Literature DB >> 31458993

Substituent Effects on the Inclusion of 1-Alkyl-6-alkoxy-quinolinium in 4-Sulfonatocalix[n]arenes.

Véronique Wintgens1, Cédric Lorthioir2, Zsombor Miskolczy3, Catherine Amiel1, László Biczók3.   

Abstract

The effect of the chain length of the alkyl and alkoxy substituents on the binding characteristics of 1-alkyl-6-alkoxy-quinolinium cations was studied using 4-sulfonatocalix[4]arene (SCX4) and 4-sulfonatocalix[6]arene (SCX6) in neutral aqueous solutions at 298 K. Isothermal calorimetric titrations showed enthalpy-controlled inclusion with 1:1 stoichiometry. The equilibrium constants of complexation were always larger for the confinement in SCX4 than in its SCX6 homologue because the better matching between the host and guest sizes allowed more exothermic interaction. The binding affinity diminished with the lengthening of the aliphatic chain of the guests in the case of the association with SCX4, but insignificant change was found for SCX6 complexes. The most substantial change in the enthalpic and entropic contributions to the driving force of complex production occurred when the alkyl chain was linked to the heterocyclic nitrogen and the number of its carbon atoms varied between 1 and 4. 1H NMR spectra evidenced that in SCX6, the 1-alkyl-6-alkoxy-quinolinium cations could be included within the macrocycle cavity. In the case of SCX4, the quinolinium ring is always inside the host, but the alkyl chain is included within SCX4 only for a short chain length (n up to 4). In contrast, the alkoxy chain displays a very weak interaction with the cavity irrespective of the length. Because of the outward orientation from the host, the lengthening of the alkoxy substituent of the quinolinium moiety barely influenced the thermodynamics of inclusion in SCX4. Distinct linear enthalpy-entropy correlations were found for the encapsulation in SCX4 and SCX6.

Entities:  

Year:  2018        PMID: 31458993      PMCID: PMC6645118          DOI: 10.1021/acsomega.8b00736

Source DB:  PubMed          Journal:  ACS Omega        ISSN: 2470-1343


Introduction

The biocompatible, highly water-soluble 4-sulfonatocalix[n]arene (SCXn) macrocycles represent a particularly important and intensely studied family of cavitands because of their capability to produce various supramolecular architectures,[1−3] fluorescent sensing systems,[4−6] and host–guest complexes.[7,8] Their π-electron-rich, flexible cavity confines various biologically important compounds,[9−11] drugs,[12−14] and photochromic substances,[15] thereby enhancing the solubility and stability of the guests. The binding between surfactants and SCXn can induce association into nanoparticles,[16] vesicles,[17,18] or supramolecular micelles.[19,20] Such self-assemblies have great potential in the design of stimuli-responsive aggregates and drug delivery vehicles.[21,22] 6-Methoxyquinolinium derivatives are important fluorophores because they can be used in aqueous solution in a wide pH range and emit substantially Stokes-shifted strong fluorescence. Members of this class of compounds were applied as probes for the detection of the intracellular Cl– levels[23−25] and the monitoring of Cl– transport across cell membranes.[26,27] The photophysical behavior and inclusion complex formation of 6-methoxy-1-methylquinolinium (C1C1OQ+) were investigated,[28] and the substantial change of its fluorescence was used to detect the embedment of a herbicide in 4-sulfonatocalix[4]arene (SCX4).[29] For the rational design of tailor-made self-assembled systems incorporating SCXn hosts, the deeper understanding of the relationship between the molecular structure of the components and the driving force of encapsulation is of crucial importance. In the present study, we reveal how the systematic variation of the length and the location of the alkyl chain in quinolinium derivatives influence the thermodynamics of binding and the structure of the produced inclusion complex. We focus on two types of guests, 1-methyl-6-alkoxy-quinolinium (C1COQ+, n = 1, 2, 4, 6) and 1-alkyl-6-methoxy-quinolinium (CC1OQ+, n = 1, 2, 4, 6, 8) cations, and the number of sulfonatophenol units in the SCXn cavitands is varied from n = 4 to 6. We intend to deal only with 1:1 inclusion complexes. Therefore, the larger SCX8 homologue, producing associates of various stoichiometries, were not encompassed in the present work. On the basis of the reported deprotonation constants,[30] we infer that one phenolic OH of SCX4 dissociated, whereas two phenolic OH substituents lost protons in 4-sulfonatocalix[6]arene (SCX6) at neutral pH. Therefore, SCX4 and SCX6 had 5 and 8 negative charges under our experimental conditions, respectively. The formulas of the employed compounds are presented in Scheme .
Scheme 1

