999精品在线视频,手机成人午夜在线视频,久久不卡国产精品无码,中日无码在线观看,成人av手机在线观看,日韩精品亚洲一区中文字幕,亚洲av无码人妻,四虎国产在线观看 ?

Synthesis, Crystal Structure, Spectroscopy and Hirshfeld Analysis of 4,6-Diamino-2-cyclopropylaminopyrimidine-5-carbonitrile with Different Solvents: N,N-dimethylformamide, Methanol and Water①

2022-04-16 03:06:44GEShuWangSUNBaiWang
結構化學 2022年3期

GE Shu-Wang SUN Bai-Wang

(School of Chemistry and Chemical Engineering, Southeast University, Nanjing 210096, China)

ABSTRACT Three new solvates of 4,6-diamino-2-cyclopropylamino-5-pyrimidine carbonitrile (DCL): crystal 1 (DCL with N,N-dimethylformamide (DMF)), crystal 2 (DCL with methanol) and crystal 3 (DCL with water)were synthesized and characterized by single-crystal X-ray diffraction, thermal behaviour, Hirshfeld surface and powder X-ray powder diffraction (PXRD). 1H and 13C NMR spectra confirm solvent molecules existing in the crystal lattice. Crystal 1 forms a 1:1 DCL:DMF crystal; crystal 2 gives a 1:0.5 DCL:methanol crystal and crystal 3 gets a 1:1.5 DCL:H2O crystal. The three crystals are all primarily stabilized by a strong N-H???N hydrogen bonding interaction between DCL and the solvents. The structures are stabilized by H???H, N-H???O, N-H???N and O-H???O intermolecular interactions. When crystal 2 is dried at 150 °C, the new polymorph with no solvate is obtained.

Keywords: dicyclanil, crystal, spectroscopy, Hirshfeld surfaces; DOI: 10.14102/j.cnki.0254-5861.2011-3359

1 INTRODUCTION

So far, the solvate of active pharmaceutical ingredients is a hot topic and it achieves remarkable development in “crystal engineering”[1-6]. Polymorphism and hydrate formation are especially powerful means to alternate crystal forms of drugs[7]. If the crystals of pharmaceuticals are engineered,the properties like bioavailability, stability, and processibility could be optimized[8,9].

Dicyclanil (DCL)[10,11]is one of the most important growth regulators for insect of the newer generation. DCL can kill dipster and flea and prevent fly, mosquito becoming pupa or imago. Especially, it can prevent animal from the disoperation of mosquito and Aedes aegypti. DCL’s toxicity is very low, and therefore its safety is better.

However, we can complicate the manufacturing process of solid DCL due to its ability to afford polymorphs, hydrates and other solvates. It is very important for pharmaceutical industry to determine the optimal and controlled conditions to obtain the solid with known properties[12].

Up to now, eight polymorphic unsolvated crystals, A, B, C,D, E, F, G and H, have been patented[13,14]. The most stable polymorph D crystallizes from octanol, and there is still no report about solvate. The crystal structures of three solvates of DCL:N,N-dimethylformamide (DMF) (1:1), DCL: methanol (2:1) and DCL:H2O (1:1) are present in this paper.These crystals were characterized by TGA, DSC, IR, and single-crystal diffraction. Furthermore, molecular Hirshfeld surfaces of DCL in crystals were performed. The N-H???N hydrogen bond between DCL and solvents plays a key role.

2 EXPERIMENTAL

2. 1 Materials and methods

Methanol, DMF was commercially available from J&K SCIENTIFIC LTD, and DCL provided by Changzhou Yabang Pharmaceutical & Chemical Co., LTD. All of the reagent grade solvents from Sinopharm Chemical Reagent Co., Ltd were used directly without further purification. Infrared spectra were recorded on a SHIMADZU IR prestige-21 FTIR-8400S spectrometer from 4000 to 400 cm-1with the samples in potassium bromide pellets. DSC and TGA measurements were carried out by a Mettler-Toledo TGA/DSC STAReSystem at the 10 K·min-1heating rate under a dry N2atmosphere flowing at 20 cm3·min-1over a range of 40~400 °C. We analysized the TGA/DSC data with STAReSoftware. NMR spectra were recorded on a Varian FT-400 MHz instrument. Also, by taking a solvent peak as reference,we recorded the chemical shifts in parts per million (ppm) on the scale.

