organic compounds\(\def\hfill{\hskip 5em}\def\hfil{\hskip 3em}\def\eqno#1{\hfil {#1}}\)

Journal logoIUCrDATA
ISSN: 2414-3146

3-(4-Methyl­phen­yl)-5-phenyl-1,2-thia­zole

crossmark logo

aDepartment of Chemistry, BMS Institute of Technology & Management, Autonomous under Visvesvaraya Technological University, Avalahalli, Yelahanka, Bengaluru 560064, Karnataka, India, and bResearch Center, Department of Physics, Government Engineering College, Bedarapura, Chamarajanagara 571313, Karnataka, India
*Correspondence e-mail: [email protected], [email protected]

Edited by M. Bolte, Goethe-Universität Frankfurt, Germany (Received 30 July 2026; accepted 9 August 2026; online 20 August 2026)

The title compound, C16H13NS, crystallizes in the monoclinic space group P21/c with two independent mol­ecules in the asymmetric unit. Both mol­ecules adopt a non-planar structure. No classical hydrogen bonds are found in the crystal structure.

3D view (loading...)
[Scheme 3D1]
Chemical scheme
[Scheme 1]

Structure description

1,2-Thiazole derivatives are an important class of sulfur- and nitrogen-containing heterocyclic compounds and their structural diversity and electronic properties make them of interest in organic and medicinal chemistry (Kaberdin & Potkin, 2002View full citation). The asymmetric unit of the title compound (2) comprises two independent mol­ecules, A and B (Fig. 1[link]). Both mol­ecules adopt a non-planar geometry as evidenced by the dihedral angles between the mean planes of the terminal phenyl rings (C4–C9 and C10–C15) of 11.1 (2) and 11.3 (2)° in molecules A and B, respectively. The bond lengths and bond angles are in good agreement with the literature values (Fait et al., 2021View full citation; Guseinov et al., 2026View full citation; Meundaeng et al., 2019View full citation; Sreenatha et al., 2018View full citation; Sreenatha et al., 2021View full citation). There are no classical hydrogen bonds in the crystal structure.The packing of the title compound is shown in Fig. 2[link].

[Figure 1]
Figure 1
The mol­ecular structure of 2 with displacement ellipsoids drawn at the 50% probability level.
[Figure 2]
Figure 2
Packing of the title compound viewed along the b axis.

Synthesis and crystallization

The title compound was synthesized (Fig. 3[link]) using a literature procedure (Zhang et al., 2021View full citation). A pressure tube was charged with compound 1 [(N-methoxy-1-(4-methylphenyl)-3-phenylprop-2-yn-1-imine)] (0.2 mmol), Na2S (0.3 mmol, 23.4 mg), NaHCO3 (0.4 mmol, 33.6 mg), and H2O (1.2 mmol, 21.6 mg) in N,N-dimethylformamide (DMF) (2 ml) in the presence of air under sealed conditions.The reaction mixture was stirred at 90°C in an oil bath for 13–15 h until the starting material was consumed completely by TLC (spotted from micro work-up of aliquots). After the completion of the reaction, as indicated by the TLC, the mixture was poured into ethyl acetate and washed with brine (2 × 15 ml). The combined organic layers were dried over anhydrous MgSO4 and evaporated under vacuum. The residue was purified by flash column chromatography using petroleum ether/ethyl acetate as the eluent to afford the desired product 2 in 78% yield. 0.5 g of compound 2 were dissolved in 5 ml of DMF and allowed to undergo slow evaporation. Crystals obtained were isolated and subjected to single-crystal XRD studies.

[Figure 3]
Figure 3
Synthesis scheme for the title compound.

Refinement

Crystal data and structure refinement details are summarized in Table 1[link].

