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The crystal structure of the glass-forming molecular liquid triphenyl phosphite [TPP, P(OC6H5)3, six torsional degrees of freedom] has been solved ab initio at 110 K from powder synchrotron X-ray diffraction data by real-space methods (simulated annealing) followed by rigid-body Rietveld refinements. The symmetry is trigonal, with a rhombohedral lattice, space group R\bar{3}. The associated hexagonal cell, which is a sixfold multiple of the previously published less-symmetric monoclinic cell [Hédoux et al. (1999). Phys. Rev. B, 60, 9390–9395], is unusually large [V = 7075.7 (4) Å3, Z = 18] and displays a noteworthy platelet-like shape [a = 37.766 (1) and c = 5.7286 (2) Å]. The TPP molecule does not exhibit the ideal C3 symmetric propeller shape, its conformation being on the contrary almost mirror-symmetric, with the pseudo-mirror plane passing through the P—O1 bond and two carbon atoms in para position with respect to the O1 atom. The hitherto unknown topological features of crystalline TPP, including unusual intermolecular weak C—H...O hydrogen-bonding networks, are presented and discussed in the scope of the `glacial state' problem.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S0021889802000511/vi0154sup1.cif
Contains datablocks znvo, tpp110kdata

rtv

Rietveld powder data file (CIF format) https://doi.org/10.1107/S0021889802000511/vi0154sup2.rtv
Contains datablock tpp110kprofile

CCDC reference: 214221

Computing details top

Data collection: NICE; cell refinement: JANA2000; program(s) used to solve structure: DASH; program(s) used to refine structure: JANA2000; molecular graphics: CAMERON; software used to prepare material for publication: JANA2000.