Chemical Formulas of the Guest and Host Compounds

Results and Discussion

Thermodynamics of Inclusion in SCXn

To get insight into the driving force of the confinement of 1-alkyl-6-alkoxy-quinolinium (CCOQ+) in SCX4 or SCX6 cavitands, isothermal titration calorimetry (ITC) measurements were performed. Figure shows representative results corresponding to the titration of SCX4 by C8C1OQ+ and the determination of the dilution enthalpy of the titrant. The released heat decreased upon successive additions of the ligand until the value of the dilution heat was reached because of the gradual reduction of the amount of the free binding sites. The inflexion point appeared at the equimolar component concentration, indicating the 1:1 stoichiometry of the resulting complex. The nonlinear least-squares fit of the enthalpograms provided the binding constant (K) and the enthalpy change upon encapsulation (ΔH). The standard free enthalpy (ΔG) and entropy changes (ΔS) were deduced on the basis of the following equationwhere R is the gas constant and T stands for the temperature.
Figure 1

Variation of the integrated heat evolved per injection during the titration of 0.1 mM SCX4 solution by 2 mM C8C1OQ+ solution (■). The line represents the fit with a 1:1 complexation model, whereas (□) displays the heat released per injection of the titrant into water.

Variation of the integrated heat evolved per injection during the titration of 0.1 mM SCX4 solution by 2 mM C8C1OQ+ solution (■). The line represents the fit with a 1:1 complexation model, whereas (□) displays the heat released per injection of the titrant into water. Similar experiments were carried out with various CCOQ+–SCXn pairs, and the results are summarized in Table . All quinolinium derivatives display larger binding affinity to SCX4 than to SCX6 because the tighter fit into the smaller and more rigid homologue results in more exothermic (6–7 kJ mol–1 difference) host–guest interactions. The better match of the size of the guests with the cavity of SCX4 ensures the more efficient limitation of the degrees of freedom of the components resulting in more substantial entropy diminution (2–4 kJ mol–1TΔS difference) for the encapsulation in SCX4.
Table 1

Binding Constants and Thermodynamic Parameters for Inclusion Complex Formation in Neutral Aqueous Solution at 298 K

