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In the title compound, [ZnCl2(C6H5NO)2], the ZnII atom lies on a mirror plane, and is coordinated by two N atoms from two pyridine-3-carbaldehyde ligands and two Cl ligands in a distorted tetra­hedral geometry. The packing is governed by inter­molecular C—H...O hydrogen-bonding inter­actions.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536807057881/zl2084sup1.cif
Contains datablocks I, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536807057881/zl2084Isup2.hkl
Contains datablock I

CCDC reference: 672694

Key indicators

  • Single-crystal X-ray study
  • T = 296 K
  • Mean [sigma](C-C) = 0.003 Å
  • R factor = 0.022
  • wR factor = 0.061
  • Data-to-parameter ratio = 18.0

checkCIF/PLATON results

No syntax errors found



Alert level C PLAT232_ALERT_2_C Hirshfeld Test Diff (M-X) Zn1 - Cl2 .. 5.06 su PLAT480_ALERT_4_C Long H...A H-Bond Reported H4 .. O1 .. 2.66 Ang.
Alert level G PLAT794_ALERT_5_G Check Predicted Bond Valency for Zn1 (2) 1.99
0 ALERT level A = In general: serious problem 0 ALERT level B = Potentially serious problem 2 ALERT level C = Check and explain 1 ALERT level G = General alerts; check 0 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 0 ALERT type 3 Indicator that the structure quality may be low 1 ALERT type 4 Improvement, methodology, query or suggestion 1 ALERT type 5 Informative message, check

Comment top

Coordination compounds of the type ZnL2Cl2 (L = 2-NH2py, 4-CNpy, 4-CH3py, 4-CH3COpy,3-NH2COpy, etc (py = pyridine)) have been previously prepared and studied by several groups (Qin et al., 1999; Steffen & Palenik, 1977; Lynton & Sears, 1971; Ide et al., 2002). In this paper, we report the crystal structure of the new mononuclear zinc complex Zn(3-CHOpy)2Cl2 (where 3-CHOpy is 3-pyridinecarboxaldehyde or nicotinaldehyde).

As illustrated in Fig. 1, the ZnII centre lies on a symmetry plane, defined by the zinc atom and the two chlorine atoms. The zinc center is coordinated to two N atoms from two 3-pyridinecarboxaldehyde ligands and two Cl atoms, and displays a distorted tetrahedral geometry. In the packing, C—H···O hydrogen bonding interactions (Table 1) stabilize the structural components (Fig. 2).

Related literature top

Similar complexes have been previously prepared and studied by: Ide et al. (2002); Lynton & Sears (1971); Qin et al. (1999); Steffen & Palenik (1977).

Experimental top

The title compound was prepared by the addition of ZnCl2 (1.0 mmol) to an ethanol solution (20 ml) of pyridine-3-carbalehyde (nicotinaldehyde, 2.0 mmol). The mixture was stirred at 80°C for 2 h and filtered. Colorless prismatic single crystals were obtained from the filtrate upon slow evaporation of the solvent over several days.

Refinement top

All H atoms on aromatic rings were placed in calculated positions (C—H = 0.93 Å) and were refined using a riding model with Uiso(H) = 1.2Ueq(C).

Computing details top

Data collection: APEX2 (Bruker, 2004); cell refinement: SAINT (Bruker, 2004); data reduction: SAINT (Bruker, 2004); program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: XP in SHELXTL (Bruker, 2004); software used to prepare material for publication: SHELXTL (Bruker, 2004).

