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Crystal structures of 3,4,5-tri­phenyl­toluene and 3,4,5-tri­phenyl­benzyl bromide

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aInstitut für Organische Chemie, Technische Universität Bergakademie Freiberg, Leipziger Str. 29, D-09596 Freiberg/Sachsen, Germany
*Correspondence e-mail: [email protected]

Edited by J. Reibenspies, Texas A & M University, USA (Received 16 June 2025; accepted 18 July 2025; online 31 July 2025)

This article describes the crystal structures of 3,4,5-tri­phenyl­toluene, C25H20 (1), and 3,4,5-tri­phenyl­benzyl bromide, C25H19Br (2), which represent two inter­mediates of a multistep synthesis of a phenyl­acetic acid derivative. Compound 1 crystallizes from methanol in two polymorphic forms, with the space groups P2/n (1a) and P21/c (1b). In both cases, van der Waals forces significantly contribute to the cohesion of the crystal structure and the two polymorphs are characterized by similar modes of mol­ecular inter­connection. Compound 2 crystallizes from n-hexane in the space group P1, showing a similar pattern of noncovalent inter­actions to 1a and 1b. In all reported structures, the aromatic framework of the mol­ecules adopts a paddlewheel-like conformation.

1. Chemical context

3,4,5-Tri­phenyl­toluene (1) and 3,4,5-tri­phenyl­benzyl bromide (2) are inter­mediates of a multistep synthesis of 2-(3,4,5-tri­phenyl­phen­yl)acetic acid, which we have recently described (Mazik & Seidel, 2024[Mazik, M. & Seidel, P. (2024). Molbank 2024, M1837.]; Seidel et al., 2024[Seidel, P., Gottwald, F., Meier, E. & Mazik, M. (2024). Acta Cryst. E80, 1198-1201.]). Phenyl­acetic acid and its derivatives are versatile organic compounds, with a variety of valuable properties, including inter­esting biological activities (Cook, 2019[Cook, S. D. (2019). Plant Cell Physiol. 60, 243-254.]; Jiao et al., 2022[Jiao, M., He, W., Ouyang, Z., Shi, Q. & Wen, Y. (2022). Front. Microbiol. 13, 964019-964036.]; Perez et al., 2023[Perez, V. C., Zhao, H., Lin, M. & Kim, J. (2023). Plants 12, 266.]). For example, anti-cancer effects can be attributed to 3,4-di­hydroxy­phenyl­acetic acid (Gao et al., 2006[Gao, K., Xu, A., Krul, C., Venema, K., Liu, Y., Niu, Y., Lu, J., Bensoussan, L., Seeram, N. P., Heber, D. & Henning, S. M. (2006). J. Nutr. 136, 52-57.]), which is a metab­olite of the neurotransmitter dopamine and other compounds such as rutin (Olthof et al., 2003[Olthof, M. R., Hollman, P. C. H., Buijsman, M. N. C. P., van Amelsvoort, J. M. M. & Katan, M. B. (2003). J. Nutr. 133, 1806-1814.]), a flavonoid with a diverse pharmacological spectrum (Agrawal et al., 2021[Agrawal, P. K., Agrawal, C. & Blunden, G. (2021). Nat. Prod. Commun. 16, 1-12.]; Mazik, 2022[Mazik, M. (2022). ChemMedChem 17, e202200157.]). Furthermore, it should be mentioned that phenyl­acetic acid is a building block of many well-known medicines, including ibuprofen, diclofenac and flurbiprofen. In addition, phenyl­acetic acid and its derivatives are starting materials for the synthesis of a large number of pharmaceuticals (Vardanyan & Hruby, 2006[Vardanyan, R. S. & Hruby, V. J. (2006). Synthesis of Essential Drugs pp. 19-55. Amsterdam: Elsevier.]). Examples include bendazole, camylofin, triafungin, phenacenide, lorcainide, phenindione, cyclo­pentolate and penicillin.

[Scheme 1]

The aforementioned 2-(3,4,5-tri­phenyl­phen­yl)acetic acid and its amide 2-(3,4,5-tri­phenyl­phen­yl)acetamide were synthesized by us as part of studies to develop new anti­carcinogenic substances. In this paper we describe the crystal structures of compounds 1 and 2. Inter­estingly, two polymorphic forms were found in the case of 3,4,5-tri­phenyl­toluene (1).

2. Structural commentary

3,4,5-Tri­phenyl­toluene (1) crystallizes in two different forms, denoted as 1a and 1b. Recrystallization of the compound from methanol yielded colorless blocks of the monoclinic space group P2/n with one mol­ecule in the asymmetric unit of the cell (1a, see Fig. 1[link]a). Leaving the mother liquor to cool further lead to the crystallization of the second polymorphic form (1b) in the space group P21/c with two independent mol­ecules in the asymmetric unit of the cell (mol­ecules I and II, see Fig. 1[link]b).

[Figure 1]
Figure 1
Perspective view of the independent mol­ecules in structures (a) 1a and (b) 1b including atom labelling and ring specification. Displacement ellipsoids are shown at the 50% probability level.

Despite these symmetry-related differences, the conformations of the mol­ecules in both crystal structures are similar. In the case of polymorph 1a, the three phenyl rings (BD) are inclined at angles of 40.0 (1), 65.0 (1) and 47.6 (1)° with respect to the plane of the central arene ring (A). In the crystal of polymorph 1b, the analogous angles amount to 57.2 (1)/49.3 (1), 63.9 (1)/63.4 (1) and 60.2 (1)/59.2 (1)° for mol­ecules I and II, respectively, giving rise to a paddlewheel-like arrangement of phenyl groups around the central arene ring.

Crystals of 3,4,5-tri­phenyl­benzyl bromide (2) exhibit the space group PMathematical equation and contain one mol­ecule in the asymmetric unit of the cell (see Fig. 2[link]). In this structure, the phenyl ring labelled C is disordered over two positions with an approximate 50:50 occupancy. Both disordered positions are characterized by similar tilt angles relative to the central arene ring, being 61.6 (3) and 60.7 (3)°. The inclination angles of rings B and D relative to the central ring (A) are 58.2 (1) and 55.2 (1)°, respectively, so that the mol­ecular conformation once again resembles a paddlewheel. The torsion angle given by the atomic sequence C2—C1—C7—Br1 is 95.2 (2)°.

[Figure 2]
Figure 2
Perspective view of the mol­ecular structure of 2, with displacement ellipsoids representing the 50% probability level. The ring denoted C is disordered over two positions, whereby the minor component is displayed in gray and without labeling.

3. Supra­molecular features

The two polymorphs of compound 1 are characterized by similar modes of mol­ecular inter­connection, since short directional inter­actions are limited to a few C—H⋯π bonds (see Table 1[link]). In 1a this kind of inter­action {d[H7ACg(D)] = 2.87 Å, C—H⋯Cg = 134°; d[H19⋯Cg(B)] = 2.97 Å, C—H⋯Cg = 145°} generates mono-periodic supra­molecular networks extending parallel to the crystallographic b-axis, as shown in Fig. 3[link]. Since no directional inter­molecular inter­actions between these 1D aggregates are observed, van der Waals forces contribute significantly to the cohesion of the crystal structure.

Table 1
Geometric data (A, °) of inter­molecular inter­actions

Cg denotes the centers of gravity of aromatic rings corresponding to the following atoms: A′: C26–C31; B: C8–C13; B′: C33–C38; C: C14–C19; D: C20–C25.

C—H⋯Br/Cg C—H H⋯Br/Cg C⋯Br/Cg C—H⋯Br/Cg
1a        
C7—H7ACg(D)i 0.98 2.87 3.625 (1) 134
C13—H13⋯Cg(C)ii 0.95 2.97 3.536 (1) 120
C19—H19⋯Cg(B)iii 0.95 2.97 3.790 (1) 145
         
1b        
C46—H46⋯Cg(A′)iv 0.95 2.98 3.931 (1) 176
C50—H50⋯Cg(B′)v 0.95 2.91 3.631 (1) 134
         
2        
C6—H6⋯Br1vi 0.95 3.11a 4.045 (2) 170
C7—H7ACg(B)vii 0.99 2.81 3.608 (2) 138
C12—H12⋯Cg(D)viii 0.95 3.03a 3.846 (2) 144
Note: (a) distances slightly above commonly employed thresholds (H⋯Br: 3.05 Å, H⋯Cg: 3.00 Å; Bondi, 1964[Bondi, A. (1964). J. Phys. Chem. 68, 441-451.]). Symmetry codes: (i) −x + 1, −y + 1, −z + 1; (ii) x, y, z (intra); (iii) x, y + 1, z; (iv) −x, −y + 1, −z; (v) −x, −y + 1, −z + 1; (vi) −x + 2, −y + 1, −z; (vii) −x + 1, −y + 2, −z; (viii) x − 1, y + 1, z.
[Figure 3]
Figure 3
Motif in the crystal structure of 1a showing the mode of noncovalent inter­molecular bonding. Hydrogen atoms excluded from noncovalent bonding are omitted for clarity.

Similarly, in the crystal structure of the second polymorph of compound 1 (polymorph 1b), the two crystallographically non-equivalent mol­ecules form linear chain-like aggregates in which the mol­ecules are linked by weak C—H⋯π contacts, as shown in Fig. 4[link] for mol­ecule II {d[H46⋯Cg(A′)] = 2.98 Å, C—H⋯Cg = 176°; d[H50⋯Cg(B′)] = 2.91 Å, C—H⋯Cg = 134°}. The aggregates formed by mol­ecules I and II are structurally similar, each running along the c-axis direction. Since no further directional inter­actions are observed in the crystal structure of this polymorph, van der Waals forces are also likely to contribute significantly to its cohesion. Packing differences between the two polymorphs are illustrated in Fig. 5[link].

