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

Journal logoCRYSTALLOGRAPHIC
COMMUNICATIONS
ISSN: 2056-9890

Crystal structures and Hirshfeld surface comparison of fumarate and bromide salts of the etoxazole metabolite designated R7 (aminium ions)

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aDepartment of Physical Sciences, Amrita School of Engineering, Amrita Vishwa Vidyapeetham, Bengaluru-560 035, India, bDepartment of Applied Sciences, New Horizon College of Engineering, Bengaluru-560 103, India, cDepartment of Studies in Chemistry, University of Mysore, Manasagangotri, Mysuru-570 006, India, and dDepartment of Chemistry, University of Kentucky, Lexington, KY, 40506-0055, USA
*Correspondence e-mail: [email protected]

Edited by X. Hao, Institute of Chemistry, Chinese Academy of Sciences (Received 23 February 2026; accepted 27 February 2026; online 5 March 2026)

Etoxazole (C21H23F2NO2) is a fluorinated insecticide/acaricide that acts as an inhibitor of chitin biosynthesis. Its degradation products include several persistent environmental contaminants, including a metabolite designated ‘R7’ (C19H25F2NO3), which has a readily protonated amine group, to give the R7H+ cation, namely, 2-aza­niumyl-2-(4-tert-butyl-2-eth­oxy­phen­yl)ethyl 2,6-di­fluoro­benzoate. This paper reports the crystal structures of two salts of R7H+: the bromide (I: C21H26F2NO3+·Br) and the 3-carb­oxy­prop-2-enoate (hereafter fumarate) (II: C21H26F2NO3+·C4H3O4). Although the R7H+ cations in I and II are chemically identical, the salts crystallize in substanti­ally different structures. Crystals of I are tetra­gonal, space-group type P421c, whereas those of II are monoclinic, space-group type P21/n, each containing one cation–anion pair in their respective asymmetric units (Z′ = 1). The R7H+ cation in both structures feature a central 2-aza­niumyl linker connecting 4-tert-butyl-2-eth­oxy­phenyl and 2,6-di­fluoro­benzoate rings. Cation conformation is primarily governed by different torsional degrees of freedom, leading to distinct overall conformations. The crystal packing in I is driven by N—H⋯Br hydrogen bonds, ππ and C—H⋯π inter­actions, which arrange the cations into columns parallel to the crystallographic c-axis. In contrast, the packing in II consists of N—H⋯O hydrogen bonds to adjacent fumarate anions, forming extended hydrogen-bonded chains. The fumarate anions are sandwiched between R7H+ cations, placing the fumarate double bond between aromatic rings. Hirshfeld-surface analysis shows that inter­molecular contacts in both structures are dominated by inter­actions involving hydrogen (93.4% in I, 92.2% in II).

1. Chemical context

Etoxazole [C21H23F2NO2, systematic name 4-(4-tert-butyl-2-eth­oxy­phen­yl)-2-(2,6-di­fluoro­phen­yl)-4,5-di­hydro-1,3-oxazole], is an oxazoline-based fluorinated insecticide/acaricide, which acts as an inhibitor of chitin biosynthesis. It was developed as a new-generation pesticide to address the growing resistance of spider mites to traditional acaricides, and was selected for development in 1990, achieving registration in 1998 (Suzuki et al., 2002View full citation). This classification reflects its superior bioactivity and novel target compared to established chitin synthesis inhibitors, pyrethroids, and organophosphate (Li et al., 2014View full citation) and has been deployed globally since 1998 (Park et al., 2020View full citation). The synthesis and activity of various 2,4-diphenyl-1,3-oxazolines with acaricidal/insecticidal properties were reported by Suzuki et al. (2002View full citation). Metabolic studies of etoxazole by Sun et al. (2019View full citation), Macar et al. (2022View full citation) and others, have revealed several distinct metabolites resulting from oxidative degradation, especially of its oxazoline ring. These environmental contaminants have been found in plants, earthworms, and soil (Sun et al., 2019View full citation), as well as in rats (Yilmaz et al., 2017View full citation). In view of the agricultural and environmental significance of etoxazole and its metabolites, we have recently reported the crystal structures of etoxazole itself (Sowbhagya et al., 2025aView full citation), as well as the etoxazole metabolites designated R13 (Mohan Kumar et al., 2024View full citation) and R4 (Sowbhagya et al., 2025bView full citation). Another related degradation product of etoxazole is the R7 metabolite [C19H25F2NO3, systematic name: 2-amino-2-(4-tert-butyl-2-eth­oxy­phen­yl)ethyl 2,6-di­fluoro­benzoate], which has an amino group that readily protonates to form an aminium ion, R7H+. This paper reports crystal structures of the bromide (I: C21H26BrF2NO3) and fumarate (II: C25H29F2NO7) salts of R7H+.

[Scheme 1]

2. Structural commentary

In spite of having chemically identical cations, the crystal structures of I and II are substanti­ally different. Crystals of I are tetra­gonal, space-group type PMathematical equation21c, whereas those of II are monoclinic, space-group type P21/n, though both have one mol­ecule in their respective asymmetric units (Z′ = 1).

The R7H+ cation in each salt is comprised of a central 2-aza­niumyl (CH2CHNH3+) linker flanked by 4-tert-butyl-2-eth­oxy­phenyl and 2,6-di­fluoro­benzoate substituted rings, as shown in Figs. 1[link] and 2[link]. No unusual bond lengths or angles are found in either structure. The conformations of the R7H+ cations are governed primarily by torsional degrees of freedom about the C3—C4, C2—C3, O1—C2, and C1—C16 bonds. These are shown qualitatively in a least-squares overlay plot (Fig. 3[link]) and qu­anti­fied in Table 1[link]. In the central 2-aza­niumyl moiety, atom C3 is stereogenic , but both structures are strictly racemic (I is non-centrosymmetric but possesses a c-glide). The chosen asymmetric units for I and II both had C3 assigned as R. A least-squares fit overlay of all 27 non-H cation atoms, however, yields a smaller r.m.s. deviation (1.1328 Å vs 1.5544 Å) when one structure is inverted relative to the other. Thus, the R enanti­omer of R7H+ in I has a better overall fit to the S enanti­omer of II and vice versa, which emphasizes the distinct conformations of the two structures.

