer corresponds reasonably well
to the experimental data; however, non-symmetrical structures being
in dynamic equilibrium are also possible.
Interactions with Anions
in Benzene
Expecting that
in less polar environments, the anion-sealed capsules may be more
stable (thermodynamically and kinetically), we undertook attempts
to obtain anion-sealed capsules in benzene. Without Alk4NX being added, only P4C and R4C have detectable
solubility in benzene, exhibiting patterns characteristic for (P4C)6 or (R4C)6(H2O)8 (Figure a,f). With positive experience in the application of mechanochemical
ball milling as a method to initialize interaction between the components,[25−28] we used this method to pre-treat the samples.
Figure 5
Interactions of macrocycles M with Alk4NX
in benzene. 1H NMR spectra for (a) (P4C)6, (b) P4C + Oct4NCl, (c) P4C + Oct4NBr, (d) P4H + Oct4NCl,
(e) P4H + Oct4NBr, (f) (R4C)6(H2O)8, (g) R4C +
Oct4NCl, (h) R4C + Oct4NBr, (i) R4H + Oct4NCl, and (j) R4H + Oct4NBr (x—Oct4N+ signals and s—solvent).
Partial 1H NMR spectra for (k) (P4C)6 and (l) (P4C)6Br24–, (m) partial 1H NMR and DOSY spectrum of (P4C)6 + (P4C)6Br24–, and (n) changes of diffusion coefficients (D) upon variation of the concentration of the macrocycle
(C(Alk4NX) 40 mM, C(M) 4–40 mM). All samples were prepared mechanochemically
and dissolved in C6D6 (see the experimental
part for the procedures, 600 MHz, 298 K).
Interactions of macrocycles M with Alk4NX
in benzene. 1H NMR spectra for (a) (P4C)6, (b) P4C + Oct4NCl, (c) P4C + Oct4NBr, (d) P4H + Oct4NCl,
(e) P4H + Oct4NBr, (f) (R4C)6(H2O)8, (g) R4C +
Oct4NCl, (h) R4C + Oct4NBr, (i) R4H + Oct4NCl, and (j) R4H + Oct4NBr (x—Oct4N+ signals and s—solvent).
Partial 1H NMR spectra for (k) (P4C)6 and (l) (P4C)6Br24–, (m) partial 1H NMR and DOSY spectrum of (P4C)6 + (P4C)6Br24–, and (n) changes of diffusion coefficients (D) upon variation of the concentration of the macrocycle
(C(Alk4NX) 40 mM, C(M) 4–40 mM). All samples were prepared mechanochemically
and dissolved in C6D6 (see the experimental
part for the procedures, 600 MHz, 298 K).Macrocycles and the respective salts (1–8 equiv) were dry-milled
in a planetary ball mill, and the solids were treated with benzene-d6. Resorcinarenes (R4C or R4H) with 1 or 2 equiv of Oct4NX remained insoluble.
However, the addition of 4–8 equiv of Oct4NX leads
to a substantial increase in solubility of R4C and R4H. Solubility in benzene, especially of the previously insoluble
macrocycles, is a strong indication of the formation of closed-shell
structures, which engages polar hydroxyl groups and saturates “solvation
spheres” of anions. The signals in the 1H NMR spectra
are sharp, and the chemical shifts are anion-dependent but remain
insensitive to the cations’ size and the concentration (Figures and S85–S98). The fact that at least 4 equiv
of the salt are needed for good solubility supports (M)6(X–)24 stoichiometry. 1H
NMR signals of OHlateral for resorcinarene-based capsules
appear at δ ≈ 10 ppm for chlorides and at δ ≈
9.5 ppm for bromides, reflecting a typical trend and hydrogen bond
accepting ability of anions. Particularly notable are the positions
of signals of CHcentral because they move from their typical
position at ca δ = 6.4 ppm (observed, e.g., for (RC)6(H2O)8, Figure f) to δ = 7.3–7.6 and exhibit higher values of δ
for bromides than for chlorides (Figure g,h, a similar trend is also observed during
titrations in THF, Figure ). These downfield shifts indicate that the interactions with
anions for resorcinarenes involve not only hydroxyl groups but also
CH···anion interactions, and these contributions seem
to be particularly relevant for interactions with large bromide anions,
which is in line with the suggested binding motif.Pyrogallolarenes
(P4H and P4C) also form
anion-sealed capsules in benzene-d6. P4H, initially insoluble in benzene-d6, becomes soluble (partially or fully) upon the addition of
Alk4NX and mechanochemical pre-treatment. The ratio of P4H:Alk4NX in the dissolved part of the sample
is at least 1:4, and the chemical shifts remain independent of the
various concentrations of the Alk4NX. The downfield shifts
of hydroxyl group signals are consistent with the involvement of all
OH groups in hydrogen bonding interactions with anions, with chlorides
inducing higher downfield shifts than bromides. P4C behaves
differently because the P4C:Alk4NX ratio in
the solution roughly follows the ratio in the solid samples (starts
from 1:0.8, not like in previous cases from 1:4). The signals in the 1H NMR spectrum show concentration-dependent chemical shifts,
and the final values of Δδ are much lower than for complexes
of other macrocycles. This indicates that interactions of P4C with anions are weaker than those of other macrocycles despite its
higher solubility in benzene. Thanks to a stepwise transformation
from (P4C)6 to (P4C)6(Br–)24, we were able to detect the
simultaneous presence of two capsular forms in one sample, and DOSY
measurements confirm that the anion-sealed species are larger than
neutral hydrogen-bonded capsules (Figure k–m).The crucial role of anions
in the self-assembly process was further
supported by experiments with salts containing other, non-interacting
anions. After mechanochemical pre-treatment of the macrocycles mixed
with But4NF, But4NPF6, But4NH2PO4, But4NHSO3, But4NNO3, or Pen4NI (4 equiv), we found
no traces of dissolution of the resulting samples in benzene.