Table 1
Experimental details

Crystal data
Chemical formula C16H13NS
Mr 251.33
Crystal system, space group Monoclinic, P21/c
Temperature (K) 293
a, b, c (Å) 28.7454 (18), 7.3669 (5), 12.2221 (7)
β (°) 96.675 (2)
V3) 2570.7 (3)
Z 8
Radiation type Mo Kα
μ (mm−1) 0.23
Crystal size (mm) 0.27 × 0.25 × 0.22
 
Data collection
Diffractometer Bruker APEX
No. of measured, independent and observed [I > 2σ(I)] reflections 108451, 5931, 3157
Rint 0.154
(sin θ/λ)max−1) 0.652
 
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.078, 0.256, 1.03
No. of reflections 5931
No. of parameters 327
H-atom treatment H-atom parameters constrained
Δρmax, Δρmin (e Å−3) 0.55, −0.47
Computer programs: APEX (Bruker, 2012View full citation), SAINT (Bruker, 2012View full citation), SHELXT 2018/2 (Sheldrick, 2015aView full citation), SHELXL2019/2 (Sheldrick, 2015bView full citation) and Mercury (Macrae et al., 2020View full citation).

Structural data


Computing details top

3-(4-Methylphenyl)-5-phenyl-1,2-thiazole top
Crystal data top
C16H13NSF(000) = 1056
Mr = 251.33Dx = 1.299 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
a = 28.7454 (18) ÅCell parameters from 5931 reflections
b = 7.3669 (5) Åθ = 2.9–27.6°
c = 12.2221 (7) ŵ = 0.23 mm1
β = 96.675 (2)°T = 293 K
V = 2570.7 (3) Å3Block, colorless
Z = 80.27 × 0.25 × 0.22 mm
Data collection top
Bruker APEX
diffractometer
θmax = 27.6°, θmin = 2.9°
Radiation source: graphiteh = 3737
SAINT (Bruker, 2012) scansk = 99
108451 measured reflectionsl = 1515
5931 independent reflections5931 standard reflections every 200 reflections
3157 reflections with I > 2σ(I) intensity decay: none
Rint = 0.154
Refinement top
Refinement on F20 restraints
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.078H-atom parameters constrained
wR(F2) = 0.256 w = 1/[σ2(Fo2) + (0.1108P)2 + 2.3809P]
where P = (Fo2 + 2Fc2)/3
S = 1.03(Δ/σ)max = 0.033
5931 reflectionsΔρmax = 0.55 e Å3
327 parametersΔρmin = 0.47 e Å3
Special details top

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

Refinement. The methyl H atoms were placed in calculated positions using the rotating-group model (HFIX 137) and refined as riding atoms with U(H)=1.5Ueq(C). All other H atoms were positioned geometrically and refined using a riding model with U(H)=1.2Ueq(C).