Table 1
Conformation-defining torsion angles (°) in I and II

Torsion angle I II
C5—C4—C3—C2 98.7 (3) −117.45 (12)
C4—C3—C2—O1 178.0 (2) 160.96 (9)
C3—C2—O1—C1 −120.5 (3) 170.25 (9)
C2—O1—C1—C16 175.2 (2) 175.71 (10)
O1—C1—C16—C21 −144.0 (3) 134.09 (12)
N1—C3—C2—O1 −58.2 (3) −73.64 (10)
N1—C3—C4—C9 155.1 (3) −61.61 (13)
C9—O2—C10—C11 67.6 (4) 164.55 (11)
C4—C9—O2—C10 −161.5 (3) −168.79 (10)
C8—C7—C13—C14 165.0 (2) 123.99 (12)
[Figure 1]
Figure 1
An ellipsoid plot (50% probability) of I. Hydrogen atoms are drawn as small arbitrary circles.
[Figure 2]
Figure 2
An ellipsoid plot (50% probability) of II. Hydrogen atoms are drawn as small arbitrary circles.
[Figure 3]
Figure 3
A least-squares-fit overlay of R7H+ cations from I and II.

3. Supra­molecular features

In I, the only conventional hydrogen-bond donor is the ammonium nitro­gen atom, N1, which forms hydrogen bonds to three symmetry-related Br anions. These are: N1—H1A⋯Br1i, N1—H1B⋯Br1ii, and N1—H1C⋯Br1 (symmcodes and distances are given in Table 2[link]). In addition, the contact N1—H1A⋯F1ii and three weak contacts with C—H as donor are flagged as ‘potential hydrogen bonds' by SHELXL (details in Table 2[link]). There are also ππ and C—H⋯π contacts in I. Di­fluoro­benzene ring C16–C21 π-stacks with its counterpart at (1 − x, 2 − y, z) DCgCg = 3.814 (2) Å, while ring C4–C9 is in close contact with H18ii, DCg⋯H = 2.73 Å. Each type of inter­action is shown in Fig. 4[link]a. In combination, these contacts connect the R7H+ cations into columns parallel to the c-axis, which pack in a square array to give the overall tetra­gonal packing symmetry, as shown in Fig. 4[link]b.

Table 2
Hydrogen-bond geometry (Å, °) for I[link]

D—H⋯A D—H H⋯A DA D—H⋯A
N1—H1A⋯Br1i 0.88 2.57 3.337 (2) 147
N1—H1A⋯F1ii 0.88 2.52 3.073 (3) 122
N1—H1B⋯Br1ii 0.88 2.39 3.259 (2) 170
N1—H1C⋯Br1 0.88 2.38 3.252 (2) 175
C10—H10A⋯Br1iii 0.99 2.75 3.650 (3) 152
C2—H2B⋯O2 0.99 2.62 3.116 (4) 111
C8—H8⋯Br1iii 0.95 3.10 4.040 (3) 170
Symmetry codes: (i) Mathematical equation; (ii) Mathematical equation; (iii) Mathematical equation.
[Figure 4]
Figure 4
(a) A partial packing plot of I. Hydrogen bonds are shown as thick dotted lines, N—H⋯F contacts as open dashed lines, ππ stacked rings by thin dashed lines, and C—H⋯π contacts as dotted lines. (b) A view down the crystallographic c-axis showing the fourfold symmetry.

In II, the R7H+ ammonium group also forms three conventional hydrogen bonds. Two of these are to O4 of adjacent fumarate anions, namely N1—H1C⋯O4 and N1—H1A⋯O4i (distances, angles and symmcodes are given in Table 3[link]). The remaining hydrogen bond is intra­molecular, N1—H1B⋯O2, within the R7H+ cation. Atom H1B is also in close contact with a symmetry-related fumarate O7, i.e., N1—H1B⋯O7ii, but the angle is small (111.5°, Table 3[link]). In addition, the fumarate anions form extended O6—H6A⋯O5iv hydrogen-bonded chains. As in I, there are also weaker contacts with C—H as donor, which are also given in Table 3[link]. There is no ππ stacking of rings in I, but the central double bond of the fumarate anion sits sandwiched between the planes of ring C4–C9 and C16–C19i at a distances of 3.512 and 3.636, Å, respectively between ring and double-bond centroids. These inter­actions are shown in Fig. 5[link].

Table 3
Hydrogen-bond geometry (Å, °) for II[link]

D—H⋯A D—H H⋯A DA D—H⋯A
N1—H1A⋯O4i 0.89 1.89 2.7160 (12) 152
N1—H1B⋯O2 0.89 2.30 2.8889 (12) 123
N1—H1B⋯O7ii 0.89 2.36 2.8103 (13) 112
N1—H1C⋯O4 0.89 1.84 2.6915 (12) 158
C2—H2A⋯O7ii 0.99 2.53 3.1832 (15) 123
C2—H2B⋯O3iii 0.99 2.48 3.1727 (15) 127
O6—H6A⋯O5iv 0.92 1.62 2.5184 (11) 165
Symmetry codes: (i) Mathematical equation; (ii) Mathematical equation; (iii) Mathematical equation; (iv) Mathematical equation.
[Figure 5]
Figure 5
A partial packing plot of II. Hydrogen bonds are shown as thick dotted lines and overlap of the fumarate double bond with aromatic rings as thin dashed lines.

A Hirshfeld surface analysis using CrystalExplorer (Spackman et al., 2021View full citation) shows that the most important inter­molecular contacts for the R7H+ cation in I and II involve hydrogen (93.4% in I, 92.2% in II), with over 50% being H⋯H in both structures. These are summarized pairwise for ease of comparison in Fig. 6[link].

[Figure 6]
Figure 6
Hirshfeld-surface fingerprint plots of the most abundant types of atom-atom contacts in I and II. (a),(b) H⋯H contacts, (c),(d) H⋯F, (e),(f) H⋯C, (g),(h) H⋯O/Br and H⋯O contacts. For ease of comparison of the hydrogen-bonding contacts of the ammonium cation, panel (g) is a composite of H⋯O and H⋯Br contacts.

4. Database survey

A search of the Cambridge Structural Database (CSD v6.0, April 2025: Groom et al., 2016View full citation) using a search fragment consisting of the R7 backbone but with the tert-butyl, eth­oxy, and fluoride substituents set to ‘any group' and the carbon–nitro­gen and carbon­yl–group bonds set to ‘any type' returned 64 hits. Of these, none includes either unsubstituted amino (–NH2) or ammonium (–NH3+) groups. Furthermore, only three structures include fluorine substituents: CSD refcodes AFABUE (Maligres et al., 2002View full citation) and CIBKUT (Seiler et al., 1999View full citation) have –CF3 groups, while LEZRIU (Xing et al., 2018View full citation) has a single fluorine atom at the 4-position of the benzoate ring, but otherwise have little in common with R7. Other related structures include the parent mol­ecule etoxazole (DULGUQ: Sowbhagya et al., 2025aView full citation) and its R4 (ULOVAW: Sowbhagya et al., 2025bView full citation) and R13 (UGUQUM: Mohan Kumar et al., 2024View full citation) metabolites.