 SCX4
SCX6
GuestK, 104 M–1ΔG, kJ mol–1ΔH, kJ mol–1TΔS, kJ mol–1K, 104 M–1ΔG, kJ mol–1ΔH, kJ mol–1TΔS, kJ mol–1
C1C1OQ+I46.2 ± 1.8–32.4–38.7 ± 0.4–6.38.8 ± 0.4–28.3–32.1 ± 0.3–3.8
C2C1OQ+Br46.2 ± 1.8–32.4–40.7 ± 0.4–8.37.5 ± 0.3–27.8–33.4 ± 0.3–5.6
C4C1OQ+I32.3 ± 1.3–31.5–42.6 ± 0.4–11.18.2 ± 0.4–28.1–35.6 ± 0.4–7.5
C6C1OQ+Br23.9 ± 1.0–30.7–41.6 ± 0.4–10.98.8 ± 0.4–28.3–35.8 ± 0.4–7.5
C8C1OQ+Br19.2 ± 0.8–30.4–41.7 ± 0.4–11.38.6 ± 0.3–28.2–35.6 ± 0.4–7.4
C1C1OQ+I46.2 ± 1.8–32.4–38.7 ± 0.4–6.38.8 ± 0.4–28.3–32.1 ± 0.3–3.8
C1C2OQ+I40.5 ± 1.6–32.0–37.8 ± 0.4–5.811.4 ± 0.5–28.9–33.3 ± 0.3–4.5
C1C4OQ+I39.3 ± 1.6–32.0–37.8 ± 0.4–5.810.1 ± 0.4–28.6–30.1 ± 0.3–1.5
C1C6OQ+I30.6 ± 1.2–31.3–37.8 ± 0.4–6.510.4 ± 0.4–28.6–28.8 ± 0.3–0.2
Figure depicts the correlations between the binding constants and the number of carbon atoms in the aliphatic chain of the guest molecules. Decreasing trends were observed when SCX4 served as a host, and the extent of this variation was more pronounced for the CC1OQ+ class of compounds than for the C1COQ+ family. In contrast, the K values of SCX6 complexes were practically independent of the length of the alkyl group because the entropy contribution counterbalanced the ΔH variation in the series of compounds (Table ). The binding constants of the CCOQ+ embedment in SCX4 were significantly larger than the corresponding values reported for 1-methyl-3-alkylimidazolium[31] (Cmim+) and alkylammonium[32] (CNH3+) guests. For these guests, the increase of the hydrophobicity and aromatic character follows this order: CNH3+ < Cmim+ < CCOQ+. In particular, the quinolinium derivatives participate in the strongest hydrophobic host–guest interactions and additionally, are able to interact via π–π binding between the aromatic ring of the guest and the π-electron-rich core of SCX4. These two interactions will both contribute to the ΔH diminution. Indeed, the removal of a weaker-bound hydration shell from the cationic moiety in the course of host–guest complexation requires less desolvation energy for CCOQ+. The more substantial binding affinity of CCOQ+ cations to SCX4 compared with that of Cmim+ and CNH3+ arises from the larger enthalpy gain. For example, the ΔH values of SCX4 complex formation at 298 K are −17.9, −33.9, and −37.9 kJ mol–1 for C4NH3+, C4mim+, and C1C4OQ+, respectively, whereas the ΔS values of these processes are 16.6, −19.0 and −19.5 J mol–1 K–1, respectively.[31,32] In the case of the confinement in SCX6, CCOQ+ cations had about 1 order of magnitude larger binding constant than Cmim+ guests[31] because of the less negative ΔS for the encapsulation of the former class of compounds.
Figure 2

Equilibrium constants for the complexation of CC1OQ+ (squares) or C1COQ+ (triangles) with SCX4 (empty symbols) and SCX6 (filled symbols) as a function of the number of carbon atoms in the aliphatic chain of the guests at pH 7 and 298 K.

Equilibrium constants for the complexation of CC1OQ+ (squares) or C1COQ+ (triangles) with SCX4 (empty symbols) and SCX6 (filled symbols) as a function of the number of carbon atoms in the aliphatic chain of the guests at pH 7 and 298 K. The enthalpy-driven exothermic formation of all CCOQ+ complexes were accompanied by unfavorable entropy change, implying that the release of water from the hydrate shell of the constituents upon association does not counterbalance the loss of entropy due to the inclusion of the guest in the host cavity. The variation of the enthalpy and entropy terms with the alkyl substituent significantly differed for CC1OQ+–SCX4 and C1COQ+–SCX4 (Figure S1). In the case of the former complexes, the gradual lengthening of the carbon chain from methyl to butyl led to ΔH and TΔS reduction, but the change levelled off upon further extension of the aliphatic group. In contrast, ΔH and TΔS were practically independent of the molecular structure of C1COQ+–SCX4, but both quantities increased with the alkyl length for the encapsulation of C1COQ+ in SCX6. The thermodynamic parameters of CC1OQ+ embedment in SCX4 followed a similar trend to that found for the inclusion in SCX6. The latter cavitand may adopt inverted double partial cone conformation.[33] The manner of CC1OQ+ inclusion in the partial cone of SCX6 probably resembles the location in SCX4. We found two distinct linear correlations when the entropy variation of the SCX4 and SCX6 complexes of quinolinium derivatives (TΔS) was plotted as a function of the binding enthalpy (ΔH) (Figure ). The experimental data were fitted by the following relationship[34]where the slope (α) indicates the extent to which the enthalpy change is counterbalanced by the concomitant entropy loss upon complex formation.
Figure 3

