research communications\(\def\hfill{\hskip 5em}\def\hfil{\hskip 3em}\def\eqno#1{\hfil {#1}}\)

Journal logoCRYSTALLOGRAPHIC
COMMUNICATIONS
ISSN: 2056-9890

Synthesis and structure of 4-[(2,3,4,5,6-penta­fluoro­phen­­oxy)carbon­yl]phenyl 4-(dodec­yl­oxy)benzoate

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aDepartment of Physics, Yuvaraja's College, University of Mysore, Mysore, Karnataka-570005, India, bDepartment of Physics, Government Science College, Chitradurga, Karnataka-577501, India, cRaman Research Institute, C. V. Raman Avenue, Sadashivanagar, Bengaluru, Karnataka-560086, India, and dDepartment of PG Studies and Research in Physics, UCS, Tumkur University, Tumkur, Karnataka-572103, India
*Correspondence e-mail: [email protected]

Edited by W. T. A. Harrison, University of Aberdeen, United Kingdom (Received 6 April 2026; accepted 14 April 2026; online 17 April 2026)

In the title compound, C32H33F5O5, the dihedral angle between the central carbonyl­pheyl and peripheral perfluoro­phen­oxy and (dodec­yloxy)benzoate rings are 85.24 (2) and 78.98 (2)ο, respectively, indicating that the central ring is almost normal to both adjacent rings. The pendant C12 alkyl chain adopts an all-anti conformation. In the crystal, weak C—H⋯O hydrogen bonds connect the mol­ecules, forming S(7) chains propagating along the [010] direction. The packing is consolidated by C—F⋯π inter­actions and weak ππ stacking. The Hirshfeld surface analysis reveals that the major contributions to the two-dimensional fingerprint plots are from H⋯H (45%),F⋯H/H⋯F (18.5%), O⋯H/H⋯O (9.7%), C⋯H/H⋯C (9.4%), F⋯C/C⋯F (7.3%), and F⋯F (1.9%) contacts. An energy framework calculation shows that dispersion energy (–383.4 kJ mol−1) makes by far the largest contribution.

1. Chemical context

Phenyl­benzoate-based three-ring calamitic liquid crystals incorporating a 4-(dodec­yloxy)benzoate terminal unit are well-established mesogens in which the dodec­yloxy chain promotes layered organization, while ester linkages preserve the required rod-like geometry (Cakar et al., 2022View full citation). The introduction of a perfluoro­phen­oxy group at the opposite terminus is expected to influence both inter­molecular inter­actions and physicochemical properties through fluorination (Ashmawy et al., 2017View full citation; Podruczna et al., 2014View full citation). Beyond their mesomorphic behaviour, derivatives bearing the 4-(dodec­yloxy)benzoate motif have attracted attention due to their biological activities. In closely related systems, structural modification of the terminal substituent and alkyl chain length has been shown to significantly affect biological performance. For instance, bis­(dodec­yloxy)benzoate–poly(amido­amine) conjugates exhibit pronounced anti­cancer activity against a range of human cancer cell lines (Castillo-Rodrez et al., 2023View full citation), while flutamide-linked 3,5-bis­(dodec­yloxy)benzoate derivatives demonstrate effective inhibition toward U-251, PC-3, K-562 and HCT-15 cell lines (Medina-Rojas et al., 2020View full citation; Lukáč et al., 2024View full citation). Similarly, incorporation of long alkyl chains in heterocyclic benzoate derivatives enhances corrosion inhibition efficiency, indicating strong surface adsorption driven by hydro­phobic inter­actions (Kadhim et al., 2023View full citation).

More generally, elongation of alkyl chains in organic mol­ecules is known to enhance lipophilicity, thereby improving membrane permeability and facilitating cellular uptake, which is a key factor in drug design. This effect has been demonstrated in several systems, including alkyl­ated caffeic acid derivatives exhibiting anti­cancer properties, cinnamic acid analogues showing anti-tuberculosis activity (De et al., 2011View full citation), and amide-based compounds with improved anti-inflammatory behaviour upon chain extension (Matta et al., 2020View full citation). In this context, the present structural study of the title compound, C32H33F5O5 (I), provides insight into the mol­ecular conformation of the C12-alkyl chain and the inter­molecular contacts governing crystal packing, which may contribute to both its mesomorphic characteristics and potential biological inter­actions (Koshti et al., 2023View full citation; Singh et al., 2016View full citation).

