2.1 Binding modes between CyP6Q[6] and amino acids in the solution phase
Fig. 1 shows the crystal structure of Gly@CyP6Q[6] (complex 1).. Analysis of the single-crystal structure shows that complex 1 belongs to the triclinic system with the centrosymmetric space group P-1. An oak ridge thermal-ellipsoid plot program (ORTEP) representation of the asymmetric unit is shown in the Supporting Information (Fig. S1). It contains two halves of CyP6Q[6], two protonated glycine molecules, and one free [CdCl4]2- ion. In the single-crystal structure of complex 1, each CyP6Q[6] contains two glycine molecules. The carboxyl group of each glycine molecule is included in the cavity of the CyP6Q[6], but its amino and methylene groups remain outside. The nitrogen atoms (N26 and N13) of the respective glycine molecules form two hydrogen bonds with two portal oxygen atoms (O5, O6 and O15, O16) of CyP6Q[6], and the N–H···O distances are in the range 2.752–3.035 Å. It is interesting to note that a hydrogen bond is established between the nitrogen atom of a glycine molecule included by the cucurbituril and a chlorine atom (Cl1) of the counter ion [CdCl4]2-, with an N–H···Cl distance of 3.228 Å. This is not the case for the other amino acid molecule included by the cucurbituril. At the same time, there is also a dipolar interaction between this counter ion and a methylene proton on the outer wall of the other cucurbituril molecule. [CdCl4]2- thus acts as a bridging unit to link the cucurbituril with the amino acid (shown by purple dotted lines in Fig. 1).
Fig. 2 shows the crystal structure of L-Lys@CyP6Q[6] (complex 2).. Analysis of the single-crystal structure shows that complex 2 belongs to the monoclinic system with centrosymmetric space group P21/c. An ORTEP representation of the asymmetric unit is shown in Fig. S2. It contains half of CyP6Q[6], a protonated lysine molecule (occupancy ratio 0.5), and a free [CdCl4]2- ion. In the single-crystal structure of complex 2, each CyP6Q[6] contains a lysine molecule. The carboxyl and amino groups of this lysine molecule, and the carbon atom (C2) to which they are bound, lie outside of the portal of CyP6Q[6], while the rest of the molecule is within the cavity. The amino nitrogen atom (N1) and hydroxyl oxygen atom (O2) of the lysine molecule outside of the portal of CyP6Q[6] form four hydrogen bonds (N1-H1C···O4, N1-H1A···O6, N1-H1C···O7, and O2-H2···O7) with three oxygen atoms (O4, O6, and O7) of a portal of CyP6Q[6], with lengths in the range 2.334–3.062 Å. The nitrogen atom (N2) of the terminal amino group of lysine inside the cavity forms a hydrogen bond with a portal carbonyl oxygen atom of the cucurbituril with a distance of 2.952 Å. Unlike in complex 1, the counter ion does not interact with the amino acid in this complex, but only surrounds the cucurbituril through dipole interactions (Fig. S5).
Fig. 3 shows the crystal structure of L-Leu@CyP6Q[6] (complex 3).. Complexes 3 and 4 both comprise leucine and CyP6Q[6]. Complex 3 belongs to the triclinic system with chiral space group P1, whereas complex 4 belongs to the monoclinic system with chiral space group C2. The main part of the asymmetric unit of these two complexes is composed of a CyP6Q[6] host and a leucine molecule, and has the same binding mode. The difference is that the counter ion of complex 3 (Fig. S3) is [ZnCl3·H2O]-, whereas that of complex 4 (Fig. S4) is [ZnCl4]2-. Structural analysis of the main parts of these two complexes (taking complex 3 as an example; Fig. 3) shows that there is a hydrogen bond between the hydroxyl oxygen (O13) of the leucine molecule and a portal carbonyl oxygen (O1) of the cucurbituril, with an O13–H13···O1 distance of 2.629 Å. There are also hydrogen bonds between the amino nitrogen (N25) of the leucine molecule and three portal carbonyl oxygen atoms (O5, O7, O9) of the cucurbituril, with distances in the range 2.740–2.890 Å.
The counter ions of complex 3 are paired around the cucurbituril by ion-dipole interactions, and there is also an ion-dipole interaction between the two paired counter ions. Although the counter ions of complex 4 also surround the cucurbituril through ion-dipole interactions, there is no weak interaction between them. This difference results in very different stacking patterns of these two complexes. Fig. 4 shows stack views of complexes 3 and 4 along the c-axis. From Fig. 4a, b, it can clearly be seen that all of the cucurbituril units in complex 3 have the same orientation, whereas those in complex 4 have two orientations with an included angle of 67.9°. Due to the different orientations of the cucurbituril moieties, there is a significantly larger channel along the c-axis in complex 4 than in complex 3.
