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The mol­ecule of the title compound, C23H27N3O2, adopts a conformation having no inter­nal symmetry so that the compound exhibits conformational chirality. The mol­ecules are linked by a combination of C-H...O and C-H...[pi](arene) hydrogen bonds into a chain of rings in which two types of centrosymmetric ring alternate.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S0108270109054602/sk3357sup1.cif
Contains datablocks global, I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108270109054602/sk3357Isup2.hkl
Contains datablock I

CCDC reference: 774029

Comment top

We report here the structure and supramolecular aggregation of the title compound, (I) (Fig. 1); this compound was prepared by acetylation of the amine, (II), whose structure was reported several years ago (Abonía et al., 2007). Compound (I) was originally prepared as a possible intermediate for the synthesis of new, fused pyrazolobenzazepine derivatives with potential biological applications (Lucács et al., 2001; Wikström et al., 2002; Crecente-Campo et al., 2009), and here we compare its structure with those of the precursor, (II), and some analogues of (II) (Castillo et al., 2009).

The molecular conformation of compound (I) can conveniently be considered in terms of the orientations of the three substituents bonded to the pyrazole ring relative to the plane of the pyrazole ring itself, as indicated by the leading torsion angles (Table 1). The unsubstituted ring makes a dihedral angle of 50.3 (2)° with the pyrazole ring; coplanarity of these two rings would lead to some short non-bonded contacts, in particular between the H atom bonded to atom C12 (Fig. 1) and the atoms of the amide group. As often found in systems of this type (Abonía et al., 2007; Castillo et al., 2009) the tert-butyl group adopts an orientation in which one of the methyl C atoms, here C32, is close to, but no precisely in, the plane of the adjacent pyrazole ring: in (I), atom C32 is displaced by only 0.111 (2) Å from the plane of the pyrazole ring. Although the amide unit based on atoms N51 and C58 is planar, this plane is almost orthogonal to that of the pyrazole ring, as the torsion angles N1—C5—N51—C57 and N1—C5—N51—C58 show (Table 1). On the other hand, the methoxy group is almost coplanar with the adjacent phenyl ring and the methyl atom C541 is displaced from the plane of this ring by only 0.100 (2) Å. Accordingly, the exocyclic bond angles at atom C54 differ by almost 10° (Table 1). The remaining bond distances and angles present no unusual values.

The conformation means that the molecules of compound (I) exhibit no internal symmetry and hence they are conformationally chiral; however, the centrosymmetric space group accommodates equal numbers of the two conformational enantiomers. The non-acylated precursor, (II), adopts a rather similar conformation to that of (I) but it crystallizes in the enantiomeric pair of space groups P41212 and P43212, so that each crystal contains only a single conformational enantiomer (Abonía et al., 2007). While it was not possible to determine the correct space group for the crystal selected for data collection, because of the absence of significant resonant scattering, it was concluded that the distribution of the crystalline products between the two space groups was essentially statistical. Despite their very close similarities in constitution and conformation, the series of compounds (II)–(VII) (Abonía et al., 2007; Castillo et al., 2009) exhibit a wide range of crystallization behaviour and some unexpected isomorphisms. Thus, compounds (II) (X = OMe) and (IV) (X = Me) are isomorphous in the enantiomeric space groups P41212 and P43212, and compounds (III) X = H), (V) X = CF3) and (VII) X = Br) are isomorphous in space group C2/c, but compound (VI) X = Cl) is isomorphous with neither (IV) nor (VII).

The molecules of compound (I) are linked into a chain of centrosymmetric edge-fused rings by a combination of one C—H···O hydrogen bond and one C—H···π(arene) hydrogen bond (Table 2), in which the unsubstituted phenyl ring (C11–C16) provides the donor in the C—H···O hydrogen bond as well as acting as the acceptor in the C—H···π(arene) hydrogen bond. This latter interaction may be an important influence on the orientation of the phenyl ring relative to the pyrazole core of the molecule.