5. Synthesis and crystallization

Solutions of the etoxazole metabolite R7 (100 mg, 0.265 mmol) in methanol (5 ml) were mixed with either equimolar qu­anti­ties of a methano­lic solution of fumaric acid (31 mg) or 2 ml of HBr (48% aqueous solution) in 10 ml of methanol and stirred for an hour at 313 K. The mixtures were set aside for slow evaporation for 24 h. The resulting crystals, suitable for X-ray diffraction analysis, were collected by filtration and air dried.

6. Refinement

Crystal data, data collection and structure refinement details are summarized in Table 4[link]. All hydrogen atoms were found in difference-Fourier maps, but subsequently included in the refinement using riding models. Carbon-bound hydrogen atoms were affixed with constrained distances set to 0.95 Å (Csp2—H), 0.98 Å (RCH3), 0.99 Å (R2CH2) and 1.00 Å (R3CH). Hydrogen atoms bound to nitro­gen and oxygen used riding models that allowed their bond distances to refine. Uiso(H) parameters were set to values of either 1.2Ueq or 1.5Ueq (RCH3, RNH3, OH) of the attached atom.

Table 4
Experimental details

  I II
Crystal data
Chemical formula C21H26F2NO3+·Br C21H26F2NO3+·C4H3O4
Mr 458.34 493.49
Crystal system, space group Tetragonal, PMathematical equation21c Monoclinic, P21/n
Temperature (K) 100 100
a, b, c (Å) 15.2984 (2), 15.2984 (2), 17.8818 (3) 12.0615 (2), 15.3673 (3), 14.0141 (3)
α, β, γ (°) 90, 90, 90 90, 110.506 (1), 90
V3) 4185.07 (13) 2432.96 (8)
Z 8 4
Radiation type Mo Kα Mo Kα
μ (mm−1) 2.00 0.11
Crystal size (mm) 0.21 × 0.19 × 0.18 0.19 × 0.18 × 0.12
 
Data collection
Diffractometer Bruker D8 Venture dual source Bruker D8 Venture dual source
Absorption correction Multi-scan (SADABS; Krause et al., 2015View full citation) Multi-scan (SADABS; Krause et al., 2015View full citation)
Tmin, Tmax 0.830, 0.928 0.917, 0.971
No. of measured, independent and observed [I > 2σ(I)] reflections 75181, 4795, 4496 42339, 5576, 4976
Rint 0.049 0.031
(sin θ/λ)max−1) 0.650 0.650
 
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.024, 0.058, 1.03 0.036, 0.101, 1.03
No. of reflections 4795 5576
No. of parameters 259 324
H-atom treatment H atoms treated by a mixture of independent and constrained refinement H atoms treated by a mixture of independent and constrained refinement
Δρmax, Δρmin (e Å−3) 0.80, −0.44 0.34, −0.21
Absolute structure Flack x determined using 1911 quotients [(I+)−(I)]/[(I+)+(I)] (Parsons et al., 2013View full citation)
Absolute structure parameter 0.018 (3)
Computer programs: APEX5 (Bruker, 2023View full citation), SHELXT (Sheldrick, 2015aView full citation), SHELXL2025/1 (Sheldrick, 2015bView full citation), XP in SHELXTL (Sheldrick, 2008View full citation), over-lay (Parkin, 2025View full citation) and publCIF (Westrip, 2010View full citation).

Supporting information


Computing details top

2-Azaniumyl-2-(4-tert-butyl-2-ethoxyphenyl)ethyl 2,6-difluorobenzoate bromide (I) top
Crystal data top
C21H26F2NO3+·BrDx = 1.455 Mg m3
Mr = 458.34Mo Kα radiation, λ = 0.71073 Å
Tetragonal, P421cCell parameters from 9610 reflections
a = 15.2984 (2) Åθ = 2.6–27.5°
c = 17.8818 (3) ŵ = 2.00 mm1
V = 4185.07 (13) Å3T = 100 K
Z = 8Irregular block, colourless
F(000) = 18880.21 × 0.19 × 0.18 mm
Data collection top
Bruker D8 Venture dual source
diffractometer
4795 independent reflections
Radiation source: microsource4496 reflections with I > 2σ(I)
Detector resolution: 7.41 pixels mm-1Rint = 0.049
φ and ω scansθmax = 27.5°, θmin = 1.9°
Absorption correction: multi-scan
(SADABS; Krause et al., 2015)
h = 1919
Tmin = 0.830, Tmax = 0.928k = 1916
75181 measured reflectionsl = 2323
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.024H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.058 w = 1/[σ2(Fo2) + (0.0243P)2 + 2.4223P]
where P = (Fo2 + 2Fc2)/3
S = 1.03(Δ/σ)max = 0.002
4795 reflectionsΔρmax = 0.80 e Å3
259 parametersΔρmin = 0.44 e Å3
0 restraintsAbsolute structure: Flack x determined using 1911 quotients [(I+)-(I-)]/[(I+)+(I-)] (Parsons et al., 2013)
Primary atom site location: structure-invariant direct methodsAbsolute structure parameter: 0.018 (3)
Special details top

Experimental. The crystal was mounted using polyisobutene oil on the tip of a fine glass fibre, which was fastened in a copper mounting pin with electrical solder. It was placed directly into the cold gas stream of a liquid-nitrogen based cryostat (Hope, 1994; Parkin & Hope, 1998).

Diffraction data were collected with the crystal at 100K.

