1-[5-(4-Bromo­phen­yl)-3-(4-fluoro­phen­yl)-4,5-dihydro-1H-pyrazol-1-yl]butan-1-one

Fun, H.-K.; Loh, W.-S.; Sapnakumari, M.; Narayana, B.; Sarojini, B.K.

doi:10.1107/S1600536812034368

organic compounds

CRYSTALLOGRAPHIC
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ISSN: 2056-9890

Volume 68| Part 9| September 2012| Pages o2655-o2656

doi:10.1107/S1600536812034368

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1-[5-(4-Bromophenyl)-3-(4-fluorophenyl)-4,5-dihydro-1H-pyrazol-1-yl]butan-1-one

Hoong-Kun Fun,^a ^*‡ Wan-Sin Loh,^a § M. Sapnakumari,^b B. Narayana ^b and B. K. Sarojini ^c

^aX-ray Crystallography Unit, School of Physics, Universiti Sains Malaysia, 11800 USM, Penang, Malaysia, ^bDepartment of Studies in Chemistry, Mangalore University, Mangalagangotri 574 199, India, and ^cDepartment of Chemistry, P.A. College of Engineering, Nadupadavu, Mangalore 574 153, India
^*Correspondence e-mail: hkfun@usm.my

(Received 27 July 2012; accepted 2 August 2012; online 8 August 2012)

In the title compound, C₁₉H₁₈BrFN₂O, the benzene rings form dihedral angles of 5.38 (7) and 85.48 (7)° with the mean plane of the 4,5-dihydro-1H-pyrazole ring (r.m.s. deviation = 0.0849 Å), which approximates to an envelope conformation with the –CH₂– group as the flap. The dihedral angle between the benzene rings is 82.86 (7)°. In the crystal, C—H⋯F and C—H⋯O hydrogen bonds link the molecules to form inversion dimers and together these generate chains along [011]. The crystal packing also features C—H⋯π interactions.

Related literature

For background to pyrazoline derivatives, see: Fun et al. (2010 ); Samshuddin et al. (2011 ). For related structures, see: Fun, Quah et al. (2012 ); Fun, Loh et al. (2012 ). For the stability of the temperature controller used for the data collection, see: Cosier & Glazer (1986 ).

Experimental

Crystal data

C₁₉H₁₈BrFN₂O
M_r = 389.26
Triclinic, $[P \overline 1]$
a = 6.7502 (3) Å
b = 10.1253 (5) Å
c = 13.7792 (8) Å
α = 105.354 (1)°
β = 98.976 (1)°
γ = 107.369 (1)°
V = 838.01 (7) Å³
Z = 2
Mo Kα radiation
μ = 2.47 mm⁻¹
T = 100 K
0.28 × 0.23 × 0.08 mm

Data collection

Bruker SMART APEXII DUO CCD diffractometer
Absorption correction: multi-scan (SADABS; Bruker, 2009 ) T_min = 0.546, T_max = 0.823
17838 measured reflections
4816 independent reflections
4458 reflections with I > 2σ(I)
R_int = 0.023

Refinement

R[F² > 2σ(F²)] = 0.025
wR(F²) = 0.066
S = 1.06
4816 reflections
218 parameters
H-atom parameters constrained
Δρ_max = 0.49 e Å⁻³
Δρ_min = −0.63 e Å⁻³

Table 1
Hydrogen-bond geometry (Å, °)

Cg1 and Cg2 are the centroids of the C1–C5 and C10–C15 benzene rings, respectively.

D—H⋯A	D—H	H⋯A	D⋯A	D—H⋯A
C11—H11A⋯F1ⁱ	0.95	2.37	3.1873 (17)	144
C14—H14A⋯O1ⁱⁱ	0.95	2.57	3.1832 (16)	122
C5—H5A⋯Cg2ⁱⁱⁱ	0.95	2.68	3.5453 (15)	152
C17—H17B⋯Cg1^iv	0.99	2.70	3.5488 (14)	144
Symmetry codes: (i) -x+2, -y+1, -z+1; (ii) -x+1, -y+2, -z+2; (iii) x+1, y, z; (iv) x-1, y, z.

