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The Sn atom in the title compound, [Sn(CH3)2(C10H6NO2)Cl], has a distorted SnC2NOCl trigonal-bipyramidal geometry with the quinoline N atom and Cl atom occupying the axial sites.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536807058229/hb2653sup1.cif
Contains datablocks I, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536807058229/hb2653Isup2.hkl
Contains datablock I

CCDC reference: 672689

Key indicators

  • Single-crystal X-ray study
  • T = 298 K
  • Mean [sigma](C-C) = 0.008 Å
  • R factor = 0.031
  • wR factor = 0.091
  • Data-to-parameter ratio = 15.4

checkCIF/PLATON results

No syntax errors found



Alert level C PLAT242_ALERT_2_C Check Low Ueq as Compared to Neighbors for Sn1
0 ALERT level A = In general: serious problem 0 ALERT level B = Potentially serious problem 1 ALERT level C = Check and explain 0 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 0 ALERT type 4 Improvement, methodology, query or suggestion 0 ALERT type 5 Informative message, check

Comment top

Organotin esters of carboxylic acids are widely used as biocides, as fungicides and, in industry, as homogeneous catalysts. Studies on organotin complexes containing carboxylate ligands with an additional donor atom (e.g. N, O or S) that is available for coordinating to the Sn atom have revealed that new structural types may lead to different activities. We have therefore synthesized the title compound, (I), and present its crystal structure here.

The molecular structure of (I) is shown in Fig. 1. The Sn1 assumes a trigonal-bipyramidal coordination geometry (Table 1) with atoms N1 and Cl1 in axial positions [N1—Sn1—Cl1 = 156.47 (10) °] and the C atoms of the two methyl groups and the ligand Cl atom in equatorial positions. Associated with the sum of the angles subtended at the Sn1 in the equatorial plane is 358.7°, indicating approximate coplanarity for these atoms;. The Sn—O and Sn—N distnaces in (I) are close to those in related compounds (Ma et al., 2004).

Related literature top

For related materials, see: Ma et al. (2004).

Experimental top

The reaction was carried out under nitrogen atmosphere. Quinaldic acid (1 mmol) and sodium ethoxide (1.2 mmol) were added to benzene (30 ml) in a Schlenk flask and stirred for 0.5 h. Dimethyltin chloride (1 mmol) was then added to the reactor and the reaction mixture was stirred for 12 h at 313 K. The resulting clear solution was evaporated under vacuum. The product was crystallized from a mixture of dichloromethane/methanol (1:1 v/v) to yield colourless blocks of (I) (yield 85%; m.p. 422 K). Analysis calculated (%) for C12H12ClNO2Sn (Mr = 356.37): C, 40.44; H, 3.39; N, 3.93. found: C, 40.37; H, 3.42; N, 4.06.

Refinement top

The H atoms were positioned geometrically (C—H = 0.93–0.96 Å) and refined as riding with Uiso(H) = 1.2Ueq(C) or 1.5Ueq(methyl C).

Computing details top

Data collection: SMART (Siemens, 1996); cell refinement: SAINT (Siemens, 1996); data reduction: SAINT (Siemens, 1996); program(s) used to solve structure: SHELXS97 (Sheldrick, 1997a); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997a); molecular graphics: SHELXTL (Sheldrick, 1997b); software used to prepare material for publication: SHELXTL (Sheldrick, 1997b).