[Figure 4]
Figure 4
Supra­molecular chains in the crystal structure 1b. Hydrogen atoms excluded from noncovalent inter­molecular bonding are omitted for clarity.
[Figure 5]
Figure 5
Excerpt of the packing in the crystal structure of (a) 1a and (b) 1b viewed along the crystallographic b- and c-axis directions, respectively. In the latter case, the structure domains formed by crystallographically non-equivalent mol­ecules I and II are highlighted by different colors. All hydrogen atoms are omitted for clarity.

The presence of the additional Br atom in the crystal structure of 2 has little effect on the mode of inter­molecular association. As shown in Fig. 6[link] and Table 1[link], the crystal structure contains a single short contact, H7ACg(B) (d = 2.81 Å, C—H⋯Cg = 138°), grouping mol­ecules into pairs. Other linkage patterns are characterized by distances larger than the van der Waals criterion [e.g. H12⋯Cg(D)]. The same applies to the Br atom, for which the closest neighbour (H6) is located at a distance of 3.11 Å. Although the geometry is almost linear (C—H⋯Br = 170°), the contact distance is slightly above the sum of the van der Waals radii according to Bondi (3.05 Å; Bondi, 1964[Bondi, A. (1964). J. Phys. Chem. 68, 441-451.]). The corresponding packing diagram is shown in Fig. 7[link].

[Figure 6]
Figure 6
Mode of hydrogen bonding in the crystal structure of 2. Only the major disorder component of ring C is shown. Orange contacts slightly exceed the sum of the van der Waals radii.
[Figure 7]
Figure 7
Packing diagram of 2 viewed along the crystallographic b-axis direction. Only the major component of the disordered arene ring C is shown. All hydrogen atoms are omitted for clarity.

4. Database survey

A search conducted in the Cambridge Structural Database (CSD, Version 5.46, updated November 2024; Groom et al., 2016[Groom, C. R., Bruno, I. J., Lightfoot, M. P. & Ward, S. C. (2016). Acta Cryst. B72, 171-179.]) for methyl and halogenomethyl benzene derivatives with one to five phenyl substituents on the benzene ring only revealed the crystal structure of 1-methyl-2,3,4,5,6-penta­phenyl­benzene (PUNVAW; Gagnon et al., 2010[Gagnon, E., Maris, T., Arseneault, P.-M., Maly, K. E. & Wuest, J. D. (2010). Cryst. Growth Des. 10, 648-657.]). Crystallographic studies have been published for methyl and halogenomethyl benzenes with fewer than five phenyl substituents, but the structures most similar to 1 or 2 are not published in the CSD database (for example, 5′-methyl-1,1′:3′,1′′-terphenyl; Hofer & Peebles, 1951[Hofer, L. J. E. & Peebles, W. C. (1951). Anal. Chem. 23, 690-695.]).

The structure PUNVAW is a solvate structure with two mol­ecules of 1-methyl-2,3,4,5,6-penta­phenyl­benzene in two different conformations and half a benzene mol­ecule in the asymmetric unit. The phenyl substituents on the central benzene ring of all host mol­ecules exhibit a paddlewheel arrangement, which is typical for such systems and also occurs in both 1 and 2. The conformations differ in the arrangement of the phenyl substituents relative to the plane of the central benzene ring. While the basic sense of rotation remains the same, the substituents are arranged more steeply in one conformation than in the other. The crystal structure is mainly characterized by C—H⋯π inter­actions involving the phenyl substituents in positions 1, 2 and 3, or 1 and 3, respectively, of the central benzene ring.

The mol­ecules of one conformer are additionally linked by a C—H⋯π inter­action between the central benzene ring and a phenyl substituent of a second mol­ecule. The remaining substituents participate only in intra­molecular C-H⋯π inter­actions. This also applies to the methyl group, which exerts no discernible influence on the packing. Only a weak van der Waals inter­action with the enclosed solvent is likely.

5. Synthesis and crystallization

Compounds 1 and 2 were prepared as previously described (Mazik & Seidel, 2024[Mazik, M. & Seidel, P. (2024). Molbank 2024, M1837.]). Recrystallization of 1 from methanol yielded polymorph 1a, while polymorph 1b slowly crystallized from the respective mother liquor after further cooling. Crystals of 2 were acquired through recrystallization from n-hexane.

6. Refinement

Crystal data, data collection and structure refinement details are summarized in Table 2[link]. All non-hydrogen atoms were refined anisotropically, while hydrogen atoms were positioned geometrically and refined isotropically using a riding model [Uiso(Harene) = Uiso(Hmethyl­ene) = 1.2 Ueq(C); Uiso(Hmeth­yl) = 1.5 Ueq(C)]. C—H bond distances were set to 0.95 Å (arene), 0.98 Å (meth­yl) and 0.99 Å (methyl­ene), respectively.

Table 2
Experimental details

  1a 1b 2
Crystal data
Chemical formula C25H20 C25H20 C25H19Br
Mr 320.41 320.41 399.31
Crystal system, space group Monoclinic, P2/n Monoclinic, P21/c Triclinic, PMathematical equation
Temperature (K) 163 123 193
a, b, c (Å) 17.0701 (8), 6.0801 (2), 17.4451 (8) 19.9859 (6), 19.9669 (7), 9.2138 (3) 10.0859 (6), 10.2444 (7), 11.3564 (7)
α, β, γ (°) 90, 98.933 (4), 90 90, 94.073 (2), 90 65.309 (5), 76.095 (5), 66.367 (5)
V3) 1788.63 (13) 3667.5 (2) 972.95 (12)
Z 4 8 2
Radiation type Mo Kα Mo Kα Mo Kα
μ (mm−1) 0.07 0.07 2.12
Crystal size (mm) 0.22 × 0.12 × 0.06 × 0.09 (radius) 0.2 × 0.19 × 0.18 × 0.16 (radius) 0.50 × 0.40 × 0.25
 
Data collection
Diffractometer Stoe Stadivari Stoe Stadivari Stoe IPDS 2T
Absorption correction Multi-scan (LANA; Stoe & Cie, 2024a[Stoe & Cie (2024a). LANA. Stoe & Cie, Darmstadt, Germany.]) Multi-scan (LANA; Stoe & Cie, 2024a[Stoe & Cie (2024a). LANA. Stoe & Cie, Darmstadt, Germany.]) Integration [X-SHAPE (Stoe & Cie, 2021[Stoe & Cie (2021). X-SHAPE. Stoe & Cie, Darmstadt, Germany.]) and X-RED32 (Stoe & Cie, 2023[Stoe & Cie (2023). X-RED32. Stoe & Cie, Darmstadt, Germany.])]
Tmin, Tmax 0.956, 0.991 0.959, 0.965 0.617, 0.813
No. of measured, independent and observed [I > 2σ(I)] reflections 36658, 4524, 3319 50810, 7601, 6404 22755, 4702, 4072
Rint 0.038 0.025 0.033
(sin θ/λ)max−1) 0.671 0.628 0.660
 
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.043, 0.114, 1.04 0.041, 0.109, 1.05 0.028, 0.069, 1.06
No. of reflections 4524 7601 4702
No. of parameters 227 453 290
No. of restraints 0 0 84
H-atom treatment H-atom parameters constrained H-atom parameters constrained H-atom parameters constrained
Δρmax, Δρmin (e Å−3) 0.24, −0.23 0.28, −0.25 0.41, −0.38
Computer programs: X-AREA (including Recipe and Integrate) (Stoe & Cie, 2024b[Stoe & Cie (2024b). X-AREA. Stoe & Cie, Darmstadt, Germany.]), X-RED32 (Stoe & Cie, 2023[Stoe & Cie (2023). X-RED32. Stoe & Cie, Darmstadt, Germany.]), SHELXT2018/2 (Sheldrick, 2015a[Sheldrick, G. M. (2015a). Acta Cryst. A71, 3-8.]), SHELXL2019/3 (Sheldrick, 2015b[Sheldrick, G. M. (2015b). Acta Cryst. C71, 3-8.]) OLEX2 (Dolomanov et al., 2009[Dolomanov, O. V., Bourhis, L. J., Gildea, R. J., Howard, J. A. K. & Puschmann, H. (2009). J. Appl. Cryst. 42, 339-341.]), XP in SHELXTL (Sheldrick, 2008[Sheldrick, G. M. (2008). Acta Cryst. A64, 112-122.]), ORTEP-3 for Windows (Farrugia, 2012[Farrugia, L. J. (2012). J. Appl. Cryst. 45, 849-854.]) and publCIF (Westrip 2010[Westrip, S. P. (2010). J. Appl. Cryst. 43, 920-925.]).