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
S1A0.04414 (5)0.42640 (18)0.76380 (9)0.0778 (4)
N1A0.09737 (11)0.3869 (5)0.7700 (2)0.0587 (9)
C1A0.02596 (13)0.3317 (5)0.6397 (3)0.0492 (9)
C2A0.06513 (13)0.2617 (5)0.6003 (3)0.0508 (9)
C3A0.10614 (13)0.2910 (5)0.6732 (3)0.0508 (9)
C4A0.15425 (13)0.2372 (5)0.6552 (3)0.0501 (9)
C5A0.16452 (14)0.1602 (6)0.5572 (3)0.0607 (10)
C6A0.21023 (14)0.1149 (6)0.5426 (3)0.0641 (11)
C7A0.24701 (14)0.1462 (5)0.6239 (3)0.0608 (10)
C8A0.23581 (15)0.2197 (6)0.7218 (4)0.0673 (11)
C9A0.19126 (14)0.2632 (6)0.7373 (3)0.0626 (11)
C10A0.02311 (12)0.3329 (5)0.5904 (3)0.0475 (8)
C11A0.05764 (15)0.4254 (5)0.6392 (3)0.0600 (10)
C12A0.10290 (15)0.4257 (6)0.5934 (4)0.0705 (12)
C13A0.11644 (15)0.3342 (6)0.4969 (4)0.0702 (12)
C14A0.08254 (15)0.2414 (6)0.4467 (4)0.0667 (11)
C15A0.03708 (14)0.2408 (5)0.4923 (3)0.0563 (10)
C16A0.29642 (15)0.0953 (7)0.6074 (5)0.0864 (15)
H2A0.0646070.2018730.5331570.061*
H5A0.1405410.1386510.5008180.073*
H6A0.2162920.0623220.4765450.077*
H8A0.2596380.2397360.7788020.081*
H9A0.1853220.3117340.8045220.075*
H11A0.0494580.4883210.7046330.072*
H12A0.1251630.4888100.6277190.085*
H13A0.1475590.3344020.4659630.084*
H14A0.0910410.1789900.3812750.080*
H15A0.0149040.1780160.4574920.068*
H16A0.3171200.1934920.6311550.130*
H16B0.2981600.0711440.5308300.130*
H16C0.3054990.0113010.6498350.130*
S1B0.43349 (5)0.5505 (2)0.70884 (10)0.0845 (5)
N1B0.37844 (12)0.5644 (5)0.6509 (3)0.0685 (10)
C1B0.45945 (13)0.6522 (5)0.6095 (3)0.0553 (10)
C2B0.42449 (13)0.7000 (5)0.5282 (3)0.0572 (10)
C3B0.37930 (14)0.6495 (5)0.5530 (3)0.0574 (10)
C4B0.33506 (13)0.6768 (5)0.4805 (3)0.0524 (9)
C5B0.33329 (14)0.7855 (6)0.3882 (3)0.0624 (11)
C6B0.29269 (15)0.8109 (6)0.3201 (3)0.0686 (12)
C7B0.25081 (14)0.7279 (6)0.3411 (3)0.0610 (10)
C8B0.25289 (14)0.6182 (6)0.4341 (4)0.0642 (11)
C9B0.29366 (14)0.5922 (6)0.5025 (3)0.0583 (10)
C10B0.50983 (13)0.6700 (5)0.6126 (3)0.0523 (9)
C11B0.54025 (14)0.5850 (6)0.6950 (3)0.0628 (11)
C12B0.58746 (16)0.6008 (7)0.6975 (4)0.0801 (14)
C13B0.60644 (17)0.7032 (7)0.6184 (5)0.0831 (15)
C14B0.57752 (16)0.7858 (6)0.5366 (4)0.0732 (12)
C15B0.52998 (14)0.7693 (6)0.5326 (3)0.0623 (10)
C16B0.20659 (15)0.7537 (7)0.2656 (4)0.0795 (13)
H2B0.4299090.7591730.4637080.069*
H5B0.3604660.8429660.3718610.075*
H6B0.2928330.8849710.2585540.082*
H8B0.2257580.5606200.4505160.077*
H9B0.2937400.5178400.5640460.070*
H11B0.5279180.5166730.7487600.075*
H12B0.6071100.5428270.7524980.096*
H13B0.6387500.7156400.6210790.100*
