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In the title complex, [Sn2(CH3)4(C8H6N2O4)2(CH4O)2], each SnIV ion exists in a distorted penta­gonal–bipyramidal coordination environment, coordinated by three O atoms and one N atom from the pyruvic acid 2-furoic acid hydrazone ligands, one O atom from a methanol mol­ecule and two axial C atoms from trans methyl groups, thus forming a dimeric mol­ecule, which has crystallographic \overline{1} symmetry. In the dimeric structure there are also intra­molecular hydrogen bonds, which contribute to the crystal stability and compactness.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536806017612/kj2006sup1.cif
Contains datablocks I, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536806017612/kj2006Isup2.hkl
Contains datablock I

CCDC reference: 613747

Key indicators

  • Single-crystal X-ray study
  • T = 298 K
  • Mean [sigma](C-C) = 0.008 Å
  • R factor = 0.037
  • wR factor = 0.091
  • Data-to-parameter ratio = 14.1

checkCIF/PLATON results

No syntax errors found



Alert level B PLAT430_ALERT_2_B Short Inter D...A Contact O1 .. O1 .. 2.80 Ang.
Alert level C PLAT241_ALERT_2_C Check High Ueq as Compared to Neighbors for O4
0 ALERT level A = In general: serious problem 1 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 2 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

Computing details top

Data collection: SMART (Siemens, 1996); cell refinement: SMART; 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.