[Scheme 1]

2. Structural commentary

The mol­ecular structure of (I) is shown in Fig. 1[link]. The dihedral angle between the aromatic rings of the perfluoro­phen­oxy (C1–C6) and carbonyl­phenyl (C8–C13) fragments are 85.24 (2)° and the corresponding dihedral angle for the carbonyl­phenyl and (dodec­yloxy)benzoate (C15–C20) rings is 78.98 (2)°, thus, the central ring is close to normal to both peripheral rings. The torsion angles associated with the C8—C7—O1—C1 and C15—C14—O3—C11 ester linkages are 175.6 (3) and 172.2 (3)°, respectively, indicating the expected anti-periplanar conformations. The pendant C12 alkyl chain adopts an all-anti conformation with the largest torsion angle deviation from ±180° being −173.1 (4)° for C21—C22—C23—C24. Two short intra­molecular C—H⋯O contacts (Table 1[link]) are observed. Otherwise, the bond length and the bond angles may be regarded as normal.

Table 1
Hydrogen-bond geometry (Å, °)

Cg2 and Cg3 are the centroids of the C8–C13 and C15–C20 rings, respectively.

D—H⋯A D—H H⋯A DA D—H⋯A
C13—H13⋯O1 0.93 2.39 2.715 (4) 100
C16—H16⋯O3 0.93 2.42 2.730 (4) 100
C9—H9⋯O4i 0.93 2.60 3.250 (4) 128
C3—F2⋯Cg3ii 1.34 (1) 3.44 (1) 3.899 (5) 100 (1)
C5—F4⋯Cg3iii 1.33 (1) 3.18 (1) 3.604 (4) 98 (1)
C6—F5⋯Cg2iv 1.33 (1) 3.42 (1) 3.917 (4) 102 (1)
Symmetry codes: (i) Mathematical equation; (ii) Mathematical equation; (iii) Mathematical equation; (iv) Mathematical equation.
[Figure 1]
Figure 1
The mol­ecular structure of (I) showing 50% probability ellipsoids. Short intramolecular —H⋯O contacts are shown as green dashed lines.

.

3. Supra­molecular features

In the crystal, weak C9—H9⋯O4 hydrogen bonds (Table 1[link]) connect the mol­ecules into infinite S(7) chains propagating along the [010] direction as shown in Fig. 2[link]. The packing is consolidated by C—F⋯π inter­actions (Fig. 3[link], Table 1[link]) , viz.: C6—F5⋯Cg2, C3—F2⋯Cg3 and C5—F4⋯Cg3, where Cg2 and Cg3 are the centroids of the C8–C13 and C15–C20 rings, respectively. Very weak aromatic ππ stacking between pairs of Cg2 rings related by inversion symmetry with a centroid–centroid distance of 4.079 (2) Å and a slippage of 2.212 Å is also seen (Fig. 4[link]).

[Figure 2]
Figure 2
Detail of the packing of (I) showing C—H⋯O hydrogen bonds (blue dashed lines) connecting the mol­ecules into S(7) [010] chains.
[Figure 3]
Figure 3
Detail of the packing of (I) showing C—F⋯π inter­actions as blue dashed lines.
[Figure 4]
Figure 4
Detail of the packing of (I) showing aromatic ππ stacking.

4. Hirshfeld surface analysis

The Hirshfeld surface analysis was performed using CrystalExplorer (Spackman et al., 2021View full citation). Fig. 5[link] illustrates the Hirshfeld surface of (I) mapped over dnorm and shape-index. The red triangular-shaped region, if viewed normal to the centre of the carbonyl­phenyl ring indicates the existence of ππ stacking. The two-dimensional fingerprint plots (Fig. 6[link]) indicate that the major contributions to the crystal packing of (I) are from H⋯H: (45%), F⋯H/H⋯F: (18.5%), O⋯H/H⋯O: (9.7%), C⋯H/H⋯C: (9.4%), F⋯C/C⋯F: (7.3%),, F⋯F: (1.9%) contacts. Inter­action energies for (I) were computed using the basis set B3LYP\631-G(d,p) for mol­ecular pairs within a cluster of 3.8 Å radius, giving Eele = −37.6 kJ mol−1, Epol = −15.6 kJ mol−1, Edis = −383.4 kJ mol−1 and Erep = +128.4 kJ mol−1. The energy framework topologies are shown in Fig. 7[link].

[Figure 5]
Figure 5
View of the three-dimensional Hirshfeld surface of (I) plotted over (a) dnorm and (b) shape-index.
[Figure 6]
Figure 6
The two-dimensional fingerprint plots for (I) for different contact types.
[Figure 7]
Figure 7
The topology of the energy frameworks for (I) representing Coulombic, dispersion and total energy.

