Open Access Article
Urszula Bąchor
a,
Ewa Drozd-Szczygieł
*a,
Remigiusz Bąchor
*b,
Lucjan Jerzykiewiczb,
Robert Wieczorekb and
Marcin Mączyńskia
aDepartment of Organic Chemistry, Faculty of Pharmacy, Wroclaw Medical University, Borowska 211A, 50-556 Wroclaw, Poland. E-mail: ewa.drozd-szczygiel@umed.wroc.pl
bFaculty of Chemistry, University of Wroclaw, F. Joliot-Curie 14, 50-383 Wrocław, Poland. E-mail: remigiusz.bachor@chem.uni.wroc.pl
First published on 3rd September 2021
Herein we present a synthesis and characterization of a new and unique low-weight heterocyclic compound 5-amino-2-(5-amino-3-methyl-1,2-oxazol-4-yl)-3-methyl-2,3-dihydro-1,3,4-oxadiazol-2-ylium bromide with the unusual electron charge delocalization owing the local positive charge at the carbon atom of oxadiazole moiety. X-ray single crystal of C7H10N5O2·Br− showed the molecule crystalized in monoclinic, space group P21/c. Both five membered rings are planar and twisted forming the ring motif with the counter ion where H⋯Br interactions are one of the dominant. The presented compound is characterized by high ionization efficiency in ESI-MS mode and undergoes dissociation within oxadiazole moiety under ESI-MS/MS conditions even under low collision energies. The presented compound is an interesting example of heterocyclic stable carbocation which may serve as a new lead structure.
| Identification code | 3e | |
| Empirical formula | C7H10BrN5O2 | |
| Formula weight | 276.10 | |
| Temperature | 100(2) K | |
| Wavelength | 1.54184 Å | |
| Crystal system | Monoclinic | |
| Space group | P21/c | |
| Unit cell dimensions | a = 15.2177(2) Å | α = 90° |
| b = 6.76340(10) Å | β = 109.445(2)° | |
| c = 11.0057(2) Å | γ = 90° | |
| Volume | 1068.13(3) Å3 | |
| Z | 4 | |
| Density (calculated) | 1.717 Mg m−3 | |
| Absorption coefficient | 5.209 mm−1 | |
| F(000) | 552 | |
| Crystal size | 0.192 × 0.104 × 0.088 mm3 | |
| Theta range for data collection | 3.080 to 75.438° | |
| Index ranges | −18 ≤ h ≤ 19, −8 ≤ k ≤ 7, −13 ≤ l ≤ 13 | |
| Reflections collected | 25 170 |
|
| Independent reflections 2189 | [R(int) = 0.0242] | |
| Completeness to theta = 67.684° | 100.0% | |
| Absorption correction | Analytical | |
| Max. and min. transmission | 0.917 and 0.816 | |
| Refinement method | Full-matrix least-squares on F2 | |
| Data/restraints/parameters | 2189/0/157 | |
| Goodness-of-fit on F2 | 1.119 | |
| Final R indices [I > 2σ(I)] | R1 = 0.0197, wR2 = 0.0541 | |
| Largest diff. peak and hole | 0.314 and −0.458 e Å−3 | |
| N(11)–C(12) | 1.299(2) |
| N(11)–N(12) | 1.3921(18) |
| N(12)–C(11) | 1.303(2) |
| N(12)–C(13) | 1.458(2) |
| N(13)–C(12) | 1.319(2) |
| N(21)–C(22) | 1.3015(18) |
| N(21)–O(21) | 1.4407(16) |
| N(22)–C(23) | 1.3333(19) |
| O(11)–C(11) | 1.3481(19) |
| O(11)–C(12) | 1.3818(18) |
| O(21)–C(23) | 1.3436(17) |
| C(11)–C(21) | 1.431(2) |
| C(21)–C(23) | 1.3848(19) |
| C(21)–C(22) | 1.431(2) |
| C(22)–C(24) | 1.4854(19) |
| C(12)–N(11)–N(12) | 102.59(13) |
| C(11)–N(12)–N(11) | 111.64(14) |
| C(11)–N(12)–C(13) | 129.02(14) |
| N(11)–N(12)–C(13) | 119.30(13) |