H14B0.5902700.8537170.4832220.088*
H15B0.5107450.8249930.4759320.075*
H16D0.1946450.6375710.2401690.119*
H16E0.2128540.8262090.2037410.119*
H16F0.1838350.8138890.3044430.119*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
S1A0.0913 (9)0.0871 (9)0.0564 (6)0.0087 (7)0.0140 (6)0.0128 (6)
N1A0.069 (2)0.070 (2)0.0332 (15)0.0157 (17)0.0129 (13)0.0029 (14)
C1A0.064 (2)0.041 (2)0.0427 (18)0.0008 (17)0.0098 (16)0.0043 (15)
C2A0.061 (2)0.047 (2)0.0443 (19)0.0006 (18)0.0054 (17)0.0013 (16)
C3A0.060 (2)0.046 (2)0.0458 (19)0.0005 (17)0.0034 (16)0.0044 (16)
C4A0.059 (2)0.043 (2)0.0463 (19)0.0030 (17)0.0022 (16)0.0026 (16)
C5A0.063 (3)0.074 (3)0.043 (2)0.002 (2)0.0046 (17)0.0007 (19)
C6A0.060 (3)0.080 (3)0.051 (2)0.012 (2)0.0007 (18)0.001 (2)
C7A0.058 (2)0.050 (2)0.073 (3)0.0021 (19)0.001 (2)0.006 (2)
C8A0.064 (3)0.062 (3)0.069 (3)0.005 (2)0.016 (2)0.008 (2)
C9A0.061 (3)0.067 (3)0.056 (2)0.003 (2)0.0077 (19)0.013 (2)
C10A0.054 (2)0.040 (2)0.0492 (19)0.0006 (16)0.0101 (16)0.0062 (16)
C11A0.074 (3)0.054 (2)0.054 (2)0.001 (2)0.0129 (19)0.0041 (18)
C12A0.054 (3)0.072 (3)0.088 (3)0.010 (2)0.020 (2)0.003 (2)
C13A0.060 (3)0.070 (3)0.080 (3)0.003 (2)0.006 (2)0.005 (2)
C14A0.065 (3)0.065 (3)0.070 (3)0.005 (2)0.005 (2)0.009 (2)
C15A0.059 (2)0.054 (2)0.057 (2)0.0022 (19)0.0120 (18)0.0084 (18)
C16A0.061 (3)0.085 (4)0.110 (4)0.008 (2)0.000 (3)0.001 (3)
S1B0.0821 (9)0.1074 (11)0.0650 (7)0.0073 (7)0.0128 (6)0.0202 (7)
N1B0.063 (2)0.088 (3)0.056 (2)0.0101 (19)0.0108 (16)0.0065 (18)
C1B0.057 (2)0.047 (2)0.061 (2)0.0029 (17)0.0046 (18)0.0113 (18)
C2B0.053 (2)0.057 (2)0.061 (2)0.0001 (18)0.0033 (18)0.0039 (18)
C3B0.062 (2)0.054 (2)0.057 (2)0.0087 (19)0.0096 (18)0.0096 (18)
C4B0.051 (2)0.057 (2)0.051 (2)0.0054 (18)0.0099 (16)0.0064 (17)
C5B0.055 (2)0.073 (3)0.059 (2)0.003 (2)0.0104 (18)0.009 (2)
C6B0.070 (3)0.077 (3)0.059 (2)0.003 (2)0.007 (2)0.010 (2)
C7B0.057 (2)0.060 (3)0.065 (2)0.008 (2)0.0019 (19)0.011 (2)
C8B0.054 (2)0.069 (3)0.072 (3)0.004 (2)0.015 (2)0.003 (2)
C9B0.060 (2)0.060 (3)0.056 (2)0.0007 (19)0.0103 (18)0.0038 (18)
C10B0.054 (2)0.047 (2)0.055 (2)0.0014 (17)0.0033 (17)0.0122 (17)
C11B0.061 (3)0.065 (3)0.061 (2)0.004 (2)0.0007 (19)0.004 (2)
C12B0.057 (3)0.092 (4)0.087 (3)0.013 (2)0.012 (2)0.017 (3)
C13B0.059 (3)0.086 (4)0.106 (4)0.007 (3)0.015 (3)0.037 (3)
C14B0.069 (3)0.068 (3)0.085 (3)0.005 (2)0.022 (2)0.010 (2)
C15B0.064 (3)0.056 (3)0.067 (2)0.002 (2)0.005 (2)0.002 (2)
C16B0.062 (3)0.080 (3)0.093 (3)0.008 (2)0.009 (2)0.004 (3)