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. Refinement progress was checked using Platon (Spek, 2020) and by an R-tensor (Parkin, 2000). The final model was further checked with the IUCr utility checkCIF.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Br10.62255 (2)0.58962 (2)0.39254 (2)0.01946 (8)
F10.57938 (12)0.78020 (12)0.58387 (9)0.0244 (4)
F20.34194 (13)0.97753 (13)0.58768 (10)0.0315 (5)
O10.46509 (15)0.79073 (13)0.47217 (11)0.0210 (5)
O20.27044 (14)0.80263 (14)0.31527 (11)0.0218 (4)
O30.4237 (2)0.93037 (16)0.45861 (13)0.0469 (8)
N10.41590 (16)0.62168 (16)0.42530 (12)0.0179 (4)
H1A0.3844 (11)0.5764 (10)0.4118 (9)0.027*
H1B0.4117 (13)0.6290 (6)0.4739 (10)0.027*
H1C0.4708 (12)0.6127 (8)0.4132 (9)0.027*
C10.4477 (2)0.8717 (2)0.49735 (16)0.0212 (6)
C20.45015 (19)0.77420 (19)0.39362 (18)0.0209 (6)
H2A0.5055360.7569440.3690780.025*
H2B0.4280660.8277520.3689480.025*
C30.38341 (18)0.70115 (18)0.38652 (15)0.0173 (5)
H30.3283930.7203970.4118410.021*
C40.36260 (19)0.68309 (19)0.30538 (15)0.0170 (6)
C50.39957 (18)0.61581 (19)0.26437 (14)0.0188 (6)
H50.4419880.5790180.2870630.023*
C60.3753 (2)0.60129 (19)0.19004 (15)0.0201 (6)
H60.4010340.5544580.1629430.024*
C70.31381 (19)0.65487 (19)0.15526 (15)0.0170 (6)
C80.27756 (19)0.7236 (2)0.19644 (16)0.0175 (6)
H80.2361740.7614100.1735540.021*
C90.30155 (19)0.73723 (19)0.27069 (15)0.0171 (6)
C100.1902 (2)0.8458 (2)0.29526 (18)0.0290 (7)
H10A0.1945330.8673210.2431860.035*
H10B0.1814940.8969790.3283140.035*
C110.1127 (2)0.7860 (3)0.30182 (19)0.0391 (9)
H11A0.0589840.8190860.2922200.059*
H11B0.1105550.7612480.3523390.059*
H11C0.1179190.7386440.2651850.059*
C120.2838 (2)0.64002 (19)0.07426 (15)0.0195 (6)
C130.1847 (2)0.6239 (3)0.07394 (19)0.0356 (8)
H13A0.1657040.6092150.0231440.053*
H13B0.1544160.6768200.0907530.053*
H13C0.1708230.5754310.1077300.053*
C140.3291 (3)0.5618 (2)0.03807 (17)0.0317 (8)
H14A0.3090980.5557380.0137470.048*
H14B0.3147010.5085750.0659920.048*
H14C0.3924830.5708400.0387240.048*
C150.3045 (2)0.7211 (2)0.02736 (17)0.0266 (7)
H15A0.2846340.7118350.0241440.040*
H15B0.3676790.7315380.0276010.040*
H15C0.2743500.7719240.0485830.040*
C160.45887 (19)0.87692 (19)0.58045 (16)0.0184 (6)
C170.52045 (19)0.82971 (19)0.62108 (16)0.0197 (6)
C180.5267 (2)0.8323 (2)0.69799 (16)0.0220 (6)
H180.5703110.7996950.7235170.026*
C190.4672 (2)0.8839 (2)0.73735 (17)0.0244 (7)
H190.4693490.8855330.7904320.029*
C200.4056 (2)0.9324 (2)0.69972 (17)0.0234 (6)
H200.3651030.9676760.7264790.028*
C210.4032 (2)0.92928 (19)0.62289 (17)0.0220 (6)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Br10.01987 (14)0.02421 (15)0.01431 (11)0.00078 (11)0.00101 (12)0.00146 (12)
F10.0237 (9)0.0264 (9)0.0230 (9)0.0065 (8)0.0018 (7)0.0009 (7)
F20.0326 (10)0.0308 (10)0.0312 (11)0.0145 (8)0.0093 (8)0.0051 (8)
O10.0334 (12)0.0155 (10)0.0140 (9)0.0006 (9)0.0079 (8)0.0011 (8)
O20.0258 (11)0.0241 (11)0.0154 (9)0.0063 (9)0.0050 (8)0.0046 (8)
O30.089 (2)0.0268 (13)0.0252 (11)0.0228 (14)0.0070 (14)0.003 (1)
N10.0205 (12)0.0193 (12)0.014 (1)0.0003 (12)0.0012 (9)0.0008 (9)
C10.0248 (15)0.0183 (14)0.0205 (14)0.0000 (13)0.0014 (11)0.0000 (12)
C20.0263 (15)0.0237 (14)0.0127 (11)0.0035 (11)0.0033 (13)0.0004 (13)
C30.0195 (13)0.0193 (13)0.0130 (12)0.0013 (11)0.0013 (12)0.0018 (11)
C40.0188 (14)0.0188 (14)0.0135 (13)0.0028 (11)0.0015 (10)0.0009 (10)
C50.0182 (14)0.0214 (15)0.0170 (12)0.0033 (12)0.0017 (10)0.0013 (11)
C60.0246 (15)0.0191 (15)0.0167 (12)0.0030 (13)0.0005 (12)0.0009 (10)
C70.0185 (14)0.0199 (14)0.0127 (12)0.0046 (12)0.0014 (11)0.0027 (11)
C80.0178 (14)0.0185 (14)0.0161 (13)0.0009 (11)0.0023 (11)0.0020 (11)
C90.0179 (14)0.0190 (14)0.0145 (13)0.0020 (11)0.0014 (11)0.0002 (11)
C100.0338 (18)0.0326 (18)0.0206 (15)0.0144 (15)0.0054 (13)0.0057 (13)
C110.0228 (18)0.067 (3)0.0278 (18)0.0075 (18)0.0006 (14)0.0051 (17)
C120.0276 (16)0.0190 (15)0.0118 (12)0.0013 (12)0.0031 (11)0.0007 (11)
C130.0316 (18)0.053 (2)0.0224 (15)0.0098 (18)0.0063 (14)0.0077 (16)
C140.054 (2)0.0239 (17)0.0171 (14)0.0089 (16)0.0062 (14)0.0036 (12)
C150.041 (2)0.0237 (16)0.0150 (14)0.0003 (15)0.0021 (13)0.0007 (12)
C160.0206 (14)0.0142 (13)0.0203 (13)0.0025 (12)0.0029 (11)0.0005 (11)
C170.0210 (14)0.0147 (14)0.0235 (15)0.0017 (11)0.0008 (11)0.0017 (11)
C180.0227 (16)0.0217 (16)0.0216 (15)0.0008 (13)0.0044 (12)0.0011 (12)
C190.0284 (16)0.0243 (16)0.0205 (14)0.0049 (13)0.0023 (12)0.0018 (13)
C200.0237 (15)0.0227 (16)0.0239 (14)0.0010 (13)0.0008 (12)0.0065 (12)
C210.0208 (14)0.0180 (14)0.0273 (16)0.0008 (11)0.0050 (11)0.0009 (11)
Geometric parameters (Å, º) top
F1—C171.353 (3)C10—C111.502 (5)
F2—C211.349 (3)C10—H10A0.9900
O1—C11.345 (4)C10—H10B0.9900
O1—C21.445 (4)C11—H11A0.9800
O2—C91.365 (3)C11—H11B0.9800
O2—C101.439 (4)C11—H11C0.9800
O3—C11.192 (4)C12—C141.527 (4)
N1—C31.485 (3)C12—C151.531 (4)
N1—H1A0.878 (18)C12—C131.535 (5)
