Literature DB >> 23424445

N-(7-Dibromo-methyl-5-methyl-1,8-naphthyridin-2-yl)acetamide-pyrrolidine-2,5-dione (1/1).

Gao-Zhang Gou1, Jun-Feng Kou, Qing-Di Zhou, Shao-Ming Chi.   

Abstract

In the title co-crystal, C(12)H(11)Br(2)N(3)O·C(4)H(5)NO(2), the naphthyridine derivative and the pyrrolidine-2,5-dione mol-ecules have crystallographic mirror-plane symmetry with all non-H atoms, except the Br atom, located on the mirror plane. In the crystal, N-H⋯N, N-H⋯O and C-H⋯O hydrogen bonds link the mol-ecules into heterodimers. These dimers are further linked into a one-dimensional structure along [010] by weak C-Br⋯O inter-actions [Br⋯O = 3.028 (5) Å and C-Br⋯O = 158.52 (4)°].

Entities:  

Year:  2013        PMID: 23424445      PMCID: PMC3569222          DOI: 10.1107/S1600536812051112

Source DB:  PubMed          Journal:  Acta Crystallogr Sect E Struct Rep Online        ISSN: 1600-5368


Related literature

For coordination properties of 1,8-naphthyridine ligands, see: Gan et al. (2011 ▶); Chang et al. (2011 ▶); Das et al. (2012 ▶); Li et al. (2011 ▶). For similar structures, see: Li et al. (2011 ▶). For applications of similar compounds, see: Samadi et al. (2011 ▶); Li et al. (2012 ▶); Tanaka et al. (2012 ▶). For information on their synthesis, see: Henry & Hammond (1977 ▶); Wang et al. (2008 ▶).

Experimental

Crystal data

C12H11Br2N3O·C4H5NO2 M = 472.15 Monoclinic, a = 11.537 (2) Å b = 7.0093 (14) Å c = 11.632 (2) Å β = 106.57 (3)° V = 901.6 (3) Å3 Z = 2 Mo Kα radiation μ = 4.52 mm−1 T = 293 K 0.21 × 0.19 × 0.18 mm

Data collection

Rigaku R-AXIS RAPID diffractometer Absorption correction: multi-scan (ABSCOR; Higashi, 1995 ▶) T min = 0.450, T max = 0.497 7056 measured reflections 1723 independent reflections 1220 reflections with I > 2σ(I) R int = 0.042

