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Tetra­hydro-1-benzazepines have been described as potential anti­parasitic drugs for the treatment of chagas disease and leishmaniasis, two of the most important so-called `forgotten tropical diseases' affecting South and Central America, caused by Trypanosoma cruzi and Leishmania chagasi parasites, respectively. Continuing our extensive work describing the structural characteristics of some related compounds with inter­esting biological properties, the crystallographic features of three ep­oxy-1-benzazepines, namely (2SR,4RS)-6,8-dimethyl-2-(naphthalen-1-yl)-2,3,4,5-tetra­hydro-1H-1,4-ep­oxy-1-benzazepine, (1), (2SR,4RS)-6,9-dimethyl-2-(naphthalen-1-yl)-2,3,4,5-tetra­hydro-1H-1,4-ep­oxy-1-benzazepine, (2), and (2SR,4RS)-8,9-dimethyl-2-(naphthalen-1-yl)-2,3,4,5-tetra­hydro-1H-1,4-ep­oxy-1-benzazepine, (3), all C22H21NO, and two 1-benzazepin-4-ols, namely 7-fluoro-cis-2-[(E)-styr­yl]-2,3,4,5-tetra­hydro-1H-1-benzazepin-4-ol, C18H18FNO, (4), and 7-fluoro-cis-2-[(E)-pent-1-en­yl]-2,3,4,5-tetra­hydro-1H-1-benzazepin-4-ol, C15H20FNO, (5), are described. Some peculiarities in the crystallization behaviour were found, involving significant variations in the crystalline structures as a result of modest changes in the peripheral substituents in (1)-(3) and the occurrence of discrete disorder due to the mol­ecular overlay of enanti­omers with more than one conformation in (5). In particular, an inter­esting phase change on cooling was observed for compound (5), accompanied by an approximate fourfold increase of the unit-cell volume and a change of the Z' value from 1 to 4. This transition is a consequence of the partial ordering of the pentenyl chains in half of the mol­ecules breaking half of the \overline{3} symmetry axes observed in the room-temperature structure of (5). The structural assembly in all the title compounds is characterized by not only (N,O)-H...(O,N) hydrogen bonds, but also by unconventional C-H...O contacts, resulting in a wide diversity of packing.

Supporting information

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Crystallographic Information File (CIF) https://doi.org/10.1107/S2053229616004885/wq3111sup1.cif
Contains datablocks Compound_1, Compound_2, Compound_3, Compound_4, Compound_5a, Compound_5b

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Contains datablock Compound_1

hkl

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Contains datablock Compound_2

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Contains datablock Compound_5a

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Contains datablock Compound_5b

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Figure showing the conformers of (5LT)

CCDC references: 1470211; 1470210; 1470209; 1470208; 1470207; 1470206

Introduction top

\ Tetra­hydro-1-benzazepines have been described as potential anti­parasitic drugs for the treatment of chagas disease and leishmaniasis, two of the most important, so-called `forgotten tropical diseases' affecting South and Central America, caused by Trypanosoma cruzi and Leishmania chagasi parasites, respectively (Gómez-Ayala et al., 2010). A simple synthetic approach for the stereoselective synthesis of exo-2-aryl-1,4-ep­oxy­tetra­hydro-1-benzazepines and the alcohol derivatives exo-2-aryl-1,4-tetra­hydro-1-benzazepine-4-ols, through the selective oxidation of substituted ortho-allyl-N-benzyl­anilines and subsequent intra­molecular 1,3-dipolar cyclo­addition of the formed nitro­nes and posterior opening of the epoxide, was described (Gómez-Ayala et al., 2006; Acosta, Palma & Bahsas, 2010; Acosta et al., 2012) and systematically applied to prepare new compounds in the search for molecules with better biological activity against these parasites. Part of this systematic study of particularly active molecules (Acosta et al., 2009; Acosta et al., 2008; Acosta, Palma, Bahsas et al., 2010; Gómez et al., 2008, 2009, 2010, 2011; Sanabria et al., 2010; Blanco et al., 2012a,b,c; Yépes et al., 2012, 2013; Guerrero et al., 2014; Sanabría et al., 2014) included the crystal structure determination. Two series of structures are presented and their conformation and packing are described and compared in this paper: (2SR,4RS)-6,8-di­methyl-2-(naphthalen-1-yl)-2,3,4,5-tetra­hydro-\ 1H-1,4-ep­oxy-1-benzazepine, (1), (2SR,4RS)-6,9-di­methyl-2-(naphthalen-1-yl)-2,3,4,5-tetra­hydro-\ 1H-1,4-ep­oxy-1-benzazepine, (2), (2SR,4RS)-8,9-di­methyl-2-(naphthalen-1-yl)-2,3,4,5-tetra­hydro-\ 1H-1,4-ep­oxy-1-benzazepine, (3), are ep­oxy-1-benzazepines differing only in the position of two methyl groups in the 6-, 8- and 9-positions in the fused benzene ring, and 7-fluoro-cis-2-[(E)-styryl]-2,3,4,5-tetra­hydro-1H-1-\ benzazepin-4-ol, (4), and 7-fluoro-cis-2-[(E)-pent-1-enyl]-2,3,4,5-tetra­hydro-1H-\ 1-benzazepin-4-ol, (5), are 1-benzazepin-4-ols replacing both methyl residues for fluorine at the 7-position 7, differing in the residues at the 2-position.

Experimental top

Synthesis and crystallization top

The syntheses of the compounds (1)–(5) were carried out following our previously estabished experimental conditions (Acosta, Palma & Bahsas, 2010; Acosta et al., 2012). Particular details are described as follows. Recrystallization of (1)–(3) by slow evaporation of a solution in heptane gave crystals of suitable size and quality for single-crystal X-ray diffraction. In the case of compounds (4) and (5), the recrystallization was performed from a heptane–ethyl acetate (1:1 v/v) mixture which also gave crystals suitable for single-crystal X-ray diffraction.

Compounds (1)–(3) top

Sodium tungstate dihydrate, Na2WO4·2H2O (7 mol%), followed by 30% aqueous hydrogen peroxide solution (0.30 mol), were added to a stirred and cooled (273 K) solution of the appropriate di­methyl-substituted 2-allyl-N-(naphthalen-1-yl­methyl)­aniline (0.10 mol) in methanol (20 ml). The resulting mixtures were then stirred at ambient temperature for 72 h. Each mixture was filtered and the solvent removed under reduced pressure. Toluene (30 ml) was added to the solid residue and the resulting solution was heated under reflux for 18 h. After cooling each solution to ambient temperature, the solvent was removed under reduced pressure and the crude product was purified by chromatography on silica using heptane–ethyl acetate (compositions ranged from 60:1 to 10:1 v/v) as eluent to give compounds (1)–(3) with yields of 69, 67 and 59%, respectively (see Scheme 1).

Compounds (4) and (5) top

To stirred and ice-bath-cooled methano­lic solutions of the 1,4-ep­oxy cyclo­adducts were added zinc powder (10 mmol), glacial acetic acid (7 mmol) and hydro­chloric acid (7 mmol, 37% HCl). The resulting mixtures were stirred at 273 K for an additional 30 min and the crude products were filtered. Each filtrate was then basified with 25% aqueous NH4OH to pH 8, extracted with EtOAc (3 × 50 ml), and the combined organic layers were dried over anhydrous Na2SO4. The solvent was removed under reduced pressure and the crude product was purified by column chromatography (silica gel, heptane–EtOAc, 10:1 to 1:1 v/v) to give the compounds (4) and (5) with yields of 93 and 90%, respectively (see Scheme 2).

Refinement top

Crystal data, data collection and structure refinement details are summarized in Table 1. H atoms were placed in calculated positions (C—H = 0.93–1.00 Å) and included as riding contributions with isotropic displacement parameters set at 1.2-1.5 times of the Ueq value of the parent atom. H atoms belonging to OH and NH groups were located in difference density maps and refined freely. Some low-angle reflections strongly affected by the experiment, attenuated by the beam stop, for instance, were omitted for the final refinements, viz. for (1) 366 and 366, for (2) 011 and for (5) 120.

Results and discussion top

The two groups of compounds described show different conformational and packing characteristics due to the size and position of substituents and the different conformations of the benzodiazepine nucleus (rigid in the epoxides and more flexible in the alcohols).

Three structural isomers of naphthalen-1-yl-substituted tetra­hydro-1-benzazepines with inter­esting crystallization behaviour top

The non-enanti­oselective synthesis pathway (Gómez-Ayala et al., 2010; Acosta, Palma & Bahsas, 2010; OR Acosta, Palma, Bahsas et al., 2010) that produce racemic mixtures of the structural isomers (1), (2) and (3), however, they crystallize in different forms. Compound (1) crystallizes as a racemate in the space group P21/c, with Z' = 2, where the two molecules in the asymmetric unit were selected to have the same absolute configuration [(2S, 4R), as shown in Fig. 1]. Compund (2) crystallizes in the Schonke space group P212121, selecting the same (2S,4R) absolute configuration for the refinement (Fig. 2a), and compound (3) crystallizes in the Sohncke space group P21 and the crystal selected for structure determination was the (2S, 4R) enanti­omer (Fig. 2b). This crystallization behaviour of slightly different isomers in different space groups with different crystalline symmetries has been described previously for this kind of compound (Acosta et al., 2008; Acosta, Palma, Bahsas et al., 2010).

The A conformer in (1) is conformationally identical to molecules (2) and (3), since the ep­oxy­benzazepine nucleus is rather rigid, as shown by the overlay of the nuclei of (1A) and (2) with (3) (atoms N1, O1, C2, C3, C4, C5, C5A, C6, C7, C8, C9 and C9A), that give r.m.s. deviations of 0.0345 and 0.0249 Å, respectively. The dihedral angle between the naphthyl and benzyl rings are 88.14 (6), 87.66 (9) and 85.74 (6)° in (1A), (2) and (3), respectively, which indicates that the orthogonal conformation of the rings is the most stable for these molecules. Considering the conformation of the fused rings in the nuclei of the molecules (1A), (2) and (3), the five- (O1/N1/C2–C4) and six-membered (O1/N1/C9A/C5A/C5/C4) rings adopt an inter­mediate conformation between half-chair and envelope (Table 2) (Cremer & Pople, 1975).

The (1B) conformer in (1) shows a similar but not identical conformation of the ep­oxy­benzazepine nucleus with respect to (1A) [r.m.s. deviation = 0.045 Å, larger than that of (1A) and (2) with (3)] with slightly different puckering parameters for the five- and six-memebred rings than those observed between (1A), (2) and (3) (Table 2). The main difference between (1B) and the other molecules is the dihedral angle between the naphthyl and benzyl rings of 4.26 (6)°, indicating that both rings are almost parallel and that molecule (1B) shows a relatively planar arrangement.

Even though the three compounds show different space groups, a motif of inter­molecular inter­actions seems to be common to the three structures that form chains of molecules related by a 21 screw axis in the three cases along b. In the three compunds, weak C—H···O and C—H···π inter­actions direct the formation of chains (Tables 3, 4 and 5). In (1A), one C2A—H2A···O1Ai [symmetry code: (i) -x+1, y+1/2] and one C5A—H5AA···Cg1A2ii [Cg1A2 is the centroid of the C20A–C24A/C29A ring; symmetry code: (ii) -x+1, y-1/2, -z+1/2] inter­action connect molecules related by a 21 screw axis (Fig. 3a), in (2), only one weak C82—H82···O1i [symmetry code: (i) -x+1, y+1/2, ???] hydrogen bond connects consecutive molecules (Fig. 3b), and in (3), one C8—H8···O1iii [symmetry code: (iii) x, y+1, z] and two C27—H27···Cg31iv and C28—H28···Cg32iv [Cg31 and Cg32 are the centroids of the C20–C24/C29 and C24–C29 rings, respectively; symmetry code: (iv) -x, y+1/2, -z+1] connect consecutive molecules (Fig. 3c), with additional C—H···π or van der Waals inter­actions connecting parallel chains. The case of compound (1) is more complex, though, since the crystal is centrosymmetric, therefore inverted chains of (1A) (2R,4S) enanti­omers also run parallel to the b axis; furthermore, molecule (1B), with a different conformation, is also present. It is inter­esting, however, that molecules (1A) pack in separate layers from (1B) which form inversion dimers through C4B—H4B···O1Bv [symmetry code: (v) -x+2, -y, -z+1] and each molecule stacks with another inverted molecule along b (Fig. 3a). Chains of dimers, related by the c-glide plane have an parallel disposition of the planar benzyl and naphthyl ring that allows for C—H···π inter­actions.

Two new examples in the tetra­hydro-1-benzazepine series: occurrence of discrete disorder top

Compounds (4) and (5) crystallize as racemates in the centrosymmetric Pbca and R3 space groups, respectively; both compounds were studied at room temperature and at 100 K. Compound (4) shows the same structure at both temperatures, but compound (5) shows a phase transition between room temperature, i.e. compound (5RT), and 100 K, i.e. compound (5LT), as will be described below.

For both compounds, the seven-membered ring adopts a chair conformation (Table 2) with the hy­droxy, and styryl/pentenyl substituents [in (4) and (5)] in equatorial positions and the fluoro­benzyl ring in a bis­ectional conformation, as shown in Fig. 4. Even though the seven-memebered ring of the tetra­hydro­benzazepine nucleus has conformational freedom, all the independent molecules in (4), (5RT) and (5LT) show a very consistent conformation, with a maximum average r.m.s. deviation of 0.0794 Å of the common 7-fluoro­tetra­hydro­benzazepine nucleus (atoms N1, O1, C2, C3, C4, C5, C52, C6, C7, C8, C9 and C92) between the molecule in (4) and molecule 3 of (5LT).

In the molecule of (4), the C22–C28 plane containing the styryl group is oriented towards the 7-fluoro­tetra­hydro­benzazepine nucleus, making a dihedral angle of 60.99 (5)° (Fig. 4a). This general conformation is conserved at room temperature and 100 K. In this molecule, the styryl group is not completely planar since the C24—C23—C22—C21 torsion angle, which has a value of 168.68 (13)°, is slightly distorted considering that only Csp2 atoms are involved. The heterocyclic ring (atoms N1/C2–C5/C5A/C9A) in both compounds has similar puckering parameters values (Table 2) (Cremer & Pople, 1975).

Atoms of the pentenyl chain of the room-temperature structure of compound (5), denoted (5RT), exhibited high anisotropic displacement ellipsoids in the initial refinement cycles consistent with positional disorder in two different conformations of the same chain, slightly rotated along the C2—C10 bond, and were modelled as such (Fig. 4b). This positional disorder turned out to be very important when a new data collection was performed at 100 K, denoted (5LT), where it was observed that this disorder would correspond to the co-existence of various possible conformations of the pentenyl residue (Fig. 4c). The disorder in the room-temperature structure was refined successfully assuming two pentenyl chains in the same conformation with refined occupancies of 48.3 (5) and 51.7 (5)%, and an average C11—C12—C13—C14 torsion angle of -167.9° (Fig. 4b). However, the data at 100 K revealed that in fact it is possible to differentiate a new conformation as result of a rotation in the C12—C13 bond giving rise to a structure with a Z' value of 4. The four independent molecules in the asymmetric unit, each with different degree of disorder, are the result of the averaging of different proportions of two main different conformation of the pentenyl chain [with one of the conformations showing two possible torsion angles as in (5RT)]. In this sense, molecules 1 (2R,4S) and 2 (2S,4R) (see Fig. 4c) correspond to two ordered conformers, with torsion angles (C111—C112—C113—C114 and C211—C212—C213—C214) of -179.22 (14) and 72.11 (16)°, respectively (called conformers α and β in Fig. S1 of the Supporting information). Molecule 3 (2S,4R) shows disorder, similar to that of (5RT), successfully described as the co-existence of two chains with the same α conformation but in slightly different positions, with occupancies of 84.1 (2) and 15.9 (2)% and torsion angles of 176.06 (19) and 174.5 (11)°. Molecule 4 (2S,4R) represents a mixture of both α and β conformers, with two orientations of the former, with occupancies of 31.9 (8) and 34.0 (8)%, and an average torsion angle of ~176.5°, and a third one corresponding to the β conformer having an occupancy of 34.2 (3) and a torsion angle of 71.5 (6)° (see Fig. S1 in the Supporting information). The molecular connectivity in (5) (Tables 6 and 7) is quite different from that in (4). At room temperature, six molecules are connected by N1—H1N···O1i [symmetry code: (i) x-y+2/3, x+1/3, -z+4/3] [not in Table 6, but in Table 8 for compound (4)?] hydrogen bonds in a racemic ring parallel to (001), leaving the pentenyl substituents oriented to the centre and the F atoms oriented outward, describing a threefold rotoinversion axis with [001] direction (Fig. 5a). Each six-membered ring is connected to six other equivalent structures along the three dimensions connected by six pairs of N1—H1N···O1i and O1—H1O···N1ii [symmetry code: (ii) -y+2/3, x-y+1/3, z+1/3] [not in Table 6, but in Table 8 for compound (4)?] hydrogen bonds generating R44(8) motifs (Fig. 5b). Each pair of enanti­omers are also related by an inversion centre at (1/2, 1/2, 1/2) and connected between them by probably induced dipolar inter­actions involving the halogen substituent. In a supra­molecular perspective, a view along [001] allows one to differentiate the centre of the rings at (2/3, 1/3, z) and (1/3, 2/3, z) (Fig. 5a). The structure at 100 K is transformed in a superstructure of the crystal structure at room temperature since the conformers (see Fig. S1 in the Supporting information) are perceptibly different. In this case, the molecular connectivity remains as room temperature and each individual molecule in the asymmetric unit constitutes a racemic sixfold molecular ring by N(1,2,3,4)1—H(1,2,3,4)N···O(3i,1ii,2iii,4iv)1 [symmetry codes: (i) x, y, z+1; (ii) -y+2/3, x-y+1/3, z-2/3; (iii) x-y+2/3, x+1/3, -z+1/3; (iv) y-1/3, -x+y+1/3, -z+4/3] hydrogen bonds (Table 7). However, the presence of both α and β conformers break half of the threefold rotoinversion axes observed at room temperature leaving a threefold screw axis with [001] direction in the centre of each molecular ring (Fig. 5c).

The supra­molecular assembly of both molecules in their crystals differ significantly, as expected for the very different sizes of the styryl and pentenyl substituents. In compound (4), each molecule is connected to four equivalent molecules at the same z value by two pairs of N1—H1N···O1i and O1—H1O···N1ii [symmetry codes: (i) x, y-1, z; (ii) -x+3/2, y+1/2, z] hydrogen bonds (Table 8), where atoms N1 and O1 act each as donor and acceptor. Hydrogen-bonded molecules form enanti­omorphic chains along the [010] direction (Fig. 6). The chains have a polar disposition, since all molecules in a chain are related by the b-glide plane normal to a (Fig. 6a). This makes the F atoms from all the molecules lie on the same side of the chain, leaving all nonpolar moieties on the other side. Each chain connects with an inverted chain on the [001] direction through weak C6—H6···F1iii [symmetry code: (iii) -x+1, -y+1, -z+1] dipolar inter­actions (2.47 Å) (Jelsch et al., 2015) (Figs. 6b and 6c). The inter­actions among double chains in the [100] and [001] directions are weak and probably dipolar or van der Waals in nature since no weak hydrogen bonds or ππ stacking inter­actions are detected.

Compund (5) shows different structures at room temperature and 100 K, with the low-temperature structure crystallizing in a klassengleiche subgroup of the room-temperature one, with a quadrupling of the unit-cell volume in the (110) plane. The descriptions of (5LT) could be obtained from that of (5RT) by the matrix P = [200 220 001] (Inter­national Tables for Crystallography, 2011). In order to confirm the group/subgroup relation of both structures and determine the degree of distortion of one respect to the other, the ordered part of the molecule in the (5RT) crystal was transformed into the subgroup of (5LT) using TRANSTRU program in the Bilbao Crystallography Server (Aroyo, Kirov et al., 2006; Aroyo, Perez-Mato et al., 2006; Aroyo et al., 2011) and the output structure, consisting of the ordered nuclei of the molecules was compared with the same nuclei in the (5LT) structure (all pentenyl residues, ordered and disordered, were removed) using COMPSTRU (Tasci et al., 2012) and an almost perfect overlap was obtained with an average/maximum atom displacement of 0.1667/0.2539 Å (for atom F1A). These deviations are very small considering the temperature difference and the fact that the room-temperature structure shows one molecule with the pentenyl chain split in two main positions, while the 100 K structure shows four independent molecules, two of them ordered and the other two displaying two and three different pentenyl chain conformations. This strongly suggests that the phase transition observed between room temperature and 100 K could be entirely explained by the partial ordering of the pentenly chains in half of the molecules, that breaks half of the 3 symmetry axes of the room-temperature structure on cooling. The refinement of the 100 K structure using the room-temperature model (R3 space group with halved a and b unit-cell parameters) using hkl data transformed using the inverse of the matrix above, provides a reasonable but significantly poorer model, with unreasonable displacement parameters (too high for a low-temperature model), a higher R factor and a much larger degree of disorder of the pentenyl chain that is very hard to model with less than three separate conformations. This clearly justifies the use of the subgroup to model the 100 K structure and again confirm that the ordering of the pentenyl chains is key to this phase transition.