N1—H1B0.878 (18)C13—H13A0.9800
N1—H1C0.878 (18)C13—H13B0.9800
C1—C161.498 (4)C13—H13C0.9800
C2—C31.519 (4)C14—H14A0.9800
C2—H2A0.9900C14—H14B0.9800
C2—H2B0.9900C14—H14C0.9800
C3—C41.511 (4)C15—H15A0.9800
C3—H31.0000C15—H15B0.9800
C4—C51.385 (4)C15—H15C0.9800
C4—C91.394 (4)C16—C171.392 (4)
C5—C61.398 (4)C16—C211.393 (4)
C5—H50.9500C17—C181.379 (4)
C6—C71.395 (4)C18—C191.395 (4)
C6—H60.9500C18—H180.9500
C7—C81.399 (4)C19—C201.377 (5)
C7—C121.536 (4)C19—H190.9500
C8—C91.393 (4)C20—C211.375 (4)
C8—H80.9500C20—H200.9500
C1—O1—C2117.1 (2)C10—C11—H11B109.5
C9—O2—C10119.2 (2)H11A—C11—H11B109.5
C3—N1—H1A109.5C10—C11—H11C109.5
C3—N1—H1B109.5H11A—C11—H11C109.5
H1A—N1—H1B109.5H11B—C11—H11C109.5
C3—N1—H1C109.5C14—C12—C15108.0 (3)
H1A—N1—H1C109.5C14—C12—C13108.7 (3)
H1B—N1—H1C109.5C15—C12—C13109.4 (3)
O3—C1—O1124.1 (3)C14—C12—C7112.3 (3)
O3—C1—C16124.9 (3)C15—C12—C7109.6 (2)
O1—C1—C16111.0 (3)C13—C12—C7108.8 (2)
O1—C2—C3108.4 (2)C12—C13—H13A109.5
O1—C2—H2A110.0C12—C13—H13B109.5
C3—C2—H2A110.0H13A—C13—H13B109.5
O1—C2—H2B110.0C12—C13—H13C109.5
C3—C2—H2B110.0H13A—C13—H13C109.5
H2A—C2—H2B108.4H13B—C13—H13C109.5
N1—C3—C4111.7 (2)C12—C14—H14A109.5
N1—C3—C2109.8 (2)C12—C14—H14B109.5
C4—C3—C2110.9 (2)H14A—C14—H14B109.5
N1—C3—H3108.1C12—C14—H14C109.5
C4—C3—H3108.1H14A—C14—H14C109.5
C2—C3—H3108.1H14B—C14—H14C109.5
C5—C4—C9118.7 (2)C12—C15—H15A109.5
C5—C4—C3124.0 (3)C12—C15—H15B109.5
C9—C4—C3117.4 (3)H15A—C15—H15B109.5
C4—C5—C6120.9 (3)C12—C15—H15C109.5
C4—C5—H5119.6H15A—C15—H15C109.5
C6—C5—H5119.6H15B—C15—H15C109.5
C7—C6—C5120.6 (3)C17—C16—C21115.3 (3)
C7—C6—H6119.7C17—C16—C1124.6 (3)
C5—C6—H6119.7C21—C16—C1120.1 (3)
C6—C7—C8118.4 (3)F1—C17—C18117.4 (3)
C6—C7—C12122.4 (3)F1—C17—C16119.0 (3)
C8—C7—C12119.3 (3)C18—C17—C16123.5 (3)
C9—C8—C7120.6 (3)C17—C18—C19118.3 (3)
C9—C8—H8119.7C17—C18—H18120.8
C7—C8—H8119.7C19—C18—H18120.8
O2—C9—C8125.1 (3)C20—C19—C18120.4 (3)
O2—C9—C4114.2 (2)C20—C19—H19119.8
C8—C9—C4120.8 (3)C18—C19—H19119.8
O2—C10—C11112.0 (3)C21—C20—C19119.1 (3)
O2—C10—H10A109.2C21—C20—H20120.4
C11—C10—H10A109.2C19—C20—H20120.4
O2—C10—H10B109.2F2—C21—C20117.7 (3)
C11—C10—H10B109.2F2—C21—C16119.0 (3)
H10A—C10—H10B107.9C20—C21—C16123.3 (3)
C10—C11—H11A109.5
C2—O1—C1—O32.5 (5)C6—C7—C12—C140.3 (4)
C2—O1—C1—C16175.2 (2)C8—C7—C12—C14179.3 (3)
C1—O1—C2—C3120.5 (3)C6—C7—C12—C15120.3 (3)
O1—C2—C3—N158.2 (3)C8—C7—C12—C1560.6 (4)
O1—C2—C3—C4177.9 (2)C6—C7—C12—C13120.1 (3)
N1—C3—C4—C524.0 (4)C8—C7—C12—C1358.9 (4)
C2—C3—C4—C598.7 (3)O3—C1—C16—C17148.9 (4)
N1—C3—C4—C9155.1 (2)O1—C1—C16—C1733.5 (4)
C2—C3—C4—C982.2 (3)O3—C1—C16—C2133.7 (5)
C9—C4—C5—C61.0 (4)O1—C1—C16—C21144.0 (3)
C3—C4—C5—C6178.1 (3)C21—C16—C17—F1177.2 (3)
C4—C5—C6—C70.6 (5)C1—C16—C17—F15.3 (4)
C5—C6—C7—C80.4 (4)C21—C16—C17—C180.9 (5)
C5—C6—C7—C12178.6 (3)C1—C16—C17—C18176.6 (3)
C6—C7—C8—C90.9 (4)F1—C17—C18—C19179.1 (3)
C12—C7—C8—C9178.1 (3)C16—C17—C18—C191.0 (5)
C10—O2—C9—C819.4 (4)C17—C18—C19—C201.5 (5)
C10—O2—C9—C4161.5 (3)C18—C19—C20—C210.1 (5)
C7—C8—C9—O2179.5 (3)C19—C20—C21—F2179.9 (3)
C7—C8—C9—C40.5 (4)C19—C20—C21—C162.1 (5)
C5—C4—C9—O2178.6 (3)C17—C16—C21—F2179.7 (3)
C3—C4—C9—O22.2 (4)C1—C16—C21—F22.7 (4)
C5—C4—C9—C80.5 (4)C17—C16—C21—C202.5 (4)
C3—C4—C9—C8178.7 (3)C1—C16—C21—C20175.2 (3)
C9—O2—C10—C1167.6 (3)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N1—H1A···Br1i0.882.573.337 (2)147
N1—H1A···F1ii0.882.523.073 (3)122
N1—H1B···Br1ii0.882.393.259 (2)170
N1—H1C···Br10.882.383.252 (2)175
C10—H10A···Br1iii0.992.753.650 (3)152
C2—H2B···O20.992.623.116 (4)111
C8—H8···Br1iii0.953.104.040 (3)170
Symmetry codes: (i) x+1, y+1, z; (ii) y+1, x, z+1; (iii) x1/2, y+3/2, z+1/2.
2-Azaniumyl-2-(4-tert-butyl-2-ethoxyphenyl)ethyl 2,6-difluorobenzoate 3-carboxyprop-2-enoate (II) top
Crystal data top
C21H26F2NO3+·C4H3O4F(000) = 1040
Mr = 493.49Dx = 1.347 Mg m3
Monoclinic, P21/nMo Kα radiation, λ = 0.71073 Å
a = 12.0615 (2) ÅCell parameters from 9544 reflections
b = 15.3673 (3) Åθ = 2.2–27.4°
c = 14.0141 (3) ŵ = 0.11 mm1
β = 110.506 (1)°T = 100 K
V = 2432.96 (8) Å3Irregular block, colourless
Z = 40.19 × 0.18 × 0.12 mm
Data collection top
Bruker D8 Venture dual source
diffractometer
5576 independent reflections
Radiation source: microsource4976 reflections with I > 2σ(I)
Detector resolution: 7.41 pixels mm-1Rint = 0.031
φ and ω scansθmax = 27.5°, θmin = 1.9°
Absorption correction: multi-scan
(SADABS; Krause et al., 2015)
h = 1514
Tmin = 0.917, Tmax = 0.971k = 1919
42339 measured reflectionsl = 1818
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)] = 0.036Hydrogen site location: difference Fourier map
wR(F2) = 0.101H atoms treated by a mixture of independent and constrained refinement
S = 1.03 w = 1/[σ2(Fo2) + (0.0478P)2 + 0.9503P]
where P = (Fo2 + 2Fc2)/3
5576 reflections(Δ/σ)max = 0.001
324 parametersΔρmax = 0.34 e Å3
0 restraintsΔρmin = 0.21 e Å3
Special details top