In the first of these interactions, the aryl atom C14 in the molecule at (x, y, z) acts as hydrogen-bond donor to the carbonyl atom O58 in the molecule at (-x, 1 - y, 1 - z), so forming a centrosymmetric R22(20) (Bernstein et al., 1995) ring, centred at (0, 1/2, 1/2). In the second interaction, the aryl atom C52 at (x, y, z) acts as hydrogen-bond donor to the aryl ring (C11–C16) in the molecule at (1 - x, 1 - y, 1 - z), so forming a second centrosymmetric ring, this time centred at (1/2, 1/2, 1/2). Propagation by inversion of these two motifs thus generates a chain of edge-fused rings running parallel to the [100] direction, with the rings built from paired C—H···O hydrogen bonds centred at (n, 1/2, 1/2), where n represents an integer, and those built from paired C—H···π(arene) hydrogen bonds centred at (n + 1/2, 1/2, 1/2), where n again represents an integer (Fig. 2).

The supramolecular aggregation in compound (I) may be briefly contrasted with that in compounds (II)–(VII). (Abonía et al., 2007; Castillo et al., 2009). In each of compounds (III)–(VII) the crystal structures are dominated by N—H···π hydrogen bonds, often accompanied by C—H···π hydrogen bonds, leading to the formation of a finite dimer in compound (IV), a simple chain in (III), a chain of rings in (VI), and sheets in both (V) and (VII). In compound (II), however, the N—H bond plays no role in the intermolecular aggregation, which instead is determined by a single C—H···N hydrogen bond, which forms a simple C(9) chain.

Related literature top

For related literature, see: Abonía et al. (2007); Bernstein et al. (1995); Castillo et al. (2009); Crecente-Campo, Vázquez-Tato & Seijas (2009); Lucács et al. (2001); Wikström et al. (2002).

Experimental top

Sodium borohydride (3.8 mmol) was added portion-wise during the course of 1 h to a solution of 5-amino-(E)-3-tert-butyl-N-(4-methoxybenzylidene)-1-phenyl-1H-pyrazole (1.50 mmol) in methanol (10 cm3). After the reduction was complete, the volume of the solution was reduced to around 3 cm3 under reduced pressure, and water (5 cm3) was then added. The resulting mixture was extracted with ethyl acetate (2 x 5 cm3) and the combined extracts were dried with anhydrous sodium sulfate; then the solvent was removed to give the pure amine intermediate, (II) (see scheme), in 98% isolated yield. A mixture of the amine intermediate, (II), obtained above (0.89 mmol) and acetic anhydride (0.18 g, 2.0 mmol) was heated to 373 K in an oil bath for 10 min. After the reaction was completed, the mixture was cooled to ambient temperature and water (3 cm3) was added. The resulting solid product, (I), was collected by filtration in quantitative yield. Colourless crystals suitable for single-crystal X-ray diffraction were grown by slow evaporation of a solution in methanol: m.p. 390 K; MS (IE 70 eV) m/z (%) 377 (7 [M+]), 121 (100), 77 (6). Analysis found C,73.1, H 7.4, N 11.12%; C23H27N 3O2 requires C 73.2, H 7.2, N 11.1%.

Refinement top

All H atoms were located in difference maps and then treated as riding atoms in geometrically idealized positions, with C—H distances 0.95 Å (aromatic and pyrazole), 0.98 Å (CH3) or 0.99 Å (CH2), and with Uiso(H) = kUeq(C), where k = 1.5 for the methyl groups, which were permitted to rotate but not to tilt, and 1.2 for all other H atoms.

Computing details top

Data collection: COLLECT (Hooft, 1999); cell refinement: DIRAX/LSQ (Duisenberg et al., 2000); data reduction: EVALCCD (Duisenberg et al., 2003); program(s) used to solve structure: SIR2004 (Burla et al., 2005); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: PLATON (Spek, 2009); software used to prepare material for publication: SHELXL97 (Sheldrick, 2008) and PLATON (Spek, 2009).

