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In the title complex, [Sn(CH3)2(C14H11N3O3)], the Sn atom is in a distorted trigonal-bipyramidal coordination, with Sn-O distances of 2.138 (2) and 2.176 (2) Å. The dihedral angles between the two chelated benzene rings and the O-Sn-N group are 71.73 (9) and 83.30 (9)°.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S160053680903726X/kp2231sup1.cif
Contains datablocks I, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S160053680903726X/kp2231Isup2.hkl
Contains datablock I

CCDC reference: 750564

Key indicators

  • Single-crystal X-ray study
  • T = 298 K
  • Mean [sigma](C-C) = 0.005 Å
  • R factor = 0.032
  • wR factor = 0.087
  • Data-to-parameter ratio = 16.9

checkCIF/PLATON results

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Alert level C PLAT222_ALERT_3_C Large Non-Solvent H Ueq(max)/Ueq(min) ... 3.07 Ratio PLAT241_ALERT_2_C Check High Ueq as Compared to Neighbors for O3
0 ALERT level A = In general: serious problem 0 ALERT level B = Potentially serious problem 2 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 1 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

In the structure of the title compound, (I), (Fig. 1) the Sn1 atom is in a distored trigonal-bipyramidal coordination formed by a tridentate ligand of the azomethine N atom, the hydroxyl O atom and the carbonyl O atom (Table 1). The dihedral angles between the two chelated benzene rings: O2—Sn1—N2 and O3—Sn1—N2 are 83.30 (9) and 71.73 (9)°, respectively. The Sn atom is coordinated in distorted trigonal-bipyramidal arrangement with O2 and O3 located in the axial positions [O2—Sn1—O3 = 155.02 (9)°] and the C15, C16 and N2 in the equatorial positions. The sum of the C15—Sn1—C16 [146.08 (14)], C15—Sn1—N2 [106.13 (11)] and C16—Sn1—N2 [107.23 (11)°] bond angles is 359.44°, indicating approximate co-planarity for these atoms. Comparing the length of CN 1.270Å and C—N 1.470 Å, both bonds, C8—N2 (1.287 (4) Å) and C9—N1 (1.304 (4) Å) should be CN. The N1—N2 bond (1.400 (3) Å) is a single-bond (Yang et al., 1999). The Sn1—N2 distance is close to the sum of the covalent radii of 2.15Å (Sanderson, 1967), indicating a strong Sn—N interaction. Very similar structural parameters were observed in the compound studied by Yearwood et al. (2002).

Related literature top

For covalent radii, see: Sanderson (1967). For bond-lengh data, see: Yang et al. (1999). For a related structure, see: Yearwood et al. (2002).

Experimental top

A mixture of dimethyltin oxide (0.3295 g, 2.0 mmol) and 3-methoxy-2-oxideobenzaldehyde(3-pyridyl)methyl-hydrazone (0.5420 g, 2.0 mmol) in methanol (50 ml) was heated under reflux for 6 h. The obtained clear solution was evaporated under vacuum. The product was crystallized from a mixture of dichloromethane/ethanol (1:1) to yield blocks of (I). Yield 0.5936 g, 71%, m.p. 453 K, analysis, calculated for C16H17N3O3Sn: C 45.97, H, 4.10; N 10.06%; found: C 46.02, H 4.05, N, 10.09%.

Refinement top

H atoms were positioned with idealized geometry with C—H = 0.93 Å for aromatic H atomds and 0.96 Å for methyl H atoms and were constrained to ride on their parent atoms with Uiso(H) = 1.2Ueq(C) or 1.5Ueq(for methyl groups).

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, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: SHELXTL (Sheldrick, 2008); software used to prepare material for publication: SHELXTL (Sheldrick, 2008).