Supporting information


Computing details top

5-Methyl-1,2,3-triphenylbenzene (1a) top
Crystal data top
C25H20F(000) = 680
Mr = 320.41Dx = 1.190 Mg m3
Monoclinic, P2/nMo Kα radiation, λ = 0.71073 Å
a = 17.0701 (8) ÅCell parameters from 27898 reflections
b = 6.0801 (2) Åθ = 1.8–30.8°
c = 17.4451 (8) ŵ = 0.07 mm1
β = 98.933 (4)°T = 163 K
V = 1788.63 (13) Å3Block, colourless
Z = 40.22 × 0.12 × 0.06 × 0.09 (radius) mm
Data collection top
Stoe Stadivari
diffractometer
3319 reflections with I > 2σ(I)
Detector resolution: 5.81 pixels mm-1Rint = 0.038
rotation method, ω scansθmax = 28.5°, θmin = 2.4°
Absorption correction: multi-scan
(LANA; Stoe & Cie, 2024a)
h = 2222
Tmin = 0.956, Tmax = 0.991k = 88
36658 measured reflectionsl = 2323
4524 independent reflections
Refinement top
Refinement on F2Primary atom site location: dual
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.043H-atom parameters constrained
wR(F2) = 0.114 w = 1/[σ2(Fo2) + (0.0547P)2 + 0.3522P]
where P = (Fo2 + 2Fc2)/3
S = 1.04(Δ/σ)max < 0.001
4524 reflectionsΔρmax = 0.24 e Å3
227 parametersΔρmin = 0.23 e Å3
0 restraints
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
C10.38754 (7)0.4218 (2)0.39397 (7)0.0272 (3)
C20.36343 (7)0.2941 (2)0.32872 (7)0.0273 (3)
H20.3183930.2016790.3276410.033*
C30.40321 (7)0.29685 (19)0.26445 (6)0.0245 (2)
C40.46930 (7)0.43711 (18)0.26478 (6)0.0241 (2)
C50.49296 (7)0.57198 (19)0.33007 (7)0.0251 (2)
C60.45192 (7)0.5604 (2)0.39331 (7)0.0277 (3)
H60.4686850.6504630.4373020.033*
C70.34587 (8)0.4080 (2)0.46383 (7)0.0348 (3)
H7A0.3587920.2678070.4905420.052*
H7B0.2884350.4175210.4471820.052*
H7C0.3632520.5297140.4992460.052*
C80.37152 (7)0.14970 (19)0.19821 (7)0.0252 (2)
C90.34393 (7)0.06064 (19)0.21337 (7)0.0298 (3)
H90.3495580.1117020.2654030.036*
C100.30864 (8)0.1952 (2)0.15386 (8)0.0345 (3)
H100.2896420.3363070.1654200.041*
C110.30092 (8)0.1252 (2)0.07782 (8)0.0362 (3)
H110.2765430.2175420.0370420.043*
C120.32895 (8)0.0806 (2)0.06128 (8)0.0330 (3)
H120.3244620.1284840.0089450.040*
C130.36354 (7)0.2170 (2)0.12085 (7)0.0285 (3)
H130.3820740.3582700.1088260.034*
C140.51397 (7)0.44349 (19)0.19752 (7)0.0255 (3)
C150.55489 (7)0.2590 (2)0.17779 (7)0.0307 (3)
H150.5549630.1280840.2075090.037*
C160.59553 (8)0.2659 (2)0.11495 (8)0.0380 (3)
H160.6234120.1395120.1018740.046*
C170.59577 (9)0.4551 (3)0.07120 (8)0.0426 (4)
H170.6236760.4587730.0281510.051*
C180.55527 (9)0.6392 (2)0.09021 (8)0.0381 (3)
H180.5551460.7692540.0600200.046*
C190.51490 (8)0.6343 (2)0.15319 (7)0.0296 (3)
H190.4876490.7617940.1663210.036*
C200.56168 (7)0.7268 (2)0.33745 (7)0.0270 (3)
C210.63667 (8)0.6655 (2)0.32259 (7)0.0321 (3)
H210.6444950.5227940.3029710.039*
C220.70009 (9)0.8115 (3)0.33624 (8)0.0401 (3)
H220.7509850.7675870.3263260.048*
C230.68919 (9)1.0207 (3)0.36424 (8)0.0435 (4)
H230.7324581.1205360.3732360.052*
C240.61549 (9)1.0835 (2)0.37899 (8)0.0401 (3)
H240.6079911.2268950.3982350.048*
C250.55222 (8)0.9385 (2)0.36589 (7)0.0322 (3)
H250.5016710.9836460.3763880.039*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C10.0266 (6)0.0322 (6)0.0230 (5)0.0018 (5)0.0043 (5)0.0017 (5)
C20.0248 (6)0.0292 (6)0.0282 (6)0.0022 (5)0.0049 (5)0.0014 (5)
C30.0245 (6)0.0251 (6)0.0235 (6)0.0010 (5)0.0022 (4)0.0002 (4)
C40.0245 (6)0.0249 (6)0.0229 (5)0.0014 (4)0.0043 (4)0.0007 (4)
C50.0259 (6)0.0255 (6)0.0236 (5)0.0003 (5)0.0027 (5)0.0011 (5)
C60.0296 (6)0.0301 (6)0.0228 (6)0.0006 (5)0.0024 (5)0.0030 (5)
C70.0330 (7)0.0459 (8)0.0269 (6)0.0043 (6)0.0084 (5)0.0025 (6)
C80.0209 (6)0.0270 (6)0.0281 (6)0.0005 (5)0.0051 (5)0.0031 (5)
C90.0283 (6)0.0282 (6)0.0337 (7)0.0007 (5)0.0071 (5)0.0007 (5)
C100.0323 (7)0.0271 (6)0.0450 (8)0.0030 (5)0.0094 (6)0.0061 (5)
C110.0333 (7)0.0362 (7)0.0393 (7)0.0052 (6)0.0056 (6)0.0153 (6)
C120.0322 (7)0.0399 (7)0.0271 (6)0.0016 (6)0.0054 (5)0.0059 (5)
C130.0275 (6)0.0289 (6)0.0293 (6)0.0015 (5)0.0051 (5)0.0031 (5)
C140.0231 (6)0.0299 (6)0.0232 (5)0.0045 (5)0.0026 (4)0.0043 (5)
C150.0287 (6)0.0319 (6)0.0315 (6)0.0009 (5)0.0046 (5)0.0039 (5)
C160.0333 (7)0.0417 (7)0.0412 (7)0.0008 (6)0.0126 (6)0.0125 (6)
C170.0424 (8)0.0547 (9)0.0348 (7)0.0092 (7)0.0192 (6)0.0075 (7)
C180.0435 (8)0.0409 (7)0.0315 (7)0.0098 (6)0.0110 (6)0.0021 (6)
C190.0311 (7)0.0298 (6)0.0285 (6)0.0035 (5)0.0061 (5)0.0014 (5)
C200.0303 (6)0.0300 (6)0.0196 (5)0.0038 (5)0.0009 (5)0.0019 (5)
C210.0318 (7)0.0380 (7)0.0268 (6)0.0045 (5)0.0051 (5)0.0020 (5)
C220.0310 (7)0.0559 (9)0.0328 (7)0.0094 (6)0.0031 (6)0.0028 (6)
C230.0431 (8)0.0460 (8)0.0379 (8)0.0212 (7)0.0047 (6)0.0045 (6)
C240.0503 (9)0.0302 (7)0.0357 (7)0.0090 (6)0.0064 (6)0.0008 (6)
C250.0355 (7)0.0304 (6)0.0286 (6)0.0005 (5)0.0016 (5)0.0016 (5)
Geometric parameters (Å, º) top
C1—C21.3865 (17)C12—C131.3878 (17)
C1—C61.3864 (17)C13—H130.9500
C1—C71.5058 (16)C14—C151.3924 (17)
C2—H20.9500C14—C191.3959 (17)
C2—C31.3982 (16)C15—H150.9500
C3—C41.4135 (16)C15—C161.3861 (18)
C3—C81.4948 (16)C16—H160.9500
C4—C51.4107 (16)C16—C171.381 (2)
C4—C141.4959 (15)C17—H170.9500
C5—C61.3975 (16)C17—C181.383 (2)
C5—C201.4940 (17)C18—H180.9500
C6—H60.9500C18—C191.3849 (17)
C7—H7A0.9800C19—H190.9500
C7—H7B0.9800C20—C211.3955 (18)
C7—H7C0.9800C20—C251.3980 (17)
C8—C91.4021 (17)C21—H210.9500
C8—C131.3964 (17)C21—C221.3915 (19)
C9—H90.9500C22—H220.9500
C9—C101.3840 (18)C22—C231.385 (2)
C10—H100.9500C23—H230.9500
C10—C111.380 (2)C23—C241.377 (2)
C11—H110.9500C24—H240.9500
C11—C121.3858 (19)C24—C251.3853 (19)
C12—H120.9500C25—H250.9500
C2—C1—C7121.07 (11)C8—C13—H13119.5
C6—C1—C2117.91 (11)C12—C13—C8120.99 (12)
C6—C1—C7121.01 (11)C12—C13—H13119.5
C1—C2—H2118.9C15—C14—C4120.62 (11)
C1—C2—C3122.17 (11)C15—C14—C19118.91 (11)
C3—C2—H2118.9C19—C14—C4120.47 (10)
C2—C3—C4119.39 (10)C14—C15—H15119.9
C2—C3—C8116.76 (10)C16—C15—C14120.21 (12)
C4—C3—C8123.85 (10)C16—C15—H15119.9
C3—C4—C14121.08 (10)C15—C16—H16119.8