Role of
Cations
Although self-assembly is predominantly
anion-dependent, cationic species are inherently present as counterions.
Alk4N+ can reside either inside or outside the
cavity, and due to the dynamic nature of the capsules, they can be
in a fast exchange between these positions and various forms of uncompleted
species (free or non-specifically aggregated).1H
NMR signals of Alk4N+ undergo upfield shifts
upon addition of macrocycles (both in THF-d8 and in benzene-d6). For all Alk4N+, the largest Δδ is observed for
the methylene protons next to the nitrogen (−CH2–N+, Δδmax ≈ −0.48
ppm, Figure d), while
other signals experience considerably smaller shifts (Δδmax < −0.17 ppm, Figure S118a). Analysis of Δδ for various Alk4NX indicates
that the effect of cation size (But4NCl vs Oct4NCl) is smaller than the effect of the anion type (Alk4NCl vs Alk4NBr) and chlorides impose larger Δδ
values than bromides (Figure d). These properties are interpreted in terms of ion pairing
of Alk4N+ with anion-based capsules (either
inside or outside the cavity, Figure e,f), which is stronger for capsules containing chlorides
than bromides. An upfield shift of −CH2–N+ signals can be explained by electrostatic attractions within
an ion pair that change the conformation of Alk4N+ so that the cationic core is exposed and placed in the proximity
of the aromatic walls of the capsules (Figures f and S118c).
Figure 6
Interactions
of capsules with cations in [D8]THF: (a,b)
changes in diffusion coefficients (D) during the
titration of P4H with Alk4NX and a comparison
with concentration-dependent changes of Pen4NBr alone (the
same concentration of Alk4NX, 2.5 ÷ 30 mM), (c) diffusion
coefficients (D) for the samples of P4H (mmol) + Pro4NCl (1 ÷ 5 equiv), ball-milled and
dissolved in [D8]THF; the ratio between components was
calculated by integration of the spectral (d) changes in 1H chemical shifts (Δδ) of −CH2N+ signals during titration of P4H with Alk4NX [all experiments at 298 K, 600 MHz, analyte: C(P4H) = 2.5 mM and titrant: C(P4H) = 2.5 mM + C(Alk4NX) = 65
mM]. A model of the anion-sealed capsule with (e) three Pro4N+ in the cavity, and (f) Bu4N+ interacting
externally (the atoms in the front were partially removed to visualize
the interior of the cavity).
