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, (C
12H
17)
2TeO
2 or C
24H
34O
2Te, 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
CCDC reference: 2141192
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
C24H34O2Te | Dx = 1.354 Mg m−3 |
Mr = 482.11 | Mo Kα radiation, λ = 0.71073 Å |
Orthorhombic, Pbcn | Cell parameters from 8824 reflections |
a = 9.3633 (3) Å | θ = 2.8–29.6° |
b = 14.2339 (5) Å | µ = 1.27 mm−1 |
c = 17.7479 (5) Å | T = 108 K |
V = 2365.37 (13) Å3 | Prism, clear light colourless |
Z = 4 | 0.30 × 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-1 | Rint = 0.053 |
profile data from ω–scans | θmax = 29.3°, θmin = 2.6° |
Absorption correction: multi-scan (CrysAlis PRO; Rigaku OD, 2015) | h = −12→12 |
Tmin = 0.818, Tmax = 1.000 | k = −19→16 |
21761 measured reflections | l = −22→24 |
2971 independent reflections | |
Refinement top
Refinement on F2 | 0 restraints |
Least-squares matrix: full | Hydrogen site location: inferred from neighbouring sites |
R[F2 > 2σ(F2)] = 0.025 | H-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 reflections | Δρmax = 0.54 e Å−3 |
127 parameters | Δρmin = −1.04 e Å−3 |
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 | x | y | z | Uiso*/Ueq | |
Te1 | 0.500000 | 0.53742 (2) | 0.750000 | 0.00967 (6) | |
C10 | 0.6523 (2) | 0.70236 (15) | 0.84991 (11) | 0.0158 (4) | |
H10 | 0.583709 | 0.649197 | 0.856669 | 0.019* | |
C3 | 0.8157 (2) | 0.69996 (15) | 0.62209 (12) | 0.0187 (5) | |
H3 | 0.856198 | 0.700172 | 0.573005 | 0.022* | |
C9 | 0.6527 (3) | 0.5808 (2) | 0.50988 (14) | 0.0379 (7) | |
H9A | 0.566523 | 0.619365 | 0.514888 | 0.057* | |
H9B | 0.632229 | 0.526568 | 0.477602 | 0.057* | |
H9C | 0.729227 | 0.618348 | 0.487286 | 0.057* | |
C5 | 0.7956 (2) | 0.77154 (14) | 0.74427 (13) | 0.0184 (4) | |
H5 | 0.822371 | 0.819981 | 0.778276 | 0.022* | |
C6 | 0.7021 (2) | 0.70135 (14) | 0.76827 (11) | 0.0146 (4) | |
O1 | 0.42877 (17) | 0.46605 (10) | 0.67467 (8) | 0.0171 (3) | |
C1 | 0.6651 (2) | 0.63136 (13) | 0.71543 (12) | 0.0127 (4) | |
C12 | 0.7792 (3) | 0.68515 (18) | 0.90270 (13) | 0.0250 (5) | |
H12A | 0.823966 | 0.624878 | 0.890237 | 0.038* | |
H12B | 0.745638 | 0.683768 | 0.954985 | 0.038* | |
H12C | 0.849184 | 0.735792 | 0.896628 | 0.038* | |
C7 | 0.6995 (3) | 0.54663 (16) | 0.58752 (11) | 0.0198 (5) | |
H7 | 0.622176 | 0.505677 | 0.608286 | 0.024* | |
C11 | 0.5734 (3) | 0.79367 (16) | 0.86969 (13) | 0.0247 (5) | |