Figures top
[Figure 1] Fig. 1. The molecular structure of the title complex, showing 50% probability displacement ellipsoids. Unlabelled atoms are related to the labelled atoms by the symmetry operator (x, 1.5 - y, z).
[Figure 2] Fig. 2. Packing diagram of the title complex, viewed along the a axis. Dashed lines indicate the C—H···O hydrogen bonds.
Dichloridobis(pyridine-3-carbaldehyde-κN)zinc(II) top
Crystal data top
[ZnCl2(C6H5NO)2]F(000) = 704
Mr = 350.49Dx = 1.683 Mg m3
Orthorhombic, PnmaMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ac 2nCell parameters from 1650 reflections
a = 5.8445 (1) Åθ = 1.4–28.0°
b = 19.2032 (3) ŵ = 2.16 mm1
c = 12.3216 (2) ÅT = 296 K
V = 1382.89 (4) Å3Prismatic, colourless
Z = 40.20 × 0.18 × 0.18 mm
Data collection top
Bruker APEXII area-detector
diffractometer
1639 independent reflections
Radiation source: fine-focus sealed tube1412 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.027
ϕ and ω scansθmax = 27.5°, θmin = 2.0°
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
h = 77
Tmin = 0.659, Tmax = 0.682k = 2423
11915 measured reflectionsl = 1416
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.022Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.061H-atom parameters constrained
S = 1.05 w = 1/[σ2(Fo2) + (0.0316P)2 + 0.3618P]
where P = (Fo2 + 2Fc2)/3
1639 reflections(Δ/σ)max < 0.001
91 parametersΔρmax = 0.24 e Å3
0 restraintsΔρmin = 0.26 e Å3
Crystal data top
[ZnCl2(C6H5NO)2]V = 1382.89 (4) Å3
Mr = 350.49Z = 4
Orthorhombic, PnmaMo Kα radiation
a = 5.8445 (1) ŵ = 2.16 mm1
b = 19.2032 (3) ÅT = 296 K
c = 12.3216 (2) Å0.20 × 0.18 × 0.18 mm
Data collection top
Bruker APEXII area-detector
diffractometer
1639 independent reflections
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
1412 reflections with I > 2σ(I)
Tmin = 0.659, Tmax = 0.682Rint = 0.027
11915 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0220 restraints
wR(F2) = 0.061H-atom parameters constrained
S = 1.05Δρmax = 0.24 e Å3
1639 reflectionsΔρmin = 0.26 e Å3
91 parameters
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 > 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.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
C10.4874 (3)0.65200 (8)0.05903 (13)0.0386 (4)
H10.46980.67650.12360.046*
C20.6525 (3)0.60094 (9)0.05413 (15)0.0420 (4)
C30.6773 (3)0.56404 (9)0.04233 (17)0.0515 (5)
H30.78650.52900.04830.062*
C40.5380 (4)0.58012 (9)0.12864 (15)0.0516 (5)
H40.55120.55600.19380.062*
C50.3783 (3)0.63254 (9)0.11717 (14)0.0450 (4)
H50.28600.64360.17620.054*
C60.7926 (3)0.58667 (10)0.15072 (16)0.0542 (5)
H60.76590.61330.21250.065*
Cl10.12237 (11)0.75000.14568 (5)0.05127 (17)
Cl20.00885 (11)0.75000.15928 (5)0.05020 (17)
N10.3506 (2)0.66815 (7)0.02492 (11)0.0368 (3)
O10.9395 (3)0.54290 (8)0.15522 (14)0.0800 (5)
Zn10.12503 (4)0.75000.01246 (2)0.03558 (10)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C10.0421 (9)0.0379 (9)0.0360 (8)0.0006 (7)0.0002 (7)0.0014 (6)
C20.0414 (9)0.0367 (8)0.0479 (9)0.0022 (7)0.0022 (7)0.0041 (7)
C30.0547 (11)0.0388 (9)0.0610 (11)0.0089 (8)0.0137 (9)0.0008 (8)
C40.0683 (12)0.0435 (10)0.0429 (10)0.0012 (9)0.0087 (9)0.0087 (8)
C50.0541 (11)0.0441 (9)0.0369 (8)0.0041 (8)0.0010 (7)0.0015 (7)
C60.0513 (11)0.0511 (11)0.0601 (11)0.0052 (9)0.0048 (9)0.0071 (9)
Cl10.0436 (4)0.0672 (4)0.0430 (3)0.0000.0112 (3)0.000
Cl20.0504 (4)0.0647 (4)0.0355 (3)0.0000.0057 (3)0.000
N10.0385 (7)0.0361 (7)0.0359 (7)0.0005 (6)0.0002 (5)0.0009 (5)
O10.0728 (10)0.0789 (11)0.0884 (12)0.0346 (9)0.0138 (9)0.0078 (9)
Zn10.03358 (17)0.03874 (16)0.03444 (15)0.0000.00213 (10)0.000
Geometric parameters (Å, º) top
C1—N11.344 (2)C5—N11.336 (2)
C1—C21.377 (2)C5—H50.9300
C1—H10.9300C6—O11.203 (2)
C2—C31.391 (3)C6—H60.9300
C2—C61.471 (3)Cl1—Zn12.1876 (7)
C3—C41.374 (3)Cl2—Zn12.2223 (6)
C3—H30.9300N1—Zn12.0571 (14)
C4—C51.380 (3)Zn1—N1i2.0571 (14)
C4—H40.9300
N1—C1—C2123.20 (15)C4—C5—H5118.6
N1—C1—H1118.4O1—C6—C2124.41 (19)
C2—C1—H1118.4O1—C6—H6117.8
C1—C2—C3118.24 (17)C2—C6—H6117.8
C1—C2—C6119.17 (17)C5—N1—C1117.67 (15)
C3—C2—C6122.58 (17)C5—N1—Zn1122.16 (12)
C4—C3—C2119.00 (17)C1—N1—Zn1120.02 (11)
C4—C3—H3120.5N1i—Zn1—N199.65 (8)
C2—C3—H3120.5N1i—Zn1—Cl1111.56 (4)
C3—C4—C5119.03 (17)N1—Zn1—Cl1111.56 (4)
C3—C4—H4120.5N1i—Zn1—Cl2105.48 (4)
C5—C4—H4120.5N1—Zn1—Cl2105.48 (4)
N1—C5—C4122.85 (17)Cl1—Zn1—Cl2120.83 (3)
N1—C5—H5118.6
Symmetry code: (i) x, y+3/2, z.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C3—H3···O1ii0.932.493.342 (2)152
C4—H4···O1iii0.932.663.562 (2)164
Symmetry codes: (ii) x+2, y+1, z; (iii) x+3/2, y+1, z1/2.

