Crystal structure of N-(tert-but­­oxy­carbon­yl)glycyl-(Z)-β-bromo­de­hydro­alanine methyl ester [Boc–Gly–(β-Br)^(Z)ΔAla–OMe]

The title compound, C₁₁H₁₇BrN₂O₅, is a de­hydro­amino acid with a C=C bond between the α- and β-C atoms. The amino acid residues are linked trans to each other and there are no strong intra­molecular hydrogen bonds. The torsion angles indicate a non-helical conformation of the mol­ecule. The dipeptide folding is influenced by an inter­molecular N—H⋯O hydrogen bond and also minimizes steric repulsion. In the crystal, mol­ecules are linked by strong N—H⋯O hydrogen bonds, generating (001) sheets. The sheets are linked by weak C—H⋯O and C—H⋯Br bonds and short Br⋯Br [3.4149 (3) Å] inter­actions.

1. Chemical context

De­hydro­amino acids are analogues of amino acids characterized by the presence of an unsaturated doubled bound between the α- and β-carbon atoms in their structure. These compounds were found to be components of natural products (Bonauer et al., 2006), with lanti­biotics being especially important since they are an important class of natural bacteriocins produced by Gram-positive bacteria (Willey & van der Donk, 2007). The development of synthetic methods for the preparation of de­hydro­peptides allows researchers to search for their practical applications and to use them as substrates for the production of peptidomimetics. One of the inter­esting classes of such mimetics are β-bromo-de­hydro­amino acids and their derivatives, which are usually obtained by radical halogenation of de­hydro­amino acids using N-bromo­succinimide (NBS). This reaction proceeds in two steps, namely by halogenation of de­hydro­amino acids, which gives α-bromo-imines, followed by tautomerization to the desired products upon treatment with an amine (Coleman & Carpenter, 1993; Zhang et al., 2002). β-Bromo-de­hydro­amino acid derivatives are useful substrates in coupling reactions with alkynes (Singh et al., 2003) or organoboranes (Collier et al. 2002; Zhang et al., 2002). Further asymmetric hydrogenation of their double bound allows non-proteinogenic α-amino acids and their derivatives to be obtained. Another important reaction of β-bromo-α,β-de­hydro­amino acid derivatives in drug research is their coupling cyclization in which oxazole derivatives are produced (Liu et al., 2014).

2. Structural commentary

The mol­ecular structure of the title compound, (I), is shown in Fig. 1. The amino acids in the compound are linked trans to each other. The ω² angle (C9—C10—N12—C13) is 175.79 (16)°, while ω³ (O5—C6—N8—C9) is 176.12 (15)°. There are no strong intra­molecular hydrogen bonds. The values of the φ^2,3 and ψ^2,3 angles corresponds to a non-helical conformation (Venkatachalam, 1968). The dipeptide folds accordingly to the inter­molecular N—H⋯O-type hydrogen bonds. The β-bromo-de­hydro­alanine moiety shows typical geometrical tendencies. The C10—N12 bond is longer [1.366 (2) Å] than a typical bond in alanine, while the N12—C13 bond is shorter [1.406 (2) Å]. This effect is common for other de­hydro-residues (Ajó et al., 1979; Pieroni et al. 1975; Rzeszotarska et al., 2002; Jain & Chauhan, 1996). This indicates conjugation between the side chain of de­hydro­alanine and the peptide bond. The torsion angles around the Br(H)C=C grouping are −0.9 (3) and −174.28 (13)° (N12—C13—C14—Br15 and C16—C13—C14—Br15, respectively), meaning the stereochemistry about the bond is especially planar. This is consistent with the nature of an sp²-hybridized carbon on C13. The valance angles around the de­hydro­alanine group show some unusual values, especially N12—C13—C14 [124.27 (18)°], which may correspond to the presence of the bromine atom in the structure. The other angles are normal, as the backbone of the mol­ecule is folded to minimize steric repulsion. The Boc group features two short intra­molecular C—H⋯O contacts

Figure 1 The mol­ecular structure of Boc–Gly–(β-Br)^(Z)ΔAla–OMe along with selected intra­molecular hydrogen bonds (dashed lines), drawn with 50% displacement ellipsoids.