C5—C4—C3118.83 (10)C17—C16—C15120.46 (13)
C5—C4—C14120.09 (10)C17—C16—H16119.8
C4—C5—C20123.94 (10)C16—C17—H17120.1
C6—C5—C4119.49 (11)C16—C17—C18119.82 (12)
C6—C5—C20116.55 (10)C18—C17—H17120.1
C1—C6—C5122.17 (11)C17—C18—H18119.9
C1—C6—H6118.9C17—C18—C19120.13 (13)
C5—C6—H6118.9C19—C18—H18119.9
C1—C7—H7A109.5C14—C19—H19119.8
C1—C7—H7B109.5C18—C19—C14120.46 (12)
C1—C7—H7C109.5C18—C19—H19119.8
H7A—C7—H7B109.5C21—C20—C5123.13 (11)
H7A—C7—H7C109.5C21—C20—C25118.13 (11)
H7B—C7—H7C109.5C25—C20—C5118.58 (11)
C9—C8—C3119.47 (10)C20—C21—H21119.7
C13—C8—C3122.75 (10)C22—C21—C20120.65 (13)
C13—C8—C9117.67 (11)C22—C21—H21119.7
C8—C9—H9119.4C21—C22—H22119.9
C10—C9—C8121.16 (12)C23—C22—C21120.15 (14)
C10—C9—H9119.4C23—C22—H22119.9
C9—C10—H10119.9C22—C23—H23120.1
C11—C10—C9120.29 (12)C24—C23—C22119.82 (13)
C11—C10—H10119.9C24—C23—H23120.1
C10—C11—H11120.2C23—C24—H24119.9
C10—C11—C12119.61 (12)C23—C24—C25120.29 (13)
C12—C11—H11120.2C25—C24—H24119.9
C11—C12—H12119.9C20—C25—H25119.5
C11—C12—C13120.28 (12)C24—C25—C20120.96 (13)
C13—C12—H12119.9C24—C25—H25119.5
C1—C2—C3—C41.30 (18)C6—C5—C20—C2545.84 (15)
C1—C2—C3—C8179.43 (11)C7—C1—C2—C3177.20 (11)
C2—C1—C6—C50.88 (18)C7—C1—C6—C5178.26 (12)
C2—C3—C4—C50.42 (17)C8—C3—C4—C5178.79 (11)
C2—C3—C4—C14179.42 (11)C8—C3—C4—C141.37 (17)
C2—C3—C8—C939.15 (16)C8—C9—C10—C110.91 (19)
C2—C3—C8—C13136.89 (12)C9—C8—C13—C120.46 (18)
C3—C4—C5—C61.43 (17)C9—C10—C11—C120.2 (2)
C3—C4—C5—C20179.96 (11)C10—C11—C12—C130.9 (2)
C3—C4—C14—C1564.33 (16)C11—C12—C13—C80.60 (19)
C3—C4—C14—C19115.28 (13)C13—C8—C9—C101.22 (18)
C3—C8—C9—C10175.02 (11)C14—C4—C5—C6178.41 (11)
C3—C8—C13—C12175.64 (11)C14—C4—C5—C200.12 (17)
C4—C3—C8—C9141.62 (12)C14—C15—C16—C170.1 (2)
C4—C3—C8—C1342.35 (17)C15—C14—C19—C180.60 (18)
C4—C5—C6—C10.79 (18)C15—C16—C17—C180.1 (2)
C4—C5—C20—C2149.16 (17)C16—C17—C18—C190.3 (2)
C4—C5—C20—C25135.58 (12)C17—C18—C19—C140.7 (2)
C4—C14—C15—C16179.41 (11)C19—C14—C15—C160.21 (18)
C4—C14—C19—C18179.02 (12)C20—C5—C6—C1179.43 (11)
C5—C4—C14—C15115.50 (13)C20—C21—C22—C230.5 (2)
C5—C4—C14—C1964.88 (15)C21—C20—C25—C240.02 (18)
C5—C20—C21—C22174.93 (11)C21—C22—C23—C240.4 (2)
C5—C20—C25—C24175.48 (11)C22—C23—C24—C250.1 (2)
C6—C1—C2—C31.94 (18)C23—C24—C25—C200.1 (2)
C6—C5—C20—C21129.41 (13)C25—C20—C21—C220.35 (18)
5-Methyl-1,2,3-triphenylbenzene (1b) top
Crystal data top
C25H20F(000) = 1360
Mr = 320.41Dx = 1.161 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
a = 19.9859 (6) ÅCell parameters from 25627 reflections
b = 19.9669 (7) Åθ = 2.3–29.4°
c = 9.2138 (3) ŵ = 0.07 mm1
β = 94.073 (2)°T = 123 K
V = 3667.5 (2) Å3Block, colorless
Z = 80.2 × 0.19 × 0.18 × 0.16 (radius) mm
Data collection top
Stoe Stadivari
diffractometer
6404 reflections with I > 2σ(I)
Detector resolution: 5.81 pixels mm-1Rint = 0.025
rotation method, ω scansθmax = 26.5°, θmin = 2.3°
Absorption correction: multi-scan
(LANA; Stoe & Cie, 2024a)
h = 2525
Tmin = 0.959, Tmax = 0.965k = 2425
50810 measured reflectionsl = 1111
7601 independent reflections
Refinement top
Refinement on F2Primary atom site location: dual
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.041H-atom parameters constrained
wR(F2) = 0.109 w = 1/[σ2(Fo2) + (0.0491P)2 + 1.1196P]
where P = (Fo2 + 2Fc2)/3
S = 1.05(Δ/σ)max = 0.001
7601 reflectionsΔρmax = 0.28 e Å3
453 parametersΔρmin = 0.25 e Å3
0 restraints
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
C10.43442 (6)0.43766 (6)0.23070 (13)0.0295 (3)
C20.41940 (6)0.50432 (6)0.20010 (13)0.0283 (3)
H20.3745070.5162100.1701170.034*
C30.46810 (6)0.55428 (6)0.21200 (13)0.0263 (3)
C40.53462 (6)0.53750 (6)0.25797 (13)0.0266 (3)
C50.55064 (6)0.47015 (6)0.28724 (13)0.0273 (3)
C60.50064 (6)0.42158 (6)0.27263 (13)0.0295 (3)
H60.5121290.3761090.2918720.035*
C70.38059 (7)0.38470 (7)0.21950 (16)0.0372 (3)
H7A0.4009600.3405670.2375820.056*
H7B0.3577710.3856050.1217970.056*
H7C0.3480190.3934830.2918500.056*
C80.44871 (6)0.62421 (6)0.17107 (13)0.0263 (3)
C90.48006 (6)0.65775 (7)0.06174 (14)0.0312 (3)
H90.5156350.6365720.0162140.037*
C100.45999 (7)0.72143 (7)0.01881 (14)0.0335 (3)
H100.4813120.7434240.0568430.040*
C110.40886 (6)0.75324 (7)0.08589 (15)0.0330 (3)
H110.3950860.7970360.0566310.040*
C120.37802 (6)0.72083 (6)0.19563 (15)0.0318 (3)
H120.3433960.7427360.2428760.038*
C130.39735 (6)0.65642 (6)0.23729 (14)0.0285 (3)
H130.3752830.6342410.3116170.034*
C140.58664 (6)0.59108 (6)0.27643 (13)0.0286 (3)
C150.64089 (6)0.59274 (7)0.18986 (16)0.0374 (3)
H150.6460700.5585530.1198330.045*
C160.68751 (7)0.64434 (9)0.20571 (18)0.0475 (4)
H160.7241280.6455620.1454320.057*
C170.68100 (8)0.69390 (8)0.30849 (19)0.0484 (4)
H170.7131050.7289700.3188150.058*
C180.62784 (8)0.69236 (7)0.39604 (17)0.0427 (4)
H180.6234490.7261320.4673780.051*
C190.58082 (7)0.64135 (7)0.37956 (14)0.0335 (3)
H190.5440790.6406900.4395460.040*
C200.62024 (6)0.44898 (6)0.33616 (13)0.0279 (3)
C210.65379 (6)0.40242 (6)0.25571 (14)0.0308 (3)
H210.6325030.3844600.1687900.037*
C220.71813 (7)0.38208 (7)0.30172 (15)0.0347 (3)
H220.7409890.3508800.2451400.042*
C230.74931 (6)0.40687 (7)0.42941 (15)0.0349 (3)
H230.7932890.3925060.4608440.042*
C240.71608 (7)0.45276 (7)0.51126 (15)0.0353 (3)
H240.7370190.4695280.5996730.042*
C250.65231 (7)0.47412 (7)0.46398 (14)0.0326 (3)
H250.6301400.5063330.5193680.039*
C260.06069 (6)0.57493 (6)0.20846 (14)0.0297 (3)
C270.00534 (6)0.58734 (6)0.17877 (13)0.0279 (3)
H270.0169360.6302020.1435230.033*
C280.05505 (6)0.53860 (6)0.19928 (13)0.0259 (3)
C290.03855 (6)0.47472 (6)0.25041 (13)0.0265 (3)
C300.02865 (6)0.46117 (6)0.27609 (13)0.0278 (3)
C310.07677 (6)0.51114 (7)0.25494 (13)0.0300 (3)
H310.1219810.5013740.2728030.036*
C320.11277 (7)0.62934 (7)0.19349 (17)0.0391 (3)
H32A0.1487900.6158230.1217590.059*
H32B0.0920910.6707590.1612380.059*
H32C0.1313560.6368960.2877220.059*