2. 2 Preparation of the crystals (1~3)

Crystal 1: DCL (400 mg) was stirred in DMF (30 mL),which was stirred for about 30 minutes before evaporating at 25 ℃. Colorless needle-like crystals of crystal 1 were separated from the liquor a few days later.

Crystal 2: DCL (300 mg) was suspended in 30 mL of methanol/water (95:5). After heating to 64 °C and stirring for about 35 mintures before evaporation at 25 ℃, colorless crystals 2 in plate form were separated several days later.

Crystal 3: DCL (1 g) was stirred in DMF (50 mL) for approximately half an hour. The distilled water (50 mL) was added in the solution. After slowly evaporating the solvent at 25 ℃, colorless block-like crystals of crystal 3 were separated from the liquor after one month.

2. 3 X-ray crystallographic study

The single crystal X-ray diffraction data of crystals 1, 2 and 3 were obtained at 293 K by using the Rigaku SCXmini diffractometer with anω-scan mode using a graphitemonochromated MoKαradiation (λ= 0.071073 nm)[15]. We integeated the lattice parameters using vector analysis and refined them from the diffraction matrix. The absorption correction was finished based on the Bruker SADABS program with multi-scan method. Crystal data and refinements for these three crystals are listed in Table 1. The structure solution and refinement were respectively performed with SHELXS-97 and SHELXL-97[16]. All the nonhydrogen atoms were anisotropically refined, while the hydrogen ones were inserted in calculated positions and fixed during the least-squares[17]. The molecular graphics were drawn with mercury[18]and diamond program[19].

Table 1. Crystal and Experiment Data for Crystals 1~3

2. 4 X-ray powder diffraction

X-ray powder diffraction measurements of crystals 1~3 and DCL were recorded on a D8 ADVANCE XRD (Bruker,Germany) with CuKαradiation (λ= 1.54056 ?) at 40 mA and 45 kV. Into a glass holder the sample was packed to collect the diffraction patterns over a 5~45° 2θrange at the scan rate of 3 °·min-1.

2. 5 Hirshfeld surface calculations

We performed Molecular Hirshfeld surface calculations by using the CrystalExplorer program[20], and the principles have been reported in literature[21-25]. When reading cif files of crystals 1~3 into the CrystalExplorer program for analysis,all the hydrogen bond lengths were modified automatically to typical neutron-derived values (N-H = 1.009, C-H =1.083 ?). Displayed by using the standard 0.6~2.6 ? withdeanddidistance scales, the 2-D fingerprint plots are shown on the graph axes.

Table 2. Hydrogen Bonds in Crystals 1, 2 and 3

3 RESULTS AND DISCUSSION

3. 1 Crystal structures of crystals 1~3

DCL forms a 1:1 solvate with DMF (crystal 1) and crystallizes in space groupP21/nwithZ= 4. The DCL molecules in crystal 1 are self-assembled through various kinds of weak interactions. The important interactions are as follows:N(5)-H(5A)???N(2) (dD???A(?)= 2.993 ?, ∠D-H???A = 170°),N(5)-H5B???O(1) (dD???A(?)= 2.929 ?, ∠D-H???A = 136°), and N(4)-H(4B)???N(6) (dD???A(?)= 3.011 ?, ∠D-H???A = 164°)(Fig. 1a). The hydrogen bonds of crystals 1~3 are all given in Table 2. The oxygen atom (O1) of DMF participates in hydrogen bonding with N(5)-H from a neighbor molecule,getting a hydrogen-bonded dimeric motif of DCL molecules with DMF molecules. Scuh dimeric motifs connecte with each other through N-H???N hydrogen bonds to get hydrogenbonded sheets along plane (100) (Fig. 1b). Besiedes strong hydrogen bonds, weak interactions like C-H???πalso make contribution to the stability of the crystal. One C-H bond of the methyl groups of DMF is involved in C-H???π(dD??A(?)=3.780 ?) interaction (Fig. 1c) which is much weaker compared to the related hydrogen bonds. The distance of two sixmembered rings of DCL with a neighboring DCL molecule is 7.574 ? (Fig. 1d), so no significantπ???πintermolecular interaction appears. The N-H???N and N-H???O interactions contribute the most in crystal 1.