Data collection: APEX2 (Bruker, 2009); cell refinement: SAINT (Bruker, 2009); data reduction: SAINT; program(s) used to solve structure: SHELXTL (Sheldrick, 2008 ); program(s) used to refine structure: SHELXTL; molecular graphics: SHELXTL; software used to prepare material for publication: SHELXTL and PLATON (Spek, 2009 ).

Supporting information

Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536812034368/hb6918sup1.cif

Structure factors: contains datablock I. DOI: 10.1107/S1600536812034368/hb6918Isup2.hkl

Supporting information file. DOI: 10.1107/S1600536812034368/hb6918Isup3.cml

checkCIF report

Comment top

In continuation of our work on synthesis of pyrazoline derivatives (Fun et al., 2010; Samshuddin et al., 2011), the title compound is prepared and its crystal structure is reported.

In the title compound, Fig. 1, the benzene rings (C1–C6 & C10–C15) form dihedral angles of 5.38 (7) and 85.48 (7)°, respectively, with the mean plane of 4,5-dihydro-1H-pyrazole ring (N1/N2/C7–C9, r.m.s. deviation = 0.0849 Å). The dihedral angle between the two benzene rings is 82.86 (7) °. Bond lengths and angles are comparable with those in related structures (Fun, Quah et al., 2012; Fun, Loh et al., 2012).

In the crystal packing as shown in Fig. 2, C11—H11A···F1 and C14—H14A···O1 hydrogen bonds (Table 1) link the molecules to form dimers, generating chains along the [011]. The crystal packing is further consolidated by C17—H17B···Cg1 and C5—H5A···Cg2 (Table 1) interactions, where Cg1 and Cg2 are the centroids of C1–C5 and C10–C15 benzene rings, respectively.

Related literature top

For background to pyrazoline derivatives, see: Fun et al. (2010); Samshuddin et al. (2011). For related structures, see: Fun, Quah et al. (2012); Fun, Loh et al. (2012). For the stability of the temperature controller used for the data collection, see: Cosier & Glazer (1986).

Experimental top

A mixture of (2E)-3-(4-bromophenyl)-1-(4-fluorophenyl)prop-2-en-1-one (3.05 g, 0.01 mol) and hydrazine hydrate (0.48 ml, 0.01 mol) in 30 ml butyric acid was refluxed for 6 h. The reaction mixture was cooled and poured into 50 ml ice-cold water. The precipitate was collected by filtration and purified by recrystallization from ethanol. Colourless plates were grown from acetone solution by slow evaporation method. M. p.: 383–385 K.

Computing details top

Data collection: APEX2 (Bruker, 2009); cell refinement: SAINT (Bruker, 2009); data reduction: SAINT (Bruker, 2009); program(s) used to solve structure: SHELXTL (Sheldrick, 2008); program(s) used to refine structure: SHELXTL (Sheldrick, 2008); molecular graphics: SHELXTL (Sheldrick, 2008); software used to prepare material for publication: SHELXTL (Sheldrick, 2008) and PLATON (Spek, 2009).

Figures top

	Fig. 1. The molecular structure of the title compound, showing 50% probability displacement ellipsoids.
	Fig. 2. The crystal packing of the title compound, viewed along the a axis. H atoms not involved in the intermolecular interactions (dashed lines) have been omitted for clarity.

1-[5-(4-Bromophenyl)-3-(4-fluorophenyl)-4,5-dihydro-1H-pyrazol-1- yl]butan-1-one top

Crystal data top

C₁₉H₁₈BrFN₂O	Z = 2
M_r = 389.26	F(000) = 396
Triclinic, P1	D_x = 1.543 Mg m⁻³
Hall symbol: -P 1	Mo Kα radiation, λ = 0.71073 Å
a = 6.7502 (3) Å	Cell parameters from 9994 reflections
b = 10.1253 (5) Å	θ = 3.1–33.0°
c = 13.7792 (8) Å	µ = 2.47 mm⁻¹
α = 105.354 (1)°	T = 100 K
β = 98.976 (1)°	Plate, colourless
γ = 107.369 (1)°	0.28 × 0.23 × 0.08 mm
V = 838.01 (7) Å³