Figures top
[Figure 1] Fig. 1. The molecular structure of compound (I) showing the atom-labelling scheme. Displacement ellipsoids are drawn at the 30% probability level.
[Figure 2] Fig. 2. A stereoview of part of the crystal structure of compound (I) showing the formation of a chain of hydrogen-bonded rings running parallel to the [100] direction. For the sake of clarity, the H atoms not involved in the motifs shown have been omitted.
N-(3-tert-Butyl-1-phenyl-1H-pyrazol-5-yl)-N- (4-methoxybenzyl)acetamide top
Crystal data top
C23H27N3O2Z = 2
Mr = 377.48F(000) = 404
Triclinic, P1Dx = 1.208 Mg m3
Hall symbol: -P 1Mo Kα radiation, λ = 0.71073 Å
a = 9.8325 (3) ÅCell parameters from 4079 reflections
b = 9.8649 (4) Åθ = 3.0–26.1°
c = 12.0365 (3) ŵ = 0.08 mm1
α = 97.468 (2)°T = 120 K
β = 95.512 (2)°Block, colourless
γ = 114.643 (1)°0.18 × 0.12 × 0.10 mm
V = 1037.44 (5) Å3
Data collection top
Bruker Nonius KappaCCD
diffractometer
4079 independent reflections
Radiation source: Bruker Nonius FR591 rotating anode3269 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.047
Detector resolution: 9.091 pixels mm-1θmax = 26.1°, θmin = 3.0°
ϕ and ω scansh = 1212
Absorption correction: multi-scan
(SADABS; Sheldrick, 2003)
k = 1212
Tmin = 0.986, Tmax = 0.992l = 1414
18936 measured reflections
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)] = 0.042H-atom parameters constrained
wR(F2) = 0.102 w = 1/[σ2(Fo2) + (0.0371P)2 + 0.359P]
where P = (Fo2 + 2Fc2)/3
S = 1.05(Δ/σ)max = 0.001
4079 reflectionsΔρmax = 0.20 e Å3
259 parametersΔρmin = 0.21 e Å3
0 restraintsExtinction correction: SHELXL97 (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0.048 (4)
Crystal data top
C23H27N3O2γ = 114.643 (1)°
Mr = 377.48V = 1037.44 (5) Å3
Triclinic, P1Z = 2
a = 9.8325 (3) ÅMo Kα radiation
b = 9.8649 (4) ŵ = 0.08 mm1
c = 12.0365 (3) ÅT = 120 K
α = 97.468 (2)°0.18 × 0.12 × 0.10 mm
β = 95.512 (2)°
Data collection top
Bruker Nonius KappaCCD
diffractometer
4079 independent reflections
Absorption correction: multi-scan
(SADABS; Sheldrick, 2003)
3269 reflections with I > 2σ(I)
Tmin = 0.986, Tmax = 0.992Rint = 0.047
18936 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0420 restraints
wR(F2) = 0.102H-atom parameters constrained
S = 1.05Δρmax = 0.20 e Å3
4079 reflectionsΔρmin = 0.21 e Å3
259 parameters
Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
N10.44674 (13)0.62459 (13)0.37549 (9)0.0201 (3)
N20.59005 (13)0.73012 (13)0.37241 (10)0.0218 (3)
C30.63534 (16)0.66918 (16)0.28598 (12)0.0214 (3)
C40.52111 (16)0.52545 (16)0.23298 (12)0.0225 (3)
H40.52570.45920.17020.027*
C50.40220 (15)0.50091 (15)0.29046 (12)0.0197 (3)