Geometric parameters (Å, º) top
S1A—N1A1.551 (4)S1B—N1B1.660 (4)
S1A—C1A1.696 (4)S1B—C1B1.674 (4)
C3A—C2A1.409 (5)C3B—N1B1.353 (5)
C3A—N1A1.425 (5)C3B—C2B1.417 (5)
C3A—C4A1.479 (5)C3B—C4B1.477 (5)
C4A—C9A1.388 (5)C10B—C15B1.399 (6)
C4A—C5A1.388 (5)C10B—C11B1.403 (5)
C10A—C11A1.394 (5)C10B—C1B1.450 (5)
C10A—C15A1.395 (5)C4B—C5B1.380 (5)
C10A—C1A1.468 (5)C4B—C9B1.397 (5)
C7A—C6A1.383 (5)C1B—C2B1.374 (5)
C7A—C8A1.386 (6)C11B—C12B1.359 (6)
C7A—C16A1.505 (6)C11B—H11B0.9300
C1A—C2A1.375 (5)C9B—C8B1.371 (6)
C2A—H2A0.9300C9B—H9B0.9300
C11A—C12A1.355 (6)C7B—C8B1.390 (6)
C11A—H11A0.9300C7B—C6B1.400 (6)
C8A—C9A1.354 (6)C7B—C16B1.494 (6)
C8A—H8A0.9300C5B—C6B1.365 (5)
C9A—H9A0.9300C5B—H5B0.9300
C5A—C6A1.387 (5)C2B—H2B0.9300
C5A—H5A0.9300C8B—H8B0.9300
C12A—C13A1.374 (6)C6B—H6B0.9300
C12A—H12A0.9300C15B—C14B1.367 (6)
C15A—C14A1.360 (5)C15B—H15B0.9300
C15A—H15A0.9300C12B—C13B1.387 (7)
C6A—H6A0.9300C12B—H12B0.9300
C14A—C13A1.390 (6)C14B—C13B1.367 (7)
C14A—H14A0.9300C14B—H14B0.9300
C13A—H13A0.9300C13B—H13B0.9300
C16A—H16A0.9600C16B—H16D0.9600
C16A—H16B0.9600C16B—H16E0.9600
C16A—H16C0.9600C16B—H16F0.9600
N1A—S1A—C1A99.56 (17)N1B—S1B—C1B98.40 (18)
C2A—C3A—N1A112.6 (3)N1B—C3B—C2B115.0 (4)
C2A—C3A—C4A126.4 (3)N1B—C3B—C4B119.4 (4)
N1A—C3A—C4A121.0 (3)C2B—C3B—C4B125.6 (4)
C9A—C4A—C5A117.3 (4)C15B—C10B—C11B117.5 (4)
C9A—C4A—C3A120.5 (3)C15B—C10B—C1B121.5 (4)
C5A—C4A—C3A122.3 (3)C11B—C10B—C1B121.0 (4)
C11A—C10A—C15A117.2 (3)C5B—C4B—C9B117.8 (4)
C11A—C10A—C1A121.7 (3)C5B—C4B—C3B121.1 (4)
C15A—C10A—C1A121.1 (3)C9B—C4B—C3B121.1 (4)
C6A—C7A—C8A116.8 (4)C3B—N1B—S1B106.9 (3)
C6A—C7A—C16A121.1 (4)C2B—C1B—C10B129.8 (4)
C8A—C7A—C16A122.0 (4)C2B—C1B—S1B106.8 (3)
C2A—C1A—C10A130.2 (3)C10B—C1B—S1B123.3 (3)
C2A—C1A—S1A106.7 (3)C12B—C11B—C10B121.0 (4)
C10A—C1A—S1A123.1 (3)C12B—C11B—H11B119.5
C1A—C2A—C3A112.3 (3)C10B—C11B—H11B119.5
C1A—C2A—H2A123.8C8B—C9B—C4B120.4 (4)
C3A—C2A—H2A123.8C8B—C9B—H9B119.8
C3A—N1A—S1A108.7 (2)C4B—C9B—H9B119.8
C12A—C11A—C10A121.4 (4)C8B—C7B—C6B116.6 (4)
C12A—C11A—H11A119.3C8B—C7B—C16B122.1 (4)
C10A—C11A—H11A119.3C6B—C7B—C16B121.3 (4)
C9A—C8A—C7A122.1 (4)C6B—C5B—C4B121.7 (4)
C9A—C8A—H8A119.0C6B—C5B—H5B119.2
C7A—C8A—H8A119.0C4B—C5B—H5B119.2
C8A—C9A—C4A121.6 (4)C1B—C2B—C3B112.9 (4)
C8A—C9A—H9A119.2C1B—C2B—H2B123.5
C4A—C9A—H9A119.2C3B—C2B—H2B123.5
C6A—C5A—C4A120.6 (4)C9B—C8B—C7B122.2 (4)
C6A—C5A—H5A119.7C9B—C8B—H8B118.9
C4A—C5A—H5A119.7C7B—C8B—H8B118.9
C11A—C12A—C13A121.1 (4)C5B—C6B—C7B121.4 (4)
C11A—C12A—H12A119.4C5B—C6B—H6B119.3