5. Database survey

A search of the Cambridge Structural Database (CSD version 6.01, March 2026; Groom et al., 2016View full citation) for structures containing the 4-(dodec­yloxy) benzoate moiety yielded eleven hits. Among these, five structures with CSD refcodes FOCDIN (Kanji Kubo et al., 2018View full citation), PUWDES, SANCAO and PUWREG (Dutronc et al., 2016View full citation), and TUVCAP (Cheng et al., 2010View full citation) are substituted with long alkyl chains or aromatic rings that are nearly planar, showing only slight deviations. The dihedral angles between these substituent planes and the 4-(dodec­yloxy) benzoate moiety are 82.3, 70.1, 47.5, 57.7 and 79.0°, respectively. In the title compound, the dihedral angle between the 4-(dodec­yloxy)benzoate ring and the (undecyl­oxyphen­yl)acrylate fragment is 78.98 (2)°, which lies within the range observed for related structures. However, a notable difference is observed in the torsion angle: in the reported structures, the torsion angle between the substituted oxygen atom and the adjacent atom of the almost planar fragment ranges from approximately 1° to 10°, indicating near coplanarity in those segments. In contrast, in the title compound, the torsion angle between the dodec­yloxy chain and the phenyl ring is 172.1°, indicating that these groups are nearly coplanar and adopt an anti (extended) conformation, with only a small deviation (∼8°) from the ideal 180°.

6. Synthesis and crystallization

The reaction mixture of 2,3,4,5,6-penta­fluoro­phenol (0.184 g, 1 eq) and 4-{[4-(dodec­yloxy)benzo­yl]­oxy}benzoic acid (0.426 g, 1 eq) in di­chloro­methane was stirred at room temperature overnight using a DCC esterification process in the presence of N,N-di­methyl­amino­pyrimidine as a catalyst. The insoluble byproduct of di­cyclo­hexyl urea was removed by filtration. The filtrate was washed with 5% acetic acid solution in water, and then with pure water. The filtrate was passed through silica gel, and then left for a week to grow crystals for X-ray studies. 1H NMR (500 MHz, CDCl3): δ 8.12–8.02 (m, 4H, Ar-H), 7.54 (m, 2H, Ar-H), 7.10 (d, J = 8.5 Hz, 2H, Ar-H), 4.01 (t, J = 6.5Hz, 2H, –OCH2–), 1.74–1.25 (m, 20H, CH2-alk­yl), 0.91 (t, J = 4.5Hz, 3H, –CH3) ppm. Elemental analysis (%) calculated: C, 64.86; H, 5.61; F, 16.03; found C, 64.90; H, 5.65; F, 16.09%.

7. Refinement

Crystal data, data collection and structure refinement details are summarized in Table 2[link]. All H atoms were positioned with idealized geometry and refined using a riding model with C—H = 0.93–0.97 Å and Uiso(H) = 1.2Ueq(C) or 1.5Ueq(methyl C).

Table 2
Experimental details

Crystal data
Chemical formula C32H33F5O5
Mr 592.58
Crystal system, space group Monoclinic, P21/c
Temperature (K) 297
a, b, c (Å) 25.212 (3), 8.8684 (11), 13.7665 (18)
β (°) 102.518 (4)
V3) 3004.8 (7)
Z 4
Radiation type Mo Kα
μ (mm−1) 0.11
Crystal size (mm) 0.32 × 0.27 × 0.21
 
Data collection
Diffractometer Bruker SMART APEXII CCD
Absorption correction Multi-scan (SADABS; Krause et al., 2015View full citation)
Tmin, Tmax 0.964, 0.976
No. of measured, independent and observed [I > 2σ(I)] reflections 64189, 6157, 3592
Rint 0.108
(sin θ/λ)max−1) 0.626
 
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.087, 0.216, 1.08
No. of reflections 6157
No. of parameters 379
H-atom treatment H-atom parameters constrained
Δρmax, Δρmin (e Å−3) 0.17, −0.20
Computer programs: APEX2 and SAINT (Bruker, 2017View full citation), SHELXT (Sheldrick, 2015aView full citation), SHELXL2019/3 (Sheldrick, 2015bView full citation), Mercury (Macrae et al., 2020View full citation) and publCIF (Westrip, 2010View full citation).