Data collection top

Bruker SMART APEXII DUO CCD diffractometer	4816 independent reflections
Radiation source: fine-focus sealed tube	4458 reflections with I > 2σ(I)
Graphite monochromator	R_int = 0.023
ϕ and ω scans	θ_max = 30.0°, θ_min = 2.2°
Absorption correction: multi-scan (SADABS; Bruker, 2009)	h = −9→9
T_min = 0.546, T_max = 0.823	k = −14→14
17838 measured reflections	l = −19→19

Refinement top

Refinement on F²	Primary atom site location: structure-invariant direct methods
Least-squares matrix: full	Secondary atom site location: difference Fourier map
R[F² > 2σ(F²)] = 0.025	Hydrogen site location: inferred from neighbouring sites
wR(F²) = 0.066	H-atom parameters constrained
S = 1.06	w = 1/[σ²(F_o²) + (0.0342P)² + 0.3618P] where P = (F_o² + 2F_c²)/3
4816 reflections	(Δ/σ)_max = 0.001
218 parameters	Δρ_max = 0.49 e Å⁻³
0 restraints	Δρ_min = −0.63 e Å⁻³

Crystal data top

C₁₉H₁₈BrFN₂O	γ = 107.369 (1)°
M_r = 389.26	V = 838.01 (7) Å³
Triclinic, P1	Z = 2
a = 6.7502 (3) Å	Mo Kα radiation
b = 10.1253 (5) Å	µ = 2.47 mm⁻¹
c = 13.7792 (8) Å	T = 100 K
α = 105.354 (1)°	0.28 × 0.23 × 0.08 mm
β = 98.976 (1)°

Data collection top

Bruker SMART APEXII DUO CCD diffractometer	4816 independent reflections
Absorption correction: multi-scan (SADABS; Bruker, 2009)	4458 reflections with I > 2σ(I)
T_min = 0.546, T_max = 0.823	R_int = 0.023
17838 measured reflections

Refinement top

R[F² > 2σ(F²)] = 0.025	0 restraints
wR(F²) = 0.066	H-atom parameters constrained
S = 1.06	Δρ_max = 0.49 e Å⁻³
4816 reflections	Δρ_min = −0.63 e Å⁻³
218 parameters

Special details top

Experimental. The crystal was placed in the cold stream of an Oxford Cryosystems Cobra open-flow nitrogen cryostat (Cosier & Glazer, 1986) operating at 100.0 (1) K.

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

Refinement. Refinement of F² against ALL reflections. The weighted R-factor wR and goodness of fit S are based on F², conventional R-factors R are based on F, with F set to zero for negative F². The threshold expression of F² > σ(F²) is used only for calculating R-factors(gt) etc. and is not relevant to the choice of reflections for refinement. R-factors based on F² are statistically about twice as large as those based on F, and R- factors based on ALL data will be even larger.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å²) top