C330.12415 (6)0.55626 (6)0.16156 (13)0.0253 (2)
C340.15971 (6)0.51591 (6)0.07041 (13)0.0298 (3)
H340.1413030.4741940.0380400.036*
C350.22134 (6)0.53576 (7)0.02654 (14)0.0329 (3)
H350.2445340.5081330.0371680.039*
C360.24941 (6)0.59586 (7)0.07517 (14)0.0319 (3)
H360.2916270.6097020.0444300.038*
C370.21566 (6)0.63542 (7)0.16847 (15)0.0326 (3)
H370.2351460.6762380.2035730.039*
C380.15341 (6)0.61599 (6)0.21143 (14)0.0286 (3)
H380.1305370.6437270.2754950.034*
C390.09169 (6)0.42294 (6)0.28125 (13)0.0291 (3)
C400.09113 (7)0.36267 (7)0.20527 (16)0.0366 (3)
H400.0561650.3536610.1326000.044*
C410.14143 (8)0.31563 (7)0.23514 (19)0.0477 (4)
H410.1412340.2750150.1814030.057*
C420.19170 (8)0.32765 (8)0.34259 (19)0.0520 (4)
H420.2255100.2949630.3639500.062*
C430.19285 (8)0.38723 (8)0.41908 (17)0.0455 (4)
H430.2275790.3956240.4926450.055*
C440.14330 (7)0.43470 (7)0.38837 (15)0.0346 (3)
H440.1444550.4757050.4407790.042*
C450.04948 (6)0.39414 (6)0.32844 (13)0.0285 (3)
C460.09862 (6)0.35775 (6)0.24755 (14)0.0291 (3)
H460.1186560.3756350.1593240.035*
C470.11828 (6)0.29543 (6)0.29584 (14)0.0317 (3)
H470.1514250.2706370.2397260.038*
C480.09013 (7)0.26911 (7)0.42475 (14)0.0334 (3)
H480.1038220.2264350.4573060.040*
C490.04170 (7)0.30545 (7)0.50628 (14)0.0379 (3)
H490.0224170.2878120.5954460.046*
C500.02145 (7)0.36731 (7)0.45801 (14)0.0364 (3)
H500.0119970.3917380.5140620.044*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C10.0315 (6)0.0291 (6)0.0285 (6)0.0021 (5)0.0072 (5)0.0024 (5)
C20.0252 (6)0.0304 (6)0.0294 (6)0.0016 (5)0.0036 (5)0.0012 (5)
C30.0264 (6)0.0277 (6)0.0252 (6)0.0025 (5)0.0040 (5)0.0006 (5)
C40.0256 (6)0.0283 (6)0.0262 (6)0.0013 (5)0.0047 (5)0.0015 (5)
C50.0290 (6)0.0277 (6)0.0256 (6)0.0027 (5)0.0063 (5)0.0013 (5)
C60.0342 (7)0.0246 (6)0.0303 (6)0.0023 (5)0.0070 (5)0.0013 (5)
C70.0372 (7)0.0326 (7)0.0420 (7)0.0060 (6)0.0039 (6)0.0005 (6)
C80.0241 (6)0.0266 (6)0.0277 (6)0.0008 (5)0.0026 (5)0.0023 (5)
C90.0290 (6)0.0343 (7)0.0302 (6)0.0035 (5)0.0016 (5)0.0006 (5)
C100.0348 (7)0.0331 (7)0.0322 (7)0.0010 (6)0.0001 (5)0.0053 (5)
C110.0347 (7)0.0242 (6)0.0387 (7)0.0005 (5)0.0069 (5)0.0011 (5)
C120.0291 (6)0.0268 (6)0.0393 (7)0.0013 (5)0.0010 (5)0.0066 (5)
C130.0258 (6)0.0275 (6)0.0322 (6)0.0027 (5)0.0017 (5)0.0028 (5)
C140.0245 (6)0.0281 (6)0.0327 (6)0.0021 (5)0.0012 (5)0.0088 (5)
C150.0290 (7)0.0410 (8)0.0425 (7)0.0041 (6)0.0048 (6)0.0125 (6)
C160.0270 (7)0.0555 (10)0.0602 (10)0.0025 (7)0.0051 (6)0.0236 (8)
C170.0368 (8)0.0443 (9)0.0619 (10)0.0137 (7)0.0119 (7)0.0203 (8)
C180.0458 (8)0.0339 (8)0.0465 (8)0.0075 (6)0.0103 (7)0.0075 (6)
C190.0341 (7)0.0303 (7)0.0355 (7)0.0016 (5)0.0016 (5)0.0056 (5)
C200.0288 (6)0.0257 (6)0.0298 (6)0.0018 (5)0.0065 (5)0.0073 (5)
C210.0306 (6)0.0295 (7)0.0328 (6)0.0009 (5)0.0058 (5)0.0011 (5)
C220.0301 (7)0.0335 (7)0.0414 (7)0.0048 (5)0.0098 (6)0.0006 (6)
C230.0276 (6)0.0379 (7)0.0392 (7)0.0048 (5)0.0028 (5)0.0093 (6)
C240.0366 (7)0.0379 (7)0.0309 (6)0.0018 (6)0.0001 (5)0.0049 (6)
C250.0372 (7)0.0315 (7)0.0297 (6)0.0064 (6)0.0056 (5)0.0028 (5)
C260.0275 (6)0.0307 (7)0.0306 (6)0.0018 (5)0.0003 (5)0.0078 (5)
C270.0287 (6)0.0249 (6)0.0297 (6)0.0011 (5)0.0004 (5)0.0030 (5)
C280.0270 (6)0.0247 (6)0.0258 (6)0.0019 (5)0.0009 (5)0.0030 (5)
C290.0276 (6)0.0259 (6)0.0259 (6)0.0020 (5)0.0022 (5)0.0034 (5)
C300.0296 (6)0.0283 (6)0.0256 (6)0.0048 (5)0.0031 (5)0.0048 (5)
C310.0247 (6)0.0349 (7)0.0307 (6)0.0040 (5)0.0036 (5)0.0075 (5)
C320.0325 (7)0.0374 (8)0.0473 (8)0.0056 (6)0.0025 (6)0.0085 (6)
C330.0247 (6)0.0247 (6)0.0263 (6)0.0006 (5)0.0005 (5)0.0037 (5)
C340.0320 (6)0.0286 (6)0.0288 (6)0.0011 (5)0.0016 (5)0.0004 (5)
C350.0303 (7)0.0388 (7)0.0298 (6)0.0029 (5)0.0040 (5)0.0003 (5)
C360.0233 (6)0.0384 (7)0.0339 (7)0.0017 (5)0.0011 (5)0.0071 (6)
C370.0275 (6)0.0274 (6)0.0421 (7)0.0023 (5)0.0027 (5)0.0018 (5)
C380.0266 (6)0.0251 (6)0.0340 (6)0.0023 (5)0.0008 (5)0.0004 (5)
C390.0302 (6)0.0262 (6)0.0318 (6)0.0013 (5)0.0087 (5)0.0040 (5)
C400.0425 (8)0.0272 (7)0.0412 (7)0.0018 (6)0.0110 (6)0.0008 (6)
C410.0591 (10)0.0272 (7)0.0591 (10)0.0066 (7)0.0207 (8)0.0022 (7)
C420.0512 (9)0.0442 (9)0.0614 (10)0.0185 (7)0.0112 (8)0.0158 (8)
C430.0399 (8)0.0502 (9)0.0463 (8)0.0090 (7)0.0031 (6)0.0129 (7)
C440.0333 (7)0.0353 (7)0.0355 (7)0.0013 (6)0.0043 (5)0.0050 (6)
C450.0273 (6)0.0300 (7)0.0290 (6)0.0040 (5)0.0079 (5)0.0041 (5)
C460.0265 (6)0.0287 (6)0.0323 (6)0.0003 (5)0.0030 (5)0.0038 (5)
C470.0293 (6)0.0279 (7)0.0381 (7)0.0031 (5)0.0047 (5)0.0083 (5)
C480.0378 (7)0.0278 (7)0.0360 (7)0.0046 (5)0.0119 (6)0.0029 (5)
C490.0446 (8)0.0415 (8)0.0279 (6)0.0084 (6)0.0041 (6)0.0022 (6)
C500.0380 (7)0.0420 (8)0.0294 (6)0.0136 (6)0.0035 (5)0.0028 (6)
Geometric parameters (Å, º) top
C1—C21.3891 (18)C26—C271.3887 (17)
C1—C61.3898 (18)C26—C311.3888 (19)
C1—C71.5068 (18)C26—C321.5041 (18)
C2—H20.9500C27—H270.9500
C2—C31.3925 (17)C27—C281.3939 (17)
C3—C41.4067 (16)C28—C291.4070 (17)
C3—C81.4905 (17)C28—C331.4902 (16)
C4—C51.4042 (17)C29—C301.4066 (17)
C4—C141.4930 (17)C29—C391.4949 (17)
C5—C61.3922 (18)C30—C311.3899 (18)
C5—C201.4924 (17)C30—C451.4919 (17)
C6—H60.9500C31—H310.9500
C7—H7A0.9800C32—H32A0.9800
C7—H7B0.9800C32—H32B0.9800
C7—H7C0.9800C32—H32C0.9800
C8—C91.3948 (18)C33—C341.3944 (18)
C8—C131.3886 (17)C33—C381.3919 (17)
C9—H90.9500C34—H340.9500
C9—C101.3827 (18)C34—C351.3814 (18)
C10—H100.9500C35—H350.9500
C10—C111.3855 (19)C35—C361.3855 (19)
C11—H110.9500C36—H360.9500
C11—C121.3818 (19)C36—C371.3786 (19)
C12—H120.9500C37—H370.9500
C12—C131.3892 (18)C37—C381.3874 (18)
C13—H130.9500C38—H380.9500
C14—C151.3913 (18)C39—C401.3918 (18)
C14—C191.3927 (19)C39—C441.3959 (19)
C15—H150.9500C40—H400.9500
C15—C161.390 (2)C40—C411.389 (2)
C16—H160.9500C41—H410.9500
C16—C171.382 (3)C41—C421.381 (2)
C17—H170.9500C42—H420.9500
C17—C181.379 (2)C42—C431.382 (2)
C18—H180.9500C43—H430.9500
