Thiravidamani Senthil
Pandian
a,
Yusun
Choi
a,
Venkatesan
Srinivasadesikan
b,
Ming-Chang
Lin
*b and
Jongmin
Kang
*a
aDepartment of Chemistry, Sejong University, Seoul, 143-747, South Korea. E-mail: kangjm@sejong.ac.kr; chemmcl@emory.edu
bCenter for Interdisciplinary Molecular Science, Department of Applied Chemistry, National Chiao Tung University, Hsinchu 300, Taiwan
First published on 3rd November 2014
A novel chromogenic anion receptor 1 based on acylhydrazone and pyrazole has been designed and synthesized. Chromogenic anion receptor 1 forms stable 1:
1 complexes with dihydrogen phosphate (H2PO4−) and other halide (Cl−, Br−) anions in DMSO solution, as shown by UV-vis, fluorescence and 1H NMR spectroscopic experiments. The pyrazole containing host 1 in the optimized geometry of the complex has been noted as planar. The planarity of the host with the H2PO4− anion resulted from four strong N–H⋯O and two weak C–H⋯O types of H-bonding. In total six H-bonding and the planarity of the host in the complex are responsible for the high binding energy. The addition of an excess of more basic anions (F− and CH3COO−) induces stepwise deprotonation, an event signalled by the appearance of a bright yellow color. The intensity of the fluorescence spectrum increases when hydrogen bonding occurs and decreases when deprotonation occurs, which is evidenced by fluorescence titrations.
As anions display a wide range of geometries, the design and synthesis of artificial receptors that exhibit high binding affinity and selectivity to a targeted anion still remain great challenges. Among various noncovalent interactions, hydrogen-bonding interactions are particularly useful and effective in this regard. To achieve high binding affinity and good selectivity, hydrogen bonding moieties are arranged in space in a rigid and convergent manner. In addition, receptors bearing multiple hydrogen bonding moieties have been shown to be useful to promote cooperative binding, which would result in enhanced binding affinity.11,12 Previously we have achieved selective and cooperative hydrogen bonding for dihydrogen phosphate utilizing acylhydrazone and indole.13 Recently, we also found that similar selective and cooperative hydrogen bonding for dihydrogen phosphate could be achieved by introducing the pyrazole group instead of the indole group. From modeling, we found that six H-bonding resulting from four strong N–H⋯O and two weak C–H⋯O types of H-bonding and the planarity of the host in the complex are responsible for the high binding energy. Here we would like to report the synthesis and the anion binding phenomena of receptor 1. The binding phenomena of receptor 1 could be monitored by UV-vis, fluorescence and 1H NMR spectra.
Receptor 1 was synthesized by reacting anthracene-1,8-dicarbaldehyde15 and 3-(4-nitrophenyl)-1H-pyrazole-5-carbohydrazide in ethanol using acetic acid as a catalyst with a yield of 49%.
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Fig. 1 Family of spectra recorded over the course of titrating a 20 μM DMSO solution of receptor 1 with increasing amounts of tetrabutylammonium dihydrogen phosphate. |
Receptor 1 showed a strong fluorescence emission spectrum in DMSO as expected. The excitation wavelength was 394 nm and emission wavelengths were 422, 452 and 475 nm. The intensity of the emission spectrum from 20 μM solution of receptor 1 gradually increased as the concentration of tetrabutylammonium dihydrogen phosphate salts was increased (1–23 equiv.), which also indicates the association between receptor 1 and dihydrogen phosphate (Fig. 2).
Hydrogen bond formation was also confirmed by 1H NMR titration. In the 1H NMR of receptor 1, not only amide N–H and pyrazole N–H peaks but also imine C–H peak is broad probably due to the slow rotation of two pyrazole arms. When dihydrogen phosphate was added, two N–H peaks showed intense broadening and the imine C–H peak (Hi) showed a downfield shift (Fig. 3). We believe that these phenomena were caused by a slow equilibrium between receptor 1 and dihydrogen phosphate as well as the complexation of added dihydrogen phosphate by receptor 1 through amide N–H, pyrazole N–H, and imine C–H hydrogen bond formation.16–18 Furthermore, anthracene 9-H(H9) showed an upfield shift. In fact, two effects are expected as a result of hydrogen bond formation between receptor 1 and the anion. (i) A through-bond propagation increases the electron density in the anthracene ring, which causes a shielding effect and promotes an upfield shift; (ii) a through-space effect increases a polarization of C–H bonds, which causes deshielding and promotes a downfield shift. In this case, the through-bond propagation dominates, and an upfield shift is observed for the anthracene 9-H peak.