3. Supra­molecular features

In the crystal, mol­ecules form two strong twin N—H⋯O (N8—H8A⋯O17ⁱ and N12—H12A⋯O7ⁱⁱ) and one weak accompanying C9—H9A⋯O11ⁱ hydrogen bonds (Fig. 1 and Table 1), forming infinite sheets in the (001) plane [symmetry codes: (i) −x + 2, −y, −z + 1 and (ii) −x + 3, −y, −z + 1]. The sheets are connected to each other by weak C14—H14A⋯O11ⁱⁱⁱ and C19—H19B⋯Br15ⁱⁱⁱ hydrogen bonds and one Br⋯Br^iv [3.4149 (3) Å] halogen bond (Fig. 2) of type I (Mukherjee & Desiraju, 2014) [symmetry codes: (iii) −x + 2, −y + 1, −z + 1; (iv) −x + 3, −y + 1, −z + 1].

Table 1
Hydrogen-bond geometry (Å, °)

D—H⋯A	D—H	H⋯A	D⋯A	D—H⋯A
C2—H2A⋯O7	0.96	2.51	3.058 (2)	116
C3—H3A⋯O7	0.96	2.44	3.007 (3)	117
N8—H8A⋯O17^i	0.86	2.19	3.018 (2)	162
C9—H9A⋯O11^i	0.97	2.61	3.255 (2)	124
N12—H12A⋯O7^ii	0.86	2.04	2.901 (2)	174
C14—H14A⋯O11^iii	0.93	2.43	3.095 (2)	129
C19—H19B⋯Br15^iii	0.96	3.14	3.668 (3)	117
Symmetry codes: (i) -x+2, -y, -z+1; (ii) -x+3, -y, -z+1; (iii) -x+2, -y+1, -z+1.

Figure 2 A packing diagram of (I), viewed along the b axis, showing the inter­molecular hydrogen-bonding scheme (dashed lines).

4. Synthesis and crystallization

Boc–Gly–ΔAla and its methyl ester were prepared according to the methodology described by Makowski et al. (1985) and Cossec et al. (2008). The β-bromo-vinyl derivative was obtained based on a procedure described previously (Bull et al., 2007). For this purpose 0.129 g (0.5 mM) of Boc–Gly–ΔAla–OMe was dissolved in 2.5 ml of di­chloro­methane and cooled to 193 K. Then, bromine 0.027 ml (0.5 mM) was added. The solution was stirred over 10 minutes followed by addition of tri­ethyl­amine 0.210 ml (1.5 mM). After 15 minutes, the mixture was quenched with 20 ml of saturated aqueous NaHCO₃ and warmed to room temperature. The product was extracted by di­chloro­methane (3 × 15 ml). The organic layer was washed with brine (3 × 10 ml) and dried over anhydrous Na₂SO₄. Evaporation of the solvent at reduced pressure gave 0.119 g (0.35 mM) of crude product (70% yield). Recrystal­lization was performed from mixtures of diethyl ether/ethyl acetate­(2:1)/hexane solvents, yielding irregular colourless crystals. It is worth noting that in the case of our study, the formation of only the Z isomer was observed while in the preceding paper, the bromination of de­hydro­alanine-containing compound gave the E isomer. ¹H NMR (400 MHz, DMSO) δ 1.38 (s, (s, 9H, C—H_{3 t-Boc}), 3.67 (s, 3H, O—CH₃), 3.69 (d, J = 6.2 Hz, 2H, C—H_{2 Gly}), 7.05 (t, J = 6.2 Hz, 1H, N—H_Gly), 7.30 (s, 1H, C=CHBr), 9.63 (s, 1H, N—H_{β-Br–ΔAla}). ¹³C NMR (101 MHz, DMSO) δ 28.21, 42.79, 52.54, 78.12, 113.26, 132.88, 155.80, 162.63, 168.80. Melting point = 386–388 K.