C110.35766 (16)0.66222 (16)0.45032 (11)0.0206 (3)
C120.27899 (19)0.56247 (17)0.51741 (13)0.0307 (4)
H120.28370.46790.51540.037*
C130.1929 (2)0.60322 (19)0.58795 (15)0.0384 (4)
H130.13670.53480.63330.046*
C140.18784 (18)0.74143 (18)0.59302 (13)0.0316 (4)
H140.12910.76810.64200.038*
C150.26851 (17)0.84108 (18)0.52666 (13)0.0267 (3)
H150.26600.93680.53050.032*
C160.35299 (16)0.80138 (16)0.45454 (12)0.0240 (3)
H160.40750.86920.40810.029*
C310.78820 (16)0.76085 (16)0.25340 (13)0.0243 (3)
C320.8253 (2)0.66268 (19)0.16361 (16)0.0397 (4)
H32A0.82680.57550.19360.059*
H32B0.92490.72300.14440.059*
H32C0.74780.62660.09530.059*
C330.91334 (17)0.82470 (19)0.35810 (15)0.0353 (4)
H33A0.89030.88940.41470.053*
H33B1.01090.88470.33580.053*
H33C0.91880.74080.39070.053*
C340.77956 (18)0.89327 (18)0.20399 (14)0.0311 (4)
H34A0.69910.85340.13740.047*
H34B0.87690.95360.18160.047*
H34C0.75710.95740.26150.047*
N510.25424 (13)0.38195 (12)0.27122 (10)0.0204 (3)
C510.27037 (16)0.13326 (15)0.23943 (11)0.0201 (3)
C520.38457 (17)0.09610 (17)0.28144 (12)0.0261 (3)
H520.43760.14090.35680.031*
C530.42250 (17)0.00439 (18)0.21611 (13)0.0281 (4)
H530.50100.02800.24670.034*
C540.34618 (16)0.07127 (16)0.10558 (12)0.0218 (3)
C550.23038 (16)0.03786 (16)0.06177 (12)0.0219 (3)
H550.17620.08440.01310.026*
C560.19448 (16)0.06479 (16)0.12890 (12)0.0219 (3)
H560.11610.08870.09840.026*
C570.22972 (17)0.24092 (15)0.31406 (12)0.0225 (3)
H57A0.12160.18780.32180.027*
H57B0.29100.26840.39070.027*
O540.39547 (12)0.16561 (12)0.04702 (9)0.0281 (3)
C580.13542 (16)0.39108 (17)0.20805 (12)0.0230 (3)
O580.00863 (11)0.28455 (12)0.18798 (9)0.0316 (3)
C590.16800 (18)0.53697 (18)0.16580 (14)0.0309 (4)
H59A0.08360.52140.10730.046*
H59B0.26170.56810.13340.046*
H59C0.17980.61630.22920.046*
C5410.32253 (19)0.23165 (19)0.06787 (13)0.0327 (4)
H54A0.21620.30150.06930.049*
H54B0.37410.28750.10370.049*
H54C0.32710.15130.10960.049*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
N10.0193 (6)0.0164 (6)0.0210 (6)0.0049 (5)0.0032 (5)0.0015 (5)
N20.0179 (6)0.0173 (6)0.0264 (6)0.0042 (5)0.0038 (5)0.0032 (5)
C30.0204 (7)0.0191 (7)0.0264 (7)0.0098 (6)0.0040 (6)0.0055 (6)
C40.0226 (7)0.0186 (7)0.0262 (8)0.0096 (6)0.0052 (6)0.0015 (6)
C50.0195 (7)0.0154 (7)0.0226 (7)0.0069 (6)0.0018 (5)0.0024 (5)
C110.0191 (7)0.0209 (7)0.0186 (7)0.0069 (6)0.0016 (5)0.0003 (5)
C120.0414 (10)0.0201 (8)0.0309 (8)0.0121 (7)0.0138 (7)0.0047 (6)
C130.0476 (11)0.0263 (9)0.0395 (10)0.0103 (8)0.0247 (8)0.0079 (7)
C140.0288 (8)0.0304 (9)0.0329 (9)0.0110 (7)0.0111 (7)0.0007 (7)
C150.0266 (8)0.0254 (8)0.0295 (8)0.0142 (7)0.0019 (6)0.0017 (6)
C160.0244 (8)0.0230 (8)0.0241 (7)0.0095 (6)0.0038 (6)0.0055 (6)
C310.0201 (7)0.0182 (7)0.0343 (8)0.0076 (6)0.0071 (6)0.0048 (6)