	x	y	z	U_iso*/U_eq
Br1	0.29346 (2)	1.105034 (15)	0.629792 (11)	0.02435 (5)
F1	1.22640 (16)	0.30984 (10)	0.49188 (7)	0.02653 (19)
O1	0.44837 (15)	0.73712 (10)	0.95847 (7)	0.01715 (18)
N1	0.69619 (17)	0.56573 (11)	0.78382 (8)	0.01292 (18)
N2	0.65164 (17)	0.67234 (11)	0.85431 (8)	0.01310 (19)
C1	0.8653 (2)	0.39253 (14)	0.64641 (10)	0.0171 (2)
H1A	0.7351	0.3438	0.6608	0.020*
C2	0.9522 (2)	0.31297 (15)	0.57824 (11)	0.0201 (2)
H2A	0.8834	0.2100	0.5457	0.024*
C3	1.1414 (2)	0.38745 (16)	0.55897 (10)	0.0184 (2)
C4	1.2486 (2)	0.53618 (15)	0.60412 (10)	0.0175 (2)
H4A	1.3788	0.5836	0.5892	0.021*
C5	1.1603 (2)	0.61528 (14)	0.67260 (10)	0.0150 (2)
H5A	1.2310	0.7182	0.7049	0.018*
C6	0.96862 (19)	0.54438 (13)	0.69403 (9)	0.0133 (2)
C7	0.87764 (19)	0.62814 (13)	0.76656 (9)	0.0127 (2)
C8	0.98525 (19)	0.78883 (13)	0.83134 (10)	0.0149 (2)
H8A	1.0376	0.8493	0.7883	0.018*
H8B	1.1065	0.8046	0.8891	0.018*
C9	0.80040 (19)	0.82300 (13)	0.87232 (9)	0.0131 (2)
H9A	0.8511	0.8801	0.9484	0.016*
C10	0.68978 (19)	0.89988 (13)	0.81387 (9)	0.0129 (2)
C11	0.6768 (2)	0.87756 (14)	0.70818 (10)	0.0165 (2)
H11A	0.7482	0.8192	0.6735	0.020*
C12	0.5613 (2)	0.93907 (14)	0.65294 (10)	0.0183 (2)
H12A	0.5527	0.9229	0.5810	0.022*
C13	0.4586 (2)	1.02469 (14)	0.70504 (10)	0.0167 (2)
C14	0.4748 (2)	1.05360 (13)	0.81074 (10)	0.0158 (2)
H14A	0.4084	1.1155	0.8458	0.019*
C15	0.59010 (19)	0.99012 (13)	0.86442 (9)	0.0143 (2)
H15A	0.6012	1.0085	0.9367	0.017*
C16	0.48284 (19)	0.63837 (13)	0.89729 (9)	0.0128 (2)
C17	0.34922 (19)	0.47749 (13)	0.86741 (9)	0.0137 (2)
H17A	0.4423	0.4249	0.8877	0.016*
H17B	0.2912	0.4363	0.7909	0.016*
C18	0.1640 (2)	0.45162 (14)	0.91894 (10)	0.0157 (2)
H18A	0.0674	0.5007	0.8965	0.019*
H18B	0.2213	0.4959	0.9954	0.019*
C19	0.0363 (2)	0.28890 (16)	0.89136 (11)	0.0226 (3)
H19A	−0.0778	0.2765	0.9279	0.034*
H19B	0.1321	0.2396	0.9123	0.034*
H19C	−0.0274	0.2459	0.8161	0.034*

Atomic displacement parameters (Å²) top

	U¹¹	U²²	U³³	U¹²	U¹³	U²³
Br1	0.02830 (8)	0.02231 (8)	0.02494 (8)	0.01276 (6)	0.00379 (5)	0.00926 (5)
F1	0.0359 (5)	0.0316 (5)	0.0200 (4)	0.0222 (4)	0.0148 (4)	0.0051 (3)
O1	0.0176 (4)	0.0163 (4)	0.0177 (4)	0.0058 (3)	0.0095 (3)	0.0033 (3)
N1	0.0128 (4)	0.0133 (4)	0.0136 (4)	0.0056 (4)	0.0056 (4)	0.0037 (4)
N2	0.0127 (4)	0.0109 (4)	0.0156 (5)	0.0035 (4)	0.0068 (4)	0.0030 (4)
C1	0.0156 (5)	0.0162 (5)	0.0185 (6)	0.0053 (4)	0.0053 (5)	0.0042 (5)
C2	0.0235 (6)	0.0180 (6)	0.0174 (6)	0.0097 (5)	0.0041 (5)	0.0018 (5)
C3	0.0242 (6)	0.0247 (6)	0.0122 (5)	0.0163 (5)	0.0071 (5)	0.0054 (5)
C4	0.0169 (6)	0.0244 (6)	0.0167 (5)	0.0108 (5)	0.0085 (5)	0.0092 (5)
C5	0.0142 (5)	0.0174 (5)	0.0153 (5)	0.0070 (4)	0.0058 (4)	0.0058 (4)
C6	0.0128 (5)	0.0162 (5)	0.0123 (5)	0.0069 (4)	0.0041 (4)	0.0047 (4)
C7	0.0110 (5)	0.0134 (5)	0.0137 (5)	0.0047 (4)	0.0036 (4)	0.0040 (4)
C8	0.0110 (5)	0.0142 (5)	0.0187 (5)	0.0032 (4)	0.0066 (4)	0.0037 (4)
C9	0.0117 (5)	0.0120 (5)	0.0147 (5)	0.0026 (4)	0.0059 (4)	0.0032 (4)
C10	0.0126 (5)	0.0115 (5)	0.0134 (5)	0.0027 (4)	0.0057 (4)	0.0027 (4)
C11	0.0190 (6)	0.0170 (5)	0.0154 (5)	0.0077 (5)	0.0096 (5)	0.0041 (4)
C12	0.0224 (6)	0.0186 (6)	0.0151 (5)	0.0072 (5)	0.0083 (5)	0.0054 (5)
C13	0.0168 (5)	0.0142 (5)	0.0194 (6)	0.0050 (4)	0.0054 (5)	0.0063 (4)
C14	0.0151 (5)	0.0131 (5)	0.0193 (6)	0.0046 (4)	0.0078 (4)	0.0036 (4)
C15	0.0145 (5)	0.0132 (5)	0.0142 (5)	0.0034 (4)	0.0072 (4)	0.0026 (4)
C16	0.0113 (5)	0.0154 (5)	0.0124 (5)	0.0046 (4)	0.0041 (4)	0.0052 (4)
C17	0.0123 (5)	0.0140 (5)	0.0146 (5)	0.0035 (4)	0.0048 (4)	0.0048 (4)
C18	0.0127 (5)	0.0191 (5)	0.0165 (5)	0.0039 (4)	0.0063 (4)	0.0080 (4)
C19	0.0180 (6)	0.0216 (6)	0.0240 (7)	−0.0006 (5)	0.0067 (5)	0.0087 (5)