Structure description top

\ Tetra­hydro-1-benzazepines have been described as potential anti­parasitic drugs for the treatment of chagas disease and leishmaniasis, two of the most important, so-called `forgotten tropical diseases' affecting South and Central America, caused by Trypanosoma cruzi and Leishmania chagasi parasites, respectively (Gómez-Ayala et al., 2010). A simple synthetic approach for the stereoselective synthesis of exo-2-aryl-1,4-ep­oxy­tetra­hydro-1-benzazepines and the alcohol derivatives exo-2-aryl-1,4-tetra­hydro-1-benzazepine-4-ols, through the selective oxidation of substituted ortho-allyl-N-benzyl­anilines and subsequent intra­molecular 1,3-dipolar cyclo­addition of the formed nitro­nes and posterior opening of the epoxide, was described (Gómez-Ayala et al., 2006; Acosta, Palma & Bahsas, 2010; Acosta et al., 2012) and systematically applied to prepare new compounds in the search for molecules with better biological activity against these parasites. Part of this systematic study of particularly active molecules (Acosta et al., 2009; Acosta et al., 2008; Acosta, Palma, Bahsas et al., 2010; Gómez et al., 2008, 2009, 2010, 2011; Sanabria et al., 2010; Blanco et al., 2012a,b,c; Yépes et al., 2012, 2013; Guerrero et al., 2014; Sanabría et al., 2014) included the crystal structure determination. Two series of structures are presented and their conformation and packing are described and compared in this paper: (2SR,4RS)-6,8-di­methyl-2-(naphthalen-1-yl)-2,3,4,5-tetra­hydro-\ 1H-1,4-ep­oxy-1-benzazepine, (1), (2SR,4RS)-6,9-di­methyl-2-(naphthalen-1-yl)-2,3,4,5-tetra­hydro-\ 1H-1,4-ep­oxy-1-benzazepine, (2), (2SR,4RS)-8,9-di­methyl-2-(naphthalen-1-yl)-2,3,4,5-tetra­hydro-\ 1H-1,4-ep­oxy-1-benzazepine, (3), are ep­oxy-1-benzazepines differing only in the position of two methyl groups in the 6-, 8- and 9-positions in the fused benzene ring, and 7-fluoro-cis-2-[(E)-styryl]-2,3,4,5-tetra­hydro-1H-1-\ benzazepin-4-ol, (4), and 7-fluoro-cis-2-[(E)-pent-1-enyl]-2,3,4,5-tetra­hydro-1H-\ 1-benzazepin-4-ol, (5), are 1-benzazepin-4-ols replacing both methyl residues for fluorine at the 7-position 7, differing in the residues at the 2-position.

Sodium tungstate dihydrate, Na2WO4·2H2O (7 mol%), followed by 30% aqueous hydrogen peroxide solution (0.30 mol), were added to a stirred and cooled (273 K) solution of the appropriate di­methyl-substituted 2-allyl-N-(naphthalen-1-yl­methyl)­aniline (0.10 mol) in methanol (20 ml). The resulting mixtures were then stirred at ambient temperature for 72 h. Each mixture was filtered and the solvent removed under reduced pressure. Toluene (30 ml) was added to the solid residue and the resulting solution was heated under reflux for 18 h. After cooling each solution to ambient temperature, the solvent was removed under reduced pressure and the crude product was purified by chromatography on silica using heptane–ethyl acetate (compositions ranged from 60:1 to 10:1 v/v) as eluent to give compounds (1)–(3) with yields of 69, 67 and 59%, respectively (see Scheme 1).

To stirred and ice-bath-cooled methano­lic solutions of the 1,4-ep­oxy cyclo­adducts were added zinc powder (10 mmol), glacial acetic acid (7 mmol) and hydro­chloric acid (7 mmol, 37% HCl). The resulting mixtures were stirred at 273 K for an additional 30 min and the crude products were filtered. Each filtrate was then basified with 25% aqueous NH4OH to pH 8, extracted with EtOAc (3 × 50 ml), and the combined organic layers were dried over anhydrous Na2SO4. The solvent was removed under reduced pressure and the crude product was purified by column chromatography (silica gel, heptane–EtOAc, 10:1 to 1:1 v/v) to give the compounds (4) and (5) with yields of 93 and 90%, respectively (see Scheme 2).

The two groups of compounds described show different conformational and packing characteristics due to the size and position of substituents and the different conformations of the benzodiazepine nucleus (rigid in the epoxides and more flexible in the alcohols).

The non-enanti­oselective synthesis pathway (Gómez-Ayala et al., 2010; Acosta, Palma & Bahsas, 2010; OR Acosta, Palma, Bahsas et al., 2010) that produce racemic mixtures of the structural isomers (1), (2) and (3), however, they crystallize in different forms. Compound (1) crystallizes as a racemate in the space group P21/c, with Z' = 2, where the two molecules in the asymmetric unit were selected to have the same absolute configuration [(2S, 4R), as shown in Fig. 1]. Compund (2) crystallizes in the Schonke space group P212121, selecting the same (2S,4R) absolute configuration for the refinement (Fig. 2a), and compound (3) crystallizes in the Sohncke space group P21 and the crystal selected for structure determination was the (2S, 4R) enanti­omer (Fig. 2b). This crystallization behaviour of slightly different isomers in different space groups with different crystalline symmetries has been described previously for this kind of compound (Acosta et al., 2008; Acosta, Palma, Bahsas et al., 2010).

The A conformer in (1) is conformationally identical to molecules (2) and (3), since the ep­oxy­benzazepine nucleus is rather rigid, as shown by the overlay of the nuclei of (1A) and (2) with (3) (atoms N1, O1, C2, C3, C4, C5, C5A, C6, C7, C8, C9 and C9A), that give r.m.s. deviations of 0.0345 and 0.0249 Å, respectively. The dihedral angle between the naphthyl and benzyl rings are 88.14 (6), 87.66 (9) and 85.74 (6)° in (1A), (2) and (3), respectively, which indicates that the orthogonal conformation of the rings is the most stable for these molecules. Considering the conformation of the fused rings in the nuclei of the molecules (1A), (2) and (3), the five- (O1/N1/C2–C4) and six-membered (O1/N1/C9A/C5A/C5/C4) rings adopt an inter­mediate conformation between half-chair and envelope (Table 2) (Cremer & Pople, 1975).

The (1B) conformer in (1) shows a similar but not identical conformation of the ep­oxy­benzazepine nucleus with respect to (1A) [r.m.s. deviation = 0.045 Å, larger than that of (1A) and (2) with (3)] with slightly different puckering parameters for the five- and six-memebred rings than those observed between (1A), (2) and (3) (Table 2). The main difference between (1B) and the other molecules is the dihedral angle between the naphthyl and benzyl rings of 4.26 (6)°, indicating that both rings are almost parallel and that molecule (1B) shows a relatively planar arrangement.

Even though the three compounds show different space groups, a motif of inter­molecular inter­actions seems to be common to the three structures that form chains of molecules related by a 21 screw axis in the three cases along b. In the three compunds, weak C—H···O and C—H···π inter­actions direct the formation of chains (Tables 3, 4 and 5). In (1A), one C2A—H2A···O1Ai [symmetry code: (i) -x+1, y+1/2] and one C5A—H5AA···Cg1A2ii [Cg1A2 is the centroid of the C20A–C24A/C29A ring; symmetry code: (ii) -x+1, y-1/2, -z+1/2] inter­action connect molecules related by a 21 screw axis (Fig. 3a), in (2), only one weak C82—H82···O1i [symmetry code: (i) -x+1, y+1/2, ???] hydrogen bond connects consecutive molecules (Fig. 3b), and in (3), one C8—H8···O1iii [symmetry code: (iii) x, y+1, z] and two C27—H27···Cg31iv and C28—H28···Cg32iv [Cg31 and Cg32 are the centroids of the C20–C24/C29 and C24–C29 rings, respectively; symmetry code: (iv) -x, y+1/2, -z+1] connect consecutive molecules (Fig. 3c), with additional C—H···π or van der Waals inter­actions connecting parallel chains. The case of compound (1) is more complex, though, since the crystal is centrosymmetric, therefore inverted chains of (1A) (2R,4S) enanti­omers also run parallel to the b axis; furthermore, molecule (1B), with a different conformation, is also present. It is inter­esting, however, that molecules (1A) pack in separate layers from (1B) which form inversion dimers through C4B—H4B···O1Bv [symmetry code: (v) -x+2, -y, -z+1] and each molecule stacks with another inverted molecule along b (Fig. 3a). Chains of dimers, related by the c-glide plane have an parallel disposition of the planar benzyl and naphthyl ring that allows for C—H···π inter­actions.

Compounds (4) and (5) crystallize as racemates in the centrosymmetric Pbca and R3 space groups, respectively; both compounds were studied at room temperature and at 100 K. Compound (4) shows the same structure at both temperatures, but compound (5) shows a phase transition between room temperature, i.e. compound (5RT), and 100 K, i.e. compound (5LT), as will be described below.

For both compounds, the seven-membered ring adopts a chair conformation (Table 2) with the hy­droxy, and styryl/pentenyl substituents [in (4) and (5)] in equatorial positions and the fluoro­benzyl ring in a bis­ectional conformation, as shown in Fig. 4. Even though the seven-memebered ring of the tetra­hydro­benzazepine nucleus has conformational freedom, all the independent molecules in (4), (5RT) and (5LT) show a very consistent conformation, with a maximum average r.m.s. deviation of 0.0794 Å of the common 7-fluoro­tetra­hydro­benzazepine nucleus (atoms N1, O1, C2, C3, C4, C5, C52, C6, C7, C8, C9 and C92) between the molecule in (4) and molecule 3 of (5LT).

In the molecule of (4), the C22–C28 plane containing the styryl group is oriented towards the 7-fluoro­tetra­hydro­benzazepine nucleus, making a dihedral angle of 60.99 (5)° (Fig. 4a). This general conformation is conserved at room temperature and 100 K. In this molecule, the styryl group is not completely planar since the C24—C23—C22—C21 torsion angle, which has a value of 168.68 (13)°, is slightly distorted considering that only Csp2 atoms are involved. The heterocyclic ring (atoms N1/C2–C5/C5A/C9A) in both compounds has similar puckering parameters values (Table 2) (Cremer & Pople, 1975).

Atoms of the pentenyl chain of the room-temperature structure of compound (5), denoted (5RT), exhibited high anisotropic displacement ellipsoids in the initial refinement cycles consistent with positional disorder in two different conformations of the same chain, slightly rotated along the C2—C10 bond, and were modelled as such (Fig. 4b). This positional disorder turned out to be very important when a new data collection was performed at 100 K, denoted (5LT), where it was observed that this disorder would correspond to the co-existence of various possible conformations of the pentenyl residue (Fig. 4c). The disorder in the room-temperature structure was refined successfully assuming two pentenyl chains in the same conformation with refined occupancies of 48.3 (5) and 51.7 (5)%, and an average C11—C12—C13—C14 torsion angle of -167.9° (Fig. 4b). However, the data at 100 K revealed that in fact it is possible to differentiate a new conformation as result of a rotation in the C12—C13 bond giving rise to a structure with a Z' value of 4. The four independent molecules in the asymmetric unit, each with different degree of disorder, are the result of the averaging of different proportions of two main different conformation of the pentenyl chain [with one of the conformations showing two possible torsion angles as in (5RT)]. In this sense, molecules 1 (2R,4S) and 2 (2S,4R) (see Fig. 4c) correspond to two ordered conformers, with torsion angles (C111—C112—C113—C114 and C211—C212—C213—C214) of -179.22 (14) and 72.11 (16)°, respectively (called conformers α and β in Fig. S1 of the Supporting information). Molecule 3 (2S,4R) shows disorder, similar to that of (5RT), successfully described as the co-existence of two chains with the same α conformation but in slightly different positions, with occupancies of 84.1 (2) and 15.9 (2)% and torsion angles of 176.06 (19) and 174.5 (11)°. Molecule 4 (2S,4R) represents a mixture of both α and β conformers, with two orientations of the former, with occupancies of 31.9 (8) and 34.0 (8)%, and an average torsion angle of ~176.5°, and a third one corresponding to the β conformer having an occupancy of 34.2 (3) and a torsion angle of 71.5 (6)° (see Fig. S1 in the Supporting information). The molecular connectivity in (5) (Tables 6 and 7) is quite different from that in (4). At room temperature, six molecules are connected by N1—H1N···O1i [symmetry code: (i) x-y+2/3, x+1/3, -z+4/3] [not in Table 6, but in Table 8 for compound (4)?] hydrogen bonds in a racemic ring parallel to (001), leaving the pentenyl substituents oriented to the centre and the F atoms oriented outward, describing a threefold rotoinversion axis with [001] direction (Fig. 5a). Each six-membered ring is connected to six other equivalent structures along the three dimensions connected by six pairs of N1—H1N···O1i and O1—H1O···N1ii [symmetry code: (ii) -y+2/3, x-y+1/3, z+1/3] [not in Table 6, but in Table 8 for compound (4)?] hydrogen bonds generating R44(8) motifs (Fig. 5b). Each pair of enanti­omers are also related by an inversion centre at (1/2, 1/2, 1/2) and connected between them by probably induced dipolar inter­actions involving the halogen substituent. In a supra­molecular perspective, a view along [001] allows one to differentiate the centre of the rings at (2/3, 1/3, z) and (1/3, 2/3, z) (Fig. 5a). The structure at 100 K is transformed in a superstructure of the crystal structure at room temperature since the conformers (see Fig. S1 in the Supporting information) are perceptibly different. In this case, the molecular connectivity remains as room temperature and each individual molecule in the asymmetric unit constitutes a racemic sixfold molecular ring by N(1,2,3,4)1—H(1,2,3,4)N···O(3i,1ii,2iii,4iv)1 [symmetry codes: (i) x, y, z+1; (ii) -y+2/3, x-y+1/3, z-2/3; (iii) x-y+2/3, x+1/3, -z+1/3; (iv) y-1/3, -x+y+1/3, -z+4/3] hydrogen bonds (Table 7). However, the presence of both α and β conformers break half of the threefold rotoinversion axes observed at room temperature leaving a threefold screw axis with [001] direction in the centre of each molecular ring (Fig. 5c).

The supra­molecular assembly of both molecules in their crystals differ significantly, as expected for the very different sizes of the styryl and pentenyl substituents. In compound (4), each molecule is connected to four equivalent molecules at the same z value by two pairs of N1—H1N···O1i and O1—H1O···N1ii [symmetry codes: (i) x, y-1, z; (ii) -x+3/2, y+1/2, z] hydrogen bonds (Table 8), where atoms N1 and O1 act each as donor and acceptor. Hydrogen-bonded molecules form enanti­omorphic chains along the [010] direction (Fig. 6). The chains have a polar disposition, since all molecules in a chain are related by the b-glide plane normal to a (Fig. 6a). This makes the F atoms from all the molecules lie on the same side of the chain, leaving all nonpolar moieties on the other side. Each chain connects with an inverted chain on the [001] direction through weak C6—H6···F1iii [symmetry code: (iii) -x+1, -y+1, -z+1] dipolar inter­actions (2.47 Å) (Jelsch et al., 2015) (Figs. 6b and 6c). The inter­actions among double chains in the [100] and [001] directions are weak and probably dipolar or van der Waals in nature since no weak hydrogen bonds or ππ stacking inter­actions are detected.

Compund (5) shows different structures at room temperature and 100 K, with the low-temperature structure crystallizing in a klassengleiche subgroup of the room-temperature one, with a quadrupling of the unit-cell volume in the (110) plane. The descriptions of (5LT) could be obtained from that of (5RT) by the matrix P = [200 220 001] (Inter­national Tables for Crystallography, 2011). In order to confirm the group/subgroup relation of both structures and determine the degree of distortion of one respect to the other, the ordered part of the molecule in the (5RT) crystal was transformed into the subgroup of (5LT) using TRANSTRU program in the Bilbao Crystallography Server (Aroyo, Kirov et al., 2006; Aroyo, Perez-Mato et al., 2006; Aroyo et al., 2011) and the output structure, consisting of the ordered nuclei of the molecules was compared with the same nuclei in the (5LT) structure (all pentenyl residues, ordered and disordered, were removed) using COMPSTRU (Tasci et al., 2012) and an almost perfect overlap was obtained with an average/maximum atom displacement of 0.1667/0.2539 Å (for atom F1A). These deviations are very small considering the temperature difference and the fact that the room-temperature structure shows one molecule with the pentenyl chain split in two main positions, while the 100 K structure shows four independent molecules, two of them ordered and the other two displaying two and three different pentenyl chain conformations. This strongly suggests that the phase transition observed between room temperature and 100 K could be entirely explained by the partial ordering of the pentenly chains in half of the molecules, that breaks half of the 3 symmetry axes of the room-temperature structure on cooling. The refinement of the 100 K structure using the room-temperature model (R3 space group with halved a and b unit-cell parameters) using hkl data transformed using the inverse of the matrix above, provides a reasonable but significantly poorer model, with unreasonable displacement parameters (too high for a low-temperature model), a higher R factor and a much larger degree of disorder of the pentenyl chain that is very hard to model with less than three separate conformations. This clearly justifies the use of the subgroup to model the 100 K structure and again confirm that the ordering of the pentenyl chains is key to this phase transition.

Synthesis and crystallization top

The syntheses of the compounds (1)–(5) were carried out following our previously estabished experimental conditions (Acosta, Palma & Bahsas, 2010; Acosta et al., 2012). Particular details are described as follows. Recrystallization of (1)–(3) by slow evaporation of a solution in heptane gave crystals of suitable size and quality for single-crystal X-ray diffraction. In the case of compounds (4) and (5), the recrystallization was performed from a heptane–ethyl acetate (1:1 v/v) mixture which also gave crystals suitable for single-crystal X-ray diffraction.

Refinement details top

Crystal data, data collection and structure refinement details are summarized in Table 1. H atoms were placed in calculated positions (C—H = 0.93–1.00 Å) and included as riding contributions with isotropic displacement parameters set at 1.2-1.5 times of the Ueq value of the parent atom. H atoms belonging to OH and NH groups were located in difference density maps and refined freely. Some low-angle reflections strongly affected by the experiment, attenuated by the beam stop, for instance, were omitted for the final refinements, viz. for (1) 366 and 366, for (2) 011 and for (5) 120.

Computing details top

For all compounds, data collection: APEX2 (Bruker, 2006); cell refinement: SAINT (Bruker, 2006); data reduction: SAINT (Bruker, 2006). Program(s) used to solve structure: SIR92 (Altomare et al., 1994) for Compound_1, Compound_2, Compound_4; SUPERFLIP (Palatinus & Chapuis, 2007) for Compound_3, Compound_5a, Compound_5b. Program(s) used to refine structure: SHELXL2014 (Sheldrick, 2015) for Compound_1, Compound_3, Compound_4, Compound_5a, Compound_5b; SHELXL2014 (Sheldrick, 2008a, 2015b) for Compound_2. For all compounds, molecular graphics: Mercury (Macrae et al., 2008); software used to prepare material for publication: SHELXL2014 (Sheldrick, 2015).