C320.0308 (9)0.0288 (9)0.0583 (11)0.0103 (8)0.0223 (8)0.0026 (8)
C330.0202 (8)0.0323 (9)0.0476 (10)0.0051 (7)0.0022 (7)0.0130 (8)
C340.0281 (8)0.0269 (8)0.0407 (9)0.0109 (7)0.0117 (7)0.0137 (7)
N510.0187 (6)0.0148 (6)0.0247 (6)0.0049 (5)0.0028 (5)0.0021 (5)
C570.0255 (8)0.0169 (7)0.0218 (7)0.0061 (6)0.0049 (6)0.0036 (6)
C510.0199 (7)0.0149 (7)0.0216 (7)0.0034 (6)0.0047 (5)0.0042 (5)
C520.0279 (8)0.0269 (8)0.0208 (7)0.0111 (7)0.0011 (6)0.0022 (6)
C530.0279 (8)0.0323 (9)0.0272 (8)0.0171 (7)0.0007 (6)0.0064 (6)
C540.0232 (7)0.0183 (7)0.0258 (7)0.0096 (6)0.0073 (6)0.0058 (6)
C550.0218 (7)0.0205 (7)0.0202 (7)0.0071 (6)0.0013 (6)0.0018 (6)
C560.0198 (7)0.0210 (7)0.0244 (7)0.0087 (6)0.0023 (6)0.0041 (6)
O540.0302 (6)0.0290 (6)0.0293 (6)0.0187 (5)0.0033 (4)0.0003 (4)
C5410.0344 (9)0.0309 (9)0.0331 (9)0.0179 (8)0.0044 (7)0.0050 (7)
C580.0216 (8)0.0238 (8)0.0212 (7)0.0085 (6)0.0042 (6)0.0001 (6)
O580.0200 (6)0.0307 (6)0.0361 (6)0.0053 (5)0.0009 (5)0.0026 (5)
C590.0285 (8)0.0288 (9)0.0344 (9)0.0123 (7)0.0002 (7)0.0070 (7)
Geometric parameters (Å, º) top
N1—N21.3666 (16)C34—H34A0.9800
N1—C51.3680 (18)C34—H34B0.9800
N1—C111.4325 (18)C34—H34C0.9800
N2—C31.3385 (18)N51—C581.3733 (18)
C3—C41.406 (2)N51—C571.4799 (17)
C3—C311.517 (2)C57—C511.507 (2)
C4—C51.367 (2)C57—H57A0.9900
C4—H40.9500C57—H57B0.9900
C5—N511.4101 (17)C51—C521.390 (2)
C11—C121.382 (2)C51—C561.3922 (19)
C11—C161.387 (2)C52—C531.379 (2)
C12—C131.390 (2)C52—H520.9500
C12—H120.9500C53—C541.391 (2)
C13—C141.379 (2)C53—H530.9500
C13—H130.9500C54—O541.3672 (17)
C14—C151.382 (2)C54—C551.388 (2)
C14—H140.9500C55—C561.394 (2)
C15—C161.385 (2)C55—H550.9500
C15—H150.9500C56—H560.9500
C16—H160.9500O54—C5411.4272 (18)
C31—C321.529 (2)C541—H54A0.9800
C31—C331.532 (2)C541—H54B0.9800
C31—C341.534 (2)C541—H54C0.9800
C32—H32A0.9800C58—O581.2250 (17)
C32—H32B0.9800C58—C591.507 (2)
C32—H32C0.9800C59—H59A0.9800
C33—H33A0.9800C59—H59B0.9800
C33—H33B0.9800C59—H59C0.9800
C33—H33C0.9800
N2—N1—C5111.09 (11)C31—C34—H34A109.5
N2—N1—C11119.51 (11)C31—C34—H34B109.5
C5—N1—C11128.69 (12)H34A—C34—H34B109.5
C3—N2—N1105.23 (11)C31—C34—H34C109.5
N2—C3—C4110.88 (12)H34A—C34—H34C109.5
N2—C3—C31119.53 (12)H34B—C34—H34C109.5
C4—C3—C31129.44 (13)C58—N51—C5121.35 (11)
C5—C4—C3105.73 (13)C58—N51—C57119.72 (11)
C5—C4—H4127.1C5—N51—C57118.81 (11)
C3—C4—H4127.1N51—C57—C51114.13 (11)
C4—C5—N1107.05 (12)N51—C57—H57A108.7
C4—C5—N51131.42 (13)C51—C57—H57A108.7
N1—C5—N51121.43 (12)N51—C57—H57B108.7
C12—C11—C16120.77 (13)C51—C57—H57B108.7
C12—C11—N1120.70 (13)H57A—C57—H57B107.6
C16—C11—N1118.53 (12)C52—C51—C56117.71 (13)
C11—C12—C13118.69 (15)C52—C51—C57119.98 (13)