Interactions
of capsules with cations in [D8]THF: (a,b)
changes in diffusion coefficients (D) during the
titration of P4H with Alk4NX and a comparison
with concentration-dependent changes of Pen4NBr alone (the
same concentration of Alk4NX, 2.5 ÷ 30 mM), (c) diffusion
coefficients (D) for the samples of P4H (mmol) + Pro4NCl (1 ÷ 5 equiv), ball-milled and
dissolved in [D8]THF; the ratio between components was
calculated by integration of the spectral (d) changes in 1H chemical shifts (Δδ) of −CH2N+ signals during titration of P4H with Alk4NX [all experiments at 298 K, 600 MHz, analyte: C(P4H) = 2.5 mM and titrant: C(P4H) = 2.5 mM + C(Alk4NX) = 65
mM]. A model of the anion-sealed capsule with (e) three Pro4N+ in the cavity, and (f) Bu4N+ interacting
externally (the atoms in the front were partially removed to visualize
the interior of the cavity).Ion pairing was also confirmed by DOSY both in THF-d8 (Figure a,b) and benzene-d6 (Figure n). In THF-d8, in the absence of the macrocycles, D(Alk4N+) values decrease monotonically with
increasing concentration of Alk4NX, in line with concentration-dependent
non-specific aggregation (Figures a and S101d). On the contrary,
in the presence of the macrocycles, the profiles of changes are substantially
different. Upon addition of Alk4NX to M (constant
concentration) in THF-d8, the titration
curve with respect to D(Alk4N+) is non-monotonic (Figure a,b). It is interpreted assuming that Alk4N+ forms an ion pair(s) with a large and highly negatively charged
capsule, which leads to a low D(Alk4N+) value when the relative concentration of the capsules is
high (initial points) and to an increase in the D(Alk4N+) value as the amount of Alk4NX increases. In line with this interpretation, D(M) values remain at the same level in this experiment
and weaker ion pairing with capsules containing Br– leads to less pronounced effects (Figure b). In benzene-d6, non-specific Alk4NX aggregation is very strong (Figure S116) and the macrocycles have limited
solubility. Therefore, the reversed titrations were performed at constant
Alk4NX concentration (Figure n). In such a case, D(Alk4N+) values are expected to stay constant in absence
of specific interactions. However, upon the addition of the macrocycles, D(Alk4N+) values systematically increase—up
to the values of the postulated anion-sealed capsules. These observations
are in line with the hypothesis that cations form ion pairs with large
anion-sealed capsules.To check the possibility of encapsulation
of smaller cations, Met4NX, Et4NX, and Pro4NX were also tested.
All these salts are soluble neither in THF nor in benzene. Therefore,
the samples containing macrocycles and the respective salts (at a
ratio of 1:1 up to 1:8) were ball-milled and subsequently treated
with benzene or THF. In benzene, all samples remained insoluble. Quite
surprisingly, most of them were also insoluble in THF, even though
the macrocycles in their “free” forms were readily soluble
in THF. Only P4C/Pro4NBr and P4C/Pro4NCl were partially dissolved in THF-d8 but revealed distinct behaviors. For P4C/Pro4NBr, the ratio between dissolved components remains
constant, 1:1, irrespective of the initial ratio in the solid sample
(Figure S110). Importantly, D(Pro4N+) values indicate the formation of small
species, most likely by the complexation of cations in the monomeric
cavitand. On the contrary, for P4C/Pro4NCl,
the ratio between dissolved components is variable—from 1:1
to the maximum limiting value of 1:4 (Figure S109). In P4C/Pro4NCl, the D values for the macrocycle and the cation are ratio-dependent and
much lower than in P4C/Pro4NBr. Particularly
striking is the abrupt differentiation of D values
between P4C signals and Pro4N+ signals
at the 1:4 ratio (Figure c). These data confirm that (1) four Cl– per macrocycle are needed for capsule formation and (2) tight ion
pairing involves less than four Pro4N+ per macrocycle;
therefore, at the P4C/Pro4NCl 1:4 ratio, there
is an exchange between “bound” and “free”
cations, leading to a higher D(Pro4N+) value. Although it is uncertain if the cations reside inside
or outside the cavity (or both), our models indicate that three Pro4N+ cations can fit in the cavity (occupancy 32%),
but placing four cations leads to steric hindrance (although possible
from the point of view of occupancy). For comparison, the hexameric
capsule (R4C)6(H2O)8 can accommodate two Eth4N+ cations as reported
by Cohen.[4f]Low-temperature experiments
for P4C/Pro4NCl and P4C/Pen4NCl show that within the
temperature range 298 ÷ 233 K, the complexes remain dynamic (Figures S119–S122).
Interactions
with Anions in Chloroform
C-alkyl-substituted
macrocycles P4C and R4C are known to spontaneously
and quantitatively form self-assembled capsules (R4C)6(H2O)8 and (P4C)6 in chloroform and encapsulate suitably sized Alk4N+ cations (up to Oct4N+).[4a] It has been reported that Alk4NX
salts have to be added in small amounts for encapsulation because,
otherwise, they induce disassembly.[4a] Here,
we evaluate the ability of anions to become components of self-assembled
species, and therefore, we used higher amounts of Alk4NX
and systematically screened various [4]arenes by DOSY.The spectra
of P4C in chloroform indicate the formation of hexamers
(P4C)6, in line with the previous findings.
