Literature DB >> 35910121

Synthesis, Crystal Structures, and Density Functional Theory Studies of Two Salt Cocrystals Containing Meldrum's Acid Group.

Wulan Zeng1, Xia Wang1, Yunju Zhang2.   

Abstract

Two salt cocrystals, C31H34N4O8 (DDD) and C17H20N2O8 (MDD), were synthesized and their structures were determined by single-crystal X-ray diffraction. DDD is made up of one (C13H13O8)- anion, one (C9H11N2)+ cation, and one 5,6-dimethyl-1H-benzo[d]imidazole molecule. MDD consists of one (C4H7N2)+ cation and one (C13H13O8)- anion. DDD and MDD belong to the monoclinic, P21/c space group and triclinic, P-1 space group, respectively. A 1D-chained structure of DDD was constituted by N-H···N and N-H···O hydrogen bonds. However, a 1D-chained structure of MDD was bridged by N-H···O hydrogen bonds. Their density functional theory-optimized geometric structures with a B3LYP/6-311G(d,p) basis set fit well with those of crystallographic studies. By calculating their thermodynamic properties, the correlation equations of C 0 p,m , S 0 m , H 0 m , and temperature T were obtained. By comparing the experimental electronic spectra with the calculated electronic spectra, it is found that the PBEPBE/6-311G(d,p) method can simulate the UV-Vis spectra of DDD and MDD. In addition, the fluorescence spectra in the EtOH solution analysis show that the yellowish-green emission occurs at 570 nm (λex = 310 nm) for DDD and the purplish-blue emission occurs at 454 nm (λex = 316 nm) for MDD.
© 2022 The Authors. Published by American Chemical Society.

Entities:  

Year:  2022        PMID: 35910121      PMCID: PMC9330170          DOI: 10.1021/acsomega.2c01761

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


Introduction

As an important kind of N-heterocycle, imidazole and its derivatives have been widely applied in various fields including medicinal chemistry,[1] bio-organic chemistry,[2] fuel cells and solar cells,[3,4] mild steel corrosion,[5] electrocatalysts,[6] agriculture,[7] industry,[8] organic light-emitting diodes (OLEDs),[9,10] colorimetric and fluorometric chemosensors,[11] and luminescent materials.[12] As another kind of N-heterocycle, benzimidazole and its derivatives have also received significant attention owing to their potential applications in fluorescent sensors,[13,14] fluorescent probes,[15] chemodosimeters,[16] OLEDs,[17] and phosphorescent organic light-emitting diodes (PhOLEDs).[18] Recently, Meldrum’s acid plays an increasingly important role in the synthesis of pharmacologically active compounds such as dual inhibitors of AChE and BChE in the treatment of Alzheimer’s disease,[19] antibacterial agents,[20] anticancer agents,[21] and antioxidant agents.[22] In particular, C-5-substituted derivatives of Meldrum’s acid have attracted considerable interest owing to their structure and unique properties. Different synthetic routes toward the C(5)-position of Meldrum’s acid have been reported.[23−26] Based on the above facts, a series of C-5-substituted derivatives of Meldrum’s acid were prepared by our group during the past 10 years.[27−30] However, to the best of our knowledge, most of the reported preparation methods are step by step, and each intermediate needs to be isolated and purified. In this work, two salt cocrystals containing Meldrum’s acid group are available via a simple one-pot eco-friendly method. Furthermore, less theoretical calculations or vibrational analyses have been carried out on Meldrum’s derivatives coupled with a benzo[d]imidazole or imidazole nucleus. As a part of ongoing research, two new compounds (Chart ), 5,6-dimethyl-1H-benzo[d]imidazol-3-ium5-((2,2-dimethyl-4,6-dioxo-1,3-dioxan-5-ylidene)methyl)-2,2-dimethyl-4,6-dioxo-1,3-dioxan-5-ide,5,6-dimethyl-1H-benzo[d]imidazole (DDD) and 2-methyl-1H-imidazol-3-ium5-((2,2-dimethyl-4,6-dioxo-1,3-dioxan-ylidene)methyl)-2,2-dimethyl-4,6-dioxo-1,3-dioxan-5-ide (MDD), were obtained by reacting Meldrum’s acid with 5,6-dimethyl-1H-benzo[d]imidazole and 2-methyl-1H-imidazole in the mixture of trimethoxymethane and ethanol. Their crystal structures, vibrational frequencies, thermodynamic properties, and electronic spectra along with density functional theory (DFT) or time-dependent DFT (TD-DFT) calculational results are also reported.
Chart 1

Synthetic Routes of MDD and DDD

Experimental and Theoretical Methods

Physical Methods

IR data were obtained on a Nicolet 5700 FT-IR Spectrometer. The UV–Vis absorption and fluorescence spectra were collected on a TU-1901 spectrometer and an RF-5301PC fluorospectrophotometer, respectively. The C, H, and N atoms of the two compounds were recorded on an Elementar Vario EL III elemental instrument. The NMR (1H and 13C) spectra in CDCl3 were obtained on a Bruker AVANCE III HD instrument (400 MHz).