C13A—C12A—H12A119.4C7B—C6B—H6B119.3
C14A—C15A—C10A121.2 (4)C14B—C15B—C10B121.0 (4)
C14A—C15A—H15A119.4C14B—C15B—H15B119.5
C10A—C15A—H15A119.4C10B—C15B—H15B119.5
C7A—C6A—C5A121.6 (4)C11B—C12B—C13B120.2 (5)
C7A—C6A—H6A119.2C11B—C12B—H12B119.9
C5A—C6A—H6A119.2C13B—C12B—H12B119.9
C15A—C14A—C13A120.6 (4)C13B—C14B—C15B120.4 (5)
C15A—C14A—H14A119.7C13B—C14B—H14B119.8
C13A—C14A—H14A119.7C15B—C14B—H14B119.8
C12A—C13A—C14A118.5 (4)C14B—C13B—C12B119.8 (5)
C12A—C13A—H13A120.8C14B—C13B—H13B120.1
C14A—C13A—H13A120.8C12B—C13B—H13B120.1
C7A—C16A—H16A109.5C7B—C16B—H16D109.5
C7A—C16A—H16B109.5C7B—C16B—H16E109.5
H16A—C16A—H16B109.5H16D—C16B—H16E109.5
C7A—C16A—H16C109.5C7B—C16B—H16F109.5
H16A—C16A—H16C109.5H16D—C16B—H16F109.5
H16B—C16A—H16C109.5H16E—C16B—H16F109.5
C2A—C3A—C4A—C9A175.5 (4)N1B—C3B—C4B—C5B170.4 (4)
N1A—C3A—C4A—C9A6.4 (6)C2B—C3B—C4B—C5B11.9 (6)
C2A—C3A—C4A—C5A4.7 (6)N1B—C3B—C4B—C9B10.1 (6)
N1A—C3A—C4A—C5A173.4 (3)C2B—C3B—C4B—C9B167.6 (4)
C11A—C10A—C1A—C2A174.2 (4)C2B—C3B—N1B—S1B0.2 (4)
C15A—C10A—C1A—C2A5.7 (6)C4B—C3B—N1B—S1B178.2 (3)
C11A—C10A—C1A—S1A5.2 (5)C1B—S1B—N1B—C3B0.2 (3)
C15A—C10A—C1A—S1A174.8 (3)C15B—C10B—C1B—C2B9.9 (6)
N1A—S1A—C1A—C2A0.6 (3)C11B—C10B—C1B—C2B168.9 (4)
N1A—S1A—C1A—C10A179.0 (3)C15B—C10B—C1B—S1B174.5 (3)
C10A—C1A—C2A—C3A179.3 (3)C11B—C10B—C1B—S1B6.7 (5)
S1A—C1A—C2A—C3A0.2 (4)N1B—S1B—C1B—C2B0.2 (3)
N1A—C3A—C2A—C1A0.3 (4)N1B—S1B—C1B—C10B176.2 (3)
C4A—C3A—C2A—C1A178.5 (3)C15B—C10B—C11B—C12B0.8 (6)
C2A—C3A—N1A—S1A0.7 (4)C1B—C10B—C11B—C12B179.7 (4)
C4A—C3A—N1A—S1A179.0 (3)C5B—C4B—C9B—C8B0.2 (6)
C1A—S1A—N1A—C3A0.7 (3)C3B—C4B—C9B—C8B179.7 (4)
C15A—C10A—C11A—C12A0.1 (6)C9B—C4B—C5B—C6B0.1 (6)
C1A—C10A—C11A—C12A179.9 (4)C3B—C4B—C5B—C6B179.6 (4)
C6A—C7A—C8A—C9A1.5 (7)C10B—C1B—C2B—C3B176.0 (4)
C16A—C7A—C8A—C9A179.1 (4)S1B—C1B—C2B—C3B0.2 (4)
C7A—C8A—C9A—C4A0.3 (7)N1B—C3B—C2B—C1B0.0 (5)
C5A—C4A—C9A—C8A1.6 (6)C4B—C3B—C2B—C1B177.8 (3)
C3A—C4A—C9A—C8A178.2 (4)C4B—C9B—C8B—C7B0.0 (6)
C9A—C4A—C5A—C6A1.2 (6)C6B—C7B—C8B—C9B0.2 (6)
C3A—C4A—C5A—C6A178.7 (4)C16B—C7B—C8B—C9B179.0 (4)
C10A—C11A—C12A—C13A0.1 (7)C4B—C5B—C6B—C7B0.1 (7)
C11A—C10A—C15A—C14A0.2 (6)C8B—C7B—C6B—C5B0.3 (6)
C1A—C10A—C15A—C14A179.8 (4)C16B—C7B—C6B—C5B179.1 (4)
C8A—C7A—C6A—C5A1.9 (6)C11B—C10B—C15B—C14B1.5 (6)
C16A—C7A—C6A—C5A179.5 (4)C1B—C10B—C15B—C14B179.7 (4)
C4A—C5A—C6A—C7A0.6 (7)C10B—C11B—C12B—C13B0.5 (7)
C10A—C15A—C14A—C13A0.0 (6)C10B—C15B—C14B—C13B0.8 (7)
C11A—C12A—C13A—C14A0.3 (7)C15B—C14B—C13B—C12B0.5 (7)
C15A—C14A—C13A—C12A0.2 (7)C11B—C12B—C13B—C14B1.1 (7)
 

