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The crystal structure of the title compound, [ZnCl2(C6H8N2O2)]n, consists of a zigzag chain in which adjacent ZnCl2 groups are bridged by 1-carboxyl­atomethyl-3-methyl­imidazolium through its two O atoms. The environment around the Zn atom can be described as a cis-ZnO2Cl2 tetrahedron. The formation of the chain is strengthened by π–π stacking inter­actions between adjacent imidazole ring planes (π–π distance = 3.618 Å).

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536807046545/rk2036sup1.cif
Contains datablocks I, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536807046545/rk2036Isup2.hkl
Contains datablock I

CCDC reference: 663651

Key indicators

  • Single-crystal X-ray study
  • T = 296 K
  • Mean [sigma](C-C) = 0.006 Å
  • R factor = 0.033
  • wR factor = 0.068
  • Data-to-parameter ratio = 16.9

checkCIF/PLATON results

No syntax errors found



Alert level C PLAT029_ALERT_3_C _diffrn_measured_fraction_theta_full Low ....... 0.97 PLAT066_ALERT_1_C Predicted and Reported Transmissions Identical . ? PLAT380_ALERT_4_C Check Incorrectly? Oriented X(sp2)-Methyl Moiety C1
Alert level G REFLT03_ALERT_4_G Please check that the estimate of the number of Friedel pairs is correct. If it is not, please give the correct count in the _publ_section_exptl_refinement section of the submitted CIF. From the CIF: _diffrn_reflns_theta_max 27.70 From the CIF: _reflns_number_total 1994 Count of symmetry unique reflns 1200 Completeness (_total/calc) 166.17% TEST3: Check Friedels for noncentro structure Estimate of Friedel pairs measured 794 Fraction of Friedel pairs measured 0.662 Are heavy atom types Z>Si present yes PLAT033_ALERT_2_G Flack Parameter Value Deviates 2 * su from zero. 0.05 PLAT794_ALERT_5_G Check Predicted Bond Valency for Zn1 (2) 2.02
0 ALERT level A = In general: serious problem 0 ALERT level B = Potentially serious problem 3 ALERT level C = Check and explain 3 ALERT level G = General alerts; check 1 ALERT type 1 CIF construction/syntax error, inconsistent or missing data 1 ALERT type 2 Indicator that the structure model may be wrong or deficient 1 ALERT type 3 Indicator that the structure quality may be low 2 ALERT type 4 Improvement, methodology, query or suggestion 1 ALERT type 5 Informative message, check

Comment top

It is known that the research of coordination polymers receives great interest nowadays, because they may afford new materials with useful properties, such as catalytic activity, microporosity and so on (Shi et al., 2004). Recently, we have synthesized and reported cadmium polymer with 1-methyl-3-carboxymethylimidazole (Shi et al., 2007). As an extension of our work in this field, we synthesized the title compound and solved its crystal structure (I).

The asymmetric unit of (I) contains one Zn atom, one 1-methyl-3-carboxymethylimidazole molecule, and two chlorine atoms (Fig. 1). The structure of (I) is a one-dimensional coordination chain in which the adjacent (ZnCl2) groups are bridged by 1-methyl-3-carboxymethylimidazole through its two O atoms with the distance of 4.8362 (4)Å (a-translation) between two adjacent Zn atoms. There exists π-π interaction between the adjacent imidazole-ring planes (π-π distance = 3.618 Å), which strengthens the formation of the chain.

Related literature top

For related literature, see: Shi et al. (2004, 2007).

For related literature, see: Sheldrick (1997).

Experimental top

A mixture of ZnCl2 (1 mmol), ion liquid 1-methyl-3-carboxymethylimidazole hydroxide (1 mmol) and water (20 ml) was sealed in a 25 ml Teflon-lined stainless steel reactor and heated at 393 K for 48 h. A colourless solution was obtained after cooling the reaction to room temperature, colourless single crystals were obtained after three weeks.

Refinement top

The H atoms bonded to C atoms were positioned geometrically (aromatic C–H = 0.93Å and aliphatic C–H = 0.97 Å, Uiso(H) = 1.2Ueq(C)). In the X-ray diffraction experiment 794 Friedel pairs were measured.