Figures top
[Figure 1] Fig. 1. The two independent molecules of compound (1), both shown as the (2S,4R) enantiomorph. The molecular structures show displacement ellipsoids drawn at the 50% probability level. H atoms are shown as small spheres of arbitrary radii.
[Figure 2] Fig. 2. The molecular structure of (a) compound (2) and (b) compound (3), showing displacement ellipsoids drawn at the 50% probability level. H atoms are shown as small spheres of arbitrary radii.
[Figure 3] Fig. 3. The crystal structures of (a) compound (1), (b) compound (2) and (c) compound (3), showing the formation of hydrogen-bonded chains along the [010] direction.
[Figure 4] Fig. 4. The molecular structures of (a) compound (4), (b) compound (5) at room temperature and (c) compound (5) at 100 K with Z' = 4, showing displacement ellipsoids drawn at the 50% probability level.
[Figure 5] Fig. 5. (a) The packing of compound (5) at room temperature, showing the molecular rings with threefold rotoinvertion symmetry. (b) Compound (5) at room temperature, showing the R44(8) motifs. (c) The packing of compound (5) at 100 K, shown as the superstructure of the crystal structure at room temperature.
[Figure 6] Fig. 6. (a) The packing of the compound (4). Views along (b) [100] and (c) [010], showing the (N,O)—H···(O,N) and C—H···F hydrogen bonds.
(Compound_1) (2SR,4RS)-6,8-Dimethyl-2-(naphthalen-1-yl)-2,3,4,5-tetrahydro-1H-1,4-epoxy-1-benzazepine top
Crystal data top
C22H21NOF(000) = 1344
Mr = 315.40Dx = 1.300 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
a = 24.8049 (10) ÅCell parameters from 9740 reflections
b = 10.7126 (5) Åθ = 2.5–27.4°
c = 12.1932 (4) ŵ = 0.08 mm1
β = 95.929 (1)°T = 100 K
V = 3222.7 (2) Å3Parallelipiped, less
Z = 80.45 × 0.35 × 0.20 mm
Data collection top
Bruker Kappa APEXII
diffractometer
6012 reflections with I > 2σ(I)
π and ω scansRint = 0.040
Absorption correction: multi-scan
(SADABS; Bruker, 2006)
θmax = 27.5°, θmin = 2.1°
Tmin = 0.640, Tmax = 0.746h = 3229
48596 measured reflectionsk = 1213
7121 independent reflectionsl = 1115
Refinement top
Refinement on F20 restraints
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.047H-atom parameters constrained
wR(F2) = 0.122 w = 1/[σ2(Fo2) + (0.0523P)2 + 2.1093P]
where P = (Fo2 + 2Fc2)/3
S = 1.04(Δ/σ)max = 0.001
7121 reflectionsΔρmax = 0.37 e Å3
437 parametersΔρmin = 0.26 e Å3
Crystal data top
C22H21NOV = 3222.7 (2) Å3
Mr = 315.40Z = 8
Monoclinic, P21/cMo Kα radiation
a = 24.8049 (10) ŵ = 0.08 mm1
b = 10.7126 (5) ÅT = 100 K
c = 12.1932 (4) Å0.45 × 0.35 × 0.20 mm
β = 95.929 (1)°
Data collection top
Bruker Kappa APEXII
diffractometer
7121 independent reflections
Absorption correction: multi-scan
(SADABS; Bruker, 2006)
6012 reflections with I > 2σ(I)
Tmin = 0.640, Tmax = 0.746Rint = 0.040
48596 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0470 restraints
wR(F2) = 0.122H-atom parameters constrained
S = 1.04Δρmax = 0.37 e Å3
7121 reflectionsΔρmin = 0.26 e Å3
437 parameters
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
C28B0.90602 (6)0.47577 (14)0.66839 (12)0.0197 (3)
H28B0.94280.48930.65630.024*
C21B0.86514 (6)0.22394 (14)0.46455 (12)0.0209 (3)
H21B0.87960.17490.40960.025*
C22B0.81091 (6)0.20496 (15)0.48594 (12)0.0235 (3)
H22B0.78950.14380.44530.028*
C23B0.78897 (6)0.27362 (15)0.56446 (12)0.0219 (3)
H23B0.75240.26000.57820.026*
C27B0.88377 (6)0.54502 (15)0.74688 (12)0.0230 (3)
H27B0.90510.60560.78830.028*
C26B0.82940 (6)0.52654 (15)0.76618 (12)0.0239 (3)
H26B0.81410.57500.82040.029*
C25B0.79852 (6)0.43897 (15)0.70720 (12)0.0224 (3)
H25B0.76190.42710.72090.027*
C24B0.82058 (6)0.36549 (14)0.62571 (11)0.0193 (3)
C29B0.87542 (6)0.38444 (13)0.60482 (11)0.0178 (3)
C20B0.89752 (6)0.31156 (13)0.52118 (11)0.0172 (3)
C21A0.40742 (6)0.75903 (14)0.28172 (11)0.0183 (3)
H21A0.43000.71290.33490.022*
C22A0.35143 (6)0.76661 (14)0.29133 (12)0.0200 (3)
H22A0.33670.72450.35000.024*
C23A0.31807 (6)0.83392 (14)0.21706 (12)0.0190 (3)
H23A0.28040.83900.22470.023*
C24A0.33970 (6)0.89639 (13)0.12832 (11)0.0171 (3)
C25A0.30620 (6)0.96909 (14)0.05136 (12)0.0201 (3)
H25A0.26860.97650.05920.024*
C26A0.32723 (6)1.02862 (14)0.03388 (12)0.0219 (3)
H26A0.30431.07710.08450.026*
C27A0.38279 (6)1.01832 (14)0.04672 (12)0.0208 (3)
H27A0.39711.05900.10660.025*
C28A0.41652 (6)0.94975 (14)0.02680 (11)0.0179 (3)
H28A0.45400.94400.01730.021*
C29A0.39618 (6)0.88722 (13)0.11701 (11)0.0158 (3)
C20A0.43018 (6)0.81698 (13)0.19693 (11)0.0158 (3)
N1A0.52000 (5)0.75543 (11)0.28857 (9)0.0164 (3)
O1A0.51701 (4)0.62248 (9)0.26606 (8)0.0186 (2)
C2A0.49058 (6)0.80977 (13)0.18739 (11)0.0157 (3)
H2A0.50480.89540.17510.019*
C3A0.50543 (6)0.72134 (14)0.09308 (11)0.0185 (3)
H3AA0.47250.69220.04740.022*
H3AB0.52960.76360.04510.022*
C4A0.53460 (6)0.61237 (14)0.15643 (11)0.0190 (3)
H4A0.52260.53090.12200.023*
C5A0.59618 (6)0.62154 (14)0.16806 (11)0.0190 (3)
H5AA0.61210.54160.19650.023*
H5AB0.60890.63740.09490.023*
C6A0.66938 (6)0.76068 (14)0.26448 (11)0.0185 (3)
C7A0.68360 (6)0.86332 (15)0.33189 (12)0.0207 (3)
H7A0.72070.88670.34440.025*
C8A0.64515 (6)0.93285 (14)0.38160 (11)0.0199 (3)
C9A0.59144 (6)0.89464 (14)0.36574 (11)0.0184 (3)
H9A0.56460.93910.40010.022*
N1B0.99146 (5)0.27205 (11)0.59408 (9)0.0168 (3)
O1B0.99060 (4)0.14348 (9)0.55752 (8)0.0201 (2)
C2B0.95622 (6)0.33158 (13)0.50117 (11)0.0167 (3)
H2B0.96400.42310.49960.020*
C3B0.97530 (6)0.26920 (14)0.39758 (11)0.0187 (3)
H3BA0.94410.24730.34370.022*
H3BB1.00010.32460.36150.022*
C4B1.00495 (6)0.15132 (14)0.44408 (11)0.0203 (3)
H4B0.99230.07570.40080.024*
C5B1.06598 (6)0.16314 (15)0.45203 (12)0.0221 (3)
H5BA1.07730.18470.37890.027*
H5BB1.08290.08260.47560.027*
C6B1.13816 (6)0.30607 (15)0.54831 (12)0.0227 (3)
C7B1.15254 (6)0.40022 (16)0.62457 (12)0.0242 (3)
H7B1.18900.42850.63360.029*
C8B1.11508 (6)0.45440 (15)0.68815 (12)0.0227 (3)
C9B1.06216 (6)0.41094 (14)0.67492 (11)0.0193 (3)
H9B1.03600.44590.71770.023*
C5A20.61473 (6)0.72585 (14)0.24602 (11)0.0170 (3)
C6A20.71170 (6)0.69000 (15)0.20949 (13)0.0243 (3)
H6AA0.74750.72560.23200.036*
H6AB0.70380.69640.12930.036*
H6AC0.71130.60200.23150.036*
C8A20.66182 (7)1.04589 (15)0.45163 (13)0.0249 (3)
H8AA0.63031.07820.48490.037*
H8AB0.67581.11060.40530.037*
H8AC0.69011.02200.50990.037*
C9A20.57655 (6)0.79158 (14)0.29984 (11)0.0166 (3)
C5B21.08444 (6)0.26388 (14)0.53455 (11)0.0193 (3)
C6B21.17984 (7)0.25149 (18)0.48023 (13)0.0305 (4)
H6BA1.18020.16040.48790.046*
H6BB1.21570.28480.50600.046*
H6BC1.17070.27380.40260.046*
C8B21.13274 (7)0.55414 (16)0.77154 (13)0.0310 (4)
H8BA1.14870.62410.73440.046*
H8BB1.15970.51950.82780.046*
H8BC1.10130.58360.80660.046*
C9B21.04695 (6)0.31645 (13)0.59952 (11)0.0170 (3)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C28B0.0206 (7)0.0186 (8)0.0196 (7)0.0005 (6)0.0012 (5)0.0010 (5)
C21B0.0265 (8)0.0190 (8)0.0173 (7)0.0007 (6)0.0023 (6)0.0015 (5)
C22B0.0253 (8)0.0220 (8)0.0224 (7)0.0053 (6)0.0018 (6)0.0007 (6)
C23B0.0196 (7)0.0234 (8)0.0224 (7)0.0019 (6)0.0008 (6)0.0036 (6)
C27B0.0290 (8)0.0201 (8)0.0196 (7)0.0013 (6)0.0001 (6)0.0027 (6)
C26B0.0297 (8)0.0230 (8)0.0191 (7)0.0072 (6)0.0033 (6)0.0009 (6)
C25B0.0226 (8)0.0256 (8)0.0191 (7)0.0041 (6)0.0029 (6)0.0034 (6)
C24B0.0219 (7)0.0184 (7)0.0170 (6)0.0022 (6)0.0005 (5)0.0042 (5)
C29B0.0223 (7)0.0152 (7)0.0154 (6)0.0010 (6)0.0002 (5)0.0036 (5)
C20B0.0219 (7)0.0140 (7)0.0155 (6)0.0006 (6)0.0009 (5)0.0026 (5)
C21A0.0218 (7)0.0175 (7)0.0152 (6)0.0009 (6)0.0003 (5)0.0015 (5)
C22A0.0234 (8)0.0199 (8)0.0174 (7)0.0024 (6)0.0054 (5)0.0007 (6)
C23A0.0164 (7)0.0199 (8)0.0212 (7)0.0011 (6)0.0044 (5)0.0030 (6)
C24A0.0214 (7)0.0130 (7)0.0166 (6)0.0008 (5)0.0004 (5)0.0046 (5)
C25A0.0197 (7)0.0185 (8)0.0214 (7)0.0020 (6)0.0007 (5)0.0037 (6)
C26A0.0267 (8)0.0180 (8)0.0197 (7)0.0034 (6)0.0044 (6)0.0004 (6)
C27A0.0272 (8)0.0178 (7)0.0170 (7)0.0018 (6)0.0003 (6)0.0025 (5)
C28A0.0200 (7)0.0171 (7)0.0164 (6)0.0014 (6)0.0011 (5)0.0005 (5)
C29A0.0204 (7)0.0125 (7)0.0141 (6)0.0012 (5)0.0003 (5)0.0023 (5)
C20A0.0197 (7)0.0133 (7)0.0142 (6)0.0012 (5)0.0008 (5)0.0020 (5)
N1A0.0197 (6)0.0146 (6)0.0147 (5)0.0001 (5)0.0001 (4)0.0015 (4)
O1A0.0239 (5)0.0145 (5)0.0177 (5)0.0011 (4)0.0031 (4)0.0021 (4)
C2A0.0198 (7)0.0155 (7)0.0116 (6)0.0008 (5)0.0005 (5)0.0019 (5)
C3A0.0198 (7)0.0212 (8)0.0144 (6)0.0018 (6)0.0012 (5)0.0003 (5)
C4A0.0233 (8)0.0173 (7)0.0161 (7)0.0004 (6)0.0015 (5)0.0010 (5)
C5A0.0220 (8)0.0174 (7)0.0176 (7)0.0025 (6)0.0024 (5)0.0018 (5)
C6A0.0200 (7)0.0190 (7)0.0166 (6)0.0017 (6)0.0014 (5)0.0076 (5)
C7A0.0173 (7)0.0242 (8)0.0200 (7)0.0035 (6)0.0006 (5)0.0067 (6)
C8A0.0245 (8)0.0204 (8)0.0140 (6)0.0019 (6)0.0011 (5)0.0034 (5)
C9A0.0219 (7)0.0214 (8)0.0119 (6)0.0021 (6)0.0015 (5)0.0021 (5)
N1B0.0231 (6)0.0115 (6)0.0157 (6)0.0002 (5)0.0021 (5)0.0004 (4)
O1B0.0302 (6)0.0125 (5)0.0182 (5)0.0009 (4)0.0051 (4)0.0005 (4)
C2B0.0225 (7)0.0142 (7)0.0133 (6)0.0005 (6)0.0006 (5)0.0010 (5)
C3B0.0226 (7)0.0183 (7)0.0154 (6)0.0017 (6)0.0029 (5)0.0009 (5)
C4B0.0311 (8)0.0155 (7)0.0148 (6)0.0004 (6)0.0041 (6)0.0027 (5)
C5B0.0294 (8)0.0200 (8)0.0176 (7)0.0050 (6)0.0053 (6)0.0012 (6)
C6B0.0239 (8)0.0275 (9)0.0166 (7)0.0028 (6)0.0022 (6)0.0088 (6)
C7B0.0223 (8)0.0285 (9)0.0210 (7)0.0040 (6)0.0024 (6)0.0085 (6)
C8B0.0298 (8)0.0210 (8)0.0158 (7)0.0030 (6)0.0044 (6)0.0054 (6)
C9B0.0265 (8)0.0183 (8)0.0127 (6)0.0028 (6)0.0005 (5)0.0028 (5)
C5A20.0203 (7)0.0174 (7)0.0132 (6)0.0009 (6)0.0011 (5)0.0050 (5)
C6A20.0194 (8)0.0244 (8)0.0294 (8)0.0019 (6)0.0046 (6)0.0050 (6)
C8A20.0280 (8)0.0229 (8)0.0227 (7)0.0052 (6)0.0023 (6)0.0008 (6)
C9A20.0186 (7)0.0197 (7)0.0114 (6)0.0003 (6)0.0001 (5)0.0052 (5)
C5B20.0251 (8)0.0184 (8)0.0144 (6)0.0023 (6)0.0019 (5)0.0039 (5)
C6B20.0241 (8)0.0430 (11)0.0249 (8)0.0051 (7)0.0054 (6)0.0081 (7)
C8B20.0384 (10)0.0273 (9)0.0247 (8)0.0075 (7)0.0091 (7)0.0005 (7)
C9B20.0222 (7)0.0157 (7)0.0128 (6)0.0011 (6)0.0001 (5)0.0043 (5)
Geometric parameters (Å, º) top
C28B—C27B1.371 (2)C2A—C3A1.5629 (19)
C28B—C29B1.419 (2)C3A—C4A1.539 (2)
C21B—C20B1.374 (2)C4A—C5A1.523 (2)
C21B—C22B1.411 (2)C5A—C5A21.508 (2)
C22B—C23B1.364 (2)C6A—C7A1.396 (2)
C23B—C24B1.421 (2)C6A—C5A21.402 (2)
C27B—C26B1.407 (2)C6A—C6A21.507 (2)
C26B—C25B1.367 (2)C7A—C8A1.397 (2)
C25B—C24B1.421 (2)C8A—C9A1.388 (2)
C24B—C29B1.424 (2)C8A—C8A21.514 (2)
C29B—C20B1.437 (2)C9A—C9A21.393 (2)
C20B—C2B1.516 (2)N1B—O1B1.4471 (15)
C21A—C20A1.376 (2)N1B—C9B21.4513 (18)
C21A—C22A1.408 (2)N1B—C2B1.4998 (17)
C22A—C23A1.367 (2)O1B—C4B1.4658 (16)
C23A—C24A1.424 (2)C2B—C3B1.5459 (19)
C24A—C25A1.420 (2)C3B—C4B1.540 (2)
C24A—C29A1.425 (2)C4B—C5B1.512 (2)
C25A—C26A1.368 (2)C5B—C5B21.514 (2)
C26A—C27A1.407 (2)C6B—C7B1.393 (2)
C27A—C28A1.374 (2)C6B—C5B21.401 (2)
C28A—C29A1.4240 (19)C6B—C6B21.509 (2)
C29A—C20A1.4343 (19)C7B—C8B1.397 (2)
C20A—C2A1.517 (2)C8B—C9B1.386 (2)
N1A—C9A21.4480 (18)C8B—C8B21.508 (2)
N1A—O1A1.4509 (16)C9B—C9B21.393 (2)
N1A—C2A1.4858 (16)C5A2—C9A21.397 (2)
O1A—C4A1.4525 (17)C5B2—C9B21.401 (2)
C27B—C28B—C29B121.56 (14)C5A—C4A—C3A114.40 (12)
C20B—C21B—C22B121.63 (14)C5A2—C5A—C4A110.14 (12)
C23B—C22B—C21B120.60 (14)C7A—C6A—C5A2119.05 (14)
C22B—C23B—C24B120.24 (14)C7A—C6A—C6A2120.83 (13)
C28B—C27B—C26B120.17 (14)C5A2—C6A—C6A2120.10 (14)
C25B—C26B—C27B120.21 (14)C6A—C7A—C8A122.21 (14)
C26B—C25B—C24B120.84 (14)C9A—C8A—C7A118.09 (14)
C25B—C24B—C23B121.32 (14)C9A—C8A—C8A2121.10 (14)
C25B—C24B—C29B119.34 (14)C7A—C8A—C8A2120.80 (14)
C23B—C24B—C29B119.34 (13)C8A—C9A—C9A2120.51 (14)
C28B—C29B—C24B117.88 (13)O1B—N1B—C9B2108.04 (11)
C28B—C29B—C20B122.73 (13)O1B—N1B—C2B100.56 (10)
C24B—C29B—C20B119.39 (13)C9B2—N1B—C2B111.79 (11)
C21B—C20B—C29B118.80 (13)N1B—O1B—C4B103.82 (10)
C21B—C20B—C2B122.47 (13)N1B—C2B—C20B108.23 (11)
C29B—C20B—C2B118.71 (12)N1B—C2B—C3B103.27 (11)
C20A—C21A—C22A121.42 (13)C20B—C2B—C3B116.78 (12)
C23A—C22A—C21A120.65 (13)C4B—C3B—C2B103.21 (11)
C22A—C23A—C24A120.10 (13)O1B—C4B—C5B106.46 (11)
C25A—C24A—C23A121.29 (13)O1B—C4B—C3B103.96 (11)
C25A—C24A—C29A119.20 (13)C5B—C4B—C3B113.07 (12)
C23A—C24A—C29A119.50 (13)C4B—C5B—C5B2109.53 (12)
C26A—C25A—C24A120.98 (14)C7B—C6B—C5B2119.24 (14)
C25A—C26A—C27A120.18 (13)C7B—C6B—C6B2120.32 (15)
C28A—C27A—C26A120.43 (14)C5B2—C6B—C6B2120.43 (15)
C27A—C28A—C29A121.00 (14)C6B—C7B—C8B122.15 (14)
C28A—C29A—C24A118.20 (12)C9B—C8B—C7B118.17 (14)
C28A—C29A—C20A122.77 (13)C9B—C8B—C8B2121.45 (15)
C24A—C29A—C20A119.03 (13)C7B—C8B—C8B2120.34 (15)
C21A—C20A—C29A119.28 (13)C8B—C9B—C9B2120.63 (14)
C21A—C20A—C2A121.32 (12)C9A2—C5A2—C6A118.79 (13)
C29A—C20A—C2A119.39 (12)C9A2—C5A2—C5A119.49 (13)
C9A2—N1A—O1A108.10 (11)C6A—C5A2—C5A121.70 (13)
C9A2—N1A—C2A111.22 (11)C9A—C9A2—C5A2121.22 (13)
O1A—N1A—C2A102.50 (10)C9A—C9A2—N1A117.60 (13)
N1A—O1A—C4A103.47 (10)C5A2—C9A2—N1A121.17 (13)
N1A—C2A—C20A111.14 (11)C6B—C5B2—C9B2118.79 (14)
N1A—C2A—C3A103.92 (11)C6B—C5B2—C5B121.89 (14)
C20A—C2A—C3A113.39 (11)C9B2—C5B2—C5B119.31 (13)
C4A—C3A—C2A102.99 (11)C9B—C9B2—C5B2120.99 (14)
O1A—C4A—C5A107.67 (11)C9B—C9B2—N1B117.34 (13)
O1A—C4A—C3A103.59 (11)C5B2—C9B2—N1B121.63 (13)
C20B—C21B—C22B—C23B0.2 (2)C6A2—C6A—C7A—C8A178.20 (13)
C21B—C22B—C23B—C24B0.1 (2)C6A—C7A—C8A—C9A2.3 (2)
C29B—C28B—C27B—C26B0.0 (2)C6A—C7A—C8A—C8A2178.25 (13)
C28B—C27B—C26B—C25B0.4 (2)C7A—C8A—C9A—C9A21.5 (2)
C27B—C26B—C25B—C24B0.1 (2)C8A2—C8A—C9A—C9A2179.07 (13)
C26B—C25B—C24B—C23B179.56 (14)C9B2—N1B—O1B—C4B66.29 (12)
C26B—C25B—C24B—C29B0.6 (2)C2B—N1B—O1B—C4B50.95 (12)
C22B—C23B—C24B—C25B179.42 (14)O1B—N1B—C2B—C20B82.23 (12)
C22B—C23B—C24B—C29B0.4 (2)C9B2—N1B—C2B—C20B163.33 (11)
C27B—C28B—C29B—C24B0.6 (2)O1B—N1B—C2B—C3B42.17 (12)
C27B—C28B—C29B—C20B179.27 (14)C9B2—N1B—C2B—C3B72.27 (13)
C25B—C24B—C29B—C28B0.9 (2)C21B—C20B—C2B—N1B103.42 (15)
C23B—C24B—C29B—C28B179.22 (13)C29B—C20B—C2B—N1B74.69 (15)
C25B—C24B—C29B—C20B179.01 (13)C21B—C20B—C2B—C3B12.5 (2)
C23B—C24B—C29B—C20B0.9 (2)C29B—C20B—C2B—C3B169.40 (12)
C22B—C21B—C20B—C29B0.6 (2)N1B—C2B—C3B—C4B18.56 (14)
C22B—C21B—C20B—C2B178.69 (13)C20B—C2B—C3B—C4B100.06 (14)
C28B—C29B—C20B—C21B179.16 (13)N1B—O1B—C4B—C5B80.74 (13)
C24B—C29B—C20B—C21B0.9 (2)N1B—O1B—C4B—C3B38.89 (13)
C28B—C29B—C20B—C2B1.0 (2)C2B—C3B—C4B—O1B11.42 (14)
C24B—C29B—C20B—C2B179.11 (12)C2B—C3B—C4B—C5B103.62 (13)
C20A—C21A—C22A—C23A1.0 (2)O1B—C4B—C5B—C5B248.84 (15)
C21A—C22A—C23A—C24A0.5 (2)C3B—C4B—C5B—C5B264.69 (15)
C22A—C23A—C24A—C25A178.65 (14)C5B2—C6B—C7B—C8B0.0 (2)
C22A—C23A—C24A—C29A0.6 (2)C6B2—C6B—C7B—C8B179.14 (14)
C23A—C24A—C25A—C26A179.84 (14)C6B—C7B—C8B—C9B0.8 (2)
C29A—C24A—C25A—C26A0.9 (2)C6B—C7B—C8B—C8B2178.66 (14)
C24A—C25A—C26A—C27A0.1 (2)C7B—C8B—C9B—C9B20.5 (2)
C25A—C26A—C27A—C28A0.8 (2)C8B2—C8B—C9B—C9B2178.30 (13)
C26A—C27A—C28A—C29A0.3 (2)C7A—C6A—C5A2—C9A22.9 (2)
C27A—C28A—C29A—C24A0.7 (2)C6A2—C6A—C5A2—C9A2178.76 (13)
C27A—C28A—C29A—C20A178.61 (13)C7A—C6A—C5A2—C5A175.77 (13)
C25A—C24A—C29A—C28A1.35 (19)C6A2—C6A—C5A2—C5A2.5 (2)
C23A—C24A—C29A—C28A179.40 (13)C4A—C5A—C5A2—C9A23.82 (17)
C25A—C24A—C29A—C20A178.03 (12)C4A—C5A—C5A2—C6A174.86 (12)
C23A—C24A—C29A—C20A1.22 (19)C8A—C9A—C9A2—C5A21.5 (2)
C22A—C21A—C20A—C29A0.4 (2)C8A—C9A—C9A2—N1A178.84 (12)
C22A—C21A—C20A—C2A179.38 (13)C6A—C5A2—C9A2—C9A3.8 (2)
C28A—C29A—C20A—C21A179.91 (13)C5A—C5A2—C9A2—C9A174.96 (12)
C24A—C29A—C20A—C21A0.7 (2)C6A—C5A2—C9A2—N1A176.61 (12)
C28A—C29A—C20A—C2A1.1 (2)C5A—C5A2—C9A2—N1A4.67 (19)
C24A—C29A—C20A—C2A178.28 (12)O1A—N1A—C9A2—C9A152.72 (11)
C9A2—N1A—O1A—C4A68.06 (12)C2A—N1A—C9A2—C9A95.49 (14)
C2A—N1A—O1A—C4A49.48 (12)O1A—N1A—C9A2—C5A227.63 (16)
C9A2—N1A—C2A—C20A157.54 (12)C2A—N1A—C9A2—C5A284.15 (15)
O1A—N1A—C2A—C20A87.16 (12)C7B—C6B—C5B2—C9B21.1 (2)
C9A2—N1A—C2A—C3A80.15 (13)C6B2—C6B—C5B2—C9B2179.77 (13)
O1A—N1A—C2A—C3A35.15 (13)C7B—C6B—C5B2—C5B179.15 (13)
C21A—C20A—C2A—N1A10.41 (18)C6B2—C6B—C5B2—C5B0.0 (2)
C29A—C20A—C2A—N1A168.59 (12)C4B—C5B—C5B2—C6B171.67 (13)
C21A—C20A—C2A—C3A106.23 (15)C4B—C5B—C5B2—C9B28.55 (18)
C29A—C20A—C2A—C3A74.77 (16)C8B—C9B—C9B2—C5B20.6 (2)
N1A—C2A—C3A—C4A9.28 (14)C8B—C9B—C9B2—N1B177.22 (12)
C20A—C2A—C3A—C4A111.52 (12)C6B—C5B2—C9B2—C9B1.4 (2)
N1A—O1A—C4A—C5A78.62 (12)C5B—C5B2—C9B2—C9B178.81 (13)
N1A—O1A—C4A—C3A42.92 (12)C6B—C5B2—C9B2—N1B176.36 (12)
C2A—C3A—C4A—O1A19.79 (14)C5B—C5B2—C9B2—N1B3.4 (2)
C2A—C3A—C4A—C5A97.11 (13)O1B—N1B—C9B2—C9B152.18 (11)
O1A—C4A—C5A—C5A244.43 (15)C2B—N1B—C9B2—C9B98.08 (14)
C3A—C4A—C5A—C5A270.10 (15)O1B—N1B—C9B2—C5B225.66 (16)
C5A2—C6A—C7A—C8A0.1 (2)C2B—N1B—C9B2—C5B284.08 (16)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C2A—H2A···O1Ai1.002.613.4061 (17)137
C5A—H5AA···Cg1A2ii1.002.603.5600 (16)163
C4B—H4B···O1Biii1.002.433.1601 (18)129
Symmetry codes: (i) x+1, y+1/2, z+1/2; (ii) x+1, y1/2, z+1/2; (iii) x+2, y, z+1.
(Compound_2) (2SR,4RS)-6,9-Dimethyl-2-(naphthalen-1-yl)-2,3,4,5-tetrahydro-1H-1,4-epoxy-1-benzazepine top
Crystal data top
C22H21NODx = 1.217 Mg m3
Mr = 315.40Mo Kα radiation, λ = 0.71073 Å
Orthorhombic, P212121Cell parameters from 9810 reflections
a = 7.5541 (3) Åθ = 2.8–23.6°
b = 14.7914 (5) ŵ = 0.07 mm1
c = 15.4049 (5) ÅT = 298 K
V = 1721.28 (11) Å3Parallelipiped, less
Z = 40.51 × 0.32 × 0.25 mm
F(000) = 672
Data collection top
Bruker Kappa APEXII
diffractometer
4013 reflections with I > 2σ(I)
π and ω scansRint = 0.041
Absorption correction: multi-scan
(SADABS; Bruker, 2006)
θmax = 31.5°, θmin = 2.6°
Tmin = 0.86, Tmax = 0.98h = 1111
69991 measured reflectionsk = 2121
5630 independent reflectionsl = 2120
Refinement top
Refinement on F2Hydrogen site location: inferred from neighbouring sites
Least-squares matrix: fullH-atom parameters constrained
R[F2 > 2σ(F2)] = 0.043 w = 1/[σ2(Fo2) + (0.0474P)2 + 0.1943P]
where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.109(Δ/σ)max < 0.001
S = 1.03Δρmax = 0.17 e Å3
5630 reflectionsΔρmin = 0.16 e Å3
220 parametersAbsolute structure: Refined as an inversion twin
0 restraintsAbsolute structure parameter: 0 (2)
Crystal data top
C22H21NOV = 1721.28 (11) Å3
Mr = 315.40Z = 4
Orthorhombic, P212121Mo Kα radiation
a = 7.5541 (3) ŵ = 0.07 mm1
b = 14.7914 (5) ÅT = 298 K
c = 15.4049 (5) Å0.51 × 0.32 × 0.25 mm
Data collection top
Bruker Kappa APEXII
diffractometer
5630 independent reflections
Absorption correction: multi-scan
(SADABS; Bruker, 2006)
4013 reflections with I > 2σ(I)
Tmin = 0.86, Tmax = 0.98Rint = 0.041
69991 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.043H-atom parameters constrained
wR(F2) = 0.109Δρmax = 0.17 e Å3
S = 1.03Δρmin = 0.16 e Å3
5630 reflectionsAbsolute structure: Refined as an inversion twin
220 parametersAbsolute structure parameter: 0 (2)
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.