Figures top
[Figure 1] Fig. 1. The molecular structure of the title complex with 30% displacement ellipsoids (H atoms omitted for clarity).
[N'-(3-Methoxy-2-oxidobenzylidene)nicotinohydrazidato]dimethyltin(IV) top
Crystal data top
[Sn(CH3)2(C14H11N3O3)]F(000) = 1664
Mr = 418.02Dx = 1.689 Mg m3
Monoclinic, C2/cMo Kα radiation, λ = 0.71073 Å
Hall symbol: -C 2ycCell parameters from 4244 reflections
a = 26.121 (8) Åθ = 2.2–27.6°
b = 9.795 (3) ŵ = 1.57 mm1
c = 13.227 (4) ÅT = 298 K
β = 103.666 (4)°Block, yellow
V = 3288.4 (17) Å30.35 × 0.16 × 0.12 mm
Z = 8
Data collection top
Bruker SMART CCD area-detector
diffractometer
3574 independent reflections
Radiation source: fine-focus sealed tube3115 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.023
ϕ and ω scansθmax = 27.0°, θmin = 1.6°
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
h = 3320
Tmin = 0.609, Tmax = 0.834k = 1212
9367 measured reflectionsl = 1316
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)] = 0.032Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.087H-atom parameters constrained
S = 1.00 w = 1/[σ2(Fo2) + (0.0558P)2 + 0.5213P]
where P = (Fo2 + 2Fc2)/3
3574 reflections(Δ/σ)max < 0.001
211 parametersΔρmax = 0.48 e Å3
0 restraintsΔρmin = 0.54 e Å3
Crystal data top
[Sn(CH3)2(C14H11N3O3)]V = 3288.4 (17) Å3
Mr = 418.02Z = 8
Monoclinic, C2/cMo Kα radiation
a = 26.121 (8) ŵ = 1.57 mm1
b = 9.795 (3) ÅT = 298 K
c = 13.227 (4) Å0.35 × 0.16 × 0.12 mm
β = 103.666 (4)°
Data collection top
Bruker SMART CCD area-detector
diffractometer
3574 independent reflections
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
3115 reflections with I > 2σ(I)
Tmin = 0.609, Tmax = 0.834Rint = 0.023
9367 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0320 restraints
wR(F2) = 0.087H-atom parameters constrained
S = 1.00Δρmax = 0.48 e Å3
3574 reflectionsΔρmin = 0.54 e Å3
211 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
C10.17768 (17)0.0742 (5)0.0099 (5)0.112 (2)
H1A0.19130.06220.05090.169*
H1B0.17290.16970.02080.169*
H1C0.20210.03680.06930.169*
C20.12735 (12)0.1271 (3)0.0369 (2)0.0486 (7)
C30.17073 (12)0.1957 (3)0.0522 (3)0.0543 (8)
H30.20310.15150.03910.065*
C40.16700 (14)0.3308 (3)0.0870 (3)0.0598 (9)
H40.19660.37610.09730.072*
C50.11962 (12)0.3952 (3)0.1057 (3)0.0530 (7)
H50.11710.48520.12860.064*
C60.07437 (12)0.3282 (3)0.0910 (2)0.0450 (7)
C70.07714 (12)0.1931 (3)0.0542 (2)0.0441 (7)
C80.02708 (12)0.4074 (3)0.1159 (2)0.0461 (6)
H80.03010.49440.14210.055*
C90.10299 (11)0.4315 (3)0.1225 (2)0.0453 (7)
C100.14890 (11)0.5246 (3)0.1563 (2)0.0458 (7)
C110.14558 (15)0.6528 (3)0.1969 (3)0.0579 (8)
H110.11330.68720.20320.069*
C120.19100 (16)0.7297 (4)0.2282 (3)0.0701 (10)
H120.18980.81720.25490.084*