Fig. 1. (a) Hydrogen-bonded dimers, (b) Packing of the molecules of crystal 1 viewed along the (100) plane,(c) C-H···π interactions and (d) π···π interactions

Crystal 2 forms a 2:1 (DCL:methanol) crystal in space groupP1withZ= 2. Different from crystal 1, the DCL molecules self-assemble into dimers only by N(12)-H(12A)???N(3)interactions (dD???A(?)= 2.988 ?, ∠D-H???A = 172°) and the methanol molecules form self-assembled dimers through O(1)-H(1)???O(1) interactions (dD???A(?)= 2.995 ?, ∠DH???A = 140°) (Fig. 2a). Similarity appears in the packing of DCL molecules in crystal 2 with 1. Also, C-H???πinteractions help stabilize the lattice. One C-H bond of the methyl groups of the methanol molecule is involved in C-H???π(dD???A(?)= 3.551 ?) interaction (Fig. 2b). But the strength ofπ???πinteraction exists in crystal 2. The distances of two sixmembered rings of DCL with a neighboring DCL molecule are 3.675 or 3.850 ? (Fig. 2c). The guest methanol molecules are embedded through O-H???O interactions in cavities caused by the assembly of DCL molecules along thea-axis (Fig. 2d).

Although the crystal data of 2 are obtained, it is still hard to confirm the existence of water or methanol molecule in the crystal lattice. More work and efforts were required to answer this question. Solid-state 13C spectrum can be used to identify whether the crystal is hydrate or non-hydrate, which can be characterized by 13C peak of the solvent in lattice of crystal 2 (Fig. 3). The chemical shift (161.3 ppm) observed suggests the existence of methanol in 2. It is also verified by1H NMR spectra that the hydrogen of CH3OH corresponds to the chemical shifts 3.3 and 2.8 ppm (3:1) in Fig. 4.

Fig. 2. (a) Hydrogen-bonded dimers, (b) C-H…π interactions and (c) π…π interactions,(d) Packing of crystal 2 viewed along the a-axis

Fig. 3. 13C NMR spectra of crystal 1 and the solvate is DMSO

Fig. 4. 1H NMR spectra of crystal 1 and the solvate is DMSO

Crystal 3 is ofC2/cspace group, and an asymmetric unit contains 3 water molecules and 2 DCL molecules. This structure is not an exception to 2 according to the dimers formed by N(5)-H(5B)???O(W1) (dD???A(?)= 2.939 ?, ∠DH???A = 156°), O(W2)-H(W2A)???N(3) (dD???A(?)= 2.828 ?,∠D-H???A = 155°), O(W1)-H(W1A)???N(9) (dD??A(?)= 2.821 ?,∠D-H???A = 164°), and N(11)-H(11B)??? O(W2) (dD???A(?)=2.941 ?, ∠D-H???A = 146°) interactions. Howerer, the dimeric assemblies here are connected one another by bridging water molecules (Fig. 5a). The oxygen atom O(W3)-H of H2O participates in intermolecular hydrogen bonding with O(W2) or O(W1) of a neighboring molecule.One N-H bond of amino group of DCL molecule takes part in N-H???π(dD???A(?)= 3.722 or 3.734 ?) interactions (Fig. 5b).Theπ???πinteration (dD???A(?)= 3.486 ?) (Fig. 5c) is stronger than that in crystals 1 and 2. The water assisted assembly in crystal 3 makes a modified host system with a butterfly-like structure (Fig. 5d).

Fig. 5. (a) Hydrogen-bonded dimers, (b) N-H…π interactions and (c) π…π interactions,(d) Packing of the molecules (viewed along the a-axis) of crystal 3

3. 2 Thermogravimetric analysis and dynamic scanning calorimetry crystals 1~3 and DCL (4)

Thermal behaviors of crystals 1, 2 and 3 together with their raw materials (4-DCL) were studied on a STAReSystem (from Mettler-Toledo) at a heating rate of 10 °C per minute in a 50~400 °C range, as shown in Fig. 6. The melting points of 4-DCL, crystals 1, 2 and 3 are found to be 253.2, 254.5, 251.3 and 252.1 °C in turn. No significant differences are observed among the samples tested at the meting points. This indicates that the heating process does not result in the formation of primary forms, which is confirmed by the XRPD measurement. But the solvents lose at different temperature ranges: 80~120, 60~100 and 50~100 °C with the mass loss of about 28.4%, 8.9% and 12.6%(w/w) for crystals 1~3, respectively. In fact, the theoretical contents of solvents for 1~3 should be 27.8%, 8.4% and 12.4% (w/w) for DMF, methanol and water correspondingly.The results indicate that the theoretical data are in good agreement with the experimental ones.