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Fig. 3 1H NMR spectra of 2 mM of receptor 1 containing increasing amounts of tetrabutylammonium dihydrogen phosphate (0–6.6 equiv.) in DMSO-d6. |
The stoichiometry between receptor 1 and dihydrogen phosphate was determined to be 1:
1 using a UV-vis Job plot in DMSO-d6 (Fig. 4). A Benesi–Hildebrand plot19 by the use of change at 433 nm in the UV-vis spectrum and at 475 nm in the fluorescence spectrum gave the association constants for dihydrogen phosphate. The calculated association constants for dihydrogen phosphate were 1.2 × 104 by UV-vis titration and 1.1 × 104 by fluorescence titration.
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Fig. 4 Job plots of receptor 1 with tetrabutylammonium dihydrogen phosphate and tetrabutylammonium chloride obtained by the UV-vis spectrum in DMSO. |
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Fig. 5 A family of spectra recorded over the course of titrating a 20 μM DMSO solution of receptor 1 with increased amounts of tetrabutylammonium bromide. |
The existence of the isosbestic point for UV-vis titrations of receptors 1 with chloride suggests a 1:
1 complexation, and this was also confirmed by Job's plot analysis (Fig. 4).
In fluorescence titration with chloride, the intensity of the emission spectrum gradually increased as the concentration of tetrabutylammonium chloride salts was increased (1–150 equiv.), which also indicates hydrogen bonding between receptor 1 and chloride (Fig. 6).
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Fig. 6 The change of fluorescence spectra over the course of titration of 20 μM DMSO solutions of receptor 1 when tetrabutylammonium chloride was added. |
The association constants calculated for chloride were 8.0 × 102 for UV-vis titration and 5.7 × 102 for fluorescence titration. Other halides such as bromide showed similar behaviors toward chloride; calculated binding constants for other anions are summarized in Table 1.
Anion | UV | Fluorescence |
---|---|---|
DP – deprotonation. | ||
H2PO4− | 1.2 × 104 | 1.1 × 104 |
HSO4− | 1.1 × 103 | 1.2 × 103 |
Cl− | 8.0 × 102 | 5.7 × 102 |
Br− | 5.3 × 102 | 5.2 × 102 |
CH3COO− | DP | DP |
F− | DP | DP |
The selective sensing ability of receptor 1 for tetrahedral shaped anions such as dihydrogen phosphate and hydrogen sulfate could be seen from fluorescence intensity change with binding anions. No significant fluorescence intensity changes were observed upon the addition of 22 equiv. of halides such as chloride and bromide (Fig. 7). This result shows that receptor 1 has an optimum geometry for dihydrogen phosphate.
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Fig. 7 Fluorescence intensity changes of 1 (20 μM) upon the addition of various anions (22 equiv.) in DMSO at λex = 460 nm 1, host 1 alone; 2, H2PO4−; 3, HSO4−; 4, Cl−; 5, Br−. |
In UV-vis titration with acetate, a similar phenomenon was observed with an isosbestic point at 343 nm. In fluorescence titration with acetate, the intensity of the emission spectrum from 20 μM solution of receptor 1 gradually decreased as the concentration of tetrabutylammonium acetate salts was increased (1–80 equiv.). The decrease of fluorescence intensity was also observed with hydroxide (see ESI†). Therefore, it could be concluded that only deprotonation occurred with acetate. It was not easy to figure out which hydrogen is deprotonated first between pyrazole N–H(H29, H57) and amide N–H(H45, H72) from receptor 1 as both peaks are too broad. Therefore we tried the 1H NMR titration of 3-(4-nitrophenyl)-1H-pyrazole-5-carbohydrazide, which showed the pyrazole peak and the amide peak clearly. When we added 0.5 equivalents of tetrabutylammonium fluoride, we observed that the pyrazole peak disappeared first (Fig. 9). From this experiment, we suggest that pyrazole N–H(H29, H57) would be deprotonated first from receptor 1 although we cannot see the deprotonation phenomena of receptor 1 clearly through 1H NMR.