Refinement. Refined as a 2-component inversion twin

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
N10.9800 (2)0.52882 (10)0.31021 (10)0.0423 (3)
O10.9286 (2)0.43694 (9)0.33014 (10)0.0568 (4)
C20.9364 (2)0.57663 (11)0.39184 (11)0.0377 (4)
H20.91250.64030.37880.045*
C30.7626 (3)0.53080 (15)0.42245 (13)0.0485 (4)
H3A0.76850.51510.48350.058*
H3B0.66140.56990.41290.058*
C40.7519 (3)0.44603 (14)0.36570 (14)0.0577 (5)
H40.72130.39310.40090.069*
C50.6282 (3)0.45441 (15)0.28903 (15)0.0612 (6)
H5A0.61950.39680.25920.073*
H5B0.51090.47130.30890.073*
C60.5982 (3)0.55849 (14)0.15960 (12)0.0501 (5)
H60.48690.53410.14880.060*
C70.6613 (3)0.62674 (14)0.10782 (13)0.0509 (5)
H70.59180.64780.06230.061*
C80.8273 (3)0.66520 (12)0.12205 (12)0.0461 (4)
C90.9331 (2)0.63197 (12)0.18904 (11)0.0407 (4)
C201.0829 (2)0.57094 (11)0.45868 (11)0.0392 (4)
C211.2146 (3)0.50741 (14)0.45314 (14)0.0492 (5)
H211.21730.46790.40620.059*
C221.3460 (3)0.50135 (16)0.51779 (16)0.0607 (6)
H221.43330.45720.51340.073*
C231.3470 (3)0.55880 (16)0.58620 (15)0.0601 (6)
H231.43570.55410.62780.072*
C241.2156 (3)0.62541 (14)0.59503 (13)0.0488 (5)
C251.2122 (4)0.68617 (16)0.66644 (14)0.0626 (6)
H251.29990.68210.70860.075*
C261.0850 (4)0.74953 (16)0.67460 (14)0.0661 (7)
H261.08580.78860.72190.079*
C270.9521 (4)0.75635 (14)0.61188 (14)0.0611 (6)
H270.86480.80030.61770.073*
C280.9485 (3)0.69931 (13)0.54195 (13)0.0499 (5)
H280.85840.70460.50120.060*
C820.8909 (4)0.74143 (16)0.06431 (15)0.0690 (7)
H82A0.99630.72300.03440.104*
H82B0.91610.79360.09920.104*
H82C0.80050.75600.02280.104*
C921.1147 (3)0.67050 (16)0.20596 (15)0.0568 (5)
H92A1.17600.67810.15190.085*
H92B1.18010.62990.24250.085*
H92C1.10340.72800.23430.085*
C291.0806 (2)0.63220 (12)0.53094 (11)0.0410 (4)
C5A0.6987 (3)0.52552 (12)0.22777 (12)0.0443 (4)
C9A0.8675 (2)0.56170 (11)0.24071 (11)0.0384 (4)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
N10.0461 (8)0.0365 (7)0.0444 (8)0.0033 (6)0.0020 (7)0.0003 (6)
O10.0657 (9)0.0355 (6)0.0692 (9)0.0050 (7)0.0012 (8)0.0036 (6)
C20.0380 (8)0.0373 (8)0.0380 (8)0.0039 (7)0.0012 (7)0.0031 (7)
C30.0395 (9)0.0625 (11)0.0435 (10)0.0025 (8)0.0005 (8)0.0102 (9)
C40.0630 (13)0.0467 (11)0.0633 (13)0.0132 (10)0.0025 (10)0.0147 (10)
C50.0634 (13)0.0558 (12)0.0645 (13)0.0229 (10)0.0061 (11)0.0019 (10)
C60.0475 (11)0.0545 (10)0.0484 (10)0.0077 (9)0.0069 (9)0.0148 (9)
C70.0582 (12)0.0535 (10)0.0410 (10)0.0029 (10)0.0102 (9)0.0068 (9)
C80.0582 (12)0.0444 (9)0.0356 (9)0.0014 (8)0.0018 (8)0.0049 (8)
C90.0433 (9)0.0424 (8)0.0363 (8)0.0003 (8)0.0039 (7)0.0072 (7)
C200.0353 (8)0.0385 (8)0.0439 (9)0.0005 (7)0.0010 (7)0.0107 (7)
C210.0407 (10)0.0476 (10)0.0593 (11)0.0042 (8)0.0019 (9)0.0096 (9)
C220.0370 (10)0.0629 (13)0.0823 (16)0.0086 (9)0.0019 (10)0.0257 (12)
C230.0427 (11)0.0694 (13)0.0682 (13)0.0091 (10)0.0185 (10)0.0267 (12)
C240.0458 (10)0.0515 (10)0.0492 (10)0.0164 (9)0.0089 (9)0.0194 (9)
C250.0709 (15)0.0672 (14)0.0496 (11)0.0296 (13)0.0192 (11)0.0122 (10)
C260.0900 (18)0.0605 (13)0.0477 (11)0.0238 (14)0.0030 (12)0.0040 (10)
C270.0774 (16)0.0526 (11)0.0533 (11)0.0014 (11)0.0038 (11)0.0043 (10)
C280.0568 (12)0.0472 (10)0.0458 (10)0.0028 (9)0.0060 (9)0.0012 (8)
C820.0864 (18)0.0655 (13)0.0552 (12)0.0094 (13)0.0058 (12)0.0149 (11)
C920.0458 (11)0.0675 (13)0.0572 (12)0.0125 (10)0.0024 (10)0.0045 (10)
C290.0425 (9)0.0407 (8)0.0397 (9)0.0071 (8)0.0034 (8)0.0108 (7)
C5A0.0483 (10)0.0402 (8)0.0443 (9)0.0050 (8)0.0008 (8)0.0082 (7)
C9A0.0422 (9)0.0359 (7)0.0371 (8)0.0034 (7)0.0023 (7)0.0085 (7)
Geometric parameters (Å, º) top
N1—O11.446 (2)C9—C9A1.400 (2)
N1—C9A1.451 (2)C9—C921.508 (3)
N1—C21.480 (2)C20—C211.371 (3)
O1—C41.450 (3)C20—C291.435 (3)
C2—C201.514 (2)C21—C221.409 (3)
C2—C31.551 (3)C22—C231.354 (3)
C3—C41.531 (3)C23—C241.405 (3)
C4—C51.511 (3)C24—C251.421 (3)
C5—C5A1.510 (3)C24—C291.423 (3)
C6—C71.372 (3)C25—C261.348 (4)
C6—C5A1.384 (3)C26—C271.397 (4)
C7—C81.395 (3)C27—C281.369 (3)
C8—C91.395 (3)C28—C291.418 (3)
C8—C821.514 (3)C5A—C9A1.397 (3)
O1—N1—C9A108.33 (14)C21—C20—C2121.75 (17)
O1—N1—C2102.06 (13)C29—C20—C2118.92 (15)
C9A—N1—C2109.66 (13)C20—C21—C22120.7 (2)
N1—O1—C4103.89 (14)C23—C22—C21121.0 (2)
N1—C2—C20112.86 (14)C22—C23—C24120.77 (19)
N1—C2—C3103.77 (14)C23—C24—C25122.1 (2)
C20—C2—C3112.82 (14)C23—C24—C29119.2 (2)
C4—C3—C2103.24 (16)C25—C24—C29118.6 (2)
O1—C4—C5106.37 (18)C26—C25—C24121.7 (2)
O1—C4—C3104.08 (16)C25—C26—C27119.9 (2)
C5—C4—C3114.32 (18)C28—C27—C26120.9 (2)
C5A—C5—C4109.11 (17)C27—C28—C29120.8 (2)
C7—C6—C5A120.65 (19)C28—C29—C24118.09 (18)
C6—C7—C8121.40 (19)C28—C29—C20122.90 (16)
C9—C8—C7119.21 (18)C24—C29—C20119.01 (18)
C9—C8—C82121.02 (19)C6—C5A—C9A118.28 (18)
C7—C8—C82119.77 (19)C6—C5A—C5121.72 (18)
C8—C9—C9A118.63 (17)C9A—C5A—C5119.97 (18)
C8—C9—C92121.06 (17)C5A—C9A—C9121.78 (17)
C9A—C9—C92120.31 (17)C5A—C9A—N1120.77 (16)
C21—C20—C29119.30 (17)C9—C9A—N1117.44 (16)
C9A—N1—O1—C466.50 (17)C23—C24—C25—C26179.6 (2)
C2—N1—O1—C449.16 (17)C29—C24—C25—C260.1 (3)
O1—N1—C2—C2084.80 (17)C24—C25—C26—C270.2 (3)
C9A—N1—C2—C20160.50 (14)C25—C26—C27—C280.1 (3)
O1—N1—C2—C337.66 (16)C26—C27—C28—C290.5 (3)
C9A—N1—C2—C377.04 (16)C27—C28—C29—C240.6 (3)
N1—C2—C3—C413.45 (17)C27—C28—C29—C20179.87 (18)
C20—C2—C3—C4109.03 (17)C23—C24—C29—C28179.27 (18)
N1—O1—C4—C581.05 (18)C25—C24—C29—C280.3 (2)
N1—O1—C4—C340.02 (18)C23—C24—C29—C200.3 (2)
C2—C3—C4—O115.50 (18)C25—C24—C29—C20179.85 (17)
C2—C3—C4—C5100.11 (19)C21—C20—C29—C28179.47 (18)
O1—C4—C5—C5A49.5 (2)C2—C20—C29—C281.2 (3)
C3—C4—C5—C5A64.8 (2)C21—C20—C29—C240.1 (2)
C5A—C6—C7—C80.2 (3)C2—C20—C29—C24178.37 (15)
C6—C7—C8—C91.6 (3)C7—C6—C5A—C9A1.9 (3)
C6—C7—C8—C82179.03 (19)C7—C6—C5A—C5176.3 (2)
C7—C8—C9—C9A0.9 (3)C4—C5—C5A—C6168.88 (18)
C82—C8—C9—C9A179.70 (18)C4—C5—C5A—C9A9.2 (3)
C7—C8—C9—C92179.07 (18)C6—C5A—C9A—C92.5 (3)
C82—C8—C9—C920.3 (3)C5—C5A—C9A—C9175.63 (17)
N1—C2—C20—C2117.7 (2)C6—C5A—C9A—N1178.99 (16)
C3—C2—C20—C2199.5 (2)C5—C5A—C9A—N12.9 (3)
N1—C2—C20—C29164.02 (15)C8—C9—C9A—C5A1.1 (2)
C3—C2—C20—C2978.74 (19)C92—C9—C9A—C5A178.87 (17)
C29—C20—C21—C220.6 (3)C8—C9—C9A—N1179.66 (15)
C2—C20—C21—C22177.71 (17)C92—C9—C9A—N10.3 (2)
C20—C21—C22—C231.0 (3)O1—N1—C9A—C5A25.6 (2)
C21—C22—C23—C240.7 (3)C2—N1—C9A—C5A84.97 (19)
C22—C23—C24—C25179.44 (19)O1—N1—C9A—C9155.80 (14)
C22—C23—C24—C290.1 (3)C2—N1—C9A—C993.59 (18)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C82—H82···O1i0.962.663.587 (3)164
Symmetry code: (i) x+2, y+1/2, z+1/2.
(Compound_3) (2SR,4RS)-8,9-Dimethyl-2-(naphthalen-1-yl)-2,3,4,5-tetrahydro-1H-1,4-epoxy-1-benzazepine top
Crystal data top
C22H21NOF(000) = 336
Mr = 315.40Dx = 1.262 Mg m3
Monoclinic, P21Mo Kα radiation, λ = 0.71073 Å
a = 7.2201 (2) ÅCell parameters from 9843 reflections
b = 7.8128 (3) Åθ = 2.8–30.2°
c = 14.7409 (5) ŵ = 0.08 mm1
β = 93.690 (2)°T = 100 K
V = 829.80 (5) Å3Paralelipiped, less
Z = 20.30 × 0.30 × 0.15 mm
Data collection top
Bruker Kappa APEXII
diffractometer
4638 reflections with I > 2σ(I)
π and ω scansRint = 0.023
Absorption correction: multi-scan
(SADABS; Bruker, 2006)
θmax = 30.3°, θmin = 1.4°
Tmin = 0.92, Tmax = 0.99h = 1010
27947 measured reflectionsk = 1111
4874 independent reflectionsl = 2020
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.033H-atom parameters constrained
wR(F2) = 0.092 w = 1/[σ2(Fo2) + (0.0566P)2 + 0.1148P]
where P = (Fo2 + 2Fc2)/3
S = 1.04(Δ/σ)max < 0.001
4874 reflectionsΔρmax = 0.30 e Å3
219 parametersΔρmin = 0.19 e Å3
1 restraintAbsolute structure: Flack x determined using 2066 quotients [(I+)-(I-)]/[(I+)+(I-)] (Parsons et al., 2013)
Primary atom site location: iterativeAbsolute structure parameter: 0.1 (3)
Crystal data top
C22H21NOV = 829.80 (5) Å3
Mr = 315.40Z = 2
Monoclinic, P21Mo Kα radiation
a = 7.2201 (2) ŵ = 0.08 mm1
b = 7.8128 (3) ÅT = 100 K
c = 14.7409 (5) Å0.30 × 0.30 × 0.15 mm
β = 93.690 (2)°
Data collection top
Bruker Kappa APEXII
diffractometer
4874 independent reflections
Absorption correction: multi-scan
(SADABS; Bruker, 2006)
4638 reflections with I > 2σ(I)
Tmin = 0.92, Tmax = 0.99Rint = 0.023
27947 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.033H-atom parameters constrained
wR(F2) = 0.092Δρmax = 0.30 e Å3
S = 1.04Δρmin = 0.19 e Å3
4874 reflectionsAbsolute structure: Flack x determined using 2066 quotients [(I+)-(I-)]/[(I+)+(I-)] (Parsons et al., 2013)
219 parametersAbsolute structure parameter: 0.1 (3)
1 restraint
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
N10.15129 (17)0.35804 (16)0.21245 (8)0.0165 (2)
O10.09164 (15)0.19439 (14)0.17551 (7)0.0205 (2)
C20.08542 (18)0.35174 (18)0.30555 (9)0.0150 (2)
H20.06430.47090.32740.018*
C30.10421 (19)0.2564 (2)0.29297 (10)0.0187 (3)
H3A0.11270.16370.33830.022*
H3B0.20940.33640.29830.022*
C40.1017 (2)0.1839 (2)0.19629 (10)0.0209 (3)
H40.14510.06240.19450.025*
C50.2114 (2)0.2901 (2)0.12504 (10)0.0227 (3)
H5A0.21690.22960.06590.027*
H5B0.33990.30600.14320.027*
C60.2051 (2)0.5930 (2)0.06265 (10)0.0230 (3)
C70.1176 (2)0.7511 (2)0.05942 (10)0.0254 (3)
H70.17460.84030.02380.030*
C80.0513 (2)0.7813 (2)0.10715 (10)0.0230 (3)
H80.10640.89150.10500.028*
C90.1414 (2)0.65198 (18)0.15833 (9)0.0189 (3)
C200.22202 (18)0.26185 (18)0.37162 (9)0.0149 (2)
C210.37597 (19)0.1793 (2)0.34334 (10)0.0189 (3)
H210.40010.18090.28070.023*
C220.4994 (2)0.0918 (2)0.40580 (11)0.0227 (3)
H220.60400.03400.38460.027*
C230.46936 (19)0.0897 (2)0.49629 (11)0.0218 (3)
H230.55330.03090.53760.026*
C240.31329 (18)0.17489 (19)0.52887 (9)0.0170 (3)
C250.2805 (2)0.1761 (2)0.62270 (10)0.0208 (3)
H250.36510.11930.66460.025*
C260.1294 (2)0.2575 (2)0.65411 (10)0.0220 (3)
H260.11000.25760.71720.026*
C270.0027 (2)0.3414 (2)0.59219 (10)0.0210 (3)
H270.10310.39660.61380.025*
C280.03096 (19)0.34389 (19)0.50090 (10)0.0178 (3)
H280.05520.40180.46030.021*
C620.3885 (2)0.5624 (3)0.01018 (12)0.0316 (4)
H62A0.41410.65700.03250.047*
H62B0.48740.55580.05250.047*
H62C0.38290.45470.02360.047*
C920.3224 (2)0.6848 (2)0.21182 (10)0.0230 (3)
H92A0.40710.58880.20370.035*
H92B0.30000.69650.27640.035*
H92C0.37790.79050.19020.035*
C290.18719 (18)0.26126 (18)0.46621 (9)0.0147 (2)
C5A0.1198 (2)0.46197 (19)0.11569 (9)0.0193 (3)
C9A0.0542 (2)0.49217 (18)0.16048 (9)0.0170 (3)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
N10.0208 (5)0.0128 (5)0.0158 (5)0.0005 (4)0.0010 (4)0.0013 (4)
O10.0228 (5)0.0150 (5)0.0240 (5)0.0001 (4)0.0026 (4)0.0053 (4)
C20.0153 (5)0.0133 (6)0.0165 (5)0.0015 (5)0.0019 (4)0.0008 (5)
C30.0171 (6)0.0178 (6)0.0210 (6)0.0004 (5)0.0003 (5)0.0013 (5)
C40.0217 (6)0.0162 (6)0.0247 (6)0.0019 (5)0.0009 (5)0.0031 (6)
C50.0229 (7)0.0239 (7)0.0208 (6)0.0028 (6)0.0030 (5)0.0036 (5)
C60.0242 (7)0.0286 (8)0.0160 (6)0.0067 (6)0.0002 (5)0.0013 (6)
C70.0318 (8)0.0257 (7)0.0188 (6)0.0095 (6)0.0031 (6)0.0045 (6)
C80.0311 (7)0.0187 (7)0.0197 (6)0.0026 (6)0.0066 (6)0.0029 (5)
C90.0230 (7)0.0187 (7)0.0154 (6)0.0001 (5)0.0033 (5)0.0003 (5)
C200.0151 (5)0.0113 (5)0.0182 (6)0.0002 (5)0.0012 (4)0.0010 (5)
C210.0176 (6)0.0160 (6)0.0234 (6)0.0014 (5)0.0048 (5)0.0015 (6)
C220.0160 (6)0.0200 (7)0.0328 (8)0.0057 (6)0.0061 (5)0.0055 (6)
C230.0161 (6)0.0191 (7)0.0299 (7)0.0026 (5)0.0009 (5)0.0067 (6)
C240.0154 (6)0.0134 (6)0.0218 (6)0.0016 (5)0.0007 (5)0.0030 (5)
C250.0233 (7)0.0178 (6)0.0208 (6)0.0055 (5)0.0030 (5)0.0049 (6)
C260.0301 (7)0.0179 (6)0.0181 (6)0.0078 (6)0.0031 (5)0.0004 (5)
C270.0250 (7)0.0161 (6)0.0227 (7)0.0012 (6)0.0075 (5)0.0008 (6)
C280.0188 (6)0.0141 (6)0.0206 (6)0.0022 (5)0.0025 (5)0.0003 (5)
C620.0271 (8)0.0422 (10)0.0246 (7)0.0097 (7)0.0056 (6)0.0028 (7)
C920.0255 (7)0.0223 (7)0.0212 (6)0.0057 (6)0.0013 (5)0.0005 (6)
C290.0150 (5)0.0108 (5)0.0183 (6)0.0009 (5)0.0013 (4)0.0009 (5)
C5A0.0216 (6)0.0201 (7)0.0161 (6)0.0014 (5)0.0000 (5)0.0023 (5)
C9A0.0209 (6)0.0167 (6)0.0136 (5)0.0022 (5)0.0014 (5)0.0004 (5)
Geometric parameters (Å, º) top
N1—O11.4445 (15)C9—C9A1.400 (2)
N1—C9A1.4516 (18)C9—C921.504 (2)
N1—C21.4819 (17)C20—C211.3730 (19)
O1—C41.4504 (18)C20—C291.4328 (17)
C2—C201.5135 (18)C21—C221.415 (2)
C2—C31.5591 (19)C22—C231.365 (2)
C3—C41.535 (2)C23—C241.419 (2)
C4—C51.520 (2)C24—C251.4182 (19)
C5—C5A1.507 (2)C24—C291.4245 (17)
C6—C71.390 (2)C25—C261.369 (2)
C6—C5A1.406 (2)C26—C271.411 (2)
C6—C621.509 (2)C27—C281.374 (2)
C7—C81.389 (2)C28—C291.4229 (18)
C8—C91.396 (2)C5A—C9A1.4008 (19)
O1—N1—C9A108.54 (10)C21—C20—C2121.96 (12)
O1—N1—C2102.36 (10)C29—C20—C2118.67 (11)
C9A—N1—C2109.87 (11)C20—C21—C22121.16 (13)
N1—O1—C4103.76 (10)C23—C22—C21120.57 (13)
N1—C2—C20112.13 (11)C22—C23—C24120.30 (13)
N1—C2—C3103.74 (11)C25—C24—C23121.29 (13)
C20—C2—C3112.69 (11)C25—C24—C29119.29 (12)
C4—C3—C2102.93 (11)C23—C24—C29119.42 (12)
O1—C4—C5106.80 (12)C26—C25—C24121.31 (13)
O1—C4—C3104.16 (11)C25—C26—C27119.64 (13)
C5—C4—C3113.79 (13)C28—C27—C26120.60 (14)
C5A—C5—C4109.70 (12)C27—C28—C29121.10 (13)
C7—C6—C5A118.84 (14)C28—C29—C24118.05 (12)
C7—C6—C62120.59 (15)C28—C29—C20122.76 (12)
C5A—C6—C62120.57 (16)C24—C29—C20119.19 (11)
C8—C7—C6121.34 (15)C9A—C5A—C6119.15 (14)
C7—C8—C9120.94 (15)C9A—C5A—C5119.50 (13)
C8—C9—C9A117.59 (14)C6—C5A—C5121.36 (14)
C8—C9—C92121.23 (14)C9—C9A—C5A122.05 (13)
C9A—C9—C92121.14 (13)C9—C9A—N1116.95 (12)
C21—C20—C29119.36 (12)C5A—C9A—N1121.00 (13)
C9A—N1—O1—C466.84 (13)C24—C25—C26—C270.3 (2)