C130.23784 (17)0.6734 (4)0.2190 (3)0.0701 (11)
H130.26830.72510.24160.084*
C140.19835 (12)0.4796 (3)0.1490 (3)0.0563 (8)
H140.20060.39380.12020.068*
C150.07460 (13)0.0606 (3)0.1813 (2)0.0564 (8)
H15A0.07280.03420.16250.085*
H15B0.05440.07600.23230.085*
H15C0.11060.08580.20990.085*
C160.03460 (15)0.1988 (3)0.1120 (3)0.0562 (8)
H16A0.06490.24380.12580.084*
H16B0.00360.25180.14050.084*
H16C0.03100.11000.14350.084*
N10.05804 (9)0.4727 (2)0.1381 (2)0.0477 (6)
N20.01913 (9)0.3731 (3)0.10640 (18)0.0445 (5)
N30.24269 (11)0.5509 (3)0.1802 (3)0.0683 (8)
O10.12845 (9)0.0056 (3)0.0043 (2)0.0690 (7)
O20.03632 (8)0.1225 (2)0.03858 (18)0.0546 (5)
O30.11123 (10)0.3162 (2)0.0820 (2)0.0604 (6)
Sn10.043848 (7)0.17888 (2)0.049245 (14)0.04388 (10)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C10.066 (3)0.083 (3)0.202 (6)0.031 (2)0.060 (3)0.070 (3)
C20.0429 (16)0.0581 (18)0.0459 (16)0.0086 (14)0.0129 (12)0.0022 (14)
C30.0378 (16)0.072 (2)0.0542 (19)0.0055 (14)0.0135 (14)0.0008 (15)
C40.0459 (18)0.069 (2)0.069 (2)0.0046 (15)0.0219 (16)0.0008 (16)
C50.0518 (18)0.0535 (18)0.0568 (19)0.0003 (14)0.0190 (14)0.0026 (15)
C60.0419 (16)0.0540 (17)0.0397 (15)0.0042 (12)0.0107 (12)0.0063 (12)
C70.0394 (15)0.0581 (18)0.0354 (14)0.0030 (12)0.0103 (11)0.0039 (12)
C80.0472 (17)0.0458 (15)0.0459 (16)0.0028 (13)0.0120 (12)0.0027 (13)
C90.0451 (16)0.0492 (16)0.0418 (15)0.0110 (13)0.0104 (12)0.0012 (13)
C100.0479 (16)0.0466 (16)0.0421 (15)0.0124 (13)0.0091 (12)0.0037 (13)
C110.061 (2)0.0536 (18)0.061 (2)0.0123 (15)0.0173 (16)0.0053 (15)
C120.082 (3)0.0534 (19)0.076 (3)0.023 (2)0.022 (2)0.0120 (19)
C130.057 (2)0.079 (3)0.071 (3)0.0297 (18)0.0076 (18)0.0001 (19)
C140.0514 (18)0.0535 (18)0.062 (2)0.0115 (15)0.0101 (15)0.0008 (16)
C150.060 (2)0.061 (2)0.0445 (17)0.0025 (15)0.0053 (14)0.0008 (14)
C160.075 (2)0.0510 (18)0.0452 (18)0.0102 (16)0.0203 (16)0.0036 (14)
N10.0450 (14)0.0442 (13)0.0535 (15)0.0077 (11)0.0107 (11)0.0006 (11)
N20.0445 (14)0.0462 (13)0.0426 (13)0.0091 (11)0.0100 (10)0.0005 (11)
N30.0507 (17)0.0673 (19)0.085 (2)0.0174 (14)0.0116 (14)0.0038 (16)
O10.0457 (12)0.0708 (15)0.0958 (19)0.0155 (11)0.0277 (12)0.0276 (14)
O20.0400 (11)0.0565 (13)0.0689 (15)0.0080 (10)0.0162 (10)0.0079 (11)
O30.0509 (14)0.0569 (14)0.0793 (18)0.0155 (10)0.0269 (12)0.0220 (11)
Sn10.04134 (14)0.04977 (15)0.04093 (14)0.01097 (8)0.01049 (9)0.00053 (8)
Geometric parameters (Å, º) top
C1—O11.423 (4)C10—C141.390 (4)
C1—H1A0.9600C11—C121.383 (5)
C1—H1B0.9600C11—H110.9300
C1—H1C0.9600C12—C131.374 (6)
C2—O11.367 (4)C12—H120.9300
C2—C31.373 (5)C13—N31.323 (5)
C2—C71.431 (4)C13—H130.9300
C3—C41.397 (4)C14—N31.332 (4)
C3—H30.9300C14—H140.9300
C4—C51.359 (5)C15—Sn12.092 (3)
C4—H40.9300C15—H15A0.9600
C5—C61.405 (4)C15—H15B0.9600
C5—H50.9300C15—H15C0.9600
