Literature DB >> 21754545

1,4-Bis(5-methyl-1H-1,2,4-triazol-3-yl)benzene tetra-hydrate.

Ai-Xin Zhu, Xiu-Li Chen, Zhen Li, Yuan-Chao Du, Hong-Can Wang.   

Abstract

In the title compound, C(12)H(12)N(6)·4H(2)O, the two triazole rings adopt a cis configuration with a crystallographic twofold axis passing through the central benzene group. The benzene and triazole rings are almost coplanar with a dihedral angle of 5.5 (1)°. In the crystal, water mol-ecules are joined together by OW-H⋯OW hydrogen bonds to form a one-dimensional zigzag chain. These water chains are further connected to the organic mol-ecule, forming a three-dimensional network by inter-molecular OW-H⋯N and N-H⋯OW hydrogen bonds. Moreover, π-π stacking inter-actions between triazole rings [centroid-centroid distances = 3.667 (1)-3.731 (1) Å] are observed. One of the water mol-ecules shows one of the H atoms to be disordered over two positions.

Entities:  

Year:  2011        PMID: 21754545      PMCID: PMC3089122          DOI: 10.1107/S1600536811015133

Source DB:  PubMed          Journal:  Acta Crystallogr Sect E Struct Rep Online        ISSN: 1600-5368


Related literature

For applications of 1,2,4-triazole and its derivatives in coordination chemistry, see: Zhang et al. (2005 ▶); Ouellette et al. (2006 ▶); Zhu et al. (2009 ▶). For the structures of ruthenium complexes with pyridine-2-yl-1,2,4-triazole-based ligands, see: Passaniti et al. (2002 ▶). For the previous synthesis of the title compound, see: Bahçeci et al. (2005 ▶).

Experimental

Crystal data

C12H12N6·4H2O M = 312.34 Monoclinic, a = 12.7343 (19) Å b = 13.937 (2) Å c = 9.0648 (14) Å β = 100.893 (3)° V = 1579.8 (4) Å3 Z = 4 Mo Kα radiation μ = 0.10 mm−1 T = 293 K 0.35 × 0.28 × 0.08 mm

Data collection

Bruker APEX CCD diffractometer Absorption correction: multi-scan (SADABS; Sheldrick, 1996 ▶) T min = 0.966, T max = 0.992 4670 measured reflections 1542 independent reflections 1286 reflections with I > 2σ(I) R int = 0.021