C2—N1—O1—C449.28 (12)C25—C26—C27—C280.9 (2)
O1—N1—C2—C2084.76 (12)C26—C27—C28—C290.5 (2)
C9A—N1—C2—C20160.08 (11)C27—C28—C29—C240.3 (2)
O1—N1—C2—C337.12 (12)C27—C28—C29—C20179.63 (13)
C9A—N1—C2—C378.04 (13)C25—C24—C29—C280.81 (19)
N1—C2—C3—C412.43 (14)C23—C24—C29—C28179.32 (14)
C20—C2—C3—C4109.07 (13)C25—C24—C29—C20179.14 (14)
N1—O1—C4—C579.98 (13)C23—C24—C29—C200.73 (19)
N1—O1—C4—C340.73 (13)C21—C20—C29—C28179.95 (14)
C2—C3—C4—O116.50 (15)C2—C20—C29—C281.0 (2)
C2—C3—C4—C599.41 (14)C21—C20—C29—C240.01 (19)
O1—C4—C5—C5A48.20 (15)C2—C20—C29—C24179.07 (12)
C3—C4—C5—C5A66.15 (16)C7—C6—C5A—C9A2.7 (2)
C5A—C6—C7—C80.1 (2)C62—C6—C5A—C9A177.31 (13)
C62—C6—C7—C8179.88 (14)C7—C6—C5A—C5177.46 (14)
C6—C7—C8—C91.6 (2)C62—C6—C5A—C52.5 (2)
C7—C8—C9—C9A0.7 (2)C4—C5—C5A—C9A8.16 (18)
C7—C8—C9—C92178.66 (14)C4—C5—C5A—C6172.01 (13)
N1—C2—C20—C217.43 (19)C8—C9—C9A—C5A1.9 (2)
C3—C2—C20—C21109.19 (15)C92—C9—C9A—C5A176.00 (13)
N1—C2—C20—C29173.53 (12)C8—C9—C9A—N1178.78 (12)
C3—C2—C20—C2969.86 (16)C92—C9—C9A—N13.28 (19)
C29—C20—C21—C220.8 (2)C6—C5A—C9A—C93.7 (2)
C2—C20—C21—C22178.19 (14)C5—C5A—C9A—C9176.48 (13)
C20—C21—C22—C231.0 (2)C6—C5A—C9A—N1177.07 (12)
C21—C22—C23—C240.2 (2)C5—C5A—C9A—N12.8 (2)
C22—C23—C24—C25179.25 (14)O1—N1—C9A—C9154.16 (12)
C22—C23—C24—C290.6 (2)C2—N1—C9A—C994.67 (14)
C23—C24—C25—C26179.64 (14)O1—N1—C9A—C5A26.55 (16)
C29—C24—C25—C260.5 (2)C2—N1—C9A—C5A84.62 (15)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C8—H8···O1i0.952.593.3880 (19)142
C27—H27···Cg31ii0.952.863.6294 (16)139
C28—H28···Cg32ii0.952.903.6116 (16)133
Symmetry codes: (i) x, y+1, z; (ii) x, y+1/2, z+1.
(Compound_4) 7-Fluoro-cis-2-[(E)-styryl]-2,3,4,5-tetrahydro-1H-1-\ benzazepin-4-ol top
Crystal data top
C18H18FNODx = 1.281 Mg m3
Mr = 283.33Mo Kα radiation, λ = 0.71073 Å
Orthorhombic, PbcaCell parameters from 9770 reflections
a = 7.5932 (3) Åθ = 2.4–29.8°
b = 7.5859 (4) ŵ = 0.09 mm1
c = 51.010 (3) ÅT = 100 K
V = 2938.2 (2) Å3Parallelepiped, less
Z = 80.30 × 0.25 × 0.20 mm
F(000) = 1200
Data collection top
Bruker Kappa APEXII
diffractometer
3407 reflections with I > 2σ(I)
π and ω scansRint = 0.027
Absorption correction: multi-scan
(SADABS; Bruker, 2006)
θmax = 30.3°, θmin = 1.6°
Tmin = 0.90, Tmax = 0.98h = 1010
40696 measured reflectionsk = 1010
3764 independent reflectionsl = 6769
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)] = 0.045Hydrogen site location: mixed
wR(F2) = 0.108H atoms treated by a mixture of independent and constrained refinement
S = 1.09 w = 1/[σ2(Fo2) + (0.0371P)2 + 2.0455P]
where P = (Fo2 + 2Fc2)/3
3764 reflections(Δ/σ)max = 0.001
198 parametersΔρmax = 0.32 e Å3
0 restraintsΔρmin = 0.23 e Å3
Crystal data top
C18H18FNOV = 2938.2 (2) Å3
Mr = 283.33Z = 8
Orthorhombic, PbcaMo Kα radiation
a = 7.5932 (3) ŵ = 0.09 mm1
b = 7.5859 (4) ÅT = 100 K
c = 51.010 (3) Å0.30 × 0.25 × 0.20 mm
Data collection top
Bruker Kappa APEXII
diffractometer
3764 independent reflections
Absorption correction: multi-scan
(SADABS; Bruker, 2006)
3407 reflections with I > 2σ(I)
Tmin = 0.90, Tmax = 0.98Rint = 0.027
40696 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0450 restraints
wR(F2) = 0.108H atoms treated by a mixture of independent and constrained refinement
S = 1.09Δρmax = 0.32 e Å3
3764 reflectionsΔρmin = 0.23 e Å3
198 parameters
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
O10.58993 (12)0.76036 (12)0.39113 (2)0.0191 (2)
N10.52091 (13)0.18488 (14)0.39564 (2)0.0147 (2)
F10.41254 (14)0.24707 (13)0.50268 (2)0.0359 (2)
C20.42190 (15)0.29702 (16)0.37707 (2)0.0149 (2)
H20.30010.31450.38410.018*
C30.50905 (16)0.47789 (16)0.37386 (2)0.0159 (2)
H3A0.63240.45950.36820.019*
H3B0.44780.54170.35960.019*
C40.51013 (16)0.59518 (16)0.39810 (2)0.0163 (2)
H40.38530.61820.40330.020*
C50.60719 (16)0.51906 (16)0.42174 (2)0.0161 (2)
H5A0.72590.48230.41590.019*
H5B0.62340.61510.43470.019*
C60.49800 (17)0.37683 (17)0.46270 (2)0.0204 (3)
H60.52170.48390.47170.025*
C70.43774 (18)0.23177 (19)0.47628 (2)0.0230 (3)
C80.40179 (17)0.07342 (18)0.46443 (3)0.0213 (3)
H80.36260.02520.47430.026*
C90.42478 (16)0.06272 (17)0.43749 (2)0.0178 (2)
H90.39900.04470.42870.021*
C210.40917 (16)0.21035 (17)0.35058 (2)0.0175 (2)
H210.33780.26770.33790.021*
C220.48755 (16)0.06184 (17)0.34316 (2)0.0189 (3)
H220.55610.00260.35600.023*
C230.47892 (17)0.02029 (17)0.31701 (2)0.0194 (3)
C240.59407 (19)0.1587 (2)0.31126 (3)0.0260 (3)
H240.67420.19840.32430.031*
C250.5932 (2)0.2391 (2)0.28677 (3)0.0305 (3)
H250.67310.33220.28310.037*
C260.4756 (2)0.1834 (2)0.26774 (3)0.0287 (3)
H260.47510.23760.25100.034*
C270.3588 (2)0.04858 (19)0.27327 (3)0.0268 (3)
H270.27730.01130.26030.032*
C280.35978 (19)0.03281 (18)0.29769 (2)0.0230 (3)
H280.27880.12520.30130.028*
C5A0.52398 (15)0.36544 (16)0.43571 (2)0.0156 (2)
C9A0.48504 (15)0.20665 (16)0.42300 (2)0.0145 (2)
H1N0.503 (2)0.071 (2)0.3910 (3)0.016 (4)*
H1O0.705 (3)0.743 (3)0.3911 (3)0.038 (5)*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O10.0207 (4)0.0099 (4)0.0268 (5)0.0010 (3)0.0003 (4)0.0033 (3)
N10.0191 (5)0.0097 (5)0.0153 (5)0.0002 (4)0.0008 (4)0.0010 (4)
F10.0618 (6)0.0304 (5)0.0156 (4)0.0003 (4)0.0054 (4)0.0026 (3)
C20.0149 (5)0.0127 (6)0.0170 (5)0.0006 (4)0.0016 (4)0.0019 (4)
C30.0172 (5)0.0124 (5)0.0181 (5)0.0004 (4)0.0010 (4)0.0034 (4)
C40.0164 (5)0.0101 (5)0.0222 (6)0.0006 (4)0.0005 (4)0.0029 (4)
C50.0182 (5)0.0115 (5)0.0185 (5)0.0013 (4)0.0012 (4)0.0002 (4)
C60.0270 (6)0.0166 (6)0.0177 (6)0.0022 (5)0.0009 (5)0.0007 (5)
C70.0297 (6)0.0251 (7)0.0142 (5)0.0032 (6)0.0006 (5)0.0039 (5)
C80.0232 (6)0.0192 (6)0.0214 (6)0.0011 (5)0.0003 (5)0.0077 (5)
C90.0177 (5)0.0145 (6)0.0213 (6)0.0017 (5)0.0027 (4)0.0028 (5)
C210.0191 (5)0.0162 (6)0.0171 (5)0.0031 (5)0.0039 (4)0.0030 (4)
C220.0198 (6)0.0200 (6)0.0168 (6)0.0003 (5)0.0034 (4)0.0011 (5)
C230.0235 (6)0.0170 (6)0.0178 (6)0.0033 (5)0.0000 (5)0.0007 (5)
C240.0275 (7)0.0266 (7)0.0240 (6)0.0029 (6)0.0017 (5)0.0016 (5)
C250.0342 (7)0.0289 (8)0.0283 (7)0.0014 (6)0.0042 (6)0.0065 (6)
C260.0407 (8)0.0270 (7)0.0184 (6)0.0099 (6)0.0042 (6)0.0034 (5)
C270.0401 (8)0.0233 (7)0.0170 (6)0.0078 (6)0.0048 (5)0.0033 (5)
C280.0311 (7)0.0180 (6)0.0200 (6)0.0015 (5)0.0036 (5)0.0018 (5)
C5A0.0156 (5)0.0134 (6)0.0176 (5)0.0025 (4)0.0008 (4)0.0014 (4)
C9A0.0131 (5)0.0146 (6)0.0158 (5)0.0012 (4)0.0014 (4)0.0016 (4)
Geometric parameters (Å, º) top
O1—C41.4367 (14)C8—C91.3880 (17)
N1—C9A1.4312 (15)C9—C9A1.3957 (17)
N1—C21.4786 (15)C21—C221.3292 (18)
F1—C71.3649 (14)C22—C231.4739 (17)
C2—C211.5058 (17)C23—C281.3970 (18)
C2—C31.5321 (16)C23—C241.3974 (19)
C3—C41.5235 (17)C24—C251.390 (2)
C4—C51.5264 (16)C25—C261.385 (2)
C5—C5A1.5050 (16)C26—C271.382 (2)
C6—C71.3785 (19)C27—C281.3904 (18)
C6—C5A1.3936 (17)C5A—C9A1.3995 (17)
C7—C81.372 (2)
C9A—N1—C2117.48 (10)C21—C22—C23126.59 (12)
N1—C2—C21110.88 (10)C28—C23—C24118.28 (12)
N1—C2—C3111.35 (9)C28—C23—C22123.04 (12)
C21—C2—C3108.83 (10)C24—C23—C22118.68 (12)
C4—C3—C2116.02 (10)C25—C24—C23121.02 (13)
O1—C4—C3108.10 (10)C26—C25—C24119.93 (14)
O1—C4—C5108.78 (10)C27—C26—C25119.75 (13)
C3—C4—C5115.01 (10)C26—C27—C28120.53 (13)
C5A—C5—C4117.65 (10)C27—C28—C23120.48 (13)
C7—C6—C5A119.61 (12)C6—C5A—C9A118.76 (11)
F1—C7—C8118.75 (12)C6—C5A—C5118.63 (11)
F1—C7—C6118.32 (12)C9A—C5A—C5122.40 (11)
C8—C7—C6122.92 (12)C9—C9A—C5A119.82 (11)
C7—C8—C9117.54 (12)C9—C9A—N1119.24 (11)
C8—C9—C9A121.33 (12)C5A—C9A—N1120.71 (11)
C22—C21—C2126.64 (11)
C9A—N1—C2—C21154.56 (10)C22—C23—C24—C25179.08 (13)
C9A—N1—C2—C384.10 (12)C23—C24—C25—C260.7 (2)
N1—C2—C3—C465.54 (13)C24—C25—C26—C270.4 (2)
C21—C2—C3—C4171.93 (10)C25—C26—C27—C280.7 (2)
C2—C3—C4—O1177.68 (9)C26—C27—C28—C230.1 (2)
C2—C3—C4—C560.58 (14)C24—C23—C28—C271.1 (2)
O1—C4—C5—C5A168.01 (10)C22—C23—C28—C27179.41 (12)
C3—C4—C5—C5A70.62 (14)C7—C6—C5A—C9A1.06 (18)
C5A—C6—C7—F1179.62 (12)C7—C6—C5A—C5173.82 (12)
C5A—C6—C7—C80.2 (2)C4—C5—C5A—C6126.84 (12)
F1—C7—C8—C9178.58 (12)C4—C5—C5A—C9A58.48 (16)
C6—C7—C8—C91.3 (2)C8—C9—C9A—C5A0.20 (18)
C7—C8—C9—C9A1.04 (19)C8—C9—C9A—N1174.73 (11)
N1—C2—C21—C226.00 (17)C6—C5A—C9A—C91.26 (17)
C3—C2—C21—C22116.81 (14)C5—C5A—C9A—C9173.41 (11)
C2—C21—C22—C23178.19 (12)C6—C5A—C9A—N1175.70 (11)
C21—C22—C23—C2811.9 (2)C5—C5A—C9A—N11.03 (17)
C21—C22—C23—C24168.68 (13)C2—N1—C9A—C9120.88 (12)
C28—C23—C24—C251.4 (2)C2—N1—C9A—C5A64.65 (14)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N1—H1N···O1i0.904 (17)2.450 (16)3.2709 (14)151 (13)
O1—H1O···N1ii0.88 (2)2.14 (2)3.0187 (14)172.9 (16)
C5—H5A···N1ii0.992.673.3657 (16)128
C6—H6···F1iii0.952.473.4236 (16)177
C5—H5A···O1iv0.992.533.4027 (15)148
Symmetry codes: (i) x, y1, z; (ii) x+3/2, y+1/2, z; (iii) x+1, y+1, z+1; (iv) x+3/2, y1/2, z.
(Compound_5a) 7-Fluoro-cis-2-[(E)-pent-1-enyl]-2,3,4,5-tetrahydro-1H-1-benzazepin-4-ol top
Crystal data top
C15H20FNODx = 1.207 Mg m3
Mr = 249.32Mo Kα radiation, λ = 0.71073 Å
Trigonal, R3:HCell parameters from 9421 reflections
a = 25.119 (2) Åθ = 2.8–22.2°
c = 11.2812 (12) ŵ = 0.08 mm1
V = 6164.2 (12) Å3T = 298 K
Z = 18Parallelepiped, less
F(000) = 24120.30 × 0.25 × 0.20 mm
Data collection top
Bruker Kappa APEXII
diffractometer
2024 reflections with I > 2σ(I)
π and ω scansRint = 0.036
Absorption correction: multi-scan
(SADABS; Bruker, 2006)
θmax = 26.4°, θmin = 2.6°
Tmin = 0.68, Tmax = 0.74h = 3131
34372 measured reflectionsk = 3126
2814 independent reflectionsl = 1414
Refinement top
Refinement on F2Primary atom site location: iterative
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.066Hydrogen site location: mixed
wR(F2) = 0.229H atoms treated by a mixture of independent and constrained refinement
S = 1.07 w = 1/[σ2(Fo2) + (0.1155P)2 + 11.0098P]
where P = (Fo2 + 2Fc2)/3
2814 reflections(Δ/σ)max < 0.001
212 parametersΔρmax = 0.55 e Å3
159 restraintsΔρmin = 0.41 e Å3
Crystal data top
C15H20FNOZ = 18
Mr = 249.32Mo Kα radiation
Trigonal, R3:Hµ = 0.08 mm1
a = 25.119 (2) ÅT = 298 K
c = 11.2812 (12) Å0.30 × 0.25 × 0.20 mm
V = 6164.2 (12) Å3
Data collection top
Bruker Kappa APEXII
diffractometer
2814 independent reflections
Absorption correction: multi-scan
(SADABS; Bruker, 2006)
2024 reflections with I > 2σ(I)
Tmin = 0.68, Tmax = 0.74Rint = 0.036
34372 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.066159 restraints
wR(F2) = 0.229H atoms treated by a mixture of independent and constrained refinement
S = 1.07 w = 1/[σ2(Fo2) + (0.1155P)2 + 11.0098P]
where P = (Fo2 + 2Fc2)/3
2814 reflectionsΔρmax = 0.55 e Å3
212 parametersΔρmin = 0.41 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.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/UeqOcc. (<1)
N10.44770 (10)0.47721 (10)0.65896 (18)0.0460 (5)
F10.53114 (10)0.41476 (10)1.06076 (18)0.0891 (7)
C20.39810 (12)0.49241 (11)0.6739 (2)0.0480 (6)
C30.33455 (11)0.43494 (12)0.6811 (2)0.0494 (6)
H3A0.30410.44800.68320.059*
H3B0.32790.41160.60870.059*
H1N0.4810 (14)0.5102 (14)0.634 (3)0.062 (8)*
C40.32254 (10)0.39220 (11)0.7848 (2)0.0448 (6)
H40.32830.41480.85890.054*
H20.4062 (13)0.5176 (13)0.745 (3)0.054 (7)*
C50.36406 (11)0.36420 (11)0.7852 (2)0.0454 (6)
H5A0.34600.32850.83660.055*
H5B0.36530.35020.70570.055*
C60.45135 (13)0.39216 (12)0.9261 (2)0.0530 (6)
H60.42600.35660.96870.064*
C70.51085 (14)0.43021 (14)0.9618 (3)0.0616 (7)
O70.25956 (8)0.34478 (9)0.77523 (17)0.0593 (6)
H7O0.2424 (9)0.3368 (13)0.846 (3)0.089*
C80.54992 (14)0.48273 (15)0.9022 (3)0.0675 (8)
H80.59020.50760.92760.081*
C90.52822 (12)0.49807 (13)0.8031 (3)0.0566 (7)
H90.55420.53380.76160.068*
C10A0.39929 (15)0.53013 (13)0.5698 (3)0.0644 (11)0.483 (5)
H10A0.40250.51360.49810.077*0.483 (5)
C11A0.3970 (8)0.5805 (5)0.5554 (10)0.089 (3)0.483 (5)
H11A0.39900.60200.62410.107*0.483 (5)
C12A0.3909 (5)0.6096 (6)0.4329 (11)0.118 (3)0.483 (5)
H12A0.38700.64550.44930.141*0.483 (5)
H12B0.35420.57980.39120.141*0.483 (5)
C13A0.4515 (6)0.6295 (6)0.3498 (9)0.115 (3)0.483 (5)
H13A0.48990.65150.39320.138*0.483 (5)
H13B0.44970.59510.30700.138*0.483 (5)
C14A0.4386 (9)0.6712 (6)0.2717 (14)0.148 (5)0.483 (5)
H14A0.43900.66070.19000.222*0.483 (5)
H14B0.46970.71320.28480.222*0.483 (5)
H14C0.39900.66580.29120.222*0.483 (5)
C10B0.39929 (15)0.53013 (13)0.5698 (3)0.0644 (11)0.517 (5)
H10B0.39750.51620.49270.077*0.517 (5)
C11B0.4029 (7)0.5829 (4)0.5902 (8)0.078 (2)0.517 (5)
H11B0.40470.59580.66820.094*0.517 (5)
C12B0.4042 (4)0.6253 (4)0.4865 (7)0.096 (2)0.517 (5)
H12C0.43810.66670.49940.115*0.517 (5)
H12D0.36640.62700.48850.115*0.517 (5)
C13B0.4115 (6)0.6019 (5)0.3546 (8)0.112 (3)0.517 (5)
H13C0.44570.59430.35920.134*0.517 (5)
H13D0.37490.56240.34100.134*0.517 (5)
C14B0.4214 (8)0.6408 (6)0.2428 (13)0.150 (4)0.517 (5)
H14D0.41420.61590.17360.224*0.517 (5)
H14E0.46290.67460.24160.224*0.517 (5)
H14F0.39340.65630.24350.224*0.517 (5)
C5A0.42899 (11)0.40696 (11)0.8254 (2)0.0435 (6)
C9A0.46799 (11)0.46087 (11)0.7641 (2)0.0438 (6)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
N10.0457 (11)0.0416 (11)0.0437 (11)0.0167 (9)0.0038 (9)0.0029 (9)
F10.0927 (14)0.1043 (15)0.0805 (13)0.0569 (12)0.0324 (11)0.0035 (11)
C20.0540 (14)0.0443 (13)0.0463 (14)0.0251 (11)0.0033 (11)0.0000 (10)
C30.0476 (13)0.0537 (14)0.0480 (14)0.0262 (11)0.0002 (10)0.0032 (11)
C40.0407 (12)0.0495 (13)0.0398 (12)0.0192 (10)0.0006 (9)0.0003 (10)
