Literature DB >> 22259496

Chlorido{2-[(dimethyl-amino)-meth-yl]phenyl-κN,C}tellurium.

Prakul Rakesh, Harkesh B Singh, Ray J Butcher.   

Abstract

The crystal structure of the title compound, C(9)H(12)ClNTe, contains isolated mol-ecules with no close TeCl inter-molecular contacts and has the same composition as a previously published structure [Engman et al. (2004 ▶). Phospho-rus Sulfur Silicon Relat. Elem.179, 285-292]. However, in this case, the compound has crystallized in a centrosymmetric space group, unlike the previously published structure which contained enanti-omerically pure chiral mol-ecules. In all other aspects, the metrical parameters are similar. The mol-ecules with a T-shaped coordination environment about the Te atom are linked into dimers by C-H⋯Cl inter-actions.

Entities:  

Year:  2011        PMID: 22259496      PMCID: PMC3254548          DOI: 10.1107/S1600536811054328

Source DB:  PubMed          Journal:  Acta Crystallogr Sect E Struct Rep Online        ISSN: 1600-5368


Related literature

For a related structure, see: Engman et al. (2004 ▶). For related syntheses, see: Singh et al. (1990 ▶); Kaur et al. (1995 ▶).

Experimental

Crystal data

C9H12ClNTe M = 297.25 Monoclinic, a = 6.4514 (6) Å b = 7.0287 (7) Å c = 23.847 (2) Å β = 95.967 (9)° V = 1075.49 (17) Å3 Z = 4 Mo Kα radiation μ = 2.96 mm−1 T = 295 K 0.45 × 0.36 × 0.12 mm

Data collection

Oxford Diffraction Xcalibur Ruby Gemini diffractometer Absorption correction: multi-scan (CrysAlis PRO; Oxford Diffraction, 2007 ▶) T min = 0.504, T max = 1.000 7778 measured reflections 3587 independent reflections 2998 reflections with I > 2σ(I) R int = 0.023