5. Refinement

Crystal data, data collection and structure refinement details are summarized in Table 2. All H atoms were positioned geometrically and treated as riding on their parent C or N atoms: for methyl groups, C—H = 0.96 Å and U_iso (H) = 1.5U_eq(C); for N atoms, N—H = 0.86 Å and U_iso (H) = 1.2U_eq(C); for secondary C atoms, C—H = 0.97 Å and U_iso (H) = 1.2U_eq(C), with no refinement of their parameters.

Table 2
Experimental details

Crystal data
Chemical formula	C11H17BrN2O5
Mr	337.17
Crystal system, space group	Triclinic, P
Temperature (K)	100
a, b, c (Å)	9.0431 (4), 9.3160 (4), 9.7540 (4)
α, β, γ (°)	83.381 (3), 75.420 (4), 64.863 (4)
V (Å^3)	719.92 (6)
Z	2
Radiation type	Mo Kα
μ (mm^−1)	2.87
Crystal size (mm)	0.30 × 0.25 × 0.20
Data collection
Diffractometer	Oxford Diffraction Xcalibur
Absorption correction	Multi-scan (CrysAlis RED; Oxford Diffraction, 2010)
Tmin, Tmax	0.655, 1.000
No. of measured, independent and observed [I > 2σ(I)] reflections	4860, 2780, 2490
Rint	0.016
(sin θ/λ)max (Å^−1)	0.617
Refinement
R[F^2 > 2σ(F^2)], wR(F^2), S	0.024, 0.066, 1.06
No. of reflections	2780
No. of parameters	172
H-atom treatment	H-atom parameters constrained
Δρmax, Δρmin (e Å^−3)	0.53, −0.43
Computer programs: CrysAlis CCD and CrysAlis RED (Oxford Diffraction, 2010), SHELXS2014 and SHELXL2014 (Sheldrick, 2008), SHELXTL (Sheldrick, 2008).

Supporting information

S1. Chemical context

De­hydro­amino acids are analogues of amino acids characterized by the presence of an unsaturated doubled bound between the α- and β-carbon atoms in their structure. These compounds were found to be components of natural products (Bonauer et al., 2006), with lanti­biotics being especially important since they are an important class of natural bacteriocins produced by Gram-positive bacteria (Willey & van der Donk, 2007). The development of synthetic methods for the preparation of de­hydro­peptides allows researchers to search for their practical applications and to use them as substrates for the production of peptidomimetics. One of the inter­esting classes of such mimetics are β-bromo-de­hydro­amino acids and their derivatives, which are usually obtained by radical halogenation of de­hydro­amino acids using N-bromo­succinimide (NBS). This reaction proceeds in two steps, namely by halogenation of de­hydro­amino acids, which gives α-bromo-imines, followed by tautomerization to the desired products upon treatment with an amine (Coleman & Carpenter, 1993; Zhang et al., 2002). β-Bromo-de­hydro­amino acid derivatives are useful substrates in coupling reactions with alkynes (Singh et al., 2003) or organoboranes (Collier et al. 2002; Zhang et al., 2002). Further asymmetric hydrogenation of their double bound allows non-proteinogenic α-amino acids and their derivatives to be obtained. Another important reaction of β-bromo-α,β-de­hydro­amino acid derivatives in drug research is their coupling cyclization in which oxazole derivatives are produced (Liu et al., 2014).