Enthalpy–entropy correlation for the 1:1 inclusion of CC1OQ+ (blue square) or C1COQ+ (red triangle) in SCX4 or SCX6 in neutral aqueous solution at 298 K.

Enthalpy–entropy correlation for the 1:1 inclusion of CC1OQ+ (blue square) or C1COQ+ (red triangle) in SCX4 or SCX6 in neutral aqueous solution at 298 K. Enthalpy–entropy compensation has been observed for host–guest binding[35−38] because the exothermicity of association usually restricts the movement of the constituents, thereby causing growing entropy loss. In the case of the confinement in SCX4, α = 1.21 and TΔS0 = 40.0 kJ mol–1 were calculated, whereas α = 1.06 and TΔS0 = 30.4 kJ mol–1 were derived from the thermodynamic data of SCX6 complexes. The larger slope (α) and intercept (TΔS0) of the linear ΔH versus TΔS relationship for the confinement in the smaller SCX4 cavitand is due to the tighter binding and the release of more water molecules from the solvation shell of the reactants than in the case of the association with SCX6. The parameters found for CCOQ+–SCX4 complexes in the present study resemble those reported for the embedment of Cmim+ cations in SCX4 (α = 1.38 and TΔS0 = 40.3 kJ mol–1).[31] In the case of SCX6 host, α and TΔS0 for the inclusion of CCOQ+ guests were larger than those found for Cmim+ (α = 0.80 and TΔS0 = 16.6 kJ mol–1),[31] and approached the values previously found for 1:1 Cmim+–SCX8 associates (α = 0.96 and TΔS0 = 27.9 kJ mol–1).[39] The much larger TΔS0 of CCOQ+–SCX6 complexes relative to that of Cmim+–SCX6 implies that more water molecules are expelled from the host interior upon the entry of the bulkier, more hydrophobic quinolinium headgroup. The looser binding of the smaller methylimidazolium moiety causes less extensive desolvation and as a consequence, smaller entropy gain contribution. The close to unity α of CCOQ+–SCX6 complexes indicates that the change of ΔH, arising from the variation of the substitution pattern of the guest, is almost completely offset by the accompanying entropy modification. When the smaller, more hydrophilic headgroup of Cmim+ is encapsulated in SCX6, fewer degrees of freedom are limited and less water is released from the hydrate shell of the constituents into the bulk solution. As a consequence, ΔS changes in a smaller extent in the series of Cmim+–SCX6 complexes than upon the inclusion of CCOQ+ in SCX6.