2.2 Interactions between CyP6Q[6] and amino acids in the solution phase
CyP6Q[6] shows good solubility in many solvents, most notably in water, in which it is 1 to 2 orders of magnitude more soluble than ordinary cucurbituril. Because the amino acids that make up the protein required for animal nutrition are mostly present in aqueous systems, the good water solubility of CyP6Q[6] facilitates the study of its interactions with amino acids. In the present work, the binding behavior of CyP6Q[6] with the above three amino acids was investigated in D2O. In 1H NMR, the cavity of CyP6Q[6] has a shielding effect on proton signals, whereas outside of the portals, in the vicinity of the carbonyl oxygen atoms, the proton signals are subjected to a deshielding effect. According to this theory, analysis of the 1H chemical shifts and splittings of the signals of protons of amino acids and the host provides insight into the binding mode between them. Fig. 5 shows the changes in the 1H NMR spectrum of the guest Gly as it is dropped into a solution of the host CyP6Q[6]. The results show that the peak due to the α protons of Gly shifts upfield, indicating that this unit enters the cavity of the cucurbituril. Considering the ion-dipole and hydrophobic effects, it may be speculated that the carboxyl group and methylene unit of Gly enter the cavity, while the amino group is fixed at the portal of CyP6Q[6]. This binding mode is basically similar to the crystal structure in the solid phase. However, a difference is that the methylene unit lies outside of the portal in the solid phase, but inside the cavity in the liquid phase. At up to two molar equivalents of Gly with respect to CyP6Q[6], the α protons show only one signal. Beyond two molar equivalents, two signals due to this unit appear, corresponding to bound and free Gly. This indicates that CyP6Q[6] and Gly form a 1:2 inclusion complex, and that the exchange frequency is slower than the operating frequency of the 1H NMR spectrometer.
The changes in the 1H NMR spectrum of the guest L-Leu upon its incremental addition to CyP6Q[6] are shown in Fig. 6. Two sets of proton resonances for L-Leu are observed, indicating that the frequency of binding and release of L-Leu in CyP6Q[6] is slower than the operating frequency of the 1H NMR spectrometer, consistent with the observations for Gly. A difference is that the α proton signals of l-Leu shift downfield, whereas the signals of the remaining alkyl chain protons shift upfield, suggesting that only the alkyl chain of L-Leu enters cucurbituril, while the carboxyl group remains outside of the portal. At the same time, it can be further seen in Fig. 6 that the ε and λ proton signals of the two methyl groups are split into two groups of signals from the original overlapping signal, indicating that these methyl groups are in different positions in the cucurbituril. A similar splitting is seen for the β and γ proton signals. The β protons give rise to two signals due to optical isomerism, so three peaks due to the β and γ protons are seen. When a sub-stoichiometric amount of L-Leu is added to CyP6Q[6], it displays only one set of signals. Once it is in excess, another set of signals due to free L-Leu appears. This indicates that CyP6Q[6] forms a 1:1 complex with L-Leu, as in the solid-phase crystal structure.
As shown in Fig. 7, titration 1H NMR spectroscopy was also used to investigate the binding behavior between CyP6Q[6] and L-Lys. Similarly to L-Leu, the α proton signals of L-Lys shift downfield, while the signals of the other alkyl chain protons shift upfield, indicating that its alkyl chain enters the cavity of the cucurbituril, while the two amino groups are fixed at the portals, forming a structure similar to that of butanediamine@CyP6Q[6]. The methine unit at which the carboxyl α proton is linked to one of the amino groups remains outside of the portal, forming a 1:1 complex of L-Lys@CyP6Q[6]. The cavity of CyP6Q[6] is large enough to accommodate the L-Lys alkyl chain in its fully extended form, as corroborated by the crystal structure. It is worth noting that during the titration process, when the amount of L-Lys added reached 0.5 equivalents with respect to CyP6Q[6], its peaks suddenly broadened and even disappeared. This phenomenon may feasibly be attributed to the exchange frequency of L-Lys in and out of the cavity of the cucurbituril exceeding the operating frequency of the 1H NMR spectrometer, such that the detected 1H NMR signals are averages of various intermediate states of the host–guest interaction. Averaging over a multitude of states will make the signals of the guest tend towards the baseline. Of course, it may also be enrichment of lysine that causes the disappearance of the signal of the guest proton. The specific cause is still unclear, and further research is needed.
2.3 Isothermal titration calorimetry
Isothermal titration calorimetry (ITC) experiments (Fig. S8) were performed to determine the thermodynamic parameters of the above three amino acids and CyP6Q[6] in water, providing insight into the thermal stability and driving force of the interactions. Table 1 shows that the enthalpies and entropies of the interactions of the three amino acids with CyP6Q[6] are both negative. From the contributions of these two thermodynamic parameters to the Gibbs free energy, it can be seen that the three systems are enthalpy-driven, and the driving force is determined by the ion-dipole interaction and the hydrophobic effect. The alkyl chain of the amino acid is more inclined to enter the cavity of the host due to the hydrophobic effect, allowing water molecules originally in the cavity of the CyP6Q[6] to enter the aqueous phase, thereby reducing the entropy of the system. Moreover, 2Gly@CyP6Q[6] evidently has the largest binding constant among the three studied systems, which may be due to the fact that there is some interaction between the two amino acids in addition to the interaction between glycine and cucurbituril. Its crystal structure (Fig. 1) shows that the carboxyl groups of both glycine molecules are also involved in hydrogen bonds, forming a more stable structure, so their binding constants are an order of magnitude higher than those for the other two amino acids. For lysine and leucine with the same number of carbon atoms, the binding constants are relatively close, but that of lysine is slightly higher due to a dipolar interaction of the amino groups.
Table 1. Thermodynamic parameters of the interactions of amino acids with CyP6Q[6]
Experiment
|
∆H (KJ/mol)
|
T∆S (KJ/mol)
|
Ka (m-1)
|
Gly·CyP6Q[6]
|
-48.47
|
-15.42
|
6.15×105
|
l-Leu·CyP6Q[6]
|
-59.11
|
-34.82
|
1.80×104
|
l-Lys·CyP6Q[6]
|
-35.66
|
-10.85
|
2.23×104
|