Preparation of Two Cocrystals

The synthetic method of the two compounds was the same as that in our earlier report.[31] Briefly, a mixture of Meldrum’s acid (0.72 g, 5 mmol) and trimethoxymethane (0.635 g, 6 mmol) was dissolved in EtOH (20 mL) and refluxed at 70 °C for 2–2.5 h. Then, 2-methyl-1H-imidazole (0.41 g, 5 mmol) was added to the reaction solution and the mixture continued refluxing for another 5 h. The solution was cooled, and the product was filtered, washed, dried, and recrystallized at room temperature in EtOH to collect red block-shaped crystals of MDD. Yield, 48.5%. Found: C, 53.62%; H, 5.38%; N, 7.41%. Calc. for C17H20N2O8: C, 53.68%; H, 5.30%; N, 7.37%. m.p.: 172.6–173.0 °C. FT-IR(KBr) cm–1: 1718, 1678 (C=O), 1456 (C–N), 1275, 1190 (C–O). 1H NMR (400 MHz, CDCl3, δppm): 7.52 (s, 1H), 7.00 (s, 1H), 5.45 (s, 1H), 3.53 (s, 3H), 2.73 (s, 1H), 2.18 (s, 1H), 1.76 (s, 6H), 1.25 (s, 6H). 13C NMR (125 MHz, CDCl3, δppm): 150, 118, 101, 94, 26, 11. The preparation method of DDD was the same as that of MDD except that 5,6-dimethyl-1H-benzo[d] imidazole (0.73 g, 5 mmol) replaced 2-methyl-1H-imidazole (0.41 g, 5 mmol) to get a red powder (DDD). Yield, 28.5%. m.p.: 173.8–174.5 °C. Found: C, 63.58%; H, 5.85%; N, 9.52%. Calc. for C31H34N4O8: C, 63.04%; H, 5.80%; N, 9.49%. FT-IR(KBr) cm–1: 1698, 1633 (C=O), 1449 (C–N), 1272, 1197 (C–O). 1H NMR (400 MHz, CDCl3, δppm): 14.23 (d, 1H), 9.11 (d, 1H), 8.78 (s, 1H), 7.68 (s, 3H), 5.35 (s, 1H), 3.09 (s, 6H), 2.44 (s, 6H), 2.20 (s, 3H), 1.94 (s, 6H), 1.25 (s, 6H). 13C NMR (125 MHz, CDCl3, δppm): 150, 140, 134, 132, 115, 101, 94, 26, 19. Red block-shaped crystals appeared by using solvents (v petroleum ether/v acetone = 1:1).

X-ray Diffraction Analysis of DDD and MDD

The X-ray data of DDD and MDD were collected on a Spider Rapid IP (Rigaku, Japan) detector. The molecular structures of the two compounds were ascertained by SHELXL-2015 and SHELXT-2015.[32,33] The H atoms of the two compounds were placed in calculated positions and refined using the riding coordinates with C–H distances of 0.93–0.97 Å and N–H distances of 0.86 Å. Uiso(H) = 1.2Ueq(C) for aromatic/amide H atoms, and Uiso(H) = 1.5Ueq(C) for methyl H atoms.

Computational Methods

DFT calculations of DDD and MDD were performed with the Gaussian 09[34] package using a hybrid functional, namely, B3LYP or PBEPBE at the basis set 6-311G(d,p).[35,36] TD-DFT[37,38] calculations were used to predict the electronic spectra of the two compounds. The calculated vibrational frequencies and electronic spectra were obtained at the B3LYP/6-311G(d,p) level and the PBEPBE/6-311G(d,p) level.