The addition of But4NCl leads to the gradual disintegration
of the hexamers to monomers, and 1H NMR spectra show two
separate sets of signals having different diffusion coefficients, D (Figure a). D values and chemical shifts for both species
remain invariable during the titration (Figure b). At 4 equiv of But4NCl being
added, initially formed capsules (P4C)6 are
completely disintegrated. Disassembly requires higher amounts of But4NBr than But4NCl (Figure c), indicating that disassembly is anion-mediated
and reflecting a higher hydrogen bonding affinity of chlorides than
bromides.
Figure 7
Interactions of macrocycles with Alk4NX in chloroform:
(a) 1H NMR and DOSY spectra of mixture P4C (2.5 mM) + OctNCl (65 mM), (b) diffusion coefficients (D) for all
species during titration of P4C with OctNCl, and (c) profiles of the
anion-induced disassembly (all in CDCl3, 600 MHz, 298 K).
Interactions of macrocycles with Alk4NX in chloroform:
(a) 1H NMR and DOSY spectra of mixture P4C (2.5 mM) + OctNCl (65 mM), (b) diffusion coefficients (D) for all
species during titration of P4C with OctNCl, and (c) profiles of the
anion-induced disassembly (all in CDCl3, 600 MHz, 298 K).These data demonstrate that in chloroform, interactions
between
macrocycles and anions are distinctly different than in other solvents:
addition of Alk4NX leads to the disintegration of neutral
hydrogen-bonded hexamers and the anion-based capsules are not re-assembled.
Stability of Complexes
Due to the complex character
of equilibria, various solubility values, and possible cooperative
effects, we were not able to determine absolute association constants.
However, the relative order of stability can be estimated based on
a general rule that, for the same stoichiometry and identical initial
concentrations, a stronger interaction gives a stronger curvature
of a titration curve.[29] Thus, the data
were normalized to the 0–1 range (Δδ or D), and data were analyzed to determine the relative strength
of interactions (Figure S103). The plots
suggest that for a given macrocycle, the complexes with chlorides
are always stronger than those with bromides, which reflects the order
of the hydrogen bonding ability of anions. However, the preference
toward chlorides is less pronounced for resorcinarenes than for pyrogallolarenes.
This may reflect the particular role of CH···anion
interactions for bromides and a good fit between this large anion
and a small central atom (here hydrogen, see binding motif). Among
the chloride complexes with various macrocycles, the order of stability
is as follows: P4H > R4H ≈ R4C > P4C. Thus, lower-rim crowded macrocycles
are less prone to form complexes, which suggests that some conformational
flexibility is required for optimal interactions.The stability
of P4H/Pen4NCl toward the addition of polar
solvents was tested by adding water or methanol (0 ÷ 5% vol/vol)
to its solution in THF-d8. The addition
of polar solvents leads to an increase in D values
of the components, indicating gradual disassembly (Figure S117). It should be noted that water exerts weaker
effects than methanol, when added in the same amounts. The relatively
low sensitivity to traces of water in THF (<2%) is also supported
by the high reproducibility of the results from experiments performed
using different batches of solvent (see Figure S123).
Role of the Solvent
The question
about the role of
the solvent, especially the non-intuitive formation of the complexes
in THF but not in less polar chloroform, was posed and theoretically
discussed in the previous paper.[14] Here,
we evaluated the influence of a solvent on anion binding by using
reference non-macrocyclic polyphenols—resorcinol (R), pyrogallol (P), and catechol (C). These
polyphenols were titrated with But4NX in CDCl3, THF-d8, and CD3CN (Figure ).
Figure 8
1H NMR titrations
of pyrogallol (P), catechol
(C), and resorcinol (R) with But4NCl in CDCl3, THF-d8, and
MeCN-d3: (a) signals of OH for P and C and (b) signals of CHcentral for R. Solid lines represent fitted curves and dashed lines represent
theoretical curves for the 1:1 model (all experiments at 298 K and
400 MHz). (c) Diffusion coefficients (D) for all
species during titrations of P (10 mM) and P4H (2.5 mM) with Alk4NCl.
1H NMR titrations
of pyrogallol (P), catechol
(C), and resorcinol (R) with But4NCl in CDCl3, THF-d8, and
MeCN-d3: (a) signals of OH for P and C and (b) signals of CHcentral for R. Solid lines represent fitted curves and dashed lines represent
theoretical curves for the 1:1 model (all experiments at 298 K and
400 MHz). (c) Diffusion coefficients (D) for all
species during titrations of P (10 mM) and P4H (2.5 mM) with Alk4NCl.In THF and CD3CN (used for comparison with the literature),[17] the titration results were fitted using OH signals
with 1:1 models (Figure a). The association constants (K) are considerably
higher in THF (reflecting its lower ε) than in CD3CN, and the order of stability is P > R > C. The formation of complexes in THF was also
detected
by DOSY (Figures c
and S125). For example, upon the addition
of Alk4NCl salt, the values of D(P) decrease to values similar to those of D(Alk4NCl), reflecting the formation of complexes that
have a size similar to the size of the salt itself but smaller than
in the case of macrocyclic ligands (Figure c). These control experiments explain why
macrocyclic compounds, composed of similar phenolic building blocks,
also interact with anions in THF.Determination of stability
of anion complexes of P, R, and C in chloroform is difficult due
to disappearance of OH signals. Therefore, the comparison between
solvents was made only for R using its CHcentral signal (Figure b).