S2. Structural commentary

The molecular structure of the title compound, (I), is shown in Fig. 1. The amino acids in the compound are linked trans to each other. The ω² angle (C9—C10—N12—C13) is 175.79 (16)°, while ω³ (O5—C6—N8—C9) is 176.12 (15)°. There are no strong intra­molecular hydrogen bonds. The values of the ϕ^2,3 and ψ^2,3 angles corresponds to a non-helical conformation (Venkatachalam, 1968). The dipeptide folds accordingly to the inter­molecular N—H···O-type hydrogen bonds. The β-bromo-de­hydro­alanine moiety shows typical geometrical tendencies. The C10—N12 bond is longer [1.366 (2) Å] than a typical bond in alanine, while the N12—C13 bond is shorter [1.406 (2) Å]. This effect is common for other de­hydro-residues (Ajó et al., 1979; Pieroni et al. 1975; Rzeszotarska et al., 2002; Jain & Chauhan, 1996). This indicates conjugation between the side chain of de­hydro­alanine and the peptide bond. The torsion angles around the Br(H)C═ C grouping are -0.9 (3) and -174.28 (13)° (N12—C13—C14—Br15 and C16—C13—C14—Br15, respectively), meaning the stereochemistry about the bond is especially planar. This is consistent with the nature of an sp²-hybridized carbon on C13. The valance angles around the de­hydro­alanine group show some unusual values, especially N12—C13—C14 [124.27 (18)°], which may correspond to the presence of the bromine atom in the structure. The other angles are normal, as the backbone of the molecule is folded to minimize steric repulsion. The Boc group features two short intra­molecular C—H···O contacts

S3. Supra­molecular features

In the crystal, molecules form two strong twin N—H···O (N8—H8A···O17ⁱ and N12—H12A···O7ⁱⁱ) and one weak accompanying C9—H9A···O11ⁱ hydrogen bonds (Fig. 1), forming infinite sheets in the (001) plane [symmetry codes: (i) -x + 2, -y, -z + 1 and (ii) -x + 3, -y, -z + 1]. The sheets are connected to each other by weak C14—H14A···O11ⁱⁱⁱ and C19—H19B···Br15ⁱⁱⁱ hydrogen bonds and one Br···Br^iv [3.4149 (3) Å] halogen bond of type I (Mukherjee & Desiraju, 2014) [symmetry codes: (iii) -x + 2, -y + 1, -z + 1; (iv) -x + 3, -y + 1, -z + 1].

S4. Synthesis and crystallization

Boc–Gly–ΔAla and its methyl ester were prepared according to the methodology described by Makowski et al. (1985) and Cossec et al. (2008). The β-bromo-vinyl derivative was obtained based on a procedure described previously (Bull et al., 2007). For this purpose 0.129 g (0.5 mM) of Boc–Gly–ΔAla–OMe was dissolved in 2.5 ml of di­chloro­methane and cooled to 193 K. Then, bromine 0.027 ml (0.5 mM) was added. The solution was stirred over 10 minutes followed by addition of tri­ethyl­amine 0.210 ml (1.5 mM). After 15 minutes, the mixture was quenched with 20 ml of saturated aqueous NaHCO₃ and warmed to room temperature. The product was extracted by di­chloro­methane (3 × 15 ml). The organic layer was washed with brine (3 × 10 ml) and dried over anhydrous Na₂SO₄. Evaporation of the solvent at reduced pressure gave 0.119 g (0.35 mM) of crude product (70% yield). Recrystallization was performed from mixtures of di­ethyl ether/ethyl acetate­(2:1)/hexane solvents, yielding irregular colourless crystals. It is worth noting that in the case of our study, the formation of only the Z isomer was observed while in the preceding paper, the bromination of de­hydro­alanine-containing compound gave the E isomer. ¹H NMR (400 MHz, DMSO) δ 1.38 (s, (s, 9H, C—H_{3 t-Boc}), 3.67 (s, 3H, O—CH₃), 3.69 (d, J = 6.2 Hz, 2H, C—H_{2 Gly}), 7.05 (t, J = 6.2 Hz, 1H, N—H_Gly), 7.30 (s, 1H, C═CHBr), 9.63 (s, 1H, N—H_{β-Br–ΔAla}). ¹³C NMR (101 MHz, DMSO) δ 28.21, 42.79, 52.54, 78.12, 113.26, 132.88, 155.80, 162.63, 168.80. Melting point = 386–388 K.

