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Only two crystal structures of diorganotel­lur­ones have been reported to date, both of which contain cocrystallized solvents and one of which is stabilized by intra­molecular Te—N secondary bonding interactions. This work describes the crystal structure of bis­(2,6-diiso­propyl­phen­yl) tel­lur­one, (C12H17)2TeO2 or C24H34O2Te, the first well-defined diorganotel­lur­one without cocrystallized solvents and without stabilizing intramolecular contacts. The mol­ecule has crystallographic twofold symmetry, with half the mol­ecule as the asymmetric unit. The mol­ecular structure is com­pared to previously reported tel­lur­ones and those com­puted at the density functional theory DFT/B3PW91 level. The mol­ecules form two-dimensional layers as a result of a weak inter­molecular hydrogen-bonding network. The layers are then stacked in an anti­parallel manner to form the crystal packing structure. The Hirshfeld surface analysis was employed to visualize and qu­antify the inter­molecular contacts in the mol­ecular crystal structure, and the contribution of O...H and H...H inter­actions was found to be the dominating factor.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S2053229622000353/eq3003sup1.cif
Contains datablocks 3, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2053229622000353/eq30033sup2.hkl
Contains datablock 3

CCDC reference: 2141192

Computing details top

Data collection: CrystalClear-SM Expert (Rigaku, 2011); cell refinement: CrystalClear-SM Expert (Rigaku, 2011); data reduction: CrystalClear-SM Expert (Rigaku, 2011); program(s) used to solve structure: SHELXT (Sheldrick, 2015a); program(s) used to refine structure: SHELXL2018 (Sheldrick, 2015b); molecular graphics: OLEX2 (Dolomanov et al., 2009); software used to prepare material for publication: OLEX2 (Dolomanov et al., 2009).