Structure description top

It is known that the research of coordination polymers receives great interest nowadays, because they may afford new materials with useful properties, such as catalytic activity, microporosity and so on (Shi et al., 2004). Recently, we have synthesized and reported cadmium polymer with 1-methyl-3-carboxymethylimidazole (Shi et al., 2007). As an extension of our work in this field, we synthesized the title compound and solved its crystal structure (I).

The asymmetric unit of (I) contains one Zn atom, one 1-methyl-3-carboxymethylimidazole molecule, and two chlorine atoms (Fig. 1). The structure of (I) is a one-dimensional coordination chain in which the adjacent (ZnCl2) groups are bridged by 1-methyl-3-carboxymethylimidazole through its two O atoms with the distance of 4.8362 (4)Å (a-translation) between two adjacent Zn atoms. There exists π-π interaction between the adjacent imidazole-ring planes (π-π distance = 3.618 Å), which strengthens the formation of the chain.

For related literature, see: Shi et al. (2004, 2007).

For related literature, see: Sheldrick (1997).

Computing details top

Data collection: SMART (Bruker, 2004); cell refinement: SMART (Bruker, 2004) and SAINT (Bruker, 2004); data reduction: XPREP (Bruker 2002); program(s) used to solve structure: SHELXTL (Bruker 2002); program(s) used to refine structure: SHELXTL (Bruker 2002); molecular graphics: SHELXTL (Bruker 2002); software used to prepare material for publication: SHELXTL (Bruker 2002).

Figures top
[Figure 1] Fig. 1. A view of the molecule of (I) with the atom-labelling scheme. Displacement ellipsoids are drawn at the 50% probability. H atoms are presented as spheres with arbitrary radius. Symmetry code: (i) -1 + x, y, z;
[Figure 2] Fig. 2. The one-dimensional chain in crystal structure of (I).
catena-Poly[[dichloridozinc(II)]-µ-1-carboxylatomethyl-3-methylimidazolium-\ κ2O:O'] top
Crystal data top
[ZnCl2(C6H8N2O2)]F(000) = 276
Mr = 276.43Dx = 1.814 Mg m3
Monoclinic, PcMo Kα radiation, λ = 0.71073 Å
Hall symbol: P -2ycCell parameters from 1309 reflections
a = 4.8362 (4) Åθ = 2.8–27.7°
b = 10.5820 (9) ŵ = 2.92 mm1
c = 10.1164 (7) ÅT = 296 K
β = 102.183 (5)°Prism, colourless
V = 506.06 (7) Å30.35 × 0.11 × 0.05 mm
Z = 2
Data collection top
Bruker P4
diffractometer
1994 independent reflections
Radiation source: fine-focus sealed tube1691 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.020
ω scansθmax = 27.7°, θmin = 2.8°
Absorption correction: empirical (using intensity measurements)
(SADABS; Sheldrick, 1996)
h = 66
Tmin = 0.687, Tmax = 0.864k = 1313
3003 measured reflectionsl = 1212
Refinement top
Refinement on F2Secondary atom site location: Difmap
Least-squares matrix: FullHydrogen site location: Geom
R[F2 > 2σ(F2)] = 0.033H-atom parameters constrained
wR(F2) = 0.068 w = 1/[σ2(Fo2) + (0.025P)2],
where P = (Fo2 + 2Fc2)/3
S = 1.01(Δ/σ)max < 0.001
1994 reflectionsΔρmax = 0.45 e Å3
118 parametersΔρmin = 0.59 e Å3
0 restraintsAbsolute structure: Flack (1983)
Primary atom site location: DirectAbsolute structure parameter: 0.055 (15)
Crystal data top
[ZnCl2(C6H8N2O2)]V = 506.06 (7) Å3
Mr = 276.43Z = 2
Monoclinic, PcMo Kα radiation
a = 4.8362 (4) ŵ = 2.92 mm1
b = 10.5820 (9) ÅT = 296 K
c = 10.1164 (7) Å0.35 × 0.11 × 0.05 mm
β = 102.183 (5)°
Data collection top
Bruker P4
diffractometer
1994 independent reflections
Absorption correction: empirical (using intensity measurements)
(SADABS; Sheldrick, 1996)
1691 reflections with I > 2σ(I)
Tmin = 0.687, Tmax = 0.864Rint = 0.020
3003 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.033H-atom parameters constrained
wR(F2) = 0.068Δρmax = 0.45 e Å3
S = 1.01Δρmin = 0.59 e Å3
1994 reflectionsAbsolute structure: Flack (1983)
118 parametersAbsolute structure parameter: 0.055 (15)
0 restraints
Special details top