Experimental. The crystal was mounted using polyisobutene oil on the tip of a fine glass fibre, which was fastened in a copper mounting pin with electrical solder. It was placed directly into the cold gas stream of a liquid-nitrogen based cryostat (Hope, 1994; Parkin & Hope, 1998).

Diffraction data were collected with the crystal at 100K.

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. Refinement progress was checked using Platon (Spek, 2020) and by an R-tensor (Parkin, 2000). The final model was further checked with the IUCr utility checkCIF.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
F10.67039 (8)0.57077 (6)0.21102 (6)0.0434 (2)
F20.85345 (9)0.79866 (6)0.43330 (9)0.0529 (3)
O10.76401 (7)0.55478 (5)0.41727 (6)0.02341 (18)
O20.88984 (7)0.39851 (5)0.69176 (6)0.02211 (18)
O30.93824 (8)0.62310 (6)0.45018 (8)0.0378 (2)
N10.67234 (8)0.48113 (6)0.56665 (7)0.01848 (19)
H1A0.6474 (7)0.5332 (5)0.5391 (4)0.028*
H1B0.7273 (5)0.4881 (5)0.6284 (6)0.028*
H1C0.6112 (8)0.4514 (4)0.5722 (5)0.028*
C10.83341 (10)0.61834 (8)0.40508 (9)0.0249 (2)
C20.82292 (10)0.48524 (7)0.48618 (9)0.0231 (2)
H2A0.8754670.5090550.5521640.028*
H2B0.8707510.4492400.4564880.028*
C30.72419 (10)0.43206 (7)0.50020 (8)0.0193 (2)
H30.6607260.4264280.4317100.023*
C40.75887 (9)0.34111 (7)0.54008 (8)0.0185 (2)
C50.70565 (10)0.26951 (7)0.48146 (8)0.0221 (2)
H50.6459920.2784770.4167170.026*
C60.73754 (10)0.18537 (7)0.51519 (9)0.0230 (2)
H60.6997170.1377220.4732080.028*
C70.82469 (10)0.16949 (7)0.61028 (8)0.0198 (2)
C80.87624 (10)0.24084 (7)0.67047 (8)0.0195 (2)
H80.9342670.2318020.7360200.023*
C90.84405 (9)0.32533 (7)0.63609 (8)0.0185 (2)
C100.99214 (10)0.38980 (8)0.78240 (9)0.0252 (2)
H10A1.0515360.3514240.7698670.030*
H10B0.9699710.3646170.8382430.030*
C111.04123 (13)0.48013 (9)0.80978 (12)0.0401 (4)
H11A1.0576830.5056070.7520270.060*
H11B1.1146390.4773140.8690480.060*
H11C0.9833330.5162710.8261060.060*
C120.86045 (11)0.07546 (7)0.64402 (9)0.0231 (2)
C130.90985 (13)0.03290 (9)0.56848 (10)0.0325 (3)
H13A0.8499490.0348490.4998840.049*
H13B0.9305310.0277900.5882320.049*
H13C0.9806900.0644200.5689810.049*
C140.75153 (12)0.02405 (8)0.64565 (10)0.0304 (3)
H14A0.6893780.0266240.5782040.046*
H14B0.7220550.0495590.6962870.046*
H14C0.7738380.0367330.6634840.046*
C150.95581 (12)0.07098 (8)0.75090 (9)0.0282 (3)
H15A0.9759120.0100150.7695470.042*
H15B0.9256080.0978830.8003390.042*
H15C1.0266860.1021850.7509460.042*
C160.76319 (11)0.68173 (8)0.32678 (10)0.0262 (3)
C170.68208 (12)0.65686 (10)0.2331 (1)0.0333 (3)
C180.61531 (13)0.71439 (12)0.16093 (12)0.0452 (4)
H180.5603830.6945440.0978810.054*
C190.63056 (15)0.80174 (12)0.18290 (15)0.0521 (5)
H190.5836350.8426560.1348300.062*
C200.71214 (15)0.83136 (11)0.27283 (16)0.0509 (4)
H200.7239160.8919480.2859550.061*
C210.77655 (13)0.77084 (9)0.34364 (12)0.0375 (3)
O40.47353 (7)0.38720 (5)0.53105 (6)0.02278 (18)
O50.40305 (8)0.25232 (6)0.53032 (6)0.0292 (2)
O60.74564 (8)0.26663 (5)0.85732 (6)0.0274 (2)
H6A0.8000 (14)0.2498 (4)0.9192 (13)0.041*
O70.68739 (8)0.12803 (6)0.85259 (7)0.0313 (2)
C220.47330 (9)0.31260 (7)0.56934 (8)0.0192 (2)
C230.56755 (9)0.29645 (7)0.67107 (8)0.0197 (2)
H230.6153760.3438690.7056300.024*
C240.58657 (10)0.21927 (7)0.71429 (8)0.0217 (2)
H240.5383050.1724320.6786660.026*
C250.67817 (10)0.20027 (7)0.81480 (8)0.0213 (2)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
F10.0488 (5)0.0455 (5)0.0311 (4)0.0028 (4)0.0082 (4)0.0020 (4)
F20.0510 (6)0.0265 (4)0.0756 (7)0.0040 (4)0.0153 (5)0.0059 (4)
O10.0237 (4)0.0208 (4)0.0242 (4)0.0011 (3)0.0066 (3)0.0057 (3)
O20.0215 (4)0.0164 (4)0.0205 (4)0.0018 (3)0.0026 (3)0.0011 (3)
O30.0224 (4)0.0356 (5)0.0520 (6)0.0002 (4)0.0089 (4)0.0142 (5)