C18—C191.3868 (19)C43—C441.385 (2)
C19—H190.9500C44—H440.9500
C20—C211.3908 (18)C45—C461.3942 (17)
C20—C251.3938 (18)C45—C501.3895 (19)
C21—H210.9500C46—H460.9500
C21—C221.3858 (18)C46—C471.3876 (18)
C22—H220.9500C47—H470.9500
C22—C231.383 (2)C47—C481.3816 (19)
C23—H230.9500C48—H480.9500
C23—C241.386 (2)C48—C491.3871 (19)
C24—H240.9500C49—H490.9500
C24—C251.3846 (18)C49—C501.3831 (19)
C25—H250.9500C50—H500.9500
C2—C1—C6117.75 (12)C27—C26—C31117.92 (12)
C2—C1—C7121.04 (12)C27—C26—C32120.94 (12)
C6—C1—C7121.21 (12)C31—C26—C32121.12 (12)
C1—C2—H2119.0C26—C27—H27119.1
C1—C2—C3122.05 (11)C26—C27—C28121.80 (12)
C3—C2—H2119.0C28—C27—H27119.1
C2—C3—C4119.57 (11)C27—C28—C29119.77 (11)
C2—C3—C8118.90 (11)C27—C28—C33117.82 (11)
C4—C3—C8121.50 (11)C29—C28—C33122.38 (11)
C3—C4—C14119.94 (11)C28—C29—C39120.70 (11)
C5—C4—C3118.92 (11)C30—C29—C28118.68 (11)
C5—C4—C14121.13 (11)C30—C29—C39120.59 (11)
C4—C5—C20121.61 (11)C29—C30—C45121.24 (11)
C6—C5—C4119.76 (11)C31—C30—C29119.86 (11)
C6—C5—C20118.63 (11)C31—C30—C45118.89 (11)
C1—C6—C5121.93 (12)C26—C31—C30121.91 (12)
C1—C6—H6119.0C26—C31—H31119.0
C5—C6—H6119.0C30—C31—H31119.0
C1—C7—H7A109.5C26—C32—H32A109.5
C1—C7—H7B109.5C26—C32—H32B109.5
C1—C7—H7C109.5C26—C32—H32C109.5
H7A—C7—H7B109.5H32A—C32—H32B109.5
H7A—C7—H7C109.5H32A—C32—H32C109.5
H7B—C7—H7C109.5H32B—C32—H32C109.5
C9—C8—C3120.69 (11)C34—C33—C28121.62 (11)
C13—C8—C3120.65 (11)C38—C33—C28120.02 (11)
C13—C8—C9118.62 (12)C38—C33—C34118.28 (11)
C8—C9—H9119.6C33—C34—H34119.5
C10—C9—C8120.80 (12)C35—C34—C33120.91 (12)
C10—C9—H9119.6C35—C34—H34119.5
C9—C10—H10119.9C34—C35—H35119.9
C9—C10—C11120.15 (12)C34—C35—C36120.19 (12)
C11—C10—H10119.9C36—C35—H35119.9
C10—C11—H11120.2C35—C36—H36120.2
C12—C11—C10119.55 (12)C37—C36—C35119.55 (12)
C12—C11—H11120.2C37—C36—H36120.2
C11—C12—H12119.8C36—C37—H37119.8
C11—C12—C13120.40 (12)C36—C37—C38120.40 (12)
C13—C12—H12119.8C38—C37—H37119.8
C8—C13—C12120.47 (12)C33—C38—H38119.7
C8—C13—H13119.8C37—C38—C33120.64 (12)
C12—C13—H13119.8C37—C38—H38119.7
C15—C14—C4121.09 (12)C40—C39—C29121.47 (12)
C15—C14—C19118.70 (12)C40—C39—C44118.71 (12)
C19—C14—C4120.20 (11)C44—C39—C29119.82 (11)
C14—C15—H15120.0C39—C40—H40119.8
C16—C15—C14120.08 (15)C41—C40—C39120.34 (14)
C16—C15—H15120.0C41—C40—H40119.8
C15—C16—H16119.7C40—C41—H41119.9
C17—C16—C15120.51 (14)C42—C41—C40120.27 (15)
C17—C16—H16119.7C42—C41—H41119.9
C16—C17—H17120.0C41—C42—H42120.0
C18—C17—C16119.92 (14)C41—C42—C43120.02 (14)
C18—C17—H17120.0C43—C42—H42120.0
C17—C18—H18120.1C42—C43—H43120.0
C17—C18—C19119.76 (15)C42—C43—C44119.93 (15)
C19—C18—H18120.1C44—C43—H43120.0
C14—C19—H19119.5C39—C44—H44119.6
C18—C19—C14121.02 (13)C43—C44—C39120.72 (14)
C18—C19—H19119.5C43—C44—H44119.6
C21—C20—C5120.17 (11)C46—C45—C30119.79 (11)
C21—C20—C25118.74 (12)C50—C45—C30121.26 (11)
C25—C20—C5121.07 (11)C50—C45—C46118.95 (12)
C20—C21—H21119.8C45—C46—H46120.0
C22—C21—C20120.32 (12)C47—C46—C45120.05 (12)
C22—C21—H21119.8C47—C46—H46120.0
C21—C22—H22119.7C46—C47—H47119.7
C23—C22—C21120.50 (12)C48—C47—C46120.63 (12)
C23—C22—H22119.7C48—C47—H47119.7
C22—C23—H23120.2C47—C48—H48120.2
C22—C23—C24119.67 (12)C47—C48—C49119.50 (12)
C24—C23—H23120.2C49—C48—H48120.2
C23—C24—H24120.0C48—C49—H49119.9
C25—C24—C23119.90 (13)C50—C49—C48120.12 (13)
C25—C24—H24120.0C50—C49—H49119.9
C20—C25—H25119.6C45—C50—H50119.6
C24—C25—C20120.84 (12)C49—C50—C45120.75 (12)
C24—C25—H25119.6C49—C50—H50119.6
C1—C2—C3—C40.76 (18)C26—C27—C28—C290.46 (18)
C1—C2—C3—C8177.37 (11)C26—C27—C28—C33178.81 (11)
C2—C1—C6—C51.43 (18)C27—C26—C31—C301.96 (18)
C2—C3—C4—C51.64 (17)C27—C28—C29—C301.62 (17)
C2—C3—C4—C14177.70 (11)C27—C28—C29—C39176.50 (11)
C2—C3—C8—C9120.99 (13)C27—C28—C33—C34128.22 (13)
C2—C3—C8—C1356.62 (16)C27—C28—C33—C3848.42 (16)
C3—C4—C5—C61.00 (17)C28—C29—C30—C311.89 (17)
C3—C4—C5—C20179.91 (11)C28—C29—C30—C45179.18 (11)
C3—C4—C14—C15115.74 (13)C28—C29—C39—C40117.85 (14)
C3—C4—C14—C1962.99 (16)C28—C29—C39—C4462.14 (16)
C3—C8—C9—C10176.91 (11)C28—C33—C34—C35174.45 (11)
C3—C8—C13—C12177.98 (11)C28—C33—C38—C37175.25 (11)
C4—C3—C8—C957.10 (16)C29—C28—C33—C3450.09 (17)
C4—C3—C8—C13125.29 (13)C29—C28—C33—C38133.28 (12)
C4—C5—C6—C10.56 (18)C29—C30—C31—C260.09 (18)
C4—C5—C20—C21121.67 (13)C29—C30—C45—C46122.39 (13)
C4—C5—C20—C2559.68 (17)C29—C30—C45—C5058.50 (17)
C4—C14—C15—C16177.87 (12)C29—C39—C40—C41179.43 (12)
C4—C14—C19—C18178.55 (12)C29—C39—C44—C43179.70 (12)
C5—C4—C14—C1564.94 (16)C30—C29—C39—C4064.06 (16)
C5—C4—C14—C19116.33 (13)C30—C29—C39—C44115.95 (13)
C5—C20—C21—C22179.26 (12)C30—C45—C46—C47179.88 (11)
C5—C20—C25—C24177.97 (12)C30—C45—C50—C49179.26 (12)
C6—C1—C2—C30.76 (18)C31—C26—C27—C282.24 (18)
C6—C5—C20—C2159.24 (16)C31—C30—C45—C4658.67 (16)
C6—C5—C20—C25119.42 (14)C31—C30—C45—C50120.43 (14)
C7—C1—C2—C3178.93 (12)C32—C26—C27—C28176.59 (12)
C7—C1—C6—C5178.26 (12)C32—C26—C31—C30176.86 (12)
C8—C3—C4—C5176.44 (11)C33—C28—C29—C30176.65 (11)
C8—C3—C4—C144.22 (17)C33—C28—C29—C395.22 (17)
C8—C9—C10—C110.98 (19)C33—C34—C35—C361.27 (19)
C9—C8—C13—C120.32 (18)C34—C33—C38—C371.50 (18)
C9—C10—C11—C120.13 (19)C34—C35—C36—C370.49 (19)
C10—C11—C12—C130.93 (19)C35—C36—C37—C381.23 (19)
C11—C12—C13—C81.17 (18)C36—C37—C38—C330.22 (19)
C13—C8—C9—C100.74 (18)C38—C33—C34—C352.24 (18)
C14—C4—C5—C6178.33 (11)C39—C29—C30—C31176.23 (11)
C14—C4—C5—C200.76 (18)C39—C29—C30—C452.69 (17)
C14—C15—C16—C170.8 (2)C39—C40—C41—C421.3 (2)
C15—C14—C19—C180.21 (19)C40—C39—C44—C430.31 (19)
C15—C16—C17—C180.1 (2)C40—C41—C42—C431.2 (2)
C16—C17—C18—C190.6 (2)C41—C42—C43—C440.4 (2)
C17—C18—C19—C140.5 (2)C42—C43—C44—C390.4 (2)
C19—C14—C15—C160.88 (19)C44—C39—C40—C410.56 (19)
C20—C5—C6—C1178.56 (11)C45—C30—C31—C26179.04 (11)
C20—C21—C22—C231.2 (2)C45—C46—C47—C480.72 (19)
C21—C20—C25—C240.70 (19)C46—C45—C50—C490.1 (2)
C21—C22—C23—C240.5 (2)C46—C47—C48—C490.06 (19)
C22—C23—C24—C250.8 (2)C47—C48—C49—C500.5 (2)