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Fig. 9 1H NMR spectra of 2 mM of 3-(4-nitrophenyl)-1H-pyrazole-5-carbohydrazide containing increasing amounts of tetrabutylammonium fluoride (0–3 equiv.) in DMSO-d6. |
Fig. 10 shows color change of solutions of receptor 1 after adding various anions in DMSO. Color changes from light green to purple or intense yellow were observed in the presence of hydroxide, fluoride or acetate, whereas dihydrogen phosphate did not induce any color change. UV-vis titration results and these color changes suggest that deprotonation events occurred due to hydroxide, fluoride and acetate but hydrogen bonding occurs between dihydrogen phosphate and receptor 1.
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Fig. 10 Color changes of receptor 1 at 100 μM in DMSO when treated with 80 equivalents of various anions. |
The other anions did not induce any color changes even when added in excess. The examples of selectively sensing acetate from dihydrogen phosphate are relatively limited due to the similarity of their basicity. However, they were able to be differentiated by considering the different color responses observed.
The B3LYP hybrid functional consists of Becke's exchange functional, the Lee–Yang–Parr correlation functional, and a Hartree–Fock exchange term. The DFT has been successfully used to study hydrogen-bonded complexes,20 even for the most weakly bonded systems.21 The calculated binding energy is corrected for the basis set superposition error (BSSE) using the counter poise method.22 The experimental binding constant of a newly synthesized compound shows similarity to the previously reported receptors,13 which was unexpected because the present receptor seems to be formed possibly by four strong N–H⋯O and two weak C–H⋯O types of H-bonding. So, we have decided to investigate the binding process more accurately using the state-of-the-art density functional theory. Fig. 11 shows the optimized structure of the host and its H2PO4− complex optimized at the B3LYP level23–26 using the 6-31g(d) basis set. The binding energies of experimental and theoretical values are reported in Table 2.
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Fig. 11 Most stable structure of the host·H2PO4− complex in the solvent phase (DMSO as a solvent) optimized using B3LYP/6-31g(d) in Gaussian 09. Dashed lines denote the hydrogen bonds (strong and weak). See Table 3 for geometrical parameters and Mulliken charges. Atom numbering included. Atom colors: grey-carbon; red-oxygen; blue-nitrogen; white-hydrogen; orange-phosphorus. |
BE | ||
---|---|---|
Anions | Exp. (UV) | Calc. (DFT) |
a Units are in kcal mol−1. Experimental binding energy is derived from the UV binding constant. DFT calculations are performed at (B3LYP/6-31G(d)) using a polarizable continuum model in DMSO. The basis set superposition error is corrected. | ||
H2PO4− | −5.56 | −24.96 |
HSO4− | −4.15 | −16.27 |
Cl− | −3.96 | −13.04 |
Br− | −3.71 | −11.69 |
The experimental binding energy is derived from the binding constant (UV experiments). For the solvent effect the DMSO is considered using the PCM (polarizable continuum model).27 The binding energy calculation and computational details have been described in the ESI.† All calculations have been computed by using the Gaussian 09 suite of programs.28
To obtain the complex structure, several geometries have been considered for optimization. Here, we chose the lowest-energy structure as a representative one. All geometries of the host, the guest and the complex have been optimized without any stringent optimization criteria. We could not perform the second derivatives due to the size of the system and the limitation of computational resources. We assume that the experimental binding energies should correlate with the calculated binding energy value (see Table 2). When we compare the calculated binding energy with the experimental binding energy, we noted the difference between the theory and the experiment. The divergence is not unexpected due to the crude solvation model used in the theoretical calculation and the host–anion complex interactions are rather complicated. The chronological order of binding energies derived from the theoretical calculation for host–anion complexes is consistent with the experimental results (see Table 2). Furthermore, the results have been focused on the host·H2PO4− complex due to its large binding energy and specific binding properties towards the pyrazole receptor in the current study.
Theoretically the calculated structure contains all experimentally observed H-bonding elements (Fig. 11). The remarkable result of the computed binding configuration of the host–H2PO4− complex reveals that all the N–H protons have acted as donors for H2PO4−. Overall, four N–H⋯O types of H-bonding have been observed in the host–H2PO4− complex. Moreover, two additional weak C–H⋯O types of H-bonding have also been observed. The newly introduced pyrazole group instead of the indole group in our previous report shows the strong binding with H2PO4− due to the strong four N–H⋯O types of H-bonding. And, the pyrazole containing host in the optimized geometry of the complex has been interestingly noted to be planar, which is not the case in the indole containing host optimized geometry of the complex in our previous report.13 The planarity of the host with a strong H-bonding has produced the highest binding energy for the presently investigated pyrazole containing host complex. The bond angle of ∠N48H29O78 is observed to be 160.9° in the complex. All hydrogen atoms in the cage of the pyrazole containing host point towards the oxygen of the H2PO4− anion and form H-bonding in the complex. We have also attempted to optimize the geometry to form the H-bonding with O–H83 in the H2PO4− anion with N49 in the pyrazole ring. But the optimized results give a similar type of geometry as shown in Fig. 11 of the present study, due to the long distance between O–H83 and N49, 4.834 Å, which is too far for H-bonding. The hydrogen bonding configurations are denoted by dashed lines in Fig. 11 and the corresponding H-bonding lengths are listed in Table 3. In general the X–H⋯B H-bonding length is longer than that of corresponding individual monomers. Once the H-bonding becomes shortened it strengthens the complex.