H11A | 0.638093 | 0.847183 | 0.863096 | 0.037* | |
H11B | 0.541189 | 0.791052 | 0.922176 | 0.037* | |
H11C | 0.490671 | 0.801042 | 0.836407 | 0.037* | |
C2 | 0.7233 (2) | 0.62752 (15) | 0.64246 (11) | 0.0149 (4) | |
C4 | 0.8500 (2) | 0.77180 (15) | 0.67175 (13) | 0.0200 (5) | |
H4 | 0.910993 | 0.821341 | 0.655928 | 0.024* | |
C8 | 0.8368 (4) | 0.4881 (2) | 0.58284 (18) | 0.0458 (8) | |
H8A | 0.821057 | 0.434007 | 0.549748 | 0.069* | |
H8B | 0.862889 | 0.466090 | 0.633303 | 0.069* | |
H8C | 0.914138 | 0.526958 | 0.562475 | 0.069* | |
Atomic displacement parameters (Å2) top | U11 | U22 | U33 | U12 | U13 | U23 |
Te1 | 0.01162 (9) | 0.00776 (9) | 0.00963 (9) | 0.000 | 0.00042 (7) | 0.000 |
C10 | 0.0130 (10) | 0.0162 (10) | 0.0181 (10) | 0.0010 (9) | −0.0037 (8) | −0.0068 (8) |
C3 | 0.0168 (11) | 0.0198 (11) | 0.0193 (10) | −0.0030 (9) | 0.0015 (9) | 0.0047 (9) |
C9 | 0.0498 (19) | 0.0453 (16) | 0.0185 (12) | −0.0211 (14) | −0.0036 (12) | 0.0009 (11) |
C5 | 0.0163 (11) | 0.0134 (9) | 0.0254 (11) | −0.0014 (8) | −0.0067 (9) | −0.0030 (9) |
C6 | 0.0128 (10) | 0.0127 (9) | 0.0183 (10) | 0.0025 (8) | −0.0039 (8) | −0.0019 (7) |
O1 | 0.0204 (8) | 0.0156 (7) | 0.0152 (7) | −0.0051 (6) | −0.0006 (6) | −0.0054 (6) |
C1 | 0.0125 (10) | 0.0099 (9) | 0.0158 (9) | −0.0033 (8) | −0.0033 (8) | 0.0022 (8) |
C12 | 0.0223 (13) | 0.0316 (13) | 0.0211 (11) | 0.0080 (11) | −0.0076 (10) | −0.0055 (10) |
C7 | 0.0233 (12) | 0.0218 (11) | 0.0143 (10) | −0.0095 (10) | 0.0053 (9) | −0.0023 (8) |
C11 | 0.0212 (13) | 0.0249 (12) | 0.0281 (12) | 0.0057 (10) | −0.0029 (10) | −0.0116 (10) |
C2 | 0.0149 (11) | 0.0144 (10) | 0.0153 (9) | −0.0001 (9) | −0.0022 (8) | 0.0005 (8) |
C4 | 0.0141 (11) | 0.0156 (10) | 0.0302 (12) | −0.0041 (9) | −0.0040 (9) | 0.0056 (9) |
C8 | 0.0439 (18) | 0.0379 (16) | 0.0557 (19) | 0.0092 (14) | −0.0019 (15) | −0.0271 (14) |
Geometric parameters (Å, º) top
Te1—O1 | 1.8067 (14) | C5—C4 | 1.384 (3) |
Te1—O1i | 1.8067 (14) | C6—C1 | 1.411 (3) |
Te1—C1 | 2.134 (2) | C1—C2 | 1.406 (3) |
Te1—C1i | 2.134 (2) | C12—H12A | 0.9800 |
C10—H10 | 1.0000 | C12—H12B | 0.9800 |
C10—C6 | 1.522 (3) | C12—H12C | 0.9800 |
C10—C12 | 1.533 (3) | C7—H7 | 1.0000 |
C10—C11 | 1.536 (3) | C7—C2 | 1.525 (3) |
C3—H3 | 0.9500 | C7—C8 | 1.534 (4) |
C3—C2 | 1.394 (3) | C11—H11A | 0.9800 |
C3—C4 | 1.388 (3) | C11—H11B | 0.9800 |
C9—H9A | 0.9800 | C11—H11C | 0.9800 |
C9—H9B | 0.9800 | C4—H4 | 0.9500 |