Figures top
[Figure 1] Fig. 1. The molecular structure of (I), showing 50% probability displacement ellipsoids. H atoms have been omitted for clarity.
Chloridodimethyl(quinaldato)tin(IV) top
Crystal data top
[Sn(CH3)2(C10H6NO2)Cl]F(000) = 696
Mr = 356.37Dx = 1.747 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ybcCell parameters from 3020 reflections
a = 10.093 (10) Åθ = 2.2–26.9°
b = 10.245 (10) ŵ = 2.07 mm1
c = 13.763 (7) ÅT = 298 K
β = 107.811 (10)°Block, colourless
V = 1355 (2) Å30.43 × 0.22 × 0.10 mm
Z = 4
Data collection top
Siemens SMART CCD
diffractometer
2370 independent reflections
Radiation source: fine-focus sealed tube1864 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.035
ω scansθmax = 25.0°, θmin = 2.1°
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
h = 1111
Tmin = 0.470, Tmax = 0.820k = 1112
6777 measured reflectionsl = 1612
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)] = 0.031Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.092H-atom parameters constrained
S = 1.00 w = 1/[σ2(Fo2) + (0.050P)2 + 1.111P]
where P = (Fo2 + 2Fc2)/3
2370 reflections(Δ/σ)max < 0.001
154 parametersΔρmax = 0.52 e Å3
0 restraintsΔρmin = 0.64 e Å3
Crystal data top
[Sn(CH3)2(C10H6NO2)Cl]V = 1355 (2) Å3
Mr = 356.37Z = 4
Monoclinic, P21/cMo Kα radiation
a = 10.093 (10) ŵ = 2.07 mm1
b = 10.245 (10) ÅT = 298 K
c = 13.763 (7) Å0.43 × 0.22 × 0.10 mm
β = 107.811 (10)°
Data collection top
Siemens SMART CCD
diffractometer
2370 independent reflections
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
1864 reflections with I > 2σ(I)
Tmin = 0.470, Tmax = 0.820Rint = 0.035
6777 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0310 restraints
wR(F2) = 0.092H-atom parameters constrained
S = 1.00Δρmax = 0.52 e Å3
2370 reflectionsΔρmin = 0.64 e Å3
154 parameters
Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Sn10.84595 (3)0.38500 (3)0.11961 (2)0.04570 (15)
Cl10.9399 (2)0.58899 (17)0.20610 (15)0.1085 (7)
N10.6902 (3)0.2501 (3)0.0062 (2)0.0404 (8)
O10.7184 (3)0.5072 (3)0.0152 (2)0.0527 (8)
O20.5316 (4)0.5410 (4)0.1171 (3)0.0745 (11)
C10.6110 (5)0.4669 (5)0.0584 (4)0.0491 (11)
C20.5919 (4)0.3224 (4)0.0701 (3)0.0432 (10)
C30.4796 (5)0.2692 (5)0.1459 (3)0.0559 (12)
H30.41100.32260.18760.067*
C40.4729 (6)0.1371 (6)0.1573 (4)0.0630 (15)
H40.39930.09960.20770.076*
C50.5757 (5)0.0577 (5)0.0939 (4)0.0557 (12)
C60.6834 (5)0.1170 (4)0.0167 (4)0.0472 (11)
C70.7870 (5)0.0395 (5)0.0500 (4)0.0608 (13)
H70.85830.07800.10160.073*
C80.7814 (7)0.0936 (5)0.0380 (6)0.0799 (19)
H80.84930.14530.08220.096*
C90.6768 (8)0.1520 (6)0.0385 (6)0.085 (2)
H90.67650.24230.04530.102*
C100.5746 (8)0.0815 (6)0.1038 (5)0.0765 (19)
H100.50450.12290.15450.092*
C110.7655 (5)0.3133 (5)0.2328 (4)0.0623 (13)
H11A0.68550.36380.23320.093*
H11B0.83510.31970.29820.093*
H11C0.73890.22370.21880.093*
C121.0181 (5)0.3270 (6)0.0735 (5)0.0815 (18)
H12A1.02490.38220.01880.122*
H12B1.00600.23810.05050.122*
H12C1.10160.33440.13010.122*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Sn10.0431 (2)0.0443 (2)0.0489 (2)0.00363 (13)0.01283 (14)0.00114 (14)
Cl10.1292 (16)0.0709 (11)0.0931 (13)0.0353 (10)0.0139 (11)0.0156 (9)
N10.051 (2)0.035 (2)0.0390 (19)0.0010 (16)0.0183 (16)0.0001 (15)
O10.0593 (19)0.0362 (18)0.060 (2)0.0000 (14)0.0143 (16)0.0035 (15)
O20.079 (2)0.062 (2)0.072 (2)0.016 (2)0.007 (2)0.024 (2)
C10.056 (3)0.045 (3)0.050 (3)0.005 (2)0.021 (2)0.007 (2)
C20.048 (2)0.044 (3)0.040 (2)0.003 (2)0.0166 (19)0.001 (2)
C30.056 (3)0.071 (4)0.041 (3)0.007 (2)0.015 (2)0.001 (2)
C40.062 (3)0.084 (4)0.048 (3)0.028 (3)0.024 (2)0.023 (3)
C50.071 (3)0.053 (3)0.055 (3)0.018 (3)0.037 (3)0.018 (3)
C60.062 (3)0.035 (2)0.056 (3)0.004 (2)0.035 (2)0.005 (2)
C70.073 (3)0.041 (3)0.070 (3)0.008 (2)0.024 (3)0.002 (2)
C80.109 (5)0.038 (3)0.111 (5)0.017 (3)0.060 (4)0.011 (3)
C90.124 (6)0.036 (3)0.128 (6)0.017 (4)0.089 (5)0.022 (4)
C100.108 (5)0.055 (4)0.095 (5)0.027 (3)0.074 (4)0.028 (3)
C110.065 (3)0.072 (4)0.052 (3)0.012 (3)0.021 (2)0.007 (3)
C120.057 (3)0.082 (4)0.120 (5)0.012 (3)0.049 (3)0.029 (4)
Geometric parameters (Å, º) top
Sn1—O12.040 (3)C5—C101.433 (8)
Sn1—C112.098 (5)C6—C71.407 (7)
Sn1—C122.109 (5)C7—C81.373 (7)
Sn1—N12.390 (4)C7—H70.9300
Sn1—Cl12.448 (2)C8—C91.379 (9)
N1—C21.333 (5)C8—H80.9300
N1—C61.371 (5)C9—C101.351 (10)
O1—C11.304 (5)C9—H90.9300
O2—C11.215 (5)C10—H100.9300
C1—C21.495 (7)C11—H11A0.9600
C2—C31.395 (6)C11—H11B0.9600
C3—C41.362 (7)C11—H11C0.9600
C3—H30.9300C12—H12A0.9600
C4—C51.396 (8)C12—H12B0.9600
C4—H40.9300C12—H12C0.9600
C5—C61.404 (7)
O1—Sn1—C11115.73 (17)C6—C5—C10119.0 (6)
O1—Sn1—C12111.2 (2)N1—C6—C5120.8 (5)
C11—Sn1—C12131.8 (2)N1—C6—C7119.3 (4)
O1—Sn1—N173.22 (14)C5—C6—C7119.9 (4)
C11—Sn1—N190.98 (18)C8—C7—C6119.1 (6)
C12—Sn1—N192.2 (2)C8—C7—H7120.4
O1—Sn1—Cl183.42 (11)C6—C7—H7120.4
C11—Sn1—Cl196.77 (17)C7—C8—C9121.1 (6)
C12—Sn1—Cl198.9 (2)C7—C8—H8119.4
N1—Sn1—Cl1156.47 (10)C9—C8—H8119.4
C2—N1—C6118.7 (4)C10—C9—C8121.8 (6)
C2—N1—Sn1110.4 (3)C10—C9—H9119.1
C6—N1—Sn1130.7 (3)C8—C9—H9119.1
C1—O1—Sn1123.3 (3)C9—C10—C5119.1 (6)
O2—C1—O1122.8 (4)C9—C10—H10120.5
O2—C1—C2120.6 (4)C5—C10—H10120.5
O1—C1—C2116.5 (4)Sn1—C11—H11A109.5
N1—C2—C3123.2 (4)Sn1—C11—H11B109.5
N1—C2—C1115.7 (4)H11A—C11—H11B109.5
C3—C2—C1121.1 (4)Sn1—C11—H11C109.5
C4—C3—C2118.4 (5)H11A—C11—H11C109.5
C4—C3—H3120.8H11B—C11—H11C109.5
C2—C3—H3120.8Sn1—C12—H12A109.5
C3—C4—C5120.4 (5)Sn1—C12—H12B109.5
C3—C4—H4119.8H12A—C12—H12B109.5
C5—C4—H4119.8Sn1—C12—H12C109.5
C4—C5—C6118.5 (5)H12A—C12—H12C109.5
C4—C5—C10122.6 (6)H12B—C12—H12C109.5