Results and Discussion

Crystal Structures of the Two Salt Cocrystals

The key parameters of the two salts are summarized in Table . Their molecular structures with hydrogen atoms are shown in Figure .
Table 1

Crystal Structure Details for MDD and MDDa

 compound
 DDDMDD
formulaC31H34N4O8C17H20N2O8
CCDC18179412014484
color/shapered/blockred/block
Mr590.62380.35
crystal system, space groupmonoclinic, P21/ctriclinic, P-1
a, b, c (Å)13.2873(6), 16.9107(6), 14.3356(6)9.936(2), 10.556(2), 10.880(2)
α, β, γ (°)90, 103.2430(10), 90113.33(3) 100.27(3), 112.39(3)
crystal size (mm)0.1 × 0.08 × 0.040.25 × 0.18 × 0.10
wavelength (Å)0.710730.71073
θ ranges (°)3.06–27.4843.476–27.47
V3)3135.5(2)893.0(3)
Z42
F(000)1248400
D (g·cm–3)1.2511.415
hh/–kk/–ll–17, 17/–20, 21/–18, 18–12, 12/–13, 13/–14, 13
total, unique, and [I > 2σ(I)] reflections30,494, 7196, 29558248, 3960, 3295
no. of reflections, restraints, parameters7196, 0, 3963960, 0, 244
R(int)0.04620.0393
R, wR, S0.0541, 0.1311, 0.8900.0539, 0.1383, 1.108
(Δρ)max, (Δρ)min (e/Å3)0.290, −0.1940.386, −0.356

w = [σ2(Fo2) + (0.0902P)2]−1, where P = (Fo2 + 2Fc2)/3 for DDD; w = [σ2(Fo2) + (0.0821P)2 + 0.1051P]−1, where P = (Fo2 + 2Fc2)/3 for MDD.

Figure 1

ORTEP drawings of DDD and MDD with 30% probability thermal ellipsoids.

ORTEP drawings of DDD and MDD with 30% probability thermal ellipsoids. w = [σ2(Fo2) + (0.0902P)2]−1, where P = (Fo2 + 2Fc2)/3 for DDD; w = [σ2(Fo2) + (0.0821P)2 + 0.1051P]−1, where P = (Fo2 + 2Fc2)/3 for MDD. As shown in Figure , the molecular structure of DDD includes one (C13H13O8)− anion, one (C9H11N2)+ cation, and one 5,6-dimethyl-1H-benzo[d]imidazole molecule. However, MDD consists of one (C13H13O8)− and one (C4H7N2)+. The central C(7) atom is bridged by two Meldrum’s acid moieties, which forms the (C13H13O8)− anion in the two compounds. As shown in Table , bond lengths C7–C8 (1.384 (3) Å) and C7–C3 (1.374 (3) Å) (DDD) and C6–C7 (1.380 (2) Å) and C7–C8 (1.398 (2) Å) (MDD) are both larger than the C=C double bond and shorter than the C–C single bond, which form a conjugated system. Their bond angles (C3–C7=C8 (128.81 (19)°) (DDD) and C6–C7=C8 (130.91 (13)°) (MDD)) also both resemble that of our earlier report (131.19 (1)°).[31] The two 1,3-dioxane rings of the (C13H13O8)− anion in the two compounds are both in a distorted envelope conformation, with their puckering parameters as follows: for ring 1 (O1, O2, C1–C4) in DDD: Q = 0.4616 (2) Å, Q (2) = 0.4360 (2) Å, Q (3) = 0.1518 (2) Å, ϑ = 109.2 (2)°, φ = 243.4 (2)°; ring 2 (O7, O8, C8–C11) in DDD: Q = 0.4726 (2) Å, Q (2) = 0.4501 (2) Å, Q (3) = 0.1440 Å, ϑ = 72.26 (2)°, φ = 299.9 (2)°; ring 3 (O3, O4, C8–C11) in MDD: Q = 0.4372 Å, Q (2) = 0.4073 (2) Å, Q (3) = 0.1589 (2) Å, ϑ = 111.31 (3)°, φ = 118.5595 (2)°; ring 4 (O5, O6, C3–C6) in MDD: Q = 0.4728 (2) Å, Q (2) = 0.4529 (2) Å, Q (3) = 0.1357 (2) Å, ϑ = 106.68 (2)°, φ = 243.4468 (2)°.
Table 2

Main Bond Lengths (Å) and Bond Angles (°) by X-ray and DFT Calculations for DDD and MDD