C50.0478 (13)0.0412 (12)0.0418 (13)0.0181 (10)0.0012 (10)0.0027 (9)
C60.0587 (15)0.0557 (15)0.0513 (15)0.0337 (13)0.0018 (12)0.0029 (12)
C70.0658 (17)0.0717 (18)0.0590 (17)0.0430 (16)0.0138 (14)0.0040 (14)
O70.0418 (9)0.0710 (12)0.0495 (11)0.0166 (9)0.0016 (8)0.0092 (9)
C80.0541 (16)0.0657 (18)0.081 (2)0.0289 (14)0.0206 (15)0.0135 (16)
C90.0488 (14)0.0485 (14)0.0675 (18)0.0205 (11)0.0045 (12)0.0019 (12)
C10A0.069 (2)0.0536 (17)0.0644 (19)0.0259 (15)0.0082 (15)0.0126 (14)
C11A0.093 (4)0.084 (4)0.095 (5)0.047 (3)0.015 (4)0.024 (3)
C12A0.120 (4)0.103 (4)0.116 (5)0.045 (3)0.017 (4)0.013 (4)
C13A0.119 (5)0.110 (4)0.102 (4)0.046 (4)0.025 (4)0.022 (4)
C14A0.156 (8)0.126 (8)0.134 (8)0.049 (7)0.023 (6)0.024 (6)
C10B0.069 (2)0.0536 (17)0.0644 (19)0.0259 (15)0.0082 (15)0.0126 (14)
C11B0.083 (4)0.074 (3)0.078 (4)0.040 (3)0.015 (4)0.021 (3)
C12B0.113 (4)0.080 (3)0.092 (4)0.046 (3)0.035 (3)0.022 (3)
C13B0.120 (5)0.107 (4)0.087 (4)0.040 (4)0.013 (4)0.019 (4)
C14B0.175 (9)0.125 (8)0.137 (6)0.066 (7)0.002 (7)0.042 (6)
C5A0.0465 (12)0.0452 (12)0.0430 (12)0.0260 (10)0.0003 (10)0.0019 (10)
C9A0.0464 (13)0.0418 (12)0.0451 (13)0.0235 (10)0.0003 (10)0.0034 (10)
Geometric parameters (Å, º) top
N1—C9A1.430 (3)C7—C81.365 (5)
N1—C21.484 (3)C8—C91.380 (4)
F1—C71.361 (3)C9—C9A1.393 (4)
C2—C10A1.500 (4)C10A—C11A1.306 (5)
C2—C31.528 (4)C11A—C12A1.606 (10)
C3—C41.512 (3)C12A—C13A1.639 (11)
C4—O71.431 (3)C13A—C14A1.522 (11)
C4—C51.522 (3)C11B—C12B1.572 (8)
C5—C5A1.506 (3)C12B—C13B1.645 (10)
C6—C71.372 (4)C13B—C14B1.537 (10)
C6—C5A1.398 (4)C5A—C9A1.395 (3)
C9A—N1—C2116.44 (19)C8—C9—C9A121.1 (3)
N1—C2—C10A108.6 (2)C11A—C10A—C2135.5 (6)
N1—C2—C3112.2 (2)C10A—C11A—C12A127.5 (10)
C10A—C2—C3108.6 (2)C11A—C12A—C13A110.2 (10)
C4—C3—C2117.1 (2)C14A—C13A—C12A93.2 (11)
O7—C4—C3106.11 (19)C11B—C12B—C13B113.5 (7)
O7—C4—C5110.1 (2)C14B—C13B—C12B121.7 (10)
C3—C4—C5113.0 (2)C9A—C5A—C6118.7 (2)
C5A—C5—C4114.8 (2)C9A—C5A—C5121.8 (2)
C7—C6—C5A119.8 (3)C6—C5A—C5119.4 (2)
F1—C7—C8119.3 (3)C9—C9A—C5A119.6 (2)
F1—C7—C6118.4 (3)C9—C9A—N1119.5 (2)
C8—C7—C6122.3 (3)C5A—C9A—N1120.8 (2)
C7—C8—C9118.4 (3)
C9A—N1—C2—C10A158.9 (2)C10A—C11A—C12A—C13A63.7 (19)
C9A—N1—C2—C381.0 (3)C11A—C12A—C13A—C14A162.5 (10)
N1—C2—C3—C463.2 (3)C11B—C12B—C13B—C14B172.6 (12)
C10A—C2—C3—C4176.7 (2)C7—C6—C5A—C9A0.6 (4)
C2—C3—C4—O7176.5 (2)C7—C6—C5A—C5178.6 (2)
C2—C3—C4—C562.8 (3)C4—C5—C5A—C9A62.1 (3)
O7—C4—C5—C5A165.3 (2)C4—C5—C5A—C6118.6 (2)
C3—C4—C5—C5A76.3 (3)C8—C9—C9A—C5A0.5 (4)
C5A—C6—C7—F1179.5 (2)C8—C9—C9A—N1178.0 (3)
C5A—C6—C7—C80.2 (4)C6—C5A—C9A—C91.0 (4)
F1—C7—C8—C9179.1 (3)C5—C5A—C9A—C9178.3 (2)
C6—C7—C8—C90.7 (5)C6—C5A—C9A—N1178.5 (2)
C7—C8—C9—C9A0.3 (5)C5—C5A—C9A—N10.8 (3)
N1—C2—C10A—C11A133.6 (11)C2—N1—C9A—C9116.0 (3)
C3—C2—C10A—C11A104.1 (12)C2—N1—C9A—C5A66.5 (3)
C2—C10A—C11A—C12A172.1 (8)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N1—H1N···O7i0.88 (3)2.49 (3)3.356 (3)171 (3)
O7—H7O···N1ii0.882.022.889 (3)169
C9—H9···O7i0.932.633.451 (4)147
Symmetry codes: (i) xy+2/3, x+1/3, z+4/3; (ii) y+2/3, xy+1/3, z+1/3.
(Compound_5b) 7-Fluoro-cis-2-[(E)-pent-1-enyl]-2,3,4,5-tetrahydro-1H-1-benzazepin-4-ol top
Crystal data top
C15H20FNODx = 1.262 Mg m3
Mr = 249.32Mo Kα radiation, λ = 0.71073 Å
Trigonal, R3:HCell parameters from 9791 reflections
a = 49.395 (2) Åθ = 2.9–27.4°
c = 11.1802 (5) ŵ = 0.09 mm1
V = 23623 (2) Å3T = 100 K
Z = 72Parallelepiped, less
F(000) = 96480.30 × 0.25 × 0.20 mm
Data collection top
Bruker Kappa APEXII
diffractometer
8771 reflections with I > 2σ(I)
π and ω scansRint = 0.043
Absorption correction: multi-scan
(SADABS; Bruker, 2006)
θmax = 27.5°, θmin = 1.4°
Tmin = 0.89, Tmax = 0.98h = 6262
124259 measured reflectionsk = 6364
12035 independent reflectionsl = 1413
Refinement top
Refinement on F2459 restraints
Least-squares matrix: fullHydrogen site location: mixed
R[F2 > 2σ(F2)] = 0.046H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.122 w = 1/[σ2(Fo2) + (0.048P)2 + 28.8932P]
where P = (Fo2 + 2Fc2)/3
S = 1.02(Δ/σ)max = 0.001
12035 reflectionsΔρmax = 0.44 e Å3
786 parametersΔρmin = 0.28 e Å3
Crystal data top
C15H20FNOZ = 72
Mr = 249.32Mo Kα radiation
Trigonal, R3:Hµ = 0.09 mm1
a = 49.395 (2) ÅT = 100 K
c = 11.1802 (5) Å0.30 × 0.25 × 0.20 mm
V = 23623 (2) Å3
Data collection top
Bruker Kappa APEXII
diffractometer
12035 independent reflections
Absorption correction: multi-scan
(SADABS; Bruker, 2006)
8771 reflections with I > 2σ(I)
Tmin = 0.89, Tmax = 0.98Rint = 0.043
124259 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.046459 restraints
wR(F2) = 0.122H atoms treated by a mixture of independent and constrained refinement
S = 1.02 w = 1/[σ2(Fo2) + (0.048P)2 + 28.8932P]
where P = (Fo2 + 2Fc2)/3
12035 reflectionsΔρmax = 0.44 e Å3
786 parametersΔρmin = 0.28 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.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/UeqOcc. (<1)
N110.34466 (3)0.40532 (3)1.00064 (10)0.0169 (2)
F110.27312 (2)0.37140 (2)0.58610 (7)0.0270 (2)
C4110.29720 (4)0.59163 (4)0.57416 (16)0.0377 (4)0.319 (8)
H11C0.29860.60020.65160.045*0.319 (8)
C4120.2953 (3)0.6093 (3)0.4671 (7)0.0305 (11)0.319 (8)
H12E0.28120.61740.48850.037*0.319 (8)
H12F0.31630.62760.45440.037*0.319 (8)
C4130.2844 (2)0.59265 (19)0.3497 (7)0.0308 (13)0.319 (8)
H13E0.26410.57320.36050.037*0.319 (8)
H13F0.29970.58700.31960.037*0.319 (8)
C4140.28076 (17)0.61383 (14)0.2595 (6)0.0300 (14)0.319 (8)
H14G0.27150.60210.18570.045*0.319 (8)
H14H0.30130.63190.24190.045*0.319 (8)
H14I0.26720.62110.29310.045*0.319 (8)
C4150.29720 (4)0.59163 (4)0.57416 (16)0.0377 (4)0.341 (3)
H150.29210.59360.65450.045*0.341 (3)
C4160.30233 (12)0.62061 (12)0.5067 (5)0.0299 (9)0.341 (3)
H16A0.28480.62450.52040.036*0.341 (3)
H16B0.32200.63930.53230.036*0.341 (3)
C4170.30403 (10)0.61315 (11)0.3761 (4)0.0273 (9)0.341 (3)
H17A0.31900.60540.36760.033*0.341 (3)
H17B0.31200.63250.32830.033*0.341 (3)
C4180.27235 (13)0.58869 (13)0.3269 (5)0.0323 (12)0.341 (3)
H18A0.27440.58540.24160.048*0.341 (3)
H18B0.25730.59590.33740.048*0.341 (3)
H18C0.26500.56900.37000.048*0.341 (3)
C4190.29720 (4)0.59163 (4)0.57416 (16)0.0377 (4)0.340 (8)
H19A0.29810.60110.64920.045*0.340 (8)
C4200.2958 (3)0.6069 (2)0.4514 (7)0.0306 (11)0.340 (8)
H20A0.27840.61120.45800.037*0.340 (8)
H20B0.31530.62740.44630.037*0.340 (8)
C4210.29209 (17)0.59085 (15)0.3319 (6)0.0289 (11)0.340 (8)
H21A0.27250.57040.33290.035*0.340 (8)
H21B0.30970.58700.32040.035*0.340 (8)
C4220.29106 (17)0.61025 (12)0.2260 (6)0.0293 (14)0.340 (8)
H22A0.28900.59910.15110.044*0.340 (8)
H22B0.31040.63060.22440.044*0.340 (8)
H22C0.27310.61340.23520.044*0.340 (8)
C4100.29701 (4)0.56496 (4)0.56497 (14)0.0307 (4)
C49A0.26156 (3)0.49464 (3)0.76169 (12)0.0185 (3)
C490.23086 (3)0.48294 (3)0.80082 (13)0.0224 (3)
H9C0.21750.48830.75850.027*
C480.21945 (3)0.46363 (3)0.90032 (14)0.0254 (3)
H8C0.19850.45550.92610.030*
H2O0.2841 (4)0.4991 (5)0.5109 (18)0.050 (6)*
C470.23945 (3)0.45664 (3)0.96036 (13)0.0240 (3)
H3O0.3292 (4)0.4518 (4)0.1705 (17)0.041 (5)*
C460.26982 (3)0.46764 (3)0.92451 (12)0.0205 (3)
H6C0.28290.46220.96830.025*
H1O0.3815 (4)0.3372 (4)0.8117 (17)0.043 (5)*
C45A0.28138 (3)0.48676 (3)0.82365 (12)0.0178 (3)
H4O0.3758 (4)0.5448 (4)0.8477 (18)0.044 (5)*
C450.31449 (3)0.49801 (3)0.78342 (12)0.0175 (3)
H5CA0.31390.49010.70160.021*
H5CB0.32380.48890.83670.021*
C440.33575 (3)0.53372 (3)0.78294 (12)0.0178 (3)
H4C0.33240.54250.85850.021*
H2N0.3134 (4)0.4083 (4)0.2895 (14)0.026 (4)*
C430.32988 (3)0.54921 (3)0.67663 (12)0.0195 (3)
H3CA0.33290.54010.60260.023*
H3CB0.34590.57170.67720.023*
H1N0.3431 (3)0.4215 (4)1.0311 (14)0.023 (4)*
C420.29770 (3)0.54646 (3)0.67063 (12)0.0197 (3)
H2C0.29410.55530.74550.024*
H10C0.2965 (4)0.5564 (4)0.4860 (17)0.045 (5)*
H3N0.4201 (4)0.5736 (4)0.0348 (14)0.027 (4)*
H4N0.2554 (4)0.5138 (4)0.6247 (14)0.024 (4)*
O110.37855 (2)0.34202 (2)0.88342 (9)0.0209 (2)
N210.31433 (3)0.42554 (3)0.31909 (10)0.0169 (2)
F210.39145 (2)0.45825 (2)0.71821 (7)0.0300 (2)
O210.28801 (2)0.49469 (2)0.43828 (9)0.0223 (2)
C220.28152 (3)0.41842 (3)0.34093 (11)0.0173 (3)
H2B0.27410.40720.41910.021*
C120.37836 (3)0.41447 (3)0.99245 (12)0.0174 (3)
H2A0.38790.42830.92120.021*
N310.40300 (3)0.55637 (3)0.00756 (10)0.0185 (2)
F310.37125 (2)0.59685 (2)0.40456 (8)0.0333 (2)
O310.33407 (2)0.45989 (2)0.09972 (9)0.0210 (2)
N410.27191 (3)0.51345 (3)0.65589 (10)0.0193 (2)
F410.22883 (2)0.43795 (2)1.05925 (8)0.0328 (2)
O410.36780 (2)0.54157 (2)0.77562 (9)0.0221 (2)
C230.27900 (3)0.44792 (3)0.34420 (12)0.0187 (3)
H3BA0.28770.45950.26860.022*
H3BB0.25660.44160.34670.022*
C130.38308 (3)0.38618 (3)0.98311 (12)0.0181 (3)
H3A0.40580.39390.98260.022*
H3B0.37440.37341.05640.022*
C320.40991 (3)0.53030 (3)0.00136 (12)0.0186 (3)
H2D0.42230.53300.07580.022*
C240.29539 (3)0.47014 (3)0.44786 (12)0.0185 (3)
H4B0.28690.45870.52490.022*
C140.36875 (3)0.36484 (3)0.87580 (11)0.0175 (3)
H140.37730.37730.80080.021*
C330.38020 (3)0.49827 (3)0.00420 (12)0.0181 (3)
H3DA0.36810.49600.06950.022*
H3DB0.38640.48200.00190.022*
C340.35875 (3)0.49174 (3)0.11100 (12)0.0180 (3)
H4D0.37070.49410.18630.022*
C250.33097 (3)0.48406 (3)0.44610 (12)0.0184 (3)
H5BA0.33860.49120.36380.022*
H5BB0.34060.50260.49880.022*
C150.33288 (3)0.34862 (3)0.87380 (12)0.0176 (3)
H15A0.32470.33000.82150.021*
H15B0.32490.34130.95560.021*
C350.34482 (3)0.51345 (3)0.11627 (12)0.0183 (3)
H5DA0.33770.51500.03510.022*
H5DB0.32620.50380.16880.022*
C35A0.36701 (3)0.54597 (3)0.16138 (12)0.0187 (3)
C25A0.34204 (3)0.46199 (3)0.48536 (11)0.0176 (3)
C15A0.32065 (3)0.36931 (3)0.83032 (11)0.0166 (3)
C160.30230 (3)0.36121 (3)0.72687 (11)0.0185 (3)
H6A0.29760.34270.68430.022*
C170.29108 (3)0.38009 (3)0.68695 (12)0.0204 (3)
C360.35949 (3)0.55690 (3)0.26442 (12)0.0216 (3)
H6D0.34070.54370.30670.026*
C260.36144 (3)0.46957 (3)0.58553 (12)0.0205 (3)
H6B0.36710.48810.62940.025*
C180.29731 (3)0.40719 (3)0.74472 (12)0.0218 (3)
H8A0.28930.41990.71540.026*
C370.37940 (3)0.58679 (4)0.30412 (13)0.0253 (3)
C270.37238 (3)0.45005 (3)0.62031 (12)0.0224 (3)
C190.31558 (3)0.41541 (3)0.84723 (12)0.0199 (3)
H9A0.32020.43410.88840.024*
C380.40681 (3)0.60682 (3)0.24662 (13)0.0269 (3)
H8D0.42010.62740.27570.032*
C280.36511 (3)0.42299 (3)0.56027 (12)0.0219 (3)
H8B0.37320.41010.58550.026*
C19A0.32728 (3)0.39686 (3)0.89089 (11)0.0168 (3)
C390.41454 (3)0.59611 (3)0.14481 (13)0.0235 (3)
H9D0.43350.60950.10400.028*
C290.34556 (3)0.41512 (3)0.46162 (12)0.0199 (3)
H9B0.34000.39640.41930.024*
C1100.39442 (3)0.43229 (3)1.10426 (12)0.0183 (3)
H10A0.38480.42361.17900.022*
C29A0.33387 (3)0.43422 (3)0.42330 (11)0.0169 (3)
C1110.42101 (3)0.45923 (3)1.10490 (12)0.0207 (3)
H11A0.42970.46811.02920.025*
C39A0.39492 (3)0.56594 (3)0.10127 (12)0.0188 (3)
C2100.26079 (3)0.39767 (3)0.24270 (12)0.0188 (3)
H10B0.26580.40470.16240.023*
C1120.43889 (3)0.47726 (3)1.21326 (12)0.0240 (3)
H12A0.44280.49891.20610.029*
H12B0.45950.47841.21300.029*
C2110.23589 (3)0.37001 (3)0.26272 (12)0.0201 (3)
H11B0.23290.36280.34300.024*
C1130.42333 (3)0.46421 (3)1.33300 (12)0.0259 (3)
H13A0.41980.44281.34260.031*
H13B0.40270.46301.33470.031*
C2120.21183 (3)0.34868 (3)0.17418 (12)0.0226 (3)
H12C0.19180.34760.19370.027*
H12D0.20870.32740.18510.027*
C1140.44315 (4)0.48443 (4)1.43649 (13)0.0292 (3)
H14A0.43250.47521.51230.044*
H14B0.44620.50551.42850.044*
H14C0.46350.48561.43540.044*
C3100.42927 (3)0.53233 (3)0.10552 (13)0.0246 (3)0.841 (2)
H10D0.42210.53360.18310.029*0.841 (2)
C3110.45638 (4)0.53238 (5)0.09460 (18)0.0219 (4)0.841 (2)
H11D0.46270.53060.01610.026*0.841 (2)
C3120.47778 (4)0.53507 (4)0.19651 (14)0.0243 (4)0.841 (2)
H12G0.49960.54960.17170.029*0.841 (2)
H12H0.47580.51430.20890.029*0.841 (2)
C3130.47219 (4)0.54616 (4)0.31500 (14)0.0263 (4)0.841 (2)
H13G0.47300.56640.30360.032*0.841 (2)
H13H0.45110.53090.34480.032*0.841 (2)
C3140.49656 (6)0.55001 (8)0.4072 (2)0.0279 (6)0.841 (2)
H14J0.49350.55900.48060.042*0.841 (2)
H14K0.49430.52960.42490.042*0.841 (2)
H14L0.51750.56400.37530.042*0.841 (2)
C3150.42927 (3)0.53233 (3)0.10552 (13)0.0246 (3)0.159 (2)
H15C0.42330.53960.17370.029*0.159 (2)
C3160.4522 (2)0.5269 (3)0.1319 (8)0.0275 (17)0.159 (2)
H16C0.46320.52340.06960.033*0.159 (2)
C3170.46092 (17)0.5261 (2)0.2607 (7)0.0246 (13)0.159 (2)
H17C0.44780.53080.31440.030*0.159 (2)
H17D0.45760.50510.28100.030*0.159 (2)
C3180.49498 (18)0.5505 (2)0.2755 (8)0.0315 (16)0.159 (2)
H18D0.50770.54690.21570.038*0.159 (2)
H18E0.49780.57150.26170.038*0.159 (2)
C3190.5060 (4)0.5487 (5)0.4001 (9)0.032 (3)0.159 (2)
H19D0.50440.52830.41160.049*0.159 (2)
H19E0.52770.56530.41020.049*0.159 (2)
H19F0.49280.55140.45920.049*0.159 (2)
C2140.24464 (4)0.35197 (4)0.00572 (13)0.0307 (4)
H14D0.24780.35730.09090.046*
H14E0.23850.32990.00480.046*
H14F0.26410.36520.03800.046*
C2130.21896 (3)0.35743 (3)0.04241 (13)0.0248 (3)
H13C0.19970.34490.00500.030*
H13D0.22540.37980.03220.030*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
N110.0186 (6)0.0182 (6)0.0144 (5)0.0096 (5)0.0010 (4)0.0021 (4)
F110.0271 (4)0.0340 (5)0.0193 (4)0.0148 (4)0.0085 (3)0.0012 (4)
C4110.0301 (7)0.0378 (7)0.0467 (8)0.0181 (6)0.0053 (6)0.0203 (6)
C4120.0296 (15)0.0302 (15)0.0358 (15)0.0181 (13)0.0027 (14)0.0090 (13)
C4130.030 (2)0.0295 (17)0.0336 (17)0.0154 (15)0.0001 (17)0.0063 (15)
C4140.030 (3)0.036 (2)0.027 (2)0.018 (2)0.002 (2)0.0070 (19)