Experimental details

Crystal data
Chemical formula[Sn(CH3)2(C10H6NO2)Cl]
Mr356.37
Crystal system, space groupMonoclinic, P21/c
Temperature (K)298
a, b, c (Å)10.093 (10), 10.245 (10), 13.763 (7)
β (°) 107.811 (10)
V3)1355 (2)
Z4
Radiation typeMo Kα
µ (mm1)2.07
Crystal size (mm)0.43 × 0.22 × 0.10
Data collection
DiffractometerSiemens SMART CCD
diffractometer
Absorption correctionMulti-scan
(SADABS; Sheldrick, 1996)
Tmin, Tmax0.470, 0.820
No. of measured, independent and
observed [I > 2σ(I)] reflections
6777, 2370, 1864
Rint0.035
(sin θ/λ)max1)0.595
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.031, 0.092, 1.00
No. of reflections2370
No. of parameters154
H-atom treatmentH-atom parameters constrained
Δρmax, Δρmin (e Å3)0.52, 0.64

Computer programs: SMART (Siemens, 1996), SAINT (Siemens, 1996), SHELXS97 (Sheldrick, 1997a), SHELXL97 (Sheldrick, 1997a), SHELXTL (Sheldrick, 1997b).

Selected bond lengths (Å) top
Sn1—O12.040 (3)Sn1—N12.390 (4)
Sn1—C112.098 (5)Sn1—Cl12.448 (2)
Sn1—C122.109 (5)
 

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