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 > 2σ(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.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Zn10.03320 (7)0.76339 (4)0.06177 (5)0.03457 (14)
Cl10.0646 (3)0.96102 (10)0.13316 (14)0.0511 (3)
Cl20.0059 (2)0.61405 (10)0.21919 (13)0.0468 (3)
C10.3986 (10)0.8408 (5)0.6340 (4)0.0485 (12)
H1A0.45900.92680.62880.073*
H1B0.49070.80520.71920.073*
H1C0.19740.83860.62630.073*
C20.4180 (10)0.6411 (4)0.5010 (5)0.0415 (11)
H2A0.32300.58930.55100.050*
C30.5240 (9)0.6061 (4)0.3952 (4)0.0395 (11)
H3A0.51460.52600.35660.047*
C40.6128 (8)0.8075 (4)0.4347 (5)0.0339 (10)
H4A0.67560.88990.42890.041*
C50.7844 (8)0.7217 (4)0.2374 (4)0.0352 (9)
H5A0.89720.64650.23350.042*
H5B0.91110.79380.24950.042*
C60.5754 (8)0.7356 (4)0.1059 (4)0.0317 (9)
N10.4738 (8)0.7668 (3)0.5229 (4)0.0355 (9)
N20.6513 (7)0.7124 (4)0.3538 (4)0.0305 (8)
O10.6675 (6)0.7498 (3)0.0018 (3)0.0518 (9)
O20.3161 (5)0.7312 (3)0.1078 (3)0.0481 (9)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Zn10.02622 (18)0.0510 (3)0.0276 (2)0.0024 (3)0.00809 (14)0.0035 (3)
Cl10.0555 (6)0.0378 (6)0.0633 (8)0.0024 (5)0.0199 (6)0.0084 (6)
Cl20.0494 (6)0.0366 (6)0.0562 (7)0.0000 (5)0.0149 (5)0.0038 (5)
C10.060 (3)0.056 (3)0.032 (3)0.006 (2)0.014 (2)0.005 (2)
C20.045 (2)0.045 (3)0.038 (3)0.006 (2)0.014 (2)0.005 (2)
C30.046 (2)0.035 (3)0.039 (3)0.002 (2)0.012 (2)0.0028 (19)
C40.031 (2)0.041 (2)0.030 (2)0.0055 (16)0.007 (2)0.002 (2)
C50.0240 (17)0.051 (3)0.032 (2)0.0018 (18)0.0103 (16)0.003 (2)
C60.0272 (18)0.041 (2)0.029 (2)0.0004 (17)0.0096 (16)0.0044 (18)
N10.035 (2)0.045 (2)0.027 (2)0.0004 (16)0.0067 (17)0.0027 (17)
N20.0275 (17)0.042 (2)0.024 (2)0.0023 (16)0.0103 (15)0.0028 (17)
O10.0256 (13)0.105 (3)0.0262 (18)0.0044 (15)0.0089 (12)0.0114 (16)
O20.0210 (13)0.091 (3)0.0336 (17)0.0011 (14)0.0078 (12)0.0107 (17)
Geometric parameters (Å, º) top
Zn1—O21.985 (3)C3—H3A0.9300
Zn1—O1i2.011 (3)C4—N11.298 (6)
Zn1—Cl22.2231 (13)C4—N21.335 (6)
Zn1—Cl12.2281 (12)C4—H4A0.9300
C1—N11.477 (6)C5—N21.460 (6)
C1—H1A0.9600C5—C61.499 (6)
C1—H1B0.9600C5—H5A0.9700
C1—H1C0.9600C5—H5B0.9700
C2—C31.334 (6)C6—O11.235 (5)