Fig. 6-1. TGA profiles of 1~3 and 4-DCL

Fig. 6-2. DSC profiles of crystals 1~3 and4-DCL

3. 3 IR of crystals 1~3 and DCL (4)

IR spectra of crystals 4-DCL and crystals 1~3 are shown in Fig. 7 in the 4000~400 cm-1region. The absorption peaks around 3420 and 3160 cm-1can be attributed to the stretching vibration of NH2and NH groups, and those around 2194 cm-1to that of C≡N. The aromatic C=C stretching of DCL molecule occurs at 1570 cm-1. The strong peak at 1460 cm-1is due to the C-H deformation. The peaks at 1660 and 1150 cm-1result from the C=O stretching vibration of carboxylic group in crystal 1. The broad peak observed at 3410 cm-1is caused by the presence of OH stretching vibration in crystals 2 and 3. There is no significant differences in the four curves.

Fig. 7. IR spectra of crystals 1~3 and dicyclanil (4-DCL)

3. 4 Powder X-ray diffraction analysis of 1~3 and DCL (4)

The crystals 1~3 and 4-DCL show unique powder X-ray diffraction patterns (Figs. 8 and 9), and such diffraction is remarkably useful for the identification of structural relationships between different solvated crystal forms of DCL. The PXRD patterns of crystals 1~3 and 4-DCL are distinguishable in Fig. 8. The results show that when slovates are different, the positon of peak will change. When crystals 1~3 and 4-DCL were dried at 150 °C for 1 h, the data of PXRD are the same in crystals 1 and 3 (Fig. 9), which is similar to 4-DCL before heating. But in crystal 2, there are no gross structural changes accompanying the desolvation process. This is a new polymorph with no solvate.

Fig. 8. XPRD of crystals 1~3 and dicyclanil (4-DCL)

Fig. 9. XPRD of crystals 1~3 and dicyclanil(4-DCL) after heating to 150 °C

3. 5 Hirshfeld surface analysis of crystals 1~3

The 2D fingerprint plots and 3D Hirshfeld surfaces, unique for all crystal structures and polymorph, of DCL in 1~3 are depected in Fig. 11, clearly showing similarities and differences of the effections on different coformers on intermolecular interactions of DCL. Two types of dicyclanil molecules in crystals 1 and 3 are identified as 1a, 1b and 3a, 3b. 1a represents the dicyclanil molecule which connects with the near methanol molecule (Fig. 11-1a-b), while 1b is the dicyclanil molecule that connects with the far methanol molecule (Fig. 11-1b-b). 3a shows the dicyclanil molecule connected with two water molecules (Fig. 11-3a-b), while 3b stands for the dicyclanil molecule connecting one water molecule (Fig. 11-3b-b). In crystals 1~3, the main intermolecular interactions around dicyclanil are H???H, O???H,C???H, N???H, C???N and N???N and contacts. For the "butterfly",the widths result from the contributions to the total Hirshfeld surfaces (Table 3). In Table 3, we cannot find C-C contact in crystal 1, which is confirmed by its crystal structure.

Fig. 11-1a-b displays the Hirshfeld surface analysis for DCL in crystal 1. The deep red large circular depressions which are visible on the side of 3D Hirshfeld surfaces correspond to the obvious hydrogen bonding contacts; small red cycles on the surfaces show the C-H???πinteractions,while in the 2D fingerprint plots, blue color points indicate the short contacts of H???H, H???O, and H???N interactions. The H???H interactions reflected in the middle of scattered points(in the 2D fingerprint plot, Fig. 11-1a) occupy 46.7% of total Hirshfeld surfaces. Also, N???H interactions make a relatively remarkable contribution, 31.1%, to the total Hirshfeld surfaces of 1.

The Hirshfeld surface analysis for DCL in crystal 2 (Fig.11-2a-b) is different from Fig. 11-1a-b and Fig.11-1b-b. The C???C interactions have significant contribution to the total Hirshfeld surfaces of crystal 2, which comprises 3.6%,differrnt from the O???H hydrogen bonding interactions comprising 0.8%. The other interactions are similar to crystal 1.