C23—C24—C25—C201.4 (2)C48—C49—C50—C450.5 (2)
C25—C20—C21—C220.58 (19)C50—C45—C46—C470.75 (18)
5-(Bromomethyl)-1,2,3-triphenylbenzene (2) top
Crystal data top
C25H19BrZ = 2
Mr = 399.31F(000) = 408
Triclinic, P1Dx = 1.363 Mg m3
a = 10.0859 (6) ÅMo Kα radiation, λ = 0.71073 Å
b = 10.2444 (7) ÅCell parameters from 22401 reflections
c = 11.3564 (7) Åθ = 2.8–28.4°
α = 65.309 (5)°µ = 2.12 mm1
β = 76.095 (5)°T = 193 K
γ = 66.367 (5)°Block, colorless
V = 972.95 (12) Å30.50 × 0.40 × 0.25 mm
Data collection top
Stoe IPDS 2T
diffractometer
4702 independent reflections
Radiation source: sealed X-ray tube, 12 x 0.4 mm long-fine focus4072 reflections with I > 2σ(I)
Plane graphite monochromatorRint = 0.033
Detector resolution: 6.67 pixels mm-1θmax = 28.0°, θmin = 2.8°
rotation method scansh = 1313
Absorption correction: integration
[X-Shape (Stoe & Cie, 2021) and X-Red32 (Stoe & Cie, 2023)]
k = 1313
Tmin = 0.617, Tmax = 0.813l = 1414
22755 measured reflections
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.028H-atom parameters constrained
wR(F2) = 0.069 w = 1/[σ2(Fo2) + (0.0285P)2 + 0.4117P]
where P = (Fo2 + 2Fc2)/3
S = 1.06(Δ/σ)max = 0.001
4702 reflectionsΔρmax = 0.41 e Å3
290 parametersΔρmin = 0.38 e Å3
84 restraints
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*/UeqOcc. (<1)
Br10.95434 (2)0.68998 (3)0.09304 (2)0.04730 (7)
C10.68276 (16)0.67536 (18)0.07518 (14)0.0279 (3)
C30.45011 (15)0.71019 (17)0.20467 (14)0.0249 (3)
C40.46676 (15)0.55617 (17)0.23675 (13)0.0252 (3)
C50.59163 (16)0.46289 (17)0.18471 (14)0.0265 (3)
C60.69677 (16)0.52465 (18)0.10428 (14)0.0292 (3)
H60.78000.46210.06850.035*
C70.79841 (17)0.7371 (2)0.01017 (16)0.0339 (3)
H7A0.75560.84910.05380.041*
H7B0.83950.69140.07820.041*
C80.31466 (15)0.81793 (17)0.24693 (14)0.0259 (3)
C90.32032 (19)0.89833 (19)0.31745 (16)0.0343 (3)
H90.41120.88430.34000.041*
C100.1933 (2)0.9994 (2)0.35506 (18)0.0452 (4)
H100.19781.05220.40490.054*
C110.0614 (2)1.0234 (2)0.32064 (19)0.0460 (5)
H110.02481.09300.34620.055*
C120.05446 (18)0.9462 (2)0.24889 (19)0.0415 (4)
H120.03640.96360.22410.050*
C130.18000 (17)0.84313 (19)0.21296 (16)0.0330 (3)
H130.17430.78920.16470.040*
C14A0.3550 (17)0.490 (2)0.3181 (13)0.026 (2)0.50 (3)
C15A0.3200 (16)0.4786 (18)0.4481 (12)0.032 (2)0.50 (3)
H15A0.36820.51610.48240.039*0.50 (3)
C16A0.2167 (14)0.4134 (14)0.5300 (11)0.0344 (19)0.50 (3)
H16A0.19470.40730.61800.041*0.50 (3)
C17A0.1483 (10)0.3588 (11)0.4793 (15)0.0339 (18)0.50 (3)
H17A0.07780.31430.53270.041*0.50 (3)
C18A0.1808 (12)0.3678 (13)0.3526 (14)0.0323 (17)0.50 (3)
H18A0.13290.32900.31930.039*0.50 (3)
C19A0.2827 (14)0.4327 (17)0.2722 (12)0.0251 (16)0.50 (3)
H19A0.30360.43780.18460.030*0.50 (3)
C14B0.3540 (17)0.493 (2)0.3343 (13)0.025 (2)0.50 (3)
C15B0.3300 (14)0.4972 (16)0.4580 (10)0.0238 (16)0.50 (3)
H15B0.37930.54400.48100.029*0.50 (3)
C16B0.2326 (12)0.4322 (16)0.5479 (11)0.0332 (17)0.50 (3)
H16B0.21800.43140.63400.040*0.50 (3)
C17B0.1564 (10)0.3684 (11)0.5141 (14)0.0319 (18)0.50 (3)
H17B0.09160.32240.57730.038*0.50 (3)
C18B0.1745 (12)0.3718 (13)0.3891 (15)0.0329 (19)0.50 (3)
H18B0.11820.33400.36380.039*0.50 (3)
C19B0.2761 (16)0.4314 (19)0.3001 (14)0.033 (2)0.50 (3)
H19B0.29220.42980.21470.040*0.50 (3)
C200.61581 (15)0.29975 (17)0.21167 (14)0.0269 (3)
C210.61479 (17)0.19301 (19)0.33827 (15)0.0332 (3)
H210.59680.22440.41010.040*
C220.63976 (18)0.04182 (19)0.36014 (16)0.0350 (4)
H220.63870.02970.44670.042*
C230.66621 (17)0.00542 (18)0.25649 (17)0.0337 (3)
H230.68290.10910.27180.040*
C240.66829 (19)0.09861 (19)0.13063 (17)0.0360 (4)
H240.68670.06640.05920.043*
C250.64342 (18)0.25058 (19)0.10846 (15)0.0327 (3)
H250.64540.32140.02170.039*
C20.55917 (16)0.76671 (17)0.12599 (14)0.0271 (3)
H20.54870.86980.10680.033*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Br10.03013 (9)0.07091 (15)0.04878 (12)0.02408 (9)0.00427 (7)0.02660 (10)
C10.0258 (7)0.0339 (8)0.0231 (7)0.0129 (6)0.0008 (5)0.0077 (6)
C30.0244 (6)0.0301 (7)0.0216 (6)0.0103 (6)0.0026 (5)0.0094 (5)
C40.0250 (6)0.0299 (7)0.0208 (6)0.0118 (6)0.0024 (5)0.0069 (5)
C50.0277 (7)0.0279 (7)0.0221 (7)0.0093 (6)0.0030 (5)0.0070 (6)
C60.0272 (7)0.0325 (8)0.0254 (7)0.0099 (6)0.0013 (5)0.0104 (6)
C70.0309 (7)0.0399 (9)0.0291 (8)0.0171 (7)0.0027 (6)0.0090 (7)
C80.0262 (7)0.0262 (7)0.0235 (7)0.0105 (6)0.0008 (5)0.0066 (5)
C90.0364 (8)0.0382 (9)0.0307 (8)0.0119 (7)0.0049 (6)0.0144 (7)
C100.0529 (11)0.0437 (10)0.0388 (10)0.0100 (8)0.0004 (8)0.0228 (8)
C110.0373 (9)0.0413 (10)0.0425 (10)0.0035 (8)0.0077 (7)0.0150 (8)
C120.0249 (7)0.0421 (10)0.0476 (10)0.0098 (7)0.0001 (7)0.0102 (8)
C130.0286 (7)0.0350 (8)0.0363 (8)0.0131 (6)0.0032 (6)0.0113 (7)
C14A0.025 (3)0.022 (3)0.022 (3)0.001 (2)0.003 (2)0.006 (2)
C15A0.033 (3)0.032 (3)0.037 (3)0.012 (2)0.006 (2)0.015 (2)
C16A0.037 (4)0.030 (3)0.027 (3)0.010 (2)0.002 (2)0.005 (2)
C17A0.028 (2)0.028 (2)0.039 (5)0.0102 (15)0.000 (3)0.006 (3)
C18A0.032 (2)0.027 (2)0.035 (4)0.0122 (18)0.001 (3)0.008 (3)
C19A0.026 (2)0.026 (2)0.023 (3)0.0123 (18)0.003 (2)0.004 (2)
C14B0.022 (3)0.027 (3)0.023 (4)0.013 (3)0.002 (2)0.004 (2)
C15B0.025 (2)0.027 (3)0.017 (2)0.0108 (18)0.0018 (16)0.0062 (18)
C16B0.028 (2)0.037 (3)0.029 (3)0.0121 (19)0.003 (2)0.008 (2)
C17B0.028 (2)0.028 (3)0.030 (4)0.0101 (17)0.001 (2)0.003 (2)
C18B0.030 (2)0.030 (2)0.038 (5)0.0119 (17)0.001 (3)0.012 (3)
C19B0.036 (3)0.034 (3)0.027 (4)0.011 (2)0.001 (3)0.011 (3)
C200.0236 (6)0.0270 (7)0.0266 (7)0.0074 (6)0.0023 (5)0.0073 (6)
C210.0338 (8)0.0328 (8)0.0254 (7)0.0069 (6)0.0018 (6)0.0081 (6)
C220.0330 (8)0.0301 (8)0.0301 (8)0.0088 (6)0.0030 (6)0.0016 (6)
C230.0299 (7)0.0264 (8)0.0434 (9)0.0093 (6)0.0085 (6)0.0087 (7)
C240.0428 (9)0.0335 (8)0.0354 (9)0.0118 (7)0.0081 (7)0.0143 (7)
C250.0393 (8)0.0314 (8)0.0255 (7)0.0126 (7)0.0049 (6)0.0070 (6)
C20.0276 (7)0.0287 (7)0.0268 (7)0.0127 (6)0.0032 (5)0.0083 (6)