Refinement

R[F 2 > 2σ(F 2)] = 0.051 wR(F 2) = 0.164 S = 1.12 1723 reflections 148 parameters H-atom parameters constrained Δρmax = 0.72 e Å−3 Δρmin = −0.92 e Å−3 Data collection: PROCESS-AUTO (Rigaku, 1998 ▶); cell refinement: PROCESS-AUTO; data reduction: CrystalClear (Rigaku/MSC, 2006 ▶); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: DIAMOND (Brandenburg,1999 ▶); software used to prepare material for publication: SHELXL97. Click here for additional data file. Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536812051112/gk2541sup1.cif Click here for additional data file. Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812051112/gk2541Isup2.hkl Click here for additional data file. Supplementary material file. DOI: 10.1107/S1600536812051112/gk2541Isup3.cml Additional supplementary materials: crystallographic information; 3D view; checkCIF report
C12H11Br2N3O·C4H5NO2F(000) = 468
Mr = 472.15Dx = 1.739 Mg m3
Monoclinic, P21/mMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ybCell parameters from 25 reflections
a = 11.537 (2) Åθ = 3.4–25.0°
b = 7.0093 (14) ŵ = 4.52 mm1
c = 11.632 (2) ÅT = 293 K
β = 106.57 (3)°Block, colourless
V = 901.6 (3) Å30.21 × 0.19 × 0.18 mm
Z = 2
Rigaku R-AXIS RAPID diffractometer1723 independent reflections
Radiation source: fine-focus sealed tube1220 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.042
ω scanθmax = 25.0°, θmin = 3.4°
Absorption correction: multi-scan (ABSCOR; Higashi, 1995)h = −13→13
Tmin = 0.450, Tmax = 0.497k = −8→7
7056 measured reflectionsl = −13→13
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.051Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.164H-atom parameters constrained
S = 1.12w = 1/[σ2(Fo2) + (0.0757P)2 + 1.6111P] where P = (Fo2 + 2Fc2)/3
1723 reflections(Δ/σ)max < 0.001
148 parametersΔρmax = 0.72 e Å3
0 restraintsΔρmin = −0.92 e Å3
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.
xyzUiso*/Ueq
C10.5310 (7)0.25000.7838 (6)0.0437 (17)
C20.4522 (7)0.25000.8575 (7)0.0486 (18)
H2A0.36890.25000.82260.058*
C30.4977 (7)0.25000.9803 (6)0.0452 (17)
C40.6257 (7)0.25001.0284 (6)0.0405 (16)
C50.6882 (7)0.25001.1520 (6)0.0482 (18)
H5A0.64460.25001.20800.058*
C60.8109 (7)0.25001.1903 (7)0.053 (2)
H6A0.85180.25001.27170.063*
C70.8749 (6)0.25001.1028 (6)0.0456 (18)
C80.6974 (7)0.25000.9487 (6)0.0415 (16)
C90.4859 (8)0.25000.6506 (7)0.058 (2)
H9A0.55540.25000.61800.069*
C100.4146 (7)0.25001.0597 (7)0.0491 (18)
H10A0.33190.25001.01120.074*
H10B0.42980.13821.10940.074*
C111.0841 (7)0.25001.2427 (7)0.055 (2)
C121.2128 (7)0.25001.2408 (8)0.067 (2)
H12A1.26520.25001.32140.101*
H12B1.22790.13821.19970.101*
C130.0377 (8)0.25000.8080 (8)0.057 (2)
C140.0885 (8)0.25000.7021 (8)0.069 (2)
H14A0.13680.13840.70230.082*
C15−0.0232 (9)0.25000.5948 (8)0.080 (3)
H15A−0.02510.13870.54630.095*
C16−0.1280 (8)0.25000.6435 (8)0.056 (2)
N10.6503 (6)0.25000.8271 (5)0.0477 (15)
N20.8206 (6)0.25000.9860 (5)0.0461 (15)
N31.0008 (6)0.25001.1320 (5)0.0524 (16)
H3A1.03030.25001.07190.063*
N4−0.0857 (6)0.25000.7663 (5)0.0502 (16)
H4A−0.13220.25000.81240.060*
O11.0553 (6)0.25001.3339 (5)0.093 (3)
O20.0955 (5)0.25000.9136 (5)0.0759 (19)
O3−0.2342 (6)0.25000.5882 (6)0.081 (2)
Br10.38805 (7)0.02689 (12)0.59139 (6)0.0801 (4)
U11U22U33U12U13U23
C10.041 (4)0.052 (4)0.042 (4)0.0000.018 (3)0.000