N10.0176 (4)0.0158 (4)0.0195 (4)0.0016 (3)0.0033 (3)0.0016 (3)
C10.0246 (6)0.0222 (6)0.0295 (6)0.0015 (4)0.0116 (5)0.0033 (5)
C20.0226 (5)0.0202 (5)0.0256 (6)0.0035 (4)0.0072 (4)0.0048 (4)
C30.0214 (5)0.0167 (5)0.0173 (5)0.0015 (4)0.0037 (4)0.0002 (4)
C40.0193 (5)0.0166 (5)0.0182 (5)0.0018 (4)0.0049 (4)0.0011 (4)
C50.0244 (5)0.0196 (5)0.0175 (5)0.0012 (4)0.0015 (4)0.0001 (4)
C60.0281 (6)0.0170 (5)0.0198 (5)0.0003 (4)0.0031 (4)0.0019 (4)
C70.0216 (5)0.0175 (5)0.0199 (5)0.0021 (4)0.0069 (4)0.0006 (4)
C80.0191 (5)0.0194 (5)0.0178 (5)0.0025 (4)0.0038 (4)0.0012 (4)
C90.0179 (5)0.0171 (5)0.0191 (5)0.0002 (4)0.0049 (4)0.0015 (4)
C100.0219 (5)0.0206 (5)0.0233 (5)0.0013 (4)0.0043 (4)0.0003 (4)
C110.0325 (7)0.0236 (6)0.0436 (8)0.0011 (5)0.0123 (6)0.0007 (6)
C120.0288 (6)0.0166 (5)0.0215 (5)0.0038 (4)0.0057 (4)0.0006 (4)
C130.0413 (7)0.0276 (6)0.0283 (6)0.0116 (5)0.0119 (5)0.0006 (5)
C140.0354 (7)0.0228 (6)0.0299 (6)0.0009 (5)0.0078 (5)0.0039 (5)
C150.0341 (6)0.0212 (6)0.0248 (6)0.0056 (5)0.0047 (5)0.0040 (5)
C160.0238 (6)0.0247 (6)0.0339 (6)0.0033 (5)0.0151 (5)0.0092 (5)
C170.0302 (6)0.0433 (8)0.0305 (6)0.0035 (6)0.0155 (5)0.0113 (6)
C180.0337 (7)0.0687 (11)0.0364 (8)0.0105 (7)0.0162 (6)0.0246 (7)
C190.0404 (8)0.0587 (11)0.0656 (11)0.0195 (8)0.0292 (8)0.0401 (9)
C200.0474 (9)0.0308 (8)0.0837 (13)0.0131 (7)0.0342 (9)0.0248 (8)
C210.0330 (7)0.0286 (7)0.0536 (9)0.0012 (5)0.0188 (6)0.0072 (6)
O40.0183 (4)0.0208 (4)0.0251 (4)0.0018 (3)0.0023 (3)0.0076 (3)
O50.0288 (4)0.0240 (4)0.0226 (4)0.0066 (3)0.0063 (3)0.0042 (3)
O60.0294 (4)0.0214 (4)0.0199 (4)0.0031 (3)0.0060 (3)0.0028 (3)
O70.0328 (5)0.0211 (4)0.0286 (4)0.0010 (4)0.0035 (4)0.0078 (3)
C220.0179 (5)0.0191 (5)0.0181 (5)0.0016 (4)0.0030 (4)0.0024 (4)
C230.0187 (5)0.0190 (5)0.0174 (5)0.0016 (4)0.0014 (4)0.0000 (4)
C240.0215 (5)0.0192 (5)0.0187 (5)0.0021 (4)0.0002 (4)0.0007 (4)
C250.0216 (5)0.0203 (5)0.0188 (5)0.0006 (4)0.0032 (4)0.0017 (4)
Geometric parameters (Å, º) top
F1—C171.3547 (17)C11—H11C0.9800
F2—C211.3436 (19)C12—C131.5314 (17)
O1—C11.3357 (14)C12—C151.5376 (16)
O1—C21.4488 (13)C12—C141.5400 (17)
O2—C91.3698 (13)C13—H13A0.9800
O2—C101.4338 (13)C13—H13B0.9800
O3—C11.2015 (15)C13—H13C0.9800
N1—C31.4950 (14)C14—H14A0.9800
N1—H1A0.893 (8)C14—H14B0.9800
N1—H1B0.893 (8)C14—H14C0.9800
N1—H1C0.893 (8)C15—H15A0.9800
C1—C161.4898 (16)C15—H15B0.9800
C2—C31.5127 (16)C15—H15C0.9800
C2—H2A0.9900C16—C171.3881 (19)
C2—H2B0.9900C16—C211.3894 (19)
C3—C41.5089 (15)C17—C181.372 (2)
C3—H31.0000C18—C191.375 (3)
C4—C51.3886 (15)C18—H180.9500
C4—C91.3986 (15)C19—C201.377 (3)
C5—C61.3841 (16)C19—H190.9500
C5—H50.9500C20—C211.383 (2)
C6—C71.3996 (15)C20—H200.9500
C6—H60.9500O4—C221.2661 (13)
C7—C81.3903 (15)O5—C221.2452 (14)
C7—C121.5345 (15)O6—C251.3106 (14)
C8—C91.3920 (15)O6—H6A0.922 (18)
C8—H80.9500O7—C251.2182 (14)
C10—C111.5052 (17)C22—C231.5003 (14)
C10—H10A0.9900C23—C241.3149 (16)
C10—H10B0.9900C23—H230.9500
C11—H11A0.9800C24—C251.4831 (15)
C11—H11B0.9800C24—H240.9500
C1—O1—C2116.21 (9)C13—C12—C15108.35 (10)
C9—O2—C10118.56 (8)C7—C12—C15112.08 (9)
C3—N1—H1A109.5C13—C12—C14109.37 (10)
C3—N1—H1B109.5C7—C12—C14109.78 (10)
H1A—N1—H1B109.5C15—C12—C14108.27 (10)
C3—N1—H1C109.5C12—C13—H13A109.5
H1A—N1—H1C109.5C12—C13—H13B109.5
H1B—N1—H1C109.5H13A—C13—H13B109.5
O3—C1—O1124.64 (11)C12—C13—H13C109.5
O3—C1—C16124.72 (11)H13A—C13—H13C109.5
O1—C1—C16110.63 (10)H13B—C13—H13C109.5
O1—C2—C3105.09 (9)C12—C14—H14A109.5
O1—C2—H2A110.7C12—C14—H14B109.5
C3—C2—H2A110.7H14A—C14—H14B109.5
O1—C2—H2B110.7C12—C14—H14C109.5
C3—C2—H2B110.7H14A—C14—H14C109.5
H2A—C2—H2B108.8H14B—C14—H14C109.5
N1—C3—C4111.02 (9)C12—C15—H15A109.5
N1—C3—C2109.19 (9)C12—C15—H15B109.5
C4—C3—C2114.82 (9)H15A—C15—H15B109.5