| C(22)–N(21)–O(21) | 106.02(11) |
| C(11)–O(11)–C(12) | 104.39(12) |
| C(23)–O(21)–N(21) | 108.69(10) |
| N(12)–C(11)–O(11) | 108.20(13) |
| N(12)–C(11)–C(21) | 130.31(15) |
| O(11)–C(11)–C(21) | 121.48(13) |
| N(11)–C(12)–N(13) | 129.72(15) |
| N(11)–C(12)–O(11) | 113.14(13) |
| N(13)–C(12)–O(11) | 117.13(14) |
| C(23)–C(21)–C(11) | 127.35(14) |
| C(23)–C(21)–C(22) | 104.78(12) |
| C(11)–C(21)–C(22) | 127.76(13) |
| N(21)–C(22)–C(21) | 111.40(12) |
| N(21)–C(22)–C(24) | 119.91(12) |
| C(21)–C(22)–C(24) | 128.68(12) |
| N(22)–C(23)–O(21) | 117.33(12) |
| N(22)–C(23)–C(21) | 133.62(13) |
| O(21)–C(23)–C(21) | 109.05(12) |
| C(12)–N(11)–N(12)–C(11) | −1.93(13) |
| C(12)–N(11)–N(12)–C(13) | 176.10(11) |
| C(22)–N(21)–O(21)–C(23) | 0.02(14) |
| N(11)–N(12)–C(11)–O(11) | 1.64(13) |
| C(13)–N(12)–C(11)–O(11) | −176.15(11) |
| N(11)–N(12)–C(11)–C(21) | −179.43(13) |
| C(13)–N(12)–C(11)–C(21) | 2.8(2) |
| C(12)–O(11)–C(11)–N(12) | −0.65(13) |
| C(12)–O(11)–C(11)–C(21) | −179.69(12) |
| N(12)–N(11)–C(12)–N(13) | −177.98(14) |
| N(12)–N(11)–C(12)–O(11) | 1.50(13) |
| C(11)–O(11)–C(12)–N(11) | −0.61(14) |
| C(11)–O(11)–C(12)–N(13) | 178.94(12) |
| N(12)–C(11)–C(21)–C(23) | 41.3(2) |
| O(11)–C(11)–C(21)–C(23) | −139.88(14) |
| N(12)–C(11)–C(21)–C(22) | −134.27(15) |
| O(11)–C(11)–C(21)–C(22) | 44.5(2) |
| O(21)–N(21)–C(22)–C(21) | 1.44(15) |
| O(21)–N(21)–C(22)–C(24) | −178.33(12) |
| C(23)–C(21)–C(22)–N(21) | −2.33(16) |
| C(11)–C(21)–C(22)–N(21) | 174.04(14) |
| C(23)–C(21)–C(22)–C(24) | 177.41(13) |
| C(11)–C(21)–C(22)–C(24) | −6.2(2) |
| N(21)–O(21)–C(23)–N(22) | 178.65(11) |
| N(21)–O(21)–C(23)–C(21) | −1.50(15) |
| C(11)–C(21)–C(23)–N(22) | 5.7(3) |
| C(22)–C(21)–C(23)–N(22) | −177.92(15) |
| C(11)–C(21)–C(23)–O(21) | −174.13(13) |
| C(22)–C(21)–C(23)–O(21) | 2.26(15) |
The 1.299(2) Å C12–N11 bond is the shortest whilst the 1.458(2) Å C13–N12 bond is the longest among the C–N bonds of the two heterocyclic rings (Table 2). These differences in bond lengths may be explained by the occurrence to the distribution of the positive charge between the atoms of heterocyclic rings and the fixation of the conjugate bond system. As a consequence of conjugation both five-membered rings are planar with maximum deviation of the carbon atoms from the least-squares planes by 0.008(2) Å and 0.014(1) Å for 1,3,4-oxadiazole ring and 0.014(1) Å for isoxazole ring, respectively. Moreover, as expected, the amino and methyl groups lie in the planes of these heterocyclic rings, with the torsion angles in the range of 1.1(1) to 5.7(3)° (Table 3). These observations confirm the presence of the electron delocalization through the chemical bonds. This delocalization of the electron, also support shortening the bond length between the 1,3,4-oxadiazole and isoxazole rings (C(11)–C(21) 1.431(2) Å). In addition, these rings are twisted about 75.5(3)°. The crystal structure of the analyzed compound is stabilized by hydrogen bonds and the presence of other weak intermolecular interactions (Fig. 2). The percentages of main interactions, quantified by Hirshfeld surface analysis is shown in Fig. 3.
