| Literature DB >> 33390633 |
Abdel Majid A Adam1, Hosam A Saad1, Amnah M Alsuhaibani2, Moamen S Refat1, Mohamed S Hegab3.
Abstract
Around the world, the antibiotic azithromycin (Entities:
Keywords: Azithromycin; Charge–transfer; Iodine; Solvent effect; Tri–iodide ion
Year: 2020 PMID: 33390633 PMCID: PMC7764390 DOI: 10.1016/j.molliq.2020.115187
Source DB: PubMed Journal: J Mol Liq ISSN: 0167-7322 Impact factor: 6.165
Scheme 1Structure of the AZM molecule.
Fig. 1Strong color change upon mixing iodine (far left; violet) with AZM (middle; colorless) to produce the AZM-I2 CT complex (far right; brown) in the CH2Cl2 solvent.
Fig. 2Representative image of (A) free AZM (white) and (B) the solid AZM-I2 CT complex (brown).
Fig. 3Electronic absorption spectra of the AZM donor (5.0×10−4 M), the iodone acceptor (5.0×10−4 M), and the resulting AZM-I2 complex in CH2Cl2, CH3Cl, CCl4 and C6H5Cl solvents.
Fig. 4Stoichiometry of the interaction between AZM and I2 in solution-state determined by Method 1: Job's continuous variation, and Method 2: spectrophoometric titration.
Fig. 5The 1:1 and 1:2 Benesi-Hildebrand plots of the AZM–I2 complex prepared in different solvents.
Spectroscopic parameters of the AZM-I2 complex at 298 K according to solvent.
| Property | Value | |||
|---|---|---|---|---|
| CH2Cl2 | CCl4 | C6H5Cl | CH3Cl | |
| 364 | 364 | 372 | 510 | |
| Formation constant; | 74×106 | 257×106 | 107×106 | 2.7×106 |
| Free energy change; | −4.49×104 | −4.80×104 | −4.58×104 | −3.67×104 |
| Extinction coefficient; | 16.8×10 | 10.3×103 | 6×103 | 175×103 |
| Resonance energy; | 0.42 | 0.31 | 0.21 | 0.62 |
| Energy of interaction; | 3.42 | 3.34 | 3.42 | 2.44 |
| Ionization potential; | 9.96 | 9.87 | 9.95 | 8.76 |
| Dissociation energy; | 3.48 | 3.47 | 3.47 | 3.26 |
| Oscillator strength; | 1.209 | 0.557 | 0.431 | 7.583 |
| Dipole moment; | 3.06 | 2.10 | 1.83 | 9.06 |
| Correlation coefficient; | 0.9909 | 0.9991 | 0.9906 | 0.9853 |
Fig. 6IR spectra of the free AZM, and the resultant CT complex in CH2Cl2 solvent.
FT-IR frequencies with their tentative vibrational assignments for free AZM and the CT complex prepared in the CH2Cl2 solvent.
| Wavenumber (cm−1) | Mode of vibration | |
|---|---|---|
| Free AZM | CT complex | |
| 3486, 3238 | 3355 | ν(O-H) |
| 2972 | 2965 | νas(CH3) |
| 2932 | 2930 | νas(CH2) |
| 2887 | 2883 | νs(CH3) |
| 2830, 2782 | – | νs(CH2) |
| 1718 | 1720 | νas(C=O) |
| 1660 | 1626 | νs(C=O) |
| 1450 | 1455 | δsciss(CH3) |
| 1374 | 1378 | δsciss(CH2) |
| 1260 | 1255 | δrock(CH2) |
| 1175 | 1169 | νas(C-N) |
| 1088 | 1046 | νs(C-N) |
| 1040 | 1000 | ν(C-O) |
| 984 | 950 | ν(C-C) |
| 898 | 893 | δ(O-H) in-plane bending |
| 832 | – | δrock(CH3) |
| 794 | 798 | δwag(CH2) |
| 731 | 750 | δ(O-H) out-of-plane bending |
| 560 | 575 | δtwist(CH2) |
Fig. 7Raman spectrum of AZM–I2 complex in CH2Cl2 solvent.
Fig. 8XRD spectra of the solid CT products prepared in CH2Cl2, CH3Cl, CCl4 and C6H5Cl solvents.