Supporting information


Computing details top

4-[(2,3,4,5,6-pentafluorophenoxy)carbonyl]phenyl 4-(dodecyloxy)benzoate top
Crystal data top
C32H33F5O5F(000) = 1240
Mr = 592.58Prism
Monoclinic, P21/cDx = 1.310 Mg m3
Hall symbol: -P 2ybcMo Kα radiation, λ = 0.71073 Å
a = 25.212 (3) ÅCell parameters from 3592 reflections
b = 8.8684 (11) Åθ = 2–27°
c = 13.7665 (18) ŵ = 0.11 mm1
β = 102.518 (4)°T = 297 K
V = 3004.8 (7) Å3Prism, colourless
Z = 40.32 × 0.27 × 0.21 mm
Data collection top
Bruker SMART APEXII CCD
diffractometer
6157 independent reflections
Radiation source: fine-focus sealed tube3592 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.108
Detector resolution: 1.97 pixels mm-1θmax = 26.4°, θmin = 2.8°
φ and Ω scansh = 3131
Absorption correction: multi-scan
(SADABS; Krause et al., 2015)
k = 1110
Tmin = 0.964, Tmax = 0.976l = 1717
64189 measured reflections
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)] = 0.087Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.216H-atom parameters constrained
S = 1.08 w = 1/[σ2(Fo2) + (0.0703P)2 + 1.9288P]
where P = (Fo2 + 2Fc2)/3
6157 reflections(Δ/σ)max < 0.001
379 parametersΔρmax = 0.17 e Å3
0 restraintsΔρmin = 0.20 e Å3
0 constraints
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
O20.62659 (10)0.8834 (3)0.00610 (18)0.0711 (7)
O30.39899 (9)0.7824 (3)0.11380 (17)0.0692 (7)
O10.58408 (10)0.7223 (3)0.12246 (18)0.0797 (8)
O40.43103 (11)0.6248 (3)0.2388 (2)0.0893 (9)
O50.20585 (10)0.8468 (3)0.32820 (19)0.0843 (8)
C10.62584 (15)0.7373 (4)0.1729 (3)0.0635 (9)
C20.67148 (17)0.6497 (5)0.1492 (3)0.0745 (11)
C30.71051 (16)0.6580 (5)0.2045 (3)0.0820 (12)
C40.70352 (17)0.7543 (5)0.2838 (3)0.0784 (12)
C50.65836 (16)0.8418 (4)0.3073 (3)0.0676 (10)
C60.61994 (14)0.8345 (4)0.2515 (3)0.0628 (9)
C70.58815 (15)0.8070 (4)0.0374 (2)0.0542 (8)
C80.53892 (13)0.7883 (3)0.0036 (2)0.0502 (8)
C90.53588 (13)0.8741 (4)0.0864 (2)0.0536 (8)
H90.5647250.9362440.1151610.064*
C100.49039 (14)0.8676 (4)0.1260 (2)0.0573 (9)
H100.4883600.9238810.1820600.069*
C110.44813 (14)0.7770 (4)0.0817 (2)0.0581 (9)
C120.45047 (15)0.6890 (4)0.0004 (3)0.0678 (10)
H120.4217610.6256610.0272610.081*
C130.49620 (15)0.6963 (4)0.0393 (3)0.0649 (9)
H130.4981830.6391220.0950400.078*
C140.39587 (14)0.7057 (4)0.1983 (3)0.0598 (9)
C150.34493 (13)0.7394 (4)0.2292 (2)0.0576 (8)
C160.30507 (14)0.8343 (4)0.1765 (3)0.0622 (9)
H160.3096060.8770810.1171770.075*
C170.25925 (14)0.8656 (4)0.2107 (3)0.0692 (10)
H170.2325810.9276490.1738490.083*
C180.25225 (14)0.8051 (4)0.3004 (3)0.0640 (9)
C190.29130 (15)0.7095 (5)0.3536 (3)0.0752 (11)
H190.2867060.6667330.4128780.090*
C200.33676 (15)0.6785 (4)0.3181 (3)0.0713 (10)
H200.3630310.6147700.3544620.086*
C210.20080 (16)0.8107 (5)0.4269 (3)0.0887 (13)