The amino group of the cation and the bromide anion are connected to form a ring R24(8) motif (Fig. 4). These ring motifs are arranged along the b-axis of the unit cell. Moreover, cations of the analyzed compound are connected each other via N(22)–H(3)⋯N(21)[−x + 1,y − 1/2,−z + 3/2] hydrogen bonding generates C(8) chains of cations propagating in [010] with adjacent ions related by the screw axis (Fig. 5). This C(8) chains are stabilized by additional the N(22)–H(4)⋯Br(1)[x,−y + 1/2,z + 1/2] interaction.
On the presented mass spectrum obtained in the positive ion mode (Fig. 6) high intense signal at m/z 196.0830 corresponding to the M+ ion of model compound is observed. The obtained m/z value is in good agreement with calculated m/z ratio which is equal to 196.0829. The enlarged isotope pattern confirms the ion charge and low amount of carbon atom in the analyzed cation. Other signal have not been identified. The observed even m/z value is in agreement with the nitrogen rule for even-electron ions in ESI-MS mode. Ionization of this compound is the consequence of its chemical structure containing positive charge. To determine the chemical structure of the analyzed compound the ESI-MS/MS analysis under different collision energies was performed (Fig. 7).
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| Fig. 7 ESI-MS/MS spectra of analyzed compound obtained at different collision energy. Parent ion m/z 196.0830, collision energy (A) 10 eV, (B) 20 eV, (C) 30 eV. | ||
The obtained MS/MS spectra present a small amount of signals corresponding to the parent ion even under higher collision energy (Fig. 7). The most common signals are at m/z 154.0615, m/z 127.0507, m/z 110.0242 and m/z 82.0287. The fragmentation pathways and the possible structure of formed fragment ions are presented in the Fig. 8. The obtained m/z values of fragment ions are in a good agreement with the calculated ones and meet the nitrogen rule for even-electron ions.
The analyzed compound is thermodynamically stable dual-ring ion (see Fig. 9) with enthalpy H = −696.461666 hartree.
Compound consists of one oxadiazole and one oxazole rings, connected by C–C bond (1.413 Å). Please note that the rings planes are twisted, as expected, and the N6–C2–C15–C4 dihedral angle equals 35.2°.
The OCNNC oxadiazole ring builds interatomic distances 1.362 Å, 1.294 Å, 1.380 Å, 1.310 Å and 1.343 Å where atoms number 14, 1, 3, 6 and 2 are used respectively (see Table 5). The second, smaller in diameter oxazole ring, builds interatomic distances 1.412 Å, 1.312 Å, 1.388 Å, 1.442 Å and 1.291 Å between N, O, C, C, C of the ring atoms as presented in Table 5.
| Atoms | DFT | Exp. |
|---|---|---|
| C1–N11 | 1.329 | 1.319 |
| C1–O14 | 1.362 | 1.382 |
| C1–N3 | 1.294 | 1.299 |
| N3–N6 | 1.380 | 1.392 |
| O14–C2 | 1.343 | 1.348 |
| N6–C7 | 1.452 | 1.458 |
| C2–C15 | 1.413 | 1.431 |
| C15–C5 | 1.442 | 1.431 |
| C5–C18 | 1.488 | 1.486 |
| C5–N17 | 1.291 | 1.301 |
| N17–O16 | 1.412 | 1.441 |
| O16–C4 | 1.312 | 1.343 |
| C4–C15 | 1.388 | 1.385 |
| C4–N22 | 1.343 | 1.333 |
Each ring is substituted with methyl and amino group. Due to different bond type between methyl groups and rings only comparison involving amino groups is accessible here. Interestingly the C1–N11 distance ∼1.33 Å is shorter that C4–N22 ∼ 1.34 Å that suggests increase of the double bond character between C1–N11 in comparison to C4–N22 bond.