Geometric parameters (Å, º) top

Br1—C13	1.8991 (13)	C9—C10	1.5177 (17)
F1—C3	1.3606 (14)	C9—H9A	1.0000
O1—C16	1.2322 (15)	C10—C15	1.3960 (16)
N1—C7	1.2901 (16)	C10—C11	1.3978 (17)
N1—N2	1.3888 (13)	C11—C12	1.3894 (19)
N2—C16	1.3608 (15)	C11—H11A	0.9500
N2—C9	1.4846 (15)	C12—C13	1.3902 (17)
C1—C2	1.3891 (17)	C12—H12A	0.9500
C1—C6	1.4013 (17)	C13—C14	1.3872 (18)
C1—H1A	0.9500	C14—C15	1.3918 (18)
C2—C3	1.381 (2)	C14—H14A	0.9500
C2—H2A	0.9500	C15—H15A	0.9500
C3—C4	1.375 (2)	C16—C17	1.5127 (17)
C4—C5	1.3957 (16)	C17—C18	1.5219 (16)
C4—H4A	0.9500	C17—H17A	0.9900
C5—C6	1.3975 (17)	C17—H17B	0.9900
C5—H5A	0.9500	C18—C19	1.5232 (19)
C6—C7	1.4660 (16)	C18—H18A	0.9900
C7—C8	1.5148 (17)	C18—H18B	0.9900
C8—C9	1.5394 (16)	C19—H19A	0.9800
C8—H8A	0.9900	C19—H19B	0.9800
C8—H8B	0.9900	C19—H19C	0.9800

C7—N1—N2	107.76 (10)	C15—C10—C9	120.04 (11)
C16—N2—N1	122.03 (10)	C11—C10—C9	121.35 (10)
C16—N2—C9	125.22 (10)	C12—C11—C10	121.24 (11)
N1—N2—C9	112.69 (9)	C12—C11—H11A	119.4
C2—C1—C6	120.32 (12)	C10—C11—H11A	119.4
C2—C1—H1A	119.8	C11—C12—C13	118.64 (12)
C6—C1—H1A	119.8	C11—C12—H12A	120.7
C3—C2—C1	118.28 (12)	C13—C12—H12A	120.7
C3—C2—H2A	120.9	C14—C13—C12	121.63 (12)
C1—C2—H2A	120.9	C14—C13—Br1	119.20 (9)
F1—C3—C4	118.22 (12)	C12—C13—Br1	119.17 (10)
F1—C3—C2	118.38 (12)	C13—C14—C15	118.73 (11)
C4—C3—C2	123.40 (12)	C13—C14—H14A	120.6
C3—C4—C5	117.96 (12)	C15—C14—H14A	120.6
C3—C4—H4A	121.0	C14—C15—C10	121.14 (11)
C5—C4—H4A	121.0	C14—C15—H15A	119.4
C4—C5—C6	120.54 (12)	C10—C15—H15A	119.4
C4—C5—H5A	119.7	O1—C16—N2	119.59 (11)
C6—C5—H5A	119.7	O1—C16—C17	123.68 (11)
C5—C6—C1	119.50 (11)	N2—C16—C17	116.72 (10)
C5—C6—C7	120.20 (11)	C16—C17—C18	112.50 (10)
C1—C6—C7	120.30 (11)	C16—C17—H17A	109.1
N1—C7—C6	121.06 (11)	C18—C17—H17A	109.1
N1—C7—C8	113.62 (10)	C16—C17—H17B	109.1
C6—C7—C8	125.25 (10)	C18—C17—H17B	109.1
C7—C8—C9	101.79 (9)	H17A—C17—H17B	107.8
C7—C8—H8A	111.4	C17—C18—C19	111.82 (11)
C9—C8—H8A	111.4	C17—C18—H18A	109.3
C7—C8—H8B	111.4	C19—C18—H18A	109.3
C9—C8—H8B	111.4	C17—C18—H18B	109.3
H8A—C8—H8B	109.3	C19—C18—H18B	109.3
N2—C9—C10	110.08 (10)	H18A—C18—H18B	107.9
N2—C9—C8	100.37 (9)	C18—C19—H19A	109.5
C10—C9—C8	114.80 (10)	C18—C19—H19B	109.5
N2—C9—H9A	110.4	H19A—C19—H19B	109.5
C10—C9—H9A	110.4	C18—C19—H19C	109.5
C8—C9—H9A	110.4	H19A—C19—H19C	109.5
C15—C10—C11	118.55 (11)	H19B—C19—H19C	109.5