H21A0.2301120.8569870.4749170.106*
H21B0.2028280.7023200.4366810.106*
C220.14732 (15)0.8682 (6)0.4411 (3)0.0866 (13)
H22A0.1184630.8199030.3930570.104*
H22B0.1452540.9757240.4279450.104*
C230.13827 (16)0.8402 (6)0.5441 (3)0.0934 (14)
H23A0.1451170.7343720.5598650.112*
H23B0.1648650.8980470.5909060.112*
C240.08310 (16)0.8786 (6)0.5598 (3)0.0916 (13)
H24A0.0758180.9834540.5416950.110*
H24B0.0566750.8182290.5143870.110*
C250.07406 (17)0.8562 (6)0.6622 (3)0.0967 (14)
H25A0.0853320.7545460.6831990.116*
H25B0.0977220.9249780.7064410.116*
C260.01770 (18)0.8783 (6)0.6763 (3)0.1067 (16)
H26A0.0063870.9793610.6539210.128*
H26B0.0057020.8086030.6323630.128*
C270.00738 (18)0.8593 (6)0.7763 (3)0.1045 (16)
H27A0.0292930.9328700.8194330.125*
H27B0.0205580.7603440.8001350.125*
C280.04948 (18)0.8736 (7)0.7896 (3)0.1110 (17)
H28A0.0626710.9723980.7654820.133*
H28B0.0713450.7998240.7465270.133*
C290.06010 (19)0.8552 (7)0.8893 (4)0.1158 (18)
H29A0.0458400.7574730.9138310.139*
H29B0.0387120.9304810.9316990.139*
C300.1156 (2)0.8649 (7)0.9048 (4)0.1215 (19)
H30A0.1305300.9609620.8781940.146*
H30B0.1368080.7867710.8648140.146*
C310.1246 (3)0.8517 (8)1.0055 (5)0.152 (3)
H31A0.1080280.7579341.0329210.183*
H31B0.1045440.9326161.0444450.183*
C320.1787 (3)0.8546 (9)1.0231 (5)0.175 (3)
H32A0.1770980.8446031.0931330.263*
H32B0.1958060.9483740.9997990.263*
H32C0.1993130.7725840.9882010.263*
F50.57632 (9)0.9232 (3)0.27505 (17)0.0880 (7)
F40.65212 (11)0.9356 (3)0.38455 (17)0.0974 (8)
F30.74166 (10)0.7621 (3)0.3378 (2)0.1192 (10)
F10.67773 (12)0.5529 (3)0.07250 (18)0.1108 (9)
F20.75492 (11)0.5723 (4)0.1801 (2)0.1260 (10)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O20.0704 (16)0.0849 (18)0.0659 (16)0.0158 (14)0.0323 (13)0.0230 (14)
O30.0610 (14)0.0841 (17)0.0701 (16)0.0127 (12)0.0309 (12)0.0216 (13)
O10.0848 (18)0.101 (2)0.0663 (16)0.0254 (15)0.0441 (14)0.0310 (15)
O40.0836 (19)0.105 (2)0.092 (2)0.0353 (17)0.0459 (16)0.0468 (17)
O50.0609 (15)0.122 (2)0.0768 (18)0.0116 (15)0.0292 (13)0.0103 (16)
C10.068 (2)0.075 (2)0.054 (2)0.0108 (19)0.0287 (18)0.0192 (19)
C20.087 (3)0.085 (3)0.057 (2)0.004 (2)0.027 (2)0.003 (2)
C30.066 (2)0.097 (3)0.084 (3)0.021 (2)0.017 (2)0.013 (2)
C40.076 (3)0.101 (3)0.072 (3)0.005 (2)0.045 (2)0.017 (2)
C50.085 (3)0.072 (2)0.052 (2)0.005 (2)0.029 (2)0.0076 (19)
C60.063 (2)0.070 (2)0.058 (2)0.0012 (19)0.0206 (18)0.0172 (19)
C70.073 (2)0.0474 (18)0.0469 (19)0.0040 (17)0.0237 (17)0.0001 (15)
C80.063 (2)0.0490 (18)0.0421 (17)0.0023 (16)0.0202 (15)0.0013 (14)
C90.061 (2)0.056 (2)0.0489 (18)0.0051 (15)0.0213 (15)0.0039 (15)
C100.067 (2)0.063 (2)0.0477 (19)0.0049 (18)0.0237 (17)0.0023 (16)
C110.061 (2)0.063 (2)0.055 (2)0.0074 (18)0.0221 (17)0.0130 (17)