Geometric parameters (Å, º) top
Br1—C71.9711 (17)C16A—C17A1.376 (7)
C1—C21.390 (2)C16A—H16A0.9500
C1—C61.391 (2)C17A—C18A1.368 (7)
C1—C71.495 (2)C17A—H17A0.9500
C3—C21.396 (2)C18A—C19A1.386 (8)
C3—C41.410 (2)C18A—H18A0.9500
C3—C81.494 (2)C19A—H19A0.9500
C4—C51.413 (2)C14B—C15B1.383 (9)
C4—C14A1.472 (12)C14B—C19B1.384 (9)
C4—C14B1.525 (11)C15B—C16B1.388 (8)
C5—C61.396 (2)C15B—H15B0.9500
C5—C201.493 (2)C16B—C17B1.386 (7)
C6—H60.9500C16B—H16B0.9500
C7—H7A0.9900C17B—C18B1.375 (7)
C7—H7B0.9900C17B—H17B0.9500
C8—C91.391 (2)C18B—C19B1.390 (9)
C8—C131.396 (2)C18B—H18B0.9500
C9—C101.392 (2)C19B—H19B0.9500
C9—H90.9500C20—C251.389 (2)
C10—C111.375 (3)C20—C211.397 (2)
C10—H100.9500C21—C221.386 (2)
C11—C121.380 (3)C21—H210.9500
C11—H110.9500C22—C231.383 (2)
C12—C131.387 (2)C22—H220.9500
C12—H120.9500C23—C241.382 (2)
C13—H130.9500C23—H230.9500
C14A—C19A1.393 (9)C24—C251.393 (2)
C14A—C15A1.397 (9)C24—H240.9500
C15A—C16A1.403 (9)C25—H250.9500
C15A—H15A0.9500C2—H20.9500
C2—C1—C6118.69 (13)C15A—C16A—H16A121.0
C2—C1—C7121.13 (14)C18A—C17A—C16A120.7 (7)
C6—C1—C7120.18 (14)C18A—C17A—H17A119.7
C2—C3—C4119.65 (13)C16A—C17A—H17A119.7
C2—C3—C8118.59 (13)C17A—C18A—C19A120.9 (7)
C4—C3—C8121.68 (13)C17A—C18A—H18A119.5
C3—C4—C5119.25 (13)C19A—C18A—H18A119.5
C3—C4—C14A122.2 (7)C18A—C19A—C14A120.9 (8)
C5—C4—C14A118.5 (7)C18A—C19A—H19A119.5
C3—C4—C14B118.5 (7)C14A—C19A—H19A119.5
C5—C4—C14B122.1 (7)C15B—C14B—C19B119.9 (8)
C6—C5—C4119.29 (14)C15B—C14B—C4119.5 (8)
C6—C5—C20118.18 (13)C19B—C14B—C4120.6 (9)
C4—C5—C20122.53 (13)C14B—C15B—C16B118.9 (8)
C1—C6—C5121.69 (14)C14B—C15B—H15B120.6
C1—C6—H6119.2C16B—C15B—H15B120.6
C5—C6—H6119.2C17B—C16B—C15B121.0 (7)
C1—C7—Br1110.53 (11)C17B—C16B—H16B119.5
C1—C7—H7A109.5C15B—C16B—H16B119.5
Br1—C7—H7A109.5C18B—C17B—C16B119.9 (7)
C1—C7—H7B109.5C18B—C17B—H17B120.0
Br1—C7—H7B109.5C16B—C17B—H17B120.0
H7A—C7—H7B108.1C17B—C18B—C19B119.2 (7)
C9—C8—C13118.62 (14)C17B—C18B—H18B120.4
C9—C8—C3120.92 (13)C19B—C18B—H18B120.4
C13—C8—C3120.44 (14)C14B—C19B—C18B120.9 (8)
C8—C9—C10120.22 (16)C14B—C19B—H19B119.6
C8—C9—H9119.9C18B—C19B—H19B119.6
C10—C9—H9119.9C25—C20—C21118.48 (14)
C11—C10—C9120.53 (18)C25—C20—C5119.49 (13)
C11—C10—H10119.7C21—C20—C5122.01 (14)
C9—C10—H10119.7C22—C21—C20120.65 (15)
C10—C11—C12119.86 (16)C22—C21—H21119.7
C10—C11—H11120.1C20—C21—H21119.7
C12—C11—H11120.1C23—C22—C21120.27 (15)
C11—C12—C13120.09 (17)C23—C22—H22119.9
C11—C12—H12120.0C21—C22—H22119.9
C13—C12—H12120.0C24—C23—C22119.79 (15)
C12—C13—C8120.66 (16)C24—C23—H23120.1
C12—C13—H13119.7C22—C23—H23120.1
C8—C13—H13119.7C23—C24—C25120.02 (15)
C19A—C14A—C15A116.7 (9)C23—C24—H24120.0
C19A—C14A—C4122.4 (9)C25—C24—H24120.0
C15A—C14A—C4120.9 (9)C20—C25—C24120.78 (15)
C14A—C15A—C16A122.8 (8)C20—C25—H25119.6
C14A—C15A—H15A118.6C24—C25—H25119.6
C16A—C15A—H15A118.6C1—C2—C3121.39 (14)
C17A—C16A—C15A118.0 (7)C1—C2—H2119.3
C17A—C16A—H16A121.0C3—C2—H2119.3
C2—C3—C4—C52.3 (2)C4—C14A—C15A—C16A178.4 (13)
C8—C3—C4—C5174.47 (13)C14A—C15A—C16A—C17A0 (2)
C2—C3—C4—C14A179.4 (7)C15A—C16A—C17A—C18A0.1 (15)
C8—C3—C4—C14A2.7 (7)C16A—C17A—C18A—C19A0.3 (16)
C2—C3—C4—C14B173.6 (7)C17A—C18A—C19A—C14A0 (2)
C8—C3—C4—C14B9.7 (7)C15A—C14A—C19A—C18A0 (2)
C3—C4—C5—C61.0 (2)C4—C14A—C19A—C18A178.2 (13)
C14A—C4—C5—C6178.2 (7)C3—C4—C14B—C15B58.3 (17)
C14B—C4—C5—C6174.7 (7)C5—C4—C14B—C15B117.4 (13)
C3—C4—C5—C20178.68 (13)C3—C4—C14B—C19B121.8 (14)
C14A—C4—C5—C201.5 (7)C5—C4—C14B—C19B62.5 (18)
C14B—C4—C5—C205.7 (7)C19B—C14B—C15B—C16B3 (2)
C2—C1—C6—C51.2 (2)C4—C14B—C15B—C16B176.7 (13)
C7—C1—C6—C5179.33 (14)C14B—C15B—C16B—C17B2 (2)
C4—C5—C6—C10.8 (2)C15B—C16B—C17B—C18B1.3 (16)
C20—C5—C6—C1179.55 (14)C16B—C17B—C18B—C19B3.9 (16)
C2—C1—C7—Br195.19 (15)C15B—C14B—C19B—C18B1 (3)
C6—C1—C7—Br185.38 (16)C4—C14B—C19B—C18B179.2 (13)
C2—C3—C8—C958.5 (2)C17B—C18B—C19B—C14B3 (2)
C4—C3—C8—C9124.71 (16)C6—C5—C20—C2553.9 (2)
C2—C3—C8—C13119.61 (16)C4—C5—C20—C25125.77 (16)
C4—C3—C8—C1357.2 (2)C6—C5—C20—C21124.68 (16)
C13—C8—C9—C101.2 (2)C4—C5—C20—C2155.7 (2)
C3—C8—C9—C10179.39 (15)C25—C20—C21—C220.5 (2)
C8—C9—C10—C111.4 (3)C5—C20—C21—C22179.03 (14)
C9—C10—C11—C120.4 (3)C20—C21—C22—C230.1 (2)
C10—C11—C12—C130.8 (3)C21—C22—C23—C240.3 (2)
C11—C12—C13—C81.0 (3)C22—C23—C24—C250.2 (2)
C9—C8—C13—C120.0 (2)C21—C20—C25—C240.5 (2)
C3—C8—C13—C12178.22 (15)C5—C20—C25—C24179.16 (15)
C3—C4—C14A—C19A117.6 (14)C23—C24—C25—C200.2 (3)
C5—C4—C14A—C19A59.5 (17)C6—C1—C2—C30.1 (2)
C3—C4—C14A—C15A64.6 (17)C7—C1—C2—C3179.34 (14)
C5—C4—C14A—C15A118.3 (13)C4—C3—C2—C11.8 (2)
C19A—C14A—C15A—C16A1 (2)C8—C3—C2—C1174.98 (13)
Geometric data (A, °) of intermolecular interactions top
Cg denotes the centers of gravity of aromatic rings corresponding to the following atoms: A': C26–C31; B: C8–C13; B': C33–C38; C: C14–C19; D: C20–C25.
C—H···Br/CgC—HH···Br/CgC···Br/CgC—H···Br/Cg
1a
C7—H7A···Cg(D)i0.982.873.625 (1)134
C13—H13···Cg(C)ii0.952.973.536 (1)120
C19—H19···Cg(B)iii0.952.973.790 (1)145
1b
C46—H46···Cg(A')iv0.952.983.931 (1)176
C50—H50···Cg(B')v0.952.913.631 (1)134
2
C6—H6···Br1vi0.953.11a4.045 (2)170
C7—H7A···Cg(B)vii0.992.813.608 (2)138
C12—H12···Cg(D)viii0.953.03a3.846 (2)144
Note: (a) distances slightly above commonly employed thresholds (H···Br: 3.05 Å, H···Cg: 3.00 Å; Bondi, 1964). Symmetry codes: (i) -x + 1, -y + 1, -z + 1; (ii) x, y, z (intra); (iii) x, y + 1, z; (iv) -x, -y + 1, -z; (v) -x, -y + 1, -z + 1; (vi) -x + 2, -y + 1, -z; (vii) -x + 1, -y + 2, -z; (viii) x - 1, y + 1, z.
 

Acknowledgements

We would like to thank the Dr. Erich-Krüger-Stiftung for the financial support. Open Access Funding by the Publication Fund of the Technische Universität Bergakademie Freiberg is gratefully acknowledged.

Funding information

Funding for this research was provided by: Dr. Erich-Krüger-Stiftung (grant No. 02110150, TUBAF).

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