Bis[µ-pyruvic acid 2-furoic acid hydrazonato(2-)]bis[methanolbismethyltin(IV)] top
Crystal data top
[Sn2(CH3)4(C8H6N2O4)2(CH4O)2]F(000) = 1488
Mr = 374.95Dx = 1.752 Mg m3
Monoclinic, C2/cMo Kα radiation, λ = 0.71073 Å
Hall symbol: -C 2ycCell parameters from 2118 reflections
a = 20.794 (19) Åθ = 2.3–22.8°
b = 9.911 (9) ŵ = 1.81 mm1
c = 14.142 (13) ÅT = 298 K
β = 102.658 (15)°Block, colorless
V = 2844 (5) Å30.23 × 0.15 × 0.12 mm
Z = 8
Data collection top
Bruker SMART CCD area-detector
diffractometer
2538 independent reflections
Radiation source: fine-focus sealed tube1798 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.039
φ and ω scansθmax = 25.1°, θmin = 2.0°
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
h = 2417
Tmin = 0.680, Tmax = 0.812k = 1111
7350 measured reflectionsl = 1614
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)] = 0.037Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.091H atoms treated by a mixture of independent and constrained refinement
S = 1.00 w = 1/[σ2(Fo2) + (0.0451P)2 + 1.0171P]
where P = (Fo2 + 2Fc2)/3
2538 reflections(Δ/σ)max = 0.011
180 parametersΔρmax = 0.64 e Å3
0 restraintsΔρmin = 0.40 e Å3
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
Sn10.067287 (17)0.83762 (3)0.03589 (3)0.04206 (16)
N10.0107 (2)0.6685 (4)0.0856 (3)0.0395 (10)
N20.0426 (2)0.5493 (4)0.1158 (3)0.0428 (11)
O10.04143 (16)0.9006 (3)0.0242 (3)0.0455 (9)
O20.13657 (18)0.8428 (3)0.0614 (3)0.0556 (11)
O30.13082 (17)0.6622 (3)0.0738 (3)0.0522 (10)
O40.2064 (2)0.4381 (4)0.1163 (3)0.0724 (13)
O50.1720 (2)0.9157 (5)0.0109 (4)0.0709 (14)
C10.0791 (3)0.8192 (5)0.0564 (4)0.0422 (13)
C20.0501 (2)0.6837 (5)0.0912 (4)0.0389 (12)
C30.0898 (3)0.5816 (5)0.1295 (4)0.0536 (15)
H3A0.13090.56820.08400.080*
H3B0.09810.61240.19010.080*
H3C0.06590.49790.13950.080*
C40.1042 (3)0.5585 (5)0.1061 (4)0.0431 (13)
C50.1460 (2)0.4422 (5)0.1386 (4)0.0405 (12)
C60.1358 (3)0.3325 (5)0.1866 (4)0.0462 (14)
H60.09820.31110.20890.055*
C70.1938 (3)0.2544 (6)0.1969 (5)0.0641 (18)
H80.20190.17190.22870.077*
C80.2340 (3)0.3194 (7)0.1536 (5)0.0710 (19)
H70.27550.28900.14900.085*
C90.0925 (3)0.9279 (6)0.1719 (4)0.0590 (16)
H9A0.09871.02300.16450.089*
H9B0.13270.88890.20820.089*
H9C0.05790.91350.20590.089*
C110.2351 (3)0.9034 (7)0.0696 (5)0.081 (2)
H11A0.24920.98920.09810.121*
H11B0.26510.87360.03110.121*
H11C0.23430.83880.11990.121*
H10.164 (3)0.989 (6)0.019 (4)0.07 (2)*
C100.0477 (3)0.8044 (5)0.1142 (4)0.0567 (16)
H10A0.01890.72820.13020.085*
H10B0.08830.78690.13390.085*
H10C0.02710.88290.14740.085*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Sn10.0387 (2)0.0409 (2)0.0486 (3)0.00048 (17)0.01401 (17)0.00507 (19)
N10.043 (3)0.035 (2)0.043 (3)0.000 (2)0.015 (2)0.002 (2)
N20.038 (3)0.037 (2)0.054 (3)0.0021 (19)0.013 (2)0.009 (2)
O10.039 (2)0.040 (2)0.062 (3)0.0016 (16)0.0197 (18)0.0076 (18)
O20.040 (2)0.052 (2)0.080 (3)0.0078 (18)0.026 (2)0.021 (2)
O30.042 (2)0.046 (2)0.074 (3)0.0056 (17)0.023 (2)0.018 (2)
O40.058 (3)0.068 (3)0.100 (4)0.009 (2)0.036 (3)0.021 (3)
O50.040 (3)0.059 (3)0.114 (4)0.002 (2)0.018 (2)0.035 (3)
C10.035 (3)0.043 (3)0.049 (3)0.000 (2)0.010 (3)0.000 (3)
C20.041 (3)0.039 (3)0.037 (3)0.002 (2)0.009 (2)0.001 (2)
C30.042 (3)0.047 (3)0.075 (5)0.005 (3)0.021 (3)0.009 (3)
C40.042 (3)0.048 (3)0.042 (3)0.005 (2)0.013 (3)0.006 (3)
C50.037 (3)0.050 (3)0.035 (3)0.005 (2)0.010 (2)0.004 (3)
C60.036 (3)0.043 (3)0.059 (4)0.004 (3)0.010 (3)0.010 (3)
C70.069 (4)0.042 (4)0.078 (5)0.002 (3)0.010 (4)0.008 (3)
C80.047 (4)0.068 (5)0.097 (6)0.018 (3)0.013 (4)0.006 (4)
C90.066 (4)0.059 (4)0.050 (4)0.003 (3)0.008 (3)0.005 (3)
C110.060 (5)0.085 (5)0.097 (6)0.000 (4)0.015 (4)0.021 (5)
C100.070 (4)0.053 (4)0.051 (4)0.008 (3)0.022 (3)0.006 (3)
Geometric parameters (Å, º) top
Sn1—C92.082 (6)C3—H3A0.9600
Sn1—C102.098 (6)C3—H3B0.9600
Sn1—O32.178 (4)C3—H3C0.9600
Sn1—N12.248 (4)C4—C51.457 (7)
Sn1—O12.316 (4)C5—C61.323 (7)
Sn1—O52.409 (4)C6—C71.412 (7)
Sn1—O1i2.747 (4)C6—H60.9300
N1—C21.292 (6)C7—C81.310 (8)
N1—N21.377 (5)C7—H80.9300
N2—C41.320 (6)C8—H70.9300
O1—C11.276 (6)C9—H9A0.9600
O2—C11.235 (6)C9—H9B0.9600
O3—C41.297 (6)C9—H9C0.9600
O4—C51.361 (6)C11—H11A0.9600
O4—C81.364 (7)C11—H11B0.9600
O5—C111.396 (7)C11—H11C0.9600
O5—H10.84 (6)C10—H10A0.9600
C1—C21.509 (7)C10—H10B0.9600
C2—C31.481 (6)C10—H10C0.9600
C9—Sn1—C10163.0 (2)C2—C3—H3B109.5
C9—Sn1—O395.7 (2)H3A—C3—H3B109.5
C10—Sn1—O395.53 (19)C2—C3—H3C109.5
C9—Sn1—N194.3 (2)H3A—C3—H3C109.5
C10—Sn1—N1101.60 (19)H3B—C3—H3C109.5
O3—Sn1—N170.06 (15)O3—C4—N2126.2 (5)
C9—Sn1—O189.70 (19)O3—C4—C5117.8 (4)
C10—Sn1—O190.02 (19)N2—C4—C5115.9 (4)
O3—Sn1—O1139.69 (12)C6—C5—O4110.7 (4)
N1—Sn1—O169.71 (14)C6—C5—C4131.4 (5)
C9—Sn1—O586.8 (2)O4—C5—C4117.9 (4)
C10—Sn1—O583.3 (2)C5—C6—C7106.0 (5)
O3—Sn1—O576.92 (15)C5—C6—H6127.0
N1—Sn1—O5146.91 (15)C7—C6—H6127.0
O1—Sn1—O5143.37 (15)C8—C7—C6107.5 (5)
C9—Sn1—O1i82.67 (19)C8—C7—H8126.3
C10—Sn1—O1i81.61 (17)C6—C7—H8126.3
O3—Sn1—O1i153.79 (11)C7—C8—O4110.3 (5)
N1—Sn1—O1i136.11 (13)C7—C8—H7124.9
O1—Sn1—O1i66.51 (12)O4—C8—H7124.9
O5—Sn1—O1i76.88 (13)Sn1—C9—H9A109.5
C2—N1—N2119.6 (4)Sn1—C9—H9B109.5
C2—N1—Sn1121.2 (3)H9A—C9—H9B109.5
N2—N1—Sn1119.1 (3)Sn1—C9—H9C109.5
C4—N2—N1108.7 (4)H9A—C9—H9C109.5
C1—O1—Sn1118.1 (3)H9B—C9—H9C109.5
C4—O3—Sn1115.9 (3)O5—C11—H11A109.5
C5—O4—C8105.6 (4)O5—C11—H11B109.5
C11—O5—Sn1130.3 (4)H11A—C11—H11B109.5
C11—O5—H1115 (4)O5—C11—H11C109.5
Sn1—O5—H1106 (4)H11A—C11—H11C109.5
O2—C1—O1125.3 (5)H11B—C11—H11C109.5
O2—C1—C2118.2 (5)Sn1—C10—H10A109.5
O1—C1—C2116.5 (4)Sn1—C10—H10B109.5
N1—C2—C3124.9 (5)H10A—C10—H10B109.5
N1—C2—C1114.2 (4)Sn1—C10—H10C109.5
C3—C2—C1120.9 (4)H10A—C10—H10C109.5
C2—C3—H3A109.5H10B—C10—H10C109.5
Symmetry code: (i) x, y+2, z.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O5—H1···O2i0.84 (6)1.82 (6)2.643 (6)166 (6)
Symmetry code: (i) x, y+2, z.
 

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