Refinement

R[F 2 > 2σ(F 2)] = 0.043 wR(F 2) = 0.096 S = 1.20 3587 reflections 111 parameters H-atom parameters constrained Δρmax = 2.25 e Å−3 Δρmin = −0.98 e Å−3 Data collection: CrysAlis PRO (Oxford Diffraction, 2007 ▶); cell refinement: CrysAlis PRO; data reduction: CrysAlis PRO; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: XP in SHELXTL (Sheldrick, 2008 ▶); software used to prepare material for publication: SHELXTL. Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536811054328/pk2376sup1.cif Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811054328/pk2376Isup2.hkl Additional supplementary materials: crystallographic information; 3D view; checkCIF report
C9H12ClNTeF(000) = 568
Mr = 297.25Dx = 1.836 Mg m3
Monoclinic, P21/nMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ynCell parameters from 3931 reflections
a = 6.4514 (6) Åθ = 5.1–32.6°
b = 7.0287 (7) ŵ = 2.96 mm1
c = 23.847 (2) ÅT = 295 K
β = 95.967 (9)°Irregular plate, pale yellow
V = 1075.49 (17) Å30.45 × 0.36 × 0.12 mm
Z = 4
Oxford Diffraction Xcalibur Ruby Gemini diffractometer3587 independent reflections
Radiation source: fine-focus sealed tube2998 reflections with I > 2σ(I)
graphiteRint = 0.023
Detector resolution: 10.5081 pixels mm-1θmax = 32.7°, θmin = 5.1°
ω scansh = −9→9
Absorption correction: multi-scan (CrysAlis PRO; Oxford Diffraction, 2007)k = −6→10
Tmin = 0.504, Tmax = 1.000l = −35→34
7778 measured reflections
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.043Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.096H-atom parameters constrained
S = 1.20w = 1/[σ2(Fo2) + (0.0327P)2 + 1.2847P] where P = (Fo2 + 2Fc2)/3
3587 reflections(Δ/σ)max = 0.001
111 parametersΔρmax = 2.25 e Å3
0 restraintsΔρmin = −0.98 e Å3
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.
xyzUiso*/Ueq
Te0.58681 (4)0.01772 (4)0.423777 (10)0.03896 (9)
Cl0.29601 (17)−0.23269 (17)0.41307 (5)0.0537 (3)
N0.8374 (5)0.2560 (4)0.41417 (13)0.0372 (6)
C10.5512 (6)0.0787 (5)0.33640 (14)0.0347 (7)
C20.3769 (6)0.0346 (6)0.29976 (16)0.0413 (8)
H2A0.2649−0.02910.31270.050*
C30.3712 (7)0.0865 (7)0.24370 (18)0.0505 (10)
H3A0.25430.05710.21900.061*
C40.5367 (8)0.1816 (6)0.22353 (17)0.0515 (10)
H4A0.53110.21540.18570.062*
C50.7099 (7)0.2255 (5)0.26028 (16)0.0456 (9)
H5A0.82120.28990.24710.055*
C60.7191 (6)0.1741 (5)0.31665 (15)0.0366 (7)
C70.9058 (6)0.2144 (6)0.35786 (15)0.0416 (8)
H7A0.99820.10520.36040.050*
H7B0.98160.32250.34500.050*
C80.7367 (8)0.4460 (6)0.4157 (2)0.0588 (12)
H8A0.83730.54330.41040.088*
H8B0.68370.46360.45150.088*
H8C0.62400.45390.38610.088*
C91.0127 (6)0.2409 (7)0.45859 (18)0.0538 (11)
H9A1.11190.33970.45370.081*
H9B1.07860.11910.45620.081*
H9C0.96200.25390.49480.081*
U11U22U33U12U13U23
Te0.03675 (13)0.04765 (15)0.03311 (13)0.00064 (11)0.00659 (8)0.00140 (11)
Cl0.0484 (5)0.0601 (6)0.0536 (6)−0.0112 (5)0.0102 (4)0.0036 (5)
N0.0340 (14)0.0375 (15)0.0403 (16)0.0027 (12)0.0043 (12)−0.0043 (13)
C10.0397 (17)0.0331 (15)0.0320 (16)0.0061 (14)0.0069 (13)−0.0021 (13)
C20.0409 (18)0.0428 (19)0.0399 (19)0.0057 (16)0.0039 (14)−0.0059 (16)
C30.057 (2)0.050 (2)0.042 (2)0.014 (2)−0.0078 (18)−0.0079 (18)
C40.079 (3)0.039 (2)0.0348 (19)0.010 (2)0.0016 (19)0.0035 (16)
C50.066 (3)0.0367 (18)0.0357 (19)−0.0026 (18)0.0112 (17)0.0009 (15)
C60.0438 (18)0.0320 (16)0.0348 (17)−0.0002 (14)0.0071 (14)−0.0014 (14)
C70.0404 (18)0.049 (2)0.0364 (18)−0.0033 (16)0.0097 (14)−0.0003 (16)
C80.071 (3)0.043 (2)0.061 (3)0.007 (2)0.000 (2)−0.012 (2)
C90.042 (2)0.074 (3)0.043 (2)−0.007 (2)−0.0038 (17)−0.004 (2)
Te—C12.116 (3)C4—H4A0.9300
Te—N2.355 (3)C5—C61.387 (5)
Te—Cl2.5657 (11)C5—H5A0.9300
N—C91.471 (5)C6—C71.500 (5)
N—C71.486 (5)C7—H7A0.9700
N—C81.487 (5)C7—H7B0.9700
C1—C21.385 (5)C8—H8A0.9600
C1—C61.397 (5)C8—H8B0.9600
C2—C31.383 (6)C8—H8C0.9600
C2—H2A0.9300C9—H9A0.9600
C3—C41.387 (7)C9—H9B0.9600
C3—H3A0.9300C9—H9C0.9600
C4—C51.382 (6)
C1—Te—N76.45 (13)C6—C5—H5A119.8
C1—Te—Cl92.14 (10)C5—C6—C1119.7 (4)
N—Te—Cl168.59 (8)C5—C6—C7122.4 (3)
C9—N—C7111.0 (3)C1—C6—C7117.9 (3)
C9—N—C8110.7 (3)N—C7—C6109.6 (3)
C7—N—C8111.7 (3)N—C7—H7A109.7
C9—N—Te111.3 (3)C6—C7—H7A109.7
C7—N—Te102.7 (2)N—C7—H7B109.7
C8—N—Te109.3 (3)C6—C7—H7B109.7
C2—C1—C6120.1 (3)H7A—C7—H7B108.2
C2—C1—Te125.0 (3)N—C8—H8A109.5
C6—C1—Te114.9 (3)N—C8—H8B109.5
C3—C2—C1119.3 (4)H8A—C8—H8B109.5
C3—C2—H2A120.4N—C8—H8C109.5
C1—C2—H2A120.4H8A—C8—H8C109.5
C2—C3—C4121.2 (4)H8B—C8—H8C109.5
C2—C3—H3A119.4N—C9—H9A109.5
C4—C3—H3A119.4N—C9—H9B109.5
C5—C4—C3119.3 (4)H9A—C9—H9B109.5
C5—C4—H4A120.4N—C9—H9C109.5
C3—C4—H4A120.4H9A—C9—H9C109.5
C4—C5—C6120.5 (4)H9B—C9—H9C109.5
C4—C5—H5A119.8
C1—Te—N—C9−152.7 (3)C2—C3—C4—C5−0.2 (6)
Cl—Te—N—C9−154.3 (3)C3—C4—C5—C60.4 (6)
C1—Te—N—C7−33.9 (2)C4—C5—C6—C1−0.5 (6)
Cl—Te—N—C7−35.5 (5)C4—C5—C6—C7178.5 (4)
C1—Te—N—C884.8 (3)C2—C1—C6—C50.3 (5)
Cl—Te—N—C883.2 (5)Te—C1—C6—C5−178.4 (3)
N—Te—C1—C2−160.8 (3)C2—C1—C6—C7−178.7 (3)
Cl—Te—C1—C218.9 (3)Te—C1—C6—C72.6 (4)
N—Te—C1—C617.8 (2)C9—N—C7—C6163.4 (3)
Cl—Te—C1—C6−162.5 (3)C8—N—C7—C6−72.6 (4)
C6—C1—C2—C3−0.1 (5)Te—N—C7—C644.4 (3)
Te—C1—C2—C3178.4 (3)C5—C6—C7—N145.9 (3)
C1—C2—C3—C40.0 (6)C1—C6—C7—N−35.1 (5)
D—H···AD—HH···AD···AD—H···A
C9—H9C···Cli0.962.893.822 (5)163.
Table 1

Selected bond lengths (Å)

Te—C12.116 (3)
Te—N2.355 (3)
Te—Cl2.5657 (11)
Table 2

Hydrogen-bond geometry (Å, °)

D—H⋯AD—HH⋯ADAD—H⋯A
C9—H9C⋯Cli0.962.893.822 (5)163

Symmetry code: (i) .

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