C4150.0301 (7)0.0378 (7)0.0467 (8)0.0181 (6)0.0053 (6)0.0203 (6)
C4160.0289 (15)0.0305 (15)0.0327 (15)0.0167 (12)0.0035 (13)0.0080 (13)
C4170.0280 (15)0.0272 (15)0.0289 (15)0.0155 (12)0.0036 (13)0.0020 (13)
C4180.031 (2)0.035 (2)0.032 (2)0.0180 (19)0.0005 (19)0.0049 (17)
C4190.0301 (7)0.0378 (7)0.0467 (8)0.0181 (6)0.0053 (6)0.0203 (6)
C4200.0308 (15)0.0290 (15)0.0352 (15)0.0174 (12)0.0023 (14)0.0081 (13)
C4210.0294 (18)0.0279 (16)0.0314 (16)0.0158 (14)0.0002 (15)0.0069 (14)
C4220.032 (3)0.027 (2)0.028 (2)0.0147 (18)0.001 (2)0.0059 (18)
C4100.0285 (8)0.0486 (10)0.0239 (8)0.0259 (8)0.0086 (6)0.0161 (7)
C49A0.0208 (7)0.0175 (7)0.0174 (7)0.0096 (6)0.0010 (5)0.0049 (5)
C490.0203 (7)0.0235 (7)0.0254 (7)0.0123 (6)0.0017 (6)0.0039 (6)
C480.0193 (7)0.0215 (7)0.0328 (8)0.0082 (6)0.0059 (6)0.0010 (6)
C470.0274 (8)0.0181 (7)0.0234 (7)0.0091 (6)0.0057 (6)0.0023 (6)
C460.0224 (7)0.0174 (7)0.0213 (7)0.0096 (6)0.0011 (6)0.0020 (5)
C45A0.0184 (7)0.0154 (6)0.0181 (7)0.0072 (5)0.0016 (5)0.0046 (5)
C450.0187 (7)0.0186 (7)0.0164 (6)0.0102 (6)0.0013 (5)0.0018 (5)
C440.0179 (7)0.0194 (7)0.0148 (6)0.0082 (6)0.0011 (5)0.0005 (5)
C430.0213 (7)0.0196 (7)0.0166 (7)0.0095 (6)0.0015 (5)0.0008 (5)
C420.0249 (7)0.0222 (7)0.0151 (6)0.0141 (6)0.0015 (5)0.0019 (5)
O110.0280 (5)0.0257 (5)0.0157 (5)0.0184 (5)0.0018 (4)0.0022 (4)
N210.0177 (6)0.0181 (6)0.0151 (5)0.0090 (5)0.0021 (4)0.0037 (5)
F210.0293 (5)0.0378 (5)0.0230 (4)0.0168 (4)0.0125 (4)0.0041 (4)
O210.0270 (5)0.0275 (5)0.0181 (5)0.0178 (5)0.0031 (4)0.0062 (4)
C220.0164 (6)0.0189 (7)0.0143 (6)0.0071 (5)0.0000 (5)0.0008 (5)
C120.0161 (6)0.0172 (7)0.0156 (6)0.0058 (5)0.0000 (5)0.0011 (5)
N310.0185 (6)0.0178 (6)0.0163 (6)0.0069 (5)0.0011 (5)0.0011 (5)
F310.0363 (5)0.0374 (5)0.0286 (5)0.0202 (4)0.0018 (4)0.0149 (4)
O310.0231 (5)0.0174 (5)0.0166 (5)0.0056 (4)0.0019 (4)0.0003 (4)
N410.0193 (6)0.0261 (6)0.0153 (6)0.0134 (5)0.0032 (5)0.0024 (5)
F410.0324 (5)0.0291 (5)0.0334 (5)0.0127 (4)0.0128 (4)0.0121 (4)
O410.0174 (5)0.0274 (5)0.0176 (5)0.0084 (4)0.0026 (4)0.0032 (4)
C230.0163 (7)0.0215 (7)0.0172 (7)0.0087 (6)0.0010 (5)0.0026 (5)
C130.0173 (7)0.0201 (7)0.0164 (6)0.0089 (6)0.0009 (5)0.0011 (5)
C320.0175 (7)0.0214 (7)0.0160 (6)0.0091 (6)0.0005 (5)0.0008 (5)
C240.0202 (7)0.0222 (7)0.0148 (6)0.0119 (6)0.0010 (5)0.0020 (5)
C140.0212 (7)0.0203 (7)0.0139 (6)0.0126 (6)0.0002 (5)0.0006 (5)
C330.0195 (7)0.0192 (7)0.0160 (6)0.0099 (6)0.0006 (5)0.0000 (5)
C340.0176 (7)0.0176 (7)0.0156 (6)0.0064 (6)0.0012 (5)0.0004 (5)
C250.0203 (7)0.0186 (7)0.0157 (6)0.0091 (6)0.0015 (5)0.0032 (5)
C150.0200 (7)0.0178 (7)0.0144 (6)0.0091 (6)0.0002 (5)0.0009 (5)
C350.0161 (6)0.0205 (7)0.0163 (6)0.0077 (6)0.0002 (5)0.0002 (5)
C35A0.0195 (7)0.0209 (7)0.0176 (7)0.0115 (6)0.0039 (5)0.0004 (5)
C25A0.0146 (6)0.0202 (7)0.0158 (6)0.0070 (5)0.0019 (5)0.0002 (5)
C15A0.0151 (6)0.0190 (7)0.0141 (6)0.0072 (5)0.0023 (5)0.0011 (5)
C160.0172 (7)0.0200 (7)0.0159 (6)0.0076 (6)0.0011 (5)0.0011 (5)
C170.0159 (7)0.0275 (7)0.0140 (6)0.0079 (6)0.0019 (5)0.0016 (6)
C360.0208 (7)0.0249 (7)0.0206 (7)0.0126 (6)0.0010 (6)0.0006 (6)
C260.0176 (7)0.0217 (7)0.0177 (7)0.0065 (6)0.0001 (5)0.0019 (5)
C180.0196 (7)0.0240 (7)0.0235 (7)0.0122 (6)0.0009 (6)0.0056 (6)
C370.0292 (8)0.0308 (8)0.0211 (7)0.0190 (7)0.0041 (6)0.0081 (6)
C270.0180 (7)0.0292 (8)0.0163 (7)0.0091 (6)0.0035 (5)0.0004 (6)
C190.0200 (7)0.0194 (7)0.0191 (7)0.0089 (6)0.0002 (5)0.0013 (5)
C380.0246 (8)0.0242 (8)0.0305 (8)0.0112 (6)0.0068 (6)0.0090 (6)
C280.0190 (7)0.0247 (7)0.0226 (7)0.0114 (6)0.0008 (6)0.0033 (6)
C19A0.0148 (6)0.0182 (7)0.0150 (6)0.0064 (5)0.0018 (5)0.0014 (5)
C390.0205 (7)0.0229 (7)0.0242 (7)0.0088 (6)0.0035 (6)0.0025 (6)
C290.0184 (7)0.0197 (7)0.0199 (7)0.0083 (6)0.0010 (5)0.0003 (5)
C1100.0214 (7)0.0192 (7)0.0148 (6)0.0105 (6)0.0005 (5)0.0004 (5)
C29A0.0136 (6)0.0191 (7)0.0142 (6)0.0054 (5)0.0016 (5)0.0010 (5)
C1110.0221 (7)0.0214 (7)0.0180 (7)0.0103 (6)0.0011 (5)0.0006 (5)
C39A0.0192 (7)0.0219 (7)0.0169 (7)0.0114 (6)0.0030 (5)0.0008 (5)
C2100.0212 (7)0.0204 (7)0.0156 (6)0.0110 (6)0.0032 (5)0.0024 (5)
C1120.0204 (7)0.0221 (7)0.0231 (7)0.0059 (6)0.0020 (6)0.0026 (6)
C2110.0219 (7)0.0221 (7)0.0176 (7)0.0120 (6)0.0007 (5)0.0007 (5)
C1130.0238 (7)0.0252 (8)0.0212 (7)0.0066 (6)0.0022 (6)0.0027 (6)
C2120.0188 (7)0.0223 (7)0.0242 (7)0.0084 (6)0.0034 (6)0.0036 (6)
C1140.0281 (8)0.0312 (8)0.0231 (8)0.0110 (7)0.0040 (6)0.0048 (6)
C3100.0286 (8)0.0210 (7)0.0206 (7)0.0098 (6)0.0049 (6)0.0006 (6)
C3110.0266 (9)0.0180 (10)0.0206 (9)0.0109 (8)0.0057 (7)0.0001 (8)
C3120.0243 (9)0.0282 (9)0.0239 (9)0.0158 (7)0.0041 (7)0.0039 (7)
C3130.0289 (9)0.0337 (10)0.0203 (8)0.0186 (8)0.0023 (7)0.0009 (7)
C3140.0274 (14)0.0324 (11)0.0222 (10)0.0137 (11)0.0009 (9)0.0014 (8)
C3150.0286 (8)0.0210 (7)0.0206 (7)0.0098 (6)0.0049 (6)0.0006 (6)
C3160.034 (2)0.022 (2)0.025 (2)0.0130 (17)0.0087 (19)0.004 (2)
C3170.028 (2)0.026 (2)0.021 (2)0.0145 (19)0.0042 (19)0.000 (2)
C3180.030 (2)0.033 (2)0.022 (2)0.009 (2)0.005 (2)0.003 (2)
C3190.032 (5)0.036 (5)0.019 (4)0.010 (5)0.009 (4)0.001 (4)
C2140.0352 (9)0.0323 (9)0.0230 (8)0.0157 (7)0.0017 (7)0.0036 (6)
C2130.0287 (8)0.0226 (7)0.0222 (7)0.0120 (6)0.0084 (6)0.0048 (6)
Geometric parameters (Å, º) top
N11—C19A1.4347 (16)C32—C331.5283 (18)
N11—C121.4938 (17)C24—C251.5342 (18)
F11—C171.3646 (15)C14—C151.5370 (18)
C411—C4101.317 (2)C33—C341.5201 (18)
C411—C4121.511 (9)C34—C351.5378 (18)
C412—C4131.497 (10)C25—C25A1.5084 (18)
C413—C4141.527 (8)C15—C15A1.5041 (18)
C416—C4171.518 (6)C35—C35A1.5085 (18)
C417—C4181.523 (6)C35A—C361.3989 (19)
C420—C4211.515 (8)C35A—C39A1.4016 (19)
C421—C4221.540 (7)C25A—C261.3980 (18)
C410—C421.5042 (19)C25A—C29A1.4045 (19)
C49A—C491.3956 (19)C15A—C161.3989 (18)
C49A—C45A1.4040 (19)C15A—C19A1.4044 (18)
C49A—N411.4313 (17)C16—C171.3757 (19)
C49—C481.388 (2)C17—C181.375 (2)
C48—C471.374 (2)C36—C371.376 (2)
C47—F411.3660 (16)C26—C271.376 (2)
C47—C461.375 (2)C18—C191.3881 (19)
C46—C45A1.3964 (19)C37—C381.373 (2)
C45A—C451.5091 (18)C27—C281.373 (2)
C45—C441.5368 (18)C19—C19A1.3934 (19)
C44—O411.4320 (16)C38—C391.387 (2)
C44—C431.5176 (18)C28—C291.3873 (19)
C43—C421.5276 (19)C39—C39A1.3973 (19)
C42—N411.4940 (18)C29—C29A1.3972 (19)
O11—C141.4340 (15)C110—C1111.3219 (19)
N21—C29A1.4347 (16)C111—C1121.5015 (19)
N21—C221.4970 (17)C210—C2111.3227 (19)
F21—C271.3666 (15)C112—C1131.518 (2)
O21—C241.4342 (16)C211—C2121.4999 (19)
C22—C2101.5016 (18)C113—C1141.5222 (19)
C22—C231.5240 (18)C212—C2131.526 (2)
C12—C1101.5063 (18)C310—C3111.343 (2)
C12—C131.5305 (18)C311—C3121.514 (2)
N31—C39A1.4323 (17)C312—C3131.511 (2)
N31—C321.4917 (17)C313—C3141.523 (2)
F31—C371.3674 (16)C316—C3171.509 (4)
O31—C341.4350 (16)C317—C3181.510 (4)
C23—C241.5213 (18)C318—C3191.512 (4)
C13—C141.5184 (18)C214—C2131.521 (2)
C32—C3101.5024 (19)
C19A—N11—C12116.72 (10)C15A—C15—C14113.62 (11)
C410—C411—C412122.9 (5)C35A—C35—C34114.54 (11)
C413—C412—C411119.1 (8)C36—C35A—C39A118.74 (12)
C412—C413—C414109.6 (7)C36—C35A—C35119.63 (12)
C416—C417—C418112.3 (4)C39A—C35A—C35121.62 (12)
C420—C421—C422112.7 (6)C26—C25A—C29A118.75 (12)
C411—C410—C42123.74 (16)C26—C25A—C25119.16 (12)
C49—C49A—C45A119.63 (13)C29A—C25A—C25122.08 (12)
C49—C49A—N41119.29 (12)C16—C15A—C19A118.67 (12)
C45A—C49A—N41121.02 (12)C16—C15A—C15119.72 (12)
C48—C49—C49A121.30 (13)C19A—C15A—C15121.60 (11)
C47—C48—C49117.91 (13)C17—C16—C15A119.82 (12)
F41—C47—C48118.94 (13)F11—C17—C18119.20 (12)
F41—C47—C46118.51 (13)F11—C17—C16118.28 (12)
C48—C47—C46122.54 (13)C18—C17—C16122.52 (12)
C47—C46—C45A119.92 (13)C37—C36—C35A119.64 (13)
C46—C45A—C49A118.69 (12)C27—C26—C25A119.71 (13)
C46—C45A—C45119.41 (12)C17—C18—C19117.96 (13)
C49A—C45A—C45121.90 (12)F31—C37—C38119.07 (13)
C45A—C45—C44114.61 (11)F31—C37—C36118.20 (13)
O41—C44—C43106.43 (10)C38—C37—C36122.72 (13)
O41—C44—C45109.82 (10)F21—C27—C28119.07 (12)
C43—C44—C45112.84 (11)F21—C27—C26118.20 (12)
C44—C43—C42116.23 (11)C28—C27—C26122.72 (13)
N41—C42—C410108.08 (12)C18—C19—C19A121.31 (13)
N41—C42—C43112.55 (11)C37—C38—C39118.00 (13)
C410—C42—C43108.60 (11)C27—C28—C29117.90 (13)
C29A—N21—C22115.16 (10)C19—C19A—C15A119.72 (12)
N21—C22—C210109.25 (10)C19—C19A—N11119.51 (12)
N21—C22—C23112.08 (11)C15A—C19A—N11120.70 (12)
C210—C22—C23108.45 (11)C38—C39—C39A121.09 (14)
N11—C12—C110107.90 (10)C28—C29—C29A121.29 (13)
N11—C12—C13112.54 (11)C111—C110—C12124.10 (12)
C110—C12—C13108.31 (10)C29—C29A—C25A119.61 (12)
C39A—N31—C32116.73 (10)C29—C29A—N21119.36 (12)
C49A—N41—C42116.76 (10)C25A—C29A—N21121.00 (12)
C24—C23—C22116.08 (11)C110—C111—C112126.52 (13)
C14—C13—C12117.19 (11)C39—C39A—C35A119.80 (13)
N31—C32—C310107.59 (11)C39—C39A—N31119.25 (12)
N31—C32—C33112.30 (11)C35A—C39A—N31120.89 (12)
C310—C32—C33109.59 (11)C211—C210—C22123.08 (12)
O21—C24—C23106.52 (10)C111—C112—C113115.91 (12)
O21—C24—C25109.80 (11)C210—C211—C212127.95 (13)
C23—C24—C25113.00 (11)C112—C113—C114111.64 (12)
O11—C14—C13105.99 (10)C211—C212—C213116.65 (12)
O11—C14—C15110.20 (10)C311—C310—C32121.91 (14)
C13—C14—C15112.89 (11)C310—C311—C312125.68 (17)
C34—C33—C32116.27 (11)C313—C312—C311116.45 (15)
O31—C34—C33106.46 (10)C312—C313—C314111.25 (16)
O31—C34—C35109.70 (10)C316—C317—C318107.7 (7)
C33—C34—C35112.93 (11)C317—C318—C319110.1 (9)
C25A—C25—C24114.85 (11)C214—C213—C212112.71 (12)
C410—C411—C412—C41316.5 (14)C15—C15A—C16—C17180.00 (12)
C411—C412—C413—C414173.5 (8)C15A—C16—C17—F11179.65 (11)
C412—C411—C410—C42177.6 (7)C15A—C16—C17—C180.4 (2)
C45A—C49A—C49—C480.1 (2)C39A—C35A—C36—C370.2 (2)
N41—C49A—C49—C48177.53 (12)C35—C35A—C36—C37178.61 (13)
C49A—C49—C48—C470.8 (2)C29A—C25A—C26—C270.76 (19)
C49—C48—C47—F41179.33 (12)C25—C25A—C26—C27178.24 (12)
C49—C48—C47—C460.9 (2)F11—C17—C18—C19179.85 (12)
F41—C47—C46—C45A179.89 (12)C16—C17—C18—C190.2 (2)
C48—C47—C46—C45A0.2 (2)C35A—C36—C37—F31179.48 (12)
C47—C46—C45A—C49A0.78 (19)C35A—C36—C37—C380.0 (2)
C47—C46—C45A—C45178.47 (12)C25A—C26—C27—F21179.64 (12)
C49—C49A—C45A—C460.91 (19)C25A—C26—C27—C280.1 (2)
N41—C49A—C45A—C46178.27 (12)C17—C18—C19—C19A0.1 (2)
C49—C49A—C45A—C45178.32 (12)F31—C37—C38—C39179.87 (12)
N41—C49A—C45A—C450.96 (19)C36—C37—C38—C390.4 (2)
C46—C45A—C45—C44119.35 (13)F21—C27—C28—C29179.62 (12)
C49A—C45A—C45—C4461.43 (16)C26—C27—C28—C290.9 (2)
C45A—C45—C44—O41164.37 (11)C18—C19—C19A—C15A0.2 (2)
C45A—C45—C44—C4377.07 (14)C18—C19—C19A—N11176.67 (12)
O41—C44—C43—C42175.04 (11)C16—C15A—C19A—C190.00 (19)
C45—C44—C43—C4264.44 (15)C15—C15A—C19A—C19179.73 (12)
C411—C410—C42—N41129.58 (16)C16—C15A—C19A—N11176.83 (11)
C411—C410—C42—C43108.04 (17)C15—C15A—C19A—N113.44 (19)
C44—C43—C42—N4164.28 (15)C12—N11—C19A—C19114.64 (13)
C44—C43—C42—C410176.10 (12)C12—N11—C19A—C15A68.53 (16)
C29A—N21—C22—C210156.69 (11)C37—C38—C39—C39A0.6 (2)
C29A—N21—C22—C2383.09 (13)C27—C28—C29—C29A0.7 (2)
C19A—N11—C12—C110161.36 (11)N11—C12—C110—C111132.05 (14)
C19A—N11—C12—C1379.20 (14)C13—C12—C110—C111105.86 (15)
C49—C49A—N41—C42117.04 (14)C28—C29—C29A—C25A0.1 (2)
C45A—C49A—N41—C4265.59 (16)C28—C29—C29A—N21178.50 (12)
C410—C42—N41—C49A159.36 (12)C26—C25A—C29A—C290.89 (19)
C43—C42—N41—C49A80.71 (14)C25—C25A—C29A—C29178.08 (12)
N21—C22—C23—C2466.36 (14)C26—C25A—C29A—N21179.22 (12)
C210—C22—C23—C24172.95 (11)C25—C25A—C29A—N210.25 (19)
N11—C12—C13—C1460.97 (15)C22—N21—C29A—C29116.14 (13)
C110—C12—C13—C14179.82 (11)C22—N21—C29A—C25A65.52 (16)
C39A—N31—C32—C310158.27 (11)C12—C110—C111—C112176.79 (13)
C39A—N31—C32—C3381.05 (14)C38—C39—C39A—C35A0.4 (2)
C22—C23—C24—O21175.67 (11)C38—C39—C39A—N31176.81 (13)
C22—C23—C24—C2563.68 (15)C36—C35A—C39A—C390.0 (2)
C12—C13—C14—O11175.57 (11)C35—C35A—C39A—C39178.78 (12)
C12—C13—C14—C1563.70 (15)C36—C35A—C39A—N31177.17 (12)
N31—C32—C33—C3463.64 (15)C35—C35A—C39A—N311.64 (19)
C310—C32—C33—C34176.84 (12)C32—N31—C39A—C39116.01 (14)
C32—C33—C34—O31175.46 (11)C32—N31—C39A—C35A66.84 (16)
C32—C33—C34—C3564.10 (15)N21—C22—C210—C211122.85 (14)
O21—C24—C25—C25A165.75 (10)C23—C22—C210—C211114.73 (14)
C23—C24—C25—C25A75.49 (14)C110—C111—C112—C1135.0 (2)
O11—C14—C15—C15A163.06 (10)C22—C210—C211—C212173.60 (13)
C13—C14—C15—C15A78.65 (14)C111—C112—C113—C114179.24 (13)
O31—C34—C35—C35A164.07 (11)C210—C211—C212—C2139.3 (2)
C33—C34—C35—C35A77.36 (14)N31—C32—C310—C311128.42 (16)
C34—C35—C35A—C36119.81 (13)C33—C32—C310—C311109.21 (17)
C34—C35—C35A—C39A61.39 (17)C32—C310—C311—C312178.55 (15)
C24—C25—C25A—C26118.94 (13)C310—C311—C312—C31315.3 (3)
C24—C25—C25A—C29A62.09 (16)C311—C312—C313—C314176.05 (19)
C14—C15—C15A—C16118.18 (13)C316—C317—C318—C319174.7 (10)
C14—C15—C15A—C19A61.55 (16)C211—C212—C213—C21472.12 (16)
C19A—C15A—C16—C170.27 (19)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N11—H1N···O31i0.906 (16)2.287 (16)3.1897 (15)173.9 (13)
N21—H2N···O11ii0.895 (16)2.370 (17)3.2455 (15)165.8 (13)
N31—H3N···O21iii0.901 (17)2.326 (17)3.2208 (15)172.2 (14)
N41—H4N···O41iv0.893 (16)2.310 (16)3.1952 (15)170.9 (14)
O11—H1O···N11v0.869 (19)2.00 (2)2.8553 (15)166.1 (17)
O21—H2O···N410.89 (2)1.98 (2)2.8542 (15)168.6 (18)
O31—H3O···N210.864 (19)2.008 (19)2.8619 (15)169.5 (17)
O41—H4O···N31i0.88 (2)2.00 (2)2.8570 (15)167.3 (17)
Symmetry codes: (i) x, y, z+1; (ii) y+2/3, xy+1/3, z2/3; (iii) xy+2/3, x+1/3, z+1/3; (iv) y1/3, x+y+1/3, z+4/3; (v) x+y+1/3, x+2/3, z1/3.