C6—C71.406 (4)C16—Sn12.098 (3)
C6—C81.430 (4)C16—H16A0.9600
C7—O21.327 (4)C16—H16B0.9600
C8—N21.287 (4)C16—H16C0.9600
C8—H80.9300N1—N21.400 (3)
C9—O31.290 (3)N2—Sn12.200 (3)
C9—N11.304 (4)O2—Sn12.138 (2)
C9—C101.489 (4)O3—Sn12.176 (2)
C10—C111.377 (4)
O1—C1—H1A109.5C11—C12—H12120.8
O1—C1—H1B109.5N3—C13—C12124.6 (3)
H1A—C1—H1B109.5N3—C13—H13117.7
O1—C1—H1C109.5C12—C13—H13117.7
H1A—C1—H1C109.5N3—C14—C10124.5 (3)
H1B—C1—H1C109.5N3—C14—H14117.7
O1—C2—C3123.7 (3)C10—C14—H14117.7
O1—C2—C7115.5 (3)Sn1—C15—H15A109.5
C3—C2—C7120.8 (3)Sn1—C15—H15B109.5
C2—C3—C4121.1 (3)H15A—C15—H15B109.5
C2—C3—H3119.4Sn1—C15—H15C109.5
C4—C3—H3119.4H15A—C15—H15C109.5
C5—C4—C3119.3 (3)H15B—C15—H15C109.5
C5—C4—H4120.4Sn1—C16—H16A109.5
C3—C4—H4120.4Sn1—C16—H16B109.5
C4—C5—C6121.2 (3)H16A—C16—H16B109.5
C4—C5—H5119.4Sn1—C16—H16C109.5
C6—C5—H5119.4H16A—C16—H16C109.5
C5—C6—C7120.8 (3)H16B—C16—H16C109.5
C5—C6—C8115.1 (3)C9—N1—N2110.7 (2)
C7—C6—C8124.2 (3)C8—N2—N1114.8 (2)
O2—C7—C6124.5 (3)C8—N2—Sn1128.1 (2)
O2—C7—C2118.7 (3)N1—N2—Sn1117.03 (18)
C6—C7—C2116.8 (3)C13—N3—C14116.1 (3)
N2—C8—C6127.9 (3)C2—O1—C1116.2 (3)
N2—C8—H8116.0C7—O2—Sn1131.74 (19)
C6—C8—H8116.0C9—O3—Sn1114.66 (19)
O3—C9—N1125.6 (3)C15—Sn1—C16146.08 (14)
O3—C9—C10117.4 (3)C15—Sn1—O295.11 (11)
N1—C9—C10117.0 (3)C16—Sn1—O294.66 (12)
C11—C10—C14117.5 (3)C15—Sn1—O392.46 (12)
C11—C10—C9123.8 (3)C16—Sn1—O392.19 (12)
C14—C10—C9118.7 (3)O2—Sn1—O3155.02 (9)
C10—C11—C12119.0 (4)C15—Sn1—N2106.13 (11)
C10—C11—H11120.5C16—Sn1—N2107.23 (11)
C12—C11—H11120.5O2—Sn1—N283.30 (9)
C13—C12—C11118.3 (4)O3—Sn1—N271.73 (9)
C13—C12—H12120.8
O1—C2—C3—C4179.1 (3)C6—C8—N2—N1179.5 (3)
C7—C2—C3—C41.4 (5)C6—C8—N2—Sn10.4 (4)
C2—C3—C4—C50.2 (5)C9—N1—N2—C8177.8 (3)
C3—C4—C5—C60.3 (5)C9—N1—N2—Sn13.0 (3)
C4—C5—C6—C71.5 (5)C12—C13—N3—C140.2 (6)
C4—C5—C6—C8178.7 (3)C10—C14—N3—C131.2 (5)
C5—C6—C7—O2179.7 (3)C3—C2—O1—C12.4 (5)
C8—C6—C7—O20.5 (5)C7—C2—O1—C1178.0 (4)
C5—C6—C7—C22.5 (4)C6—C7—O2—Sn15.1 (4)
C8—C6—C7—C2177.7 (3)C2—C7—O2—Sn1177.7 (2)
O1—C2—C7—O20.5 (4)N1—C9—O3—Sn14.5 (4)
C3—C2—C7—O2179.9 (3)C10—C9—O3—Sn1174.16 (19)
O1—C2—C7—C6177.9 (3)C7—O2—Sn1—C15110.8 (3)
C3—C2—C7—C62.4 (4)C7—O2—Sn1—C16101.7 (3)
C5—C6—C8—N2177.5 (3)C7—O2—Sn1—O33.7 (4)
C7—C6—C8—N22.3 (5)C7—O2—Sn1—N25.1 (3)
O3—C9—C10—C11177.3 (3)C9—O3—Sn1—C15102.0 (2)
N1—C9—C10—C113.9 (4)C9—O3—Sn1—C16111.6 (2)
O3—C9—C10—C144.0 (4)C9—O3—Sn1—O25.6 (4)
N1—C9—C10—C14174.7 (3)C9—O3—Sn1—N24.2 (2)
C14—C10—C11—C120.1 (5)C8—N2—Sn1—C1595.7 (3)
C9—C10—C11—C12178.5 (3)N1—N2—Sn1—C1583.4 (2)
C10—C11—C12—C131.1 (6)C8—N2—Sn1—C1690.5 (3)
C11—C12—C13—N31.3 (6)N1—N2—Sn1—C1690.4 (2)
C11—C10—C14—N31.3 (5)C8—N2—Sn1—O22.3 (2)
C9—C10—C14—N3177.4 (3)N1—N2—Sn1—O2176.8 (2)
O3—C9—N1—N21.0 (4)C8—N2—Sn1—O3177.0 (3)
C10—C9—N1—N2177.6 (2)N1—N2—Sn1—O33.86 (19)