C20.043 (4)0.060 (5)0.045 (4)0.0000.018 (3)0.000
C30.045 (4)0.048 (4)0.050 (4)0.0000.025 (4)0.000
C40.044 (4)0.044 (4)0.039 (4)0.0000.020 (3)0.000
C50.053 (5)0.059 (5)0.041 (4)0.0000.026 (3)0.000
C60.046 (5)0.079 (6)0.036 (4)0.0000.016 (3)0.000
C70.041 (4)0.054 (4)0.044 (4)0.0000.016 (3)0.000
C80.046 (5)0.046 (4)0.035 (4)0.0000.018 (3)0.000
C90.054 (5)0.076 (6)0.047 (4)0.0000.021 (4)0.000
C100.041 (4)0.062 (5)0.051 (4)0.0000.024 (3)0.000
C110.046 (5)0.075 (6)0.041 (4)0.0000.009 (4)0.000
C120.042 (5)0.102 (7)0.057 (5)0.0000.012 (4)0.000
C130.059 (6)0.061 (5)0.058 (5)0.0000.027 (4)0.000
C140.059 (6)0.083 (6)0.074 (6)0.0000.034 (5)0.000
C150.091 (8)0.107 (8)0.052 (5)0.0000.039 (5)0.000
C160.054 (5)0.061 (5)0.054 (5)0.0000.017 (4)0.000
N10.047 (4)0.060 (4)0.043 (3)0.0000.024 (3)0.000
N20.042 (4)0.062 (4)0.039 (3)0.0000.020 (3)0.000
N30.043 (4)0.079 (5)0.041 (3)0.0000.022 (3)0.000
N40.042 (4)0.070 (4)0.042 (3)0.0000.017 (3)0.000
O10.051 (4)0.188 (8)0.041 (3)0.0000.014 (3)0.000
O20.054 (4)0.114 (6)0.057 (4)0.0000.012 (3)0.000
O30.067 (5)0.116 (6)0.057 (4)0.0000.011 (3)0.000
Br10.0936 (7)0.0929 (6)0.0563 (5)−0.0237 (4)0.0254 (4)−0.0161 (3)
C1—N11.324 (9)C9—H9A0.9800
C1—C21.417 (10)C10—H10A0.9600
C1—C91.487 (10)C10—H10B0.9600
C2—C31.373 (10)C11—O11.199 (10)
C2—H2A0.9300C11—N31.370 (10)
C3—C41.422 (10)C11—C121.490 (11)
C3—C101.509 (9)C12—H12A0.9600
C4—C81.407 (10)C12—H12B0.9601
C4—C51.413 (10)C13—O21.220 (10)
C5—C61.357 (11)C13—N41.367 (10)
C5—H5A0.9300C13—C141.508 (12)
C6—C71.418 (10)C14—C151.517 (13)
C6—H6A0.9300C14—H14A0.9600
C7—N21.324 (9)C15—C161.474 (13)
C7—N31.394 (9)C15—H15A0.9600
C8—N11.363 (9)C16—O31.210 (10)
C8—N21.363 (9)C16—N41.372 (10)
C9—Br11.936 (5)N3—H3A0.8600
C9—Br1i1.936 (5)N4—H4A0.8600
N1—C1—C2123.1 (7)C3—C10—H10A109.8
N1—C1—C9114.4 (6)C3—C10—H10B109.3
C2—C1—C9122.4 (7)H10A—C10—H10B109.5
C3—C2—C1120.5 (7)O1—C11—N3122.3 (8)
C3—C2—H2A119.7O1—C11—C12122.8 (7)
C1—C2—H2A119.7N3—C11—C12114.9 (7)
C2—C3—C4117.1 (6)C11—C12—H12A109.8
C2—C3—C10121.0 (7)C11—C12—H12B109.3
C4—C3—C10121.9 (7)H12A—C12—H12B109.5
C8—C4—C5116.5 (7)O2—C13—N4124.9 (8)
C8—C4—C3118.7 (6)O2—C13—C14126.5 (8)
C5—C4—C3124.9 (6)N4—C13—C14108.6 (8)
C6—C5—C4121.0 (7)C13—C14—C15103.6 (7)
C6—C5—H5A119.5C13—C14—H14A111.0
C4—C5—H5A119.5C15—C14—H14A111.0
C5—C6—C7118.2 (7)C16—C15—C14106.4 (7)
C5—C6—H6A120.9C16—C15—H15A110.0
C7—C6—H6A120.9C14—C15—H15A110.8
N2—C7—N3113.9 (6)O3—C16—N4124.0 (8)
N2—C7—C6123.1 (7)O3—C16—C15127.8 (8)
N3—C7—C6123.1 (7)N4—C16—C15108.2 (8)
N1—C8—N2113.6 (6)C1—N1—C8117.3 (6)
N1—C8—C4123.3 (7)C7—N2—C8118.1 (6)
N2—C8—C4123.1 (6)C11—N3—C7129.2 (7)
C1—C9—Br1111.5 (3)C11—N3—H3A115.4
C1—C9—Br1i111.5 (3)C7—N3—H3A115.4
Br1—C9—Br1i107.7 (4)C16—N4—C13113.2 (7)
C1—C9—H9A108.7C16—N4—H4A123.4
Br1—C9—H9A108.7C13—N4—H4A123.4
Br1i—C9—H9A108.7
D—H···AD—HH···AD···AD—H···A
C6—H6A···O10.932.252.838 (10)121
C9—H9A···O3ii0.982.553.507 (11)166
N4—H4A···N1iii0.862.563.317 (9)147
N4—H4A···N2iii0.862.243.045 (8)157
N3—H3A···O2ii0.862.183.038 (9)177
Table 1

Hydrogen-bond geometry (Å, °)

D—H⋯A D—HH⋯A DA D—H⋯A
C6—H6A⋯O10.932.252.838 (10)121
C9—H9A⋯O3i 0.982.553.507 (11)166
N4—H4A⋯N1ii 0.862.563.317 (9)147
N4—H4A⋯N2ii 0.862.243.045 (8)157
N3—H3A⋯O2i 0.862.183.038 (9)177

Symmetry codes: (i) ; (ii) .

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