C11—C12—H12120.7C56—C51—C57122.29 (13)
C13—C12—H12120.7C53—C52—C51121.43 (13)
C14—C13—C12120.99 (15)C53—C52—H52119.3
C14—C13—H13119.5C51—C52—H52119.3
C12—C13—H13119.5C52—C53—C54120.19 (14)
C13—C14—C15119.82 (15)C52—C53—H53119.9
C13—C14—H14120.1C54—C53—H53119.9
C15—C14—H14120.1O54—C54—C53115.54 (13)
C14—C15—C16119.98 (14)O54—C54—C55124.75 (13)
C14—C15—H15120.0C55—C54—C53119.70 (13)
C16—C15—H15120.0C54—C55—C56119.22 (13)
C15—C16—C11119.75 (14)C54—C55—H55120.4
C15—C16—H16120.1C56—C55—H55120.4
C11—C16—H16120.1C51—C56—C55121.74 (13)
C3—C31—C32110.51 (12)C51—C56—H56119.1
C3—C31—C33110.51 (12)C55—C56—H56119.1
C32—C31—C33109.76 (13)C54—O54—C541116.67 (11)
C3—C31—C34108.01 (12)O54—C541—H54A109.5
C32—C31—C34109.05 (13)O54—C541—H54B109.5
C33—C31—C34108.96 (12)H54A—C541—H54B109.5
C31—C32—H32A109.5O54—C541—H54C109.5
C31—C32—H32B109.5H54A—C541—H54C109.5
H32A—C32—H32B109.5H54B—C541—H54C109.5
C31—C32—H32C109.5O58—C58—N51120.79 (13)
H32A—C32—H32C109.5O58—C58—C59122.01 (13)
H32B—C32—H32C109.5N51—C58—C59117.20 (12)
C31—C33—H33A109.5C58—C59—H59A109.5
C31—C33—H33B109.5C58—C59—H59B109.5
H33A—C33—H33B109.5H59A—C59—H59B109.5
C31—C33—H33C109.5C58—C59—H59C109.5
H33A—C33—H33C109.5H59A—C59—H59C109.5
H33B—C33—H33C109.5H59B—C59—H59C109.5
C5—N1—N2—C31.29 (15)C4—C3—C31—C33133.91 (16)
C11—N1—N2—C3172.45 (12)N2—C3—C31—C3468.09 (17)
N1—N2—C3—C40.49 (15)C4—C3—C31—C34106.99 (17)
N1—N2—C3—C31176.43 (12)C53—C54—O54—C541177.94 (13)
N2—C3—C4—C50.46 (16)C4—C5—N51—C5892.78 (19)
C31—C3—C4—C5174.97 (14)N1—C5—N51—C57100.84 (15)
C3—C4—C5—N11.21 (15)N1—C5—N51—C5883.16 (17)
C3—C4—C5—N51175.17 (14)C4—C5—N51—C5783.22 (19)
N2—N1—C5—C41.60 (16)C58—N51—C57—C5195.56 (15)
C11—N1—C5—C4171.73 (13)C5—N51—C57—C5180.52 (15)
N2—N1—C5—N51175.22 (11)N51—C57—C51—C52118.10 (14)
C11—N1—C5—N515.1 (2)N51—C57—C51—C5663.63 (17)
N2—N1—C11—C12133.97 (14)C56—C51—C52—C530.4 (2)
C5—N1—C11—C1256.6 (2)C57—C51—C52—C53178.70 (13)
N2—N1—C11—C1645.58 (17)C51—C52—C53—C540.0 (2)
C5—N1—C11—C16123.84 (15)C52—C53—C54—O54178.14 (13)
C16—C11—C12—C131.1 (2)C52—C53—C54—C550.8 (2)
N1—C11—C12—C13179.40 (14)O54—C54—C55—C56177.61 (13)
C11—C12—C13—C141.3 (3)C53—C54—C55—C561.2 (2)
C12—C13—C14—C150.4 (3)C52—C51—C56—C550.1 (2)
C13—C14—C15—C160.6 (2)C57—C51—C56—C55178.21 (13)
C14—C15—C16—C110.8 (2)C54—C55—C56—C510.9 (2)
C12—C11—C16—C150.1 (2)C55—C54—O54—C5410.9 (2)
N1—C11—C16—C15179.61 (12)C5—N51—C58—O58176.99 (13)
N2—C3—C31—C32172.69 (13)C57—N51—C58—O581.0 (2)
C4—C3—C31—C3212.2 (2)C5—N51—C58—C593.36 (19)
N2—C3—C31—C3351.01 (18)C57—N51—C58—C59179.33 (12)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C14—H14···O58i0.952.553.389 (2)147
C52—H52···Cgii0.952.753.544 (2)142
Symmetry codes: (i) x, y+1, z+1; (ii) x+1, y+1, z+1.