Refinement

R[F 2 > 2σ(F 2)] = 0.052 wR(F 2) = 0.148 S = 1.04 1542 reflections 102 parameters H-atom parameters constrained Δρmax = 0.27 e Å−3 Δρmin = −0.25 e Å−3 Data collection: SMART (Bruker, 2004 ▶); cell refinement: SAINT (Bruker, 2004 ▶); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: DIAMOND (Brandenburg, 1999 ▶); software used to prepare material for publication: SHELXTL (Sheldrick, 2008 ▶). Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536811015133/im2280sup1.cif Supplementary material file. DOI: 10.1107/S1600536811015133/im2280Isup2.cdx Structure factors: contains datablocks I. DOI: 10.1107/S1600536811015133/im2280Isup3.hkl Supplementary material file. DOI: 10.1107/S1600536811015133/im2280Isup4.cml Additional supplementary materials: crystallographic information; 3D view; checkCIF report
C12H12N6·4H2OZ = 4
Mr = 312.34F(000) = 664
Monoclinic, C2/cDx = 1.313 Mg m3
Hall symbol: -C 2ycMo Kα radiation, λ = 0.71073 Å
a = 12.7343 (19) ŵ = 0.10 mm1
b = 13.937 (2) ÅT = 293 K
c = 9.0648 (14) ÅPlate, yellow
β = 100.893 (3)°0.35 × 0.28 × 0.08 mm
V = 1579.8 (4) Å3
Bruker APEX CCD diffractometer1542 independent reflections
Radiation source: fine-focus sealed tube1286 reflections with I > 2σ(I)
graphiteRint = 0.021
ω scansθmax = 26.0°, θmin = 2.2°
Absorption correction: multi-scan (SADABS; Sheldrick, 1996)h = −15→15
Tmin = 0.966, Tmax = 0.992k = −15→17
4670 measured reflectionsl = −11→11
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.052Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.148H-atom parameters constrained
S = 1.04w = 1/[σ2(Fo2) + (0.0816P)2 + 0.7602P] where P = (Fo2 + 2Fc2)/3
1542 reflections(Δ/σ)max < 0.001
102 parametersΔρmax = 0.27 e Å3
0 restraintsΔρmin = −0.25 e Å3
Geometry. All e.s.d.'s (except the e.s.d. in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell e.s.d.'s are taken into account individually in the estimation of e.s.d.'s in distances, angles and torsion angles; correlations between e.s.d.'s in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell e.s.d.'s is used for estimating e.s.d.'s involving l.s. planes.
Refinement. Refinement of F2 against ALL reflections. The weighted R-factor wR and goodness of fit S are based on F2, conventional R-factors R are based on F, with F set to zero for negative F2. The threshold expression of F2 > σ(F2) is used only for calculating R-factors(gt) etc. and is not relevant to the choice of reflections for refinement. R-factors based on F2 are statistically about twice as large as those based on F, and R- factors based on ALL data will be even larger. One hydrogen atom from O2W is disordered over two positions in a 0.52 (3):0.48 (3) ratio, which is freely refined with command 'PART'.
xyzUiso*/UeqOcc. (<1)
N10.66106 (13)0.34969 (11)−0.19565 (17)0.0531 (5)
H1D0.68740.3847−0.25780.064*
N20.62354 (14)0.38395 (11)−0.07499 (17)0.0522 (5)
N30.60877 (12)0.22386 (10)−0.09140 (16)0.0454 (4)
C10.68428 (18)0.19667 (15)−0.3248 (2)0.0590 (6)
H1A0.72920.1449−0.28050.088*
H1B0.72300.2361−0.38300.088*
H1C0.62180.1711−0.38870.088*
C20.65166 (14)0.25529 (13)−0.20444 (18)0.0448 (4)
C30.59264 (14)0.30486 (12)−0.01538 (19)0.0425 (4)
C40.54472 (14)0.30544 (12)0.12072 (19)0.0421 (4)
C50.52248 (17)0.22014 (13)0.1863 (2)0.0510 (5)
H5A0.53790.16220.14430.061*
C60.52170 (16)0.39108 (13)0.1860 (2)0.0510 (5)
H6A0.53580.44910.14290.061*
O1W0.73472 (14)0.45314 (11)−0.41166 (19)0.0757 (5)
H1WA0.69690.4969−0.46090.091*
H1WB0.80010.4691−0.40170.091*
O2W0.44076 (12)−0.02791 (9)0.10493 (16)0.0602 (4)
H2WA0.4240−0.08680.09280.072*
H2WB0.4790−0.00060.05000.072*0.52 (3)
H2WC0.4784−0.02770.19300.072*0.48 (3)
U11U22U33U12U13U23
N10.0657 (11)0.0516 (10)0.0484 (8)−0.0032 (8)0.0274 (8)0.0074 (7)
N20.0662 (11)0.0437 (9)0.0523 (9)−0.0025 (7)0.0257 (8)0.0035 (7)
N30.0540 (9)0.0428 (8)0.0425 (8)−0.0035 (7)0.0166 (7)−0.0015 (6)
C10.0649 (13)0.0672 (13)0.0495 (10)−0.0045 (10)0.0232 (9)−0.0060 (9)
C20.0467 (10)0.0488 (10)0.0401 (9)−0.0022 (8)0.0115 (7)0.0016 (7)
C30.0452 (10)0.0437 (9)0.0397 (9)−0.0003 (7)0.0108 (7)0.0012 (7)
C40.0448 (10)0.0431 (10)0.0396 (9)−0.0001 (7)0.0109 (7)0.0010 (7)
C50.0774 (14)0.0368 (9)0.0429 (9)0.0004 (9)0.0218 (9)−0.0027 (7)
C60.0603 (12)0.0380 (10)0.0604 (11)−0.0004 (8)0.0260 (9)0.0049 (8)
O1W0.0804 (11)0.0679 (10)0.0871 (11)0.0058 (8)0.0373 (9)0.0277 (8)
O2W0.0809 (11)0.0447 (7)0.0611 (9)−0.0064 (7)0.0289 (8)−0.0014 (6)
N1—C21.322 (3)C4—C51.382 (2)
N1—N21.360 (2)C4—C61.388 (2)
N1—H1D0.8600C5—C5i1.383 (4)
N2—C31.320 (2)C5—H5A0.9300
N3—C21.324 (2)C6—C6i1.376 (4)
N3—C31.358 (2)C6—H6A0.9300
C1—C21.484 (3)O1W—H1WA0.8500
C1—H1A0.9600O1W—H1WB0.8500
C1—H1B0.9600O2W—H2WA0.8500
C1—H1C0.9600O2W—H2WB0.8501
C3—C41.476 (2)O2W—H2WC0.8499
C2—N1—N2110.87 (14)N2—C3—C4122.67 (15)
C2—N1—H1D124.6N3—C3—C4123.69 (15)
N2—N1—H1D124.6C5—C4—C6118.63 (17)
C3—N2—N1102.31 (15)C5—C4—C3120.35 (15)
C2—N3—C3104.00 (15)C6—C4—C3121.01 (15)
C2—C1—H1A109.5C4—C5—C5i120.67 (10)
C2—C1—H1B109.5C4—C5—H5A119.7
H1A—C1—H1B109.5C5i—C5—H5A119.7
C2—C1—H1C109.5C6i—C6—C4120.69 (10)
H1A—C1—H1C109.5C6i—C6—H6A119.7
H1B—C1—H1C109.5C4—C6—H6A119.7
N1—C2—N3109.18 (15)H1WA—O1W—H1WB108.3
N1—C2—C1123.88 (16)H2WA—O2W—H2WB121.0
N3—C2—C1126.93 (17)H2WA—O2W—H2WC102.0
N2—C3—N3113.64 (16)H2WB—O2W—H2WC105.4
D—H···AD—HH···AD···AD—H···A
N1—H1D···O1W0.861.882.736 (2)173.
O1W—H1WA···N2ii0.852.082.926 (2)172.
O1W—H1WB···O2Wiii0.851.962.801 (2)170.
O2W—H2WA···N3iv0.851.952.800 (2)173.
O2W—H2WB···O2Wiv0.851.932.754 (3)164.
O2W—H2WC···O2Wi0.851.922.774 (3)178.
Table 1

Hydrogen-bond geometry (Å, °)

D—H⋯AD—HH⋯ADAD—H⋯A
N1—H1D⋯O1W0.861.882.736 (2)173
O1W—H1WA⋯N2i0.852.082.926 (2)172
O1W—H1WB⋯O2Wii0.851.962.801 (2)170
O2W—H2WA⋯N3iii0.851.952.800 (2)173
O2W—H2WB⋯O2Wiii0.851.932.754 (3)164
O2W—H2WC⋯O2Wiv0.851.922.774 (3)178

Symmetry codes: (i) ; (ii) ; (iii) ; (iv) .

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