C2—N11.366 (5)C6—O21.259 (5)
C2—H2A0.9300O1—Zn1ii2.011 (3)
C3—N21.388 (6)
O2—Zn1—O1i101.74 (11)N1—C4—H4A125.3
O2—Zn1—Cl2115.85 (11)N2—C4—H4A125.3
O1i—Zn1—Cl2103.34 (11)N2—C5—C6113.2 (3)
O2—Zn1—Cl1111.06 (11)N2—C5—H5A108.9
O1i—Zn1—Cl1107.20 (11)C6—C5—H5A108.9
Cl2—Zn1—Cl1115.87 (5)N2—C5—H5B108.9
N1—C1—H1A109.5C6—C5—H5B108.9
N1—C1—H1B109.5H5A—C5—H5B107.8
H1A—C1—H1B109.5O1—C6—O2123.9 (4)
N1—C1—H1C109.5O1—C6—C5118.1 (3)
H1A—C1—H1C109.5O2—C6—C5118.0 (3)
H1B—C1—H1C109.5C4—N1—C2108.9 (4)
C3—C2—N1107.7 (4)C4—N1—C1126.4 (4)
C3—C2—H2A126.1C2—N1—C1124.6 (4)
N1—C2—H2A126.1C4—N2—C3107.3 (4)
C2—C3—N2106.7 (4)C4—N2—C5125.9 (4)
C2—C3—H3A126.7C3—N2—C5126.6 (4)
N2—C3—H3A126.7C6—O1—Zn1ii141.3 (3)
N1—C4—N2109.4 (4)C6—O2—Zn1119.1 (3)
N1—C2—C3—N21.1 (5)C2—C3—N2—C5176.8 (4)
N2—C5—C6—O1176.9 (4)C6—C5—N2—C496.5 (5)
N2—C5—C6—O23.7 (5)C6—C5—N2—C378.6 (5)
N2—C4—N1—C20.2 (5)O2—C6—O1—Zn1ii180.0 (4)
N2—C4—N1—C1177.2 (4)C5—C6—O1—Zn1ii0.6 (7)
C3—C2—N1—C40.8 (5)O1—C6—O2—Zn15.6 (6)
C3—C2—N1—C1178.0 (4)C5—C6—O2—Zn1175.0 (3)
N1—C4—N2—C30.5 (5)O1i—Zn1—O2—C6178.3 (3)
N1—C4—N2—C5176.4 (4)Cl2—Zn1—O2—C670.5 (3)
C2—C3—N2—C41.0 (5)Cl1—Zn1—O2—C664.5 (3)
Symmetry codes: (i) x1, y, z; (ii) x+1, y, z.

Experimental details

Crystal data
Chemical formula[ZnCl2(C6H8N2O2)]
Mr276.43
Crystal system, space groupMonoclinic, Pc
Temperature (K)296
a, b, c (Å)4.8362 (4), 10.5820 (9), 10.1164 (7)
β (°) 102.183 (5)
V3)506.06 (7)
Z2
Radiation typeMo Kα
µ (mm1)2.92
Crystal size (mm)0.35 × 0.11 × 0.05
Data collection
DiffractometerBruker P4
Absorption correctionEmpirical (using intensity measurements)
(SADABS; Sheldrick, 1996)
Tmin, Tmax0.687, 0.864
No. of measured, independent and
observed [I > 2σ(I)] reflections
3003, 1994, 1691
Rint0.020
(sin θ/λ)max1)0.654
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.033, 0.068, 1.01
No. of reflections1994
No. of parameters118
H-atom treatmentH-atom parameters constrained
Δρmax, Δρmin (e Å3)0.45, 0.59
Absolute structureFlack (1983)
Absolute structure parameter0.055 (15)

Computer programs: SMART (Bruker, 2004) and SAINT (Bruker, 2004), XPREP (Bruker 2002), SHELXTL (Bruker 2002).

 

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