S5. Refinement

Crystal data, data collection and structure refinement details are summarized in Table 2. All H atoms were positioned geometrically and treated as riding on their parent C or N atoms: for methyl groups, C—H = 0.96 Å and U_iso (H) = 1.5U_eq(C); for N atoms, N—H = 0.86 Å and U_iso (H) = 1.2U_eq(C); for secondary C atoms, C—H = 0.97 Å and U_iso (H) = 1.2U_eq(C), with no refinement of their parameters.

Related literature

For general background to the use of dehydroaminoacids, see: review Bonauer et al., 2006; Coleman & Carpenter, 1993; Zhang et al., 2002; Singh et al., 2003; For a related structures, see: Ajó et al., 1979; Pieroni et al. 1975; Rzeszotarska et al., 2002 Jain & Chauhan, 1996.

Computing details

Data collection: CrysAlis CCD (Oxford Diffraction, 2010); cell refinement: CrysAlis RED (Oxford Diffraction, 2010); data reduction: CrysAlis RED (Oxford Diffraction, 2010); program(s) used to solve structure: SHELXS2014 (Sheldrick, 2008); program(s) used to refine structure: SHELXL2014 (Sheldrick, 2008); molecular graphics: SHELXTL (Sheldrick, 2008); software used to prepare material for publication: SHELXL2014 (Sheldrick, 2008).

Figures

Fig. 1. The molecular structure of Boc–Gly–(β-Br)^(Z)ΔAla–OMe along with selected intramolecular hydrogen bonds (dashed lines), drawn with 50% displacement ellipsoids.

Fig. 2. A packing diagram of (I), viewed along the b axis, showing the intermolecular hydrogen-bonding scheme (dashed lines).

N-(tert-Butoxycarbonyl)glycyl-(Z)-β-bromodehydroalanine methyl ester

Crystal data

C11H17BrN2O5	Z = 2
Mr = 337.17	F(000) = 344
Triclinic, P1	Dx = 1.555 Mg m^−3
a = 9.0431 (4) Å	Mo Kα radiation, λ = 0.71073 Å
b = 9.3160 (4) Å	Cell parameters from 4860 reflections
c = 9.7540 (4) Å	θ = 3.2–26.0°
α = 83.381 (3)°	µ = 2.87 mm^−1
β = 75.420 (4)°	T = 100 K
γ = 64.863 (4)°	Irregular, colourless
V = 719.92 (6) Å^3	0.30 × 0.25 × 0.20 mm

Data collection

Oxford Diffraction Xcalibur diffractometer	2780 independent reflections
Radiation source: fine-focus sealed tube	2490 reflections with I > 2σ(I)
Graphite monochromator	Rint = 0.016
Detector resolution: 1024 pixels mm^-1	θmax = 26.0°, θmin = 3.2°
ω scan	h = −8→11
Absorption correction: multi-scan (CrysAlis RED; Oxford Diffraction, 2010)	k = −10→11
Tmin = 0.655, Tmax = 1.000	l = −12→12
4860 measured reflections

Refinement

Refinement on F^2	0 restraints
Least-squares matrix: full	Hydrogen site location: inferred from neighbouring sites
R[F^2 > 2σ(F^2)] = 0.024	H-atom parameters constrained
wR(F^2) = 0.066	w = 1/[σ^2(Fo^2) + (0.0444P)^2] where P = (Fo^2 + 2Fc^2)/3
S = 1.06	(Δ/σ)max = 0.001
2780 reflections	Δρmax = 0.53 e Å^−3
172 parameters	Δρmin = −0.43 e Å^−3

Special details

Experimental. CrysAlis RED, Oxford Diffraction Ltd., Version 1.171.33.57 (release 26-01-2010 CrysAlis171 .NET) (compiled Jan 26 2010,14:36:55) Empirical absorption correction using spherical harmonics, implemented in SCALE3 ABSPACK scaling algorithm.