The shape of the titration curve in CDCl3 indicates that
interactions between Cl– and R are
stronger and more complex in CDCl3 than in THF-d8 and CD3CN and reflects the coexistence
of 2:1, 1:1, and 1:2 complexes (the first maximum is reached before
1 equiv and distinct changes are visible after reaching 2 equiv of
the salt). Thus, lack of formation of anion-sealed capsules by macrocyclic
compounds in chloroform cannot be attributed solely to weaker interactions
between phenolic building blocks and anions in this solvent. Other
factors (solvation of the macrocycles, entropic factors, and ion pair
formation) have to be further analyzed.
Conclusions
The
current findings shed new light on the possible modes of interactions
between pyrogallol[4]arenes and resorcin[4]arenes with tetralakylammonium
salts, pointing out the crucial role of hydrogen bonds with anions.
In weakly anion-solvating environments (THF and benzene), anion···OH/CH
interactions lead to the formation of large self-assembled capsular
species. In sharp contrast, in chloroform, the analogous interactions
lead to the destruction of initially formed hexamers and anions do
not participate in self-assembly. The newly formed anion-sealed capsules
bear a high-density negative charge and form tight but still dynamic
ion pairs with cations. These properties are expected to generate
unique recognition properties and possibly also catalytic properties.
We also think that the ability of resorcinarenes to interact with
anionic species may help to understand widely discussed Brønsted
acidity of resorcinarene capsules,[6a] unusual
selectivity in C–X bond activation,[7a] anion-dependent encapsulations in (R4C)6(H2O)8 reported by Rebek[4a] or Horiuchi,[30] and the anion-dependent
extrusion of water molecules from (R4C)6(H2O)8 mentioned by Cohen.[4d,4f]Importantly, the current results indicate that the anion-based
self-assembly mode is general—it was detected for polyphenolic
macrocycles of various ring sizes ([4]arenes and [5]arenes) having
different substitution patterns (pyrogallol and resorcinol derivatives)
and various levels of conformational rigidity (lower-rim-substituted
and unsubstituted derivatives). Thus, we envision that in the future,
it can also be found for other polyphenolic macrocycles leading to
the discovery of new anion-based closed-shell structures.
Experimental Section
General Procedure for 1H NMR Titrations
To the solution of a macrocycle (C = 0.005 M,
0.0025
mmol) in THF-d8 (0.5 mL), a solution containing
Alk4NX (C = 0.075 M, 0.075 mmol) and the macrocycle (C
= 0.005 M, 0.005 mmol) in THF-d8 (1 mL)
was added in portions. 1H NMR spectra were recorded at
303 K using Bruker 400 MHz.
General Procedure for DOSY Titrations
To the solution
of a macrocycle (C = 0.0025 M, 0.00125 mmol) in THF-d8 (0.5 mL), a solution containing Alk4NX (C = 0.0656 M, 0.0656 mmol) and the macrocycle
(C = 0.0025 M, 0.0025 mmol) in THF-d8 (1 mL) was added in portions. 1H NMR and
DOSY spectra were recorded at 303 K using Varian 600 MHz.
Preparation
of the Samples by Mechanochemistry
Solid
sample of a macrocycle (0.01 mmol) and Alk4NX (1 ÷
8 equiv) were ball-milled for 1 h in a planetary ball mill. Then,
the powder was dissolved in benzene-d6 (0.7 mL). The sample was filtered, and the solution was analyzed
by NMR.
Authors: Pellegrino La Manna; Margherita De Rosa; Carmen Talotta; Antonio Rescifina; Giuseppe Floresta; Annunziata Soriente; Carmine Gaeta; Placido Neri Journal: Angew Chem Int Ed Engl Date: 2019-11-27 Impact factor: 15.336
Authors: N Kodiah Beyeh; Dominik P Weimann; Lena Kaufmann; Christoph A Schalley; Kari Rissanen Journal: Chemistry Date: 2012-04-04 Impact factor: 5.236