cx | Host | ||
---|---|---|---|
Mulliken atomic charges (e) | |||
H40 | 0.1669 | 0.167 | |
H15 | 0.1617 | 0.1578 | |
H73 | 0.1914 | 0.167 | |
H29 | 0.4084 | 0.3833 | |
H45 | 0.4185 | 0.3632 | |
H57 | 0.4174 | 0.3833 | |
H72 | 0.4255 | 0.3632 | |
Heavy atom distance (Å) | |||
C23–O77 | 3.848 | ||
C7–O77 | 3.774 | ||
C50–O77 | 3.474 | ||
N48–O78 | 2.752 | ||
N25–O78 | 2.874 | ||
N59–O79 | 2.761 | ||
N52–O79 | 2.866 | ||
H-bond distance (Å) | |||
H40⋯O77 | 2.771 | ||
H15⋯O77 | 2.939 | ||
H73⋯O77 | 2.521 | ||
H29⋯O78 | 1.758 | ||
H45⋯O78 | 1.848 | ||
H57⋯O79 | 1.762 | ||
H72⋯O79 | 1.838 | ||
Bond angle (deg) | |||
C23H40O77 | 168.5 | ||
C7H15O77 | 134.4 | ||
C50H73O77 | 145.5 | ||
N48H29O78 | 160.9 | ||
N25H45O78 | 172.5 | ||
N59H57O79 | 133.2 | ||
N52H72O79 | 174.0 |
Complex | HOMO (eV) | LUMO (eV) | HLGa (eV) | TD-DFT calculated datab | ||||
---|---|---|---|---|---|---|---|---|
E | λ abs,cal (nm) | f | Conf.d | Wt (%) | ||||
a HOMO, LUMO, and HOMO–LUMO gaps (HLG) are calculated by the B3LYP/6-31G(d) method. b Absorption energies are calculated by the TD-DFT method at the B3LYP/6-31G(d) level. c Oscillator strength. d H and L stand for the predicted HOMO and LUMO, respectively. Ho stands for the host. | ||||||||
Ho⋯H2PO4− | −4.47 | −2.20 | 2.27 | S1 | 503 | 0.0237 | H → L | 69 |
Ho⋯Br− | −4.53 | −2.21 | 2.32 | S1 | 491 | 0.0203 | H → L | 84 |
Ho⋯Cl− | −4.54 | −2.21 | 2.33 | S1 | 489 | 0.0256 | H → L | 84 |
Ho⋯HSO4− | −4.49 | −2.21 | 2.28 | S1 | 499 | 0.014 | H → L | 74 |
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Fig. 12 Molecular orbital distribution plots of HOMO and LUMO states in the ground state of the host⋯H2PO4− complex. |
For the host–H2PO4− anion complex (see Fig. 12), the lowest energy singlet transitions are mainly from the HOMO to the LUMO. For other anion complexes reported here, they also show the similar results as HOMO to LUMO singlet transitions. The HOMO–LUMO gaps (HLGs) have also been calculated and reported in Table 4. Among the anions H2PO4− shows the lowest HLGs supporting the selective binding as confirmed from our experimental results. For both anthracene and pyrazole units FMOs are delocalized over the entire structure. To envision the above observations and the trend we carried out the TD-DFT calculations and results are listed in Table 4. In all the anion complexes the transition energies result mainly from the HOMO to the LUMO.
Footnote |
† Electronic supplementary information (ESI) available: 1H, 13C, and HRMS spectra and binding energy calculations for the optimized host–anion complexes. See DOI: 10.1039/c4nj01063a |
This journal is © The Royal Society of Chemistry and the Centre National de la Recherche Scientifique 2015 |