Experimental details

Crystal data
Chemical formula[ZnCl2(C6H5NO)2]
Mr350.49
Crystal system, space groupOrthorhombic, Pnma
Temperature (K)296
a, b, c (Å)5.8445 (1), 19.2032 (3), 12.3216 (2)
V3)1382.89 (4)
Z4
Radiation typeMo Kα
µ (mm1)2.16
Crystal size (mm)0.20 × 0.18 × 0.18
Data collection
DiffractometerBruker APEXII area-detector
diffractometer
Absorption correctionMulti-scan
(SADABS; Sheldrick, 1996)
Tmin, Tmax0.659, 0.682
No. of measured, independent and
observed [I > 2σ(I)] reflections
11915, 1639, 1412
Rint0.027
(sin θ/λ)max1)0.650
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.022, 0.061, 1.05
No. of reflections1639
No. of parameters91
H-atom treatmentH-atom parameters constrained
Δρmax, Δρmin (e Å3)0.24, 0.26

Computer programs: APEX2 (Bruker, 2004), SAINT (Bruker, 2004), SHELXS97 (Sheldrick, 1997), SHELXL97 (Sheldrick, 1997), XP in SHELXTL (Bruker, 2004), SHELXTL (Bruker, 2004).

Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C3—H3···O1i0.932.493.342 (2)152.1
C4—H4···O1ii0.932.663.562 (2)164.0
Symmetry codes: (i) x+2, y+1, z; (ii) x+3/2, y+1, z1/2.
 

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