Acknowledgements

The authors are thankful to the BMSIT&M, Bengaluru and GEC, Chamarajanagara for lab support..

References

Return to citationBruker (2012). APEX and SAINT. Bruker AXS Inc., Madison, Wisconsin, USA.  Google Scholar
Return to citationFait, M. J. G., Spannenberg, A., Kondratenko, E. V. & Linke, D. (2021). IUCrData 6, x211332.  Google Scholar
Return to citationGuseinov, F. I., Afanaseva, K. A., Gaidar, S. M., Pikina, A. M., Akkurt, M., Aliyeva, F. S., Hasanov, K. I. & Belay, A. N. (2026). Acta Cryst. E82, 14–18.  CrossRef IUCr Journals Google Scholar
Return to citationKaberdin, R. V. & Potkin, V. I. (2002). Russ. Chem. Rev. 71, 673–694.  CrossRef CAS Google Scholar
Return to citationMacrae, C. F., Sovago, I., Cottrell, S. J., Galek, P. T. A., McCabe, P., Pidcock, E., Platings, M., Shields, G. P., Stevens, J. S., Towler, M. & Wood, P. A. (2020). J. Appl. Cryst. 53, 226–235.  Web of Science CrossRef CAS IUCr Journals Google Scholar
Return to citationMeundaeng, N., Rujiwatra, A. & Prior, T. J. (2019). Acta Cryst. E75, 185–188.  CrossRef IUCr Journals Google Scholar
Return to citationSheldrick, G. M. (2015a). Acta Cryst. A71, 3–8.  Web of Science CrossRef IUCr Journals Google Scholar
Return to citationSheldrick, G. M. (2015b). Acta Cryst. C71, 3–8.  Web of Science CrossRef IUCr Journals Google Scholar
Return to citationSreenatha, N. R., Jeevan Chakravarthy, A. S., Lakshminarayana, B. N. & Hariprasad, S. (2021). J. Mol. Struct. 1225, 129116.  CrossRef Google Scholar
Return to citationSreenatha, N. R., Lakshminarayana, B. N., Ganesha, D. P. & Gnanendra, C. R. (2018). Acta Cryst. E74, 1451–1454.  Web of Science CSD CrossRef IUCr Journals Google Scholar
Return to citationZhang, Z.-Z., Chen, R., Zhang, X.-H. & Zhang, X.-G. (2021). J. Org. Chem. 86, 636–642.  Google Scholar

This is an open-access article distributed under the terms of the Creative Commons Attribution (CC-BY) Licence, which permits unrestricted use, distribution, and reproduction in any medium, provided the original authors and source are cited.

Journal logoIUCrDATA
ISSN: 2414-3146