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.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Ų)

	x	y	z	Uiso*/Ueq
C1	1.2957 (3)	−0.1495 (2)	0.9892 (2)	0.0186 (4)
C2	1.4783 (3)	−0.2662 (3)	0.9655 (2)	0.0248 (5)
H2A	1.5455	−0.2243	0.8952	0.037*
H2B	1.4904	−0.3651	0.9336	0.037*
H2C	1.5146	−0.2830	1.0527	0.037*
C3	1.2675 (3)	0.0136 (3)	1.0284 (2)	0.0291 (5)
H3A	1.3374	0.0518	0.9572	0.044*
H3B	1.2952	0.0083	1.1182	0.044*
H3C	1.1520	0.0844	1.0348	0.044*
C4	1.1870 (3)	−0.2140 (3)	1.1000 (2)	0.0313 (5)
H4A	1.0720	−0.1387	1.1146	0.047*
H4B	1.2228	−0.2316	1.1875	0.047*
H4C	1.1975	−0.3122	1.0679	0.047*
O5	1.23184 (17)	−0.14194 (16)	0.86239 (14)	0.0186 (3)
C6	1.2959 (2)	−0.0915 (2)	0.7363 (2)	0.0144 (4)
O7	1.40332 (16)	−0.03851 (15)	0.71486 (14)	0.0161 (3)
N8	1.2267 (2)	−0.10813 (19)	0.63638 (17)	0.0155 (3)
H8A	1.1573	−0.1522	0.6578	0.019*
C9	1.2670 (2)	−0.0531 (2)	0.49289 (19)	0.0149 (4)
H9A	1.2529	−0.1157	0.4283	0.018*
H9B	1.3835	−0.0685	0.4688	0.018*
C10	1.1567 (2)	0.1209 (2)	0.47430 (19)	0.0143 (4)
O11	1.00831 (16)	0.18140 (15)	0.53245 (14)	0.0179 (3)
N12	1.23628 (19)	0.20273 (18)	0.38410 (17)	0.0146 (3)
H12A	1.3421	0.1556	0.3484	0.017*
C13	1.1490 (2)	0.3623 (2)	0.34831 (19)	0.0136 (4)
C14	1.1990 (2)	0.4770 (2)	0.3536 (2)	0.0164 (4)
H14A	1.1341	0.5792	0.3266	0.020*
Br15	1.39326 (2)	0.44202 (2)	0.41252 (2)	0.02292 (9)
C16	1.0010 (2)	0.4006 (2)	0.2866 (2)	0.0163 (4)
O17	0.97138 (18)	0.30286 (17)	0.24167 (15)	0.0210 (3)
O18	0.90913 (18)	0.55685 (16)	0.28281 (16)	0.0239 (3)
C19	0.7741 (3)	0.6065 (3)	0.2098 (3)	0.0324 (5)
H19A	0.7155	0.7199	0.2129	0.049*
H19B	0.6979	0.5594	0.2552	0.049*
H19C	0.8193	0.5731	0.1130	0.049*

Atomic displacement parameters (Ų)