The DFT calculated parameters of the structure are in good agreement with presented experimental values.
| Atom | Charge | ||
|---|---|---|---|
| 0 | +1 | Delta | |
| C 1 | 0.72 | 0.74 | 0.02 |
| C 2 | 0.36 | 0.64 | 0.28 |
| N 3 | −0.41 | −0.36 | 0.05 |
| C 4 | 0.53 | 0.64 | 0.12 |
| C 5 | 0.22 | 0.25 | 0.04 |
| N 6 | −0.26 | −0.17 | 0.09 |
| C 7 | −0.35 | −0.36 | −0.01 |
| H 8 | 0.18 | 0.22 | 0.04 |
| H 9 | 0.21 | 0.23 | 0.01 |
| H 10 | 0.20 | 0.24 | 0.04 |
| N 11 | −0.81 | −0.78 | 0.04 |
| H 12 | 0.41 | 0.43 | 0.02 |
| H 13 | 0.40 | 0.42 | 0.02 |
| O 14 | −0.52 | −0.46 | 0.06 |
| C 15 | −0.32 | −0.38 | −0.06 |
| O 16 | −0.36 | −0.32 | 0.04 |
| N 17 | −0.19 | −0.12 | 0.06 |
| C 18 | −0.60 | −0.61 | −0.01 |
| H 19 | 0.21 | 0.23 | 0.01 |
| H 20 | 0.21 | 0.22 | 0.01 |
| H 21 | 0.22 | 0.25 | 0.03 |
| N 22 | −0.82 | −0.78 | 0.04 |
| H 23 | 0.39 | 0.42 | 0.03 |
| H 24 | 0.38 | 0.40 | 0.02 |
The NBO analysis describes the C2 atom as the most electrophilic with 28% positive charge accumulated.
:
3, and detected with UV Krüss Optronic 254 nm lamp. NMR spectra were recorded on high-field spectrometer Bruker Avance 500 MHz using TMS as the internal standard. Complete 1H NMR, 13C NMR, 13C NMR-DEPT135 and HMQC analysis were performed on samples dissolved in DMSO-d6. All ESI-MS experiments were performed on the LCMS-9030 qTOF Shimadzu (Shimadzu, Kyoto, Japan) device, equipped with a standard ESI source and the Nexera X2 system. Analysis was performed in the positive ion mode between 50–1000 m/z. LCMS-9030 parameters: nebulizing gas–nitrogen, nebulizing gas flow 3.0 L min−1, drying gas flow – 10L min−1, heating gas flow – 10L min−1, interface temperature 300 °C, desolvation line temperature – 400 °C, detector voltage – 2.02 kV, interface voltage 4.0 kV, collision gas–argon, collision energy was optimized between 10 and 30 eV. The injection volume was optimized depending on the intensity of the signals observed on the mass spectrum within the range of 0.1 to 1 μl. All obtained signals had a mass accuracy error in the range of 1 ppm.
Single crystals of analyzed compound suitable for X-ray analysis were grown at room temperature by slow evaporation of methanol solution. Summary of structure determination is given in Table 1. Single crystal data collection was performed on a Rigaku XtaLAB Synergy-S single crystal X-ray diffractometer with CuKα radiation. at 100 (2) K. Cell refinement, data reduction, analysis, and absorption correction were carried out with CRYSALISPro (Rigaku Oxford Diffraction, Wrocław, Poland) software. Cell refinement, data reduction, analysis, and absorption correction were carried out with CRYSALISPro (Rigaku Oxford Diffraction, Wrocław, Poland) software. The structures were solved by direct methods with SHELXS23 and refined with full-matrix least-squares techniques on F2 with SHELXL.24 The C-bonded hydrogen atoms were calculated in idealized geometry riding on their parent atoms.
The elemental analysis was performed on the elemental analyzer Vario EL III CHNS (Elementar, Germany).
Found: C, 31.06%; H, 3.58%; N, 25,78%.
Footnote |
| † Electronic supplementary information (ESI) available: 1H, 13C, 13C DEPT135, ESI-MS, X-ray crystallographic data of the analyzed compound (CIF) see supplementary materials. CCDC 2084686. For ESI and crystallographic data in CIF or other electronic format see DOI: 10.1039/d1ra05116d |
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