Molecular Structure of the SCXn Complexes

To gain insight into the structure of the inclusion complexes, 1H NMR experiments were performed. As a representative example, Figure displays the spectra of C4C1OQ+SCX4 and C1C4OQ+SCX4. The broadening observed for the peaks related to the SCX4 protons results from conformational changes of the macrocycle that could correspond to inversions of the aromatic rings[40] and/or distortions of the cone conformation.[41] These dynamical processes stand in the intermediate regime, as can be seen in Figure . In contrast, the same spectra suggest that both quinolinium derivatives undergo a fast exchange between the free and the complexed states over the characteristic NMR time scale. When the SCX4/quinolinium molar ratio is set to 2:1 and the total concentration of 10 mM is used, more than 95% of the quinolinium derivatives is complexed to SCX4 on the basis of the K value (Table ). Therefore, the 1H chemical shifts measured under such conditions allow the probing of the quinolinium location within both C4C1OQ+SCX4 and C1C4OQ+SCX4 complexes. In the case of the former complex, the resonances related to the quinolinium and the butyl protons shift upfield in comparison to the signals of the free C4C1OQ+ molecules. Figure A and Table S1 show that the most significant encapsulation-induced chemical shift variations (Δδ) are observed for the peaks assigned to H2, H3, and H4 for all studied guests. This indicates that the corresponding part of the quinolinium has the deepest immersion within the SCX4 cavity. Among the aromatic proton resonances, the H7 signal undergoes the weakest upfield shift, implying that this terminal of the quinolinium is oriented toward the aqueous phase. The Δδ value determined for the methoxy protons is the smallest in CC1OQ+–SCX4 complexes, indicating that the methoxy substituent is located far from the core of the macrocycle.
Figure 4

From top to bottom: 1H NMR spectra of 10 mM C4C1OQ+, 3.3 mM C4C1OQ+ + 6.7 mM SCX4 mixture, 10 mM C1C4OQ+, and 3.3 mM C1C4OQ+ + 6.7 mM SCX4 mixture in D2O at 298 K. The asterisks denote the peaks related to the SCX4 protons; (A,B) correspond to two distinct spectral ranges. The small triplet at 1.05 ppm results from an impurity present in the SCX4 compound. (The spectrum of neat SCX4 solution displays this small contribution.)

Figure 5

Alkyl chain length (n) dependence of the 1H chemical shift variation upon complex formation for (A) CC1OQ+–SCX4: NCH2 (■), H4 (●), CH3 (○), OCH3 (△) and (B) C1COQ+–SCX4: NCH3 (■), H4 (●), CH3 (○), OCH2 (△). Both complexes are obtained using 1:2 quinolinium/SCX4 molar ratio and a total concentration of 10 mM.