Figures top
[Figure 1]
[Figure 2]
[Figure 3]
[Figure 4]
[Figure 5]
[Figure 6]
triphenyl phosphite top
Crystal data top
C18H15O3PF(000) = 2916
Mr = 310.27Dx = 1.311 Mg m3
Trigonal, R3Synchrotron radiation, λ = 0.850871 Å
a = 37.766 (1) ŵ = 0.25 mm1
c = 5.7286 (2) ÅT = 110 K
V = 7075.7 (4) Å3colourless
Z = 18cylinder, 5 × 1 mm
Data collection top
ESRF beamline BM16
diffractometer
Scan method: continuous
Radiation source: synchrotron, ESRF beamline BM16Absorption correction: for a cylinder mounted on the ϕ axis
?
Si 111 monochromatorTmin = ?, Tmax = ?
Specimen mounting: glass capillary2θmin = 1.500°, 2θmax = 45.000°, 2θstep = 0.004°
Data collection mode: transmission
Refinement top
Refinement on Inet66 parameters
Least-squares matrix: full6 restraints
Rp = 0.0474 constraints
Rwp = 0.059Only H-atom displacement parameters refined
Rexp = 0.046Weighting scheme based on measured s.u.'s
χ2 = 2.690(Δ/σ)max = 0.006
14485 data pointsBackground function: Chebyshev polynomial
Profile function: pseudo-Voigt
Crystal data top
C18H15O3PZ = 18
Mr = 310.27Synchrotron radiation, λ = 0.850871 Å
Trigonal, R3µ = 0.25 mm1
a = 37.766 (1) ÅT = 110 K
c = 5.7286 (2) Åcylinder, 5 × 1 mm
V = 7075.7 (4) Å3
Data collection top
ESRF beamline BM16
diffractometer
Absorption correction: for a cylinder mounted on the ϕ axis
?
Specimen mounting: glass capillaryTmin = ?, Tmax = ?
Data collection mode: transmission2θmin = 1.500°, 2θmax = 45.000°, 2θstep = 0.004°
Scan method: continuous
Refinement top
Rp = 0.04714485 data points
Rwp = 0.05966 parameters
Rexp = 0.0466 restraints
χ2 = 2.690Only H-atom displacement parameters refined
Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
P0.23853 (15)0.07191 (17)0.0648 (8)0.029 (3)
O30.19150 (18)0.0520 (2)0.1450 (15)0.030 (4)*
O10.2558 (3)0.1203 (2)0.0715 (16)0.043 (4)*
O20.2521 (2)0.0641 (3)0.3153 (11)0.027 (4)*
C110.24871 (12)0.14104 (11)0.2530 (8)0.011 (2)*
C120.21488 (12)0.14655 (11)0.2382 (8)0.011 (2)*
C130.20707 (12)0.16697 (11)0.4162 (8)0.011 (2)*
C140.23309 (12)0.18176 (11)0.6088 (8)0.011 (2)*
C150.26682 (12)0.17625 (11)0.6236 (8)0.011 (2)*
C160.27463 (12)0.15584 (11)0.4457 (8)0.011 (2)*
H120.19624 (12)0.13588 (11)0.1002 (8)0.052 (11)*
H130.18288 (12)0.17098 (11)0.4057 (8)0.052 (11)*
H140.22754 (12)0.19637 (11)0.7367 (8)0.052 (11)*
H150.28542 (12)0.18694 (11)0.7618 (8)0.052 (11)*
H160.29881 (12)0.15181 (11)0.4564 (8)0.052 (11)*
C210.28958 (16)0.06614 (9)0.3528 (8)0.010 (2)*
C220.32218 (16)0.08403 (9)0.1962 (8)0.010 (2)*
C230.35729 (16)0.08131 (9)0.2360 (8)0.010 (2)*
C240.35961 (16)0.06081 (9)0.4323 (8)0.010 (2)*
C250.32701 (16)0.04293 (9)0.5890 (8)0.010 (2)*
C260.29200 (16)0.04564 (9)0.5492 (8)0.010 (2)*
H220.32038 (16)0.09877 (9)0.0558 (8)0.052 (11)*
H230.38072 (16)0.09401 (9)0.1240 (8)0.052 (11)*
H240.38474 (16)0.05894 (9)0.4609 (8)0.052 (11)*
H250.32874 (16)0.02818 (9)0.7297 (8)0.052 (11)*
H260.26862 (16)0.03289 (9)0.6615 (8)0.052 (11)*
C310.16122 (10)0.04118 (13)0.0293 (7)0.013 (2)*
C320.12334 (10)0.00751 (13)0.0257 (7)0.013 (2)*
C330.09050 (10)0.00500 (13)0.1271 (7)0.013 (2)*
C340.09545 (10)0.01626 (13)0.3348 (7)0.013 (2)*
C350.13333 (10)0.05003 (13)0.3898 (7)0.013 (2)*
C360.16627 (10)0.06244 (13)0.2371 (7)0.013 (2)*
H320.11971 (10)0.00768 (13)0.1749 (7)0.052 (11)*
H330.06339 (10)0.02924 (13)0.0878 (7)0.052 (11)*
H340.07185 (10)0.00729 (13)0.4442 (7)0.052 (11)*
H350.13688 (10)0.06532 (13)0.5385 (7)0.052 (11)*
H360.19347 (10)0.08656 (13)0.2765 (7)0.052 (11)*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
P0.023 (4)0.047 (5)0.027 (3)0.026 (4)0.011 (3)0.009 (4)
Geometric parameters (Å, º) top
O3—P1.611 (8)O1—C15iii3.216 (10)
O3—O12.542 (9)O1—C153.709 (10)
O3—O22.315 (13)O1—C16iii3.769 (10)
O3—C113.015 (8)O1—C162.439 (10)
O3—C123.265 (10)O1—C213.319 (12)
O3—C14i3.990 (11)O1—C223.479 (13)
O3—C163.986 (7)O1—C313.369 (8)
O3—C213.667 (10)O1—C363.456 (9)
O3—C311.416 (8)O2—P1.601 (10)
O3—C322.365 (6)O2—O32.315 (13)
O3—C333.661 (7)O2—O12.487 (14)
O3—C353.748 (9)O2—C112.995 (14)
O3—C35ii3.431 (9)O2—C13i3.941 (9)
O3—C362.496 (10)O2—C14i3.829 (11)
O3—C36ii3.738 (10)O2—C163.216 (12)
O1—P1.605 (9)O2—C211.394 (13)
O1—O32.542 (9)O2—C222.457 (12)
O1—O22.487 (14)O2—C233.717 (13)
O1—C111.406 (11)O2—C253.654 (13)
O1—C122.411 (13)O2—C262.365 (13)
O1—C133.692 (12)O2—C313.669 (10)
O1—C14iii3.891 (11)
O2—P—O1101.8 (5)O1—C11—C16121.2 (6)
O2—P—O392.2 (5)O1—C11—C12118.8 (5)
O1—P—O3104.5 (6)O2—C21—C26116.1 (5)
C11—O1—P124.8 (6)O2—C21—C22123.6 (5)
C21—O2—P122.5 (6)O3—C31—C32114.6 (4)
C31—O3—P118.5 (6)O3—C31—C36125.3 (3)
Symmetry codes: (i) y, x+y, z+1; (ii) x, y, z+1; (iii) x, y, z1.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C15—H15···O1ii1.002.814 (9)3.216 (10)104.7 (3)
C35—H35···O3iii1.002.97 (1)3.431 (9)109.0 (3)
Symmetry codes: (ii) x, y, z+1; (iii) x, y, z1.

Experimental details

Crystal data
Chemical formulaC18H15O3P
Mr310.27
Crystal system, space groupTrigonal, R3
Temperature (K)110
a, c (Å)37.766 (1), 5.7286 (2)
V3)7075.7 (4)
Z18
Radiation typeSynchrotron, λ = 0.850871 Å
µ (mm1)0.25
Specimen shape, size (mm)Cylinder, 5 × 1
Data collection
DiffractometerESRF beamline BM16
diffractometer
Specimen mountingGlass capillary
Data collection modeTransmission
Scan methodContinuous
2θ values (°)2θmin = 1.500 2θmax = 45.000 2θstep = 0.004
Refinement
R factors and goodness of fitRp = 0.047, Rwp = 0.059, Rexp = 0.046, χ2 = 2.690
No. of data points14485
No. of parameters66
No. of restraints6
H-atom treatmentOnly H-atom displacement parameters refined

Computer programs: NICE, JANA2000, DASH, CAMERON.

Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C15—H15···O1i1.002.814 (9)3.216 (10)104.7 (3)
C35—H35···O3ii1.002.97 (1)3.431 (9)109.0 (3)
Symmetry codes: (i) x, y, z+1; (ii) x, y, z1.
 

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