DDD
MDD
 Å
 Å
bondexp.calc.bondexp.calc.
C7–C81.384(3)1.405C7–C81.398(2)1.399
C3–C71.374(3)1.385C6–C71.380(2)1.383
O5–C91.214(3)1.204O7–C41.2096 (19)1.202
O6–C111.222(3)1.237O8–C51.2211 (17)1.223
O8–C111.350(3)1.367O6–C51.3559(19)1.361
O8–C101.425(4)1.446O6–C31.4450(17)1.448
O7–C91.367(3)1.391O5–C41.3634(2)1.384
O7–C101.432(3)1.418O5–C31.433(2)1.422
N (1)–C (14)1.339(3)1.324N1–C141.374(3)1.381
N (1)–C (15)1.377(3)1.389N1–C161.330(2)1.332
In the crystal lattice of DDD, one kind of N–H···O intermolecular interaction and two kinds of N–H···O and N–H···N intramolecular interactions can be seen in Table . The two Meldrum’s acid moieties of the (C13H13O8)− anion are connected with the (C9H11N2)+ cation and the C9H10N2 molecule by N–H···O molecular interactions, and the distances of N4···O4 and N1···O6 are 2.754 (2) and 2.743 (3) Å, respectively. However, the (C9H11N2)+ cation and C9H10N2 molecule are linked by N–H···N intramolecular interactions, and the distances of N3···N2 are 2.685 (2) Å. The bond angle of N3–H3···N2 is 174.2°. The 1D-chained structure of DDD was connected by N–H···O intermolecular interactions (Figure ). The 1D chain further constitutes the 3D-net structure (Figure ).
Table 3

Intra- and Intermolecular Interactions and π···π Stacking Interactions of DDD and MDDa

D–H···AsymmetryD···A (Å)∠D–H···A (°)
MDD   
N1–H1···O21 x, y, 1  z2.723(5)167
N2–H2···O71 x, −y, z2.953 (6)115
N2–H2···O82 +x, y, –1 + z2.833 (6)157
Cg3···Cg3x, y, z4.678(9) 
DDD   
N4–H4···O41 – x + 2, y + 1/2, –z + 3/22.754(2)157.6
N1–H1···O6intra2.743(3)171.3
N3–H3···N2intra2.685(2)174.2

C3 ring denotes ring N1, N2, and C14–C16.

Figure 2

1D chain of DDD and MDD.

Figure 3

Packing diagrams of DDD and MDD with 30% probability thermal ellipsoids.

1D chain of DDD and MDD. Packing diagrams of DDD and MDD with 30% probability thermal ellipsoids. C3 ring denotes ring N1, N2, and C14–C16. In the crystal lattice of MDD, there are three kinds of weak N–H···O intermolecular interactions and one kind of π···π stack interaction (Table ). As shown in Figure , 2-methyl-1H-imidazol-3-ium links 5-((2,2-dimethyl-4,6-dioxo-1,3-dioxan-5-ylidene) methyl)-2,2-dimethyl-4,6-dioxo-1,3-dioxin-5-ide by N–H···O molecular interactions, and the distances of N (1)···O (2), N (2)···O (8), and N (2)···O (7) are 2.723 (5), 2.833 (6), and 2.953 (6) Å, respectively. The distances of π···π stack interactions are 4.678 (9) Å. The 1D-chained structure of MDD was bridged by N–H···O intermolecular interactions (Figure ). The 3D-net network structure of MDD was also formed by the above 1D chain (Figure ).

Optimization of Molecular Geometry for MDD and DDD

The optimized geometric structures of the two compounds are carried out using DFT at the B3LYP/6-311G(d,p) level, and the values are also listed in Table . As shown in Table , most of the predicted bond lengths and angles are slightly larger than the ones measured in the experiments. It is likely because the experimental parameters of the two compounds are described in the solid state; however, the predicted values are obtained in the gas phase. Comparing the predicted values with the experimental ones, it can be found that the maximum differences in bond lengths and bond angles are 0.025 Å and 3.60° (DDD) and 0.011 Å and 1.97° (MDD), respectively, indicating that the predicted results are satisfactory and the B3LYP/6-311G(d,p) level is suitable to simulate the two crystal structures.