From top to bottom: 1H NMR spectra of 10 mM C4C1OQ+, 3.3 mM C4C1OQ+ + 6.7 mM SCX4 mixture, 10 mM C1C4OQ+, and 3.3 mM C1C4OQ+ + 6.7 mM SCX4 mixture in D2O at 298 K. The asterisks denote the peaks related to the SCX4 protons; (A,B) correspond to two distinct spectral ranges. The small triplet at 1.05 ppm results from an impurity present in the SCX4 compound. (The spectrum of neat SCX4 solution displays this small contribution.) Alkyl chain length (n) dependence of the 1H chemical shift variation upon complex formation for (A) CC1OQ+–SCX4: NCH2 (■), H4 (●), CH3 (○), OCH3 (△) and (B) C1COQ+–SCX4: NCH3 (■), H4 (●), CH3 (○), OCH2 (△). Both complexes are obtained using 1:2 quinolinium/SCX4 molar ratio and a total concentration of 10 mM. Among the alkyl protons of CC1OQ+, the increase of the alkyl chain length resulted in the largest chemical shift variation for the −CH3 protons. As shown in Figure A, the Δδ value of this signal is reduced upon the gradual increase of the number of aliphatic carbon atoms from methyl to hexyl, while the change tends to level off for CC1OQ+–SCX4 with n ≥ 6. Such a behavior suggests that the short alkyl chains (n = 1, 2, and 4) were included in SCX4. Hexyl and octyl substituents are too long to be fully embedded in SCX4. Therefore, their end is located outside the cavity, exhibiting vanishing interactions with the host. This is in accord with the results of the calorimetric experiments (Table ), which demonstrated that the exothermicity of inclusion in SCX4 initially grew upon the gradual increase of the number of aliphatic carbon atoms in the substituent linked to the heterocyclic nitrogen and then levelled off. The incorporation of the short alkyl chains (n < 6) within the macrocycle may rationalize the line broadening observed for their 1H NMR peaks in the spectrum of CC1OQ+–SCX4, as exemplified for n = 4 in Figure B. The confinement of the aliphatic chains should indeed induce a restriction in their reorientational motions and then, a reduction of their T2(1H) relaxation times compared to free CC1OQ+. As the number of carbon atoms in the alkyl chain is raised from n = 1 to 4, the Δδ values for the aromatic protons vary. In particular, a continuous increase is observed for H2 and H8 (and also NCH2), whereas the opposite trend is observed for H3 and H4. These simultaneous variations suggest an alteration of the orientation of the quinolinium ring within the SCX4 cavity resulting from the increase of the volume occupied by the alkyl chain. In the case of the C1COQ+–SCX4 complexes, the chemical shift of the 1H NMR peaks related to the alkoxy moiety is nearly unchanged with respect to the value observed for the solution of the corresponding uncomplexed quinolinium (Figure B and Table S2). Figure shows that the chemical shift of each proton of the quinolinium ring of C1COQ+ still displays a significant change upon the addition of SCX4. In particular, the peaks attributed to H2, H3, H4, and N–CH3 protons undergo the most significant upfield shift, implying that the quinolinium ring of C1COQ+ is inside the SCX4 cavity, whereas the alkoxy chain protrudes from it. The line width of the 1H NMR peaks assigned to the alkoxy group of C1COQ+–SCX4 is similar to the one observed in the spectrum of free C1COQ+ (Figure B). In contrast to CC1OQ+–SCX4 (n < 6), the aliphatic chain is not confined within the macrocycle and as a result, no significant line broadening is found. The Δδ values for the protons of the quinolinium moiety of C1COQ+ and CC1OQ+ differ for n ≥ 2 (Figure ), suggesting distinct orientations of the heterocyclic ring within SCX4. Another main difference between the C1COQ+–SCX4 and the CC1OQ+–SCX4 complexes concerns the position of the alkoxy and alkyl chains. In the case of the CC1OQ+–SCX4 complexes, the alkyl chains may be included within the SCX4 host for low n values (n < 6). As n is raised further, the alkyl chain end extends out of the cavity. This could result from a contribution of steric hindrance. In contrast, for the C1COQ+–SCX4 complexes, the shortest alkoxy group (n = 1) is already far from the interior of the host. Therefore, the increase of this chain length does not cause any Δδ change (Figure B) and the orientation of the quinolinium ring of C1COQ+–SCX4 remains unaltered. The outward orientation from the host cavity rationalizes that the lengthening of the alkoxy substituent brings about minor change in ΔH and ΔS of C1COQ+–SCX4 complex formation (Table ). Because of the lower binding affinity to SCX6, 1H NMR spectra were recorded for a 1:3 quinolinium/SCX6 molar ratio to ensure that more than 95% of the guest was confined to the host. The variations of the proton chemical shifts (Δδ) upon complexation of C1C1OQ+ with SCX6 and SCX4 are compared in Table S3 of the Supporting Information. The upfield shift of all 1H NMR peaks upon confinement in SCX6 indicates that the entire C1C1OQ+ cation is included in the spacious cavity of the host. In the case of the C1C1OQ+SCX6 complex, the upfield shift related to the H2, H3, and H4 signals were significantly smaller because of the looser binding. For the other aromatic protons of the guest, the upfield shift was found to be higher than that of the corresponding peaks in the spectrum of C1C1OQ+SCX4. In the larger SCX6 macrocycle, various orientations of the guest could be allowed, leading to an additional averaging of the corresponding 1H chemical shifts. When a methyl substituent of C1C1OQ+ was replaced by a butyl group, the chemical shift changes induced by the incorporation into SCX6 remained similar to those of C1C1OQ+SCX6 and did not depend significantly on the location of the butyl moiety (Table S4, Supporting Information). All butyl proton signals of C4C1OQ+ and C1C4OQ+ shifted upfield, indicating that the whole butyl chain interacts with SCX6. The larger and more flexible SCX6 macrocycle adapts better to the geometrical features of the guests than SCX4. The guest binding induced calixarene conformation change, the so-called “template effect” which has also been noticed for other associates,[40,42,43] may explain the slightly larger alteration of ΔH and ΔS with the substituent in the series of C1COQ+–SCX6 complexes (Table ).