C120.065 (2)0.072 (2)0.071 (2)0.0114 (18)0.0229 (19)0.008 (2)
C130.075 (2)0.066 (2)0.057 (2)0.0038 (19)0.0227 (19)0.0104 (18)
C140.064 (2)0.059 (2)0.060 (2)0.0009 (18)0.0204 (18)0.0140 (18)
C150.058 (2)0.058 (2)0.060 (2)0.0003 (16)0.0205 (17)0.0056 (17)
C160.062 (2)0.073 (2)0.053 (2)0.0039 (18)0.0164 (17)0.0042 (18)
C170.054 (2)0.089 (3)0.065 (2)0.0060 (19)0.0140 (18)0.009 (2)
C180.056 (2)0.076 (2)0.064 (2)0.0037 (19)0.0223 (18)0.0016 (19)
C190.073 (3)0.090 (3)0.072 (2)0.010 (2)0.035 (2)0.018 (2)
C200.074 (2)0.077 (3)0.070 (2)0.013 (2)0.031 (2)0.017 (2)
C210.076 (3)0.115 (4)0.085 (3)0.003 (2)0.039 (2)0.006 (3)
C220.063 (2)0.120 (4)0.083 (3)0.001 (2)0.030 (2)0.004 (3)
C230.070 (3)0.131 (4)0.087 (3)0.004 (3)0.034 (2)0.003 (3)
C240.072 (3)0.123 (4)0.088 (3)0.009 (3)0.034 (2)0.005 (3)
C250.077 (3)0.138 (4)0.083 (3)0.007 (3)0.034 (2)0.008 (3)
C260.083 (3)0.156 (5)0.092 (3)0.021 (3)0.044 (3)0.021 (3)
C270.082 (3)0.150 (5)0.090 (3)0.017 (3)0.038 (3)0.017 (3)
C280.090 (3)0.155 (5)0.100 (4)0.030 (3)0.048 (3)0.026 (3)
C290.096 (3)0.162 (5)0.103 (4)0.025 (3)0.050 (3)0.031 (3)
C300.096 (3)0.160 (5)0.127 (4)0.029 (3)0.065 (3)0.027 (4)
C310.143 (5)0.195 (7)0.146 (5)0.024 (5)0.092 (4)0.032 (5)
C320.164 (6)0.211 (7)0.187 (7)0.032 (6)0.121 (5)0.050 (6)
F50.0857 (16)0.0905 (16)0.0893 (16)0.0190 (13)0.0221 (12)0.0165 (13)
F40.132 (2)0.0965 (17)0.0726 (15)0.0045 (15)0.0419 (14)0.0069 (13)
F30.1030 (19)0.162 (3)0.119 (2)0.0048 (18)0.0805 (17)0.0161 (19)
F10.144 (2)0.119 (2)0.0723 (16)0.0181 (17)0.0282 (15)0.0150 (15)
F20.0914 (19)0.154 (3)0.132 (2)0.0431 (18)0.0236 (17)0.011 (2)
Geometric parameters (Å, º) top
O2—C71.184 (4)C19—H190.9300
O3—C141.365 (4)C20—H200.9300
O3—C111.404 (4)C21—C221.494 (5)
O1—C71.376 (4)C21—H21A0.9700
O1—C11.387 (4)C21—H21B0.9700
O4—C141.182 (4)C22—C231.505 (5)
O5—C181.358 (4)C22—H22A0.9700
O5—C211.428 (4)C22—H22B0.9700
C1—C61.366 (5)C23—C241.493 (5)
C1—C21.368 (5)C23—H23A0.9700
C2—F11.344 (4)C23—H23B0.9700
C2—C31.370 (5)C24—C251.490 (5)
C3—F21.335 (4)C24—H24A0.9700
C3—C41.368 (6)C24—H24B0.9700
C4—F31.338 (4)C25—C261.488 (5)
C4—C51.358 (5)C25—H25A0.9700
C5—F41.333 (4)C25—H25B0.9700
C5—C61.362 (5)C26—C271.466 (6)
C6—F51.334 (4)C26—H26A0.9700
C7—C81.481 (4)C26—H26B0.9700
C8—C131.378 (5)C27—C281.489 (5)
C8—C91.386 (4)C27—H27A0.9700
C9—C101.374 (4)C27—H27B0.9700
C9—H90.9300C28—C291.464 (6)
C10—C111.368 (5)C28—H28A0.9700
C10—H100.9300C28—H28B0.9700
C11—C121.376 (5)C29—C301.463 (6)
C12—C131.380 (5)C29—H29A0.9700
C12—H120.9300C29—H29B0.9700
C13—H130.9300C30—C311.458 (7)
C14—C151.469 (5)C30—H30A0.9700
C15—C161.389 (5)C30—H30B0.9700
C15—C201.393 (4)C31—C321.435 (7)
C16—C171.367 (5)C31—H31A0.9700
C16—H160.9300C31—H31B0.9700
C17—C181.392 (5)C32—H32A0.9600
C17—H170.9300C32—H32B0.9600