C9—H9C | 0.9800 | C8—H8A | 0.9800 |
C9—C7 | 1.526 (3) | C8—H8B | 0.9800 |
C5—H5 | 0.9500 | C8—H8C | 0.9800 |
C5—C6 | 1.395 (3) | | |
| | | |
O1—Te1—O1i | 111.57 (9) | C10—C12—H12A | 109.5 |
O1—Te1—C1 | 114.02 (7) | C10—C12—H12B | 109.5 |
O1—Te1—C1i | 107.31 (7) | C10—C12—H12C | 109.5 |
O1i—Te1—C1 | 107.32 (8) | H12A—C12—H12B | 109.5 |
O1i—Te1—C1i | 114.02 (7) | H12A—C12—H12C | 109.5 |
C1—Te1—C1i | 102.40 (11) | H12B—C12—H12C | 109.5 |
C6—C10—H10 | 107.7 | C9—C7—H7 | 108.1 |
C6—C10—C12 | 110.07 (18) | C9—C7—C8 | 111.4 (2) |
C6—C10—C11 | 111.89 (18) | C2—C7—C9 | 112.27 (19) |
C12—C10—H10 | 107.7 | C2—C7—H7 | 108.1 |
C12—C10—C11 | 111.62 (18) | C2—C7—C8 | 108.77 (19) |
C11—C10—H10 | 107.7 | C8—C7—H7 | 108.1 |
C2—C3—H3 | 119.2 | C10—C11—H11A | 109.5 |
C4—C3—H3 | 119.2 | C10—C11—H11B | 109.5 |
C4—C3—C2 | 121.6 (2) | C10—C11—H11C | 109.5 |
H9A—C9—H9B | 109.5 | H11A—C11—H11B | 109.5 |
H9A—C9—H9C | 109.5 | H11A—C11—H11C | 109.5 |
H9B—C9—H9C | 109.5 | H11B—C11—H11C | 109.5 |
C7—C9—H9A | 109.5 | C3—C2—C1 | 116.79 (19) |
C7—C9—H9B | 109.5 | C3—C2—C7 | 118.92 (19) |
C7—C9—H9C | 109.5 | C1—C2—C7 | 124.15 (19) |
C6—C5—H5 | 119.4 | C3—C4—H4 | 119.9 |
C4—C5—H5 | 119.4 | C5—C4—C3 | 120.2 (2) |
C4—C5—C6 | 121.11 (19) | C5—C4—H4 | 119.9 |
C5—C6—C10 | 118.42 (18) | C7—C8—H8A | 109.5 |
C5—C6—C1 | 117.18 (19) | C7—C8—H8B | 109.5 |
C1—C6—C10 | 124.33 (19) | C7—C8—H8C | 109.5 |
C6—C1—Te1 | 115.41 (15) | H8A—C8—H8B | 109.5 |
C2—C1—Te1 | 121.42 (15) | H8A—C8—H8C | 109.5 |
C2—C1—C6 | 122.97 (19) | H8B—C8—H8C | 109.5 |
| | | |
Te1—C1—C2—C3 | 171.21 (15) | C12—C10—C6—C5 | −65.0 (3) |
Te1—C1—C2—C7 | −13.1 (3) | C12—C10—C6—C1 | 112.0 (2) |
C10—C6—C1—Te1 | 11.3 (3) | C11—C10—C6—C5 | 59.7 (3) |
C10—C6—C1—C2 | −173.9 (2) | C11—C10—C6—C1 | −123.3 (2) |
C9—C7—C2—C3 | −54.1 (3) | C2—C3—C4—C5 | 1.9 (3) |
C9—C7—C2—C1 | 130.3 (2) | C4—C3—C2—C1 | 0.8 (3) |
C5—C6—C1—Te1 | −171.71 (15) | C4—C3—C2—C7 | −175.1 (2) |
C5—C6—C1—C2 | 3.2 (3) | C4—C5—C6—C10 | 176.9 (2) |
C6—C5—C4—C3 | −2.1 (3) | C4—C5—C6—C1 | −0.4 (3) |
C6—C1—C2—C3 | −3.4 (3) | C8—C7—C2—C3 | 69.7 (3) |
C6—C1—C2—C7 | 172.3 (2) | C8—C7—C2—C1 | −106.0 (3) |
Symmetry code: (i) −x+1, y, −z+3/2. |
Hydrogen-bond geometry (Å, º) top
D—H···A | D—H | H···A | D···A | D—H···A |
C7—H7···O1 | 1.00 | 2.23 | 3.183 (3) | 158 |
C4ii—H4ii···O1 | 0.95 | 2.57 | 3.455 (3) | 155 |
C5iii—H5iii···O1 | 0.95 | 2.45 | 3.360 (3) | 160 |
Symmetry codes: (ii) x+1/2, y+1/2, −z+3/2; (iii) −x+3/2, y+1/2, z. |