	U^11	U^22	U^33	U^12	U^13	U^23
C1	0.0226 (10)	0.0227 (10)	0.0121 (9)	−0.0104 (9)	−0.0065 (8)	0.0034 (8)
C2	0.0266 (11)	0.0256 (11)	0.0202 (11)	−0.0075 (9)	−0.0108 (9)	0.0066 (9)
C3	0.0397 (14)	0.0268 (12)	0.0204 (11)	−0.0129 (10)	−0.0070 (10)	−0.0014 (9)
C4	0.0369 (13)	0.0432 (14)	0.0172 (11)	−0.0222 (11)	−0.0058 (9)	0.0088 (10)
O5	0.0202 (7)	0.0248 (7)	0.0141 (7)	−0.0133 (6)	−0.0061 (6)	0.0077 (6)
C6	0.0131 (9)	0.0102 (9)	0.0158 (10)	−0.0021 (7)	−0.0029 (7)	0.0040 (7)
O7	0.0173 (7)	0.0166 (7)	0.0174 (7)	−0.0100 (6)	−0.0049 (5)	0.0028 (5)
N8	0.0169 (8)	0.0164 (8)	0.0167 (8)	−0.0105 (7)	−0.0063 (7)	0.0074 (7)
C9	0.0175 (9)	0.0136 (9)	0.0136 (9)	−0.0069 (8)	−0.0042 (7)	0.0038 (7)
C10	0.0187 (10)	0.0152 (9)	0.0126 (9)	−0.0091 (8)	−0.0065 (8)	0.0017 (7)
O11	0.0153 (7)	0.0149 (7)	0.0198 (7)	−0.0054 (6)	−0.0009 (6)	0.0035 (5)
N12	0.0120 (8)	0.0130 (8)	0.0169 (8)	−0.0050 (6)	−0.0019 (6)	0.0034 (6)
C13	0.0147 (9)	0.0143 (9)	0.0115 (9)	−0.0069 (8)	−0.0019 (7)	0.0031 (7)
C14	0.0137 (9)	0.0164 (9)	0.0191 (10)	−0.0061 (8)	−0.0049 (8)	0.0021 (8)
Br15	0.01942 (12)	0.02164 (12)	0.03230 (14)	−0.01022 (9)	−0.00996 (9)	−0.00138 (8)
C16	0.0181 (10)	0.0171 (10)	0.0130 (9)	−0.0083 (8)	−0.0032 (8)	0.0060 (8)
O17	0.0250 (8)	0.0209 (7)	0.0224 (8)	−0.0129 (6)	−0.0093 (6)	0.0028 (6)
O18	0.0222 (7)	0.0168 (7)	0.0346 (9)	−0.0061 (6)	−0.0164 (6)	0.0071 (6)
C19	0.0287 (12)	0.0290 (12)	0.0417 (14)	−0.0095 (10)	−0.0229 (11)	0.0157 (10)

Geometric parameters (Å, º)