C18—C191.382 (5)C32—H32C0.9600
C19—C201.367 (5)
C14—O3—C11118.0 (3)O5—C21—H21A110.0
C7—O1—C1116.6 (3)C22—C21—H21A110.0
C18—O5—C21117.8 (3)O5—C21—H21B110.0
C6—C1—C2119.2 (3)C22—C21—H21B110.0
C6—C1—O1119.5 (3)H21A—C21—H21B108.4
C2—C1—O1121.1 (4)C21—C22—C23113.1 (4)
C6—C1—O1119.5 (3)C21—C22—H22A109.0
C2—C1—O1121.1 (4)C23—C22—H22A109.0
F1—C2—C1119.9 (3)C21—C22—H22B109.0
F1—C2—C3119.6 (4)C23—C22—H22B109.0
C1—C2—C3120.4 (4)H22A—C22—H22B107.8
F2—C3—C4120.8 (4)C24—C23—C22115.8 (4)
F2—C3—C2119.6 (4)C24—C23—H23A108.3
C4—C3—C2119.5 (4)C22—C23—H23A108.3
F3—C4—C5120.4 (4)C24—C23—H23B108.3
F3—C4—C3119.5 (4)C22—C23—H23B108.3
C5—C4—C3120.2 (3)H23A—C23—H23B107.4
F4—C5—C4119.6 (3)C25—C24—C23116.4 (4)
F4—C5—C6120.3 (4)C25—C24—H24A108.2
C4—C5—C6120.1 (4)C23—C24—H24A108.2
F5—C6—C5119.0 (4)C25—C24—H24B108.2
F5—C6—C1120.5 (3)C23—C24—H24B108.2
C5—C6—C1120.6 (4)H24A—C24—H24B107.3
O2—C7—O1121.8 (3)C26—C25—C24116.8 (4)
O2—C7—O1121.8 (3)C26—C25—H25A108.1
O2—C7—C8127.8 (3)C24—C25—H25A108.1
O1—C7—C8110.4 (3)C26—C25—H25B108.1
O1—C7—C8110.4 (3)C24—C25—H25B108.1
C13—C8—C9120.0 (3)H25A—C25—H25B107.3
C13—C8—C7123.0 (3)C27—C26—C25118.4 (4)
C9—C8—C7116.9 (3)C27—C26—H26A107.7
C10—C9—C8120.2 (3)C25—C26—H26A107.7
C10—C9—H9119.9C27—C26—H26B107.7
C8—C9—H9119.9C25—C26—H26B107.7
C11—C10—C9119.0 (3)H26A—C26—H26B107.1
C11—C10—H10120.5C26—C27—C28118.5 (4)
C9—C10—H10120.5C26—C27—H27A107.7
C10—C11—C12122.0 (3)C28—C27—H27A107.7
C10—C11—O3119.7 (3)C26—C27—H27B107.7
C12—C11—O3118.1 (3)C28—C27—H27B107.7
C10—C11—O3119.7 (3)H27A—C27—H27B107.1
C12—C11—O3118.1 (3)C29—C28—C27118.8 (4)
C11—C12—C13118.8 (3)C29—C28—H28A107.6
C11—C12—H12120.6C27—C28—H28A107.6
C13—C12—H12120.6C29—C28—H28B107.6
C8—C13—C12120.0 (3)C27—C28—H28B107.6
C8—C13—H13120.0H28A—C28—H28B107.0
C12—C13—H13120.0C30—C29—C28120.3 (4)
O4—C14—O3121.9 (3)C30—C29—H29A107.2
O4—C14—O3121.9 (3)C28—C29—H29A107.2
O4—C14—C15126.9 (3)C30—C29—H29B107.2
O3—C14—C15111.2 (3)C28—C29—H29B107.2
O3—C14—C15111.2 (3)H29A—C29—H29B106.9
C16—C15—C20117.8 (3)C31—C30—C29119.0 (5)
C16—C15—C14123.4 (3)C31—C30—H30A107.6
C20—C15—C14118.7 (3)C29—C30—H30A107.6
C17—C16—C15120.8 (3)C31—C30—H30B107.6
C17—C16—H16119.6C29—C30—H30B107.6
C15—C16—H16119.6H30A—C30—H30B107.0
C16—C17—C18120.4 (3)C32—C31—C30120.6 (6)
C16—C17—H17119.8C32—C31—H31A107.2
C18—C17—H17119.8C30—C31—H31A107.2
O5—C18—C19125.2 (3)C32—C31—H31B107.2
O5—C18—C17115.3 (3)C30—C31—H31B107.2
C19—C18—C17119.5 (3)H31A—C31—H31B106.8
C20—C19—C18119.4 (3)C31—C32—H32A109.5
C20—C19—H19120.3C31—C32—H32B109.5
C18—C19—H19120.3H32A—C32—H32B109.5
C19—C20—C15122.0 (4)C31—C32—H32C109.5
C19—C20—H20119.0H32A—C32—H32C109.5
C15—C20—H20119.0H32B—C32—H32C109.5
O5—C21—C22108.5 (3)
C7—O1—C1—C696.2 (4)C9—C10—C11—O3172.5 (3)
C7—O1—C1—C287.9 (4)C9—C10—C11—O3172.5 (3)