Experimental details

Crystal data
Chemical formula[Sn(CH3)2(C14H11N3O3)]
Mr418.02
Crystal system, space groupMonoclinic, C2/c
Temperature (K)298
a, b, c (Å)26.121 (8), 9.795 (3), 13.227 (4)
β (°) 103.666 (4)
V3)3288.4 (17)
Z8
Radiation typeMo Kα
µ (mm1)1.57
Crystal size (mm)0.35 × 0.16 × 0.12
Data collection
DiffractometerBruker SMART CCD area-detector
diffractometer
Absorption correctionMulti-scan
(SADABS; Sheldrick, 1996)
Tmin, Tmax0.609, 0.834
No. of measured, independent and
observed [I > 2σ(I)] reflections
9367, 3574, 3115
Rint0.023
(sin θ/λ)max1)0.639
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.032, 0.087, 1.00
No. of reflections3574
No. of parameters211
H-atom treatmentH-atom parameters constrained
Δρmax, Δρmin (e Å3)0.48, 0.54

Computer programs: SMART (Siemens, 1996), SAINT (Siemens, 1996), SHELXS97 (Sheldrick, 2008), SHELXL97 (Sheldrick, 2008), SHELXTL (Sheldrick, 2008).

Selected bond lengths (Å) top
C15—Sn12.092 (3)O2—Sn12.138 (2)
C16—Sn12.098 (3)O3—Sn12.176 (2)
N2—Sn12.200 (3)
 

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