C7—N1—N2—C16	−172.51 (11)	C7—C8—C9—N2	17.81 (11)
C7—N1—N2—C9	10.01 (13)	C7—C8—C9—C10	−100.16 (11)
C6—C1—C2—C3	−0.1 (2)	N2—C9—C10—C15	94.86 (13)
C1—C2—C3—F1	−179.72 (12)	C8—C9—C10—C15	−152.80 (11)
C1—C2—C3—C4	0.3 (2)	N2—C9—C10—C11	−82.31 (14)
F1—C3—C4—C5	179.79 (11)	C8—C9—C10—C11	30.03 (16)
C2—C3—C4—C5	−0.2 (2)	C15—C10—C11—C12	−2.23 (19)
C3—C4—C5—C6	−0.02 (19)	C9—C10—C11—C12	174.98 (12)
C4—C5—C6—C1	0.20 (19)	C10—C11—C12—C13	0.3 (2)
C4—C5—C6—C7	179.61 (11)	C11—C12—C13—C14	2.1 (2)
C2—C1—C6—C5	−0.13 (19)	C11—C12—C13—Br1	−178.25 (10)
C2—C1—C6—C7	−179.54 (12)	C12—C13—C14—C15	−2.6 (2)
N2—N1—C7—C6	−179.32 (10)	Br1—C13—C14—C15	177.84 (9)
N2—N1—C7—C8	3.50 (14)	C13—C14—C15—C10	0.53 (19)
C5—C6—C7—N1	176.94 (12)	C11—C10—C15—C14	1.81 (18)
C1—C6—C7—N1	−3.66 (18)	C9—C10—C15—C14	−175.44 (11)
C5—C6—C7—C8	−6.23 (18)	N1—N2—C16—O1	−179.08 (11)
C1—C6—C7—C8	173.18 (12)	C9—N2—C16—O1	−1.92 (18)
N1—C7—C8—C9	−14.48 (14)	N1—N2—C16—C17	2.02 (16)
C6—C7—C8—C9	168.48 (11)	C9—N2—C16—C17	179.18 (11)
C16—N2—C9—C10	−74.12 (14)	O1—C16—C17—C18	1.59 (17)
N1—N2—C9—C10	103.27 (11)	N2—C16—C17—C18	−179.55 (10)
C16—N2—C9—C8	164.49 (11)	C16—C17—C18—C19	−177.81 (11)
N1—N2—C9—C8	−18.12 (12)

Hydrogen-bond geometry (Å, º) top

D—H···A	D—H	H···A	D···A	D—H···A
C11—H11A···F1ⁱ	0.95	2.37	3.1873 (17)	144
C14—H14A···O1ⁱⁱ	0.95	2.57	3.1832 (16)	122
C5—H5A···Cg2ⁱⁱⁱ	0.95	2.68	3.5453 (15)	152
C17—H17B···Cg1^iv	0.99	2.70	3.5488 (14)	144

Symmetry codes: (i) −x+2, −y+1, −z+1; (ii) −x+1, −y+2, −z+2; (iii) x+1, y, z; (iv) x−1, y, z.