Conclusions

The confinement of CCOQ+ in SCXn cavitands significantly depends not only on the location and the length of the hydrocarbon chain of the guest but also on the size of the macrocycle. Both the thermodynamic parameters of the embedment in SCXn and the structure of the resulting CCOQ+–SCXn complexes can be tuned by the variation of the number of aliphatic carbon atoms attached to the nitrogen of the quinolinium moiety, but alteration of the alkoxy chain length causes a minor effect. 1H NMR experiments demonstrated that in the case of SCX4, the short alkyl chains (n ≤ 4) may be incorporated, together with the quinolinium ring, within the host cavity, while a part of longer alkyl chains are located out of the cavity. In contrast, even the short alkoxy groups were found to display very weak interactions with SCX4, while the quinolinium ring is still found within the cavity. The larger SCX6 macrocycle allows an easier inclusion of both kinds of quinolinium (CC1OQ+ and C1COQ+), with an incorporation of either the alkyl or the alkoxy chains within the cavity when n or m ≤ 4. From a thermodynamic point of view, the tighter binding in the smaller, more rigid SCX4 brings about larger enthalpy gain accompanied by more substantial entropy diminution, which lead to considerably larger equilibrium constant than the association with SCX6. The stability of the CCOQ+–SCX6 complexes cannot be modified by the alteration of the alkyl substituent of the guest because the enthalpy variation is compensated by the concomitant entropy change. The knowledge on the relationship between the molecular structure of constituents and the thermodynamics of host–guest binding gained in the present study may be applied in the design of tailor-made supramolecular systems and self-assembled architectures.

Experimental Section

Materials

SCX4 and SCX6 were purchased from Acros Organics and used after drying under vacuum at 343 K overnight. Double-distilled water was used as a solvent, and SCXn (n = 4 or 6) solutions were neutralized by the minimum volume of concentrated NaOH. The various 1-alkyl-6-alkoxy-quinolinium salts were synthesized and characterized as described in the Supporting Information. C1COQ+ and C4C1OQ+ had I– counterions, whereas C2C1OQ+, C6C1OQ+, and C8C1OQ+ were used as Br– salts.

Sample Preparation

Stock solutions of 1-alkyl-6-alkoxy-quinolinium salts (2 mM) and SCXn (0.1 mM, adjusted to pH 7 by NaOH addition) were prepared for ITC experiments. NMR experiments were performed by mixing appropriate amounts of 1-alkyl-6-alkoxy-quinolinium (6 or 10 mM) and SCXn (6 or 10 mM, neutralized by NaOD) solutions in D2O. All the experiments were carried out at pH 7.

Instrumentation

1H NMR spectra were recorded in deuterated dimethyl sulfoxide or in D2O on a Bruker Avance II 400 MHz NMR spectrometer. ITC measurements were carried out with a MicroCal VP-ITC microcalorimeter. Quinolinium solutions were injected from the computer-controlled microsyringe at an interval of 180 s into the cell (volume = 1.4569 mL) containing 0.1 mM SCXn solution at pH 7, while stirring at 450 rpm.
  1 in total

1.  Thermodynamic Characterization of the Interaction between the Antimicrobial Drug Sulfamethazine and Two Selected Cyclodextrins.

Authors:  Hiba Mohamed Ameen; Sándor Kunsági-Máté; Balázs Bognár; Lajos Szente; Miklós Poór; Beáta Lemli
Journal:  Molecules       Date:  2019-12-13       Impact factor: 4.411

  1 in total

北京卡尤迪生物科技股份有限公司 © 2022-2023.