Thermodynamic Properties

Three main thermodynamic properties (capacity (C0), entropy (S0), and enthalpy (H0)) of MDD and DDD are listed in Table . As shown in Table , all the values of thermodynamic parameters increase with the temperature rising from 100.0 to 1000.0 K,[39] which is mainly due to the enhancement of the two molecular vibrations when the temperature rises.
Table 4

Thermodynamic Parameters of MDD and DDD

 C0p,m (J/(mol K))H0m (kJ/mol)S0m (J/(mol K))
T (K)MDDDDDMDDDDDMDDDDD
100.0186.78286.2511.0817.16438.20609.60
200.0308.42482.9335.9755.80605.89869.59
298.1422.22669.0571.84112.34750.321097.15
300.0424.33672.5272.63113.58752.941101.29
400.0532.50852.01120.57189.96890.131319.80
500.0624.931006.90178.59283.141019.201527.07
600.0700.641134.50244.99390.421140.061722.31
700.0762.341238.87318.24509.261252.851905.29
800.0813.141324.96397.09637.591358.072076.52
900.0855.461396.75480.58773.771456.362236.85
1000.0891.081457.19567.96916.551548.382387.22
The correlation equations of C0, S0, H0, and temperature T are as follows: MDD: DDD:

Electronic Analysis

The experimentally obtained absorption spectra of the two compounds in EtOH and the calculated spectra in the gas state using the TD-DFT method at the PBEPBE/6-311G(d,p) level are shown in Figure .
Figure 4

Experimental and calculated UV–Vis spectra of DDD and MDD.

Experimental and calculated UV–Vis spectra of DDD and MDD. The two compounds both present two absorption bands at 245 and 379 nm (DDD) and at 241 and 377 nm (MDD): the first absorption band is owing to the π → π* transition of the (C9H11N2)+ cation or (C4H7N2)+ cation and the second band is due to the n → π* transition of the (C13H13O8)− anion. The results resemble those of the literature reported (243 and 384).[31] The calculated spectra of the two compounds were also found to exhibit two bands at 268 and 352 nm (DDD) and at 265 and 342 nm (MDD), which illustrates that the PBEPBE/6-311G(d,p) method can simulate the experimental electronic spectra. The charge densities of four frontier molecular orbitals of the two compounds are listed in Figure . The HOMO-1 and HOMO electrons are mostly localized on both the 1,3-dioxane ring and C6–C7=C8 bonds of the (C13H13O8)− anion in the two compounds; however, the LUMO and LUMO+1 electrons are localized on the benzo[d]imidazole ring (DDD) and imidazole ring and C6–C7=C8 bonds (MDD), which are in accord with the π → π* and n → π* transitions of the experimental values. Furthermore, EHOMO and ELUMO of the two compounds are −0.160 and −0.086 eV for DDD and −0.170 and −0.076 eV for MDD at the PBEPBE/6-311G(d,p) levels, respectively. The energy HOMO–LUMO gap of 0.074 eV (DDD) is slightly smaller than that of 0.094 eV (MDD), which implies that the molecular structure of MDD is more stable.
Figure 5

Charge densities of four frontier molecular orbitals for DDD and MDD.

Charge densities of four frontier molecular orbitals for DDD and MDD.

Fluorescence Spectra

Figure shows the emission and excitation spectra of the two salts and the CIE color chromaticity in EtOH solution. DDD’s emission band appears at 570 nm when the excitation peak is 310 nm, while the compound MDD shows strong emission intensity at 454 nm when the excitation peak is 316 nm. The emission band is related to the phenyl ring structure and the substituents. The emission band of DDD is 116 nm redshifted from the emission band of MDD, which is due to more phenyl rings and methyl groups. In addition, the yellowish-green region of DDD and the purplish-blue region of MDD are decided and their color coordinates (0.3075, 0.6035) and (0.2026, 0.1693) are calculated by means of CIE1931. The relation of emission spectra and the structures of DDD and MDD can provide a new idea for the design of potential fluorescent materials.
Figure 6

(a) PL spectra of DDD and MDD in EtOH solution; (b) CIE chromaticity in EtOH solution.

(a) PL spectra of DDD and MDD in EtOH solution; (b) CIE chromaticity in EtOH solution.

Conclusions

Two new salt cocrystals, C31H34N4O8 (DDD) and C17H20N2O8 (MDD), were synthesized and characterized by elemental analysis, infrared, UV–Vis, and NMR (1H and 13C) spectroscopy and single-crystal X-ray diffraction. Their crystal structures show that DDD belongs to the monoclinic, P21/c space group, and MDD belongs to the triclinic, P-1 space group. In DDD, the (C13H13O8)− anion, (C9H11N2)+ cation, and C9H10N2 molecule were linked by N–H···O and N–H···N molecular interactions. However, in MDD, the (C13H13O8)− anion and (C4H7N2)+ cation were bridged by N–H···O intermolecular interactions. The optimized geometric structure using DFT at the B3LYP/6-311G(d,p) level is suitable to simulate the molecular structures of DDD and MDD. The calculated results of the two compounds with the TD-DFT method at the PBEPBE/6-311G(d,p) level are in accordance with experimental values.
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