Experimental details

Crystal data
Chemical formula	C₁₉H₁₈BrFN₂O
M_r	389.26
Crystal system, space group	Triclinic, P1
Temperature (K)	100
a, b, c (Å)	6.7502 (3), 10.1253 (5), 13.7792 (8)
α, β, γ (°)	105.354 (1), 98.976 (1), 107.369 (1)
V (Å³)	838.01 (7)
Z	2
Radiation type	Mo Kα
µ (mm⁻¹)	2.47
Crystal size (mm)	0.28 × 0.23 × 0.08

Data collection
Diffractometer	Bruker SMART APEXII DUO CCD diffractometer
Absorption correction	Multi-scan (SADABS; Bruker, 2009)
T_min, T_max	0.546, 0.823
No. of measured, independent and observed [I > 2σ(I)] reflections	17838, 4816, 4458
R_int	0.023
(sin θ/λ)_max (Å⁻¹)	0.703

Refinement
R[F² > 2σ(F²)], wR(F²), S	0.025, 0.066, 1.06
No. of reflections	4816
No. of parameters	218
H-atom treatment	H-atom parameters constrained
Δρ_max, Δρ_min (e Å⁻³)	0.49, −0.63

Computer programs: APEX2 (Bruker, 2009), SAINT (Bruker, 2009), SHELXTL (Sheldrick, 2008) and PLATON (Spek, 2009).

Hydrogen-bond geometry (Å, º) top

D—H···A	D—H	H···A	D···A	D—H···A
C11—H11A···F1ⁱ	0.95	2.37	3.1873 (17)	144
C14—H14A···O1ⁱⁱ	0.95	2.57	3.1832 (16)	122
C5—H5A···Cg2ⁱⁱⁱ	0.95	2.68	3.5453 (15)	152
C17—H17B···Cg1^iv	0.99	2.70	3.5488 (14)	144

Symmetry codes: (i) −x+2, −y+1, −z+1; (ii) −x+1, −y+2, −z+2; (iii) x+1, y, z; (iv) x−1, y, z.

Footnotes

‡Thomson Reuters ResearcherID: A-3561-2009.

§Thomson Reuters ResearcherID: C-7581-2009.

Acknowledgements

HKF and WSL thank Universiti Sains Malaysia (USM) for the Research University Grant (No. 1001/PFIZIK/811160). WSL also thanks the Malaysian government and USM for the post of Research Officer under the Research University Grant (No. 1001/PFIZIK/811160). BN thanks the UGC for financial assistance through SAP and BSR one time grant for the purchase of chemicals.

References

Bruker (2009). APEX2, SAINT and SADABS. Bruker AXS Inc., Madison, Wisconsin, USA. Google Scholar
Cosier, J. & Glazer, A. M. (1986). J. Appl. Cryst. 19, 105–107. CrossRef CAS Web of Science IUCr Journals Google Scholar
Fun, H.-K., Hemamalini, M., Samshuddin, S., Narayana, B. & Yathirajan, H. S. (2010). Acta Cryst. E66, o582–o583. Web of Science CSD CrossRef CAS IUCr Journals Google Scholar
Fun, H.-K., Loh, W.-S., Sapnakumari, M., Narayana, B. & Sarojini, B. K. (2012). Acta Cryst. E68, o2586. CSD CrossRef IUCr Journals Google Scholar
Fun, H.-K., Quah, C. K., Samshuddin, S., Narayana, B. & Sarojini, B. K. (2012). Acta Cryst. E68, o975. CSD CrossRef IUCr Journals Google Scholar
Samshuddin, S., Narayana, B., Baktir, Z., Akkurt, M. & Yathirajan, H. S. (2011). Der Pharma Chem. 3, 487–493. CAS Google Scholar
Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. Web of Science CrossRef CAS IUCr Journals Google Scholar
Spek, A. L. (2009). Acta Cryst. D65, 148–155. Web of Science CrossRef CAS IUCr Journals Google Scholar

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