C1—O5	1.474 (2)	C9—C10	1.518 (2)
C1—C3	1.508 (3)	C9—H9A	0.9700
C1—C2	1.517 (3)	C9—H9B	0.9700
C1—C4	1.521 (3)	C10—O11	1.220 (2)
C2—H2A	0.9600	C10—N12	1.366 (2)
C2—H2B	0.9600	N12—C13	1.406 (2)
C2—H2C	0.9600	N12—H12A	0.8600
C3—H3A	0.9600	C13—C14	1.335 (3)
C3—H3B	0.9600	C13—C16	1.494 (3)
C3—H3C	0.9600	C14—Br15	1.8715 (19)
C4—H4A	0.9600	C14—H14A	0.9300
C4—H4B	0.9600	C16—O17	1.204 (2)
C4—H4C	0.9600	C16—O18	1.337 (2)
O5—C6	1.345 (2)	O18—C19	1.447 (2)
C6—O7	1.229 (2)	C19—H19A	0.9600
C6—N8	1.338 (2)	C19—H19B	0.9600
N8—C9	1.446 (2)	C19—H19C	0.9600
N8—H8A	0.8600
O5—C1—C3	110.80 (16)	C9—N8—H8A	119.5
O5—C1—C2	109.75 (16)	N8—C9—C10	111.87 (15)
C3—C1—C2	112.96 (18)	N8—C9—H9A	109.2
O5—C1—C4	101.56 (15)	C10—C9—H9A	109.2
C3—C1—C4	110.90 (18)	N8—C9—H9B	109.2
C2—C1—C4	110.29 (18)	C10—C9—H9B	109.2
C1—C2—H2A	109.5	H9A—C9—H9B	107.9
C1—C2—H2B	109.5	O11—C10—N12	122.87 (17)
H2A—C2—H2B	109.5	O11—C10—C9	122.69 (16)
C1—C2—H2C	109.5	N12—C10—C9	114.41 (16)
H2A—C2—H2C	109.5	C10—N12—C13	121.43 (16)
H2B—C2—H2C	109.5	C10—N12—H12A	119.3
C1—C3—H3A	109.5	C13—N12—H12A	119.3
C1—C3—H3B	109.5	C14—C13—N12	124.27 (18)
H3A—C3—H3B	109.5	C14—C13—C16	118.50 (17)
C1—C3—H3C	109.5	N12—C13—C16	116.92 (16)
H3A—C3—H3C	109.5	C13—C14—Br15	123.17 (15)
H3B—C3—H3C	109.5	C13—C14—H14A	118.4
C1—C4—H4A	109.5	Br15—C14—H14A	118.4
C1—C4—H4B	109.5	O17—C16—O18	124.26 (18)
H4A—C4—H4B	109.5	O17—C16—C13	124.08 (18)
C1—C4—H4C	109.5	O18—C16—C13	111.61 (16)
H4A—C4—H4C	109.5	C16—O18—C19	115.57 (16)
H4B—C4—H4C	109.5	O18—C19—H19A	109.5
C6—O5—C1	121.71 (14)	O18—C19—H19B	109.5
O7—C6—N8	124.52 (17)	H19A—C19—H19B	109.5
O7—C6—O5	125.30 (17)	O18—C19—H19C	109.5
N8—C6—O5	110.18 (16)	H19A—C19—H19C	109.5
C6—N8—C9	120.96 (15)	H19B—C19—H19C	109.5
C6—N8—H8A	119.5
C3—C1—O5—C6	62.8 (2)	C9—C10—N12—C13	175.79 (16)
C2—C1—O5—C6	−62.6 (2)	C10—N12—C13—C14	130.6 (2)
C4—C1—O5—C6	−179.35 (17)	C10—N12—C13—C16	−55.9 (2)
C1—O5—C6—O7	−4.7 (3)	N12—C13—C14—Br15	−0.9 (3)
C1—O5—C6—N8	174.87 (15)	C16—C13—C14—Br15	−174.28 (13)
O7—C6—N8—C9	−4.3 (3)	C14—C13—C16—O17	159.29 (19)
O5—C6—N8—C9	176.12 (15)	N12—C13—C16—O17	−14.6 (3)
C6—N8—C9—C10	−86.1 (2)	C14—C13—C16—O18	−18.4 (2)
N8—C9—C10—O11	−38.0 (3)	N12—C13—C16—O18	167.72 (16)
N8—C9—C10—N12	143.70 (16)	O17—C16—O18—C19	−4.6 (3)
O11—C10—N12—C13	−2.5 (3)	C13—C16—O18—C19	173.12 (17)

Hydrogen-bond geometry (Å, º)

D—H···A	D—H	H···A	D···A	D—H···A
C2—H2A···O7	0.96	2.51	3.058 (2)	116
C3—H3A···O7	0.96	2.44	3.007 (3)	117
N8—H8A···O17^i	0.86	2.19	3.018 (2)	162
C9—H9A···O11^i	0.97	2.61	3.255 (2)	124
N12—H12A···O7^ii	0.86	2.04	2.901 (2)	174
C14—H14A···O11^iii	0.93	2.43	3.095 (2)	129
C19—H19B···Br15^iii	0.96	3.14	3.668 (3)	117

Symmetry codes: (i) −x+2, −y, −z+1; (ii) −x+3, −y, −z+1; (iii) −x+2, −y+1, −z+1.