Experimental details

Crystal data
Chemical formulaC23H27N3O2
Mr377.48
Crystal system, space groupTriclinic, P1
Temperature (K)120
a, b, c (Å)9.8325 (3), 9.8649 (4), 12.0365 (3)
α, β, γ (°)97.468 (2), 95.512 (2), 114.643 (1)
V3)1037.44 (5)
Z2
Radiation typeMo Kα
µ (mm1)0.08
Crystal size (mm)0.18 × 0.12 × 0.10
Data collection
DiffractometerBruker Nonius KappaCCD
diffractometer
Absorption correctionMulti-scan
(SADABS; Sheldrick, 2003)
Tmin, Tmax0.986, 0.992
No. of measured, independent and
observed [I > 2σ(I)] reflections
18936, 4079, 3269
Rint0.047
(sin θ/λ)max1)0.618
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.042, 0.102, 1.05
No. of reflections4079
No. of parameters259
H-atom treatmentH-atom parameters constrained
Δρmax, Δρmin (e Å3)0.20, 0.21

Computer programs: COLLECT (Hooft, 1999), DIRAX/LSQ (Duisenberg et al., 2000), EVALCCD (Duisenberg et al., 2003), SIR2004 (Burla et al., 2005), SHELXL97 (Sheldrick, 2008) and PLATON (Spek, 2009).

Selected bond and torsion angles (º) top
O54—C54—C53115.54 (13)C54—O54—C541116.67 (11)
O54—C54—C55124.75 (13)
N2—N1—C11—C12133.97 (14)N1—C5—N51—C57100.84 (15)
N2—C3—C31—C32172.69 (13)N1—C5—N51—C5883.16 (17)
N2—C3—C31—C3351.01 (18)C5—N51—C57—C5180.52 (15)
N2—C3—C31—C3468.09 (17)N51—C57—C51—C52118.10 (14)
C53—C54—O54—C541177.94 (13)C5—N51—C58—O58176.99 (13)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C14—H14···O58i0.952.553.389 (2)147
C52—H52···Cgii0.952.753.544 (2)142
Symmetry codes: (i) x, y+1, z+1; (ii) x+1, y+1, z+1.
 

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