The Hirshfeld surface analysis for DCL in crystal 3 is similar to that in crystal 2. The H···H hydrogen bonds still contribute most significantly to the total Hirshfeld surfaces(47.7%), a bit more than the value in 2a-b, and a longer contact follows the N???H interactions (31.2%), a little less than that in 2b-b. Besides, the C???C, C???O, and N???O intermolecular interactions are found and summarized in Table 3.

Fig. 11. 2-D fingerprint plots of DCL (left) and Hirshfeld surface analysis of DCL (right) in crystals 1~3

Table 3. Contacts Contributions to the Hirshfeld Surfaces of DCL in Crystals 1~3

4 CONCLUSION

we have studied in detail the crystal structures, IR, thermal behaviour, Hirshfeld surface and PXRD of three new crystals: 1(Dicyclanil (DCL) with N,N-dimethylformamide (DMF)), 2(DCL with methanol) and 3 (DCL with water).1H and13C NMR spectra can be used to comfirm the slovate of methanol in cryatal 2. The Hirshfeld surface together with fingerprint plot analysis, acting as a novel method to visualize intermolecular interactions, shows that in these three crystals the close contacts of DCL are dominated by H???H, N???H, H???O andπ???πinteractions. Detailed structural investigations of such three crystals suggest that the N-H???N and N-H???O hydrogen bonds between DCL and solvents play essential roles in forming the elementary structure of the crystals. The new polymorph without solvate was obtained by drying the crystal 2 at 150 °C.

主站蜘蛛池模板: 亚洲成aⅴ人片在线影院八| 久久婷婷综合色一区二区| 亚洲精品无码AV电影在线播放| 色综合热无码热国产| 国产精品美女免费视频大全| 久久精品视频亚洲| 国产Av无码精品色午夜| 欧美亚洲激情| 国产精品夜夜嗨视频免费视频| 日本午夜视频在线观看| 无码aaa视频| 97视频在线观看免费视频| 日韩国产黄色网站| 黄色网站在线观看无码| 亚洲色无码专线精品观看| 特级欧美视频aaaaaa| 一级毛片免费的| 亚洲综合香蕉| 99er精品视频| 国产小视频免费| 精品精品国产高清A毛片| 欧美日韩在线观看一区二区三区| 理论片一区| 99在线观看免费视频| www.91在线播放| 曰韩免费无码AV一区二区| 亚洲日韩AV无码精品| 国产成人凹凸视频在线| 国产微拍一区二区三区四区| 亚洲成a∧人片在线观看无码| 亚洲第一精品福利| 一级毛片中文字幕| 女人18毛片久久| 欧美不卡二区| 在线观看亚洲成人| 亚洲成人免费在线| 亚洲国语自产一区第二页| 日韩高清中文字幕| 日韩黄色在线| 午夜成人在线视频| 国产后式a一视频| 免费人成视网站在线不卡| 国产一级特黄aa级特黄裸毛片| 欧美a在线| 日韩精品视频久久| 亚欧成人无码AV在线播放| 午夜福利无码一区二区| 亚洲国产成人麻豆精品| 六月婷婷精品视频在线观看| 亚洲日韩第九十九页| 久久这里只有精品免费| 97久久免费视频| 日本亚洲欧美在线| 在线精品视频成人网| 天堂在线视频精品| 国产黑丝一区| 亚洲美女操| 国产精品九九视频| 中国国产高清免费AV片| 国产精品乱偷免费视频| 天天躁夜夜躁狠狠躁躁88| 欧美成人午夜视频| 国产第一福利影院| 三上悠亚一区二区| 91尤物国产尤物福利在线| 2020国产在线视精品在| 麻豆精品国产自产在线| 成人免费一级片| 亚洲最新在线| 萌白酱国产一区二区| 亚洲欧洲日产国产无码AV| 91小视频在线播放| 亚洲性影院| 伊人久久综在合线亚洲2019| 亚洲精品在线91| 日韩精品高清自在线| 久久一日本道色综合久久| 2019年国产精品自拍不卡| 国产精品女主播| 色有码无码视频| 免费看a毛片| 国产中文一区a级毛片视频|