N1—C3—H3107.2C12—C15—H15C109.5
C4—C3—H3107.2H15A—C15—H15C109.5
C2—C3—H3107.2H15B—C15—H15C109.5
C5—C4—C9117.6 (1)C17—C16—C21115.70 (12)
C5—C4—C3120.28 (9)C17—C16—C1123.17 (12)
C9—C4—C3122.13 (10)C21—C16—C1121.13 (12)
C6—C5—C4121.51 (10)F1—C17—C18118.27 (14)
C6—C5—H5119.2F1—C17—C16117.86 (12)
C4—C5—H5119.2C18—C17—C16123.85 (15)
C5—C6—C7120.95 (10)C17—C18—C19117.77 (16)
C5—C6—H6119.5C17—C18—H18121.1
C7—C6—H6119.5C19—C18—H18121.1
C8—C7—C6117.86 (10)C18—C19—C20121.64 (14)
C8—C7—C12122.55 (10)C18—C19—H19119.2
C6—C7—C12119.6 (1)C20—C19—H19119.2
C7—C8—C9120.95 (10)C19—C20—C21118.43 (16)
C7—C8—H8119.5C19—C20—H20120.8
C9—C8—H8119.5C21—C20—H20120.8
O2—C9—C8124.1 (1)F2—C21—C20119.16 (14)
O2—C9—C4114.79 (9)F2—C21—C16118.27 (13)
C8—C9—C4121.1 (1)C20—C21—C16122.56 (16)
O2—C10—C11106.22 (9)C25—O6—H6A109.5
O2—C10—H10A110.5O5—C22—O4126.13 (10)
C11—C10—H10A110.5O5—C22—C23117.83 (10)
O2—C10—H10B110.5O4—C22—C23116.04 (10)
C11—C10—H10B110.5C24—C23—C22122.6 (1)
H10A—C10—H10B108.7C24—C23—H23118.7
C10—C11—H11A109.5C22—C23—H23118.7
C10—C11—H11B109.5C23—C24—C25124.52 (10)
H11A—C11—H11B109.5C23—C24—H24117.7
C10—C11—H11C109.5C25—C24—H24117.7
H11A—C11—H11C109.5O7—C25—O6124.32 (10)
H11B—C11—H11C109.5O7—C25—C24121.09 (10)
C13—C12—C7108.94 (10)O6—C25—C24114.58 (10)
C2—O1—C1—O33.44 (18)C8—C7—C12—C151.27 (16)
C2—O1—C1—C16175.71 (10)C6—C7—C12—C15179.17 (11)
C1—O1—C2—C3170.25 (9)C8—C7—C12—C14121.63 (12)
O1—C2—C3—N173.64 (10)C6—C7—C12—C1458.81 (14)
O1—C2—C3—C4160.96 (9)O3—C1—C16—C17132.61 (14)
N1—C3—C4—C5118.11 (11)O1—C1—C16—C1746.55 (16)
C2—C3—C4—C5117.45 (12)O3—C1—C16—C2146.75 (19)
N1—C3—C4—C961.61 (13)O1—C1—C16—C21134.09 (12)
C2—C3—C4—C962.83 (14)C21—C16—C17—F1176.68 (11)
C9—C4—C5—C61.68 (17)C1—C16—C17—F12.72 (18)
C3—C4—C5—C6178.60 (11)C21—C16—C17—C181.76 (19)
C4—C5—C6—C70.26 (18)C1—C16—C17—C18178.84 (12)
C5—C6—C7—C81.34 (17)F1—C17—C18—C19178.03 (12)
C5—C6—C7—C12178.24 (11)C16—C17—C18—C190.4 (2)
C6—C7—C8—C91.49 (16)C17—C18—C19—C201.8 (2)
C12—C7—C8—C9178.08 (10)C18—C19—C20—C212.4 (2)
C10—O2—C9—C812.17 (16)C19—C20—C21—F2177.63 (14)
C10—O2—C9—C4168.79 (10)C19—C20—C21—C160.9 (2)
C7—C8—C9—O2179.04 (10)C17—C16—C21—F2179.64 (12)
C7—C8—C9—C40.06 (17)C1—C16—C21—F20.95 (19)
C5—C4—C9—O2177.55 (10)C17—C16—C21—C201.1 (2)
C3—C4—C9—O22.17 (15)C1—C16—C21—C20179.53 (13)
C5—C4—C9—C81.52 (16)O5—C22—C23—C247.78 (17)
C3—C4—C9—C8178.76 (10)O4—C22—C23—C24171.94 (11)
C9—O2—C10—C11164.55 (11)C22—C23—C24—C25179.7 (1)
C8—C7—C12—C13118.63 (12)C23—C24—C25—O7176.53 (12)
C6—C7—C12—C1360.93 (14)C23—C24—C25—O63.43 (17)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N1—H1A···O4i0.891.892.7160 (12)152
N1—H1B···O20.892.302.8889 (12)123
N1—H1B···O7ii0.892.362.8103 (13)112
N1—H1C···O40.891.842.6915 (12)158
C2—H2A···O7ii0.992.533.1832 (15)123
C2—H2B···O3iii0.992.483.1727 (15)127
O6—H6A···O5iv0.921.622.5184 (11)165
Symmetry codes: (i) x+1, y+1, z+1; (ii) x+3/2, y+1/2, z+3/2; (iii) x+2, y+1, z+1; (iv) x+1/2, y+1/2, z+1/2.
Conformation-defining torsion angles (°) in I and II top
Torsion angleIII
C5—C4—C3—C298.7 (3)-117.45 (12)
C4—C3—C2—O1178.0 (2)160.96 (9)
C3—C2—O1—C1-120.5 (3)170.25 (9)
C2—O1—C1—C16175.2 (2)175.71 (10)
O1—C1—C16—C21-144.0 (3)134.09 (12)
N1—C3—C2—O1-58.2 (3)-73.64 (10)
N1—C3—C4—C9155.1 (3)-61.61 (13)
C9—O2—C10—C1167.6 (4)164.55 (11)
C4—C9—O2—C10-161.5 (3)-168.79 (10)
C8—C7—C13—C14165.0 (2)123.99 (12)
 

Acknowledgements

The authors thank Honeychem Pharma Research Pvt. Ltd., Peenya Industrial Area, Bengaluru-560 058, India, for the gift sample of R7.

Funding information

The D8 Venture diffractometer was funded by the NSF (MRI CHE1625732), and by the University of Kentucky.

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