Experimental details

(Compound_1)(Compound_2)(Compound_3)
Crystal data
Chemical formulaC22H21NOC22H21NOC22H21NO
Mr315.40315.40315.40
Crystal system, space groupMonoclinic, P21/cOrthorhombic, P212121Monoclinic, P21
Temperature (K)100298100
a, b, c (Å)24.8049 (10), 10.7126 (5), 12.1932 (4)7.5541 (3), 14.7914 (5), 15.4049 (5)7.2201 (2), 7.8128 (3), 14.7409 (5)
α, β, γ (°)90, 95.929 (1), 9090, 90, 9090, 93.690 (2), 90
V3)3222.7 (2)1721.28 (11)829.80 (5)
Z842
Radiation typeMo KαMo KαMo Kα
µ (mm1)0.080.070.08
Crystal size (mm)0.45 × 0.35 × 0.200.51 × 0.32 × 0.250.30 × 0.30 × 0.15
Data collection
DiffractometerBruker Kappa APEXIIBruker Kappa APEXIIBruker Kappa APEXII
Absorption correctionMulti-scan
(SADABS; Bruker, 2006)
Multi-scan
(SADABS; Bruker, 2006)
Multi-scan
(SADABS; Bruker, 2006)
Tmin, Tmax0.640, 0.7460.86, 0.980.92, 0.99
No. of measured, independent and
observed [I > 2σ(I)] reflections
48596, 7121, 6012 69991, 5630, 4013 27947, 4874, 4638
Rint0.0400.0410.023
(sin θ/λ)max1)0.6490.7340.709
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.047, 0.122, 1.04 0.043, 0.109, 1.03 0.033, 0.092, 1.04
No. of reflections712156304874
No. of parameters437220219
No. of restraints001
H-atom treatmentH-atom parameters constrainedH-atom parameters constrainedH-atom parameters constrained
w = 1/[σ2(Fo2) + (0.0523P)2 + 2.1093P]
where P = (Fo2 + 2Fc2)/3
w = 1/[σ2(Fo2) + (0.0474P)2 + 0.1943P]
where P = (Fo2 + 2Fc2)/3
w = 1/[σ2(Fo2) + (0.0566P)2 + 0.1148P]
where P = (Fo2 + 2Fc2)/3
Δρmax, Δρmin (e Å3)0.37, 0.260.17, 0.160.30, 0.19
Absolute structure?Refined as an inversion twinFlack x determined using 2066 quotients [(I+)-(I-)]/[(I+)+(I-)] (Parsons et al., 2013)
Absolute structure parameter?0 (2)0.1 (3)


(Compound_4)(Compound_5a)(Compound_5b)
Crystal data
Chemical formulaC18H18FNOC15H20FNOC15H20FNO
Mr283.33249.32249.32
Crystal system, space groupOrthorhombic, PbcaTrigonal, R3:HTrigonal, R3:H
Temperature (K)100298100
a, b, c (Å)7.5932 (3), 7.5859 (4), 51.010 (3)25.119 (2), 25.119 (2), 11.2812 (12)49.395 (2), 49.395 (2), 11.1802 (5)
α, β, γ (°)90, 90, 9090, 90, 12090, 90, 120
V3)2938.2 (2)6164.2 (12)23623 (2)
Z81872
Radiation typeMo KαMo KαMo Kα
µ (mm1)0.090.080.09
Crystal size (mm)0.30 × 0.25 × 0.200.30 × 0.25 × 0.200.30 × 0.25 × 0.20
Data collection
DiffractometerBruker Kappa APEXIIBruker Kappa APEXIIBruker Kappa APEXII
Absorption correctionMulti-scan
(SADABS; Bruker, 2006)
Multi-scan
(SADABS; Bruker, 2006)
Multi-scan
(SADABS; Bruker, 2006)
Tmin, Tmax0.90, 0.980.68, 0.740.89, 0.98
No. of measured, independent and
observed [I > 2σ(I)] reflections
40696, 3764, 3407 34372, 2814, 2024 124259, 12035, 8771
Rint0.0270.0360.043
(sin θ/λ)max1)0.7090.6250.649
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.045, 0.108, 1.09 0.066, 0.229, 1.07 0.046, 0.122, 1.02
No. of reflections3764281412035
No. of parameters198212786
No. of restraints0159459
H-atom treatmentH atoms treated by a mixture of independent and constrained refinementH atoms treated by a mixture of independent and constrained refinementH atoms treated by a mixture of independent and constrained refinement
w = 1/[σ2(Fo2) + (0.0371P)2 + 2.0455P]
where P = (Fo2 + 2Fc2)/3
w = 1/[σ2(Fo2) + (0.1155P)2 + 11.0098P]
where P = (Fo2 + 2Fc2)/3
w = 1/[σ2(Fo2) + (0.048P)2 + 28.8932P]
where P = (Fo2 + 2Fc2)/3
Δρmax, Δρmin (e Å3)0.32, 0.230.55, 0.410.44, 0.28
Absolute structure???
Absolute structure parameter???

Computer programs: APEX2 (Bruker, 2006), SAINT (Bruker, 2006), SIR92 (Altomare et al., 1994), SUPERFLIP (Palatinus & Chapuis, 2007), SHELXL2014 (Sheldrick, 2015), SHELXL2014 (Sheldrick, 2008a, 2015b), Mercury (Macrae et al., 2008).

Selected ring-puckering parameters (Å, °) top
For compounds (1)–(3), ring-puckering parameters in the five-membered rings refer to the atom sequence O1–N1–C2–C3–C4 and those in the six-membered rings refer to the atom sequence O1–N1–C9A–C5A–C5–C4. For compounds (4) and (5), ring-puckering parameters in the seven-membered rings refer to the atom sequence N1–C2–C3–C4–C5–C5A–C9A.
Five-membered rings
MoleculeQ2φ2
(1A)0.4489 (14)191.38 (19)
(1B)0.4678 (14)202.91 (19)
(2)0.443 (2)197.0 (3)
(3)0.4431 (14)195.7 (2)
Idealized half-chair234°
Idealized envelope180°
Six-membered rings
MoleculeQθφ
(1A)0.6289 (13)55.02 (13)348.05 (17)
(1B)0.6332 (14)53.46 (13)342.82 (17)
(2)0.629 (2)53.01 (18)342.4 (2)
(3)0.6260 (14)53.20 (13)343.83 (17)
Idealized half-chair50.8°330°
Idealized envelope54.7°360°
Seven-membered rings
MoleculeQ2φ2φ3
(4)0.3446 (12)164.5 (2)230.19 (11)
(5RT)0.385 (3)154.7 (4)231.6 (2)
(5LT), Molecule 10.4038 (15)148.8 (2)231.63 (13)
(5LT), Molecule 20.3760 (15)158.2 (2)231.28 (13)
(5LT), Molecule 30.3708 (15)153.3 (2)231.88 (14)
(5LT), Molecule 40.3790 (15)152.7 (2)231.65 (13)
Hydrogen-bond geometry (Å, º) for (Compound_1) top
D—H···AD—HH···AD···AD—H···A
C2A—H2A···O1Ai1.002.613.4061 (17)137
C5A—H5AA···Cg1A2ii1.002.603.5600 (16)163
C4B—H4B···O1Biii1.002.433.1601 (18)129
Symmetry codes: (i) x+1, y+1/2, z+1/2; (ii) x+1, y1/2, z+1/2; (iii) x+2, y, z+1.
Hydrogen-bond geometry (Å, º) for (Compound_2) top
D—H···AD—HH···AD···AD—H···A
C82—H82···O1i0.9592.663.587 (3)164
Symmetry code: (i) x+2, y+1/2, z+1/2.
Hydrogen-bond geometry (Å, º) for (Compound_3) top
D—H···AD—HH···AD···AD—H···A
C8—H8···O1i0.952.593.3880 (19)141.9
C27—H27···Cg31ii0.952.863.6294 (16)139
C28—H28···Cg32ii0.952.903.6116 (16)133
Symmetry codes: (i) x, y+1, z; (ii) x, y+1/2, z+1.
Hydrogen-bond geometry (Å, º) for (Compound_4) top
D—H···AD—HH···AD···AD—H···A
N1—H1N···O1i0.904 (17)2.450 (16)3.2709 (14)151 (13)
O1—H1O···N1ii0.88 (2)2.14 (2)3.0187 (14)172.9 (16)
C5—H5A···N1ii0.992.673.3657 (16)127.6
C6—H6···F1iii0.952.473.4236 (16)176.8
C5—H5A···O1iv0.992.533.4027 (15)147.5
Symmetry codes: (i) x, y1, z; (ii) x+3/2, y+1/2, z; (iii) x+1, y+1, z+1; (iv) x+3/2, y1/2, z.
Hydrogen-bond geometry (Å, º) for (Compound_5a) top
D—H···AD—HH···AD···AD—H···A
N1—H1N···O7i0.88 (3)2.49 (3)3.356 (3)171 (3)
O7—H7O···N1ii0.882.022.889 (3)168.8
C9—H9···O7i0.932.633.451 (4)147.3
Symmetry codes: (i) xy+2/3, x+1/3, z+4/3; (ii) y+2/3, xy+1/3, z+1/3.
Hydrogen-bond geometry (Å, º) for (Compound_5b) top
D—H···AD—HH···AD···AD—H···A
N11—H1N···O31i0.906 (16)2.287 (16)3.1897 (15)173.9 (13)
N21—H2N···O11ii0.895 (16)2.370 (17)3.2455 (15)165.8 (13)
N31—H3N···O21iii0.901 (17)2.326 (17)3.2208 (15)172.2 (14)
N41—H4N···O41iv0.893 (16)2.310 (16)3.1952 (15)170.9 (14)
O11—H1O···N11v0.869 (19)2.00 (2)2.8553 (15)166.1 (17)
O21—H2O···N410.89 (2)1.98 (2)2.8542 (15)168.6 (18)
O31—H3O···N210.864 (19)2.008 (19)2.8619 (15)169.5 (17)
O41—H4O···N31i0.88 (2)2.00 (2)2.8570 (15)167.3 (17)
Symmetry codes: (i) x, y, z+1; (ii) y+2/3, xy+1/3, z2/3; (iii) xy+2/3, x+1/3, z+1/3; (iv) y1/3, x+y+1/3, z+4/3; (v) x+y+1/3, x+2/3, z1/3.
 

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