Bis(2,6-diisopropylphenyl) tellurone top
Crystal data top
C24H34O2TeDx = 1.354 Mg m3
Mr = 482.11Mo Kα radiation, λ = 0.71073 Å
Orthorhombic, PbcnCell parameters from 8824 reflections
a = 9.3633 (3) Åθ = 2.8–29.6°
b = 14.2339 (5) ŵ = 1.27 mm1
c = 17.7479 (5) ÅT = 108 K
V = 2365.37 (13) Å3Prism, clear light colourless
Z = 40.30 × 0.25 × 0.20 mm
F(000) = 984
Data collection top
Rigaku Saturn724+ (2x2 bin mode)
diffractometer
2348 reflections with I > 2σ(I)
Detector resolution: 28.5714 pixels mm-1Rint = 0.053
profile data from ω–scansθmax = 29.3°, θmin = 2.6°
Absorption correction: multi-scan
(CrysAlis PRO; Rigaku OD, 2015)
h = 1212
Tmin = 0.818, Tmax = 1.000k = 1916
21761 measured reflectionsl = 2224
2971 independent reflections
Refinement top
Refinement on F20 restraints
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.025H-atom parameters constrained
wR(F2) = 0.055 w = 1/[σ2(Fo2) + (0.009P)2 + 2.7225P]
where P = (Fo2 + 2Fc2)/3
S = 1.10(Δ/σ)max < 0.001
2971 reflectionsΔρmax = 0.54 e Å3
127 parametersΔρmin = 1.04 e Å3
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Te10.5000000.53742 (2)0.7500000.00967 (6)
C100.6523 (2)0.70236 (15)0.84991 (11)0.0158 (4)
H100.5837090.6491970.8566690.019*
C30.8157 (2)0.69996 (15)0.62209 (12)0.0187 (5)
H30.8561980.7001720.5730050.022*
C90.6527 (3)0.5808 (2)0.50988 (14)0.0379 (7)
H9A0.5665230.6193650.5148880.057*
H9B0.6322290.5265680.4776020.057*
H9C0.7292270.6183480.4872860.057*
C50.7956 (2)0.77154 (14)0.74427 (13)0.0184 (4)
H50.8223710.8199810.7782760.022*
C60.7021 (2)0.70135 (14)0.76827 (11)0.0146 (4)
O10.42877 (17)0.46605 (10)0.67467 (8)0.0171 (3)
C10.6651 (2)0.63136 (13)0.71543 (12)0.0127 (4)
C120.7792 (3)0.68515 (18)0.90270 (13)0.0250 (5)
H12A0.8239660.6248780.8902370.038*
H12B0.7456380.6837680.9549850.038*
H12C0.8491840.7357920.8966280.038*
C70.6995 (3)0.54663 (16)0.58752 (11)0.0198 (5)
H70.6221760.5056770.6082860.024*
C110.5734 (3)0.79367 (16)0.86969 (13)0.0247 (5)
H11A0.6380930.8471830.8630960.037*
H11B0.5411890.7910520.9221760.037*
H11C0.4906710.8010420.8364070.037*
C20.7233 (2)0.62752 (15)0.64246 (11)0.0149 (4)
C40.8500 (2)0.77180 (15)0.67175 (13)0.0200 (5)
H40.9109930.8213410.6559280.024*
C80.8368 (4)0.4881 (2)0.58284 (18)0.0458 (8)
H8A0.8210570.4340070.5497480.069*
H8B0.8628890.4660900.6333030.069*
H8C0.9141380.5269580.5624750.069*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Te10.01162 (9)0.00776 (9)0.00963 (9)0.0000.00042 (7)0.000
C100.0130 (10)0.0162 (10)0.0181 (10)0.0010 (9)0.0037 (8)0.0068 (8)
C30.0168 (11)0.0198 (11)0.0193 (10)0.0030 (9)0.0015 (9)0.0047 (9)
C90.0498 (19)0.0453 (16)0.0185 (12)0.0211 (14)0.0036 (12)0.0009 (11)
C50.0163 (11)0.0134 (9)0.0254 (11)0.0014 (8)0.0067 (9)0.0030 (9)
C60.0128 (10)0.0127 (9)0.0183 (10)0.0025 (8)0.0039 (8)0.0019 (7)
O10.0204 (8)0.0156 (7)0.0152 (7)0.0051 (6)0.0006 (6)0.0054 (6)
C10.0125 (10)0.0099 (9)0.0158 (9)0.0033 (8)0.0033 (8)0.0022 (8)
C120.0223 (13)0.0316 (13)0.0211 (11)0.0080 (11)0.0076 (10)0.0055 (10)
C70.0233 (12)0.0218 (11)0.0143 (10)0.0095 (10)0.0053 (9)0.0023 (8)
C110.0212 (13)0.0249 (12)0.0281 (12)0.0057 (10)0.0029 (10)0.0116 (10)
C20.0149 (11)0.0144 (10)0.0153 (9)0.0001 (9)0.0022 (8)0.0005 (8)
C40.0141 (11)0.0156 (10)0.0302 (12)0.0041 (9)0.0040 (9)0.0056 (9)
C80.0439 (18)0.0379 (16)0.0557 (19)0.0092 (14)0.0019 (15)0.0271 (14)
Geometric parameters (Å, º) top
Te1—O11.8067 (14)C5—C41.384 (3)
Te1—O1i1.8067 (14)C6—C11.411 (3)
Te1—C12.134 (2)C1—C21.406 (3)
Te1—C1i2.134 (2)C12—H12A0.9800
C10—H101.0000C12—H12B0.9800
C10—C61.522 (3)C12—H12C0.9800
C10—C121.533 (3)C7—H71.0000
C10—C111.536 (3)C7—C21.525 (3)
C3—H30.9500C7—C81.534 (4)
C3—C21.394 (3)C11—H11A0.9800
C3—C41.388 (3)C11—H11B0.9800
C9—H9A0.9800C11—H11C0.9800
C9—H9B0.9800C4—H40.9500
C9—H9C0.9800C8—H8A0.9800
C9—C71.526 (3)C8—H8B0.9800
C5—H50.9500C8—H8C0.9800
C5—C61.395 (3)
O1—Te1—O1i111.57 (9)C10—C12—H12A109.5
O1—Te1—C1114.02 (7)C10—C12—H12B109.5
O1—Te1—C1i107.31 (7)C10—C12—H12C109.5
O1i—Te1—C1107.32 (8)H12A—C12—H12B109.5
O1i—Te1—C1i114.02 (7)H12A—C12—H12C109.5
C1—Te1—C1i102.40 (11)H12B—C12—H12C109.5
C6—C10—H10107.7C9—C7—H7108.1
C6—C10—C12110.07 (18)C9—C7—C8111.4 (2)
C6—C10—C11111.89 (18)C2—C7—C9112.27 (19)
C12—C10—H10107.7C2—C7—H7108.1
C12—C10—C11111.62 (18)C2—C7—C8108.77 (19)
C11—C10—H10107.7C8—C7—H7108.1
C2—C3—H3119.2C10—C11—H11A109.5
C4—C3—H3119.2C10—C11—H11B109.5
C4—C3—C2121.6 (2)C10—C11—H11C109.5
H9A—C9—H9B109.5H11A—C11—H11B109.5
H9A—C9—H9C109.5H11A—C11—H11C109.5
H9B—C9—H9C109.5H11B—C11—H11C109.5
C7—C9—H9A109.5C3—C2—C1116.79 (19)
C7—C9—H9B109.5C3—C2—C7118.92 (19)
C7—C9—H9C109.5C1—C2—C7124.15 (19)
C6—C5—H5119.4C3—C4—H4119.9
C4—C5—H5119.4C5—C4—C3120.2 (2)
C4—C5—C6121.11 (19)C5—C4—H4119.9
C5—C6—C10118.42 (18)C7—C8—H8A109.5
C5—C6—C1117.18 (19)C7—C8—H8B109.5
C1—C6—C10124.33 (19)C7—C8—H8C109.5
C6—C1—Te1115.41 (15)H8A—C8—H8B109.5
C2—C1—Te1121.42 (15)H8A—C8—H8C109.5
C2—C1—C6122.97 (19)H8B—C8—H8C109.5
Te1—C1—C2—C3171.21 (15)C12—C10—C6—C565.0 (3)
Te1—C1—C2—C713.1 (3)C12—C10—C6—C1112.0 (2)
C10—C6—C1—Te111.3 (3)C11—C10—C6—C559.7 (3)
C10—C6—C1—C2173.9 (2)C11—C10—C6—C1123.3 (2)
C9—C7—C2—C354.1 (3)C2—C3—C4—C51.9 (3)
C9—C7—C2—C1130.3 (2)C4—C3—C2—C10.8 (3)
C5—C6—C1—Te1171.71 (15)C4—C3—C2—C7175.1 (2)
C5—C6—C1—C23.2 (3)C4—C5—C6—C10176.9 (2)
C6—C5—C4—C32.1 (3)C4—C5—C6—C10.4 (3)
C6—C1—C2—C33.4 (3)C8—C7—C2—C369.7 (3)
C6—C1—C2—C7172.3 (2)C8—C7—C2—C1106.0 (3)
Symmetry code: (i) x+1, y, z+3/2.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C7—H7···O11.002.233.183 (3)158
C4ii—H4ii···O10.952.573.455 (3)155
C5iii—H5iii···O10.952.453.360 (3)160
Symmetry codes: (ii) x+1/2, y+1/2, z+3/2; (iii) x+3/2, y+1/2, z.
 

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