C6—C1—C2—F1179.6 (3)O3—O3—C11—C100.00 (12)
O1—C1—C2—F13.6 (5)C14—O3—C11—C1079.7 (4)
O1—C1—C2—F13.6 (5)C14—O3—C11—C12105.6 (4)
C6—C1—C2—C30.8 (6)C10—C11—C12—C132.1 (5)
O1—C1—C2—C3175.1 (3)O3—C11—C12—C13172.4 (3)
O1—C1—C2—C3175.1 (3)O3—C11—C12—C13172.4 (3)
F1—C2—C3—F21.6 (6)C9—C8—C13—C120.3 (5)
C1—C2—C3—F2179.7 (4)C7—C8—C13—C12177.2 (3)
F1—C2—C3—C4178.6 (4)C11—C12—C13—C81.3 (5)
C1—C2—C3—C40.1 (6)C11—O3—C14—O47.3 (5)
F2—C3—C4—F30.2 (6)C11—O3—C14—O30 (56)
C2—C3—C4—F3179.9 (4)C11—O3—C14—C15172.2 (3)
F2—C3—C4—C5179.4 (4)O4—C14—C15—C16178.9 (4)
C2—C3—C4—C50.4 (6)O3—C14—C15—C161.6 (5)
F3—C4—C5—F40.1 (6)O3—C14—C15—C161.6 (5)
C3—C4—C5—F4179.7 (4)O4—C14—C15—C203.8 (6)
F3—C4—C5—C6179.3 (3)O3—C14—C15—C20175.6 (3)
C3—C4—C5—C60.3 (6)O3—C14—C15—C20175.6 (3)
F4—C5—C6—F50.4 (5)C20—C15—C16—C170.5 (5)
C4—C5—C6—F5179.0 (3)C14—C15—C16—C17177.8 (3)
F4—C5—C6—C1179.3 (3)C15—C16—C17—C181.3 (6)
C4—C5—C6—C11.3 (6)C21—O5—C18—C1911.1 (6)
C2—C1—C6—F5178.8 (3)C21—O5—C18—C17169.2 (3)
O1—C1—C6—F55.2 (5)C16—C17—C18—O5178.5 (3)
O1—C1—C6—F55.2 (5)C16—C17—C18—C191.8 (6)
C2—C1—C6—C51.6 (5)O5—C18—C19—C20178.9 (4)
O1—C1—C6—C5174.4 (3)C17—C18—C19—C201.4 (6)
O1—C1—C6—C5174.4 (3)C18—C19—C20—C150.5 (6)
C1—O1—C7—O23.6 (5)C16—C15—C20—C190.1 (6)
C1—O1—C7—O10 (82)C14—C15—C20—C19177.5 (4)
C1—O1—C7—C8175.6 (3)C18—O5—C21—C22179.4 (3)
O2—C7—C8—C13179.8 (3)O5—C21—C22—C23178.3 (4)
O1—C7—C8—C130.6 (5)C21—C22—C23—C24173.1 (4)
O1—C7—C8—C130.6 (5)C22—C23—C24—C25178.1 (4)
O2—C7—C8—C92.8 (5)C23—C24—C25—C26173.6 (5)
O1—C7—C8—C9176.4 (3)C24—C25—C26—C27179.2 (5)
O1—C7—C8—C9176.4 (3)C25—C26—C27—C28176.9 (5)
C13—C8—C9—C100.1 (5)C26—C27—C28—C29179.8 (5)
C7—C8—C9—C10177.2 (3)C27—C28—C29—C30178.6 (5)
C8—C9—C10—C110.9 (5)C28—C29—C30—C31177.7 (6)
C9—C10—C11—C121.9 (5)C29—C30—C31—C32177.4 (6)
Hydrogen-bond geometry (Å, º) top
Cg2 and Cg3 are the centroids of the C8–C13 and C15–C20 rings, respectively.
D—H···AD—HH···AD···AD—H···A
C13—H13···O10.932.392.715 (4)100
C16—H16···O30.932.422.730 (4)100
C9—H9···O4i0.932.603.250 (4)128
C3—F2···Cg3ii1.34 (1)3.44 (1)3.899 (5)100 (1)
C5—F4···Cg3iii1.33 (1)3.18 (1)3.604 (4)98 (1)
C6—F5···Cg2iv1.33 (1)3.42 (1)3.917 (4)102 (1)
Symmetry codes: (i) x+1, y+1/2, z+1/2; (ii) x+1, y+1, z; (iii) x+1, y+2, z; (iv) x+1, y+1/2, z1/2.
 

Acknowledgements

The authors acknowledge the Raman Research Institute, Bangalore, and Center of Innovative Science, Engineering and Education (CISEE), UCS, Tumkur University for constant support in extending the laboratory facilities. KA is thankful to BSPM's lab for use of their computing facilities at Department of PG Studies and Research in Physics, Albert Einstein Block, UCS, Tumkur University, Tumkur.

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